Metal working – Method of mechanical manufacture – Electrical device making
Reexamination Certificate
2002-04-17
2004-09-07
Tugbang, A. Dexter (Department: 3729)
Metal working
Method of mechanical manufacture
Electrical device making
C029S603070, C029S603080, C029S603120, C029S603160, C029S603180, C300S013000, C300S013000
Reexamination Certificate
active
06785954
ABSTRACT:
BACKGROUND OF THE INVENTION
1. Field of the Invention
This invention relates generally to the fabrication of a giant magnetoresistive (GMR) magnetic field sensor of the bottom spin-valve (BSV) type and more specifically to methods for eliminating undesirable oxidations and diffusions during annealing and patterning when forming lead overlay (LOL) type lead layers.
2. Description of the Related Art
Magnetic read heads whose sensors make use of the giant magnetoresistive effect (GMR) in the bottom spin-valve configuration (BSV) are being increasingly required to read information recorded on magnetic media at ultra-high area densities (e.g. >45 Gb/in
2
). To be capable of reading such area densities, the sensor must be able to resolve extremely high linear bit densities (BPI) and track densities (TPI), which, in turn, requires that it have an extremely narrow trackwidth and thin free layer to maintain high signal output. Unfortunately, narrow trackwidth designs tend to have reductions in both signal amplitude and sensor stability. A viable approach to obtaining high signal strength and narrow trackwidth is to use the lead overlay (LOL) design, wherein the physical trackwidth is defined by the longitudinal separation distance between the inner edges of the lead overlay while the contiguous junction longitudinal hard bias layers are placed beneath the leads and are separated by a greater longitudinal distance than the leads.
FIG. 1
is a highly schematic diagram of a cross-sectional view of such a lead overlay configuration. The two separated lead segments (
2
) are formed over the sensor stack (
4
) and are separated longitudinally by a physical trackwidth (
6
). The actual contiguous junction edges (
8
) are contacted by the longitudinal hard (permanent magnetic) bias layers (
10
) which are seen to lie substantially beneath the lead layers. The bias layers contact the edges of the free layer (
12
) at the junction and pin its magnetization to improve sensor stability and eliminate thermally induced domain breakup. It is to be noted that there is an important difference between the physical trackwidth (
6
) which is defined by the physical placement of the lead edges and the effective or actual trackwidth of the sensor, the magnetic read width (MRW), which is the width that is responsible for the production of the bulk of the sensor signal. Since a portion of the sensor beneath the lead overlay is also capable of producing a signal (“side reading”), the effective trackwidth is typically greater than the physical trackwidth. One of the objects of sensor design is to reduce the effective trackwidth, which typically involves a corresponding reduction in physical trackwidth. In a very narrow sensor with a very narrow stack formation, the portion of the free layer pinned by the bias layer constitutes a dead zone as far as free layer response is concerned and so the strength of the bias layer may actually contribute to sensor instability rather than reduce it.
The standard prior art method of forming the LOL is to define the device regions (stack junctions and LOL edges) by lift-off photoresist patterning. To have the LOL perform optimally, good electrical contact between the LOL layer and the upper surface of the stack is a necessity. This requires extensive cleaning of the upper stack surface, which is typically achieved by an ion-beam etch (IBE) to remove oxide layers formed on the portions of the stack surface to be contacted (typically a Ta capping layer). The etching process is particularly critical when the stack is a bottom spin valve configuration, since that configuration has the free layer directly below the surface being etched. After the etching has been completed, the LOL layer, which is typically a Ta/Au/Ta tri-layer, is deposited. When very narrow physical trackwidths are being formed it is almost impossible to avoid shorting between the LOL edges.
The generic structure (i.e. prior art) of a bottom spin valve stack and LOL layer can be seen by referring to FIG.
2
. This highly schematic cross-sectional view shows the essential stack layers in the following order, which may be considered as extending vertically upward from a substrate (
10
), wherein the longitudinal (or lateral) direction is from left-to-right and the transverse direction is perpendicular to the plane of the drawing. On the substrate (
10
) there is first seen a seed layer (
20
), which is typically a structure enhancing layer of NiCr. On the seed layer there is formed a pinning layer (
30
) of antiferromagnetic material, typically MnPt. On the pinning layer there is then formed a pinned layer (
40
), which, in this example, is a synthetic antiferromagnetic tri-layer comprising a lower ferromagnetic layer (designated AP
2
) (
42
) of CoFe, a coupling layer (
44
) of Ru and an upper ferromagnetic layer (designated AP
1
) (
46
) which is also a layer of CoFe. On the pinned layer is then formed a non-magnetic spacer layer (
50
), which is typically a layer of Cu. On the spacer layer is then formed a ferromagnetic free layer (
60
), which is here a tri-layer of CoFe (
62
), NiFe (
64
) and Cu (
66
). On the free layer is then formed a capping layer (
70
), typically a Ta layer approximately 10-20 angstroms thick, but ideally 5-10 angstroms thick. When this stack is exposed to an oxidizing ambient or to annealing to fix the magnetizations of the pinned and free layers, the capping layer (
70
) is oxidized to a depth of approximately 7 angstroms to form a 20 angstroms thick TaOx insulating layer which also serves as a specularly reflecting layer that greatly enhances sensor signal output. Pinarbasi (U.S. Pat. No. 6,208,491 B1) provides a stack structure similar to this in which a variety a capping layers are shown to improve the magnetoresistive coefficient (dr/R). Gill et al. (U.S. Pat. No. 6,278,590 B1) provides a bottom spin valve sensor, without a LOL configuration, that is incorporated within a merged read-write head. Sato et al. (U.S. Pat. No. 5,923,503) provides a spin valve sensor that is formed within an etched region of a longitudinal bias layer and conductive lead layer that have been formed on a non-magnetic substrate. Wiitala (U.S. Pat. No. 6,188,549 B1) provides high performance magnetic gap layers for use when incorporating spin valve read sensors within merged read/write configurations.
None of the above prior art references disclose a LOL configuration. If we return to the illustration of
FIG. 2
, the LOL layer (
80
) formed on the upper surface of the capping layer, is a tri-layer of Ta (
82
), Au (
84
) and Ta (
86
). The first Ta layer (
82
) serves as an adhesion layer for the Au and both the first and second (
86
) Ta layers diffuse into the Au layer during annealing to provide structural strength to the Au layer and help to eliminate lead smearing and electromigration.
If the configuration of
FIG. 2
is to be capable of reading area densities exceeding 45 Gb/in
2
, an effective trackwidth of approximately 0.2 microns is needed. This, in turn, requires a physical trackwidth of less than 0.15 microns. Such a narrow trackwidth is not well suited to be defined by an additive photoresistive lift-off process which adds new conductive material to an upper stack surface, but would be more advantageously formed by a subtractive etching process, such as a reactive ion etch (RIE), applied to remove material from an already formed conductive layer. It is the object of the present invention to provide such a novel lead overlay-bottom spin valve (LOL-BSV) structure in which a narrow physical trackwidth is obtained by RIE and in which other significant advantages are also obtained.
SUMMARY OF THE INVENTION
It is a first object of the present invention to provide a high signal output, magnetically stable, longitudinally hard biased bottom spin valve (BSV) GMR sensor capable of reading high area density magnetic recordings of densities exceeding 45 Gb/in
2
(gigabits per square inch).
It is a second object of the present invention to provide such a BSV GMR sensor having a LOL configuration that
Chen Mao-Min
Chien Chen-Jung
Han Cherng-Chyi
Horng Cheng T.
Tong Ru-Ying
Ackerman Stephen B.
Headway Technologies Inc.
Kim Paul D
Saile George O.
Tugbang A. Dexter
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