Abstract:
A spin accumulation sensor having a three terminal design that allows the free layer to be located at the air bearing surface. A non-magnetic conductive spin transport layer extends from a free layer structure (located at the ABS) to a reference layer structure removed from the ABS. The sensor includes a current or voltage source for applying a current across a reference layer structure. The current or voltage source has a lead that is connected with the non-magnetic spin transport layer and also to electric ground. Circuitry for measuring a signal voltage measures a voltage between a shield that is electrically connected with the free layer structure and the ground. The free layer structure can include a spin diffusion layer that ensures that all spin current is completely dissipated before reaching the lead to the voltage source, thereby preventing shunting of the spin current to the voltage source.

Description:
FIELD OF THE INVENTION 
       [0001]    The present invention relates to magnetoresistive sensors and more particularly to a spin accumulation sensor having a three terminal configuration and a spin diffusion layer allowing the practical application of the spin accumulation sensor in a data recording system. 
       BACKGROUND OF THE INVENTION 
       [0002]    The heart of a computer&#39;s long term memory is an assembly that is referred to as a magnetic disk drive. The magnetic disk drive includes a rotating magnetic disk, write and read heads that are suspended by a suspension arm adjacent to a surface of the rotating magnetic disk and an actuator that swings the suspension arm to place the read and write heads over selected circular tracks on the rotating disk. The read and write heads are directly located on a slider that has an air bearing surface (ABS). The suspension arm biases the slider toward the surface of the disk, and when the disk rotates, air adjacent to the disk moves along with the surface of the disk. The slider flies over the surface of the disk on a cushion of this moving air. When the slider rides on the air bearing, the write and read heads are employed for writing magnetic transitions to and reading magnetic transitions from the rotating disk. The read and write heads are connected to processing circuitry that operates according to a computer program to implement the writing and reading functions. 
         [0003]    The write head has traditionally included a coil layer embedded in first, second and third insulation layers (insulation stack), the insulation stack being sandwiched between first and second pole piece layers. A gap is formed between the first and second pole piece layers by a gap layer at an air bearing surface (ABS) of the write head and the pole piece layers are connected at a back gap. Current conducted to the coil layer induces a magnetic flux in the pole pieces which causes a magnetic field to fringe out at a write gap at the ABS for the purpose of writing the aforementioned magnetic transitions in tracks on the moving media, such as in circular tracks on the aforementioned rotating disk. 
         [0004]    In present read head designs, a TMR sensor is employed for sensing magnetic fields from the rotating magnetic disk. The sensor includes a tunneling barrier layer, sandwiched between first and second ferromagnetic layers, referred to as a reference and a free layer. First and second leads are connected to the sensor for applying a sense voltage across the barrier. The magnetization of the reference layer is fixed perpendicular to the air bearing surface (ABS) and the magnetization of the free layer is oriented parallel to the ABS, but free to rotate in response to external magnetic fields. The magnetization of the reference layer is fixed by either direct exchange-pinning with an antiferromagnetic layer, or by strong antiferromagnetic coupling to a third ferromagnetic “pinned” layer which is exchange-pinned by an antiferromagnetic layer. 
         [0005]    When the magnetizations of the reference and free layers are parallel with respect to one another, tunneling current across the barrier is maximized. When the magnetizations of the reference and free layer are antiparallel, tunneling current is minimized. The change in conductance of the TMR varies as cos θ, where θ is the angle between the magnetizations of the reference and free layers. In a read mode the resistance of the TMR sensor changes proportionally to the magnitudes of the magnetic Fields from the rotating disk. When a sense voltage is applied to the TMR sensor, resistance changes cause current changes that are detected and processed as playback signals. 
         [0006]    More recently researchers have developed perpendicular magnetic recording systems. Older longitudinal recording system, such as one that incorporates the write head described above, stores data as magnetic bits oriented longitudinally along a track in the plane of the surface of the magnetic disk. This longitudinal data bit is recorded by a fringing field that forms between the pair of magnetic poles separated by a write gap. 
         [0007]    A perpendicular recording system, by contrast, records data as magnetizations oriented perpendicular to the plane of the magnetic disk. The magnetic disk has a magnetically soft underlayer covered by a thin magnetically hard top layer. The perpendicular write head has a write pole with a very small cross section and a return pole having a much larger cross section. A strong, highly concentrated magnetic field emits from the write pole in a direction perpendicular to the magnetic disk surface, magnetizing the magnetically hard top layer. The resulting magnetic flux then travels through the soft underlayer, returning to the return pole where it is sufficiently spread out and weak that it will not erase the signal recorded by the write pole when it passes back through the magnetically hard top layer on its way back to the return pole. While the advent of perpendicular magnetic data recording systems have provided advances in increasing data density, still further increases in data density are needed. 
         [0008]    As the areal density of recording increases, the size of the read sensor decreases. Read sensor technology such as TMR was introduced when the technology preceding it was not able to deliver the necessary signal and signal-to-noise ratio al the necessarily smaller sensor sizes. Similarly, TMR read sensors may find a limited range of device size (and hence limited areal density) below which it too may be inadequate to achieve necessary signal-to-noise performance. 
       SUMMARY OF THE INVENTION 
       [0009]    The present invention provides a spin accumulation read head sensor that has a three terminal design that allows the free layer to be located at the air bearing surface without unnecessary shunting of spin current, interference with the hard bias stabilization, or the fabrication difficulty of establishing a fourth contact at or near the air bearing surface. The sensor includes a reference layer structure located away from the air bearing surface and a free layer structure located at the air bearing surface. An internal non-magnetic, conductive spin-transport conducting layer extends from the reference layer structure to the free layer structure. For the present invention, removing the reference layer structure from the ABS allows its size to be substantially larger than that of the free layer structure, thereby reducing technical difficulties and signal-to-noise degradation associated with scaling down the size of the reference layer structure concomitantly with the free layer as required to achieve increased areal recording density. 
         [0010]    A current or voltage source applied across the reference layer structure through a second lead connection results in spin-polarized electrical current through the reference layer which returns to a first current lead that is connected to a common “ground” connection. Simultaneously, a pure spin current can flow from the reference layer structure to and through the free layer structure through the aforementioned conductive spin-transport conducting layer. If the spin-conductance through the free layer is dependent on the orientation of the free layer magnetization relative to that of the reference layer, a (voltage sensing) amplifier connected to ground on one side, and to a third lead connection that is in electrical contact with the free-layer structure, can then detect a change in voltage generated across the free layer structure when the spin-current is modulated by the rotation of the free layer magnetization in response to magnetic signal fields from the rotating magnetic disk. For example, the conventional top and bottom magnetic shields of the read head can act as either of the first/ground and third lead connections (one shield being ground while the other is the third lead), such that the signal voltage is the measured electric potential difference between top and bottom shields, as is typically the case for a TMR sensor. However, because the third lead connection is the only external electrical connection to the free layer structure in the three-terminal design of the present invention, none of the spin current from the reference layer reaching the free layer structure will be otherwise shunted into a fourth lead connection to the opposite side of the free layer structure that is electrically connected to the third lead. In prior art spin accumulation devices a fourth lead is present and shunts some of the spin current, reducing the signal. 
         [0011]    The free layer structure can include an insulating layer on that side (top or bottom) opposite to that electrically connected to the third lead, to keep it electrically insulated from direct contact to the shield layer serving as the first/ground lead connection. The free layer structure can also include a spin diffusion layer between the free layer and the shield acting as the third lead connection. This spin diffusion layer can be constructed of a metallic conductor having a short spin diffusion length, such as Pt, Ir or Re, and acts to diffuse the spin polarity of the spin current before it reaches the shield. This prevents the direction of the shield magnetization from playing the role of a second reference layer in influencing the spin-conductance through the free layer structure. 
         [0012]    These and other features and advantages of the invention will be apparent upon reading of the following detailed description of preferred embodiments taken in conjunction with the Figures in which like reference numerals indicate like elements throughout. 
     
    
     
       BRIEF DESCRIPTION OF THE DRAWINGS 
         [0013]    For a fuller understanding of the nature and advantages of this invention, as well as the preferred mode of use, reference should be made to the following detailed description read in conjunction with the accompanying drawings which are not to scale. 
           [0014]      FIG. 1  is a schematic illustration of a disk drive system in which the invention might be embodied; 
           [0015]      FIG. 2  is a side cross sectional view of a prior art spin accumulation device; 
           [0016]      FIG. 3  is a top down view of the prior art spin accumulation device as viewed from line  3 - 3  of  FIG. 2 ; 
           [0017]      FIG. 4  is a side cross sectional view of a spin accumulation sensor according to an embodiment of the present invention; and 
           [0018]      FIG. 5  is a top down sectional view of the spin accumulation sensor as viewed from line  5 - 5  of  FIG. 4 . 
       
    
    
     DETAILED DESCRIPTION OF THE EMBODIMENTS 
       [0019]    The following description is of the best embodiments presently contemplated for carrying out this invention. This description is made for the purpose of illustrating the general principles of this invention and is not meant to limit the inventive concepts claimed herein. 
         [0020]    Referring now to  FIG. 1 , there is shown a disk drive  100  embodying this invention. As shown in  FIG. 1 , at least one rotatable magnetic disk  112  is supported on a spindle  114  and rotated by a disk drive motor  118 . The magnetic recording on each disk is in the form of annular patterns of concentric data tracks (not shown) on the magnetic disk  112 . 
         [0021]    At least one slider  113  is positioned near the magnetic disk  112 , each slider  113  supporting one or more magnetic head assemblies  121 . As the magnetic disk rotates, slider  113  moves radially in and out over the disk surface  122  so that the magnetic head assembly  121  may access different tracks of the magnetic disk where desired data are written. Each slider  113  is attached to an actuator arm  119  by way of a suspension  115 . The suspension  115  provides a slight spring force which biases slider  113  against the disk surface  122 . Each actuator arm  119  is attached to an actuator means  127 . The actuator means  127  as shown in  FIG. 1  may be a voice coil motor (VCM). The VCM comprises a coil movable within a fixed magnetic field, the direction and speed of the coil movements being controlled by the motor current signals supplied by controller  129 . 
         [0022]    During operation of the disk storage system, the rotation of the magnetic disk  112  generates an air bearing between the slider  113  and the disk surface  122  which exerts an upward force or lift on the slider. The air bearing thus counter-balances the slight spring force of suspension  115  and supports slider  113  off and slightly above the disk surface by a small, substantially constant spacing during normal operation. 
         [0023]    The various components of the disk storage system are controlled in operation by control signals generated by control unit  129 , such as access control signals and internal clock signals. Typically, the control unit  129  comprises logic control circuits, storage means and a microprocessor. The control unit  129  generates control signals to control various system operations such as drive motor control signals on line  123  and head position and seek control signals on line  128 . The control signals on line  128  provide the desired current profiles to optimally move and position slider  113  to the desired data track on disk  112 . Write and read signals are communicated to and from write and read heads  121  by way of recording channel  125 . 
         [0024]      FIG. 2  shows a side cross sectional view of a prior art spin accumulation device. It should be pointed out that the device shown in  FIG. 2  is a theoretical device only, the geometry of which is the natural extrapolation from devices of analogous geometry and equivalent four-terminal electrical connections discussed in the prior art literature. The device suffers from certain challenges (which will be discussed below) that render such a device unsuitable for use in an operational data recording system. 
         [0025]    The device  200  includes a reference magnetic layer  202  and a free magnetic layer  204 . The reference magnetic layer  202  is located a distance away from the free layer  204 , which in a read head would be located at an air bearing surface which is indicated by the dashed line denoted “ABS”. As mentioned before, the reference layer  202  has a magnetization  210  that is fixed in direction, and is typically perpendicular to the ABS. The free magnetic layer  204  would be located with an edge disposed at the ABS. A non-magnetic, conductive spin-transport conducting layer  206  extends from the reference layer  202  to the free layer  204 . The layer  206  should be comprised of electrically conductive material with spin-diffusion length preferably longer than the distance between reference layer  202  and free layer  204 . 
         [0026]    A layer of antiferromagnetic material (AFM layer)  208  can be formed over and exchange coupled with the reference magnetic layer  202 , to pin the magnetization  210  of the reference layer  202  in a desired direction perpendicular to the ABS plane. In addition, a first thin, non-magnetic, contact layer  212  can be provided between the reference layer  202  and the non-magnetic spin-conductive layer  206 . Similarly, a second thin, non-magnetic, contact layer  214  can be provided between the free magnetic layer  204  and the spin-conductive layer  206 . The contact layers  212  and  214  are chosen to promote spin-dependent electrical transport between the spin-conductive layer  206  and the reference layer  202  or the free layer  204 , respectively, and can comprise either electrically conductive metallic-like layers, or tunnel barrier layers analogous to those used for TMR sensors in the prior art. 
         [0027]    As can be seen, the device  200  is a four terminal device. A current source  216  applies an electrical current  218  across the reference layer structure, comprising an electrical contact layer  230 , the AFM layer  208 , reference layer  202 , and contact layer  212 , and which then enters the non-magnetic spin-conductive layer  206 . As mentioned before, the reference layer  202  has a magnetization  210  that is fixed perpendicular to the ABS. Since the contact layer  212  promotes spin-dependent transport, this will result in a spin polarization of the electrons (polarized collinearly with the direction of the magnetization  210 ) which enter the spin-conductive layer  206 . The purely electrical (or charge) component of this spin-polarized current  218  must necessarily return to the current source  216  through the ground connection. However, a pure spin current  220  of this spin-polarized current can additionally flow in the other direction along the spin-conductive layer  206  towards the free layer  204 . Provided the spin diffusion length of spin-conductive layer  206  is comparable to or longer than the distance between reference and free layers, the magnitude (or degree of polarization) of this spin current will be mostly undiminished across this distance, and can possibly flow up through the free layer structure ( 214 ,  204 ,  228 ). If the contact layer  214  promotes spin-dependent transport between conductive layer  206  and the free-layer  204 , a pure spin-current through the free layer structure will generate a purely electrical voltage across the free layer structure which can be detected by a voltage sensing amplifier  224  suitably connected across the free layer structure. 
         [0028]    The free layer  204  has a magnetization that is biased in a direction parallel with the ABS as indicated by arrow head symbol  222 . While this magnetization is biased parallel with the ABS, it is free to rotate in response to an external magnetic field. The biasing for the magnetization  222  is provided by hard magnetic bias layers  302 ,  304 , that can be seen in  FIG. 3 .  FIG. 3  shows a top down view as seen from line  3 - 3  of  FIG. 2 . The hard bias layers  302 ,  304  are magnetostatically coupled with the free layer  204  and are separated from the free layer  204  by thin insulation layers  306 ,  308 . 
         [0029]    The effective spin-impedance of a spin current traversing the contact layer  214  depends upon the orientation of the magnetization  214  relative to the polarization vector of the spin current, which as mentioned above, is determined by the magnetization  210  of the reference layer  202 . The closer the magnetization  222  of the free  204  is to being parallel with the magnetization  210  of the reference layer  202 , the lower the spin-impedance across the contact layer  214  will be. Conversely, the more antiparallel the magnetization  222  is with magnetization  210 , the higher the spin-impedance across the contact layer  214  will be. Therefore, as the magnetization  222  rotates in response to an external magnetic field, the effective spin-impedance across the contact layer  214  will change. The product of the (change in) effective spin-impedance and the magnitude of the spin-current flowing up into the free layer structure determine the signal voltage detected by amplifier  224 . 
         [0030]    The above described structure, however, suffers from drawbacks that have made the implementation of such a device practically impossible. For example, in order for the structure to read the voltage across free layer  204  and second barrier layer  214 , one side of the amplifier  224  must be electrically connected to the conductive layer  206  at a fourth contact point  226 . In practice, the metallization at such a contact point will necessarily be relatively massive compared to the thin spin-conductive layer  206 , and will behave as a perfect “spin-sink” of essentially zero spin-impedance for any spin current reaching contact point  226 . Hence, to avoid shunting essentially all the spin-current away from the free layer structure ( 214 ,  204 ,  228 ) and into the contact point  226 , it would be necessary to keep the location of contact point  226  a distance away from free-layer structure ( 214 ,  204 ,  228 ) that is preferably larger than the spin-diffusion length of layer  206 . Even so, this would only partially alleviate the shunting problem, since the extended region of layer  206  would still act as an alternative, low to moderate spin-impedance shunt path for spin-current to travel away from and bypassing the free-layer structure ( 214 ,  204 ,  228 ), and dissipate (via spin-flip scattering) in this extended region. 
         [0031]    However, this partial Fix regarding a distant location for the contact point  226  is itself virtually impossible in practice. As can be seen, this requires that the layer  206  must extend far beyond the air bearing surface (ABS). This of course is unacceptable in an actual device, because the free layer must be located right at the ABS in order to effectively detect a magnetic signal. In addition, it would be very difficult to extend layer  206  sideways from the free layer structure ( 214 ,  204 ,  228 ) and parallel to the ABS, because these sides of the device are occupied by hard magnetic bias layers  302 ,  304  and insulation layers  306 ,  308  (as shown in  FIG. 3 ) which are needed to bias the magnetization  222  of the free layer. Further yet, the size of the read gap is limited to only a few tens of nanometers in order to meet linear resolution requirements for the read-back signal. Making a fourth electrical contact to the free-layer structure ( 214 ,  204 ,  228 ) at/near the ABS and inside the read gap would be exceedingly difficult. Therefore, there is a need for a structure that can allow a spin accumulation device to be implemented in a functioning data recording system. 
         [0032]    With reference now to  FIG. 4 , a device  400  is provided that includes a reference layer structure  402  located away from an air bearing surface (ABS) and a free layer structure  404  located at the ABS. A non-magnetic, conductive spin-transport conducting layer  406 , which for example can be made of copper, extends from the reference layer structure  402  to the free layer structure  404  and to the ABS. The reference layer structure  402  and free layer structure  404  are separated by a distance that is not greater than, and is preferably less than, the spin diffusion length of the spin-conductive layer  406 . The spin-conductive layer  406  can extend to the Air Bearing Surface (ABS). The reference layer structure  402 , free layer structure  404  and non-magnetic spin-conductive layer  406  are sandwiched between first and second magnetic shields  408 ,  410  which can be constructed of a material such as NiFe, or some other suitable magnetic, electrically conductive material. The non-magnetic spin-conductive layer  406  can be separated from the first shield  408  by an electrically insulating layer  412  such as alumina. A non-magnetic, electrically insulating fill layer  407  such as alumina can be provided to fill the space between the free layer structure  402  and the reference layer structure  404 . 
         [0033]    The reference layer structure  402  includes a ferromagnetic reference layer  414 , which has a magnetization  416  that is fixed in a direction nominally perpendicular to the ABS. The reference layer can be exchange coupled with a layer of antiferromagnetic material (AFM layer  418 ) such as IrMn or PtMn which keeps the magnetization  416  pinned in the desired direction. An electrically conductive lead  420  can be provided over the AFM layer  418 , and is separated from the second shield  410  by an electrically insulating layer  422 . The electrically conductive lead layer  420  can extend out the sides and/or toward the back of the sensor  400  although this is not shown in  FIG. 4 . In addition, because the layers in the reference layer structure  402  are removed from the ABS, they can be made thicker and more numerous than the layers of the free layer structure  404  which are located at the ABS, with no affect on read gap (i.e. linear recording density). Similarly, the layers of the reference layer structure can be made wider in their planar dimensions with no affect on the track-width (i.e., recording track density) resolution of the read head. Therefore, although the free layer structure  404  and reference layer structure  402  are shown being about the same size and thickness, the reference layer structure  402  could be both wider and thicker than the free layer structure  404 . 
         [0034]    The lead  420  can be constructed of an electrically conductive material such as Au, Cu or some other material, and the insulating layer  422  can be alumina or some other electrically insulating material. A thin first contact layer  424  is sandwiched between the reference layer  414  and the non-magnetic spin-conductive layer  406 . The contact layer  424  can be constructed of a tunneling barrier material such as alumina or MgO, a purely metallic layer such as Cu, or a hybrid “nano-oxide” layer consisting of a matrix of small conductive “pinholes” (e.g., Cu) inside an insulating material. The latter can have spin-dependent transport properties similar to a metal contact layer, but with a larger resistance-area product that is more comparable to that of a tunneling barrier. 
         [0035]    The free layer structure  404  includes a magnetic free layer  426  having a magnetization that is biased in a direction nominally parallel with the ABS as indicated by arrow head symbol  428 .  FIG. 5 , shows hard magnetic bias layers  502 ,  504  formed at either side of the free layer  426 . These hard bias layers  502 ,  504  are magnetostatically coupled with the free layer  426  to bias the magnetization  428  parallel with the ABS. The bias layers  502 ,  504  are separated from the free layer structure  402  by insulation layers  506 ,  508 . 
         [0036]    The free layer  426  can be constructed of one or more layers of Co, CoFe, NiFe or some other suitable magnetic material. A second nonmagnetic contact layer  430  is sandwiched between the free layer and the non-magnetic spin-conductive layer  406 . Like the first contact layer  424 , the second contact layer  430  can be constructed of a tunneling barrier material such as alumina or MgO, a purely conductive layer such as Cu, or a hybrid “nano-oxide” layer of a matrix of small conductive “pinholes (e.g., Cu) inside an insulating material. A layer of material having a short spin diffusion length (spin diffusing layer  432 ) is located between the free layer  426  and the second shield layer  410 . This layer can be constructed of a material such as Pt, Ir or Re. The purpose of spin-diffusion layer  432  is to avoid having the direction of the second shield magnetization act as a secondary reference layer in influencing the spin-conductance through the free layer structure. 
         [0037]    With continued reference to  FIG. 4 , a current source  434  is provided to supply a current through the reference layer structure  404 . The current source  434  applies the current via a lead  436  that is connected with the lead layer  420 , and another lead layer  438  that is connected with the non-magnetic metal and also with a ground. The connection with ground can be made at a location far removed from the ABS. 
         [0038]    The application of an electrical current through the reference layer  414  and the first contact layer  424  results in a spin current  405  that travels through the non-magnetic spin-conductive layer  406  toward the ABS and the free layer structure  402 . As the spin current  405  reaches the second contact layer  430 , the effective spin-impedance across contact layer  430  depends upon the relative orientation of the magnetization  428  of the free layer  426  relative to the magnetization  416  of the reference layer  414 . The more parallel the magnetization  428  is with the magnetization  416 , the lower the spin-impedance across the contact  430  will be. Conversely, the more antiparallel the magnetizations  428 ,  416  are, the higher the spin-impedance will be. The product of the effective spin-impedance and the magnitude of the spin-current flowing up into the free layer structure determines the signal voltage detected by amplifier  440 . 
         [0039]    As can be seen, the structure  402  is advantageously configured as a three terminal device rather than a four terminal device. The voltage detected across amplifier  440  is that existing between the electrical contacts to the second shield  410 , and the common ground that the current lead  438  is connected to. In practice, it is convenient to have the first shield  408  electrically connecting to (and/or establishing) this common ground, and then establishing electrical connection  438  by physical contact with shield  408 . This could be done eliminating the insulation layer  412  at some location away from the reference layer structure  402 , and allowing direct electrical contact of conductive layer  406  with the first shield  408 . The location of the establishment of this ground connection should physically be separated from the location of the reference layer structure  402  by one or more times the spin diffusion length of spin-conductive layer  406 . This effectively eliminates as much as possible an undesired, secondary path to for the spin current injected into conductive layer  406  to flow that shunts it away from flowing up and into the free layer structure as is desired. This connection to a common ground can be made at a location that is removed from the ABS, and removed from the spin accumulation device  402 . 
         [0040]    Because no electrical/charge current flows from the reference layer structure  402  towards the free layer structure  404  through the spin-conductive layer  406 , the electrical potential of layer  406  is essentially constant in this region. The electrical potential of layer  406  in this region is similarly independent of the pure spin-current flow through layer  406 , and thus independent of the orientation of magnetization  428  of the free layer. The electrical potential of spin-conductive layer  406  is thus constant with respect to ground potential, the actual value determined by the level of the DC injected current  434  and the static electrical impedance between the reference layer structure  402  and the ground connection  438 . By widening out the shape of the conductive layer  406  in the back end toward ground connection  438 , this static impedance can be made relatively small. Hence, at signal frequencies, the potential of conductive layer  406  below the location of the free layer structure is electrically equivalent to ground. For this reason, measurement via the amplifier  440  of the AC electric signal potential between the second shield  410  and ground is electrically equivalent to a four terminal measurement with a hypothetical, perfectly spin-reflecting fourth terminal connection to layer  406  at or near the air bearing surface. Therefore, the present invention can achieve superior performance to an actual four terminal structure without the drawbacks which would make a physical implementation of a four terminal spin-accumulation sensor a practical impossibility. 
         [0041]    Therefore, the present invention provides several advantages that render the spin accumulation device  402  practical for use in a magnetic data recording system. These include the simpler and practically feasible fabrication of a three terminal electrical configuration, the elimination of signal loss due to spin-current shunting by a physical fourth lead terminal, and no compromise in functionality of the hard bias or narrow gap linear read-back resolution, allowing greater data density than would be otherwise possible if additional lead layers were needed. 
         [0042]    It should be pointed out that the structure shown, for example, in  FIGS. 4 and 5  are for representation purposes only. Other variations would also be possible. For example, although the reference layer structure  402  was shown having the AFM  418  above the reference layer  414 , and the contact layer  424  below the reference layer  414 , this arrangement could be reversed. Similarly, although the free layer structure  404  is shown in  FIG. 4  as having the contact layer  430  below the free layer  426 , the order of these layers could also be reversed or otherwise rearranged. In addition, the spin-conductive layer  406  could be above the reference and free layer structures  402 ,  404  rather than below. Also, the ground connection could be made to the upper shield  410  rather than to the bottom shield  408 , or could be made to some structure other than the shields altogether. Additionally, this device can be used in other applications of sensors able to detect magnetic fields on size scales below a few microns, such as scanning probe apparatus. 
         [0043]    While various embodiments have been described above, it should be understood that they have been presented by way of example only, and not limitation. Other embodiments falling within the scope of the invention may also become apparent to those skilled in the art. Thus, the breadth and scope of the invention should not be limited by any of the above-described exemplary embodiments, but should be defined only in accordance with the following claims and their equivalents.