JP3390713B2 - Magneto-optical recording medium - Google Patents

Description

Detailed Description of the Invention

[0001]

TECHNICAL FIELD The present invention relates to a high density magneto-optical recording medium.

Although a magneto-optical disk is known as a high density recording medium, a higher density is demanded as the amount of information increases. Higher density can be realized by narrowing the intervals of recording marks, but recording and reproduction thereof are limited by the size of the light beam (beam spot) on the medium.

When it is set that only one recording mark exists in the beam spot, output waveforms corresponding to "1" and "0" can be observed as a reproduction signal depending on whether or not there is a recording mark.

However, if the recording marks are closely spaced so that a plurality of recording marks are present in the beam spot, the reproduction output does not change even if the beam spot on the medium moves, so that the output waveform becomes a straight line. The presence or absence of recording marks cannot be identified.

In order to reproduce a small recording mark having a period less than such a beam spot, the beam spot may be narrowed down. The size of the beam spot depends on the wavelength λ of the light source and the numerical aperture NA of the objective lens. It is restricted by and cannot be narrowed down sufficiently.

[0006]

2. Description of the Related Art Recently, there has been proposed a reproducing method using a magnetic induction super-resolution technique for reproducing a recording mark below a beam spot by using the existing optical system as it is. This is a reproducing method in which one mark in the beam spot is reproduced while another mark is masked to improve the reproducing resolution.

Therefore, in the super-resolution disc medium, in addition to the recording layer for recording marks, a mask layer or reproducing layer for hiding other marks so that only one mark is reproduced at the time of signal reproduction. Is the minimum required.

A magneto-optical recording medium using a perpendicularly magnetized film as a reproducing layer is proposed in Japanese Patent Laid-Open No. 3-88156. However, the conventional technique described in this publication has a problem that the device cannot be miniaturized because an initializing magnetic field of about several kilo Oersted is required to initialize the reproducing layer.

On the other hand, a magneto-optical recording medium using a magnetic film in the reproducing layer which has an easy axis of in-plane magnetization at room temperature and a perpendicular easy axis of magnetization at a predetermined temperature or higher is disclosed in JP-A-5-8171.
Proposed in No. 7.

The reproducing principle of this prior art will be briefly described with reference to FIG. As shown in FIG. 7C, the magneto-optical disk 2 includes a magnetic reproducing layer 6 and a magnetic recording layer 8 on a transparent substrate 4.
Are laminated.

At room temperature, the magnetic reproducing layer 6 has an easy axis of magnetization in the in-plane direction, but when the reproducing power is applied and the temperature exceeds a predetermined temperature, the easy axis of magnetization changes in the vertical direction. The magnetic recording layer 8 is a perpendicular magnetization film. Reference numeral 10 indicates a light beam.

Since the intensity distribution of the light beam has a Gaussian distribution as shown in FIG. 7A, when the disc is stationary, the temperature distribution on the disc is higher in the central portion than in the peripheral portion. Has become.

However, since the disk 2 actually rotates in the direction of arrow R, the temperature distribution on the disk is as shown in FIG.
As shown in (B), the front side of the beam spot in the disc movement direction has a high temperature.

Since the temperature distribution is generated in this way, the easy axis of magnetization of the magnetic reproducing layer 6 is directed in the in-plane direction in a region where the temperature in the beam spot is low, so that the Kerr rotation angle of the reflected light is almost zero. Becomes In the high temperature region, the easy axis of magnetization of the magnetic reproducing layer 6 changes from the in-plane direction to the perpendicular direction.

At this time, the perpendicular magnetization of the magnetic reproducing layer 6 is coupled with the magnetization of the magnetic recording layer 8 by the exchange force and is aligned in the magnetization direction of the magnetic recording layer 8. Therefore, the magnetization recorded in the magnetic recording layer 8 is aligned. Can be transferred to. The size of this transfer area can be changed by the reproduction laser beam power or the rotation of the disk.

By controlling the size of the mask of the magnetic reproducing layer in such a manner that only one recording mark can be reproduced, the same effect as that of substantially reducing the area of the beam spot can be obtained. The resolution is improved and high density recording / playback can be realized.

[0017]

As described above, the intensity distribution of the laser beam 10 with which the disk 2 is irradiated has a Gaussian distribution, and since the disk 2 is rotating in the direction of arrow R, the magnetic reproducing layer is formed. A low temperature region and a high temperature region are generated on the disk 6, and the high temperature region is shifted to the downstream side or rear side of the beam spot formed on the disk.

As described above, since the high temperature region in the beam spot for reproducing information is shifted to the downstream side, the intensity of the laser beam becomes relatively weak, and in the prior art described in Japanese Patent Laid-Open No. 5-81717, a large light beam is emitted. There is a problem that a magnetic signal cannot be obtained.

Further, since the optical mask is formed only on the upstream side within the beam spot, the size of the opening for reproducing information cannot be reduced to a very small size.

Therefore, an object of the present invention is to provide a high-density magneto-optical recording medium capable of accurately recording a smaller mark than the conventional one and reproducing with a larger magneto-optical signal than the conventional one.

[0021]

According to the present invention, there is provided a magneto-optical recording medium comprising a multilayer magnetic film containing a rare earth metal and a transition metal as main components and having an easy axis of magnetization perpendicular to the film surface. A reproducing layer and an easy axis of magnetization in the in-plane direction provided on the reproducing layer at room temperature, the magnetic moment of rare earth is dominant, and at least Gd as a rare earth metal, Fe as a transition metal, and compensation up to the Curie temperature It has no temperature and is made of non-magnetic material consisting of Si at 10 to 60 at
% Control layer and a recording layer having an easy axis of magnetization perpendicular to the film surface provided on the control layer, and the Curie temperatures of the reproducing layer, the control layer and the recording layer are respectively Tc.
1, Tc2 and Tc3, and the coercive forces of the reproducing layer and the recording layer at room temperature are Hc1 and Hc3, respectively,
Curie temperature of each magnetic layer is Tc1> Tc2, Tc3>
Provided is a magneto-optical recording medium satisfying the relationship of Tc2 and coercive forces of the reproducing layer and the recording layer at room temperature satisfying the relationship of Hc3> Hc1.

When reproducing the information recorded on the magneto-optical recording medium of the present invention having the reproducing layer, the control layer and the recording layer, the temperature gradient generated in the beam spot formed on the recording medium is used to make The feature is that the mark is reproduced accurately.

In the region where the temperature is low in the beam spot, the magnetization of the reproducing layer is oriented in the direction of the reproducing bias magnetic field to form an up-spin mask or a down-spin mask, and in the high temperature region above the Curie temperature of the control layer, the magnetization of the control layer is The magnetization of the reproducing layer disappears and the magnetization of the reproducing layer faces the reproducing bias magnetic field to form an up-spin mask or a down-spin mask.

In the intermediate temperature region (opening), the magnetization direction of the recording layer is transferred to the reproducing layer via the control layer, and the information recorded in the recording layer can be reproduced.

That is, when the magneto-optical output is differentially detected, a region having a low temperature and a region having a high temperature in the beam spot act as a mask, and the magneto-optical signal at this portion is not read out. The magneto-optical signal can be read. Therefore, it is possible to accurately read a mark having a size smaller than the diffraction limit of the laser wavelength.

[0026]

DESCRIPTION OF THE PREFERRED EMBODIMENTS The structure of a magneto-optical recording medium according to an embodiment of the present invention will be described with reference to FIG. Reference numeral 12d is a magneto-optical recording medium, which is usually disk-shaped. Si is formed on the transparent substrate 14 such as glass by, for example, sputtering.
A dielectric layer 16 made of N or the like is laminated. The dielectric layer 16 prevents oxidation and corrosion of the magnetic layer laminated thereon.

As the transparent substrate 14, resins such as polycarbonate, polymethylmethacrylate, amorphous polyolefin and the like can be adopted. In addition, the dielectric layer 16
As the metal nitride such as AlN, SiO2, Al2O
A metal oxide such as 3 and a metal sulfide such as ZnS can be used.

On the dielectric layer 16, a magnetic reproducing layer 1 made of a rare earth-transition metal amorphous alloy film such as GdFeCo.
8'is stacked. The magnetic reproducing layer 18 ′ has an easy axis of magnetization in the direction perpendicular to the substrate 14.

A magnetic control layer 20 'formed of a rare earth-transition metal amorphous alloy film such as GdFeCo is laminated on the magnetic reproducing layer 18'. The magnetic control layer 20 'has an easy axis of magnetization in the in-plane direction at room temperature.

A magnetic recording layer 22 made of a rare earth-transition metal amorphous alloy film such as TbFeCo is laminated on the magnetic control layer 20 '. The magnetic recording layer 22 has an easy axis of magnetization in the direction perpendicular to the substrate 14.

Reproducing layer 18 ', control layer 20' and recording layer 2
When the Curie temperatures of 2 are Tc1, Tc2, and Tc3, the Curie temperatures of the magnetic layers satisfy the relationships of Tc2 <Tc1 and Tc2 <Tc3.

When the coercive forces of the reproducing layer 18 'and the recording layer 22 at room temperature are Hc1 and Hc3, Hc1 <H
It is necessary to satisfy the relationship of c3.

The reproducing layer 18 'can be formed of an amorphous alloy film of TbGdFeCo, and the control layer 20' is GdF.
It is possible to form the amorphous alloy film of e. Further, preferably, a non-magnetic material selected from the group consisting of Si, Al and Ti is added to the control layer 20 '.

A protective film 24 is laminated on the magnetic recording layer 22 to complete the magneto-optical recording medium 12d. This protective film 24
Is provided for the purpose of preventing entry of water, oxygen, or a substance such as a halogen element from the air and protecting the magnetic recording layer 22.

The protective film 24 is made of metal nitride such as SiN or AlN, metal oxide such as SiO2 or Al2O3, and ZnS.
And the like are formed from metal sulfides.

Referring to FIG. 2, there is shown a schematic diagram of a magneto-optical disk device which can be used in the information reproducing method of the present invention. The magneto-optical disk 30 is configured by laminating a three-layer magnetic layer 28 on a transparent substrate 14. The magneto-optical disk 30 is rotated by a spindle motor 32.

Reference numeral 34 is an electromagnet driven by an electromagnet drive circuit 36, and applies a bias magnetic field in a predetermined direction to the magneto-optical disk 30. The direction of the bias magnetic field is switched between upward and downward depending on the direction of the current flowing through the electromagnet 34.

Alternatively, 34 may be replaced with a small permanent magnet that generates a magnetic field of about several hundred Oersteds. In this case, the direction of the bias magnetic field is switched by rotating the S and N poles of the magnet by 180 °.

A data signal to be written is generated by the signal generation circuit 38 and input to the laser drive circuit 40. As a result, the laser drive circuit 40 modulates and drives the laser diode 42 according to the data signal.

The laser beam generated by the laser diode 42 is collimated by the collimator lens 44, transmitted through the beam splitter 46, and focused on the magnetic layer 28 of the magneto-optical disk 30 by the objective lens 48.

While applying a bias magnetic field in a predetermined direction by the electromagnet 34, the laser diode 42 is driven to irradiate the laser beam on the magnetic layer 28 of the magneto-optical disk 30, whereby a data signal is written on the disk 30.

On the other hand, when reproducing the information (data signal) recorded on the magneto-optical disk 30, the laser diode 42 is driven on the magneto-optical disk 30 while applying the bias magnetic field in the predetermined direction by the electromagnet 34. Irradiate the playback beam power.

The reflected light from the magneto-optical disk 30 is collimated by the objective lens 48, and then the beam splitter 4
The information reflected by 6 passes through the analyzer 50, is focused on the photodetector 54 by the lens 52, and the information recorded on the magneto-optical disk 30 is reproduced as an electric signal.

Next, the data erasing method of this embodiment will be described with reference to FIG. The recording medium is irradiated with the laser beam while applying the bias magnetic field Hb downward.
The recording layer 2 is heated by raising the temperature to the Curie temperature of 2
The magnetization direction of 2 is set downward.

When the recording medium is moved away from the laser beam, the temperature of the recording medium is lowered to room temperature. At room temperature, the control layer 20 'becomes an in-plane magnetized film, and the reproducing layer 18' and the recording layer 22 are not magnetically coupled. Therefore, the magnetization of the reproducing layer 18 'is aligned downward with a magnetic field as small as the erasing bias magnetic field.

Next, with reference to FIG. 4, a data writing method of this embodiment will be described. When the bias magnetic field Hb is applied in the direction opposite to the erasing direction, that is, in the upward direction, only the recording portion is irradiated with the strong laser beam, and only the magnetization in the portion where the data is recorded is upward.

When the recording medium is moved away from the laser beam, the temperature of the recording medium is lowered to room temperature. At room temperature, the control layer 20 'becomes an in-plane magnetized film, and the reproducing layer 18' and the recording layer 22 are not magnetically coupled. Therefore, the magnetization of the reproducing layer 18 'is aligned upward with a magnetic field as small as the bias magnetic field.

Next, with reference to FIG. 5, a data single mask reproducing method in the present embodiment will be described. In the beam spot 58 irradiated on the track 64, a low temperature region having a temperature of Tcopy or lower and a control layer 2 having a temperature of Tcopy or higher.
A high temperature region below the Curie temperature Tc2 of 0'is formed.

The up-spin mask 60 is formed in the low temperature region in the beam spot 58, and the opening 6 is formed in the high temperature region.
2 is formed. This state is described in the above-mentioned JP-A-5-817.
Similar to the state of No. 17 during data reproduction, the opening 6
The magneto-optical signal can be read out via 2.

When the reproducing laser power is further increased, as shown in FIG. 6, the magnetization of the reproducing layer 18 ′ in the beam spot 58 is oriented toward the reproducing bias magnetic field Hr and the magnetization of the recording layer 22 is exchange-coupled by exchange coupling. An intermediate temperature region transferred to the control layer 20 'and the reproduction layer 18' and a high temperature region of the Curie temperature Tc2 or higher of the control layer 20 'are formed.

In the low temperature region and the high temperature region, the reproduction layer 18 '
Up spin masks 60 and 68 whose magnetization directions are aligned with the bias magnetic field Hr are formed, and the two up spin masks 6 are formed.
The opening 62 is formed in the intermediate temperature region between 0 and 68.

In the up-spin mask portion 68, since the recording medium is heated to the Curie temperature Tc2 or higher of the control layer 20 ', the magnetization of the control layer 20' disappears and the reproducing layer 1
8'and the recording layer 22 are not magnetically coupled.

Therefore, since the reproducing layer 18 'has a small coercive force at room temperature, its magnetization direction is oriented in the direction of the reproducing bias magnetic field Hr. That is, in the temperature region above the Curie temperature of the control layer 20 ', the magnetization of the reproducing layer 18' is always upward, and no magneto-optical signal is output, which functions as a kind of mask.

Therefore, it is possible to form a very small opening 62 as compared with the conventional method described in JP-A-5-81717. Further, since the opening 62 is formed at the center of the beam spot where the laser intensity is relatively stronger than the edge of the beam spot, a large magneto-optical signal can be obtained.

Example 1 TbFeCo and first GdFe were placed in a sputtering apparatus.
Co, a second GdFeCo and Si target and 1.
A polycarbonate substrate having a track pitch of 2 μm was set, and the inside of the chamber of the sputtering device was set to 10
^It was evacuated to ^-5 Pa.

Next, a film thickness of 70 nm is formed on the substrate under the following conditions.
Was formed into a film by the DC sputtering method. This film not only has the function of protecting the magnetic layer from oxidation, but also has the enhancing effect of increasing the magneto-optical signal.

Gas pressure: 0.3 Pa Sputtering gas: Argon, Nitrogen partial pressure: Argon: Nitrogen = 6: 4 Input power: 0.8 kW Next, the chamber was evacuated again to 10 ⁻⁵ Pa,
A first GdFeC film is formed on the silicon nitride film under the following conditions.
o, the second GdFeCo, and TbFeCo were successively formed in this order by the DC sputtering method.

Gas pressure: 0.5 Pa Sputtering gas: Argon input power: 1 kW The composition, film thickness and magnetic characteristics of each magnetic layer are as shown in Table 1.

[0059]

[Table 1]

In Table 1, the compensation temperature "-" indicates that the compensation temperature is not below the Curie temperature.

Further, a silicon nitride film having a film thickness of 100 nm was formed on the recording layer by the same method as described above. The silicon nitride film serves to prevent the magnetic film from being oxidized.

The recording characteristics of the magneto-optical disk manufactured as described above were examined by using the apparatus shown in FIG. The wavelength of the laser used is 780 nm. First, the entire surface of the magneto-optical disk was erased, that is, initialized. At this time, the laser power was 9 mW and a downward bias magnetic field was applied.

Information is recorded on the disc at a linear velocity of 3 m / sec.
While rotating at, apply an upward bias magnetic field in the direction opposite to that at the time of initialization, write power 4 mW, frequency 7.
It was performed at 5 MHz and a light emission duty ratio of 26%. The length of the mark recorded on the disc is about 0.4 μm.

Next, the reproducing characteristics of this magneto-optical disk were examined. The reproducing bias magnetic field applied at this time was directed upward. With a reproducing power of 1.5 mW, the output of the magneto-optical signal with respect to the previously recorded signal was not obtained. This is probably because the entire reproducing layer 18 'forms an up-spin mask.

With a reproducing power of 1.6 mW, the magnetization direction of the recording layer 22 was transferred to the reproducing layer 18 'via the control layer 20', and a magneto-optical signal output could be obtained. This is because the magnetization direction of the recording layer 22 within the beam spot is the control layer 20 '.
It is considered that the up-spin mask and the opening were formed because a region having a temperature equal to or higher than the temperature transferred to the reproduction layer 18 ′ was formed. Signal-to-noise ratio (C /
N) was 42 dB.

At a reproducing power of 1.7 mW, the magnetization of the recording layer 22 is oriented in the direction of the bias magnetic field, that is, in the upward direction, and the diameter of the region (opening) where the control layer 20 ′ is exchange-coupled with the recording layer 22 is 0.4 μm. C / N of 46 dB due to
I was able to get

Next, it was examined whether or not the composition of the reproducing layer 18 'could be sufficiently used with other compositions. As a result, in the case where the reproducing layer 18 'is made of TbFeCo or DyFeCo, the coercive force becomes large, so that the magnetization direction of the reproducing layer 18' cannot be initialized with a magnitude of the bias magnetic field and super-resolution reproduction is performed. I couldn't.

Example 2 In Example 1, a material made of GdFeCo was used for the reproducing layer 18 '. However, the composition margin of the GdFeCo film showing the perpendicular magnetic anisotropy is not wide, and it may be difficult to control the composition. Therefore, in this example, an attempt was made to add a small amount of Tb capable of increasing the perpendicular magnetic anisotropy to GdFeCo. The experiment was conducted as follows.

TbFeCo, T in the sputtering device
A bGdFeCo, GdFeCo, and Si target and a polycarbonate substrate having a track pitch of 1.2 μm were set, and the inside of the chamber of the sputtering apparatus was evacuated to 10 ⁻⁵ Pa.

Next, a film thickness of 70 nm is formed on the substrate under the following conditions.
Was formed into a film by the DC sputtering method. This film not only has the function of protecting the magnetic film from oxidation, but also has the enhancing effect of increasing the magneto-optical signal.

Gas pressure: 0.3 Pa Sputtering gas: Argon, Nitrogen partial pressure: Argon: Nitrogen = 6: 4 Input power: 0.8 kW Next, the chamber was evacuated again to 10 ⁻⁵ Pa,
TbGdFeCo on the silicon nitride film under the following conditions,
GdFeCo and TbFeCo were successively formed in this order by the DC sputtering method.

Gas pressure: 0.5 Pa Sputtering gas: Argon input power: 1 kW Table 2 shows the composition, film thickness and magnetic characteristics of each magnetic layer.

[0073]

[Table 2]

Further, a silicon nitride film having a film thickness of 100 nm was formed on the recording layer by the same method as described above. This silicon nitride film serves to prevent the magnetic film from being oxidized.

The reproducing characteristics of the magneto-optical disk thus manufactured were examined under the same conditions as in Example 1. The reproducing bias magnetic field applied at this time was directed upward. With a reproducing power of 1.4 mW, the output of the magneto-optical signal with respect to the previously recorded signal was not obtained. This is probably because the entire reproducing layer 18 'forms an upspin mask.

With a reproducing power of 1.5 mW, the magnetization direction of the recording layer 22 was transferred to the reproducing layer 18 'through the control layer 20', and a magneto-optical signal output could be obtained. This is because the magnetization direction of the recording layer 22 within the beam spot is the control layer 20 '.
It is considered that the up-spin mask and the opening were formed because a region having a temperature equal to or higher than the temperature transferred to the reproduction layer 18 ′ was formed. Signal-to-noise ratio (C /
N) was 42 dB.

At a reproducing power of 1.6 mW, the reproducing layer 18 '
Is directed in the direction of the bias magnetic field, that is, in the upward direction, and the diameter of the region (opening) where the control layer 20 ′ is exchange-coupled with the recording layer 22 is about 0.4 μm.
I was able to get

This C / N was the same as in Example 1. This is because the addition of Tb to the reproducing layer 18 'increases the magnetic anisotropy and reduces the noise, while the GdF
It is considered that the magneto-optical effect was lowered by adding Tb to eCo.

Then, these effects are canceled out, and the first embodiment is shown.
Probably because the same result as was obtained. However, Tb
By adding, the composition margin of the reproducing layer 18 'can be widened.

Example 3 In order to study the composition of the control layer 20 ', the composition of the control layer 20' was TbFeCo or DyFe showing in-plane magnetization.
A three-layer film recording medium in which Co and GdFeCo were changed was manufactured as a prototype, and its recording / reproducing characteristics were examined. Here, the recording conditions are the same as those in the first embodiment. The results are shown in Table 3.

[0081]

[Table 3]

This indicates that when the control layer 20 'is made of TbFeCo or DyFeCo, the recording / reproducing characteristics are not good, and the composition of the control layer 20' is GdF.
It has been found that eCo is suitable.

Further, GdFe suitable for the control layer 20 '
The Co composition was examined. When the control layer 20 ′ was made of GdFeCo, the reproduction characteristics when the Co content was changed were measured by the same method as in Example 12. The results are shown in Table 4.
Shown in.

[0084]

[Table 4]

From these results, the Co content is 0 to 5 at.
It can be seen that the C / N is improved in%. It is considered that this is because the Curie temperature of the control layer 20 'was lowered and a mask was formed also on the trailing edge of the spot of the laser beam to form a double mask and the resolution was increased.

Example 4 From Example 3, it was found that when the Curie temperature of the control layer 20 'was lowered, a double mask was formed and C / N was improved. Therefore, an attempt was made to add a nonmagnetic metal to the control layer 20 'for the purpose of lowering the Curie temperature of the control layer 20'.

A magneto-optical recording medium having a control layer 20 'in which a non-magnetic element was added to GdFeCo was manufactured as a prototype and its reproducing characteristic was examined. The reproduction characteristics were measured by the same method as in Example 1. The results are shown in Table 5.

[0088]

[Table 5]

From the above results, it was proved effective to add a non-magnetic material to the control layer 20 '. Next, the non-magnetic material added to the control layer 20 'was Si, and changes in the reproducing characteristics with respect to changes in the amount of Si added were examined.

The composition and film thickness of the reproducing layer 18 ', the control layer 20' and the recording layer 22 are the same as in Example 1. That is, the composition of the control layer 20 'is Gd39Fe56Co5. It was decided to add Si to this composition. The amount of Si was determined by changing the number of Si chips placed on the target of the control layer 20 'made of GdFeCo. The results are shown in Table 6.

[0091]

[Table 6]

From this result, the Si content is 10 to 60.
It was found that a high C / N can be obtained in a wide range of at%. Further, when the Si content is 70 at% or more, the exchange coupling force between the reproducing layer 18 'and the recording layer 22 becomes small, so that C
/ N decreases.

[0093]

According to the present invention, it is possible to provide a magneto-optical recording medium capable of high-density recording, and to further improve the reproduction output by completely masking the mark adjacent to the mark to be reproduced. It has the effect of being able to. Also, crosstalk is improved.

[Brief description of drawings]

FIG. 1 is a configuration diagram of a magneto-optical recording medium according to an embodiment of the present invention.

FIG. 2 is a schematic configuration diagram of a magneto-optical disk device.

FIG. 3 is a diagram illustrating data erasing.

FIG. 4 is a diagram illustrating writing of data.

FIG. 5 is a diagram illustrating a single mask reproducing method,
(A) is a plan view and (B) is a longitudinal sectional view of the recording medium.

6A and 6B are diagrams illustrating a data reproducing method according to an embodiment, in which FIG. 6A is a plan view and FIG. 6B is a longitudinal sectional view of a recording medium.

FIG. 7 is a diagram illustrating a reproduction principle of a conventional example.

[Explanation of symbols]

14 Transparent substrate 16 Dielectric layer 18 'playback layer 20 'control layer 22 recording layer 24 Protective film 58 beam spot 60 upspin mask 62 opening 68 Up Spin Mask

Continuation of the front page (56) Reference JP-A-5-182269 (JP, A) JP-A-5-205336 (JP, A) JP-A-7-14230 (JP, A) JP-A-7-85516 (JP , A) (58) Fields investigated (Int.Cl. ⁷ , DB name) G11B 11/105

Claims (3)

(57) [Claims] 1. A magneto-optical recording medium comprising a multilayer magnetic film containing a rare earth metal and a transition metal as main components, comprising: a reproducing layer having an easy axis of magnetization perpendicular to the film surface; and a reproducing layer on the reproducing layer. provided the room temperature showed an easy axis of magnetization in-plane direction, the magnetic moment of the rare earth is dominant, and has no compensation temperature up to the Curie temperature include Fe as the transition metal comprises Gd least as rare earth metals, from more Si
Comprising a control layer of non-magnetic material containing 10～60At%, comprising a recording layer having an easy axis of magnetization in the direction perpendicular to the film surface provided on the control layer, the reproducing layer, the control layer, the recording When the Curie temperatures of the layers are Tc1, Tc2, and Tc3, and the coercive forces of the reproducing layer and the recording layer at room temperature are Hc1 and Hc3, respectively, the Curie temperatures of the magnetic layers have a relationship of Tc1> Tc2 Tc3> Tc2. A magneto-optical recording medium satisfying the above conditions, and the coercive forces of the reproducing layer and the recording layer at room temperature satisfy the relationship of Hc3> Hc1. 2. The magneto-optical recording medium according to claim 1, wherein the composition of the reproducing layer contains GdFeCo as a main component. 3. The magneto-optical recording medium according to claim 1, wherein the composition of the control layer contains GdFe as a main component.