Magneto-optical medium

Abstract: A magneto-optical recording medium (10) having a recording layer (13), a reproducing layer (11) and an intermediate layer (12) for magnetically coupling the recording layer (13) and the reproducing layer (11) in a stationary state, in which the magnetic coupling between the recording layer (13) and the reproducing layer (11) is lost in an area (14) in which a temperature is increased to be higher than a predetermined temperature by the radiation of a light upon reproducing and in which a recorded information held in the recording layer (13) is read out from the reproducing layer (11) in the radiated area (5) except the area in which the magnetic coupling is lost. This magneto-optical recording medium (13) is characterized in that a Curie temperature of the intermediate layer (12) is selected to be 150°C or more. Also, an apparatus for recording and/or reproducing a magneto-optical recording medium (10) is provided.

Description: BACKGROUND OF THE INVENTION Field of the Invention The present invention relates to a magneto-optical recording medium according to the preamble of claim 1. Description of the Prior Art A magneto-optical disc in which an information is erasable has a magneto-optical recording layer. When this magneto-optical layer is irradiated with a laser beam and then heated, the magnetization direction (recording pit) of the heated portion is converted into a magnetization direction corresponding to the external magnetic field associated with a recording information, thereby the information signal being recorded. Upon playback, the recorded information signal is played back by effectively utilizing a Kerr effect in which a laser beam is irradiated on the track of the recording pit and a polarized plane of a reflected light is rotated by the magnetization direction. When a magneto-optical disc is formed as a bilayer or more magneto-optical disc having a reflecting layer in addition to the magneto-optical layer, a Faraday effect also is utilized. A recording linear density of an information on the magneto-optical disc is determined by a carrier-to-noise (C/N) ratio of a reproduced signal. In the magneto-optical recording and/or reproduction of the conventional magneto-optical disc (hereinafter this conventional magneto-optical disc is referred to as an MO disc), as shown in FIG. 8, substantially the whole area of a beam spot 5, i.e., the laser beam light radiated area on the MO disc is employed as a reproduced signal detection area so that the linear recording density of the MO disc, which can be reproduced, is determined by the spot diameter of the laser beam. If a diameter d of the laser beam spot 5 is smaller than a pitch τ of a recording pit 4 as shown in FIG. 8A, then two recording pits 4 cannot enter the laser beam spot 5 and a reproduced output has a waveform shown in FIG. 8B, thus making it possible to read the reproduced signal. However, as shown in FIG. 8C, if the recording pits 4 are formed at high density and the diameter d of the laser beam spot 5 becomes larger than the pitch τ of the recording pit 4, then two recording pits 4, for example, enter the same laser beam spot 5 simultaneously and therefore the waveform of the reproduced output becomes substantially constant as shown in FIG. 8D. As a consequence, the two recording pits 4 cannot be reproduced separately and the reproduction becomes impossible. The spot diameter d depends upon a wavelength λ of the laser beam and an numerical aperture NA of an objective lens. Accordingly, it has been proposed to make the recording high in density by utilizing a laser light of short wavelength λ or by reducing the spot diameter d of the laser beam by increasing the numerical aperture NA of the objective lens. However, these proposals have unavoidable limits from from a laser light source and optical system standpoint and these unavoidable limits hinder the magneto-optical disc from becoming high in recording density. Similarly, a track density is mainly restricted by a crosstalk component from adjacent tracks. In the prior art, the amount of the crosstalk component depends upon the laser beam spot diameter d , which also hinders the the magneto-optical disc from becoming high in recording density. The assignee of the present application has previously proposed a novel magneto-optical disc in which a readable linear recording density and the track density can be increased without varying the laser beam spot diameter and a method of reproducing such novel magneto-optical disc (see EP-A-0 415 449 A2 which falls within the terms of Art. 54(3)). This novel magneto-optical disc will hereinafter be referred to as an MSR (magneto-optical super resolution) disc. In this MSR disc, by effectively utilizing a temperature distribution provided by the relative movement of the magneto-optical recording medium and the reproducing laser spot 5, the recording pit 4 of the magneto-optical recording medium is allowed to occur only in a predetermined temperature area upon playback, thereby a resolution in the playback being increased. As an example of MSR disc reproducing system, a so-called-rear aperture detection type reproducing system and a so-called front aperture detection type reproducing system are proposed. Initially, the rear aperture detection type MSR disc reproducing system will be described with reference to FIGS. 2A and 2B. FIG. 2A is a schematic top view illustrating a recording pattern of a magneto-optical recording medium 10 and FIG. 2B is a schematic cross-sectional view illustrating the magnetization state of the magneto-optical recording medium 10. In this case, as shown in FIG. 2A, the magneto-optical recording medium 10 is relatively moved in the direction shown by an arrow D relative to the laser beam spot 5 formed by the laser beam. As shown in FIG. 2B, for example, the magneto-optical recording medium 10, e.g., magneto-optical disc having a reproducing layer 11 formed of at least a vertical magnetization layer and a recording layer 13 and, more preferably, an intermediate layer 12 interposed between the two layers 11 and 13 is employed. In FIG. 2B, solid line arrows schematically indicate the directions of the magnetic moment and in the illustrated example, the downward arrows indicate initial state, e.g., "0" in binary value. Further, in FIG. 2B, the upward arrows, i.e., magnetic domains formed by the upward magnetization indicate "1" of binary value and in this state, an information recording pit 4 is formed at least on the recording layer 13 in the form of "1". A reproducing mode in such magneto-optical recording medium 10 will be described below. Initially, by the application of an initialized magnetic field Hi from the outside, the reproducing layer 11 is magnetized in the downward direction in FIG. 2B and is thereby initialized. That is, although the recording pits are lost in the reproducing layer 11, the magnetization directions of the reproducing layer 11 and the recording layer 13 are held in the opposite direction by magnetic walls produced in the intermediate layer 12 at the portion where the recording pits 4 are formed so that the recording pit 4 is left as a latent image recording pit 81. On the other hand, the magneto-optical recording medium 10 is supplied at least at its reproducing portion with a reproducing magnetic field H, whose direction is opposite to that of the initialized magnetic field H;. In this state, when the area having the latent image recording pit 81 thus initialized is entered under the laser beam spot 5 in accordance with the movement of the medium 10 and the portion whose temperature is increased by the irradiation of laser beams is moved to the top of the under side of the beam spot 5, i.e., to the left of FIG. 2, then a high temperature area 14 is substantially produced on the top of the spot 6 as shown by a hatched area a in FIG. 2A. In this high temperature area 14, the magnetic wall of the intermediate layer 12 is lost and the magnetization of the recording layer 13 is transferred to the reproducing layer 14 by an exchange force, whereby the latent image recording pit 81 existing in the recording layer 13 is embossed on the reproducing layer 11 as the reproducible recording pit 4. Accordingly, if the rotation of the polarizing plane of the laser beam spot 5 by the Kerr effect due to the magnetization direction in the reproducing layer 11 or due to the Faraday effect is detected, then the recording pit 4 can be read out. At that time, in a low temperature area 15 within the laser beam spot 5 except the high temperature area 14, the latent image recording pit 81 is not embossed on the reproducing layer 11 and therefore the readable recording pit 4 exists only in the high temperature area 14 of narrow width. As a consequence, even when a plurality of recording pits 4 are entered into the laser beam spot 5, that is, even in the magneto-optical recording medium 10 of high density recording type, only the signal recording pit 4 can be read out, which can make it possible to perform the reproduction of high resolution. In order to carry out the above-mentioned playback of high resolution, the initialized magnetic field H i , the reproduced magnetic field H r , coercive force of each magnetic layer, thickness, magnetization, magnetic wall energy or the like are selected in response to temperatures of the high temperature area 14 and of the low temperature area 15 within the laser beam spot 5 More specifically, assuming that H C1 represents a coercive force of the reproducing layer 11, M S1 a saturated magnetization thereof and h 1 a film thickness thereof, then a condition for initializing only the reproducing layer 11 is given by the following equation (1): Hi > H C1 + ρ W2 /2M S1 h 1 where ρ W2 is the magnetic wall energy between the reproducing layer 11 and the recording layer 13. Further, assuming that H C3 represents a coercive force of the recording layer 13, M S3 a saturated magnetization thereof and h 3 a film thickness thereof, then a condition such that the information of the recording layer 13 is maintained by the magnetic field is given by the following equation (2): Hi < H C3 - ρ W2 /2M S3 H 3 In order to maintain the magnetic wall provided by the intermediate layer 12 between the reproducing layer 11 and the recording layer 13 even after the initialized magnetic field Hi, the condition expressed by the following equation (3) must be established: H C1 > ρ W2 /2M S1 H 1 Then, at a temperature T H selected within the high temperature area 14, the condition expressed by the following equation (4) must be satisfied: H C1 - ρ W2 /2M S1 H 1 < H r < H C1 + ρ W2 /2M S1 h 1 By the application of the reproducing magnetic field H r which can establish the above-mentioned equation (4), the magnetization of the latent image recording pit 81 of the recording layer 13 can be transferred, i.e., embossed as the recording pit 4 on the reproducing layer 11 only at its portion where the magnetic wall provided by the intermediate layer 12 exists. While the magneto-optical recording medium 10 of the MSR type is composed of the reproducing layer 11, the intermediate layer 12 and the recording layer 13 in a trilayer structure, the magneto-optical recording medium 10 is not limited to the trilayer structure and may be applied to a four-layer structure in which a reproducing auxiliary layer 91 is provided on the intermediate layer 12 side of the reproducing layer 11 as shown in a schematic enlarged cross-sectional view forming FIG. 3. The reproducing auxiliary layer 91 is adapted to assist the characteristics of the reproducing layer 11. By this reproducing auxiliary layer 91, the coercive force of the reproducing layer 11 can be compensated for at room temperature, and the magnetization of the reproducing layer 11 arranged by the initialized magnetic field H; can stably exist regardless of the existence of the magnetic wall. Further, the coercive force is rapidly reduced near a reproducing temperature so that the magnetic wall confined within the intermediate layer 12 can be spread to the reproducing auxiliary layer 91. Finally, the reproducing layer 11 is inverted and the magnetic wall is lost, thereby the recording pit 4 being embossed satisfactorily. When the magneto-optical recording medium 10 is formed in a four-layer structure fashion in which the reproducing auxiliary layer 91 is provided as described above, the coercive force H C1 of the reproducing layer 11 is replaced with a coercive force H CA given by the following equation (5) and ρ W2 /M S1 h 1 is replaced with ρ W2 /(M S1 h 1 + M SS h S ): H CA = (M S1 h 1 H C1 + M SS h S H CS )/(M S1 h 1 + M SS h S ) (inequality of H C1 < H CA < H CS is established in the above-mentioned rear aperture detection type MSR disc) where M SS , h S and H CS represent the saturated magnetization, the film thickness and the coercive force of the reproducing auxiliary layer 91, respectively. The MSR disc of the front aperture detection type will be described next with reference to FIGs. 4A and 4B. FIG. 4A is a schematic top view illustrative of the recording pattern of the magneto-optical recording medium 10 and FIG. 4B is a schematic cross-sectional view illustrative of the magnetization state. In FIGS. 4A and 4B, like parts corresponding to those of FIGS. 2A and 2B are marked with the same reference numerals and therefore need not be described in detail. In this case, the initialized magnetic field H i is not required. The reproducing mode of such magneto-optical recording medium 10 will be described. In this case, the following equation (6) must be established in the high temperature area 14 so that, even within the laser beam spot 5, the magnetizations in the high temperature area 14 are arranged in the downward direction in FIG. 4B by the reproducing magnetic field H, applied from the outside, thereby the recording pit 4 in the reproducing layer 11 being erased. That is, in this MSR disc of the front aperture detection type, the resolution can be increased by reproducing the recording pit 4 within the low temperature area 15 of the beam spot 5. H r > H C1 + ρ W2 /2M S1 h 1 At that time, under the condition that the recording pit 4 is erased, various conditions such as a coercive force or the like are set in such a fashion that the recording pit 4 is left as the latent image recording pit 81 in the recording layer 13. Thus, at room temperature, the magnetization of the recording layer 13, i.e., the recording pit 4 can be transferred to the reproducing layer 11 and held in the reproducible condition. According to the above-mentioned MSR discs of the rear aperture detection type and the front aperture detection type, since the recording pit in the area of one portion of the reproducing laser beam spot is reproduced, the resolution in the playback mode can be improved. Further, such a proposal of the magneto-optical recording medium has been made. That is, the above-mentioned two MSR discs of the rear aperture detection type and the front aperture detection type are combined and temperature distributions in which temperature is lowered from the front side of the moving direction of the magneto-optical recording medium 10 relative to the laser beam spot 5 to the rear side are respectively provided under the laser beam spot 5 of the magneto-optical recording medium 10 as a high temperature area 14, an intermediate temperature area 16 and a low temperature area 15 to thereby allow the high temperature area 14 to function as the MSR disc of the front aperture detection type described in FIG. 4 and also to thereby allow the intermediate temperature area 16 and the low temperature area 15 to function as the temperature area 14 and the low temperature area 15 described in connection with FIG. 2. According to the MSR disc provided by the combination of the rear aperture detection type MSR disc and the front aperture detection type MSR disc, since the recording pit 4 embossed on the reproducing layer 11 as shown by the hatched area in FIG. 5 is limited in the narrow intermediate temperature area 16 sandwiched between the high temperature area 14 and the low temperature area 15, the resolution in the playback mode can be improved more. Incidentally, it is preferable that the MSR disc suitable for recording and reproducing of high resolution can be recorded and/or reproduced by an ordinary magneto-optical disc drive apparatus according to a recording and/or reproducing system which will be described below with reference to FIGS. 6 and 7. That is, in the disc medium used in the data storage such as an external storage of the computer, in order to facilitate the data processing and the data access, the track area on a disc medium D is divided at every sector S of a proper length so that data can be processed at the unit of the sector S as shown in FIG. 6. Then, sector control informations such as a physical address on the disc D or the like are recorded on each sector S and the sector control information is written in advance in the disc as an emboss signal. FIG. 7 shows an ISO standard sector format of the WO (write once optical disc)/MO (erasable type optical disc). As shown in FIG. 7, one sector is composed of a header portion HD and a recording data portion DA, and the header portion HD is recorded (pre-formatted) on the optical disc medium in advance as the emboss signal as earlier noted. The header portion HD is composed of a sector synchronizing (sync.) portion and an address portion. The sector sync. portion is used to relatively identify the interval between the sectors and sector control informations such as physical address on the disc or the like are recorded on the address portion. The physical address is composed of, for example, a track address and a sector address. In some cases, physical addresses might be sectors having serial numbers. The recording data is recorded only in the recording data portion DA in association with the sector control information of the header portion HD (associated information is stored in a directory area). However, since the magneto-optical recording medium, particularly, the magneto-optical recording medium of the front aperture detection type is arranged so as to read the recorded signal by changing the magnetization state of the reproducing layer in the playback mode, the magnetic characteristic thereof is changed at a relatively low temperature in such a manner that the magnetization is changed under a predetermined temperature condition. Accordingly, if the above magneto-optical recording medium is recorded and/or reproduced by the ordinary magneto-optical disc drive apparatus, the magnetic characteristic becomes unstable and a reproduced output is fluctuated. There is then the risk that the recorded signal cannot be played back precisely. Furthermore, considering the recording and/or reproducing apparatus of the MSR disc, it is preferable that the MO disc, which is now widely and commercially available on the market, can be recorded and/or reproduced by this recording and/or reproducing apparatus. In that case, it is preferable that the recording and/or reproducing apparatus can commonly use the hardwares for recording and/or reproducing the above two discs, thereby being simplified in arrangement. In addition to the above-described prior art the following documents which are prior art under Article 54(3) EPC describe a magneto-optical recording medium: EP-A-0 492 553 A2, EP-A-0 415 449 A2, EP-A-0 492 581 A2, EP-A-0 526 641 A1 and EP-A-0 536 404 A1. Furthermore, EP-A-0 319 004 A2 describes a magneto-optical recording medium comprising an intermediate layer of TbFeCoCr having a Curie temperature of 130 °C and EP-A-0 318 925 A3 describes a magneto-optical recording medium having an intermediate layer of DyFeCo with a Curie temperature of 93 °C. OBJECTS AND SUMMARY OF THE INVENTION Therefore, it is an object of the present invention to provide an improved magneto-optical medium in which the aforesaid shortcomings and disadvantages encountered with the prior art can be eliminated. More specifically, it is an object of the present invention to provide a magneto-optical recording medium which can be recorded and/or reproduced at high density and which can be recorded and/or reproduced by a conventional magneto-optical recording and/or reproducing apparatus. This is achieved by according to claim 1. The preceding and other objects, features, and advantages of the present invention will become apparent from the following detailed description of illustrative embodiments thereof to be read in conjunction with the accompanying drawings, in which like reference numerals are used to identify the same or similar parts in the several views. BRIEF DESCRIPTION OF THE DRAWINGS FIG. 1 is a schematic cross-sectional view illustrative of an embodiment of a magneto-optical recording medium according to the present invention; FIGS. 2A and 2B are respectively schematic diagrams used to explain an MSR disc of a relief type; FIG. 3 is a schematic cross-sectional view illustrative of a magneto-optical recording medium; FIGS. 4A and 4B are respectively schematic diagrams used to explain an MSR disc of an erase type; FIG. 5 is a schematic diagram used to explain an MSR disc of other type; FIG. 6 is a schematic diagram showing an example of a sector format of the magneto-optical disc; FIG. 7 is a diagram showing a format of one sector; FIGS. 8A through 8D are respectively schematic diagrams used to explain a relation between a laser beam spot diameter and a recording density of a reproducible recording pit; FIG. 9 is a graph graphing the change of Curie temperature such that the composition is changed in accordance with an adding amount of Aℓ to Tb 0.25 (Fe 0.95 CO 0.05 ) 0.75 ; FIG. 10 is a graph graphing the change of Curie temperature such that the composition is changed in accordance with an adding amount of Aℓ to Tb 0.3 Fe 0.7 ; FIG. 11 is a graph graphing the change of Curie temperature such that the composition is changed in accordance with an adding amount of Co to Tb 0.25 Fe 0.75 . DESCRIPTION OF THE PREFERRED EMBODIMENTS Referring to the drawings in detail and initially to FIG. 1, an embodiment of a magneto-optical recording medium 10 according to the present invention will be described in detail. In this case, the magneto-optical recording medium 10 is the MSR disc of the front aperture detection type. As shown in FIG. 1, a substrate 17 is made of a transparent material such as polycarbonate (PC) or the like. On one major surface of the substrate 17, there are deposited a dielectric layer 18 made of, for example, an SiN layer having a thickness of 800 Å, a reproducing layer 11, an intermediate layer 12, a recording layer 13 and a surface protecting layer 19 having a thickness of 800 Å by some suitable method such as the sputtering-process or the like, in that order. In the ordinary magneto-optical drive apparatus, the revolution rate of the magneto-optical recording medium is 2400 r.p.m., a recording innermost periphery r is 30 mm, an upper limit of environmental temperature is 50°C and an upper limit of the laser output is 1.5 mW according to the standards of ISO (International Organization for Standardization). When these standardized values are associated with the above-mentioned MSR disc, then the rise of temperature is about 100°C in the recording innermost periphery. Considering the environmental temperature, the temperature is assumed to rise up to about 150°C. In the magneto-optical recording medium 10 according to the present invention, a Curie temperature T C2 of the intermediate layer 12 is selected to be 150°C or more so that, when this magneto-optical recording medium 10 is utilized in the ordinary magneto-optical disc drive apparatus, the temperature of the magneto-optical recording medium 10 can be avoided from rising more than the Curie temperature T C2 of the intermediate layer 12. More specifically, even when the above-mentioned MSR disc 10 is utilized by the ordinary magneto-optical disc drive apparatus, it is possible to reliably avoid fluctuation of reproduced output due to the influence exerted on the recording pit by the erasure of magnetic characteristics of the intermediate temperature based on temperature dependence. Therefore, the magnetizations of the respective magnetic layers, particularly, the magnetization of the intermediate layer 12 can be held reliably so that this MSR disc can be accurately and positively recorded and/or reproduced by the ordinary magneto-optical disc drive apparatus. In this embodiment, the reproducing layer 11 is made of GdFeCo and 300 Å in thickness, and the recording layer 13 is made of TbFeCo or the like and 400 Å. Then, the intermediate layer 12 is 200 Å in thickness, for example, and the composition thereof is {Tb(Fe 0.95 Co 0.05 )} 0.35 Aℓ 0.05 of, for example, the TbfeCoAℓ system. The curie temperature T C2 thereof is selected to be 150°C. FIG. 9 shows a graph graphing the change of Curie temperature when z in (Tb 0.25 (Fe 0.95 CO 0.05 ) 0.75 ) 1-z Aℓ z was changed. From FIG. 9, it can be understood that this Curie temperature T C2 is proper because the Curie temperature is lowered in proportion to the increase of the containing amount of Aℓ in the TbFeCoAℓ system. FIG. 10 is a graph graphing the change of Curie temperature when z in (Tb 0.3 Fe 0.7 ) 1-z Aℓ z was changed. As shown in FIG. 10, it can be appreciated that the Curie temperature is lowered in accordance with the increase of z , i.e., the containing amount of Aℓ in the TbFeAℓ system. On the other hand, FIG. 10 is a graph graphing the change of Curie temperature when z in Tb 0.25 (Fe 1-z Co z ) 0.75 was changed. As shown in FIG. 10, it can be understood that the Curie temperature is lowered in proportion to the increase of the containing amount of Co. If the composition ratio of various materials is examined as described above, then it is possible to select the Curie temperature to be a predetermined one, i.e., 150°C or more. Since the Curie temperature Tc of the intermediate layer 12 is selected to be 150°C as described above, it is to be understood that this MSR disc can be normally recorded and/or reproduced by the ordinary magneto-optical disc drive apparatus. While the magneto-optical recording medium suitably applied to the MSR disc of particularly the front aperture detection type is described in the above-mentioned embodiment of the present invention, the present invention is not limited to the magneto-optical recording medium thus arranged and various modifications may be possible. If the present invention is applied to the magneto-optical recording medium of the MSR type serving as both rear aperture detection type and front aperture detection type which can achieve the playback of high resolution and in which the magnetic layer of the magneto-optical recording medium is formed as a four-layer structure formed of the reproducing layer 11, the reproducing auxiliary layer 91, the intermediate layer 12, the recording layer 13 or the like as, for example, shown in FIG. 3 so that the recording pit is embossed on the reproducing layer 11 only at its narrow area of the predetermined temperature range as described in FIG. 5, by selecting the Curie temperature T C2 of the reproducing auxiliary layer 91 to be 150°C or more (cf. European patent application EP 92 102 091.3 published as EP-A-0 498 461 e.g. on p. 14 Table 1), the magnetic characteristics can be prevented from being fluctuated at a relatively low temperature and the magneto-optical disc drive apparatus can produce a stable reproduced output, which can therefore effect the accurate and reliable recording and/or reproduction. As described above, in the magneto-optical recording medium 10 of the present invention, the Curie temperature T C2 of the intermediate layer 12 is selected to be 150°C or more so that, even when this magneto-optical recording medium is utilized in the ordinary magneto-optical disc drive apparatus, the temperature of the magneto-optical recording medium 10 can be avoided from rising higher than the Curie temperature T C2 of the intermediate layer 12. Thus, the fluctuation of the reproduced output or the like due to the temperature dependence of the magnetic characteristics of the intermediate layer 12 can be avoided positively and the recording pit 4 of the recording layer 13 can be reliably held in the reproducing layer 11, which enables the magneto-optical recording medium of this invention to be recorded and/or reproduced even by the ordinary magneto-optical disc drive apparatus accurately and reliably.

Claims: A magneto-optical recording medium (10) having a recording layer (13), a reproducing layer (11) and an intermediate layer (12) for magnetically coupling said recording layer (13) and said reproducing layer (11) in a stationary state, in which the magnetic coupling between said recording layer (13) and said reproducing layer (11) is lost in an area (14) in which a temperature is increased to be higher than a predetermined temperature by the radiation of light upon reproducing and in which a recorded information held in said recording layer (13) is read out from said reproducing layer (11) in the radiated area (5) except the area (14) in which said magnetic coupling is lost and in which a Curie temperature of said intermediate layer (12) is selected to be 150° C or more, characterized in that said intermediate layer (12) is composed of TbfeCoAl or TbFeAl. The magneto-optical recording medium (10) according to claim 1, wherein an upper limit of an output power of said radiated light is 1.5 mW and said radiated light is moved at the speed of 1.2 m/S relative to said magneto-optical recording medium (10) to thereby reproduce the recorded information.

Inventors: FUKUMOTO ATSUSHI, NAKAO ISAMU, OHTA MASUMI, UDAGAWA TOSHIKI, YOSHIMURA SHUNI, FUKUMOTO, ATSUSHI, NAKAO, ISAMU, OHTA, MASUMI, UDAGAWA, TOSHIKI, YOSHIMURA, SHUNI
Applicants: SONY CORP, SONY CORPORATION
Application year: 1992
Main classification: G11B11
IPC codes: G11B11, G11B19