# Patent

## Title
Asymmetric correlated electron switch operation

## Abstract

Subject matter disclosed herein may relate to correlated electron switches that are capable of asymmetric set or reset operations.

## Background
BACKGROUND
Field
Subject matter disclosed herein may relate to a correlated electron switch device.
Information
Integrated circuit devices, such as electronic switching devices, for example, may be found in a wide range of electronic device types. For example, memory and/or logic devices may incorporate electronic switches that may be used in computers, digital cameras, cellular telephones, tablet devices, personal digital assistants, etc. Factors related to electronic switching devices, such as may be incorporated in memory and/or logic devices that may be of interest to a designer in considering suitability for any particular application may include physical size, storage density, operating voltages, and/or power consumption, for example. Other example factors that may be of interest to designers may include cost of manufacture, ease of manufacture, scalability, and/or reliability. Also, there appears to be an ever increasing need for memory and/or logic devices that exhibit characteristics of lower power and/or higher speed.



BRIEF DESCRIPTION OF THE DRAWINGS
Claimed subject matter is particularly pointed out and distinctly claimed in the concluding portion of the specification. However, both as to organization and/or method of operation, together with objects, features, and/or advantages thereof, it may best be understood by reference to the following detailed description if read with the accompanying drawings in which:
FIG. 1a shows block diagram of an example embodiment of a correlated electron switch (CES) device comprising a correlated electron material, in accordance with an embodiment.
FIG. 1b depicts an example symbol for a correlated electron switch.
FIG. 2 is a schematic diagram of an equivalent circuit of a CES, in accordance with an embodiment.
FIG. 3 shows a plot of current density versus voltage for a CES, according to an embodiment.
FIG. 4 is a plot illustrating symmetric operation of a CES device according to an embodiment.
FIGS. 5A through 5D are plots illustrating symmetric operation of a CES device according particular embodiments.
FIG. 6 is a plot illustrating asymmetric operation of a CES device in accordance with an embodiment.
FIGS. 7A through 7I are diagrams illustrating structures of CES devices according to particular embodiments.



Reference is made in the following detailed description to accompanying drawings, which form a part hereof, wherein like numerals may designate like parts throughout to indicate corresponding and/or analogous components. It will be appreciated that components illustrated in the figures have not necessarily been drawn to scale, such as for simplicity and/or clarity of illustration. For example, dimensions of some components may be exaggerated relative to other components. Further, it is to be understood that other embodiments may be utilized. Furthermore, structural and/or other changes may be made without departing from claimed subject matter. It should also be noted that directions and/or references, for example, such as up, down, top, bottom, and so on, may be used to facilitate discussion of drawings and/or are not intended to restrict application of claimed subject matter. Therefore, the following detailed description is not to be taken to limit claimed subject matter and/or equivalents.
DETAILED DESCRIPTION
References throughout this specification to one implementation, an implementation, one embodiment, an embodiment and/or the like means that a particular feature, structure, and/or characteristic described in connection with a particular implementation and/or embodiment is included in at least one implementation and/or embodiment of claimed subject matter. Thus, appearances of such phrases, for example, in various places throughout this specification are not necessarily intended to refer to the same implementation or to any one particular implementation described. Furthermore, it is to be understood that particular features, structures, and/or characteristics described are capable of being combined in various ways in one or more implementations and, therefore, are within intended claim scope, for example. In general, of course, these and other issues vary with context. Therefore, particular context of description and/or usage provides helpful guidance regarding inferences to be drawn.
The terms, “and”, “or”, “and/or” and/or similar terms, as used herein, include a variety of meanings that also are expected to depend at least in part upon the particular context in which such terms are used. Typically, “or” if used to associate a list, such as A, B or C, is intended to mean A, B, and C, here used in the inclusive sense, as well as A, B or C, here used in the exclusive sense. In addition, the term “one or more” and/or similar terms is used to describe any feature, structure, and/or characteristic in the singular and/or is also used to describe a plurality and/or some other combination of features, structures and/or characteristics. Likewise, the term “based on” and/or similar terms are understood as not necessarily intending to convey an exclusive set of factors, but to allow for existence of additional factors not necessarily expressly described. Of course, for all of the foregoing, particular context of description and/or usage provides helpful guidance regarding inferences to be drawn. It should be noted that the following description merely provides one or more illustrative examples and claimed subject matter is not limited to these one or more illustrative examples; however, again, particular context of description and/or usage provides helpful guidance regarding inferences to be drawn.
Particular aspects of the present disclosure incorporate correlated electron material (CEM) to form a correlated electron switch (CES), such as, for example, in memory and/or logic devices. CES devices may also be utilized in other types of electronic circuits, such as, for example, filter circuits, as discussed more fully below. However, the scope of claimed subject matter is not limited in scope in these respects. In this context, a CES may exhibit a substantially abrupt conductor/insulator transition arising from electron correlations rather than solid state structural phase changes (e.g., crystalline/amorphous in phase change memory (PCM) devices or filamentary formation and conduction in resistive RAM devices). In one aspect, a substantially abrupt conductor/insulator transition in a CES may be responsive to a quantum mechanical phenomenon, in contrast to melting/solidification or filament formation, for example. Such a quantum mechanical transition between conductive and insulative states, and/or between first and second impedance states, in a CES may be understood in any one of several aspects. As used herein, the terms “conductive state”, “lower impedance state”, and/or “metal state” may be interchangeable, and/or may at times be referred to as a “conductive/lower impedance state.” Similarly, the terms “insulative state” and “higher impedance state” may be used interchangeably herein, and/or may at times be referred to as an “insulative/higher impedance state.”
In an aspect, a quantum mechanical transition of correlated electron switch material between an insulative/higher impedance state and a conductive/lower impedance state may be understood in terms of a Mott transition. In a Mott transition, a material may switch from an insulative/higher impedance state to a conductive/lower impedance state if a Mott transition condition occurs. The Mott criteria is defined by (nC)1/3 a≈0.26, where nC is a concentration of electrons and “a” is the Bohr radius. When a critical carrier concentration is achieved such that the Mott criteria is met, the Mott transition will occur and the state of the CES will change from a higher resistance/higher capacitance state to a lower resistance/lower capacitance state.
In another aspect, the Mott transition is controlled by a localization of electrons. When carriers are localized, the strong coulomb interaction between the electrons splits the bands of the CEM to create an insulator. When electrons are no longer localized, the weak coulomb interaction dominates and the band splitting is removed, resulting in a metal (conductive) band. This is sometimes explained as a “crowded elevator” phenomenon. While an elevator has only a few people in it, the people can move around easily, which is analogous to a conductive/lower impedance state. While the elevator reaches a certain concentration of people, on the other hand, the people can no longer move, which is analogous to the insulative/higher impedance state. However, it should be understood that this classical explanation provided for illustrative purposes, like all classical explanations of quantum phenomenon, is only an incomplete analogy, and that claimed subject matter is not limited in this respect.
In a further aspect, switching from an insulative/higher impedance state to a conductive/lower impedance state may bring about a change in capacitance in addition to a change in resistance. That is, in an aspect, a CES may comprise the property of variable resistance together with the property of variable capacitance. For example, in a metal state, a CEM may have substantially zero electric field, and therefore substantially zero capacitance. Similarly, in an insulative/higher impedance state (in which electron screening may be very imperfect due to lower density of free electrons), an external electric field may be capable of penetrating the CEM and therefore the CEM will have capacitance due to a physical change in the dielectric function of the CEM. Thus, for example, a transition from an insulative/higher impedance state to a conductive/lower impedance state in a CES may result in changes in both resistance and capacitance, in an aspect.
In an embodiment, a CES device may switch impedance states responsive to a Mott-transition in a majority of the volume of the CEM of a CES device. In an embodiment, a CES device may comprise a “bulk switch.” As used herein, the term “bulk switch” refers to at least a majority volume of a CEM of a CES device switching impedance states, such as responsive to a Mott-transition. For example, in an embodiment, substantially all of a CEM of a CES device may switch from an insulative/higher impedance state to a conductive/lower impedance state or from a conductive/lower impedance state to an insulative/higher impedance state responsive to a Mott-transition. In an aspect, a CEM may comprise one or more transition metal oxides, one or more rare earth oxides, one or more oxides of one or more f-block elements of the periodic table, one or more rare earth transitional metal oxide perovskites, yttrium, and/or ytterbium, although claimed subject matter is not limited in scope in this respect. In an embodiment, a device, such as CES device, may comprise CEM including one or more materials selected from a group comprising aluminum, cadmium, chromium, cobalt, copper, gold, iron, manganese, mercury, molybdenum, nickel, palladium, rhenium, ruthenium, silver, tin, titanium, vanadium, and zinc (which may be linked to a cation such as oxygen or other types of ligands), or combinations thereof, although claimed subject matter is not limited in scope in this respect.
FIG. 1a shows an example embodiment 100 of a CES device comprising CEM, such as material 102, sandwiched between conductive terminals, such as conductive terminals 101 and 103. In an embodiment, a CES device, such as CES device 100, may comprise a variable impeder device. As utilized herein, the terms “correlated electron switch” and “variable impeder” may be interchangeable. At least in part through application of a critical voltage and a critical current between the terminals, such as between conductive terminals 101 and 103, the CEM, such as material 102, may transition between the aforementioned conductive/lower impedance state and insulative/higher impedance state. As mentioned, CEM, such as material 102, in a variable impeder device, such as variable impeder 100, may transition between a first impedance state and a second impedance state due to a quantum mechanical transition of the correlated electron switch material as a result an applied critical voltage and an applied critical current, as described in more detail below. Also, as mentioned above, a variable impeder device, such as variable impeder device 100, may exhibit properties of both variable resistance and variable capacitance.
In a particular embodiment, a variable impeder device, such as variable impeder device 100, may comprise CEM that may transition between or among a plurality of detectable impedance states based, at least in part, on a transition of at least a majority portion of the CEM between an insulative/higher impedance state and a conductive/lower impedance state due to a quantum mechanical transition of the correlated electron switch material. For example, in an embodiment, a variable impeder device may comprise a bulk switch, in that substantially all of a CEM of a variable impeder device may switch from an insulative/higher impedance state to a conductive/lower impedance state or from a conductive/lower impedance state to an insulative/higher impedance state responsive to a Mott-transition. In this context, an “impedance state” means a detectable state of a variable impeder device that is indicative of a value, symbol, parameter and/or condition, just to provide a few examples. In one particular embodiment, as described below, an impedance state of a variable impeder device may be detected based, at least in part, on a signal detected on terminals of the variable impeder device in a read and/or sense operation. In another particular embodiment, as described below, a variable impeder device may be placed in a particular impedance state to represent or store a particular value, symbol, and/or parameter, and/or to achieve a particular capacitance value for the variable impeder device by application of one or more signals across terminals of the variable impeder device in a “write” and/or “program” operation, for example. Of course, claimed subject matter is not limited in scope to the particular example embodiments described herein.
FIG. 1b depicts an example symbol 110 that may be utilized, for example, in electrical circuit schematic diagrams to notate a CES and/or a variable impeder device. Example symbol 110 is meant to remind the viewer of the variable resistance and variable capacitance properties of a CES and/or variable impeder device, such as variable impeder device 100. Example symbol 110 is not meant to represent an actual circuit diagram, but is merely meant as an electrical circuit diagram symbol. Of course, claimed subject matter is not limited in scope in these respects.
FIG. 2 depicts a schematic diagram of an equivalent circuit of an example variable impeder device, such as variable impeder device 100. As mentioned, a variable impeder device may comprise characteristics of both variable impedance and variable capacitance. For example, an equivalent circuit for a variable impeder device may, in an embodiment, comprise a variable resistor, such as variable resistor 210 in parallel with a variable capacitor, such as variable capacitor 220. Of course, although a variable resistor 210 and variable capacitor 220 are depicted in FIG. 2 as comprising discrete components, a variable impeder device, such as variable impeder device 100, may comprise a substantially homogenous CEM, such as CEM 102, wherein the CEM comprises characteristics of variable capacitance and variable resistance.
Table 1 below depicts an example truth table for an example variable impeder device, such as variable impeder device 100.







TABLE 1







Correlated Electron Switch Truth Table










Resistance
Capacitance







Rhigh(Vapplied)
Chigh(Vapplied)



Rlow(Vapplied)
Clow(Vapplied)~0










In an embodiment, example truth table 120 shows that a resistance of a variable impeder device, such as variable impeder device 100, may transition between a lower resistance state and a higher resistance state that is a function, at least in part, of a voltage applied across the CEM. In an embodiment, a resistance of a lower resistance state may be 10-100,000 times lower than a resistance of a higher impedance state, although claimed subject matter is not limited in scope in this respect. Similarly, example truth table 120 shows that a capacitance of a variable impeder device, such as variable impeder device 100, may transition between a lower capacitance state, which for an example embodiment may comprise approximately zero, or very little, capacitance, and a higher capacitance state that is a function, at least in part, of a voltage applied across the CEM. It should be noted that a variable impeder is not a resistor, but rather comprises a device having properties of both variable capacitance and variable resistance. In an embodiment, resistance and/or capacitance values depend, at least in part, on an applied voltage.
FIG. 3 shows a plot of current density versus voltage across electrically conductive terminals, such as electrically conductive terminals 101 and 103, for a variable impeder device, such as example variable impeder device 100, according to an embodiment. Based, at least in part, on a voltage applied to terminals of a variable impeder device (e.g., in a write operation), such as variable impeder device 100, a CEM, such as CEM 102, may be placed in a conductive/lower impedance state or an insulative/higher impedance state. For example, application of a voltage Vreset and current density Jreset may place the variable impeder device in an insulative/higher impedance state, and application of a voltage Vset and a current density Jset may place the variable impeder device in a conductive/lower impedance state. That is, a “set” operation may place a variable impeder device, such as variable impeder device 100, into a conductive/lower impedance state, and a “reset” operation may place a variable impeder device, such as variable impeder device 100, into an insulative/higher impedance state, in an embodiment. Following placement of the variable impeder device in a lower impedance state or a higher impedance state, the particular state of the variable impeder device may be detected at least in part by application of a voltage Vread (e.g., in a read operation) and detection of a current or current density at terminals, such as electrically conductive terminals 101 and 103, of a variable impeder device, such as variable impeder device 100.
In an embodiment, a CEM of a variable impeder device may include, for example, any TMO, such as, for example, peroskovites, Mott insulators, charge exchange insulators, and/or Anderson disorder insulators. In a particular embodiment, a CES device may be formed from materials such as nickel oxide, cobalt oxide, iron oxide, yttrium oxide and peroskovites such as Cr doped strontium titanate, lanthanum titanate, and the manganite family including praesydium calcium manganite, and praesydium lanthanum manganite, to provide a few examples. In an embodiment, oxides incorporating elements with incomplete d and f orbital shells may exhibit sufficient impedance switching properties for use in a CES device. In an embodiment, a CES may be prepared without electroforming. Other embodiments may employ other transition metal compounds without deviating from claimed subject matter. For example, {M(chxn)2Br}Br2 where M may comprise Pt, Pd, or Ni, and chxn comprises 1R,2R-cyclohexanediamine, and other such metal complexes may be used without deviating from the scope of claimed subject matter.
In one aspect, the variable impeder device of FIG. 1 may comprise materials that comprise TMO metal oxide variable impedance materials, though it should be understood that these are exemplary only, and are not intended to limit the scope of claimed subject matter. Particular implementations may employ other variable impedance materials as well. Nickel oxide, NiO, is disclosed as one particular TMO. NiO materials discussed herein may be doped with extrinsic ligands, which may stabilize variable impedance properties by passivating the interfacing and allowing for adjustable voltages and impedances, in an embodiment. In a particular embodiment, NiO variable impedance materials disclosed herein may include a carbon containing ligand, which may be indicated by NiO(Cx). Here, one skilled in the art may determine a value of x for any specific carbon containing ligand and any specific combination of carbon containing ligand with NiO simply by balancing valences, in an embodiment. In another particular example embodiment, NiO doped with extrinsic ligands may be expressed as NiO(Lx), where Lx is a ligand element or compound and x indicates a number of units of the ligand for one unit of NiO. One skilled in the art may determine a value of x for any specific ligand and any specific combination of ligand with NiO or any other transition metal simply by balancing valences, in an embodiment.
According to an embodiment, if sufficient bias is applied (e.g., exceeding a band-splitting potential) and the aforementioned Mott condition is met (injected electron holes=the electrons in the switching region), the variable impeder device may rapidly switch from a conductive/lower impedance state to an insulator state via the Mott transition. This may occur at point 308 of the plot in FIG. 3. At this point, electrons are no longer screened and become localized. This correlation splits the bands to form an insulator. While the CEM of the variable impeder device is still in the insulative/higher impedance state, current may generated by transportation of holes. If enough bias is applied across terminals of the variable impeder device, electrons may be injected into a metal-insulator-metal (MIM) diode over the potential barrier of the MIM device. If enough electrons have been injected and enough potential is applied across terminals to achieve a set condition, an increase in electrons may screen electrons and remove a localization of electrons, which may collapse the band-splitting potential forming a metal, thereby placing the variable impeder device in a conductive/lower impedance state.
According to an embodiment, current in a CEM of a variable impeder device may be controlled by an externally applied “compliance” condition determined based, at least in part, on the external current limited during a write operation to achieve a set condition to place the variable impeder device in a conductive/lower impedance state. This externally applied compliance current also sets the subsequent reset condition current density requirement. As shown in the particular implementation of FIG. 3, a current density Jcomp applied during a write operation at point 316 to place the variable impeder device in a conductive/lower impedance state may determine a compliance condition for placing the variable impeder device in an insulative/higher impedance state in a subsequent write operation. As shown, the CEM of the variable impeder device may be subsequently placed in an insulative/higher impedance state by application of a current density Jreset≧Jcomp at a voltage Vreset at point 308, wherein Jcomp may be externally applied, in an embodiment.
A compliance current, such as an externally applied compliance current, therefore may set a number of electrons in a CEM of a variable impeder device which are to be “captured” by holes for the Mott transition. In other words, a current applied in a write operation to place a variable impeder device in a conductive/lower impedance state may determine a number of holes to be injected to the CEM of the variable impeder device for subsequently transitioning the variable impeder device to an insulative/higher impedance state. As discussed more fully below, a compliance current may be applied dynamically.
As pointed out above, a transition to an insulative/higher impedance state may occur in response to a Mott transition at point 308. As pointed out above, such a Mott transition may occur at a condition in a CEM of a variable impeder device in which a concentration of electrons n equals a concentration of electron holes p. This condition occurs when the following Mott criteria is met, as represented by expression (1) as follows:




  
    
      
        
          
            
              λ
              TF
            
            ⁢
            
              n
              
                1
                3
              
            
          
          =
          
            C
            ~
            0.26
          
        
        ⁢
        
          

        
        ⁢
        
          n
          =
          
            
              (
              
                C
                
                  λ
                  TF
                
              
              )
            
            3
          
        
      
    
    
      
        (
        1
        )
      
    
  




where:

λTF is a Thomas Fermi screening length; and
C is a constant which equals approximately 0.26 for the Mott transition.
According to an embodiment, a current or current density in a region 304 of the plot shown in FIG. 3 may exist in response to an injection of holes from a voltage signal applied across terminals, such as terminals 101 and 103, of a variable impeder device, such as variable impeder device 100. Here, injection of holes may meet a Mott transition criterion for the conductive to insulator transition at current IMI as a critical voltage VMI is applied across terminals, such as terminal 101 and 103, of a variable impeder device, such as variable impeder device 100. This may be modeled according to expression (2) as follows:




  
    
      
        
          
            
              I
              MI
            
            ⁡
            
              (
              
                V
                MI
              
              )
            
          
          =
          
            
              
                d
                
                  Q
                  ⁡
                  
                    (
                    
                      V
                      MI
                    
                    )
                  
                
              
              
                d
                t
              
            
            ≈
            
              
                Q
                ⁡
                
                  (
                  
                    V
                    MI
                  
                  )
                
              
              t
            
          
        
        ⁢
        
          

        
        ⁢
        
          
            Q
            ⁡
            
              (
              
                V
                MI
              
              )
            
          
          =
          
            qn
            ⁡
            
              (
              
                V
                MI
              
              )
            
          
        
      
    
    
      
        (
        2
        )
      
    
  




Where Q(VMI) is the charge injected (hole or electron) and is a function of the applied voltage. As used herein, the notation “MI” signifies a metal-to-insulator transition, and the notation “IM” signifies an insulator-metal transition. That is, “VMI” refers to a critical voltage and “IMI” refers to a critical current to transition a CEM from a conductive/lower impedance state to an insulative/higher impedance state. Similarly, “VIM” refers to a critical voltage and “IIM” refers to a critical current to transition a CEM from an insulative/higher impedance state to a conductive/lower impedance state.

Injection of holes to enable a Mott transition may occur between bands and in response to critical voltage VMI. and critical current IMI. By equating electron concentration n with the needed charge concentration to result in a Mott transition by holes injected by IMI in expression (2) according to expression (1), a dependency of such a critical voltage VMI on Thomas Fermi screening length λTF may be modeled according to expression (3) as follows:




  
    
      
        
          
            
              I
              MI
            
            ⁡
            
              (
              
                V
                MI
              
              )
            
          
          =
          
            
              
                Q
                ⁡
                
                  (
                  
                    V
                    MI
                  
                  )
                
              
              t
            
            =
            
              
                
                  qn
                  ⁡
                  
                    (
                    
                      V
                      MI
                    
                    )
                  
                
                t
              
              =
              
                
                  q
                  t
                
                ⁢
                
                  
                    (
                    
                      C
                      
                        λ
                        TF
                      
                    
                    )
                  
                  3
                
              
            
          
        
        ⁢
        
          

        
        ⁢
        
          
            
              J
              reset
            
            ⁡
            
              (
              
                V
                MI
              
              )
            
          
          =
          
            
              
                J
                MI
              
              ⁡
              
                (
                
                  V
                  MI
                
                )
              
            
            =
            
              
                
                  
                    I
                    MI
                  
                  ⁡
                  
                    (
                    
                      V
                      MI
                    
                    )
                  
                
                
                  A
                  CEM
                
              
              =
              
                
                  q
                  
                    
                      A
                      CEM
                    
                    ⁢
                    t
                  
                
                ⁢
                
                  
                    (
                    
                      C
                      
                        
                          λ
                          TF
                        
                        ⁡
                        
                          (
                          
                            V
                            MI
                          
                          )
                        
                      
                    
                    )
                  
                  3
                
              
            
          
        
      
    
    
      
        (
        3
        )
      
    
  




Wherein ACEM is a cross-sectional area of a CEM, such as CEM 102, of a variable impeder device, such as variable impeder device 100, and wherein Jreset (VMI), depicted at point 308 of example plot 300, is a current density through the CEM, such as CEM 102, to be applied to the CEM at a critical voltage VMI to place the CEM of the variable impeder device in an insulative/higher impedance state. In an embodiment, a CEM may be switched between a conductive/lower impedance state and an insulative/higher impedance state at least in part by a disproportionation reaction.

According to an embodiment, a CEM, such as CEM 102, of a variable impeder device, such as variable impeder device 100, may be placed in a conductive/lower impedance state (e.g., by transitioning from an insulative/higher impedance state) by injection of a sufficient number of electrons to satisfy a Mott transition criteria.
In transitioning a CEM of a variable impeder device to a conductive/lower impedance state, as enough electrons have been injected and the potential across terminals of the variable impeder device overcomes a critical switching potential (e.g., Vset), injected electrons begin to screen and unlocalize double-occupied electrons to reverse a disproportion reaction and closing the bandgap. A current density Jset (VMI), depicted at point 314 of FIG. 3, for transitioning the CEM of the variable impeder device to the conductive/lower impedance state in a metal-insulator Mott transition at a critical voltage VMI enabling transition to the conductive/lower impedance state may be represented according to expressions (4) as follows:




  
    
      
        
          
            
              I
              MI
            
            ⁡
            
              (
              
                V
                MI
              
              )
            
          
          =
          
            
              
                d
                
                  Q
                  ⁡
                  
                    (
                    
                      V
                      MI
                    
                    )
                  
                
              
              
                d
                t
              
            
            ≈
            
              
                Q
                ⁡
                
                  (
                  
                    V
                    MI
                  
                  )
                
              
              t
            
          
        
        ⁢
        
          

        
        ⁢
        
          
            Q
            ⁡
            
              (
              
                V
                MI
              
              )
            
          
          =
          
            qn
            ⁡
            
              (
              
                V
                MI
              
              )
            
          
        
        ⁢
        
          

        
        ⁢
        
          
            
              I
              MI
            
            ⁡
            
              (
              
                V
                MI
              
              )
            
          
          =
          
            
              
                Q
                ⁡
                
                  (
                  
                    V
                    MI
                  
                  )
                
              
              t
            
            =
            
              
                
                  qn
                  ⁡
                  
                    (
                    
                      V
                      MI
                    
                    )
                  
                
                t
              
              =
              
                
                  q
                  t
                
                ⁢
                
                  
                    (
                    
                      C
                      
                        a
                        B
                      
                    
                    )
                  
                  3
                
              
            
          
        
        ⁢
        
          

        
        ⁢
        
          
            
              J
              set
            
            ⁡
            
              (
              
                V
                IM
              
              )
            
          
          =
          
            
              
                J
                injection
              
              ⁡
              
                (
                
                  V
                  IM
                
                )
              
            
            =
            
              
                
                  J
                  IM
                
                ⁡
                
                  (
                  
                    V
                    IM
                  
                  )
                
              
              =
              
                
                  
                    
                      I
                      IM
                    
                    ⁡
                    
                      (
                      
                        V
                        IM
                      
                      )
                    
                  
                  
                    A
                    CEM
                  
                
                =
                
                  
                    q
                    
                      
                        A
                        CEM
                      
                      ⁢
                      t
                    
                  
                  ⁢
                  
                    
                      (
                      
                        C
                        
                          a
                          B
                        
                      
                      )
                    
                    3
                  
                
              
            
          
        
      
    
    
      
        (
        4
        )
      
    
  




where:

aB is a Bohr radius.
According to an embodiment, a “read window” 302 for detecting a memory state of a variable impeder device in a read operation may be set out as a difference between a portion 306 the plot of FIG. 3 while the CEM of the variable impeder device is in an insulative/higher impedance state and a portion 304 of the plot FIG. 3 while the CEM of the variable impeder device is in a conductive/lower impedance state at a read voltage Vread. In a particular implementation, read window 302 may be used to determine the Thomas Fermi screening length λTF of a CEM, such as correlated electron switch material 102, of a variable impeder device, such as variable impeder device 100. For example, at a voltage Vreset, current densities Jreset and Jset may be related to according to expression (5) as follows:




  
    
      
        
          
            λ
            TF
          
          ⁡
          
            (
            
              @
              
                V
                reset
              
            
            )
          
        
        =
        
          
            
              a
              B
            
            ⁡
            
              (
              
                
                  J
                  reset
                
                
                  J
                  off
                
              
              )
            
          
          
            1
            3
          
        
      
    
    
      
        (
        5
        )
      
    
  




wherein Joff represents a current density of a CEM in an insulative/higher impedance state at Vreset. See, for example, point 309 of FIG. 3.

In another embodiment, a “write window” 310 for placing a CEM of variable impeder device in an insulative/higher impedance or conductive/lower impedance state in a write operation may be set out as a difference between Vreset and Vset. Establishing |Vset|>|Vreset| may enable a switch between the conductive/lower impedance and insulative/higher impedance state. Vreset may comprise approximately the band splitting potential caused by the correlation and Vset may comprise approximately twice the band splitting potential, such that the read window may comprise approximately the band-splitting potential. In particular implementations, a size of write window 310 may be determined, at least in part, by materials and doping of the CEM of the variable impeder device.
In an embodiment, a process for reading a value represented as an impedance state of a variable impeder device, such as variable impeder device 100, may comprise a voltage being applied to a CEM of a variable impeder device. At least one of a current and/or current density within a CEM of a variable impeder device may be measured, and an impedance state of a CEM of a variable impeder device may be determined, at least in part, on the measured current and/or current density, in an embodiment.
Additionally, in an embodiment, an impedance of an impedance state may depend at least in part on a combination of a capacitance and a resistance of a CEM of a variable impeder device. In an embodiment, the determined impedance state may comprise one of a plurality of impedance states. A first impedance state may comprise a lower resistance and lower capacitance, and a second impedance state may comprise a higher resistance and a higher capacitance, for example. Also, in an embodiment, a ratio of the impedances of the plurality of impedance states may be proportional to a physical property of the CEM of the variable impeder device. In an embodiment, the physical property of the CEM of the variable impeder device may comprise at least one of a Thomas Fermi screening length and a Bohr radius. Further, in an embodiment, individual impedance states of the plurality of impedance states may be associated with a data value. Additionally, in an embodiment, a difference in current between a first impedance state and a second impedance state at a predetermined voltage provides an indication of a read window. However, claimed subject matter is not limited in scope in these respects.
In an embodiment, a plurality of electrons may be provided to a CEM of a variable impeder device such that the CEM enters a first impedance state. A plurality of holes may be provided to the CEM such that the CEM enters a second impedance state. Also, in an embodiment, the plurality of electrons may cause a voltage across the CEM to be greater than a set voltage threshold, and the plurality of holes may cause the voltage across the CEM to be equal to or greater than a reset voltage threshold. Further, in an embodiment, a voltage across the CEM may cause a current density in the CEM to be equal to or greater than a set current density and/or a set current, and a voltage across the CEM may cause a current density in the CEM to be equal to or greater than a reset current density and/or a reset current.
Also, in an embodiment, a set voltage across the CEM and a set current density through a CEM of a variable impeder device may be exceeded. Additionally, a reset voltage across a CEM and a reset current density through a CEM of a variable impeder device may be exceeded. Further, in an embodiment, individual impedance states of a plurality of impedance states may be associated with a data value.
In an embodiment, at least one of a reset voltage, a set voltage, and a difference between the set voltage and the reset voltage are proportional to a physical property of a CEM of a variable impeder device. A physical property of a CEM may include at least one of a strong electron potential due to localization, and/or a correlation of electrons, for example. Also, in an embodiment, a difference in the set voltage and the reset voltage may provide an indication of a size of at least one of a write/program window.
According to an embodiment, a write operation as discussed above may be characterized by a particular voltage condition and a particular current condition sufficient to place a CES in a particular impedance state. For example, a set operation to place a CES in a low impedance or conductive state may be characterized by a “set voltage condition” (e.g., Vset) and a “set current condition” (Iset). For example, point 314 in the plot of FIG. 3 indicates a particular set voltage condition along a voltage axis and a particular set current condition along a current or current density axis. Similarly, a reset operation to place a CES in a high impedance or insulative state may be characterized by a “reset voltage condition” (e.g., Vreset) and a “reset current condition” (Ireset). Additionally, as pointed out above, a particular reset current condition for a CES may be determined based, at least in part, on a compliance current (Icomp) applied at point 316 in a previous set operation.
As may be observed from the plot of FIG. 3, a programming signal to place a CES in a low impedance or conductive state may satisfy a set voltage condition having a positive polarity and a set current condition having a positive polarity. Likewise a programming signal to place a CES in a high impedance or insulative state may satisfy a reset voltage condition having a positive polarity and a reset current condition having a positive polarity. In particular embodiments, as illustrated in FIG. 4, write operation may be performed by meeting alternative voltage and current conditions in different polarities. In this context, operation in the voltage versus current plot of FIG. 4 with current and voltage both having a positive polarity places operation in the first quadrant while operation with current and voltage having a negative polarity places operation in the third quadrant. For example, point 408 may define a first set voltage condition of Vset_1 and a first set current condition Iset_1 in a first quadrant while point 410 may define a second set voltage condition of Vset_2 and a second reset current condition Iset_2 in a third quadrant. In other words a particular CES device having operational characterized by the plot of FIG. 4 may be placed in a low impedance or conductive state by application of a programming signal having a voltage Vset_1 and a current Iset_1 (at point 408), or by application of a programming signal having a voltage Vset_2 and a current Iset_2 (at point 410).
Likewise, point 402 may define a first reset voltage condition of Vreset_1 and a first reset current condition Ireset_1 in a first quadrant while point 404 may define a second reset voltage condition of Vreset_2 and a second reset current condition Ireset_2 in a third quadrant. In other words a particular CES device having operational characterized by the plot of FIG. 4 may be placed in a high impedance or insulative state by application of a programming signal having a voltage Vreset_1 and a current Ireset_1 (at point 402), or by application of a programming signal having a voltage Vreset_2 and a current Ireset_2 (at point 404). Here, first and second reset current conditions Ireset_1 and Ireset_2 may be determined based on a magnitude of a compliance current applied in a previous set operation at either point 406 or 412.
In the particular embodiment of FIG. 4, a CES device may be characterized as having symmetric voltage and current conditions for write operations to place the CES in a particular impedance state. Here, as discussed above, first set voltage and current conditions (Vset_1 and Iset_1) are symmetric with second set voltage and current conditions (Vset_2 and Iset_2) in that |Vset_1|≈|Vset_2| and |Iset_1|≈|Iset_2|. Likewise, first reset voltage and current conditions (Vreset_1 and Ireset_1) are symmetric with second set voltage and current conditions (Vreset_2 and Ireset_2) in that |Vreset_1|≈|Vreset_2| and |Ireset_1|≈|Ireset_2. In this context, symmetric voltage conditions for a particular write operation are polar opposite voltages of substantially the same magnitude. Similarly, symmetric current conditions for a particular write operation are polar opposite currents of substantially the same magnitude.
In particular embodiments, FIGS. 5A through 5D are plots illustrating symmetric operation of a CES device according particular embodiments such as the CES device discussed above with reference to FIG. 4. Here, it may observed that a set operation and a reset operation may occur in the same or different quadrants of a voltage vs. current mapping. In FIG. 5A, for example, set voltage and current conditions at point 504 (Vset_1 and Iset_1) are in the first quadrant as reset voltage and current conditions at point 502 (Vreset_1 and Ireset_1). Similarly in FIG. 5B, set voltage and current conditions at point 510 (Vset_2 and Iset_2) are in the third quadrant as reset voltage and current conditions at point 508 (Vreset_2 and Ireset_2) are also in the third quadrant. In contrast, in FIG. 5C, set voltage and current conditions at point 516 (Vset_2 and Iset_2) are in the third quadrant while reset voltage and current conditions at point 514 (Vreset_1 and Ireset_1) are in the first quadrant. Also, in FIG. 5D, set voltage and current conditions at point 522 (Vset_1 and Iset_1) are in the first quadrant while reset voltage and current conditions at point 520 (Vreset_2 and Ireset_2) are in the third quadrant. As may be observed, set voltage and current conditions in the first quadrant in FIGS. 5A and 5D at points 504 and 522 are symmetric with set voltage and current conditions in the third quadrant in FIGS. 5B and 5C. Similarly, reset voltage and current conditions in the first quadrant in FIGS. 5A and 5C at points 502 and 524 are symmetric with reset voltage and current conditions in the third quadrant in FIGS. 5B and 5D at points 508 and 520. It should be understood that a set or reset operations may occur either the first or third quadrants regardless of whether a most recent write operation occurred in the first quadrant of the third quadrant.
FIG. 6 shows plots illustrating asymmetric operation of a CES device in accordance with an embodiment. In a first quadrant of a voltage vs current plot for write operations according to an embodiment, first set voltage and current conditions are shown at point 610 (Vset_1 and Iset_1) and first reset voltage and current conditions are shown at point 606 (Vreset_1 and Ireset_1). The third quadrant of the plot of FIG. 6 shows three alternative plots with corresponding alternative second set voltage and current conditions, and corresponding second reset voltage and current conditions. A first alternative plot defines second set voltage and current conditions at point 622 (Vset_2 and Iset_2), and second reset voltage and current conditions at point 616 (Vreset_2 and Ireset_2). For this particular alternative plot, it may be observed that the first set voltage and current conditions of point 622 are symmetric with the second set voltage and current conditions of point 610 in the first quadrant (e.g., |Vset_1|≈|Vset_2| and |Iset_1|≈|Iset_2|). Likewise, it may be observed that the first reset voltage and current conditions of point 616 are symmetric with the second set voltage and current conditions of point 606 in the first quadrant (e.g., |Vreset_1|≈|Vreset_2| and |Ireset_1|≈|Ireset_2|).
A second alternative plot in the third quadrant defines second set voltage and current conditions at point 614, and second reset voltage and current conditions at point 612. Here, it may be observed that the second set voltage and current conditions at point 614 in the third quadrant are asymmetric with the first set voltage and current conditions at point 610 in the first quadrant in that |Vset_1|>>|Vset_2| and |Iset_1|>>|Iset_2|. Likewise, it may be observed that the second reset voltage and current conditions at point 612 in the third quadrant are asymmetric with the first reset voltage and current conditions at point 606 in the first quadrant in that |Vreset_1|>>|Vreset_2| and |Ireset_1|>>|Ireset_2|.
A third alternative plot in the third quadrant defines second set voltage and current conditions at point 620, and second reset voltage and current conditions at point 618. Here, it may be observed that the second set voltage and current conditions at point 620 in the third quadrant are asymmetric with the first set voltage and current conditions at point 610 in the first quadrant in that |Vset_1|<<|Vset_2| and |Iset_1|<<|Iset_2|. Likewise, it may be observed that the second reset voltage and current conditions at point 618 in the third quadrant are asymmetric with the first reset voltage and current conditions at point 606 in the first quadrant in that |Vreset_1|<<|Vreset_2| and |Ireset_1|<<|Ireset_2|.
According to an embodiment, and with reference to nomenclature for set and reset voltage and current conditions established in FIG. 4, first and second set voltage conditions for a CES device are “asymmetric” if a difference between |Vset_1| and |Vset_2| is large enough to significantly or measurably affect operation or behavior of a circuit implementing the CES device. Similarly, first and second set current conditions are similarly asymmetric if a difference between |Iset_1| and |Iset_2| is large enough to significantly or measurably affect operation or behavior of a circuit implementing the CES device. First and second reset voltage conditions, and first and second reset current conditions of a CES device are similarly asymmetric if a difference between |Vreset_1| and |Vreset_2|, or a difference between |Ireset_1| and |Ireset_2| is large enough to significantly or measurably affect operation or behavior of a circuit incorporating the CES device.
In a particular implementation, a CES may be formed by coupling a CEM substrate between conductive terminals. According to an embodiment, a process for manufacturing a CES device may affect a composition of structure of a CEM substrate so as to provide a CES having asymmetric voltage or current conditions for a set or reset operation as described above. FIGS. 7A through 7I are diagrams illustrating structures of CES devices according to particular embodiments. FIG. 7A shows a structure of a CES comprising CEM substrate (e.g., a transition metal oxide) formed between terminals 702 and 710. A center portion 706 of the CEM is maintained in an intrinsic state while equal portions 704 and 708 are doped as P-type regions. Here, the symmetry of the structure of the CEM between terminals 702 and 710 may provide symmetric set voltage and current conditions, and symmetric reset voltage and current conditions as discussed above (e.g., as illustrated in the plot of FIG. 4). As described below in particular implementations, altering the composition or structure of CEM between terminals may introduce asymmetric behavior in set and reset operations.
Asymmetries described above may be introduced in a CES device (e.g., in a manufacturing process) using any one of several techniques to affect a structure or composition of a CEM substrate of CES. For example, as a bias and injected charge is applied to terminals of a CES device to place the CES device in a particular impedance state, physical properties or structure of the CES device may affect a rate of carrier injection. In a set operation to place a CES device in a low impedance or conductive state, for example, the CES device may be controlled via electron injection over a metal/insulator barrier.
In one implementation, the structure or composition of CES device of FIG. 7A may be altered as shown in FIG. 7B to introduce an asymmetry in set or reset voltage or current conditions. As shown in FIG. 7B, region 714 is more heavily P-type doped than region 718. In another implementation as shown in FIG. 7C, a region 724 is P-typed doped, region 728 is N-type doped and region 726 is maintained in an intrinsic state to provide a PIN structure. In such a PIN structure, injection of electrons may be amplified by injection via N-type doped region 728. This may tune switching behavior in a CES device by introducing different set voltage and current conditions and/or different reset voltage and current conditions in a reverse polarity (e.g., third quadrant).
FIGS. 7D and 7E illustrate an example of how asymmetric operation may be introduced in an IPI device. FIG. 7D shows a CES device comprising equally formed intrinsic regions 734 and 738 separated by a P-type doped region 736. As shown in FIG. 7E, asymmetric set or reset voltage or current conditions may be introduced by replacing intrinsic region 738 with a P or P+ doped region 748. Additionally, asymmetric operation may be introduced by using asymmetric dimensions and/or asymmetric doping as illustrated in FIGS. 7F through 7I. In the CES device shown FIG. 7F, for example, an asymmetric size of P-type doped portions 754 and 758 separated by intrinsic region 756 may introduce asymmetries. This may be further altered by introducing gradient in a concentration of P-type doping as illustrated in FIG. 7G. Here, a concentration of P-type doping in region 768 is highest toward terminal 770 and lowest toward intrinsic region 766 according to a gradient. In FIG. 7H, P-type doped regions 782 and 786 may be the same dimensions. However, asymmetry of set or reset voltage or current conditions may be introduced by introduced by applying a gradient to a concentration in P-type doping in regions 782 and 786. As shown, a higher P-type doping concentration in region 782 occurs toward intrinsic region 784 and a lower P-type doping concentration occurs toward terminal 780, and a higher P-type concentration in region 786 occurs toward terminal 788 and a lower P-type doping concentration occurs toward intrinsic region 784. FIG. 7I shows a single P-type doped region 794 between terminals 790 and 792. A P-type doping concentration gradient provides a highest concentration toward terminal 792 and a lowest P-type doping concentration toward terminal 790.
As described previously, in an embodiment, a voltage may be applied to a CEM of a CES device. Also, in an embodiment, at least one of a current density and/or a current within the CEM may be measured, and an impedance state of the CES dependent on the measured current and/or current density may be determined. In an embodiment, the impedance state may be dependent on a combination of a capacitance and a resistance of the CEM. Further, in an embodiment, the impedance state may comprise one of a plurality of impedance states, wherein a first of the plurality of impedance states has a lower impedance than a second of the plurality of impedance states. In an embodiment, the first impedance state may have a lower resistance and a lower capacitance, and the second impedance state may have a higher resistance and a higher capacitance. Additionally, in an embodiment, a ratio of impedances of the plurality of impedance states may be proportional to a physical property of the CEM. The physical property of the CEM may include, for example, a Thomas Fermi screening length and/or a Bohr radius. Also, in an embodiment, individual impedance states of the plurality of impedance states may be associated with a data value. Further, a difference in current between the first impedance state and the second impedance state at a determined voltage may provide an indication of a read window, in an embodiment.
As also described previously, in an embodiment, a plurality of electrons may be provided to a CEM of a CES device such that the CES enters a first impedance state, and a plurality of holes may be provided to the CEM such that the CES enters a second impedance state. Also, in an embodiment, the plurality of electrons may cause a voltage across the CEM to be greater than a set voltage condition, and the plurality of holes may cause the voltage across the CEM to be equal to or greater than a reset voltage condition. Additionally, the voltage across the CEM may cause a current density in the CEM to be equal to or greater than a set current density and/or a set current condition, and the voltage across the CEM may cause the current density in the CEM to be equal to or greater than a reset current density and/or a reset current, in an embodiment. Further, in an embodiment, a set voltage across the CEM and a set current density through the CEM may be exceeded, and a reset voltage across the CEM and a reset current density through the CEM may be exceeded, in an embodiment. Also, in an embodiment, individual impedance states may be associated with a data value. Additionally, at least one of the reset voltage, the set voltage, and a difference between the set voltage and the reset voltage may be proportional to a physical property of the CEM, wherein the physical property of the CEM may include at least one of a strong electron potential due to localization and/or a correlation of the electrons, in an embodiment. Further, in an embodiment, the difference between the set voltage and the reset voltage may provide an indication of a size of at least one of a write window and/or a programming window.
In a further embodiment, as described previously, a plurality of electrons may be provided to a CEM of a CES device such that a current and/or current density within the CEM exceeds a first threshold and a voltage across the CEM exceeds a second threshold. Further, in an embodiment, switching from a first impedance state to a second impedance state may result from the current and/or current density exceeding the second threshold. The first impedance state may have a higher resistance and a higher capacitance, and the second impedance state has a lower resistance and a lower capacitance, in an embodiment. Additionally, the first threshold may be dependent on at least one of a current and/or current density required to enable a Mott transition in the CEM, a voltage required to inject electrons over a metal insulator barrier within the CEM, and/or a voltage greater or equal to twice the band-splitting potential, in an embodiment.
An another embodiment, a plurality of electrons may be provided to a CEM of a CES device such that a concentration of electrons within the CEM exceeds a threshold, and a switching from a first impedance state to a second impedance state may occur as a result of the concentration of electrons exceeding the threshold for a Mott transition. Further, in an embodiment, at least one of the plurality of electrons may be recombined with at least one of a plurality of holes within the CEM to enable the switching from the first impedance state to the second impedance state. In an embodiment, the concentration of the plurality of electrons and/or holes may be dependent at least in part on at least one physical property associated with the CEM. The at least one physical property may include, for example the Bohr radius. Further, in an embodiment, the threshold may be dependent at least in part on a current and/or current density required to enable the Mott transition. Also, in an embodiment, a resistance and/or capacitance (or impedance) of the CEM may be substantially different, such as a result of the Mott transition, for example. Additionally, a switching from the first impedance state to the second impedance state may be caused by a disproportionation reaction, in an embodiment.
As discussed above, a CEM of a CES device may be provided with a plurality of holes such that a concentration of holes within the CEM exceeds a threshold, and switching from a first impedance state to a second impedance state may occur as a result of the concentration of holes exceeding the threshold, in an embodiment. The first impedance state may comprise a lower resistance, lower capacitance state, and the second impedance state may comprise a higher resistance, higher capacitance state, for example. Also, in an embodiment, the threshold may depend, at least in part, on at least one of a current and/or current density required to enable a Mott-like transition within the CEM, and/or a voltage greater or equal to the band-splitting potential. Additionally, in an embodiment, the threshold may be dependent on a current and/or currently density required to enable a Mott-like transition. In an embodiment, at least one of the plurality of holes may be recombined with a respective at least one of a plurality of electrons within the CEM to enable switching from the first impedance state to the second impedance state. Also, a concentration of the plurality of electrons and/or holes may be dependent at least in part on at least one physical property associated with the CEM. The at least one physical property may include, for example, a Thomas Fermi screening length. Further, in an embodiment, the switching from the first impedance state to the second impedance state may be caused by a disproportionation reaction. Also, in an embodiment, resistance and/or capacitance of the CEM may be substantially different, such as between the first impedance state and the second impedance state, for example.
As also discussed previously, a variable impeder device may comprise a CEM capable of operating in a first impedance state and a second impedance state. In an embodiment, the first impedance state may comprise a lower resistance, lower capacitance state, and the second impedance state may comprise a higher resistance, higher capacitance state. Also, in an embodiment, a change in the capacitance may be dependent on at least one material property associated with the CEM. In an embodiment, the CEM may comprises one or more of: one or more transition metal oxides, one or more rare earth oxides, one or more oxides of one or more f-block elements of the periodic table, one or more rare earth transitional metal oxide perovskites, yttrium, and/or ytterbium. Additionally, in an embodiment, a transition from the first impedance state to the second impedance state of the variable impeder device may depend at least in part on an applied critical bias and a critical current/current density.
In the preceding description, various aspects of claimed subject matter have been described. For purposes of explanation, specifics, such as amounts, systems and/or configurations, as examples, were set forth. In other instances, well-known features were omitted and/or simplified so as not to obscure claimed subject matter. While certain features have been illustrated and/or described herein, many modifications, substitutions, changes and/or equivalents will now occur to those skilled in the art. It is, therefore, to be understood that the appended claims are intended to cover all modifications and/or changes as fall within claimed subject matter.

## Claims

1. A correlated electron switch (CES) device comprising:
first and second terminals; and
a portion of a correlated electron material (CEM) substrate coupled between the first and second terminals, wherein the CEM substrate is non-uniformly doped between the first and second terminals, and at least a portion of the CEM substrate intrinsic,
wherein the CES is capable of being placed in a conductive or low impedance state responsive to a first or second set operation, or an insulative or high impedance memory state responsive to a first or second reset operation, and
wherein the first set operation is asymmetric with the second set operation.

2. The CES device of claim 1, and wherein:
the first set operation is characterized by a first set voltage condition and a first set current condition across the first and second terminals,
the second set operation is characterized by a second set voltage condition and a second set current condition across the first and second terminals,
a polarity of the first set voltage condition is opposite a polarity of the second set voltage condition, and
a magnitude of the first set voltage condition is greater than a magnitude of the second set voltage condition.

3. The CES device of claim 2, wherein a polarity of the first set current condition is opposite a polarity of the second set current condition, and wherein a magnitude of the first set current condition is greater than a magnitude of the second set current condition.

4. The CES device of claim 1, wherein the first reset operation is asymmetric with the second reset operation.

5. The CES device of claim 4, wherein the first reset operation is characterized by a first reset voltage condition and a first reset current condition across the first and second terminals, and the second reset condition is characterized by a second reset voltage condition and a second reset current condition across the first and second terminals, and
wherein a polarity of the first reset voltage condition is opposite a polarity of the second reset voltage condition, and wherein a magnitude of the first reset voltage condition is greater than a magnitude of the second reset voltage condition.

6. The CES device of claim 5, wherein a polarity of the first reset current condition is opposite a polarity of the second reset current condition, and wherein a magnitude of the first reset current condition is greater than a magnitude of the second reset current condition.

7. The CES device of claim 1, wherein the CES device is configurable to be in the conductive or low impedance state, or the insulative or high impedance state based, at least in part, on a screening length of CEM of the CEM substrate and responsive to localization properties of electrons in the CEM.

8. A method comprising:
forming first and second terminals on at least a portion of a correlated electron material (CEM) substrate to form a correlated electron switch (CES), wherein the CES is capable of being placed in a conductive or low impedance state responsive to a first or second set operation, or an insulative or high impedance memory state responsive to a first or second reset operation;
maintaining at least a portion of the CEM substrate intrinsic; and
affecting a structure or composition of the CEM substrate such that the first set operation is asymmetric with the second set operation by applying a P-type doping or an N-type doping over at least a portion of the CEM substrate.

9. The method of 8, wherein the CEM substrate comprises a transition metal oxide.

10. The method of claim 8, wherein affecting the structure or composition of the CEM substrate further affects the structure or composition of the CEM substrate such that the first reset operation is asymmetric with the second reset operation.

11. The method of claim 8, wherein affecting the structure or composition of the CEM substrate further comprises affecting a concentration of doping over at least a portion of the CEM substrate according to a gradient.

12. The method of claim 8, wherein the CES is configurable to be in the conductive or low impedance state, or the insulative or high impedance state based, at least in part, on a screening length of CEM of the CEM substrate and responsive to localization properties of electrons in the CEM.