YOKE TYPE THIN-FILM MAGNETIC HEAD

Abstract: A yoke type thin-film magneto-resistive head of the present invention comprises a magneto-resistive element (2) that detects magnetic field generated in the magnetic recording medium as resistance change, a yoke (1,5), that lead magnetic flux from the head gap to the above mentioned magneto-resistive element, a DC magnetic field application system, that applies a desirable weak magnetic field to the above men­ tioned longitudinal direction of magneto-resistive element (2), and a conductor (4,4), that applies a desirable bias magnetic field to the above mentioned magneto-resistive element (2) in the strip width direction, the easy axis of magnetization of said magneto-resistive element (2) is inclined 20° - 40° to mentioned longitudinal direction of magneto-resistive element, so that, anisotropic angle dispersion conditions are relaxed, at the same time, by applying a desirable bias magnetic field to the magneto-resistive element (2) in the strip width direction, and by shifting the operating point to a point being excellent in linearity, Barkhausen noise, caused by magnetization switching generated in the magnetic field area with a direction the same as the bias magnetic field direction, can be suppressed, and the reproducing output signal can be of high fidelity.

Description: This invention relates to a yoke type thin-film magneto-resistive head (hereinafter called "YMR head"), which detects signals recorded in a magnetic recording medium by using a magneto-resistive element (hereinafter called "MR element") to which is applied a ferromagnetic film magneto-resistive effect. The structure of the YMR head, which is well known and applied, is indicated in Fig. 7. The upper yoke (1,5) is usually made of about 0.5 - 1.0µm permalloy film, and structures magnetic flux introduction leading the signal magnetic field generated in the magnetic recording medium to the MR element (2). Ferromagnetic film (3,3) has large magnetic coercive force and high electric conductivity. It is made of Co-P, Ni-Co, and Ni-Co-P and so on, with a film thickness of 1000 - 2000 Å. The lead conductor (4,4) is made of Al-Cu film or other conductive metal film, with a film thickness of 1000 - 2000 Å. Located below the above mentioned MR element (2) is the conductor (6), made of Al-Cu film or other conductive metal film, which is set to apply a bias magnetic field to the MR element. The lower yoke (7) is made of substrate with high magnetic permeability. For this magnetic substrate, poly-crystal Ni-Zn ferrite substrate, single crystal or poly-crystal Mn-Zn ferrite substrate is normally used. The head gap (10) is set at about 0.2 - 0.3µm, since the recording wave length actually used is about 0.5µm at minimum. Also at a location close to the head gap is located the magnetic recording medium (9), as indicated in Fig. 8. Between the magnetic recording medium (9) and the head gap (10), spacing (8) is formed. In a YMR head of this structure, the direction of the easy axis of magnetization of MR element (2) is set along the longitudinal direction of the MR element (2) when the MR element was fabricated. Detection of the signal magnetic field generated from the above mentioned magnetic recording medium (9) is performed by flowing sense current along the longitudinal direction of the MR element (2), and sensing voltage changes which occur at both ends of such an MR element. The MR element (2) operating point is shifted to a point being excellent in linearity by applying a desirable bias magnetic field, generated by flowing current through the conductor (6), to the MR element. Also, by ferromagnetic exchange coupling between the above ferromagnetic film (3,3) and the MR element (2), a weak magnetic field is applied in the longitudinal direction of MR element (2). This weak magnetic field puts MR element (2) into a single magnetic domain condition, and suppresses Barkhausen noise occurring by preventing MR element (2) magnetization from discontinuously changing. In conventional YMR heads, generally all direction of the easy axis of magnetization in the entire area of MR element (2) are not in the same direction. This is because the angle dispersion of the easy axis of magnetization tends to occur when the MR element (2) is made, or when the above mentioned head gap (10) and upper yoke (1,5) are formed. This causes the easy axis dispersion in each area of MR element (2). It is difficult to prevent this dispersion. Suppose that the direction of easy axis of magnetization of points a, b, c, d, and e of MR element (2) are in the arrowhead (→) directions, as indicated in Fig. 9. The weak magnetic field direction, the longitudinal direction of MR element (2) caused by ferromagnetic film (3), is graphically shown to be from left to right, that is, in the direction of arrows. Then the magnetization curve of MR element (2) strip width direction in individual a, b, c, d, and e points are indicated by (a) - (e) of Fig. 10 respectively. In the ΔR/R curve corresponding to such an MR element (2) reproducing output, discontinuous jumps occur in parts of the ΔR/R curve by responding to magnetic transition in MR element (2), as indicated in Fig. 10(f). This generates Barkhausen noise. At the same time, if the above mentioned direction of the easy axis of magnetization is set along the longitudinal direction when the MR element (2) is made, the distribution of the direction of the easy axis of magnetization in MR element (2) becomes distributed in both positive and negative directions of the longitudinal direction. Consequently, on the axis of abscissa of the ΔR/R curve, that is, on both negative and positive sides of magnetic field Ha, the signal magnetic field, discontinuous jumps occur. Therefore, when the MR element (2) operating point is shifted to a point being excellent in linearity by a bias magnetic field, Barkhausen noise will occur in whatever positive or negative magnetic field direction such an operating point is shifted. This has been a problem. From DE-A-3,644,388 of the present applicant, there is known a YMR head in which the easy axis of magnetisation of the MR element is inclined to the longitudinal direction at an angle in the range 5° to 20°, and the local angle dispersion is limited to within about ±10°. Such a narrow range of angle dispersion is difficult to achieve in practice, so that the manufacturing cost is undesirably raised. An object of this invention is to offer a YMR head which can achieve a good in linearity and high fidelity reproduced output signal by suppressing Barkhausen noise, which is contained in the reproduced output signal. This is based on attention given to magneto-resistive characteristic polarity changes according to the angle made by the direction of the easy axis of magnetization of the MR element, and the signal magnetic field direction. The above-mentioned Barkhausen noise that usually occurs is caused by the shift of the magnetic domain wall, that is, the border surface of magnetization, where magnetization directions in magnetic substance differ. Since Barkhausen noise causes discontinuous jumps in both negative and positive areas of the magneto-resistive characteristic, the reproduced output signal has discontinuous jump. On the other hand, the magneto-resistive characteristic of MR elements itself have a characteristic like Gaussian distribution curve, in which the shape broadens toward its bottom. Hence, a part with excellent linearity exists, and a reproduced output signal proportional to the signal magnetic field can be attained by applying a required bias magnetic field. This is caused by the influence of diamagnetic fields, which occur at both side edges of MR elements. However, in the YMR head, in which the MR element is located in a more rear position than the contact plane with magnetic recording medium, the above mentioned diamagnetic field rarely occurs, which is the cause of non-linearity of reproduced output signals. In order to avoid non-linear components in MR element reproduced output signals, structuring is very complicated. Considering conditions in which the magnetic head itself must be compact in order to increase memory capacity, the structure should be simple. Another object of this invention is to offer a YMR head which can achieve undistorted reproduced output signals being excellent in linearity, by shifting discontinuous jumps in the above-mentioned reproduced output signal, which cannot be prevented only by shifting the operating point to a point being excellent in linearity of the MR element by applying a bias magnetic field to the MR element in the strip width direction, to one of the positive or negative area. Still another object of this invention is to make the magnetic head itself compact and simple in structure, and to offer a YMR head which can avoid non-linearity of reproduced output signals. In accordance with the invention, a yoke type thin-film magneto-resistive head comprises a magneto-resistive strip element which detects signal magnetic field from a magnetic recording medium by resistance change, a yoke which leads magnetic flux from a head gap to said magneto-resistive strip element, a DC magnetic field application means that applies weak magnetic field to said magneto-resistive strip element in the longitudinal direction, and a conductor which applies bias magnetic field to said magneto-resistive strip element in the width direction, characterised in that the easy axis of magnetization of said magneto-resistive strip element is inclined by 20° - 40° to the longitudinal direction of the magneto-resistive element. If the inclination of the easy axis of magnetization lies in the range 30° - 40°, the maximum angle dispersion of the easy axis is preferably ± 40°. The above mentioned magnetic recording medium can be magnetic tape or disk, the type used in audio or video tape recorders et cetera. The angle of the easy axis of magnetization in the above mentioned MR element can be inclined in either direction of the positive or negative side longitudinal direction. Fig. 1 is an explanatory diagram indicating distribution of the magnetic easy axis when the anisotropic inclination angle of the magnetic easy axis ϑ to the longitudinal direction of MR element is set at 30°. Fig. 2 (a) to (e) are wave diagrams of magnetization curves of MR elements of individual a - e points of Fig. 1 in strip width directions. Fig. 2 (f) is an ΔR/R curve diagram that corresponds to the reproduced output of the MR element. Fig. 3 is a concept diagram, indicating a single magnetic domain model. Fig. 4 to 6 are ΔR/R wave diagram for different values of each anisotropic axis angle ϑ. Fig. 7 is a perspective view indicating the current well known and adopted YMR head structure. Fig. 8 is a plan view of the current well known and adopted YMR head. Fig. 9 is an explanatory diagram indicating currently used examples and the distribution of the magnetic easy axis. Fig. 10 (a) to (e) are wave diagrams of MR element magnetization curves in the strip width direction for individual a - e points of Fig. 9. Fig. 10 (f) is an ΔR/R wave diagram corresponding to the reproduced output of the MR element. What follows is an explanation of embodiment examples of this invention, based on Fig. 1 to 8. For convenience sake, explanation is again done using Fig. 7 and 8, and part symbols in Fig. 1 correspond to those of Fig. 7 and 8. The yoke type thin-film magneto-resistive head (hereinafter called "YMR head") related to this invention, as indicated in Fig. 7 and 8, is equipped with a magneto-resistive element (hereinafter called "MR element") (2), which detects the signal magnetic field generated in magnetic recording medium (9) as a resistance change; upper yoke (1,5), which leads the signal magnetic flux from head gap (10) to the above mentioned MR element (2); ferromagnetic film (3,3) as a DC magnetic field application system, which applies a desirable weak magnetic field along the longitudinal direction of the MR element (2) in order to make the MR element (2) a single magnetic domain; and a conductor (6), which applies the desirable bias magnetic field to the MR element (2) in the strip width direction. In such a YMR head, the direction of the easy axis of magnetization in the MR element (2), as indicated in Fig. 1, is inclined 30° clockwise to the MR element (2) longitudinal direction. In the above mentioned structure, a weak magnetic field is applied to the MR element (2) in the direction of arrows, that is, as graphically expressed as a left to right direction, by the above mentioned ferromagnetic film (3,3). Concerning the direction of the easy axis of magnetization in MR element (2), in an MR element individual part, almost a similar degree of angle dispersion is given in both positive and negative direction to the direction of the set up easy axis of magnetization. Here, if the maximum inclination degree of local easy axis of magnetization caused by this dispersion of angle is ±30° or so, the direction of the easy axis of magnetization is distributed in the range of 0° - 60° to the longitudinal direction in the MR element total area. For example, at the point a on MR element (2), the easy axis of magnetization inclines about 60° to the longitudinal direction, and at the e point, it is almost in the same direction as the longitudinal direction. As a consequence, the area, where the direction of the easy axis of magnetization is inclined counterclockwise to the longitudinal direction, does not exist, in this example. At this time, the magnetization curve of MR element strip width direction at the individual a, b, c, d, and e points come to be (a) - (e) respectively, as indicated in Fig. 2. The ΔR/R curve corresponding to the MR element reproduced output, indicated in Fig. 2 (f) causes discontinuous jumps to a part of the curve, only in the negative side area of magnetic field Ha. As a consequence, when the MR element (2) operating point is shifted to a point being excellent in linearity by a bias magnetic field, if a bias magnetic field is applied such that the operation point is set in the positive side area of magnetic field Ha, Barkhausen noise occurrence can be avoided when the YMR head reproduces a signal magnetic field. Besides, when an MR element (2) is made, if the easy axis of magnetization is inclined 30° counterclockwise, opposite the one indicated in Fig. 1, and other conditions remain the same, in the ΔR/R curve, discontinuous jumps occur at the positive side area of magnetic field Ha, and, as in Fig. 2 (f), the result is opposite in the positive and negative area of magnetic field Ha. In this case, if a bias magnetic field is applied such that the MR element (2) operating point is set in the negative side or magnetic field Ha, Barkhausen noise will not occur in reproduced output signals. The next explanation concerns the manner of determining the inclination angle of the easy axis or magnetization to the longitudinal direction (hereinafter called "anisotropic inclination angle"), when the MR element (2) is made. The MR element (2) in the YMR head responds to magnetic signals in small diamagnetic field conditions due to magnetic coupling of the upper side yoke (1,5) and lower side yoke (7). Also, because of the weak magnetic field applied to the MR element (2) by ferromagnetic film (3) with a high coercive force, the MR element (2) is in a single magnetic domain condition. Considering these points, the appropriate value of an anisotropic inclination angle can be estimated by using a single magnetic domain model, this indicated in Fig. 3. In Fig. 3, ϑ is an anisotropic inclination angle, H E is a weak magnetic field applied to the MR element (2) by ferromagnetic film (3), M S is saturation magnetization of the MR element, and Ha is an external magnetic field corresponding to the signal magnetic field. Here, based on the characteristics of the MR element (2) experimentally made, the magnetisation M S rotation angle ψ to the easy axis of magnetization is calculated in this manner: when M S = 796 [emu/cc] and the anisotropic magnetic field H K = 4.0 [O e ], concerning a certain appropriate value H E , the total anisotropic energy of magnetization M S , magneto-static energy of magnetization M S and H E , the magneto-static energy of magnetization M S and Ha reaches a minimum. Then, as indicated in Fig. 4 to 6, three kinds of ΔR/R curves are attained according to the value of anisotropic inclination angle ϑ. The ΔR/R curve in Fig. 4 is a case that indicates that magnetization switching has not occurred, with only unsymmetrical characteristics appearing. The ΔR/R curve in Fig. 5 is a case indicating that magnetization switching occurred, at either the positive side area or the negative side area of the external magnetic field Ha. The ΔR/R curve in Fig. 6 is a case indicating that magnetization switching has occurred at both positive and negative side areas of the external magnetic field Ha. However, such magnetization switching, as indicated in Fig. 6, differs from the Barkhausen noise, indicated in Fig. 10 (f). When an external magnetic field Ha is applied within either the positive or negative side area, magnetization switching does not occur. As a consequence, magnetization switching as the cause of Barkhausen noise is expressed in Fig. 5. The range of anisotropic inclination angle ϑ which makes the ΔR/R curve in Fig. 5, (minimum inclination angle ϑ₁, maximum inclination angle ϑ₂), are calculated as indicated in chart 1, when the H E values is changed in the ranged of 0.5 - 2.0 [O e ]. In this case, both minimum inclination angle ϑ₁ and maximum inclination angle ϑ₂ have the same result in both negative and positive values. Besides, the positive value has a clockwise angle, the negative value has a counterclockwise angle. Chart 1 H E (o e ) Θ₁ ( · ) Θ₂ ( · ) H E (o e ) Θ₁ ( · ) Θ₂ ( · ) 0.5 7.18 7.24 1.3 18.97 20.28 0.6 8.63 8.73 1.4 20.49 22.22 0.7 10.08 10.24 1.5 22.02 24.30 0.8 11.54 11.97 1.6 23.58 26.57 0.9 13.00 13.37 1.7 25.15 29.11 1.0 14.48 15.00 1.8 26.74 32.08 1.1 15.96 16.68 1.9 28.36 35.90 1.2 17.46 18.44 2.0 30.00 45.00 The angle dispersion of easy axis in MR element (2) is greatly influenced by the surface roughness of the substrate on which it is formed. For example, in a surface roughness of about 10Å of glass substrate, the local inclination angle of the easy axis of magnetization caused by angle dispersion in MR element (2) is a maximum of ±20° or so. But, the base surface roughness of the MR element (2) formed on the YMR head is more than about 20Å. In this case, the local inclination angle of the easy axis of magnetization caused by angle dispersion in MR element (2) sometimes is a maximum of ±40° or so. Even in such cases, preferably it is better to cause magnetization switching in either one area of the positive or negative side of magnetic field Ha, that is the signal magnetic field, as indicated in Fig. 2 (f). Here, let us say, a weak magnetic field is applied to the MR element (2) by ferromagnetic film (3), and the MR element (2) is in a single magnetic domain condition. In this case, if the MR element (2) anisotropic inclination angle ϑ is set at about 40°, Barkhausen noise caused by angle dispersion in MR element (2) can be suppressed. This is because when the local inclination angle of the easy axis of magnetization caused by angle dispersion MR element (2) is at a maximum ±40°, if the anisotropic inclination angle ϑ is set at 40°, the easy axis of magnetization on MR element (2) is dispersed in the range of 0° - 80°, hence no counterclockwise inclined area exists, in this case. On the other hand, concerning the case in which the above mentioned MR element (2) anisotropic inclination angle ϑ is set at 50°, if the local inclination angle of the easy axis of magnetization, caused by angle dispersion in MR element (2), is at a maximum ±40°, in this case, the easy axis of magnetization on MR element (2) will disperse in the range of 10° - 90°. In this case as well, Barkhausen noise can be suppressed. However, if the anisotropic inclination angle ϑ is set at 50°, MR element (2) permeability will remarkable decline, which causes a reduction in reproducing sensitivity. If MR element (2) anisotropic inclination angle ϑ is set at 60°, the easy axis of magnetization in MR element (2) disperses in the range of 20° - 100°, which causes a further reduction in reproducing sensitivity. At the same time, in the area where direction of the easy axis of magnetization exceeds 90°, a magnetic domain wall is generated in MR element (2), and it is possible to cause Barkhausen noise by irreversible magnetic domain wall movement caused by signal magnetic field application. As a consequence, the upper limit of an anisotropic inclination angle ϑ is around 40°. Even in cases when H E = 1.0 [O e ], and the maximum local inclination angle of the easy axis of magnetization caused by angle dispersion in MR element (2) is ±40° and unchanged, and MR element (2) anisotropic inclination angle ϑ set at around 30°, Barkhausen noise caused by angle dispersion in MR element (2) can be avoided. In other words, as mentioned above, if the anisotropic inclination angle ϑ is set at around 30°, the easy axis of magnetization disperses in the range of 0° - 70°, and the area inclining counterclockwise exists in the range of -10° - 0°. However, magnetic switching occurs in either one area of the positive or negative side of the magnetic field Ha, the signal magnetic field, only when easy axis of magnetization in MR element (2) inclines by about 14.5° - 15° to the positive or negative side, as is clearly shown in chart 1. Hence, no magnetization switching will occur even in the area of counterclockwise inclination in a range of -10° - 0° as in the above case. Because of this, when magnetic field Ha, the signal magnetic field, is applied, the magnetization switching causing Barkhausen noise will not occur in the positive area of Ha. Consequently, if MR element (2) operating point is set in the positive area, Barkhausen noise can be suppressed. Also, if the anisotropic angle ϑ is set at -30°, the MR element (2) operating point can be set in the negative area. When H E = 1.5 [O e ] and the local inclination angle of the easy axis of magnetization caused by angle dispersion in MR element (2) is a maximum of ±40° and unchanged, if MR element (2) anisotropic inclination angle ϑ is set at about 18°, Barkhausen noise caused by angle dispersion in MR element (2) can be avoided. This is because, as chart 1 clearly indicates, ϑ₁ of H E = 1.5 [O e ] is approximately 22°. However, H E = 1.5 [O e ] is a rather large magnetic field value, very difficult to apply to the entire MR element (2) area. Also, even if this value could be realized by the actual YMR head, a drastic output declination will be caused, because MR element (2) anisotropic magnetic field H K is 4 - 5 [O e ]. Because of this, when the local inclination angle of the easy axis of magnetization caused by angle dispersion in MR element (2) is a maximum of ±40°, it is realistic to set the anisotropic inclination angle ϑ at more than about 30°. On the other hand, it is possible to control the inclination angle of the easy axis of magnetization caused by angle dispersion in MR element (2) to a maximum ±30° or so, in this case, the anisotropic inclination angle ϑ is sufficient to be about 20°, for the above mentioned reasons. However, compared to the MR element (2), with an inclination angle of the easy axis of magnetization controlled at a maximum ±40° or so, it is unavoidably disadvantageous in a manufacturing condition. Consequently, it is to be determined whether to make the anisotropic inclination angle ϑ 20° by controlling the local inclination angle of the easy axis of magnetization caused by angle dispersion in MR element (2) at a maximum ±30° or so, or to make the anisotropic inclination angle ϑ to be more than 30° and to ease the angle dispersion in MR element (2) conditions, these possibilities weighed against manufacturing conditions, production costs, etc. Thus there is an inseparable relationship between the angle dispersion in MR element (2) scale and the anisotropic inclination angle ϑ value, and for the just mentioned reasons, it is appropriate to set the MR element (2) anisotropic inclination angle ϑ in the range of 20° - 40°. The YMR head related to this invention, as previously mentioned, is a YMR head that includes a MR element, that detects the signal magnetic field generated in the magnetic recording medium as a resistance change, a yoke, that leads magnetic flux from the head gap to the above mentioned MR element, a DC magnetic field application system, that applies a desirable weak magnetic field to the longitudinal direction of the above mentioned MR element, and a conductor, that applies a desirable bias magnetic field in the strip width direction of the above mentioned MR element wherein the special feature is that the easy axis of magnetization of the above mentioned MR element is inclined 20° - 40° to the longitudinal direction of the MR element. Also, the above mentioned magnetic recording medium may be made of magnetic tape or disk. The above mentioned MR element may be a thin film shaped magnetic sensor with a longitudinal direction and a strip width direction, and structured that by applying detection current to its longitudinal direction it can convert signal magnetic field changes to an output voltage that corresponds to the resistance change at both ends of the MR element. Based on the above structure, to either area of the positive or negative side in magnetic field Ha, corresponding to the signal magnetic field, that is the axis of abscissa of the ΔR/R curve, the points causing discontinuous jumps can be removed. As a consequence, when the MR element operating point is shifted to a point being excellent in linearity by a bias magnetic field, if such an operating point is set in the above mentioned area without discontinuous jumps in the above mentioned magnetic field Ha, magnetization switching, which occurs in the magnetic field area with a direction the same as the bias magnetic field, can be suppressed. Therefore, Barkhausen noise caused by this magnetization switching can be suppressed, and the reproduced output signal reproduced by such a YMR head can be made to be of high fidelity. In addition to this, the above mentioned DC magnetic field application system may be structured so that it applies a weak magnetic field caused by ferromagnetic exchange coupling with the MR element on the longitudinal direction of the MR element, which causes the MR element to be in a single magnetic domain condition. Because of this, the discontinuous changes of the internal magnetization in MR element can be avoided. The above mentioned DC magnetic field application system may be mace of film-thick 1000 - 2000 Å ferromagnetic film, with a large magnetic coercive force and high electric conductivity. The above mentioned conductor may be made of Al-Cu thin-film or other conductive metal thin film, and by controlling current applied to this, it causes a desirable bias magnetic field in the above MR element strip width direction, which shifts the MR element operating point to a point being excellent in linearity. The above mentioned yoke may be structured by an upper side yoke, made of 0.5 - 1.0µm permalloy, and a lower side yoke, made of highly permeable magnetic substrate, and structured so that it can form magnetic flux introduction that lead the signal magnetic field to the above mentioned MR element. The above mentioned head gap may be set at 0.2 - 0.3µm so that the signal magnetic field with about a minimum 0.5µm wave length can be reproduced from the magnetic recording medium, and structured such that spacing can be formed between the magnetic recording medium and the head gap. In addition to this, the above mentioned MR element may be structured, at manufacturing time, such that by setting its easy axis of magnetization with a 20° - 40° incline to the MR element longitudinal direction, it can ease the anisotropic axis angle dispersion condition, and attain good output characteristic in linearity. Thus, structurally, this invention inclines the easy axis of magnetization of the MR element to the MR element longitudinal direction by 20° - 40°, so all directions of the easy axis of magnetization become either almost clockwise or counterclockwise. As a result, the condition of angle dispersion of easy axis of both positive and negative directions can be relaxed. Because of this, magnetization switching that accompanies large angle dispersion of easy axis can be avoided, and the occurrence of Barkhausen noise as well can be avoided. The above mentioned MR element can make the magnetic head itself compact, and avoid non-linear characteristic in reproduced output signals with a non-complicated simple structure by only inclining the easy axis of magnetization to the longitudinal direction of MR element by 20° - 40° at manufacturing time. The invention being thus described, it will be obvious that the same may be varied in many ways. Such variations are not to be regarded as a departure from the scope of the invention. There are described above novel features which the skilled man will appreciate give rise to advantages. These are each independent aspects of the invention to be covered by the present application, irrespective of whether or not they are included within the scope of the following claims.

Claims: A yoke type thin-film magneto-resistive head comprising a magneto-resistive strip element (2) which detects signal magnetic field from a magnetic recording medium (9) by resistance change, a yoke (1, 5, 7) which leads magnetic flux from a head gap (10) to said magneto-resistive strip element, a DC magnetic field application means (3, 3) that applies weak magnetic field to said magneto-resistive strip element in the longitudinal direction, and a conductor (6) which applies bias magnetic field to said magneto-resistive strip element in the width direction, characterised in that the easy axis of magnetization of said magneto-resistive strip element (2) is inclined by 20° - 40° to the longitudinal direction of the magneto-resistive element. A yoke type thin-film magneto-resistive head according to claim 1, wherein said easy axis of magnetization is inclined by 30°-40° to the longitudinal direction of the magneto-resistive element and has a maximum angle dispersion of ± 40°. A yoke type thin-film magneto-resistive head according to claim 1 or claim 2, including means (4,4) for applying detection current in the longitudinal direction of said magneto-resistive strip element to convert signal magnetic field changes, corresponding to the resistance changes in both ends of the magneto-resistive element, to output voltage. A yoke type thin-film magneto-resistive head according to any one of claims 1 to 3, wherein said DC magnetic field application means (3, 3) is capable of causing said magneto-resistive element (2) to be in a single magnetic domain condition by applying said weak magnetic field. A yoke type thin-film magneto-resistive head according to claim 4, wherein said DC magnetic field application comprises ferromagnetic film (3, 3) disposed at both ends of said magneto-resistive strip element. A yoke type thin-film magneto-resistive head according to claim 5, wherein said ferromagnetic film (3, 3) has a thickness in the range 1000Å - 2000Å. A yoke type thin-film magneto-resistive head according to any one of the preceding claims, wherein said conductor (6) is made of Al-Cu thin-film or other conductive metal thin-film. A yoke type thin-film magneto-resistive head according to any one of the preceding claims, wherein said yoke comprises an upper yoke (1, 5), made of 0.5 - 1.0 µm permalloy film, and a lower yoke (7), made of magnetic substrate with high magnetic permeability. A yoke type thin-film magneto-resistive head according to any one of the preceding claims, wherein said head gap (10) is set at 0.2 - 0.3 µm. A yoke type thin-film magneto-resistive head according to any one of the preceding claims, wherein said magnetic recording medium (9) is made of magnetic tape or disk.

Inventors: SHIIBA, KENGO
Applicants: SHARP KABUSHIKI KAISHA
Application year: 1989
Main classification: G11B5
IPC codes: G11B5