JP2002230815A - Disk recorder/player - Google Patents

Abstract

PROBLEM TO BE SOLVED: To provide a disk recorder/player which can always set optimum laser power according to the change of a disk temperature. SOLUTION: The disk recorder/player is provided with a laser drive circuit 15 which supplies a driving signal to an optical head 4 so as to adjust the power of a laser beam emitted from the optical head 4, an error-correcting circuit 11 for detecting the error rate of a reproduced signal, and a system controller 10 which controls the operation of a laser drive circuit during signal regeneration and signal record on the basis of the output of the error-correcting circuit 11. The system controller 10 optimizes the power of the laser beam during signal recording or signal regenerating so that the error rate does not exceed a specified value, and registers the relation between a disk temperature and an optimal laser power on a control table. Then, when seting the laser power, the optimal laser power according to the disk temperature is read from the control table.

Description

DETAILED DESCRIPTION OF THE INVENTION

[0001]

BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a disk recording / reproducing apparatus for irradiating a disk with laser light from an optical head to record a signal on the disk or reproduce a signal from the disk.

[0002]

2. Description of the Related Art Conventionally, rewritable, large-capacity, and highly reliable magneto-optical disks have been developed as recording media for disk recording / reproducing apparatuses. Widely used as memory. Particularly in recent years, FIG.
As shown in the figure, the land (17)
And the groove (18) are formed alternately, and the land (17) and the groove
Techniques have been developed to increase the recording density by recording signals in both (18).

The land (17) and the groove (18) meander (wobble) as shown in the figure, and the meandering frequency is FM-modulated at a predetermined center frequency. By controlling the rotation of the magneto-optical disk so that the detected wobble signal always has the center frequency, constant linear velocity control is realized. Further, the wobble signal is subjected to FM modulation as described above and contains various information (wobble information) such as address information. At the time of signal reproduction, various control operations are realized based on the wobble information. You.

In a disk recording / reproducing apparatus of the laser pulse magnetic field modulation type, a magneto-optical disk is irradiated with a laser beam when reproducing a signal, and the magneto-optical disk is also irradiated with a laser beam when recording a signal. Then, the magneto-optical disk is locally heated. Further, in a magneto-optical disk utilizing magnetic super-resolution, the laser power for signal reproduction is increased, and signal reading is started when the temperature of the beam spot area reaches a predetermined value. Since the laser power at the time of signal reproduction is set lower than the laser power at the time of signal recording, there is no possibility that the recorded signal will be damaged by the signal reproduction.

In a disk recording / reproducing apparatus, an optimum value exists for the laser beam power (recording power) at the time of signal recording and an optimum value for the laser beam power (reproduction power) at the time of signal reproduction. If the bit error rate deviates from the predetermined value, the bit error rate of the reproduction signal increases. If the bit error rate exceeds a predetermined value, normal reproduction operation becomes difficult (see FIG. 14).

Therefore, conventionally, at the time of system startup, a signal is reproduced while gradually changing the reproduction power, and an error rate is calculated, or the recording power is gradually increased, for a test track provided in advance on the magneto-optical disk. A method has been proposed in which a signal is recorded while changing the data rate, an error rate of the reproduced signal is calculated, and the optimum reproducing power and recording power that minimize the error rate are searched.

[0007]

However, in the case of a magneto-optical disk, the temperature of the disk gradually rises due to the irradiation of the laser beam, and the optimum recording power and the optimum reproducing power change accordingly. Therefore, even if the laser power is optimal at the time of starting the system, the laser power deviates from the optimal value in the subsequent normal operation, and there is a problem that normal signal recording and signal reproduction become difficult. still,
This problem can be solved by a method in which the temperature is constantly monitored and the laser power is optimized every time a temperature change occurs, but the arithmetic processing for the optimization is frequently repeated. This method has a problem that it is difficult to realize.

An object of the present invention is to provide a disk recording / reproducing apparatus which can always set an optimum laser power according to a change in disk temperature.

[0009]

A disk recording / reproducing apparatus according to the present invention comprises a laser drive circuit capable of supplying a drive signal to an optical head and adjusting the power of laser light emitted from the optical head; An evaluation data detection circuit for detecting evaluation data indicating the quality of the reproduction state is provided, and a control circuit for controlling the operation of the laser drive circuit based on the output of the evaluation data detection circuit. The control circuit includes a temperature detecting means for detecting the temperature of the disk, a laser power optimizing means for optimizing the power of the laser beam at the time of signal recording or signal reproduction so that the evaluation data does not exceed a specified value, Means for storing the relationship between the disk temperature and the optimum laser power, table registration means for registering the disk temperature and the optimum laser power in the table means, and optimum laser power deriving means for deriving the optimum laser power according to the disk temperature from the table means And with.

In the disk recording / reproducing apparatus of the present invention, the optimization of the laser power is performed at the time of start-up and during the normal operation, and the relationship between the disk temperature and the optimum laser power is stored in the table means. If the optimum laser power is already registered in the table, it is no longer necessary to optimize the laser power, and it is only necessary to read out and set the optimum laser power at that temperature from the table means. Therefore, the load of arithmetic processing is reduced as compared with a disk recording / reproducing apparatus that optimizes laser power every time a temperature change occurs.

In a specific configuration, the laser power optimizing means executes laser power optimization each time the disk temperature changes by a predetermined temperature, and the table registering means stores the temperature obtained from the laser power registering means and the optimum laser power. Registration processing means for registering the power in the table means, and a laser at each temperature in a temperature range between the temperature at which the optimum laser power is already registered in the table means and the temperature at which the laser power optimization is newly performed. Arithmetic processing means for calculating the optimum value of the power by interpolation.

According to the specific configuration, the optimization of the laser power is performed every time the disk temperature changes by a predetermined temperature, and for the temperature at which the optimization of the laser power is not performed, the optimum laser at a temperature near the temperature is optimized. Since the optimum value is calculated from the power by interpolation, the amount of arithmetic processing required to register all data (relationship between temperature and optimum laser power) in the table means is greatly reduced. Incidentally, even by the interpolation processing, it is possible to obtain a substantially optimum laser power which does not hinder the recording and the reproduction of the signal.

In a more specific configuration, the table registration means has already been obtained by optimization or interpolation for a temperature which has not been optimized by the laser power optimization means or interpolated by the arithmetic processing means. Approximate value calculating means for calculating an approximate value of the optimum laser power based on the optimum laser power at the vicinity temperature and predetermined temperature gradient data indicating a ratio of the change of the optimum laser power to the temperature change.

According to this specific configuration, the temperature at which the optimum laser power has not yet been calculated by the optimization by the laser power optimizing means or the interpolation by the arithmetic processing means is first obtained by optimization or interpolation. An approximate value of the optimum laser power is calculated based on the optimum laser power at the vicinity temperature and predetermined temperature gradient data indicating a rate of change of the optimum laser power with respect to the temperature, and the relationship between the temperature and the approximate value of the optimum laser power is calculated. Is stored in the table means. Thereafter, the temperature becomes a temperature at which the laser power has not been optimized by optimization or interpolation, and when the optimum laser power is calculated at that temperature, the approximate value is replaced by the optimum laser power. Then, an interpolation process using the optimum laser power at that temperature is further performed, and the table means is updated. Therefore,
The optimum laser power at each temperature or its approximate value is always registered in the table means, and the approximate value is gradually replaced with the optimal value.

Here, the principle of laser power optimization in the disk recording / reproducing apparatus according to the present invention will be described. In signal reproduction, for example, as shown in FIG. 15, the reproduction power changes to change the error rate of the reproduction signal in a quadratic curve. For example, in the characteristic curve shown by the solid line, the error rate is optimized to be the minimum value. The reproduction power Pr exists, and the laser power at the time of signal reproduction needs to be set between the lower limit reproduction power Prmin and the upper limit reproduction power Prmax, which are two limit values at which the error rate becomes lower than the specified value. . Similarly, for signal recording, there is an optimum recording power Pw at which the error rate becomes the minimum value, and the laser power at the time of signal recording is the two limit values at which the error rate of the reproduced signal falls below the specified value. A certain lower limit recording power Pwmin and an upper limit recording power P
It must be set between wmax.

FIG. 17 shows the ranges of the reproduction power Pr and the recording power Pw in which the error rate is below the specified value, respectively.
In setting w, if it is set to an arbitrary value within this range, it is considered that there is no problem in signal recording and reproduction,
Since the characteristics shown in FIG. 17 fluctuate due to the warpage of the disk or the like, it is desirable to set the reproduction power and the recording power within the range as close to the center position as possible. Therefore, for example, as a method of optimizing the reproduction power, an average value of the lower limit reproduction power Prmin and the upper limit reproduction power Prmax at which the error rate falls below a specified value is calculated, and the result is determined as the optimum reproduction power. A method can be adopted.

However, as shown in FIG. 17, the reproduction power Pr at which the error rate falls below the prescribed value is the recording power Pw at which the error rate falls below the prescribed value.
For example, the recording power Pw is 6.5 mW or more.
In the range of 8.0 mW, the limit reproduction power Pr at which the error rate falls below the specified value changes according to the recording power. Therefore, within this recording power range, the lower limit recording power P at which the error rate falls below the specified value.
When the average value of wmin and the upper limit recording power Pwmax is defined as the optimum reproduction power, the value of the optimum reproduction power is as shown in FIG.
It is a position greatly deviated from the center position of the range shown in
If the characteristics shown in FIG. 17 fluctuate, the reproduction power may greatly deviate from the optimum value, and the error rate may exceed the specified value.

Therefore, in the present invention, in order to set the reproducing power and the recording power to the values at the center positions as much as possible in the range shown in FIG.
First, an optimum reproduction power is calculated by searching for a lower limit reproduction power Prmin at which the error rate falls below a specified value, and then adding a predetermined value to the searched lower limit reproduction power Prmin.

Here, the predetermined value is an area in which the reproduction power does not depend on the recording power in the relationship shown in FIG. 17, that is, the maximum reproduction power of 2.56 mW and the minimum reproduction power of 1.80 mW when the recording power is 8.0 mW or more. 0.36 mW, which is a half of the difference of 84 mW, or a value close to it (for example, 0.4 mW) can be adopted. As a result, an optimum value for the reproduction power that does not depend on the recording power can be obtained.

As shown in FIG. 15, when the variation characteristic of the error rate with respect to the reproduction power changes from the solid line to the broken line or the chain line, the optimum value of the reproduction power becomes Pr.
Is changed to Pr 'or Pr ", the lower limit reproduction power Prmin is accordingly changed to Prmin' or Prmi.
n ", and the difference between the optimum values Pr, Pr 'and Pr" and the lower limit reproduction powers Prmin, Prmin' and Prmin "becomes a substantially constant value N, so that the lower limit reproduction power Pr
By adding this difference N to min, Prmin 'and Prmin ", optimum reproducing powers Pr, Pr' and Pr" can be obtained respectively.

Similarly, instead of adding the predetermined value N to the lower limit reproduction power Prmin and multiplying the lower limit reproduction power Prmin by a predetermined value α, the accurate optimum reproduction powers Pr, Pr 'and P
r ″ can be obtained.

[0022]

According to the disk reproducing apparatus of the present invention, it is possible to always set the optimum laser power with a relatively small amount of arithmetic processing regardless of the disk temperature.

[0023]

DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENTS A preferred embodiment of the present invention applied to a disk recording / reproducing apparatus using a magneto-optical disk as a recording medium will be specifically described with reference to the drawings. As shown in FIG. 1, a disk recording / reproducing apparatus according to the present invention includes a spindle motor (2) for rotating and driving a magneto-optical disk (1). A temperature sensor (16) is mounted near the magneto-optical disk (1).

As a signal reproducing system, a laser driving circuit (1
5), an optical head (4), a reproduction signal amplification circuit (5), a reproduction signal detection circuit (7), and an error correction circuit (11). At the time of signal reproduction, the laser drive circuit (15) controls the optical head (4). Is driven to irradiate the magneto-optical disk (1) with laser light. On the other hand, as a signal recording system, a magnetic head drive circuit (14)
And a magnetic head (3), and at the time of signal recording, the laser drive circuit (15) and the optical head (4) operate to locally heat the magneto-optical disk (1). Further, as a control system, a servo circuit (6), an external synchronization signal generation circuit
(8), a system controller (10), a memory (9), a delay circuit (12), and a timing pulse generation circuit (13).

The optical head (4) irradiates a laser beam to the magneto-optical disk (1) and detects the reflected light as an optical signal and a magneto-optical signal. The reproduction signal amplification circuit (5) is an optical head
After amplifying the optical signal and magneto-optical signal obtained from (4),
A focus error signal and a tracking error signal included in the optical signal are supplied to a servo circuit (6). The reproduction signal amplification circuit (5) supplies an optical signal detected due to the discontinuous area formed at a constant interval in the groove of the magneto-optical disk (1) to the external synchronization signal generation circuit (8). At the same time, a magneto-optical signal is supplied to a reproduction signal detection circuit (7).

The external synchronizing signal generation circuit (8) generates an external synchronizing signal and supplies it to the servo circuit (6) and the delay circuit (12). The servo circuit (6) executes a focus servo and a tracking servo with respect to an actuator (not shown) mounted on the optical head (4) based on the focus error signal and the tracking error signal, and based on an external synchronization signal. The rotation of the spindle motor (2) is controlled.

The reproduction signal detection circuit (7) supplies the detected reproduction signal to the error correction circuit (11), and the error correction circuit (11)
Demodulates the reproduction signal, detects an error in the reproduction data obtained thereby, corrects the error, and outputs the corrected reproduction data to the subsequent circuit. The delay circuit (12) creates a synchronization signal in which the phase of the external synchronization signal is delayed by a predetermined time, and outputs the synchronization signal to the timing pulse generation circuit (13). When recording a signal, the timing pulse generation circuit (13) uses the recording data modulated by a predetermined method and a delay circuit.
Receiving the synchronization signal input from (12), the
Generate a pulse signal for applying an alternating magnetic field to (1),
A pulse signal (write clock) for irradiating the magneto-optical disk (1) with pulse light is generated and supplied to the laser drive circuit (15). At the time of signal reproduction, the reproduction signal detection circuit (7)
The reproduction analog signal is converted into a digital signal based on the synchronization signal (read clock) from the delay circuit (12).

The magnetic head drive circuit (14) generates a drive signal for the magnetic head (3) based on the pulse signal from the timing pulse generation circuit (13). Magnetic head (3)
Applies an alternating magnetic field to the magneto-optical disk (1) based on a drive signal from the magnetic head drive circuit (14). The laser drive circuit (15) drives a semiconductor laser (not shown) provided in the optical head (4) based on a pulse signal from the timing pulse generation circuit (13). The optical head (4) generates a laser beam based on a drive signal from the laser drive circuit (15) and irradiates the magneto-optical disk (1).

The system controller (10) controls the operation of the delay circuit (12) based on the external synchronization signal obtained from the external synchronization signal generation circuit (8). Further, the system controller (10) calculates a bit error rate based on the error correction information obtained from the error correction circuit (11), and controls the operation of the laser drive circuit (15) according to the result. Furthermore, the system controller (10) includes a temperature sensor (16).
Are stored in a management table in the memory (9), and the optimum read power and the optimum write power obtained in the test read and test write described later are stored in a management table. To control the laser power.

The laser drive circuit (15) adjusts the power of the laser beam emitted from the optical head (4) at the time of signal reproduction according to the laser power control signal Cp supplied from the system controller (10) as described later. I do. In the management table, as shown in FIG. 5, for each temperature, read power Pr, write power Pw, flag TestRW indicating whether test read / write has been executed, and flag indicating whether interpolation processing described later has been completed , And a flag indicating whether the temperature has actually been experienced.

FIG. 2 shows the overall flow of the procedure executed by the system controller (10). First, when a new magneto-optical disk is inserted in step S1,
In step S2, after clearing the previous management table, a reference table defining a reference value (initial value) of the relationship between the temperature and the laser power (Pr or Pw) is created. Next, in step S3, an initial temperature T_initial is detected. In step S4, a predetermined reference temperature Tdef, reference laser powers Pwdef and Prdef, and an initial temperature T_initial are calculated.
Find the laser power at startup.

Thereafter, in step S5, the initial temperature T_
Initial is set to the current temperature T and the internal temperature held by the system, and the test read / write and management table update routine of step S6 is executed. Test lead /
In the write and management table update routine, FIG.
In step S21, a test read and a test write (TestRW) are performed using a predetermined test track as shown in FIG.
To calculate the optimum laser powers Pr and Pw.
Then, in step S23, based on the calculation result,
The laser powers Pr and Pw at the temperature T specified in the management table are updated.

Next, in step S24, the TestRW term for the temperature at which the laser power was optimized is checked. Subsequently, in step S25, TestR
Using the data on the two temperatures checked in the W term, the optimum laser powers Pr and Pw are derived by interpolation processing for each temperature between these two temperatures. Then, in step S26, a check is made on the interpolated term regarding the temperature at which the interpolation processing has been performed, and
The management table update procedure ends.

For example, as shown in FIG. 6, when the relationship between the disk temperature and the initial value of the laser power, that is, the gradient of the change in the laser power with respect to the disk temperature (hereinafter referred to as the temperature gradient) is defined, When the temperature is 25 ° C. and the optimum laser power calculated by performing the test read / write is “62”, the initial value “64” of the laser power is updated to “62”. Next, in the interpolation process, the laser power at other temperatures is reduced by the same value “2” with the laser power at 25 ° C. as a base point, thereby performing the interpolation while maintaining the temperature gradient, and setting the management table. Update it. FIG. 7 shows an example in which the relationship between the disk temperature and the initial value of the laser power is updated by test reading / writing at 25 ° C. Thus, the management table is updated while keeping the temperature gradient constant.

Thereafter, at the time of normal reproduction, first, at step S7 of FIG. 2, the disk temperature T is detected, and at step S8
Then, it is determined whether or not the disk temperature has risen by 5 ° C. or more.
, The system temperature T_sys is updated to the temperature T. Next, in step S10, it is determined whether or not the temperature is the temperature already experienced in the management table. If the determination is no, the test read / write shown in FIG. And a management table update routine is executed.

For example, in the example of FIG. 6, when the first test read / write is performed at 30 ° C., the optimum laser power obtained by the test read / write is “5”.
9 ”, the laser power“ 57 ”is updated to“ 59 ”, and the laser power between 25 ° C. and 30 ° C. is obtained by interpolation processing (linear interpolation).
For the above temperature range, an interpolation process for keeping the temperature gradient constant is performed, and the management table is updated. FIG.
Indicates a state in which the management table has been updated by the test read / write.

Further, the second test read / write
When the test is performed at 5 ° C., the optimum laser power obtained by the test read / write as shown in FIG.
When the power is 0, the laser power “54” is updated to “50”, and the laser power between 30 ° C. and 35 ° C. is obtained by an interpolation process (linear interpolation). 9 shows a state in which the management table is updated by performing the interpolation processing for keeping the temperature gradient constant, and updating the management table by the test read / write.

In this way, each time a temperature change of 5 ° C. or more occurs, test read / write is executed, an optimum laser power at that temperature is obtained, and an interpolation process using the data is executed. , The management table will be updated. When all the experienced items in the management table are checked, in the subsequent normal operation, the read power P is referred by referring to the relationship between the temperature and the laser power stored in the management table.
r and the write power Pw are set, and signal recording and reproduction are performed.

That is, in the normal operation, after detecting the disk temperature in step S31 as shown in FIG. 4, it is determined in step S32 whether or not a recording / reproducing request has been issued. At this time, the management table is referred to in step S33, and in step S34, the laser powers Pr and Pw according to the temperature at that time are set. Then, in step S35, the recording and reproducing operations are executed, and the procedure ends.

Next, a method for optimizing the reproduction power will be described. In the present embodiment, in the test read for determining the optimum reproduction power, in order to search the lower limit value Prmin of the smaller one of the two limit values of the reproduction power at which the error rate becomes lower than the specified value. , FIG. 13 and FIG. That is,
Assuming the three states shown in FIG. 13 based on the initial value of the reproducing power, when the reproducing power is lower than the lower limit value as in A, the reproducing power is increased, and as in B, the reproducing power is lower and upper limit values. During the time, lower the playback power, C
When the reproducing power is higher than the upper limit value as shown in FIG. 14, the reproducing power is lowered to change the reproducing power to the lower limit value Prmin shown in FIG. Thereafter, the optimum reproduction power Pr is obtained by adding a predetermined value N to the reproduction power.

In order to distinguish between the states A and C in FIG. 13, the present embodiment employs a procedure utilizing the following principle. That is, the signal recorded on the magneto-optical disk has a data format in which a plurality of frames are arranged in chronological order, each frame is provided with a header portion, and each header portion has a short length as shown in FIG. A first reference signal of a single frequency having a period (2T) and a second reference signal of a single frequency having a long period (8T) are recorded, and the amplitude W1 of the reproduction signal of the first reference signal and the second reference signal are recorded. The ratio (W2 / W1) of the amplitude W2 of the reproduced signal of the two reference signals is as shown in FIG.
It increases as the reproduction power Pr increases. Therefore, when the ratio is lower than the predetermined set value, FIG.
If the ratio is lower than a predetermined set value, the state of C in FIG. 13 can be determined.

FIG. 10 shows a specific procedure for optimizing the reproduction power by the test read for the groove of the test track provided in advance on the magneto-optical disk. First, at step S42 in FIG.
An initial value is set as w, and recording on a test track is performed in step S43. Next, in step S44, an initial value is set as the reproduction power Pr, and
At 45, the test track is reproduced, and the quality of the reproduction is determined based on whether the error rate at that time exceeds a threshold value. Here, when it is determined to be OK, it is the state of B in FIG. 13, so the reproduction power Pr is reduced by the unit power ("1") in step S46, and the reproduction of the test track is performed again in step S47. Do,
After determining the quality of the reproduction, the process returns to step S46, and the same procedure is repeated.

As a result, if it is determined as NG in step S47, the flow shifts to step S48 to set the reproduction power Pr
Is increased by a unit power (“1”) as the lower limit value Pr1, and in step S49, the lower limit reproduction power Pr
A predetermined value N (= 0.4 mW) is added to 1 to obtain the optimum reproduction power Pr_opt, and the procedure is terminated. In determining the optimum reproduction power Pr_opt, the lower limit reproduction power P
It is also possible to adopt a method of multiplying r1 by a predetermined value α. Here, the predetermined value α can be determined in advance as a value depending on the system.

On the other hand, when it is determined as NG in step S45, it is in the state of A or C in FIG.
19 is determined based on the principle described with reference to FIG. That is, in step S50 of FIG.
It is determined whether the ratio (W2 / W1) of the reference signal is greater than the set value A, thereby recognizing the direction in which the reproduction power is changed. Note that the ratio of the reference signal (W2 /
Instead of W1), it is also possible to recognize the direction in which the reproduction power is changed depending on whether or not the difference (W2−W1) between the reference signals exceeds a set value.

When the determination in step S50 is affirmative, the state is as shown in FIG. 13C, so that the flow shifts to step S51 to reduce the reproduction power Pr by a predetermined value n. It is determined whether or not the reproduction power Pr is higher than the set lower limit value Pr_min. If the determination is yes here, the process proceeds to step S53,
The reproduction of the test track is performed to determine the quality of the reproduction. When it is determined as NG in step S53, the process returns to step S51 to repeat the process of reducing the reproduction power Pr by the predetermined value n. As a result, in step S53, O
If it is determined to be K, it has changed to the state of B in FIG.
The process shifts to step S46 to obtain the optimum reproduction power Pr_opt by executing the above-described procedure, and ends the procedure.

When it is determined NO in step S50, the state is as shown in FIG. 13A, and the flow shifts to step S57 to increase the reproduction power Pr by the unit power ("1"). In S58, it is determined whether or not the reproduction power Pr is smaller than the set upper limit value Pr_max. If the determination is yes here, the process proceeds to step S59, where the test track is reproduced, and the quality of the reproduction is determined. When it is determined as NG in step S59, the process returns to step S57, and the process of increasing the reproduction power Pr is repeated. As a result, when it is determined to be OK in step S59, the process proceeds to step S60, in which the reproducing power Pr at that time is set to the lower limit value Pr1, and then the process proceeds to step S60.
49, the lower limit reproduction power Pr1 is set to the predetermined value N
(= 0.4 mW) to obtain the optimum reproduction power Pr_opt, and the procedure ends.

When it is determined NO in step S52 or S58, the process proceeds to step S54,
After increasing the recording power Pw by the predetermined value n, the process proceeds to step S55, where the recording power Pw is increased to the set upper limit value Pw_
It is determined whether the value is smaller than max. If the determination is yes, the process proceeds to step S43, and the process proceeds to the test track write procedure. If the determination is no, the alarm “ NG "and the test track is registered as NG.

The optimum read power Pr_opt can be obtained by the same procedure for the test read for the land of the test track.

In determining the optimum recording power, a method similar to the above-described reproducing power optimizing method can be used. FIG. 11 shows a specific procedure for optimizing the recording power by this method. After the test read is completed, the initial value of the recording power that is not optimal but recordable,
In a state where the optimum reproducing power has been determined, first, in step S63, the recording power Pw is set to an initial value, and in step S64, recording and reproduction with respect to the test track are performed to determine the quality of the reproduction. If it is determined as NG here, an alarm "NG" is issued in step S65, and the test track is registered as NG. or,
During the operation, the recording power is kept at the initial value.

On the other hand, when it is determined that the recording power Pw is OK in step S64, the recording power Pw is reduced by the unit power "1", and in step S67, it is determined whether the recording power Pw is larger than the set lower limit value Pw_min. If not, the process proceeds to step S65 to issue an alarm "NG" and register the test track as NG. During the operation, the recording power is kept at the initial value. When it is determined to be Yes in step S67,
In step S68, recording and reproduction are performed on the test track to determine the quality of the reproduction. Here, if it is determined to be OK, the process proceeds to step S69, after changing the write data or shifting the write position, returns to step S66, and repeats the procedure for reducing the recording power. Thereafter, when it is determined as NG in step S68, the process proceeds to step S70, in which the unit power “1” is added to the recording power Pw at that time, and the lower limit value Pw1 is set.
After that, the flow shifts to step S71, in which a predetermined value N is added to the lower limit recording power Pr1, to obtain the optimum recording power Pw_opt, and the procedure ends. Incidentally, in determining the optimum recording power Pw_opt, a method of multiplying the lower limit recording power Pw1 by a predetermined value α can be adopted. Here, the predetermined value α can be determined in advance as a value depending on the system.

In order to determine the optimum recording power, FIG.
The relationship between the recording power and the bit error rate is shown in FIG.
A method of approximation by a quadratic curve can be adopted. For example, using a test track provided in advance on a disc, a signal is recorded on the test track with a different laser power, and then the signal is reproduced with an appropriate laser power, and the reproduced signal is reproduced. Detect the error rate. As a result, as shown in FIG.
And the relationship between the laser power (recording power) and the error rate at P3 is plotted. The relationship can be approximately represented by a quadratic curve, and the quadratic curve is uniquely determined if coordinate values at at least three points are determined. Therefore, a quadratic curve representing the relationship between the laser power and the error rate can be obtained using the values of the laser power and the error rate at the three points P1, P2, and P3, and as shown in FIG. The laser power corresponding to the peak of the curve is the optimum laser power Pwo that minimizes the error rate.

FIG. 12 shows a procedure for optimizing recording power based on quadratic curve approximation. In the state where the initial value of the recording power which is not optimal but is recordable and the optimal reproduction power are determined after the test read is completed, first, in step S83, the recording power Pw is set to the initial value.
In step S84, recording and reproduction are performed on the test track to determine the quality of the reproduction. If it is determined as NG here, an alarm “NG” is issued in step S85, and the test track is registered as NG.
During the operation, the recording power is kept at the initial value.

On the other hand, if it is determined in step S84 that the data is OK, the recording power Pw1 and the bit error rate BER at that time are stored in the memory. Next, step S8
At 7, the recording power Pw is reduced by a predetermined value n,
In step S88, recording and reproduction are performed on the test track, and the quality of the reproduction is determined. Here, when it is determined to be OK, the procedure returns to step S87, and the procedure for lowering the recording power is repeated. As a result, step S88
When it is determined that the recording power Pw2 is NG, the process proceeds to step S89, and the NG recording power Pw2 and the bit error rate BER are stored in the memory.

Subsequently, in step S90, after increasing the recording power Pw by a predetermined value n, recording and reproduction are performed on the test track in step S91 to determine the quality of reproduction. Here, when it is determined to be OK, the procedure returns to step S90, and the procedure for increasing the recording power is repeated. As a result, if it is determined in step S91 that it is NG, the process proceeds to step S92, and the NG recording power Pw3 and bit error rate BER are stored in the memory. Thereafter, in step S93, the three data points (Pw1, BER1), (Pw2, BER) stored in the memory are stored.
2) Using (Pw3, BER3), the relationship between the laser power and the bit error rate is approximated by a quadratic curve, and the recording power serving as the central axis of the curve is calculated as the optimum value Pw_opt. Then, in step S94, the optimum value Pw_opt is set as the recording power Pw, and the procedure ends.

As described above, according to the disk recording / reproducing apparatus of the present invention, in the test read for determining the optimum reproducing power, the optimum reproducing power independent of the recording power is determined in the state where the optimum recording power is unknown. It is possible to determine the optimum recording power in a smaller number of steps by using the optimum reproduction power obtained in the test read in the test write for determining the optimum recording power after that. As a result, it is possible to set high-precision optimal reproduction power and optimal recording power through simple procedures throughout the entire system. As a result, after starting the system, it is possible to shift to signal reproduction or signal recording in a short time, and it is possible to accurately perform signal reproduction and signal recording.

[Brief description of the drawings]

FIG. 1 is a block diagram illustrating a configuration of a disk recording / reproducing apparatus according to the present invention.

FIG. 2 is a flowchart showing a procedure of laser power control in the apparatus.

FIG. 3 is a flowchart of a test read / write and management table update routine.

FIG. 4 is a flowchart showing a control procedure of a recording / reproducing operation in a normal operation.

FIG. 5 is a table illustrating a data structure of a management table.

FIG. 6 is a chart showing a specific example of management table update.

FIG. 7 is a graph showing the relationship between the temperature of the management table and the laser power at the time of startup.

FIG. 8 is the same graph as that of the management table in the first test read / write.

FIG. 9 is a graph of the management table in the second test read / write according to the first embodiment;

FIG. 10 is a flowchart showing a procedure for optimizing the reproduction power.

FIG. 11 is a flowchart illustrating a procedure of recording power optimization.

FIG. 12 is a flowchart illustrating another procedure of recording power optimization.

FIG. 13 is a graph illustrating a procedure for optimizing the reproduction power.

FIG. 14 is a graph showing a relationship between a reproduction power and an error rate.

FIG. 15 is a graph illustrating the principle of reproduction power optimization.

FIG. 16 is a graph illustrating the principle of recording power optimization.

FIG. 17 is a diagram illustrating a relationship between recording power and reproduction power satisfying a specified value.

FIG. 18 is a waveform diagram of two reference signals written in a header section of a reproduction signal.

FIG. 19 is a graph showing the relationship between the amplitude ratio of the reproduction signals of both reference signals and the reproduction power.

FIG. 20 is an enlarged perspective view showing lands and grooves formed on the magneto-optical disk.

[Explanation of symbols]

 (1) Magneto-optical disk (3) Magnetic head (4) Optical head (7) Reproduction signal detection circuit (9) Memory (10) System controller (11) Error correction circuit (15) Laser drive circuit

Continuation of the front page (51) Int.Cl. ⁷ Identification FI FI Theme Court II (Reference) H01S 5/068 H01S 5/068 (72) Inventor Shuji Baba 2-5-5-1 Keihanhondori, Moriguchi-shi, Osaka, Sanyo F term in Denki Co., Ltd. (reference) 5D075 AA03 CD11 5D090 AA01 BB10 CC01 CC04 GG33 JJ07 KK03 5D119 AA09 AA23 BA01 BB05 HA30 HA45 HA54 5F073 BA06 EA15 GA02 GA14

Claims (3)

[Claims] In a disk reproducing apparatus for irradiating a laser beam to a disk from an optical head to record a signal on the disk or to reproduce a signal from the disk, a drive signal is supplied to the optical head so that the optical head A laser drive circuit capable of adjusting the power of the emitted laser light, an evaluation data detection circuit for detecting evaluation data indicating the quality of the signal reproduction state, and an operation of the laser drive circuit based on the output of the evaluation data detection circuit A temperature detecting means for detecting the temperature of the disk, and optimizing the power of the laser beam during signal recording or signal reproduction so that the evaluation data does not exceed a specified value. Laser power optimizing means, table means for storing the relationship between disk temperature and optimum laser power, and disk temperature and optimum A disk recording / reproducing apparatus comprising: a table registration unit for registering a laser power; and an optimum laser power derivation unit for deriving an optimum laser power according to a disk temperature from the table unit. 2. The laser power optimizing means executes laser power optimization each time the disk temperature changes by a predetermined temperature, and the table registration means stores the temperature obtained from the laser power registration means and the optimum laser power in a table. Registration processing means for registering in the means, and optimization of the laser power at each temperature in a temperature range between the temperature at which the optimum laser power is already registered in the table means and the temperature at which the laser power optimization is newly performed. 2. The disk recording / reproducing apparatus according to claim 1, further comprising an arithmetic processing means for calculating a value by interpolation. 3. The table registration means further includes, for a temperature which has not been optimized by the laser power optimizing means or interpolated by the arithmetic processing means, an optimum laser of a nearby temperature which has already been obtained by optimization or interpolation. 3. A disk recording / reproducing apparatus according to claim 2, further comprising an approximate value calculating means for calculating an approximate value of the optimum laser power based on the power and predetermined temperature gradient data indicating a ratio of a change of the optimum laser power to a temperature change. apparatus.