BOTTOM ELECTRODES FOR USE WITH METAL OXIDE RESISTIVITY SWITCHING LAYERS
In a first aspect, a metal-insulator-metal (“MIM”) stack is provided that includes a first conductive layer, a resistivity-switching layer having a metal oxide layer formed above the first conductive layer, a material layer between the first conductive layer and the resistivity-switching layer, and a second conductive layer above the resistivity-switching layer. The first conductive layer includes a multi-layer metal-silicide stack, and the material layer has a Gibbs free energy of formation per O between about −3 and −6 eV. A memory cell may be formed from the MIM stack. Numerous other aspects are provided.
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This application is a continuation of U.S. patent application Ser. No. 13/047,098, filed on Mar. 14, 2011, now U.S. Pat. No. 8,354,660, which claims priority to U.S. Provisional Patent Application Ser. No. 61/314,577, filed Mar. 16, 2010, each of which is incorporated by reference herein in its entirety for all purposes.
BACKGROUNDThe present invention relates to memory arrays and more particularly to bottom electrodes for use with metal oxide resistivity switching layers. Reversible resistivity-switching materials such as metal oxides may be used as storage elements in memory arrays. For example, U.S. Pat. No. 7,812,404, filed May 9, 2005 and titled “Non-Volatile Memory Cell Comprising A Diode And A Resistance-Switching Material,” which is hereby incorporated by reference herein in its entirety, describes a rewriteable non-volatile memory cell that includes a diode coupled in series with an RRS material such as a metal oxide or metal nitride.
However, fabricating memory devices from metal oxide rewriteable resistivity-switching materials with desirable switching characteristics is difficult; and improved memory devices that employ metal oxide resistivity-switching materials are desirable.
SUMMARYIn a first aspect of the invention, a metal-insulator-metal stack is provided that includes a first conductive layer, a resistivity-switching layer having a metal oxide layer formed above the first conductive layer, a material layer between the first conductive layer and the resistivity-switching layer, and a second conductive layer above the resistivity-switching layer. The first conductive layer includes a multi-layer metal-silicide stack, and the material layer has a Gibbs free energy of formation per O between about −3 and −6 eV. A memory cell may be formed from the MIM stack.
In a second aspect of the invention, a method is provided of forming a metal-insulator-metal stack. The method includes forming a first conductive layer having a multi-layer metal-silicide stack, forming a resistivity-switching layer having a metal oxide layer above the first conductive layer, forming a material layer between the first conductive layer and the resistivity-switching layer, and forming a second conductive layer above the resistivity-switching layer. The material layer has a Gibbs free energy of formation per O between about −3 and −6 eV. Numerous other aspects are provided.
Other features and aspects of this invention will become more fully apparent from the following detailed description, the appended claims and the accompanying drawings.
A metal-insulator-metal (“MIM”) stack formed from a reversible resistivity switching (“RRS”) material sandwiched between two metal or otherwise conducting layers may serve as a resistance-switching element for a memory cell. The two conducting layers may serve as the top and bottom electrodes of the resistance-switching element, and may be used to apply an electric field across the RRS material that changes the resistivity of the RRS material from a high value to a low value and vice versa.
In accordance with embodiments of the present invention, novel MIM stacks are provided that employ metal oxide resistivity-switching layers. Methods of forming such MIM stacks, as well as methods of employing such MIM stacks in three-dimensional (“3D”) memory arrays, are also provided.
These and other embodiments of the invention are described below with reference to
MIM Stacks with SiGe Bottom Electrodes
In accordance with some embodiments of the invention, MIM stacks are provided that employ bottom electrodes comprised of a silicon germanium alloy. For example,
The RRS material 104 may include, for example, HfOX, ZrOX, NiOX, TiOX, TaOX, NbOX, AlXOY, another metal oxide (“MOX”) layer, any combination of these metal oxides, or another suitable switching material. In some embodiments, the top electrode 106 may include titanium nitride, tantalum nitride, tungsten nitride, combinations of the same, a metal/metal nitride stack such as Ti/TiN, Ta/TaN, W/WN or another similar layer. In other embodiments, the top electrode 106 may include heavily doped semiconductor such as n+ silicon or p+ silicon, heavily doped germanium, or heavily doped silicon-germanium. Other materials and/or configurations may be used for the top electrode 106.
Use of an n+ Si bottom electrode may improve the switching characteristics of a metal oxide such as HfO2 by effectively lowering the free energy for forming oxygen vacancies within the metal oxide. Typically, such an n+ Si electrode is formed by depositing an amorphous or polysilicon n+ Si layer and then annealing the n+ Si layer to improve its crystallinity and surface properties prior to formation of a metal oxide layer over the n+ Si layer. Such an anneal is generally achieved via a rapid thermal anneal (“RTA”) at a temperature of about 750° C. However, when forming a multi layer, 3 dimensional memory array, use of such a high RTA temperature for each memory layer may exceed the thermal budget of the memory array.
In accordance with some embodiments of the present invention, the bottom electrode of an MIM stack may include a layer of SiGe alloy having, for example, between about 5 to about 35 atm % Ge and an n+ doping concentration of about 5×1019-5×1021 atoms/cm3, in some embodiments about 2×1020 atoms/cm3. Such a SiGe alloy layer may be formed at a substantially lower temperature than a polycrystalline n+ Si bottom electrode layer as the presence of Ge lowers the crystallization temperature.
For example, in some embodiments, a polycrystalline SiGe alloy layer may be deposited at a temperature of about 600° C. or lower, and in some embodiments, about 550° C. or lower without requiring an additional high temperature anneal to improve crystallinity of the SiGe layer (depending on the atm % of Ge employed). Alternatively, an amorphous SiGe alloy layer be deposited at a lower deposition temperature and crystallized using an RTA of about 600° C. or less, and in some embodiments, about 550° C. or less (depending on the atm % of Ge employed).
In particular embodiments, SiGe bottom electrodes with about 5-35 atm % Ge significantly reduce deposition and/or crystallization anneal temperatures while still providing ample Si for oxygen vacancy formation within metal oxide switching layers. Exemplary thicknesses for the SiGe bottom electrode 108 range from about 2 to 100 nanometers. Other atm % of Ge, doping types, doping levels, annealing temperatures and/or layer thicknesses may be used.
In some embodiments, the additional layer(s) 110 may include, for example, titanium, titanium oxide, tantalum, tantalum oxide, tungsten, tungsten oxide, etc. In yet other embodiments, the additional layer(s) 110 may include a metal/metal oxide layer stack such as Ti/TiOX, Zr/ZrOX, Ni/NiOX, Al/AlXOY, Ta/TaOX, Nb/NbOX, Hf/HfOX, or any suitable layer stack.
For example, the bottom electrode 108 (SiGe) may have a thickness of about 2 to 100 nanometers, in other embodiments about 10-60 nanometers, and in some embodiments about 20 nanometers. The Ti or TiOX layer 110 may have a thickness of about 0.5-10 nanometers, and in some embodiments about 2 nanometers. When TiOX is employed, x may be about 1.2-2, and in some embodiments about 1.5. The hafnium oxide layer 104 may have a thickness of about 3-12 nanometers, and in some embodiments about 5 nanometers, with x being about 1.2-2.0 and in some embodiments about 1.7. The TiN top electrode 106 may have a thickness of about 2 to 100 nanometers, in other embodiments about 10-60 nanometers, and in some embodiments about 20 nanometers. The doping concentration of the n+ SiGe bottom electrode 108 may be about 5×1019-5×1021 atoms/cm3 and in some embodiments about 2×1020 atoms/cm3 with about 5-35 atm % Ge. Other film thicknesses, x values, atm % of Ge and/or doping concentrations may be used.
In general, the top electrode 106 may include, for example, titanium nitride, tantalum nitride, tungsten nitride, combinations of the same, a metal/metal nitride stack such as Ti/TiN, Ta/TaN, W/WN or another similar barrier layer. The metal/metal oxide layer stack 110 may include, for example, Ti/TiOX, Zr/ZrOX, Ni/NiOX, Al/AlXOY, Ta/TaOX, Nb/NbOX, Hf/HfOX or another similar layer stack. The RRS material 104 may include, for example, HfOX, ZrOX, NiOX, TiOX, TaOX, NbOX or AlXOY, any combination of these metal oxides, or another suitable switching material.
In some embodiments, the metal/metal-oxide layer stack 110 may be formed from a different material than is employed for the RRS material 104. For example, a Ti/TiOX layer stack may be employed with a HfOX, ZrOX, NiOX, TaOX, NbOX or AlXOY switching material. A Zr/ZrOX layer stack may be used with a HfOX, NiOX, TiOX, TaOX, NbOX or AlXOY switching material. A Ni/NiOX layer stack may be used with a HfOX, ZrOX, TiOX, TaOX, NbOX or AlXOY switching material. An Al/AlXOY layer stack may be employed with a HfOX, ZrOX, NiOX, TiOX, TaOX, or NbOX switching material. A Ta/TaOX layer stack may be employed with a HfOX, TiOX, ZrOX, NiOX, NbOX or AlXOY switching material. A Nb/NbOX layer stack may be employed with a HfOX, TiOX, ZrOX, NiOX, TaOX or AlXOY switching material. A Hf/HfOX layer stack may be employed with a NbOX, TiOX, ZrOX, NiOX, TaOX or AlXOY switching material.
In other embodiments, the metal/metal oxide layer stack 110 may be formed from a similar material to that employed for the RRS material 104. For example, a Ti/TiOX layer stack may be employed with a TiOX switching layer. However, in such embodiments, the metal oxide of the layer stack may have a different crystalline structure or other property compared to that of the switching material (e.g., amorphous versus crystalline structure). The metal oxide layer of the metal/metal-oxide layer stack 110 may serve as a “buffer” layer that allows formation/elimination of oxygen vacancies within the switching material to be more controllable and/or repeatable, which may improve the endurance/longevity of the switching material 104.
MIM Stacks with Multi-Layer Silicide Bottom Electrodes
In accordance with some embodiments of the invention, MIM stacks are provided that employ bottom electrodes comprised of a two or more silicide layers. For example,
The RRS material 104 may include, for example, HfOX, ZrOX, NiOX, TiOX, TaOX, NbOX, AlXOY, another MOX layer, or another suitable switching material. In some embodiments, the top electrode 106 may include titanium nitride, tantalum nitride, tungsten nitride, combinations of the same, a metal/metal nitride stack such as Ti/TiN, Ta/TaN, W/WN or another similar layer. In other embodiments, the top electrode 106 may include heavily doped semiconductor such as n+ silicon or p+ silicon, heavily doped germanium, or heavily doped silicon-germanium. Other materials and/or configurations may be used for the top electrode 106.
As stated, use of an n+ Si bottom electrode may improve the switching characteristics of a metal oxide such as HfO2 by effectively lowering the free energy for forming oxygen vacancies within the metal oxide. However, use of an n+ Si electrode typically requires a relatively high temperature anneal (e.g., about 750° C.) to improve crystallinity and surface properties of the n+ Si electrode prior to formation of a metal oxide layer over the n+ Si layer. When forming a multi layer, 3 dimensional memory array, use of such a high temperature anneal for each memory layer may exceed the thermal budget of the memory array.
In accordance with embodiments of the present invention, the bottom electrode 108 may include two or more layers of metal silicide. In some embodiments, one or more of such metal silicide layers may be formed at temperatures lower than 750° C., such as 600° C. or less, and in some embodiments, about 500-550° C. or less, depending on the type of silicide employed.
For example, cobalt silicide typically may be formed at temperatures of about 300-800° C. and nickel silicide typically may be formed at temperatures of about 400-800° C., depending on factors such as the ratio of Co or Ni atoms to Si atoms. Titanium silicide and tungsten silicide typically require higher formation temperatures ranging from about 500-900° C. for titanium silicide and about 1000° C. or more for tungsten silicide. In any case, use of metal silicides may still provide ample Si for oxygen vacancy formation.
Exemplary materials that may be used for the first metal-silicide layer 108a and/or the second metal-silicide layer 108b include titanium silicide, tantalum silicide, tungsten silicide, nickel silicide, cobalt silicide or molybdenum silicide, although other metal-silicides may be used. In some embodiments, the lower (first) metal-silicide layer 108a may be formed at a lower temperature than the upper (second) metal-silicide layer 108b. In such instances, the lower metal-silicide layer 108a may serve as a crystallization seed layer or “template” for the upper metal-silicide layer 108b, allowing the upper metal-silicide layer 108b to be formed at a lower temperature.
For instance, the first metal-silicide layer 108a may include nickel silicide or cobalt silicide while the second metal-silicide layer 108b may include titanium silicide. Alternatively, the first metal-silicide layer 108a may include titanium silicide and the second metal-silicide layer 108b may include tungsten silicide. Other combinations of silicide layers may be used.
Exemplary thicknesses for the first and/or second metal-silicide layers 108a and 108b range from about 2 to about 50 nanometers. Other thicknesses may be used for either or both layers. While two metal-silicide layers are shown in
In some embodiments, the additional layer(s) 110 may include, for example, titanium, titanium oxide, tantalum, tantalum oxide, tungsten, tungsten oxide, etc.
In yet other embodiments, the additional layer(s) 110 may include a metal/metal oxide layer stack such as Ti/TiOX, Zr/ZrOX, Ni/NiOX, Al/AlXOY, Ta/TaOX, Nb/NbOX, Hf/HfOX, or any suitable layer stack.
As an example, each metal-silicide layer 108a or 108b of the bottom electrode 108 may have a thickness of about 2 to 50 nanometers, in other embodiments about 5-25 nanometers, and in some embodiments about 20 nanometers. The Ti or TiOX layer 110 may have a thickness of about 0.5-10 nanometers, and in some embodiments about 2 nanometers. When TiOX is employed, x may be about 1.2-2, and in some embodiments about 1.5. The hafnium oxide layer 104 may have a thickness of about 3-12 nanometers, and in some embodiments about 5 nanometers, with x being about 1.2-2.0 and in some embodiments about 1.7. The TiN top electrode 106 may have a thickness of about 2 to 100 nanometers, in other embodiments about 10-60 nanometers, and in some embodiments about 20 nanometers. Other film thicknesses, x values and/or doping concentrations may be used.
In general, the top electrode 106 may include, for example, titanium nitride, tantalum nitride, tungsten nitride, combinations of the same, a metal/metal nitride stack such as Ti/TiN, Ta/TaN, W/WN or another similar barrier layer. The metal/metal oxide layer stack 110 may include, for example, Ti/TiOX, Zr/ZrOX, Ni/NiOX, Al/AlXOY, Ta/TaOX, Nb/NbOX, Hf/HfOX or another similar layer stack. The RRS material 104 may include, for example, HfOX, ZrOX, NiOX, TiOX, TaOX, NbOX or AlXOY or another suitable switching material.
In some embodiments, the metal/metal-oxide layer stack 110 may be formed from a different material than is employed for the RRS material 104. For example, a Ti/TiOX layer stack may be employed with a HfOX, ZrOX, NiOX, TaOX, NbOX or AlXOY switching material. A Zr/ZrOX layer stack may be used with a HfOX, NiOX, TiOX, TaOX, NbOX or AlXOY switching material. A Ni/NiOX layer stack may be used with a HfOX, ZrOX, TiOX, TaOX, NbOX or AlXOY switching material. An Al/AlXOY layer stack may be employed with a HfOX, ZrOX, NiOX, TiOX, TaOX, or NbOX switching material. A Ta/TaOX layer stack may be employed with a HfOX, TiOX, ZrOX, NiOX, NbOX or AlXOY switching material. A Nb/NbOX layer stack may be employed with a HfOX, TiOX, ZrOX, NiOX, TaOX or AlXOY switching material. A Hf/HfOX layer stack may be employed with a NbOX, TiOX, ZrOX, NiOX, TaOX or AlXOY switching material.
In other embodiments, the metal/metal oxide layer stack 110 may be formed from a similar material to that employed for the RRS material 104. For example, a Ti/TiOX layer stack may be employed with a TiOX switching layer. However, in such embodiments, the metal oxide of the layer stack may have a different crystalline structure or other property compared to that of the switching material (e.g., amorphous versus crystalline structure).
In some embodiments, the metal, metal nitride or metal oxide layer 212 may include one or more of silicon, silicon nitride or oxide, aluminum, aluminum nitride or oxide, lanthanum, lanthanum nitride or oxide, molybdenum, molybdenum nitride or oxide, tantalum, tantalum nitride or oxide, chromium, chromium nitride or oxide, hafnium, hafnium nitride or oxide, niobium, niobium nitride or oxide, vanadium, vanadium nitride or oxide, zirconium, or zirconium nitride or oxide. In other embodiments an alloy such as n+ SiGe may be used as the metal, metal nitride or metal oxide layer 212. Other materials may also be employed.
Certain metals may promote oxygen vacancy formation in metal oxides by making oxygen vacancy formation more energetically favorable, effectively reducing the Gibbs free energy of forming oxygen vacancies within the metal oxides. See, for example, Roberston et al., “Fermi level pinning by defects in HfO2-metal gate stacks,” Appl. Phys. Letters 91, 132912 (2007), which describes oxygen vacancy formation in a HfO2 gate oxide/Si channel system.
In some embodiments of the present invention, the additional metal, metal nitride or metal oxide layer 212 may be selected so as to have a Gibbs free energy of formation per O between about −3 and −6 eV so as to promote oxygen vacancy formation within the metal oxide RRS material 104. Exemplary metals that may be suitable include, for example, Yb, Tb, Y, So, La, Hf, Mg, Zr, Ta, Nb, V, Zn, W, Mo, Ti, Al, Cr, Si, Ni, Re, Co, Cu, Ru, Rh, Pd, and Ir.
Metal nitrides (or metal oxides) of these metals may render oxygen vacancy formation energetically more favorable within resistivity-switching metal oxides. Accordingly, in some embodiments, the additional metal, metal nitride or metal oxide layer 212 may be formed from one or more metals, metal nitrides or metal oxides of the above-listed materials, or any other materials having a Gibbs free energy of formation per O between about −3 and −6 eV.
Exemplary thicknesses for the metal, metal nitride or metal oxide layer 212 may range from about 10 to about 100 angstroms. Other thicknesses may be used.
In some embodiments, the metal, metal nitride or metal oxide bottom electrode 108 may include one or more of silicon, silicon nitride or oxide, aluminum, aluminum nitride or oxide, lanthanum, lanthanum nitride or oxide, molybdenum, molybdenum nitride or oxide, tantalum, tantalum nitride or oxide, chromium, chromium nitride or oxide, hafnium, hafnium nitride or oxide, niobium, niobium nitride or oxide, vanadium, vanadium nitride or oxide, zirconium or zirconium nitride or oxide. Other materials may also be employed.
As described above, the metal, metal nitride or metal oxide bottom electrode 108 may be selected to promote oxygen vacancy formation in the metal oxide switching layer 104. For example, the metal, metal nitride or metal oxide bottom electrode 108 may be selected so as to have a Gibbs free energy of formation per O between about −3 and −6 eV. Exemplary metals that may fall within this range include, for example, Yb, Tb, Y, So, La, Hf, Mg, Zr, Ta, Nb, V, Zn, W, Mo, Ti, Al, Cr, Si, Ni, Re, Co, Cu, Ru, Rh, Pd, and Ir.
Metal nitrides (or metal oxides) of these metals may similarly render oxygen vacancy formation more energetically favorable within resistivity-switching metal oxides. Accordingly, in some embodiments, the metal, metal nitride or metal oxide bottom electrode 108 may be formed from one or more metals, metal nitrides or metal oxides of the above-listed materials, or any other materials having a Gibbs free energy of formation per O between about −3 and −6 eV.
Exemplary thicknesses for the metal, metal nitride or metal oxide bottom electrode 108 may range from about 10 to about 100 angstroms. Other thicknesses may be used. In one particular embodiment, the metal, metal nitride or metal oxide bottom electrode 108 may include chromium, chromium nitride, hafnium, hafnium nitride, niobium, niobium nitride, vanadium, vanadium nitride, zirconium or zirconium nitride.
Exemplary Inventive Memory CellSteering element 404 may include a thin film transistor, a diode, a metal-insulator-metal tunneling current device, a punch-through diode, a Schottky-diode or another similar steering element that exhibits non-ohmic conduction by selectively limiting the voltage across and/or the current flow through MIM stack 402.
In this manner, memory cell 400 may be used as part of a two or three dimensional memory array and data may be written to and/or read from memory cell 400 without affecting the state of other memory cells in the array. In some embodiments, steering element 404 may be omitted, and memory cell 400 may be used with a remotely located steering element.
Exemplary Embodiments of Memory Cells and Memory ArraysAs described above with reference to
In some embodiments, a barrier layer 408 may be formed between MIM stack 402 and diode 404, and a barrier layer 410 may be formed between MIM stack 402 and second conductor 406b. An additional barrier layer 412 may be formed between diode 404 and first conductor 406a. Barrier layers 408, 410 and 412 may include titanium, titanium nitride, tantalum, tantalum nitride, tungsten, tungsten nitride, molybdenum, combinations of the same, or another similar barrier layer. Barrier layer 210 may be separate from or part of second conductor 406b and barrier layer 412 may be separate from or part of first conductor 406a.
Diode 404 may include any suitable diode such as a vertical polycrystalline p-n or p-i-n diode, whether upward pointing with an n-region above a p-region of the diode or downward pointing with a p-region above an n-region of the diode, a p-n-p or n-p-n punch through diode, a Schottky diode or the like. Exemplary embodiments of diode 204 are described below with reference to
In the embodiment of
First conductor 406a and/or second conductor 406b may include any suitable conductive material such as tungsten, any appropriate metal, heavily doped semiconductor material, a conductive silicide, a conductive silicide-germanide, a conductive germanide, a highly conductive carbon or the like. In the embodiment of
In the embodiment of
In some embodiments, the memory levels may be formed as described in U.S. Pat. No. 6,952,030, titled “High-Density Three-Dimensional Memory Cell,” which is hereby incorporated by reference herein in its entirety for all purposes. For instance, the second (top) conductors of a first memory level may be used as the first (bottom) conductors of a second memory level that is positioned above the first memory level as shown in
For example, as shown in memory array 416b in
If the MIM stacks 402 are bipolar, in embodiments in which conductors are shared between memory levels as in
A monolithic three dimensional memory array is one in which multiple memory levels are formed above a single substrate, such as a wafer, with no intervening substrates. The layers forming one memory level are deposited or grown directly over the layers of an existing level or levels. In contrast, stacked memories have been constructed by forming memory levels on separate substrates and adhering the memory levels atop each other, as in Leedy, U.S. Pat. No. 5,915,167, titled “Three Dimensional Structure Memory.” The substrates may be thinned or removed from the memory levels before bonding, but as the memory levels are initially formed over separate substrates, such memories are not true monolithic three dimensional memory arrays.
Exemplary Stacked Memory CellsWith reference to
MIM stack 502a may include any of the MIM stacks previously described, or any other suitable MIM stack. In
Diode 504a may include any two terminal, non-linear steering element such as a p-n or p-i-n junction diode, a punch through diode, a tunneling oxide device, a Schottky diode, or the like. In
With reference to
Exemplary widths for bit lines 506a and/or spacings between bit lines 506a range from about 200 to about 2500 angstroms, although other conductor widths and/or spacings may be used. Bit lines 506a may be separated from one another by dielectric material (not shown) such as silicon dioxide, silicon nitride, silicon oxynitride, low K dielectric, etc., and/or other dielectric materials.
Barrier layer 512 is formed over bit line 506a. Barrier layer 512 may be about 20 to about 500 angstroms, and in some embodiments about 100 angstroms, of titanium nitride or another suitable barrier layer such as tantalum nitride, tungsten nitride, tungsten, molybdenum, combinations of one or more barrier layers, barrier layers in combination with other layers such as titanium/titanium nitride, tantalum/tantalum nitride or tungsten/tungsten nitride stacks, or the like. Other barrier layer materials and/or thicknesses may be employed.
Semiconductor material used to form the diode 504a is formed over barrier layer 512. In the embodiment of
In at least one embodiment, p+ silicon layer 504a-1 may be formed, for example, from about 100 to about 1000 angstroms, in some embodiments about 100 angstroms, of p+ silicon with a doping concentration of about 1021 cm−3. Other layer thicknesses and/or doping concentrations may be used. P+ silicon layer 504a-1 may be doped in situ, for example, by flowing an acceptor gas during deposition, or ex situ, for example, via implantation.
After deposition of p+ silicon layer 504a-1, a lightly doped, intrinsic and/or unintentionally doped amorphous or polycrystalline silicon layer 504a-2 may be formed over p+ silicon layer 504a-1. CVD or another suitable deposition method may be employed to deposit intrinsic silicon layer 504a-2. In at least one embodiment, intrinsic silicon layer 504a-2 may be about 500 to about 4800 angstroms, in some embodiments about 2500 angstroms, in thickness. Other intrinsic layer thicknesses may be used.
Additional silicon may be deposited and doped by ion implantation or doped in situ during deposition to form an n+ silicon layer 504a-3. Further, in some embodiments, a diffusion process may be employed. In at least one embodiment, the resultant n+ silicon layer 504a-3 may have a thickness of about 100 to about 1000 angstroms, in some embodiments about 100 angstroms, with a doping concentration of about 1021 cm−3. Other layer thicknesses and/or doping concentrations may be used.
Following formation of n+ silicon layer 504a-3, a silicide-forming metal layer stack 508 may be deposited over n+ silicon layer 504a-3. Exemplary silicide-forming metals include sputter or otherwise deposited titanium or cobalt. In some embodiments, a silicide-forming metal layer stack 508 is formed from about 1-4 nanometers of titanium and about 15-25 nanometers of titanium nitride. Other silicide-forming metal layer materials and/or thicknesses may be used.
An RTA step may be performed to form a silicide region by reaction of silicide-forming metal such as Ti with n+ region 504a-3. In some embodiments, the RTA may be performed at about 540° C. for about 1 minute, to cause silicide-forming metal and the deposited silicon of diode 504a to interact to form a silicide layer, consuming all or a portion of the silicide-forming metal.
In other embodiments, a silicide layer may be formed by sputtering a silicide target or by co-sputtering silicide forming metal and silicon.
As described in U.S. Pat. No. 7,176,064, titled “Memory Cell Comprising A Semiconductor Junction Diode Crystallized Adjacent To A Silicide,” which is hereby incorporated by reference herein in its entirety for all purposes, silicide-forming materials such as titanium and/or cobalt react with deposited silicon during annealing to form a silicide layer. The lattice spacing of titanium silicide and cobalt silicide are close to that of silicon, and it appears that such silicide layers may serve as “crystallization templates” or “seeds” for adjacent deposited silicon as the deposited silicon crystallizes (e.g., a silicide layer may enhance the crystalline structure of silicon diode 504a during annealing). Lower resistivity silicon thereby is provided. Similar results may be achieved for silicon-germanium alloy and/or germanium diodes.
Following formation of metal layer stack 508, bottom electrode 108 of MIM stack 502a may be formed. In some embodiments, bottom electrode 108 may include a layer of SiGe alloy having, for example, between about 5 to about 35 atm % Ge and an n+ doping concentration of about 5×1019-5×1021 atoms/cm3, and in some embodiments about 2×1020 atoms/cm3. As stated, SiGe bottom electrodes with about 5-35 atm % Ge significantly reduce crystalline anneal temperatures while still providing ample Si for oxygen vacancy formation.
In some embodiments, low temperature processes such as low pressure chemical vapor deposition (“LPCVD”) or plasma enhanced chemical vapor deposition (“PECVD”) may be employed to form the SiGe bottom electrode 108. Exemplary temperature ranges at which the SiGe bottom electrode 108 may be formed (crystallized) are 600° C. or less, and in some embodiments 550° C. or less. Exemplary thicknesses for the SiGe bottom electrode 108 range from about 2 to 100 nanometers. Other atm % of Ge, doping types, doping levels, formation temperatures and/or layer thicknesses may be used in other embodiments.
Following formation of the bottom electrode 108, RRS material 104 may be formed by atomic layer deposition (“ALD”) or another suitable method. For example, the RRS material 104 may include HfOX, ZrOX, NiOX, TiOX, TaOX, NbOX, AlXOY, combinations of one or more of these metal oxides, or another suitable switching material. In the embodiment of
Following formation of the RRS material 104, a metal/metal oxide layer stack 110 may be formed. The metal/metal oxide layer stack 110 may include, for example, Ti/TiOX, Zr/ZrOX, Ni/NiOX, Al/AlXOY, Ta/TaOX, Nb/NbOX, Hf/HfOX or another similar layer stack. In the embodiment shown, the metal/metal oxide layer stack 110 may include Ti layer 110b having a thickness of about 0.5-10 nanometers, and in some embodiments about 2 nanometers and TiOX layer 110a having a thickness of about 0.5-6 nanometers, and in some embodiments about 1 nanometer; and x may be about 1.2-2.0 and in some embodiments about 1.5. Other thicknesses and/or x values may be used.
The TiOX layer 110a may be formed, for example, by depositing a layer of Ti over the HfOX layer 104 and then oxidizing the Ti to form the TiOX layer 110a. For example, a layer of Ti may be deposited via PVD and then oxidized in the same ALD chamber used to form the HfOX layer 104 (e.g., by not flowing the Hf precursor). The Ti layer 110b may then be formed over the TiOX layer 110a.
Top electrode 106 is formed over Ti layer 110b. For example, top electrode 106 may include titanium nitride, tantalum nitride, tungsten nitride, combinations of the same, a metal/metal nitride stack such as Ti/TiN, Ta/TaN, W/WN or another similar barrier layer. In the embodiment shown, the top electrode 106 may include about 10-60 nanometers, and in some embodiments about 20 nanometers of TiN. Other layer thicknesses may be used. In some embodiments, n+ SiGe layer 108, HfOX layer 104, TiOX layer 110a, Ti Layer 110b and/or TiN layer 106 may be formed in a single cluster tool (e.g., without breaking vacuum) to improve the interfaces between the various layers.
To etch the above described MIM stack and diode layers into a pillar structure 514 (as shown in
-
- (1) deposit a metal hard mask over the top TiN electrode 106, such as about 500-1000 angstroms of W;
- (2) deposit an oxide hard mask over the metal hard mask, such as about 1000-2000 angstroms of SiXOY;
- (3) deposit a polysilicon hard mask over the oxide hard mask, such as about 500-2000 angstroms of polysilicon; and
- (4) deposit photoresist over the polysilicon hard mask, such as about 1000-3000 angstroms of photoresist.
The photoresist layer then may be exposed and developed, and the polysilicon hard mask layer may be etched using, for example, HBr, Cl2, O2, and/or He in a suitable high-density plasma etch chamber. Following stripping (asking) of the photoresist, the oxide hard mask may be etched through the patterned and etched polysilicon hard mask using, for example, C4F6, O2, and Ar in a suitable medium-density plasma etch chamber. The metal hard mask may then be etched through the patterned and etched oxide hard mask using, for example, NF3, Ar, N2, Cl2, He, and/or O2 in a suitable high-density plasma etch chamber.
Thereafter, the TiN top electrode 106 may be etched using, for example, HBr, Cl2, and/or He; the Ti/TiOX metal layer stack 110 may be etched using, for example, CF4, Cl2, He, and/or N2; the HfOX RRS material 104 may be etched using, for example, HBr, Cl2, He, and/or N2; the n+ SiGe bottom electrode 108 may be etched using, for example, HBr, Cl2, He, O2 and/or N2; the Ti/TiN layer stack 508 may be etched using, for example, HBr, Cl2, and/or He; the polysilicon diode 504a may be etched using, for example, HBr, Cl2, He, O2 and/or N2; and the TiN layer 512 may be etched using, for example, HBr, Cl2, and/or He. All of these etch processes may be performed, for example, in a suitable high-density plasma etch chamber. Other etch chemistries and/or processes may be employed.
The resulting pillar structure 514 may be surrounded by a suitable dielectric to isolate it from other similar pillar structures (not shown) on the same memory level. For example, approximately 200-7000 angstroms of silicon dioxide may be deposited and planarized using chemical mechanical polishing or an etchback process to remove excess dielectric material and form a planar surface for receiving word line 506b. Additionally, a thin silicon nitride liner, such as about 50 to 200 angstroms, may be deposited prior to silicon dioxide deposition.
Word line 506b may be formed from any suitable conductive material such as tungsten, another suitable metal, heavily doped semiconductor material, a conductive silicide, a conductive silicide-germanide, a conductive germanide, or the like deposited by any suitable method (e.g., CVD, PVD, etc.). Other conductive layer materials may be used. For example, conductive material may be deposited and etched to form word line 506b (and other word lines not separately shown). In at least one embodiment, such word lines are substantially parallel, substantially coplanar conductors that extend in a different direction than bit line(s) 506a (as shown in
Word line 506b may be isolated from other word lines via a suitable dielectric fill and etchback process. Thereafter, an additional memory cell (not shown) may be formed over the word line 506b in a manner similar to that used to form the memory cell 500a.
Following formation of the memory cell 500a (and/or any additional memory cell layers/levels to be formed above memory cell stack 500a), the resultant structure may be annealed to crystallize the deposited semiconductor material of diode 504a (and/or to form silicide regions by reaction of silicide-forming metal from layer 508 with silicon region(s) of the diode 504a).
As stated above, the lattice spacing of titanium silicide and cobalt silicide are close to that of silicon, and it appears that silicide layers may serve as “crystallization templates” or “seeds” for adjacent deposited silicon as the deposited silicon crystallizes (e.g., a silicide layer may enhance the crystalline structure of silicon diodes during annealing at temperatures of about 600-800° C.). Lower resistivity diode material thereby is provided. Similar results may be achieved for silicon-germanium alloy and/or germanium diodes.
Thus in at least one embodiment, a crystallization anneal may be performed for about 10 seconds to about 2 minutes in nitrogen at a temperature of about 600 to 800° C., and in some embodiments between about 650 and 750° C. Other annealing times, temperatures and/or environments may be used.
The foregoing description discloses only exemplary embodiments of the invention. Modifications of the above disclosed apparatus and methods which fall within the scope of the invention will be readily apparent to those of ordinary skill in the art. For instance, MIM stacks may be placed above or below steering elements within any memory cells.
Accordingly, although the present invention has been disclosed in connection with exemplary embodiments thereof, it should be understood that other embodiments may fall within the spirit and scope of the invention, as defined by the following claims.
Claims
1. A metal-insulator-metal stack comprising:
- a first conductive layer comprising a multi-layer metal-silicide stack;
- a resistivity-switching layer comprising a metal oxide layer formed above the first conductive layer;
- a material layer disposed between the first conductive layer and the resistivity-switching layer, wherein the material layer has a Gibbs free energy of formation per O between about −3 and −6 eV; and
- a second conductive layer formed above the resistivity-switching layer.
2. The metal-insulator-metal stack of claim 1, wherein the multi-layer metal-silicide stack comprises:
- a first metal-silicide layer comprising one of titanium silicide, tantalum silicide, tungsten silicide, nickel silicide, cobalt silicide or molybdenum silicide; and
- a second metal-silicide layer comprises a different one of titanium silicide, tantalum silicide, tungsten silicide, nickel silicide, cobalt silicide or molybdenum silicide.
3. The metal-insulator-metal stack of claim 2, wherein the first metal-silicide layer comprises nickel silicide and the second metal-silicide layer comprises titanium silicide.
4. The metal-insulator-metal stack of claim 2, wherein the first metal-silicide layer comprises cobalt silicide and the second metal-silicide layer comprises titanium silicide.
5. The metal-insulator-metal stack of claim 2, wherein the first metal-silicide layer comprises titanium silicide and the second metal-silicide layer comprises tungsten silicide.
6. The metal-insulator-metal stack of claim 1, wherein the first conductive layer has a thickness of about 2-100 nanometers.
7. The metal-insulator-metal stack of claim 1, wherein the metal oxide layer comprises one or more of HfOX, ZrOX, NiOX, TiOX, TaOX, NbOX or AlXOY.
8. The metal-insulator-metal stack of claim 1, wherein the second conductive layer comprises a layer stack having at least one of a titanium layer and a titanium oxide layer formed over the resistivity-switching layer and a titanium nitride layer formed thereover.
9. The metal-insulator-metal stack of claim 1, wherein the material layer comprises a metal, a metal nitride or a metal oxide.
10. The metal-insulator-metal stack of claim 1, wherein the material layer comprises at least one of aluminum, aluminum nitride, lanthanum, lanthanum nitride, molybdenum, molybdenum nitride, tantalum, tantalum nitride, chromium, chromium nitride, hafnium, hafnium nitride, niobium, niobium nitride, vanadium, vanadium nitride, zirconium or zirconium nitride.
11. A memory cell comprising:
- the metal-insulator-metal stack of claim 1; and
- a steering element coupled to the metal-insulator-metal stack.
12. The memory cell of claim 11, wherein the steering element comprises a vertical polysilicon diode.
13. A method of forming a metal-insulator-metal stack comprising:
- forming a first conductive layer comprising a multi-layer metal-silicide stack;
- forming a resistivity-switching layer comprising a metal oxide layer above the first conductive layer;
- forming a material layer between the first conductive layer and the resistivity-switching layer, wherein the material layer has a Gibbs free energy of formation per O between about −3 and −6 eV; and
- forming a second conductive layer above the resistivity-switching layer.
14. The method of claim 13, wherein the multi-layer metal-silicide stack comprises:
- a first metal-silicide layer comprising one of titanium silicide, tantalum silicide, tungsten silicide, nickel silicide, cobalt silicide or molybdenum silicide; and
- a second metal-silicide layer comprises a different one of titanium silicide, tantalum silicide, tungsten silicide, nickel silicide, cobalt silicide or molybdenum silicide.
15. The method of claim 14, wherein the first metal-silicide layer comprises nickel silicide and the second metal-silicide layer comprises titanium silicide.
16. The method of claim 14, wherein the first metal-silicide layer comprises cobalt silicide and the second metal-silicide layer comprises titanium silicide.
17. The method of claim 14, wherein the first metal-silicide layer comprises titanium silicide and the second metal-silicide layer comprises tungsten silicide.
18. The method of claim 14, wherein the first conductive layer has a thickness of about 2-100 nanometers.
19. The method of claim 13, wherein the metal oxide layer comprises one or more of HfOX, ZrOX, NiOX, TiOX, TaOX, NbOX or AlXOY.
20. The method of claim 13, wherein the material layer comprises a metal, a metal nitride, or a metal oxide.
21. A memory cell formed using the method of claim 13.
Type: Application
Filed: Jan 14, 2013
Publication Date: May 23, 2013
Applicant: SANDISK 3D LLC (Milpitas, CA)
Inventor: SanDisk 3D LLC (Milpitas, CA)
Application Number: 13/740,766
International Classification: H01L 45/00 (20060101);