Abstract:
A frequency demodulating circuit, optical disk and preformatting device having a decoder for decoding a bit “0” and a bit “1” for reproducing address information recorded as a wobble groove. The decoder determines whether an output is a digital “1” or a digital “0” so that even if the waveform of the reproduced signal is erratic or unstable due to a defect, a digital “1” or a digital “0” can be correctly identified by utilizing window pulses. Changes in the slop of a zero cross point of the groove wobble are prevented from occurring by making the groove wobble amplitude fluctuate according to the signal frequency modulation which also greatly reduces jitter and allowing satisfactory acquisition of the address information. Oversampling clock signals of biphase bits are generated by frequency division of data clock signals. Since demodulation is accomplished with a single phase lock loop circuit in the data system using clock signals for both the data and the addresses, the configuration can be made extremely simple. By means of polarity of the playback signal mark having phase information, it is determined whether the beam that scans the optical disk is above the land or above the groove. The marks containing phase information are formed on the base disk surface solely by the on and off control of the paired cutting beams with respect to the direction of the time axis, for easy preformatting of a mark to permit acquiring (phase) position information with high precision.

Description:
This is a divisional of application Ser. No. 09/074,814, filed May 8, 1998, which is a continuation-in-part of application Ser. No. 09/009,595, filed Jan. 20, 1998 now abandoned. 
    
    
     BACKGROUND OF THE INVENTION 
     1. Field of the Invention 
     The present invention relates to a frequency demodulating circuit, optical disk apparatus and preformatting device. 
     2. Description of Related Art 
     In the conventional art, an optical disk has been proposed in which frequency modulation of biphase modulated address information ADM is performed and grooves are recorded in a wobbling state corresponding to the post-modulated signal. This groove wobble as shown in FIG. 40 may for instance, when the digital data is “1” per one bit (biphase 1 bit) of the address information ADM, become 4.25 waves (period of 4.25 on the sine wave), whereas when the digital data is “0” per a biphase 1 bit of the address information ADM, the groove wobble becomes 3.75 waves (period of 3.75 on the sine wave). In this case, the groove wobble is a fixed amount regardless of the frequencies of the post-modulated signals. 
     FIG. 41 is a block diagram showing a sample layout of a frequency demodulating circuit  100  of the conventional art used to acquire address information ADM from a groove wobble reproduction signal, in other words a wobble signal S WB . This frequency demodulating circuit  100  contains a capacitor  101  for blocking the DC component, and a comparator  102  for converting the wobble signal S WB  into the binary signal P WB  whose DC component has been removed by setting a threshold value of zero. 
     Also, the frequency demodulating circuit  100  includes a voltage-controlled oscillator  103   a , a phase comparator  103   b , and also a low-pass filter  103   c , which constitute a PLL (phase-locked loop) circuit  103 . The phase comparator  103   b  compares the phases of the output signal of this voltage-controlled oscillator  103   a  and the pulse signal P WB  output from the comparator  102 . The low-pass filter  103   c  derives the low frequency component of the phase error signal output from this phase comparator  103   b  in order to obtain a control signal which is supplied to the voltage controlled oscillator  103   a.    
     This frequency demodulating circuit  100  also contains another low-pass filter  104  for deriving the low frequency component of an output signal from the low-pass filter  103   c ; another capacitor  105  for removing the DC component; and another comparator  106  to acquire the address information ADM from the output signal of the low-pass filter  104 , whose DC component is removed while setting a threshold value of zero. 
     Also, the frequency demodulating circuit  100  contains an edge detector  107  for detecting a rising edge and falling edge of the address information ADM output from the comparator  106 ; and a monostable multivibrator  108  capable of obtaining a pulse signal of a predetermined width while using an edge detection signal output from his edge detector  107 . 
     The frequency demodulating circuit  100  further includes another voltage-controlled oscillator  109   a , another phase comparator  109   b , and another low-pass filter  109   c , which constitutes another PLL circuit  109 . The phase comparator  109   b  executes a phase comparison between the output signal of this voltage-controlled oscillator  109   a  and the pulse signal output from the monostable multivibrator  108 . The low-pass filter  109   c  derives a low frequency component from a phase error signal output from this phase comparator  109   b  in order to produce a control signal which is supplied to the voltage-controlled oscillator  109   a.    
     The operation of the frequency demodulating circuit  100  shown in FIG. 41 will next be described. The wobble signal S WB  is supplied via the capacitor  101  to the comparator  102  in order to be converted into a binary signal P WB . As previously described, the address information ADM which has been biphase-modulated is frequency-modulated, and this frequency-modulated signal is recorded as a groove wobble on the optical disk. As a result, as shown in FIG. 42A, the wobble signal S WB  has 4.25 waves when the digital data is “1”, and has 3.75 waves when the digital data is “0” in correspondence with the 1 bit (biphase 1 bit) of the address information ADM similar to the frequency-modulated signal. Such a binary signal PW B  as shown in FIG. 42B is therefore output from the comparator  102 . 
     On the other hand, since the frequency of the wobble signal S WB  corresponding to “1” is different from the frequency of the wobble signal S WB  corresponding to “0”, the output signal of the low-pass filter  103   c  which constitutes the PLL circuit  103  is shown in FIG.  42 C. As a result, the address information ADM is produced from the low-pass filter  106 , as indicated in FIG.  42 D. The edge of this address information ADM is then detected by the edge detector  107 . The edge detection signal is supplied as a trigger signal to the PLL circuit  109  and the pulse signal output from the monostable multivibrator  108  is supplied as a reference signal to this PLL circuit  109 . As a result, a clock signal “ACK” which is synchronized with the address information is acquired from the voltage-controlled oscillator  109   a  to constitute the PLL circuit  109  as shown in FIG.  42 E. 
     As previously described, the frequency demodulating circuit  100  shown in FIG. 41 has two signal systems of the PLL circuits  103  and  109  which constitute an overly complex circuit configuration. 
     As explained previously, the amplitude of the wobble groove recorded on the optical disk is a fixed amount regardless of the frequency of the signal after modulation so that as shown in the enlarged view in FIG. 40, a change in the slope (or deflection) occurs at the zero crosspoint of the groove wobble corresponding to the junction of the “1” and the “0” of the address information ADM. Consequently, large jitter is prone to occur on the time axis of the wobble signal S WB  that matches the junction point of the “1” and the “0” of the address information ADM. This jitter prevents the demodulation circuit from acquiring error-free address information ADM. 
     The assignee of this invention and others are currently in the midst of developing the next generation of optical magnetic disks (ASMO) and are proposing an magneto-optical disk in which clock marks hold address information by means of the groove wobbles and preformatting is performed. In this previously undisclosed magneto-optical disk apparatus, a data clock signal is acquired in order to record and reproduce data by utilizing the reproduction signal of this clock mark. 
     A reproduction signal S CM  of the clock marks is shown in FIG.  43 A. This reproduction signal S CM  functions as shown in FIG. 43B to form a P CM  signal showing the timing of the zero (0) crosspoint. A data clock signal is acquired by means of the PLL circuit while referring to this pulse P CM  signal. 
     The above mentioned clock mark CM is formed as shown in FIGS. 44A and 44B while using a pair of cutting beams to cut-formed the surface of the base disk. Writing is performed radially across the surface of the disk base with a lands  12 L and a grooves  12   b  being alternately formed. The groove  12 G is cut to a specified depth Da as shown in the cross sectional view in FIG. 44B by using the cutting beams. Excluding the beams Ba, Bb, FIG. 44 shows a lateral reduction of one-tenth when the vertical direction is set as 1, just the same as in FIG. 45 related later. 
     The flat surface is one side of the cutting edge  11   a  in the groove  12 G and the other cutting edge  11   b  is wobbled. The address information (shown by sine wave) ADM and the clockmark CM (one cycle of sine wave ) are consecutively formed in this address information ADM (shown by sine wave). 
     One pair of cutting beams Ba, Bb is used as shown in FIG. 44A as the cutting beams for performing wobble cutting. The cutting beams Ba, Bb scan the surface of the base disk in a partially overlapping state as shown in the figure. In this example, a groove wobble is formed by means of the cutting beam Ba. 
     When reproducing the clock mark CM formed in the groove  12 G in the groove wobble by means of the P PB  beam shown in FIG. 45, both the reproduction signal S CM  of the clock mark CM acquired during scanning of the land  12 L and the reproduction signal S CM  of the clock mark CM acquired during scanning of the groove  12 G form signals of identical polarity as shown in FIG.  43 A. 
     Accordingly, whether the beam P PB  is scanning above the land  12 L or scanning above the groove  12 G cannot currently be determined by means of this reproduction signal S CM . However, if it can be determined from the polarity of the reproduction signal S CM , whether the beam P PB  is currently scanning above the land  12 L or scanning above the groove  12 G, and servo control of the optical pickup system can then be accurately performed. 
     Further, as related above, the amplitude Wa (FIG. 44A, of the clock mark formed in the groove  12 G by means of the wobble groove, is extremely small. The clock mark CM for the reproduction signal S CM  shown in FIG. 43A has a poor signal to noise ratio. Accordingly, the clock signal acquired by using this reproduction signal S CM  has a large jitter and for instance cannot be used as a clock signal for data reproduction. Further, control of the first cutting beam Ba is difficult since the clock signal must be formed accompanied by drastic level fluctuations of the zero cross point, the smaller the amplitude Wa. 
     SUMMARY OF THE INVENTION 
     It is therefore an object of this invention to provide an optical disk apparatus in which one signal system of these PLL circuits is reduced to a simple configuration for performing demodulation. 
     It is therefore another object of this invention to provide an optical disk apparatus in which jitter is reduced at the time axis of the wobble signal S WB  that matches the junction point of the “1” and the “0” of the address information ADM and thus allow satisfactory acquisition of address information. 
     It is still another object of this invention to provide a preformatting device that can easily preformat marks having highly precise position (phase) information. 
     It is a further object of this invention to provide an optical disk apparatus that easily identifies whether the beam is above the groove or above the land by utilizing a polarized reproduction signal of a mark having phase information to determine whether the beam scanning the optical disk is above the land or above the groove. 
     In the optical disk apparatus of one aspect of this invention for driving an optical disk on which a groove wobble corresponding to a signal acquired from frequency modulated, biphase modulated address information, and a mark for expressing phase information placed inside said wobble are preformatted; and along with making the biphase bit count “a” (“a” is a natural number) between two of adjacent said marks, the channel bit count is made “n” (“n” is a natural number) between two of said adjacent marks wherein, said optical disk has first clock signal reproduction means to generate a first clock signal utilizing an “n” frequency multiple of the reproduction signal of said clock mark and, wobble signal reproduction means to reproduce from said optical disk a wobble signal corresponding to said groove wobble and, frequency demodulation means to acquire said address information by frequency demodulation of said wobble signal and, said frequency demodulation means has; a second clock signal generator to generate a second clock signal by dividing a data clock signal supplied from said first clock signal reproduction means by 1/M(M=n/(a·s)) in which a clock “s” (“s” is a natural number) is an oversampling value of said biphase bit and a waveform shaping unit to shape the waveform of said wobble signal and a detector to acquire said address information by processing with said second clock signal for said binary signal. 
     In this invention therefore, a biphase bit oversampling clock signal is generated by frequency division from a data clock signal which is an integer ratio of data clock signal and frequency of the biphase bit oversampling clock signal. Utilizing this clock signal allows acquisition of address information by frequency demodulation of the wobble signal obtained with the wobble signal reproduction means. 
     A optical disk apparatus of another aspect of this invention for driving an optical disk formed with alternate grooves and lands radially across the disk surface containing recording tracks; and marks preformatted with phase information wherein; marks having said phase information are formed on one end of said land or said groove and have a first concavity or protrusion at parallel falling sides in said radial direction and, a said land or said groove formed on the other side, parallel in the radial direction and constituting a second concavity or protrusion in the track rising direction also matching the falling direction, and whether the laser beam scanning said optical disk is above said land or above said groove can be detected from the polarity of the reproduction signal on the mark. 
     In a further aspect of this invention, in the lands and grooves, the concavities and protrusions comprising the marks containing the phase information, protrude in opposite directions. Consequently, the polarity of the mark reproduction signal will have a respectively different polarity according to whether the beam is scanning a land or a groove. This means that whether the beam is over a groove or a land can easily be determined by means of the polarity of the mark reproduction signal. 
     A preformatting device in yet another aspect of this invention is provided for cut-forming the surface of the base disk to form grooves and marks containing phase information on said base disk wherein said preformatting device comprises: a light source for generating a first and a second cutting beam, optical means for joining said first and second cutting beams to mutually overlap so that said first and second cutting beams overlap to irradiate a portion of the surface of the base disk, cutting beam control means for controlling on and off switching of said first and second cutting beams and, control means for controlling operation of said cutting beam control means. The control means is regulated such that said first cutting beam is turned off only for a fixed period immediately before the timing of said mark to be formed, and said second cutting beam is turned off only for a fixed period immediately after the timing of said mark to be formed. 
     In a yet further aspect of this invention, a first and a second cutting beam overlap and the junction of their light beams irradiates the surface of the base disk and cut-forms a groove in that surface. The first cutting beam is turned off for a fixed period immediately before the timing of said mark to be formed, and at one side of the groove, a protrusion is formed in parallel in the falling section towards the track where the mark is to be formed in the radial direction of the disk. The second cutting beam turns off for a fixed interval immediately after the timing of the mark to be formed. Accordingly, a protrusion is formed on the other side of the groove in parallel in the rising section towards the track where the mark is to be formed in the radial direction of the disk. The pairs of protrusions formed in these grooves are marks having phase information. 
     In the optical disk preformatted with the marks having the phase information as described above, when a mark is scanned by a beam, a signal having a one cycle sine wave is acquired. As related above, since the mark is formed by controlling the on and off switching of the cutting beam, the mark reproduction signal undergoes a sudden level change at the zero crosspoint. Consequently, the zero crosspoint can accurately be detected with no effect from jitter, even if the amount of protrusion from the pair of protrusions comprising the marks is small. 
     In a still further aspect of this invention, a frequency demodulator circuit has a waveform shaping section for forming a frequency modulated signal expressing the digital data to acquire a binary signal, clock signal generating unit for generating clock signals having a frequency corresponding to “1” of said address information, and also having a frequency higher than said frequency signal by a common multiple, which corresponds to “0” of said digital area; and a detector for acquiring said digital data based on clock signals corresponding to said binary information. 
     The optical disk apparatus of this invention further drives an optical disk on which a groove wobble corresponding to a signal acquired from frequency modulated address information, and a post-modulated signal are recorded; wobble signal reproduction means for reproducing from said optical disk a wobble signal corresponding to said groove wobble and, frequency demodulation means for acquiring said address information by frequency demodulation of said wobble signal and said frequency demodulation means has :a waveform shaping unit for acquiring a binary signal from a wave shaped from the wobble signal, a wobble signal frequency corresponding to said address information of “1”, clock signal generator means for acquiring a clock signal having a frequency multiple of said wobble signal corresponding to said address information of “0”, a detector for acquiring said address information by processing said binary signal with said clock signal. 
     In this aspect of the invention, the digital data, for instance the frequency modulated signal containing address information is shaped by a waveform shaping unit and converted into a binary signal. Then a clock signal generator, for instance a PLL circuit is used to obtain a clock signal which is a common multiple (for instance the lowest common multiple frequency) higher than the frequency modulated signal corresponding respectively to the digital data “1” and “0”. 
     Based on this clock signal, the binary signal corresponding to “1” has a pattern of “1” and “0” comprised of the first clock portion; and the binary signal corresponding to “0” has a pattern of “1” and “0” comprised of the second clock portion. In the detector, a binary signal pattern using this clock signal is detected and demodulation of the digital data then performed. 
     In an optical disk apparatus of a further aspect of this invention in which the address information is frequency modulated and the post-modulation signal is recorded on an optical disk as a groove wobble. This groove wobble amplitude is made to change according to the frequency of the signal after modulation. This change in groove wobble amplitude prevents a deflection near the groove wobble zero crosspoint corresponding to the junction point of the waveform expressing “0” and the waveform expressing “1” of the address information. 
     In this invention, the groove wobble amplitude is made to change according to the frequency of the signal after modulation, and a fixed amount of deflection is applied to the groove wobble zero crosspoint corresponding to the junction point of the waveform expressing “0” and “1” of the address information. This process reduces jitter along the time axis of the wobble signal S WB  corresponding to the junction of the “0” and “1” of the address information. 
    
    
     BRIEF DESCRIPTION OF THE DRAWINGS 
     FIG. 1 is a block diagram showing the magneto-optical disk apparatus of the first embodiment of this invention. 
     FIG. 2 is a flat view showing the sector layout of the magneto-optical disk. 
     FIGS. 3A through 3D are timing charts illustrating the sector (wobble address frame) format. 
     FIG. 4 is a drawing showing one sector (wobble address frame) of the address information prior to biphase modulation. 
     FIG. 5 is a drawing showing a sample layout of the groove wobble. 
     FIG. 6 is a perspective view showing the optical system of the optical head. 
     FIG. 7 is a view showing the structure of the photodetector for the optical system of the optical head and the spots formed above the photodetector. 
     FIG. 8 is a view illustrating the structure of the Wollaston prism constituting the optical system of the optical head. 
     FIG. 9 is a view showing isolation of light rays by the Wollaston prism. 
     FIG. 10 is a block diagram showing the layout of the ADIP decoder. 
     FIGS. 11A through 11F are timing flowcharts illustrating the operation of the ADIP decoder. 
     FIG. 12 is a block diagram snowing the layout of the detector. 
     FIG. 13 is a block diagram showing the layout of the edge detector circuit. 
     FIGS.  14 A through  14 F′ are waveforms illustrating the operation of the detector. 
     FIGS.  15  through  15 F′ are waveforms illustrating the operation of the detector. 
     FIGS.  16 A through  16 F′ are waveforms illustrating the operation of the detector. 
     FIGS.  17 A through  17 F′ are waveforms illustrating the operation of the ejector. 
     FIGS.  18 A through  18 G′ are waveforms illustrating the operation of the detector. 
     FIG. 19 is a block diagram showing the structure of another embodiment of the detector. 
     FIG. 20 is a block diagram showing the rising edge of the detector. 
     FIG. 21 is a block diagram showing the falling edge of the detector. 
     FIGS.  22 A through  22 I′ are waveforms illustrating the operation of the detector. 
     FIG. 23 is a block diagram showing the structure of another embodiment of the ADIP decoder. 
     FIGS. 24A through 24C are timing flowcharts describing the clock used by ADIP decoder. 
     FIG. 25 is a block diagram showing the structure of the data clock reproducing device. 
     FIGS. 26A through 26E are timing charts describing the operation of the data clock reproducing device. 
     FIG. 27 is a block diagram showing the structure of the magneto-optical disk apparatus of the second embodiment of this invention. 
     FIG. 28 is a block diagram showing the structure of the preformatting device. 
     FIGS. 29A through 29C are waveforms illustrating the on and off switching for the cutting beam and the clock mark signal. 
     FIG. 30 is a concept view of the on and off switching of the cutting beam. 
     FIGS. 31A through 31G show the interrelation of the clock marks and theirs reproduction signals. 
     FIG. 32 is a block diagram showing the structure of the polarity discriminator. 
     FIGS. 33A and 33B are concept views showing the on/off switching of the cutting beam and the wobble (fixed shift). 
     FIG. 34 is a concept view showing the on/off switching of the cutting beam and the wobble (fixed shift). 
     FIGS. 35A through 35D are timing charts illustrating the laser beam modulation by the data clock signal. 
     FIG. 36 is a block diagram showing the structure of the magneto-optical disk apparatus of the third embodiment of this invention. 
     FIGS. 37A through 37D are timing charts illustrating the laser beam modulation by the data clock signal. 
     FIG. 38 is a block diagram showing the structure of the magneto-optical disk apparatus of the fourth embodiment of this invention. 
     FIGS. 39A through 39D are timing charts illustrating the laser beam modulation by the data clock signal. 
     FIG. 40 is a drawing showing a sample structure of a wobble groove of the conventional art. 
     FIG. 41 is a block diagram showing the structure of the frequency demodulation circuit of the conventional art. 
     FIGS. 42A through 42E are timing charts illustrating the operation of the frequency demodulation circuit. 
     FIGS. 43A through 43D are drawings showing the clock mark reproduction signal for the magneto-optical disk apparatus relating to the present invention. 
     FIGS. 44A and 44B are drawings showing the interrelation of the cutting beam and clock mark. 
     FIG. 45 is a drawing showing the clock mark on the land and groove. 
    
    
     DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENTS 
     Hereafter the first embodiment of this invention will be described while referring to the accompanying drawings. The structure of a magneto-optical disk apparatus  10  of the first embodiment of this invention is shown in FIG.  1 . 
     A magneto-optical disk  11  accommodated in the magneto-optical disk apparatus  10  will first be described. FIG. 11 shows the layout of a sector of the magneto-optical disk  11 . A track “0” to a track “n” are formed on this magneto-optical disk  11  in a spiral form from an inner circumferential side thereof to an outer circumferential side thereof. Further, the magneto-optical disk  11  is divided up into zones, with the “0” to “m 1 ” sectors contained circumferentially in the tracks of zone X 1  on the inner circumferential side; while the “0” to “mn (m2&gt;m1)” sectors are contained in the tracks of zone X 2  on the outer circumferential side. 
     The format of a sector (wobble address frame) is shown in A-O of FIG.  3 . As shown in FIG. 3A, groove portions  12 G and land portions  12 L are alternately formed radially on the magneto-optical disk  11 , and data is recorded on any one of the groove portions  12 G and land portions  12 L, or both of these portions  12 G and  12 L. One side of a groove portion  12 G is brought for instance, into a wobbling state in response to biphase-modulated address information ADM. 
     In this case, the address information ADM is frequency-modulated (namely, FM), and the groove portions  12 G are wobbled to correspond to the FM modulated signal. In other words, this FM modulated signal is recorded as a groove wobble. It should be understood that since one side of the groove portion  12 G is wobbled, consequently one side of the land portion  12 L is brought into a wobbling state in response to the address information ADM. 
     This address information ADM has already been subjected to biphase modulation. Performing biphase modulation on the address information to acquire and use address information ADM is known as a method to prevent the generation of the DC components (DC free). The “1” bit of the address information prior to biphase modulation corresponds to a biphase “2” bit. 
     As shown in FIG. 5, a groove wobble becomes 4 waves per 1 bit of the address information ADM (biphase 1 bit) when the digital data is “1”, whereas a groove wobble becomes 3 waves per 1 bit of the address information ADM (biphase 1 bit) when the digital data is “0”. Moreover, the amplitude of this groove wobble is varied in response to the frequencies of modulated signals. Also, as shown in an enlarged view in FIG. 5, the slope of the groove wobble at the zero cross point which corresponds to the junction between “1” of the address information ADM and “0” of this address information is not allowed to change. 
     Here, a groove wobble within a 1-sector (1 wobble address frame) period contains the data prior to biphase modulation, for example, 42 bit data. This 42 bit data is made up of a 4 bit sync (synchronization) signal data, 24 bit frame address data, a 6 bit reserve bit, and a 14 bit CRC (cyclic redundancy check) code, as indicated in FIG.  4 . 
     Further, as shown in FIG. 3B, when a 1 sector is comprised for instance of 24 segments. A clock mark CM as shown in FIG. 3A is preformatted to be multiplexed with the groove wobble at a boundary position of each of the segments. Then, as shown in FIG. 3C, a 60 byte data region is formed in each of these segments and further, a 6 byte fixed pattern region is formed therein to correspond to the boundary position of the respective segments. As will be discussed later, when writing data, NRZI data is written into the data region, whereas a 2T-fixed pattern signal synchronized with the NRZI data is recorded on the fixed pattern region (symbol “T” is a bit interval of data). 
     Here, 1 sector on the magneto-optical disk  11  is comprised of 42 segments, and a clock markCM is preformatted at the boundary position of each segment so that the high speed bit count “a” between adjacent clock marks becomes 2 bits. Also on this magneto-optical disk  11 , along with a 60 bit data zone being formed within each segment, a 6 bit fixed pattern region is formed which corresponds to the boundary position of each segment so that the channel bit count “n” between the adjacent clock marks becomes 528 bits. 
     The magneto-optical disk apparatus  10  shown in FIG. 10 will now be described. This disk apparatus  10  contains a spindle motor  13  for rotating the magneto-optical disk  11 . The magneto-optical disk  11  is rotary-driven at a constant angular velocity during the recording operation and the reproducing operation. A frequency generator  14  for detecting the rotation speed of the spindle motor  13  is mounted on a rotary shaft of the spindle motor  13 . 
     The disk apparatus  10  further contains a magnetic head  15  for generating an external magnetic field; a magnetic head driver  16  for controlling the generation of the magnetic field by this magnetic head  15 ; an optical head  17  constituted by a semiconductor laser, an objective lens, a photodetector and the like; and a laser driver  18  for controlling light emission of the semiconductor laser by this optical head  17 . Both the magnetic head  15  and the optical head  17  are arranged opposite to each other in such a manner that the magneto-optical disk  11  is sandwiched between the magnetic head  15  and the optical head  17 . A laser power control signal S PC  is supplied from a servo controller (will discussed later) via a D/A converter  19  to the laser driver  18 , so that the power of the laser light emitted from the semiconductor laser of the optical head  17  can reach a record power P W  during recording operation. During reproducing, the power P W  is regulated to become reproduction power P R.    
     While data is written (during recording ), as explained later, both the recording data Dr and a fixed pattern signal S FP  are supplied to the magnetic head driver  16 , so that magnetic fields corresponding to the recording data Dr and the fixed pattern signal S FP  are generated from the magnetic head  15 . The recording data Dr is then recorded in the data region of the magneto-optical disk  11 , and also a fixed pattern signal S FP  is recorded in the fixed pattern region corresponding to the data region into which the recording data Dr is recorded by the magnetic field in conjunction with the laser beam emitted from the optical head  17 . 
     FIG. 6 schematically illustrates a structure of the optical system of the optical head  17 . The optical head  17  contains a semiconductor laser  31 , a collimator lens  32 , a beam splitter  33 , a raising mirror  34 , and an objective lens  35 . The semiconductor laser  31  is employed so as to produce a laser beam LB. The collimator lens  32  is employed to collimate divergent light of the laser beam LB emitted from this semiconductor laser  31  to produce parallel light. The beam splitter  33  is employed to split the laser beam LB into two sets of laser light beams, namely transmission light and reflection light. The reflecting mirror  34  is used to change the optical path of the laser beam LB. The objective lens  35  is then employed to irradiate the laser beam LB onto a recording surface (recording film) of the magneto-optical disk  11 . 
     This optical head  17  further contains a Wollaston prism (polarization plane detecting prism)  36 , a condenser lens  37 , a photodetector  39 , and a multi-lens  38 . The Wollaston prism  36  is employed to isolate the laser beam which is reflected from a reflection plane  33   b  of the beam splitter  33  and then is projected outside this beam splitter  33  as three sorts of laser beams, depending upon differences in polarization directions. The condenser lens  37  is employed to condense the three sorts of laser beams (parallel light) output from this Wollaston prism  36 . The three sorts of laser beams projected from this condenser lens  37  are then irradiated onto the photodetector  39 . The multi-lens  38  is positioned between the condenser lens  37  and the photodetector  39 . 
     The multi-lens  38  is comprised of a combination of a convex lens and cylindrical lens. The reason for using this cylindrical lens is that, a focus error signal can be obtained by way of the well-known astigmatism method. As indicated in FIG. 7, the photodetector  39  is arranged by a 4-split photodiode  39   m , and two sets of photodiodes  39   i ,  39   j.    
     A sample structure of the Wollaston prism  36  is shown in FIG.  8 . This prism  36  is comprised of rectangular prisms  36   a  and  36   b  made of a single-axial crystal, such as quartz. In this case, an optical axis Axb of the prism  36   b  is set to be inclined 45 degrees with respect to an optical axis Axa of the prism  36   a.    
     In this kind of optical arrangement, the quartz has two different refractive indexes for the polarization planes of incident light. As a result, when the linear polarization light “La” having a polarization plane Ppo inclined by 45 degrees with respect to the optical axis Axa of the prism  36   a , is input into this prism  36   a , this linear polarization light La is separated into a polarization component Lb 1  and another polarization component Lb 2 , as shown in FIG. 9 in this prism  36   a . The polarization plane perpendicular to the optical axis Axa, and the polarization component Lb 2  have this polarization component Lb 2  parallel to the optical axis Axa. Furthermore, in another prism  36   b , the polarization component Lb 1  is separated into a polarization component Lc 1  having such a polarization plane parallel to the optical axis Axb and another polarization component Lc 2  having such a polarization plane perpendicular to the optical axis Axb. Moreover, the polarization component Lb 2  is separated into a polarization component Lc 3  having such a polarization plane parallel to the optical axis Axb and another polarization component Lc 4  having such a polarization plane perpendicular to the optical axis Axb. 
     Here, it should be understood that the polarization components Lc 1  and Lc 2  have polarization planes perpendicular to the optical axis Axa of the prism  36   a , and the respective light amounts are equal to one-fourth the amount of light from the linear polarization light La. On the other hand, the polarization components Lc 3  and Lc 4  have polarization planes parallel to the optical axis Axa of the prism  36   a , and the respective light amounts thereof are equal to one-fourth the amount of light from the linear polarization light La. The light projection angle of the polarization component Lc 2  from the prism  36   b  is equal to the polarization component Lc 3  from this prism  36   b . As a result, three sets of laser beams Li, Lm, Lj are separately acquired from the Wollaston prism  36 . 
     The operation of the optical head  17  shown in FIG. 14 will now be described. The laser beam LB which is projected from the semiconductor laser  31  as divergent light is collimated by the collimator lens  32  to form the parallel laser light which is then input to the beam splitter  33 . The light path of the laser beam which has passed through the multilayer film  33   a  of the beams splitter  33  is changed to a right angle by the reflecting mirror  34 , and then the resulting laser beam is then irradiated onto the recording plane of the magneto-optical disk  11  via the objective lens  35 . 
     The laser beam reflected onto the recording plane of the magneto-optical disk  11  is input via the objective lens  35  and the mirror  34  into the beam splitter  33 . The laser beam Lr reflected onto the multilayer film  33   a  of the beam splitter  33  is further reflected on the reflection plane  33   b  of the beam splitter  33  and is then projected outside this beam splitter  33 . This projected laser light is input into the Wollaston prism  36 . 
     The laser beam Lr related to the reflection from the recording surface of the magneto-optical disk  11  is thus input into the Wollaston prism  36 . Although not described in the foregoing descriptions, such a polarization plane when there is no rotation (Kerr rotation) of the polarization plane on the recording surface of the magneto-optical disk  11  is set to be inclined by 45 degrees with respect ro the optical axis Axa (refer to a relationship between the polarization plane Ppo of linear polarization light La and optical axis Axa). As a result, the three sets of laser beams Li, Lm, Lj can be separately obtained from the laser beam Lr by way of the Wollaston prism  36  in a similar manner to the above-explained case in which the linear polarization light La was input. 
     In this case, the polarization plane of the laser beam Lr is slightly rotated along either the clockwise direction or the counterclockwise direction in accordance with the magnetizing direction of the recording film of the magneto-optical disk  11 , so that a size amount relationship is established for the light amounts of the laser beams Li and Lj in accordance with the magnetizing directions of the recording film of the magneto-optical disk  11 . As a consequence, light amounts of the laser beams Li and Lj are detected and then are subtracted from each other, so that a reproduction signal corresponding to the data (signal) recorded by the magneto-optical manner can be acquired. It should be noted that even when the polarization plane of the laser beam Lr is rotated, the light amount of the laser beam Lm is fixed. 
     As explained previously, the three sets of laser beams Li, Lm, Lj projected from the Wollaston prism  36  are input via the condenser lens  37  and the multi-lens  38  into the photodetector  39 . As shown In FIG. 7, the spots SPi, SPm, SPj are formed by the respective laser beams Li, Lm, Lj on the photodiodes  39   i ,  39   m ,  39   j  which constitute the photodetector  39 . 
     In this case, assuming now that detection signals of the four photodiodes Da to Dd which constitute the 4-split photodiode  39   m  are “Sa” to “Sd” respectively, and also detection signals of the photodiodes Di, Dj which constitute the photodiodes  39   i ,  39   j  are “Si”, “Sj”, the below-mentioned calculation is performed in an amplifier circuit unit (not shown) of the optical head  17 , so that a reproduction signal S MO , an astigmatism type focus error signal S FE , and a push-pull signal S PP  are produced from the recording region: 
     
       
         S MO =Si−Sj 
       
     
     
       
         S FE =(Sa+Sc)−(Sb+Sd) 
       
     
     
       
         S PP =(Sa+Sb)−(Sc+Sd) 
       
     
     Now referring back to FIG. 1, the magneto-optical disk apparatus  10  contains a servo controller  41  equipped with a CPU (central processing unit). The focus error signal S FE  produced by the optical head  17  is supplied via an A/D converter  42  to the servo controller  41 . The push-pull signal S PP  produced by the optical head  17  is such a signal made by synthesizing a tracking error signal S TE  by way of the push-pull method, a wobble signal (FM signal) S WB  corresponding to the groove wobble of the magneto-optical disk  11 , and a clock mark reproduction signal S CM  corresponding to a clock mark CM of the magneto-optical disk  11 . Here, the signals S TE , S WB  and S CM  are in different frequency bands. Accordingly, the signals S TE , S WB  and S CM  can respectively be extracted by the push-pull signal S PP  using the low-pass filter and band-pass filter. 
     The tracking error signal S TE  which is extracted from the push-pull signal S PP  by a low-pass filter  43  is supplied via an A/D converter  44  to the servo controller  41 . Furthermore, a frequency signal SFG output from the above-described frequency generator  14  is supplied to this servo controller  41 . 
     The operation of the servo controller  41  is controlled by a system controller  51  (explained later). An actuator  45  containing a tracking coil, a focus coil, and further a linear motor for moving the optical head  17  along the radial direction is controlled by this servo controller  41  to thereby execute servo control of the tracking operation and the focusing operation. The servo controller  41  further controls movement of the optical head  17  in the radial direction. Also, the spindle motor  13  is controlled by the servo controller  41  in such a manner that, as previously explained, the magneto-optical disk  11  is rotated at a constant angular velocity when the recording operation and the reproducing operation are carried out. 
     The magneto-optical disk apparatus  10  includes a system controller  51  equipped with a CPU, a data buffer  52 , and a SCSI (Small Computer System Interface) interface  53  used to transfer/receive data and commands with a host computer. The system controller  51  controls the overall system of this disk apparatus  10 . 
     The magneto-optical disk apparatus  10  also includes an ECC (Error Correction Code) circuit  54 , and a data modulator  55 . This ECC circuit  54  performs an error correction code sum processing of the write data supplied from the host computer via the SCSI interface  53 , and also an error correction process operation with respect to output data of a data demodulator (discussed later). The data modulator  55  converts the write data to which the error correction code has been added by this ECC circuit  54  into NRZI (Non Return to Zero Inverted) data to thereby obtain the recording data Dr and also produce the above-explained fixed pattern signal S FP.    
     The magneto-optical disk apparatus  10  further includes an equalizer circuit  56 , an A/D converter  57 , a data discriminator  58 , and a data demodulator  59 . The equalizer circuit  56  compensates for a frequency characteristic of the reproduction signal S MO  produced from the optical head  17 . The A/D converter  57  A/D converts the output analog signal from this equalizer circuit  56  into a digital signal. The data discriminator  58  digitally executes a data discriminating process with respect to the output digital data from this A/D converter  57  to thereby obtain reproduction data Dp. The data demodulator  59  executes an NRZI inverse-conversion process of the reproduction data Dp output from this data discriminator  58  to thereby obtain the read data. The data discriminator  58  is comprised of a binary circuit and a Viterbi decoder. 
     The magneto-optical disk apparatus  10  further contains an ADIP (Address In Pre-groove) decoder  60 , a data clock reproducer  70 , and a timing generator  90 . The ADIP decoder  60  decodes the wobble signal S WB  contained in the push-pull signal S PP  produced from the optical head  17  to thereby obtain a frame synchronization signal FD and frame address data FAD. The data clock reproducer  70  is employed to acquire a data clock signal DCK from the clock mark reproduction signal S CM  contained in the push-pull signal S PP , and also the reproduction signal S MO  corresponding to the fixed pattern region of the magneto-optical disk  11 . The timing generator  90  generates timing signals such as a read gate signal and a write gate signal, which are required for the respective circuits of the entire system by using the frame synchronization signal FD, the frame address data FAD, and the data clock signal DCK. The frame address data FAD is also supplied to the servo controller  41 , and the data clock signal DCK is supplied as the sampling clock to the A/D converter  57 . 
     The structure of the ADIP decoder  60  is shown in FIG.  10 . This ADIP decoder  60  comprises a bandpass filter  61  for extracting a wobble signal S WB  from the push-pull signal S PP , a capacitor  61  for blocking the direct current, and a comparator  63  for converting a wobble signal S WB  whose threshold equals zero into a pulse signal (binary signal) P WB.    
     This ADIP decoder  60  further has a PLL circuit  64  comprising a voltage control oscillator  64   a , a frequency divider  64   b  to divide by {fraction (1/24)} the clock signal CD 24  output from the voltage control oscillator  64   a , a phase comparator  64   c  for performing phase comparison of the pulse signal P WB  output from the comparator  63  and the signal output from the frequency divider  64 , and a low-pass filter  64   d  for acquiring a control signal extracted from the low frequency components of the phase differential signal output from the phase comparator  64   c , for input to the voltage control oscillator  64   a.    
     This ADIP decoder  60  further performs frequency demodulation of the clock signal CK 24  output from the voltage controlled oscillator  64   a  with respect to the binary signal P WB  output from the comparator  63 , in order to acquire the address information ADM. This ADIP decoder  60  also has an address converter  68  to perform synchronous detection, biphase demodulation, and error detection of the address information ADM output from the detector  67  by utilizing the clock signal ACK synchronized with the address information ADM acquired from the detector  67  and acquire a frame synchronizing signal FD and frame address data FAD. 
     Next, the operation of the ADIP decoder  60  as shown in FIG. 10 is described. A wobble signal S WB  is extracted from the bandpass filter  61  by means of the push-pull signal S PP . Then, this wobble signal S WB  is converted into a pulse signal P WB  supplied to a comparator  63  by way of the capacitor  62 . As shown above, frequency modulation is performed on the address information ADM after having been biphase modulated, and this post-modulated signal then recorded as a groove wobble. Consequently, this wobble signal S WB  has 4 waves during “1” for a 1 bit of the address information ADM (biphase 1 bit), as shown in FIG. 11A, just the same as with the signal after frequency modulation; and this wobble signal S WB  has 3 waves during “0”. Consequently, as shown in FIG. 11B, the pulse (binary) signal P WB  is acquired from the comparator  63 . The amplitude of this wobble signal S WB  is proportional to the amplitude of the groove wobble of the magneto-optical disk  11 . 
     When the frequency of the wobble signal S WB  corresponding to the bit “1” is equal to “fa” and the frequency of the wobble signal S WB  corresponding to the bit “0” is equal to “fb”, an oscillating frequency of a voltage-controlled oscillator  64   a  is set in such a manner that this oscillating frequency is varied near frequencies (=6 fa=8fb) higher than these frequencies fa, fb by a common frequency multiple. As a result, as indicated in FIG. 11C, from the voltage-controlled oscillator  64   a , a clock signal CK 24  is obtained which has a frequency (fc=6Fa−8Fb), namely, the frequency higher than the biphase bit frequency by 24 times, and is synchronized with the pulse signal P WB.    
     Assuming now that this clock signal CK 24  is set to the reference, a 1 time period of a pulse signal P WB  corresponding to the biphase 1 bit=“1” has a 6T-pattern comprised of “1” for 3 clocks and “0” for 3 clocks, whereas a pulse signal P WB  corresponding to the biphase 1 bit=“0” has an 8T-pattern constructed of “1” for 4 clocks and “0” for 4 clocks. 
     When the 8T-pattern is continuously detected from the pulse signal P WB , the detector  67  outputs a “0” in synchronization with the clock signal ACK (shown in FIG. 11D) during the subsequent biphase 1 bit period. On the other hand, when the 6T-pattern is continuously detected from the pulse signal P WB , the decoding process circuit  67  outputs “1” in synchronization with the clock signal ACK (shown in FIG. 11D) during the subsequent biphase 1 bit period. 
     In other words, the detector  67  executes the demodulating process operation with respect to the pulse signal P WB , so that the address information ADM (shown in FIG. 11E) corresponding to the groove wobble is output in synchronization with the clock signal ACK along with this clock signal ACK from this detector  67 . The clock mark CM for the reproduction signal S CM  is shown in FIG.  11 F. 
     This address information ADM is supplied to an address converter  68 , and then this parallel data is supplied to a decoder  69 . In the address converter  68  performs synchronization detection, biphase demodulation, and the error detection with respect to the address information ADM, so that both a frame synchronization signal FD and frame address data FAD are obtained. As a consequence, the frame address data FAD obtained from the address information ADM is output from the address converter  68  in combination with the frame synchronization signal FD. 
     The structure of the detector  67  is shown in FIG.  12 . This detector  67  has a biphase period detecting circuit  102  to detect by pulse signal P WB  pattern discrimination, the change point (threshold point) between the biphase bit “1” and the biphase bit “0” and acquire a clock signal CK BP  for biphase bit synchronization. This detector  67  also has a 5-bit counter  103  to supply a reset signal to this clock signal CK BP  and to supply this as a clock signal for counting. 
     The detector  67  further has a window pulse generating circuit  104  to generate a window pulse P W 0   for the biphase bit “0” and another window pulse P W 1   for the biphase bit “1” based on the output from the counter  103  The window pulse P W 0   for the biphase bit “ 0 ” is a pulse output from the counter  103  in response to a rising edge and a falling edge of a pulse signal P WB  having a normal interval (8T-pattern). Thus, 6 window pulses are obtained within the biphase period. Similarly, another window pulse P W 1   for the biphase bit “1” is such a pulse output from the counter  103  in response to a rising edge and a falling edge of a pulse signal P WB  having a normal interval (8T-pattern). Thus, 8 window pulses are generated within one biphase period. 
     The detector  67  further has an edge detecting circuit  110  to detect the rising edge and a falling edge of a pulse signal P WB  using the clock signal CK 24  and output as the edge detection pulse Pe. 
     The structure of this edge detecting circuit  110  is shown in FIG.  13 . This edge detecting circuit  110  contains two-stage type D flipflop circuits  111  and  112  comprised of an exclusive-OR circuit  113  and triggered by the clock signal CK 24 . The pulse signal P WB  is applied to the data D terminal of the first D flipflop circuit  111 , so that a non-inverted output is obtained at the Q terminal which is supplied to the data terminal D of the D flip-flop circuit  112 . The signals acquired from the non-inverted terminals Q of the D flipflop circuits  111  and  112  are supplied to the input of exclusive-or circuit  113 . The output from this a exclusive-OR circuit  113  is then output by the edge detection pulse Pe. 
     Returning to FIG. 12, the detector  67  further has a window pulse generating circuit  104  to generate a window pulse P W 0   and a window pulse P W 1   which are gated by the edge detection pulse Pe. The AND gates  121 ,  122  which function as coincidence detection circuits and the respective edge detection pulses Pe are counted by the edge pulse counters  123 ,  124  and the count values x and y then compared. In the next biphase bit period, the comparator circuit  125  outputs the address information ADM based on these comparison results. 
     Here, the clock signals CK BP  are supplied as the respective biphase bit period reset signals to the edge pulse counters  123  and  124 . This clock signal CK BP  is also supplied to as a timing signal to the comparator circuit  125 . In this comparator circuit  125 , a bit “0” is output as address information ADM when x is greater than y; and a bit “1” is output as address information ADM when y is greater than x. 
     This detector  67  also has a frequency divider  126  to output a clock signal ACK (see FIG. 11D) synchronized with the address information ADM, after dividing the clock signal CK by 24 ({fraction (1/24)}) while referring to the clock signal CK BP.    
     The operation of the detector  67  is next described while referring to FIG. 12. A pulse signal P WB  and a clock signal CK 24  are supplied to a biphase period detector  102  and a biphase period clock signal CK BP  obtained. In the 5 bit counter  103 , this clock signal CK BP  is supplied as a reset signal and the clock signal CK 24  supplied as a clock signal for counting. Thus, each biphase bit period is first reset in the 5 bit counter  103  and then counting performed by the clock signal CK 24 . This count is performed from “0” to “23” in base  10 . 
     The count output from the 5 bit counter  103  is supplied to the window pulse generator  104  and based on the output from the 5 bit counter  103 , a window pulse P W 0   for counting the biphase bit “0” and a window pulse P W 1   for counting the biphase bit “1” are generated and each is supplied as gating signals to the AND gates  121  and  122 . 
     On the other hand, a pulse signal P WB  and a clock signal CK 24  are supplied to an edge detector circuit  110 . The rising edge and falling edge of the pulse signal P WB  are detected and an edge detection pulse Pe obtained. This edge detection pulse Pe is supplied to the AND gates  121 ,  122 . This edge detection pulse Pe is also supplied as gating pulses from the AND gates  121 ,  122  to the respective edge pulse counters  123 ,  124  and each biphase 1 bit period then counted. 
     The count values x and y from the edge pulse counters  123 ,  124  counted prior to the biphase 1 bit period are then compared in the comparator circuit  125 . Then, in the next biphase 1 bit period, the address information ADM is output based on these comparison results. 
     For instance, when the wobble signal S WB  for the biphase 1 bit period shown in FIG. 14A corresponds to the biphase bit “0”, the pulse (binary) signal P WB  is consecutively counted 3 times as shown in FIG. 14B in an 8T pattern and an edge detector pulse Pe is acquired as shown in FIG.  14 D and FIG.  14 D 1 . The clock signal CK 24  is shown in FIG.  14 C. 
     Then, in order to form the window pulse P W 0   as shown in FIG. 14E for supply to the AND gate  121 , the gate output POO for supply to the edge pulse counter  123  is set so that x=6 as shown in FIG.  14 F. However, in order to form the window pulse P W 1   as shown in FIG.  14 E′ for supply to the AND gate  122 , the gate output PO 1  for supply to the edge pulse counter  124  is set so that y=2 as shown in FIG.  14 F′. Accordingly, in the next biphase 1 bit period a bit “0” is output as the address information ADM from the comparator circuit  125 . 
     When a wobble signal S WB  for a biphase 1 bit period corresponds to a biphase bit “1” as shown in FIG. 15A, the 6T pattern as shown in FIG. 15B of the pulse signal (binary) P WB  repeats consecutively 4 times, and an edge detector pulse Pe is acquired as shown in FIG.  15 D′. The clock signal CK 24  is shown in FIG.  15 C. 
     Then, in order to form the window pulse P W 0   as shown in FIG. 15E for supply to the AND gate  121 , the gate output POO for supply to the edge pulse counter  123  is set so that x=2 as shown in FIG.  15 F. However, in order to form the window pulse P W 1   as shown in FIG.  15 E′ for supply to the AND gate  122 , the gate output PO 1  for supply to the edge pulse counter  124  is set so that y=8 as shown in FIG.  15 F′. Accordingly, in the next biphase 1 bit period a bit “1” is output as the address information ADM from the comparator circuit  125 . 
     Next, the deformation of the wobble signal S WB  when defects such as in the magneto-optical disk  11  occur are explained next For instance, when defects such as shown in FIG. 16A occur in a case where the wobble signal S WB  of the biphase 1 bit period matches the biphase bit “0”, a pulse (binary) signal P WB  such as in FIG. 16B is obtained, and an edge detector pulse Pe as shown in FIG. 16D, FIG.  16 D′ is acquired. The clock signal CK 24  is shown in FIG.  16 C. 
     Then, in order to form the window pulse P W 0   as shown in FIG. 16E for supply to the AND gate  121 , one gate output POO for supply to the edge pulse counter  123  is set so that x=6 as shown in FIG.  16 F. However, in order to form the window pulse P W 1   as shown in FIG.  16 E′ for supply to the AND gate  122 , the gate output PO 1  for supply to the edge pulse counter  124  is set so that y=3 as shown in FIG.  16 F′. Accordingly, in the next biphase 1 bit period a bit “0” is output as the address information ADM from the comparator circuit  125 . 
     When the wobble signal S WB  of the biphase 1 bit period corresponds to biphase bit “1”, and deformation occurs as shown in FIG. 17A due to defects, a pulse (binary) signal P WB  such as in FIG. 17B is obtained, and an edge detection pulse Pe is acquired as shown in FIG.  17 D and  17 D′. The clock signal CK 24  is shown in FIG.  17 C. 
     Since the window pulse P W 0   which is supplied to the AND gate  121  is formed as shown in FIG. 17E, the gate output POO which is supplied to the edge pulse counter  123  is set so that x=1 as shown in FIG.  17 F. However, since the window pulse P W 1   which is supplied to the AND gate  122  is formed as shown in FIG.  17 E′, the gate output PO 1  which is supplied to the edge pulse counter  124  is set so that y=6 as shown in FIG.  17 F′. Accordingly, in the next biphase 1 bit period a bit “1” is output as the address information ADM from the comparator circuit  125 . 
     Thus, in the detector  67  shown in FIG. 12, even if deformation occurs in the wobble signal S WB  as shown in FIG.  16 A and FIG. 17A, satisfactory address information ADM is acquired even if defects are present in the wobble S WB  signal. The quality of the address information ADM is the same as that when no defects were present in the wobble signal. 
     However, when deformation occurs due to defects such as shown in FIG. 16A and 17A, the difference between the x and y becomes large as explained above so that even if a bit “0” or a bit “1” can be identified only the size of the x and y, a correct address information ADM can be acquired. However when the difference between x and y is slight it is sometimes difficult to determine whether to identify the information as a bit “0” or a bit “1”. 
     For instance when deformation occurs as shown in FIG. 18A in the biphase 1 bit period of the wobble signal S WB , the pulse (binary) signal P WB  appears as shown in FIG.  18 B and an edge detection pulse Pe as shown in FIG. 18D (FIG.  18 E=FIG.  18 E′) is acquired. The clock signal CK 24  is shown in FIG.  18 C. 
     Then, in order to form the window pulse P W 0   as shown in FIG. 18F for supply to the AND gate  121 , the gate output POO for supply to the edge pulse counter  123  is set so that x=4 as shown in FIG.  18 G. In the event of a bit “0”, x=6 can be assumed. 
     However, in order to form the window pulse P W 1   as shown in FIG.  18 F′ for supply to the AND gate  122 , the gate output PO 1  for supply to the edge pulse counter  124  is set so that y=6 as shown in FIG.  17 G′. In the event of bit “1”, x=8 can be assumed. 
     Accordingly, in a simple comparison, a bit “1” can be identified since x is less than y. However, this cannot be immediately determined to actually be bit “1” because when the respective count outputs “x” and “y” are compared with the original count outputs to be detected, both count outputs “x” and “y” have the same errors in view of such a point that there is a count which has a shortage of two. 
     A more accurate determination is possible by adding a further condition to the window, and isolating the rising edge and the falling edge and then detecting these edges. 
     Another structure of the detector  67 A is shown in FIG.  19 . Here the rising edge and the falling edges are isolated and detected. FIG. 19 is shown with the identical symbols in sections corresponding to FIG.  12 . 
     This detector  67 A utilizes the clock signal CK 24  and detects the boundary (dividing line) of the biphase bit “1” and “0” by identification with the pulse signal P WB  by means of the biphase period detecting circuit  102  and acquire the clock signal CK BP  for biphase bit synchronization. This detector  67  also has a 5-bit counter  103  to supply a reset signal to this clock signal CK BP  and to supply this as a clock signal for counting. 
     The detector  67 A has window pulse generator  104  and based on the output from the 5 bit counter  103 , a window pulse P W 0   u and P W 0   d for counting the biphase bit “0” and a window pulse P W 1   u and P W 1   d for counting the biphase bit “1”. 
     Here, the window pulse P W 0   u is a pulse output in response to the rising edge of pulse signal P WB  of a genuine 8T pattern, and 3 pulses are generated in the biphase 1 bit interval. The window pulse P W 0   d is a pulse output in response to the falling edge of pulse signal P WB  of a genuine 8T pattern, and 3 pulses are generated in the biphase 1 bit interval. 
     Further, the window pulse P W 1   u is a pulse output in response to the rising edge of pulse signal P WB  of a genuine 6T pattern, and 4 pulses are generated in the biphase 1 bit interval. The window pulse P W 1   d is a pulse output in response to the falling edge of pulse signal P WB  of a genuine 6T pattern, and 4 pulses are generated in the biphase 1 bit interval. 
     Further, the detector  67 A has a rising edge detector  130  for detecting the rising edge of the pulse signal P WB  and output an edge detector pulse Peu by utilizing a clock signal CK 24 . The detector  67 A also has an edge detector circuit  140  to detect the rising edge of a pulse signal P WB  utilizing a clock signal CK 24  in the same way, and output an edge detector pulse Ped. 
     The structure of the rising edge detector  130  is shown in FIG.  20 . This edge detector  130  is comprised of a 2 stage flipflop circuits  131 ,  132  triggered by the clock signal CK 24 , and an AND circuit  133 . The pulse signal P WB  is supplied to the data terminal D or the D flipflop circuit  131 . The signal obtained from the non-inverting output terminal Q of the D flipflop circuit  131  is supplied to the data terminal D of the D flipflop circuit  132 . Then, the signals obtained from the non-inverting output terminal Q of the D flipflop circuit  131  and from the inverting Q bar output terminal of the D flipflop circuit  132  are supplied to the input of the AND circuit  133 . An edge detector pulse Peu is output from this AND circuit  133 . 
     Also, the structure of the falling edge detector  140  is shown in FIG.  21 . This edge detector  140  is comprised of a 2 stage flipflop circuits  141 ,  142  triggered by the clock signal CK 24 , and also comprised of an AND circuit  143 . The pulse signal P WB  is supplied to the data terminal D of the D flipflop circuit  141 . The signal obtained from the non-inverting output terminal Q of the D flipflop circuit  141  is supplied to the data terminal D of the D flipflop circuit  142 . Then, the signals obtained from the non-inverting output terminal Q of the D flipflop circuit  141  and from the inverting Q bar output terminal of the D flipflop circuit  142  are supplied to the input of the AND circuit  143 . An edge detector pulse Ped is output from this AND circuit  133 . 
     Returning now to FIG. 19, the detector  67 A further has a window pulse generating circuit  104  to generate a window pulse P W 0   u and a window pulse P W 0   d which are utilized as gated edge detection pulses Peu, Ped. The AND gates  151 ,  152  function as coincidence detection circuits and the respective edge detection pulses Peu and Ped for the window pulses P W 1   u and P W 1   d generated by the window pulse generating circuit  104  and supplied to the AND gates  153 ,  154  in the detector  67 A which function as coincidence detection circuits. 
     The detector  67 A further comprises an edge pulse counter  155 ,  156  for counting the edge detection pulses Peu, Ped respectively gated from the AND gates  151  and  152 , an edge pulse counters  157 ,  158  for counting the edge detection pulse Peu, Ped gated from the AND gates  153 ,  154 , an adder  159  for adding the counts from the edge pulse counters  155  and  156 , and an adder  160  for adding the counts from the edge pulse counters  157  and  158 . The detector  67 A also compares the x (output from the adder  159 ) total count of the edge pulse counters  155  and  156  counted in the previous biphase 1 bit interval, with the y (output value from the adder  160 ) total count of the edge pulse counters  157  and  158  counted in the previous biphase 1 bit interval. In the next biphase 1 bit interval, the comparator  161  outputs the address information ADM based on the results of the comparison. 
     Here, the clock signal CK BP  of each biphase bit period is supplied as a reset signal in the edge pulse counters  155 - 158 . Also, the clock signal CK BP  is supplied as a timing signal to the comparator circuit  161 . In this comparator circuit  161 , a bit “0” is output as address information ADM when x is greater than y; and a bit “1” is output as address information ADM when y is greater than x. 
     The detector  67 A also has a frequency divider  126  to output a clock signal ACK (see FIG. 11D) synchronized with the address information ADM, after dividing the clock signal CK by 24 ({fraction (1/24)}) while referring to the clock signal CK BP.    
     The operation of the detector  67  is next described while referring to FIG. 19. A pulse signal P WB  and a clock signal CK 24  are supplied to a biphase period detector  102  and a biphase period go clock signal CK BP  obtained. In the 5 bit counter  103 , this clock signal CK BP  is supplied as a reset signal and the clock signal CK 24  supplied as a clock signal for counting. Thus, each biphase bit period is first reset in the 5 bit counter  103  and then counting performed by the clock signal CK 24 . This count is performed from “0” to “23” in base  10 . 
     The count output from the 5 bit counter  103  is supplied to the window pulse generator  104 A and based on the output from the 5 bit counter  103 , a window pulse P W 0   u, P W 0   d for counting the biphase bit “0” and a window pulse P W 1   u, P W 1   d for counting the biphase bit “1” are generated and each is supplied as gating signals to the AND gates  151 - 154 . 
     On the other hand, a pulse signal P WB  and a clock signal CK 24  are supplied to an edge detector circuit  130 . The rising edge of the pulse signal P WB  is detected and an edge detection pulse Peu obtained. This edge detection pulse Peu is supplied respectively to the AND gates  151 ,  153 . In the same way, a pulse signal P WB  and a clock signal CK 24  are supplied to an edge detector circuit  140 . The falling edge of the pulse signal P WB  is detected and an edge detection pulse Ped obtained. This edge detection pulse Ped is supplied respectively to the AND gates  152 ,  154 . 
     The edge detection pulses Peu and Ped gated to the AND gates  151  and  152 , are respectively supplied to the edge pulse counters  155  and  156  and counted at each biphase 1 bit period. Further, the edge detection pulses Peu and Ped gated to the AND gates  153  and  154 , are respectively supplied to the edge pulse counters  157  and  158  and counted at each biphase 1 bit period. 
     The comparator circuit  161  compares the total x from the count by the edge pulse counters  155 ,  156  counted in the previous biphase 1 bit period, with the total y count from the edge pulse counters  157 ,  158  counted in the previous biphase 1 bit period. The address information ADM is output in the next biphase 1 bit period based on these comparison results. 
     The operation in the detector  67 A shown in FIG. 19 when deformation occurs as shown in FIG. 22A (= 18 A) the biphase 1 bit period of the wobble signal S WB  is explained next. The pulse (binary) signal P WB  appears as shown in FIG.  22 B and an edge detection pulse Peu corresponding to the rising edge as shown in FIG. 22E (= 22 E′) is acquired and an edge detection pulse Ped corresponding to the falling edge in FIG. 22G (=FIG.  22 G′ ) is acquired. The clock signal CK 24  is shown in FIG.  22 C. The edge detection pulse Pe which combines the edge detection pulse Peu and Ped is shown in FIG.  22 D. 
     Then, in order to form the window pulses P W 0   u, P W 0   d as shown in FIGS. 22F and 22H for supply to the AND gates  151 ,  152 , the gate outputs Aou, Aod for supply to the edge pulse counter  155 ,  156  are set so that x=1 as shown in FIG.  22 I. However, in order to form the window pulses P W 1   u, P W 1   d as shown in FIGS.  22 F′ and  22 H′ for supply to the AND gates  153 ,  154 , the gate outputs A 1 u, A 1 d for supply to the edge pulse counters  157 ,  158  are set so that y=6 as shown in FIG.  22 I′. Accordingly, the x, y differential has become sufficiently large so that correct detection results are obtained even just by using the comparison results as is. 
     Accordingly, the x, y results are utilized as is, in the comparator circuit  161  and a bit “1” is output as address information ADM in the next biphase 1 bit period. 
     This arrangement has the benefit that a more accurate identification is possible by also using the edge information from the pulse signal P WB  in addition to the window pulse. 
     Next, the ADIP decoder  60  shown in FIG. 10 contains a PLL circuit  64  and has a relatively complex configuration. 
     As related above, the biphase bit count “a” between adjacent clock marks is two bits. The channel bit count “n” between adjacent clock marks is 528 bits. Further, the oversampling value for the biphase bit is 24 clocks. As related later on, in the data clock reproducer  70 , the reproduction signal S CM  of the clock mark is a multiple n=528 and a data clock signal DCK is obtained. In this case, the frequency of the data clock signal DCK and the oversampling clock signal CK 24  for the biphase bit are related by means of an integer ratio. In other words, the frequency of the data clock DCK signal is set as f dck and when the frequency of the signal CK is set as f  24 , then f dck=11×f  24 . Here, frequency division of the data clock signal DCK can be performed and a clock signal CK 24  generated. 
     The configuration of another aspect of the ADIP decoder  60 A is shown in FIG.  23 . The data clock signal DCK is frequency divided and a clock signal CK 24  acquired. In this FIG. 23, symbols identical to the portions of FIG. 10 are used so a detailed description is omitted here. 
     This ADIP decoder  60 A has a frequency divider  60  to divide the data clock signal reproduced by the data clock reproducer  70  by 1/M and generate an oversampling clock signal CK 24 . Here, M=n/(a·s) and in this embodiment, M=528/(2·24)=11. The clock signal CK 24  generated in this frequency divider  69  is used in the detector  69  ( 67 A). The timing for the reproduction signal S CM  of the clock mark CM, the data clock signal DCK and the oversampling clock signal CK 24  of the biphase bit are shown in FIGS. 24 A through C. 
     The ADIP decoder  60  shown in FIG. 23 is identical to the ADIP decoder  60  shown in the another configuration in FIG. 10 so a detailed description is omitted here. This ADIP decoder  60  however operates in the same manner as the ADIP decoder  60  shown in FIG. 10 and a frame address data FAD and frame synchronizing signal FD are acquired from the address converter  68 . 
     This ADIP decoder  60  as shown in FIG. 23 acquires a clock signal S 24  so that a PLL circuit is not needed and has the benefit of a simpler configuration compared to the ADIP decoder  60  shown in FIG.  10 . 
     Also in FIG. 25, there is shown the configuration of the data clock reproducer  70 . This data clock reproducer  70  contains a band-pass filter  71  for extracting a clock mark reproduction signal S CM  from the push-pull signal S PP , a capacitor  72  for removing the DC component, and an edge detector  73  for acquiring a pulse signal P CM  to show the timing of a zero cross point from the clock mark reproduction signal S CM.    
     This data clock reproducer  70  also contains a capacitor  74  for removing the DC component of the reproduction signal S MO ; a comparator  75  for converting the reproduction signal S MO  into a pulse (binary) signal P MO  while setting a threshold value=0; and an AND circuit  76  for AND-gating this pulse signal P MO  by using the fixed pattern gate signal SG supplied from the timing generator  90  to output a pulse signal P FP  corresponding to the reproduction signal S MO  of the fixed pattern region of the magneto-optical disk  11 . In this case, as indicated in FIG. 3D, the fixed pattern gate signal SG becomes “1” in the time period during which the reproduction signal S MO  of the fixed pattern region is obtained, and becomes “0” in other time periods. 
     In this timing generator  90 , a pulse signal P CM  is supplied to show the 0 cross point timing of the above mentioned clock mark reproduction signal S CM . Also, in this timing generator  90 , the data clock signal DCK is counted and a fixed pattern gate signal SG is generated based on the timing of this pulse (binary) signal P CM.    
     This data clock reproducer  70  further contains a voltage controlled oscillator  77 , a frequency divider  78 , a phase comparator  79 , and a low-pass filter  80 , which constitute a PLL circuit. The frequency divider  78  frequency-divides a data clock signal DCK output from this voltage-controlled oscillator  77  by 1/N (here N=n=528). The phase detector  79  performs a phase comparison between a pulse signal P CM  output from the edge detector  73  and an output signal of the frequency divider  78 . The low-pass filter  80  filters out the low frequency component of a phase error signal output from this phase comparator  79 . 
     This data clock reproducer  70  furthermore includes another phase comparator  81 , a high-pass filter  82 , and an adder  84 . The phase comparator  81  performs phase comparison between the pulse signal P FP  output from the AND circuit  76  and the output signal from the frequency divider  78 . The high-pass filter  82  filters out high frequency components of the phase error signal output from this phase comparator  81 . The adder  84  adds the output signal from the low-pass filter  80  to the output signal of the high-pass filter  29  which is supplied via a connection switch  83 . To this connection switch  83 , a switch control signal SW is supplied from the system controller  51 . As a result, the connection switch  83  is turned OFF when the data is written (recorded), whereas the connection switch  83  is turned ON when the data is read (reproduced). 
     The operation of the data clock reproducer  70  shown in FIG. 25 will next be explained. The clock mark reproduction signal (represented in FIG. 26A) is extracted from the push-pull signal S PP , and then this clock mark reproduction signal S CM  is supplied via the capacitor  72  to the edge detector  73 . A pulse signal P CM  (shown in FIG. 26B) is obtained from the edge detector  73 , which indicates the timing of the zero cross point of the clock mark reproduction signal. 
     The reproduction signal S MO  output from the optical head  17  (see FIG. 1) is supplied via the capacitor  74  to the comparator  75  so as to be converted into the pulse (binary) signal P MO . Then, the pulse signal P FP  (shown in FIG. 26D) corresponding to the reproduction signal S MO  of the fixed pattern region SG (shown in FIG. 26C) of the magneto-optical disk  11  is derived from this pulse (binary) signal P MO  by the AND circuit  76 . 
     Then, when the data is written (recorded), since the connection switch  83  is turned OFF, the PLL circuit is comprised of a voltage-controlled oscillator  77 , a frequency divider  78 , a phase comparator  79 , and a low-pass filter  80 . Only the low frequency component of the phase error signal output from the phase comparator  79  is supplied as the control signal to the voltage-controlled oscillator  77 . As a consequence, the data clock signal DCK is generated from the voltage-controlled oscillator  77 , and the phase of this data clock signal DCK is control led by the low frequency component of the phase information possessed by the clock mark reproduction signal S CM.    
     Further, when the data is read (reproduced), since the connection switch  83  is turned ON, the PLL circuit is comprised of the voltage-controlled oscillator  77 , the frequency divider  78 , the phase comparators  79 ,  81  and the low-pass filter  80 . An addition signal produced by adding the low frequency component of the phase error signal output from the phase comparator  79  to the low frequency component of the phase error signal output from the phase comparator  79  is supplied as the control signal to the voltage-controlled oscillator  77 . As a consequence, the data clock signal DCK is produced from the voltage-controlled oscillator  77 , and the phase of this data clock signal DCK is controlled by the low frequency component of the phase information possessed by the clock mark reproduction signal S CM  and the high frequency component of the phase information possessed by the reproduction signal S MO  of the fixed pattern region. It should be understood that FIG. 26E shows the data clock signal DCK. 
     A description will now be made of the magneto-optical disk apparatus  10  operation indicated in FIG.  1 . When a data write command is supplied from the host computer to the system controller  51 , the data writing process (recording process) operation is carried out. In this case, with respect to the write data received by the SCSI interface  53  and stored in the data buffer  52 , the error correction code adding process operation is executed by the ECC circuit  54 , and furthermore the conversion operation to the NRZI data is carried out by the data modulator  55 . Then, both the recording data Dr and the fixed pattern signal S FP  are supplied from the data demodulator  55  to the magnetic head driver  16 , so that the recording data Dr is recorded into the data region as the target position of the magneto-optical disk  11 , and also the fixed pattern signal S FP  is recorded into the fixed pattern region corresponding to the data region into which the recording data Dr is recorded. 
     When a data read command is supplied from the host computer to the system controller  51 , the data reading process (reproducing process) operation is carried out. In this case, the reproduction signal S MO  is obtained from such a data region functioning as the target position of the magneto-optical disk  11  and from the fixed pattern region corresponding to this data region. The frequency characteristic of this reproduction signal S MO  is compensated by the equalizer circuit  56 , and this reproduction signal S MO  is converted into the digital signal by using the data clock DCK by the A/D converter  57 . Thereafter, the digital data is discriminated by the data discriminator  58  to thereby obtain reproduction data Dp. Then, the NRZI inverse conversion is carried out on this reproduction data Dp by the data demodulator  59 , and the error correction process operation is performed by the ECC circuit  54 , so that the read data is obtained. This read data is then temporarily stored in the data buffer  52 , and thereafter is transmitted via the SCSI interface  53  to the host computer at a predetermined timing. 
     In the data writing process operation and the data reading process operation, it should be noted that both the magnetic head  51  and the optical head  17  are seek-controlled to the target position by the servo controller  41 . In this case, the seek operation is carried out with reference to the frame address data FAD output from the ADIP decoder  60 . Also, when the data is written (recorded), the data clock signal DCK is produced from the data clock reproducer  70 , the phase of which is controlled by the low frequency component of the phase information held by the clock mark reproduction signal S CM . The data writing process operation is carried out synchronously with this data clock signal DCK. On the other hand, when the data is read (reproduced), the data clock signal DCK is produced from the data clock reproducer  70 , the phase of which is controlled by the low frequency component of the phase information held by the clock mark reproduction signal S CM , and the high frequency component of the phase information held by the reproduction signal S MO  of the fixed pattern region. The data reading process operation is carried out synchronously with the data clock signal DCK. 
     In the magneto-optical disk apparatus  10  operation of FIG. 1, when the data is read (reproduced), the data clock signal DCK (see FIG. 25) may be acquired from the data clock reproducer  70 , the phase of which is controlled by the low frequency component of the phase information held by the clock mark reproduction signal S CM , and the high frequency component of the phase information held by the reproduction signal S MO  of the fixed pattern region. Thus, even when the signal to noise (S/N) ratio of the clock mark reproduction signal S CM  is low, it is possible to obtain the clock signal synchronized with the reproduction data with high precision. Thus, the precision of the data reading process operation can be increased. 
     Also, the amplitude of the groove wobble of the magneto-optical disk  11  is varied in response to the frequency of the post-modulated signal, and the slope of the groove wobble at the zero cross point which corresponds to the junction between the address information ADM of “1” and the address information ADM of “0” (see FIG. 5) is prevented from being changed. As a result, the jitter component of the wobble signal S WB  along the time axis direction, which corresponds to the junction between the address information ADM of “1” and the address information ADM of “0” is reduced, so that the address information ADM can be obtained under better conditions by the ADIP decoder  60  (see FIG.  10 ). As previously explained, in this embodiment mode, the waveform numbers of the groove wobbles corresponding to the address information of “1” and “0” are each selected to be integers. Since all junctions of the groove wobbles corresponding to the address information ADM of “1” and “0” become the zero crosspoints, this is a particularly effective arrangement. 
     Also, in the ADIP decoder  60 , the address information ADM is obtained by way of the demodulating process operation by employing a clock signal CK 24  having such a frequency “fc” (=6 fa=8 fb) higher than the frequencies “fa” and “fb” of the wobble signals S WB  by a common frequency multiple, which corresponds to the data of the address information ADM of “1” and “0” (see FIG.  10 ). As a consequence, since the decoding process circuit can be arranged by employing only one signal system of the PLL circuit, there is the advantage that the arrangement of the ADIP decoder  60  can be simplified. In this case, while the waveform numbers of the groove wobbles corresponding to the address information ADM of “1” and “0” are selected to be the proper integers, since the pulse signals output from the comparator  63  in response to the address information ADM of “1” and “0” always have the same shapes, it is possible to easily perform the demodulating process operation by using the clock signal CK 24  in the decoding process circuit  67  ( 67 A). 
     Also, the frequency of the data clock signal DCK and the oversampling clock signal CK 24  for the biphase bit are related by means of an integer ratio. Here, frequency division of the data clock signal DCK is performed and a clock signal CK 24  acquired to allow a simpler configuration for the ADIP decoder  60 A FIG.  23 ). 
     Further in the ADIP decoder  60 ,  60 A of the detector  67  ( 67 A) wave detection of the bit “0” and bit “1” is performed using the window pulses so that even if defects are present in the wobble S WB  signal, the quality of the address information ADM is the same as that when no deformation was present in the wobble signal. 
     The second embodiment of this invention is next described. The structure of a magneto-optical disk apparatus  10   a  of the first embodiment of this invention is shown in FIG.  27 . The reference numerals of FIG. 27 are identical to those shown in FIG. 1 so a detailed description is omitted here. 
     An optical disk  11 A used in this magneto-optical disk apparatus  10 A is formed with alternate grooves and lands radially across the disk surface containing recording tracks. The lands or the grooves are preformatted with clock marks containing phase information. 
     These clock marks CM differ from the marks shown in FIGS. 44A and 44B in that these clock marks CM have a first protrusion CM with a parallel falling edge section formed radially at one end of the groove and, a second protrusion CM with a parallel rising edge section formed radially at the other end of the groove. 
     A preformatting device  200  as shown in FIG. 28 is utilized to preformat the surface of the base disk with the above mentioned clock marks CM and the address information ADM by groove wobbles. 
     This preformatting device  200  has a cutting light source  201 . A helium-cadium (He—Cd) laser may for instance be used as the laser light source. 
     The cutting beam (laser) output from the light source  201  is isolated into two optical path beams by a half mirror  20 . One of these beams, a beam Ba is supplied to a switch  204  by way of a half mirror  202 , while the other beam Bb is supplied directly to a switch  205 . 
     These switches  204 ,  205  regulate the output and stopping of the laser beams. In the example here, an electro optical modulator is utilized. These switches  204 ,  205  are controlled based on control signals Ca, Cb from the beam on/off controller  206 . The control beam signal output timing of the on/off controller  206  is regulated by a controller  207 . 
     The wobble status of the cutting beams Ba, Bb whose on/off is regulated, are controlled by beam wobble controllers  211 ,  212 . An AOM (acoustic optical modulator) is used in the example given here as the beam wobble controllers  211  and  212 . The wobble quantity of these beam wobble control  211  and  212  is regulated by control signals Fa, Fb from a beam wobble controller  213 . Actually, the wobble quantity is controlled by the amplitude levels of the control signal Fa, Fb. Also, the wobble direction is controlled by the polarity of the control signals Fa, Fb. When the control signal has a triangular waveform, the wobble marks form a triangular wave. When supplied with a sine wave the wobble marks will form a triangular wave. 
     The cutting beams Ba, Bb controlled by the wobble status are input to an optical system  215  and a light junction formed by these beams overlapping in one section as shown in FIG.  30 . In this case, a pair of prisms  216 ,  217  are utilized. The cutting beams  216 ,  217  are thus made to overlap at one junction as shown in FIG. 30 by means of the pair of prisms  216 ,  217 . 
     These cutting beams Ba, Bb which form a light junction are irradiated onto a surface  11   f  of the base disk  11 E by means of the objective lens  218  and a groove  12 G and (disk counting for both grooves and groove wobble) a groove wobble formed. Here, a rotation-drive mechanism  219  is provided to rotate a base disk  11 E radially and drive in the x direction. The base disk  11 E is driven one spiral for each rotation of the base disk  11 E. In other words, driven a distance equal to the distance from one groove to the next groove. 
     The clock mark CM is formed by controlling the cutting the surface  11   f  of the base disk  11 E. Cutting of the base disk  11 E is performed when the laser beam is irradiated onto the surface  11   f  of the base disk  11 E. However, when laser beam irradiation of the surface  11   f  of the base disk  11 E is stopped, no cutting of the base disk  11 E is performed. 
     Accordingly, by setting as the boundary, the zero cross point (timing to) of the clock mark CM reproduction signal S CM  (FIG. 29A) to be obtained, the clock mark CM can be formed by switching the cutting beams Ba and Bb on and off. In other words, the cutting beam Ba is switched off (FIG. 29B) from a specified position prior to the cross point up to the zero cross point; while the cutting beam Bb is switched off (FIG. 29C) up to a specified position immediately after the zero cross point. 
     In this case, the scanning tracks TRa, TRb of the cutting beams Ba, Bb are respectively shown in FIG.  30 . Accordingly, the land  12 L and the groove  12 G are formed on the surface  11   f  of the base disk  11 E. 
     An examination of the groove  12 G shows that the upper edge is one side of the groove wobble edge and that the lower edge is a flat surface. This upper edge is formed according to the off period of the beam Ba so that a rectangular protrusion  4   a  projects internally. On the other hand, the lower edge is formed according to the off period of the beam Bb so that a rectangular protrusion  4   b  projects internally. 
     Conversely, an examination of the land  12 L shows that the upper edge is one side of the groove wobble edge and that the lower edge is a flat surface. This lower edge is formed according to the off period of the beam Ba so that a rectangular protrusion  4   a  projects externally. On the other hand, the upper edge is formed according to the off period of the beam Bb so that a rectangular protrusion  4   b  projects externally. 
     These pair of protrusions  4   a ,  4   b  formed by the beams Ba, Bb, comprise the clock mark CM. The edge of this pair of protrusions  4   a ,  4   b  has a steep ecgie, consequently the protrusion  4   a  of the ON edge  4   a ′ and zhe protrusion  4   b  of the OFF edge  4   b ′ have corresponding positions in the track direction and are therefore formed with the same radius. 
     Returning to FIG. 27, the optical disk  11 A has the above related preformatting performed on the base disk  11 E by means of the preformatting device  200  as shown in FIG.  28 . Accordingly, the surface of the optical disk  11 A as shown in FIG. 31A is formed with the same lands  12 L and the grooves  12 G on the surface  11   f  of the base disk  11 E as shown in FIG.  30 . 
     When the clock marks CM (protrusions  4   a ,  4   b ) preformatted on the optical disk  11 A as shown in FIG. 31A are reproduced by means of the beam P PB  shown in the figure, a reproduction signal S CM  as shown in FIG. 31B is obtained. In this case, when differential between the signal Su from the upper part of Pu for the scan tracks  5 , and the Sd signal from the lower part of Pd is set (push-pull signal: S PP =Su−Sd); only the differential for the protrusions  4   a ,  4   b  becomes larger during scanning of the land  12 L. Furthermore, since this polarity is reversed, the reproduction signal S CM  becomes the signal SL as shown by the solid line in FIG.  31 B. The reproduction signal of S CM =SL is a steep level change in the vicity of the zero cross point. 
     In contrast, when scanning the grooves  12 G, the reproduction signal S CM  becomes a signal SG as shown by the dashed line in FIG. 31B since the polarity of the protrusions  4   a ,  4   b  becomes reversed, and the polarity is inverted for the above mentioned signal SL. The reproduction signal of S CM =SG is also a steep level change in the vicinity of the zero cross point. 
     A pulse (binary) signal P CM  (shown in FIG. 31C) is acquired which shows the timing of the zero crosspoint of the clock mark S CM  (SL, SG) extracted from the push-pull signal S PP  by means of the edge detector  73  (see FIG. 25) in the data clock reproducer  70 . A data clock signal DCK is reproduced based on this pulse (binary) signal P CM.    
     This magneto-optical disk apparatus  10 A has a polarity identification circuit  46  to identify whetherthebeam P PB  isabove the land  12 L or above the groove  12 G by means of the polarity of the clock mark signal S CM . The identification signal SGL acquired by this polarity identification circuit  46  is supplied to a servo controller  41  in this embodiment. In this servo controller  41  a selection is made based on the identification signal SGL, whether to use the tracking servo for the land  12 L or the tracking servo for the groove  12 G (servo signal polarity differs between the land and groove). Then, basedon the tracking servo that was selected, an actuator  45  is controlled by means of the tracking control signal from the servo controller  41  so that tracking is performed by the beam over the land  12 L or over the groove  12 G. 
     The structure of the polarity identification circuit  46  is shown in FIG.  32 . This polarity identification circuit  46  is comprised of a bandpass filter  46   a  for extracting a clock mark reproduction signal S CM  from the push pull S PP , a capacitor  46   b  for removing the DC components, a comparator  46   c  for comparing the clock mark reproduction signal S CM  with the positve threshold value TH 1 , and a comparator  46   d  for comparing the clock mark reproduction signal S CM  with the negative threshold value TH 2 . 
     In this case, in the comparator  46   c , the clock mark signal S CM  is supplied to the non-inverted input terminal, and the threshold value TH 1  is supplied to the inverted input terminal. The output signal S 1  of this comparator  46   c  becomes “1” when S CM  is greater than or equal to TH 1 ; and becomes “0” when the S CM  is less than TH 1 . In the comparator  46   d , the clock mark signal S CM  is supplied to the inverted input terminal, and the threshold value TH 2  is supplied to the non-inverted input terminal. The output signal S 2  from this comparator  46  becomes “1” when S CM  is less than or equal to TH 2  and becomes “0” when S CM  is greater than TH 1 . 
     The polarity identification circuit  46  has a groove/land identifier circuit  46   e  for identifying whether the beam P PB  is above the land  12 L or above the groove  12 G by means of the polarity of the clock mark signal S CM  based on the output signals S 1 , S 2 ; and then issue an identification signal SGL. In this groove/land identifier circuit  46   e , timing pulses t1, t2 (shown in FIG. 31F) are supplied from a timing generator  90  (see FIG. 1) to show the approximate timing for “to” of the zero cross point timing of the clock mark signal S CM.    
     In this groove/land identifier circuit  46   e , when the output signal S 1  becomes “1” at timing t1 and the output signal S 2  becomes “1” at timing t2, the beam P PB  is determined to be over the groove  12 G and a “1” is output as an identifier signal SGL. However when the output S 2  becomes “1” at timing t1 and the output signal S 1  becomes “1” at timing t2, the beam P PB  is determined to be over the land  12 L and a “0” is output as an identifier signal SGL. 
     Next, the operation of the polarity identification circuit  46  of FIG. 32 is explained. When the beam P PB  is scanning over a groove  12 G, the clock mark reproduction signal S CM  becomes a signal SG shown in the dashed line in FIG.  31 B. Consequently, the output signals S 1 , S 2  of the comparators  46   c ,  46   d  become as shown in FIG. 31D, and the output signal S 1  becomes “1” at the timing t1 and the output signal S 2  becomes “1” at timing t2. Accordingly, in the groove/land identifier circuit  46   e , the beam P PB  is determined to be over the groove  12 G and a “1” is output as the identifier signal SGL. 
     On the other hand, when the beam P PB  is scanning over the land  12 L, the clock mark reproduction signal S CM  becomes a signal SL shown in the solid line in FIG.  31 B. Consequently, the output signals S 1 , S 2  of the comparators  46   c ,  46   d  become as shown in FIG. 31E, and the output signal S 2  becomes “1” at the timing t1 and the output signal S 1  becomes “1” at timing t2. Accordingly, in the groove/land identifier circuit  46   e , the beam P PB  is determined to be over the land  12 L and a “0” is output as the identifier signal SGL. 
     However, in the exampte in FIG. 30, since the direction that the protrusions  4   a ,  4   b  of the land  12 L and groove  12 G face is determined by the on/off switching of the cutting beams Ba, Bb, as can be seen, the land  12 L is fatter than the groove  12 G (wider). Consequently, the amplitude levels of the signals SL, SG used as the clock mark reproduction signals S CM  will be different (see FIG.  31 B). 
     This difference in amplitude levels is due to forming of the clock marks CM (protrusions  4   a ,  4   b ) just by the on/off switching of the cutting beams Ba, Bb as shown in the example in FIG.  30 . In order to eliminate this difference, as for instance shown in FIG. 33A, the cutting beam Bb can be shifted to the land  12 L side (fixed quantity wobble) for at least the off period of the cutting beam Ba. The shifting of this beam Bb is performed by the beam wobble control  212  shown in FIG.  28 . 
     When beam wobble control is performed, the pitch Wa of the groove  12 G matches the pitch Wb of the land  12 L in the off period of the cutting beam Ba. This process allows the differential between the amplitude levels of signals SL, SG of the clock mark reproduction signal S CM  to be corrected as shown in FIG.  33 B. However, the difference in the positive and negative sides of the amplitude levels cannot be eliminated. In the example shown in FIG. 34, the difference in positive and negative amplitude levels has been set to allow correction. 
     In this case, the beam Ba, Bb on/off switching timing “to” is set as the boundary and both the beams Ba, Bb shifted in mutually opposite directions (fixed quantity wobble) around the boundary. Consequently, for the cutting beam Ba, a control signal Ca as shown in FIG. 34A is supplied to the switch  204 ; a control signal Fa as shown in FIG. 34B is supplied to the beam wobble control  211 . 
     In the same way, for the cutting beam Bb, a control signal Cb as shown in FIG. 34C is supplied to the switch  205 , and a control signal Fb as shown in FIG. 34D is supplied to the beam wobble control  212 . The interval for shifting the beam Ba, Bb by means of these control signals Fa, Fb is optional. In this example, the beam off period is approximately ½. 
     The beams Ba, Bb are each set in mutually different directions for wobbling by means of supplying these control signals Fa, Fb as shown in FIGS. 34B and 34D so that for instance, the cutting of the groove  12 G is performed as shown by the diagonal line in FIG.  34 E. Consequently, the relation of the land  12 L and the groove  12 G becomes that shown in FIG.  34 F and the imbalance in width between the land  12 L and the groove  12 G is eliminated. Accordingly, as shown in FIG. 34G, the difference between the amplitude levels of signals SL and SG of the clock mark reproduction signal S CM  is completely eliminated. 
     In tree example in FIG. 34, a triangular waveform is shown the control signals Fa, Fb however a sine wave or other waveforms may also be used. The width and amplitude of the triangular waveform, in other words the wobble quantity and other items merely constitute one example. For instance if the wobble quantity is increased, then the amplitude levels of the signals SL, SG can be increased by that amount. 
     As mentioned above, in the clock mark CM preformatted on the optical disk  11 A, on examining the groove  12 G shows it comprises a pair of protrusions  4   a    4   b  formed to protrude internally from both sides. However, instead of these protrusions  4   a    4   b , a pair of concavities can be formed to protrude externally at track direction positions matching these protrusions  4   a    4   b  and these concavities may be used as the clock mark CM. 
     Returning to FIG. 27, when writing data (during record) in the disk apparatus  10 A, during record of the record data Dr and the fixed pattern signal S PP , modulation of the laser beam is performed with the data clock signal DCK. Accordingly, the data clock signal DCK reproduced by the data clock reproducer  70  is supplied to a laser driver  18 . This method for modulating the laser beam with a data clock signal DCK is for instance listed in U.S. Pat. No. 5,182,734. 
     Even when writing data (during record), reproduction of the clock mark CM is performed by the optical disk  11 A. As related above, when the laser beam is modulated by the data clock signal DCK, a weighted clock mark reproduction signal S CM ′ (shown in FIG. 43) is acquired. When filtering is performed with a low-pass filter in order to remove the data clock signal DCK from this clock mark reproduction signal S CM ′, the waveform in the vicinity of the zero cross point become indistinct. When a data clock signal DCK is reproduced by utilizing the clock mark signal S CM  as phase information, jitter occurs in this data clock signal DCK and adverse effects are exerted on the recording of data. 
     Whereupon, in the disk apparatus  10 A in FIG. 27, during writing of data, a control signal CT 1  as shown in FIG. 35B is supplied to the laser driver  18  from the system controller  51 . The period (clock mark period) T CM  in which the clock mark reproduction signal S CM  (shown in FIG. 35A) is acquired is set so that the laser beam is not modulated by the data clock signal DCK as shown in FIG.  35 D. Also, a power control signal as shown in FIG. 35C is supplied to the servo controller  41  from the system controller  51  and in the preformat period T CM , the laserbeam power is the reproduction power P R  and not record power P W.    
     Thus, as shown in FIG. 35A since the laser beam is set so as not to be modulated by the data clock signal DCK during the preformat period T CM , a non-weighted data clock signal S CM  can be acquired. from the data clock signal DCK. Consequently , highly accurate phase information from the zero cross point of the clock mark reproduction signal S CM  can be acquired and satisfactory reproduction of the data clock reproduction signal DCK can be obtained. 
     The disk apparatus  10 A in FIG. 27 has the same structure as the disk apparatus  10  shown in FIG.  1  and the operation is identical. The disk apparatus  10 A shown in FIG. 27, therefore has an effect identical to the disk apparatus  10  shown in FIG.  1 . 
     Further, in this disk apparatus  10 A, the beam P PB  scanning the optical disk  11 A can be determined to be over a land or over a groove by means of the polarity of the clock mark reproduction signal S CM . The beam P PB  can be easily identified as being over either over a land or over a groove. 
     During data writing, the laser beam is controlled in the preformat period T CM  so as not to be modulated by the data clock signal DCK. Accordingly, a non-weighted data clock signal S CM  can be acquired from the data clock signal DCK and highly accurate phase information from the zero cross point of the clock mark reproduction signal S CM  acquired so that satisfactory reproduction of the data clock reproduction signal DCK can be obtained. 
     In the preformatting device  200  shown in FIG. 28, on/off control along the time axis of the cutting beams Ba, Bb is performed and a pair of protrusions  4   a ,  4   b  formed as clock marks CM. The level change in the vicinity of the cross point of the reproduction signal S CM  for the click marks CM ( 4   a ,  4   b ) formed in this way, is steep so that highly accurate phase information can be obtained from the zero cross point of this clock mark reproduction signal S CM  satisfactory reproduction of the data clock reproduction signal DCK can be achieved. 
     Next, the third embodiment of this invention is described. The structure of the optical disk apparatus  10 B of third embodiment is shown in FIG.  36 . The same reference numerals as in FIG. 27 are used in FIG. 26 so a detailed description is omitted here. 
     In the disk apparatus  10 A in FIG. 27, the laser beam is controlled in the preformat period T CM  so as not to be modulated by the data clock signal DCK and the laser beam power is controlled to be the reproduction power P R  however in the optical disk apparatus  10 B of third embodiment, during the clock mark period T CM , the laser beam DCK is substituted with the clock signal DCK; and modulation performed with the high frequency signal HF. 
     An oscillator  91  to output a high frequency signal HF is provided in the disk apparatus  10 B, and this high frequency signal HF is supplied to the laser driver  18 . A frequency band is selected for this high frequency signal HF so as to reduce the noise of the semiconductor laser and the frequency used is generally known to be approximately 500 MHz. 
     In the disk apparatus  10 B during data writing, a control signal CT 2  is supplied to the oscillator  91  from the system controller as shown in FIG.  37 B. The high frequency signal HF is supplied to the laser driver  19  by oscillator  91  only for the clock mark period T CM . Accordingly, as shown in FIG. 37D, the laser beam is modulated by the high frequency signal HF in the clock mark period T CM  with the date clock signal DCK. The laser beam power is normally controlled in record power P W  status as shown in FIG. 37C however, control may also be accomplished with the reproduction power P R  only in the preformat period TM. 
     Thus, when the laser beam is modulated by the high frequency signal HF in the preformat period T CM , the push-pull signal SP output during clock mark CM reproduction is obtained with the high frequency signal HF in a weighted status, however this high frequency signal HF is present in a frequency band that is considerably higher than the clock mark reproduction signal S CM  frequency band. Accordingly as shown in FIG. 37A, the clock mark reproduction signal S CM  can be extracted by (see FIG. 25) the bandpass filter  71  with no effects whatsoever being exerted by this high frequency signal HF. The phase information can also be acquired with high accuracy from the zero cross point of this clock mark reproduction signal S CM  and satisfactory reproduction of the data clock reproduction signal DCK can be achieved. 
     Next, the fourth embodiment of this invention is described. The structure of the optical disk apparatus  10 C of the fourth embodiment is shown in FIG.  38 . The same reference numerals as in FIG. 36 are used in FIG. 38 so a detailed description is omitted here. 
     In the optical disk apparatus  10 B in FIG. 36, the laser beam was modulated by high frequency signal HF during the clock mark period T CM  however in the optical disk apparatus  10 C in FIG. 38, during the clock mark period T CM , the data clock signal DCK is used and modulation is performed at twice the frequency with the clock signal  2 DCK. 
     Consequently, in the optical disk apparatus  10 C, a doubler circuit  92  is provided to double the data clock signal DCK and acquire a data clock signal  2 DCK. The laser driver  18  is then supplied with this data clock signal  2 DCK. Also, during data writing in the optical disk apparatus  10 C, a control signal CT 3  is supplied to the laser driver  18  from the system controller  51  as shown in FIG. 39B, and the laser beam is modulated by the clock signal  2 DCK as shown in FIG. 39D during the clock mark period T CM . The laser beam power is normally controlled in record power P W  status as shown in FIG.  39 C. 
     Thus, when the laser beam is modulated by the clock signal  2 DCK during the preformat period T CM , the push-pull signal S PP  output during clock mark CM reproduction is acquired in a weighted status however the clock clark signal  2 DCK is in a much higher frequency band than the clock mark reproduction signal S CM . Accordingly, as shown in FIG. 39A, this lock mark reproduction signal S CM  can be extracted by the bandpass filter oc (see FIG. 29) while being affeted in no way whatsoever by the clock signal  2 DCK. Further, phase information can be obtained with high accuracy from the zero cross point, and a satisfactory reproduction of the data clock signal DCK achieved. 
     The optical disk apparatus  10 D, is provided just with a doubler circuit  92 . As can se seen in FIG. 36 in which the optical disk apparatus  10 B is also provided with an oscillator  91 , the optical disk apparatus  10 D has a simpler structure and is less expensive. Further, in the optical disk apparatus  10 C shown in FIG. 38 there is no switching between the record power and the reproduction power P R  so that compared to optical disk apparatus  10 A, the optical disk apparatus  10 C has the advantage of simple power control of the semiconductor laser. 
     The example in the above embodiments showed in the optical disk  11 , a groove  12 G wobbled only on one side however, the groove  12 G may also be wobbled on both sides. 
     Also, in the above-explained embodiment, the clock mark CM is preformatted on the wobbled side of the groove portion  12 G. However, the clock mark CM may be preformatted on the non-wobbled side of the groove  12 G, and moreover the clock marks CM may be preformatted on both sides of this groove  12 G. 
     Further in the above embodiments, the waveform numbers of the groove wobbles corresponding to the address information of “1” and “0” are respectively selected to be “4” and “3”, but need not be limited to these numbers. 
     Still further, in the above embodiments, the fixed pattern region of the recording region is provided to correspond to the recording position of the clock mark CM in an. one-to-one relationship. However, this fixed pattern region need not necessarily be positioned to correspond to the recording position of the clock mark CM. The total number of these fixed pattern regions may for instance be selected to be smaller than the clock marks CM. 
     Yet further in the above embodiments, the 2T fixed pattern signal is recorded in synchronization with the NRZI data in the fixed pattern region of the magneto-optical disk  11 . Alternatively, either a 1T fixed pattern signal or a 3T or higher fixed pattern signal may also be recorded. However it should be understood that when the pattern interval becomes small, the amplitude of the reproduction signal S MO  will decrease and the S/N ratio would deteriorate due to the MTF (Modulation Transfer Function). Conversely, when the pattern interval is extended, the fixed pattern region must be widened, in order for the edge numbers for phase comparison to be obtained as the same number, with the result that the data region into which the data can be recorded becomes narrow. 
     Even further, in the above embodiments in the ADIP decoder  60 , the demodulating process operation is carried out by utilizing a clock signal CK 24  having a frequency “fc” (=6 fa=8 fb) higher than the frequencies “fa” and “fb” of the wobble signals S WB  by a common frequency multiple, which corresponds to the data of the address information ADM of “1” and “0”. Alternatively, a similar demodulating process operation may be performed may be performed by utilizing a clock signal having a frequency higher than these frequencies “fa” and “fb” of the wobble signal S WB  by another common frequency multiple. 
     Still yet further, in the above embodiments, the unique idea of the present invention is applied to the magneto-optical disk apparatus  10 . Alternatively, this unique idea may similarly be applied to other types of optical disk apparatus capable of handling an optical disk in which address information is frequency-modulated, and the frequency-modulated signal is recorded as a groove wobble.