Mixed Ionic-Elecronic Conductive Materials For Alkali Metal Transport During Battery Cycling, and Batteries Incorporating Same

Abstract

A mixed ionic-electronic conductor (MIEC) in contact with a solid electrolyte includes a material having a bandgap less than 3 eV. The material includes an end-member phase directly connected to an alkali metal by a tie-line in an equilibrium phase diagram. The material is thermodynamically stable with a solid electrolyte. The MIEC includes plurality of open pores, formed within the MIEC, to facilitate motion of the alkali metal to at least one of store the alkali metal in the plurality of open pores or release the alkali metal from the plurality of open pores. The solid electrolyte has an ionic conductivity to ions of the alkali metal greater than 1 mS cm−1, a thickness less than 100 μm, and comprises at least one of a ceramic or a polymer.

Description

BACKGROUND

An all-solid-state battery (also referred to herein as “a solid-state battery”) includes a solid anode, a solid cathode, and a solid electrolyte disposed between the anode and the cathode. Compared to a conventional battery that uses a liquid electrolyte, a solid-state battery may achieve a higher energy density due, in part, to the solid electrolyte occupying a smaller volume, thus enabling the battery to be packaged more compactly. The energy density of the solid-state battery may be further enhanced by using a pure alkali metal anode. For example, the theoretical gravimetric capacity of pure lithium (Li) is 3861 mAh/g, which is ten times larger than the theoretical gravimetric capacity of conventional graphite anodes at 372 mAh/g. Although the density of Li (0.534 g/cm³) is lower than graphite (1.6 g/cm³), the volumetric capacity of Li (3861 mAh/g×0.534 g/cm³=2062 mAh/cm³) is still three times larger than graphite (372 mAh/g×1.6 g/cm³=600 mAh/cm³). Furthermore, the solid-state battery may be safer and more durable than a conventional battery because (1) the solid electrolyte may be formed from materials that are less flammable and less toxic than conventional liquid electrolytes and (2) the solid electrolyte does not leak unlike a liquid electrolyte.

SUMMARY

Disclosed herein is a mixed ionic-electronic conductor (MIEC). Embodiments of the MIEC include a material having a bandgap less than 3 eV. The material includes an end-member phase directly connected to an alkali metal by a tie-line in an equilibrium phase diagram. The material is thermodynamically stable with a solid electrolyte. The MIEC includes a plurality of open pores, formed within the MIEC, to facilitate motion of the alkali metal to at least one of store the alkali metal in the plurality of open pores or release the alkali metal from the plurality of open pores. The solid electrolyte is ionically conductive to ions of the alkali metal. The solid electrolyte has an ionic conductivity to ions of the alkali metal greater than 1 mS cm⁻¹, a thickness less than 100 μm, and includes at least one of a ceramic or a polymer. In one embodiment, the material may exclude any lanthanides and/or any rare earth metals.

In an embodiment, the solid electrolyte includes the polymer. The polymer may include at least one of a polyethylene, a polypropylene, a polyethylene oxide, a polyacetal, a polyolefin, a poly(alkylene oxide), a polymethacrylate, a polycarbonate, a polystyrene, a polyester, a polyamide, a polyimide, a polyamideimide, a polyarylate, a polyarylsulfone, a polyethersulfone, a polyphenylene sulfide, a polyvinyl chloride, a polysulfone, a polyimide, a polyetherimide, a polytetrafluoroethylene, a polyetherketone, a polyether etherketone, a polyether ketone, a polybenzoxazole, a polyphthalide, a polyanhydride, a polyvinyl ether, a polyvinyl thioether, a polyvinyl alcohol, a polyvinyl ketone, a polyvinyl halide, a polyvinyl nitrile, a polyvinyl ester, a polysulfonate, a polysulfide, a polythioester, a polysulfone, a polysulfonamide, a polyurea, a polyphosphazene, a polysilazane, a polyethylene terephthalate, a polybutylene terephthalate, a polyurethane, an ethylene propylene diene rubber, a polytetrafluoroethylene, a fluorinated ethylene propylene, a perfluoroalkoxyethylene, a polychlorotrifluoroethylene, or a polyvinylidene fluoride.

In another embodiment, the solid electrolyte includes the ceramic. The ceramic may include at least one of Li₇La₃Zr₂O₁₂; Li₃OX wherein X is at least one of Cl, Br, or I; Li₃SX wherein X is at least one of Cl, Br, or I; Li_1.3Al_0.3Ti_1.7(PO₄)₃; Li₆PS₅Cl; Li₁₀MP₂S₁₂ wherein M is at least one of Ge, Si, or Sn; Li₃PS₄: Li₇P₃Sn; Li₃N; Li₂S; LiBH₄: Li₃BO₃; Li₂S—P₂S₅; Li₂S—P₂S₅-L₄SiO₄; Li₂S—Ga₂S₃—GeS₂; Li₂S—Sb₂S₃—GeS₂; Li_3.25—Ge_0.25—P_0.75S₄; (La_1−xLi_x)TiO₃ wherein 0<x<1; Li₆La₂CaTa₂O₁₂; Li₆La₂ANb₂O₁₂ wherein A is at least one of Ca, Sr, or Ba; Li₆La₃Zr_1.5WO₁₂; Li_6.5La₃Zr_1.5TaO₁₂; Li_6.625Al_0.25La₃Zr₂O₁₂; Li₃BO_2.5N_0.5; Li₉SiAlO₈; Li_1+xAl_xGe_2−x(PO₄)₃; Li_1+xAl_xTi_2−x(PO₄)₃; Li_1+xTi_2−xAl_xSi_y(PO₄)_3−y wherein 0<x<1 and 0≤y<1; LiAl_xZr_2−x(PO₄)₃; LiTi_xZr_2−x(PO₄)₃ wherein 0<x<2; Li₆PS₅X, wherein X is at least one of Cl, Br, or I; Li₂In_xSc_0.666−xCl₄ wherein 0≤x≤0.666; or Li_3−xE_1−xZr_xCl₆ wherein E is at least one of Y or Er.

In another embodiment, the solid electrolyte may include at least one of a polyether solid electrolyte, a thiophosphate solid electrolyte, or a garnet-type solid electrolyte. The solid electrolyte may include the polyether solid electrolyte, which may include polyethylene oxide (PEO). The solid electrolyte may include the thiophosphate solid electrolyte, which may include Li₁₀GeP₂S₁₂ (LGPS) or Li₆PS₅X, wherein X is at least one of Cl, Br, or. The solid electrolyte may include the garnet-type solid electrolyte, which may include Li₇La₃Zr₂O (LLZO).

Another embodiment of the present technology includes an anode. The anode includes the MIEC described above, where the MIEC does not reversibly store and release the alkali metal. The anode's MIEC may have a thickness of about 0.5 μm to about 67 μm. The MIEC may have a porosity greater than 45%. The anode may have an areal capacity of about 6±0.5 mAh cm⁻². The anode may include the alkali metal. Another embodiment of the present technology includes a battery. The battery includes the anode described above and the solid electrolyte described above.

Another embodiment of the present technology includes an anode including a MIEC. The MIEC includes at least one of A_xB_y, A_xB_yC, or A_xB_yC_zD_w and a plurality of open pores, formed within the MIEC, to facilitate motion of an alkali metal to at least one of store the alkali metal in the plurality of open pores or release the alkali metal from the plurality of open pores. The MIEC does not reversibly store and release the alkali metal. The at least one of A_xB_y, A_xB_yC_z, or A_xB_yC_zD_w includes an end-member phase directly connected to an alkali metal by a tie-line in an equilibrium phase diagram. A is an alkali metal. At least one of B or C is at least one of an alkaline earth metal, a group 13 element, Sc, Y, Ti, Zr, Hf, V, Nb, Ta, Cr, Mo, W, Mn, Fe, Co, Ni, Cu, Zn, Cd, Hg, C, N, Si, Sn, Pb, Bi, La, Ce, Nd, Sm, Eu, Gd, Ho, Er, or Yb. X, y, z, and w each have a value of about 1 to about 149.

Both B and C may be at least one of an alkaline earth metal, a group 13 element, Sc, Y, Ti, Zr, Hf, V, Nb, Ta, Cr, Mo, W, Mn, Fe, Co, Ni, Cu, Zn, Cd, Hg, C, N, Si, Sn, Pb, Bi, La, Ce, Nd, Sm, Eu, Gd, Ho, Er, or Yb. B may be an alkaline earth metal. B may be a group 13 element. B may be a period 4 transition metal. B may be a period 5 transition metal. B may be a period 6 transition metal. B may be a lanthanide.

Another embodiment of the present technology includes an anode. The anode includes the MIEC described above, and a plurality of open pores, formed within the MIEC, to facilitate motion of an alkali metal to store the alkali metal in the plurality of open pores and/or release the alkali metal from the plurality of open pores. The MIEC does not reversibly store and/or release the alkali metal. The alkali metal may include at least one of lithium (Li), sodium (Na), or potassium (K).

Another embodiment of the present technology includes an anode. The anode MIEC including Ti_wAl_xC_yNi_z and a plurality of open pores, formed within the MIEC, to facilitate motion of an alkali metal to store the alkali metal in the plurality of open pores and/or release the alkali metal from the plurality of open pores. W, x, y, and z each have a value less than or equal to 8.

Another embodiment of the present technology includes a battery including the anode described above and a solid electrolyte. The solid electrolyte is coupled to a portion of the MIEC. The solid electrolyte includes polyethylene oxide (PEO).

It should be appreciated that all combinations of the foregoing concepts and additional concepts discussed in greater detail below (provided such concepts are not mutually inconsistent) are contemplated as being part of the inventive subject matter disclosed herein. In particular, all combinations of claimed subject matter appearing at the end of this disclosure are contemplated as being part of the inventive subject matter disclosed herein. It should also be appreciated that terminology explicitly employed herein that also may appear in any disclosure incorporated by reference should be accorded a meaning most consistent with the particular concepts disclosed herein.

BRIEF DESCRIPTION OF THE DRAWINGS

The skilled artisan will understand that the drawings primarily are for illustrative purposes and are not intended to limit the scope of the inventive subject matter described herein. The drawings are not necessarily to scale; in some instances, various aspects of the inventive subject matter disclosed herein may be shown exaggerated or enlarged in the drawings to facilitate an understanding of different features. In the drawings, like reference characters generally refer to like features (e.g., functionally similar and/or structurally similar elements).

FIG. 1 shows a cross-sectional view of an exemplary battery with an anode formed, in part, using a mixed ionic-electronic conductor (MIEC) shaped as a honeycomb structure.

FIG. 2 shows a tubule formed by the MIEC of FIG. 1 plated with Li.

FIG. 3 shows another exemplary anode coupled to a composite solid electrolyte.

FIG. 4A shows an exemplary process where Li is deposited and/or stripped in a hollow tubule formed by the MIEC.

FIG. 4B shows an exemplary process where Li is deposited and/or stripped in a tubule formed by the MIEC with a three-dimensional (3D) structure inside the tubule.

FIG. 4C shows an exemplary process where Li diffuses through a coherent and incoherent boundary.

FIG. 4D shows the transport of Li across a smooth and a rough surface.

FIG. 5A shows Li being stripped in a tubule by a combination of dislocation motion and an interfacial diffusion mechanism.

FIG. 5B shows Li being stripped in a tubule by only the interfacial diffusion mechanism of FIG. 5A.

FIG. 6A shows a diagram of an exemplary MIEC formed from an array of carbon hollow tubules (CHT) arranged as a honeycomb structure.

FIG. 6B shows the volumetric capacity of the MIEC of FIG. 6A based on the weight of Li and the CHT as a function of porosity.

FIG. 6C shows the gravimetric capacity of the MIEC of FIG. 6A based on the weight of Li and the CHT as a function of porosity.

FIG. 7A shows an exemplary equilibrium phase diagram between Li, silicon (Si), and aluminum (Al).

FIG. 7B shows an exemplary equilibrium phase diagram between Li, titanium (Ti), and nitrogen (N₂).

FIG. 7C shows an exemplary equilibrium phase diagram between Li, Si, and nickel (Ni).

FIG. 8 shows a schematic of an experiment to characterize the deposition and/or stripping of Li in one or more tubules using a transmission electron microscope (TEM).

FIG. 9A shows a TEM image of an exemplary single CHT in contact with a solid electrolyte (SE). The scale bar is 1 μm.

FIG. 9B shows a magnified TEM image of the single CHT and SE of FIG. 9A. The scale bar is 100 nm.

FIG. 9C shows a TEM image of an exemplary single CHT. The scale bar is 100 nm.

FIG. 9D shows a magnified TEM image of the single CHT of FIG. 9C. The scale bar is 20 nm.

FIG. 10 shows a series of TEM images of Li being plated within a single CHT. The Li crystal is shown in dark gray and the Li front is marked by the arrow. The scale bar is 100 nm.

FIG. 11 shows a series of TEM images of Li being stripped within a single CHT. The Li crystal is shown in dark gray and the Li front is marked by the arrow. The scale bar is 100 nm.

FIG. 12A shows a selected area electron diffraction (SAED) pattern of an exemplary CHT with no Li, which is indicated by an amorphous ring. The scale bar is 5 nm⁻¹.

FIG. 12B shows a SAED pattern of an exemplary CHT plated with Li, which is indicated by the stable (110) and (110) reflections perpendicular and parallel to the CHT axis, respectively.

The diffraction spots located on the red dashed circle correspond to the lattice spacing for (110) BCC Li planes of 0.248 nm. The scale bar is 5 nm⁻¹.

FIG. 13 shows SAED patterns of an exemplary CHT obtained after Li plating, which are used to determine the crystal phase of the Li. The diffraction patterns were recorded with a camera length of 100 cm. The scale bars are 5 nm¹.

FIG. 14A shows a high resolution transmission electron microscope (HRTEM) image of a Li crystal forming with (110) crystal planes inside a CHT. The scale bar is 100 nm.

FIG. 14B shows a magnified HRTEM image of the CHT of FIG. 14A before Li deposition.

The scale bar is 2 nm.

FIG. 14C shows a magnified HRTEM image of the CHT of FIG. 14A after Li deposition.

The scale bar is 2 nm.

FIG. 15A shows electron energy loss spectroscopy (EELS) spectra of the Li K-edge measured after Li deposition inside a CHT.

FIG. 15B shows a reference EELS spectra of the Li K-edge for a Li metal dendrite measured at cryogenic conditions. [Li, Y. et al., Science 358, 506-510 (2017)]

FIG. 16A shows a reference EELS spectra of the Li K-edge for Li₂O (red) and LiOH (black). The Li K-edge peaks for Li₂O and LiOH rise at about 58.2 eV, 62.7 eV and 75 eV. [Zheng, H. et al., Sci. Rep. 2, 542 (2012)].

FIG. 16B shows a reference EELS spectra of the Li K-edge for Li₂O₂ and Li₂CO₃. [Basak, S. et al., Ultramicroscopy 188, 52-58 (2018)]

FIG. 17A shows a TEM image of a single long CHT. The scale bar is 2 μm.

FIG. 17B shows a magnified TEM image of section (A) of the CHT of FIG. 17A. The scale bar is 100 nm.

FIG. 17C shows a magnified TEM image of section (B) of the CHT of FIG. 17A. The scale bar is 100 nm.

FIG. 17D shows a series of TEM images where section (A) of the CHT of FIG. 17A is plated with Li.

FIG. 17E shows a series of TEM images where section (B) of the CHT of FIG. 17A is stripped of Li.

FIG. 18A shows a TEM image of an exemplary CHT having a local 3D porous structure disposed inside the cavity of the CHT before Li plating. The scale bar is 100 nm.

FIG. 18B shows a TEM image of the CHT of FIG. 18A after Li plating. The scale bar is 100 nm.

FIGS. 18C-18F show a series of TEM images of a local 3D porous structure in a CHT being plated with Li. The scale bars are 50 nm.

FIG. 19 shows a series of TEM images of an exemplary CHT where Li is being stripped. A void space is present between the Li metal and the solid electrolyte. The scale bar is 100 nm.

FIG. 20A shows a series of TEM images of two aligned CHT's being plated with Li. The respective fronts of Li metal in each CHT is indicated by the white arrow. The scale bar is 100 nm.

FIG. 20B shows a series of TEM images of the two aligned CHT's of FIG. 20A being stripped of Li. The respective fronts of Li metal in each CHT is indicated by the white arrow. The scale bar is 100 nm.

FIG. 20C shows EELS spectra acquired at the cross in FIG. 20A before and after Li plating.

FIG. 20D shows EELS spectra of the Li K-edge with fine structure after Li plating and background subtraction.

FIG. 21A shows a TEM image of three aligned CHT's before Li plating. The scale bar is 100 nm.

FIG. 21B shows a TEM image of three aligned CHT's after Li plating. The scale bar is 100 nm.

FIG. 22A shows a series of TEM images of an exemplary CHT being plated with Li. The CHT has an inner diameter of about 200 nm and a wall thickness of 50 nm. The scale bars are 100 nm.

FIG. 22B shows a series of TEM images of the CHT of FIG. 22A being stripped of Li. The scale bars are 100 nm.

FIG. 23A shows a series of TEM images of an exemplary CHT being plated with Li. The CHT has an inner diameter of about 100 nm and a wall thickness of 60 nm. The scale bars are 100 nm.

FIG. 23B shows a series of TEM images of the CHT of FIG. 23A being stripped of Li. The scale bars are 100 nm.

FIG. 24 shows a series of TEM images of an exemplary carbon nanotube being plated with Li. The carbon nanotube has an inner diameter of about 30 nm and a wall thickness of 50 nm. The scale bar is 50 nm.

FIG. 25 shows a series of TEM images of an exemplary carbon nanotube being plated with Li. The carbon nanotube has an inner diameter of about 60 nm and a wall thickness of about 60 nm. The scale bar is 50 nm.

FIG. 26A shows a scanning electron microscope (SEM) image of several exemplary CHT's. The scale bar is 100 nm.

FIG. 26B shows an electron-dispersive x-ray (EDX) map of carbon (C) of the CHT's of FIG. 26A. The scale bar is 100 nm.

FIG. 26C shows an EDX map of oxygen (O) of the CHT's of FIG. 26A. The scale bar is 100 nm.

FIG. 26D shows an EDX map of zinc (Zn) of the CHT's of FIG. 26A. The scale bar is 100 nm.

FIG. 27A shows x-ray photoelectron spectroscopy (XPS) spectra of the CIs line acquired using the CHT's of FIG. 27A.

FIG. 27B shows XPS spectra of the Zn2p_3/2 line acquired using the CHT's of FIG. 27A.

FIG. 27C shows XPS spectra of the O1s line acquired using the CHT's of FIG. 27A.

FIG. 28A shows EDX spectra of the CHT's of FIG. 26A before acid treatment.

FIG. 28B shows EDX spectra of the CHT's of FIG. 26A after acid treatment.

FIG. 29 shows a table of the ratio of Zn and O in the CHT's of FIG. 26A before and after acid treatment.

FIG. 30A shows a dark-field TEM image of Li wetting the outer surface of an exemplary CHT. This image shows Li is plated inside the CHT before being extruded out of the CHT with additional deposition. The dark-field image was acquired when the (110) diffraction beam of the Li crystal (see inset) is allowed to pass through the objective aperture. The dashed circle denotes the selected area aperture. The scale bar is 100 nm.

FIG. 30B shows a dark-field TEM image of the CHT of FIG. 30A where Li begins to wet the outer surface of the CHT. The scale bar is 100 nm.

FIG. 30C shows a dark-field TEM image of the CHT of FIG. 30A where Li wets the outer surface of the CHT along a length of 100 nm. The scale bar is 100 nm.

FIG. 30D shows a dark-field TEM image of the CHT of FIG. 30A where Li wets the outer surface of the CHT along a length of 140 nm. The scale bar is 100 nm.

FIG. 30E shows a dark-field TEM image of the CHT of FIG. 30A where Li begins to grow outward from the outer surface of the CHT. The scale bar is 100 nm.

FIG. 31 shows a TEM image of the outer surface of an exemplary CHT before Li plating.

The scale bar is 2 nm.

FIGS. 32A-32C show a series of TEM images of Li₂O being grown out of a carbon tubule surface. The scale bar is 2 nm.

FIG. 32D shows a HRTEM image of the Li₂O layer growing out of the CHT surface.

FIG. 33 shows a HRTEM image of a layer of Li₂O on outer surface of CHT. The scale bar is 2 nm.

FIG. 34A shows a TEM image of a Li whisker grown from a single CHT. ZnO_x is disposed inside the CHT within the selected area aperture. The scale bar is 100 nm.

FIG. 34B shows a SAED pattern showing the side edges of the Li whisker in {110} planes.

FIG. 34C shows a HRTEM image of the Li₂O on the Li whisker. The Li₂O is measured with a lattice spacing of 0.27 nm between the Li₂O (111) planes on the side edge of the whisker corresponding to the interface of Kurdjumov-Sachs {110}BCC Li//{111}FCC Li₂O orientation relationship indicated by the inset of FIG. 34B. The scale bar is 2 nm.

FIG. 35A shows a HRTEM image of in situ lateral growth of Li₂O on the outer layer of one thick flake of Li. The {111} planes are shown to be parallel to the outer surface and the advancement of {111} planes are marked between red dashed lines. The scale bar is 2 nm.

FIG. 35B shows a HRTEM image of the outer layer of one thick flake of Li of FIG. 35A taken at a later time. The {111} planes are shown to be parallel to the outer surface and the advancement of {111} planes are marked between red dashed lines. The scale bar is 2 nm

FIG. 35C shows EELS spectra of the Li K-edge on the outer layer of Li₂O. A shoulder features is observed indicating the presence of Li₂O.

FIG. 36A shows an exemplary first charging profile of a CHT.

FIG. 36B shows an exemplary plating/stripping profile of a CHT.

FIGS. 37A-37K each show a series of TEM images of Li being plated and stripped along a single exemplary CHT for a single cycle (from a 1^st cycle to a 100^th cycle). The scale bars in each image are 100 nm.

FIG. 38A shows a series of TEM images of a single exemplary CHT being plated with sodium (Na). The scale bar is 100 nm.

FIG. 38B shows a series of TEM images of the single CHT of FIG. 38A being stripped of Na. The scale bar is 100 nm.

FIG. 38C shows a SAED pattern of the Na-plated single CHT of FIG. 38B showing that the Na is a single crystal.

FIG. 39A shows a field-emission scanning electron microscope (FESEM) image of an exemplary carbonaceous MIEC beehive (also referred to herein as a “honeycomb”). The scale bar is 1 μm.

FIG. 39B shows a magnified FESEM image of the respective ends of the MIEC beehive of FIG. 39A. The scale bar is 200 nm.

FIG. 39C shows a magnified FESEM image of the respective sides of the MIEC beehive of FIG. 39A. The scale bar is 500 nm.

FIG. 40 shows a TEM image of the MIEC beehive of FIG. 39A. The scale bar is 200 nm.

FIG. 41A shows a FESEM image of an exemplary ZnO-coated carbonaceous beehive. The scale bar is 2 μm.

FIG. 41B shows an EDX map of C in the ZnO-coated carbonaceous beehive of FIG. 41A. The scale bar is 2 μm.

FIG. 41C shows an EDX map of O in the ZnO-coated carbonaceous beehive of FIG. 41A. The scale bar is 2 μm.

FIG. 41D shows an EDX map of Zn in the ZnO-coated carbonaceous beehive of FIG. 41A. The scale bar is 2 μm.

FIG. 42 shows an exemplary load-displacement curve of the MIEC beehive measured based on nanoindentation tests.

FIG. 43 shows a FESEM image of an exemplary carbonaceous beehive covered with a layer of LiPON. The scale bar is 200 nm.

FIG. 44A shows a top view of an exemplary carbonaceous MIEC beehive.

FIG. 44B shows an image of an exemplary P(EO/EM/AGE)/LiTFSI solid electrolyte film.

FIG. 44C shows a bottom view of the MIEC beehive of FIG. 44A. The platinum (Pt) layer is shown.

FIG. 44D shows a FESEM image of the MIEC beehive of FIG. 44A. As shown, the aligned carbon tubes are bonded to the Pt layer. The scale bar is 500 nm.

FIG. 45A shows a schematic of an exemplary half-cell using a MIEC beehive to evaluate electrochemical performance.

FIG. 45B shows an exemplary charge/discharge profile for Li plating of a half-cell.

FIG. 45C shows an exemplary charge/discharge profile for Li stripping of a half-cell.

FIG. 45D shows the overpotential and CE of the half-cell at various current densities.

FIG. 45E shows the charge/discharge voltage profile of the Li/SE/MIEC beehive half-cell as a function of time.

FIG. 45F shows a comparison of the current density and areal capacity of the anode in the present disclosure and previous anodes used in all-solid-state batteries. The pink symbol represents a half-cell with a 3D MIEC beehive on the Pt layer as a Li host. The green symbol represents a half-cell with a carbon-coated Cu foil as a Li host.

FIG. 46 shows an image of an exemplary LiFePO₄ cathode.

FIG. 47A shows the charge/discharge profile at 0.1 C of an exemplary full-cell all-solid-state battery with the MIEC beehive. The battery is a 1× excess Li-pre-deposited MIEC/SE/LiFePO₄ battery.

FIG. 47B shows the capacity and Coulombic efficiency (CE) as a function of the number of cycles for the all-solid-state battery of FIG. 47A. The blue line is the CE of the all-solid-state battery with the 3D MIEC beehive.

FIG. 48A shows a FESEM image of the open pore structure of the MIEC before Li plating. The scale bar is 100 nm.

FIG. 48B shows a FESEM image of the open pore structure of the MIEC after Li plating. The scale bar is 100 nm.

FIG. 49A shows a schematic of an exemplary titanium nitride (TiN) MIEC beehive fabrication process.

FIG. 49B shows a FESEM image of an exemplary TiN MIEC with a beehive open-pore structure formed from TiN nanotubes. The scale bar is 500 nm.

FIG. 49C shows a magnified FESEM image of the sides of the MIEC beehive of FIG. 49B. The scale bar is 100 nm.

FIG. 49D shows a FESEM image of the ends of the MIEC beehive of FIG. 49B.

The scale bar is 500 nm.

FIG. 49E shows a magnified FESEM image of the ends of the MIEC beehive of FIG. 49D. The scale bar is 100 nm.

FIG. 50A shows a load-displacement curve of an exemplary TiN MIEC measured using a nanoindentation test.

FIG. 50B shows an exemplary charge/discharge profile for Li plating/stripping in a TiN MIEC half-cell. The pink line is for a TiN MIEC beehive on as a Li host.

FIG. 50C shows the overpotential and CE of the TiN MIEC half-cell at various current densities. The pink line is for a TiN MIEC beehive on as a Li host.

FIG. 50D shows the charge/discharge voltage profile of the Li/SE/TiN MIEC beehive half-cell as a function of time. The pink line is for a TiN MIEC beehive on as a Li host

FIG. 51A shows an exemplary charge/discharge profile for Li plating/stripping in a TiN MIEC full-cell battery.

FIG. 51B shows the capacity and Coulombic efficiency (CE) as a function of the number of cycles for the TiN MIEC full-cell battery of FIG. 51A. The blue line is the CE of the TiN MIEC full-cell battery.

FIG. 52A shows an image of an exemplary MIEC formed using an anodic aluminum oxide (AAO) template.

FIG. 52B shows a SEM image of the ends of the AAO MIEC of FIG. 52A.

FIG. 52C shows a SEM image of the sides of the AAO MIEC of FIG. 52A.

FIG. 53A shows an image of an exemplary MIEC formed using a silicon mesh.

FIG. 53B shows a SEM image of the ends of the Si MIEC of FIG. 53A.

FIG. 53C shows a magnified SEM image of the ends of the SI MIEC of FIG. 53B.

FIG. 53D shows a SEM image of the sides of the Si MIEC of FIG. 53A.

FIG. 54 shows an equilibrium phase diagram between TiFe and Li₇La₃Zr₂O₁₂.

FIG. 55 shows an equilibrium phase diagram between Li and Li₇La₃Zr₂O₁₂.

FIG. 56 shows the relationship between anode thickness and porosity for MIECs with different areal capacities.

DETAILED DESCRIPTION

Following below are more detailed descriptions of various concepts related to, and implementations of, an anode that includes a mixed ionic-electronic conductor (MIEC) forming an open pore structure to facilitate the transport of an alkali metal during charging or discharging of a battery. It should be appreciated that various concepts introduced above and discussed in greater detail below may be implemented in multiple ways. Examples of specific implementations and applications are provided primarily for illustrative purposes so as to enable those skilled in the art to practice the implementations and alternatives apparent to those skilled in the art.

The figures and example implementations described below are not meant to limit the scope of the present implementations to a single embodiment. Other implementations are possible by way of interchange of some or all of the described or illustrated elements. Moreover, where certain elements of the disclosed example implementations may be partially or fully implemented using known components, in some instances only those portions of such known components that are necessary for an understanding of the present implementations are described, and detailed descriptions of other portions of such known components are omitted so as not to obscure the present implementations.

In the discussion below, various examples of a MIEC, a solid electrolyte, an anode formed from the MIEC, an open pore structure, and a battery formed from the anode and the solid electrolyte. It should be appreciated that one or more features discussed in connection with a given example may be employed in other examples according to the present disclosure, such that the various features disclosed herein may be readily combined in a given system according to the present disclosure (provided that respective features are not mutually inconsistent).

An Exemplary Anode with a Mixed Ionic-Electronic Conductor (MIEC)

FIG. 1 shows an exemplary battery 1000 that comprises an anode 1100 and a solid electrolyte 1400. The anode 1100 may include a mixed ionic-electronic conductor (MIEC) 1110 that forms an open pore structure 1120. When the battery 1000 is being charged and/or discharged, an alkali metal 1300 may be transported into and/or out of the open pore structure 1120. Said in another way, the MIEC 1110 functions as a host for the alkali metal 1300 by storing and/or releasing the alkali metal 1300 via the open pore structure 1120. The open pore structure 1120 formed by the MIEC 1110 may have pores that extend across the MIEC 1110 between a first end 1112 and a second end 1114. The anode 1100 may include a current collector 1140 disposed on the first end 1112 of the MIEC 1110. The solid electrolyte 1400 may be disposed on the second end 1114 of the MIEC 1110.

The MIEC 1110 may be electrically conducting and ionically conducting with respect to an alkali metal ion 1310 in order to facilitate a reduction and/or oxidation reaction of the alkali metal 1300 during a charge or discharge process, respectively. For example, when the battery 1000 is being charged, alkali metal ions 1310 will be transported from a cathode (not shown), across the solid electrolyte 1400, and into the anode 1100 through the second opening 1114 of the MIEC 1110. A power source (not shown), such as a voltage source, may supply electrons 1320 to the anode 1100 through the current collector 1140. The electrons 1320 and the alkali metal ions 1310 may be transported by the MIEC 1110, resulting in the reduction of the alkali metal ion 1310 to a neutral alkali metal 1300, which is then stored within the open pore structure 1120. As the battery 1000 is charged, the amount of alkali metal 1300 in the open pore structure 1120 may increase, thus occupying a larger portion of the open pore structure 1120. In some implementations, the alkali metal 1300 may have a front (e.g., a surface on the alkali metal 1300 that interfaces the inert gas in the open pore structure 1120) that progressively moves within the open pore structure 1120 as the alkali metal 1300 backfills the open pore structure 1120.

When the battery 1000 is being discharged, the alkali metal 1300 undergoes an oxidation reaction that results in the generation of an electron 1320 and an alkali metal ion 1310. The electrons 1320 are transported out of the MIEC 1110 through the current collector 1140. The tendency for electrons 1320 to preferentially flow towards the current collector 1140 is based, in part, on the solid electrolyte 1400 being electrically insulating. The alkali metal ions 1310 are transported out of the MIEC 1110 towards the cathode and solid electrolyte 1400 through the second opening 1114. As alkali metal ions are transported from the anode 1100 to the cathode, the amount of alkali metal 1300 stored within the open pore structure 1120 may decrease, resulting in a retraction of the front of the alkali metal 1300.

The reserved pore space in the open pore structure 1120 may help relieve the stresses generated by the alkali metal 1300 (hydrostatic and deviatoric) by allowing the alkali metal 1300 to backfill. In this manner, the likelihood of fracturing the anode 1100 when cycling the battery 1000 may be substantially reduced while maintaining electronic and ionic contact. In some implementations, the transport of alkali metal 1300 may also be aided by alkaliphilic capillary wetting of the open pore structure 1120.

As described above, the open pore structure 1120 may be used to transport the alkali metal 1300 into and/or out of the MIEC 1110 for storage when charging the battery 1000 and/or release when discharging the battery 1000. The shape and dimensions of the open pore structure 1120 formed by the MIEC 1110 may thus affect the capacity and the charge/discharge rate of the battery 1000.

Generally, the open pore structure 1120 may include a plurality of pores that form percolation pathways extending across the MIEC 1110. The pores and/or percolation pathways may be separated by a portion of the MIEC 1110 (e.g., a wall). The plurality of pores may be substantially open to allow the alkali metal 1300 to enter and/or leave the MIEC 1110 through the solid electrolyte 1400 when cycling the battery 1000. In some implementations, the percolation pathways may intersect with one another. For example, two or more percolation pathways may merge into a single pathway and/or one percolation pathway may split into two or more percolation pathways. More generally, the tortuosity of the open pore structure may be small (e.g., about 1 corresponding to highly aligned percolation pathways) or large (e.g., greater than 1 corresponding to highly twisted percolation pathways).

The open pore structure 1120 may be a substantially isotropic structure where the orientation of the percolation pathways is distributed uniformly about a 4π solid angle space. For instance, the open pore structure 1120 may be a foam-like structure comprising a plurality of spherical cavities joined together to form the percolation pathways through which the alkali metal 1300 is deposited/stripped.

The open pore structure 1120 may be a substantially aligned array of cylindrical cavities that extend from a first end 1112 of the MIEC 1110 to a second end 1114 of the MIEC 1110. In some implementations, the first end 1112 and the second end 1114 may be disposed on opposite sides of the MIEC 1110, hence, the array of cylindrical cavities may be substantially straight. In some implementations, the first end 1112 and the second end 1114 may be disposed on sides of the MIEC 1110 that are not parallel. Thus, the array of cylindrical cavities may be uniformly curved or bent such that the respective ends of the cylindrical cavities terminate at the first end 1112 and the second end 1114. In this manner, the MIEC 1110 and/or the open pore structure 1120 may be shaped to conform to the form factor of the battery 1000 (e.g., a flat planar cell or a cylindrical cell).

FIG. 1 shows an exemplary open pore structure 1120 shaped as an array of aligned tubules 1210 within the MIEC 1110. The array of tubules 1210 may be arranged in various forms including, but not limited to a grid and a honeycomb structure. As shown, each tubule 1210 is separated from a neighboring tubule 1210 by a wall 1200 of the MIEC 1110. Each tubule 1210 may have a cross-sectional width Wand each wall 1200 may have a thickness w. The height, h, of the open pore structure 1120 may extend across the entirety of the MIEC 1110. In some implementations, the width, W, of the tubule 1210 may be less than about 300 nm. In some implementations, the thickness of the wall 1200, w, may be between about 1 nm to about 30 nm. In some implementations, the height, h, of the tubules 1210 may be at least about 10 μm.

The MIEC 1110 may be fabricated using various approaches including, but not limited to a growth process (e.g., the open pore structure 1120 is formed during the growth of the MIEC 1110 from a substrate) and/or an etching process (e.g., the MIEC 1110 is deposited onto a substrate as a homogenous medium and the open pore structure 1120 is then formed by etching into the MIEC 1110). For example, the aligned tubules 1210 shown in FIG. 1 may be formed by growing the tubules 1210 from a substrate with a sufficient packing density such that the average separation distance between tubules is less than about 300 nm. In another example, the aligned tubules 1210 may be formed by etching a substrate in an anisotropic manner (e.g., deep reactive-ion etching) to form an array of highly aligned, large aspect ratio cavities (e.g., aligned cylindrical cavities).

In some implementations, the battery 1000 may be cycled by applying alternating negative and positive overpotentials. This may cause the alkali metal 1300 to move into and/or out of the open pore structure 1120 in a similar manner to a mechanical pump, resulting in a cyclical load applied to the MIEC 1110 that may cause fatigue. The MIEC 1110 and the open pore structure 1120 should thus be designed to have walls 1200 with a sufficiently large mechanical strength and ductility to accommodate the stresses generated by P_LiMetal and capillarity thereby reducing the risk of fracture and/or fatigue in the MIEC 1110.

Generally, the pores of the open pore structure 1120 may vary in size and shape. However, in some implementations, it may be preferable for the pores (e.g., the tubules 1210) to be substantially uniform in terms of size, shape, and/or alkaliphilicity to reduce the formation of dead lithium and/or provide spatially uniform transport of the alkali metal 1300.

Prior to the alkali metal 1300 infiltrating the open pore structure 1120, the open spaces of the open pore structure 1120 may be evacuated and/or contain an inert gas phase. For ease of manufacture, it may be preferable for the open pore structure 1120 to initially contain a gas phase at P_gas=1 atm (10⁵ Pa). The solid electrolyte 1400 should preferably form a hermetic seal on the second end 1114 of the MIEC 1110, otherwise the alkali metal 1300 may readily plate or flow through the solid electrolyte 1400 causing an electrical short with the cathode. The current collector 1140 should also preferably form a hermetic seal on the first end 1112 of the MIEC 1110. As a result, the deposition of the alkali metal 1300 in the open pore structure 1120 may compress the inert gas phase, resulting in a local P_gas that increases as more alkali metal 1300 is deposited. The rise in P_gas may be proportional to the compression ratio of the gas (e.g., P_gas may be about 10 atm for a compression ratio of about 10×).

The rise in P_gas generally does not affect the transport of the alkali metal 1300. For example, the pressure generated by Li, P_LiMetal, may be about 10² MPa according to the Nernst equation, which is substantially larger than P_gas. In other words, the alkali metal 1300 may readily act as a piston to compress the gas. However, heterogeneities within the open pore structure 1120 may cause the alkali metal 1300 to be deposited non-uniformly. The non-uniform plating of the alkali metal 1300 may give rise to a pressure difference ΔP_gas between adjacent tubules 1210, which may bend or, in some instances, burst the wall 1200 of the MIEC 1110. Thus, in some implementations, the wall 1200 of the MIEC 1110 may be designed to be non-hermetic to allow P_gas to equilibrate from cell to cell. In this manner, the internal pressure of the MIEC 1110 may be more homogenous, thus reducing the likelihood of one tubule 1210 expanding and collapsing a neighboring tubule 1210.

In some implementations, the height, h, of the open pore structure 1120 and the MIEC 1110 may include a reserved space for the inert gas phase to be compressed without generating exceedingly large P_gas. For example, FIG. 2 shows an exemplary tubule 1210 that is filled with the alkali metal 1300. A compression ratio of 10× corresponds to at least 90% of the free volume of the open pore structure 1120 being filled with the alkali metal 1300 with the remainder being the compressed gas. As described above, this compression ratio may be readily satisfied due to the large pressures generated by the alkali metal 1300. Although a portion of the open pore structure 1120 should be reserved for the gas phase, the volumetric capacity of the anode 1100 may still be enhanced due to the large volume fraction of alkali metal 1300. In general, the open pore structure 1120 may be shaped such that the alkali metal 1300 plated into the open pore structure 1120 may occupy at least about 30% of the total volume of the MIEC 1110.

The current collector 1140 may be formed from various electrically conductive materials including, but not limited to copper, aluminum, silver, and gold. In some implementations, the current collector 1140 may be a film that is deposited onto the MIEC 1110 or a substrate from which the MIEC 1110 is grown and/or deposited.

The solid electrolyte 1400 may have an ionic conductivity to ions of the alkali metal greater than or equal to 1 mS cm⁻¹ (e.g., 1 mS cm⁻¹, 2 mS cm⁻¹, 5 mS cm⁻¹, or 10 mS cm⁻¹) and a thickness less than or equal to 100 μm (e.g., 1 μm, 5 μm, 10 μm, 20 μm, 50 μm, 80 μm, or 100 μm).

The solid electrolyte 1400 may be formed from various materials including, but not limited to polymers and/or ceramics. The polymer may include at least one of a polyethylene, a polypropylene, a polyethylene oxide, a polyacetal, a polyolefin, a poly(alkylene oxide), a polymethacrylate, a polycarbonate, a polystyrene, a polyester, a polyamide, a polyimide, a polyamideimide, a polyarylate, a polyarylsulfone, a polyethersulfone, a polyphenylene sulfide, a polyvinyl chloride, a polysulfone, a polyimide, a polyetherimide, a polytetrafluoroethylene, a polyetherketone, a polyether etherketone, a polyether ketone, a polybenzoxazole, a polyphthalide, a polyanhydride, a polyvinyl ether, a polyvinyl thioether, a polyvinyl alcohol, a polyvinyl ketone, a polyvinyl halide, a polyvinyl nitrile, a polyvinyl ester, a polysulfonate, a polysulfide, a polythioester, a polysulfone, a polysulfonamide, a polyurea, a polyphosphazene, a polysilazane, a polyethylene terephthalate, a polybutylene terephthalate, a polyurethane, an ethylene propylene diene rubber, a polytetrafluoroethylene, a fluorinated ethylene propylene, a perfluoroalkoxyethylene, a polychlorotrifluoroethylene, or a polyvinylidene fluoride. Any of the compounds listed above may be the sole component of the solid electrolyte or may be used in combination.

The ceramic may include an antiperovskite structure having the formula Li₃O_X and/or Li₃SX₃ wherein X is at least one of Cl, Br, or I, or a super halide such as BH₄ or BF₄. An exemplary antiperovskite is Li₃OCl.

The ceramic may include a phosphate-type solid electrolyte such as a NASICON structure of the general formula Li_1±xM1_xM_2−x(PO₄)₃, wherein M is Al, Ga, In, Sc, Cr, Fe, Ta, or Nb; M2 is Ti, Zr, Hf, Si, or Ge, and wherein the number of moles of lithium per formula unit is 0<x<2, 0.2<1±x<1.8, 0.4>1±x<0.6. For example, the NASICON structure can be LiTi₂(PO₄)₃, Li_1+xAl_xGe_2−x(PO₄)₃ (LAGP), Li_1+xAl_xTi_2−x(PO₄)₃ (LATP), Li_1+xTi_2−xAl_xSi_y(PO₄)_3−y, Li_1−xTi_2−xTa_x(PO₄)₃ wherein 0<x<1 and 0≤y<1, LiAl_xZr_2−x(PO₄)₃, and/or LiTi_XZr_2−x(PO₄)₃ wherein 0<x<2.

The ceramic can also include an oxide-type solid electrolyte such as a perovskite structure having the general formula (La_1−xLi_x)TiO₃ (LLTO)) wherein 0<x<1 The ceramic can also include a sulfide or glassy sulfide such as Li₆PS₅X wherein X is Cl, Br, or I, Li₁₀MP₂S₁₂ wherein M is Ge, Si, or Sn; Li₂S—P₂S₅, Li₂S—P₂S₅-L₄SiO₄, Li₂S—GeS₂, Li₂S—Sb₂S₃—GeS₂, Li_3.25—Ge_0.25—P_0.75S₄, or Li₁PS₄, Li₇P₃S₁₁. The ceramic can also include Li—N, Li₂S, LiBH₄, or Li₃BO₃, optionally including derivatives with dopants on the cation or anion sites. The ceramic can be a garnet-type oxide, e.g., Li₇La₃Zr₂O₁₂. Optionally, the garnet-type oxide can further include one or more dopants, for example selected from Al, Ge, Ga, W, Ta, Nb, Ca, Y, Fe, or a combination thereof, wherein the dopant, if present, is contained in an amount of greater than 0 to 3 moles per formula unit in the unit formula Li₇La₃Zr₂O₁₂ on the La-site, and greater than 0 to 2 moles per formula unit on the Zr site. The ceramic may also include a lithium mixed-metal chlorospinel, e.g., Li₂In_xSc_0.666−xCl₄ wherein 0≤x≤0.666; or Li_3−xE_1−xZr_xCl₆ wherein E is at least one of Y or Er. Any of the compounds listed above may be the sole component of the solid electrolyte or may be used in combination.

In some embodiments, the deposition metal can be sodium, and the solid electrolyte can include an oxide-type solid electrolyte such as sodium β-Al₂O₃ or NASICON (Na_1+xZr₂Si_xP_3−xO₁₂, 0<x<3); a sulfide type (e.g., Na₃PS₄); a closo-borate; or a polymer electrolyte such as poly(ethylene oxide) with a dissolved salt such as NaAsF₆.

For example, the solid electrolyte may include Li₇La₃Zr₂O₁₂; Li_1.3Al_0.3Ti_1.7(PO₄)₃; Li₆PS₅Cl; Li₁₀MP₂S₁₂ wherein M is at least one of Ge, Si, or Sn; Li₃PS₄; Li₇P₃S₁₁; Li₃N; Li₂S; LiBH₄; Li₃BO₃; Li₂S—P₂S₅; Li₂S—P₂S₅-L₄SiO₄; Li₂S—Ga₂S₃—GeS₂; Li₂S—Sb₂S₃—GeS₂; Li_3.25—Ge_0.25—P_0.75S₄; (La_1−xLi_x)TiO₃ wherein 0<x<1; Li₆La₂CaTa₂O₁₂; Li₆La₂ANb₂O₁₂ wherein A is at least one of Ca, Sr, or Ba; Li₆La₃Zr_1.5WO₁₂; Li_6.5La₃Zr_1.5TaO₁₂; Li_6.625Al_0.25La₃Zr₂O₁₂; Li₃BO_2.5N_0.5; Li₉SiAlO₈; Li_1+xAl_xGe_2−x(PO₄)₃; Li_1+xAl_xTi_2−x(PO₄)₃; Li_1+xTi_2−xAl_xSi_y(PO₄)_3−y wherein 0<x<1 and 0≤y<1; LiAl_xZr_2−x(PO₄)₃; LiTi_xZr_2−x(PO₄)₃ wherein 0<x<2; Li₆PS₅X, wherein X is at least one of Cl, Br, or I, or a combination thereof.

As another example, the solid electrolyte may include a polyether, a thiophosphate, and/or a garnet-type material. Examples of polyether solid electrolytes include polyethylene oxide (PEO). Examples of thiophosphate solid electrolytes include Li₁₀GeP₂Si₂ (LGPS), Li₆PS₅X with X being at least one of Cl, Br, or I), and Li₃PS₃ (LPS). Examples of garnet-type solid electrolytes include Li₇La₃Zr₂O (LLZO). The interface between the MIEC 1110 and the solid electrolyte 1400 is where the alkali metal 1300 is typically deposited first (when charging the battery 1000) and, hence, where P_LiMetal is initiated. Thus, the way the solid electrolyte 1400 is coupled to the MIEC 1110 may affect the durability of the battery 1000. In some implementations, the tubules 1210 of the MIEC 1110 may be partially inserted and/or planted into the solid electrolyte 1400 as shown in FIG. 1 to provide greater mechanical strength. In some implementations, the portion 1500 of the wall 1200 of the MIEC 1110 inserted into the solid electrolyte 1400 should be an electronic and Li-ion insulator (ELI) to avoid issues related to the mechanical coupling between the MIEC 1110 and the solid electrolyte 1400. Said in another way, the ELI root 1500 should only provide mechanical support to the MIEC 1110. The solid electrolyte 1400 may be formed from a compliant material, such as PEO, to reduce the likelihood of brittle root-fracture caused by the deposition of alkali metal 1300 at the interface between the MIEC 1110 and the solid electrolyte 1400.

In some implementations, the solid electrolyte 1400 may be a composite formed from multiple materials. For example, the solid electrolyte 1400 may include both ceramic and polymer materials, thereby taking advantage of the respective benefits of each of these types of solid electrolytes. As an example, a polymer solid electrolyte may have favorable mechanical properties like a high ductility, but a lower ionic conductivity; and a ceramic solid electrolyte may have less favorable mechanical properties like brittleness, but a higher ionic conductivity. For example, FIG. 3 shows the solid electrolyte may include a ductile polymer solid electrolyte 1400a, such as PEO, to securely couple to the tubules of the MIEC 1110. The ductile solid electrolyte 1400a may have a thickness sufficient to blunt small cracks (e.g., between about 100 nm to 500 nm). The solid electrolyte 1400 may also include a brittle ceramic solid electrolyte 1400b disposed on the ductile solid electrolyte 1400a. The brittle solid electrolyte may be a more ionically conductive medium, such as LGPS, which is less electrochemically stable against Li, but more Li⁺-conductive.

The charge/discharge rate of the battery 1000 depends, in part, on the manner in which the alkali metal 1300 is transported through the open pore structure 1120. In some implementations, the alkali metal 1300 may be transported as a solid-phase (e.g., a creep mechanism) within the open pore structure 1120. For many applications, it may be preferable to operate the battery 1000 at near room temperature (e.g., between about −20° C. and about 60° C.). At such temperatures, the alkali metal 1300 is typically a solid phase.

For example, the alkali metal 1300 may be Li, which is a soft metal at room temperature with a melting point of T_M=180° C. At a temperature of 300 K (e.g., room temperature), the homologous temperature for Li metal is T/T_M=0.66. Thus, the alkali metal 1300 may exhibit an appreciable creep strain rate {dot over (ε)}(T,σ) where σ is the deviatoric shear stress. The creep strain rate applied to a solid alkali metal 1300, such as Li at T=300 K, may deform the alkali metal 1300 to such an extent that the alkali metal 1300 may be viewed as behaving like an incompressible work fluid. Said in another way, the creep strain rate may deform the alkali metal 1300 thereby causing the alkali metal 1300 to advance and/or retract within the open pore structure 1120 as if the alkali metal 1300 were a fluid with an effective viscosity of η≡σ/{dot over (ε)}(T,σ). The creep strain rate may be caused by various creep mechanisms including, but not limited to a diffusion mechanism (e.g., an interfacial-diffusion Coble creep mechanism, a bulk-diffusion Nabarro-Herring creep mechanism), a dislocation slip mechanism, and a combination of a diffusion and dislocation mechanism.

A purely diffusional creep mechanism, such as lattice-diffusional Nabarro-Herring creep or interfacial-diffusional Coble creep, may exhibit a strain rate of {dot over (ε)}(T,σ)∂σ. Thus, the viscosity q depends on T and grain size, but not on a. The alkali metal 1300 thus behave like a Newtonian fluid when viewed from a continuum mechanics viewpoint. In contrast, a dislocation creep mechanism, such as power-law creep, may exhibit a viscosity η∂σ^1-n with n>1. This implies the alkali metal 1300 behaves like a shear-thinning, non-Newtonian fluid. Both types of mechanisms, however, may be used to transport the alkali metal 1300 within the open pore structure 1120 with the driving force being the chemical potential gradient −Ω∇P_LiMetal(x), which is related to the pressure gradient.

Although different transport mechanisms (e.g., dislocation vs. diffusion creep, interfacial Coble creep vs. bulk Nabarro-Herring creep) may be used to transport the alkali metal 1300 in the open pore structure 1120, the transport rate of the alkali metal 1300 may vary between the different mechanisms. In other words, the type of transport mechanism used may influence the overall transport rate of the alkali metal 1300, which in turn affects the current density and charge/discharge rate of the battery 1000. The contribution of different creep mechanisms on the transport rate of the alkali metal 1300 may depend on various factors including, but not limited to the grain size of the alkali metal 1300, the shape of the open pore structure 1120, and the size of the open pore structure 1120 (e.g., a characteristic width along a cross-section of a pore in the open pore structure 1120).

For example, a Coble creep mechanism typically contributes substantially to the transport of alkali metal 1300 when the characteristic width of the pores in the open pore structure 1120 are less than about 300 nm and the homologous temperature of the alkali metal 1300 is about T/T_M≈⅔. The creep strain rate due to the Coble creep may be estimated as follows,

$\begin{array}{cc}\stackrel{.}{\varepsilon }=K\frac{{\delta }_I{D}_I\Omega }{D^3{k}_{B}T}\sigma & \left(1\right)\end{array}$

where {dot over (ε)} is creep strain rate due to the Coble creep mechanism, K is a dimensionless constant, δ_I is the nominal interfacial diffusion layer thickness, D_I is the interfacial diffusion diffusivity, Ω is the atomic volume, D is the diameter size, k_B is Boltzmann constant, T is temperature, and σ is the yield stress.

As shown in Eq. (1), the yield stress σ∂D³ or σ=kD³ for a fixed creep strain rate. Thus, the stress that arises from Coble diffusional creep, which is applied to the portions of the MIEC 1110 forming the open pore structure 1120 (e.g., the walls of the MIEC 1110) by the alkali metal 1300, decreases as the characteristic width of each pore in the open pore structure 1120 and the alkali metal 1300 contained therein becomes smaller. By using a smaller pore to reduce the mechanical stress applied to the MIEC 1110, mechanical degradation of the MIEC 1110 and the solid electrolyte 1400 covering the MIEC 1110 may be substantially reduced. However, the thickness of the walls of the MIEC 1110 should remain sufficiently thick (e.g., between about 1 nm to about 30 nm) to sustain electrochemically generated mechanical stress.

Eq. (1) also shows that the creep strain rate {dot over (ε)} scales with D⁻³ for a fixed stress. Thus, as D decreases, the creep strain rate may increase substantially. The transport of alkali metal 1300 is primarily driven by the Coble creep mechanism if the pores in the open pore structure 1120 have a diameter less than about 300 nm.

FIG. 4A shows the Coble creep mechanism may facilitate the transport of alkali metal 1300 in the open pore structure 1120 with a “rail-guided” behavior. As shown, the alkali metal ions (or atom) 1310 and the electrons 1320 may diffuse along a phase boundary 1330 between the alkali metal 1300 and the wall 1200 of the MIEC 1110. In this manner, the phase interface 1330 of the wall 1200 of the MIEC 1110 functions as a “rail”, which “guides” the transport of alkali metal ions (or atom) 1310 and electrons 1320. When the alkali metal ions 1310 undergo a reduction reaction with the electrons 1320, the resulting alkali metal 1300 precipitates out onto a front 1340 of previously deposited alkali metal 1300. Thus, the transport of alkali metal 1300 occurs via progressive plating/stripping of alkali metal 1300 along said front 1340.

The “rail-guided” behavior may also be used to transport alkali metal 1300 even when internal obstructions/obstacles are present within the open pore structure 1120. For example, FIG. 4B shows the Coble creep mechanism may occur along both the wall 1200 of the MIEC 1110 forming the pore and the surface of the obstruction 1220 (e.g., a three-dimensional structure disposed in the pore). However, the diffusion rate and/or the diffusion path length may vary depending on the orientation of the obstruction 1220. For instance, FIG. 4B shows the obstruction 1220 may be oriented at an angle relative to the wall 1200 resulting in the alkali metal ions (or atom) 1310 being transported along two different directions.

The diffusion rate of the alkali metal 1300 may also vary depending on whether a coherent or incoherent boundary is formed between the alkali metal 1300 and the wall 1200 of the MIEC 1110 and/or the surface of the obstruction 1220. FIG. 4C shows that a coherent boundary is formed when the atomic planes of the alkali metal 1300 and the MIEC 1110 are substantially aligned and matched. Otherwise, the presence of vacancy defects on the MIEC 1110 and/or the alkali metal 1300 may result in a semicoherent or incoherent boundary. The diffusion rate generally depends on the free volume of the interfacial region defined between the MIEC 1110 and the alkali metal 1300. Typically, a larger free volume results in a higher diffusion rate. FIG. 4C shows that a coherent boundary may have a free volume that is locally dispersed with a delta-function like distribution. Said in another way, a coherent boundary has limited vacancy defects resulting in a small free volume and, hence, a low diffusion rate. In contrast, an incoherent boundary may have a larger free volume resulting in a higher diffusion rate.

In some implementations, the MIEC 1110 may support multiple types of phase boundaries. For example, a MIEC 1110 formed from lithiated carbon and a lithiophilic coating (Li₂O) may have two phase boundaries: (1) a phase boundary between the Li metal and the Li₂O crystal (a few nanometers thick) and (2) a phase boundary between Li metal and lithiated carbon. In some implementations, the phase boundary between Li and Li₂O crystals may not exhibit a matched lattice due, in part, to the Li₂O being nanocrystalline, resulting in an incoherent boundary with a fast diffusion rate. Additionally, a MIEC 1110 formed from carbon may contain a mixture of graphite and amorphous carbon. As a result, the phase boundary between the Li metal and the lithiated carbon may have a free volume that spatially varies (i.e., not sharply localized at a certain site) between clusters of amorphous carbon, which may also increase the diffusion rate.

The local diffusion path length of the alkali metal 1300 may also vary based on the shape of the wall 1200 and/or the obstruction 1220 since the alkali metal 1300 follows the topology of a surface during deposition. FIG. 4D shows a comparison of the local diffusion path length between a rough surface (or a local structure with fine curvature) and a smooth surface. As shown, the local diffusion path length of the alkali metal 1300 is longer for the rough surface compared to the smooth surface.

In some implementations, the process of stripping alkali metal 1300 from the MIEC 1110 may generate a void plug 1350 (also referred to herein as “void space”) that grows between residual alkali metal 1300 and the solid electrolyte 1400. The presence of the void plug 1350, however, may not prevent the remaining alkali metal 1300 from being stripped. Rather, the void plug 1350 may continue to grow as more residual alkali metal 1300 is stripped from the MIEC 1110 by transporting the alkali metal 1300 along the interface and/or surface of the MIEC 1110. FIGS. 5A and 5B show two possible mechanisms for transport in the presence of a void plug. FIG. 5A shows a combination of dislocation and interfacial diffusion mechanisms may transport the alkali metal 1300. FIG. 5B shows only the interfacial diffusion mechanism transports alkali metal 1300. When a void plug occurs between the solid electrolyte 1400 and the residual alkali metal, dislocation power-law creep may be excluded as a transport mechanism since dislocation slip cannot occur in a void. Therefore, interfacial diffusion may be the primary mechanism for the deposition and stripping of the alkali metal 1300. In some implementations, interfacial diffusion may enable the alkali metal 1300 to climb over obstacles within the open pore structure 1120.

In some implementations, it may be preferable to design the open pore structure 1120 to preferentially increase contributions from a particular creep mechanism. For example, the shape and dimensions of the open pore structure may be chosen such that the alkali metal 1300 is driven primarily by a fast interfacial-diffusion creep mechanism, thereby achieving a desired current density through the MIEC 1110. In some implementations, an interfacial diffusion mechanism may also render the transport of alkali metal 1300 less dependent on the material used to form the MIEC 1110.

To illustrate the impact different transport mechanisms may have on the design and material choice of the MIEC 1110, the following example describes a MIEC 1110 applied to a Li battery. However, it should be appreciated that other alkali metals and performance metrics may be used depending on the application of the battery 1000. Batteries used in industrial applications should preferably exhibit an areal capacity Q about 3 mAh/cm² and a current density J≡dQ/dt about 3 mA/cm². In implementations where the alkali metal 1300 is Li, a typical Li-containing anode (LMA) may have an overpotential Uversus Li⁺/Li of approximately 50 mV.

As described above, the open pore structure 1120 formed by the MIEC 1110 may include multiple percolation pathways (e.g., about 10¹⁰ tubules) for alkali metal 1300 to flow through the MIEC 1110. The large number of percolation pathways may lead to heterogeneities within the MIEC 1110 that cause transport and reactions (e.g., an oxidation reaction, a reduction reaction) to vary spatially across the MIEC 1110. Additionally, an overpotential may be applied to the alkali metal 1300 to drive an electric current through the battery 1000. However, the overpotential may also cause the alkali metal 1300 to generate a pressure applied to the MIEC 1110 forming the open pore structure 1120. Due to the presence of heterogeneities within the MIEC 1110, the pressure produced by the alkali metal 1300 may vary spatially, resulting in an unbalanced load that may cause portions of the MIEC 1110 to deform or, in some instances, fracture.

The pressure generated by Li when subjected to an overpotential may be expressed as maxP_LiMetal [MPa]=7410U[V]. Thus, a larger overpotential directly results in a larger pressure applied to the MIEC 1110, which may lead to more rapid mechanical degradation of the MIEC 1110. For reference, an overpotential U=50 mV produces a pressure maxP_LiMetal=370 MPa according to the relation above.

In practice, it is preferable to limit the overpotential U in order to reduce the mechanical load applied within the MIEC 1110. However, the overpotential U, which is a global parameter for the battery 1000, should still be sufficiently large to provide a desired global average current density J. Based on the typical overpotential U=50 mV, the average transport conductance of the MIEC 1110 may be estimated to be equal to or greater than about 3 mA/cm²/50 mV=0.06 S/cm².

For purposes of illustration, the open pore structure 1120 may be a honeycomb structure with substantially aligned tubules. The effective transport conductance of the MIEC 1110 with a honeycomb open pore structure 1120 may be expressed as (κ_MIEC/h)×w/(w+W), where κ_MIEC [S/cm] is an effective Li conductivity, and w/(w+W) is the fill factor by the MIEC 1110 assuming substantially straight pores and a tortuosity=1. FIG. 6A shows an exemplary MIEC 1110 structured as a beehive (also referred to herein as “honeycomb”). FIGS. 6B and 6C show the volumetric and gravimetric capacity, respectively, of the MIEC 1110. Based on FIGS. 6B and 6C, the height h of the tubules should be at least about 20 μm in order for the anode 1100 to provide a capacity Q about 3 mAh/cm². The preferred height includes space for the inert host in the open pore structure 1120. For h=20 μm, the effective longitudinal transport conductance should be as follows,

κ_MIEC×w/(w+W)>0.06 S/cm²×20 μm=0.12 mS/cm  (2)

Various mechanisms may contribute to the effective transport conductance, κ_MIEC, of the MIEC 1110. For example, bulk diffusion of the alkali metal 1300 may occur within the MIEC 1110. The bulk diffusivity, κ_MIEC^bulk, may be expressed as follows,

κ_MIEC^bulk˜e²c_LiDL_Li^bulk/k_BT  (3)

where c_Li (unit 1/cm³) is the Li atom concentration, k_B is the Boltzmann constant, and D_Li^bulk is the tracer diffusivity of Li atom in bulk MIEC 1110.

Based on Eq. (3), the contribution of bulk diffusion to the conductance of the MIEC 1110 may depend on the bulk diffusivity, D_Li^bulk, which may vary for different materials. Additionally, the MIEC 1110 should be compatible with the alkali metal 1300, which may be accomplished by alkaliating the material forming the MIEC 1110. For example, the MIEC 1110 may be compatible with Li when lithiated to below 0 V vs Li⁺/Li. Several anode materials may be used to form the MIEC 1110 including, but not limited to graphite or hard carbon (e.g., LiC₆), silicon (e.g., Li₂₂Si₅), and aluminum (e.g., Li₉Al₄). These materials are commonly used as anodes in previous Li batteries. Additional materials may be used to form the MIEC 1110 based on their electrochemical stability as will be described in further detail below. The bulk transport properties of carbon, silicon, and aluminum may be estimated to be the following: (1) LiC₆ has a c_Li=1.65×10²²/cm³ and an optimistic D_Li^bulk about 10⁻⁷ cm²/s, (2) Li₂₂Si₅ has a c_Li=5.3×10²²/cm³ and an optimistic D_Li^bulk about 10⁻¹¹ cm²/s, and (3) Li₉Al₄ has a c_Li=4×10²²/cm³ and an optimistic D_Li^bulk about 10⁻⁹ cm²/s.

Using Eq. (3), lithiated aluminum, Li₉Al₄, exhibits a κ_MIEC(Li₉Al₄) about 0.25 mS/cm, which is sufficient to satisfy the condition in Eq. (2). The MIEC fill factor is thus

$w/\left(w+W\right)=\frac{0.12\frac{\mathrm{mS}}{\mathrm{cm}}}{k_{\mathrm{MIEC}}}$

about 0.5. For a 100 nm wide pore, w=W about 100 nm. In other words, the width of the tubules and the walls of the MIEC 1110 should be comparable in size. For lithiated silicon (Li₂₂Si₅), the bulk diffusivity of D_Li^bulk about 10⁻¹¹ cm²/s results in κ_MIEC(Li₂₂Si₅) about 0.003 mS/cm, which does not satisfy the condition in Eq. (2).

Lithiated carbon, LiC₆, exhibits the largest c_LiD_Li^bulk amongst the three materials yielding a κ_MIEC^bulk(LiC₆) about 0.01 S/cm based on Eq. (3). These estimates are based on previous diffusivity data, which exhibited large uncertainties. For a more conservative estimate, the diffusivity may thus be assumed to be D_Li^bulk about 10^−g cm²/s, resulting in κ_MIEC^bulk(LiC₆) about 1 mS/cm. For LiC₆, the fill factor of the MIEC 1110 should preferably be equal to or greater than

$w_{\min }/\left(w_{\min }+W\right)=\frac{0.12\frac{\mathrm{mS}}{\mathrm{cm}}}{k_{\mathrm{MIEC}}}$

about 0.1. For a tubule width W about 100 nm, the thickness of the wall of the MIEC 1110 should thus be at least about w about 10 nm. These dimensions are similar to conventional graphite or hard carbon anodes used in Li-ion batteries (LIB), which typically have a film thickness of about 100 μm and are known to support a current density of 3 mA/cm² at an overpotential of about 50 mV.

However, an industrial LIB graphite anode typically operates near borderline conditions. A current density greater than about 3 mA/cm² through the LIB graphite anode may cause the local potential to drop below 0V vs Li⁺/Li. Under these conditions, Li metal would precipitate out of the anode resulting in the generation of new SEI when the Li metal contacts the flooding liquid electrolyte in the battery. The precipitation of Li metal and the generation of new SEI may severely degrade the cycle life and safety of LIB anodes.

Unlike conventional LIB graphite anodes, it is actually preferable for the alkali metal 1300 in the anode 1100 to “spill out” from the open pore structure 1120 of the MIEC 1110. The difference between the anode 1100 and previous anodes is the open pore structure 1120 formed by the MIEC 1110 enables a more controlled flow of alkali metal 1300. As described above, the open pore structure 1120 may substantially reduce or, in some instances, prevent a buildup of pressure P_LiMetal, which may otherwise crack the solid electrolyte 1400. Additionally, the MIEC 1110 may be electrochemically stable against the alkali metal 1300, thus substantially reducing or, in some instances, preventing the generation of new SEI since the expanding and/or shrinking portions of the alkali metal 1300 are in contact with only the MIEC 1110.

The above example shows that in implementations where the alkali metal 1300 is transported primarily by bulk diffusion in the MIEC 1110, the materials used to form the MIEC 1110 should preferably exhibit a sufficiently large diffusivity to meet a desired current density. For example, the MIEC 1110 should be formed from a material having D_Li^bulk at least about 10⁻⁸ cm²/s to achieve a desired current density of J about 3 mA/cm².

However, bulk diffusion is not the only mechanism that may contribute to the transport of alkali metal 1300 within the MIEC 1110. Interfacial transport of alkali metal 1300 may also occur along the surfaces of the MIEC 1110 (e.g., the interface between the MIEC 1110 and the open pore structure 1120). In some implementations, the contribution of interfacial transport to the overall transport conductance of the MIEC 1110 may be substantial, particularly for smaller sized tubules (e.g., tubules with a width W=100 nm and a wall thickness w=10 nm) where the surface area is large relative to the volume of the MIEC 1110. In some implementations, the MIEC 1110 may support fast-diffusion paths of width δ_interface (typically taken to be 2 Å) at the phase boundary between the MIEC 1110 and the alkali metal 1300 (e.g., the red/gray interface in FIG. 1) or the surface of the MIEC 1110 (e.g., the red/white interface in FIG. 1). The contributions of both the bulk and interfacial diffusion mechanisms to the overall effective transport conductance may be included by adding a size-dependent factor to the conductance as follows,

κ_MIEC=κ_MIEC^bulk×(1+2D_Li^interfaceδ_interface/D_Li^bulkw)  (4)

The surface diffusivity of alkali metal 1300 may be estimated using empirical formulations. For example, the surface diffusivity of Li on a BCC Li metal may be estimated as follows,

D _Li ^surface=0.014 exp(−6.54T_M/T)[cm²/s]  (5)

Eq. (5) has been shown to accurately predict the diffusivity of monatomic metals. At room temperature, Eq. (5) predicts D_Li^surface=7×10⁻⁷ cm²/s in BCC Li, which is 70× larger than D_Li^bulk about 10⁻⁸ cm²/s in LiC₆ in the previous example. The geometric factor, 2δ_interface/w, is approximately 4 Å/10 nm= 1/25. If D_Li^interface is assumed to be similar to D_Li^surface, the contribution of interfacial diffusion to the overall conductance may still be 3× larger than bulk diffusion within the MIEC 1110 for LiC₆.

Generally, the phase boundary between the MIEC 1110 and the alkali metal 1300 may have a lower atomic free volume compared to a free alkali metal surface. Thus, D_Li^interface may be smaller than D_Li^interface=7×10⁻⁷ cm²/s. For example, experimental diffusivity data suggests that D_Li^interface≈2×10⁻⁷ cm²/s, which is still comparable to the bulk diffusivity of LiC₆. For Li₉Al₄ and Li₂₂Si₅, D_Li^interface is several orders of magnitude larger than D_Li^bulk. In particular, the ratio D_Li^interface/D_Li^bulk is 200 for Li₉Al₄ and 20,000 for Li₂₂Si₅, which is substantially larger than the geometric factor 2δ_interface/w ( 1/25 for w=10 nm). As a result, the contribution of bulk diffusion in the MIEC 1110 for these materials may be treated as being negligible. Thus, interfacial diffusion alone may yield an effective 1MIEC about 1 mS/cm, which satisfies the conditions in Eq. (2). The MIEC fill factor is thus w/(w+W)=0.1.

When interfacial diffusion is substantial, the MIEC 1110 may achieve a desired current density even when formed from materials with a poor bulk diffusivity, such as Li₉Al₄ and Li₂₂Si₅, since the diffusion flux along the δ_interface≈2 Å MIEC/metal incoherent interface and/or MIEC surface is substantially larger than the bulk diffusion through the wall of the MIEC 1110. As a result, the ionic transport within the open pore structure 1120 may depend solely on the dimensions of the open pore structure 1120, which allows the MIEC 1110 to be formed from a broader range of electrochemically stable materials. For example, the MIEC 1110 may be formed from a material that exhibits desirable mechanical properties (e.g., toughness, yield strength, ductility) despite having a low bulk diffusivity.

As described above, the MIEC 1110 may be formed from typical anode materials such as carbon, silicon, and aluminum. More generally, the MIEC 1110 may be formed from a material that is electrochemically stable against the alkali metal 1300 such that the MIEC 1110 does not decompose to form fresh SEI at the interface between the MIEC 1110 and the alkali metal 1300. The alkali metal 1300 may be various types of metals including, but not limited to lithium, sodium, and potassium. In some implementations, only the MIEC 1110 (and not the solid electrolyte 1400) may be formed of an electrochemically stable material since the front 1340 of the alkali metal 1300 remains in contact with only the MIEC 1110 when extending into the open pore structure 1120 or receding from the open pore structure 1120. In this manner, no new SEI is formed as the battery 1000 is cycled. In some implementations, the MIEC 1110 and the solid electrolyte 1400 may both be formed of an electrochemically stable material, thus eliminating the generation of SEI during cycling and initial charging of the battery 1000. It should be appreciated that if the MIEC 1110 crumbles into pieces that are then embedded into the alkali metal 1300, electronic and ionic percolation is still possible since the MIEC 1110 is electrically and ionically conductive.

The MIEC 1110 may be made compatible with the alkali metal 1300 by alkaliating the MIEC 1110. Referring to the above example, a MIEC 1110 used in a Li battery may be lithiated to below 0V vs Li⁺/Li to form compounds such as LiC₆ using carbon, Li₂₂Si₅ using silicon, and Li₉Al₄ using aluminum. Electrochemical stability of the MIEC 1110 may be evaluated on the basis that a thermodynamically stable compound is formed between the MIEC 1110 and the alkali metal 1300.

For example, FIG. 7A shows an equilibrium phase diagram between Li, Al, and Si. An electrochemically stable compound is formed when the alkaliated compound (e.g., a lithiated material in this case) is directly connected to the BCC Li metal phase by a tie-line. As shown, Li₂₂Si₅ and Li₉Al₄ are end-member phases directly connected to Li by tie-lines (A) and (B), respectively. The electrochemical stability of other materials may be evaluated in a similar manner, i.e., the alkialated compound has a direct tie-line to the alkali metal 1300. FIG. 7B shows another equilibrium phase diagram between Li, Ti, and N₂. As shown, numerous electrochemically stable lithiated compounds may be used including Li₃N, Li₅TiN₃, TiN, Ti₂N, and Ti. FIG. 7C shows yet another equilibrium phase diagram between Li, Ni, and Si. In this case, the electrochemically stable lithiated compounds are Ni, LiSiNi₂, and Li₂₂Si₅ (as before).

As evidenced by the phase diagrams of FIGS. 7A-7C, the MIEC 1110 may be formed from a wide range of materials, especially when compared to the solid electrolyte 1400, of which few materials are electrochemically stable against the alkali metal 1300. This provides greater flexibility in terms of using materials with desirable electrical, ionic, and mechanical properties. If the MIEC 1110 and the open pore structure 1120 are shaped and dimensioned such that the alkali metal 1300 is primarily driven by the interfacial transport mechanisms describe above, the ionic and/or electron transport properties and the mechanical stability of the MIEC 1110 may be decoupled from the material composition. This provides additional flexibility since a material may be selected for the MIEC 1110 based on fewer material parameters.

For example, the MIEC 1110 may be formed from a material having a large mechanical toughness (e.g., the material absorbs a large amount of energy before fracturing) to withstand the mechanical stresses generated by the alkali metal 1300 when cycling the battery 1000. In another example, the MIEC 1110 may be formed from a material that has an incoherent boundary/interface with the alkali metal 1300 to increase the free volume of the phase boundary and, in turn, increase the diffusion transport rate. In another example, the MIEC 1110 may be formed from a passive material (e.g., TiN) that does not store and/or release the alkali metal 1300 when cycling the battery 1000. For such materials, the alkali metal 1300 is primarily stored and/or release from the open pore structure 1120 formed by the MIEC 1110.

In some implementations, the surfaces of the MIEC 1110 forming the open pore structure 1120 may also be coated with an alkaliphilic coating to increase the electrical and ionic conductance between the MIEC 1110 and the alkali metal 1300. For example, a thin ZnO_x film (e.g., about 1 nm) may be deposited onto the surfaces of the open pore structure 1120 in cases where the alkali metal 1300 is Li. The deposition of Li metal onto the ZnO_x coating may cause a layer of Li₂O to form at the interface between the MIEC 1110 and the alkali metal 1300. The Li₂O film may increase the wettability of the Li metal to the MIEC 1110, ensuring contact is maintained as more alkali metal 1300 is deposited in the open pore structure 1120. The alkaliphilic coating may thus provide a deformable, wetting, and lubricating film to enhance contact and transport of the alkali metal 1300 in the MIEC 1110.

A First Exemplary Demonstration with a Single Carbon Hollow Tubule (CHT)

A demonstration of the MIEC 1110 will now be described. Specifically, the transport of the alkali metal 1300 through the open pore structure 1120 was observed and characterized by performing experiments where Li metal was transported through individual carbon hollow tubule (CHT). FIG. 8 shows a schematic diagram of the experimental setup 2000. As shown, the setup 2000 comprises a solid-state nanobattery 1000 electrically coupled to a voltage source 2500.

The nanobattery 1000 included an anode 1100 comprising one or more CHT's 2100. The CHT's 2100 were coupled to a transmission electron microscope (TEM) copper grid 2140 using silver conductive epoxy. Thus, the CHT's 2100 served as the MIEC 1110 and the copper grid 2140 served as the current collector 1140. The nanobattery 1000 also included a counter-electrode 2200 comprising a tungsten probe 2210, which was coated with Li metal 2220 in a glove box filled with Ar gas. A solid electrolyte 1400 comprising poly (ethylene oxide) (PEO) and Lithium bis(trifluoromethanesulfonyl)imide (LiTFSI) were dissolved in 1-Butyl-1-methylpyrrolidinium bis(trifluoromethylsulfonyl)imide (ionic liquid). The Li metal 2220 on the tungsten probe 2210 was then coated with an approximately 50 μm thick film of the solid electrolyte 1400 inside the glove box filled with Ar gas.

The nanobattery 1000 was placed in a TEM (JEOL 2010F) for in situ imaging and characterization at 200 kV. Specifically, the TEM included a Nanofactory STM/TEM holder, which held the counter-electrode 2200 via the tungsten probe 2210. The anode 1100 was mounted to a sample holder. After loading the counter-electrode 2200 and the anode 1100 into the TEM, the STM/TEM holder supporting the counter-electrode 2200 was moved until the solid electrolyte 1400 contacted the free ends of the CHT's 2100, thus completing the assembly of the nanobattery 1000.

The voltage source 2500 was used, in part, to electrically control the transport of Li metal into and/or out of the MIEC 1110. Specifically, lithium plating and stripping in the CHTs 2100 were realized by applying −2 V and +2 V with respect to the lithium metal.

The CHT's 2100 were synthesized using the following steps: (1) obtaining a solution by dissolving 1 g of polyacrylonitrile (PAN, Aldrich) and 1.89 g of Zn(Ac)₂.2H₂O in 30 mL of dimethylformamide (DMF, Aldrich) solvent, (2) synthesizing PAN/Zn(Ac)₂ composite fibers via electrospinning by using the solution of (1) at 17 kV of working voltage, 0.05 mm/min of flow rate, and 20 cm of electrospinning distance, (3) forming a layer of Zeolitic Imidazolate Framework (ZIF-8) on the surface of the composite fibers by adding the fibers into an ethanol solution containing 2-methylimidazole (0.65 g, Aldrich), and (4) heating the synthesized core-shell composite fibers at 600-700° C. for 12 h to obtain the CHTs with some lithiophilic ZnO_x. In step (3), a trace amount of cobalt acetate was introduced into the composite fibers to improve the degree of the graphitization of the synthesized CHTs.

FIGS. 9A and 9B show TEM images of the CHT's 2100 coupled to the solid electrolyte (SE) 2230 after assembly in the TEM. FIGS. 9C and 9D show magnified TEM images of a single CHT 2100 fabricated using the above method. As shown, the resultant CHT's 2100 had an inner diameter W of about 100 nm and a wall thickness w of about 20 nm. FIG. 9D also shows the CHT 2100 is nanoporous. Thus, the CHT's 2100, as constructed, would allow the inert gas phase in a battery 1000 to equilibrate when depositing Li in the open pore structure 1120.

The in-situ TEM experiments were performed under conditions that reduced electron beam damage. Li metal is sensitive to electron beam irradiation in a TEM due, in part, to the elastic and inelastic scattering between the incident electron beam and the sample. The elastic interactions from electron-nucleus scattering may lead to sputtering damage. The inelastic interactions from electron-electron scattering may cause damage due to specimen heating and radiolysis. When taking images and/or video of the nanobattery 1000, an electron beam current of about 1.5 mA/cm² was used to reduce damage. Images were also acquired at a slight underfocus condition to enhance the contrast. The electron beam was also banked prior to imaging the sample and the exposure time (e.g., for taking a video) was limited to 2 minutes. The electron beam was also blanked while plating and stripping Li, except when making observations, to reduce the effect of electron beam impinging on the sample.

The nanobattery 1000 was also characterized by other instruments including a high-resolution TEM (HRTEM), a field emission scanning electron microscopy (FESEM, FEI Helios 600 Dual Beam FIB), an energy-dispersive X-ray spectroscope (EDX, oxford), and an X-ray photoelectron spectroscopy (XPS, PHI5600).

FIG. 10 shows a series of TEM images where Li is progressively plated along a single CHT with ZnO_x. As shown, the Li exhibits a front (indicated by the white arrow) that moves along the CHT as more Li is deposited. The Li initially underwent electrodeposition at the end of the CHT and proceeded to fill the initial void plug of the tubule. FIG. 11 shows a series of TEM images where Li is progressively stripped along the CHT of FIG. 10. FIGS. 10 and 11 thus show Li can be reversible deposited/stripped within a CHT.

FIGS. 12A and 12B show selected area electron diffraction (SAED) patterns before and after the Li metal front passes a portion of the CHT, respectively. The SAED patterns were acquired using a spread electron beam with an electron beam current below 1 mA/cm² to reduce irradiation damage. FIG. 12A shows a ring pattern indicating the CHT had an amorphous morphology. FIG. 12B shows a pattern with well-defined spots that correspond to the crystal planes of Li. In particular, the (110)_{BCC Li} is found to be perpendicular to the longitudinal axis of the CHT and the (110)_{BCC Li} is found to be parallel to the CHT axis. A circle intersecting the spots in the SAED pattern of FIG. 12B indicates the lattice spacing is about 0.248 nm.

FIG. 13 further shows the SAED patterns of the CHT with Li may be used to evaluate the crystal structure of Li. In particular, the two pairs of symmetric diffraction spots in the two SAED patterns were offset by a measured angle of 60° from one another. The indexing and the measured 60° angle between the two pairs of the symmetric spots match the standard indexed diffraction patterns for a BCC crystal in a [111] beam direction under six-fold symmetry. Additionally, the distance between the collected diffraction spots is similar to BCC lattice of Li. These results suggest the Li being transported through the CHT is indeed a solid-phase and, in fact, substantially single crystalline.

FIGS. 14A-14C show HRTEM images of a portion of the CHT as a fresh Li crystal is formed within the CHT. The HRTEM images of the Li metal plated inside the tubule were acquired using an electron beam current of about 0.3-0.5 Å/cm². FIG. 14C shows that when the Li crystal was first formed, lattice fringes with 0.248 nm lattice spacing were observed corresponding to the Li (110) planes. The Li lattice fringes remained for several seconds before vanishing due to electron beam irradiation damage. The CHTs helped to reduce irradiation damage when imaging the Li inside the tubule. The Li₂O is also robust to electron beam irradiation. Sputtering damage due to elastic scattering was reduced by confining the Li inside the CHT. For inelastic scattering, the CHT provided sufficient thermal and electrical conduction to dissipate heat generated by electron irradiation.

FIG. 15A shows electron energy loss spectroscopy (EELS) spectra of the Li K-edge measured after Li deposition inside the CHT using an approximately parallel electron beam in diffraction mode with an energy resolution of 1.5 eV. The EELS spectra were collected using a scanning transmission electron microscope (STEM) mode. The electron beam spot size was about 1 nm with a semi-convergence angle of about 5 mrad and a semi-collection angle of about 10 mrad. As shown, the Li K-edge obtained exhibited a shoulder at 55.9 eV and a peak rising at 62.5 eV. These spectral features are similar to the features of the Li K-edge previously measured from a Li metal dendrite at cryogenic conditions (see FIG. 15B), further confirming the presence of Li in the CHT.

FIG. 16A shows another reference EELS spectra of Li K-edges for Li₂O and LiOH with peaks appearing at 58.2 eV, 62.7 eV and 75 eV. FIG. 16B shows another reference EELS spectra of Li K-edges for Li₂O₂ and Li₂CO₃. A clear difference may be observed when comparing the measured EELS spectra of FIG. 15A to the reference EELS spectra of FIGS. 16A and 16B This indicates the Li phase deposited in the CHT is not Li₂O, LiOH, Li₂O₂ or Li₂CO₃. In other words, the EELS spectra show the Li phase deposited and stripped from the CHT is not a Li oxide or another phase.

FIGS. 17A-17E show TEM images of a long CHT, which was used to demonstrate Li metal transport across distances of several microns (i.e., a length scale comparable to the height of the MIEC 1110 in the battery 1000). FIG. 17A shows a low magnification image of the long CHT and FIGS. 17B and 17C show magnified images of sections (A) and (B) along the long CHT. FIG. 17D shows Li metal plating at section (A) of the CHT and FIG. 17E shows Li metal stripping at section (B) of the CHT. Section (B) of the long CHT was measured to be over 6 μm away from the solid electrolyte 1400. Thus, observations of Li metal at section (B) indicates the length of Li plated along the CHT was at least 6 μm.

FIGS. 18A-18F show TEM images of a CHT with obstructions disposed in the interior space of the CHT. FIGS. 18A and 18B show low magnification images of a section of the CHT before and after Li plating, respectively. These images show that Li deposition may still occur despite the presence of the obstructions within the CHT. This may be attributed to the Li metal being primarily driven by interfacial diffusion, which is insensitive to obstacles and/or obstructions within the MIEC 1110. In other words, interfacial diffusion may enable the Li metal to “climb over” obstructions within the CHT by following a more tortuous path due to the local structures of the obstructions in the CHT.

FIGS. 18C-18F show a series of images of a particular section of the CHT where Li first diffuses along the surface of a local 3D structure inside the CHT followed by Li plating and filling the open pores in the CHT. The thermodynamic driving force originating from the overpotential (chemical potential) may drive an atomic fountain-like behavior causing Li to fill the open pores and, on average, guide the Li flux along the overall direction of the CHT channel. Said in another way, the multi-tip-deposition of Li may initially fill the inside spaces defined by the 3D structures/obstructions in the CHT. Although Li plating may locally follow the surfaces of the 3D structures defining said spaces, the overall direction of Li deposition is ultimately confined by the walls of the CHT and, hence, should follow the longitudinal axis of the CHT (e.g., the overall “rail”) as shown in FIGS. 18A and 18B.

As previously described, multiple types of creep mechanisms (e.g., interfacial diffusion, power-law dislocation) may contribute to the transport of alkali metal 1300 in the open pore structure 1120. To distinguish between the two creep mechanisms, experiments were performed based on the schematic of FIG. 5B. It should be appreciated that the stripping process depicted in FIG. 5A may allow both interfacial diffusion mechanism and dislocation motion mechanism to co-exist; hence, an in-situ TEM experiment would be unable to differentiate between the two mechanisms. However, the schematic of FIG. 5B includes a void space between the Li metal and the solid electrolyte. In this configuration, the dislocation-slip mechanism cannot occur due to the presence of the void space, thus observation of Li transport would imply interfacial diffusion along the MIEC wall interior or interface.

FIG. 19 show a series of TEM images of Li being stripped from a CHT with a void space between the Li metal and the solid electrolyte 1400. As shown, Li metal may still be stripped despite the presence of the void space in the CHT. The white arrows in FIG. 19 indicate the movement of the free surface of the Li metal crystal (LiBCC) as Li atoms on said free surface diffuse towards the Li(BCC)/MIEC interface and undergo interfacial diffusion. The stripping rate of Li was also measured to be similar to other experiments with no void space, which suggests dislocation power-law creep does not contribute appreciably to Li transport. Instead, these results indicate the transport of Li through the CHT is driven primarily by interfacial diffusion (i.e., Coble creep).

The mechanism for transporting alkali metal 1300 across a single pore in the open pore structure 1120 is scalable. For example, FIGS. 20A and 20B show two neighboring CHT's may also rail-guide Li plating and/or stripping along the length of each tubule. The filling ratio of Li inside the tubule was estimated by an EELS thickness measurement. The thickness measurement was performed using an absolute log-ratio method, which is based on the following,

$\begin{array}{cc}\frac{t}{\lambda }=\ln \left(\frac{I_t}{I_0}\right)& \left(6\right)\end{array}$

where t stands for the thickness, λ stands for effective mean free path, I_t is the intensity integrated over the EELS spectrum, and Jo is the intensity integrated under a zero loss peak.

The accelerating voltage, semi-convergence, and semi-collection angles previous described and the atomic number, Z_eff, was used to calculate X. Before Li plating, Z_eff=6 for the CHT. After Li plating, Z_eff may be estimated based on a mixture of Li and CHT at the location where the EELS signal was recorded. For example, an atomic ratio between Li and C may be estimated to be 0.56:1 based on the observed geometry of the tubule (e.g., an inner diameter of about 100 nm and a wall thickness of about 28 nm). Thus, Z_eff may be estimated using the following,

$\begin{array}{cc}{Z}_{\mathrm{eff}}=\frac{{\sum }_i{f}_i{Z}_i^{1.3}}{{\sum }_i{f}_i{Z}_i^{0.3}}& \left(7\right)\end{array}$

Based on Eq. (7) and the above values, Z_eff=5.1 after Li plating. FIGS. 20C and 20D show EELS spectra before and after Li plating at the location marked (+) in FIG. 20A. The Li K-edge of Li was obtained by background subtraction. Based on the EELS spectra, the thickness of the CHT before and after Li plating were estimated to be about 68 nm and about 160 nm. Therefore, the thickness difference, which corresponds to the thickness of the Li plated, was estimated to be about 92 nm (the inner-diameter of the tubule is about 100 nm).

As further demonstration of the scalable nature of the MIEC 1110 mechanisms described herein, FIGS. 21A and 21B show another set of TEM images where Li is plated simultaneously along three aligned tubules. In FIG. 21B, the brightness is darker, indicating deposition of Li, despite blurring caused by thicker walls of each CHT. Larger scale demonstrations of an exemplary MIEC 1110 are described in further detail below.

As previously mentioned, the transport of the alkali metal 1300 may be primarily driven by the Coble creep mechanism when the characteristic width of each pore in the open pore structure 1120 is less than about 300 nm. For example, FIGS. 22A and 22B show Li plating and stripping, respectively, in a CHT with a 200 nm diameter. FIGS. 23A and 23B show Li plating and stripping, respectively, in a CHT with a 100 nm diameter. FIG. 24 shows Li plating in a CHT with a 30 nm diameter. FIG. 25 shows Li plating in a CHT with a 60 nm diameter. The wall thicknesses ranged between about 50 to 60 nm.

For FIGS. 24 and 25, the small amount of Li deposited within the CHT results in a low image contrast; hence, the presence of Li is difficult to observe. To show Li was plated in these smaller tubules, a large reverse bias voltage of 10 V may be applied, causing Li to overflow from the CHT. This is indicated by a bulge of Li in FIG. 24 and a leak of Li in FIG. 25.

As described above, the open pore structure 1120 formed by the MIEC 1110 may be coated with an alkaliphilic coating that increases wettability towards the alkali metal 1300, thus increasing ionic and electrical contact with the MIEC 1110. Experiments were performed to characterize the interface between the BCC Li metal (the alkali metal 1300) and a Li₂O coating (the alkaliphilic coating) formed, in part, by coating the CHT with ZnO_x, which results a conversion/alloying reaction of ZnO_x+(2x+y)Li=ZnLi_y+xLi₂O. Due to challenges in observing the Li₂O coating inside the CHT, the Li metal was intentionally over-plated during deposition in order to increase the pressure P_LiMetal(x) until Li metal whiskers were extruded out of the CHT. The Li whiskers, which included the Li₂O coating, were then analyzed.

FIG. 26A shows an SEM image of an exemplary CHT coated with ZnO_x. FIGS. 26B-26D show EDX maps of C, O, and Zn, respectively. As shown, the ZnO_x coating is uniformly distributed in the CHT. FIGS. 27A-27C show corresponding XPS spectra for the Cis, Zn2P_3/2, and O1s lines, which further confirms the presence of ZnO_x. For instance, the O1s peak in FIG. 27C may be attributed to a sum of two peaks corresponding to C—O and Zn—O. FIGS. 28A and 28B show EDX spectra of the CHT sample before and after acid treatment. FIG. 29 shows a table of the Zn and O ratios in the CHT samples before and after said acid treatment. The stoichiometry of ZnO_x may be estimated from FIG. 29 to be x about (10.01−9.09)/2.03=0.45. The atomic ratio of zinc atoms of zinc oxide to carbon atoms is about 2%.

FIGS. 30A-30E show a series of dark-field images of an exemplary CHT being over-plated with Li. FIG. 30A shows the Li metal is initially plated inside the CHT. FIG. 30B shows that after additional deposition of Li, the Li metal breaks through the CHT wall and begins to wet the outer surface of the CHT. FIGS. 30C and 30D show that with further Li deposition, the Li metal spreads across the exterior surface of the CHT. FIG. 30E shows that after Li sufficiently wets the outer surface of the CHT, subsequent deposition of Li results in an outgrowth of Li, thus forming the Li whisker.

FIG. 31 shows a HRTEM image of the CHT before Li plating. As shown, no Li₂O layer was observed to be present on the outer surface of the CHT. FIGS. 32A-32C show the Li₂O layer growing from the outer surface of the CHT as the Li metal is being over-plated in the CHT. FIG. 32D shows a magnified image of FIG. 32C where the lattice fringes of the Li₂O coating are observable. As shown, the lattice fringes exhibit a spacing of 0.27 nm corresponding to the lattice spacing of the Li₂O (111) planes. FIG. 33 shows an HRTEM image of the Li₂O coating formed onto the carbon surface of the CHT.

FIG. 34A shows an image of a Li whisker extending from the outer surface of the CHT. As shown, the whisker exhibits favorable parallel interfaces between the {110} crystal planes of Li metal and the {111} crystal planes of Li₂O (i.e. {110}_{BCC Li}//{111}_{FCC Li2O}). FIG. 34B shows a SAED pattern of the Li whisker and the Li₂O coating where the side edges of the Li whisker are shown as {110}_BCC planes. FIG. 34C further shows an HRTEM image of the Li₂O layer on the Li metal. The side edges of the Li₂O coating present{111}_FCC planes.

The Li₂O layer has an FCC crystal structure, thus the {110}_BCC//{111}_FCC orientation relationship is similar to the Kurdjumov-Sachs orientation relationship (OR) in various steels. Both the {111}_FCC and {110}_BCC are slip planes, thus the orientation relationship may be formed due to minute local slippage. The OR provides strong adhesion between the Li and Li₂O phases, thus enabling the Li₂O crystalline layer to remain attached to the Li metal as a lubricant layer. The lateral growth of the Li₂O layer by interfacial diffusion was observed on a thicker Li metal nanostructure outside the tubule. FIGS. 35A and 35B show the {111}_Li2O planes, which are parallel to the outer surface of the CHT, advancing outwards. FIG. 35C shows EELS spectra of the Li K-edge on the outer layer of Li₂O. Li₂O is shown as a shoulder feature in the spectra. These results show that post-formed Li₂O nanocrystals may also creep and re-arrange to wet the Li metal.

Based on the results above, a few-nm thick Li₂O layer may function as a ‘lubricant’ by enabling slight slippage between the Li and Li₂O surfaces, which increases the mechanical durability and provides strong adhesion between the Li metal and the MIEC, thus ensuring lithiophilicity on the MIEC wall.

In some implementations, the thin lubricant layer may spread onto at least one of the current collector 1140 and/or the solid electrolyte 1400. Once this occurs, a thin wetting layer of Li metal may follow, forming an atomically-thin, but effective ionic and electronic conduction channel (“composite interfacial MIEC”). The thin wetting layer of Li metal may ensure any Li metal in the open pore structure 1120 (e.g., the Li metal beads α, β, and γ in FIG. 1) is connected to the MIEC 1110. In other words, the thin wetting layer of Li may prevent the formation of patches with poor conductivity that may otherwise generate dead Li in the MIEC 1110.

Cycling tests were also performed on a single CHT where Li metal was continually transported into and out of the CHT. FIG. 36A shows the charging profile (voltage as a function of time) for the first cycle (i.e., first lithiation) at a galvanostatic current of 50 pA. As shown, the voltage progressively decreases when larger than 0 V. This sloped voltage feature is attributed to the lithiation of the CHT, which enables the CHT to function as the MIEC 1110. When the voltage falls below 0 V during the same lithiation cycle, the voltage saturates to a stable plateau at about −0.25 V corresponding to the plating of Li metal inside the CHT.

FIG. 36B shows the charging profile for subsequent cycles after the CHT is first lithiated at a galvanostatic current of 50 pA. As shown, the voltage remains fairly stable below 0 V when charging the CHT, which corresponds to BCC Li being plated inside the CHT. When discharging the CHT, the voltage remains stable above 0 V corresponding to BCC Li being stripped form the CHT. The charge process occurred at an overpotential of about −0.15 V and the discharge process occurred at an overpotential of about 0.25V. FIG. 36B also shows corresponding TEM images of the CHT, the CHT after Li plating, and the CHT after Li stripping. As shown, the CHT after Li plating is a darker gray, which indicates Li metal filled the CHT.

FIGS. 37A-37K each show a series of TEM images of the CHT being charged (Li deposition) and discharged (Li stripping) for the 1^st, 10^th, 20^th, 30^th, 40^th, 50^th, 60^th, 70^th, 80^th, 90^th, and 100^th cycle. As shown, the CHT remains mechanically intact after 100 cycles of Li metal plating and stripping.

The experimental demonstrations described above have focused on using Li as the alkali metal 1300 in the MIEC 1110. However, it should be appreciated that the transport mechanisms and the designs for the MIEC 1110 and open pore structure 1120 are general and may be applied to other materials including, but not limited to sodium (Na) and potassium (K). For example, FIG. 38A shows a series of TEM images where Na metal is deposited inside a CHT. FIG. 38B shows a series of TEM images of Na metal being stripped from the CHT. Similar to the Li metal experiments, the Na metal may be transported through the interior space of the CHT with a well-defined front. This suggests Na metal may also be transported through the CHT by interfacial diffusion. FIG. 38C shows a SAED pattern of the CHT after being plated with Na metal. As shown, the pattern exhibits well-defined spots corresponding to Na crystal planes. This suggests the Na metal is transported as a substantially single crystalline solid in the CHT.

A Second Exemplary Demonstration with a Carbonaceous MIEC Beehive

The previous demonstration evaluated the transport of alkali metal 1300 through a single (or few) tubules representing the MIEC 1110. To demonstrate the scalability and use of the MIEC 1110 in a practical device, a large scale MIEC was fabricated and integrated into a cm×cm all-solid-state full cell battery. Specifically, a carbonaceous MIEC beehive was fabricated with about 10¹⁰ aligned tubules where each tubule had an aspect ratio on the order of about 10². A half-cell and a full-cell were then assembled with the carbonaceous MIEC beehive for use with Li metal. It should be appreciated the techniques previously described may also be used to characterize the carbonaceous MIEC beehive.

The carbonaceous MIEC beehive was synthesized as a Li host using the following steps: (1) growing a layer of carbon onto the inner surface of an anodic aluminum oxide (AAO) template using chemical vapor deposition (CVD) with a C₂H₂ gas flow rate of 90 sccm at 640° C., (2) depositing a layer of Pt onto the bottom of the AAO template as the current conductor via sputtering, (3) etching the AAO template using a 3M NaOH aqueous solution with a small amount of ethanol to obtain the carbonaceous MIEC beehive, and (4) depositing a 1 nm-thick ZnO layer onto the inner-surface of MIEC beehive using atomic layer deposition (ALD) to enhance the lithiophilicity of the MIEC beehive.

FIGS. 39A-39C show FESEM images of an exemplary carbonaceous MIEC beehive. As shown, the carbonaceous MIEC beehive is comprised of an array of aligned CHT's. FIG. 40 shows a TEM image of a couple CHT's within the carbonaceous MIEC beehive. FIG. 41A shows a SEM image of a portion of the carbonaceous MIEC beehive comprising several tubules. FIGS. 41B-41D show EDX maps of the portion of carbonaceous MIEC beehive of FIG. 41A for C, O, and Zn, respectively. As shown, the 1 nm-thick ZnO layer deposited on the surface of the CHT's is uniform.

Nanoindentation tests were performed to evaluate whether the carbonaceous MIEC beehive can sustain a gas-pressurized environment. FIG. 42 shows a load-displacement curve of the carbonaceous MIEC beehive, which indicates the measured nominal hardness is about 65 MPa.

This hardness is sufficient to sustain at least a gas pressure of about 10¹ MPa (i.e., a compression ratio of 10×) when the gas is compressed by Li metal deposition in the MIEC.

A half-cell 3000 was assembled that included the carbonaceous MIEC beehive, a solid electrolyte, and a Li metal counter-electrode. First, a about 200 nm thick layer of lithium phosphorus oxynitride (LiPON) was deposited onto the MIEC beehive via sputtering deposition to obstruct the open pores, thereby reducing the inflow of polymeric solid electrolyte into the MIEC beehive during testing at 55° C. FIG. 43 shows a FESEM image of an exemplary carbonaceous MIEC beehive partially covered with LiPON. The LiPON does not necessarily provide hermiticity to the carbonaceous MIEC beehive. However, a 50 μm thick contiguous polymeric solid electrolyte layer disposed thereafter does provide hermeticity. A P(EO/EM/AGE)/LiTFSI film (KISCO Ltd.) was used as the solid electrolyte for the half-cell 3000. The MIEC beehive and a Li metal chip (more than 100× excess) were pressed onto opposing sides of the solid electrolyte film to complete assembly of a 2032 coin cell. The Li metal chip was used as the counter-electrode. No (ionic) liquid or gel electrolyte was used.

FIG. 44A shows an image of an exemplary carbonaceous MIEC beehive. The cm×cm×50 μm piece was plated with Pt as the current collector 1140 (see FIG. 44C) and was readily handled during assembly without the MIEC beehive being damaged. FIG. 44B shows an image of an exemplary P(EO/EM/AGE)/LiTFSI film. FIG. 44D shows an FESEM image of the carbonaceous MIEC beehive coated with Pt as the current collector 1140.

FIG. 45A shows a schematic of an exemplary half-cell 3000 using the carbonaceous MIEC beehive for testing. As shown, a voltage source is coupled to the Li counter-electrode and the Pt current collector. The obtained Li/SE/MIEC beehive half-cell 3000 was tested at different current densities of 0.125, 0.25 and 0.5 mA/cm². The half-cell 3000 was initially cycled for several cycles to stabilize the interface between the solid electrolyte and the electrode. Additionally, a reference half-cell was constructed using a carbon-coated Cu foil as the Li host for comparison with the half-cell 3000 using the carbonaceous MIEC beehive.

FIGS. 45B and 45C show exemplary charge/discharge profiles for Li plating and stripping, respectively. The pink line represents the half-cell 3000 with the carbonaceous MIEC beehive and the green line represents the half-cell using the carbon-coated Cu foil as the Li host. FIG. 45D shows the overpotential and Coulombic efficiency (CE) as various current densities. The CE was obtained by calculating the ratio of the discharge and the charge capacity. FIG. 45E shows the charge/discharge voltage profile as a function of time for the half-cells to evaluate cycling stability. When compared to the reference half-cell, the half-cell 3000 with the MIEC exhibits a lower overpotential (39 mV vs 250 mV at 0.125 mA/cm²), a higher CE (97.12% vs 74.34% at 0.125 mA/cm²), and better cycling stability as indicated by the longer lifetime of the half-cell with the MIEC in FIG. 45E.

FIG. 45F shows a chart of the capacity and current density as measured for the half-cell 3000 with the MIEC and the reference half-cell and compared against previously demonstrated batteries. As shown, the half-cell 3000 is able to cycle a large amount of Li metal with a large areal capacity of about 1.5 mAh/cm², which is substantially larger than the reference half-cell (about 1.0 mAh/cm²) and previous all-solid-state batteries (up to about 0.5 mAh/cm²).

A full-cell was also assembled and tested using the carbonaceous MIEC beehive. The full-cell included a LiFePO₄ cathode, which was constructed from the active material LiFePO₄ (60 wt %), polyethylene oxide (PEO, 20 wt %), LiTFSI (10 wt %), and carbon black (10 wt %). The mass loading was 4-6 mg (LiFePO₄)/cm². FIG. 46 shows an image of an exemplary LiFePO₄ cathode. An exemplary 2032 coin cell was constructed using the carbonaceous MIEC beehive as the anode (pre-deposited with only 1× excess Li), the LiFePO₄ electrode as the cathode, and a solid electrolyte in an Ar-filled glove box. It should be appreciated that previous all-solid-state batteries typically use commercial Li foil (100× excess), which results in less efficient use of Li. The all-solid-state battery was tested at 55° C. with a LAND battery tester between 2.5 and 3.85 V. Again no (ionic) liquid or gel electrolyte was used. A reference full-cell was also constructed using a carbon-coated Cu foil as the Li host. Prior to testing, 1× excess Li was also pre-deposited into the Li host of the reference full-cell.

FIG. 47A shows the charge/discharge profile at 0.1 C of the two full-cells. FIG. 47B shows the capacity and CE of the full-cells as a function of the cycling number. The pink line represents the full-cell with the carbonaceous MIEC beehive, and the green line represents the reference full-cell. When compared to the reference full-cell, the full-cell with the carbonaceous MIEC beehive shows a lower overpotential (0.25 V vs 0.45 V), a higher discharge capacity (164 mAh/g vs 123 mAh/g), and a higher CE (99.83% vs 82.22%) at 0.1 C. Furthermore, the full-cell with the carbonaceous MIEC beehive shows little degradation in performance for over 50 cycles with a parsimonious lithium inventory. The full-cell with the carbonaceous MIEC beehive exhibited and average CE of 99.82% and a gravimetric capacity approaching 900 mAh/g (previous all-solid-state batteries yielded a capacity of about 100-300 mAh/g).

FIGS. 48A and 48B further show FESEM images of the carbonaceous MIEC beehive extracted from the full-cell before and after Li plating. As shown, the Li metal was well deposited inside the tubules of the carbonaceous MIEC beehive.

These results show that a practical full-cell device may be constructed using the MIEC 1110 according to theoretically derived design parameters (h=10-100 μm to ensure capacity, W about 100 nm to ensure interfacial Coble creep, w about 10 nm to ensure mechanical robustness, and hermetic soft SE cap for pressurization).

A Third Exemplary Demonstration with a Non-Carbonaceous MIEC Beehive

The MIEC 1110 may be formed from a broad range of materials that are electrochemically stable against the alkali metal 1300. In particular, the MIEC 1110 and the open pore structure 1120 may be configured to transport alkali metal 1300 primarily by an interfacial diffusion mechanism. As described above, this allows for greater flexibility when selecting the material to construct the MIEC 1110 because the electronic and ionic transport properties depend primarily on the structure and dimensions of the open pore structure 1120 rather than the material composition of the MIEC 1110.

To demonstrate the general applicability of the designs and mechanisms described herein, another exemplary MIEC 1110 was fabricated from titanium nitride (TiN). As shown in the equilibrium phase diagram of FIG. 7B, TiN is thermodynamically and electrochemically stable against Li. Thus, when TiN is in naked contact with Li metal, no reactions will occur and no SEI is formed. Additionally, TiN is a mechanically robust material (e.g., TiN is used as anti-wear coatings and drill bits), naturally metallic, and forms an incoherent interface with the Li metal.

A TiN honeycomb MIEC was synthesized by reacting anodized TiO₂ template with ammonia gas as shown in FIG. 49A. The TiN MIEC was fabricated to have the same dimensional parameters as the carbonaceous MIEC beehive described previously (e.g., about 10¹⁰ parallel capped cylinders). FIGS. 49B-49E show various SEM images of an exemplary TiN MIEC. As shown, the MIEC is formed as a closed packed array of TiN tubules in a honeycomb arrangement. The TiN MIEC was found to be mechanically robust. For instance, a cm×cm piece of the MIEC 1110 was readily handled by a user's hands without fracturing. The TiN MIEC also exhibits a hardness up to about 2 GPa based on a nanoindentation test as shown in FIG. 50A. A 1 nm-thick Al₂O₃ (or ZnO) layer was deposited onto the inner-surface of the TiN MIEC beehive using atomic layer deposition (ALD) to enhance the lithiophilicity of the TiN MIEC beehive.

A half-cell 3000 was assembled with the TiN MIEC using a similar architecture to the carbonaceous MIEC previously described. The half-cell 3000 was tested at 55° C. FIG. 50B shows an exemplary Li plating and stripping voltage profile as a function of the capacity. FIG. 50C shows the overpotential and CE at various current densities. FIG. 50D shows the charge/discharge profiles of the Li/SE/TiN MIEC beehive half-cell 3000 as a function of time. The pink line represents the half-cell 3000 with the TiN MIEC. The green line represents a half-cell with a TiN-coated Ti foil as the Li host. As shown, the half-cell 3000 exhibits a lower overpotential (45 mV vs 250 mV for the reference half-cell at 0.125 mA/cm²), a higher Coulombic efficiency (97% vs 65% for the reference half-cell at 0.125 mA/cm²), and greater cycling stability. The half-cell 3000 was also able to cycle a large amount of Li metal with an areal capacity of 1.5 mAh/cm², which is substantially higher than previous all-solid batteries (typically less than 0.5 mAh/cm²).

An all-solid-state full-cell was also assembled using the TiN MIEC. Specifically, the full cell comprised (1× excess) Li predeposited TiN MIEC beehive/SE/LiFePO₄ battery. A 1×excess amount of Li metal was predeposited electrochemically inside the TiN MIEC beehive before the full cell was cycled. FIG. 51A shows an exemplary charge/discharge profile of the full-cell. FIG. 51B shows the cycling life of the full-cell. A reference full-cell was also assembled using TiN-coated Ti foil as the Li host. Compared to the reference full-cell, the full-cell with the TiN MIEC exhibited a lower overpotential (0.17 V vs 0.4 V), a higher discharge capacity (162 mAh/g vs 117 mAh/g), and a higher CE (99.95% vs 85.09%) at 0.1 C. Additionally, the parsimonious excess Li full cell showed almost no degradation and maintained a high average CE up to 99.72% for over 50 cycles. These results show that the design of the MIEC 1110 and the transport mechanisms within the open pore structure 1120 are applicable to a broad range of materials.

FIGS. 52A-52C shows another exemplary MIEC 1110 formed from anodized aluminum oxide (AAO). FIG. 52A shows an image of a cm×cm piece of the AAO MIEC. FIGS. 52B and 52C show SEM images of the open pore structure formed within the AAO MIEC. As shown, the AAO MIEC may be formed with substantially aligned tubules. FIG. 53A shows yet another exemplary MIEC formed from a silicon mesh. FIGS. 53B-53D show the silicon MIEC may have highly aligned tubules arranged in a closed pack array.

MIEC Chemical Compositions

In some implementations, any of the MIECs described above may be formed from various binary, tertiary, or quaternary compound materials having a particular set of properties. These properties include electronic conductivity (>10⁶ S/m), electrochemical stability against the alkali metal, and electrochemical stability against the solid electrolyte. Electrochemical stability of the MIEC against the alkali metal reduces or substantially prevents the MIEC from decomposing to form fresh SEI at the interface between the MIEC and the alkali metal. Electrochemical stability of the MIEC against the solid electrolyte reduces or substantially prevents the MIEC from decomposing to form fresh SEI at the interface between the MIEC and the solid electrolyte. Electrochemical stability may be evaluated based on thermodynamic stability.

The MIEC material may be computationally chosen from a database (e.g., The Materials Project: A materials genome approach to accelerating materials innovation) using the property criteria above. Specifically, a list of binary, tertiary, and quaternary compounds was generated. From this list, to screen for materials that are electronically conductive, any materials having a bandgap smaller than 3 eV were selected. Electrochemical stability of the MIEC against the alkali metal was screened using equilibrium phase diagrams. Materials with an end-member phase directly connected to an alkali metal by a tie-line in an equilibrium phase diagram were selected. Electrochemical stability of the MIEC against the solid electrolyte was screened using equilibrium phase diagrams and/or through experimentation. Materials with an end-member phase directly connected to the solid electrolyte by a tie-line in an equilibrium phase diagram were selected. Electrochemical stability against the solid electrolyte was screened experimentally by measuring the impedance over time of a bilayer of MIEC and solid electrolyte. Any materials having an impedance change over time less than 20% per hour were selected. The resulting list includes MIEC materials that have all three properties.

FIG. 55 shows an example equilibrium phase diagram between MIEC TiFe and the solid electrolyte Li₇La₃Zr₂O₁₂(LLZO). An electrochemically stable compound is formed when the two compounds are directly connected by a tie-line. As shown, TiFe and LLZO are end-member phases directly connected to each other by a tie-line. Therefore, the MIEC TiFe is electrochemically stable against the solid electrolyte LLZO. For comparison, FIG. 56 shows an equilibrium phase diagram between Li metal and the solid electrolyte LLZO. As shown, Li and LLZO are not directly connected to each other by a tie-line. Instead, there is a lower energy intermediate phase between Li and LLZO, indicating that unstable phases (e.g., Zr₄O, Li₂O, or La₂O₃) may be formed at the interface between Li and LLZO.

In some implementations, the list of MIEC materials is additionally screened to select inexpensive chemical elements. Materials that only include inexpensive chemical elements may be cheaper to produce and may be preferably for large scale production. In one implementation, inexpensive chemical elements may be screened by excluding any lanthanide elements. In another implementation, inexpensive chemical elements may be screened by excluding any rare earth metals. In another implementation, inexpensive chemical elements may be screened by excluding any compounds that include any of the following elements: beryllium, scandium, vanadium, gallium, germanium, krypton, niobium, technetium, ruthenium, palladium, gold, indium, tellurium, xenon, hafnium, tantalum, rhenium, osmium, iridium, platinum, silver, thallium, praseodymium, neodymium, promethium, terbium, dysprosium, thulium, and lutetium.

The accompanying APPENDICES constitute part of the present disclosure. The APPENDICES 1-3 include lists of MIEC materials that may be used as anodes in lithium, sodium, and potassium-based batteries, respectively. The APPENDICES include the chemical formulas, Materials Project identification number (“Material ID”), bandgaps (eV), density (g/cm³), price (USD), number of atoms in the compound, and price per atom for each of the MIEC materials. Compound price was calculated using prices of each element in in the compound. For example, if the prices of elements A and B are PA and PB, respectively, the price for A₂B₃ is 2×P_A+3×P_B. The price per atom is the compound price divided by the number of atoms in the compound's chemical formula. For example, for the compound A₂B₃, the price per atom is (2×P_A+3×P_B)/(2+3). The price per atom is a way of comparing prices between compounds with different numbers of atoms, since a compound with a fewer number of atoms will likely have a lower compound price, as calculated here, than a compound with a higher number of atoms.

All of the materials in the APPENDICES have an energy above hull equal to zero, indicating thermodynamic stability.

The MIEC material may include an aluminum (Al) alloy. For example, the MIEC material may be formed from aluminum alloyed with nickel, cobalt, iron, molybdenum, or vanadium.

The MIEC material may include a barium (Ba) compound. For example, the MIEC material may be formed from a barium compound including sodium, mercury, lead, boron, carbon, copper, lithium, or strontium.

The MIEC material may include beryllium (Be) or a beryllium compound. For example, the beryllium compound may include carbon or copper.

The MIEC material may include a calcium (Ca) compound. For example, the calcium compound may include gallium, copper, nitrogen, silicon, zinc, boron, beryllium, copper, magnesium, or nickel.

The MIEC material may include cerium (Ce) or a cerium compound. For example, the cerium compound may include carbon, gallium, silicon, aluminum, boron, copper, gallium, nitrogen, or zinc.

The MIEC material may include cobalt (Co) or a cobalt compound. For example, the cobalt compound may include nickel, tungsten, or boron.

The MIEC material may include chromium (Cr) or a chromium compound. For example, the chromium compound may include carbon, boron, silicon, or nickel.

The MIEC material may include cesium (Ce) or a cesium compound. For example, the cesium compound may include carbon.

The MIEC material may include erbium (Er) or an erbium compound. For example, the erbium compound may include aluminum, carbon, gallium, boron, or nitrogen.

The MIEC material may include europium (Eu) or a europium compound. For example, the europium compound may include nitrogen, gallium, silicon, boron, carbon, or mercury.

The MIEC material may include iron (Fe) or an iron compound. For example, the iron compound may include cobalt, boron, cobalt, silicon, boron, or nickel.

The MIEC material may include gadolinium (Ga) or a gadolinium compound. For example, the gadolinium compound may include boron, carbon, indium, aluminum, boron, gallium, or nitrogen.

The MIEC material may include hafnium (Hf) or a hafnium compound. For example, the hafnium compound may include nitrogen or carbon.

The MIEC material may include holmium (Ho) or a holmium compound. For example, the holmium compound may include aluminum, carbon, gallium, or boron.

The MIEC material may include potassium (K) or a potassium compound. For example, the potassium compound may include carbon.

The MIEC material may include lithium (Li) or a lithium compound. For example, the lithium compound may include indium, chromium, nitrogen, lead, tin, silicon, aluminum, calcium, nitrogen, cerium, europium, gallium, gadolinium, tellurium, hafnium, holmium, neodymium, samarium, ytterbium, yttrium, zinc, copper, zirconium, cadmium, mercury, scandium, titanium, molybdenum, manganese, boron, beryllium, cobalt, erbium, magnesium, and/or nickel.

The MIEC material may include a magnesium (Mg) compound. For example, the magnesium compound may include copper or nickel.

The MIEC material may include manganese (Mn) or a manganese compound. For example, the manganese compound may include carbon, boron, chromium, cobalt, niobium, silicon, iron, aluminum, nickel and/or vanadium.

The MIEC material may include molybdenum (Mo) and/or sodium (Na).

The MIEC material may include niobium (Nb) or a niobium compound. For example, the niobium compound may include boron, nitrogen, cobalt, chromium, iron, nickel, vanadium, and/or tungsten.

The MIEC material may include neodymium (Nd) or a neodymium compound. For example, the neodymium compound may include boron, carbon, cobalt, gallium, silicon, aluminum, copper, nitrogen, or zinc.

The MIEC material may include nickel (Ni) or a nickel compound. For example, the nickel compound may include boron, molybdenum, or tungsten.

The MIEC material may include rubidium (Rb) or a rubidium compound. For example, the rubidium compound may include carbon.

The MIEC material may include scandium (Sc) or a scandium compound. For example, the scandium compound may include iron, silicon, aluminum, carbon, cobalt, gallium, indium, boron, copper, nitrogen, and/or zinc.

The MIEC material may include samarium (Sm) or a samarium compound. For example, the samarium compound may include boron, carbon, gallium, silicon, aluminum, boron, copper, or nitrogen.

The MIEC material may include strontium (Sr) or a strontium compound. For example, the strontium compound may include lithium, mercury, cobalt, nitrogen, tellurium, lead, chromium, calcium, silicon, tin, or magnesium.

The MIEC material may include tantalum (Ta) or a tantalum compound. For example, the tantalum compound may include aluminum, beryllium, nitrogen, silicon, or tungsten.

The MIEC material may include titanium (Ti) or a titanium compound. For example, the titanium compound may include manganese, carbon, cobalt, copper, gallium, manganese, iron, nickel, nitrogen, zinc, aluminum, and/or boron.

The MIEC material may include vanadium (V) or a vanadium compound. For example, the vanadium compound may include boron, carbon, chromium, iron, nickel, cobalt, silicon, and/or tungsten.

The MIEC material may include tungsten (W) or a tungsten compound. For example, the tungsten compound may include carbon.

The MIEC material may include yttrium (Y) or an yttrium compound. For example, the yttrium compound may include nickel, carbon, cobalt, gallium, lead, silicon, tin, aluminum, boron, copper, iron, magnesium, manganese, zinc, or nitrogen.

The MIEC material may include ytterbium (Yb) or an ytterbium compound. For example, the ytterbium compound may include carbon, gallium, silicon, nitrogen, boron, indium, tellurium, aluminum, copper, or mercury.

The MIEC material may include zirconium (Zr) or a zirconium compound. For example, the zirconium compound may include carbon, copper, beryllium, nitrogen, silicon, iron, scandium, manganese, or nickel.

FIG. 56 shows the relationship between anode thickness and porosity for MIECs with different areal capacities. The graph shows the anode minimum anode thickness needed for a given MIEC porosity and desired areal capacity. The three exemplary areal capacities are 3.4 mAh cm⁻², 4 mAh cm⁻², and 6 mAh cm⁻². The trends show that MIECs with higher porosity can have the desired areal capacities with smaller thickness as compared to MIECS with lower porosity. For example, for an areal capacity of 6 mAh cm⁻², a 150 μm thick MIEC can have 20% porosity or higher. On the other hand, an anode approaching a porosity of 100% can be as thin as 30 μm in thickness. The graph compares the MIEC trends to a graphite anode with a thickness of 67 μm, illustrating that MIECs thinner than 67 μm may have an areal capacity of 6 mAh cm⁻² with porosities of about 45% or higher.

CONCLUSION

While various inventive embodiments have been described and illustrated herein, those of ordinary skill in the art will readily envision a variety of other means and/or structures for performing the function and/or obtaining the results and/or one or more of the advantages described herein, and each of such variations and/or modifications is deemed to be within the scope of the inventive embodiments described herein. More generally, those skilled in the art will readily appreciate that all parameters, dimensions, materials, and configurations described herein are meant to be exemplary and that the actual parameters, dimensions, materials, and/or configurations will depend upon the specific application or applications for which the inventive teachings is/are used. Those skilled in the art will recognize or be able to ascertain, using no more than routine experimentation, many equivalents to the specific inventive embodiments described herein. I_t is, therefore, to be understood that the foregoing embodiments are presented by way of example only and that, within the scope of the appended claims and equivalents thereto, inventive embodiments may be practiced otherwise than as specifically described and claimed. Inventive embodiments of the present disclosure are directed to each individual feature, system, article, material, kit, and/or method described herein. In addition, any combination of two or more such features, systems, articles, materials, kits, and/or methods, if such features, systems, articles, materials, kits, and/or methods are not mutually inconsistent, is included within the inventive scope of the present disclosure.

Also, various inventive concepts may be embodied as one or more methods, of which an example has been provided. The acts performed as part of the method may be ordered in any suitable way. Accordingly, embodiments may be constructed in which acts are performed in an order different than illustrated, which may include performing some acts simultaneously, even though shown as sequential acts in illustrative embodiments.

All definitions, as defined and used herein, should be understood to control over dictionary definitions, definitions in documents incorporated by reference, and/or ordinary meanings of the defined terms.

The indefinite articles “a” and “an,” as used herein in the specification and in the claims, unless clearly indicated to the contrary, should be understood to mean “at least one.”

The phrase “and/or,” as used herein in the specification and in the claims, should be understood to mean “either or both” of the elements so conjoined, i.e., elements that are conjunctively present in some cases and disjunctively present in other cases. Multiple elements listed with “and/or” should be construed in the same fashion, i.e., “one or more” of the elements so conjoined. Other elements may optionally be present other than the elements specifically identified by the “and/or” clause, whether related or unrelated to those elements specifically identified. Thus, as a non-limiting example, a reference to “A and/or B”, when used in conjunction with open-ended language such as “comprising” can refer, in one embodiment, to A only (optionally including elements other than B); in another embodiment, to B only (optionally including elements other than A); in yet another embodiment, to both A and B (optionally including other elements); etc.

As used herein in the specification and in the claims, “or” should be understood to have the same meaning as “and/or” as defined above. For example, when separating items in a list, “or” or “and/or” shall be interpreted as being inclusive, i.e., the inclusion of at least one, but also including more than one, of a number or list of elements, and, optionally, additional unlisted items. Only terms clearly indicated to the contrary, such as “only one of” or “exactly one of,” or, when used in the claims, “consisting of,” will refer to the inclusion of exactly one element of a number or list of elements. In general, the term “or” as used herein shall only be interpreted as indicating exclusive alternatives (i.e., “one or the other but not both”) when preceded by terms of exclusivity, such as “either,” “one of,” “only one of,” or “exactly one of” “Consisting essentially of,” when used in the claims, shall have its ordinary meaning as used in the field of patent law.

As used herein in the specification and in the claims, the phrase “at least one,” in reference to a list of one or more elements, should be understood to mean at least one element selected from any one or more of the elements in the list of elements, but not necessarily including at least one of each and every element specifically listed within the list of elements and not excluding any combinations of elements in the list of elements. This definition also allows that elements may optionally be present other than the elements specifically identified within the list of elements to which the phrase “at least one” refers, whether related or unrelated to those elements specifically identified. Thus, as a non-limiting example, “at least one of A and B” (or, equivalently, “at least one of A or B,” or, equivalently “at least one of A and/or B”) can refer, in one embodiment, to at least one, optionally including more than one, A, with no B present (and optionally including elements other than B); in another embodiment, to at least one, optionally including more than one, B, with no A present (and optionally including elements other than A); in yet another embodiment, to at least one, optionally including more than one, A, and at least one, optionally including more than one, B (and optionally including other elements); etc.

In the claims, as well as in the specification above, all transitional phrases such as “comprising,” “including,” “carrying,” “having,” “containing,” “involving,” “holding,” “composed of,” and the like are to be understood to be open-ended, i.e., to mean including but not limited to. Only the transitional phrases “consisting of” and “consisting essentially of” shall be closed or semi-closed transitional phrases, respectively, as set forth in the United States Patent Office Manual of Patent Examining Procedures, Section 2111.03.

					Total
Material ID	Chemical Formula	Band Gap	Density	Price	No. Atoms	Unit Price
mp-16514	Al3Ni5	0	6.717313154	74.87	8	9.36
mp-284	AlCo	0	6.136768975	34.59	2	17.29
mp-2658	AlFe	0	5.791723495	2.214	2	1.11
mp-1183162	AlFe3	0	6.647849573	3.062	4	0.77
mp-259	AlMo3	0	8.470007673	122.09	4	30.52
mp-1487	AlNi	0	5.906844592	15.69	2	7.85
mp-2593	AlNi3	0	7.466731653	43.49	4	10.87
mp-1387	AlV3	0	5.367846693	1156.79	4	289.2
mp-569025	Bal9Na29Li13	0.0147	2.190395396	1217.495	61	19.96
mp-8094	Ba2Hg	0	5.677447644	30.75	3	10.25
mp-21246	Ba2Pb	0.0383	5.787075882	2.55	3	0.85
mp-954	BaB6	0.0623	4.281989038	22.355	7	3.19
mp-1214417	BaC6	0	3.961948599	1.007	7	0.14
mp-30428	BaCu	0	4.510555041	6.275	2	3.14
mp-210	BaLi4	0	1.84849371	342.675	5	68.53
mp-1227650	BaSr4	0	2.867111399	26.995	5	5.4
mp-87	Be	0	1.895724397	857	1	857
mp-1569	Be2C	1.4433	2.461261614	1714.122	3	571.37
mp-2031	Be2Cu	0	5.046496677	1720	3	573.33
mp-1227357	Be3Cu	0	4.407823439	2577	4	644.25
mp-568793	Ca28Ga11	0	2.585516676	1693.8	39	43.43
mp-12614	Ca2Cu	0	2.62950025	10.7	3	3.57
mp-2686	Ca2N	0	2.161682878	4.84	3	1.61
mp-2517	Ca2Si	0.2915	2.165187656	6.4	3	2.13
mp-2786	Ca5Zn3	0	2.763436877	19.4	8	2.42
mp-1213975	CaB4	0	2.631299144	17.07	5	3.41
mp-865	CaB6	0.1835	2.437995559	24.43	7	3.49
mp-1845	CaBe13	0	1.9473521	11143.35	14	795.95
mp-585949	CaCu	0	3.622394066	8.35	2	4.17
mp-1882	CaCu5	0	6.536938774	32.35	6	5.39
mp-2432	CaMg2	0	1.731927308	6.99	3	2.33
mp-2295	CaNi2	0	5.661732669	30.15	3	10.05
mp-774	CaNi5	0	6.747575602	71.85	6	11.97
mp-567332	Ce	0	8.91786665	4.71	1	4.71
mp-20181	Ce2C3	0	7.074733812	9.786	5	1.96
mp-19920	Ce3Ga	0	8.078079142	162.13	4	40.53
mp-570175	Ce5Si3	0	6.736034132	28.65	8	3.58
mp-2088	CeAl2	0	5.124395241	8.29	3	2.76
mp-1974	CeB4	0	5.80804567	19.43	5	3.89
mp-2801	CeCu2	0	8.065457036	16.71	3	5.57
mp-581942	CeCu6	0	8.455393218	40.71	7	5.82
mp-1018276	CeGa	0	6.849881989	152.71	2	76.36
mp-2493	CeN	0	7.942475673	4.85	2	2.42
mp-1385	CeZn2	0	7.159182995	9.81	3	3.27
mp-54	Co	0	8.959676195	32.8	1	32.8
mp-1183837	Co3Ni	0	9.020551201	112.3	4	28.07
mp-2157	Co3W	0	12.92411922	133.7	4	33.42
mp-20857	CoB	0	7.456589549	36.48	2	18.24
mp-90	Cr	0	7.274080971	9.4	1	9.4
mp-723	Cr23C6	0	7.16779993	216.932	29	7.48
mp-569424	Cr2B	0	6.745889607	22.48	3	7.49
mp-20937	Cr3C2	0	6.795180146	28.444	5	5.69
mp-729	Cr3Si	0	6.625100709	29.9	4	7.48
mp-15617	Cr5B3	0	6.587365994	58.04	8	7.25
mp-1196316	Cr7C3	0	7.055496191	66.166	10	6.62
mp-1080664	CrB	0	6.267642518	13.08	2	6.54
mp-784631	CrNi2	0	8.620907303	37.2	3	12.4
mp-1184151	Cs	0.1362	1.885761278	61800	1	61800
mp-28861	CsC8	0	2.893417416	61800.976	9	6866.78
mp-1184115	Er	0	9.037772387	26.4	1	26.4
mp-1102875	Er2Al	0	7.795030975	54.59	3	18.2
mp-1225044	Er2C	0	8.678709228	52.922	3	17.64
mp-1203719	Er3C4	0	8.934402703	79.688	7	11.38
mp-1198546	Er3Ga2	0	8.725322058	375.2	5	75.04
mp-1212833	Er4C7	0	8.047974214	106.454	11	9.68
mp-1188739	ErAl	0	7.003065103	28.19	2	14.09
mp-1208	ErAl2	0	6.140750389	29.98	3	9.99
mp-1774	ErB2	0	8.881021436	33.76	3	11.25
mp-2847	ErB4	0	6.998729948	41.12	5	8.22
mp-1018077	ErGa	0	8.420288617	174.4	2	87.2
mp-19830	ErN	0.2716	10.56582866	26.54	2	13.27
mp-1057315	Eu	0	6.086594594	31.4	1	31.4
mp-1212961	Eu2N	0	7.081393454	62.94	3	20.98
mp-672286	Eu3Ga2	0	6.8305628	390.2	5	78.04
mp-1190061	Eu5Si3	0	6.153676988	162.1	8	20.26
mp-20874	EuB6	0	4.963690743	53.48	7	7.64
mp-1103990	EuC6	0	4.7983116	32.132	7	4.59
mp-11375	EuHg	0	9.836400238	61.6	2	30.8
mp-13	Fe	0	8.096264696	0.424	1	0.42
mp-601848	Fe11Co5	0	8.108531664	168.664	16	10.54
mp-1915	Fe2B	0	7.490316494	4.528	3	1.51
mp-601820	Fe3Co	0	8.136129184	34.072	4	8.52
mp-2199	Fe3Si	0	7.388613931	2.972	4	0.74
mp-601842	Fe9Co7	0	8.206826997	233.416	16	14.59
mp-1080525	FeB	0	6.887696687	4.104	2	2.05
mp-2090	FeCo	0	8.290362741	33.224	2	16.61
mp-2213	FeNi	0	8.452470899	14.324	2	7.16
mp-1418	FeNi3	0	8.700535754	42.124	4	10.53
mp-155	Gd	0	8.001978666	28.6	1	28.6
mp-28366	Gd2B5	0	6.836473994	75.6	7	10.8
mp-1224869	Gd2C	0	7.676989498	57.322	3	19.11
mp-1189998	Gd2C3	0	7.992746631	57.566	5	11.51
mp-1184479	Gd3In	0	8.319657649	252.8	4	63.2
mp-1078585	GdAl	0	6.301011344	30.39	2	15.2
mp-19923	GdAl2	0	5.660330479	32.18	3	10.73
mp-1105563	GdB4	0	6.464597962	43.32	5	8.66
mp-20353	GdGa	0	7.531847056	176.6	2	88.3
mp-940	GdN	0	9.164612692	28.74	2	14.37
mp-103	Hf	0	13.1832226	900	1	900
mp-864647	Hf2N	0	13.23693362	1800.14	3	600.05
mp-1224388	Hf3N2	0	13.38748853	2700.28	5	540.06
mp-21075	HfC	0	12.57416771	900.122	2	450.06
mp-2828	HfN	0	13.68399725	900.14	2	450.07
mp-10659	Ho	0	8.822554243	57.1	1	57.1
mp-16502	Ho2Al	0	7.595654792	115.99	3	38.66
mp-1640	Ho2C	0	8.412835248	114.322	3	38.11
mp-1202754	Ho3C4	0	8.700157642	171.788	7	24.54
mp-1197194	Ho3Ga2	0	8.474139572	467.3	5	93.46
mp-15238	Ho4C5	0	8.4097617	229.01	9	25.45
mp-1154	Ho4C7	0.5867	7.857241425	229.254	11	20.84
mp-1188420	HoAl	0	6.849503074	58.89	2	29.45
mp-391	HoAl2	0	6.026340563	60.68	3	20.23
mp-2267	HoB2	0	8.64241442	64.46	3	21.49
mp-569281	HoB4	0	6.870160089	71.82	5	14.36
mp-1018073	HoGa	0	8.171440104	205.1	2	102.55
mp-1184905	K	0	0.868387443	13.6	1	13.6
mp-28930	KC8	0	1.94998649	14.576	9	1.62
mp-1018134	Li	0	0.57309457	85.6	1	85.6
mp-510430	Li13In3	0	2.471080344	1613.8	16	100.86
mp-530262	Li15Cr2N9	1.3186	2.264412819	1304.06	26	50.16
mp-574275	Li17Pb4	0	3.961250168	1463.2	21	69.68
mp-573471	Li17Sn4	0	2.589548849	1530	21	72.86
mp-29720	Li21Si5	0	1.194591756	1806.1	26	69.47
mp-1210753	Li2Al	0	1.381340819	172.99	3	57.66
mp-570466	Li2Ca	0	1.083251032	173.55	3	57.85
mp-865892	Li2CaPb	0	4.99870701	175.55	4	43.89
mp-865964	Li2CaSn	0	3.437484923	192.25	4	48.06
mp-8181	Li2CeN2	1.2874	4.945453705	176.19	5	35.24
mp-867474	Li2EuSn	0	5.218903259	221.3	4	55.32
mp-29210	Li2Ga	0	2.981136533	319.2	3	106.4
mp-865483	Li2GdIn	0	5.813516989	366.8	4	91.7
mp-865349	Li2GdTl	0	7.399440183	4399.8	4	1099.95
mp-1097065	Li2HfN2	1.9339	7.258069278	1071.48	5	214.3
mp-865622	Li2HoIn	0	6.080581177	395.3	4	98.82
mp-571109	Li2Nd2Si3	0	4.610515699	291.3	7	41.61
mp-866181	Li2NdIn	0	5.26976998	395.7	4	98.92
mp-866179	Li2NdTl	0	6.985206985	4428.7	4	1107.17
mp-865882	Li2SmIn	0	5.493008058	352.1	4	88.03
mp-866200	Li2SmTl	0	7.290083353	4385.1	4	1096.28
mp-866180	Li2YbPb	0	7.62836771	190.3	4	47.57
mp-866191	Li2YbSi	0	5.138016993	190	4	47.5
mp-866192	Li2YbSn	0	6.162863309	207	4	51.75
mp-1185233	Li2YIn	0	4.476946026	369.2	4	92.3
mp-865867	Li2YTl	0	6.296269637	4402.2	4	1100.55
mp-1222617	Li2ZnCu3	0	5.201276115	191.75	6	31.96
mp-3216	Li2ZrN2	1.6072	4.272989517	208.58	5	41.72
mp-13944	Li3AlN2	2.9373	2.334211251	258.87	6	43.14
mp-867343	Li3Cd	0	2.969003856	259.53	4	64.88
mp-1646	Li3Hg	0	5.233841055	287	4	71.75
mp-1094591	Li3Mg	0	0.919301997	259.12	4	64.78
mp-2251	Li3N	0.9986	1.288608955	256.94	4	64.23
mp-542435	Li3ScN2	2.2441	2.445093005	3717.08	6	619.51
mp-7396	Li3Tl	0	5.009351079	4456.8	4	1114.2
mp-1029592	Li3YN2	2.119	3.139913994	288.08	6	48.01
mp-567219	Li4Ca3(SiN3)2	2.3729	2.81096793	353.69	15	23.58
mp-686208	Li5SiN3	2.1599	2.190394385	430.12	9	47.79
mp-686129	Li5TiN3	1.5626	2.368619669	440.12	9	48.9
mp-1197580	Li6Ca17Hg9	0	4.365574053	825.35	32	25.79
mp-8804	Li6MoN4	2.6302	2.904801508	554.26	11	50.39
mp-1211433	Li6Yb17Hg9	0	8.55124306	1076.1	32	33.63
mp-5515	Li7MnN4	0.6562	2.411213393	601.58	12	50.13
mp-862318	LiAl2Ni	0	3.917294341	103.08	4	25.77
mp-867272	LiAlCu2	0	5.265673911	99.39	4	24.85
mp-867812	LiAlNi2	0	5.466499909	115.19	4	28.8
mp-1001835	LiB	0	1.356921364	89.28	2	44.64
mp-9244	LiBC	1.1272	2.15144616	89.402	3	29.8
mp-1018783	LiBeB	0	1.419715181	946.28	3	315.43
mp-29463	LiBeN	2.6955	1.928563009	942.74	3	314.25
mp-1021323	LiC12	0	2.019463894	87.064	13	6.7
mp-862632	LiCa2Al	0	1.724526216	92.09	4	23.02
mp-867805	LiCa2Ga	0	2.481138243	238.3	4	59.58
mp-867211	LiCa2In	0	2.904955219	257.3	4	64.33
mp-867167	LiCa2Tl	0	4.179821486	4290.3	4	1072.58
mp-6799	LiCa4(BN2)3	2.2792	2.595016582	106.88	14	7.63
mp-1020031	LiCaAlN2	2.7906	2.909897562	90.02	5	18
mp-31468	LiCaN	1.3816	2.335579398	88.09	3	29.36
mp-867293	LiCo2Si	0	6.177891606	152.9	4	38.22
mp-862658	LiCu3	0	6.929195303	103.6	4	25.9
mp-984635	LiErSn	0	7.092056446	130.7	3	43.57
mp-1097959	LiEu4(BN2)3	0	6.087092205	223.08	14	15.93
mp-867197	LiGaNi2	0	6.993255153	261.4	4	65.35
mp-1185392	LiGd2Al	0	5.827301916	144.59	4	36.15
mp-1185394	LiGd2Ga	0	6.702072283	290.8	4	72.7
mp-1191877	LiGdSn	0	6.511111198	132.9	3	44.3
mp-1192002	LiHoSn	0.0064	6.978275183	161.4	3	53.8
mp-37906	LiMgN	2.2707	2.387696644	88.06	3	29.35
mp-1191015	LiNdSn	0.0033	5.906106429	161.8	3	53.93
mp-10181	LiSiNi2	0	5.957779615	115.1	4	28.77
mp-1190768	LiSmSn	0	6.237720383	118.2	3	39.4
mp-862555	LiY2Al	0	3.595054674	149.39	4	37.35
mp-864769	LiYb2Tl	0	8.131782807	4319.8	4	1079.95
mp-14208	LiYSi	0	3.416483679	118.3	3	39.43
mp-504790	LiYSn	0	5.088427374	135.3	3	45.1
mp-1934	LiZn	0	4.082778098	88.15	2	44.07
mp-867252	LiZn2Ni	0	6.431958586	104.6	4	26.15
mp-1185421	LiZnNi2	0	6.737390407	115.95	4	28.99
mp-1038	MgCu2	0	5.816113247	14.32	3	4.77
mp-2675	MgNi2	0	6.032501485	30.12	3	10.04
mp-35	Mn	0	8.265241283	1.82	1	1.82
mp-542830	Mn23C6	0	7.843043604	42.592	29	1.47
mp-20318	Mn2B	0	7.609817023	7.32	3	2.44
mp-864955	Mn2CrCo	0	7.716185888	45.84	4	11.46
mp-12659	Mn2Nb	0	8.479514449	89.24	3	29.75
mp-10118	Mn3B4	0	6.153079405	20.18	7	2.88
mp-1185970	Mn3Co	0	8.77177245	38.26	4	9.56
mp-20211	Mn3Si	0	7.078772648	7.16	4	1.79
mp-21256	Mn7C3	0	7.858680097	13.106	10	1.31
mp-771	MnAl	0	5.127964867	3.61	2	1.81
mp-5529	MnFe2Si	0	7.393942888	4.368	4	1.09
mp-11501	MnNi3	0	8.49819932	43.52	4	10.88
mp-316	MnV	0	7.40626179	386.82	2	193.41
mp-864953	MnV2Cr	0	7.151615215	781.22	4	195.31
mp-864984	MnV3	0	6.851730115	1156.82	4	289.2
mp-129	Mo	0	10.02490812	40.1	1	40.1
mp-10172	Na	0	1.028520018	3.43	1	3.43
mp-75	Nb	0	8.427646884	85.6	1	85.6
mp-1080021	Nb2B3	0	7.075689381	182.24	5	36.45
mp-1079585	Nb2N	0	8.022840826	171.34	3	57.11
mp-20689	Nb3B2	0	7.752632878	264.16	5	52.83
mp-10255	Nb3B4	0	7.190484651	271.52	7	38.79
mp-7250	Nb6Co7	0	8.885808577	743.2	13	57.17
mp-2580	NbB	0	7.429359441	89.28	2	44.64
mp-450	NbB2	0	6.793798027	92.96	3	30.99
mp-977426	NbCo3	0	9.188007818	184	4	46
mp-548	NbCr2	0	7.767773551	104.4	3	34.8
mp-1221111	NbFe	0	8.52821509	86.024	2	43.01
mp-1192350	NbFe2	0	8.803120472	86.448	3	28.82
mp-1220799	NbNi	0	8.842814701	99.5	2	49.75
mp-1451	NbNi3	0	8.950269576	127.3	4	31.82
mp-1220522	NbVCo	0	8.073557923	503.4	3	167.8
mp-1220374	NbVCr	0	7.38520832	480	3	160
mp-1220599	NbVNi	0	7.996372687	484.5	3	161.5
mp-1220316	NbW	0	13.43138832	120.9	2	60.45
mp-123	Nd	0	6.758696201	57.5	1	57.5
mp-567415	Nd2B5	0	5.945180936	133.4	7	19.06
mp-1800	Nd2C3	0	6.738088162	115.366	5	23.07
mp-356	Nd2Co17	0	8.660874962	672.6	19	35.4
mp-1084826	Nd2Co3	0	8.309643274	213.4	5	42.68
mp-1106011	Nd3Co	0	7.282343973	205.3	4	51.33
mp-1203103	Nd3Ga2	0	6.751687929	468.5	5	93.7
mp-1104652	Nd5Co2	0	7.325776628	353.1	7	50.44
mp-567735	Nd5Si3	0	6.280952658	292.6	8	36.58
mp-355	Nd5Si4	0	5.868754711	294.3	9	32.7
mp-864637	NdAl	0	5.570964592	59.29	2	29.64
mp-400	NdAl2	0	5.0585345	61.08	3	20.36
mp-1632	NdB4	0	5.768965554	72.22	5	14.44
mp-13392	NdCu	0	7.323929471	63.5	2	31.75
mp-11852	NdCu2	0	7.992310976	69.5	3	23.17
mp-1140	NdCu5	0	8.263727547	87.5	6	14.58
mp-1448	NdGa	0	6.683010873	205.5	2	102.75
mp-2524	NdGa2	0	6.886526887	353.5	3	117.83
mp-2599	NdN	0.4304	7.627429946	57.64	2	28.82
mp-9967	NdSi	0	5.927845124	59.2	2	29.6
mp-1053	NdZn	0	6.949623598	60.05	2	30.02
mp-30800	NdZn2	0	7.028659264	62.6	3	20.87
mp-23	Ni	0	9.047689544	13.9	1	13.9
mp-2536	Ni2B	0	8.10839559	31.48	3	10.49
mp-2058	Ni3B	0	8.260441597	45.38	4	11.35
mp-11506	Ni3Mo	0	9.512797164	81.8	4	20.45
mp-11507	Ni4Mo	0	9.438041633	95.7	5	19.14
mp-30811	Ni4W	0	11.89007194	90.9	5	18.18
mp-1179656	Rb	0	1.572308149	15500	1	15500
mp-568643	RbC8	0	2.448462356	15500.976	9	1722.33
mp-67	Sc	0	3.023050896	3460	1	3460
mp-505554	Sc(FeSi)2	0	5.391728323	3464.248	5	692.85
mp-11220	Sc2Al	0	3.024174766	6921.79	3	2307.26
mp-29941	Sc2C	0	3.118296979	6920.122	3	2306.71
mp-3618	Sc2FeSi2	0	4.124423954	6923.824	5	1384.76
mp-685209	Sc39N34	0	4.065969645	134944.76	73	1848.56
mp-862259	Sc3Al	0	3.083513198	10381.79	4	2595.45
mp-28733	Sc3C4	0	3.561973189	10380.488	7	1482.93
mp-27162	Sc3Co	0	3.959797526	10412.8	4	2603.2
mp-4755	Sc3Fe2Si3	0	4.348194174	10385.948	8	1298.24
mp-30666	Sc3Ga2	0	4.417556977	10676	5	2135.2
mp-19713	Sc3In	0	4.443026391	10547	4	2636.75
mp-15661	Sc4C3	0.4656	3.799358905	13840.366	7	1977.2
mp-7822	Sc5Si3	0	3.252082867	17305.1	8	2163.14
mp-331	ScAl	0	3.099620451	3461.79	2	1730.89
mp-813	ScAl2	0	3.00975007	3463.58	3	1154.53
mp-2252	ScB2	0	3.660544064	3467.36	3	1155.79
mp-2212	ScCo	0	5.682768497	3492.8	2	1746.4
mp-253	ScCo2	0	6.582231542	3525.6	3	1175.2
mp-1169	ScCu	0	5.222540494	3466	2	1733
mp-1018149	ScCu2	0	6.252104019	3472	3	1157.33
mp-1095443	ScFe2	0	6.089662863	3460.848	3	1153.62
mp-22701	ScFeSi	0	4.848691618	3462.124	3	1154.04
mp-2857	ScN	0.325	4.245782373	3460.14	2	1730.07
mp-11566	ScZn	0	4.846371151	3462.55	2	1731.28
mp-86	Sm	0	7.336111094	13.9	1	13.9
mp-570421	Sm2B5	0	6.38117091	46.2	7	6.6
mp-1219177	Sm2C	0	6.96379353	27.922	3	9.31
mp-569335	Sm2C3	0	7.342820428	28.166	5	5.63
mp-1195872	Sm3Ga2	0	7.290128233	337.7	5	67.54
mp-1106373	Sm5Si3	0	6.518409369	74.6	8	9.32
mp-978951	SmAl	0	5.946082179	15.69	2	7.85
mp-2358	SmAl2	0	5.345095455	17.48	3	5.83
mp-8546	SmB4	0	6.100418512	28.62	5	5.72
mp-980769	SmCu	0	7.954064255	19.9	2	9.95
mp-1077154	SmCu2	0	8.113356985	25.9	3	8.63
mp-227	SmCu5	0	8.498335586	43.9	6	7.32
mp-477	SmGa2	0	7.243944997	309.9	3	103.3
mp-749	SmN	0.0215	8.356280164	14.04	2	7.02
mp-1025489	SmSi	0	6.372031659	15.6	2	7.8
mp-1187073	Sr	0	2.676562284	6.68	1	6.68
mp-866669	Sr17(Li2Hg3)3	0	4.786163431	898.96	32	28.09
mp-569001	Sr2LiCoN2	0.2622	4.10702732	132.04	6	22.01
mp-862746	Sr2LiTl	0	4.61772008	4298.96	4	1074.74
mp-1245	Sr2N	0	3.493077187	13.5	3	4.5
mp-30828	Sr2Pb	0.0363	5.3028318	15.36	3	5.12
mp-12906	Sr3CrN3	0	4.25248097	29.86	7	4.27
mp-568322	Sr3Li3(NiN)4	0	3.967801457	333	14	23.79
mp-9723	Sr4Li(BN2)3	2.603	3.740877325	124.2	14	8.87
mp-242	SrB6	0.035	3.417060889	28.76	7	4.11
mp-2080	SrBe13	0	2.424044218	11147.68	14	796.26
mp-1208630	SrC6	0	3.270211156	7.412	7	1.06
mp-7084	SrCaSi	0.4225	2.831609127	10.73	3	3.58
mp-1025402	SrCu	0	4.000956388	12.68	2	6.34
mp-867174	SrLi2Pb	0	5.32533621	179.88	4	44.97
mp-867171	SrLi2Sn	0	3.93559603	196.58	4	49.14
mp-15845	SrLi4N2	0.9413	2.399527683	349.36	7	49.91
mp-1187198	SrMg2	0	2.399508735	11.32	3	3.77
mp-50	Ta	0	16.38780395	312	1	312
mp-1193531	Ta2Al	0	12.51251642	625.79	3	208.6
mp-11278	Ta2Be	0	13.76091757	1481	3	493.67
mp-1189402	Ta2Be17	0	5.097220738	15193	19	799.63
mp-1079438	Ta2N	0	15.39304112	624.14	3	208.05
mp-1078957	Ta3Be2	0	13.0790515	2650	5	530
mp-568646	Ta3Si	0	13.88613422	937.7	4	234.43
mp-1187206	Ta3W	0	17.11634231	971.3	4	242.82
mp-1989	Ta5Si3	0	12.7874257	1565.1	8	195.64
mp-567842	TaBe12	0	4.277046508	10596	13	815.08
mp-1102049	TaBe3	0	8.223856335	2883	4	720.75
mp-1217811	TaW	0	17.65981087	347.3	2	173.65
mp-979289	TaW3	0	18.29084553	417.9	4	104.47
mp-72	Ti	0	4.64683663	11.7	1	11.7
mp-1202079	Ti21Mn25	0	6.379828993	291.2	46	6.33
mp-10721	Ti2C	0	4.43976924	23.522	3	7.84
mp-1191331	Ti2Co	0	5.816331995	56.2	3	18.73
mp-742	Ti2Cu	0	5.722180363	29.4	3	9.8
mp-30671	Ti2Ga	0	5.649651788	171.4	3	57.13
mp-863690	Ti2MnCo	0	6.64951189	58.02	4	14.5
mp-861983	Ti2MnFe	0	6.549536628	25.644	4	6.41
mp-865712	Ti2MnNi	0	6.578268698	39.12	4	9.78
mp-8282	Ti2N	0	4.881545292	23.54	3	7.85
mp-1808	Ti2Ni	0	5.725014052	37.3	3	12.43
mp-1014229	Ti2Zn	0	5.462441931	25.95	3	8.65
mp-1823	Ti3Al	0	4.248868625	36.89	4	9.22
mp-1025170	Ti3B4	0	4.557547557	49.82	7	7.12
mp-2643	Ti3Cu4	0	6.748300444	59.1	7	8.44
mp-30672	Ti3Ga	0	5.416551144	183.1	4	45.77
mp-1217247	Ti4CoNi	0	5.790096873	93.5	6	15.58
mp-1217201	Ti4Mn5V3	0	6.366540898	1210.9	12	100.91
mp-2108	Ti5Si3	0	4.347039406	63.6	8	7.95
mp-27919	Ti8C5	0	4.54143797	94.21	13	7.25
mp-1217065	Ti8Cu3Ni	0	5.757515978	125.5	12	10.46
mp-1953	TiAl	0	3.833901613	13.49	2	6.74
mp-7857	TiB	0	4.575880615	15.38	2	7.69
mp-1145	TiB2	0	4.487425163	19.06	3	6.35
mp-631	TiC	0	4.879907059	11.822	2	5.91
mp-823	TiCo	0	6.714495322	44.5	2	22.25
mp-608	TiCo3	0	7.948540457	110.1	4	27.52
mp-568636	TiCr2	0	6.234565538	30.5	3	10.17
mp-2078	TiCu	0	6.440936363	17.7	2	8.85
mp-12546	TiCu3	0	7.648117875	29.7	4	7.42
mp-1216850	TiCuNi	0	7.255741497	31.6	3	10.53
mp-305	TiFe	0	6.642034602	12.124	2	6.06
mp-866141	TiFe2Si	0.4023	6.758127762	14.248	4	3.56
mp-1949	TiMn2	0	6.901373985	15.34	3	5.11
mp-865652	TiMn2Si	0	6.352313333	17.04	4	4.26
mp-865678	TiMn2V	0	6.93063331	400.34	4	100.08
mp-865656	TiMn2W	0	10.69468704	50.64	4	12.66
mp-865537	TiMnCo2	0	7.350147653	79.12	4	19.78
mp-1216946	TiMnCr	0	6.555149755	22.92	3	7.64
mp-492	TiN	0	5.340297483	11.84	2	5.92
mp-1216666	TiNbCr4	0	7.031469819	134.9	6	22.48
mp-1048	TiNi	0	6.412985726	25.6	2	12.8
mp-1409	TiNi3	0	7.958129861	53.4	4	13.35
mp-1216621	TiW	0	11.85552569	47	2	23.5
mp-146	V	0	6.312904043	385	1	385
mp-9208	V2B3	0	5.360224268	781.04	5	156.21
mp-20648	V2C	0	5.741137786	770.122	3	256.71
mp-865490	V2CrFe	0	7.348434541	779.824	4	194.96
mp-33090	V2N	0	6.096388132	770.14	3	256.71
mp-2091	V3B2	0	5.846064712	1162.36	5	232.47
mp-569270	V3B4	0	5.426880995	1169.72	7	167.1
mp-1585	V3Co	0	6.985026991	1187.8	4	296.95
mp-1187695	V3Cr	0	6.599355542	1164.4	4	291.1
mp-1079399	V3Fe	0	6.896938402	1155.424	4	288.86
mp-7226	V3Ni	0	6.898754916	1168.9	4	292.23
mp-1216708	V3Ni2	0	7.272789251	1182.8	5	236.56
mp-2567	V3Si	0	5.77814219	1156.7	4	289.18
mp-1206441	V5B6	0	5.503664211	1947.08	11	177.01
mp-568671	V5Si3	0	5.379232288	1930.1	8	241.26
mp-10126	V5SiB2	0	5.621737698	1934.06	8	241.76
mp-28731	V6C5	0	5.617822598	2310.61	11	210.06
mp-1216443	V6FeNi	0	6.865814535	2324.324	8	290.54
mp-1188283	V8N	0	6.188837954	3080.14	9	342.24
mp-9973	VB	0	5.631694261	388.68	2	194.34
mp-1491	VB2	0	5.10857069	392.36	3	130.79
mp-542614	VCo3	0	8.706330003	483.4	4	120.85
mp-1216394	VCr	0	6.919500541	394.4	2	197.2
mp-1187696	VCr3	0	7.195388401	413.2	4	103.3
mp-866134	VFe3	0	7.739814966	386.272	4	96.57
mp-11531	VNi2	0	8.166036424	412.8	3	137.6
mp-171	VNi3	0	8.437749253	426.7	4	106.67
mp-1216231	VW	0	13.07376045	420.3	2	210.15
mp-1187702	VW3	0	16.12824395	490.9	4	122.72
mp-91	W	0	18.85400756	35.3	1	35.3
mp-1894	WC	0	15.3503693	35.422	2	17.71
mp-1187739	Y	0	4.547349703	31	1	31
mp-1200338	Y15Ni32	0	7.163935221	909.8	47	19.36
mp-1334	Y2C	0	4.535817916	62.122	3	20.71
mp-574339	Y2Ni7	0	7.692491082	159.3	9	17.7
mp-1200613	Y3C4	0	4.91444971	93.488	7	13.36
mp-1105598	Y3Co	0	5.148898384	125.8	4	31.45
mp-1204352	Y3Ga2	0	5.289220334	389	5	77.8
mp-1105633	Y3Ni	0	5.094566393	106.9	4	26.73
mp-582134	Y3Ni2	0	5.562940279	120.8	5	24.16
mp-9459	Y4C5	0	4.729248328	124.61	9	13.85
mp-1200885	Y4C7	0.6144	4.541710694	124.854	11	11.35
mp-1188292	Y5Pb3	0	7.410237154	161	8	20.12
mp-2538	Y5Si3	0	4.43624154	160.1	8	20.01
mp-567412	Y5Sn3	0	5.778885589	211.1	8	26.39
mp-2322	YAl2	0	3.879200231	34.58	3	11.53
mp-972364	Yb	0	7.00586663	17.1	1	17.1
mp-1542	YB2	0	5.045298476	38.36	3	12.79
mp-9546	Yb2C3	0	8.726729992	34.566	5	6.91
mp-1102309	Yb2Ga	0	8.278283684	182.2	3	60.73
mp-1207599	Yb2Si	0.0437	7.742296269	35.9	3	11.97
mp-864675	Yb3N2	0.4892	10.30057431	51.58	5	10.32
mp-637	YB4	0	4.30848155	45.72	5	9.14
mp-680653	Yb8In3	0	8.040724614	637.8	11	57.98
mp-570438	Yb8Tl3	0	9.225045302	12736.8	11	1157.89
mp-969	YbAl2	0	5.949727005	20.68	3	6.89
mp-1189298	YbB4	0	6.949843493	31.82	5	6.36
mp-419	YbB6	0.1059	5.614593733	39.18	7	5.6
mp-1103975	YbC6	0	5.687258796	17.832	7	2.55
mp-1857	YbCd	0	8.562931183	19.83	2	9.92
mp-1937	YbCu	0	9.051707971	23.1	2	11.55
mp-567538	YbCu2	0	9.550793637	29.1	3	9.7
mp-1607	YbCu5	0	9.333348732	47.1	6	7.85
mp-396	YbGa	0	8.564556702	165.1	2	82.55
mp-2545	YbHg	0	11.72288518	47.3	2	23.65
mp-865373	YCo	0	5.420377438	63.8	2	31.9
mp-1294	YCo2	0	7.581892784	96.6	3	32.2
mp-1080443	YCu	0	5.830094464	37	2	18.5
mp-2698	YCu2	0	6.706395025	43	3	14.33
mp-2797	YCu5	0	7.535186104	61	6	10.17
mp-1570	YFe2	0	6.872989898	31.848	3	10.62
mp-11385	YFe5	0	7.107153348	33.12	6	5.52
mp-11420	YGa	0	5.438626464	179	2	89.5
mp-615	YMg	0	3.419333592	33.32	2	16.66
mp-22508	YMn12	0	7.697063754	52.84	13	4.06
mp-2114	YN	0.2858	5.742757452	31.14	2	15.57
mp-1364	YNi	0	6.05878909	44.9	2	22.45
mp-569196	YNi3	0	7.60099949	72.7	4	18.18
mp-2152	YNi5	0	7.801971483	100.5	6	16.75
mp-2516	YZn	0	5.55941478	33.55	2	16.77
mp-131	Zr	0	6.4460921	37.1	1	37.1
mp-684623	Zr10C9	0	6.396416519	372.098	19	19.58
mp-1216441	Zr14Cu51	0	8.184391095	825.4	65	12.7
mp-2544	Zr2Be17	0	3.115805578	14643.2	19	770.69
mp-193	Zr2Cu	0	6.968518148	80.2	3	26.73
mp-1014265	Zr2N	0	6.644608678	74.34	3	24.78
mp-1278	Zr2Si	0	5.972090741	75.9	3	25.3
mp-31205	Zr3Fe	0	6.808804543	111.724	4	27.93
mp-1188062	Zr3Sc	0	5.604938366	3571.3	4	892.83
mp-1207024	Zr3Si2	0	5.812221304	114.7	5	22.94
mp-582924	Zr6Fe23	0	7.603506886	232.352	29	8.01
mp-1188077	Zr7Cu10	0	7.760947992	319.7	17	18.81
mp-30445	ZrBe13	0	2.771775575	11178.1	14	798.44
mp-11283	ZrBe5	0	3.623393534	4322.1	6	720.35
mp-2795	ZrC	0	6.50296405	37.222	2	18.61
mp-903	ZrCr2	0	7.10910703	55.9	3	18.63
mp-1190681	ZrFe2	0	7.66641483	37.948	3	12.65
mp-2116	ZrMn2	0	7.670876059	40.74	3	13.58
mp-1352	ZrN	0	7.098978293	37.24	2	18.62
mp-1077791	ZrSc2	0	4.15936576	6957.1	3	2319.03
mp-893	ZrSi	0	5.562650989	38.8	2	19.4
mp-134	Al	0	2.72005	1.79	1	1.79
mp-3805	Al(FeB)2	0	5.791994	9.998	5	2
mp-29110	Al2(FeSi)3	0.2303	5.163781	9.952	8	1.24
mp-568153	Al22Mo5	0	4.244949	239.88	27	8.88
mp-985806	Al2Cu	0	4.064939	9.58	3	3.19
mp-867780	Al3Cr	0	3.815306	14.77	4	3.69
mp-1190708	Al3Fe2Si	0	4.725578	7.918	6	1.32
mp-622209	Al3Ni	0	4.034332	19.27	4	4.82
mp-1057	Al3Ni2	0	4.767799	33.17	5	6.63
mp-16514	Al3Ni5	0	6.717313	74.87	8	9.36
mp-2554	Al3V	0	3.714657	390.37	4	97.59
mp-31019	Al45Cr7	0	3.226501	146.35	52	2.81
mp-1591	Al4C3	1.3422	2.930804	7.526	7	1.08
mp-593	Al4Cu9	0	6.853923	61.16	13	4.7
mp-16515	Al4Ni3	0	5.093005	48.86	7	6.98
mp-1229054	Al53Fe17Si12	0	3.847798	122.478	82	1.49
mp-196	Al5Co2	0	4.338446	74.55	7	10.65
mp-570001	Al6Fe	0	3.428138	11.164	7	1.59
mp-1229249	Al79(Fe13Si9)2	0	3.829625	183.034	123	1.49
mp-2733	Al8Mo3	0	5.003747	134.62	11	12.24
mp-16488	Al9Co2	0	3.608519	81.71	11	7.43
mp-284	AlCo	0	6.136769	34.59	2	17.29
mp-1699	AlCr2	0	5.748722	20.59	3	6.86
mp-2500	AlCu	0	5.356855	7.79	2	3.9
mp-12802	AlCu3	0	7.287482	19.79	4	4.95
mp-2658	AlFe	0	5.791723	2.214	2	1.11
mp-867878	AlFe2Si	0	6.28905	4.338	4	1.08
mp-1183162	AlFe3	0	6.64785	3.062	4	0.77
mp-259	AlMo3	0	8.470008	122.09	4	30.52
mp-1487	AlNi	0	5.906845	15.69	2	7.85
mp-2593	AlNi3	0	7.466732	43.49	4	10.87
mp-1387	AlV3	0	5.367847	1156.79	4	289.2
mp-576	B13C2	0	2.438648	48.084	15	3.21
mp-5506	Ba(AlSi)2	0	3.475027	7.255	5	1.45
mp-567643	Ba12Na15Li8N6	0	2.425386	740.39	41	18.06
mp-6645	Ba14Na14CaN6	0	2.757389	55.06	35	1.57
mp-645662	Ba14Na14LiN6	0	2.711592	138.31	35	3.95
mp-569025	Ba19Na29Li13	0.0147	2.190395	1217.495	61	19.96
mp-567701	Ba21Al40	0	3.884213	77.375	61	1.27
mp-8093	Ba2Cd	0	4.503964	3.28	3	1.09
mp-1102914	Ba2Eu3Si7	0	4.946268	106.65	12	8.89
mp-8094	Ba2Hg	0	5.677448	30.75	3	10.25
mp-1813	Ba2Mg17	0	2.238174	39.99	19	2.1
mp-1892	Ba2N	0	4.403708	0.69	3	0.23
mp-21246	Ba2Pb	0.0383	5.787076	2.55	3	0.85
mp-9905	Ba2Si	0.0553	4.278608	2.25	3	0.75
mp-1981	Ba2Sn	0.0155	4.834448	19.25	3	6.42
mp-9578	Ba3(AlSi)2	0	3.898588	7.805	7	1.11
mp-30905	Ba3(BN2)2	2.5259	4.542904	8.745	9	0.97
mp-8868	Ba3NaN	0	3.386127	4.395	5	0.88
mp-1619	Ba3Si4	0.0012	3.952257	7.625	7	1.09
mp-2631	Ba4Al5	0	3.901347	10.05	9	1.12
mp-9705	Ba4Na(BN2)3	2.4682	4.48226	16.41	14	1.17
mp-568512	Ba6Mg23	0	2.597055	55.01	29	1.9
mp-570400	Ba7Al10	0	3.910774	19.825	17	1.17
mp-30429	Ba8Ga7	0	4.702519	1038.2	15	69.21
mp-1105101	Ba9In4	0	4.681514	670.475	13	51.58
mp-1903	BaAl4	0	3.425432	7.435	5	1.49
mp-13149	BaAlSi	0	3.806506	3.765	3	1.25
mp-954	BaB6	0.0623	4.281989	22.355	7	3.19
mp-1214417	BaC6	0	3.961949	1.007	7	0.14
mp-16253	BaCaSi	0.1767	3.413084	4.325	3	1.44
mp-527	BaCd	0	5.290471	3.005	2	1.5
mp-11266	BaCd2	0	6.05756	5.735	3	1.91
mp-1029375	BaCN2	2.982	3.498345	0.677	4	0.17
mp-30428	BaCu	0	4.510555	6.275	2	3.14
mp-1219	BaGa2	0	5.17334	296.275	3	98.76
mp-335	BaGa4	0	5.942574	592.275	5	118.45
mp-2197	BaHg	0	7.458275	30.475	2	15.24
mp-31509	BaIn	0	5.565138	167.275	2	83.64
mp-22141	BaIn2	0	6.050443	334.275	3	111.42
mp-1935	BaMg2	0	3.030975	4.915	3	1.64
mp-1001	BaN2	0	4.760885	0.555	3	0.19
mp-11820	BaNa2	0	2.217756	7.135	3	2.38
mp-20136	BaPb	0	6.68722	2.275	2	1.14
mp-1067235	BaSi	0	4.286154	1.975	2	0.99
mp-1477	BaSi2	0.791	3.628158	3.675	3	1.22
mp-872	BaSn	0	5.242658	18.975	2	9.49
mp-30434	BaTl2	0	8.346846	8400.275	3	2800.09
mp-87	Be	0	1.895724	857	1	857
mp-27757	Be4B	0	1.981767	3431.68	5	686.34
mp-569304	C	2.6904	1.274371	0.122	1	0.12
mp-132	Ca	0	1.569031	2.35	1	2.35
mp-7704	Ca(AlSi)2	0	2.347097	9.33	5	1.87
mp-568793	Ca28Ga11	0	2.585517	1693.8	39	43.43
mp-12614	Ca2Cu	0	2.6295	10.7	3	3.57
mp-1227300	Ca2GaSi	0	2.915363	154.4	4	38.6
mp-1103139	Ca2Hg	0	4.924543	34.9	3	11.63
mp-2686	Ca2N	0	2.161683	4.84	3	1.61
mp-30478	Ca2Pb	0.0771	4.775951	6.7	3	2.23
mp-2517	Ca2Si	0.2915	2.165188	6.4	3	2.13
mp-22735	Ca2Sn	0.0596	3.412531	23.4	3	7.8
mp-18167	Ca3Cd2	0	3.620507	12.51	5	2.5
mp-30473	Ca3Ga5	0	4.266022	747.05	8	93.38
mp-11288	Ca3Hg2	0	5.581053	67.45	5	13.49
mp-844	Ca3N2	1.1111	2.606386	7.33	5	1.47
mp-640340	Ca4MgAl3	0	2.018737	17.09	8	2.14
mp-1227465	Ca4Zn51	0	6.385063	139.45	55	2.54
mp-793	Ca5Si3	0	2.188848	16.85	8	2.11
mp-2786	Ca5Zn3	0	2.763437	19.4	8	2.42
mp-1190736	Ca8Al3	0	1.895136	24.17	11	2.2
mp-1191538	Ca8In3	0	2.9916	519.8	11	47.25
mp-2404	CaAl2	0	2.425285	5.93	3	1.98
mp-570150	CaAlSi	0	2.354365	5.84	3	1.95
mp-1213975	CaB4	0	2.631299	17.07	5	3.41
mp-865	CaB6	0.1835	2.437996	24.43	7	3.49
mp-1845	CaBe13	0	1.947352	11143.35	14	795.95
mp-1073	CaCd	0	4.408706	5.08	2	2.54
mp-1444	CaCd2	0	5.485134	7.81	3	2.6
mp-585949	CaCu	0	3.622394	8.35	2	4.17
mp-1882	CaCu5	0	6.536939	32.35	6	5.39
mp-6914	CaGa	0	3.478416	150.35	2	75.17
mp-11284	CaGa2	0	4.589511	298.35	3	99.45
mp-11286	CaHg	0	7.21503	32.55	2	16.27
mp-20263	CaIn	0	4.457749	169.35	2	84.67
mp-1039148	CaMg	0	1.713629	4.67	2	2.33
mp-1184449	CaMg149	0.499	1.754975	348.03	150	2.32
mp-2432	CaMg2	0	1.731927	6.99	3	2.33
mp-5473	CaMgSi	0.0159	2.228699	6.37	3	2.12
mp-1009657	CaN2	0	2.887755	2.63	3	0.88
mp-1563	CaSi	0	2.377161	4.05	2	2.02
mp-2861	CaTl	0	6.802615	4202.35	2	2101.18
mp-30483	CaZn	0	3.270684	4.9	2	2.45
mp-18567	CaZn11	0	6.439707	30.4	12	2.53
mp-1725	CaZn2	0	4.415864	7.45	3	2.48
mp-1734	CaZn5	0	5.681812	15.1	6	2.52
mp-16266	CaZnSi	0	3.460967	6.6	3	2.2
mp-567332	Ce	0	8.917867	4.71	1	4.71
mp-3035	Ce(FeSi)2	0	6.676439	8.958	5	1.79
mp-20181	Ce2C3	0	7.074734	9.786	5	1.96
mp-19920	Ce3Ga	0	8.078079	162.13	4	40.53
mp-21412	Ce3Tl	0	9.143027	4214.13	4	1053.53
mp-570175	Ce5Si3	0	6.736034	28.65	8	3.58
mp-1196829	Ce5Si4	0	6.040718	30.35	9	3.37
mp-2801	CeCu2	0	8.065457	16.71	3	5.57
mp-581942	CeCu6	0	8.455393	40.71	7	5.82
mp-11317	CeFe5	0	7.942088	6.83	6	1.14
mp-20245	CeFeSi	0	6.792241	6.834	3	2.28
mp-1025450	CeFeSi2	0	6.195414	8.534	4	2.13
mp-1018276	CeGa	0	6.849882	152.71	2	76.36
mp-2209	CeGa2	0	6.913058	300.71	3	100.24
mp-862696	CeGa3	0	7.143669	448.71	4	112.18
mp-1039345	CeMg2	0	4.198994	9.35	3	3.12
mp-2493	CeN	0	7.942476	4.85	2	2.42
mp-21115	CeSi	0	6.016047	6.41	2	3.21
mp-1898	CeSi2	0	5.496005	8.11	3	2.7
mp-1206755	CeTl	0	9.953953	4204.71	2	2102.36
mp-54	Co	0	8.959676	32.8	1	32.8
mp-19905	Co2Si	0	7.586966	67.3	3	22.43
mp-1139	Co3Mo	0	9.788206	138.5	4	34.62
mp-1183837	Co3Ni	0	9.020551	112.3	4	28.07
mp-2157	Co3W	0	12.92412	133.7	4	33.42
mp-20857	CoB	0	7.45659	36.48	2	18.24
mp-7577	CoSi	0	6.633921	34.5	2	17.25
mp-2379	CoSi2	0	4.964464	36.2	3	12.07
mp-90	Cr	0	7.274081	9.4	1	9.4
mp-723	Cr23C6	0	7.1678	216.932	29	7.48
mp-569424	Cr2B	0	6.74589	22.48	3	7.49
mp-8780	Cr2N	0	6.723825	18.94	3	6.31
mp-20937	Cr3C2	0	6.79518	28.444	5	5.69
mp-729	Cr3Si	0	6.625101	29.9	4	7.48
mp-15617	Cr5B3	0	6.587366	58.04	8	7.25
mp-1196316	Cr7C3	0	7.055496	66.166	10	6.62
mp-1080664	CrB	0	6.267643	13.08	2	6.54
mp-1078278	CrB4	0	4.279143	24.12	5	4.82
mp-1183691	CrN	0	6.763021	9.54	2	4.77
mp-784631	CrNi2	0	8.620907	37.2	3	12.4
mp-8937	CrSi2	0	5.015723	12.8	3	4.27
mp-1184151	Cs	0.1362	1.885761	61800	1	61800
mp-1199908	Cs7NaSi8	1.5761	3.10064	432617.03	16	27038.56
mp-28861	CsC8	0	2.893417	61800.976	9	6866.78
mp-30	Cu	0	8.888275	6	1	6
mp-14266	Cu15Si4	0	7.743605	96.8	19	5.09
mp-1184115	Er	0	9.037772	26.4	1	26.4
mp-1225044	Er2C	0	8.678709	52.922	3	17.64
mp-1203719	Er3C4	0	8.934403	79.688	7	11.38
mp-1212833	Er4C7	0	8.047974	106.454	11	9.68
mp-31167	Er5Si3	0	8.045293	137.1	8	17.14
mp-1105965	Er5Tl3	0	10.3935	12732	8	1591.5
mp-1774	ErB2	0	8.881021	33.76	3	11.25
mp-2847	ErB4	0	6.99873	41.12	5	8.22
mp-1955	ErCu	0	9.463506	32.4	2	16.2
mp-1024991	ErCu2	0	9.341568	38.4	3	12.8
mp-30579	ErCu5	0	9.420409	56.4	6	9.4
mp-378	ErSi	0	7.710454	28.1	2	14.05
mp-1057315	Eu	0	6.086595	31.4	1	31.4
mp-1213070	Eu2Sn	0	6.901469	81.5	3	27.17
mp-867318	Eu3Tl	0	8.006177	4294.2	4	1073.55
mp-1190061	Eu5Si3	0	6.153677	162.1	8	20.26
mp-20111	EuAl2	0	4.988962	34.98	3	11.66
mp-582799	EuAl4	0	4.00127	38.56	5	7.71
mp-20874	EuB6	0	4.963691	53.48	7	7.64
mp-1103990	EuC6	0	4.798312	32.132	7	4.59
mp-1087547	EuCu	0	7.049618	37.4	2	18.7
mp-1071732	EuCu2	0	7.840235	43.4	3	14.47
mp-2066	EuCu5	0	8.369253	61.4	6	10.23
mp-11375	EuHg	0	9.8364	61.6	2	30.8
mp-20394	EuPb	0	9.426836	33.4	2	16.7
mp-21279	EuSi	0	5.904327	33.1	2	16.55
mp-1072248	EuSi2	0	5.454986	34.8	3	11.6
mp-567833	EuSn	0	6.837518	50.1	2	25.05
mp-13	Fe	0	8.096265	0.424	1	0.42
mp-601848	Fe11Co5	0	8.108532	168.664	16	10.54
mp-1915	Fe2B	0	7.490316	4.528	3	1.51
mp-601820	Fe3Co	0	8.136129	34.072	4	8.52
mp-1804	Fe3N	0	7.421216	1.412	4	0.35
mp-2199	Fe3Si	0	7.388614	2.972	4	0.74
mp-601842	Fe9Co7	0	8.206827	233.416	16	14.59
mp-1080525	FeB	0	6.887697	4.104	2	2.05
mp-2090	FeCo	0	8.290363	33.224	2	16.61
mp-6988	FeN	0	6.127073	0.564	2	0.28
mp-2213	FeNi	0	8.452471	14.324	2	7.16
mp-1418	FeNi3	0	8.700536	42.124	4	10.53
mp-871	FeSi	0.1664	6.33388	2.124	2	1.06
mp-1714	FeSi2	0.6976	4.958878	3.824	3	1.27
mp-11397	Ga3Ni2	0	7.682462	471.8	5	94.36
mp-11398	Ga3Ni5	0	8.802756	513.5	8	64.19
mp-21589	Ga9Ni13	0	8.532837	1512.7	22	68.76
mp-1183995	GaCu3	0	8.629827	166	4	41.5
mp-804	GaN	1.7376	5.923651	148.14	2	74.07
mp-815	GaNi3	0	8.937909	189.7	4	47.42
mp-155	Gd	0	8.001979	28.6	1	28.6
mp-28366	Gd2B5	0	6.836474	75.6	7	10.8
mp-1224869	Gd2C	0	7.676989	57.322	3	19.11
mp-1189998	Gd2C3	0	7.992747	57.566	5	11.51
mp-1205813	Gd2MgSi2	0	5.904292	62.92	5	12.58
mp-579628	Gd2Tl	0	9.733823	4257.2	3	1419.07
mp-1199486	Gd5Si4	0	6.902406	149.8	9	16.64
mp-1105563	GdB4	0	6.464598	43.32	5	8.66
mp-22266	GdB6	0	5.311474	50.68	7	7.24
mp-614455	GdCu	0	8.506838	34.6	2	17.3
mp-1077933	GdCu2	0	8.348842	40.6	3	13.53
mp-636253	GdCu5	0	8.925302	58.6	6	9.77
mp-11422	GdHg	0	11.17449	58.8	2	29.4
mp-2636	GdMg	0	5.379276	30.92	2	15.46
mp-20534	GdMg3	0	3.976209	35.56	4	8.89
mp-601371	GdSi	0	6.899145	30.3	2	15.15
mp-21192	GdSi2	0	6.050126	32	3	10.67
mp-19966	GdTl	0	10.45587	4228.6	2	2114.3
mp-103	Hf	0	13.18322	900	1	900
mp-1224756	Hf14Cu51	0	10.7533	12906	65	198.55
mp-30581	Hf2Cu	0	12.40424	1806	3	602
mp-864647	Hf2N	0	13.23693	1800.14	3	600.05
mp-7353	Hf3Cu8	0	10.98414	2748	11	249.82
mp-1224388	Hf3N2	0	13.38749	2700.28	5	540.06
mp-776470	Hf3N4	1.0064	11.51383	2700.56	7	385.79
mp-976128	Hf5Sc	0	11.46515	7960	6	1326.67
mp-1200988	Hf7Cu10	0	11.40178	6360	17	374.12
mp-21075	HfC	0	12.57417	900.122	2	450.06
mp-2363	HfMo2	0	11.27481	980.2	3	326.73
mp-2828	HfN	0	13.684	900.14	2	450.07
mp-10659	Ho	0	8.822554	57.1	1	57.1
mp-569851	Ho10Si17	0	6.713993	599.9	27	22.22
mp-1640	Ho2C	0	8.412835	114.322	3	38.11
mp-1202754	Ho3C4	0	8.700158	171.788	7	24.54
mp-15238	Ho4C5	0	8.409762	229.01	9	25.45
mp-1154	Ho4C7	0.5867	7.857241	229.254	11	20.84
mp-13236	Ho5Si3	0	7.80741	290.6	8	36.33
mp-1181055	Ho5Tl3	0	10.21932	12885.5	8	1610.69
mp-2267	HoB2	0	8.642414	64.46	3	21.49
mp-569281	HoB4	0	6.87016	71.82	5	14.36
mp-12899	HoSi	0	7.513612	58.8	2	29.4
mp-1540	HoTl	0	11.27726	4257.1	2	2128.55
mp-1184905	K	0	0.868387	13.6	1	13.6
mp-1225049	K18Na46Tl31	0	3.927045	130602.58	95	1374.76
mp-3949	K7LiSi8	1.693	1.693421	194.4	16	12.15
mp-28930	KC8	0	1.949986	14.576	9	1.62
mp-1217	KSi	1.2619	1.742992	15.3	2	7.65
mp-784	KZn13	0	6.22728	46.75	14	3.34
mp-1018134	Li	0	0.573095	85.6	1	85.6
mp-510430	Li13In3	0	2.47108	1613.8	16	100.86
mp-672287	Li13Si4	0	1.283597	1119.6	17	65.86
mp-1222798	Li14MgSi4	0.1059	1.286984	1207.52	19	63.55
mp-574275	Li17Pb4	0	3.96125	1463.2	21	69.68
mp-573471	Li17Sn4	0	2.589549	1530	21	72.86
mp-29720	Li21Si5	0	1.194592	1806.1	26	69.47
mp-1210753	Li2Al	0	1.381341	172.99	3	57.66
mp-570466	Li2Ca	0	1.083251	173.55	3	57.85
mp-29210	Li2Ga	0	2.981137	319.2	3	106.4
mp-31324	Li2In	0	3.818917	338.2	3	112.73
mp-1105932	Li2MgSi	0.218	1.705165	175.22	4	43.8
mp-16506	Li3Al2	0	1.53862	260.38	5	52.08
mp-867343	Li3Cd	0	2.969004	259.53	4	64.88
mp-9568	Li3Ga2	0	3.489024	552.8	5	110.56
mp-1646	Li3Hg	0	5.233841	287	4	71.75
mp-867226	Li3In	0	3.062221	423.8	4	105.95
mp-21293	Li3In2	0	4.325351	590.8	5	118.16
mp-1094591	Li3Mg	0	0.919302	259.12	4	64.78
mp-2251	Li3N	0.9986	1.288609	256.94	4	64.23
mp-7396	Li3Tl	0	5.009351	4456.8	4	1114.2
mp-1205930	Li5Ga4	0	3.760163	1020	9	113.33
mp-12283	Li5Tl2	0	5.534064	8828	7	1261.14
mp-30761	Li7Pb2	0	4.575943	603.2	9	67.02
mp-1201871	Li7Si3	0	1.477568	604.3	10	60.43
mp-30767	Li7Sn2	0	2.974648	636.6	9	70.73
mp-1067	LiAl	0	1.754628	87.39	2	43.7
mp-10890	LiAl3	0	2.237075	90.97	4	22.74
mp-3161	LiAlSi	0.1426	1.966694	89.09	3	29.7
mp-1001835	LiB	0	1.356921	89.28	2	44.64
mp-1222413	LiB3	0.088	1.756194	96.64	4	24.16
mp-1021323	LiC12	0	2.019464	87.064	13	6.7
mp-1437	LiCd	0	5.162727	88.33	2	44.16
mp-862658	LiCu3	0	6.929195	103.6	4	25.9
mp-1094889	LiMg	0	1.294794	87.92	2	43.96
mp-866755	LiMg149	0	1.74405	431.28	150	2.88
mp-973374	LiMg2	0	1.425083	90.24	3	30.08
mp-1198027	LiSi2B	1.1654	2.370184	92.68	4	23.17
mp-973391	LiSiB6	1.6991	2.340913	109.38	8	13.67
mp-14208	LiYSi	0	3.416484	118.3	3	39.43
mp-1934	LiZn	0	4.082778	88.15	2	44.07
mp-975799	LiZn3	0	5.75487	93.25	4	23.31
mp-567224	Mg(SiB6)2	1.9371	2.461378	49.88	15	3.33
mp-1185596	Mg149Al	0.5011	1.772538	347.47	150	2.32
mp-1185581	Mg149Cd	0.5742	1.814631	348.41	150	2.32
mp-1185597	Mg149Ga	0.4779	1.801585	493.68	150	3.29
mp-1185579	Mg149Hg	0.5682	1.854374	375.88	150	2.51
mp-1185594	Mg149In	0.5296	1.800697	512.68	150	3.42
mp-1185570	Mg149Pb	0.383	1.857156	347.68	150	2.32
mp-1185631	Mg149Sc	0.2496	1.774147	3805.68	150	25.37
mp-1185637	Mg149Sn	0.4181	1.816858	364.38	150	2.43
mp-1185635	Mg149Tl	0.4888	1.861349	4545.68	150	30.3
mp-1185642	Mg149Zn	0.578	1.775147	348.23	150	2.32
mp-2151	Mg17Al12	0	2.094692	60.92	29	2.1
mp-1094909	Mg2Cd	0	4.055133	7.37	3	2.46
mp-30650	Mg2Ga	0	3.211673	152.64	3	50.88
mp-2137	Mg2Ni	0	3.481329	18.54	3	6.18
mp-1367	Mg2Si	0.2935	1.97537	6.34	3	2.11
mp-1201511	Mg3(Al9V)2	0	2.81921	809.18	23	35.18
mp-30490	Mg3Cd	0	3.471382	9.69	4	2.42
mp-1559	Mg3N2	1.5099	2.661929	7.24	5	1.45
mp-1185790	Mg3Sc	0	2.138724	3466.96	4	866.74
mp-1222150	Mg4AlB10	0	2.738712	47.87	15	3.19
mp-680671	Mg4Zn7	0	4.902722	27.13	11	2.47
mp-1770	Mg5Ga2	0	2.981947	307.6	7	43.94
mp-1094116	MgAl2	0	2.29486	5.9	3	1.97
mp-1207086	MgAlB4	0	2.910035	18.83	6	3.14
mp-763	MgB2	0	2.637301	9.68	3	3.23
mp-365	MgB4	0.365	2.504416	17.04	5	3.41
mp-978275	MgB7	1.4635	2.618328	28.08	8	3.51
mp-30091	MgB9N	1.9608	2.577471	35.58	11	3.23
mp-2675	MgNi2	0	6.032501	30.12	3	10.04
mp-864941	MgSc2	0	2.6532	6922.32	3	2307.44
mp-978269	MgZn2	0	5.080755	7.42	3	2.47
mp-35	Mn	0	8.265241	1.82	1	1.82
mp-542830	Mn23C6	0	7.843044	42.592	29	1.47
mp-20318	Mn2B	0	7.609817	7.32	3	2.44
mp-9981	Mn2N	0	6.98777	3.78	3	1.26
mp-12659	Mn2Nb	0	8.479514	89.24	3	29.75
mp-15819	Mn3Al9Si	0	3.905078	23.27	13	1.79
mp-10118	Mn3B4	0	6.153079	20.18	7	2.88
mp-1185970	Mn3Co	0	8.771772	38.26	4	9.56
mp-20211	Mn3Si	0	7.078773	7.16	4	1.79
mp-2856	Mn4Al11	0	4.068219	26.97	15	1.8
mp-505622	Mn4N	0	7.329288	7.42	5	1.48
mp-680339	Mn4Si7	0.8013	5.260601	19.18	11	1.74
mp-21256	Mn7C3	0	7.85868	13.106	10	1.31
mp-771	MnAl	0	5.127965	3.61	2	1.81
mp-173	MnAl6	0	3.352783	12.56	7	1.79
mp-1106184	MnB4	0	4.493457	16.54	5	3.31
mp-1104792	MnBe12	0	2.58107	10285.82	13	791.22
mp-11270	MnBe2	0	4.819797	1715.82	3	571.94
mp-5529	MnFe2Si	0	7.393943	4.368	4	1.09
mp-1221619	MnFeSi2	0	6.145428	5.644	4	1.41
mp-1001836	MnGa	0	7.715924	149.82	2	74.91
mp-1009130	MnN	0.0945	5.922482	1.96	2	0.98
mp-11501	MnNi3	0	8.498199	43.52	4	10.88
mp-1431	MnSi	0	5.972686	3.52	2	1.76
mp-316	MnV	0	7.406262	386.82	2	193.41
mp-864984	MnV3	0	6.85173	1156.82	4	289.2
mp-129	Mo	0	10.02491	40.1	1	40.1
mp-1552	Mo2C	0	8.94399	80.322	3	26.77
mp-10172	Na	0	1.02852	3.43	1	3.43
mp-1029705	Na15Cr7N19	0.6963	2.757658	119.91	41	2.92
mp-21895	Na15Pb4	0	3.28967	59.45	19	3.13
mp-30794	Na15Sn4	0	2.382357	126.25	19	6.64
mp-31430	Na2In	0	2.931312	173.86	3	57.95
mp-865625	Na2MgSn	0.0234	2.785914	27.88	4	6.97
mp-30795	Na2Tl	0	4.426418	4206.86	3	1402.29
mp-262	Na3B20	0	2.146003	83.89	23	3.65
mp-28630	Na3BN2	1.6631	2.118291	14.25	6	2.38
mp-983509	Na3Cd	0	2.461205	13.02	4	3.26
mp-541291	Na3MoN3	1.4285	3.137351	50.81	7	7.26
mp-16839	Na3WN3	1.7694	4.437512	46.01	7	6.57
mp-571095	Na7Ga13	0	4.12335	1948.01	20	97.4
mp-541787	Na8Hg3	0	3.977038	118.04	11	10.73
mp-34763	NaAlB14	1.7015	2.657945	56.74	16	3.55
mp-27335	NaAlSi	0	2.069717	6.92	3	2.31
mp-865051	NaCa2Tl	0	4.075919	4208.13	4	1052.03
mp-866047	NaEuTl2	0	8.049246	8434.83	4	2108.71
mp-1186271	NaMg149	0.5472	1.750189	349.11	150	2.33
mp-1030657	NaNbN2	2.2984	3.738886	89.31	4	22.33
mp-865108	NaSmHg2	0	9.297066	77.73	4	19.43
mp-10811	NaSr4(BN2)3	2.4848	3.719149	42.03	14	3
mp-5475	NaTaN2	1.3323	7.914573	315.71	4	78.93
mp-1029711	NaVN2	0.945	2.811362	388.71	4	97.18
mp-950	NaZn13	0	6.241478	36.58	14	2.61
mp-75	Nb	0	8.427647	85.6	1	85.6
mp-18427	Nb2Al	0	6.789454	172.99	3	57.66
mp-569989	Nb2C	0	7.673756	171.322	3	57.11
mp-1079585	Nb2N	0	8.022841	171.34	3	57.11
mp-11393	Nb3Ga2	0	8.136718	552.8	5	110.56
mp-1192618	Nb4Fe4Si7	0	6.627655	355.996	15	23.73
mp-13686	Nb5Si3	0	6.967601	433.1	8	54.14
mp-2760	Nb6C5	0	7.503639	514.21	11	46.75
mp-542995	Nb6Fe16Si7	0	7.716441	532.284	29	18.35
mp-1842	NbAl3	0	4.501844	90.97	4	22.74
mp-1221111	NbFe	0	8.528215	86.024	2	43.01
mp-1192350	NbFe2	0	8.80312	86.448	3	28.82
mp-1209887	NbFeSi	0	7.175613	87.724	3	29.24
mp-1196167	NbFeSi2	0	6.407325	89.424	4	22.36
mp-2634	NbN	0	7.984187	85.74	2	42.87
mp-12104	NbSi2	0	5.57744	89	3	29.67
mp-1220316	NbW	0	13.43139	120.9	2	60.45
mp-123	Nd	0	6.758696	57.5	1	57.5
mp-567415	Nd2B5	0	5.945181	133.4	7	19.06
mp-1800	Nd2C3	0	6.738088	115.366	5	23.07
mp-356	Nd2Co17	0	8.660875	672.6	19	35.4
mp-1084826	Nd2Co3	0	8.309643	213.4	5	42.68
mp-1106011	Nd3Co	0	7.282344	205.3	4	51.33
mp-1203103	Nd3Ga2	0	6.751688	468.5	5	93.7
mp-1533	Nd3Tl	0	8.457986	4372.5	4	1093.12
mp-1104652	Nd5Co2	0	7.325777	353.1	7	50.44
mp-567735	Nd5Si3	0	6.280953	292.6	8	36.58
mp-355	Nd5Si4	0	5.868755	294.3	9	32.7
mp-1632	NdB4	0	5.768966	72.22	5	14.44
mp-1929	NdB6	0	4.908784	79.58	7	11.37
mp-13392	NdCu	0	7.323929	63.5	2	31.75
mp-11852	NdCu2	0	7.992311	69.5	3	23.17
mp-1140	NdCu5	0	8.263728	87.5	6	14.58
mp-1448	NdGa	0	6.683011	205.5	2	102.75
mp-2524	NdGa2	0	6.886527	353.5	3	117.83
mp-11467	NdHg	0	10.08719	87.7	2	43.85
mp-1327	NdMg	0	4.772306	59.82	2	29.91
mp-1787	NdMg3	0	3.533555	64.46	4	16.11
mp-2599	NdN	0.4304	7.62743	57.64	2	28.82
mp-9967	NdSi	0	5.927845	59.2	2	29.6
mp-884	NdSi2	0	5.35905	60.9	3	20.3
mp-571405	NdTl	0	9.670593	4257.5	2	2128.75
mp-23	Ni	0	9.04769	13.9	1	13.9
mp-2536	Ni2B	0	8.108396	31.48	3	10.49
mp-4091	Ni2Mo3N	0	9.425318	148.24	6	24.71
mp-2058	Ni3B	0	8.260442	45.38	4	11.35
mp-11506	Ni3Mo	0	9.512797	81.8	4	20.45
mp-640067	Ni4B3	0	7.579792	66.64	7	9.52
mp-11507	Ni4Mo	0	9.438042	95.7	5	19.14
mp-30811	Ni4W	0	11.89007	90.9	5	18.18
mp-1179656	Rb	0	1.572308	15500	1	15500
mp-1202504	Rb7NaSi8	1.6841	2.462322	108517.03	16	6782.31
mp-568643	RbC8	0	2.448462	15500.976	9	1722.33
mp-1029828	RbCrN2	0.1903	4.05414	15509.68	4	3877.42
mp-67	Sc	0	3.023051	3460	1	3460
mp-29941	Sc2C	0	3.118297	6920.122	3	2306.71
mp-31348	Sc2In	0	4.870412	7087	3	2362.33
mp-685209	Sc39N34	0	4.06597	134944.76	73	1848.56
mp-28733	Sc3C4	0	3.561973	10380.488	7	1482.93
mp-30666	Sc3Ga2	0	4.417557	10676	5	2135.2
mp-1200767	Sc3Ga5	0	5.465766	11120	8	1390
mp-861910	Sc3Hg	0	6.095376	10410.2	4	2602.55
mp-19713	Sc3In	0	4.443026	10547	4	2636.75
mp-1186974	Sc3Tl	0	5.95077	14580	4	3645
mp-15661	Sc4C3	0.4656	3.799359	13840.366	7	1977.2
mp-7822	Sc5Si3	0	3.252083	17305.1	8	2163.14
mp-17695	Sc5Sn3	0	5.104694	17356.1	8	2169.51
mp-2252	ScB2	0	3.660544	3467.36	3	1155.79
mp-1169	ScCu	0	5.22254	3466	2	1733
mp-1018149	ScCu2	0	6.252104	3472	3	1157.33
mp-11411	ScGa	0	4.705647	3608	2	1804
mp-932	ScGa3	0	6.02691	3904	4	976
mp-11471	ScHg	0	9.281451	3490.2	2	1745.1
mp-1207100	ScIn	0	5.842138	3627	2	1813.5
mp-2857	ScN	0.325	4.245782	3460.14	2	1730.07
mp-9969	ScSi	0	3.336116	3461.7	2	1730.85
mp-11566	ScZn	0	4.846371	3462.55	2	1731.28
mp-13503	ScZn2	0	5.692297	3465.1	3	1155.03
mp-862260	ScZn3	0	6.031671	3467.65	4	866.91
mp-1219746	ScZn6	0	6.527959	3475.3	7	496.47
mp-149	Si	0.8527	2.281194	1.7	1	1.7
mp-27276	Si12Ni31	0	7.616395	451.3	43	10.5
mp-2291	Si2Ni	0	4.724646	17.3	3	5.77
mp-1620	Si2W	0	9.68978	38.7	3	12.9
mp-568656	SiC	2.0411	3.171908	1.822	2	0.91
mp-351	SiNi	0	5.981087	15.6	2	7.8
mp-1118	SiNi2	0	7.347407	29.5	3	9.83
mp-828	SiNi3	0	7.87571	43.4	4	10.85
mp-86	Sm	0	7.336111	13.9	1	13.9
mp-570421	Sm2B5	0	6.381171	46.2	7	6.6
mp-1219177	Sm2C	0	6.963794	27.922	3	9.31
mp-569335	Sm2C3	0	7.34282	28.166	5	5.63
mp-319	Sm2Tl	0	9.21902	4227.8	3	1409.27
mp-1106373	Sm5Si3	0	6.518409	74.6	8	9.32
mp-8546	SmB4	0	6.100419	28.62	5	5.72
mp-6996	SmB6	0	5.111503	35.98	7	5.14
mp-980769	SmCu	0	7.954064	19.9	2	9.95
mp-1077154	SmCu2	0	8.113357	25.9	3	8.63
mp-227	SmCu5	0	8.498336	43.9	6	7.32
mp-1025489	SmSi	0	6.372032	15.6	2	7.8
mp-13955	SmSi2	0	5.661701	17.3	3	5.77
mp-2541	SmTl	0	10.22034	4213.9	2	2106.95
mp-1187073	Sr	0	2.676562	6.68	1	6.68
mp-705522	Sr28In11	0	3.772801	2024.04	39	51.9
mp-1245	Sr2N	0	3.493077	13.5	3	4.5
mp-30828	Sr2Pb	0.0363	5.302832	15.36	3	5.12
mp-1106	Sr2Si	0.3434	3.353462	15.06	3	5.02
mp-978	Sr2Sn	0.1528	4.212174	32.06	3	10.69
mp-1218375	Sr2Zn5Si3	0	4.993594	31.21	10	3.12
mp-7068	Sr3(AlSi)2	0	3.159108	27.02	7	3.86
mp-13427	Sr3Hg2	0	5.878161	80.44	5	16.09
mp-1109	Sr5Al9	0	3.185371	49.51	14	3.54
mp-542484	Sr5Cd3	0	4.068645	41.59	8	5.2
mp-746	Sr5Si3	0	3.349596	38.5	8	4.81
mp-17720	Sr5Sn3	0	4.296219	89.5	8	11.19
mp-30782	Sr6Mg23	0	2.168975	93.44	29	3.22
mp-30667	Sr8Ga7	0	4.01657	1089.44	15	72.63
mp-2775	SrAl4	0	2.89718	13.84	5	2.77
mp-3698	SrAlSi	0	3.162717	10.17	3	3.39
mp-242	SrB6	0.035	3.417061	28.76	7	4.11
mp-2080	SrBe13	0	2.424044	11147.68	14	796.26
mp-1208630	SrC6	0	3.270211	7.412	7	1.06
mp-7084	SrCaSi	0.4225	2.831609	10.73	3	3.58
mp-30496	SrCd	0	4.884926	9.41	2	4.71
mp-677	SrCd2	0	5.74978	12.14	3	4.05
mp-1025402	SrCu	0	4.000956	12.68	2	6.34
mp-2726	SrCu5	0	6.972726	36.68	6	6.11
mp-182	SrGa2	0	4.754548	302.68	3	100.89
mp-1827	SrGa4	0	5.572999	598.68	5	119.74
mp-542	SrHg	0	7.325554	36.88	2	18.44
mp-608072	SrIn	0	4.661916	173.68	2	86.84
mp-20074	SrIn2	0	5.762914	340.68	3	113.56
mp-1187198	SrMg2	0	2.399509	11.32	3	3.77
mp-29973	SrN	0	3.854518	6.82	2	3.41
mp-10564	SrN2	0	4.089657	6.96	3	2.32
mp-2661	SrSi	0	3.451942	8.38	2	4.19
mp-1727	SrSi2	0	3.472602	10.08	3	3.36
mp-1698	SrSn	0	4.849131	25.38	2	12.69
mp-2434	SrTl	0	6.949817	4206.68	2	2103.34
mp-12724	SrZn	0	3.978955	9.23	2	4.62
mp-18026	SrZn11	0	6.671607	34.73	12	2.89
mp-672707	SrZn13	0	6.710137	39.83	14	2.84
mp-569426	SrZn2	0	4.961627	11.78	3	3.93
mp-1435	SrZn5	0	5.826695	19.43	6	3.24
mp-9556	SrZnSi	0	4.139152	10.93	3	3.64
mp-50	Ta	0	16.3878	312	1	312
mp-1193531	Ta2Al	0	12.51252	625.79	3	208.6
mp-1079438	Ta2N	0	15.39304	624.14	3	208.05
mp-1867	Ta2Ni	0	14.78623	637.9	3	212.63
mp-568646	Ta3Si	0	13.88613	937.7	4	234.43
mp-1187206	Ta3W	0	17.11634	971.3	4	242.82
mp-1989	Ta5Si3	0	12.78743	1565.1	8	195.64
mp-869	TaAl3	0	6.813776	317.37	4	79.34
mp-12678	TaMn2	0	12.19994	315.64	3	105.21
mp-1279	TaN	0	13.99559	312.14	2	156.07
mp-570491	TaNi3	0	12.03461	353.7	4	88.42
mp-11192	TaSi2	0	8.940924	315.4	3	105.13
mp-567276	TaV2	0	10.38566	1082	3	360.67
mp-1217811	TaW	0	17.65981	347.3	2	173.65
mp-979289	TaW3	0	18.29085	417.9	4	104.47
mp-72	Ti	0	4.646837	11.7	1	11.7
mp-1202079	Ti21Mn25	0	6.379829	291.2	46	6.33
mp-10721	Ti2C	0	4.439769	23.522	3	7.84
mp-742	Ti2Cu	0	5.72218	29.4	3	9.8
mp-30671	Ti2Ga	0	5.649652	171.4	3	57.13
mp-30673	Ti2Ga3	0	6.382991	467.4	5	93.48
mp-861983	Ti2MnFe	0	6.549537	25.644	4	6.41
mp-8282	Ti2N	0	4.881545	23.54	3	7.85
mp-1808	Ti2Ni	0	5.725014	37.3	3	12.43
mp-1014229	Ti2Zn	0	5.462442	25.95	3	8.65
mp-1823	Ti3Al	0	4.248869	36.89	4	9.22
mp-1025170	Ti3B4	0	4.557548	49.82	7	7.12
mp-2643	Ti3Cu4	0	6.7483	59.1	7	8.44
mp-30672	Ti3Ga	0	5.416551	183.1	4	45.77
mp-5659	Ti3SiC2	0	4.474908	37.044	6	6.17
mp-1079460	Ti3Sn	0	6.048169	53.8	4	13.45
mp-2108	Ti5Si3	0	4.347039	63.6	8	7.95
mp-995201	Ti5Si3C	0	4.457871	63.722	9	7.08
mp-505527	Ti5Si4	0	4.254735	65.3	9	7.26
mp-11750	Ti6Si2B	0	4.445879	77.28	9	8.59
mp-27919	Ti8C5	0	4.541438	94.21	13	7.25
mp-1953	TiAl	0	3.833902	13.49	2	6.74
mp-567705	TiAl2	0	3.536391	15.28	3	5.09
mp-542915	TiAl3	0	3.365706	17.07	4	4.27
mp-7857	TiB	0	4.575881	15.38	2	7.69
mp-1145	TiB2	0	4.487425	19.06	3	6.35
mp-631	TiC	0	4.879907	11.822	2	5.91
mp-568636	TiCr2	0	6.234566	30.5	3	10.17
mp-2078	TiCu	0	6.440936	17.7	2	8.85
mp-12546	TiCu3	0	7.648118	29.7	4	7.42
mp-1188441	TiCu4	0	7.892997	35.7	5	7.14
mp-305	TiFe	0	6.642035	12.124	2	6.06
mp-866141	TiFe2Si	0.4023	6.758128	14.248	4	3.56
mp-8648	TiFeSi	0	5.624878	13.824	3	4.61
mp-21662	TiFeSi2	0	5.143236	15.524	4	3.88
mp-2767	TiGa	0	6.197683	159.7	2	79.85
mp-571342	TiGa2	0	6.575088	307.7	3	102.57
mp-1949	TiMn2	0	6.901374	15.34	3	5.11
mp-865652	TiMn2Si	0	6.352313	17.04	4	4.26
mp-865656	TiMn2W	0	10.69469	50.64	4	12.66
mp-21606	TiMnSi2	0	4.998157	16.92	4	4.23
mp-492	TiN	0	5.340297	11.84	2	5.92
mp-1048	TiNi	0	6.412986	25.6	2	12.8
mp-1409	TiNi3	0	7.95813	53.4	4	13.35
mp-7092	TiSi	0	4.224309	13.4	2	6.7
mp-1077503	TiSi2	0	4.027105	15.1	3	5.03
mp-1216621	TiW	0	11.85553	47	2	23.5
mp-1014230	TiZn	0	6.036543	14.25	2	7.12
mp-21289	TiZn3	0	6.69766	19.35	4	4.84
mp-146	V	0	6.312904	385	1	385
mp-1216643	V10Si6B	0	5.323133	3863.88	17	227.29
mp-9208	V2B3	0	5.360224	781.04	5	156.21
mp-20648	V2C	0	5.741138	770.122	3	256.71
mp-33090	V2N	0	6.096388	770.14	3	256.71
mp-2091	V3B2	0	5.846065	1162.36	5	232.47
mp-569270	V3B4	0	5.426881	1169.72	7	167.1
mp-1585	V3Co	0	6.985027	1187.8	4	296.95
mp-1187695	V3Cr	0	6.599356	1164.4	4	291.1
mp-1216481	V3Cr3Si2	0	6.213883	1186.6	8	148.33
mp-1079399	V3Fe	0	6.896938	1155.424	4	288.86
mp-972071	V3Mo	0	7.371335	1195.1	4	298.77
mp-7226	V3Ni	0	6.898755	1168.9	4	292.23
mp-1216708	V3Ni2	0	7.272789	1182.8	5	236.56
mp-2567	V3Si	0	5.778142	1156.7	4	289.18
mp-30883	V4Zn5	0	6.973256	1552.75	9	172.53
mp-1206441	V5B6	0	5.503664	1947.08	11	177.01
mp-568671	V5Si3	0	5.379232	1930.1	8	241.26
mp-10126	V5SiB2	0	5.621738	1934.06	8	241.76
mp-28731	V6C5	0	5.617823	2310.61	11	210.06
mp-1188283	V8N	0	6.188838	3080.14	9	342.24
mp-1216445	V9Cr3B8	0	6.010542	3522.64	20	176.13
mp-9973	VB	0	5.631694	388.68	2	194.34
mp-1491	VB2	0	5.108571	392.36	3	130.79
mp-542614	VCo3	0	8.70633	483.4	4	120.85
mp-1216394	VCr	0	6.919501	394.4	2	197.2
mp-1187696	VCr3	0	7.195388	413.2	4	103.3
mp-866134	VFe3	0	7.739815	386.272	4	96.57
mp-1018027	VN	0	6.23865	385.14	2	192.57
mp-11531	VNi2	0	8.166036	412.8	3	137.6
mp-171	VNi3	0	8.437749	426.7	4	106.67
mp-10711	VSi2	0	4.640836	388.4	3	129.47
mp-1216231	VW	0	13.07376	420.3	2	210.15
mp-1187702	VW3	0	16.12824	490.9	4	122.72
mp-11578	VZn3	0	7.294936	392.65	4	98.16
mp-91	W	0	18.85401	35.3	1	35.3
mp-1894	WC	0	15.35037	35.422	2	17.71
mp-1187739	Y	0	4.54735	31	1	31
mp-1199133	Y11Sn10	0	6.169806	528	21	25.14
mp-1334	Y2C	0	4.535818	62.122	3	20.71
mp-21294	Y2In	0	5.66966	229	3	76.33
mp-1200613	Y3C4	0	4.91445	93.488	7	13.36
mp-1105835	Y3In5	0	6.657923	928	8	116
mp-9459	Y4C5	0	4.729248	124.61	9	13.85
mp-1200885	Y4C7	0.6144	4.541711	124.854	11	11.35
mp-1188292	Y5Pb3	0	7.410237	161	8	20.12
mp-2538	Y5Si3	0	4.436242	160.1	8	20.01
mp-567412	Y5Sn3	0	5.778886	211.1	8	26.39
mp-1188434	Y5Tl3	0	7.379251	12755	8	1594.38
mp-972364	Yb	0	7.005867	17.1	1	17.1
mp-1542	YB2	0	5.045298	38.36	3	12.79
mp-9546	Yb2C3	0	8.72673	34.566	5	6.91
mp-11544	Yb2Pb	0	9.844348	36.2	3	12.07
mp-1207599	Yb2Si	0.0437	7.742296	35.9	3	11.97
mp-570050	Yb2Sn	0	8.771931	52.9	3	17.63
mp-864675	Yb3N2	0.4892	10.30057	51.58	5	10.32
mp-637	YB4	0	4.308482	45.72	5	9.14
mp-1189298	YbB4	0	6.949843	31.82	5	6.36
mp-419	YbB6	0.1059	5.614594	39.18	7	5.6
mp-1103975	YbC6	0	5.687259	17.832	7	2.55
mp-1857	YbCd	0	8.562931	19.83	2	9.92
mp-1187653	YbCd3	0	8.670607	25.29	4	6.32
mp-1937	YbCu	0	9.051708	23.1	2	11.55
mp-567538	YbCu2	0	9.550794	29.1	3	9.7
mp-1607	YbCu5	0	9.333349	47.1	6	7.85
mp-864757	YbN2	0	8.325277	17.38	3	5.79
mp-10651	YbSi	0	7.137531	18.8	2	9.4
mp-1077404	YbSi2	0	6.315081	20.5	3	6.83
mp-915	YCd	0	6.30281	33.73	2	16.86
mp-1331	YCd2	0	6.972865	36.46	3	12.15
mp-1080443	YCu	0	5.830094	37	2	18.5
mp-2698	YCu2	0	6.706395	43	3	14.33
mp-2797	YCu5	0	7.535186	61	6	10.17
mp-2399	YHg	0	9.24362	61.2	2	30.6
mp-22704	YIn	0	6.291689	198	2	99
mp-615	YMg	0	3.419334	33.32	2	16.66
mp-1188082	YMg149	0.2723	1.786909	376.68	150	2.51
mp-865376	YMg3	0	2.731204	37.96	4	9.49
mp-2114	YN	0.2858	5.742757	31.14	2	15.57
mp-9972	YSi	0	4.464026	32.7	2	16.35
mp-22179	YTiSi	0	4.422839	44.4	3	14.8
mp-11575	YTl	0	8.800691	4231	2	2115.5
mp-131	Zr	0	6.446092	37.1	1	37.1
mp-684623	Zr10C9	0	6.396417	372.098	19	19.58
mp-1216441	Zr14Cu51	0	8.184391	825.4	65	12.7
mp-2544	Zr2Be17	0	3.115806	14643.2	19	770.69
mp-1018104	Zr2Cd	0	7.235683	76.93	3	25.64
mp-628	Zr2Co	0	7.170771	107	3	35.67
mp-193	Zr2Cu	0	6.968518	80.2	3	26.73
mp-1215517	Zr2MnFe3	0	7.605015	77.292	6	12.88
mp-1014265	Zr2N	0	6.644609	74.34	3	24.78
mp-328	Zr2Ni	0	7.189329	88.1	3	29.37
mp-2717	Zr2Ni7	0	8.441843	171.5	9	19.06
mp-1278	Zr2Si	0	5.972091	75.9	3	25.3
mp-31310	Zr3(Mn2Si3)2	0	5.882738	128.78	13	9.91
mp-30619	Zr3Co	0	6.915076	144.1	4	36.03
mp-31205	Zr3Fe	0	6.808805	111.724	4	27.93
mp-277	Zr3N4	1.2736	6.14326	111.86	7	15.98
mp-1188062	Zr3Sc	0	5.604938	3571.3	4	892.83
mp-1207024	Zr3Si2	0	5.812221	114.7	5	22.94
mp-1215386	Zr3Ti2Si3	0	5.343721	139.8	8	17.48
mp-17435	Zr4Fe4Si7	0	6.038802	161.996	15	10.8
mp-1106020	Zr5SiSn3	0	7.175692	243.3	9	27.03
mp-510522	Zr5Sn3	0	7.32854	241.6	8	30.2
mp-543001	Zr5Sn4	0	7.607774	260.3	9	28.92
mp-30569	Zr6Co23	0	8.29963	977	29	33.69
mp-1192960	Zr6Fe16Si7	0	7.260913	241.284	29	8.32
mp-582924	Zr6Fe23	0	7.603507	232.352	29	8.01
mp-1188077	Zr7Cu10	0	7.760948	319.7	17	18.81
mp-1472	ZrB2	0	6.033105	44.46	3	14.82
mp-30445	ZrBe13	0	2.771776	11178.1	14	798.44
mp-11283	ZrBe5	0	3.623394	4322.1	6	720.35
mp-2795	ZrC	0	6.502964	37.222	2	18.61
mp-2283	ZrCo	0	7.64963	69.9	2	34.95
mp-929	ZrCo2	0	8.422444	102.7	3	34.23
mp-1190681	ZrFe2	0	7.666415	37.948	3	12.65
mp-1102452	ZrFeSi	0	6.48392	39.224	3	13.07
mp-2116	ZrMn2	0	7.670876	40.74	3	13.58
mp-2049	ZrMo2	0	8.470044	117.3	3	39.1
mp-1352	ZrN	0	7.098978	37.24	2	18.62
mp-556	ZrNi	0	7.396409	51	2	25.5
mp-485	ZrNi3	0	8.426585	78.8	4	19.7
mp-1077791	ZrSc2	0	4.159366	6957.1	3	2319.03
mp-893	ZrSi	0	5.562651	38.8	2	19.4
mp-1515	ZrSi2	0	4.846511	40.5	3	13.5
mp-675	ZrW2	0	13.52059	107.7	3	35.9
mp-570276	ZrZn	0.0231	6.949384	39.65	2	19.82
mp-1401	ZrZn2	0	7.229958	42.2	3	14.07
mp-864889	ZrZn3	0	7.245114	44.75	4	11.19
mp-134	Al	0	2.720049585	1.79	1	1.79
mp-10010	Al(CoSi)2	0	5.38758579	70.79	5	14.16
mp-1214980	Al11(CoSi)6	0	4.376129548	226.69	23	9.86
mp-11227	Al12W	0	3.857812654	56.78	13	4.37
mp-29110	Al2(FeSi)3	0.2303	5.163780949	9.952	8	1.24
mp-568153	Al22Mo5	0	4.244948798	239.88	27	8.88
mp-530274	Al23B50	0	3.044723378	225.17	73	3.08
mp-985806	Al2Cu	0	4.064939117	9.58	3	3.19
mp-1214851	Al3Co3Si4	0	4.618943212	110.57	10	11.06
mp-867780	Al3Cr	0	3.815305682	14.77	4	3.69
mp-1190708	Al3Fe2Si	0	4.725578345	7.918	6	1.32
mp-622209	Al3Ni	0	4.034331992	19.27	4	4.82
mp-1057	Al3Ni2	0	4.767798907	33.17	5	6.63
mp-16514	Al3Ni5	0	6.717313154	74.87	8	9.36
mp-31019	Al45Cr7	0	3.226501467	146.35	52	2.81
mp-1591	Al4C3	1.3422	2.930804107	7.526	7	1.08
mp-593	Al4Cu9	0	6.853922942	61.16	13	4.7
mp-16515	Al4Ni3	0	5.093005275	48.86	7	6.98
mp-1229054	Al53Fe17Si12	0	3.847798315	122.478	82	1.49
mp-196	Al5Co2	0	4.338445784	74.55	7	10.65
mp-30337	Al5W	0	5.700302322	44.25	6	7.38
mp-570001	Al6Fe	0	3.428138324	11.164	7	1.59
mp-1229249	Al79(Fe13Si9)2	0	3.829625029	183.034	123	1.49
mp-2733	Al8Mo3	0	5.003746922	134.62	11	12.24
mp-16488	Al9Co2	0	3.608519273	81.71	11	7.43
mp-284	AlCo	0	6.136768975	34.59	2	17.29
mp-1699	AlCr2	0	5.748722101	20.59	3	6.86
mp-2500	AlCu	0	5.356855143	7.79	2	3.9
mp-12802	AlCu3	0	7.287481775	19.79	4	4.95
mp-2658	AlFe	0	5.791723495	2.214	2	1.11
mp-867878	AlFe2Si	0	6.289050137	4.338	4	1.08
mp-1183162	AlFe3	0	6.647849573	3.062	4	0.77
mp-259	AlMo3	0	8.470007673	122.09	4	30.52
mp-1487	AlNi	0	5.906844592	15.69	2	7.85
mp-2593	AlNi3	0	7.466731653	43.49	4	10.87
mp-1228043	AlSiNi2	0	6.061604569	31.29	4	7.82
mp-1228041	AlSiNi6	0	7.76613683	86.89	8	10.86
mp-576	B13C2	0	2.438647853	48.084	15	3.21
mp-122	Ba	0	3.583054105	0.275	1	0.28
mp-5506	Ba(AlSi)2	0	3.475027368	7.255	5	1.45
mp-1029457	Ba(CoN)2	0	5.554370311	66.155	5	13.23
mp-567701	Ba21Al40	0	3.884212974	77.375	61	1.27
mp-8093	Ba2Cd	0	4.503963702	3.28	3	1.09
mp-8094	Ba2Hg	0	5.677447644	30.75	3	10.25
mp-1892	Ba2N	0	4.403707635	0.69	3	0.23
mp-9905	Ba2Si	0.0553	4.278608479	2.25	3	0.75
mp-1981	Ba2Sn	0.0155	4.834448032	19.25	3	6.42
mp-1018178	Ba2Zn	0	4.272596092	3.1	3	1.03
mp-9578	Ba3(AlSi)2	0	3.898587575	7.805	7	1.11
mp-10736	Ba3N	0	3.84449865	0.965	4	0.24
mp-1619	Ba3Si4	0.0012	3.952256738	7.625	7	1.09
mp-2631	Ba4Al5	0	3.901346877	10.05	9	1.12
mp-570400	Ba7Al10	0	3.91077423	19.825	17	1.17
mp-30429	Ba8Ga7	0	4.702519133	1038.2	15	69.21
mp-28685	Ba8Ni6N7	0	5.519552142	86.58	21	4.12
mp-1105101	Ba9In4	0	4.681514321	670.475	13	51.58
mp-1903	BaAl4	0	3.425431948	7.435	5	1.49
mp-13149	BaAlSi	0	3.806505582	3.765	3	1.25
mp-954	BaB6	0.0623	4.281989038	22.355	7	3.19
mp-1214417	BaC6	0	3.961948599	1.007	7	0.14
mp-16253	BaCaSi	0.1767	3.413083529	4.325	3	1.44
mp-527	BaCd	0	5.290471212	3.005	2	1.5
mp-11266	BaCd2	0	6.057559503	5.735	3	1.91
mp-505765	BaCoN	0	5.562269068	33.215	3	11.07
mp-30428	BaCu	0	4.510555041	6.275	2	3.14
mp-29199	BaCuN	0.0476	5.610479725	6.415	3	2.14
mp-1219	BaGa2	0	5.173339705	296.275	3	98.76
mp-335	BaGa4	0	5.942574395	592.275	5	118.45
mp-2197	BaHg	0	7.458274924	30.475	2	15.24
mp-31509	BaIn	0	5.565138269	167.275	2	83.64
mp-22141	BaIn2	0	6.050442559	334.275	3	111.42
mp-210	BaLi4	0	1.84849371	342.675	5	68.53
mp-1001	BaN2	0	4.760885188	0.555	3	0.19
mp-1247744	BaNa	0	2.601470147	3.705	2	1.85
mp-11820	BaNa2	0	2.217756088	7.135	3	2.38
mp-21653	BaNiN	0	5.723687745	14.315	3	4.77
mp-1067235	BaSi	0	4.286153704	1.975	2	0.99
mp-1477	BaSi2	0.791	3.628158493	3.675	3	1.22
mp-872	BaSn	0	5.2426579	18.975	2	9.49
mp-672225	BaZn13	0	6.875821892	33.425	14	2.39
mp-30435	BaZn2	0	5.504924829	5.375	3	1.79
mp-303	BaZn5	0	6.23064523	13.025	6	2.17
mp-87	Be	0	1.895724397	857	1	857
mp-1569	Be2C	1.4433	2.461261614	1714.122	3	571.37
mp-1183425	Be3Co	0	4.301352688	2603.8	4	650.95
mp-865168	Be3Ni	0	4.213290212	2584.9	4	646.23
mp-27757	Be4B	0	1.981767282	3431.68	5	686.34
mp-1071690	Be5Co	0	3.603654583	4317.8	6	719.63
mp-2773	BeCo	0	6.479698338	889.8	2	444.9
mp-1033	BeNi	0	6.359073941	870.9	2	435.45
mp-132	Ca	0	1.569030745	2.35	1	2.35
mp-7704	Ca(AlSi)2	0	2.347097201	9.33	5	1.87
mp-12614	Ca2Cu	0	2.62950025	10.7	3	3.57
mp-2686	Ca2N	0	2.161682878	4.84	3	1.61
mp-2517	Ca2Si	0.2915	2.165187656	6.4	3	2.13
mp-844	Ca3N2	1.1111	2.606386489	7.33	5	1.47
mp-640340	Ca4MgAl3	0	2.018737185	17.09	8	2.14
mp-1246246	Ca5(CuN2)2	0.3018	3.194817732	24.31	11	2.21
mp-793	Ca5Si3	0	2.188848043	16.85	8	2.11
mp-1190736	Ca8Al3	0	1.895135766	24.17	11	2.2
mp-2404	CaAl2	0	2.425284826	5.93	3	1.98
mp-570150	CaAlSi	0	2.354365379	5.84	3	1.95
mp-1213975	CaB4	0	2.631299144	17.07	5	3.41
mp-865	CaB6	0.1835	2.437995559	24.43	7	3.49
mp-1845	CaBe13	0	1.9473521	11143.35	14	795.95
mp-585949	CaCu	0	3.622394066	8.35	2	4.17
mp-1882	CaCu5	0	6.536938774	32.35	6	5.39
mp-1039148	CaMg	0	1.713629157	4.67	2	2.33
mp-1184449	CaMg149	0.499	1.754974539	348.03	150	2.32
mp-2432	CaMg2	0	1.731927308	6.99	3	2.33
mp-5473	CaMgSi	0.0159	2.228699165	6.37	3	2.12
mp-2295	CaNi2	0	5.661732669	30.15	3	10.05
mp-774	CaNi5	0	6.747575602	71.85	6	11.97
mp-28645	CaNiN	0	4.185006623	16.39	3	5.46
mp-1563	CaSi	0	2.377161219	4.05	2	2.02
mp-567332	Ce	0	8.91786665	4.71	1	4.71
mp-1229288	Ce15Ni32	0	9.091934601	515.45	47	10.97
mp-20181	Ce2C3	0	7.074733812	9.786	5	1.96
mp-1204381	Ce2Ni7	0	8.991082761	106.72	9	11.86
mp-1213865	Ce3Al11	0	4.225938114	33.82	14	2.42
mp-570175	Ce5Si3	0	6.736034132	28.65	8	3.58
mp-1196829	Ce5Si4	0	6.040717659	30.35	9	3.37
mp-2088	CeAl2	0	5.124395241	8.29	3	2.76
mp-567305	CeAl3	0	4.43938026	10.08	4	2.52
mp-1206597	CeAlSi	0	5.005790027	8.2	3	2.73
mp-1112	CeCo2	0	9.701049231	70.31	3	23.44
mp-2801	CeCu2	0	8.065457036	16.71	3	5.57
mp-581942	CeCu6	0	8.455393218	40.71	7	5.82
mp-11317	CeFe5	0	7.942087595	6.83	6	1.14
mp-1039345	CeMg2	0	4.198993993	9.35	3	3.12
mp-1038976	CeMg5	0	3.070870412	16.31	6	2.72
mp-2493	CeN	0	7.942475673	4.85	2	2.42
mp-21188	CeNi	0	8.086557052	18.61	2	9.3
mp-1654	CeNi2	0	9.264253029	32.51	3	10.84
mp-580354	CeNi3	0	9.035774819	46.41	4	11.6
mp-1910	CeNi5	0	8.791113399	74.21	6	12.37
mp-21115	CeSi	0	6.016046899	6.41	2	3.21
mp-1898	CeSi2	0	5.496004683	8.11	3	2.7
mp-54	Co	0	8.959676195	32.8	1	32.8
mp-19905	Co2Si	0	7.586966265	67.3	3	22.43
mp-1139	Co3Mo	0	9.788205563	138.5	4	34.62
mp-2157	Co3W	0	12.92411922	133.7	4	33.42
mp-20857	CoB	0	7.456589549	36.48	2	18.24
mp-7577	CoSi	0	6.633920595	34.5	2	17.25
mp-2379	CoSi2	0	4.964463565	36.2	3	12.07
mp-90	Cr	0	7.274080971	9.4	1	9.4
mp-723	Cr23C6	0	7.16779993	216.932	29	7.48
mp-8780	Cr2N	0	6.723825369	18.94	3	6.31
mp-20937	Cr3C2	0	6.795180146	28.444	5	5.69
mp-729	Cr3Si	0	6.625100709	29.9	4	7.48
mp-1196316	Cr7C3	0	7.055496191	66.166	10	6.62
mp-1183691	CrN	0	6.76302146	9.54	2	4.77
mp-784631	CrNi2	0	8.620907303	37.2	3	12.4
mp-8937	CrSi2	0	5.015722574	12.8	3	4.27
mp-1184151	Cs	0.1362	1.885761278	61800	1	61800
mp-1199908	Cs7NaSi8	1.5761	3.100640339	432617.03	16	27038.56
mp-1200207	Cs8Ga11	0	3.984785705	496028	19	26106.74
mp-28861	CsC8	0	2.893417416	61800.976	9	6866.78
mp-571056	CsSn	1.1371	4.131016431	61818.7	2	30909.35
mp-30	Cu	0	8.888274633	6	1	6
mp-14266	Cu15Si4	0	7.743605225	96.8	19	5.09
mp-1184115	Er	0	9.037772387	26.4	1	26.4
mp-1225044	Er2C	0	8.678709228	52.922	3	17.64
mp-1203719	Er3C4	0	8.934402703	79.688	7	11.38
mp-31167	Er5Si3	0	8.045292568	137.1	8	17.14
mp-1955	ErCu	0	9.463506465	32.4	2	16.2
mp-1024991	ErCu2	0	9.341567898	38.4	3	12.8
mp-30579	ErCu5	0	9.420409229	56.4	6	9.4
mp-19830	ErN	0.2716	10.56582866	26.54	2	13.27
mp-378	ErSi	0	7.710453561	28.1	2	14.05
mp-1057315	Eu	0	6.086594594	31.4	1	31.4
mp-1190061	Eu5Si3	0	6.153676988	162.1	8	20.26
mp-1103990	EuC6	0	4.7983116	32.132	7	4.59
mp-1087547	EuCu	0	7.049617849	37.4	2	18.7
mp-1071732	EuCu2	0	7.840235157	43.4	3	14.47
mp-2066	EuCu5	0	8.36925336	61.4	6	10.23
mp-21279	EuSi	0	5.904326861	33.1	2	16.55
mp-1072248	EuSi2	0	5.454985613	34.8	3	11.6
mp-13	Fe	0	8.096264696	0.424	1	0.42
mp-601848	Fe11Co5	0	8.108531664	168.664	16	10.54
mp-1915	Fe2B	0	7.490316494	4.528	3	1.51
mp-1194531	Fe2B7	0	4.813417026	26.608	9	2.96
mp-601820	Fe3Co	0	8.136129184	34.072	4	8.52
mp-1804	Fe3N	0	7.421215908	1.412	4	0.35
mp-2199	Fe3Si	0	7.388613931	2.972	4	0.74
mp-601842	Fe9Co7	0	8.206826997	233.416	16	14.59
mp-1080525	FeB	0	6.887696687	4.104	2	2.05
mp-2090	FeCo	0	8.290362741	33.224	2	16.61
mp-6988	FeN	0	6.127073258	0.564	2	0.28
mp-2213	FeNi	0	8.452470899	14.324	2	7.16
mp-1418	FeNi3	0	8.700535754	42.124	4	10.53
mp-871	FeSi	0.1664	6.333879998	2.124	2	1.06
mp-1714	FeSi2	0.6976	4.958877558	3.824	3	1.27
mp-20559	Ga3Co	0	7.003885998	476.8	4	119.2
mp-636368	Ga3Fe	0.575	6.809894312	444.424	4	111.11
mp-1197621	Ga4Cu9	0	8.454861321	646	13	49.69
mp-1121	GaCo	0	8.876587419	180.8	2	90.4
mp-1183995	GaCu3	0	8.629827313	166	4	41.5
mp-19870	GaFe3	0	8.032436581	149.272	4	37.32
mp-804	GaN	1.7376	5.923650599	148.14	2	74.07
mp-155	Gd	0	8.001978666	28.6	1	28.6
mp-28366	Gd2B5	0	6.836473994	75.6	7	10.8
mp-1224869	Gd2C	0	7.676989498	57.322	3	19.11
mp-1189998	Gd2C3	0	7.992746631	57.566	5	11.51
mp-1199486	Gd5Si4	0	6.902406182	149.8	9	16.64
mp-1105563	GdB4	0	6.464597962	43.32	5	8.66
mp-22266	GdB6	0	5.311473692	50.68	7	7.24
mp-614455	GdCu	0	8.506837674	34.6	2	17.3
mp-1077933	GdCu2	0	8.348842083	40.6	3	13.53
mp-636253	GdCu5	0	8.925302406	58.6	6	9.77
mp-601371	GdSi	0	6.899144562	30.3	2	15.15
mp-21192	GdSi2	0	6.050125559	32	3	10.67
mp-103	Hf	0	13.1832226	900	1	900
mp-1224756	Hf14Cu51	0	10.75330004	12906	65	198.55
mp-30581	Hf2Cu	0	12.40423989	1806	3	602
mp-7353	Hf3Cu8	0	10.98413983	2748	11	249.82
mp-1200988	Hf7Cu10	0	11.4017787	6360	17	374.12
mp-21075	HfC	0	12.57416771	900.122	2	450.06
mp-1185513	HfMg149	0.1369	1.836793837	1245.68	150	8.3
mp-11449	HfMn2	0	11.30554994	903.64	3	301.21
mp-2363	HfMo2	0	11.27480816	980.2	3	326.73
mp-1018056	HfNi	0	12.18394482	913.9	2	456.95
mp-12174	HfNi3	0	11.44805813	941.7	4	235.43
mp-10659	Ho	0	8.822554243	57.1	1	57.1
mp-5835	Ho(CoSi)2	0	7.719283863	126.1	5	25.22
mp-569851	Ho10Si17	0	6.713993228	599.9	27	22.22
mp-30969	Ho12Co7	0	9.630259551	914.8	19	48.15
mp-1640	Ho2C	0	8.412835248	114.322	3	38.11
mp-977345	Ho2Co3Si5	0	7.221989364	221.1	10	22.11
mp-1202754	Ho3C4	0	8.700157642	171.788	7	24.54
mp-622565	Ho3Co	0	9.19085619	204.1	4	51.03
mp-15238	Ho4C5	0	8.4097617	229.01	9	25.45
mp-1154	Ho4C7	0.5867	7.857241425	229.254	11	20.84
mp-1203317	Ho5(Co2Si7)2	0	6.55275451	440.5	23	19.15
mp-13236	Ho5Si3	0	7.80740996	290.6	8	36.33
mp-1193889	HoBe13	0	3.576271217	11198.1	14	799.86
mp-2396	HoCo2	0	10.22290726	122.7	3	40.9
mp-2435	HoCo5	0	9.268919768	221.1	6	36.85
mp-510688	HoCoSi	0	8.468342148	91.6	3	30.53
mp-1971	HoCu	0	9.2535428	63.1	2	31.55
mp-30584	HoCu2	0	9.05706546	69.1	3	23.03
mp-30585	HoCu5	0	9.039159021	87.1	6	14.52
mp-883	HoN	0.2401	10.23272256	57.24	2	28.62
mp-12899	HoSi	0	7.513612499	58.8	2	29.4
mp-19876	InNi	0	8.211460739	180.9	2	90.45
mp-1184905	K	0	0.868387443	13.6	1	13.6
mp-1212012	K10Tl7	0	3.784372673	29536	17	1737.41
mp-1029850	K15Cr7N19	0.8138	2.722030031	272.46	41	6.65
mp-1029869	K15Mo7N19	1.372	3.041028409	487.36	41	11.89
mp-1030950	K15W7N19	1.5737	4.208765957	453.76	41	11.07
mp-1197369	K16Na9(Tl6Cd)3	0	4.704089312	75856.66	46	1649.06
mp-1225049	K18Na46Tl31	0	3.927045378	130602.58	95	1374.76
mp-504498	K2CdPb	0.0295	4.072717098	31.93	4	7.98
mp-1079679	K2CdSn	0.0811	3.278764613	48.63	4	12.16
mp-568052	K2Ga3	0.2755	3.30315191	471.2	5	94.24
mp-1087476	K2Mg5Sn3	0	3.121450804	94.9	10	9.49
mp-1246385	K2MnN2	0	2.63171743	29.3	5	5.86
mp-1211956	K2Na4ZnSn2	0	2.673871555	80.87	9	8.99
mp-1202778	K3Cd16	0	6.101150525	84.48	19	4.45
mp-3949	K7LiSi8	1.693	1.69342103	194.4	16	12.15
mp-582929	K8In11	0	3.431014453	1945.8	19	102.41
mp-1076	KB6	0	2.288806586	35.68	7	5.1
mp-28930	KC8	0	1.94998649	14.576	9	1.62
mp-1029673	KCrN2	0	3.068116666	23.28	4	5.82
mp-11462	KHg	0	4.967016325	43.8	2	21.9
mp-1019888	KNa2BN2	1.8907	2.181667813	24.42	6	4.07
mp-1223632	KNa2WN3	2.0295	4.291152456	56.18	7	8.03
mp-1029504	KNbN2	2.0359	3.538072207	99.48	4	24.87
mp-21526	KPb	0.3735	4.934516761	15.6	2	7.8
mp-1217	KSi	1.2619	1.742991866	15.3	2	7.65
mp-542374	KSn	0.7335	3.342551901	32.3	2	16.15
mp-570755	KTaN2	2.6564	5.478996242	325.88	4	81.47
mp-1080848	KVN2	0.895	2.980739473	398.88	4	99.72
mp-784	KZn13	0	6.227279729	46.75	14	3.34
mp-1018134	Li	0	0.57309457	85.6	1	85.6
mp-510430	Li13In3	0	2.471080344	1613.8	16	100.86
mp-672287	Li13Si4	0	1.28359662	1119.6	17	65.86
mp-1222798	Li14MgSi4	0.1059	1.286983594	1207.52	19	63.55
mp-574275	Li17Pb4	0	3.961250168	1463.2	21	69.68
mp-573471	Li17Sn4	0	2.589548849	1530	21	72.86
mp-29720	Li21Si5	0	1.194591756	1806.1	26	69.47
mp-1210753	Li2Al	0	1.381340819	172.99	3	57.66
mp-570466	Li2Ca	0	1.083251032	173.55	3	57.85
mp-865965	Li2CaSi	0	1.924169662	175.25	4	43.81
mp-29210	Li2Ga	0	2.981136533	319.2	3	106.4
mp-31324	Li2In	0	3.818917214	338.2	3	112.73
mp-1105932	Li2MgSi	0.218	1.705165271	175.22	4	43.8
mp-16506	Li3Al2	0	1.538620171	260.38	5	52.08
mp-9568	Li3Ga2	0	3.489024203	552.8	5	110.56
mp-867226	Li3In	0	3.062220684	423.8	4	105.95
mp-21293	Li3In2	0	4.325351176	590.8	5	118.16
mp-1094591	Li3Mg	0	0.919301997	259.12	4	64.78
mp-2251	Li3N	0.9986	1.288608955	256.94	4	64.23
mp-30760	Li3Pb	0	5.056392137	258.8	4	64.7
mp-1185265	Li3Sn	0	3.260207542	275.5	4	68.87
mp-7396	Li3Tl	0	5.009351079	4456.8	4	1114.2
mp-1205930	Li5Ga4	0	3.760162948	1020	9	113.33
mp-30766	Li5Sn2	0	3.555816317	465.4	7	66.49
mp-12283	Li5Tl2	0	5.534063942	8828	7	1261.14
mp-30761	Li7Pb2	0	4.575943292	603.2	9	67.02
mp-1201871	Li7Si3	0	1.477568272	604.3	10	60.43
mp-30767	Li7Sn2	0	2.974647662	636.6	9	70.73
mp-1067	LiAl	0	1.754628439	87.39	2	43.7
mp-10890	LiAl3	0	2.237074984	90.97	4	22.74
mp-8204	LiAlB14	1.2932	2.498475464	138.91	16	8.68
mp-3161	LiAlSi	0.1426	1.966694453	89.09	3	29.7
mp-1001835	LiB	0	1.356921364	89.28	2	44.64
mp-1222413	LiB3	0.088	1.75619417	96.64	4	24.16
mp-20150	LiCa2Si3	0	2.202979398	95.4	6	15.9
mp-13916	LiCaSi2	0	2.129596173	91.35	4	22.84
mp-862658	LiCu3	0	6.929195303	103.6	4	25.9
mp-1094889	LiMg	0	1.294794498	87.92	2	43.96
mp-866755	LiMg149	0	1.744050353	431.28	150	2.88
mp-973374	LiMg2	0	1.425083488	90.24	3	30.08
mp-1934	LiZn	0	4.082778098	88.15	2	44.07
mp-975799	LiZn3	0	5.754870182	93.25	4	23.31
mp-1094122	Mg	0	1.774055192	2.32	1	2.32
mp-1185596	Mg149Al	0.5011	1.77253796	347.47	150	2.32
mp-1185586	Mg149Be	0.5261	1.77064398	1202.68	150	8.02
mp-1185585	Mg149Cr	0.0245	1.776729495	355.08	150	2.37
mp-1185592	Mg149Fe	0.0779	1.770594214	346.104	150	2.31
mp-1185597	Mg149Ga	0.4779	1.801585231	493.68	150	3.29
mp-1185594	Mg149In	0.5296	1.800697333	512.68	150	3.42
mp-1185627	Mg149Mn	0.1095	1.788015279	347.5	150	2.32
mp-1185565	Mg149Mo	0.1504	1.806320945	385.78	150	2.57
mp-1185589	Mg149Nb	0.1185	1.797014383	431.28	150	2.88
mp-1185599	Mg149Ni	0.0151	1.78373815	359.58	150	2.4
mp-1185570	Mg149Pb	0.383	1.857156336	347.68	150	2.32
mp-1185634	Mg149Si	0.3404	1.772682413	347.38	150	2.32
mp-1185637	Mg149Sn	0.4181	1.816857545	364.38	150	2.43
mp-1185639	Mg149Ti	0.2003	1.784807173	357.38	150	2.38
mp-1185635	Mg149Tl	0.4888	1.861349358	4545.68	150	30.3
mp-1185641	Mg149V	0.0807	1.783943552	730.68	150	4.87
mp-1185642	Mg149Zn	0.578	1.775146575	348.23	150	2.32
mp-1185655	Mg149Zr	0.0334	1.80072545	382.78	150	2.55
mp-2151	Mg17Al12	0	2.094692395	60.92	29	2.1
mp-2481	Mg2Cu	0	3.429623958	10.64	3	3.55
mp-30650	Mg2Ga	0	3.211673152	152.64	3	50.88
mp-2137	Mg2Ni	0	3.481329007	18.54	3	6.18
mp-1367	Mg2Si	0.2935	1.975370396	6.34	3	2.11
mp-1559	Mg3N2	1.5099	2.66192851	7.24	5	1.45
mp-680671	Mg4Zn7	0	4.902721695	27.13	11	2.47
mp-1770	Mg5Ga2	0	2.981947262	307.6	7	43.94
mp-1094116	MgAl2	0	2.294860205	5.9	3	1.97
mp-763	MgB2	0	2.637300884	9.68	3	3.23
mp-365	MgB4	0.365	2.504415512	17.04	5	3.41
mp-978275	MgB7	1.4635	2.618328347	28.08	8	3.51
mp-855	MgBe13	0	1.831684728	11143.32	14	795.95
mp-1038	MgCu2	0	5.816113247	14.32	3	4.77
mp-2675	MgNi2	0	6.032501485	30.12	3	10.04
mp-978269	MgZn2	0	5.080755055	7.42	3	2.47
mp-35	Mn	0	8.265241283	1.82	1	1.82
mp-542830	Mn23C6	0	7.843043604	42.592	29	1.47
mp-20318	Mn2B	0	7.609817023	7.32	3	2.44
mp-9981	Mn2N	0	6.987770318	3.78	3	1.26
mp-12659	Mn2Nb	0	8.479514449	89.24	3	29.75
mp-10118	Mn3B4	0	6.153079405	20.18	7	2.88
mp-20211	Mn3Si	0	7.078772648	7.16	4	1.79
mp-2856	Mn4Al11	0	4.068219269	26.97	15	1.8
mp-505622	Mn4N	0	7.329288096	7.42	5	1.48
mp-680339	Mn4Si7	0.8013	5.260600969	19.18	11	1.74
mp-21256	Mn7C3	0	7.858680097	13.106	10	1.31
mp-771	MnAl	0	5.127964867	3.61	2	1.81
mp-173	MnAl6	0	3.352783148	12.56	7	1.79
mp-1106184	MnB4	0	4.493457463	16.54	5	3.31
mp-1104792	MnBe12	0	2.58106982	10285.82	13	791.22
mp-11270	MnBe2	0	4.819797134	1715.82	3	571.94
mp-5529	MnFe2Si	0	7.393942888	4.368	4	1.09
mp-1221619	MnFeSi2	0	6.145428313	5.644	4	1.41
mp-1431	MnSi	0	5.972686451	3.52	2	1.76
mp-316	MnV	0	7.40626179	386.82	2	193.41
mp-864984	MnV3	0	6.851730115	1156.82	4	289.2
mp-129	Mo	0	10.02490812	40.1	1	40.1
mp-1552	Mo2C	0	8.943989697	80.322	3	26.77
mp-10172	Na	0	1.028520018	3.43	1	3.43
mp-21895	Na15Pb4	0	3.289669644	59.45	19	3.13
mp-30794	Na15Sn4	0	2.382357152	126.25	19	6.64
mp-31430	Na2In	0	2.931312327	173.86	3	57.95
mp-262	Na3B20	0	2.146002807	83.89	23	3.65
mp-28630	Na3BN2	1.6631	2.118291333	14.25	6	2.38
mp-983509	Na3Cd	0	2.461204784	13.02	4	3.26
mp-16839	Na3WN3	1.7694	4.43751207	46.01	7	6.57
mp-571095	Na7Ga13	0	4.12335022	1948.01	20	97.4
mp-541787	Na8Hg3	0	3.977038092	118.04	11	10.73
mp-27335	NaAlSi	0	2.069716943	6.92	3	2.31
mp-2315	NaB15	0	2.425916555	58.63	16	3.66
mp-1186271	NaMg149	0.5472	1.750188859	349.11	150	2.33
mp-75	Nb	0	8.427646884	85.6	1	85.6
mp-18427	Nb2Al	0	6.789453836	172.99	3	57.66
mp-1080021	Nb2B3	0	7.075689381	182.24	5	36.45
mp-569989	Nb2C	0	7.67375624	171.322	3	57.11
mp-1079585	Nb2N	0	8.022840826	171.34	3	57.11
mp-20689	Nb3B2	0	7.752632878	264.16	5	52.83
mp-10255	Nb3B4	0	7.190484651	271.52	7	38.79
mp-1326	Nb3Sn	0	8.694218122	275.5	4	68.87
mp-1192618	Nb4Fe4Si7	0	6.627655366	355.996	15	23.73
mp-13686	Nb5Si3	0	6.967600937	433.1	8	54.14
mp-2760	Nb6C5	0	7.503639379	514.21	11	46.75
mp-542995	Nb6Fe16Si7	0	7.716440808	532.284	29	18.35
mp-1842	NbAl3	0	4.501843514	90.97	4	22.74
mp-2580	NbB	0	7.429359441	89.28	2	44.64
mp-450	NbB2	0	6.793798027	92.96	3	30.99
mp-1221111	NbFe	0	8.52821509	86.024	2	43.01
mp-1192350	NbFe2	0	8.803120472	86.448	3	28.82
mp-1209887	NbFeSi	0	7.175613006	87.724	3	29.24
mp-1196167	NbFeSi2	0	6.407325461	89.424	4	22.36
mp-1220327	NbMo	0	9.231307465	125.7	2	62.85
mp-2634	NbN	0	7.984187333	85.74	2	42.87
mp-12104	NbSi2	0	5.577439821	89	3	29.67
mp-1220316	NbW	0	13.43138832	120.9	2	60.45
mp-123	Nd	0	6.758696201	57.5	1	57.5
mp-567415	Nd2B5	0	5.945180936	133.4	7	19.06
mp-1800	Nd2C3	0	6.738088162	115.366	5	23.07
mp-567735	Nd5Si3	0	6.280952658	292.6	8	36.58
mp-355	Nd5Si4	0	5.868754711	294.3	9	32.7
mp-1632	NdB4	0	5.768965554	72.22	5	14.44
mp-1929	NdB6	0	4.908783998	79.58	7	11.37
mp-13392	NdCu	0	7.323929471	63.5	2	31.75
mp-11852	NdCu2	0	7.992310976	69.5	3	23.17
mp-1140	NdCu5	0	8.263727547	87.5	6	14.58
mp-2599	NdN	0.4304	7.627429946	57.64	2	28.82
mp-9967	NdSi	0	5.927845124	59.2	2	29.6
mp-884	NdSi2	0	5.359050262	60.9	3	20.3
mp-23	Ni	0	9.047689544	13.9	1	13.9
mp-11506	Ni3Mo	0	9.512797164	81.8	4	20.45
mp-11507	Ni4Mo	0	9.438041633	95.7	5	19.14
mp-30811	Ni4W	0	11.89007194	90.9	5	18.18
mp-1179656	Rb	0	1.572308149	15500	1	15500
mp-568643	RbC8	0	2.448462356	15500.976	9	1722.33
mp-1187343	RbMg149	0.0213	1.764381967	15845.68	150	105.64
mp-67	Sc	0	3.023050896	3460	1	3460
mp-29941	Sc2C	0	3.118296979	6920.122	3	2306.71
mp-31348	Sc2In	0	4.870411778	7087	3	2362.33
mp-28733	Sc3C4	0	3.561973189	10380.488	7	1482.93
mp-27162	Sc3Co	0	3.959797526	10412.8	4	2603.2
mp-861910	Sc3Hg	0	6.095376435	10410.2	4	2602.55
mp-19713	Sc3In	0	4.443026391	10547	4	2636.75
mp-1186974	Sc3Tl	0	5.950770014	14580	4	3645
mp-15661	Sc4C3	0.4656	3.799358905	13840.366	7	1977.2
mp-7822	Sc5Si3	0	3.252082867	17305.1	8	2163.14
mp-17695	Sc5Sn3	0	5.104693989	17356.1	8	2169.51
mp-2252	ScB2	0	3.660544064	3467.36	3	1155.79
mp-2212	ScCo	0	5.682768497	3492.8	2	1746.4
mp-253	ScCo2	0	6.582231542	3525.6	3	1175.2
mp-1169	ScCu	0	5.222540494	3466	2	1733
mp-1018149	ScCu2	0	6.252104019	3472	3	1157.33
mp-11471	ScHg	0	9.281450893	3490.2	2	1745.1
mp-1207100	ScIn	0	5.84213774	3627	2	1813.5
mp-9969	ScSi	0	3.33611577	3461.7	2	1730.85
mp-27276	Si12Ni31	0	7.616395291	451.3	43	10.5
mp-2291	Si2Ni	0	4.724646143	17.3	3	5.77
mp-1620	Si2W	0	9.689780275	38.7	3	12.9
mp-569128	SiB3	1.4934	2.449973602	12.74	4	3.19
mp-568656	SiC	2.0411	3.171908241	1.822	2	0.91
mp-351	SiNi	0	5.981087135	15.6	2	7.8
mp-1118	SiNi2	0	7.347406647	29.5	3	9.83
mp-828	SiNi3	0	7.875710486	43.4	4	10.85
mp-86	Sm	0	7.336111094	13.9	1	13.9
mp-570421	Sm2B5	0	6.38117091	46.2	7	6.6
mp-1219177	Sm2C	0	6.96379353	27.922	3	9.31
mp-569335	Sm2C3	0	7.342820428	28.166	5	5.63
mp-1195872	Sm3Ga2	0	7.290128233	337.7	5	67.54
mp-1106373	Sm5Si3	0	6.518409369	74.6	8	9.32
mp-8546	SmB4	0	6.100418512	28.62	5	5.72
mp-6996	SmB6	0	5.111503219	35.98	7	5.14
mp-980769	SmCu	0	7.954064255	19.9	2	9.95
mp-1077154	SmCu2	0	8.113356985	25.9	3	8.63
mp-227	SmCu5	0	8.498335586	43.9	6	7.32
mp-477	SmGa2	0	7.243944997	309.9	3	103.3
mp-749	SmN	0.0215	8.356280164	14.04	2	7.02
mp-1025489	SmSi	0	6.372031659	15.6	2	7.8
mp-1187073	Sr	0	2.676562284	6.68	1	6.68
mp-705522	Sr28In11	0	3.772800964	2024.04	39	51.9
mp-1245	Sr2N	0	3.493077187	13.5	3	4.5
mp-1106	Sr2Si	0.3434	3.353462355	15.06	3	5.02
mp-978	Sr2Sn	0.1528	4.212174375	32.06	3	10.69
mp-542484	Sr5Cd3	0	4.068644836	41.59	8	5.2
mp-746	Sr5Si3	0	3.349595547	38.5	8	4.81
mp-17720	Sr5Sn3	0	4.296218632	89.5	8	11.19
mp-29136	Sr6Cu3N5	0.4905	4.691465073	58.78	14	4.2
mp-30782	Sr6Mg23	0	2.168974738	93.44	29	3.22
mp-242	SrB6	0.035	3.417060889	28.76	7	4.11
mp-2080	SrBe13	0	2.424044218	11147.68	14	796.26
mp-1208630	SrC6	0	3.270211156	7.412	7	1.06
mp-30496	SrCd	0	4.88492559	9.41	2	4.71
mp-677	SrCd2	0	5.749780183	12.14	3	4.05
mp-1025402	SrCu	0	4.000956388	12.68	2	6.34
mp-2726	SrCu5	0	6.972726344	36.68	6	6.11
mp-21609	SrCuN	0.2621	5.064433467	12.82	3	4.27
mp-608072	SrIn	0	4.661915979	173.68	2	86.84
mp-20074	SrIn2	0	5.762914419	340.68	3	113.56
mp-1187198	SrMg2	0	2.399508735	11.32	3	3.77
mp-29973	SrN	0	3.854517961	6.82	2	3.41
mp-10564	SrN2	0	4.089657496	6.96	3	2.32
mp-21524	SrNiN	0	5.041450539	20.72	3	6.91
mp-2661	SrSi	0	3.451941633	8.38	2	4.19
mp-1727	SrSi2	0	3.472602102	10.08	3	3.36
mp-1698	SrSn	0	4.849131237	25.38	2	12.69
mp-50	Ta	0	16.38780395	312	1	312
mp-1079438	Ta2N	0	15.39304112	624.14	3	208.05
mp-13415	Ta3B2	0	14.70362601	943.36	5	188.67
mp-10142	Ta3B4	0	13.28435248	950.72	7	135.82
mp-568646	Ta3Si	0	13.88613422	937.7	4	234.43
mp-1187206	Ta3W	0	17.11634231	971.3	4	242.82
mp-1989	Ta5Si3	0	12.7874257	1565.1	8	195.64
mp-1097	TaB	0	13.98092219	315.68	2	157.84
mp-1108	TaB2	0	12.11755213	319.36	3	106.45
mp-1279	TaN	0	13.99558899	312.14	2	156.07
mp-11192	TaSi2	0	8.940924456	315.4	3	105.13
mp-567276	TaV2	0	10.38566089	1082	3	360.67
mp-1217811	TaW	0	17.65981087	347.3	2	173.65
mp-979289	TaW3	0	18.29084553	417.9	4	104.47
mp-72	Ti	0	4.64683663	11.7	1	11.7
mp-1202079	Ti21Mn25	0	6.379828993	291.2	46	6.33
mp-10721	Ti2C	0	4.43976924	23.522	3	7.84
mp-1191331	Ti2Co	0	5.816331995	56.2	3	18.73
mp-742	Ti2Cu	0	5.722180363	29.4	3	9.8
mp-861983	Ti2MnFe	0	6.549536628	25.644	4	6.41
mp-8282	Ti2N	0	4.881545292	23.54	3	7.85
mp-1808	Ti2Ni	0	5.725014052	37.3	3	12.43
mp-30875	Ti2Sn	0.0452	6.451610675	42.1	3	14.03
mp-1014229	Ti2Zn	0	5.462441931	25.95	3	8.65
mp-1823	Ti3Al	0	4.248868625	36.89	4	9.22
mp-2643	Ti3Cu4	0	6.748300444	59.1	7	8.44
mp-1079460	Ti3Sn	0	6.048168578	53.8	4	13.45
mp-2108	Ti5Si3	0	4.347039406	63.6	8	7.95
mp-505527	Ti5Si4	0	4.254735425	65.3	9	7.26
mp-27919	Ti8C5	0	4.54143797	94.21	13	7.25
mp-1953	TiAl	0	3.833901613	13.49	2	6.74
mp-567705	TiAl2	0	3.536390592	15.28	3	5.09
mp-542915	TiAl3	0	3.3657055	17.07	4	4.27
mp-631	TiC	0	4.879907059	11.822	2	5.91
mp-823	TiCo	0	6.714495322	44.5	2	22.25
mp-608	TiCo3	0	7.948540457	110.1	4	27.52
mp-568636	TiCr2	0	6.234565538	30.5	3	10.17
mp-2078	TiCu	0	6.440936363	17.7	2	8.85
mp-12546	TiCu3	0	7.648117875	29.7	4	7.42
mp-1188441	TiCu4	0	7.89299659	35.7	5	7.14
mp-305	TiFe	0	6.642034602	12.124	2	6.06
mp-866141	TiFe2Si	0.4023	6.758127762	14.248	4	3.56
mp-8648	TiFeSi	0	5.624878094	13.824	3	4.61
mp-21662	TiFeSi2	0	5.143235694	15.524	4	3.88
mp-1949	TiMn2	0	6.901373985	15.34	3	5.11
mp-865652	TiMn2Si	0	6.352313333	17.04	4	4.26
mp-865656	TiMn2W	0	10.69468704	50.64	4	12.66
mp-21606	TiMnSi2	0	4.99815749	16.92	4	4.23
mp-492	TiN	0	5.340297483	11.84	2	5.92
mp-1048	TiNi	0	6.412985726	25.6	2	12.8
mp-1409	TiNi3	0	7.958129861	53.4	4	13.35
mp-7092	TiSi	0	4.22430874	13.4	2	6.7
mp-1077503	TiSi2	0	4.027104901	15.1	3	5.03
mp-1216621	TiW	0	11.85552569	47	2	23.5
mp-1014230	TiZn	0	6.036542638	14.25	2	7.12
mp-21289	TiZn3	0	6.697660442	19.35	4	4.84
mp-146	V	0	6.312904043	385	1	385
mp-9208	V2B3	0	5.360224268	781.04	5	156.21
mp-20648	V2C	0	5.741137786	770.122	3	256.71
mp-33090	V2N	0	6.096388132	770.14	3	256.71
mp-2091	V3B2	0	5.846064712	1162.36	5	232.47
mp-569270	V3B4	0	5.426880995	1169.72	7	167.1
mp-1585	V3Co	0	6.985026991	1187.8	4	296.95
mp-1187695	V3Cr	0	6.599355542	1164.4	4	291.1
mp-1079399	V3Fe	0	6.896938402	1155.424	4	288.86
mp-972071	V3Mo	0	7.371335048	1195.1	4	298.77
mp-7226	V3Ni	0	6.898754916	1168.9	4	292.23
mp-1216708	V3Ni2	0	7.272789251	1182.8	5	236.56
mp-30883	V4Zn5	0	6.973256469	1552.75	9	172.53
mp-1206441	V5B6	0	5.503664211	1947.08	11	177.01
mp-28731	V6C5	0	5.617822598	2310.61	11	210.06
mp-1188283	V8N	0	6.188837954	3080.14	9	342.24
mp-9973	VB	0	5.631694261	388.68	2	194.34
mp-1491	VB2	0	5.10857069	392.36	3	130.79
mp-542614	VCo3	0	8.706330003	483.4	4	120.85
mp-1216394	VCr	0	6.919500541	394.4	2	197.2
mp-1187696	VCr3	0	7.195388401	413.2	4	103.3
mp-866134	VFe3	0	7.739814966	386.272	4	96.57
mp-1018027	VN	0	6.23865029	385.14	2	192.57
mp-11531	VNi2	0	8.166036424	412.8	3	137.6
mp-171	VNi3	0	8.437749253	426.7	4	106.67
mp-91	W	0	18.85400756	35.3	1	35.3
mp-1894	WC	0	15.3503693	35.422	2	17.71
mp-1187739	Y	0	4.547349703	31	1	31
mp-1199133	Y11Sn10	0	6.16980642	528	21	25.14
mp-1200338	Y15Ni32	0	7.163935221	909.8	47	19.36
mp-1334	Y2C	0	4.535817916	62.122	3	20.71
mp-21294	Y2In	0	5.669659581	229	3	76.33
mp-574339	Y2Ni7	0	7.692491082	159.3	9	17.7
mp-1200613	Y3C4	0	4.91444971	93.488	7	13.36
mp-1105598	Y3Co	0	5.148898384	125.8	4	31.45
mp-1105835	Y3In5	0	6.657923024	928	8	116
mp-1105633	Y3Ni	0	5.094566393	106.9	4	26.73
mp-582134	Y3Ni2	0	5.562940279	120.8	5	24.16
mp-9459	Y4C5	0	4.729248328	124.61	9	13.85
mp-1200885	Y4C7	0.6144	4.541710694	124.854	11	11.35
mp-2538	Y5Si3	0	4.43624154	160.1	8	20.01
mp-567412	Y5Sn3	0	5.778885589	211.1	8	26.39
mp-1188434	Y5Tl3	0	7.379251429	12755	8	1594.38
mp-972364	Yb	0	7.00586663	17.1	1	17.1
mp-1542	YB2	0	5.045298476	38.36	3	12.79
mp-9546	Yb2C3	0	8.726729992	34.566	5	6.91
mp-1207599	Yb2Si	0.0437	7.742296269	35.9	3	11.97
mp-570050	Yb2Sn	0	8.771931394	52.9	3	17.63
mp-864675	Yb3N2	0.4892	10.30057431	51.58	5	10.32
mp-637	YB4	0	4.30848155	45.72	5	9.14
mp-1189298	YbB4	0	6.949843493	31.82	5	6.36
mp-419	YbB6	0.1059	5.614593733	39.18	7	5.6
mp-1103975	YbC6	0	5.687258796	17.832	7	2.55
mp-1857	YbCd	0	8.562931183	19.83	2	9.92
mp-1187653	YbCd3	0	8.670606633	25.29	4	6.32
mp-1193534	YBe13	0	2.590983849	11172	14	798
mp-864757	YbN2	0	8.32527653	17.38	3	5.79
mp-10651	YbSi	0	7.137531395	18.8	2	9.4
mp-1077404	YbSi2	0	6.315081244	20.5	3	6.83
mp-2806	YbSn	0	8.889744215	35.8	2	17.9
mp-865373	YCo	0	5.420377438	63.8	2	31.9
mp-1294	YCo2	0	7.581892784	96.6	3	32.2
mp-1080443	YCu	0	5.830094464	37	2	18.5
mp-2698	YCu2	0	6.706395025	43	3	14.33
mp-2797	YCu5	0	7.535186104	61	6	10.17
mp-2399	YHg	0	9.243619826	61.2	2	30.6
mp-22704	YIn	0	6.291688649	198	2	99
mp-20131	YIn3	0	7.135476219	532	4	133
mp-615	YMg	0	3.419333592	33.32	2	16.66
mp-1188082	YMg149	0.2723	1.786909137	376.68	150	2.51
mp-865376	YMg3	0	2.731203846	37.96	4	9.49
mp-2114	YN	0.2858	5.742757452	31.14	2	15.57
mp-1364	YNi	0	6.05878909	44.9	2	22.45
mp-569196	YNi3	0	7.60099949	72.7	4	18.18
mp-2152	YNi5	0	7.801971483	100.5	6	16.75
mp-9972	YSi	0	4.464025792	32.7	2	16.35
mp-11575	YTl	0	8.800691481	4231	2	2115.5
mp-1216020	Zn35Cu17	0	7.949086791	191.25	52	3.68
mp-1368	Zn8Cu5	0	8.049427048	50.4	13	3.88
mp-987	ZnCu	0	8.252022453	8.55	2	4.28
mp-131	Zr	0	6.4460921	37.1	1	37.1
mp-684623	Zr10C9	0	6.396416519	372.098	19	19.58
mp-1216441	Zr14Cu51	0	8.184391095	825.4	65	12.7
mp-2544	Zr2Bel7	0	3.115805578	14643.2	19	770.69
mp-1018104	Zr2Cd	0	7.235683329	76.93	3	25.64
mp-193	Zr2Cu	0	6.968518148	80.2	3	26.73
mp-1014265	Zr2N	0	6.644608678	74.34	3	24.78
mp-328	Zr2Ni	0	7.189329356	88.1	3	29.37
mp-2717	Zr2Ni7	0	8.441842565	171.5	9	19.06
mp-1278	Zr2Si	0	5.972090741	75.9	3	25.3
mp-31205	Zr3Fe	0	6.808804543	111.724	4	27.93
mp-277	Zr3N4	1.2736	6.143260208	111.86	7	15.98
mp-1207024	Zr3Si2	0	5.812221304	114.7	5	22.94
mp-977585	Zr3Tl	0	8.76301174	4311.3	4	1077.83
mp-1106020	Zr5SiSn3	0	7.175692279	243.3	9	27.03
mp-510522	Zr5Sn3	0	7.328539753	241.6	8	30.2
mp-543001	Zr5Sn4	0	7.607774398	260.3	9	28.92
mp-582924	Zr6Fe23	0	7.603506886	232.352	29	8.01
mp-1188077	Zr7Cu10	0	7.760947992	319.7	17	18.81
mp-1472	ZrB2	0	6.03310523	44.46	3	14.82
mp-30445	ZrBe13	0	2.771775575	11178.1	14	798.44
mp-11283	ZrBe5	0	3.623393534	4322.1	6	720.35
mp-2795	ZrC	0	6.50296405	37.222	2	18.61
mp-14208	LiYSi	0	3.416483679	118.3	3	39.43
mp-504790	LiYSn	0	5.088427374	135.3	3	45.1
mp-1934	LiZn	0	4.082778098	88.15	2	44.07
mp-867252	LiZn2Ni	0	6.431958586	104.6	4	26.15
mp-1185421	LiZnNi2	0	6.737390407	115.95	4	28.99
mp-1038	MgCu2	0	5.816113247	14.32	3	4.77
mp-2675	MgNi2	0	6.032501485	30.12	3	10.04
mp-35	Mn	0	8.265241283	1.82	1	1.82
mp-542830	Mn23C6	0	7.843043604	42.592	29	1.47
mp-20318	Mn2B	0	7.609817023	7.32	3	2.44
mp-864955	Mn2CrCo	0	7.716185888	45.84	4	11.46
mp-12659	Mn2Nb	0	8.479514449	89.24	3	29.75
mp-10118	Mn3B4	0	6.153079405	20.18	7	2.88
mp-1185970	Mn3Co	0	8.77177245	38.26	4	9.56
mp-20211	Mn3Si	0	7.078772648	7.16	4	1.79
mp-21256	Mn7C3	0	7.858680097	13.106	10	1.31
mp-771	MnAl	0	5.127964867	3.61	2	1.81
mp-5529	MnFe2Si	0	7.393942888	4.368	4	1.09
mp-11501	MnNi3	0	8.49819932	43.52	4	10.88
mp-316	MnV	0	7.40626179	386.82	2	193.41
mp-864953	MnV2Cr	0	7.151615215	781.22	4	195.31
mp-864984	MnV3	0	6.851730115	1156.82	4	289.2
mp-129	Mo	0	10.02490812	40.1	1	40.1
mp-10172	Na	0	1.028520018	3.43	1	3.43
mp-75	Nb	0	8.427646884	85.6	1	85.6
mp-1080021	Nb2B3	0	7.075689381	182.24	5	36.45
mp-1079585	Nb2N	0	8.022840826	171.34	3	57.11
mp-20689	Nb3B2	0	7.752632878	264.16	5	52.83
mp-10255	Nb3B4	0	7.190484651	271.52	7	38.79
mp-7250	Nb6Co7	0	8.885808577	743.2	13	57.17
mp-2580	NbB	0	7.429359441	89.28	2	44.64
mp-450	NbB2	0	6.793798027	92.96	3	30.99
mp-977426	NbCo3	0	9.188007818	184	4	46
mp-548	NbCr2	0	7.767773551	104.4	3	34.8
mp-1221111	NbFe	0	8.52821509	86.024	2	43.01
mp-1192350	NbFe2	0	8.803120472	86.448	3	28.82
mp-1220799	NbNi	0	8.842814701	99.5	2	49.75
mp-1451	NbNi3	0	8.950269576	127.3	4	31.82
mp-1220522	NbVCo	0	8.073557923	503.4	3	167.8
mp-1220374	NbVCr	0	7.38520832	480	3	160
mp-1220599	NbVNi	0	7.996372687	484.5	3	161.5
mp-1220316	NbW	0	13.43138832	120.9	2	60.45
mp-123	Nd	0	6.758696201	57.5	1	57.5
mp-567415	Nd2B5	0	5.945180936	133.4	7	19.06
mp-1800	Nd2C3	0	6.738088162	115.366	5	23.07
mp-356	Nd2Co17	0	8.660874962	672.6	19	35.4
mp-1084826	Nd2Co3	0	8.309643274	213.4	5	42.68
mp-1106011	Nd3Co	0	7.282343973	205.3	4	51.33

Claims

1. A mixed ionic-electronic conductor (MIEC) in contact with a solid electrolyte comprising: a material having a bandgap less than 3 eV, the material comprising an end-member phase directly connected to an alkali metal by a tie-line in an equilibrium phase diagram, and the material being thermodynamically stable with the solid electrolyte; anda plurality of open pores, formed within the MIEC, to facilitate motion of the alkali metal to at least one of store the alkali metal in the plurality of open pores or release the alkali metal from the plurality of open pores,wherein the solid electrolyte has an ionic conductivity to ions of the alkali metal greater than 1 mS cm−1, a thickness less than 100 μm, and comprises at least one of a ceramic or a polymer.

2. The MIEC of claim 1, wherein the material excludes any lanthanides.

3. The MIEC of claim 1, wherein the material excludes any rare earth metals.

4. The MIEC of claim 1, wherein: the solid electrolyte comprises the polymer; andthe polymer comprises at least one of a polyethylene, a polypropylene, a polyethylene oxide, a polyacetal, a polyolefin, a poly(alkylene oxide), a polymethacrylate, a polycarbonate, a polystyrene, a polyester, a polyamide, a polyimide, a polyamideimide, a polyarylate, a polyarylsulfone, a polyethersulfone, a polyphenylene sulfide, a polyvinyl chloride, a polysulfone, a polyimide, a polyetherimide, a polytetrafluoroethylene, a polyetherketone, a polyether etherketone, a polyether ketone, a polybenzoxazole, a polyphthalide, a polyanhydride, a polyvinyl ether, a polyvinyl thioether, a polyvinyl alcohol, a polyvinyl ketone, a polyvinyl halide, a polyvinyl nitrile, a polyvinyl ester, a polysulfonate, a polysulfide, a polythioester, a polysulfone, a polysulfonamide, a polyurea, a polyphosphazene, a polysilazane, a polyethylene terephthalate, a polybutylene terephthalate, a polyurethane, an ethylene propylene diene rubber, a polytetrafluoroethylene, a fluorinated ethylene propylene, a perfluoroalkoxyethylene, a polychlorotrifluoroethylene, or a polyvinylidene fluoride.

5. The MIEC of claim 1, wherein: the solid electrolyte comprises the ceramic; andthe ceramic comprises at least one of: Li7La3Zr2O12;Li3OX wherein X is at least one of Cl, Br, or I;Li3SX wherein X is at least one of Cl, Br, or I;Li1.3Al0.3Ti1.7(PO4)3;Li6PS5Cl;Li10MP2S12 wherein M is at least one of Ge, Si, or Sn;Li3PS4;Li7P3S11;Li3N;Li2S;LiBH4;Li3BO3;Li2S—P2S5;Li2S—P2S5-L4SiO4;Li2S—Ga2S3—GeS2;Li2S—Sb2S3—GeS2;Li3.25—Ge0.25—P0.75S4;(La1−xLix)TiO3 wherein 0<x<1;Li6La2CaTa2O12;Li6La2ANb2O12 wherein A is at least one of Ca, Sr, or Ba;Li6La3Zr1.5WO12;Li6.5La3Zr1.5TaO12;Li6.625Al0.25La3Zr2O12;Li3BO2.5N0.5;Li9SiAlO8;Li1+xAlxGe2−x(PO4)3;Li1+xAlxTi2−x(PO4)3;Li1+xTi2−xAlxSiy(PO4)3−y wherein 0<x<1 and 0≤y<1;LiAlxZr2−x(PO4)3;LiTixZr2−x(PO4)3 wherein 0<x<2;Li6PS5X, wherein X is at least one of Cl, Br, or I;Li2InxSc0.666−xCl4 wherein 0≤x≤0.666; orLi3−xE1−xZrxCl6 wherein E is at least one of Y or Er.

6. An anode comprising: the mixed ionic-electronic conductor (MIEC) of claim 1,wherein the MIEC does not reversibly store and release the alkali metal.

7. The anode of claim 6, wherein: the MIEC has a thickness of about 0.5 μm to about 67 μm;the MIEC has a porosity greater than 45%; andthe anode has an areal capacity of about 6±0.5 mAh cm−2.

8. The anode of claim 6, further comprising the alkali metal.

9. A battery comprising: the anode of claim 6; andthe solid electrolyte.

10. An anode comprising a mixed ionic-electronic conductor (MIEC), the MIEC comprising: at least one of AxBy, AxByCz, or AxByCzDw; anda plurality of open pores, formed within the MIEC, to facilitate motion of an alkali metal to at least one of store the alkali metal in the plurality of open pores or release the alkali metal from the plurality of open pores,wherein: the MIEC does not reversibly store and release the alkali metal;the at least one of AxBy, AxByCz, or AxByCzDw comprises an end-member phase directly connected to an alkali metal by a tie-line in an equilibrium phase diagram;A is the alkali metal;at least one of B, C, or D is at least one of an alkaline earth metal, a group 13 element, Sc, Y, Ti, Zr, Hf, V, Nb, Ta, Cr, Mo, W, Mn, Fe, Co, Ni, Cu, Zn, Cd, Hg, C, N, Si, Sn, Pb, Bi, La, Ce, Nd, Sm, Eu, Gd, Ho, Er, or Yb; andx, y, z, and w each have a value of about 1 to about 149.

11. The anode claim 10, wherein B, C, and D are each at least one of an alkaline earth metal, a group 13 element, Sc, Y, Ti, Zr, Hf, V, Nb, Ta, Cr, Mo, W, Mn, Fe, Co, Ni, Cu, Zn, Cd, Hg, C, N, Si, Sn, Pb, Bi, La, Ce, Nd, Sm, Eu, Gd, Ho, Er, or Yb.

12. The anode of claim 10, wherein B is an alkaline earth metal.

13. The anode of claim 10, wherein B is a group 13 element.

14. The anode of claim 10, wherein B is a period 4 transition metal.

15. The anode of claim 10, wherein B is a period 5 transition metal.

16. The anode of claim 10, wherein B is a period 6 transition metal.

17. The anode of claim 10, wherein B is a lanthanide.

18. The anode of claim 10, wherein the alkali metal comprises at least one of lithium (Li), sodium (Na), or potassium (K).

19. An anode, comprising: a mixed ionic-electronic conductor (MIEC) comprising TiwAlxCyNiz; anda plurality of open pores, formed within the MIEC, to facilitate motion of an alkali metal to at least one of store the alkali metal in the plurality of open pores or release the alkali metal from the plurality of open pores,wherein x, y, z, and w each have a value less than or equal to 8.

20. A battery comprising: the anode of claim 19; anda solid electrolyte, coupled to a portion of the MIEC, the solid electrolyte comprising polyethylene oxide (PEO).