Method of making transducer with inorganic nonferromagnetic...

Semiconductor device manufacturing: process – Having magnetic or ferroelectric component

Reexamination Certificate

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C438S073000, C360S059000, C360S110000, C360S313000, C360S317000, C360S318000

Reexamination Certificate

active

06737281

ABSTRACT:

BACKGROUND
The present invention relates to electromagnetic transducers, which may for example be employed in information storage systems or measurement and testing systems.
Conventional heads for reading or writing information on a media such as a disk or tape are formed in multiple thin film layers on a wafer substrate that is then divided into thousands of individual heads. An inductive transducer for such a head includes electrically conductive coil sections encircled by a magnetic core including first and second pole layers, the core forming a magnetic circuit. Portions of the pole layers adjacent the media are termed pole tips. The magnetic core is interrupted by a submicron nonmagnetic gap disposed between the pole tips, so that the media bit closer to the gap becomes part of the magnetic circuit of the core and communicates magnetic flux between the pole tips and the media. To write to the media electric current is flowed through the coil, which produces magnetic flux in the core encircling the coil windings, part of the magnetic flux fringing across the nonmagnetic gap adjacent to the media so as to write bits of magnetic field information in tracks on the moving media.
A magnetoresistive (MR) sensor may be formed prior to the inductive transducer, the sensor sandwiched between soft magnetic shield layers. A first soft magnetic shield layer is conventionally formed on an alumina (Al
2
O
3
) undercoat that has been formed on an Al
2
O
3
TiC wafer. The second shield layer may also serve as the first pole layer for a combined MR and inductive transducer that may be termed a merged head. A structure in which a second shield layer is separated from an adjacent first pole layer may be called a piggyback head.
Typically the first pole layer is substantially flat and the second pole layer is curved, as a part of the second pole layer is formed over the coil windings and surrounding insulation, while another part of the second pole layer nearly adjoins the first pole layer adjacent the gap. The second pole layer may also diverge from a flat plane by curving to meet the first pole layer in a region distal to the media-facing surface, sometimes termed the back gap region, although typically a nonmagnetic gap in the core does not exist at this location.
The throat height is the distance along the pole tips from the media-facing surface at which the first and second pole layers begins to diverge and are separated by more than the submicron nonmagnetic gap. The point at which the pole layers begin to diverge is called the zero throat height. Because less magnetic flux crosses the gap as the pole layers are further separated, a short throat height is desirable in obtaining a fringing field for writing to the media that is a significant fraction of the total flux crossing the gap. Typically the throat height is determined by the curve of the second pole layer away from the gap in an area termed the apex region. An angle at which the second pole layer diverges from the first at the zero throat height is termed the apex angle.
To form the curves in the second pole layer, an organic photoresist is deposited on and about the coil sections and then the wafer is cured to create sloping sides upon which the second pole layer is electroplated. Photoresist is typically employed at this stage due to the difficulty in uniformly filling regions between the coil sections and forming sloping sides in the apex region. Curing photoresist at an elevated temperature, which changes its consistency from gel to solid and can create such sloping sides, forms hardhaked photoresist. Hardbaked photoresist has a coefficient of thermal expansion that is higher than that of other materials used to form the head, and so resistive heating in the coil sections can cause the area within the pole layers to expand, resulting in protrusion of the pole tips.
Most of the soft magnetic material in a conventional head is formed of permalloy (Ni
0.8
Fe
0.2
) and most of the dielectric material, aside from the baked photoresist around the coils, is formed of alumina. Alumina, as well as the AlTiC wafer that is conventionally employed for making heads, may have been selected for use with permalloy due to substantially similar thermal expansion coefficients. Having matching thermal expansion coefficients reduces problems such as strain and cracks between layers that expand or contract by different amounts.
Current commercially available disk drive heads “fly” at a separation of less than a microinch (about 25 nanometers) from a rigid disk that may be spinning at 10,000 revolutions per minute. Thus, even a small protrusion caused by the resistive heating of the coil could result in a crash that destroys the head and/or disk and renders irretrievable any data stored on the disk. Even without a crash, contact with the disk could move the head off track, causing data errors. Alternatively, avoiding a crash or data errors may require increasing the separation of the sensor from the disk, substantially decreasing the resolution.
SUMMARY
In accordance with the present invention, an inductive transducer is disclosed having inorganic nonferromagnetic material disposed in an apex region adjacent to a submicron nonferromagnetic gap in the core. The inorganic nonferromagnetic apex region can be made by chemical etching of a layer of inorganic nonferromagnetic material, deposition of inorganic nonferromagnetic material through a mask that is then lifted-off, or anisotropic etching of a layer of inorganic nonferromagnetic material that is covered by a hardbaked photoresist mask.


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U.S. 2002/0191349 Hsu et al. High Data Rate Write Head, Dec. 19, 2002.*
IEEE Transactions on Magnetics article entitled “Pole Tip Recession (PTR) Measurements with High Accuracy, Precision, and Throughput”, By Kulkarni et al., vol. 36, No. 5, dated Sep. 2000, copyright 2000.
Transactions of the ASME article entitled “On the Thermal Behavior of Giant Magnetoresistive Heads”, By Gupta et al., vol. 123, pp. 380-387, dated Apr. 2001, copyright 2001.

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