A magnetic random access memory (MRAM) offers comparable performance to volatile static random access memory (SRAM) and comparable density with lower power consumption to volatile dynamic random access memory (DRAM). Compared to non-volatile memory (NVM) flash memory, an MRAM offers much faster access times and suffers minimal degradation over time, whereas a flash memory can only be rewritten a limited number of times. One type of an MRAM is a spin transfer torque magnetic random access memory (STT-MRAM). An STT-MRAM utilizes a magnetic tunneling junction (MTJ) written at least in part by a current driven through the MTJ. Another type of an MRAM is a spin orbit torque (SOT) MRAM (SOT-MRAM), which generally requires a lower switching current than an STT-MRAM.
Aspects of the present disclosure are best understood from the following detailed description when read with the accompanying Figures. It is noted that, in accordance with the standard practice in the industry, various features are not drawn to scale. In fact, the dimensions of the various features may be arbitrarily increased or reduced for clarity of discussion.
The following disclosure provides many different embodiments, or examples, for implementing different features of the invention. Specific examples of components and arrangements are described below to simplify the present disclosure. These are, of course, merely examples and are not intended to be limiting. For example, the formation of a first feature over or on a second feature in the description that follows may include embodiments in which the first and second features are formed in direct contact, and may also include embodiments in which additional features may be formed between the first and second features, such that the first and second features may not be in direct contact. In addition, the present disclosure may repeat reference numerals and/or letters in the various examples. This repetition is for the purpose of simplicity and clarity and does not in itself dictate a relationship between the various embodiments and/or configurations discussed.
Further, spatially relative terms, such as “beneath,” “below,” “lower,” “above,” “upper” and the like, may be used herein for ease of description to describe one element or feature's relationship to another element(s) or feature(s) as illustrated in the Figures. The spatially relative terms are intended to encompass different orientations of the device in use or operation in addition to the orientation depicted in the Figures. The apparatus may be otherwise oriented (rotated 90 degrees or at other orientations) and the spatially relative descriptors used herein may likewise be interpreted accordingly. In addition, the term “made of” may mean either “comprising” or “consisting of.” Further, in the following fabrication process, there may be one or more additional operations in/between the described operations, and the order of operations may be changed. In the present disclosure, a phrase “one of A, B and C” means “A, B and/or C” (A, B, C, A and B, A and C, B and C, or A, B and C), and does not mean one element from A, one element from B and one element from C, unless otherwise described. Materials, configurations, dimensions, processes, and/or operations described with respect to one embodiment may be employed in the other embodiments, and detailed explanation thereof may be omitted.
In an SOT-MRAM, the magnetic moment of the free magnetic layer of an MTJ film stack is switched using the spin-orbit interaction effect generated by a current flowing adjacent to the free magnetic layer of the MTJ film stack. This current can flow in a SOT induction structure. Manipulating the free magnetic layer orientation causes a resistance change of the MTJ film stack, which may be used to record a data value in the cell. The magnetic moment of the free magnetic layer may be switched spin-orbit torque only or with assistant magnetic field. There are three general types of SOT-MRAM, which depend on the orientation relationship between the magnetization of free magnetic layer and the write current flowing through the SOT induction structure. An x-type of SOT-MRAM has a free magnetic layer moment which is parallel to the current through the SOT induction structure and an assistant magnetic field which is orthogonal to the plane of the current flow in the SOT induction structure. A y-type of SOT-MRAM has a free magnetic layer moment which is perpendicular to, but in the same plane as, the direction of the current through the SOT induction structure. A z-type of SOT-MRAM has a free magnetic layer moment which is orthogonal to the plane of the current flow through the SOT induction structure and an assistant magnetic field is needed which is parallel to the current flow.
Although the present disclosure generally relates to an x-type of SOT-MRAM, some of the aspects discussed herein may be transferrable to the other types of SOT-MRAM devices, such as will be discussed below. In x-type of SOT-MRAM devices, the assistant magnetic field to switch the free magnetic layer may be generated externally to the cell, thereby complicating the cell structure. Embodiments of the present disclosure improve performance in several ways.
The SOT induction structure 10 may be formed over an optional bottom electrode 5 and/or optional buffer layer 7. The bottom electrode 5 may include one or more layers of Cu, W, Ta, TiN, TaN, Ru, Au, and Al. In some embodiments, the buffer layer 7 may function as a structural isolation layer for the SOT induction structure 10 above, i.e., to separate the structure of the bottom electrodes 5 from the structure of the SOT induction structure 10. In some embodiments, the buffer layer 7 may also function as a seed layer for the SOT induction structure 10. In some embodiments, the buffer layer 7 may include a thinly deposited insulating material layer with tunneling capability, such as MgO deposited to a thickness between 2 Å and 9 Å.
The SOT induction structure 10 may be a metal doped with at least one dopant, i.e., the SOT induction structure 10 may include a metal and the at least one dopant. With the aid of dopant, it can assist the metal to maintain the desired phase, therefore, the thickness and spin-hall angle (SHA) of SOT induction structure 10 may be increased, the resistivity may be decreased, while the good thermal stability of magnetic memory device MC1 may be maintained (data as shown in Table 1). In some embodiments, the thickness of the SOT induction structure 10 may be greater than or equal to 5 nm, and the spin-hall angle (SHA) of the SOT induction structure 10 may be greater than 0.4. In some embodiments, since the thickness may be increased, the MTJ etching recess window can be improved to decrease probability of occurrence of short or other electrical issue, but not limited to.
In some embodiments, the SOT induction structure 10 may be a doped W (doped tungsten), and the doped W may include Co, Ru, Pt, CoFeB (CFB), Ta, MgO, or combinations thereof, i.e., the SOT induction structure 10 may include a metal (W) and the at least one dopant (Co, Ru, Pt, CoFeB, Ta, MgO, or combinations thereof). For example, the at least one dopant may include hall metal, magnetic material, insulator, or combinations thereof, the hall metal may include Pt and/or Ta, the magnetic material may include Co and/or CoFeB, and the insulator may include MgO, therefore, the at least one dopant can hold up transformation from β-W to α-W, and the desired phase (β-W) is maintained.
In some embodiments, α-W is the undesired phase, β-W is a metastable structure between amorphous-W and α-W, the dopant may break the α-W texture formation, and may have different crystal structure to slow down or inhibit transformation to α-W, i.e., the desired phase (β-W) may be maintained. In some embodiments, amorphous structure (such as CoFeB), HCP structure (such as Co, Ru) and/or FCC structure (such as Pt) materials are stabilized in β-W phase due to lattice mismatch with α-W (BCC structure). In some embodiments, conductive materials (such as Co, Ru, Pt) may reduce the resistivity of doped W.
In some embodiments, the SOT induction structure 10 is not a stacked structure, the SOT induction structure 10 may not include multiple layers, therefore, there is substantially no interface in the SOT induction structure 10, and the SOT induction structure 10 may be a doping state. In some embodiments, different to alloy, a percent of the at least one dopant may be less than 10% of the SOT induction structure 10 to ensure that the metal (W) maintains the original material property, but not limited to. In some embodiments, low concentration of Co and/or low concentration of CoFeB can boost SHA without too much enhancement in resistivity.
With reference to
With reference to
The spacer layer 20 may be formed from a metal material or a dielectric material, such as a metal oxide. Where the spacer layer 20 is formed from a metal material, the spacer layer 20 may be formed of a metal material such as a non-ferromagnetic metal material such as W, Ru, Pt, Mo, Ti, Mg, the like, or combinations thereof. Where the spacer layer 20 may be formed of a dielectric material such as magnesium oxide (MgOx), cobalt oxide (CoOx), aluminum oxide (AlOx), the like, or combinations thereof. In some embodiments, the spacer layer 20 may be formed from multiple layers which each may be a different material, including a metal material and/or a dielectric material. In some embodiments, the spacer layer 20A may be formed and patterned in conjunction with the SOT induction structure 10 and may have a similar foot print as the SOT induction structure 10. In some embodiments, the spacer layer 20B may be patterned when the MTJ film stack 100 is patterned such that the spacer layer 20B may have a similar foot print as the MTJ film stack 100. In some embodiments, both the spacer layer 20A and the spacer layer 20B may be present. In some embodiments, the spacer layer 20 may be omitted.
The total thickness of the spacer layer 20 (including spacer layer 20A and spacer layer 20B) depends on the materials of the free layer 30 and the SOT induction structure 10. Depending on the materials selected for the spacer layer 20, the free layer 30, and the SOT induction structure 10, the spacer layer 20 may have a total thickness between about 2 Å and about 13 Å. In some embodiments, such as when the spacer layer 20 is made of a magnesium oxide, the spacer layer 20 may have a total thickness between about 6.5 Å and about 8.5 Å. In other embodiments, such as when the spacer layer 20 is made of magnesium, the spacer layer 20 may have a total thickness between about 10 Å and about 13 Å. In yet other embodiments, such as when the spacer layer 20 is made of titanium, the spacer layer 20 may have a total thickness between about 6.5 Å and about 10 Å. In still other embodiments, such as when the spacer layer 20 is made of tungsten, the spacer layer 20 may have a total thickness between about 5 Å and about 10 Å.
The free layer 30 may be formed of one or more ferromagnetic materials, such as cobalt iron boron (CoFeB), cobalt/palladium (CoPd), cobalt iron (CoFe), cobalt iron boron tungsten (CoFeBW), nickel iron (NiFe), Ru, Co, alloys thereof, the like, or combinations thereof. The free layer 30 may include multiple layers of different materials, such as a layer of Ru between two layers of CoFeB, a layer of Co between two layers of CoFeB, or a layer of Ru and a layer of Co between two layers of CoFeB, though other configurations of layers or materials may be used. In some embodiments, the material of the free layer 30 includes a crystalline material deposited to have a particular crystalline orientation, such as a (100) orientation. The total thickness of the free layer 30 may be between about 1 nm and about 4 nm.
In some embodiments, the barrier layer 40 is formed of one or more materials such as MgO and AlO, the like, or combinations thereof. In some embodiments, the material of the barrier layer 40 includes a crystalline material deposited to have a particular crystalline orientation, such as a (100) orientation. The material of the barrier layer 40 may be deposited to have the same crystalline orientation as the free layer 30. In some embodiments, the barrier layer 40 may have a thickness between about 0.3 nm and about 3 nm.
The reference layer 50 is second magnetic layer of which the magnetic moment does not change. The reference layer 50 may be made of any of the same materials as the free layer 30 as set forth above, and may have the same material composition as the free layer 30. In some embodiments, the reference layer 50 includes one or more layers of magnetic materials. In some embodiments, the reference layer 50 includes a layer of a combination of cobalt (Co), iron (Fe), and boron (B), such as Co, Fe, and B; Fe and B; Co and Fe; Co; and so forth. In some embodiments, the material of the reference layer 50 includes a crystalline material deposited to have a particular crystalline orientation, such as a (100) orientation. The material of the reference layer 50 may be deposited to have the same crystalline orientation as the barrier layer 40. In some embodiments, a thickness of the reference layer 50 is in a range from about 0.2 nm to about 8 nm.
The pinned layer 60 is a hard bias layer used to pin the spin polarization direction of the reference layer 50 in a fixed direction. Pinning the spin polarization direction of the reference layer 50 allows the magnetic memory device to be toggled between a low-resistance state and a high-resistance state by changing the spin polarization direction of the free layer 30 relative to the reference layer 50. Because the pinned layer 60 is formed over the reference layer 50, the example MTJ film stack 100 shown in
The pinned layer 60 may include multiple layers of different materials, in some embodiments, and may be referred to as a synthetic anti-ferromagnetic (SAF) layer. For example, the pinned layer 60 may comprise a stack of one or more ferromagnetic layers and one or more non-ferromagnetic layers. For example, the pinned layer 60 may be formed from a non-ferromagnetic layer sandwiched between two ferromagnetic layers or may be a stack of alternating non-ferromagnetic layers and ferromagnetic layers. The ferromagnetic layers may be formed of a material such as Co, Fe, Ni, CoFe, NiFe, CoFeB, CoFeBW, alloys thereof, the like, or combinations thereof. The non-ferromagnetic layers may be formed of material such as Cu, Ru, Ir, Pt, W, Ta, Mg, the like, or combinations thereof. In some embodiments, the ferromagnetic layer(s) of the pinned layer 60 may have a thickness between about 2 nm and about 5 nm. In some embodiments, a thicker pinned layer 60 may have stronger antiferromagnetic properties, or may be more robust against external magnetic fields or thermal fluctuation. In some embodiments, the non-ferromagnetic layer(s) of the pinned layer 60 may have a thickness between about 2 Å and about 10 Å. For example, the pinned layer 60 may include a layer of Ru that has a thickness of about 4 Å or about 8.5 Å, though other layers or thicknesses are possible. In some embodiments, one or more layers of the pinned layer 60 includes a crystalline material deposited to have a particular crystalline orientation, such as a (111) orientation. The pinned layer 60 may be formed to have an in-plane magnetic anisotropy (IMA), that is, in the same plane as the horizontal direction of the pinned layer 60. In some embodiments, a total thickness of the pinned layer 60 is in a range from about 3 nm to 25 nm.
In some embodiments, the pinned layer 60 may include an anti-ferromagnetic material (AFM) layer such as PtMn or IrMn to provide strong exchange bias to fix the pinned layer. This forms a “spin-valve structure” and provides better stability of the pinned layer.
The capping layer 70 may be a single or multi-layer structure that serves both to protect the layers under the capping layer 70 during subsequent processes and to provide a top electrode for an overlying via or metal line to connect to. The layer(s) may be formed of a non-ferromagnetic material such as such as Cu, Ru, Ir, Pt, W, Ta, Mg, Ti, TaN, TiN, the like, or combinations thereof. In some embodiments, the capping layer 70 may include two non-ferromagnetic material layers sandwiching another non-ferromagnetic material layer, such as another one of such as Cu, Ru, Ir, Pt, W, Ta, Mg, Ti, TaN, TiN, or the like. For example, in some embodiments, the capping layer may include Ta or Ti sandwiched between two layers of Ru. The thickness of the capping layer 70 may be between about 3 nm and about 25 nm, though other thicknesses are contemplated. In embodiments using multiple layers for the capping layer 70, each layer may be between about 1 nm and about 12 nm.
A top electrode 75 may be disposed over the capping layer 70. The top electrode 75 may be used to provide electrical connection to a conductive pattern coupled to the top of the MTJ film stack 100. The top electrode 75 may be formed of any suitable material, such as titanium, titanium nitride, tantalum, tantalum nitride, the like, or combinations thereof.
In some embodiments, the aforementioned structure may be formed in the SOT induction structure 10 by following steps. The steps of
In some embodiments, the FETs 110 are Fin Field-Effect Transistors (FinFETs) comprising fins 116, gate structures 114, and source regions 112S and drain regions 112D. As shown in
The FETs 110 shown in the Figures are representative, and some features of the FETs 110 may have been omitted from the Figures for clarity. In other embodiments, the arrangement, configuration, sizes, or shapes of features such as fins 116, dummy fins, gate structures 114, dummy gate structures 21, source regions 112S, drain regions 112D, or other features may be different than shown. In other embodiments, the FETs 110 may be another type of transistor, such as planar transistors.
In
The dielectric layer 104 may be patterned to form openings 106 that expose the source regions 112S and the drain regions 112D for subsequent formation of contact plugs 118 (see
Turning to
Turning to
The conductive lines 130A may be formed using a suitable technique such as damascene, dual-damascene, plating, deposition, the like, or combinations thereof. In some embodiments, the conductive lines 130A are formed by first depositing the dielectric layer 128A and patterning the dielectric layer 128A to form openings (e.g., using a suitable photolithography and etching process), and then filling the openings in the dielectric layer 128A with conductive material. For example, the conductive lines 130A may be formed by depositing an optional blanket barrier layer (not individually shown) over the patterned dielectric layer 128A, depositing a conductive material over the blanket barrier layer, and performing a planarization process such as a CMP process or a grinding process to remove excess portions of the blanket conductive barrier layer and the conductive material. The barrier layer or the conductive material may be similar to those described above for the contact plugs 118 (see
In some embodiments, the conductive lines 130A are formed by first depositing the optional blanket barrier layer over the dielectric layer 104 and contact plugs 118, depositing a conductive material over the blanket barrier layer, and then patterning the barrier layer and conductive material (e.g., using a suitable photolithography and etching process) to form the conductive lines 130A. The dielectric layer 128A may be deposited over the conductive lines 130A and a planarization process performed to expose the conductive lines 130A.
In
In some embodiments, the vias 126A formed under the SOT induction structure 10 may be formed using a single damascene process from copper, tungsten, or titanium nitride and can function as bottom electrode 5 (see
As illustrated in
After forming the buffer layer 7 (if used), the SOT induction structure 10 film stack may be deposited. The SOT induction structure 10 is formed using processes and materials such as those discussed above with respect to
In
Following deposition of the MTJ film stack 100 layers an anneal may be performed. If a first anneal after formation of the SOT induction structure 10 is performed, then in some embodiments, a second anneal after deposition of the MTJ film stack 100 may be performed in the presence of a horizontal magnetic field, for setting the in-plane crystal anisotropy of AFM layer. If a first anneal after formation of the SOT induction structure 10 is not performed, then the first anneal after deposition of the MTJ film stack 100 may be performed in the presence of a perpendicular magnetic field to enhance the PMA of the SOT induction structure 10. Then a second anneal may also be performed in the presence of a horizontal magnetic field to set the AFM layer.
In
In
In
In
In
In
In some embodiments, a word line 120 (coupled to a gate of FET 110) extends in the Y-direction and the source lines 125 SL1 and SL2 extend in the X-direction. The SOT induction structure 10 is located above the source or drain regions of two adjacent FETs 110 and is coupled at either end to the respective source or drain regions of the two adjacent FETs 110 by vias and metal wiring layers. The SOT induction structure 10 may have a direction which is predominantly in the X-direction, in some embodiments.
As shown in
In the present disclosure, the SOT induction structure 10 may be a metal doped with at least one dopant, therefore, with the aid of dopant, it can assist the metal to maintain the desired phase, therefore, the thickness and spin-hall angle (SHA) of SOT induction structure 10 may be increased, the resistivity may be decreased, while the good thermal stability of magnetic memory device MC1 may be maintained.
In accordance with some embodiments of the present disclosure, a magnetic memory device includes a substrate, a spin-orbit torque (SOT) induction structure, and a magnetic tunnel junction (MTJ) stack. The SOT induction structure is disposed over the substrate. The SOT induction structure includes a metal and at least one dopant. The MTJ stack is disposed over the SOT induction structure. In an embodiment, the metal may include W, and the at least one dopant may include Co, Ru, Pt, CoFeB, Ta, MgO, or combinations thereof. In an embodiment, a thickness of the SOT induction structure may be greater than or equal to 5 nm. In an embodiment, a spin-hall angle (SHA) of the SOT induction structure may be greater than 0.4. In an embodiment, a magnetic memory device may further include a spacer layer interposed in the SOT induction structure, and the SOT induction structure is separated in a plurality of portion. In an embodiment, the spacer layer may include MgO or MgO/CoFeB.
In accordance with some embodiments of the present disclosure, a magnetic memory device includes a substrate, a spin-orbit torque (SOT) induction structure, and a magnetic tunnel junction (MTJ) stack. The SOT induction structure is disposed over the substrate. The SOT induction structure includes doped W. The MTJ stack is disposed over the SOT induction structure. In an embodiment, the doped W may include hall metal, magnetic material, insulator, or combinations thereof. In an embodiment, the doped W may include Co, Ru, Pt, CoFeB, Ta, MgO, or combinations thereof. In an embodiment, a thickness of the SOT induction structure may be greater than or equal to 5 nm. In an embodiment, a spin-hall angle (SHA) of the SOT induction structure may be greater than 0.4. In an embodiment, a magnetic memory device may further include a spacer layer interposed in the SOT induction structure, and the SOT induction structure is separated in a plurality of portion. In an embodiment, the spacer layer may include MgO or MgO/CoFeB.
In accordance with some embodiments of the present disclosure, a method including providing a substrate, forming a spin-orbit torque (SOT) induction structure over the substrate, wherein the SOT induction structure comprises metal doped with at least one dopant, and forming a magnetic tunnel junction (MTJ) stack over the SOT induction structure. In an embodiment, the SOT induction structure may be formed by sputtering a metal material and a dopant material simultaneously to form doped state. In an embodiment, the SOT induction structure may be formed by: forming a plurality of metal material layers and a plurality of dopant material layers, wherein the plurality of metal material layers and the plurality of dopant material layers are alternately stacked; and performing a heating process, such that the plurality of dopant material layers are dispersed into the plurality of metal material layers to form doped state. In an embodiment, a top layer in alternately stacked layers is the metal material layer. In an embodiment, a thickness of each of the metal material layer may be less than or equal to 1.5 nm. In an embodiment, the metal comprises W, and the at least one dopant comprises Co, Ru, Pt, CoFeB, Ta, MgO, or combinations thereof. In an embodiment, a method may further include: forming a spacer layer in the SOT induction structure.
The foregoing outlines features of several embodiments so that those skilled in the art may better understand the aspects of the present disclosure. Those skilled in the art should appreciate that they may readily use the present disclosure as a basis for designing or modifying other processes and structures for carrying out the same purposes and/or achieving the same advantages of the embodiments introduced herein. Those skilled in the art should also realize that such equivalent constructions do not depart from the spirit and scope of the present disclosure, and that they may make various changes, substitutions, and alterations herein without departing from the spirit and scope of the present disclosure.
This application claims the priority benefit of U.S. Provisional application Ser. No. 63/346,905, filed on May 30, 2022. The entirety of the above-mentioned patent application is hereby incorporated by reference herein and made a part of this specification.
Number | Date | Country | |
---|---|---|---|
63346905 | May 2022 | US |