Magneto-optical recording apparatus having means for delaying an input signal for preventing bit shift

Abstract: An apparatus for recording an input signal on a magneto-optical recording medium comprises an optical head for applying a light beam to the medium, a circuit for delaying the input signal by a time for preventing a bit recorded on the medium from shifting relative to the input signal, a magnetic head for applying a magnetic field modulated in conformity with the delayed signal to that portion of the medium to which the light beam is applied, and a mortor for moving the medium relative to the light beam.

Description: BACKGROUND OF THE INVENTION Field of the Invention This invention relates to a magneto-optical recording apparatus for recording signals by applying a magnetic field modulated in conformity with a recording signal to a magneto-optical recording medium while applying a laser beam to the magneto-optical recording medium. Related Background Art In recent years, studies of an optical information recording apparatus as a memory of large capacity have been actively done. Particularly, magneto-optical recording has been drawing attention because of its capability of rewriting information. As a method of the magneto-optical recording, there is known a method of applying a magnetic field modulated in conformity with a recording signal to a magneto-optical recording medium while applying a light beam to the magneto-optical recording medium. This method is called the magnetic field modulation method, and has a feature that signals to be renewed can be overwritten without previously recorded signals being erased in advance. An example of a magneto-optical recording apparatus using the above-described method is schematically shown in Figure 1 of the accompanying drawings. In Figure 1, the reference numeral 1 designates a magneto-optical disk which is formed by attaching vertically magnetized film 3 to a glass substrate 2. This magneto-optical disk 1 is rotated about the center axis 0 - 0′. The reference numeral 4 denotes an optical head for applying a laser light to the vertically magnetized film 3 of the magneto-optical disk 1. This optical head 4 is comprised chiefly of a semiconductor laser 5 and a condensing lens 6. The optical head 4 is designed to act on the vertically magnetized film 3 so that the laser light may be focused thereon, and to be movable radially of the magneto-optical disk 1. The reference numeral 7 desingates an electromagnet disposed so as to be opposed to the optical head 4 relative to the magneto-optical disk 1 and applying a bias magnetic field to the vertically magnetized film 3. This electromagnet 7 is designed to move radially of the magneto-optical disk in operative association with the optical head 4. An electric current inverted in phase in conformity with a recording signal is supplied from a magnetic field modulation circuit 9 to the coil 8 of the electromagnet 7. The magnetic field modulation circuit 9 is operated by a recording signal input from a terminal 10. For example, when the recording signal changes as shown in (b₁) of Figure 2 of the accompanying drawings, the electromagnet 7 produces a magnetic field shown in (d₁) of Figure 2 in synchronism therewith. Here, when the recording signal is "1", a magnetic field of a predetermined intensity +H is produced in a direction with the direction of magnetization of the vertically magnetized film 3 as the upward direction. On the other hand, when the recording signal is "0", a magnetic field of a predetermined intensity -H is produced just in the opposite direction to that when the recording signal is "1". At this time, the optical head 4 continuously emits a laser light of a predetermined intensity as shown in (c₁) of Figure 2 when the recording condition is brought about, and the laser light locally illuminates the vertically magnetized film of the magneto-optical disk 1. Thus, the temperature of the vertically magnetized film in this irradiated portion rises to the curie point or higher. By the process as described above, a recording pattern as shown as a model in (e₁) of Figure 2 is formed on the vertically magnetized film. In this case, the white portions and the recording patterns indicated by hatching show the upwardly magnetized state and the downwardly magnetized state, respectively. In the above-described method, however, the spot of the light beam has a finite size, and this has led to a problem that the end portion of each bit of the recording pattern suffers from positional deviation relative to the recording signal, i.e., so-called bit shift, as shown in Figure 2. On the other hand, the shape of the recording bit becomes a chevron-like shape as shown in (e₁) of Figure 2 and therefore, there has been created a time difference t₂ between the center of the recording signal and the peak of a signal (f₁) reproduced from this recording pattern. This phenomenon will hereinafter be referred to as the peak shift. Due to this phenomenon, for example, the time t₁ to the peak of the reproduction signal (f₁) becomes shorter by (t₃ - t₂) relative to the time t₀ from a synchronizing signal reproduced from a prepit formed unevenly on the magneto-optical disk 1 to the center of "1" of the recording signal. Here, t₃ is the time difference by bit shift, and t₂ is the time difference by peak shift. EP-A-0322817, which constitutes prior art for the purpose of Art. 54(3) EPC for contracting states DE FR and GB, discloses a recording method for a magnetooptical disc and an apparatus for performing the method. In the method disclosed, the timing of the data recording is corrected for the delay time between the application of the recording magnetic field and the time at which the magnetic domain is formed in the recording medium. This is achieved by, during a test recording period recording a predetermined pattern for detecting time shifts. The difference between the time of application of the recording magnetic field and the time at which the magnetic domain is formed is detected using a reproducing light beam. The phase of the recording is then corrected so as to cancel the delay time. SUMMARY OF THE INVENTION It is the object of the present invention to solve the above-noted problems peculiar to the prior art and to provide a magnetooptical recording apparatus in which bit shift can be prevented. According to one aspect of the present invention there is provided a signal recording apparatus provided with means for applying a light beam to a magnetooptical recording medium, means for applying a magnetic field modulated according to a recording signal to that portion of the medium to which the light beam is applied, and means for moving the medium relative to the light beam, means for delaying said recording signal input to said magnetic field applying means by a time for preventing a bit recorded on the medium from shifting relative to said recording signal, said apparatus further comprising at least one of means for detecting the temperature of the medium and means for judging the relative line speed of the medium and the light beam, wherein said means for delaying is arranged to determine the delay time in conformity with at least one of the temperature detected by said temperature detecting means and the line speed judged by said speed judging means. According to a second aspect of the present invention there is provided a method for recording information on a medium by a magnetooptic effect in which a radiation beam illuminates a spot on the medium while a magnetic field applies a data signal to the spot; wherein the magnetic field signal is delayed relative to a synchronising signal to compensate for the non-zero size of the spot, at least one of the temperature of the medium and the relative line speed of the medium and the spot is detected, and the magnetic field signal is delayed relative to a synchronizing signal in conformity with the detection result. In addition to said delaying means, provision may be made of means for making the intensity of the magnetic field applied to the medium smaller in the rear portion of each pulse of a recording signal than in the other portion, whereby a recording bit can be prevented from assuming a chevron-like shape, thereby eliminating peak shift. BRIEF DESCRIPTION OF THE DRAWINGS Figure 1 is a schematic view showing an example of the magneto-optical recording apparatus according to the prior art. Figure 2 is a timing chart showing the states of the signals of various portions in the apparatus shown in Figure 1. Figure 3 is a schematic view showing a first embodiment of the magneto-optical recording apparatus of the present invention. Figure 4 is a timing chart showing the states of the signals of various portions in the apparatus shown in Figure 3. Figure 5 is a schematic view showing a second embodiemnt of the magneto-optical recording apparatus of the present invention. Figure 6 is a timing chart showing the states of the signals of various portions in the apparatus shown in Figure 5. Figures 7 and 8 are timing charts for illustrating variations in a recording pattern when the temperature of a medium changes. Figure 9 is a schematic diagram showing a third embodiment of the magneto-optical recording apparatus of the present invention. Figure 10 is a timing chart showing the states of the signals of various portions in the apparatus shown in Figure 9. Figure 11 is a schematic diagram showing a fourth embodiment of the magneto-optical recording apparatus of the present invention. Figure 12 is a schematic diagram showng a fifth embodiment of the magneto-optical recording apparatus of the present invention. DESCRIPTION OF THE PREFERRED EMBODIMENTS Figure 3 is a schematic view showing the construction of a first embodiment of the magneto-optical recording apparatus according to the present invention. In Figure 3, the reference numeral 11 designates a magneto-optical disk which is formed by attaching vertically magnetized film 13 to a glass substrate 12. A plurality of tracks are formed concentrically or spirally on the disk 11. This magneto-optical disk 11 is rotated about the center axis 0 - 0′ by a spindle motor, not shown. The reference numeral 14 denotes an optical head basically comprised of a semiconductor laser 15 and a lens 16. A laser light emitted from the semiconductor laser 15 is condensed by the lens 16 so as to be always focused on the vertically magnetized film 13. The optical head 14 is also movable radially of the magneto-optical disk 11. The reference numeral 17 designates a bias magnetic field producing head disposed in opposed relationship with the position at which the laser light is condensed by the optical head 14. The bias magnetic field producing head 17 comprises an electromagnet including a coil 18. The bias magnetic field producing head 17 is driven by a magnetic field modulation circuit 19. The reference numeral 20 denotes a delay circuit for delaying an information signal input from a terminal 21. The magnetic field modulation circuit 19 is driven in synchronism with the information signal delayed by the delay circuit 20. The amount of delay by the delay circuit 20 is a time corresponding to t₃ shown in Figure 2 which shows the prior art. The bias magnetic field producing head 17 is designed to move radially of the optical disk 11, following the optical head 14. Consider a case where in the above-described construction, as shown in Figure 4, a synchronizing signal (a₂) indicative of the beginning of an information recording area has been obtained from a prepit prerecorded on the magneto-optical disk 11. A recording signal (b₂) is input with this synchronizing signal a₂ as a reference. This recording signal (b₂) is input from the terminal 21 to the delay circuit 20, where it is delayed by the time t₃ and becomes a delay signal (c₂). Also, simultaneously with the synchronizing signal, a laser light is emitted from the optical head 14, and as indicated by (d₂), continues to be continuously applied onto the magneto-optical disk 11 with such a laser power Pw that will render the temperature of the vertically magnetized film 13 higher than the curie point. On the other hand, the magnetic field modulation circuit 19, in response to the delay signal (c₂), applies a magnetic field modulated with intensities of ±H shown in (e₂) from the bias magnetic field producing head 17 to the disk. In this manner, a pattern schematically shown in (f₂) is recorded on the vertically magnetized film 13. In Figure 4(f₂), the white portions and the hatching portions respectively represent that the vertically magnetized film is magnetized upwardly and downwardly. A signal reproduced from this recording pattern is such as shown in (g₂). Thus, the reproduction signal assumes a waveform which is not affected by the bit shift as shown in the example of the prior art. Figure 5 is a schematic view showing a second embodiment of the magneto-optical recording apparatus of the present invention. In Fgiure 5, members identical to those in Figure 3 are given identical reference numerals and need not be described in detail. The present embodiment differs from the aforedescribed embodiment in that a magnetic field waveform adjusting circuit 30 is provided between the delay circuit 20 and the magnetic field modulation circuit 19. In the present embodiment, this circuit 30 makes the magnetic field intensity in the rear end portion of the recording pulse smaller than that in the other portion. Thereby, the recording pattern is prevented from assuming a chevron-like shape, and in addition to the aforementioned bit shift, peak shift is eliminated. The recording process in the present embodiment will hereinafter be described with reference to Figure 6. When as shown in Figure 6, a synchronizing signal (a₃) is detected from the magneto-optical disk 11, a recording signal (b₃) is input with this synchronizing signal (a₃) as a reference. This recording signal (b₃) is delayed by t₃ indicated in Figure 2 by the delay circuit 20, and becomes a delay signal (c₃). On the basis of the delay signal (c₃), the magnetic field waveform adjusting circuit 30 produces a bias magnetic field of the intensity shown in (e₃) from the bias magnetic field producing head 17 through the magnetic field modulation circuit 19. This magnetic field is controlled so that its intensity may become smaller during the time corresponding to the rear portion of the bit in the pulse forming each bit than during the time corresponding to the other portion. On the other hand, a laser light of the intensity shown in (d₃) is continuously applied from the optical head 14 to the disk 11. Since the intensity of the laser light is thus constant, the width of a recorded bit depends on the intensity of the magnetic field applied. When the intensity of the magnetic field becomes weak in the rear end portion of the pulse, a bit is formed only in the higher temperature area of the temperature distribution on the vertically magnetized film 3. Accordingly, the pattern of the recorded bit becomes such as schematically shown in (f₃) and does not assume a chevron-like shape. Here, the white portions and the hatching portions respectively represent that the vertically magnetized film is magnetized upwardly and downwardly. Thus, a signal reproduced from such a recording pattern is free from bit shift and peak shift, as shown in (g₃). In the above-described embodiments, the temperature of the medium has been constant, but it is conceivable that if this temperature changes, it will affect the amount of bit shift. This will now be described with reference to Figures 7 and 8. Where data (a₄) is input when the magneto-optical disk is at a certain temperature, the changeover timing of the magnetic field (b₄) is delayed with respect to the input data. Thereupon, bit shift is compensated for, and a signal (f₄) reproduced from the recording pattern (e₄) is free from any time deviation with respect to the input data (a₄). However, when the temperature of the disk rises, the isothermal line on the magnetic film heated by a laser beam greatly widens as shown in (e₅) even if as shown in Figure 8, the laser beam is of the same laser power as what has been described above. Moreover, as compared with the case shown in Figure 7, the amount of bit shift increases. Accordingly, even if the rising timing of the magnetic field is delayed by td with respect to the input data (a₅), bit shift cannot be eliminated and thus, time deviation td′ remains between data (a₅) and the reproduction signal. Figure 9 is a schematic view showing a third embodiment of the present invention which takes the influence of the temperature of the medium upon bit shift into account. In Figure 9, the reference numeral 31 designates a magneto-optical disk which is a recording medium, the reference numeral 34 denotes a semiconductor laser unit, the reference numeral 33 designates a collimator lens for collimating a light beam emitted from the semiconductor laser, the reference numeral 32 denotes an objective lens for condensing the collimated light beam on the disk 31, and the reference numeral 35 designates a laser driver for driving the semiconductor laser unit 34. The reference numeral 36 denotes a thermistor for measuring the temperature of the surroundings of the recording medium, the reference numeral 37 designates a fixed resistor, the reference numeral 38 denotes an analog-digital (A/D) converter for converting the signal from the thermister 36 into a digital signal, the reference numeral 39 designates a magnetic field producing coil, the reference numeral 40 denotes a driver for the magnetic field producing coil 39, the reference numeral 41 designates a magnetic field modulation pulse generating circuit, and the reference numeral 42 denotes a terminal to which recording data is input. The operation of the present embodiment will now be described. The magneto-optical disk 31 is rotated at a predetermined number of rotations by a spindle motor, not shown. A certain set electric current flows from the laser driver 35 to the semiconductor laser unit 34, whereby a predetermined quantity of light is emitted therefrom. This emitted light passes through the collimator lens 33 and becomes a parallel light, and is condensed with a certain spot diameter on the disk by the objective lens 32. At this time, the thermistor 36 installed closely adjacent to the medium assumes a resistance value nearly correlated with the temperature of the medium. Accordingly, when the applied voltage to the thermistor is Vcc, a voltage value obtained by dividing Vcc by the resistance value of the thermistor and the fixed resistor 37 is input to the A/D converter 38. The output of the A/D converter 38 is input to the magnetic field modulation pulse generating circuit 41, where the amount of bit shift is calculated in accordance with the measured temperature and further, a delay time for compensating for this bit shift is calculated. Then, the circuit 41 delays the data input from the terminal 42 by the calculated time and sends it to the coil driver 40. In the coil driver 40, an electric current is caused to flow clockwisely or counter-clockwisely to the coil 39 in conformity with the data sent from the circuit 41, whereby the direction of the magnetic field is modulated. That is, in the present embodiment, the delay time of the input signal is lengthened or shortened in accordance with the rise or fall of the temperature of the medium. Thus, it is possible to compensate for the bit shift without being affected by a change in the temperature of the medium. Figure 10 schematically shows the manner of recording using the apparatus shown in Figure 9. Here, the delay time tp of the magnetic field (b₆) with respect to data (a₆) is that calculated in the aforedescribed magnetic field modulation pulse generating circuit 41 on the basis of the detected temperature of the medium. By the delay time being thus varied in conformity with the temperature of the medium, the reproduction signal (f₆) is made always free of time deviation relative to the data (a₆). In the above-described embodiment, the temperature of the environment near the medium has been detected as the temperature of the medium. However, the temperature of the medium may be directly measured as by bringing a thermistor into contact with the medium. The variation in the amount of bit shift as described with reference to Figures 7 and 8 is caused not only by a change in the temperature of the medium, but also by a change in the relative speed of the medium and the light beam. This is because any change in the speed varies the energy applied to the unit area of the medium per unit time. For example, where the magneto-optical disk is rotated at a predetermined angular speed, the line speed of the light beam relative to the medium becomes lower when the light beam is on the inner peripheral portion of the disk than when the light beam is on the outer peripheral portion of the disk. Thereupon, the isothermal line of the magnetic film widens as in the case of Figure 8 and the amount of bit shift increases. Accordingly, it is conceivable that if the delay time is set in accord with the outer peripheral portion of the disk, bit shift cannot be completely eliminated on the inner peripheral portion. A fourth embodiment of the present invention which takes the influence of the relative speed of the medium and the light beam as described above into account is shown in the schematic diagram of Figure 11. In Figure 11, members identical to those in Figure 9 are given identical reference numerals and need not be described in detal. In Figure 11, the reference numeral 44 designates a spindle motor for rotating the magneto-optical disk 31, the reference numeral 43 denotes an optical head carrying the semiconductor laser unit 34, etc. thereon, the reference numeral 46 designates a head feeding motor for moving the optical head 43 radially of the disk, and the reference numeral 45 denotes a motor control circuit for controlling the head feeding motor 46 and the spindle motor 44. The operation of the present embodiment will now be described. First, the spindle motor 44 revolves under the control of the motor control circuit 45, whereby the disk 31 is rotated at a predetermined number of rotations. Subsequently, the address of a desired track on which recording is to be effected is indicated from a host controller, not shown, to the motor control circuit 45. The motor control circuit 45 drives the head feeding motor 46 on the basis of this indication, thereby moving the optical head 43 to right beneath the desired track. The light emitted from the semiconductor laser unit 34 is condensed by the objective lens 32 and applied to this track. On the other hand, the address of the above-mentioned track is input from the motor control circuit to the magnetic field modulation pulse generating circuit 41. The circuit 41 finds from this address the line speed of the disk relative to the light beam, and a delay time for compensating for the amount of bit shift conforming to this line speed is calculated. The circuit 41 delays the data input from the terminal 42 by the calculated time, and sends a magnetic field modulation pulse based on this delayed data to the coil driver 40. The coil driver 40 drives the coil 39 by the pulse sent from the circuit 41, thereby applying a magnetic field modulated in polarity to the disk 31. By the delay time being thus varied in conformity with the movement line speed of the medium, bit shift can always be reliably prevented even when recording is effected on any track of a so-called constant angular velocity (CAV) type disk. In the above-described embodiment, the line speed has been calculated from the address of a desired track, but for example, by mounting an encoder on the optical head, the radial position may be directly detected and the delay time may be calculated by the use of the result of the detection. The variation in the amount of bit shift as previously described is caused also by the fluctuation of the power of the applied light beam. This will be apparent from the fact that the temperature distribution of the magnetic film is determined in conformity with the power of the light beam. So a magneto-optical recording apparatus in which bit shift is prevented with three factors, i.e., the intensity of the light beam, the temperature of the recording medium and the line speed of the recording medium, generally taken into account is shown in Figure 12. Figure 12 is a schematic diagram showing a fifth embodiment of the present invention. In Figure 12, members identical to those in Figures 9 and 11 are given identical reference numerals and need not be described in detail. In Figure 12, the reference numeral 47 designates a laser unit containing therein a semiconductor laser and a photodiode for receiving part of the emitted light of the laser, the reference numeral 48 denotes a current/voltage (I/V) converter for converting the output current of the photodiode into a voltage, and the reference numeral 49 designates a laser control circuit for controlling the laser driver 35 in accordance with the output of the converter 48. The laser control circuit 49 sets the reference value of the output power of the laser by a command from a centralized control circuit 50. The centralized control circuit 50 sends the address of a desired track to the motor control circuit 45, and moves the optical head 43 to right beneath a track on which recording is to be effected by the head feeding motor 46. Further, information regarding the temperature of the surroundings of the disk 31 is input to the centralized control circuit 50 through the analog-digital (A/D) converter 38. The operation of the present embodiment will now be described. The magneto-optical disk 31 is rotated at a predetermined number of rotations by the spindle motor 44. The optical head 43 is moved to right beneath a desired track in the same manner as in the fourth embodiment, on the basis of the address indicated from the centralized control circuit 50. A light of power PomW is emitted from the semiconductor laser in the laser unit 47, and is collimated through the collimator lens 33 and condensed on the disk by the objective lens 32. At this time, part of the laser light is received by the photodiode contained in the laser unit 47 and a photocurrent flows. The photocurrent is converted into a voltage by the current/voltage converter 48 and input to the laser control circuit 49. This laser control circuit 49 controls the supplied current to the laser in accordance with the input thereto, thereby performing APC (auto power control) operation. The reference power of APC is changed over by instructions from the centralized control circuit 50. The centralized control circuit 50 judges the line speed of the disk from the address of the track indicated to the motor control circuit 45, and judges the power of the light beam from the instructions to the laser control circuit 49. The centralized control circuit 50 then calculates the amount of bit shift on the basis of the line speed, the laser power and the information of the temperature of the disk input from the A/D converter 38, and calculates a delay time for compensating for this bit shift. The circuit 50 then sends this delay time to the magnetic field modulation pulse generating circuit 41. The circuit 41 delays the data input from the terminal 42 by the calculated time and sends it to the coil driver 40. In the coil driver 40, the current is caused to flow clockwise or counter-clockwise to the coil 39 in conformity with the data sent from the circuit 41 to thereby modulate the direction of the magnetic field. That is, in the present embodiment, the delay time is varied in conformity with the from-time-to-time situations (the laser power, the line speed and the temperature of the recording medium), whereby bit shift is reliably eliminated. While in the present embodiment, the power of the light beam has been judged from the instructions of the centralized control circuit 50, the power of the light beam may be directly measured, for example, by detecting the reflected light of the light beam from the disk. In the above-described embodiments, the delay time has been calculated with the temperature of the medium, etc. as parameters. The present invention permits various applications, besides the embodiments described above. For example, the medium need not always be heated to the curie point by the light beam, but may be heated to a temperature at which there is provided such a coercive force that the direction of magnetization is inverted depending on the magnetic field applied. The present invention is also applicable to the so-called compensation temperature writing method in which the medium is heated to its compensation temperature. In the present invention, the medium is not limited to the disk-like shape, but may be of any shape such as a card-like shape or a tape-like shape. The present invention covers all of the above-described applications without departing from the scope thereof defined in the appended claims.

Claims: A signal recording apparatus provided with means (14-16; 32-35; 43, 47, 48, 49; 52-54, 63) for applying a light beam to a magnetooptical recording medium (11; 31;51), means (17-19; 30; 39; 40; 58-60) for applying a magnetic field modulated according to a recording signal to that portion of the medium to which the light beam is applied, and means (44, 45; 64) for moving the medium (11; 31; 51) relative to the light beam, means (41) for delaying said recording signal input to said magnetic field applying means by a time for preventing a bit recorded on the medium (11; 31; 51) from shifting relative to said recording signal, said apparatus further comprising at least one of means (36-38) for detecting the temperature of the medium (11; 31; 51) and means (45,46) for judging the relative line speed of the medium (11;31;51) and the light beam, wherein said means for delaying (41) is arranged to determine the delay time in conformity with at least one of the temperature detected by said temperature detecting means (36-38) and the line speed judged by said speed judging means (45,46). An apparatus according to claim 1 further comprises means (50) for judging a power of the light beam applied to the medium (11;31;51), and wherein the delay time produced by said delaying means (41) is determined in conformity with the power judged by said power judging means (50). An apparatus according to claim 1, wherein said temperature detecting means (36-38) detects the temperature of the atmosphere near the medium (31). An apparatus according to claim 1, wherein said temperature detecting means comprises a thermister (36) disposed proximate to said medium (31). An apparatus according to claim 1, wherein said medium is a magnetooptical disk (31), said moving means (44) rotates said disk at a predetermined angular speed, and said speed judging means (45, 46, 50) judges the line speed by the disk radial position of that portion to which the light beam is applied. An apparatus according to claim 5, wherein a plurality of tracks are concentrically or spirally formed on said medium (31), and said light beam applying means comprises an optical head (43), and said apparatus further comprises a head feeding motor (46) for moving said optical head in the radial direction of said disk and a control circuit (50) for outputting a command to said head feeding motor (46) so as to move said optical head (43) to a position to which the light beam is applied to a desired track on said disk (31), and wherein said speed judging means (45,46,50) judges the line speed by the disk radial position of the desired track commanded by said control circuit (50). An apparatus according to claim 1, wherein said magnetic field applying means (17-19) alternately applies to said medium pulse-like magnetic fields having opposite polarities, and said apparatus further comprises means (30) for making the magnetic field intensity during a period corresponding to the rear end portion of said pulse-like magnetic fields smaller than the magnetic field intensity during the other period. An apparatus according to any one of claims 1 to 7, wherein said light beam applying means comprises an optical head (14; 43; 63) provided with a semiconductor laser (15; 34; 47) and lens (16; 32, 33; 52, 53). An apparatus according to any one of claims 1 to 8, wherein said magnetic field applying means comprises a magnetic head (17, 18; 39; 58, 59). An apparatus according to any one of claims 1 to 9, wherein said medium is a magnetooptical disk (31), and said moving means comprises a spindle motor (44; 64). A method for recording information on a medium (11; 31; 51) by a magnetooptic effect, in which a radiation beam illuminates a spot on the medium (11; 31; 51) while a magnetic field applies a data signal to the spot; wherein the magnetic field signal is delayed relative to a synchronising signal to compensate for the non-zero size of the spot, at least one of the temperature of the medium (11;31;51) and the relative line speed of the medium and the spot is detected, and the magnetic field signal is delayed relative to a synchronizing signal in conformity with the detection result. A method for recording information on a medium (11, 31, 51) by a magnetooptic effect, in which a radiation beam continuously illuminates a spot on the medium (11; 31; 51) while a magnetic field applies a data signal to the spot; and wherein the magnetic field is weakened towards the end of at least some data periods to compensate for the non-zero size of the spot. A method according to claim 12 in which the extent of the said weakening is varied in accordance with variations in one or more physical parameters of the circumstances of the recording. A method according to claim 11, wherein a power of the light beam applied to the medium (11; 31; 51) is detected, and the magnetic field signal is delayed relative to the synchronizing signal in conformity with variation of the detected power of the light beam.

Inventors: KIMURA SHUNPEI CANON DAINI FUJ, MIYAOKA YASUYUKI, OTOKAWA MITSUHIRO, KIMURA, SHUNPEI, CANON DAINI FUJIGAOKARYO, MIYAOKA, YASUYUKI, OTOKAWA, MITSUHIRO
Applicants: CANON KK, CANON KABUSHIKI KAISHA
Application year: 1990
Main classification: G11B11
IPC codes: G11B11