1. Field of the Invention
The present invention relates to a magnetoresistive head for use in magnetic recorders such as magnetic disk drives and magnetic tape devices.
2. Description of the Related Art
In recent years, attendant on the tendency toward smaller size and higher density of magnetic disk devices, the floating amount of a head slider is reduced, and realization of extremely low floating recording/reproduction or contact recording/reproduction in which the slider makes contact with a recording medium has been desired. In addition, in a conventional magnetic recording head, when the circumferential velocity (the relative velocity between the head and the medium) is reduced due to a reduction in the diameter of the magnetic disk, the reproduction output is deteriorated. In view of this, recently, magnetoresistive heads (MR heads) of which the reproduction output is independent from the circumferential velocity and which can produce a large output even at a low circumferential velocity have been vigorously developed, and have come to constitute a main stream of magnetic heads. Further, at present, magnetic heads utilizing the giant magnetoresistive (GMR) effect are also been commercialized. An increase in recording density of a magnetic disk device leads to a reduction in the recording area per bit and a reduction in the magnetic field generated. While the recording densities of the magnetic disk devices commercialized at present are around 20 Gbit/in2, the rise in the recording density is being enlarged by about 2 folds per year. Therefore, a magnetoresistive sensor and a magnetoresistive head that are capable of coping with a finer magnetic field range and capable of sensing small variations in the external magnetic field are demanded.
At present, a spin valve magnetoresistive sensor utilizing the spin valve GMR effect is widely used in magnetic heads. In the magnetoresistive sensor with the spin valve structure, the magnetization direction of a free ferromagnetic layer (free layer) is changed by a signal magnetic field, and the relative angle between this magnetization direction and the magnetization direction of a pinned ferromagnetic layer (pinned layer) is changed, whereby the resistance of the magnetoresistive sensor is changed. Where this magnetoresistive sensor is used in a magnetic head, the magnetization direction of the pinned layer is fixed in the device height direction of the magnetoresistive device, and the magnetization direction of the free layer in the condition where no external magnetic field is applied is generally designed to be in the device width direction orthogonal to the pinned layer. This ensures that the resistance of the magnetoresistive sensor is linearly increased or decreased according as the signal magnetic field direction for the magnetic recording medium is in parallel or antiparallel to the magnetization direction of the pinned layer. Such linear variations facilitate the signal processing of the magnetic disk device.
In the conventional magnetoresistive sensor, a sense current is passed in parallel to the film plane, and a resistance variation due to the external magnetic field is read. In this structure of passing the current in parallel to the GMR film plane (Current in the plane; CIP), the output is lowered when the sense region defined by a pair of electrode terminals is reduced. Besides, in the case of a spin valve magnetoresistive sensor with the CIP structure, an insulation film is required between the GMR film and each of upper and lower magnetic shields. That is to say, (the distance between the magnetic shields)=(the GMR film thickness)+(the insulation film thickness)×2. The insulation film thickness has a lower limit at about 20 nm at present, so that (the distance between the magnetic shields)=(the GMR film thickness)+about 40 nm. When the length of each record bit on the recording medium is reduced, it is impossible to cope with this, and the demand for reducing the distance between the magnetic shields to 40 nm or below cannot at present be coped with by the CIP spin valve magnetoresistive sensor.
From the foregoing, it is considered that a magnetic head of the CIP structure utilizing the spin valve GMR effect can cope with recording densities of up to 20 to 40 Gbit/in2. In addition, it is considered that, even when the specular scattering of the newest technology is applied, a recording density of 60 Gbit/in2 is the upper limit. As mentioned above, the enhancement of the recording density of the magnetic disk devices is rapid, and a recording density of 80 Gbit/in2 is demanded in the year 2002. At recording densities of 80 Gbit/in2 and above, it is very difficult even for the CIP spin valve GMR magnetic head based on the application of the newest specular scattering to cope with the recording densities, from the viewpoints of output and the distance between the magnetic shields. In order to cope with these problems, a GMR and a tunnel MR (TMR) of the structure of passing a current perpendicularly to the GMR film plane (Current Perpendicular to the Plane; CPP) have been proposed as post CIP.
The TMR has a structure including a thin insulation layer sandwiched between two ferromagnetic layers, in which the quantity of a tunnel current flowing through the insulation layer is varied by the magnetization directions of the two ferromagnetic layers. Since the TMR shoes a very large resistance variation and a good sensitivity, the TMR is considered to be promising as post spin valve GMR. The GMR with the CPP structure is characterized in that the output is enlarged when the sectional area of the portion through which the sense current flows of the GMR is reduced. This is a great advantage over the GMR with the CIP structure. Incidentally, the TMR can be considered to be a kind of the CPP structure because a current flows from the ferromagnetic layer on one side across the insulation layer to the ferromagnetic layer on the other side, and the above-mentioned advantage also applies to the TMR.
The MR head using the MR film (hereinafter, the term MR includes the GMR) has the problem that where the MR film is not a single magnetic domain, the Barkfausen noise is generated, to largely vary the reproduction output. Therefore, a magnetic domain control film is provided for controlling the magnetic domains of the MR film. As the magnetic domain control film, high coercive force films such as CoPt and antiferromagnetic films such as PdPtMn can be used.
In the MR head with the CPP structure, the sense current is passed in the direction perpendicular to the film plane of the MR film, the current magnetic field due to the sense current is in the direction of whirling in the film plane of the MR film 2 as shown in
In this instance, it is known as described in Japanese Patent Laid-open No. 2002-171013 that where a hard magnetic film is used as the magnetic domain control film, the sense current is passed in the medium-opposed end portion (air bearing surface side end portion) of the MR film so that the current magnetic field due to the sense current and the bias magnetic field due to the magnetic domain control films are in opposite directions. Hereinafter, the direction of the sense current such that the current magnetic field and the bias magnetic field are in the opposite directions will be referred to as the negative direction. On the other hand, the direction of the sense current such that the current magnetic field and the bias magnetic field are in the same direction will be referred to as the positive direction. However, when the sense current is passed in the medium-opposed end portion of the MR film so that the current magnetic field and the bias magnetic field are in the opposite directions, the magnetic field applied to the free layer is reduced through mutual canceling of the current magnetic field and the bias magnetic field due to the hard magnetic films in the medium-opposed end portion of the MR film, so that the magnetic domain control effect is reduced although the sensitivity of the magnetoresistive head is enhanced.
Further, where a hard magnetic film is used as the magnetic domain control film, the hard magnetic films are disposed on both sides of the MR film. In the magnetoresistive head with the CPP structure, it is necessary to adopt a structure in which the MR film and the hard magnetic films are separated and insulated from each other so as to prevent the sense current from being shunted to the hard magnetic films. Where the MR film and the hard magnetic films are separated from each other, the bias magnetic field from the hard magnetic films applied to the free layer of the MR film is extremely reduced. Therefore, when the sense current is passed in the negative direction, the magnetic domain control effect of the free layer is further reduced.
Accordingly, it is an object of the present invention to provide a magnetoresistive head capable of enhancing the magnetic domain control effect of a free layer of an MR film and capable of restraining the generation of the Barkhausen noise.
In accordance with one aspect of the present invention, there is provided a magnetoresistive head for detecting a magnetic signal on a recording medium as a reproduction signal comprising: a first magnetic shield; a first electrode terminal disposed on the first magnetic shield; a magnetoresistive film disposed on the first electrode terminal; magnetic domain control films disposed on both sides of the magnetoresistive film, for controlling magnetic domains of the magnetoresistive film by applying a bias magnetic field in a first direction on the magnetoresistive film; a second electrode terminal disposed on the magnetoresistive film; a second magnetic shield disposed on the second electrode terminal; and means for passing a sense current in the direction perpendicular to the film plane of the magnetoresistive film across the first and second electrode terminals so that the direction of a current magnetic field in a medium-opposed end portion of the magnetoresistive film is in the first direction.
Preferably, the magnetoresistive film includes at least one low resistance film, and at least two ferromagnetic films sandwiching the low resistance film therebetween. Alternatively, the magnetoresistive film has a ferromagnetic tunnel junction structure, or is composed of a multi-layer film structure of a ferromagnetic film or films and a nonmagnetic film or films. Preferably, the magnetic domain control film is composed of a high coercive force film. At least one of the first and second electrode terminals may function also as a magnetic shield.
In accordance with another aspect of the present invention, there is provided a magnetoresistive head for detecting a magnetic signal on a recording medium as a reproduction signal comprising: a first magnetic shield; a first electrode terminal disposed on the first magnetic shield; a magnetoresistive film disposed on the first electrode terminal; a magnetic domain control film disposed on the magnetoresistive film, for controlling magnetic domains of the magnetoresistive film by applying a bias magnetic field in a first direction on the magnetoresistive film; a second electrode terminal disposed on the domain control film; a second magnetic field disposed on the second electrode terminal; and means for passing a sense current in the direction perpendicular to the film plane of the magnetoresistive film across the first and second electrode terminal so that the direction of a current magnetic field in a medium-opposed end portion of the magnetoresistive film is in the first direction.
Preferably, the magnetic domain control film includes a nonmagnetic metal layer laminated on the magnetoresistive film, a ferromagnetic layer laminated on the nonmagnetic metal layer, and an antiferromagnetic layer laminated on the ferromagnetic layer. At least one of the first and second electrode terminals may function also as a magnetic shield.
In accordance with a further aspect of the present invention, there is provided a magnetoresistive head for detecting a magnetic signal on a recording medium as a reproduction signal comprising: a first magnetic shield; a first electrode terminal disposed on the first magnetic shield; a domain control film disposed on the first electrode terminal; a magnetoresistive film disposed on the domain control film; a second electrode terminal disposed on the magnetoresistive film; a second magnetic shield disposed on the second electrode terminal; and means for passing a sense current in the direction perpendicular to the film plane of the magnetoresistive film across the first and second electrode terminals so that the direction of a current magnetic field in a medium-opposed end portion of the magnetoresistive film is in the same direction as the direction of a bias magnetic field generated in the magnetoresistive film by the domain control film.
Preferably, the magnetic domain control film includes an antiferromagnetic layer laminated on the first electrode terminal, a ferromagnetic layer laminated on the antiferromagnetic layer, and a nonmagnetic metal layer laminated on the ferromagnetic layer. At least one of the first and second electrode terminals functions also as a magnetic shield.
Now, some embodiments of the present invention will be described below, referring to the drawings. In the description of the embodiments, substantially the same components will be denoted by the same symbols. Referring to
Symbol 12 denotes a lower electrode terminal which is formed of Cu or a combination of Cu and Au and which has a first width in the X direction. A magnetoresistive film (MR film) 14 is laminated on the lower electrode terminal 12. The MR film 14 has a second width smaller than the first width. Magnetic domain control films 18 are disposed respectively on both sides of the MR film 14. The MR film 14 and each of the magnetic domain control films 18 are disposed with a predetermined gap therebetween, whereby shunt currents from the MR film 14 into the magnetic domain control films 18 are prevented from being generated. As the magnetic domain control film 18, a high coercive force film such as CoCrPt can be used.
An upper electrode terminal 16 formed of Cu or a combination of Cu and Au is laminated on the MR film 14. The upper electrode terminal 16 has a second width substantially equal to the width of the MR film 14. Of the MR film 14, the portion not covered with the upper electrode terminal 16 functions as a back yoke for guiding a magnetic flux. While the width of the upper electrode terminal 16 is substantially equal to the width of the MR film 14 in the magnetoresistive head 10 according to this embodiment, the width of the lower electrode terminal 12 is greater than the width of the MR film 14. Therefore, concentration of the sense current occurs in the vicinity of both side portions of the MR film 14, so that the cross-sectional area of the sense current flowing through the MR film 14 can be reduced. As a result, a high reproduction output can be obtained. The width of the upper electrode terminal 16 may be set smaller than the width of the MR film 14.
The MR film 14 includes at least one low resistance film and at least two ferromagnetic films sandwiching the low resistance film therebetween. Alternatively, the MR film 14 has a ferromagnetic tunnel junction structure, or is composed of a multi-layer film structure of a ferromagnetic layer or layers and a nonmagnetic layer or layers. In other words, as the MR film 14, there can be used a spin valve GMR film such as NiFe/Cu/NiFe/IrMn, a laminated ferri-spin valve GMR film such as NiFe/Cu/CoFeB/Ru/CoFeB/PdPtMn, and a tunnel junction type MR film (TMR film) such as NiFe/Al2O3/NiFe/PdPtMn.
The magnetic domain control film 18 is so magnetized as to apply a bias magnetic field in the direction of arrow 20. Further, in the magnetoresistive head 10 according to this embodiment, a power source 22 passes a sense current across the electrode terminals 12 and 16 in the direction of arrow 24, which is the direction perpendicular to the film plane of the MR film 14. The direction of the sense current is important, and will be further described referring to
Now, referring to
Next, as shown in
Next, as shown in
Next, the photoresist 32 is patterned into a desired shape. The width of the photoresist 32 is set equal to or smaller than the width of the upper electrode terminal 16. Subsequently, the upper electrode terminal 16 is etched by ion milling or the like, using the photoresist 32 as a mask. In this instance, where the width of the photoresist 32 is smaller than the width of the upper electrode terminal 16, the width of the upper electrode terminal 16 becomes smaller than that of the MR film 14. Since reproduction characteristics are not thereby influenced greatly or the resolution in the track width direction is enhanced, good reproduction characteristics can be obtained. Next, an insulation film 38 is formed. This condition is shown in
Subsequently, the photoresist 32 is removed, and the insulation film 38 and the upper electrode terminal 16 are etched by ion milling or the like. Here, where etching is not used, a method may be adopted in which, before the formation of the insulation film 38 formed in
The magnetic shields 30, 40 and the electrode terminals 12, 16 are formed by plating or vapor deposition, whereas the MR film 14, the magnetic domain control films 18, and the insulation films 34, 38 are formed by sputtering or the like. In the magnetoresistive head 10 described above, the magnetic domain control films 18 may make electrical contact with one of the magnetic shields 30, 40 or with one of the electrode terminals 12, 16, but must not make electrical contact with both the electrodes 12, 16 or with both the magnetic shields 30, 40 functioning also as electrodes.
Referring to
Arrow 44 in
Next, referring to
In this instance, the laminated film (magnetic domain control film) 42 of the (nonmagnetic metal layer)/(ferromagnetic layer)/(antiferromagnetic layer) is so formed that the free layer of the MR film and the nonmagnetic metal layer are in laminated condition; for example, where the free layer is on the lower side in the MR film, the laminated film is so formed as to achieve sequential lamination in the manner of the (antiferromagnetic layer)/(ferromagnetic layer)/(nonmagnetic metal layer)/(free layer of MR film). On the contrary, where the free layer is on the upper side in the MR film, the laminated film is so formed as to achieve sequential lamination in the manner of the (free layer of MR film)/(nonmagnetic metal layer)/(ferromagnetic layer)/(antiferromagnetic layer). In this embodiment, the case where the free layer is on the upper side in the MR film will be described. Here, a structure may be adopted in which the lower electrode terminal 12 is not formed and the lower magnetic shield 30 functions also as the lower electrode terminal.
The MR film 14 includes at least one low resistance film and at least two ferromagnetic films sandwiching the low resistance film therebetween. Alternatively, the MR film 14 has a ferromagnetic tunnel junction structure or is composed of a multi-layer film structure of a ferromagnetic layer or layers and a nonmagnetic layer or layers. In other words, as the MR film 14, there can be used a spin valve GMR film of NiFe/Cu/NiFe/IrMn or the like, a laminated ferri-spin valve GMR film of NiFe/Cu/CoFeB/Ru/CoFeB/PdPtMn or the like, and a tunnel junction type MR film (TMR film) of NiFe/Al2O3/NiFe/PdPtMn or the like.
Next, as shown in
Subsequently, the photoresist 45 is patterned into a desired shape. The width of the photoresist 45 is set equal to or smaller than the width of the upper electrode terminal 16. Next, the upper electrode terminal 16 is etched by ion milling or the like, using the photoresist 45 as a mask. In this instance, where the width of the photoresist 45 is smaller than the width of the upper electrode terminal 16, the width of the upper electrode terminal 16 is smaller than that of the MR film 14. Since reproduction characteristics are not influenced largely or the resolution in the track width direction is enhanced, good reproduction characteristics can be obtained. Next, an insulation film 46 is formed. This condition is shown in
The magnetic shields 30, 40 and the electrode terminals 12, 16 are formed by plating or vapor deposition, whereas the MR film 14, the magnetic domain control film (laminated film) 42, and the insulation film 46 are formed by sputtering or the like. In the magnetoresistive head 10A according to this embodiment, there are used two antiferromagnetic layers, namely, an antiferromagnetic layer for fixing the magnetization of the ferromagnetic layer relative to the free layer in the MR film 14, and an antiferromagnetic layer for giving a bias magnetic field to the free layer of the MR film. In this instance, the magnetization fixing directions of the two antiferromagnetic layers differ by about 90 degrees. Therefore, in forming the two antiferromagnetic layers, it suffices to change the magnetization fixing direction by about 90 degrees by changing the applied magnetic field by about 90 degrees during a heat treatment, by using materials differing in blocking temperature.
According to the present invention, in a magnetoresistive head with a CPP structure, a sense current is passed so that the direction of a current magnetic field in a medium-opposed end portion of a free layer of an MR film coincides with the direction of a bias magnetic field due to a magnetic domain control film. It is possible to enhance the magnetic domain control effect of the free layer and to restrain the generation of the Barkhausen noise. As a result, a good reproduction signal can be obtained.
This is a continuation of PCT International Application NO. PCT/JP03/002659, filed Mar. 6, 2003, which was not published in English.
Number | Date | Country | |
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Parent | PCT/JP03/02659 | Mar 2003 | US |
Child | 11093514 | Mar 2005 | US |