A MAGNETO-OPTIC MEDIUM AND SYSTEM

Abstract: An overwritable magneto-optic recording system has a recording medium (10) with a substrate (11), a recording magnetic film (13) and a reproducing magnetic film (12) deposited on the substrate. The reproducing magnetic film (12) has a Curie temperature lower than that of the recording magnetic film (13), and coercive force Hc higher than that of the recording magnetic film. In a write process, a magnetic head (16) writes data magnetically on the recording magnetic film (13), and then, in a transfer process, an optical head (14) (which is positioned downstream in the direction of relative movement of the recording medium and the optical head) heats the recording medium higher than the Curie temperature of the reproducing magnetic film (12) so that the reproducing magnetic film loses its magnetic property. During the cooling period after heating, recorded bits in the recording magnetic film (13), are transferred to the reproducing magnetic film (12) which restores its magnetic property. In the reproducing process, the optical head (14) irradiates the reproducing magnetic film with a polarised coherent beam, and the data is reproduced on the principle that the polarisation of the reflected beam depends upon the recorded data based on the Kerr effect.

Description: The present invention relates to a magneto-optic recording medium and system, and in particular, relates to an overwritable type of medium. A prior optical disk has the advantage that the recording capacity is extremely large. However, it has the disadvantage that the recorded portion cannot be erased. An erasable optical disk is described in page 1624-1628, IEEE Transactions on magnetics, vol. mag-21, No. 5, September 1985. In that publication, an optical disk which is magnetized initially is illuminated by a laser beam under a bias magnetic field less than the anisotropic field in the opposite direction to the initial magnetic field in order to raise the temperature higher than Curie temperature. When the optical disk is cooled, the magnetization of each cell is changed to the direction of the bias field. The information data relates to on/off of said laser beam so that the direction of the magnetization relates to the binary information data. However, said disk has the disadvantage that the disk must be initialized in each recording operation by illuminating the disk with the laser beam in the initial field so that the disk is heated and is erased. In other words, the magnetization of the disk must be directed in one direction before the recording operation, or the disk must be erased before the recording operation. Therefore, no overwriting is possible in that prior disk, and so, high speed access to a disk was impossible. Therefore, an overwritable optical disk has been desired. An overwritable optical disk is described in Proc. Int. Symp. on Optical Memory, 1987, Japanese Journal of Applied Physics, Vol. 26 (1987) Supplement 26-4, pp149-154. In that publication, a recording layer is TbFeCo layer, and a recording head has both an optical head and a magnetic head. The recording layer is first heated by the optical head, and then, in the cooling duration of the layer, the layer is recorded magnetically. However, said overwritable optical disk has the disadvantages that a recording pit is not symmetrical and so noise is caused, and that the recording magnetic field disturbs the positioning operation of the operation head. Another overwritable optical disk is described in DE OS 3619618, in which a pair of magnetic layers with different Curie temperatures are used. A first layer is magnetically initialized in one direction, and new data is recorded by a laser beam which is modulated by a binary data under a bias field opposite to the initialization field. When data "1" is written, the laser beam is strong enough for heating two magnetic layers higher than the Curie temperatures, and so, the resultant magnetic field after cooling is defined by the bias magnetic field. On the other hand, when data "0" is written, the laser beam is controlled so that the first layer does not lose the magnetization, but the other magnetic layer loses the magnetization, and so, the resultant magnetic field after cooling is defined by the initial field. However, said prior art has the disadvantage that the control of the operation is complicated, since the strength of a laser beam must be modulated by binary recording data. EP-A-0258978 describes a magneto-optical recording system in which a second magnetic layer has a higher Curie point and lower coercive force than a first magnetic layer. The first and second magnetic layers are exchange coupled. In accordance with one aspect of the present invention, a magneto-optic recording medium is defined by the features of claim 1. In accordance with another aspect of the present invention, a magneto-optic recording system is defined by the features of claim 12. The present invention overcomes the disadvantages and limitations of the prior magneto-optic recording systems by providing a new and improved magneto-optic recording system. Some examples of media and systems according to the present invention will now be described with reference to the accompanying drawings, wherein:- Figure 1 is a perspective view of the recording medium and system according to one example of the present invention; Figure 2 is a side elevation, with the recording medium in cross-section, of the system shown in Figure 1; Figure 3 shows another embodiment of the magneto-optic recording system and medium according to the present invention; Figure 4 shows an example of a pattern of sector information recorded on a recording medium; Figure 5a-5c are a perspective view, enlarged view and partial cross-section of another example of a recording medium according to the present invention; Figures 6a-6b are views similar to Figures 5a-5b of a further examples of a recording medium according to the present invention; Figure 7 illustrates another embodiment of the magneto-optic recording system; Figure 8 illustrates another embodiment of the magneto-optic recording system; Figure 9 shows the characteristics curve of the embodiment of Figure 8; Figure 10 illustrates still another embodiment of the magneto-optic recording system; and, Figure 11 shows the characteristics curve of the embodiment of Figure 10. Figure 1 shows a perspective view of the magneto-optic recording system according to the present invention, and Figure 2 is a cross sectional view of Figure 1. In those Figures, the recording medium is shown by the numeral 10, which has a transparent substrate 11 made of glass. The substrate 11 has a plurality of concentric grooves which function as recording tracks, and said grooves are made by using the conventional photolithographic process after photo-polymer is painted on the glass. The second reproducing magnetic film 12 made of 77 at% Fe - 23 at% Tb is sputtered on the substrate 11 to the thickness 6·10⁻² µm (600 Å), where at% indicates atomic percent. The first recording magnetic film 13 made of 80 at% Co - 20 at% Cr is provided in the thickness of 10⁻¹ µm (1000 Å) on the second reproducing magnetic film 12. The first recording magnetic film 13 is a recording film which has relatively high Curie temperature. In the present embodiment, the direction of the magnetisation in the recording film 13 is in the thickness direction of the film, that is to say, vertical recording is used. The second reproducing magnetic film 12 is called a reproducing film having a higher coercive force than that of the first recording magnetic film 13, and a lower Curie temperature than that of the first recording magnetic film 13. The second reproducing magnetic film 13 is also magnetized in the thickness direction for vertical recording. An optical head 14 functions both to transfer the recorded data on the recording film 13 to the reproducing film 12, and to read the data on the reproducing film 12. The optical head 14 has an optical source 14a for illuminating the medium 10 with a coherent laser beam, a photo-detector 14b for sensing the optical beam reflected by the recording medium 10, and a half mirror 14c which transmits the light of the optical source 14a, but reflects the reflected beam to the photo-detector 14b. The reproduction of the recorded data is performed by using the Kerr effect in which the polarization angle depends upon the recorded data. So a polarizer and a polarization detector (not shown) are mounted in the optical head 14. The numeral 16 is a magnetic head for recording. In the present embodiment, the magnetic head is a main-pole driven single pole type for vertical recording. Of course, other magnetic heads, such as a ring type head, or an auxiliary-pole-driven single pole type head is possible for vertical recording. The width of the main pole of the magnetic head 16 is about 300 µm, which is much larger than the width of a track which is about 1.6 µm. The present invention has the advantage that the high density recording on a track of 1.6 µm width is carried out by using the wide magnetic head with the width of 300 µm, as described later. In operation, it is assumed that the recording medium 10 rotates so that the medium 10 moves in the arrow A in the figures. The magnetic head 16 records binary data on the first recording magnetic film 13. The process of the magnetic recording in the present invention is similar to that of a conventional magnetic recording process. The recording field is for instance 3,18·10⁵ A/m (4000 Oe), which is higher than the coercive force Hc of the first recording magnetic film 13. The coercive force Hc of Co-Cr film is for instance 5,57·10⁴ A/m (700 Oe). Therefore, the first recording magnetic film 13 is magnetized according to the recording data. On the other hand, the second reproducing magnetic film 12 made of Tb-Fe has a coercive force Hc of 1,19·10⁶ A/m (15000 Oe), and therefore, the second reproducing magnetic film 12 is not magnetized by the recording field generated by the magnetic head 16. Next, in transfer process, the recording medium 10 is heated by the laser beam 15 by the optical head 14. The beam power of the laser 14a is about 10 mW, which may raise the temperature of the illuminated portion of the recording medium 10 up to 150 °C. The Curie temperature of the second reproducing magnetic film 12 made of Tb-Fe is 125 °C, and the Curie temperature of the first recording magnetic film 13 made of Co-Cr is about 600 °C. The laser beam 15 of the optical head 14 has a beam diameter of about 1 µm, and both the first recording magnetic film 13 and the second reproducing magnetic film 12 are heated by the laser spot to 150 °C. When the films 12 and 13 are heated by the laser spot, the second film 12 (reproducing film) which has a lower Curie temperature loses its magnetization, while the first film 13 (recording film) retains its magnetization. Thus, the magnetic medium according to the present invention is first recorded magnetically by a magnetic head, and then, upon movement of the medium, the medium is heated by an optical head 14 which is located downstream of the magnetic head 16 along the moving path of the medium 10. Next, when the medium 10 moves further, and the temperature of the medium irradiated by the laser beam 15 is decreased, the reproducing film 12 has the magnetization again, and is magnetized in the same direction as that of the recording film 13 which is positioned close to the reproducing film 12. Thus, the magnetic pattern on the recording film 13 is transferred to the reproducing film 12 by heating and cooling the films 12 and 13. It should be appreciated that the width W₃ of a track on the reproducing film 12 is defined by the spot size of the laser beam 15, in spite of the width W₂ of the magnetic head 16, therefore, the present invention can provide the high density recording defined by an optical beam spot. The reproduction of the recorded data is performed under the principle of the Kerr effect in which the polarization angle of reflected beam depends upon the recorded data. In the reproducing process, the medium 10 is irradiated by the laser beam 15 which has the power of 2 mW, so that the reproducing film 12 is not heated to the Curie temperature. The beam reflected by the reproducing film 12 carries the recorded information, and the reflected beam is sensed by the photo-detector 14b through the half mirror 14c. The reproducing operation using the Kerr effect is conventional. The overwriting on the present recording medium 10 is performed merely by repeating the write operation mentioned above, including application of an input data to the magnetic head, and transferring data from the recording film to the reproducing film. The residual component which is not erased in the overwrite operation is about -40 dB, which is sufficiently low. The head fringing field in the overwrite operation magnetizes only the recording film 13, but does not affect the reproducing film 12, since the reproducing film 12 has the much higher coercive force Hc than that of the recording film 13. Experiment 1 The magnetic binary bits with bit length of 10 µm is recorded on the recording film 13, then, the data is transferred to the reproducing film by irradiating the films by a laser beam of 10 mW of power and 1 µm of spot size (diameter). The signal to noise ratio (S/N) of the reproduced signal is 25 dB. Next, we overwrite on the written area of the medium by the bit length of 15 µm. When we reproduce the overwritten data, after transferring the overwritten data to the reproducing film by heating the films by using the laser beam, the signal to noise ratio of the overwritten reproducing signal is 20 dB. It should be appreciated that the optical head 14 in Figs.1 and 2 functions both for heating means for the transfer process, and the reproducing head for the reproducing phase, by switching the laser beam strength. It should be understood of course that the heating means may be separated from the reproducing optical head, depending upon the design choice of the system. The present invention has the advantages as follows. Firstly, an overwritten magneto-optical recording is obtained without using a particular erasing operation. Secondly, the high speed recording defined by a magnetic recording, together with the high density recording as defined by the optical recording, are obtained simultaneously. High speed recording up to 50-60 MHz, and high density recording using µm order of track width are obtained. Further, since the recording width of the magnetic head is rather wide, no specific track servo operation for the magnetic head is necessary, and a conventional magnetic head for a wide track is available for high density recording. Further, the reproducing signal is free from noise caused by dust and/or defects in the magnetic films, since the reproducing beam irradiates the magnetic films through a glass substrate. The recording magnetic film is not restricted to Co-Cr, but also amorphous of rare earth element and transition metal element alloy, Barium ferrite, and Co-Cr films with some additives are available. Further, when longitudinal magnetic recording is used instead of vertical recording γ-Fe₂O₃ film is available as a first recording magnetic film. Also, a reproducing magnetic film is not restricted to Tb-Fe, but Mn-Bi alloy, amorphous of rare earth element and transition metal alloy, YIG, and Co-ferrite films are available, so long as it is magnetized in the thickness direction, and can have a lower Curie temperature than that of a recording film, and higher coercive force than that of a recording film. An example of a rare earth-transition alloy as recording film is described in the experiment 1A below. Experiment 1A The recording magnetic film 13 may be made of rare earth-transition metal alloy. By selecting the composition of the film, Curie temperature and coercive force are widely controlled. For example, a Gd-transition metal alloy has a higher Curie temperature and a lower coercive force than those for a Tb-transition metal alloy. A 23 at% Tb + 77 at% Fe film (reproducing film), 0.1 µm thick, is deposited on the Gd+Tb+Fe film. Curie temperature and coercive force of the Tb+Fe film are 125 °C and 1,19·10⁶ A/m (15000 Oe), respectively. A 20 at% Gd + 5 at% Tb + 75 at% Fe film (recording film), deposited on a pregrooved glass substrate by RF-magnetron sputtering method, has 180 °C Curie temperature and 6,36·10⁴ A/m (800 Oe) coercive force. The film thickness is 0.3 µm. The 0.1 µm thick protection film of SiO₂ is coated on the reproducing film. An auxiliary-pole-driven single pole type magnetic head is used for writing the data. A single pole thickness is 3 µm and core width is 300 µm The pole is made of pure iron. This single pole contacts the recording medium and slides at a relative velocity of 10 cm/sec. All-one bits with 10 µm length are recorded on the recording film. At that time, the magnetic field caused by the auxiliary-pole is 400 Oe. Next, the optical head is used for the transfer and reproducing process. A laser beam with 0.7 um diameter and 6 mW power irradiates through the glass disk substrate to transfer the magnetic information from the recording film to the reproducing film. Then, a laser beam with power of 1 mW is used for reproducing the transferred data. In both the transfer and reproducing processes the relative velocity is 5 m/sec. The S/N ratio for the reproduced data is 40 dB. By repeating the same recording, transfer and reproducing conditions, overwrite operation is completed. After the overwrite sequence, the component of the former recorded data is reduced by -35 dB. Fig.3 shows another embodiment of the present invention, in which the same numerals in Fig.3 show the same members as those in Fig.1 and Fig.2. The feature of Fig.3 is that the optical head 14 resides on the same side as that of the magnetic head 16, in view of the recording medium 10, while those heads are located on opposite sides of the recording medium in the previous embodiment. The magnetic head 16 in Fig.3 is a ring type head having a core with a gap 16b, and a coil 16a wound on the core. Said ring type head is also available for vertical recording. Since the magnetic head 16 and the optical head 14 reside on the same side of the recording medium, the sequence of two magnetic films 12 and 13 is opposite to that of the previous embodiment of Figs.1 and 2. That is to say, in the embodiment of Fig.3, the recording magnetic film 13 is attached to the substrate 11, and the reproducing magnetic film 12 is attached to the recording magnetic film 13. The substrate 11 need not be transparent in this embodiment, since the optical head 14 does not read the reproducing film through the substrate. By the way, if the recording film 13 is transparent, the sequence of the two films may be that of Fig.1 so that the optical head 14 reads the reproducing film 12 through the recording film 13. The embodiment of Fig.3 has the similar effect to that of the previous embodiment. Next, the synchronization between the write operation and the read operation is described in accordance with Figs.4 through 6. Since the present invention has a magnetic write head and an optical read head with some spacing, the synchronization between write data and read data must be considered. Fig.4 is one solution for the synchronization. In Fig.4, a sector information A is written in advance in the perpendicular direction to the data tracks in both the recording film 13 and the reproducing film 12, so that the width of the sector information A is wider than the width of a recording track by a magnetic head 16. The symbols (a) and (b) in Fig.4 show the vertical magnetization in the up or down direction of the paper. The numeral 18 is a land portion and 19 is a groove portion of a substrate. In the write process, the magnetic head 16 reads out first the sector information A, and then, a clock signal in a write circuit (not shown) is synchronized with the sector information. Then, the magnetic head 16 writes the data on the track just after the sector information A so that the write data synchronizes with an operational clock signal. In the transfer process, the magnetic pattern on the recording film is transferred to the reproducing film by heating the medium. In the reproducing process, the optical head 14 first reads out the sector information on the reproducing film, then, the clock signal in a read circuit (not shown) is synchronized with the sector information. And then, the optical head 14 reads out the data on a track so that the read out data synchronizes with an operational clock signal. It should be appreciated that the sector information which is once recorded is never erased in a plurality of overwriting operations since it is written on both the recording film and the reproducing film, and so it is used as a reference of position in both the write process and reproducing process. Thus, the correct read operation which synchronizes with the write operation is assured. In a preferred embodiment, the sector information A is binary bits with length of 20µm, a number of bits of the sector information along the moving direction of a track is 100, the width of a write track by a magnetic head is 300 µm, and the spot diameter of a laser beam is 1 µm. In our experiment, in said preferred embodiment, the relative error between the read out signal and the operational clock signal is less than 4 %, which shows that the synchronization between the write process and the read process is complete. It is preferable that a transfer process which is carried out just after write process is also synchronized with said sector information by reading said sector information by an optical head. Alternatively, a coarse synchronization in which an optical head is energized to heat the medium after a predetermined time of write process, may be possible, since the transfer process does not need the strict synchronization like the write process and the read process. Another embodiment of the sector information for synchronization of the write and the read operations is described in accordance with Figs.5 through 6. In those figures, a disk shaped substrate for magneto-optic recording is provided with concentric grooves 37 for data tracks in the circumferential direction of the disk, and at least one linear groove 38 in radial direction. The radial groove 38 is perpendicular to the circumferential grooves 37. Fig.5b is the enlarged view of the portion I of Fig.5a, and Fig.6b is the enlarged view of the portion II of Fig.6a. Fig.5c is the enlarged cross section along A-A of Fig.5b. In Figure 5 the radial groove 38 is provided on both the land portion and the groove portion of the circumferential grooves 37, and in Figure 6 the radial groove 38 is provided on only land portion of the circumferential grooves 37. In those embodiments in Figs.5 through 6, it is assumed that the whole area of the recording film and the reproducing film is initially magnetized in the vertical direction of the film plane. The magnetic field for that magnetization is for instance 20 KOe, which is higher than coercive force Hc of both the recording film and the reproducing film. It should be noted that the radial groove 38 is essentially wide sector information wider than a track width, since the radial groove 38 extends whole circumferential tracks. In the write process, a magnetic head 16 first reads out the initially recorded sector information. And, it should be appreciated that the magnetic head 16 can recognize the location of the radial groove 38, since the read out level by the magnetic head 16 depends upon the separation between the magnetic head 16 and the surface of the magnetic medium 31. In the radial groove portion, it should be noted that the head-medium separation depends upon whether the head 16 faces the land portion of a track, or a groove portion (radial groove) of a track. In other words the read out level is decreased at the radial groove portion, since the separation between the head 16 and the recording medium is large at that portion, as shown in Fig.5c. Thus, the magnetic head recognizes the radial groove by the read out level. When the magnetic head 16 recoginzes the radial groove 38, the information data is recorded after the radial groove 38. In the reproducing process, the strength of the reflected beam depends upon whether it is on the radial groove or not. Therefore, the optical head can recognize the position of the radial groove 38. When the radial groove is recognized, a clock signal of a reproducing device is synchronized with the sector information, and the data is read out by using said clock signal. Thus, in our experiment, the error between a clock signal and a reproduced signal is less than 4 %, which shows that the synchronization is complete. In the above embodiment, a bit length of initial magnetic recording for data is 2 µm, and the spot diameter of a laser beam is 1 µm. Fig.7 shows the structure of another embodiment of the recording medium according to the present invention. In the figure, the recording medium 10B has a substrate 11, a recording magnetic film 13 attached on the substrate 11, a reproducing magnetic film 12 attached on the recording magnetic film 13, and a protection film 22 attached on the reproducing magnetic film 12. The numeral 14 is an optical head, 15 is a laser beam, and 16 is a magnetic head with a ring type head core and a coil wound on the core. The numeral 16a is a coil wound on the core, and 16b is a gap of the ring type head core of the magnetic head 16. The feature of the embodiment of Fig.7 is that the recording film 13 is recorded with the magnetization directed in the plane direction of the recording film 13 (plane recording), while the embodiment of Fig.1 records the signal by the vertical magnetization which is orthogonal to the plane direction of the recording film (vertical recording). The arrow p shows the direction of the magnetization in the recording magnetic film 13, and the arrow q shows the direction of the magnetization in the reproducing magnetic film 12. Even when the recording film is magnetized in the plane direction, it is possible to transfer the magnetization in the recording film 13 to the reproducing film 12, since the plane magnetization in the recording film 13 causes some vertical component of magnetic flux. The direction of the magnetization in the reproducing film is still in the thickness direction. Experiment 2 A glass disc is used as a substrate 11. The recording magnetic film 13 made of -Fe₂O₃ with the additive of 2.0 at% Co + 2.0 at% Ti + 1.5 at% Cu is sputtered on the substrate 11 to a thickness of 0.17 µm. Then, the reproducing magnetic film 12 made of 77 at% Fe - 23 at% Tb is attached on the recording magnetic film 13 with a thickness of 0.1 µm. The protection film 22 made of SiO₂ is coated on the reproducing magnetic film 12 in order to protect the reproducing magnetic film 12. The magnetic characteristics of the films 12 and 13 are shown in the table 1. The magnetic head 16 is a ring type head made of Mn-Zn ferrite, having the core width 18.5 µm, the gap length 0.85 µm, and the number of turns is 36. The spacing between the magnetic head 16 and the recording medium 10B is 0.27 µm when the recording medium rotates with a circumferential velocity of 20 m/sec. In write process, a signal with bit length 2 µm is recorded by the write current 25 mA. This is a longitudinal recording. Then, the recording medium is heated up to 140 °C to transfer the magnetism on the recording film 13 to the reproducing film 12. In reproducing process, the optical head 14 reads out the signal on the reproducing film 12 according to the Kerr effect principle. The laser beam power in the reproducing process is 1 mW, and the circumferential velocity is 5 m/sec. The S/N ratio of the reproduced signal is 45 dB. In order to test the overwrite characteristics, a bit of 3 µm length is recorded by the magnetic head 16. Then, said bit of 3 µm length is transferred to the reproducing magnetic film 12 by heating the recording medium to 140 °C, then, the optical head 14 reads out the 3 µm bit length signal. The S/N is 43 dB. The level of 2 µm length signal which is recorded previously has the output level lower than the 3 µm length signal by 36 dB. Thus, it is confirmed that the overwrite characteristics are excellent. Experiment 3 Using the structure of Fig.7, the recording magnetic film 13 made of γ-Fe₂O₃ with the additive of 1.0 at% Os and a thickness of 0.17 µm is attached on the substrate. Then, the reproducing magnetic film 12 made of 12 at% Co - 65 at% Fe - 23 at% Tb is attached on the recording magnetic film 13 with a thickness of 0.1µm. The protection film 22 made of SiO₂ is attached on the reproducing film 12 with a thickness of 0.1 µm. The table 2 shows the magnetic characteristics of the recording magnetic film and the reproducing magnetic film. The magnetic head is a ring type head made of Mn-Zn ferrite core with the core width 18.5 µm, the gap length 0.85 µm, and 36 turns of winding. The spacing between the head and the recording medium is 0.27 µm when the circumferential velocity of the recording disk is 20 m/sec. In write process, a bit of 2 µm length is recorded by the write current 25 mA. Then, the recording medium is heated to 250 °C to transfer the recorded pattern in the recording magnetic film to the reproducing film. In reproducing process, the optical head 14 reproduces the signal on the reproducing film 12 under the condition that the laser power is 1 mW, and the circumferential velocity of the medium is 5 m/sec. The resultant S/N is 48 dB. The overwrite characteristics are tested further. A signal of 3 µm length signal is overwritten on the recording film 13. Then, the recording medium is heated to 250 °C to transfer the pattern. And, the optical head 14 reads out the signal on the reproducing film. The C/N at that time is 45 dB. And, the level of 2 µm length signal which is recorded previously is lower than the 3 µm signal by 35 dB. Thus, it is confirmed that the overwrite operation is excellent. The composition of the recording magnetic film and the reproducing magnetic film is analyzed. The magnetic flux from a magnetic head is usually several thousands Oe. Therefore, it is preferable that the coercive force of the recording film is less than 2000 Oe. It should be noted that the coercive force of γ-Fe₂O₃ increases by adding Co or Os. The 2000 Oe of coercive force is obtained by adding Co at 8 at%, or Os at 3 at%. Therefore, it is preferable that the amount of the additive is less than 8 at% when the additive is Co, and is less than 3 at% when the additive is Os. As for the reproducing magnetic film, it is essential that the coercive force at room temperature is higher than that of the recording magnetic film, and the Curie temperature is lower than that of the recording magnetic film. Preferably, the coercive force is higher than the magnetic field caused by the head, in order not to be recorded by a magnetic head. By the way, an amorphous film of rare earth element and transition metal alloy has the compensation composition in which the magnetic moment of rare earth element cancels that of transition metal, and no resultant magnetization appears. When the composition is close to the compensation composition, an extremely high coercive force is obtained. Therefore, it is preferable that the reproducing magnetic film made of amorphous thin film of rare earth element and transition metal is close to the compensation composition. The example of the compensation composition when the rare earth element is Tb and the transition metal is 85 at% Fe -15 at% Co is the composition that the ratio of Tb is 23 at%. On the other hand, a coercive force higher than 2 KOe is obtained when the ratio of Tb is in the range between 21 at% and 30 at%. Therefore, the preferable composition of the reproducing magnetic film is that Tb is included in the range from 21 at% to 30 at%. Fig.8 shows another embodiment of the magneto-optic recording medium according to the present invention. In the figure, the recording medium 10A has the substrate 11, the soft magnetic film 20 attached on the substrate 11, the first recording film 13 attached on the soft magnetic film 20, and the second reproducing magnetic film 12 attached on the first recording magnetic film 13. The numeral 14 is an optical head, 15 is a laser beam, and 16 is a magnetic head for vertical recording. The feature of the embodiment of Fig.8 is the presence of the soft magnetic film 20 between the first recording magnetic film 13 and the substrate 11. Experiment 4 A soft magnetic film 20 made of 78 at% Ni - 22 at% Fe (permalloy) having initial permeability 4000 and Curie temperature 580°C is attached on the substrate 11 with a thickness of 0.5 µm. Then, the first recording magnetic film 13 made of 78.5 at% Co - 21.5 at% Cr, having anisotropic field 3,58·10⁵ A/m (4500 Oe) and coercive force 7,96·10⁴ A/m (1000 Oe), and Curie temperature 600°C is attached on said soft magnetic film 20 with a thickness of 10⁻¹ µm (1000 Å). Then, the second reproducing magnetic film 12 made of 79 at% Fe - 21 at% Tb, having coercive force 1,19·10⁶ A/m (15000 Oe) and Curie temperature 125 °C is attached on said first recording magnetic film 13 with a thickness of 6·10⁻² µm (600 Å). The substrate 11 is made of glass having concentric track grooves produced through a photolithographic process after ultraviolet setting resin photo-polymer is painted on. The similar recording medium which is the same as above recording medium, except it has no soft magnetic film 20 is also prepared for the sake of comparison. The recording current in the magnetic head 16 for providing a predetermined reproducing output level is measured. Fig.9 shows the curves of the experimental result, in which the horizontal axis shows the write current in the magnetic head 16, and the vertical axis shows the reproducing output level (V p-p ). The curve A in Fig.9 shows the characteristics of the recording medium having the soft magnetic film, and the curve B shows the characteristics of the recording medium having no soft magnetic film. It should be noted in Fig.9 that the write current for the recording medium having the soft magnetic film is considerably smaller as compared with that of the recording medium having no soft magnetic film. Fig.10 shows still another embodiment of the recording medium according to the present invention. In the figure, the recording medium 10C has a substrate 11, a first recording magnetic film 13 attached on the substrate 11, a non-magnetic intermediate film 24 attached on the first recording magnetic film 13, a second reproducing magnetic film 12 attached on the non-magnetic intermediate film 24, and a protection film 22 attached on the second reproducing magnetic film 13. The numeral 14 is an optical head, and the numeral 16 is a magnetic head. The feature of the embodiment of Fig.10 is the presence of the non-magnetic intermediate film 24 between the first recording magnetic film 13 and the second reproducing magnetic film 12. In our analysis, when the residual magnetization is lower than the saturation magnetization like Co-Cr film, a small reverse magnetic domain exists in each magnetic domain. Although the direction of the magnetic field in the magnetic domain is defined by the write signal, a small reverse magnetic domain having the opposite direction field exists in each magnetic domain. Therefore, when the storage in the recording film is transferred to the reproducing film, the transferred storage in the reporducing film is influenced by not only the main magnetic domain, but also by the small reverse magnetic domain. As a result, the presence of the reverse magnetic domain causes an increase of noise, and/or a decrease of reproducing signal level. When the small reverse magnetic domain is assumed to be a stripe domain with the wavelength (λ), the vertical magnetic flux Hz in the thickness direction of a magnetic film is expressed by the following equation. Hz = k exp(-2πz/λ) where k is constant, and z (µm) is length from film surface. Assuming that the small reverse magnetic domain is a crystal grain with the diameter about 500 Å, and the (λ) is about 0.1 µm, which is twice as large as said diameter, the value Hz is decreased to 1/1000 when the length z increases from 0 to 0.1 µm. Therefore, it should be noted that the presence of non-magnetic intermediate film which is about twice as thick as the width of the small reverse magnetic domain can decrease considerably the influence of the small reverse magnetic domain. Thus, the reproducing magnetic film is recorded with only the desired signal. The similar analysis is possible when the recording film is amorphous film of rare earth element and transition metal alloy. Experiment 5 The recording medium of Fig.10 is manufactured. The substrate 11 is glass, on which the recording film 13 having soft magnetic film is sputtered. The recording film 13 has a permalloy film of 0.3 µm, and 81.5 at% Co - 18.5 at% Cr of 0.9 µm. The permalloy film is provided to decrease the write current as described in accordance with Figs.8 and 9. The reproducing film 12 made of 77 at% Fe - 23 at% Tb is produced with a thickness of 0.1 µm. The table 3 shows the magnetic characteristics of the recording film Co-Cr, and the reproducing film Tb-Fe. The non-magnetic intermediate film 24 between the recording film 13 and the reproducing film 12 is made of SiO₂, with the thickness 0, 0.5, 0.1, 0.2 and 0.4 µm. The protection film 22 made of SiO₂ with the thickness 0.1 µm is also coated. The write signal with the bit length 10 µm is stored in the recording film with the magnetic field 300 Oe. Next, the recording medium is heated up to 140 °C in vacuum condition to transfer the magnetic pattern on the recording film to the reproducing film. Next, the signal is reproduced with the laser beam having the laser power 1 mW. Fig.11 shows the experimental curve in which the horizontal axis shows the thickness of the non-magnetic intermediate film, and the vertical axis shows the C/N (carrier to noise ratio in dB) of the reproduced signal. Fig.11 shows that the value S/N is the maximum when the thickness is 0.1 - 0.2 µm. When the non-magnetic film is too thick, the transfer of the desired signal becomes incomplete, and so, the value S/N decreases. The desired thickness of the non-magnetic intermediate film is 1-2 times of the width of a small reverse magnetic domain. It should be noted that any combination of the above embodiments is possible to those skilled in the art. For instance, the structure of the recording medium may be one of the embodiments of Fig.1, Fig.7, Fig.8 and Fig.10. Any structure of the recording medium may have a structure for providing a sector information by one of the embodiments of Figs.4 through 6. In any type of recording medium, the sequence of the recording film and the reproducing film is arbitrary, in other words, the recording film is attached on the substrate and the reproducing film is attached on the recording film, or the reproducing film is attached on the substrate and the recording film is attached on the reporducing film. The soft magnetic film may be inserted between the recording film and the substrate in any embodiment, and the non-magnetic intermediate film may be provided between the recording film and the reproducing film in any embodiment. The protection layer may be used in any embodiment. From the foregoing, it will now be apparent that a new and improved magneto-optic recording system has been found.

Claims: A magneto-optic recording medium (10) comprising: a substrate (11) having a plurality of recording tracks and being provided with a first recording magnetic film (13) and a second reproducing magnetic film (12), the first recording magnetic film (13) having a predetermined first Curie temperature and a predetermined first coercive force, the second magnetic film (12) having a predetermined second Curie temperature and a second coercive force, wherein the first Curie temperature is higher than the second Curie temperature, and the first coercive force is lower than the second coercive force wherein both the first and second magnetic films (13, 12) of the recording medium (10) are provided with sector information in a direction perpendicular to the direction of a recording track to define a start point which indicates the start of a recorded signal. A magneto-optic recording medium (10) according to claim 1, wherein the first magnetic film (13) and the second magnetic film (12) are initially recorded with sector information in the perpendicular direction of the recording track. A magneto-optic recording medium according to claim 1 or claim 2, wherein the substrate (11) has a groove (38) extending orthogonally to the recording track. A magneto-optic recording medium according to any of claims 1 to 3, wherein the first magnetic film (13) is for vertical recording. A magneto-optic recording medium according to any of claim 1 to 3, wherein the first magnetic film (13) is for longitudinal recording. A magneto-optic recording medium according to any of the preceding claims, wherein a soft magnetic film (20) is provided between the substrate (11) and the two magnetic films (12,13). A magneto-optic recording medium according to any of the preceding claims, wherein a non-magnetic film (24) is inserted between the first magnetic film (13) and the second magnetic film (12). A magneto-optic recording medium according to any of the preceding claims, wherein the second magnetic film (12) is provided on the substrate (11), the first magnetic film (13) is provided on the second magnetic film (12), and the substrate (11) is optically transparent. A magneto-optic recording medium according to any of claims 1 to 7, wherein the first magnetic film (13) is provided on the substrate (11), and the second magnetic film (12) is provided on the first magnetic film. A magneto-optic recording medium according to any of preceding claims, wherein the first magnetic film (13) is Co-Cr, and the second magnetic film (12) is Tb-Fe. A magneto-optic recording medium according to any of claims 1 to 9, wherein the first and said second magnetic film is amorphous of rare earth and transition metal alloy. A magneto-optic recording system comprising a) a magneto-optic recording medium (10) according to any of the preceding claims; b) a magnetic head (16) positioned close to the magneto-optic recording medium (10), the head having a core and a coil wound on the core, for generating a magnetic signal having a magnetic field strength which is higher than the first coercive force and is lower than the second coercive force, whereby the magnetic signal is recorded in the first recording film (13); and c) heating means (14) located downstream along the path of relative movement between the magnetic head and the recording medium from magnetic recording head (16) for selectively heating the recording medium (10) to a temperature which is higher than the second Curie temperature and lower than the first Curie temperature, in order to transfer the magnetic pattern recorded on the first magnetic film (13) to the second magnetic film (12) wherein both the first and second magnetic films (13, 12) of the recording medium (10) are provided with sector information in a direction perpendicular to the direction of a recording track to define a start point which indicates the start point of a recorded signal. A system according to claim 12, further comprising an optical head (14) having at least a laser source (14a) and a laser sensor (14b), located close to the recording medium, for reproducing signals recorded on the second magnetic film (12) by irradiating the second magnetic film with a coherent beam and sensing the polarised angle of the reflected beam which is dependent upon the signal on the second magnetic film (12). A magneto-optic recording system according to claim 13, wherein the laser source (14a) in the optical head (14) also constitutes the heating means wherein the laser source generates a laser beam strong enough to heat the recording medium to a temperature higher than the second Curie temperature during step c. A magneto-optic recording system according to any of claims 12 to 14, wherein the substrate (10) is provided with grooves in the normal direction to a track to provide synchronisation between recording signal and reproducing signal by showing the starting point of record of the groove. A magneto-optic recording system according to any of claims 12 to 15, when dependant on claim 8, wherein the heating means is positioned on the opposite side of the medium (10) to the magnetic head. A magneto-optic recording system according to any of claims 12 to 15, when dependant on claim 9, wherein the heating means is positioned on the same side of the medium (10) as the magnetic head. A magneto-optic recording system according to claims 12 to 17, wherein the heating means heats only a part of the recording medium recorded by the magnetic head.

Inventors: HATAKEYAMA, IWAO, IIJIMA, TETSUO, ISHII, OSAMU, NONAKA, KOUTAROU
Applicants: NIPPON TELEGRAPH AND TELEPHONE CORPORATION
Application year: 1988
Main classification: G11B11
IPC codes: G11B5, G11B11