Memristors are devices that can be programmed to different resistive states by applying programming energy. After programming, the state of the memristor can be read and remains stable over a specified time period. Large crossbar arrays of memristive elements can be used in a variety of applications, including non-volatile solid state memory, programmable logic, signal processing, control systems, pattern recognition, and other applications.
FIGS, 2A-2B, each on coordinates of current (in μA) and voltage (in V), provide a comparison of switching currents for a Ta2O5 device without acceptors (
Reference is now made in detail to specific examples of the disclosed oxide-based memristor and specific examples of ways for creating the disclosed oxide-based memristor. When applicable, alternative examples are also briefly described.
As used in the specification and claims herein, the singular forms “a,” “and,” and “the” include plural referents unless the context clearly dictates otherwise.
As used in this specification and the appended claims, “approximately” and “about” mean a ±10% variance caused by, for example, variations in manufacturing processes.
In the following detailed description, reference is made to the drawings accompanying this disclosure, which illustrate specific examples in which this disclosure may be practiced. The components of the examples can be positioned in a number of different orientations and any directional terminology used in relation to the orientation of the components is used for purposes of illustration and is in no way limiting. Directional terminology includes words such as “top,” “bottom,” “front,” “back,” “leading,” “trailing,” etc.
It is to be understood that other examples in which this disclosure may be practiced exist, and structural or logical changes may be made without departing from the scope of the present disclosure. Therefore, the following detailed description is not to be taken in a limiting sense. Instead, the scope of the present disclosure is defined by the appended claims.
Memristors are nano-scale devices that may be used as a component in a wide range of electronic circuits, such as memories, switches, and logic circuits and systems. In a memory structure, a crossbar of memristors may be used. When used as a basis for memories, the memristor may be used to store a bit of information, 1 or 0. When used as a logic circuit, the memristor may be employed as configuration bits and switches in a logic circuit that resembles a Field Programmable Gate Array, or may be the basis for a wired-logic Programmable Logic Array.
When used as a switch, the memristor may either be a closed or open switch in a cross-point memory. During the last few years, researchers have made great progress in finding ways to make the switching function of these memristors behave efficiently. For example, tantalum oxide (TaOx)-based memristors have been demonstrated to have superior endurance over other na-no-scale devices capable of electronic switching. In lab settings, tantalum oxide-based memristors are capable of over 10 billion switching cycles whereas other memristors, such as tungsten oxide (WOx)- or titanium oxide (TiOx)-based memristors, may require a sophisticated feedback mechanism for avoiding over-driving the devices or an additional step of refreshing the devices with stronger voltage pulses in order to obtain an endurance in the range of 10 million switching cycles.
Memristor devices typically may comprise two electrodes sandwiching an insulating layer. One or more conducting channels in the insulating layer between the two electrodes may be formed that are capable of being switched between two states, one in which the conducting channel forms a conductive path between the two electrodes (“ON”) and one in which the conducting channel does not form a conductive path between the two electrodes (“OFF”).
A memristor may comprise a switching material, such as TiO2 or TaO2, sandwiched between two electrodes. Memristive behavior is achieved by moving mobile species (e.g., ions or vacancies) in or out of the switching material (specifically, forming a conductive channel between the two electrodes (“ON”) or removing the conductive channel (“OFF”)). Initially, when the memristor is first fabricated, the entire switching material is nonconductive. As such, an electroforming process may be required to form the conductive channel in the switching material between the two electrodes. A known electroforming process, often simply called “forming”, includes applying a sufficiently high (threshold) voltage across the electrodes for a sufficient length of time to cause the conductive channel (or active region) in the switching material to form. The threshold voltage and the length of time required for the electroforming process may depend upon the type of material used for the switching material, the first electrode, and the second electrode.
Electroforming-free devices may be desired, and effort has gone into developing such electroforming-free devices. The conventional electroforming-free devices may consist of a relatively thick conductive suboxide (e.g., Ti4O7; from a few nanometers thick to a few hundred nanometers thick in some examples and from 10 to 20 nm thick in other examples) and a relatively thin full oxide, (e.g., TiO2 or Ta2O5; about 10 nm or less in some examples and about 5 nm or less in other examples). However, because these n-type oxides may have too many native donors (e.g. oxygen vacancies) and also because they may need to be thin to be electroforming-free, the device may be too leaky, even in the OFF state (high resistance state). This results in a large switching current and smaller OFF/ON resistance ratio, which may become an issue for the commercialization of memristors.
In accordance with the teachings herein, dopants in these oxides, specifically, acceptor dopants where the native dopants are donors, can reduce the leakage current by compensating the donors, especially from the matrix oxides surrounding the channels. By adding acceptor dopants into the thin full oxide layer, a smaller switching current and a larger OFF/ON resistance ratio may be obtained. Likewise, where the native dopants are acceptors, donor dopants may be used to compensate. A further description of this case of acceptor native dopants is set forth below.
Oxygen vacancies may serve as native donors in n-type oxide and nitrogen vacancies may serve as native donors in n-type nitride semiconductors. Adding acceptors, such as Al, Fe, Co, or Ni, in TiO2 or Si, Hf, Al, Fe, Co, or Ni, in Ta2O5, for example, can compensate these donors and make the thin full oxide semiconductor more resistive by a few orders of magnitude.
Suitable acceptors may be determined by considering the valence state of the transition metal in the oxide or nitride and selecting an element having a lower valence state as the acceptor. For example, Ti has a valence state of +4.Al(+3), Fe(+3), Co(+3), and Ni(+3) all have valence states less than 4. Likewise, Ta has a valence state +5, and Si(+4), Hf(+4), Al, Fe, Co, and Ni all have valence states less than 5.
The bottom electrode 102 may be any conducting material, non-limiting examples of which include platinum (Pt), titanium nitride (TiN), tantalum nitride (TaN), tungsten (W) , tantalum (Ta), iridium (Ir), ruthenium (Ru), ruthenium oxide (RuO2), iridium oxide (IrO2), aluminum (Al), copper (Cu), titanium (Ti), niobium (Nb), molybdenum (Mo), any form of conductive carbon, and heavily-doped semiconductor materials, such as silicon (Si). The top electrode 104 may be selected from the same list as the bottom electrode 102 and may be the same or different. The thickness of each of the bottom electrode 102 and top electrode 104 may be in the range of about 5 to 100 nm.
As indicated above, acceptor dopants 112 may be added to the full oxide layer 108. Acceptor dopants 112 may reduce high leakage current, high operation energy, increase the OFF/ON resistance memory window and provide very low cost, but high-performance (low switching energy and large ON/OFF ratio) and low-energy devices. In an example, the concentration of the dopant may be in the range of about 0.1 to 40 at %; in another example, the concentration may range from about 5 to 30 at %. It appears that there are no deleterious effects in the event of over-compensation. While the dopants 112 may be acceptor dopants in
As in
In one example, the active region 106′ may be relatively larger than the first electrode 102 and the second electrode 104. In another example, the active region 106 may be relatively smaller than the first electrode 102 and the second electrode 104.
In an example, the conducting second phase 110′ may comprise a sub-oxide (or sub-nitride) of the non-conducting oxide (or nitride) first phase 108′. In another example, the conducting second phase 110′ may comprise a compound that is formed between the material comprising the first phase and an added material. As an example, consider the system TaO2:SiO2. This system may be resolved into Ta2Si:Ta2O5:SiO2. In this case, the first, insulating phase, or matrix phase, 108′ may be a mixture of Ta2O5 and SiO2, while the second, conducting phase, or dispersed phase, 110 may be Ta2Si, which is dispersed in the first phase and may form a conducting channel 114. It should be noted that the first phase 108′ may actually be a mixture of two (or more) insulating phases or a solid solution. For convenience, since such materials are insulating, the term “phase” when applied to the phase 108′ includes both single and multiple insulating (or resistive or non-conducting or matrix) phases.
An annealing operation or other thermal forming operation, such as heating by exposure to a high temperature environment or by exposure to electrical resistance heating, may be employed to form the compound conducting channels 114. For many systems, such as Ta—O, Hf—O, Y—O, and the like, electrical resistance heating that generates an elevated temperature is sufficient to form the compound conducting channels 114 locally inside the cross-sectional area. The temperature in the localized region inside the device can be several hundred degrees higher than the rest of the materials and can therefore enhance the chemical reactions in the switching materials to form the compound conducting channels 114.
In the device 150 depicted in
As depicted in
An example of the improvement provided by adding acceptor dopants is provided in the comparison
In
Adding Si dopants into a full oxide layer, such as Ta2O5 in the TaOx device shown in
1. Switching current decreases by 20 times (5 μA in
2. OFF/ON resistance ratio increases by 10 times; and
3. Switching energy decreases by over 100 times.
If the insulating layer (e.g., Ni1-xO) in the bi-layer stack is “p-type” instead, such as Ti4O7/Ni1-xO, then donors, such as Ti or Al may be used to compensate the native acceptor dopants and significantly reduce the current level through the Ni1-xO layer, resulting in low energy operation. Here, Ni is in the 2+ valence state, so dopants such as Ti(+4) and Al(+3) may be used for the compensation.
Thus, depending on the nature of the native dopants already present, a dopant of the opposite nature may be added to compensate. Extra oxygen ions in p-type oxides (such as Ni oxide, Fe oxide and Co oxide) may serve as acceptor dopants. Adding donor dopants in these semiconductors, such as Al or Si, can compensate the acceptors and make the full oxide 108, 108′ more resistive, too.
Examples for processes for adding the compensating dopant (acceptor or donor) may include, without limitation, codeposition with the full oxide 108 or 158, using two targets or using a target that has desired concentration; atomic layer deposition (ALD) involving layering the elements; reactive sputtering; thermal oxidation; or ion implantation. Any of these processes may be used to form the device 100, 150 of
Turning now to
Next, one of at least two paths may be followed, both involving forming an active region 106, 106′ on the bottom electrode 102. In the first path, the active region 106 may be formed 310 by providing a relatively thin insulating layer, such as a full oxide or full nitride layer, 108 on the bottom electrode 102. The full oxide or full nitride layer 108 may be formed by any number of methods, including, but not limited to, sputtering, ALD, evaporation, or chemical vapor deposition (CVD). The full oxide or full nitride layer 108 may be formed to a thickness within a range of a few nanometers to a few hundred nanometers. The insulating layer 108 may be doped with one or more compensating dopants 112, either during deposition of the full oxide or full nitride or after, such as by ion implantation,
A relatively thick conductive layer, such as a sub-oxide or sub-nitride layer, 110 may be formed on the insulating layer 108, with sub-oxide formed on full oxide and sub-nitride formed on full nitride. The sub-oxide or sub-nitride layer 110 may be formed by any number of methods, including those listed for the full oxide/full nitride layer. The sub-oxide or sub-nitride layer 110 may be formed to a thickness up to about 10 nm. It can be thus appreciated that the full oxide or full nitride layer 108 is relatively thin compared to the sub-oxide or sub-nitride layer 110 and that the sub-oxide or sub-nitride layer is relatively thick compared to the full oxide or full nitride layer 108.
In the second path, the active region 106′ may be formed 310′ by providing a first phase 108′ comprising an insulating layer in which is dispersed a second phase 110′ comprising an electrically conductive material for forming a switching channel 114 in the insulating layer. The insulating layer 108′ may be doped with one or more compensating dopants 112, either during deposition of the insulating layer or after, such as by ion implantation.
A top electrode 104 may be formed 315 on the active region 106, 106. The top electrode 104 may be formed by any number of methods, including those listed above for forming the bottom electrode 102.
The foregoing discussion has been directed to systems in which the insulating material and the conducting material may be metal oxides, or, in the alternative, metal nitrides. However, other materials may be used for the insulating and conducting materials. Examples include, without limitation, metal carbides, metal sulfides, metal phosphides, and mixed systems, such as ternary (e.g., TaNxOy) and above (e.g., quaternary), as well as ternary oxides, quaternary oxides, or other complex oxides, such as strontium titanate oxide (STO) or praseodymium calcium manganese oxide (POMO).
The resulting devices prepared in accordance with the teachings herein evidence high-performance (low switching energy and large ON/OFF ratio) and low-energy.
Filing Document | Filing Date | Country | Kind |
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PCT/US13/30951 | 3/13/2013 | WO | 00 |