Pinarbasi, Mustafa (Morgan Hill, CA, US)

Plaque It! Sponsored by: Flash of Genius

09/728731

07/18/2002

11/30/2000

Images are available in PDF form when logged in. To view PDFs, Login  or  Create Account (Free!)

View patents that cite this patent

Click for automatic bibliography generation

360/322

360/324.100

(IPC1-7): G11B005/39

Hoyt & Knight,Marlin Knight (PO Box 1320, Pioneer, CA, 95666, US)

1. A transducer for reading magnetic transitions from a moving magnetic material comprising: a magnetic sensor; first and second electrically conductive multilayer leads in electrical contact with the magnetic sensor, each multilayer lead comprising: a thin film layer of tantalum; a thin film layer of chromium; and a layer of rhodium, the thin film layer of tantalum being a seed layer for the thin film layer of chromium and the thin film layer of chromium being a seed layer for the layer of rhodium.

2. The transducer of claim 1 wherein the magnetic sensor is a spin valve and the first and second multilayer leads are overlaid on opposing areas of an upper surface of the spin valve separated by a central area of the upper surface of the spin valve.

3. The transducer of claim 1 further comprising first and second hard bias structures disposed on opposing sides of the magnetic sensor and wherein first and second multilayer leads are respectively overlaid on first and second hard bias structures and first and second multilayer leads extend onto an upper surface of the magnetic sensor.

4. The transducer of claim 3 wherein first and second hard bias structures further comprise an upper layer of CoPtCr which is respectively in contact with the thin film layer of tantalum in first and second multilayer leads.

5. The transducer of claim 4 wherein first and second hard bias structures further comprise a layer of chromium under the CoPtCr layer.

6. The transducer of claim 5 in which the thin film layer of tantalum in first and second multilayer leads has a first thickness and the layer of rhodium in first and second multilayer leads has a second thickness, the second thickness being greater than ten times the first thickness.

7. The transducer of claim 1 further comprising first and second hard bias structures disposed on opposing lateral surfaces of the magnetic sensor, each multilayer lead being overlaid on one of the hard bias structures and electrically contacting the magnetic sensor through the hard bias structure and an upper surface of the magnetic sensor being free from contact with the multilayer leads.

8. The transducer of claim 7 further comprising a layer of PtMn under the magnetic sensor and under first and second hard bias structures.

9. The transducer of claim 7 further comprising a layer of PtMn under the magnetic sensor and the first and second hard bias structures contacting opposing lateral surfaces of the layer of PtMn.

10. The transducer of claim 7 wherein first and second hard bias structures further comprise an upper layer of CoPtCr which is in contact with the thin film layer of tantalum.

11. The transducer of claim 10 wherein the first and second hard bias structures further comprise a layer of Cr under the CoPtCr layer.

12. The transducer of claim 11 further comprising a layer of PtMn under the magnetic sensor and under first and second hard bias structures.

13. A disk drive comprising: a disk having a thin film of ferromagnetic material on a planar surface of the disk; a spindle rotatably supporting the disk; an arm with a suspension supporting a magnetic transducer having an air bearing surface over the planar surface of the disk; and the magnetic transducer including: a magnetic sensor; and first and second multilayered conductive leads in electrical contact with the magnetic sensor, the first and second multilayered conductive leads including a thin film seed layer of tantalum followed by a thin film seed layer of chromium and followed by a layer of rhodium.

14. The disk drive of claim 13 the magnetic transducer further comprising first and second hard bias structures disposed on opposing lateral surfaces of the magnetic sensor, each multilayer lead being overlaid on one of the hard bias structures and electrically contacting the magnetic sensor through the hard bias structure, and an upper surface of the magnetic sensor being free from contact with either of the multilayer leads.

15. The disk drive of claim 14 further comprising a layer of PtMn under the magnetic sensor and under first and second hard bias structures.

16. The disk drive of claim 15 wherein first and second hard bias structures further comprise an upper layer of CoPtCr which is in contact respectively with the thin film seed layer of tantalum of first and second multilayered conductive leads.

17. A method of fabricating a transducer for reading magnetic transitions from a moving magnetic material comprising the steps of: forming a magnetic sensor; and forming the leads for the magnetic sensor by: depositing first and second tantalum pads in electrical contact with the magnetic sensor at first and second locations; depositing a thin film layer of chromium on first and second tantalum pads; and depositing a layer of rhodium on the thin film layer of chromium over first and second tantalum pads.

18. The method of claim 17 further comprising the step, executed before the step of forming a magnetic sensor, of depositing a layer of PtMn.

19. The method of claim 18 further comprising the step, executed before the step of depositing a thin film layer of tantalum, of forming first and second hard bias structures on the layer of PtMn and in electrical contact with opposing lateral surfaces of the magnetic sensor, the thin film layer of tantalum being deposited in electrical contact with the first and second hard bias structures.

20. The method of claim 19 the step of forming first and second hard bias structures further comprising depositing a layer of chromium followed by a layer of CoPtCr.

21. A transducer for reading magnetic transitions from a moving magnetic material, the transducer being fabricated by a method comprising the steps of: forming a magnetic sensor; and forming first and second leads for the magnetic sensor by: depositing first and second tantalum pads in electrical contact with the magnetic sensor at first and second locations; depositing a thin film layer of chromium on the first and second tantalum pads; and depositing a layer of rhodium on the thin film layer of chromium on the first and second tantalum pads.

22. The transducer of claim 21 the method further comprising the step, executed before the step of forming a magnetic sensor, of depositing a layer of PtMn.

23. The transducer of claim 22 the method further comprising the step, executed before the step of depositing first and second tantalum pads, of forming first and second hard bias structures on the layer of PtMn in electrical contact with opposing lateral surfaces of the magnetic sensor, and wherein the first and second tantalum pads are deposited in electrical contact with the first and second hard bias structures.

24. The transducer of claim 22, the method wherein the step of forming first and second hard bias structures further comprises depositing a layer of chromium followed by a layer of CoPtCr.

FIELD OF THE INVENTION

[0001] The invention relates to the field of magnetic transducers (heads) and more particularly to materials and structures used to form conductive leads in the heads.

BACKGROUND OF THE INVENTION

[0002] A typical prior art head and disk system is illustrated in FIG. 1 . In operation the head 10 is supported by the suspension 13 as it flies above the disk 16 . The magnetic transducer, usually called a “head,” is composed of elements that perform the task of writing magnetic transitions (the write head 23 ) and reading the magnetic transitions (the read head 12 ). The electrical signals to and from the read and write heads 12 , 23 travel along conductive paths (leads) 14 which are attached to or embedded in the suspension 13 . Typically there are two electrical contact pads (not shown) each for the read and write heads 12 , 23 . Wires or leads 14 are connected to these pads and routed in the suspension 13 to the arm electronics (not shown). The disk 16 is attached to a spindle 18 that is driven by a spindle motor 24 to rotate the disk 16 . The disk 16 comprises a substrate 26 on which a plurality of thin films 21 are deposited. The thin films 21 include ferromagnetic material in which the write head 23 records the magnetic transitions in which information is encoded.

[0003] There are several types of read heads 23 including Giant Magnetoresistive (GMR) and tunnel junction. It is important for the two leads (not shown) that provide the electrical connection to the sensor element (not shown) in a magnetoresistive head 23 to be of low resistance, to be consistently manufacturable and to be resistant to formation of shorts during the manufacturing process. Typically leads (not shown) have been made from copper, tungsten, tantalum or gold, but the requirements of heads like spin valves make these traditional simple leads inadequate. To meet the new requirements, leads with a multilayer structure have been proposed. For example, U.S. Pat. No. 5,438,470 to Ravipati, et al., suggest using a thin layer of tantalum under a layer of gold for the leads. Ravipati '470 also teaches that lower resistance leads are obtained by placing the leads in contact with the hard bias layer as well the magnetoresistive sensor. U.S. Pat. No. 5,491,600 to Chen, et al., describes leads with two refractory metal layers sandwiching a highly conductive metal layer. One embodiment is alternating layers of tantalum and gold. In the particular type of head described in Chen '600, the leads from the spin valve sensor layer stack are formed on material used for the hard bias, e.g., CoPtCr. The CoPtCr layer in turn has a Cr underlayer.

[0004] U.S. Pat. No. 5,883,764 to Pinarbasi similarly describes a multilayer lead structure, for example, 3.5 nm Ta, 3.5 nm Cr and 75 nm Ta. The hard bias layer is again CoPtCr.

[0005] The substrate on which hard bias layers are formed in some head designs is NiO or alumina. Rhodium has been used as a lead material for these heads. Other designs use PtMn as the substrate for the hard bias layer on which the leads must be formed. However, the resistance of rhodium leads is unacceptably increased when the hard bias and lead stack are formed on a PtMn substrate.

SUMMARY OF THE INVENTION

[0006] A head according to the invention includes multilayered electrically conductive leads from the magnetic sensor which include a thin tantalum seed layer followed by a thin chromium seed layer which is followed by a thicker rhodium layer. The dual seed layer of the invention significantly improves the conductivity of the rhodium. The Ta/Cr/Rh leads can be used with hard bias structures formed on a PtMn layer without having increased resistance.

BRIEF DESCRIPTION OF THE FIGURES

[0007] FIG. 1 is an illustration of the prior art showing the relationships between the head and associated components in a disk drive.

[0008] FIG. 2 is an illustration of a section, parallel to the air bearing surface, of a head with the multilayered leads according to the invention overlaid on the hard bias structures and the upper surface of the magnetic sensor.

[0009] FIG. 3 is an illustration of a section, parallel to the air bearing surface, of a head with the multilayered leads according to the invention formed on the hard bias structures which are formed on a layer of PtMn and with the leads in electrical contact with the magnetic sensor through the hard bias structures.

[0010] FIG. 4 is an illustration of a section, parallel to the air bearing surface, of a head with the multilayered leads according to the invention formed on the hard bias structures and where the layer of PtMn has been etched away completely from the surface of the gap layer except the area underneath the spin valve.

DETAILED DESCRIPTION OF THE INVENTION AND THE PREFERRED EMBODIMENTS

[0011] A first embodiment of the invention in a spin valve head 12 A is illustrated in FIG. 2 in a section view taken parallel to the air bearing surface (not shown). The improved conductivity which results from the multilayered lead structure 36 a , 36 b of the invention can be used in other embodiments as will be clear to those skilled in the art. The relative thickness of the layers are not according to scale to the allow the layers to be seen more clearly. The thickness of each layer is according to the prior art with the exceptions noted below. Gap layer 31 underlies the two hard bias structures 33 a , 33 b . The hard bias structures 33 a , 33 b are shown as a single element even though they include more than one layer, e.g., a chromium layer (not shown) followed by a CoPtCr layer (not shown). The spin valve 35 is likewise illustrated as a single entity for simplicity even though it includes several layers.

[0012] In this embodiment the multilayered leads 36 a , 36 b are of the so-called overlaid type in that they are deposited in contact with the top surface of the spin valve 35 and the hard bias structures 33 a , 33 b . The multilayered leads 36 a , 36 b include the thin tantalum layer 37 which is used as a seed layer deposited directly onto the exposed ends of the top surface the spin valve 35 and the hard bias structures 33 a , 33 b . As in the prior art the central area of the spin valve 35 will be covered with a protective material such as photoresist (not shown) which is subsequently lifted off. The tantalum layer 37 is deposited by a thin film deposition technique such as sputtering or ion beam deposition. This layer can be very thin, e.g., approximately 3.5 nm, but can also be several times as thick and still perform its function. As with other thin film seed layers, the role of the tantalum layer 37 is to affect the grain size and the crystal orientations of the subsequent layer(s). The next layer after the tantalum layer 37 is a thin film layer of chromium 38 . The chromium layer 38 thickness is on the order the tantalum layer 37 and in effect serves as a second seed layer. The chromium layer 38 is also deposited by a thin film deposition technique such as sputtering or ion beam deposition.

[0013] The chromium layer 38 is followed by a much thicker layer of rhodium 39 . As mentioned above the relative thickness of the layers as shown on FIG. 2 is not according to scale. The rhodium layer 39 is preferably much thicker than the seed layers, e.g., more than ten times thicker. A thickness of 75 nm is a reasonable value. The values of the thickness of the layers of the leads 36 a , 36 b according to the invention are not critical. The tantalum and chromium layers 37 , 38 need only be thick enough to properly establish the growth conditions for the rhodium film 39 . The rhodium film 39 needs to be thick enough to provide the conductance needed for the particular magnetic sensor being used.

[0014] FIG. 3 is a section parallel to the ABS (not shown) similar to FIG. 2 , but the spin valve head 12 B illustrated has a so-called semi-contiguous junction (not shown). In this embodiment the hard bias layers 33 a , 33 b are deposited on a layer of PtMn 41 which is deposited on the gap layer 31 . The hard bias layers 33 a , 33 b do not extend over the entire lateral surfaces of the spin valve 35 . The multilayered leads 40 a , 40 b according to the invention are deposited on top of the hard bias structures 33 a , 33 b as in the prior art and make electrical contact with the sensor 35 through the hard bias structures 33 A, 33 B . In contrast to the overlaid leads 36 a , 36 b of FIG. 2 , the leads 40 a , 40 b in this embodiment do not extend above the spin valve 35 .

[0015] FIG. 4 illustrates an alternative type of spin valve head 12 C in which the multilayered leads 40 a , 40 b according to the invention can be used. FIG. 4 is a section of a spin valve head 12 C similar to that of FIG. 3 , but in this head the PtMn layer 41 is etched away completely from the surface of the gap layer 31 except the area underneath the spin valve 35 .

[0016] As noted above Cr/CoPtCr is used in some prior art heads for the hard bias layers 33 A, 33 B. In experiments using a Cr/CoPtCr hard bias layer and a 75 nm rhodium conductive layer with varying seed layers, the resistance measurements in ohms/cm ² shown in Table 1 were obtained on bare glass substrates and on glass with 20 nm of PtMn. 1

	TABLE 1
	Seed(s)	Glass	PtMn (20 nm)
	None	1.12	1.23
	Cr	1.11	1.25
	Ta	1.19	1.2
	Ta/Cr	1.04	1.05

[0017] Each seed layer in the experiment was 3.5 nm thick. These values were obtained after 232 C annealing. Neither the Cr seed layer nor the Ta seed significantly affected the resistance in the PtMn case. The dual seed layer of Ta/Cr reduced the resistance by approximately 15%.

[0018] It is to be expected that the addition of small amounts of other elements to either the Ta seed layer 37 or the Cr seed layer 38 would produce results that are consistent with those obtained from the pure elements. For example, in the prior art small amounts of vanadium and titanium have successfully been added to thin film chromium underlayers without disrupting the bcc structure. The effect is to modulate the lattice constant. It also follows that the tantalum and chromium seed layers 37 , 38 deposited by standard thin film techniques may have a certain amount of contamination and still serve their intended purpose.

[0019] Although the embodiments of the invention have been described in a spin valve head environment, the multilayer leads as described herein are not limited to this application. Those skilled in the art will recognize that the multilayered leads of the invention may be used in other magnetic transducer types such as tunnel junctions.