JP4957472B2 - Optical pickup device, optical recording / reproducing device, and gap control method - Google Patents

Description

  The present invention relates to an optical pickup device, an optical recording / reproducing device, and a gap control method applied to an optical recording medium using near-field light.

  In recent years, in optical recording media such as optical disks and optical memory cards, near-field where light leaks from the interface when the distance between objects falls below a certain distance in order to achieve high recording density and high resolution (near field) A recording / reproducing system using light (also referred to as evanescent wave) has attracted attention. In this near-field optical recording / reproducing system, the gap between the near-field light irradiating means such as a lens and the surface of the optical recording medium is typically set to 1/2 to 1/5 of the wavelength of light used for recording or reproducing. It needs to be controlled to a very small extent.

As a condensing optical system for generating near-field light, an objective lens having a high numerical aperture such as an aspheric lens and a solid immersion lens so-called SIL (Solid Immersion Lens) is provided between the objective lens and the optical recording medium. ) Is included. When this SIL is used, the distance (gap) between the SIL and the surface of an optical recording medium such as an optical disk is set to a distance at which near-field light is generated, as described above, from 1/2 to 1/5 of the wavelength of light. It is necessary to maintain the following level. Further, in this case, it is necessary to control the attitude of the SIL so as to follow the surface vibration of the optical recording medium, and in the case of a disk-shaped optical recording medium, so-called disk surface vibration. For this purpose, for example, a control method has been proposed in which a gap is detected using a total reflected return light amount and maintained at a desired gap (see, for example, Patent Document 1).
This control method utilizes the fact that the total reflected return light amount and the gap are in a proportional relationship at the distance where near-field light is generated. That is, a method is adopted in which the total reflected return light amount is used as a gap error signal, the servo loop system is stabilized by a phase compensation filter to form a feedback servo loop, and the gap is kept constant.

  As an example, a target value to be maintained at a distance where near-field light is generated is, for example, 20 nm, an allowable deviation is 5 nm, an allowable surface shake amount is 40 μm, an optical recording medium is in a disk shape, and a disk rotational speed is 3000 rpm (rotational speed / minute). ), The required bandwidth is 8 kHz or more. In practice, however, disturbance caused by disk rotation has a strong rotational synchronization component, and even if a band of 8 kHz or more is secured, it is difficult to control the gap with high accuracy.

  In order to solve this problem, methods using repeated servos have been proposed (see, for example, Patent Document 2 and Non-Patent Document 1). The repeated servo holds an error signal for one rotation in an external memory and applies it as a feedforward signal to a gap error signal of a conventional feedback servo loop, and a gain having a peak in the rotation frequency component is obtained.

JP 2001-76358 A JP 2006-31589 A

  However, when the repetitive servo as proposed in Patent Document 2 and Non-Patent Document 1 is used, disturbance of the rotational frequency component can be effectively removed, but external disturbance for one rotation is maintained. Memory is required. For this reason, in order to read the memory, it is necessary to obtain position signals on the same circumference. As a method for obtaining this position signal, it is necessary to install a rotary encoder on a spindle motor that rotates the disk, record rotational position information on the disk, and provide a separate detector to read the position signal.

  On the other hand, if there is a method for accurately controlling the gap without repeatedly using the servo, the external memory and the configuration for reading the position information as described above become unnecessary, and the device configuration can be simplified. For example, even when a disk-shaped optical recording medium is rotated at a high rotational speed of about 3000 rpm or more, if it is not necessary to install the rotary encoder described above, the gap can be controlled with a simpler device configuration with high accuracy. Is possible.

  In view of the above problems, the present invention accurately controls the gap between the condensing optical system and the optical recording medium with a relatively simple device configuration when irradiating the optical recording medium with near-field light. With the goal.

In order to solve the above problems, an optical pickup device according to the present invention includes a light source, a condensing optical system that irradiates an optical recording medium with near-field light, and a light detection unit that detects a total reflected return light amount from the condensing optical system. A control unit that generates a gap servo signal based on the total reflected return light amount obtained from the light detection unit, and a condensing optical system at a predetermined position on the optical recording medium based on the gap servo signal generated by the control unit. And a drive unit for driving. The control unit divides the total reflected return light amount detected by the light detection unit into a relative traveling direction with respect to the optical recording medium and a direction orthogonal to the relative traveling direction, and the relative traveling direction is determined from the divided total reflected return light amount. The push-pull signal is calculated. Furthermore, the control unit feeds the calculated push-pull signal to the gap error signal indicating the error between the total amount of the total reflected return light amount detected by the light detection unit and the target value of the total reflected return light amount, thereby performing gap servo. The signal is generated .

An optical recording / reproducing apparatus according to the present invention includes a light source, a condensing optical system that irradiates the optical recording medium with near-field light, a light detection unit that detects a total reflected return light amount from the condensing optical system, and a light detection An optical pickup device comprising: a control unit that generates a gap servo signal based on the total reflected return light amount obtained from the unit; and a drive unit that drives the condensing optical system to a predetermined position on the optical recording medium; A medium mounting unit; and a drive unit that moves the optical recording medium mounting unit relative to the condensing optical system based on a gap servo signal generated by the control unit . The control unit divides the total reflected return light amount detected by the light detection unit into a relative traveling direction with respect to the optical recording medium and a direction orthogonal to the relative traveling direction, and the relative traveling direction is determined from the divided total reflected return light amount. The push-pull signal is calculated. Furthermore, the control unit feeds the calculated push-pull signal to the gap error signal indicating the error between the total amount of the total reflected return light amount detected by the light detection unit and the target value of the total reflected return light amount, thereby performing gap servo. The signal is generated .

Further, the gap control method according to the present invention detects the total reflected return light amount from the condensing optical system that irradiates the optical recording medium with near-field light, and uses the detected total reflected return light amount relative to the optical recording medium. And a push-pull signal in the relative traveling direction is calculated from the divided total reflected return light amount. A gap servo signal is obtained by feed-forwarding the calculated push-pull signal to a gap error signal indicating an error between the total amount of the total reflected return light amount and the target value of the total reflected return light amount .

  As described above, in the present invention, when controlling the gap of the condensing optical system that irradiates near-field light, the push-pull signal in the direction of travel relative to the optical recording medium, the case of a disk-shaped optical recording medium Generates a gap servo signal by feed-forwarding a push-pull signal in a tangential direction orthogonal to the radial direction. It has been clarified that by calculating the gap servo signal in this way, the residual error in the gap servo system can be improved, and the same effect as the repeated servo can be obtained. As will be described later, this is because the push-pull signal in the traveling direction relative to this optical recording medium, and in the case of a disk-shaped optical recording medium, the tangential push-pull signal has the same phase as the gap error signal. This is because it is a signal.

In the present invention, since the push-pull signal is fed forward to the gap error signal, there is an advantage that it is not necessary to provide an external memory unlike the repetitive servo. That is, in the case of a disk-shaped optical recording medium, it is not necessary to hold a repeated gap signal for one rotation.
In other words, according to the present invention, a signal equivalent to a repetitive signal is generated by calculating an optically obtained gap error signal, and feedforward servo is performed using the obtained signal, so that performance equivalent to that of a repetitive servo is achieved. Can be obtained.

  According to the present invention, when irradiating an optical recording medium with near-field light, the gap between the condensing optical system and the optical recording medium can be accurately controlled with a relatively simple device configuration.

  Examples of the best mode for carrying out the present invention will be described below, but the present invention is not limited to the following examples.

FIG. 1 is a schematic configuration diagram of an optical recording / reproducing apparatus 100 including an optical pickup device 30 according to an embodiment of the present invention. In this example, the condensing optical system 10 includes an optical lens 6 that is an objective lens made of an aspheric lens or the like, and a hemispherical or super hemispherical solid immersion lens (SIL) 7. Although FIG. 1 shows a super hemispherical SIL, it may be a hemispherical SIL. This optical pickup device 30 includes a power control unit 1, a light source 2 such as a laser diode, a collimating lens 3, a beam splitter 4, a mirror 5, a condensing optical system 10 having an optical lens 6 and SIL 7, and a branching optical path of the beam splitter 4. And a light detection unit 9 such as a four-divided photodiode. Furthermore, it has the control part 15 which produces _| generates the control signal which calculates the detection signal by the light detection part 9, and controls the drive part 11 of the condensing optical system 10, ie, the gap error signal SG. Control unit 15 may be output to the drive unit 11 generates the tilt error signal S _T for controlling the inclination (tilt) relative to the optical recording medium 20 of the SIL 7.

  The optical recording / reproducing apparatus 100 is further provided with a mounting unit 25 for mounting the optical recording medium 20 such as a disk, and a driving unit 26 that rotationally drives the mounting unit 25 with a one-dot chain line Cs as a rotation axis.

  In this configuration, the light emitted from the light source 2 is converted into parallel light by the collimator lens 3, passes through the beam splitter 4, is reflected by the mirror 5, and enters the condensing optical system 10. For example, the power control unit 1 controls the output of the light source 2 in accordance with recording information from an information storage unit (not shown) during recording. During reproduction, output control from the power control unit 1 may be omitted, and the output of the light source 2 may be constant. The recording surface on which information of the optical recording medium 20 is recorded is irradiated as near-field light by the condensing optical system 10. The return light reflected from the optical recording medium 20 is reflected by the mirror 5, reflected by the beam splitter 4, and condensed on the light detection unit 9 by the condenser lens 8.

Part of the light detected by the light detection unit 9 is output as an RF (high frequency) signal S _RF corresponding to the recording information of the optical recording medium 20 during reproduction. On the other hand, the total reflected return light amount is input to the control unit 15 that generates a signal for controlling the drive unit 11 that drives the condensing optical system 10. And gap control signal S _G generated by the feed-forward, which will be described later in the control unit 15, a tilt control signal S _T is outputted to the driver 11. The drive unit 11 includes, for example, a biaxial actuator including a voice coil motor, a triaxial actuator, or the like. The gap control drive unit and the tilt control drive unit may be provided separately, and a control signal may be input to each drive unit. Furthermore, in addition to the configuration shown in FIG. 1, various optical elements for correcting aberrations can be additionally arranged in the optical pickup device 30.

  In this optical recording / reproducing apparatus 100, the optical recording medium 20 is mounted on the above-described drive unit 26 that is driven to rotate, and for example, a horizontal movement mechanism in which the optical pickup device 30 moves in parallel along the recording surface of the optical recording medium 20. (Not shown). Then, the near field light emitted from the condensing optical system 10 is scanned along the recording track on the surface of the optical recording medium 20 in a spiral shape or a concentric shape by the interlocking of the horizontal movement mechanism and the drive unit 26. The configuration.

  FIG. 2 schematically shows the relationship between the total reflected return light quantity with respect to the gap in the optical pickup device 30 using near-field light. FIG. 2A schematically shows a gap between the end surface of the SIL 7 and the optical recording medium 20 in the condensing optical system 10 including the optical lens 6 and the SIL 7. FIG. 2B shows the relationship between the total reflected return light quantity and the gap. In this case, the total reflected return light amount is a return light amount of light (a component with an aperture ratio ≧ 1) incident at an angle that is totally reflected on the end surface of the SIL 7 facing the optical recording medium.

  As shown in FIG. 2B, the far field region Ff, which is a region that is not in the near-field state, generally corresponds to a range in which the gap is 1/2 to 1/5 or more of the wavelength of the incident laser light. In the far field region Ff, all light is totally reflected at the SIL end face, so that the total reflected return light amount is constant. On the other hand, in general, a near-field state, that is, a near-field region Fn is obtained in a gap of 1/2 to 1/5 or less of the wavelength of incident laser light. In the example shown in FIG. 2B, as an example, when the wavelength of incident light is 405 nm, the total reflected return light amount is reduced below 70 nm. The relationship between the gap and the wavelength, which is the near field region, is not uniform, and varies in the range of about 1/2 to 1/5 as described above, depending on the wavelength, the material configuration of the optical recording medium, SIL, and the like.

  In the near field region Fn, evanescent coupling occurs between the SIL end face and the surface of the optical recording medium, and a part of the total reflected return light penetrates the SIL end face and is transmitted to the optical recording medium side. For this reason, the total reflected return light amount decreases. When the SIL completely contacts the optical recording medium, all the totally reflected return light is transmitted to the optical recording medium side, so that the total reflected return light amount becomes zero. Therefore, as shown in FIG. 2B, the relationship between the gap between the SIL end face and the optical recording medium and the total reflected return light amount is gradually reduced in the near field region Fn, which was constant in the far field Ff. However, when the gap is zero, it becomes zero. In the region where the total reflected return light amount decreases, there is a region where the relationship between the gap and the total reflected return light amount is linear as shown by being surrounded by a broken line l. Therefore, in this linear range, the gap can be kept constant by forming a feedback loop with the total reflected return light amount as a gap error. That is, when the target gap is g shown in FIG. 2B, control may be performed so that the total reflected return light amount becomes r.

FIG. 3 shows an example of a servo loop in the case where gap control is performed by a normal feedback loop as a comparative example. In this case, a subtracter 141, a servo filter 143 including a phase compensation filter, a lead lag filter, and the like, a control target 144, an adder 145, and a GES calculation unit 146 are included. In FIG. 3, r1 is a gap target value (target value of the total reflected return light amount shown in FIG. 2B), d1 is a disturbance due to disk surface shake, e1 is a difference between the target value and a gap error signal (GES), e1 = y1-r1. The control object 144 is the actuator itself in which the SIL is installed, and is the drive unit 11 in FIG. The GES calculation unit 146 includes the light detection unit 9 in FIG. 1, an analog / digital converter, an amplifier, and the like.
The target signal r1 input from the input terminal 140 is supplied to the subtracter 141 together with the detection signal y1 output from the GES calculation unit 146 described later, and e1 (= y1-r1) is output. The signal e1 processed by the servo filter 143 is input to the control target 144. The adder 145 adds the disturbance d1 to the detection signal reflected by the movement of the control target 144, and the GES calculator 146 outputs GES, that is, y1.
As shown in FIG. 3, in this case, y1 which is the gap error signal GES is fed back.

However, when it is intended to control the gap by feeding back GES as described above, if the rotational speed of the optical recording medium is high (relative movement speed with respect to the optical recording medium is high), the optical recording medium may be shaken. It becomes difficult to follow. For this reason, as shown in FIG. 4, the residual error of the rotation component is superimposed on the gap error signal. In FIG. 4, the portion sandwiched between the arrows indicates the GES for one rotation. It can be seen that a component synchronized with rotation, that is, a residue error is observed.
According to the present invention, it is possible to reduce the residual error of the rotational synchronization component. Next, the case where control is performed according to the present invention will be described.

FIG. 5 is a configuration diagram of a servo loop of the control unit 15 in the optical pickup device according to the embodiment of the present invention. As shown in FIG. 5, in this case, a configuration having a subtracter 41, an adder 42, a servo filter 43 in the main loop, a control target 44, an adder 45, a GES calculation unit 46, and a servo filter 60 for a feedforward signal. It is said. As the servo filter 60, a low-pass filter or the like can be used.
The target value r input from the input terminal 40 is input to the control object 44, in this case, the drive unit 11 shown in FIG. 1, via the subtracter 41, the adder 42, and the servo filter 43. The adder 45 adds the disturbance d to the output that changes due to the movement of the controlled object 44, and the total reflected return light amount is detected by the GES computing unit 46.

  FIG. 6 is a configuration diagram of an example of the GES calculation unit 46 in FIG. In the GES calculation unit 46, the total reflected return light amount from the end surface of the SIL 7 in this case in the condensing optical system 10 is detected by the GES detection unit 46A. In the GES detection unit 46A, the total reflection return divided into four in the direction of travel relative to the optical recording medium and the direction orthogonal thereto with a four-division detector, that is, in the case of a disk-shaped optical recording medium, in the tangential direction and radial direction. The total amount of the total reflected return light amount is output as GES from the output terminal 47 and fed back to the subtractor 41.

On the other hand, based on the divided light amount, a push-pull signal in the traveling direction relative to the optical recording medium, in this case, a tangential push-pull signal Tpp, is calculated and output in the Tpp / Rpp calculation unit 46B. Note that the push-pull signal Rpp in the radial direction may be calculated from the same four-part total reflected return light amount.
The obtained Tpp is output from the output terminal 48 and added to the adder 42 via the servo filter 60. Thereby, it becomes the structure which feeds forward Tpp.

  As shown in FIG. 7A, when the end surface 7T facing the optical recording medium 20 of the SIL 7 is inclined due to surface shake or the like, the total reflected return light amount is schematically shown in FIG. As described above, the return light having a light quantity corresponding to the gap is detected at a portion where the end surface 7T is separated from the surface of the optical recording medium 20, that is, a portion which becomes a far field region. In FIG. 7C, arrows t and r indicate the tangential direction and the radial direction, respectively, and the detection regions in the light detection unit 9 divided into four in these directions are indicated as 9A, 9B, 9C, and 9D, respectively. As shown by a broken line in FIG. 7C, when an inclination between the optical recording medium 20 and the SIL 7 occurs, a difference in intensity of light amount, that is, a difference in strength of GES occurs in the tangential direction or radial direction.

Here, the signals from the regions 9A to 9D are respectively expressed as A to D, the error signal in the tangential direction is Tpp, and the error signal in the radial direction is Rpp.
Tpp = (A + D) − (B + C) (1)
Rpp = (A + B) − (C + D) (2)

Since Tpp is calculated from the gap error, it can be expressed as the following equation (3), where α and β are the slopes of the gap error in the tangential direction.
GES = A + D + B + C = (α + β) · {D / (1 + CP)} (3)

However,
α + β = 1 (4)
And The difference α−β in the degree of tilt is the tilt angle. The above equation (3) can be derived from the following consideration.

When each Laplace transform of e, r, and d in FIG. 3 is expressed as E, R, and D, from FIG.
E = Y−R (5)
-ECP + D = Y (6)
It becomes. Note that C and P indicate the output of the servo filter and the control target, respectively, and CP indicates the gain of the control unit.

When e is deleted from the above equations (5) and (6), GES, that is, Y becomes as shown in the following equation (7).
Y = (CP · R) / (1 + CP) + D / (1 + CP) (7)

In the above formula (7), the second term is a disturbance term due to the disturbance d. Therefore, in order to make GES follow the target value R completely, it is sufficient to cancel the disturbance term shown in the following equation (8).
D / (1 + CP) (8)

In other words, in the first term in the above equation (7), that is, the following equation (9), R, that is, the target value is constant, that is, a DC component.
(CP · R) / (1 + CP) (9)

In general, the DC gain of CP in the case of target value tracking servo is sufficiently larger than 1, that is,
1 << CP (10)
It is. Therefore, the above formula (9) can be expressed as the following formula (11).
{CP / (1 + CP)} · R≈ (CP / CP) · R = R (11)

That is, the gap error (the error from the target value) is the second term itself of the above equation (7). Therefore, the gap error signal GES can be expressed by the following equation (12).
GES = D / (1 + CP) (12)

Since the push-pull signal Tpp is expressed as the tilt angle (α−β) multiplied by the disturbance term expressed by the above equation (8), it can be expressed as the following equation (13).
Tpp = (α−β) · {D / (1 + CP)} = (α−β) · GES (13)

From the above equation (13), the push-pull signal Tpp is strongly influenced by GES. To eliminate the influence of GES on Tpp, either standardize Tpp with GES (divide by GES) or keep GES constant. You can see that
Regarding the method of standardizing with GES, it is possible to correctly perform tilt servo using Tpp by eliminating the influence of TPP's GES, but of course, the accuracy of gap servo cannot be improved as it is. Servo accuracy needs to be increased.

However, if GES is made constant in advance, the gap accuracy is already guaranteed, and GES = c (constant) in the above equation (13). In other words,
Tpp = (α−β) · c≈α−β (14)
Thus, a correct tilt error that is not influenced by GES can be obtained.

  From the above results, it is assumed that the Tpp error is used in the present invention in order to increase the gap accuracy. It can be understood from the following consideration that Tpp and GES are in phase.

  First, consider the case where the servo follows the disturbance and the GES is constant. At this time, from GES = c (constant), the state shown in the above equation (14) is obtained. In this case, since the GES is already small, feedforward is not necessary.

Next, consider the case where the servo does not follow the disturbance. In this case, the tilt angle physically corresponds to the inclination or differentiation of the surface shake signal D.
α−β≈s · D (15)
It becomes. Moreover, GES of the said Formula (13) is represented like the following formula | equation (16).

    D / (1 + CP) ≈D / (K / s) = K ′ · s · D (16)

  However, in the above formulas (15) and (16), s is a Laplace transform operator, which means differentiation, K represents a gain, and K ′ = 1 / K.

  In general, a Bode diagram showing a transfer function of an actuator in an optical pickup device is expressed as shown in FIG. In FIG. 8, the horizontal axis represents frequency and the vertical axis represents gain. Since the error rate is inversely proportional to the gain, the gain is increased by boosting in the relatively low frequency region indicated by the broken line F1, and becomes unstable if the slope is steep in the frequency region indicated by the broken line F2, so that the error rate becomes approximately −20 dB / dec. Compensation is made as follows. In the higher frequency region indicated by the broken line F3, second-order and third-order resonances occur. For this reason, it is understood that such resonance occurs when the servo band is simply increased.

In particular, in an optical system that irradiates near-field light, since the distance to be controlled is extremely small, it is impossible to control with high accuracy if a residual DC deviation Δe remains even a little. For this reason, it is common to include an integrator in the servo filter. The remaining deviation Δe is
Δe = D / K (17)
Therefore, if an integrator is inserted, K → ∞ and Δe → 0.

The above equation (16) will be explained. The transfer function of CP in the rotational frequency band where the servo does not follow the disturbance becomes almost integral 1 / s. That is, the gain is constant at the primary resonance of the actuator to be controlled, generally 100 Hz or less. On the other hand, as for the gain within the same frequency of the servo filter, the integrator 1 / s is inserted in order to remove the DC residual error as described above. From this,
1 + CP≈CP≈K / s (18)
Thus, the above equation (16) is derived.

  Here, the above equation (15) has a sign because it is a tilt error, and the above equation (16) has a positive gap error GES (total reflection return light amount value). Eventually, in the above equation (13), the sign follows the tilt error signal, and the amplitude is amplified and observed. That is, the servo follows the disturbance, and the amplitude increases compared to the case where the GES is constant.

  However, looking at the phase relationship, both the above formulas (15) and (16) indicate that the differential, that is, the phase advances by 90 degrees with respect to the surface blur signal D, and Tpp and GES are in the same phase. I understand.

Finally, the case where the servo does not completely follow the disturbance is expressed by the following equations (19) and (20).
α−β≈s · D (19)
D / (1 + CP) ≈D / 1 = D (20)

The above formula (19) is the same as the above formula (15).
The above equation (20) can be derived from the fact that the servo does not completely follow the disturbance, that is, the high frequency band in FIG. 8, and the gain is small and CP << 1. As for the phase relationship, it is clear from the above equations (19) and (20) that Tpp and GES are in phase with the surface blur signal D.

  From the above results, it can be seen that Tpp and GES have the same phase and similar signals. This state is shown in FIGS. In each example, the wavelength of light used is 405 nm, the numerical aperture NA of the condensing optical system is 1.84, and the target value of the gap is 25 nm. 9 shows a case where the gap completely follows the surface shake, FIG. 10 shows a case where the gap does not follow the surface shake, and FIG. 11 shows a case where the gap does not follow the surface shake completely. GES, Tpp, and runout D are respectively shown in FIG. 9, and the integration of Tpp is also shown in FIG. 9 to 11, it can be seen that GES and Tpp are similar signals, that is, there is a correlation.

  FIG. 12 shows GES, Tpp, and GES repetitive components. From FIG. 12, it can be seen that the repetitive component of GES is the same as Tpp. Therefore, it can be understood that the same compensation as that of the repetitive servo can be performed by feeding forward using the Tpp signal.

  FIG. 13 shows the result of feedforward servoing using Tpp. The wavelength of light to be used, the numerical aperture of the condensing optical system, and the target value of the gap are the same as those in the examples of FIGS. In this example, as shown in FIG. 5, feedforward is performed by passing the Tpp signal through an appropriate servo filter 60, for example, a low-pass filter, and adding the error signal e to the adder 42. The optical recording medium is in the form of a disk, and the measurement results are shown with a rotational speed of 3000 rpm.

  From the results of FIGS. 13A and 13B, it can be seen that the feed forward of the Tpp signal suppresses the repetition of GES. In addition, since the followability of the gap is improved by applying the present invention, it can be confirmed that the waveform shape of the Tpp signal amplitude is unchanged, but the amplitude is reduced. From this result, it can be seen that by adopting the configuration of the present invention, even when the rotational speed of the optical recording medium is 3000 rpm or more, the gap control can be performed satisfactorily.

  As described above, according to the present invention, by feeding forward a push-pull signal in the direction of travel relative to the optical recording medium, the same effect as that obtained when repeatedly performing servo can be obtained, particularly in a high frequency band. In addition, it is possible to suppress the influence of disturbance such as disk wobbling. Further, unlike the repetitive servo, it is not necessary to hold an external memory, that is, a repetitive gap signal for one rotation, so that the apparatus configuration can be simplified.

  In addition, the push-pull signal is calculated from the gap error signal, but since it is affected by fluctuations in the gap error (follow-up error that cannot be corrected by the gap servo), it must be standardized by the gap error. However, in the present invention, the gap followability can be improved, so that there is an effect that the normalization process as described above becomes unnecessary.

  The present invention is not limited to the configuration described in the above-described embodiment, and various modifications and changes can be made without departing from the configuration of the present invention.

1 is a schematic configuration diagram of an optical recording / reproducing apparatus including an optical pickup device according to an embodiment of the present invention. A and B are explanatory views of the total reflected return light amount. It is a block diagram which shows the servo loop by a comparative example. It is a figure which shows the waveform of the gap error signal obtained by a comparative example. It is a block diagram which shows the servo loop of the control part of the optical pick-up apparatus which concerns on embodiment of this invention. It is a block diagram of an example of the GES calculating part in the control part shown in FIG. A is a cross-sectional view showing the inclination between the SIL and the optical recording medium, B is a view showing an example of the total reflected return light amount, and C is a configuration diagram of the light detection unit. It is a figure which shows the Bode diagram of the transfer function of the control system in a common optical pick-up apparatus. It is a figure which shows a signal waveform in case a gap follows a surface blur. It is a figure which shows a signal waveform in case a gap stops following a surface shake. It is a figure which shows a signal waveform in case a gap does not follow a surface blur completely. It is a figure which shows the waveform of the repeating signal of GES, TPP, and GES. A is a diagram illustrating a signal waveform in a comparative example in which feedforward control according to the present invention is not performed, and B is a diagram illustrating a signal waveform in an embodiment in which feedforward control according to the present invention is performed.

Explanation of symbols

  1. 1. Power control unit, 2. light source; Collimating lens, 4. Beam splitter, 5. Mirror, 6; 6. optical lens; Solid immersion lens (SIL), 8. 8. condensing lens; 9. Light detection unit Control unit, 11. Drive unit, 20. Optical recording medium, 25. Mounting section, 26. Drive unit, 40. Input terminal, 41. Subtractor, 42. Adder, 43. Servo filter, 44. Control object, 45. Adder, 46. Gap error signal calculation unit, 46A. Gap error signal detector 46B. Push-pull signal calculation unit, 47,4. Output terminal, 60. Servo filter, 100. Optical recording / reproducing device

Claims (7)

A light source;
A condensing optical system for irradiating the optical recording medium with near-field light;
A light detection unit for detecting the total reflected return light amount from the condensing optical system ;
A control unit that generates a gap servo signal based on the total reflected return light amount obtained from the light detection unit;
A drive unit that drives the condensing optical system to a predetermined position on the optical recording medium based on the gap servo signal generated by the control unit ;
The control unit divides the total reflected return light amount detected by the light detection unit into a relative traveling direction with respect to the optical recording medium and a direction orthogonal to the relative traveling direction, and the divided total reflected return light amount. To calculate the push-pull signal of the relative running direction from
A gap error signal indicating an error between a target value of said optical detector return total reflection and total quantity of returned light the totally reflected and detected light, the computed the push-pull signal by feed forward, the gap servo signal Generate optical pickup device. The light converging optical system includes an optical lens, an optical pickup apparatus according to claim 1, wherein that having a a solid immersion lens. The optical recording medium is a disk-shaped medium;
The push-pull signal, the optical pickup apparatus of claim 1, wherein tangential Ru tangential direction of the push-pull signal der perpendicular to the radial direction of the optical recording medium. 4. The optical pickup device according to claim 3, wherein the rotational speed at the time of recording and / or reproduction of the optical recording medium is set to 3000 revolutions / minute or more. Light source, a focusing optical system for irradiating the near-field light on an optical recording medium, a light detector for detecting the total reflection return light quantity from the light converging optical system, the total reflection return light quantity obtained from the photo detecting portion An optical pickup device comprising: a control unit that generates a gap servo signal based on the driving unit; and a driving unit that drives the condensing optical system to a predetermined position on the optical recording medium;
A mounting portion for the optical recording medium;
A drive unit that moves the mounting unit of the optical recording medium relative to the condensing optical system based on the gap servo signal generated by the control unit ;
The control unit divides the total reflected return light amount detected by the light detection unit into a relative traveling direction with respect to the optical recording medium and a direction orthogonal to the relative traveling direction, and the divided total reflected return light amount. To calculate the push-pull signal of the relative running direction from
A gap error signal indicating an error between a target value of said optical detector return total reflection and total quantity of returned light the totally reflected and detected light, the computed the push-pull signal by feed forward, the gap servo signal Optical recording / reproducing device to be generated . The light converging optical system includes an optical lens, an optical recording reproducing apparatus according to claim 5, wherein that having a a solid immersion lens. The total reflected return light amount from the condensing optical system that irradiates the optical recording medium with near-field light is detected, and the detected total reflected return light amount is orthogonal to the relative traveling direction with respect to the optical recording medium and the relative traveling direction. Divided into the direction to calculate, the push-pull signal of the relative traveling direction is calculated from the divided total reflected return light amount,
A gap control method for obtaining a gap servo signal by feed-forwarding the calculated push-pull signal to a gap error signal indicating an error between the detected total amount of the total reflected return light amount and a target value of the total reflected return light amount .