Floating magnetic head

Abstract: A floating magnetic head has a magnetic head core (15) incorporated in a non-magnetic slider (11). The core (15) is disposed perpendicular to the plane of a magnetic disk (35). The core is bonded by glass (16) to the slider at one side of the core facing the magnetic disk, and also is bonded by a resin or bonding material to the slider at the other side of the core remote from the magnetic disk. A resin or an adhesive tape (27) is applied to the back surface of the slider, supported by a support member (26), at a predetermined ratio of the resin or the adhesive tape to the area of the back surface.

Description: This invention relates to a floating magnetic head for a magnetic disk drive, used for the storage and retrieval of data, and particularly a fixed or "hard" disk drive. An object is to provide a floating magnetic head which at least in preferred embodiments produces less noise and has improved performance and reliability. One example of a magnetic head used in a fixed magnetic disk drive is a floating magnetic head of the type in which the back side of a slider is bonded to a gimbal which is held by a load arm of the cantilever type. Such a floating magnetic head is disclosed, for example, in JP-A-1-253803 and JP-A-1-248303. The type of magnetic disk (serving as a magnetic recording medium) most commonly used heretofore comprises a substrate of an aluminium alloy coated with magnetic power of oxide. Recently, in order to meet a demand for high-density recording, there has been extensive use of magnetic disks having magnetic powder coated on a substrate by plating, sputtering or other methods. A magnetic head core for use with such a magnetic disk of a high coercive force comprises a pair of core pieces made of Mn-Zn ferrite having a high magnetic permeability at high frequency, the pair of core pieces being bonded together by primary glass. A magnetic head core 15 of a construction shown in Fig. 6 is also known. This magnetic head core 15 comprises an I-shaped core piece 21 made, for example, of Mn-Zn ferrite, and a C-shaped core piece 20 made, for example, of Mn-Zn ferrite as is the case with the core piece 21, the two core pieces 20 and 21 being bonded together by primary glass 23. A magnetic film 22a, 22b of an alloy such as Fe-Al-Si alloy is coated on the surface of at least one of the core pieces 20 and 21 by sputtering or another suitable method. A magnetic gap is provided between the joint portion between the core pieces 20 and 21. In the case where the alloy magnetic film is formed only on the core piece 20, a gap glass layer exists in the magnetic gap between this film and the surface of the core piece 21. In the case where the films are formed on both the core pieces 20 and 21, the gap glass exists between the two films. The magnetic head core 15 is attached to a slider 11 which is partly shown in Fig. 7 and is entirely shown in Fig.8. The slider 11 is of a cuboid shape having wide upper and lower surfaces of generally square shape. The slider 11 has a groove A opening to one side surface 24b thereof, core receiving grooves 14, 14 notched or formed in a pair of opposed walls defining the groove A, and pair of recesses B and C formed respectively in the central portions of the upper and lower surfaces of the slider 11. The protruding portions of the upper surface of the slider 11 either side of the recess B, and the surfaces 12 and 13 of these portions are used as air bearing surfaces. The function of the air bearing surfaces is explained here. As shown in Fig. 11, an assembly 10 formed by incorporating the core 15 into the slider 11 is used with the upper surface (having the recess B) of the slider 11 disposed in facing relation to a magnetic disk 35. When the disk 35 rotates, the upper surface of the slider 11 is very closely adjacent to the surface of the disk 35. When the disk 35 rotates at high speed, the air on the surface of the disk 35 enters an extremely small space between the slider 11 and the disk 35 due to the viscosity of the air, flows through this small space at high speed, and then is discharged from the small space. The air entry portion is formed by tapered surfaces 12a and 13a formed respectively on the surfaces 12 and 13, and the air discharge portion is formed by tapered surfaces 12b and 13b formed respectively on the surfaces 12 and 13. The high-velocity stream of the air in the microscopic space serves as the air bearing for floating the assembly 10 over the surface of the magnetic disk 35. Referring again to the manner of assembling the assembly 10, the magnetic head core 15 is inserted into the groove 14 provided at the air discharge side of the slider 11, and is provisionally retained by a spring member 31 (Fig. 7). In this condition, as shown in Fig. 7, a glass bar 28 is opposed to the groove 14 and is abutted against one side of the core 15 and part of the slider body. The glass bar 28 is heated to be softened into a fluid state, and flows into gaps 29 and 30 defined by the inner wall surfaces of the groove 14 and the core 15. The thus flown glass is cured to provide a secondary glass 16 with which the core 15 is fixed to the slider 11 (Fig. 8). Then, the bearing surfaces 12 and 13 of the assembly 10 are ground and polished. Finally, a coil (not shown) is wound on the portion defining a coil aperture 17, thereby providing the floating magnetic head with the construction as shown in Fig. 8. As shown in Figs. 9 and 10, the slider 11 of the magnetic head is bonded to a dimple point 26a of a gimbal 26 by a bonding material 27, and the gimbal 26 is held by a load arm 32 of the cantilever type in such a manner that the slider 11 is disposed in facing relation to the disk 35. The floating magnetic head of this type (Fig. 11) has been extensively used. In the above conventional floating magnetic head, core pieces of Mn-Zn ferrite having a high magnetic permeability at high frequency are used, and a coating of FE-Al-Si alloy having a high saturated flux density is used. With this arrangement, the floating magnetic head has been suitable for use in fixed disk drives of the high-density recording type. However, the density (i.e., capacity) of fixed magnetic disks, as well as the compact and high-frequency design thereof, have been improved further and new problems to be solved have arisen. A floating magnetic head supported by a cantilever-type load arm is lightly held in contact with the disk by the force of a spring 33 (Fig. 11) when the disk is stationary; however, when the disk is moving, the air on the surface of the disk moves to produce a force to lift the slider, so that the slider floats a distance of 0.2 to 0.5 µm off the disk surface. When the disk begins to rotate and when it stops, the magnetic head slides over the disk. If floating of the head is stable, stable electromagnetic conversion characteristics can be obtained. In practice, however, the slider repeatedly moves upwards and downwards a little during track seeking operations and other operations. Because of the combination of this up and down movement and the flow of the air caused by the rotating disk, the whole of the magnetic head is subjected to vibration. It is thought that this vibration is a kind of self-excited vibration in which the vibration itself applies energy to the magnetic head so as to gradually increase the amplitude of the vibration. Also, such self-excited vibration may be induced by impingement of the slider upon microscopic projections on the disk during the floating of the slider. In a known floating magnetic head, there is employed vibration-damping means, as disclosed in JP-A-63-7573, in which when the cantilever-type load arm 32 (Fig. 9) is to be fixed to a head arm 34, an adhesive tape or the like is applied to the spring 33 disposed adjacent to the proximal end of the load arm 32, thereby damping the vibration of the load arm 32. However, no measures for damping the vibration of the slider 11 per se have yet been adopted. In a conventional floating magnetic head, when the magnetic head core is to be fixedly held in the groove in the air bearing portion of the slider, the magnetic head core is fixedly bonded by the secondary glass only at the front side of the magnetic head assembly adapted to face the disk, and the four side surfaces of the magnetic head core at the back or opposite side thereof (the lower side in Fig. 8) are not fixed to the inner wall surfaces of the groove, and therefore are free. In some cases, only a part of the magnetic head core is fixed to the slider at the back side thereof to such a degree as to withstand forces produced when forming the slider; however, the magnetic head core is not completely fixed to the slider at the back side thereof. Therefore, the vibration transmitted to the magnetic head core from the slider is amplified, and the magnetic head core vibrates in a cantilever manner at a frequency different from the frequency of vibration of the slider. When the magnetic head core vibrates, it expands and contracts in directions of its height, width, eg., so that the magnetic head core is deformed. It is thought that due to this deformation, the magnetic material of the head core undergoes a reverse magneto-striction phenomenon in which its magnetized condition differs from the initial magnetized condition. In this case, it is thought that the following condition is encountered. When such reverse magneto-striction occurs, the magnetic material constituting the magnetic circuit is varied in magnetization distribution, so that the magnetic flux is changed in the magnetic head core. As a result, a voltage is produced through the coil, which constitutes a factor in the generation of noise, and the S-N (signal to noise) ratio (the ratio of the output S of the magnetic head to the noise N) and the reproduced waveform are adversely affected. Further, it is necessary to wind a coil on the portion defining the coil hole in the magnetic head core in order to generate induction magnetic field. In the case where the magnetic head core is made of Mn-Zn ferrite (particularly, Mn-Zn single crystal ferrite) having good electromagnetic conversion characteristics, when applying the coil thereto, the core may be deformed due to the load produced when the coil is wound about 20 times on the magnetic head core held in a cantilever manner. This may result in a significant risk that the magnetic head core is subjected to a cleavage fracture in a chipping is produced along the crystal plane determined by a crystal structure. It is known from JP-A-63/292411 to provide a floating magnetic head comprising: a slider of a non magnetic material having at least one air bearing surface to face a magnetic recording medium, a groove opening to one back side surface of the slider at the air discharge side of the slider, a first and a second core receiving grooves formed in a pair of opposed walls defining the said groove; a magnetic head core having a first portion, with a magnetic gap, received in a first of said grooves located on the air bearing surface side thereof, and a second portion received in a second of said grooves located in the slider on the side thereof to be remote from the magnetic recording medium; bonding means securing the first portion of the magnetic head core to the slider in the region of the first groove; bonding means for bonding the second portion of the magnetic head core to the slider in the region of the second groove. The present invention is characterised in that the bonding means for bonding the second portion of the magnetic head core to the slider in the region of the second groove is an elastic vibration-damping material. The elastic vibration-damping material is provided between at least one of the inner wall surfaces of the second groove and at least one of four side surfaces of the head core at a back side thereof. In this construction, the pair of magnetic core pieces are opposed to each other via the film of bonding glass provided at the air gap. A soft magnetic metal film may be formed on the surface of at least one of the two core pieces disposed in opposed relation to the air gap. Preferably, the height of the elastic vibration-damping material should be not less than 10% of the width (designated at w in Fig. 2) of the magnetic head core. Here, the height of the elastic vibration-damping material and the width of the magnetic head core are defined. The magnetic head is used in a manner corresponding to prior art heads with preferably the slider being held on a cantilever-type load arm via a gimbal. For example, as shown in Fig. 11, with the magnetic head core being disposed perpendicular to the plane of the magnetic disk. This perpendicular direction is the direction (Y-direction in Fig. 6) of the height of the magnetic head core, and the direction parallel to the plane of the magnetic disk is the direction (X-direction in Fig. 6) of the width of the magnetic head core. The elastic vibration-damping material may be a resin or a bonding material (or adhesives) and the like. Examples of a filler material in the resin or the bonding material comprises silica, alumina, ceramics and small pieces or powder of metal. Preferably, the filler content should be not more than 70 vol.% of the resin or the bonding material. In the above floating magnetic head, the pair of magnetic core pieces constituting the magnetic head core are made of Mn-Zn ferrite of either a polycrystal or a single crystal structure. With this arrangement, the magnetic head is more suited for use in a fixed magnetic disk device. In a conventional floating magnetic head, when the magnetic head core is to be inserted into the grooves provided at the air discharge side of the air bearing of the slider, the magnetic head core is fixed by secondary glass to the slider only at that side thereof adapted to face the disk, and the four side surfaces of the magnetic head core at the back side thereof are not completely fixed to the inner wall surfaces of the groove to be free, or is held in an almost free condition. In other words, the magnetic head core is arranged much like a cantilever-type beam or structural member having one free end and the other fixed end. On the other hand, in the floating magnetic head described herein, when the magnetic head core is to be inserted into the grooves in the slider, the magnetic head core is fixed by secondary glass to the slider at that side thereof adapted to face the disk, and further at least one of the four side surfaces of the magnetic head core at the back side thereof is fixed by an elastic vibration-damping material, such as a resin or a bonding material (or adhesives) and the like, to the inner wall surfaces of the groove in the air bearing. Therefore, the magnetic head core can be regarded as a structural member of the type in which that side of the magnetic core adapted to face the disk is fixed whereas the opposite or back side of the magnetic core is restrained by the elastic vibration-damping material. Therefore, even when the vibration of the slider propagates to the magnetic head core, the vibration is absorbed and damped by the elastic vibration-damping material provided at the back side of the magnetic head core. The resulting deformation is limited by the elastic vibration-damping material in contrast with the case where the back side is free, and therefore such deformation is much less than that of the conventional magnetic head core. As a result, the resulting reverse magneto-striction is small, and the performance and reliability of the magnetic head can be improved. Since the back side is restrained by the elastic vibration-damping material, the deformation produced when applying the coil is also small, and in the case where the magnetic core is made of Mn-Zn single crystal ferrite, the possibility of cleavage fracture produced when applying the coil is reduced. Preferably the upper limit of a filler content of the elastic vibration-damping material is limited to not more than 70 vol.%. It has been found in some cases that if the filler content exceeds 70 vol.%, the ability to absorb vibration is lowered, so that the level of produced noise becomes unacceptably high. The lower limit is not particularly defined, but desirable results are obtained with not less than 20 vol.% of the filler content. Preferably the bonding height of the elastic vibration-damping material is not less than 10% of the width of the magnetic head core. If it is less than 10%, it has been found in some cases that the vibration propagating from the slider to the magnetic head core cannot be sufficiently absorbed, so that the level of produced noise becomes unacceptably high. The upper limit of the bonding height is not so critical but it appears that its effect is saturated at about 70%. In the floating magnetic head, when the slider is to be bonded to the gimbal, preferably not less than 50% of the area of the back surface of the slider is covered with an adhesive tape or a coated resin, or not less than 50% of the back surface area of the slider bonded to the gimbal is coated with a bonding material. With this arrangement, the vibration of the slider per se is damped. Therefore, the amplitude of the vibration of the slider per se is smaller as compared with magnetic heads having no measures for damping the vibration of the slider. Furthermore the generation of self-excited vibration can be reduced or prevented. As a result, even if the magnetic head core is embedded in the grooves in the air bearing portion, and is fixed by the glass only at that side thereof adapted to face the disk with the back side of the magnetic head core being free, the vibration propagating from the slider may be small. Therefore, even when the amplitude of the vibration is amplified and also when the magnetic head core vibrates in a cantilever manner at a frequency different from that of the slider, the deformation developing in the directions of the height, width, etc., of the core is very much smaller than the deformation of a conventional magnetic head core. As a result, the resulting reverse magneto-striction is small, thereby improving the performance and reliability of the magnetic head. Thus, in a preferred embodiment of the present invention, the floating magnetic head is mounted on a cantilevered load arm via a gimbal, with resilient vibration damping means in the form of an elastic material being provided between the gimbal and the slider. In a preferred embodiment, preferably not less than 50% of the back surface of the slider is coated with an adhesive tape, a resin coating or adhesives, and preferably not less than 50% of the back surface of the slider fixed to the gimbal is coated with a bonding material or adhesives. Some embodiments of floating magnetic heads in accordance with the present invention will now be described by way of example and with reference to the accompanying drawings in which:- Fig. 1 is a perspective view of a new floating magnetic head in which a lower portion of a magnetic head core is fixed to a slider, relevant to the first and second Examples described below; Fig. 2 is an enlarged, perspective view of a portion of the magnetic head; Figs. 3A to 3H are views showing the condition in which a tape is bonded to, or a resin is coated onto a back surface of a slider, and is relevant to a third Example described below; Fig. 4 is a view showing the condition of bonding between a slider and a gimbal, and is relevant to a fourth Example described below; Fig. 5 is a cross-sectional view taken along the line V-V of Fig. 4; Fig. 6 is a perspective view of a known magnetic head core; Fig. 7 is a view showing the manner of bonding the known magnetic head core by secondary glass; Fig. 8 is a perspective view of a conventional floating magnetic head; Fig. 9 is a view showing the condition of bonding between a conventional slider and a gimbal; Fig. 10 is an enlarged, cross-sectional view taken along the line X-X of Fig. 9; and Fig. 11 is a schematic perspective view showing a conventional load arm. The basic construction of the floating magnetic head shown in Fig. 1 is generally the same as the known head shown in Fig. 8 and described earlier. Like parts of the new and known heads have been given like reference numerals, and where necessary the construction of the new head is described with reference to drawings of the known head. In a first embodiment a pair of core pieces 20 and 21 (see Fig. 6) were prepared from Mn-Zn single crystal ferrite consisting substantially of 28 mol.% MnO, 19 mol.% ZnO and the balance Fe 2 O 3 . A Fe-Al-Si type magnetic film of an alloy commonly referred to as Sendust alloy consisting of 6 wt.% Al, 8 wt.% Si and the balance being substantially Fe was coated by sputtering on that surface of the I-shaped core piece 21 facing the magnetic gap. Then the I-shaped core piece 21 was bonded to the C-shaped core piece 20 by primary glass 23 to form a magnetic head core 15. Then, this core was inserted into upper and lower grooves 14, 14 formed in an air discharge side of air bearing surfaces 12 and 13 of a slider 11 made of CaTiO 3 , and that side of the magnetic head core 15 adapted to face a disk is fixed to the slider by secondary glass 16 to prepare a floating magnetic head. The condition of generation of noise was examined. A method of measuring noise was to forcibly apply vibration to the slider from the exterior and then to stop the application of the vibration. From the time when the application of the vibration was stopped, the vibration of the slider per se began to be damped. Defining the time of stopping the application of the vibration as a start time point, a single noise generated only from the magnetic head was picked up through a reproduction circuit of the magnetic disk device, and its waveform was observed by an oscilloscope. Example 1 Magnetic head cores each fixedly held in the grooves 14 in the slider 11 were adhesively bonded at the back side thereof, with the height of bonding between the back side of the magnetic head core and the groove 14 changed variously, and a coil was wound on the portion defining a coil hole 17 of the magnetic head core 15. Then, a noise generation test was carried out. As bonding material (see reference numeral 18,19), there was used Allonalpha #2000S (trade-name of Toha Synthetic Chemical Industry Co., Ltd.; an instantaneous adhesive of cyanoacrylate type), and the filler content of the bonding material was constant, that is, 50 vol.%. With respect to the bonding at the back side, there were tested three kinds of bonding, that is, the bonding at one side surface in the direction of the width, the bonding at two side surfaces in the direction of the width, and the bonding at the two side surfaces in the direction of the width and at one side surface in the direction of the thickness. The bonding was carried out in accordance with the standard of use of Allonalpha. Results thereof are shown in Table 1. It will be appreciated from Table 1 that those magnetic heads in which the sum of the heights of the bonding surfaces is not less than 10% of the width w of the magnetic head core are clearly reduced in relative noise level as compared with the magnetic head having no bonding. However, a comparison between 40% and 70% indicates that the two magnetic heads are substantially equal in noise level to each other. Therefore, it can be concluded that the bonding up to 70% is sufficient to achieve the purpose. Sample No. Height of bonding surface Noise level 1 no bonding 100 2 5% 80 2a 5% 70 3 10% 40 3a 10% 40 4 20% 35 5a 40% 30 6b 70% 30 With respect to Sample Nos. 2, 3 and 4, one of the two side surfaces in the direction of the core width was bonded. With respect to Sample Nos. 2a, 3a and 5a, the two side surfaces in the direction of the core width were bonded. With respect to Sample No. 6, the two side surfaces in the direction of the core width and one side surface in the direction of the core thickness were bonded. The height of the bonding surface represents the ratio of the bonding height to the core width. The noise level represents the value relative to the value (100) of the magnetic head having no bonding. Example 2 Using Able-bond 410 (trade-name of Nippon Ablestick Co., Ltd; an epoxy adhesive) usually used for assembling the slider, the two side surfaces of each of magnetic head cores at the back side thereof were bonded to the air bearing groove in such a manner that the height of the bonding was generally 40% of the core width. Then, a coil was wound on the portion defining the coil hole. Then, the noise level was examined. Results thereof are shown in Table 2. Sample No. Filler content Noise level 1 no bonding 100 2 20 vol.% 25 2a 20 vol.% 20 3 50 vol.% 20 3a 60 vol.% 30 4 70 vol.% 45 5a 70 vol.% 40 6b 80 vol.% 80 With respect to Sample Nos. 2, 3, 4, 5 and 6, one of the two side surfaces in the direction of the core width was bonded. With respect to Samples Nos. 2a and 5a, both of these two side surfaces were bonded. The noise level represents the value relative to the value (100) of the magnetic head having no bonding. As is clear from Table 2, the relative noise level of those magnetic heads with the adhesive having the filler content of up to 70 vol.% is reduced to less than 50 vol.% as compared with the magnetic head whose core was not bonded at its back side. However, it will be appreciated that when the filler content exceeds 80%, the damping effect is extremely lowered. In the Examples, although two kinds of adhesives (i.e., Allonalpha and Able-bond) are used as the resin or the bonding agent, similar effects can be expected with the use of any other suitable resin and bonding agent. Example 3 An adhesive tape was bonded to a back surface 24a of the slider 11 of the magnetic head, or an epoxy resin was coated on the back surface 24a of the slider 11. A coil was applied to the slider, and the slider was attached to a gimbal 26. Then, the gimbal was held by a load arm, and the condition of generation of noises was examined. The bonding of the adhesive tape to the back surface of the slider, as well as the coating of the epoxy resin on the back surface 24a of the slider, was carried out, varying the rate of coverage of the area of the back surface 24a with the adhesive tape or the coated resin 25, as shown in Figs. 3A to 3H. Influences due to the change in the area coverage rate were examined. Results thereof are shown in Table 3. Sample No. Area coverage rate Noise level 1 no treatment 100 2 100% 20 3a 90% 20 4a 80% 25 5 65% 35 6 50% 40 7 40% 70 8a 30% 8 With respect to Sample Nos. 2, 5, 6 and 7, the adhesive tape was bonded. With respect to Sample Nos. 3a, 4a and 8a, the resin was coated. The noise level represents the value relative to the value (100) of the magnetic head subjected to no treatment. The area coverage rate represents the ratio of the covering tape or the covering resin to the entire area of the back surface 24a of the slider. As is clear from Table 3, the relative noise level can be reduced to less than 50% by covering not less than 50% of the area of the slider back surface with the adhesive tape or the coated resin. Particularly when the area coverage ratio is not less than 80%, the noise level is extremely reduced. Incidentally, the front surface or the entire side surfaces of the slider were covered with the tape or the resin, and similar tests were conducted. However, the relative noise level was 100 in the former case, and was 70 in the latter case. Thus, effects were hardly achieved. This is presumably due to the fact that the vibration of the load arm propagates to the slider via the gimbal holding it, so that the degree of damping between the slider and the gimbal is small. Example 4 A magnetic head as shown in Fig. 5 was prepared, and an adhesive 27 for bonding the gimbal 26 and the slider 11 was coated not only on the normal bonding portion (see a dimple point 26a) of the back surface 24a of the slider 11 but also on the other portion than this normal bonding portion. The rate of coverage of the area by the adhesive was varied, and the noise level was examined. Results thereof are shown in Table 4. Sample No. Area coverage rate Noise level 1 normal 100 2 30% 90 3 40% 60 4 50% 40 5 70% 25 6 80% 20 7 100% 20 The noise level represents the value relative to the value (100) of the magnetic head having the adhesive coated only on the normal portion. The area coverage rate represents the ratio of the covering adhesive to the entire area of the back surface 24a of the slider. As is clear from Table 4, as compared with the magnetic head having the adhesive coated only on the normal portion of the slider back surface, the relative noise level of those magnetic heads having the adhesive covering not less than 50% of the entire area of the slider back surface is reduced to less than 50%. Particularly when the area coverage rate is not less than 70%, the noise level is reduced markedly. In the above Examples, the adhesive tape, the coated or bonded epoxy resin were used; however, if the tape or the resin has a thickness of at least 10 µm, the intended effects can not be achieved. The upper limit of the thickness of the tape or the resin is about 200 µm, because this upper limit influences the weight of the slider. In the above Examples, although the magnetic core head is made of Mn-Zn single crystal ferrite by way of example, it may be made of polycrystal ferrite, and also may be made of any other magnetic material. The present invention can be applied to the magnetic head having no metal magnetic film or coating. As will be apparent from the above Examples, the magnetic heads, even when used in a high-density, large-capacity, compact and high-frequency fixed disk, produce less noise due to the reverse magneto-striction presumably caused by the vibration transmitted from the slider, and the S-N ratio (the ratio of the output S of the magnetic head to the noise N) is small, and the magnetic heads can produce good reproduction waveforms. Thus, the performance and the reliability of the magnetic head are improved. In certain preferred embodiments, vibration of the floating head is dampened and there is cushioning of the winding load exerted on the magnetic head core when winding a coil on the portion defining a coil hole of the magnetic core, thereby protecting the core. In the embodiments where damping means is employed between the slider and the gimbal, the area of e.g. adhesive used is significantly greater than the area over which the slider and gimbal are joined together. Adhesive is applied to the back surface of the slider over an area greater than that required for bonding. There may be variations of the broad aspects disclosed herein and of the embodiments and examples described. Protection is sought for the invention as specified in the appended claims.

Claims: A floating magnetic head comprising: a slider (11) of a non magnetic material having at least one air bearing surface (12,13) to face a magnetic recording medium (35), a groove (A) opening to one back side surface of the slider at the air discharge side of the slider, a first and a second core receiving grooves (14) formed in a pair of opposed walls defining the said groove (A); a magnetic head core (15) having a first portion, with a magnetic gap (22a), received in a first of said grooves (14) located on the air bearing surface side thereof, and a second portion received in a second of said grooves (14) located in the slider on the side thereof to be remote from the magnetic recording medium; bonding means (16) securing the first portion of the magnetic head core to the slider in the region of the first groove; bonding means (18,19) for bonding the second portion of the magnetic head core (15) to the slider (11) in the region of the second groove (14) characterised in that the means (18,19) for bonding the second portion of the magnetic head core (15) to the slider (11) in the region of the second groove (14) is an elastic vibration-damping material. A floating magnetic head as claimed in claim 1, characterised in that the elastic vibration-damping material (18,19) comprises a resin with a filler. A floating magnetic head as claimed in claim 1 or 2, characterised in that the height (h 1 ,h 2 ) of the elastic vibration-damping material (18,19) is greater than 10% of the width (w) of the magnetic head core (15). A floating magnetic head as claimed in any preceding claim, characterised in that at least one of a pair of magnetic core pieces (20,21) constituting the magnetic head core (15) has a magnetic metal film fored on a surface thereof opposed to the magnetic gap (22a). A floating magnetic head as claimed in claim 4, characterised in that the film is a Fe-Al-Si type magnetic alloy film consisting of 6 wt% of Al, 8 wt% of Si and the balance being substantially Fe. A floating magnetic head as claimed in claim 4 or 5, characterised in that the pair of magnetic core pieces (20,21) are made of single crystal of Mn-Zn ferrite. A floating magnetic head as claimed in any preceding claim, characterised in that the elastic vibration-damping material (18,19) comprises a resin containing a filler of not more than 70 vol%. A floating magnetic head as claimed in any preceding claim, characterised in that the slider (11) is mounted on a cantilever-type load arm (32) via a gimbal (26), and in that a vibration damping means (27) in the form of an elastic material is provided between the gimbal (26) and the back surface of the slider (11). A floating magnetic head as claimed in claim 8, characterised in that the elastic material (27) provided between the gimbal (26) and the back surface of the slider (11) is a resin, a bonding material or an adhesive tape. A floating magnetic head as claimed in claim 8 or 9, characterised in that the elastic material (27) provided between the gimbal (26) and the back surface of the slider (11) covers greater than 50% of the back surface of the slider (11).

Inventors: ASHIZAWA MASAAKI, GOTO RYO, ASHIZAWA, MASAAKI, GOTO, RYO
Applicants: HITACHI METALS LTD, HITACHI METALS, LTD.
Application year: 1991
Main classification: G11B5
IPC codes: G11B5