Dual free layer magnetic reader having a rear bias structure including a soft bias layer

Description

BACKGROUND

FIG. 1 depicts an air-bearing surface (ABS) view of a conventional read transducer used in magnetic recording technology applications. The conventional read transducer 10 includes shields 12 and 18, insulator 14, magnetic bias structures 16, and sensor 20. The read sensor 20 is typically a giant magnetoresistive (GMR) sensor or tunneling magnetoresistive (TMR) sensor. The read sensor 20 includes an antiferromagnetic (AFM) layer 22, a pinned layer 24, a nonmagnetic spacer layer 26, and a free layer 28. Also shown is a capping layer 30. In addition, seed layer(s) may be used. The free layer 28 has a magnetization sensitive to an external magnetic field. Thus, the free layer 28 functions as a sensor layer for the magnetoresistive sensor 20. If the sensor 20 is to be used in a current perpendicular to plane (CPP) configuration, then current is driven in a direction substantially perpendicular to the plane of the layers 22, 24, 26, and 28. Conversely, in a current-in-plane (CIP) configuration, then conductive leads (not shown) would be provided on the magnetic bias structures 16. The magnetic bias structures 16 are used to magnetically bias the free layer 28.

Although the conventional transducer 10 functions, there are drawbacks. The trend in magnetic recording is to higher density memories. The conventional read sensor 20 may not adequately read high density media. As a result, dual free layer magnetic read sensors have been developed. In such read sensors, two free layers that are biased in a scissor state by a hard magnet. The read sensor may not, however, be reliable in such a conventional magnetic reader. Such reliability issues may become particularly acute at high densities and lower track widths on the order of less than or equal to twenty nanometers. For example, in such high density dual free layer readers, the state in which the free layers are biased may be unpredictable. Accordingly, what is needed is a system and method for improving the performance of a magnetic recording read transducer.

BRIEF DESCRIPTION OF SEVERAL VIEWS OF THE DRAWINGS

FIG. 1 depicts an ABS view of a conventional magnetic recording read transducer.

FIGS. 2A-2C depicts ABS, plan and side views of an exemplary embodiment of a portion of a dual free layer magnetic read transducer.

FIGS. 3A-3B depict plan and side views of another exemplary embodiment of a portion of a dual free layer magnetic read transducer.

FIGS. 4A-4B depict plan and side views of another exemplary embodiment of a portion of a dual free layer magnetic read transducer.

FIGS. 5A-5B depict plan and side views of another exemplary embodiment of a portion of a dual free layer magnetic read transducer.

FIGS. 6A-6B depict plan and side views of another exemplary embodiment of a portion of a dual free layer magnetic read transducer.

FIG. 7 is flow chart depicting an exemplary embodiment of a method for providing a magnetic recording read transducer.

FIG. 8 is flow chart depicting another exemplary embodiment of a method for providing a magnetic recording read transducer.

FIG. 9 is flow chart depicting another exemplary embodiment of a method for providing a magnetic recording read transducer.

DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENTS

FIGS. 2A-2C depict ABS, plan and side views of an exemplary embodiment of a portion of a magnetic read transducer 100. For clarity, FIGS. 2A-2C are not to scale. The read transducer 100 may be part of a read head or may be part of a merged head that also includes a write transducer. The head of which the read transducer 100 is a part is contained in a disk drive having a media, a slider and the head coupled with the slider. Further, only a portion of the components of the read transducer 100 are depicted.

The transducer 100 includes optional soft magnetic shields 102 and 104, insulator 106, read sensor 110, side bias structures 130 and 150 and rear bias structure 160 that may be separated from the read sensor 110 by an insulating layer 155. The read sensor 110 includes a first free layer 112 and a second free layer 116 separated by a nonmagnetic spacer layer 114. The nonmagnetic spacer layer 114 may be conductive or an insulating tunneling barrier layer, such as MgO. The read sensor 110 is, therefore, a giant magnetoresistive or tunneling magnetoresistive read sensor in the embodiment shown. The free layers 112 and 116 are ferromagnetic and may include multiple layers. However, there is no AFM layer or pinned layer in the sensor 110. Instead, the free layers 112 and 116 are biased such that their magnetic moments 113 and 117, respectively are in a scissor mode. Based on the angle between the magnetic moments 113 and 117, the resistance of the read sensor 110 changes. This angle changes when the read 110 is under the influence of an external field, for example due to a bit being read. Thus, the resistance of the read sensor 110 may be used to read data. The read sensor 110 may also be configured for high density recording. Thus, in some embodiments, the track width (TW) of the read sensor 110 is not more than thirty nanometers. In some such embodiments, the track width is not more than twenty nanometers. In the embodiment shown, the shields 102 and 104 and the free layers 112 and 116 all have a stripe height, SH, in the stripe height direction. In other embodiments, however, different structures 102, 104, 112 and 116 may have different stripe heights.

The transducer 100 includes side magnetic bias structures 120 and a rear magnetic bias structure 160 that together magnetically bias the free layers 112 and 116 in a scissor mode. As can be seen in FIGS. 2A and 2B, the side bias structures 120 bias the magnetic moments 113 and 117, respectively, of the free layers 112 and 116, respectively, parallel to the ABS, in the cross-track direction. The magnetic bias structures 120 and free layers 112 and 116 are also configured to bias the magnetic moments 113 and 117 of the free layers 112 and 116, respectively, antiparallel. In some embodiments, the magnetic moments 113 and 117 of the free layers 112 and 116 are antiferromagnetically coupled. The rear magnetic bias structure 160 biases the magnetic moments 113 and 117 of the free layers 112 and 116, respectively, perpendicular to the ABS, in the stripe height direction.

Each bias structure 120 includes two magnetic bias structures 130 and 150 separated by a nonmagnetic structure 140. The first magnetic bias structure 130 magnetically biases the free layer 112 and, therefore, is adjacent to the sides of the free layer in the cross-track direction. Similarly, the second magnetic bias structure 150 magnetically biases the free layer 116 and is thus adjacent to the side of the free layer 116 in the cross-track direction. In the embodiment shown, the top surface of the first magnetic bias structure 130 is not higher than the upper surface of the first free layer 112. However, in other embodiments, the top surface of the magnetic bias structure 130 may be at another location. In some embodiments, the top surface of the first magnetic bias structure 130 is not higher than the lower surface of the second free layer 116. In other embodiments, the top surface of the first magnetic bias structure 130 is not higher than midway between the upper and lower surfaces of the second free layer 116. Although the top of the first magnetic bias structure 130 may be higher than bottom of the second free layer 116, the entire magnetic bias structure 130 is still lower than the second magnetic bias structure 150. Similarly, the bottom surface of the second magnetic bias structure 150 is not lower than the lower surface of the second free layer 116 in the embodiment depicted in FIGS. 2A-2C. However, in other embodiments, the bottom surface of the magnetic bias structure 150 may be at another location. For example, the bottom surface of the second magnetic bias structure 150 may not be lower than the upper surface of the first free layer 112. In other embodiments, the bottom surface of the magnetic structure 150 is not lower than midway between the upper and lower surfaces of the first free layer 112. Although the bottom of the second magnetic bias structure 150 may be lower than upper surface of the first free layer 112, the entire magnetic bias structure 150 is still higher than the first magnetic bias structure 130.

The magnetic bias structures 130 and 150 may take various forms. In some embodiments, both the first magnetic bias structure 130 and the second magnetic bias structure 150 are soft magnetic structures. For example, the magnetic bias structures 130 and 150 may be an alloy, multilayer or other structure that has a coercivity of not more than ten Oe. In some such embodiments, the soft magnetic bias structure(s) 130 and/or 150 have a coercivity of not more than five Oe. For example, the magnetic bias structures 130 and 150 may include CoFe and/or NiFe. In other embodiments, the magnetic bias structures 130 and/or 150 may have different magnetic properties. In some embodiments, the magnetic bias structure 130 and/or 150 may be a hard bias structure. For example, the first magnetic bias structure 130 may be an alloy or multilayer that has a sufficiently high coercivity to have its magnetic moment 132 substantially unchanged during operation of the transducer 100. In other embodiments, the first magnetic bias structure 130 may be a pinned structure. In such an embodiment, the first magnetic bias structure 130 may include a pinning layer, such as an antiferromagnetic (AFM) layer and a soft magnetic layer adjoining the pinning layer. In still other embodiments, the magnetic bias structure 130 and 150 may be configured in another manner. For example, the shield 102 is shown as being overmilled to allow for the soft bias structures 130 and 150. However, in other embodiments, the shield 102 may not be overmilled.

The first magnetic bias structure 130 may have a magnetic moment 132. The second magnetic bias structure 152 may have a magnetic moment 152. As can be seen in FIG. 2B, the magnetic moments 132 and 152 are antiferromagnetically aligned. Stated differently, the steady state orientation of the magnetic moments 132 and 152 is antiparallel. In some embodiments, the bias structures 130 and 150, and thus the magnetic moments 132 and 152, are antiferromagnetically coupled. Because of the orientations of the magnetic moments 132 and 152, the magnetic moment 113 of the first free layer 112 is biased in one direction, while the magnetic moment 117 of the second free layer 116 is biased in the opposite direction.

The magnetic transducer 100 also includes a rear bias structure 160 that is depicted as including soft bias structure 170 and hard bias structure 180. The read sensor 110 is between the rear bias structure 160 and the ABS. Further, an insulating layer 155 may separate the rear bias structure 160 from the sensor 110 and bias structures 120. In addition, although the shields 102 and 104 are shown as extending only to the stripe height of the sensor 110, the shields 102 and 104 generally extend significantly further in the stripe height direction. However, the shields 102 and 104 are also magnetically decoupled from the rear bias structure 160. Thus, the insulating layer 155 and the top insulating (not shown) may extend along the depth of the rear bias structure 160. For example, in some embodiments, the insulating layer 155 is at least ten Angstroms and not more than forty Angstroms thick. The insulating layer 155 is also nonmagnetic. Thus, the read sensor 110 may be electrically insulated from the rear bias structure 160 and not exchanged coupled with the rear soft bias structure 160. Although not depicted in FIGS. 2A-2C, an insulating capping layer may also be provided on top of the rear bias structure 160. In the embodiment shown, a nonmagnetic layer 162 is between the rear soft bias magnetic structure 170 and the rear hard bias structure 180. In other embodiments, the nonmagnetic layer 162 might be omitted. The rear bias structure 160 is shown as extending past the edges of the bias structures 120 closest to the sensor 110 in the cross-track direction. However, in other embodiments, the rear bias structure 160 may extend a different amount in the cross-track direction. Thus, the rear bias structure 160 is adjacent to the rear surface of the read sensor 110. The rear surface of the read sensor 110 is opposite to the ABS-facing surface.

The rear bias structure 160 includes at least a rear soft bias structure 170 and may include a rear hard bias structure 180. The rear soft bias structure 170 is between the rear hard bias structure 180 and the sensor 110 as well as between the rear hard bias structure 180 and the ABS. The rear hard bias structure 180 may be a hard magnetic alloy, for example having a coercivity in excess of two hundred Oersted. In some embodiments, the coercivity is greater than one thousand Oersted. For example, a CoPt alloy might be used. In other embodiments, the rear bias structure 180 may be a multilayer or other structure that functions as a hard bias structure. In other embodiments, the rear hard bias structure 180 may be omitted. The rear hard bias structure 180 has a length l2, a thickness t2 and a depth d2. In some embodiments, the rear hard bias structure 180 is separated from the rear soft bias structure 170 by the nonmagnetic layer 162. The nonmagnetic layer 162 may be conductive. In some embodiments, the thickness of the nonmagnetic layer 162 in the stripe height direction is at least ten Angstroms and not more than forty Angstroms.

The rear soft bias structure 170 has a length l1, a thickness t1 and a depth d1. Although the lengths, depths and thicknesses of the structures 170 and 180 are shown as being the same, in other embodiments, the geometries of the structures 170 and 180 may differ. However, at least the rear soft bias structure 170 is desired to be at least as wide as the track width of the sensor 110 (l1 TW). The rear soft bias structure 170 includes at least one soft material. For example, a soft magnetic alloy such as Ni_1-xFe_x and/or Co_1-yFe_y, where x is at least 0.18-0.20 and y=0.09-0.11, might be used for the rear soft bias structure 170. Thus, the coercivity of the rear soft bias structure 170 is less than one hundred Oersted. In some embodiments, the coercivity of the rear soft bias structure 170 is less than ten Oersted. Further, the rear soft bias structure 170 provides sufficient moment to bias the magnetic moments 113 and 117 of the free layers 112 and 116, respectively. For example, in some embodiments, the rear soft bias structure has a saturation magnetization-thickness product of at least one milli-emu/cm² and not more than three milli-emu/cm². In some such embodiments, the saturation magnetization-thickness product is not more than two milli-emu per cm². The thickness used in the saturation magnetization-thickness product is t1, the depth of the rear soft bias structure 170 in the down track direction. Although shown with rear hard bias structure 180, the rear soft bias structure might be used alone in some embodiments or in conjunction with another mechanism, such as an adjoining antiferromagnetic layer, that biases the magnetic moment 172 as shown.

The rear soft bias structure 170 has a magnetic moment 172 that biases the free layers 112 and 116 in a direction perpendicular to the bias direction from the magnetic bias structures 130 and 150. In the embodiment shown, this direction is perpendicular to the ABS. Similarly, the rear hard bias structure 180 has a magnetic moment 182 in a direction perpendicular to the ABS. Without the rear bias structure 160, the free layers 112 and 116 may be biased antiparallel. However, because the structures 130, 150 and 160 all magnetically bias the free layers 112 and 116, the free layers 112 and 116 are biased such that the magnetic moments 113 and 117 are in a scissor mode.

The magnetic transducer 100 may be suitable for use in high density magnetic recording applications, for example those having a sensor track width of not more than thirty nanometers. The read sensor 110 does not include an antiferromagnetic layer or a pinned layer. Consequently, the shield-to-shield spacing (S) between the shields 102 and 104 may be reduced. The use of the scissor mode may also enhance the read signal. This scissor mode may be more reliably achieved because of the presence of the soft bias structure 170. If the hard bias structure 180 is used alone, the hard bias structure 180 is subject to clustering of the permanent magnet materials. Although the overall magnetic moment 182 of the rear hard bias structure 180 is out of the ABS, as shown in FIGS. 2B and 2C, individual clusters may have their magnetic moments aligned in a different direction. For example, the magnetic moment of a cluster may be substantially parallel to the ABS or antiparallel to the magnetic moment 182. These clusters may be on the order of the size of the track width for lower track widths/high density recording applications. The cluster(s) aligned with the read sensor in the cross-track direction may be magnetized in a direction other than the desired direction of the magnetic moment 182. Thus, the read sensor 110 would not be biased as desired. Use of the rear soft bias structure 170 addresses this issue. The rear soft bias structure 170 may be seen as smoothing out the variations in magnetization due to clustering of the rear hard bias structure 180. This is because the rear soft bias structure 170 may not be subject to such clustering. When used without the rear hard bias structure 180, the rear soft bias structure 170 may still bias the free layers 112 and 116 in a direction perpendicular to the ABS. The desired scissor mode may be achieved and performance may be improved.

FIGS. 3A and 3B depict various views of another embodiment of a magnetic read transducer 100′. FIG. 3A depicts a plan view of an exemplary embodiment of the transducer 100′. FIG. 3B depicts a side view of the transducer 100′. For clarity, FIGS. 3A and 3B are not to scale. The read transducer 100′ may be part of a read head or may be part of a merged head that also includes a write transducer. The head of which the read transducer 100′ is a part is part of a disk drive having a media, a slider and the head coupled with the slider. The transducer 100′ corresponds to the transducer 100. Consequently, analogous components are labeled similarly. For example, the transducer 100′ includes a read sensor 110 having free layers 112 and 116 separated by a nonmagnetic spacer layer 114 that are analogous to such structures in the transducer 100. Thus, the components 102, 104, 110, 112, 114 116, 155, 160′ and 170′ have a similar structure and function to the components 102, 104, 110, 112, 114 116, 155, 160 and 170, respectively, depicted in FIGS. 2A-2C. Further, although an ABS view is not shown, the transducer 100′ may appear substantially the same from the ABS as the transducer 100. The transducer 100′ may also include structures analogous to the structures 120, 130, 140 and 150 depicted in FIGS. 2A-2C.

In the embodiment shown in FIGS. 3A-3B, the rear hard bias structure 180 has been omitted. In some embodiments, an antiferromagnetic layer or other biasing mechanism could also be included. For example, an antiferromagnetic layer may reside above or below (in the down track direction from) and adjoin the rear soft bias structure 170′, may be behind (in the stripe height direction from) and adjoin the rear soft bias structure 170′ or both. In such embodiments, the additional biasing mechanism may bias (or assist in biasing) the magnetization 172′ of the rear soft bias structure 170′ to be stable as shown. In other embodiments, only the rear soft bias structure 170′ might be present. Thus, the rear bias structure 160′ consists of the rear soft bias structure 170′. In such embodiments, the rear soft bias structure 170′ may be configured such that the magnetization 172′ is stable perpendicular to the ABS. For example, the rear soft bias structure 170′ may have an anisotropy such that the magnetization 172′ is stable during operation of the magnetic read transducer 100′. For example, a crystalline and/or shape anisotropy may be used to stabilize the magnetization 172′. In some embodiments, the depth, d1′, of the rear soft bias structure 170′ may be much greater than the length, l1, or height, t1, of the rear soft bias structure. In the embodiment shown, the height, t1, of the rear soft bias structure is shown as the same as that of the read sensor 110. The rear soft bias structure 170′ is also shown as having a length, l1, greater than the track width but not extending to the edges of the side bias structures 120 in the cross-track direction. In other embodiments, other geometries are possible. However, the rear soft bias structure 170′ is still desired to be at least as wide as the sensor 110 (l1≧TW).

The magnetic transducer 100′ shares the benefits of the magnetic transducer 100. Performance and biasing of the sensor 110 may thus be improved. Further, processing might be simplified by the omission of the hard bias structure 180 and layer 162 separating the soft bias structure 170′ from a hard bias structure.

FIGS. 4A and 4B depict various views of another embodiment of a magnetic read transducer 100″. FIG. 4A depicts a plan view of an exemplary embodiment of the transducer 100″. FIG. 4B depicts a side view of the transducer 100″. For clarity, FIGS. 4A and 4B are not to scale. The read transducer 100″ may be part of a read head or may be part of a merged head that also includes a write transducer. The head of which the read transducer 100″ is a part is part of a disk drive having a media, a slider and the head coupled with the slider. The transducer 100″ corresponds to the transducer(s) 100 and/or 100′. Consequently, analogous components are labeled similarly. For example, the transducer 100″ includes a read sensor 110 having free layers 112 and 116 separated by a nonmagnetic spacer layer 114 that are analogous to such structures in the transducer(s) 100 and/or 100′. Thus, the components 102, 104, 110, 112, 114 116, 155, 160″, 170″ and 180′ have a similar structure and function to the components 102, 104, 110, 112, 114 116, 155, 160/160′, 170/170′ and 180, respectively, depicted in FIGS. 2A-2C and 3A-3B. Further, although an ABS view is not shown, the transducer 100″ may appear substantially the same from the ABS as the transducer 100. The transducer 100″ may also include structures analogous to the structures 120, 130, 140 and 150 depicted in FIGS. 2A-2C.

In the embodiment shown in FIGS. 4A-4B, the rear hard bias structure 180′ and rear soft bias structure 170″ have different geometries. In addition, the nonmagnetic layer 162 shown in FIGS. 2A-2C has been omitted. In the embodiment shown, the rear soft bias structure 170″ has a length, l1′ in the cross track direction, while the hard bias structure 180′ has length l2′ in the cross track direction. Thus, the rear hard bias structure 180′ is wider than the rear soft bias structure 170″. The thicknesses, t1 and t2, of the bias structures 170″ and 180′ are shown as the same. However, in other embodiments, the thicknesses may differ. In addition, it is noted that the interface between the rear soft bias structure 170″ and the rear hard bias structure 180′ is not parallel to the ABS. This is because during fabrication, the rear soft bias structure 170″ may be ion milled to allow for refill with the material(s) for the rear hard bias structure 180′. Although not shown in the remaining drawings, this angle may be present in other embodiments. The rear bias structures 170″ and 180′ still have their magnetic moments 172″ and 182′, respectively, perpendicular to the ABS to bias the free layers 112 and 116 into a scissor state.

The magnetic transducer 100″ shares the benefits of the magnetic transducer(s) 100 and/or 100′. Further, omission of a nonmagnetic layer between the soft bias structure 170″ and the hard bias structure 180′ may improve coupling between the structures 170″ and 180′. Performance and biasing of the sensor 110 may thus be improved.

FIGS. 5A and 5B depict various views of another embodiment of a magnetic read transducer 100′″. FIG. 5A depicts a plan view of an exemplary embodiment of the transducer 100′″. FIG. 5B depicts a side view of the transducer 100′″. For clarity, FIGS. 5A and 5B are not to scale. The read transducer 100′″ may be part of a read head or may be part of a merged head that also includes a write transducer. The head of which the read transducer 100′″ is a part is part of a disk drive having a media, a slider and the head coupled with the slider. The transducer 100′″ corresponds to the transducer(s) 100, 100′ and/or 100″. Consequently, analogous components are labeled similarly. For example, the transducer 100′″ includes a read sensor 110 having free layers 112 and 116 separated by a nonmagnetic spacer layer 114 that are analogous to such structures in the transducer(s) 100, 100′ and/or 100″. Thus, the components 102, 104, 110, 112, 114 116, 155, 160′″, 162, 170′″ and 180″ have a similar structure and function to the components 102, 104, 110, 112, 114 116, 155, 160/160′/160″, 162, 170/170′/170″ and 180/180′, respectively, depicted in FIGS. 2A-2C, 3A-3B and 4A-4B. Further, although an ABS view is not shown, the transducer 100′″ may appear substantially the same from the ABS as the transducer 100. The transducer 100′″ may also include structures analogous to the structures 120, 130, 140 and 150 depicted in FIGS. 2A-2C.

In the embodiment shown in FIGS. 5A-5B, the rear hard bias structure 180″ and rear soft bias structure 170′″ have different geometries. In the embodiment shown, the rear soft bias structure 170′″ has a length, l1″ in the cross track direction, while the hard bias structure 180″ has length l2″ in the cross track direction. Thus, the rear hard bias structure 180″ is wider than the rear soft bias structure 170′″. Further, both structures 170′″ and 180″ extend further in the cross-track direction than the side bias structures 120. The thicknesses, t1 and t2′, of the bias structures 170′″ and 180″ also differ. The rear bias structures 170′″ and 180″ still have their magnetic moments 172′″ and 182″, respectively, perpendicular to the ABS to bias the free layers 112 and 116 into a scissor state.

The magnetic transducer 100′″ shares the benefits of the magnetic transducer(s) 100, 100′ and/or 100″. Performance and biasing of the sensor 110 may thus be improved.

FIGS. 6A and 6B depict various views of another embodiment of a magnetic read transducer 100″″. FIG. 6A depicts a plan view of an exemplary embodiment of the transducer 100″″. FIG. 6B depicts a side view of the transducer 100″″. For clarity, FIGS. 6A and 6B are not to scale. The read transducer 100″″ may be part of a read head or may be part of a merged head that also includes a write transducer. The head of which the read transducer 100″″ is a part is part of a disk drive having a media, a slider and the head coupled with the slider. The transducer 100″″ corresponds to the transducer(s) 100, 100′, 100″ and/or 100′″. Consequently, analogous components are labeled similarly. For example, the transducer 100″″ includes a read sensor 110 having free layers 112 and 116 separated by a nonmagnetic spacer layer 114 that are analogous to such structures in the transducer(s) 100, 100′, 100″ and/or 100′″. Thus, the components 102, 104, 110, 112, 114 116, 155, 160″″, 170′″ and 180″ have a similar structure and function to the components 102/102′, 104, 110, 112, 114 116, 155, 160/160/160″/160′″, 170/170/170″/170′″ and 180/180′, respectively, depicted in FIGS. 2A-2C, 3A-3B, 4A-4B and 5A-5B. Further, although an ABS view is not shown, the transducer 100″″ may appear substantially the same from the ABS as the transducer 100. The transducer 100″″ may also include structures analogous to the structures 120, 130, 140 and 150 depicted in FIGS. 2A-2C.

In the embodiment shown in FIGS. 6A-6B, the rear soft bias structure 170″″ and the rear hard bias structure 180′″ share an interface (i.e. nonmagnetic layer 162 is omitted). The rear bias structures 170″″ and 180″ also share geometries (l1′″=l2″, t1=t2, d1=d2). In other embodiments, the geometries may differ. The rear bias structures 170″″ and 180′″ still have their magnetic moments 172″″ and 182′″, respectively, perpendicular to the ABS to bias the free layers 112 and 116 into a scissor state.

The magnetic transducer 100″″ shares the benefits of the magnetic transducer(s) 100, 100′, 100″ and/or 100′″. Performance and biasing of the sensor 110 may thus be improved.

The magnetic transducers 100, 100′, 100″, 100′″ and 100′″ have been shown with various configurations to highlight particular features, such as differences in geometries. One of ordinary skill in the art will readily recognize that two or more of these features may be combined in various manners consistent with the method and system described herein that are not explicitly depicted in the drawings.

FIG. 7 is an exemplary embodiment of a method 200 for providing a read transducer. For simplicity, some steps may be omitted, interleaved, combined, have multiple substeps and/or performed in another order unless otherwise specified. The method 200 is described in the context of providing a magnetic recording disk drive and transducer 100. However, the method 200 may be used in fabricating the transducer 100′, 100″, 100′″ and/or 100″″. The method 200 may be used to fabricate multiple magnetic read heads at substantially the same time. The method 200 may also be used to fabricate other magnetic recording transducers. The method 200 is also described in the context of particular layers. A particular layer may include multiple materials and/or multiple sub-layers. The method 200 is described in the context of a disk drive. However, the method may be used in other applications employing a magnetoresistive and bias structures. The method 200 also may start after formation of other portions of the magnetic recording transducer.

The read sensor 110 is provided, via step 202. Step 202 may include depositing a stack of layers for the read sensor and defining the read sensor in the cross-track and stripe height directions. Further, the shield 102 and insulating layer 106 may also be provided. The side bias structures 120 are provided, via step 204. Step 204 is performed after the read sensor is defined in the cross-track direction. Thus, at least part of step 202 is performed before step 204. Step 204 may include depositing the insulating layer 106, depositing the material(s) for the magnetic bias structures 130 and 170, depositing the nonmagnetic layer 140. A mill step and planarization, such as a chemical mechanical planarization (CMP) may also be performed.

The rear bias structure 160 is provided, via step 208. Step 208 may be performed after the sensor 110 has been defined in at least the stripe height direction. Step 208 includes providing at least the soft bias structure 170. The hard bias structure 180 and optional nonmagnetic layer 162 may also be provided in step 206.

Using the method 200, the transducers 100, 100′, 100″, 100′″ and/or 100″″ may be fabricated. Thus, the benefits of one or more of the transducers 100, 100′, 100″, 100′″, and/or 100″″ may be achieved. Consequently, biasing of the free layers 112 and 116 in the read sensor 110 may be improved.

FIG. 8 is an exemplary embodiment of a method 210 for providing a rear bias structure of a read transducer. For simplicity, some steps may be omitted, interleaved, combined, have multiple substeps and/or performed in another order unless otherwise specified. The method 210 is described in the context of providing a magnetic recording disk drive and transducer 100. However, the method 210 may be used in fabricating the transducer 100′, 100″, 100′″ and/or 100″″. The method 210 may be used to fabricate multiple magnetic read heads at substantially the same time. The method 210 may also be used to fabricate other magnetic recording transducers. The method 210 is also described in the context of particular layers. A particular layer may include multiple materials and/or multiple sub-layers. The method 210 is described in the context of a disk drive. However, the method may be used in other applications employing a magnetoresistive and bias structures. The method 210 also may start after formation of other portions of the magnetic recording transducer.

The rear soft bias structure 170 is provided, via step 212. Step 212 may include depositing the layer(s) for the rear soft bias structure 170. In addition, the rear soft bias structure 170 may be defined in the stripe height direction. Thus, space may be made for the hard bias structure 180. Defining the soft bias structure 170 in the stripe height direction may include masking and ion milling the material(s) that have been deposited. In some embodiments, the length of the rear soft bias structure 170 in the cross-track direction may also be defined. This may occur when the soft bias structure 170 and the hard bias structure 180 are desired to have different lengths in the cross-track direction. In other embodiments, the lengths of the structures 170 and 180 may be defined together.

The nonmagnetic layer 172 may optionally be provided, via step 214. In other embodiments, step 214 may be omitted.

The rear hard bias structure 180 is provided, via step 216. Step 216 includes depositing the material(s) for the hard magnetic bias structure 180. In some embodiments, step 216 includes defining both bias structures 170 and 180 in the cross-track direction. In other embodiments, these features are separately defined.

Using the method 210, the rear bias structures 160, 160′, 160″, 160′″ and/or 160″″ may be fabricated. Thus, the benefits of one or more of the transducers 100, 100′, 100″, 100′″, and/or 100″″ may be achieved. Consequently, biasing of the free layers 112 and 116 in the read sensor 110 may be improved.

FIG. 9 is an exemplary embodiment of a method 220 for providing a rear bias structure of a read transducer. For simplicity, some steps may be omitted, interleaved, combined, have multiple substeps and/or performed in another order unless otherwise specified. The method 220 is described in the context of providing a magnetic recording disk drive and transducer 100. However, the method 220 may be used in fabricating the transducer 100′, 100″, 100′″ and/or 100″″. The method 220 may be used to fabricate multiple magnetic read heads at substantially the same time. The method 220 may also be used to fabricate other magnetic recording transducers. The method 220 is also described in the context of particular layers. A particular layer may include multiple materials and/or multiple sub-layers. The method 220 is described in the context of a disk drive. However, the method may be used in other applications employing a magnetoresistive and bias structures. The method 220 also may start after formation of other portions of the magnetic recording transducer.

The read sensor 110 is defined in the stripe height direction, via step 222. Step 222 may occur before or after the read sensor is defined in the cross-track direction. Step 222 may include masking and ion milling the read sensor stack. Step 222 may also include providing a nonmagnetic insulating layer 155.

The rear soft bias structure 170 is provided, via step 224. Step 224 may include depositing the layer(s) for the rear soft bias structure 170. In addition, the rear soft bias structure may be defined in the stripe height direction, via step 226. Thus, space may be made for the hard bias structure 180. Step 226 may include masking and ion milling the material(s) that have been deposited for the rear soft bias structure 170. In some embodiments, the length of the rear soft bias structure 170 in the cross-track direction may also be defined. The nonmagnetic layer 172 may optionally be provided.

The rear hard bias structure 180 is provided, via step 228. Step 228 includes depositing the material(s) for the hard magnetic bias structure 180. In some embodiments, step 228 includes defining both bias structures 170 and 180 in the cross-track direction. In other embodiments, these features are separately defined.

Using the method 220, the rear bias structures 160, 160′, 160″, 160′″ and/or 160″″ may be fabricated. Thus, the benefits of one or more of the transducers 100, 100′, 100″, 100′″, and/or 100″″ may be achieved. Consequently, biasing of the free layers 112 and 116 in the read sensor 110 may be improved.