Not Applicable
Not Applicable
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A logic gate is an arrangement of electronically controlled switches used to proceed calculations in Boolean algebra. Logic gates can be constructed from relays, diodes, transistors and other elements. The logic gates constructed from the metal-oxide-semiconductor (MOS) transistors represent basic components of digital integrated circuits (ICs). The MOS logic gates are programmable and can perform different logic functions such as NOT, AND, OR, NAND, NOR and others.
Alternatively, a magnetic tunnel junction (MTJ) is a nonvolatile reversible resistance element (RRE) employing a giant magneto-resistance (GMR) effect observed in a multilayer structure composed by at least two ferromagnetic layers separated by a thing oxide layer. When magnetizations of the ferromagnetic layers are parallel to each other, a tunneling resistance RP of the MTJ is low and is referred to as a logic state “0”. When the magnetizations of the ferromagnetic layers are anti-parallel, the resistance RAP of the MTJ is high and is referred to as a logic state “1”. In the MTJ one ferromagnetic layer, called a pinned or reference layer, has a fixed direction of the magnetization. The direction of the magnetization in the other layer that is called as a free or storage layer can be reversed from parallel to anti-parallel relatively to the direction of the magnetization in the pinned layer by applying an appropriate magnetic field or by running a spin polarized current through the MTJ in a direction perpendicular to a plane of the junction. The logic states “0” or “1” can be determined by comparing the resistance of the MTJ with a known reference resistance. The MTJ is a nonvolatile device. It doesn't lose its logic state when the power is off.
For example, the CMOS inverter requires that a source terminal of the p-channel pT and n-channel nT transistors be connected to the high voltage source (VDD) and to the low voltage source (VSS), respectively. The opposite polarity of the voltage sources is not desirable since it leads to a substantial increase of power consumption by the inverter due to a power leakage in the transistors. Moreover the opposite polarity of the voltage sources might cause a substantial reduction of a saturation current of the transistors nT and pT. This obstacle might limit a possibility of the magnetization reversal in the MTJ 22 of the nonvolatile inverter 20 hence it might prevent the MTJ from memorizing the logic state of the inverter.
In accordance with one embodiment a nonvolatile logic circuit comprises: an output terminal, a high voltage source, a low voltage source, an intermediate voltage source, a pull-up circuit comprising at least one source terminal, at least one drain terminal, and at least one gate terminal, the at least one source terminal is coupled to the high voltage source and the at least one drain terminal is coupled to the output terminal; a pull-down circuit comprising at least one source terminal, at least one drain terminal, and at least one gate terminal, wherein the at least one source terminal of the pull-down circuit is coupled to the low voltage source and the at least one drain terminal of the pull-down circuit is coupled to the output terminal; at least one input terminal coupled to the at least one gate terminal of the pull-up circuit and to the at least one gate terminal of the pull-down circuit; and a nonvolatile reversible resistance element comprising a high resistance state and a low resistance state, the reversible resistance element is coupled to the output terminal at a first end and to the intermediate voltage source at a second end, wherein an electrical potential of the intermediate voltage source is higher than the electrical potential of the low voltage source but lower than the electrical potential of the high voltage source. The resistance state of the reversible resistance element is controlled by an input signal applied to the at least one input terminal. The reversible resistance element is a transition metal oxide element or a chalcogenide element.
In accordance with another embodiment a method for preserving a logic state of a nonvolatile logic circuit comprises: providing a logic circuit comprising, a first source terminal, a second source terminal, at least one input terminal, and an output terminal to temporarily store the logic state with a power dependent status; providing a high voltage source coupled to the first source terminal, providing a low voltage source coupled to the second source terminal, providing an intermediate voltage source comprising an electrical potential higher than that of the low voltage source but lower than that of the high voltage source, providing a nonvolatile reversible resistance element comprising a low resistance state and a high resistance state, the reversible resistance element is coupled to the output terminal at a first end and to the intermediate voltage source at a second end; and providing an input signal applied to the at least one input terminal, whereby preserving the logic state of the logic circuit by the nonvolatile reversible resistance element. The nonvolatile reversible resistance element is a chalcogenide element or a transition metal oxide element.
In accordance with yet another embodiment a nonvolatile logic circuit comprises: at least one input terminal, an output terminal, a high voltage source, a low voltage source, an intermediate voltage source comprising an electrical potential higher than that of the low voltage source but lower than that of the high voltage source, at least one p-channel transistor comprising a source terminal, a drain terminal, and a gate terminal, the source terminal is coupled to the high voltage source, the drain terminal is coupled to the output terminal, and the gate terminal is coupled to the at least one input terminal; at least one n-channel transistor comprising a source terminal, a drain terminal, and a gate terminal, the source terminal of the at least one n-channel transistor is coupled to the low voltage source, the drain terminal of the at least one n-channel transistor is coupled to the output terminal, and the gate terminal of the at least one n-channel transistor is coupled to the at least one input terminal; and a nonvolatile reversible resistance element comprising a low resistance state, a high resistance state, a first end, and a second end, the reversible resistance element is electrically coupled to the output terminal at the first end and to the intermediate voltage source at the second end, wherein the resistance state of the nonvolatile reversible resistance element is controlled by an input signal applied to the at least one input terminal. The reversible resistance element is a transition metal oxide element or a chalcogenide element.
These and other aspects and embodiments, their variations and modifications are described in greater detail in the drawings, detailed description, and claims.
In the following drawings closely related figures have the same number but different alphabetic suffixes.
The nonvolatile MTJ 22A comprises at least a free (or storage) layer 31, a pinned (or reference) layer 33, and a tunnel barrier layer 35 disposed between the ferromagnetic layers 31 and 33. In the first embodiment shown in
The p-channel transistor pT requires an n-type body region, so an n-well 53 is formed in the p-substrate 51. The pT transistor has a complimentary structure to that of the nT transistor with p+-type source 62 and drain 64 regions, and the gate terminal 46. The gate terminals 36 and 46 of the nT and pT transistors, respectively, are connected in common and to the input terminal 16. The p+-source region 62 of the pT transistor is connected to the high voltage source 14 by means of the source terminal 42 and a contact 56C. The p+-drain region 64 of the transistor pT is connected to the n+-drain region 54 of the transistor nT by means of the drain terminals 44 and 34, and the contact 56B. Moreover, the n+-drain and p+-drain regions of the transistors nT and pT are connected to the MTJ 22A, and to the output terminal 18. The MTJ 22A comprises at least the pinned layer 33 adjacent the contact 56B, the free layer 31 adjacent a contact 58, and the tunnel barrier layer 35 disposed between the ferromagnetic layers 33 and 31. The free layer 31 is connected to the voltage source 38 by means of the contact 58. A structure of the MTJ 22A is simplified for exemplary purpose and may comprise several additional layers for providing a required performance.
There is wide latitude for the choice of materials and their thicknesses within various embodiments. The free ferromagnetic layer 31 may have a thickness of about 0.5 nm-3 nm. The free layer 31 can be made of ferromagnetic materials such as Fe, Co, Ni, CoFe, CoFeB, NiFe and/or similar, their based alloys and/or laminates. It should be appreciated that the free layer 31 may comprise various ferromagnetic materials with a substantial spin polarization and can vary dimensionally, including length, width and thickness depending on implementation and desirable magnetic, electrical and other characteristics without departing from the scope of the present application.
The pinned ferromagnetic layer 33 may have a thickness of about 0.5 nm-30 nm. The pinned layer 33 may comprise the ferromagnetic materials such as Fe, Co, Ni, CoFe, CoFeB, NiFe and/or similar, their based alloys and/or laminates. It should be appreciated that the pinned layer 33 may comprise various ferromagnetic materials with a substantial spin polarization and can vary dimensionally, including length, width and thickness depending on implementation and desirable magnetic, electrical and other characteristics without departing from the scope of the present application.
The tunnel barrier layer 35 may comprise an electrically insulating material such as, for example, Al2O3, MgOX, TiOX, Ta2O5, ZrOX, HfOX, Mg/MgO or similar, and their based laminates. The tunnel barrier layer 35 may have a thickness of about 0.5 nm-2 nm. It should be appreciated that the tunnel barrier layer 35 may vary dimensionally, including length, width and thickness depending on implementation and desirable electrical and other characteristics without departing from the scope of the present application.
The layers of the MTJ 22A can be made in a manner generally know in the art by deposition techniques (vacuum deposition, sputter deposition, ion-beam deposition and others), photolithography, etching, thermal treatment and other techniques used in a semiconductor and spintronics technologies. During formation of the tunnel barrier layer 35 an oxidation technique (plasma oxidation, oxidation by air or/and similar) may be used.
The terminals 32, 34, 42, 44 and the contacts 56A-56C, 58 can be made of a substantial metallic substance such as Al, AlCu, Cu, Ta/Au/Ta and/or similar materials, and/or their based laminates. The gate terminals 36 and 46 may be made of poly-Si, Al, AlCu and/or other similar materials and/or their based laminates. The terminals and contacts can be made using conventional MOS techniques.
When a logic “1” appears at the input terminal 16 (A=1) of the logic circuit 60 (
The logic circuits shown in
The perpendicular MTJs 22C and 22D can have a substantially higher thermal stability than that of the in-plane MTJs with comparable dimensions due to a substantial intrinsic crystalline anisotropy of the perpendicular ferromagnetic materials. Moreover, the perpendicular MTJs 22C and 22D can have any shape including a round that is not possible in many cases for the in-plane MTJs 22A and 22B, which frequently have to use an elliptical shape. Necessity to use the elliptical shape of MTJ results from the rather week intrinsic crystalline anisotropy of the in-plane ferromagnetic materials.
The free layer 31C may have a thickness of about 0.5 nm-3 nm. The free layer 31C can comprise ferromagnetic materials such as Fe, Co, Ni, CoFe, CoFeB, NiFe, FePt, Co/Pt, Co/Pd, CoFe/Pt, Fe/Pt, Ni/Cu and/or similar, their based alloys and/or laminates. It should be appreciated that the free layer 31C may comprise various ferromagnetic materials with a substantial spin polarization and perpendicular anisotropy or out-of plane direction of the magnetization. The free layer 31C can vary dimensionally, including length, width and thickness depending on implementation and desirable magnetic, electrical and other characteristics without departing from the scope of the present application.
The pinned layer 33C may have a thickness of about 0.5 nm-30 nm. The pinned layer 33C my comprise ferromagnetic materials such as Fe, Co, Ni, CoFePt, CoPtTa, FePt, Co/Pt, Co/Pd, CoFe/Pt, CoFeB/Pt, Ni/Cu and/or similar, their based alloys and/or laminates. It should be appreciated that the pinned layer 33C may comprise various ferromagnetic materials with a substantial spin polarization and perpendicular anisotropy or out-of plane direction of the magnetization. The pinned layer 33C can vary dimensionally, including length, width and thickness depending on implementation and desirable magnetic, electrical and other characteristics without departing from the scope of the present application.
If either input signal A or B is equal to a logic “0”, at least one of the n-channel transistors nTA or nTB will be OFF, breaking a current flow from the source VM to the source VSS through the MTJ 22A. However at least one of the p-channel transistors pTA or pTB will be ON, creating a path for current from the voltage source VDD to the voltage source VM through the MTJ 22A. Hence the mutual direction of the magnetizations (shown by arrows) in the free 31 and pinned 33 layers of the MTJ 22A will be antiparallel. It corresponds to a high resistance RAP of the MTJ 22A or to a logic “1” of the output signal Y.
If both input signals are equal to a logic “1” (A=B=1), both n-channel transistors nTA and nTB will be ON and both p-channel transistors pTA and pTB will be OFF. Hence the current will flow from the intermediate voltage source VM to the low voltage source VSS through the MTJ 22A and the transistors nTA and nTB. This direction of the current will produce a parallel direction of the magnetizations (shown by arrows) in the free 31 and pinned 33 layers. The parallel orientation of the magnetizations results in a low resistance Rp of the MTJ 22A that corresponds to a logic “0” of the output signal Y. A truth table of the logic circuit 80 is given in Table 3.
N-input nonvolatile logic circuit performing NAND logic function can be composed by using N n-channel transistors connected in series to each other, N p-channel transistors connected in parallel to each other, and at least one MTJ, connected to the output terminal of the logic circuit. The series n-channel transistors are disposed between the output terminal and the low voltage source VSS. The parallel p-channel transistors are disposed between the high voltage source VDD and the output terminal. The MTJ is positioned between the intermediate voltage source VM and the output terminal, wherein the pinned layer of the MTJ is disposed adjacent the output terminal and the free layer is disposed adjacent the intermediate voltage source VM. A gate terminal of one of the n-channel transistors is connected in common with a gate terminal of one of the p-channel transistors, and both are connected to one of the N-input terminals of the logic circuit.
pTA and pTB connected in series, and a MTJ 22A. Source terminals 32A and 32B of the n-channel transistors nTA and nTB, respectively, are connected to a low voltage source 12 (VSS). Drain terminals 34A and 34B of the n-channel transistors pTA and pTB, respectively, are connected simultaneously to an output terminal 18, to a drain terminal 44B of the p-channel transistor pTB, and to the MTJ 22A at its first end. A source terminal 42A of the transistor pTA is connected to a high voltage source 14 (VDD). Gate terminals 36A and 46A of the nTA and pTA transistors, respectively, are connected in common and to an input terminal 16A. Similarly the gate terminals 36B and 46B of the transistors nTB and pTB are connected in common and to the input terminal 16B. A second end of the MTJ 22A is electrically connected to an intermediate voltage source 38 (VM) having a free layer 31 disposed adjacent the second end.
If either one or both input signals A or B are equal to a logic “1” (
The output signal Y=1 will occur when the input signals A=B=0 appear. Both p-channel transistors pTA and pTB will be ON but the n-channel transistors nTA and nTB will be OFF. The current will flow from the high voltage source VDD to the intermediate source VM through MTJ 22A and both the p-channel transistors pTA and pTB. This direction of the write current causes the antiparallel orientation of the magnetizations in the free 31 and pinned 33 layers corresponding to a high resistance RAP of the MTJ 22A or to a logic “1” at the output (Y=1). A truth table of the logic circuit 100 is given in Table 5.
NOR nonvolatile logic circuit (
In general, each of the logic circuits 30, 60, 80-110 disclosed above is realized by using two complementary MOS (CMOS) circuits, a nMOS pull-down circuit comprising at least one n-channel transistor to connect the output terminal 18 to a low voltage source 12 (VSS), a pMOS pull-up circuit comprising at least one p-channel transistor to connect the output terminal 18 to a high voltage source 14 (VDD), and a MTJ 22 to store the output signal Y. The MTJ 22 is connected to the output terminal 18 at its first end and to an intermediate voltage source 38 (VM) at its second end. The pull-down and pull-up circuits are arranged such that one is ON and the other is OFF for any input pattern.
A generic block diagram of a nonvolatile logic circuit 120 with N input terminals 16B, 16B, . . . , and 16N is shown in
Various nonvolatile reversible resistance elements (RRE) can be used instead of the MTJs 22A-22D in the present embodiments. For example, the MTJ can be replaced by a RRE that is used in a resistive random access memory (RRAM or ReRAM), in a phase-change random access memory (PRAM or PCRAM), in a conductive bridging random access memory (CBRAM), or by other similar device. In the present embodiments the MTJs are shown for exemplarily purpose.
The storage layer 156 can be made of transition metal oxides such as perovskite-like metal oxides or binary metal oxides. The perovskite-like metal oxides can include Pr0.7Ca0.3MnO3, SrTiO3, NbSrTiO3, NbSrZrO3 CrSrZrO3, CrSrTiO3 and/or similar materials. The binary metal oxides can include NixOy, TixOy, CuxOy, TixOy, Oy, ZrxOy, HfxOy, TaxOy, WxOy, FexOy, CoxOy, ZnxOy and/or similar materials. The first and second electrodes can be made of materials consisting of a group that includes but is not limited to Ti, Ni, Cu, Ru, Pd, Ag, W, Ir, Pt, Au, Al, their based alloys and multilayers.
The resistance of the storage layer 166 depends on a crystal structure of the layer. The resistance is low when the layer 166 has a polycrystalline structure (logic “0”), and the resistance is high when the layer 166 has an amorphous structure (logic “1”). The crystal structure of the storage layer 166 can be controlled by a magnitude and duration of a current pulse applied to the storage layer 166, such that the storage layer can have a polycrystalline or amorphous structure. The magnitude and duration of the write current can be controlled by the CMOS logic circuit providing different values of the current magnitudes and durations during ON state of the pull-up and pull-down circuits.
The storage layer 166 can be made of a phase-change material, which can be set into a polycrystalline or amorphous state by a heat generated during writing. The material of the storage layer 166 can include a chalcogenide material such as GeSbTe, InSbTe, AgInSbTe, GeSnTe, GeSb, GeTe, AgSbSe, SbSe, SbTe, InSe, TeAsSiGe and similar.
The heater layer 168 has a direct contact with the storage layer 166. An area of the heater layer 168 can be smaller than the area of the storage layer 166. It allows to reduce a write current and a size of an active area in the storage layer 166. The heater layer 168 can be made from a conductive material selected from a group consisting of TiN, TiAlN, TiBN, TiSiN, TiW, Ti, TaN, TaAlN, TaBN, TaSiN, Ta, WN, WAlN, WBN, WSiN, ZrN, ZrAlN, ZrBN, ZrSiN, MoN, Mo, Al, Cu, AlCu, AlCuSi, WSi and similar. Moreover, the heater layer 168 may be made of the same material as the first electrode 152.
The material of the first electrode 152 and the second electrode 154 can include a metal having a high melting point such as Ta, Mo, W, Ti and similar.
While the specification of this application contains many specifics, these should not be construed as limitations on the scope of the application or of what may be claimed, but rather as descriptions of features specific to particular embodiments. Certain features that are described in this specification in the context of separate embodiments can also be implemented in combination in a single embodiment. Conversely, various features that are described in the context of a single embodiment can also be implemented in multiple embodiments separately or in any suitable sub-combination. Moreover, although features may be described above as acting in certain combinations and even initially claimed as such, one or more features from a claimed combination can in some cases be excised from the combination, and the claimed combination may be directed to a sub-combination or variation of a sub-combination.
It is understood that the above application is intended to be illustrative, and not restrictive. Many other embodiments will be apparent to those of skill in the art upon reviewing the above description. The scope of the embodiments should be, therefore, determined with reference to the appended claims, along with the full scope of equivalents to which such claims are entitled.
This application is a continuation-in-part of U.S. patent application Ser. No. 13/283,465, filed on Oct. 27, 2011 and claims the benefit of U.S. provisional patent application No. 61/408,550, filed on Oct. 29, 2010 by the present inventor.