Abstract:
Embodiments of the invention include a voltage-switching MTJ cell structure that includes two sub-MTJs in series. Each free layer can be switched independently from the other. Each sub-MTJ has a high and a low resistance state and the MTJ cell structure can have three or four discrete resistance states. By taking advantage of the electrical field induced anisotropy combining with the spin torque effect, free layer-1 and free layer-2 can be controlled individually by voltage pulses having selected sign (polarity) and amplitude characteristics. The MTJ cell structure can be used as a fully functional logic cell with two input bit values corresponding to the high or low resistance of the two sub-MTJ structures and the output of a logical operation, e.g. an XOR function, determined by the resistance state of each MTJ cell.

Description:
CROSS REFERENCE TO RELATED APPLICATIONS 
       [0001]    Provisional Application 61/739,716 filed Dec. 19, 2012 is included by reference herein and benefit of the priority date is hereby claimed. The subject matter of this application is related to commonly assigned co-pending applications bearing Ser. No. 13/402,123, filed 22 Feb. 2012 and Ser. No. 13/774,801, filed 22 Feb. 2013. 
     
    
     FIELD OF THE INVENTION 
       [0002]    The present invention relates to the design and use of magnetoresistive random access memory (MRAM) cells that include magnetic tunnel junctions (MTJ) memory elements and more particularly to cells that include more than one free layer that are usable as a multiple level cell (MLC) or logic device. 
       BACKGROUND OF THE INVENTION 
       [0003]    A typical STT-MRAM (spin transfer torque magnetic random access memory) MTJ (magnetic tunnel junction) device has a pinned reference layer whose magnetization is fixed in certain direction by either intrinsic anisotropy field, or through an exchange coupling field from an adjacent magnetic layer. It also has a switchable free layer, whose magnetization direction can be switched in either of two directions relative to that of the reference layer by an electric current flowing between the reference layer and free layer through an junction layer, typically an oxide of Mg, Al and Ti, or a metallic layer of Cu, Au, or Ag. The different relative angles between free layer and reference layer magnetization directions gives different resistance levels through the MTJ stack. Thus, by switching the free layer magnetization directions with the applied electric current, an STT-MRAM can be switched into high and low resistance states. The low resistance state occurs when the magnetization orientation of the two ferromagnetic layers is substantially parallel and the high resistance state occurs when they are anti-parallel. Therefore, the cells have two stable states that allow the cells to serve as non-volatile memory elements. 
         [0004]    Reading the state of the cell is achieved by detecting whether the electrical resistance of the cell is in the high or low state. Writing the cells requires a sufficiently high DC current flowing in the direction through the MTJ stack between the top and bottom metal contacts to induce a spin transfer torque (STT) that orients (switches) the free layer into the desired direction. The amount of current needed to write the cells is higher than the current needed during the read process, so that a read operation does not change the state of the cell. 
         [0005]    A study by Wang, et al. on perpendicular MTJ shows that the perpendicular anisotropy of magnetic layers in MgO based MTJ structures can be changed by the voltage applied to the magnetic layers. See Wei-Gang Wang, et al., “Electric-field-assisted switching in magnetic tunnel junctions”, Nature Materials Vol. 11, 64-68 (2012). Wang, et al. used an example MTJ layer structure (which is illustrated in  FIG. 1  herein) of bottom magnetic layer  43  of CoFeB (1.3 nm), MgO layer  42  (1.4 nm), and top magnetic layer  41  of CoFeB (1.6 nm). In the test setup as shown a small positive DC electric potential is applied to the MTJ cell to drive electrons into the bottom magnetic layer. When MgO layer  42  is thick enough and resistance across the MgO junction is high enough, the current density through the MgO junction will be low. In this case, the two magnetic layers adjacent to the MgO layer form a capacitor across the MgO layer, which is fundamentally the same as a classic parallel-plate capacitor with the MgO layer as the dielectric between the parallel plates. When a voltage is applied to the MgO junction, electrical charges will accumulate in the two magnetic layers, which is governed by the capacitor equation of Q=C×V, where Q is the net charge, C the capacitance and V the applied voltage. The applied positive voltage as shown in  FIG. 1  causes the top magnetic layer to have a positive potential, i.e. electron depletion at the top layer&#39;s interface to the MgO layer and results in the flow of electrons toward the positive potential. Wang&#39;s graph (reproduced in  FIG. 2  herein) shows the coercivity field Hc for the top and bottom layers as a function of the electric field. The perpendicular anisotropy is reflected by the measured coercivity field Hc. With increasing applied voltage and electron depletion at the top layer&#39;s interface to the MgO layer, the top magnetic layer shows increased perpendicular anisotropy. For the magnetic layer with positive potential, the positive charges at its interface with MgO are basically vacancies of conductive electrons that are depleted by the applied voltage. The layer that has negative potential (the bottom layer in this example) and, therefore, conductive electron concentration at the layer&#39;s interface to MgO, shows decreased perpendicular anisotropy. 
         [0006]    The fundamental difference between an MgO junction acting as a capacitor and a standard capacitor is that the electrons at the magnetic layers interface also induce magnetic anisotropy in the magnetic layers. The cited Wang, et al. and Alzate, et al. articles show surface perpendicular anisotropy of CoFeB layers on the sides of the MgO layer is intrinsically due to the broken-symmetry of the interface CoFe lattice of the CoFeB layer facing the MgO layer. See J. G. Alzate, et al., “Voltage-Induced Switching of Nanoscale Magnetic Tunnel Junctions”, IEDM digest, San Francisco, December 2012.  FIGS. 4A and 4B  illustrate the voltage-induced switching principle describe by Alzate, et al. In a perfectly symmetric and continuous lattice of CoFe, the electron-to-electron spin exchange coupling between the un-paired 3d electrons, which are also the conductive electrons, of Co and Fe atoms, cancel out each other&#39;s effect and produce zero anisotropy energy in a symmetric and continuous lattice. However, at the interface of CoFeB layer and MgO layer, the CoFeB layer&#39;s interface is actually CoFe facing MgO. MgO breaks the symmetry of the CoFe lattice, such that the 3d electrons of Co and Fe atoms at the interface lose their cancellation-counter-part and produce a net anisotropy energy and an effective anisotropy field perpendicular to the interface plane. Thus, under these conditions the originally soft magnetic CoFeB film can exhibit strong perpendicular anisotropy at the MgO interface and show hard magnetic behavior. 
         [0007]    Wang, et al. show that with applied voltage, the magnetic layer subjected to a positive potential, i.e. electron depletion at the layer&#39;s interface to MgO, shows increased perpendicular anisotropy. The magnetic layer that experiences a negative potential, i.e. electron concentration at the layer&#39;s interface to MgO, shows decreased perpendicular anisotropy. A possible cause of such behavior is that the magnetic layer having increased electrons will have more conductive electrons filling into the 3d-band of the interface CoFe lattice and reduced unpaired 3d-electron population; thus making the broken-symmetry induced surface perpendicular anisotropy weaker and making the magnetic layer magnetically softer. For the magnetic layer having 3d-electrons depleted, electrons will be first depleted from paired 3d-electrons due to Hund&#39;s Rules. More 3d-electrons become unpaired, which enhances the surface perpendicular anisotropy and makes the layer harder to switch by external field or STT. 
         [0008]    The voltage-induced perpendicular anisotropy effect can be used to switch MTJ by combination with spin transfer torque effect. Using an in-plane MTJ, for example, by applying a positive voltage across MTJ, which depletes electron from the free layer/MgO interface, a strong perpendicular anisotropy on the free layer will be induced, and therefore, reduce its coercivity and make it easier to switch. While the coercivity is reduced, the free layer magnetization can be set/switched with a smaller magnetic field than is needed under static conditions. It has been shown that this small magnetic field can be replaced by a field-like STT generated by the current flowing through the MTJ. A field-like STT will tend to set the MTJ to anti-parallel direction with a low applied voltage. At high applied voltage, the field-like STT will switch its direction and tend to set the MTJ to parallel direction. Therefore, the MTJ can be selectively switched in either direction with a voltage applied in a unipolar direction depending on the pulse amplitude. 
       SUMMARY OF THE INVENTION 
       [0009]    Embodiments of the invention include a voltage-switching MTJ cell structure that includes two free magnetic layers and one fixed magnetic layer separated by junction layers, which will also be generally referred to a magnetoresistive logic cell (MRLC). Both perpendicular and in-plane anisotropy embodiments are described. Embodiments of the MTJ cell structure in effect include two MTJs, which will be called sub-MTJs) in series that each include a free layer, a junction layer and the shared fixed magnetic layer. Although the preferred embodiments use a shared fixed layer, alternative embodiments that use two separate fixed layers instead of a shared fixed magnetic layer are possible. Each free layer can be switched independently from the other. Each sub-MTJ has a high and a low resistance state. The overall resistance of the MTJ cell structure is the combination of the resistance of the two sub-MTJs. If the sub-MTJs have different high and low resistance values, the MTJ cell structure can have four discrete resistance states. If the sub-MTJs have equal high and low resistance values, the MTJ structure will have only three discrete resistance states. 
         [0010]    Embodiments of the invention also include a method to set the magnetization direction, i.e. write or program, either free layer-1 or free layer-2 independently and deterministically in either magnetization direction. By taking advantage of the electrical field induced anisotropy combining with the spin torque effect, free layer-1 and free layer-2 can be controlled individually by voltage pulses having selected sign (polarity) and amplitude characteristics. The sign of the voltage pulse determines the direction of electron flow and, therefore, which of the two free layers will have an accumulation of electrons and which one will have a depletion of electrons. For example, in a perpendicular anisotropy embodiment of the invention, application of a voltage pulse will cause one of the free layers to have reduced perpendicular anisotropy, due to the accumulation of electrons at the junction interface, making it easier to switch. At the same time, the other free layer will have enhanced perpendicular anisotropy, due to the depletion of electrons at the junction interface, making it harder to switch. Temporarily creating a differential in the anisotropies, allows a properly selected pulse to switch the magnetization of one free layer while leaving the other one unchanged. The amplitude of the pulse can be selected to set the magnetization of the targeted free layer to either parallel or anti-parallel the magnetization of the fixed layer. For example, in an embodiment a relatively low amplitude positive voltage pulse can be used to set free layer-1 to the anti-parallel direction with respect to the fixed layer. Similarly, a relatively high amplitude negative voltage pulse can be used to set free layer-2 to the parallel direction with respect to the fixed layer. Thus, in embodiments of the invention a set of four selected types of pulses can be used to program the MTJ cell into the four available states. The three or four resistance-state MTJ structure can be used as a fully functional logic cell, which usually requires a much more complicated and bulky circuitry if realized entirely by conventional CMOS circuits. Input circuitry writes two input bit values into an MTJ cell by setting the high or low resistance of first and second sub-MTJ structures. Output circuitry determines a result of a logical operation by determining a current resistance state of each MTJ cell, which is mapped to a bit value. For example, in an embodiment using three resistance states of the MTJ structure, bit values (0,1) are assigned to first and second sub-junction resistance states (low, high) as inputs and the output bit value is decoded from the total resistance. The 3 total resistance states (low+low; low+high; high+high) are mapped into a single bit value. For example, one possible mapping is:
       state-1 (low+low)=“0”   state-2 (low+high)=“1”   state-3 (high+high)=“0”
 
Given these encoding assumptions, writing a “0” to both free layers will result in the MTJ structure being in state-1 and yielding a logical output value of “0”. The four possible input combinations and the corresponding output for this example achieve an XOR function. Other encodings and mappings can be used to achieve other logical functions using the MTJ structures according to the invention.
       
 
     
    
     
       BRIEF DESCRIPTION OF THE FIGURES 
         [0014]      FIG. 1  is an illustration of an MTJ layer structure used in a prior art experiment. 
           [0015]      FIG. 2  is a graph of the results of a prior art experiment using the MTJ layer structure of  FIG. 1 . 
           [0016]      FIGS. 3A and 3B  illustrate the voltage-induced switching principle used in the prior art. 
           [0017]      FIGS. 4A and 4B  illustrate the voltage-induced switching principle used in prior art. 
           [0018]      FIG. 5  is an illustration of an MTJ layer structure embodiment of the invention with perpendicular anisotropy. 
           [0019]      FIG. 6  is an illustration of an MTJ layer structure embodiment of the invention with in-plane anisotropy. 
           [0020]      FIGS. 7 and 8  illustrate a method of switching the magnetization of free layer-1 in an MTJ layer structure embodiment of the invention with perpendicular anisotropy. 
           [0021]      FIGS. 9 and 10  illustrate a method of switching the magnetization of free layer-2 in an MTJ layer structure embodiment of the invention with perpendicular anisotropy. 
           [0022]      FIG. 11A  illustrates the sub-junctions in an MTJ layer structure embodiment of the invention. 
           [0023]      FIG. 11B  illustrates the three resistance states in an MTJ layer structure embodiment of the invention in which the sub-junctions have high and low resistance states that are equal. 
           [0024]      FIG. 11C  illustrates the four resistance states in an MTJ layer structure embodiment of the invention in which the sub-junctions have high and low resistance states that are not equal. 
           [0025]      FIGS. 12A and 12B  illustrate a method of switching the magnetization of free layer-1 in an MTJ layer structure embodiment of the invention with in-plane anisotropy. 
           [0026]      FIGS. 13A and 13B  illustrate a method of switching the magnetization of free layer-2 in an MTJ layer structure embodiment of the invention with in-plane anisotropy. 
       
    
    
     DETAILED DESCRIPTION OF THE INVENTION 
       [0027]    In the following description of the embodiments of the invention, reference is made to the accompanying drawings that form a part hereof. The figures discussed herein are not drawn to scale and do not indicate actual or relative sizes. 
         [0028]    The following table shows a comparison of experimental data obtained by the inventors of the present application for embodiments of the invention versus voltage switching data published by Alzate, et al. 2012 cited above for prior art MTJ. The voltage switching MTJ shows a much smaller switching current and therefore needs very small power for cell operation, making it preferred in certain applications. 
         [0000]    
       
         
               
             
               
               
               
             
               
               
               
             
           
               
                 TABLE 1 
               
             
             
               
                   
               
               
                 Voltage Switching Data 
               
             
          
           
               
                   
                 Voltage Switching MTJ 
                   
               
               
                   
                 (based on data 
                 Spin-torque MTJ 
               
               
                   
                 published by Alzate, et 
                 (based on authors&#39; 
               
               
                   
                 al. 2012) 
                 typical device data) 
               
               
                   
                   
               
             
          
           
               
                 R low   
                 100k Ohm 
                 2k Ohm 
               
               
                 R high   
                 180k Ohm 
                 4k Ohm 
               
               
                 TMR 
                 80% 
                 100% 
               
               
                 Switching Current 
                 &lt;10 μA 
                 ~100 μA 
               
               
                 Switching Voltage 
                 400 mV-1 V 
                 300-500 mV 
               
               
                   
               
             
          
         
       
     
         [0029]      FIG. 5  is an illustration of an MTJ layer structure embodiment  50 P of the invention with perpendicular anisotropy. MTJ  50 P includes layers  51 - 55 . Current flow is between top and bottom contacts. Magnetic layers  51 ,  52 ,  55  have magnetization anisotropy perpendicular to the film plane. Magnetic free layer-1  51  serves as data storage layer-1. Magnetic layer  51  can include any of the following elements: Co, Fe, B, Ta, Ti, Ni, Pt, Pd, Cr, Cu, Mg, O, Hf, N, Cr, Mn, Zr, Ir, Si. A multi-layer structure can also be used for magnetic layer  51  that includes laminated magnetic layers and non-magnetic layers, where the magnetic layer(s) can include any of the following elements: Co, Fe, B, Ta, Ti, Ni, Pt, Pd, Cr, Cu, Mg, O, Hf, N, Cr, Mn, Zr, Ir, Si; and where nonmagnetic layer(s) can include any of the following elements: Pt, Pd, Ru, Ta, Ti, Cr, Cu, Mg, Hf, Cr, Mn, Zr, Ir, Si, C, and can also be an oxide of Mg, Al, Zn, Ta, Ti, Cu, Cr. 
         [0030]    Magnetic free layer-2  52  need not be the same material as magnetic layers  51  or  55  but the same set of element/structure choices as given above for layer  51  apply. Junction layer-1  53  should be an oxide layer of Mg, Al, Zn, Ta, Ti, Cu, Cr that give a RA of a minimum of 2 Ωμm 2 . Junction layer-2  54  should be an oxide layer of Mg, Al, Zn, Ta, Ti, Cu, Cr that give a RA of a minimum of 2 Ωμm 2 . Either layer  51  or layer  52 , or both of them, can contain multi-ferroic material or show multi-ferroic behavior. 
         [0031]    Fixed Magnetic layer  55  need not be the same material as magnetic layers  51  or  52 , but the same set of element/structure choices as described above for layer  51  apply. Each of the above mentioned free magnetic layers  51 ,  52  and/or fixed magnetic layer  55  can be a synthetic or multiple layer structure. 
         [0032]      FIG. 6  is an illustration of an MTJ layer structure embodiment  50 H of the invention with in-plane anisotropy. MTJ  50 H includes layers  51 H- 55 H. Magnetic layers  51 H,  52 H,  55 H have magnetization in-plane the film plane, but otherwise the above discussion applies to the layers, materials and structures in MTJ layer structure embodiment  50 H. 
         [0033]      FIGS. 7 and 8  illustrate a method of switching the magnetization of free layer-1  51  in an MTJ layer structure embodiment  50 P of the invention with perpendicular anisotropy. Selectively switching only the magnetization of free layer-1  51  is achieved by applying a selected voltage pulse  62 S or  62 H across the contacts. The double-headed arrow in free magnetic layer  51  indicates that its initial magnetization direction can be either up or down. The final magnetization direction of layer  51  is set relative to magnetization direction of fixed magnetic layer  55 . In this example fixed magnetic layer  55  is shown as having magnetization direction pointing up, but an embodiment with fixed layer  55  being magnetized in the down direction will function according to principles described herein with appropriate adjustments to the directions of the free layers. 
         [0034]    As illustrated in  FIG. 7 , application of voltage pulse  62 S, which has relatively small amplitude, results in setting the magnetization direction of free layer  51  in the anti-parallel direction to the fixed layer  55 . In the case shown in  FIG. 7 , this results in layer  51  being set in the down direction as shown. If alternatively the fixed layer was magnetized in the down direction, then the result would be that layer  51  would be set to the up direction by pulse  62 S. 
         [0035]    The voltage-induced switching principles discussed above apply to the structure  50 P when the selected relatively small voltage pulse  62 S is applied. The exact parameters for the amplitude and duration of the pulses  62 S and  62 H can be determined empirically for a given layer structure such as  50 P. The sign (polarity) of the voltage pulses  62 S,  62 H is selected to cause electrons to flow from free layer-1  51  to free layer-2. Accordingly current flow is from the top contact down, i.e. in the opposite direction to electron flow and the voltage is positive. 
         [0036]    The result of applying pulse  62 S is that the coercivity of free magnetic layer-2  52  is temporarily enhanced and therefore its magnetization direction is more stable and harder to switch. However, the coercivity of free magnetic layer-1  51  is temporarily reduced, making it is easier to switch. The final result is that free layer-1  51  switches if necessary to achieve the antiparallel direction with the fixed layer, but free layer-2  52  does not switch. Thus, free layer-2  52  remains in its initial magnetization direction, which can be up or down, after the pulse  62 S is applied. 
         [0037]    Similarly, applying a selected large amplitude pulse  62 H will switch the free layer-1  51  to the parallel direction in relation to the fixed layer  55  as illustrated in  FIG. 8 , while leaving the state of free layer-2  52  unchanged. 
         [0038]      FIGS. 9 and 10  illustrate a method of switching the magnetization of free layer-2  52  in the MTJ layer structure embodiment  50 P of the invention. Selectively switching only the magnetization of free layer-2  52  is achieved by applying a selected voltage pulse  63 S or  63 H across the contacts. The exact parameters for the amplitude and duration of the pulses  63 S and  63 H can be determined empirically for a given layer structure such as  50 P. In this case the voltage of the pulses is negative to cause electrons to flow from free layer-2  52  to free layer-1  51 . Accordingly current flow is from the bottom contact up, i.e. in the opposite direction to electron flow. Selectively switching only free layer-2  52  is achieved by using electron flow to increase the coercivity of free layer-1 making it temporarily harder to switch. At the same time the coercivity of free layer-2  52  is reduced making it easier to switch. Applying a relatively small amplitude negative pulse switches the free layer-2  52  to parallel the magnetization direction of the fixed layer  55 . Applying a large amplitude negative pulse switches the free layer-2 to anti-parallel the magnetization direction of the fixed layer. 
         [0039]      FIG. 11A  illustrates the sub-junctions  61 ,  62  in an MTJ layer structure embodiment of the invention.  FIG. 11B  illustrates the three resistance states in an MTJ layer structure embodiment of the invention in which the sub-junctions  61 ,  62  have high (R-high) and low (R-low) resistance states that are equal. For this embodiment state-1 as shown occurs when both sub-junction-1  61  and sub-junction-2  62  are in the low resistance state R-low. Accordingly the total resistance for the MTJ layer structure  50 P is the arithmetic sum of the two sub-junction resistances, which in this case is 2*R-low. Similarly state-3 occurs when both sub-junction-1  61  and sub-junction-2  62  are in the high resistance state R-high, which gives a total resistance of 2*R-high for the structure. State-2 occurs when the sub-junctions are in opposite resistance states, i.e., one having R-high and the other having R-low. Thus, state-2 has a total resistance of R-high+R-low. 
         [0040]      FIG. 11C  illustrates the four resistance states in an MTJ layer structure embodiment of the invention in which the sub-junctions have high and low resistance states that are not equal. In this case there are two different low resistance values (R-low-1 and R-low-2) and two different high resistance values (R-high-1 and R-high-2). As shown in  FIG. 11C , state-1 for this case occurs when both sub-junctions are in their low resistance states, yielding a total resistance of R-low-1+R-low-2. State-2 has sub-junction-1 in the low state and sub-junction-2 in the high state yielding a total resistance of R-low-1+R-high-2. Similarly state-3 has sub-junction-1 in the high state and sub-junction-2 in the low state yielding a total resistance of R-high-1+R-low-2. State-4 has a total resistance of R-high-1+R-high-2, which occurs when both sub-junctions are in the high resistance state. The 4 resistance levels need to be well separated to allow for enough sensing margin as required by the sensing circuit. 
         [0041]    The three (or four) resistance states of the MTJ structure can be used as a logic cell with bit values being written to the free layers to set the resistance of the sub-junctions and the logic operation result being read as the total resistance of the structure. In an embodiment using a three resistance states of the MTJ structure, bit values are assigned to sub-junction states as inputs and the output bit value is encoded in the total resistance. In the following example, setting a sub-junction to R-low is defined as writing an input of “0” and setting a sub-junction to R-high is defined as writing an input of “1”. For the three state output case as defined in  FIG. 11B , the mapping in this example is:
       state-1 (2*R-low)=“0”   state-2 (R-high+R-low)=“1”   state-3 (2*R-high)=“0”
 
Given these encoding assumptions, writing a “0” to both free layers will result in the MTJ structure being in state-1 and yielding a logical output value of “0”. The four possible input combinations and the corresponding output are given in the table below:
       
 
         [0000]    
       
         
               
             
               
               
               
               
               
             
               
               
               
               
               
             
           
               
                 TABLE 1 
               
             
             
               
                   
               
               
                 Example of possible input and output state mapping for 3-state 
               
               
                 device achieving a logical XOR function. 
               
             
          
           
               
                   
                 State-1 
                 State-2 
                 State-2 
                 State-3 
               
               
                   
                   
               
             
          
           
               
                 Free Layer 1 
                 0 
                 1 
                 0 
                 1 
               
               
                 Free Layer 2 
                 0 
                 0 
                 1 
                 1 
               
               
                 Output 
                 0 
                 1 
                 1 
                 0 
               
               
                 (Total Resistance) 
                 (2 * R-low) 
                 (R-high + 
                 (R-low + 
                 (2 * R-high) 
               
               
                   
                   
                 R-low) 
                 R-high) 
               
               
                   
               
             
          
         
       
     
         [0045]    In another embodiment, the output mapping can be inverted so that state-1 and state-3 correspond to output value “1” and state-2 is “0”. Given this mapping the logical function becomes XNOR. A four state embodiment can be made to function in essentially the same manner as the 3-state embodiment. 
         [0046]    The in-plane embodiments of the invention can be switched using similar switching scheme as described above for the perpendicular embodiments. The 3 or 4 resistance state-MTJ structure can also be realized with in-plane MTJs.  FIGS. 12A and 12B  illustrate a method of switching the magnetization of free layer-1  51 H in an MTJ layer structure embodiment  50 H of the invention with in-plane anisotropy. Selectively switching free layer-1  51 H only is achieved by applying a positive voltage pulse which causes electrons to move from free layer-1  51 H to free layer-2  52 H, the coercivity of layer  52 H is enhanced therefore it is more stable and harder to switch. At the same time the coercivity of layer  51 H is reduced therefore it is easier to switch. Applying a relatively small amplitude positive pulse  64 S will switch the free layer-1  51 H to the anti-parallel direction with respect to fixed magnetic layer  55 H as illustrated in  FIG. 12A . Applying a relatively large amplitude positive pulse  64 H will cause the free layer-1  51 H to switch to parallel the magnetization direction of fixed magnetic layer  55 H as illustrated in  FIG. 12B . 
         [0047]      FIGS. 13A and 1B  illustrate a method of switching the magnetization of free layer-2  52 H in an MTJ layer structure embodiment of the invention  50 H with in-plane anisotropy. Selectively switching free layer-2  52 H only is achieved by applying a negative voltage pulse which causes electrons to move from free layer-2  52 H to free layer-1  51 H, the coercivity of layer  51 H is enhanced, therefore it is more stable and harder to switch. At the same time the coercivity of layer  52 H is reduced, therefore it is easier to switch. Applying a relatively small amplitude negative pulse  65 S will switch the free layer-2  52 H to the anti-parallel direction with respect to fixed magnetic layer  55 H as illustrated in  FIG. 13A . Applying a relatively large amplitude negative pulse  65 H will cause the free layer-2  52 H to switch to parallel the magnetization direction of fixed magnetic layer  55 H as illustrated in  FIG. 13B . 
         [0048]    Although the present invention has been described in terms of specific embodiments, it is anticipated that alterations and modifications thereof will no doubt be apparent to those skilled in the art. It is therefore intended that the following claims be interpreted as covering all such alterations and modifications as fall within the true spirit and scope of the invention.