Spinvalve magnetoresistive head and method of manufacturing the same and magnetic recording/reproducing apparatus
AssigneeFujitsu Limited
InventorKen'ichiro Yamada
Life of this patent
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Abstract
In a spinvalve magnetoresistive head comprises a free magnetic layer made of soft magnetic material, a nonmagnetic intermediate layer overlapped with the free magnetic layer, and a pinning magnetic layer overlapped with the nonmagnetic intermediate layer and made of soft magnetic material, magnetization angles of the free magnetic layer and the pinning magnetic layer relative to a track core width direction are set such that a resistance-magnetic field curve is made linear, whereby symmetry of the reproduced outputs can be improved.
Claims26
A spinvalve magnetoresistive head comprising:
- a free magnetic layer made of soft magnetic material;
- a nonmagnetic intermediate layer overlapped with said free magnetic layer;
- and
- a pinning magnetic layer overlapped with said nonmagnetic intermediate layer and made of soft magnetic material;
- wherein a magnetization angle (.theta.f) of said free magnetic layer and a magnetization angle (.theta.p) of said pinning magnetic layer relative to a track core width direction are set such that an electric resistance-magnetic field curve is in a range of -10.about.+10% in an asymmetry (Asym) defined by the formula;
- Asym(%)=((cos .theta.p/cos.sup.3 .theta.f-4.multidot.amr)/(cos .theta.p.multidot.tan .theta.f-sin .theta.p-4.multidot.amr.multidot.sin .theta.f).multidot.(.differential. sin .theta.f/.differential.H)+(.differential..sup.2 sin .theta.f/.differential.H.sup.2)/(.differential. sin .theta.f/.differential.H)).multidot..DELTA.H/2
- where amr is a ratio of resistance change due to spinvalve magnetoresistance effect and resistance change due to an anisotropic magnetoresistance effect.
A magnetic disk drive comprising:
- (a) a spinvalve magnetoresistive head comprising:
- a free magnetic layer made of soft magnetic material,
- a nonmagnetic intermediate layer overlapped with said free magnetic layer, and
- a pinning magnetic layer overlapped with said nonmagnetic intermediate layer and made of soft magnetic material,
- wherein a magnetization angle (.theta.f) of said free magnetic layer and a magnetization angle (.theta.p) of said pinning magnetic layer relative to a track core width direction are set such that an electric resistance-magnetic field curve is in a range of -10.about.10% in an asymmetry (Asym) defined by the formula;
- Asym(%)=((cos .theta.p/cos.sup.3 .theta.f-4.multidot.amr)/(cos .theta.p.multidot.tan .theta.f-sin .theta.p-4.multidot.amr.multidot.sin .theta.f).multidot.(.differential. sin .theta.f/.differential.H)+(.differential..sup.2 sin .theta.f/.differential.H.sup.2)/(.differential.sin .theta.f/.differential.H)).multidot..DELTA.H/2
- where amr is a ratio of resistance change due to spinvalve magnetoresistance effect and resistance change due to an anisotropic magnetoresistance effect;
- and
- (b) a magnetic recording medium to which said spinvalve magnetoresistance head is arranged to oppose.
A method of manufacturing a spinvalve magnetoresistive head comprising the steps of:
- forming a free magnetic layer made of soft magnetic material, an intermediate layer made of soft magnetic material, an intermediate layer made of nonmagnetic material, a pinning magnetic layer made of soft magnetic material in forward order or reverse order,
- wherein a magnetization angle (.theta.f) of said free magnetic layer and a magnetization angle (.theta.p) of said pinning magnetic layer relative to a track core width direction are set such that an electric resistance-magnetic field curve is in a range of -10.about.+10% in an asymmetry (Asym) defined by the formula,
- Asym(%)=((cos .theta.p/cos.sup.3 .theta.f-4.multidot.amr)/(cos .theta.p.multidot.tan .theta.f-sin .theta.p-4.multidot.amr.multidot.sin .theta.f).multidot.(.differential. sin .theta.f/.differential.H)+(.differential..sup.2 sin .theta.f/.differential.H.sup.2)/(.differential. sin .theta.f/.differential.H)).multidot..DELTA.H/2
- where amr is a ratio of resistance change due to spinvalve magnetoresistance effect and resistance change due to an anisotropic magnetoresistance effect.
Dependencies are inferred from the claim text.