LONGITUDINAL MAGNETIC COATED RECORDING MEDIUM

Abstract: A longitudinal magnetic coated recording medium com­ prises at least plane magnetic particles (4) each having an easy magnetization axis perpendicular to the major surface thereof, preferably mixed with other particles (6), and dispersed in a magnetic film (7) formed on a nonmagnetic substrate (8), having a orientation angle ϑ of -30° to +30°. A process for producing such a recording medium comprises the step of orienting the plane magnetic particles by applying at least a magnetic field approximately in parallel to the surface of the magnetic film.

Description: BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a so-called longitudinal magnetic coated recording medium. 2. Description of the Prior Art A magnetic recording medium comprises a magnetic film which is formed on a nonmagnetic substrate and contains magnetic particles dispersed therein. The easy magnetization axis of the magnetic particles may be oriented approximately either in parallel to or perpendicular to the surface of the magnetic film. Acicular magnetic particles e.g., γ-Fe₂O₃ , are commonly used for dispersion in a magnetic film. Such magnetic particles have an easy magnetization axis in the direction of their longitudinal axis, and tend easily to orient in a direction in parallel to the surface of the magnetic film. Thus, their magnetic orientation is parallel to the surface of the magnetic film, hereinafter referred to as longitudinal orientation. When information is written in and read out of a longitudinal magnetic film by means of a ring head, the magnetic fluxes which a detecting ring head cuts are components almost parallel to the surface of the magnetic film, and the detected magnetic fluxes exhibit a normal distribution as shown by a broken line 1 in Fig. 1. On the other hand, when plane magnetic particles 4 each having an easy magnetization axis 5 perpendicular to the major surface thereof, e.g., barium ferrite, such as BaFe₁₂O₁₉, Ba₂Me₂Fe₁₂O₂₂ , Ba₃Me₂Fe₂₄O₄₁ , Ba₃Co 1.92 Fe 0.08 Fe₂₄O₄₁ as shown in Fig. 2, are dispersed in a magnetic film, the major surface of the plane magnetic particles tends to be arranged in parallel to the surface of an aluminum or polyester substrate particularly when the substrate is a disc which rotates during spin-coating. In this case, the easy magnetization axis 5 of the plane magnetic particle 4 is oriented perpendicular to the surface of the magnetic film. In such a case, the detected fluxes exhibit an abnormal asymmetric distribution, as shown by a one-point broken line 2 in Fig. 1. Furthermore, a practical magnetic recording medium, which contains perpendicular barium ferrite particles, has a certain amount of longitudinal magnetic components. Thus, the broken line 1 and one-point broken line 2 are synthesized, and thereby the detected curve is deformed as shown by a solid line 3 in Fig. 1, and the peak of the detected flux is dislocated from the original point. It is necessary to pass the detected signal through a correction circuit which comprises a delay circuit, an attenuator, etc., prior to the writing and reading of information. In addition,the output and practical recoding density are inevitably low. The hexagonal crystal platelets with easy magnetization axes normal to their planes such as barium ferrite BaFe₁₂O₁₉ etc are recognized to be effective for improving the recording density. However, barium ferrite is not practically used to produce a perpendicular recording medium due to the above-mentioned defects. Furthermore a longitudinal magnetic coated recording medium comprising barium ferrite is not realized, because it is difficult to form a longitudinal magnetic film therefrom. Wada et al to Toshiba Denki K.K. disclose in Japanese Unexamined Patent Publication No. 57-212623 a magnetic recording medium which contains barium ferrite type magnetic particles with an average size of at most 0.3 µm in an amount of at least 50% by weight of the total magnetic particles, and γ-Fe₂O₃ type or cobalt type magnetic particles with an average size of at most 0.4 µm. However, Wada et al do not teach or suggest to apply a magnetic field prior to drying the magnetic paint. Kishimoto et al to Hitachi Maxell K.K. disclose in Japanese Unexamined Patent Publication No. 59-129933 a magnetic recording medium which contains barium ferrite magnetic particles having an easy magnetization axis perpendicular to the major surface thereof and other magnetic particles having an isometric magnetic axis. However, Kishimoto et al teach to apply solely a magnetic field perpendicular to the surface of the film base, thereby forming a perpendicular magnetic coated recording medium. Taniguchi to Hitachi Maxell K.K. discloses in Japanese Unexamined Patent Publication No. 52-141612 a process for producing a magnetic recording medium wherein the surface of a substrate is coated with a magnetic paint, and passed through a magnetic field which arranges the magnetic particles, e.g., γ-Fe₂O₃ , dispersed in the magnetic paint in parallel to the running direction of the substrate, and then the paint is dried. However, Taniguchi does not refer to plane magnetic particles having an easy magnetization axis perpendicular to the major surface thereof. Ishida et al to Fujitsu K.K. disclose in Japanese Unexamined Patent Publication No. 54-9905 a process for producing a magnetic recording disc, comprising the steps of: forming a magnetic film containing isometric magnetic particles, i.e., γ-Fe₂O₃ , on the disc, applying a magnetic field perpendicular to the surface of the disc, and then applying an intrafacially orienting magnetic field parallel to the running direction of the disc. However, Ishida et al do not teach or suggest to apply a longitudinal magnetic field solely or alternate with a perpendicular magnetic field to a plane magnetic powder having an easy magnetization axis perpendicular to the major surface thereof. Yokoyama et al to Toshiba Denki K.K. disclose in Japanese Unexamined Patent Publication No. 58-6526 a magnetic recording medium produced by painting a resinous compound comprising plane magnetic particles each having an easy magnetization axis perpendicular to the major surface of the particle, e.g., hexagonal ferrite crystals, with thickness of at most 0.2 µm, and the ratio of diametric size to thickness of at least 2, the particles being magnetically arranged in the moving direction of a magnetic head. However, Yokoyama et al do not teach the process whereby the plane magnetic particles are oriented, except that a magnetic field of 2 kOe is applied to a polyethylene film coated with the magnetic resin and calendered to form a recording tape having a ratio of residual magnetization to saturation magnetization of 0.9. Yokoyama et al do not refer to the orientation angle, which the inventors originally defined as an angle where the ratio of residual magnetization to saturation magnetization Mr/Ms is the largest. In addition, it seems that the ratio of residual magnetization to saturation magnetization is 0.9, which appears to be too large to be actually attained. Moreover, the magnetic medium with barium ferrite particles magnetically arranged in the moving direction of a magnetic head, inevitably contains many pinholes, and, therefore, we believe it can not be put into practical use as it is. SUMMARY OF THE INVENTION It is an object of the present invention to provide a magnetic recording medium which dispenses with the correction of an output wave. It is another object of the present invention to provide a magnetic recording medium which exhibits a high recording characteristic, i.e., a high value in the product of output and recording density. It is still another object of the present invention to provide a magnetic recording medium which exhibits reduced noise. It is yet another object of the present invention to provide a process for producing a longitudinal magnetic coated recording medium which exhibits the advantages set forth above. These objects are attained by a longitudinal magnetic coated recording medium as defined in claim 1. The process by which such a medium can be obtained is defined in claim 5. Barium ferrite and strontium ferrite are typical plane magnetic particles each having an easy magnetization axis 5 perpendicular to the major surface of the particle 4, as shown in Fig. 2. These particles are dispersed in a magnetic paint which is applied on a substrate. The ratio of diametric size to thickness of the plane magnetic particles may be more than 3.5, and the diametric size thereof may be in the range of 0.1 to 0.3 µm. In order to orient the easy magnetization axis of the plane magnetic particles in parallel to the surface of the magnetic film, it is necessary for the plane magnetic particles to be stood up-right by applying a magnetic field substantially in parallel to the surface of the magnetic film until the magnetic paint dries. On the other hand, in order to distribute the plane magnetic particles uniformly throughout the magnetic film, it is preferable to alternately apply a magnetic field substantially in parallel to the surface of the magnetic film and another magnetic field perpendicular to the surface of the magnetic film prior to the drying step. Particularly in the case of a disc substrate, it is also advantageous to apply a magnetic field perpendicular to the surface of the magnetic film during the coating step, thereby avoiding an uneven accumulation of the plane magnetic particles. In order to prevent the occurrence of pin holes on the surface of the magnetic film, it is advisable to prepare a magnetic paint in which other particles in an amount of 10 to 30% based on the total weight of the plane magnetic particles and the other particles are dispersed. The other particles set forth above may have a size in the range of from 0.05 to 0.4 µm, and be either magnetic particles such as γ-Fe₂O₃ and cobalt adsorbed γ-Fe₂O₃ , or nonmagnetic particles such as α-Fe₂O₃ , α-Al₂O₃ and SiO₂. It is convenient if a magnetic paint is prepared by blending a paint of the plane magnetic particles, and another paint of the other particles. Thus, each of the two kinds of particles are uniformly dispersed in the paints, respectively. When the recording medium is a disc, which is spun-coated with a magnetic paint, it is advantageous to rotate the disc at a peripheral speed of at most 7 m/s, in order to avoid dropping of the plane magnetic particles, and, to rotate the disc in the orientation step at a speed lower than in the coating step. The longitudinal magnetic coated recording medium according to the present invention essentially exhibits an output wave having a symmetrical normal distribution as shown by the broken line 1 in Fig. 1, contrary to the perpendicular magnetic coated recording medium, and thus, dispenses with wave correction. In addition, this longitudinal magnetic coated recording medium exhibits a low noise and a high output. Although the recording density is somewhat lower than the conventional perpendicular recording medium, the practical recording density at which the peak-shift has a 10% deviation is higher than that of the perpendicular recording medium. The recording performance, defined as the product of output and recording density, is also higher than that of the perpendicular recording medium. We found that this recording characteristic exhibits a desirable value when the orientation angle is in the range of from -30° to +30°. The orientation angle is defined herein as an angle at which the orientation degree, i.e., the ratio of residual magnetization to saturation magnetization Mr/Ms, is largest, and the orientation angle is determined as the angle between the film plane and easy axis of magnetization. The longitudinal magnetic coated recording medium according to the present invention preferably exhibits the Mr/Ms ratio, in the direction parallel to the surface of the magnetic film, of at least 0.65, and/or the coercive forces H c in the direction parallel and perpendicular, respectively, to the surface of the magnetic film are approximately equal in the range of ±5%. As shown in Fig. 15, in the relationships between the recording density and output, referring to magnetic films containing longitudinally oriented barium ferrite (Ba-L) particles, longitudinally oriented 20% by weight of cobalt adsorbed γ-Fe₂O₃ mixed barium ferrite (Ba+Co-L) particles, longitudinally oriented cobalt adsorbed γFe₂O₃ (Co-L) particles, and perpendicularly oriented barium ferrite (Ba-P) particles, respectively, the Ba+Co-L particles show a higher cut put than those containing Ba-P and Ba-L particles, and the recording density thereof is much larger than that containing the longitudinally oriented Co-L particles. The recording density, practical recording density at which the peak-shift has a 10% deviation, and the ratio of the latter to the former referring to the magnetic films set forth above are shown in Table 1, below. Disk D₅₀ (kFRPI) D PS.10 (kFRPI) D PS.10 /D₅₀ (%) Ba-P 62 37 60 Ba-L 51 42 82 Ba+Co-L 46 42 91 Co-L 28 27 96 BRIEF DESCRIPTION OF THE DRAWINGS Figure 1 is a diagram of output waves detected by a ring head; Fig. 2 is a perspective view of a plane magnetic particle having an easy magnetization axis perpendicular to the major surface of the plane; Fig. 3 is a diagram of the process for producing a longitudinal magnetic coated recording disc; Fig. 4(A) is an oscillograph of an output wave of a longitudinal magnetic coated recording disc; Fig. 4(B) is an oscillograph of an output wave of a perpendicular magnetic coated recording disc; Fig. 5(A) is a sectional view of a film containing a cobalt adsorbed γ-Fe₂O₃ filler blended with barium ferrite; Fig. 5(B) is a sectional view of a film containing barium ferrite alone; Fig. 6(A) is a photomicrograph of the surface of a longitudinal magnetic coated recording disc, in which the magnetic film contains a cobalt adsorbed γ-Fe₂O₃ filler; Fig. 6(B) is a photomicrograph of the surface of a longitudinal magnetic coated recording disc, in which the magnetic film contains barium ferrite alone; Fig. 7 is a graph showing the relationship between the frequency and noise of longitudinal and perpendicular magnetic coated recording discs; Fig. 8 is another diagram of a process for producing a longitudinal magnetic coated recording disc; Fig. 9 is a sectional view of a magnetic film indicating the direction of orientation angle; Fig. 10 is a graph showing the relationship between recording characteristic and orientation angle; Fig. 11 is a graph showing the relationship between recording characteristic and longitudinal and perpendicular coercive forces; Fig. 12 is a graph showing the relationship between output and degree of longitudinal orientation; Fig. 13 is a graph showing the relationship between recording density and degree of longitudinal orientation; Fig. 14 is a graph showing the relationship between degree of longitudinal orientation and recording characteristic; and Fig. 15 is a graph showing the relationship between recording density and output. DESCRIPTION OF THE PREFERRED EMBODIMENTS The present invention will be more readily understood by reference to the following detailed description taken in conjunction with the accompanying drawings. The following examples refer to magnetic recording discs, and thus include parameters of centrifugal force, i.e., number of rotations which correspond to the circular speed of the disc. Example 1 Hexagonal plane barium ferrite particles 4 as shown in Fig. 2 having diametric size (d) of about 0.2 µm, and thickness (t) of about 0.02 µm were used as magnetic particles, and a magnetic paint was prepared according to the composition shown in Table 2. An aluminum disc 20.3 cm in diameter was spun-coated with the magnetic paint at 300 rpm and, thereafter, excess magnetic paint was flown off at 600 rpm which corresponds to about 6.5 m/s peripheral speed. Then, the rotation was slowed to 2 to 5 rpm as shown in Fig. 3, and this slow rotation maintained for about one minute, in order to prevent the plane surface of the particles from lying parallel to the surface of the magnetic film due to the centrifugal force. During the slow rotation, a 4 kOe longitudinal magnetic field was applied in parallel to the surface of the magnetic film. After the one minute period set forth above had elapsed, the rotation was raised again to 600 rpm, while application of the longitudinal magnetic field was maintained. Thus, the easy magnetization axis of the plane magnetic particles was oriented in parallel to the surface of the magnetic film, and the magnetic film was dried up, thereby forming a so-called longitudinal magnetic film about 0.5 µm in thickness. Thus produced magnetic recording disc was tested by means of an Mn-Zn ring-head of 0.2 µm gap length. The write and read characteristics, i.e., output, recording density, recording density at ±10% peak-shift, and overwrite at 15/30 kFRPI with the same current of 35 mA were determined, as shown in column (A) of Table 3. Corresponding data obtained from a conventional perpendicular magnetic coated recording disc, which was produced by a process similar to that set forth above except for applying a magnetic field perpendicular to the surface of the magnetic film, are shown in column (B) of Table 3. Thus a longitudinal magnetic coated recording disc exhibits a much higher output and a higher recording density after calibration of peak-shift and a better overwrite characteristic than those of the perpendicular magnetic coated recording disc. Figures 4(A) and (B) are oscillograph diagrams of the output of a magnetic recording disc detected by means of a ring head, respectively. The curve (A) is obtained by a longitudinal magnetic coated recording disc, and exhibits a symmetrical curve. Contrary to this, a conventional perpendicular magnetic coated recording disc exhibits an asymmetric curve (B). Example 2 Hexagonal plane barium ferrite particles similar to those used in Example 1, were mixed with acicular cobalt absorbed γ-Fe₂O₃ filler particles 6, as shown in Fig. 5 having a mean size of 0.3 to 0.4 µm in a weight ratio of 4:1, and a magnetic paint was prepared according to the composition shown in Table 4. The process of spin-coating the magnetic paint, orientation of the barium ferrite particles, and drying the magnetic paint were carried out in a manner similar to those of Example 1. A magnetic film 7 formed on the disc 8 as shown in Fig. 5(A) exhibits a uniform surface structure under a microscope as shown in Fig. 6(A). Contrary to this, the magnetic recording disc obtained in Example 1 exhibits pin-holes 9, as shown in Figs. 5(B) and 6(B) on the surface, which cause the generation of noise. Thus, the magnetic film 7 eliminates the pin-holes 9 where the plane magnetic particles 4 are not densely arranged. This magnetic recording disc was tasted as follows. A 10 kOe magnetic field was applied parallel to the surface of the disc, and the ratio of residual magnetization to saturation magnetization in the longitudinal direction Mr/Ms// was measured by means of a vibrated sample magnetic meter. The disc rotated at a speed of 20 m/s, and the recording density was determined by means of a Mn-Zn ring head having a gap length of 0.3 µm, and noise was integrated in the region of up to 10 MHz after DC erasing. These characteristic values are shown in column (A) in Table 5, and those obtained by the disc of Example 1 are shown in column (B) in Table 5. The noise is reduced to half of that obtained by the magnetic recording disc of Example 1 as shown by curve (A) in Fig. 7, as compared with curve (B) which is obtained by a magnetic recording disc according to Example 1. In the diagram, curve (C) represents amplifier noise. Example 3 Hexagonal plane barium ferrite particles having a diametric size of about 0.2 µm and a thickness of about 0.01 µm were mixed with nonmagnetic α-Fe₂O₃ particles having a mean size of about 0.3 to 0.4 µm in a weight ratio of 4:1, and a magnetic paint was prepared according to the composition shown in Table 3, except for replacing cobalt adsorbed γ-Fe₂O₃ with α-Fe₂O₃. A longitudinal magnetic coated recording disc was produced similar to Example 2, and the obtained recording properties were similar to those of Example 2. Example 4 Hexagonal barium ferrite particles having a diametric size of about 0.2 µm and a thickness of about 0.02 µm was mixed with other components to prepare a paint of the composition shown in Table 6. A filler paint was prepared using cobalt adsorbed γ-Fe₂O₃ particles having a mean size of at most 0.2 µm, according to the composition shown in Table 6(B). These paints were blended in a sand grinder for 3 hours, and then the same amount of the two paints was mixed and blended again in a sand grinder for 3 hours, whereby a magnetic paint having a viscosity of 0.9 poise was prepared. Then, a longitudinal magnetic coated recording disc was produced similar to the process of Example 1. Using a ring head having a gap length of 0.2 µm, noise was detected in the frequency range of up to 10 MHz. The noise was 4.5 µVrms. Contrary to this, in the case the compounds shown in Tables 6(A) and (B) were previously mixed and blended for 6 hours, and thus the magnetic paint was prepared in one step. The noise was 5.5 µVrms. Example 5 A filler paint was prepared having a similar composition as shown in Table 6(B), except that cobalt adsorbed γ-Fe₂O₃ was replaced with nonmagnetic α-Fe₂O₃ having a mean size of 0.3 to 0.4 µm. The filler paint was blended with the paint obtained according to the composition shown in Table 6(A). Thus, a magnetic recording disc was produced similar to the process of Example 4. The noise was 6.2 µVrms, as compared with 8.0 µVrms from a disc in which the magnetic paint was prepared in one step. Example 6 A barium ferrite magnetic paint and an α-Fe₂O₃ filler paint were prepared according to the compositions shown in Table 7(A), and 7(B), respectively. and were blended as in Example 4. Thus, a magnetic paint was prepared and a longitudinal magnetic coated recording disc was produced in a process similar to Example 4. The noise was 6.6 µVrms, as compared with 8.0 µVrms obtained by a disc, in which the magnetic paint was prepared in one step. Example 7 A barium ferrite paint and an α-Al₂O₃ filler paint were prepared according to the compositions shown in Table 8(A) and (B), respectively. and were blended as in Example 4. Thus, a magnetic paint was prepared, and a longitudinal magnetic coated recording disc was produced in a process similar to Example 4. The noise was 6.6 µVrms, as compared with 8.0 µVrms obtained by a disc, in which the magnetic paint was prepared in one step. Example 8 An aluminum disc of 20.3 cm diameter was spun-coated with the same magnetic paint prepared according to the composition of Example 1, and as shown in Fig. 8, the disc was rotated at 400 rpm, and thereafter at 700 rpm to flow off excess paint, and a magnetic field was applied perpendicular to the surface of the disc, thereby the plane particles of barium ferrite were uniformly distributed on the disc. The rotation was slowed to 3 ∼ 5 rpm, and magnetic fields longitudinal and perpendicular to the surface of the disc were alternately, respectively, applied for 5 minutes, whereby the orientation of the major surface of the plane particles was alternately changed to prevent mutual coagulation of the particles. Thereafter, the perpendicular magnetic field was cut and only the longitudinal magnetic field was applied, the rotation was again raised to 700 rpm, and the magnetic paint was dried. The obtained magnetic recording disc exhibits a degree of longitudinal orientation Mr/Ms of 0.70 and a recording density of 53 kFRPI. Example 9 A magnetic paint of the composition shown in Table 4, Example 2 was applied on an aluminum disc 20.3 cm in diameter. During the spin-coating, no magnetic field was applied to the disc which was rotated at 500 rpm. The orientation and drying steps were carried out as in Example 2. The obtained longitudinal magnetic coated disc exhibited the parameters shown in Table 9. Example 10 Various longitudinal magnetic coated recording discs were produced as in Example 2, except that the rotation speed in the coating steps was changed in the range of 300 to 1500 rpm. A 10 kOe magnetic field was applied at various angles from the surface of the magnetic film. The ring head had a gap length of 0.2 µm. The ratio of residual magnetization to saturation magnetization Mr/Ms, i.e., degree of longitudinal orientation was determined for each disc. Among the angles the angle ϑ, in which the value Mr/Ms is largest was defined as the orientation angle, and denominated minus in the case the orientation angle ϑ declines in the opposite direction in which the magnetic flux from the ring head 10 curves, as shown in Fig. 9. The output e₀ and recording density D₅₀ were detected by means of the ring head set forth above and their product was calculated for each disc. Their product values were plotted against the orientation angle in Fig. 10. The vertical axis is relatively graduated by setting the product of output e₀ and recording density. It was found that the desirable values of the product of output e₀ and recording density D₅₀ fall within the range of an orientation angle of from -30 to +30°, as shown in Fig. 10. The longitudinal magnetic coated recording disc produced by applying 600 rpm in Example 1 exhibited an orientation angle of 0°, when the orientation degree, recording density and output were detected similarly, except that a ring head having a gap length of 0.5 µm was used. Example 11 Longitudinal magnetic coated recording discs were produced according to Examples 1 and 2 except for changing the rotation speed. The degree of orientation, and recording density D₅₀ were determined as in Example 2. The output e₀ and longitudinal and perpendicular coercive forces Hc were also determined. The product of output e₀ and recording density D₅₀ was calculated to obtain a recording characteristic value. Figure 11 shows the relationship between longitudinal and perpendicular coercive forces Hc// and Hc ⊥, and the recording characteristic values are marked as □, o and ×, when the values are at least 50 mV kFRPI, 40 to 50 mV × kFRPI, and less than 40 mV × kFRPI, respectively. A Ba curve was obtained by barium ferrite discs, and a Ba + α curve was obtained by barium ferrite mixed with cobalt adsorbed γ-Fe₂O₃ discs. Both curves exhibited □ marks in the area in which the longitudinal an perpendicular coercive forces Hc// and Hc ⊥ are approximately equal to 700 Oe. Example 12 Longitudinal magnetic coated recording discs were produced according to Example 1, except for changing the rotation speed. The ratio of residual magnetization to saturation magnetization Mr/Ms in the longitudinal direction was determined as in Example 2. The output e₀ and recording density D₅₀ were determined by means of a ring head having a gap length of 0.2 µm, while the discs were rotated at a peripheral speed of 12.4 m/s. The output e₀ sharply increases, as shown in Fig. 12, and the recording density gradually decreases as shown in Fig. 13, with the increase in degree of longitudinal orientation. The product of output e₀ and recording density D₅₀ is 40 mV kFRPI, when the degree of longitudinal orientation is at least 0.65, as shown in Fig. 14.

Claims: A longitudinal magnetic coated recording medium comprising at least plane magnetic particles (4), each having an easy magnetization axis perpendicular to the major surface thereof and dispersed in a magnetic film (7) formed on a nonmagnetic substrate (8), the orientation angle being in the range of from -30 o to +30 o , said orientation angle being defined as an angle where the orientation degree, that is, the ratio of residual magnetization to saturation magnetization Mr/Ms, is largest, and said orientation angle being determined as the angle between the film plane and the axis of easy magnetization characterized in that said magnetic film (7) contains other particles (6) with a size in the range of 0.05 to 0.4 µm which are either magnetic particles of γ-Fe₂O₃ or cobalt adsorbed γ-Fe₂O₃, or nonmagnetic particles of α-Fe₂O₃, α-Al₂O₃ or SiO₂, mixed with said plane magnetic particles (4) in an amount of 10 to 30% based on the total weight of said plane magnetic particles and said other particles. A recording medium according to claim 1, characterized in that the orientation degree of said magnetic film, that is, the ratio of residual magnetization to saturation magnetization Mr/Ms in the direction parallel to the surface of said magnetic film, is at least 0.65, and/or that the coercive forces Hc in the direction parallel and perpendicular to the surface of said magnetic film, respectively, are equal in the range of ±5%. A recording medium according to claim 1, characterized in that said plane magnetic particles (4) are hexagonal crystals selected from the group of barium ferrite and strontium ferrite. A recording medium according to claim 1, characterized in that the diametric size of said plane magnetic particles (4) is in the range of 0.1 to 0.3 µm. A process for producing a longitudinal magnetic coated recording medium according to any of of claims 1 to 4, characterized by comprising the steps of : preparing a magnetic paint in which are dispersed said plane magnetic particles (4) each having an easy magnetization axis perpendicular to the major surface thereof and said other particles (6) in an amount of 10 to 30% based on the total weight of said plane magnetic particles (4) and said other particles; coating a nonmagnetic substrate (8) with said magnetic paint, thereby forming a magnetic film thereon; applying at least a magnetic field approximately parallel to the surface of said magnetic film (7) in the direction where said magnetic film moves relative to a magnetic head, at an area where the easy magnetization axis of said plane magnetic particles (4) dispersed in said magnetic film is to be oriented; and drying said magnetic paint, while continuing to apply said magnetic field similarly to the orientation step set forth above. A process according to claim 5, characterized by applying solely a magnetic field approximately parallel to the surface of said magnetic film (7) during the orientation step. A process according to claim 5, characterized by alternately applying a magnetic field approximately parallel to the surface of said magnetic film (7), and another magnetic field perpendicular to the surface of said magnetic film (7) at an area where the easy magnetization axis of said plane magnetic particles dispersed in said magnetic film is to be oriented, during the orientation step. A process acording to claim 5, characterized by applying a magnetic field perpendicular to the surface of said magnetic film (7) during the coating step. A process according to claim 5, characterized by preparing a paint in which said plane magnetic particles (4) are dispersed and another paint in which said particles (6) different from said plane magnetic particles are dispersed, and then blending the two paints, thereby preparing a magnetic paint. A process according to claim 5, characterized by preparing said other paint so that there are dispersed therein magnetic particles (6) of acicular γ-Fe₂O₃ or cobalt adsorbed γ-Fe₂O₃. A process according to claim 5, characterized by preparing said other paint so that there are disposed therein nonmagnetic particles (6) selected from the group of α-Fe₂O₃, α-Al₂O₃ and SiO₂. A process according to claim 5, characterized by rotating a disc as said substrate at a peripheral speed of at most 7 m/s throughout the steps of coating, orientation, and drying. A process according to claim 12, characterized by rotating said disc during the orientation step at a speed lower than in the coating step.

Inventors: FUKUSHIMA, SHIGERU, ITOH, KEN-ICHI, NARUMI, TOSHIKATU, OGAWA, SEIYA, TAKAHASHI, JUN
Applicants: FUJITSU LIMITED
Application year: 1986
Main classification: G11B5
IPC codes: G11B5