Method and apparatus for magneto-optical recording

Abstract: A method for magneto-optical recording using a magnetic recording medium and means for emitting a pulsed laser, the magnetic recording medim comprising a memory layer for retaining domains with field orientations representative of binary data, and a reference layer laminated directly or via an intermediate thermally conductive layer onto the memory layer, where the magnetic properties of the reference layer vary with the temperature in a different waqy from those of the meory layer, the domains of desired magnetization orientations being set in the memory layer by utilizing the change in magnetic property of the reference layer resulting from the temperature change, the method comprising the steps of: moving the magnetic recording medium relative to the laser pulse emission means; and controlling the temperature of the reference layer selectively by alternating the durations of the laser pulses generated by the laser pulse emission means for heating the memory layer to a temperature near or above the Curie temperature, according to the binary data to be recorded in the memory layer, thereby changing the magnetic property of the reference layer in order to record the desired binary data in the memory layer.

Description: The invention relates to a method and an apparatus for overwritable magneto-optical recording. An optical disk allows higher-density recording than a magnetic disk, but is inferior in high-speed performance, with an access time that is up to ten times as long. A method for remedying this is overwriting. Conventionally, rewriting is done during three turns or passes: erasing on the first turn, recording on the second, and error checking on the third. In contrast, overwriting will allow rewriting during only two turns, by erasing and recording simultaneously. One approach that uses two heads for erasing and recording to permit pseudo-overwriting has been proposed for overwritable magneto-optical recording. However, the system is complicated. Another method that allows simultaneous erasing and recording of adjacent tracks with two laser spots cannot be used in sector-based writing. Also a field modulation method, a light modulation method using an exchange-coupled double-layered film, and a light modulation method using a demagnetizing field have been proposed as direct overwrite methods. Of these, the light modulation overwrite method using an exchange-coupled double-layered film is superior to the field modulation system in that it provides easy high-speed modulation and allows a wide space between the bias magnet and the disk. However, there are problems in that the properties of the media must be controlled accurately, and that the laser power margins or tolerances for reading and writing become smaller. The double-layered film overwrite method disclosed in Japanese Published Unexamined Patent Application (PUPA) No. 62-175948 is explained below. The recording layer used in this method consists of two layers, a memory layer and a reference layer, which are exchange-coupled. Overwriting is performed by utilizing the difference in temperature dependence of the coercive forces (Hc) of the two layers. Figure 15 shows the magnetic properties of an overwritable disk, and Figure 16 shows a method of overwriting on this type of medium. Basically, this method utilizes the magnetic properties that the coercive force of the reference layer (Hca2) is smaller than that of the memory layer (Hca2) at room temperature (Tamb1) and that the Curie temperature of the reference layer (Tc2) is higher than that of the memory layer (Tc1). The magnitude of the external field Hini applied before laser emission is set so that Hca2 < Hini < Hca1. First, only the magnetization of the reference layer follows Hini. In the example shown in Figure 16, the direction of the magnetization of the reference layer becomes downward. The memory layer retains the recorded information, because Hca1 is large. When a recording medium in this state is irradiated with a low-power laser beam, the temperature of the recording layer TL becomes Tc1 < TL < Tc2. Thus, the magnetization of the reference layer is not reversed by the weak external field Hb, so that the magnetization of the memory layer is oriented downward during the cooling process, following the magnetization of the reference layer, as shown in Figure 16 (erasing). Thus, although the directions of the magnetic moments of similar atoms become essentially parallel to each other, in this case the directions of magnetization also become parallel to each other. When the laser power is high, the temperature of the recording layer TH becomes higher than Tc2. Thus the magnetization of the reference layer is reversed by the external field Hb, so that during the cooling process (writing) the magnetization of the memory layer is oriented in the same direction, that is, downward in Figure 26. Recording by using the magnetization of the reference layer is hereinafter referred to as the "L process" and recording by using an external field is referred to as the "H process." The name of each process is derived from the temperature of the reference layer. Figure 17 shows the experimental results of the overwriting characteristics for a double-layered film whose memory layer consists of TbFeCo and whose reference layer consists of DyFeCo, reported by Matsumoto Hiroyuki, et al. in "Magneto-optical Disk for Direct Overwrite by Light Power Modulation Method," Symposium on Optical Memory '88, Article Collection 45 (1988). The right side of Figure 17 shows the carrier level in the H process, which is a recording process with high laser power. The results are obtained by using a modulated light of 1 MHz to record on the medium with its data erased. The left side of Figure 17 shows the signal level of data left unerased during the L process, which is an erasing process with low laser power. The results are obtained by using CW light to erase signals of 1 MHz written onto a medium. When the H/L processes are done by modulating the power of pulses of long duration (the duration is hereinafter referred to as "pulse width") of the order of one hundred nanoseconds conventionally, it is necessary to divide the laser power level into three regions: PR (reading), PL (L process), and PH (H process). Accordingly, the margin or tolerance for each of them is lower than when overwriting is not performed, and therefore it is sufficient to provide only two power levels for reading and writing. Furthermore, since Tc2 is set at a high temperature to obtain a margin for laser power in the L process (PL), the medium is exposed to a high temperature in the H process, which may cause deterioration. Other problems are that the decreased margin requires accurate control of the properties of the medium, and that the characteristics of write/read are apt to be influenced by fluctuations in the laser power and ambient temperature. The magnetic recording medium disclosed in Japanese PUPA No. 62-80847 comprises a memory layer for retaining domains with desired field orientations representative of binary data, a reference layer for providing a bias field as a function of the temperature for obtaining the domains of desired magnetic field orientations in the memory layer, and a thermal isolation layer for isolating the memory layer from the reference layer. Laser pulses are emitted from the memory-layer side of the medium and the durations are changed in response to recording or erasing. During recording, the duration is typically decreased to 50 nanoseconds so that the memory layer is heated to above the Curie temperature, while the reference layer, which is isolated by the thermal isolation layer, is held at a relatively low temperature. During erasing, on the other hand, duration is typically increased to 500-600 nanoseconds so as to heat the reference layer to a sufficiently high temperature. However, sufficiently long durations of laser pulses for heating the reference layer, which is isolated by the thermal insulation layer, require slow disk rotation, hence prevent an increase in the data transfer rate. Furthermore, interposition of the thermal isolation layer is considered to make it impossible to utilize the exchange-coupling between the memory layer and the reference layer described in Japanese PUPA No. 62-175948. EP-A-0 257 530 already describes to control the duration of the laser pulses for performing the L and H process; in the L process however, the entire double layer recording medium is heated above the Curie temperature of the memory layer. Accordingly, therefore, the present invention provides apparatus for magneto-optical recording, the apparatus comprising: a magnetic recording medium comprising a memory layer and a reference layer laminated onto the memory layer either directly or via an intermediate thermally conductive layer, the Curie temperature of the reference layer being greater than or equal to the Curie temperature of the memory layer; means to apply a bias magnetic field to the recording medium; means arranged to emit laser pulses incident on the memory layer side of the magnetic recording medium; and means to selectively control the temperature difference between the reference layer and the memory layer by causing laser pulses to be emitted of either a first or a second predetermined duration in accordance with binary data thereby to record the data in the memory layer, the first predetermined value of the duration of the laser pulses being short enough so that the heating of the memory layer is completed before the whole layer reaches thermal equilibrium such as to induce a temperature difference between the memory layer and the reference layer such that half or more of the memory layer is heated to a first temperature at least equal to the Curie temperature of the memory layer so that the magnetisation of the memory layer follows the magnetisation of the reference layer and half of the reference layer is heated to a second temperature less than the Curie temperature of the reference layer so that the magnetisation direction of the reference layer is not changed from an initial state by the bias magnetic field, the second predetermined value thereof being such as to heat half of the reference layer to a temperature at least equal to the Curie temperature of the reference layer so that the magnetisation direction of the reference layer is changed from an initial state by the bias magnetic field. The present invention enables data to be recorded in the memory layer by changing the temperature gradients across the thickness of the recording medium and thus controlling the temperature of the reference layer. Various preferred features of the embodiments of the invention are set out in the dependent claims. In preferred forms of the invention, a desired set of binary data can be recorded and the selective controlling of the temperature difference can selectively control the magnetic properties of the reference layer to record the desired binary data in the memory layer. The first predetermined value of the duration of the laser pulses induces a temperature difference between the memory layer and the reference layer whilst a second longer predetermined value of the laser pulses induces no substantial temperature difference between the layers. In this case the temperature difference between the layers is controlled by selecting either the first or the second predetermined value in accordance with the binary data. This scheme makes overwrite recording possible by utilizing the exchange-coupling between the memory layer and the reference layer. It also makes it possible to increase the laser power margin by using in the L process short pulses that produce a sufficiently large temperature difference between the above two layers, while using laser pulses of long duration in the H process so that the temperature of the memory layer and that of the reference layer become high simultaneously, as in conventional cases. In the conventional light modulation overwrite method using an exchange-coupled double-layered film, the characteristics if data writing/readout are vulnerable to fluctuations in laser power and ambient temperature, and cannot cope with fluctuations in the media sensitivity, which makes the method impractical. However, the present invention remedies these problems and makes the multilayered film overwriting method feasible. A further advantage of the present invention is that the materials selected for the memory layer and the reference layer can have substantially the same Curie temperature thereby widening the choice of materials for the medium. According to another aspect of the invention, there is provided a method for magneto-optical recording using a magnetic recording medium comprising a memory layer and a reference layer laminated onto the memory layer either directly or via an intermediate thermally conductive layer, the Curie temperature of the reference layer being greater than or equal to the Curie temperature of the memory layer, the method comprising; applying a bias magnetic field to the recording medium; generating laser pulses incident on the memory layer side of the magnetic recording medium; and selectively controlling the temperature difference between the reference layer and the memory layer by causing pulses to be emitted of either a first or a second predetermined duration in accordance with binary data thereby to record the data in the memory layer, the first predetermined value of the duration of the laser pulses being short enough so that the heating of the memory layer is completed before the whole layer reaches thermal equilibrium such as to induce a temperature difference between the memory layer and the reference layer such that half or more of the memory layer is heated to a first temperature at least equal to the Curie temperature of the memory layer so that the magnetisation of the memory layer follows the magnetisation of the reference layer and half of the reference layer is heated to a second temperature less than the Curie temperature of the reference layer so that the magnetisation direction of the reference layer is not changed from an initial state by the bias magnetic field, the second predetermined value thereof being such as to heat half of the reference layer to a temperature at least equal to the Curie temperature of the reference layer so that the magnetisation direction of the reference layer is changed from an initial state by the bias magnetic field. An embodiment of the invention will now be described with reference to the accompanying drawings wherein: Figures 1 - 9, and Figure 11 are graphs showing the simulation results for temperature changes inside the magnetic recording media; Figure 10 is a graph showing the magnetic properties of a double-layered recording medium, which become usable as a result of the invention; Figure 12 is a schematic view of the experimental system; Figures 13 and 14 are graphs showing the results of the experiment; Figure 15 is a graph showing the magnetic properties of a typical double-layered film recording medium; Figure 16 is an illustration of the overwrite process using a double-layered film recording medium; and Figure 17 is a graph showing the readout characteristics of the medium after magneto-optical recording by the process shown in Figure 16. 1. Temperature Gradient Control by Laser Pulse Duration Modulation The disk structure shown in Table 1 is considered as an example of an exchange-coupled double-layer medium. A relatively thick reference layer with a large thermal conductivity is used under the memory layer. Material Constants and Parameters Used in Calculation Strength distribution: Gaussian distribution (full-width half-maximum diameter 0.9 µm) Laser light Rectangular pulse (L process : 1 nanosecond, H process : 100 nanoseconds) Incident from base side Layer structure Heat conductivity (cal/s˙k˙cm) Density (g/cm³) Specific Heat (cal/g˙k) Thickness (A) Glass substrate 0.0025 2.76 0.200 1.2 x 10⁷ Protective layer 0.003 2.20 0.180 700 Disk Recording layer Memory layer 0.095 7.87 0.097 500 Reference layer 0.095 7.87 0.097 1,500 Protective layer 0.003 2.20 0.180 700 Linear velocity: 10.7 m/s Figures 1 - 4 show the simulated change in peak temperature with time on the recording surface of a disk whose structure is outlined in Table 1. The pulse widths of the emitted lasers are assumed to be 1 nanosecond for a short pulse and 100 nanoseconds for a long pulse. The vertical axis shows the temperature change from room temperature. The values are calculated for the interface between the protective and memory layers, the memory and reference layers, and the reference and protective layers, then normalized by the peak power of the emitted laser. The l-ns pulse raises the maximum temperature of the reference layer on the side opposite to the laser emission, to only 47% of that of the laser emission side of the memory layer, and induces a temperature gradient along the thickness, while the 100-ns pulse raises the maximum temperature of the reference layer to 93% of that of the memory layer, inducing no substantial temperature gradient. A simulation was performed by using the computer program for thermal analysis given by R. Kant and K.L. Dockert in "Laser Induced Heating of a Multilayered Medium Resting on a Half Space: Part II - Moving Source," IBM Research Report RJ 5998 (59597) (1987). Figures 5 and 6 show the simulation results for the temperature rise in a disk of the same structure as in Table 1, except that the thickness of the reference layer is 1000 A. A sufficiently large temperature difference is induced by the l-ns pulse along the thickness, but not by the 100-ns pulse. Figure 7 shows the simulation results for the ratio of the temperature rise at the midpoint of the reference layer to that at the midpoint of the memory layer of the disk outlined in Table 1 when it is irradiated by pulses of various durations. These results indicate that a combination of short pulses of the order of one nanosecond and pulses longer than a few tens of nanoseconds makes it possible to control the temperature difference between the two layers. Short pulses induce temperature gradients because the heating of the recording layer is completed before the whole layer reaches thermal equilibrium. 2. Overwrite Method Using Pulse Time-Width Modulation In the conventional overwrite method by light modulation, both the memory and reference layers are heated to nearly the same temperature in both H and L processes, and writing/erasing is effected by using only the difference in the Curie temperatures of the medium's layers, as shown in Figure 15. The present invention takes advantage of the change in the temperature gradients in the recording layer by using the method described in D.1 to carry out overwriting. When short pulses are emitted, the L process is carried out by utilizing the temperature gradients and raising the temperature of the memory layer only sufficiently to change its magnetization direction (see Figure 8). Here, since the temperature rise in the reference layer is small, the coercive force of the layer is large enough to keep its magnetization direction in the initial state. When long pulses are emitted, both the memory and reference layers can be heated to sufficiently high temperatures. Therefore, the coercive forces of both layers become small, and the H process can be carried out (see Figure 9) to change their magnetization directions. In this case, it is possible in principle to overwrite even if the Curie temperatures of the memory layer and the reference layer are equal, as shown in Figure 10. Figure 11 shows as reference the simulation results for a case in which the long pulse is used even in the L process, as before. The laser power margins in the L/H processes are estimated for the case of a double-layered film of the type shown in Figure 15 on the assumption that the Curie temperature of the memory layer Tc1 equals 135°C, that of the reference layer Tc2 200°C, and the room temperature Ta 20°C. Here, it is also assumed that the L process will occur when a half or more of the memory layer is heated to a temperature of Tc1 or more while a half of the reference layer is less than Tc2 in temperature, and that the H process will occur when a half of the reference layer is heated to a temperature of Tc2 or more. According to the invention, the range of the laser power PL that causes the L process is 58 mW < PL < 132 mW (pulse width: 1 nanosecond) The range of the laser power PH that causes the H process is 8.7 mW < PH (pulse width: 100 nanoseconds) On the same assumption, the ranges in the conventional method are 5.4 mW < PLC < 8.7 mW 87 mW < PHC The ranges of the laser power in the H and L processes can be made widely different by this method. In addition, the laser power margin in the L process is improved from the conventional value 8.7/5.4 = 1.6 to 132/58 = 2.3. As described above, the invention allows overwriting by controlling the temperature gradients of the memory and reference layers, and can improve the laser power margin for data write/read. This permits overwriting whose write/read characteristics are resistant to variations in the laser power and the ambient temperature, and also increases the tolerance toward fluctuation in the sensitivity of the medium. 3. Experiment The following is an explanation of an experiment to demonstrate that the invention increases the laser power margin of the L process. In the experiment, a medium as shown in Table 2 and a system as shown in Figure 12 were used. Layer Composition Thickness Protective layer SiN 90 nm Memory layer Tb20Fe80 (Curie temp. = 130°C) 60 nm Reference layer Tb27Fe63Co10 (Curie temp. = 175°C, Compensating temp. = 155°C) 120 nm Glass substrate - 1.1 mm The thickness of each layer was estimated from the sputtering time. In the experiment, a laser pulse with a full-width half-maximum diameter of 0.47 m was emitted. The time width of the laser pulse was controlled by changing the time width of the current pulse flowing through the laser diode. The bias magnetic field was kept at 110 Oe. Domains written in the memory layer were observed with a polarizing microscope with an oil-immersion objective lens. Observation of domains make it possible to tell whether the L process has been achieved or not. Figure 13 shows the laser power range of the L process for several different pulse durations. Figure 14 shows the relationship between the pulse duration and the ratio of the maximum laser power to the minimum one in the L process, on the basis of the experimental results shown in Figure 13. The ratio increases with a decrease in the pulse duration. In particular, a 2.7-ns pulse expands the range to 1.8 times wider than that of a 56-ns pulse. These results imply that a short pulse of the order of one nanosecond heats up only the memory layer for a wide range of laser power, while the reference layer is kept at a low temperature; that is, that a short pulse induces through-thickness temperature gradients. The above description is given for a medium with a memory layer directly laminated over a reference layer. However, the scope of the invention is not limited to that example. It has been proposed, for example, to put a heat-conductive thin intermediate layer between the memory and reference layers to control the strength of the exchange-coupling. (See K. Aratani et al., "Overwriting on a Magneto-optical Disk with Magnetic Triple Layers by Means of the Light Intensity Modulation Method," Proceedings of Optical Data Storage Topical Meeting, Vol. 1078, 1989, page 258.) The proposed invention is also applicable to magneto-optical recording that uses a medium containing such an intermediate layer. In this case, the power enabling the L process has a higher maximum value than when there is no intermediate layer, and therefore the power margin for the L process increases somewhat. The invention makes it possible to overwrite a medium by controlling the temperature of the reference layer with no thermal isolation layer interposed between the memory and reference layers. It is also possible to expand the margin of the laser power because data is recorded in the memory layer while the reference layer is kept at a low temperature. There has been described a method for magneto-optical recording using a magnetic recording medium and means for emitting a pulsed laser, the magnetic recording medium comprising a memory layer for retaining domains with field orientations representative of binary data, and a reference layer laminated directly or via an intermediate thermally conductive layer onto the memory layer, where the magnetic properties of the reference layer vary with the temperature in a different way from those of the memory layer, the domains of desired magnetization orientations being set in the memory layer by utilizing the change in magnetic property of the reference layer resulting from the termperature change, comprising the steps of: moving the magnetic recording medium relative to the laser pulse emission means; and controlling the temperature of the reference layer selectively by alternating the durations of the laser pulses generated by the laser pulse emission means for heating the memory layer to a temperature near or above the Curie temperature, according to the binary data to be recorded in the memory layer, thereby changing the magnetic property of the reference layer in order to record the desired binary data in the memory layer. A first value for inducing temperature gradients along the thickness of said recording medium and a second value for inducing no substantial temperature gradients can be predetermined as the durations of the laser pulses, and either of said first and second values is selected as the duration of the laser pulse generated by said laser pulse emission means according to the binary data to be recorded in said memory layer. There has also been described an apparatus for magneto-optical recording using a magnetic recording medium and means for emitting a pulsed laser, the magnetic recording medium comprising a memory layer for retaining domains with field orientations representative of binary data, and a reference layer laminated directly or via an intermediate thermally conductive layer onto the memory layer, where the magnetic properties of the reference layer vary with the temperature in a different way from those of the memory layer, the domains of desired magnetization orientations being set in the memory layer by utilizing the magnetic property of the reference layer resulting from the temperature change, comprising: (a) means for moving the magnetic recording medium relative to the laser pulse emission means; and (b) means for controlling the temperature of the reference layer selectively by alternating the durations of the laser pulses generated by the laser pulse emission means for heating the memory layer to a temperature near or above the Curie temperature, according to the binary data to be recorded in the memory layer, thereby changing the magnetic property of the reference layer in order to record the desired binary data in the memory layer.

Claims: Apparatus for magneto-optical recording, the apparatus comprising: a magnetic recording medium comprising a memory layer and a reference layer laminated onto the memory layer either directly or via an intermediate thermally conductive layer, the Curie temperature of the reference layer being greater than or equal to the Curie temperature of the memory layer; means to apply a bias magnetic field to the recording medium; means arranged to emit laser pulses incident on the memory layer side of the magnetic recording medium; and means to selectively control the temperature difference between the reference layer and the memory layer by causing laser pulses to be emitted of either a first or a second predetermined duration in accordance with binary data thereby to record the data in the memory layer, the first predetermined value of the duration of the laser pulses being short enough so that the heating of the memory layer is completed before the whole layer reaches thermal equilibrium such as to induce a temperature difference between the memory layer and the reference layer such that half or more of the memory layer is heated to a first temperature at least equal to the Curie temperature of the memory layer so that the magnetisation of the memory layer follows the magnetisation of the reference layer and half of the reference layer is heated to a second temperature less than the Curie temperature of the reference layer so that the magnetisation direction of the reference layer is not changed from an initial state by the bias magnetic field, the second predetermined value thereof being such as to heat half of the reference layer to a temperature at least equal to the Curie temperature of the reference layer so that the magnetisation direction of the reference layer is changed from an initial state by the bias magnetic field. Apparatus as claimed in claim 1 wherein the first predetermined value is of the order of 1 nanosecond and the second predetermined value is longer than a few tens of nanoseconds. Apparatus as claimed in claim 1 or claim 2 comprising means for moving the magnetic recording medium relative to the laser pulse emission means. Method for magneto-optical recording using a magnetic recording medium comprising a memory layer and a reference layer laminated onto the memory layer either directly or via an intermediate thermally conductive layer, the Curie temperature of the reference layer being greater than or equal to the Curie temperature of the memory layer, the method comprising: applying a bias magnetic field to the recording medium; generating laser pulses incident on the memory layer side of the magnetic recording medium; and selectively controlling the temperature difference between the reference layer and the memory layer by causing pulses to be emitted of either a first or a second predetermined duration in accordance with binary data thereby to record the data in the memory layer, the first predetermined value of the duration of the laser pulses being short enough so that the heating of the memory layer is completed before the whole layer reaches thermal equilibrium such as to induce a temperature difference between the memory layer and the reference layer such that half or more of the memory layer is heated to a first temperature at least equal to the Curie temperature of the memory layer so that the magnetisation of the memory layer follows the magnetisation of the reference layer and half of the reference layer is heated to a second temperature less than the Curie temperature of the reference layer so that the magnetisation direction of the reference layer is not changed from an initial state by the bias magnetic field, the second predetermined value thereof being such as to heat half of the reference layer to a temperature at least equal to the Curie temperature of the reference layer so that the magnetisation direction of the reference layer is changed from an initial state by the bias magnetic field. A magnetic recording medium for use in apparatus as claimed in claim 1 comprising a memory layer and a reference layer either laminated directly or via an intermediate thermally conductive layer onto the memory layer, wherein the Curie temperature of the memory layer is substantially equal to the Curie temperature of the reference layer.

Inventors: OHTSUKI TOMOKO, OHTSUKI, TOMOKO
Applicants: IBM, INTERNATIONAL BUSINESS MACHINES CORPORATION
Application year: 1990
Main classification: G11B11
IPC codes: G11B11