JP2001160245A - Optical information reproducing device - Google Patents

Abstract

PROBLEM TO BE SOLVED: To efficiently and precisely set a reproducing power even through it is very difficult to set the reproducing power by a conventional method. SOLUTION: The reproducing power of a semiconductor laser 1 is set to a value larger than the reproducing power in which a normalized value by the reproducing power of the laser 1 of the reproduced signal level reproduced from a magnetic wall moving type magneto-optical medium 5 becomes the maximum.

Description

DETAILED DESCRIPTION OF THE INVENTION

[0001]

The present invention relates to an optical information reproducing apparatus for reproducing information recorded on an information recording medium such as an optical disk,
In particular, the present invention relates to an apparatus for setting a reproduction power of a light source.

[0002]

2. Description of the Related Art In recent years, networks, digital cameras,
Opportunities for handling image data have increased dramatically due to the spread of digital video and the like. In particular, media and devices suitable for recording and reproducing moving image data have been strongly demanded, and research and development have been actively conducted. In the field of optical discs, research and development of optical discs and optical disc apparatuses suitable for handling digital moving image data have been actively conducted. As such a large-capacity optical disk and optical disk device, for example,
As disclosed in Japanese Patent Application Laid-Open No. 6-290496, there is a domain wall displacement reproducing system.

[0003] In the domain wall displacement reproducing method, as described in the same publication, a minute mark which cannot be resolved by the resolution of an optical head is formed by irradiating a light spot on a medium to form a temperature gradient on the medium. The mark is enlarged and reproduced in the track direction by moving the domain wall forming the mark. By using such a domain wall displacement reproduction method, it is possible to construct a large-capacity system that has never existed before. However, not only the domain wall displacement reproducing method but also a reproducing method using magnetic super-resolution uses a temperature distribution on a medium, and thus its characteristics depend on the reproducing power.

Japanese Patent Laid-Open Publication No. Hei 10-134354 discloses that a test pattern is recorded in a plurality of areas of a land portion or a groove portion with different light amounts, the test pattern is reproduced with different light amounts, and an error rate is obtained from a reproduced signal. Is calculated to calculate the combination of the recording light amount and the reproduction light amount in the case of the reproduction signal with the least error, and set the reproduction light amount as the optimum reproduction light amount.

Japanese Patent Laid-Open Publication No. Hei 8-63817 discloses that
In a super-resolution magneto-optical disk (magnetic super-resolution optical disk) apparatus for reproducing minute marks using a detection window formed by a temperature distribution on a recording medium, a long mark and a short mark are reproduced in advance, and a length at which jitter is minimized. A method is disclosed in which the amplitude ratio between the mark reproduction signal level and the short mark reproduction signal level is determined as a reference value, and the reproduction power is set so as to be the reference value. Therefore, in the publication, a plurality of reproduction power setting areas in which predetermined control data (a long mark and a short mark for calculating an amplitude ratio) are recorded are provided on the disk side, and control data is transmitted from a reproduction power setting area close to the reproduction area. The reading power is set by reading.

[0006]

However, in the case of a magnetic super-resolution optical disk, since minute marks are detected by using the temperature distribution on the medium, the reproduction characteristics are very sensitive to the reproduction power. Therefore, Japanese Patent Application Laid-Open No. H10-134354
When the reproducing power of the magnetic super-resolution medium is set by using the method disclosed in Japanese Patent Application Publication Is calculated and it is necessary to finely change the reproduction power in order to set the reproduction power of the reproduction signal with the least error. In addition, it takes a long time to calculate the error rate, which is very inefficient.

In the domain wall displacement reproducing method, the mark is enlarged and reproduced by moving the domain wall, and the magnitude of the reproduced signal is determined by the almost instantaneous movement of the domain wall. small. Therefore, in the case of the domain wall displacement reproducing method, a large change in the amplitude ratio cannot be obtained. However, there is a problem that the reproducing power cannot be set accurately.

An object of the present invention is to provide an optical information reproducing apparatus capable of setting a reproducing power efficiently and accurately in view of the above-mentioned conventional problems.

[0009]

SUMMARY OF THE INVENTION An object of the present invention is to provide an optical information reproducing apparatus for performing super-resolution reproduction by irradiating a recording medium capable of super-resolution reproduction with a reproduction light beam from a light source. Means for setting the reproduction power of the reproduction light beam of the light source to a value larger than the reproduction power at which the value standardized by the reproduction power of the light source of the reproduction signal level reproduced from the recording medium is maximum. This is achieved by an optical information reproducing apparatus characterized in that:

[0010]

Embodiments of the present invention will be described below. First, the principle of the present invention will be described. Here, a description will be given of an example of a super-resolution reproduction method in which a domain wall is moved to move a domain wall of a mark to reproduce a minute mark. Hereinafter, a recording medium that performs reproduction by moving the domain wall is referred to as a domain wall moving type medium. The domain wall displacement reproducing method is disclosed in Japanese Patent Application Laid-Open No. 6-290496, and will be briefly described. The domain wall displacement type medium includes at least first, second, and third magnetic layers as described in the publication, and the first magnetic layer is at a temperature near the ambient temperature as compared with the third magnetic layer. It is composed of a perpendicular magnetization film having a small domain wall coercive force and a large domain wall mobility. Also, the second
Is composed of a magnetic layer having a lower Curie temperature than the first magnetic layer and the third magnetic layer, and the third magnetic layer is a perpendicular magnetization film. The tracks of the recording medium are separated magnetically, and no domain wall is formed.

The minute mark is reproduced by irradiating the recording medium with a reproduction light spot. That is, due to the temperature distribution formed by the irradiation of the light spot on the recording medium, the exchange coupling between the first and second magnetic layers is cut off near the Curie temperature Ts of the second magnetic layer, and the first magnetic layer Moves to the higher temperature to the peak position of the temperature distribution. As a result, the minute mark is enlarged, and reproduction is performed by detecting a change in the plane of polarization of the reflected light from the enlarged mark. In this way, minute marks that cannot be resolved with the resolution of the optical head can be reproduced, and a large-capacity optical disk system can be constructed.

FIG. 1 is a diagram showing a temperature distribution and a light spot intensity distribution on a domain wall displacement type medium. The solid line shows the temperature distribution, and the broken line shows the light spot intensity distribution. X0 is the peak position of the light spot intensity distribution, and XT is the temperature peak T of the temperature distribution.
The position of p is indicated by coordinates in the track moving direction. Tc is the Curie temperature of the first magnetic layer. Here, when reproducing a minute mark exceeding the normal resolution of the optical system participating in the reproduction, the reproduction signal increases, the reproduction power increases, the temperature peak value exceeds the Curie temperature of the second magnetic layer, and the signal starts to move. The level rises sharply. Further, when the reproducing power is increased, the medium temperature in the region where the domain wall is moving, particularly near the temperature peak, approaches the Curie temperature of the first magnetic layer (moving layer). Further, when the reproducing power is further increased, the signal level in some regions exceeds the Curie temperature and the signal level decreases.

FIG. 2 is a diagram showing the temperature dependence of the Kerr rotation angle of the first magnetic layer. The vertical axis is the relative Kerr rotation angle, and the horizontal axis is the temperature. T = 0 corresponds to room temperature, and T = 1 corresponds to the Curie temperature of the first magnetic layer. As can be seen from FIG. 2, the Kerr rotation angle sharply decreases near the Curie temperature Tc of the first magnetic layer. Therefore, the Kerr rotation angle becomes smaller due to its temperature dependence near the Curie temperature Tc near the temperature peak, and when the reproducing power is further increased to exceed the Curie temperature, the Kerr rotation angle in the region becomes zero. Become. As a result, when the temperature peak Tp approaches the Curie temperature Tc, even if the reproduction power is increased, the decrease in the Kerr rotation angle due to the temperature dependency is offset, so that the signal level does not increase. The signal level starts to decrease.

Further, the noise from the domain wall displacement type medium increases as the reproducing power increases, and the peak temperature of the temperature distribution becomes T
Beyond s, domain wall motion starts and decreases as the domain wall motion region increases. When the reproducing power reaches a level at which recording is started (the peak temperature is about the Curie temperature of the third magnetic layer), it tends to increase again.

FIG. 3 is a diagram showing the dependence of the signal level and noise on the reproduction power. The vertical axis represents the signal level (carrier level C) and the noise level N, and the horizontal axis represents the reproduction power. The carrier level C is shown by a solid line, and the noise level N is shown by a broken line. When the reproduction power is increased, the reproduction power Pr2
, The noise level peaks, and the carrier level C peaks at the reproduction power Pr3. The noise level decreases after the reproduction power Pr2, and the carrier level starts to decrease after the reproduction power Pr3. Playback power is Pr
At 4, the noise level starts to increase again.

In the domain wall displacement type medium, the noise level decreases as the reproducing power approaches Pr3 from Pr3 to Pr4. Then, as the reproducing power further increases and approaches Pr4, the decrease in the carrier level exceeds the decrease in the noise level. As a result, it can be seen that there is a point between the reproduction powers Pr3 and Pr4 where the ratio of the noise level to the carrier level is minimized. Therefore, the reproduction power at that point is P
Let it be r1. The reproduction power Pr3 is a point where the increase in the signal level due to the increase in the reproduction power and the decrease in the signal level due to the temperature dependence of the Kerr rotation angle almost completely cancel each other. Therefore, assuming that the reproduction power at which the signal level normalized by the reproduction power is the maximum is Pr0, Pr0 <Pr3
<Pr4 holds.

In the present invention, based on such a principle, as shown in FIG. 4, the reproducing power Pr1 is set to a value larger than the reproducing power at which the signal level standardized by the reproducing power becomes maximum. Actually, the reproduction power P
r1 is set to Pr1 ≒ 1.4 × Pr0. In FIG. 4, the horizontal axis represents the reproduction power, and the vertical axis represents the carrier level standardized by the reproduction power. Pr0 is the reproduction power at which the signal level standardized by the reproduction power is the maximum, and Pr1 is the set reproduction power.

An embodiment of the present invention will be described based on the above principle. FIG. 5 is a diagram showing a configuration of one embodiment of the present invention. In FIG. 5, reference numeral 1 denotes a semiconductor laser as a recording / reproducing light source. Laser light emitted from the semiconductor laser 1 passes through the polarization beam splitter 2, is collimated by the collimator lens 3, and enters the objective lens 4. This incident light is condensed by the objective lens 4 and is irradiated on the magneto-optical medium 5 as a minute light spot. Magneto-optical medium 5
Is used to move the domain wall of a mark recorded on the medium 5 to enlarge the mark and reproduce recorded information. The reflected light from the magneto-optical medium 5 again enters the polarization beam splitter 2 via the objective lens 4 and the collimator lens 3. In the polarization beam splitter 2, the reflected light from the medium 5 is separated from the incident light from the semiconductor laser 1 and reflected to the Wollaston prism 7 side.
This reflected light is transmitted to the Wollaston prism 7 and the sensor lens 8.
, And is detected by the signal sensor 9. The detection signal of the signal sensor 9 is output to the reproducing circuit 15 and reproduced as a magneto-optical signal.

A part of the laser light of the semiconductor laser 1 is detected by the monitor sensor 6 and detected by the detection circuit 12 as a voltage signal. The detection signal of the detection circuit 12 is supplied to the comparator 13
Is compared with the reference signal from the reference signal generator 11, and a signal corresponding to the difference is output to the laser drive circuit 14. That is, the difference signal between the detection signal and the reference signal is
, The reproduction power of the semiconductor laser 1 is set so that the reference signal and the detection signal become equal. At this time, the controller 17 performs a process of determining a reference signal. That is, the reference signal from the reference signal generator 11 is sequentially changed, and the amplitude of the magneto-optical signal from the reproducing circuit 15 at each time is detected. The magneto-optical signal of the reproducing circuit 15 is taken into the controller 17 via an A / D converter (not shown), and the controller 17 stores the reference signal and the ratio of the reference signal to the magneto-optical signal amplitude (magneto-optical signal amplitude / reference signal) in the memory 16. To be stored. The controller 17 has a memory 16
, The reference signal having the maximum ratio between the reference signal and the magneto-optical signal amplitude is detected, and this is determined as the reference signal Vm.

Next, the controller 17 multiplies the reference signal Vm of the reference signal generator 11 by a predetermined value α to generate a reference signal α ·
The reproduction power of the semiconductor laser is set as Vm. In the present embodiment, α = 1.4 as described above. That is, the optical output of the semiconductor laser 1 is set so that the reference signal is 1.4 times the laser output at Vm. The value of α is determined experimentally. FIG. 6 shows the measurement results of the carrier level C and the jitter σ of the reproduction signal with respect to the reproduction power. As measurement conditions, a domain wall displacement type medium was used, the mark length was 0.15 μm, the linear velocity was 1.5 m / s, and the NA of the optical system was
Is 0.55, and the wavelength of the semiconductor laser 1 is 680 nm. In FIG. 6, the vertical axis represents the time corresponding to the mark length of 0.15 μm as T, and the jitter value as σ / T.
(Dashed line), carrier level C (dashed-dotted line), and carrier level C / Pr (solid line) specified by reproduction power.

As is clear from FIG. 6, the reproduction power at which the carrier level C / Pr specified by the reproduction power is the maximum is about 1.3 mW and the α / T is the minimum (that is, the medium performance can be maximized). Playback power is about 1.8m
W. Therefore, α = 1.8 / 1.3 ≒ 1.38, and α ≒ 1.4 was obtained as the optimum value in the experiment. Assuming that the jitter value can be increased up to 3% with respect to the detection window width (time corresponding to a mark length of 0.15 μm) from FIG. 6, if α = 1.1 to 1.6, the performance is secured. We can see that we can do it. Therefore, the reproducing power can be set near the maximum of the ratio between the carrier level and the noise level (corresponding to the point where the jitter value becomes the minimum), and the performance of the medium can be maximized.

Here, since the signal level of the reproduction signal of the domain wall motion reproduction system does not depend on the mark length as described above,
The signal for which the carrier level is to be detected at the time of setting the reproducing power is not limited to the signal level of the mark length when α is determined, but may be the envelope width of the signal group already recorded on the magneto-optical medium 5.

Next, it is also possible to control the reproducing power after setting the reproducing power. Setting the reproduction power to the optimum value is equivalent to setting the ratio of the domain wall motion region in the reproduction light spot. Therefore, if the carrier level C / Pr standardized by the reproducing power can be kept at the value at the time of setting the reproducing power, the ratio of the domain of the light spot within the domain wall movement region can be kept constant, and the performance of the medium is always maximized. It is possible to withdraw.

Specifically, after the reproduction power of the semiconductor laser 1 is set, if the amplitude of the magneto-optical signal corresponding to the set reproduction power is S ₀ , the reference signal generator 18 controls the reference signal from the reference signal generator 18 under the control of the controller 17. Generate S ₀ . During the reproduction of information from the magneto-optical medium 5, the comparator 19 monitors the amplitude of the magneto-optical signal from the reproducing circuit 15, and outputs a reference signal to the reference signal generator 18.
With the reference signal S ₀ . When the difference between the magneto-optical signal amplitude and the reference signal S ₀ exceeds a predetermined level, the controller 17 changes the reference signal Vm of the reference signal generator 11 by ΔVm,
The light output of the semiconductor laser 1 is changed by the operation of the comparator 13 and the laser drive circuit 14 accordingly.

When the optical output of the semiconductor laser 1 changes, the denominator of the carrier level C / Pr standardized by the reproduction power also changes. Therefore, when Vm changes to Vm + ΔVm, the optimum magneto-optical signal amplitude changes from S _0. S ₀ × (Vm + (Δ
Vm / Vm)) = S ₀ ′. Therefore, the controller 17 changes the reference signal Vm of the reference signal generator 11 by ΔVm and, at the same time, sets the reference value of the reference signal generator 18 to S ₀ '. The comparator 19 monitors the amplitude of the magneto-optical signal from the reproducing circuit 15, compares the reference signal S ₀ ′, and performs the same control. Therefore, when the reproducing power increases at the reproducing power setting position, the temperature near the light spot on the medium increases as described above, and the magneto-optical signal level decreases. Therefore, the reference signal of the reference signal generator 11 is reduced. The reproduction power of the semiconductor laser 1 is reduced. For example, when the level of the magneto-optical signal decreases due to factors such as an increase in the ambient temperature and an increase in the temperature on the medium, the reproducing power is reduced assuming that the reproducing power has relatively increased. As a result, the temperature on the medium decreases, and the magneto-optical signal level returns.

When the reproduction power is reduced at the reproduction power setting position, the temperature in the vicinity of the light spot on the medium decreases, and the level of the magneto-optical signal increases. Therefore, when the level of the magneto-optical signal increases, it is considered that the reproduction power has relatively decreased, and the reference signal is increased, so that the reproduction power of the semiconductor laser 1 is increased. As a result, the temperature on the medium increases, and the magneto-optical signal level returns. Here, the magneto-optical signal level uses the envelope width of the signal group actually reproduced. As described above, by controlling the reproduction power in real time, the carrier level C / Pr standardized by the reproduction power at all times can be kept constant.

FIG. 7 is a graph conceptually showing the relationship between the reproduction power and the reproduction signal level. The horizontal axis is the reproduction power, and the vertical axis is the carrier level specified by the reproduction power. As shown in FIG. 7, the signal level normalized by the reproduction power is ΔC /
When Pr is increased, the reproduction power is increased by ΔPr1 from Pr1. When the signal level decreases by ΔC / Pr2, the reproducing power is reduced by Pr2 from Pr1. By performing such control, the carrier level standardized by the reproduction power can be kept constant.

Here, when the difference between the magneto-optical signal level and the reference signal exceeds a predetermined level, the reproducing power of the semiconductor laser 1 is changed, so that the actual switching of the reproducing power is performed in accordance with the switching of the sector of the medium 5. Do. Further, according to the experiment by the inventor of the present application, Pr1 再生 1.
When 8 mW, ΔC / Pr1 and ΔC / Pr2 are about 10
%, Pr1 and Pr2 were equivalent to the output from the objective lens 4, and were ΔPr1 ≒ ΔPr2 ≒ 0.05 to 0.1 mW. Since ΔPr1 and ΔPr2 are much smaller than Pr1, ΔC / Pr1 and ΔC / Pr2 are
Equal to the signal change monitored by Therefore, the presence or absence of a change in the signal level specified by the reproduction power is determined by the reproduction circuit 15.
And 10% as a signal change monitored by That is, the reproduction circuit 1
When the magneto-optical signal from 5 changes by 10%, the reference signal Vm of the reference signal generator 11 changes by ΔVm. This makes it possible to keep the change in α / T within approximately 1%.

Although the change of the output of the semiconductor laser 1 is required when the change in the ambient temperature is the main factor, the objective lens 4 has been described as being eccentric to the recording medium or having access to the vicinity of the current reproduction position. It is possible to cope with a change in reproduction power when the medium is moved in the radial direction.

[0030]

As described above, according to the present invention, the reproduction signal level reproduced from the recording medium is set to a value larger than the reproduction power at which the value standardized by the reproduction power of the light source becomes the maximum. , It is possible to easily set the reproducing power and to set the reproducing power with high accuracy without requiring any processing such as finely changing the reproducing power or calculating an error rate. .

[Brief description of the drawings]

FIG. 1 is a diagram showing the temperature distribution on a medium and the intensity of a light spot when reproducing is performed using a domain wall displacement type medium.

FIG. 2 is a diagram showing the temperature dependence of the Kerr rotation angle of a first magnetic layer in a domain wall displacement type medium.

FIG. 3 is a diagram showing the reproduction power dependence of a carrier level and a noise level when a domain wall displacement type medium is used.

FIG. 4 is a diagram for explaining the principle of setting the reproduction power according to the present invention.

FIG. 5 is a diagram showing a configuration of an embodiment of the present invention.

FIG. 6 is a diagram showing a measurement result for determining α in the embodiment of FIG. 5;

FIG. 7 is a diagram showing a relationship between a reproduction power and a signal level at the time of reproduction power control in the embodiment of FIG. 5;

[Explanation of symbols]

 DESCRIPTION OF SYMBOLS 1 Semiconductor laser 2 Polarization beam splitter 3 Collimator lens 4 Objective lens 5 Domain wall displacement type magneto-optical medium 6 Monitor sensor 7 Wollaston prism 8 Sensor lens 9 Signal sensor 11, 13 Reference signal generator 12 Detection circuit 13, 19 Comparator 14 Laser Drive circuit 15 Reproduction circuit 16 Memory 17 Controller

Claims (3)

[Claims] 1. An optical information reproducing apparatus for performing super-resolution reproduction by irradiating a recording medium capable of super-resolution reproduction with a reproduction light beam from a light source, the reproduction signal level of the reproduction signal reproduced from the recording medium being Means for setting the reproduction power of the light beam for reproduction of the light source to a value larger than the reproduction power at which the value standardized by the reproduction power of the light source is maximum. . 2. The setting means sets: 1.1 × Pm <Pr <1.6 × Pm, where Pr is the reproducing power to be set and Pm is the reproducing power at which the standardized value is the maximum. 2. The optical information reproducing apparatus according to claim 1, wherein the reproducing power is set so as to satisfy the condition. 3. The optical information reproducing apparatus according to claim 1, wherein the recording medium is a domain wall moving type magneto-optical medium.