JP2739043B2 - Optical disk recording and playback device - Google Patents

Description

DETAILED DESCRIPTION OF THE INVENTION

[0001]

BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to an optical disk recording / reproducing apparatus. More specifically, the present invention relates to a magnetic recording surface of a disk by applying an external magnetic field to the disk and increasing the temperature by a light spot. The present invention relates to an optical disk recording / reproducing apparatus that performs recording by reversing the direction of a magnetic field, irradiates a light spot of lower power than at the time of recording to a recording surface during reproduction, and optically reads the direction of the magnetic field.

[0002]

2. Description of the Related Art In this type of optical disk recording and reproducing apparatus,
Although it is necessary to always detect the position of the optical disk, a detection method using light is generally used for distance detection when the distance between the detector and the device under test is short.
FIG. 53 is a side sectional view showing an example of this type of conventional optical distance detecting device. In the figure, a light emitting diode 1 as a light source and a photodetector 3 are mounted on a substrate 2, and a condenser lens 4 is disposed in front of the light emitting diode 1 and the light detector. A glass window 5 is attached to an opening of a case 6 accommodating the light emitting diode 1, the photodetector 3 and the condenser lens 4, and an object to be measured 7 whose position fluctuates ahead of the glass window 5. Next, the operation will be described. A certain amount of light is emitted from the light emitting diode 1, is converted into convergent light by the condenser lens 4, and is emitted from the glass window 5 to the outside of the case 6. Reference numeral 8 denotes the optical axis of the emitted light. The emitted light is reflected by the object 7 to be measured, passes through the glass window 5 and the condenser lens 4 again, and irradiates on the photodetector 3. Reference numeral 9 denotes the optical axis of the reflected light. The amount of light irradiated onto the photodetector 3 is determined by the distance between the object 7 and the detection device and the reflectance and shape of the object 7, and is determined by the distance to the same object 7 and the light detector 3. FIG. 54 shows the relationship with the light intensity. As shown in the figure, the light intensity has a maximum value at a distance of about 4.5 mm, and decreases as the distance from the distance increases. therefore,
If the same light measurement object 7 is used and the detection distance is limited so as to fall within the linear range of the light intensity, the output of the photodetector 3 and the distance correspond one to one, and the distance can be detected. Becomes

FIG. 55 is a side view showing a main part of a conventional optical disk recording / reproducing apparatus provided with the above-described distance detecting means. In the figure, a conventional optical disc recording / reproducing apparatus
Generally, an optical disk 10 as an object to be measured, a motor 11 installed on a main body base, a base 14 mounted on the main body base through bearings 12 and 13,
4 comprises an optical head 15 supported by the base 4 and a magnetic head 16 supported by the base 14. The optical head 1
Reference numeral 5 denotes a light source for emitting the light beam L, optical components such as an objective lens for guiding the light beam L to the optical disk 10, and the optical disk 1
It comprises an optical component for guiding the reflected light from zero, a light receiving element for receiving the reflected light and converting it to an electric signal, an optical sensor for detecting a focus shift and a track shift of the light spot S and the like.

Next, the operation of the above-mentioned conventional example will be described with reference to FIG.
This will be described with reference to (a), (b) and (c) and FIG.
56 (a) to 56 (c) are side views showing the positional relationship between the magnetic head 16 and the optical disk 10, and FIG. 57 shows the magnetic field intensity B on the disk recording surface and the distance H between the optical disk 10 and the magnetic head 16. FIG. 4 is a characteristic diagram illustrating a relationship. First, the optical disk 1
0 is rotated by the motor 11. Then, the optical head 15 and the magnetic head 16 are driven in the direction of arrow A by the bearings 12, 13 and the base 14. The optical head 15 records the modulation (information) of the bias magnetic field generated by the magnetic head 16 with the light spot S.
The light spot S generally has a diameter of 1.0 to 1.5 μm.
m. Here, as shown in FIGS. 56A to 56C, when the optical disk 10 rotates, the distance H (H _{1 to} H ₃ ) between the recording surface of the optical disk 10 and the magnetic head 16 changes. The magnetic field generated by the magnetic head 16 is about 100 to 500 Oe. As shown in FIG. 57, as the distance H between the recording surface of the optical disk 10 and the magnetic head 16 increases, the magnetic field intensity increases. B decreases.

[0005]

In the above-mentioned conventional optical disk recording / reproducing apparatus, the magnetic head cannot be brought close to each other in order to prevent the magnetic head from colliding with the optical disk, and the mechanical accuracy is severe. There were challenges. SUMMARY OF THE INVENTION The present invention has been made to solve the above-described problems, and has as its object to obtain an optical disk recording / reproducing apparatus capable of reducing mechanical accuracy.

[0006]

According to a first aspect of the present invention, there is provided an optical disk recording / reproducing apparatus for irradiating an optical disk with light to record / reproduce a signal, and a radius of the optical disk integrated with the optical head. A magnetic head that generates a bias magnetic field, and a light emitting element and a photodetector provided on the same base so as to be movable integrally with the magnetic head. Distance detecting means for detecting a distance and outputting the distance information; and the magnetic head movably supported in a direction substantially perpendicular to the recording surface, so that the distance is constant according to the distance detection information. And a bimorph-type piezoelectric element actuator for driving the actuator. In the optical disk recording / reproducing apparatus according to the first aspect of the present invention, the distance between the magnetic head and the disk surface can be reduced, and the fluctuation of the magnetic field intensity is significantly reduced. Further, in the optical disk recording / reproducing apparatus according to claim 2 of the present invention, the piezoelectric element is exposed at a part of the vibrating end of the bimorph type piezoelectric element, which is different from a part to which the first electric terminal and the second electric terminal are connected. And a bimorph-type piezoelectric element actuator in which a third electric terminal connected to the notch is connected to a drive circuit. In the optical disk recording / reproducing apparatus according to the second aspect of the present invention, the drive circuit sets the drive voltage based on the acceleration voltage input from the third electric terminal. An optical disk recording / reproducing apparatus according to a third aspect of the present invention provides an actuator in which the width of the conductive metal plate serving also as the conductive plate of the driven bimorph piezoelectric element is determined based on a reference function of vibration. Have. Also,
In the optical disk recording / reproducing apparatus according to the third aspect of the present invention, the vibration level at an unnecessary resonance point is reduced.
Since the higher-order resonance level can be suppressed and the resonance frequency can be determined relatively freely, the control band can be widened and the displacement can be increased.

[0007]

DESCRIPTION OF THE PREFERRED EMBODIMENTS An optical disk recording / reproducing apparatus will be described below. FIG. 3 is a plan view of each optical element viewed from the direction of its optical axis. In the figure, a light emitting diode 2 as a light source
One of the 0, 2 photodetectors (hereinafter referred to as PD1) 21a, and the other photodetector disposed farther from the light emitting diode 20 than the PD1 21a. (Hereinafter referred to as PD2) 21b are arranged in the same plane, and this plane is hereinafter referred to as a detector plane. Also, for the reason described later, PD2 21
The light receiving area of b is set to be larger than the light receiving area of PD121a. Next, the operation will be described. Light emitting diode 2
Numeral 0 denotes a light source having a light-emitting surface having a flat structure, which is a light source having a light intensity distribution which is perpendicular to the plane of FIG. Now, if there is a mirror surface of the object to be measured above the light emitting diode 20 in parallel with the detector plane, the light emitting diode 2
The light emitted from 0 reaches the detector plane again, and PD1 21
a and PD2 21b.

FIG. 2 shows the state of the light intensity distribution of the light applied to the detector plane. 2 (a) and 2 (b) show the light intensity with respect to the position on the one-dot chain line JJ in FIG. 3, and FIG. 2 (c) shows the arrangement of each optical element.
FIG. 2A shows a light intensity distribution when the object to be measured is at a short distance, and has a strong peak intensity concentrated near the light emitting diode 20. On the other hand, FIG. 2B shows the light intensity distribution when the object to be measured is at a long distance, and has a widened distribution with a low peak intensity. Here, the phenomena shown in FIGS. 2A and 2B will be examined from the characteristics of the photodetector in FIG. FIG. 1 shows the case of the arrangement shown in FIG.
The relationship between the light intensity at the positions of PD1 21a and PD2 21b and the distance to the object to be measured is illustrated in an overlapping manner. That is, in the range of distance to be measured, PD1 21
The characteristic of a corresponds to the region of the negative gradient exceeding the maximum value of the light intensity, and the characteristic of PD2 21b corresponds to the region of the positive gradient up to the maximum value of the light intensity. Compared to PD1 21a
The reason why the maximum point of the PD2 21b is shifted downward and to the left and right in FIG.
This is because it is arranged at a position farther than the PD1 21a. The details of the relative positions between the optical elements in FIG. 3 are described in detail in the case where PD1 21a and PD22
As shown in FIG. 1, the light intensity characteristics of 1b are adjusted and set so as to correspond to mutually opposite gradient regions.

FIG. 4 is a characteristic diagram showing a relationship between a photodetector output and a distance in a range of a distance to be measured. In the figure, the output of PD1 21a is curve 22 and the output of PD2 21b is curve 23, but the magnitude of the output is almost the same because of the difference in light intensity between the two in FIG. This is because the light receiving area of the PD2 21b is set to be larger than the light receiving area of the PD1 21a. Then, the difference x between the two outputs 22 and 23 is obtained by the electric circuit shown in FIG. 5, and the ratio of the difference x to the sum y of the two outputs is calculated to calculate the normalized differential output 24. This differential output 24
FIG. 6 shows the characteristic shown in FIG. That is, by obtaining the distance from the object to be measured by the above-described calculation, it is possible to remove the influence of the change in the reflectance of the object to be measured, which has conventionally been a problem.

By the way, as shown in FIG.
Crosses zero at a certain distance. When this distance detecting device is used for a control device that keeps the distance to the object to be measured constant, if the distance of the zero cross point N is set to a target value, the differential output 24 becomes an error signal with respect to the target value. Is good. The distance of the zero-cross point N is determined by the parameters l ₁ , l ₂ , w ₁ , w ₂ , g ₁ , and g ₂ in FIG. 3, and by changing these parameters, the zero-cross point N is considerably freed. N can be set. For example, the amount of light incident on PD2 21b if Chijimere the distance g ₂ between PD1 21a and PD2 21b, so starts to increase from shorter where the distance is shorter than the zero-crossing point N. If reach out a distance g ₂ Conversely, the distance of the zero-cross point N becomes longer. The distance of the zero cross point N can also be changed by the area ratio between PD1 21a and PD2 21b. In this case, if the areas of the two are equal, the zero-cross point N becomes an infinite point, and the distance of the zero-cross point N approaches as the area of the PD2 21b increases.
A desired zero cross point N can be obtained by selecting an appropriate area ratio in which at least the area of PD2 21b is larger than the area of PD1 21a.

Next, a description will be given of another example which has been studied with particular consideration of the radiation distribution of the light emitting diode 20. That is, the emission of light from the light emitting diode can be regarded as substantially rotationally symmetric about the center of the light emitting diode.
Therefore, in order to accurately detect a change in distance, it is most efficient to use a photodetector having a concentric shape with the center of the light emitting diode as an axis so as to detect a change in light intensity. However, since it is difficult to mount electrodes for driving the light emitting diode and the photodetector in a perfect concentric shape, as shown in FIG. 7, PD1 21a, PD2
Reference numeral 21b denotes a shape lacking a part of a concentric circle, from which the electrodes 25a to 25d are extracted.

FIG. 8 shows still another example. Basically, as in FIG. 7, concentric photodetectors PD1 21a and PD22
1b and the light emitting diode 20.
21a and PD2 21b are both cut off by a chord so as to be smaller than a semicircle.
Has been arranged. In this case, the light receiving efficiency of the photodetector decreases, but the light emitting diode 20 and PD12
1a and the PD2 21b can be formed as a different chip on the mounting substrate, so that there is an advantage that the manufacture is easy. By the way, in the case where the optical disk is at a very short distance and the detection is performed only at the short distance, the area of the photodetector, particularly the PD1 21a, is reduced to increase the detection resolution, and the light emitting diode 20 and the PD1 21a, PD2 21b It is necessary to narrow the interval between In this case, in principle, even if the light emitting diode 20 and the PD1 21a and PD2 21b are in the same plane, it is possible to make the distance therebetween extremely small, but these optical elements must be electrically non-contact. Therefore, the two cannot be brought close to each other in production.

FIG. 9 et seq. Show an example suitable for the case where the optical disk is at a very short distance as described above. FIG. 9 shows each optical element formed on a printed wiring board.
10A is a front view, FIG. 10B is a plan view, and FIG. 10 is a plan view of a printed wiring board. In the drawing, a light emitting diode 20 is a light source having a flat light emitting surface and a light intensity distribution close to a completely diffused surface in an upward direction. A light emitting diode bonding wire 29 is attached to the printed wiring 28 for the light emitting diode light emitting surface electrode, and the light is emitted at a constant output. The photodetector chip 30 is attached to the photodetector cathode wiring 32 via a conductive spacer 31 with a conductive adhesive. The back surface of the photodetector chip 30, which is the cathode of the photodetector, has a printed wiring 32 for the photodetector cathode.
It is conducting. Here, the distance between the conductive spacer 31 and the light emitting diode 20 is such that the printed wiring 32 for the photodetector cathode and the printed wiring 27 for the electrode on the light emitting diode substrate side are not short-circuited even if the conductive adhesive protrudes at the time of fabrication. It is necessary to keep enough separation. Therefore,
As shown in FIG. 9A, the thickness of the conductive spacer 31 is set to be larger than the thickness of the light emitting diode 20, and the light emitting surface of the light emitting diode 20 and the light receiving surface of the photodetector chip 30 are at least arranged in the optical axis direction. The structure has a step that is greater than the thickness of the photodetector chip 30. PD121a and PD2
21b Bonding pad 33 for each anode
a and 33b are printed wirings 35a for PD1 anode via bonding wires 34a and 34b, respectively.
And PD2 are connected to the anode printed wiring 35b.

As shown in FIGS. 9 and 10, by providing a step between the light-emitting diode 20 and the photodetector chip 30, the light-emitting diode 20 and the conductive spacer 31 are sufficiently separated from each other so that their electrical insulation is achieved. In addition, the light emitting diode 20 and the photodetector chip 30 can be brought very close to each other. That is, the projection surfaces of the light emitting surface and the light receiving surface of the two in the direction of the optical axis can be made sufficiently close to each other, and if necessary, they can be partially overlapped. FIG. 11 shows the state of light emission / reflection and light reception in the above embodiment with respect to the optical disk 10.

FIG. 12 shows an example in which the above-mentioned optical distance detecting means is applied as a distance sensor for controlling a distance between a coil and a magneto-optical recording medium for applying a magnetic field to the magneto-optical recording medium. FIG. 1A is a plan view of the same, and FIG. 1B is a cross-sectional view of FIG. 1A taken along a dashed line kk. In the figure, a magnetic coil 36 is wound around a magnetic head 16. In this case, the optical disk 10 is the measured object whose distance is to be detected. The magnetic head 16 and the distance detecting device are mounted on a table 37, which is also an actuator for position control. As a means for creating a gap between the magnetic head and the magnetic medium, a gap of several μm is generally used by using an air levitation method. However, the magnetic head 16 in magneto-optical recording is several tens μm so as not to lose the advantage of being resistant to dust. It is necessary to control with a gap of ~ 100 m, and the air levitation method is not used. For this reason, it is necessary to detect the distance between the magnetic head 16 and the optical disk 10 by some method and perform control to keep the distance constant. In addition, since the actuator for control must be driven, the distance detection device needs to be small and lightweight. This embodiment satisfies such a requirement in particular. In FIG. 12, when the gap between the magnetic head 16 and the optical disc 10 is the target value g, that is, when the gap between the detector chip 30 and the optical disc 10 is d, the differential output 24 of the distance detector becomes zero. PD1 21a
And the shape arrangement of PD2 21b are set in advance. By controlling the target value so that the differential output 24 becomes 0, the gap between the magnetic head 16 and the optical disk 10 can be kept constant at the target value g.

Next, another example will be described. As described above with reference to FIG. 7, the intensity distribution of light emission from the light emitting diode can be regarded as substantially rotationally symmetric about the center of the light emitting diode. It is most accurate and efficient to use a concentric photodetector with a diode as the center. However, in this case, it is technically difficult to form each optical element in the same chip. The following embodiment solves these points. First, in FIG. 13, a disc-shaped photodetector chip 30 is provided with a through hole 30a at the center thereof. Similarly, a spacer 38 made of an insulator formed in a disk shape has a through hole 38a having a diameter larger than the through hole 30a of the photodetector chip 30 at the center thereof. 1
As shown in FIG. 4, each electrode and wiring are patterned. FIG. 14A shows a pattern on the photodetector chip 30 side, and FIG. 14B shows a pattern on the light emitting diode 20 side. Each optical element is arranged such that the center of both through holes 30 a and 38 a coincides with the center of the light emitting diode 20.
The photodetector chip 30 is attached on the cathode printed wiring 32 with a conductive adhesive. Also, PD1
21a and PD2 21b are connected to anode printed wirings 35a and 35b by bonding wires 34a and 34b, respectively. The light emitting diode 20
The chip size is set to be larger than the through hole 38a of the spacer 38, and the light emitting surface of the light emitting surface is set to the through hole 38a side, and is attached to the printed wiring 28 for the light emitting diode light emitting surface side electrode with a conductive adhesive, and as shown in FIG. The printed wiring 20 for the electrode on the side of the light emitting diode substrate 20 is connected by a bonding wire 29.

With the above configuration, the light emitting diode 20 emits light toward the through hole 30a of the photodetector chip 30, and passes through the through holes 38a, 30a to radiate above the photodetector chip 30. I do. In such a case, the exit of the photodetector chip 30 can be regarded as a secondary light source on the surface. FIGS. 16 and 17 show the states of light emission, reflection and light reception in the above example [FIG.
(a)] and the distribution of light intensity [each figure (b)]. In the former case, when the optical disk 10 is at a relatively short distance, and when the latter is at a relatively long distance, the light intensity distribution is rotationally symmetric about the optical axis of the light emitting diode 20. Therefore, as described above, the distribution of the light intensity received by the PD1 21a and PD2 21b becomes more uniform, and accurate and efficient distance detection becomes possible. Further, the light exit surface 30a, which is a secondary light source, and the light receiving surface of the PD1 21a can be disposed very close to each other, and a distance can be detected at a close position.

FIG. 18 shows another example in which the workability of patterning a printed wiring board is improved. FIG.
(a) is a plan view, and FIG. 18 (b) is a cross-sectional view of FIG. 18 (a) taken along a dashed line MM. In the figure, the conductive spacer 39 has a shape as shown in FIG. FIG. 20 is a plan view of the printed wiring board 26 on which the spacer 39 and the light emitting diode 20 are mounted, in a state where the light emitting diode 20 is mounted. The spacer 39 is formed by bonding the bonding wire 29 of the light emitting diode 20 to the photodetector chip 30.
The printed wiring board 26 has a sufficient thickness so as not to contact the printed wiring board, and is attached to the cathode printed wiring 32 on the printed wiring board 26 with a conductive adhesive. Then, the back surface, which is the cathode of the photodetector chip 30, is also adhered to the upper surface of the spacer 39 with a conductive adhesive. In this case, light from the light emitting diode 20 passes through the through hole 30a and is emitted. Is similar to the previous example. However, the printed wiring board 26 in this example is different from the spacer 38 in FIG. 14 of the previous example in that the patterning of the wiring electrodes on the substrate only needs to be performed on one side thereof, and the mounting of each component is concentrated on only one side thereof. Therefore, there is an advantage that the fabrication is simplified.

FIGS. 21 to 23 show still another example. In the figure, a conductive spacer 40 having the same thickness as the light emitting diode 20 has a shape as shown in an exploded perspective view in FIG. The upper surface of each of the light emitting diode 20 and the spacer 40 has the photodetector chip 3
0 is attached to the cathode side electrode with a conductive adhesive, and the lower surface is also attached to the printed wirings 41 and 42 patterned on the printed wiring board 26 with the conductive adhesive. However, in this example, the photodetector chip 3
Since 0 and the light emitting diode 20 are not electrically independent, special attention is required for the driving method. FIG. 23 shows an example of a driving circuit in that case. In the figure, a power supply 43 for driving a light emitting diode, a load resistor 44 of the light emitting diode 20, IV conversion amplifiers 45a and 45b, and these load resistors 46a and 46b are connected as shown. The wiring in the figure corresponds to the optical element part in the case of this example,
The anode of the light emitting diode 20 and PD1 21a and PD2
The operation is performed with the cathode of the cathode 21b at a common potential. In the case of this example, as can be seen from FIG. 21, the distance between the light emitting surface of the light emitting diode 20 and the upper end of the through hole 30a which is a substantial light emitting port is equal to the photodetector chip 3.
Since the thickness is reduced to the same value as the thickness of 0, there is an advantage that the amount of light emitted to the optical disk 10 increases accordingly and the detection sensitivity increases.

Next, another example will be described. FIG. 24 is a side view showing a main part of this example, and FIG. 25 is an exploded perspective view of a main part of the electromagnetic actuator in this example. In these figures, a cylindrical yoke 47 fixed to the base 14, a permanent magnet 48 positioned and joined inside the yoke 47, a ring-shaped magnetic member 49 fixed to the yoke 47, Elastic support members 50 and 51 fixed to two upper and lower positions on the inner side;
Coil bobbin 5 supported at upper and lower two places by 0 and 51
2, a control coil 53 wound around the coil bobbin 52, and a substrate 54 supported on one end of the coil bobbin 52.
And the light emitting element 20 installed on the dust board 54 and the substrate 5
4 and a two-divided photodetector 21.
In addition, the yoke 47 to the control coil 53 form an electromagnetic actuator. Further, the magnetic head 16 is
The optical head 15 includes a reflection mirror 55, an objective lens 56, and the like. By the way, in this example, a distance detecting means is formed by the light emitting element 20 and the two-segment light detector 21, and the driving means is formed by an electromagnetic actuator. The shielding means is provided by the magnetic member 49. According to the above configuration, first, a deviation in distance between the recording surface of the optical disk 10 and the magnetic head 16 is detected. That is, the light emitted by the light emitting element 20 is
The light is reflected to 0 and enters the two-divided photodetector 21. Since the intensity distribution of the incident light changes depending on the above-described distance, the two-piece photodetector 21 can detect a distance shift between the two. Then, a current based on the information of the distance shift is applied to the control coil 53, and the magnetic head 16 is driven in the direction of the arrow V by the electromagnetic force between the permanent magnet 48 and the distance shift is eliminated. Therefore, the distance between the recording surface of the optical disk 10 and the magnetic head 16 is kept almost constant. The magnetic member 49 functions as a shield for magnetic flux leaking from the magnetic circuit including the yoke 47 and the permanent magnet 48 to the magnetic head 16. Thereby, the fluctuation of the magnetic field strength can be remarkably reduced, and the magnetic head 16
And the optical disk 10 can be brought closer to each other.

FIG. 26 is a side view showing a main part of another example. In FIG. 26, a support member 57 supported at one end of a coil bobbin 52 and a balancer 58 attached to the end of the support member 57 are shown. Have. The same reference numerals as those in FIG. 24 denote the same parts. The magnetic head 16 is supported by the yoke 47 only by the elastic support member 51 via the support member 57 and the coil bobbin 52. The electromagnetic actuator includes a yoke 47 to a magnetic member 49, a magnetic support member 51 to a control coil 53, a support member 57, and a balancer 58. The substrate 54 is fixed to a support member 57.

FIG. 27 is a side view showing a main part of still another example, which includes a fixed base 59 fixed to the base 14 and an elastic support member 60 supported by the fixed base 59. The magnetic head 16 is supported by the elastic support member 60 via the substrate 54. The electromagnetic actuator is
The yoke 47 includes a magnetic member 49, a coil bobbin 52, a control coil 53, a fixed base 59, and an elastic support member 60. As described above, in each of the examples shown in FIGS. 26 and 27, the operation of detecting the distance between the optical disk 10 and the magnetic head 16 and the operation of driving the magnetic head 16 are the same as those in the above-described embodiment of FIG. It is. In each of the above examples, the magnetic circuit is formed by the cylindrical yoke 47 and the permanent magnet 48 magnetized in the radial direction, but the same operation can be expected even if the magnetic circuit is formed by other members. Also, the method of detecting the distance between the optical disk 10 and the magnetic head 16 is not limited to the above-described method, and a desired method can be achieved by a method using capacitance or a method using a signal from an optical head. It goes without saying that it can be done. By the way, in the above description, the case where the magnetic head 16 is used to eliminate the deviation in the distance between the optical disk 10 and the magnetic head 16 has been described. However, for example, it is also used to escape the magnetic head when loading or unloading the optical disk. It goes without saying that you can do it. That is, when attaching / detaching the optical disc,
Direction of moving the magnetic head away from the optical disk (3 to 10 mm
Degree).

Next, a first embodiment of the present invention will be described with reference to FIGS. FIG. 28 is a side view of a main part,
FIG. 29 is a perspective view of a piezoelectric element actuator, and FIG. 30 is a side view showing a positional relationship among a disk, a magnetic head, and an optical spet. In the drawings, the same or corresponding parts as those in FIGS. 1 to 27 are denoted by the same reference numerals. In the figure, a bimorph piezoelectric element 61 having one end fixed to a base 14 is shown.
A magnetic head 16 is mounted on a free end of the magnetic head. The objective lens 56 provided in the optical head 15 is driven by a lens actuator 62. Next, the operation will be described. The piezoelectric element actuator 61 is based on the fixed end,
Displacement in the direction of the arrow (B) according to the amount of energization is possible. As shown in FIG. 30, the objective lens 56 is displaced in the direction of the arrow (C) by the lens actuator 62. At this time, the distance between the recording surface 10a of the optical disk 10 and the lens 56 is kept substantially constant (D). The magnetic head 16 is driven by applying a voltage to the piezoelectric element 61 with a voltage proportional to an input voltage of a lens actuator 62 that drives a lens 56 provided on the optical head 15. Thereby, the distance (H) between the magnetic head 16 and the optical disk recording surface 10a is calculated.
Can be kept almost constant.

Next, another embodiment of the present invention will be described with reference to FIG.
1 to 33 will be described. In FIG. 31, a holder 63 fixed to the base 14 is provided with two pairs of position sensors. That is, the first position sensor detects the position of the surface of the optical disk 10 by using the light emitting element 20A and the two-part light receiving element 21A as shown in FIG. As shown in FIG. 33, the second position sensor is likewise a light emitting element 2
0b and a two-divided light receiving element 21b for detecting the position of the surface of the piezoelectric element 61. With the above configuration, the optical disc 1
0 can be detected and the distance (H) between the surface of the magnetic head 16 and the magnetic head 16 can be detected. By driving the piezoelectric element 61 so as to correct the amount of change (Δx) in this distance, the change in magnetic field strength (B) can be detected. Can be significantly reduced (see FIG. 34).

Next, still another embodiment of the present invention will be described with reference to FIGS. In FIG. 35, a light-emitting element 20 and a two-segment photodetector 21 are provided on a piezoelectric element actuator 61. However, the optical disk 10 is omitted in the figure. FIG. 36 shows a cross section taken along a dashed line (E) in the figure. The light emitted from the light emitting element 20 is reflected by the optical disk 10 and is incident on the photodetector 21. The light intensity distribution on the photodetector 21 changes as shown in FIG. 2 depending on the distance between the piezoelectric element actuator 61 and the optical disk 10. Therefore, the output obtained by subtracting the two photodetectors 21 is as shown in FIG. 37, and the distance can be detected from the differential output. Actually, the distance signal fluctuates at various frequencies, and the driving voltage for the piezoelectric element is also an AC voltage having the same frequency as the distance signal. Therefore, the bimorph piezoelectric element 61 is displaced in various directions at the arrow B direction. . At this time, the frequency characteristic of the amount of displacement of the bimorph type piezoelectric element 61 is determined based on the design dimensions at the time of manufacture, and is as shown in FIG. 38, for example.

FIG. 38 shows frequency characteristics when the driving voltage is fixed. The horizontal axis represents frequency f and the vertical axis represents displacement d. F ₀ is the primary resonance frequency, f ₁ is the secondary resonance frequency,
f ₂ represents the third-order resonance frequency. When the bimorph piezoelectric element 61 having such frequency characteristics is actually driven and controlled, when a required driving voltage is applied to the distance signal near the frequencies f ₁ and f ₂ , the displacement d becomes unnecessarily large. I will. Usually, the bimorph piezoelectric element 61-2
The secondary and tertiary resonance frequencies f ₁ and f ₂ are relatively low, and the resonance level is high. Therefore, the actuator using the bimorph piezoelectric element 61 has the frequency f ₁
It can be controlled accurately only with the following narrow band.

The invention of claim 2 described below has been made in order to solve the above problems, and the displacement can be accurately controlled even at the secondary and tertiary resonance frequencies, so that the control band can be widened. This implements a bimorph piezoelectric element actuator. FIG. 39 is a perspective view showing an embodiment of the second aspect of the present invention, in which a part of the vibrating end of a bimorph-type piezoelectric element 61 composed of piezoelectric elements 61a and 61b and a conductive plate 61c has one electrode peeled off. The first electric terminal 65 exposing the piezoelectric element 61a, and the piezoelectric elements 61a and 61b
Leads out a second electric terminal 66. Notch 64
Is connected to the drive circuit 68.

Next, the operation will be described with reference to the frequency characteristic diagram of FIG. First, the frequency characteristic of the bimorph piezoelectric element 61 is measured, and a coefficient for outputting an appropriate drive voltage V at each of the resonance frequencies f ₁ and f ₂ is calculated, and is set in the drive circuit 68 in advance. And
As shown in FIG. 40, the amount of displacement d at each of the resonance frequencies f ₁ and f ₂ is made smaller so that the characteristic of the amount of displacement d of the bimorph piezoelectric element 61 changes uniformly with respect to the frequency f. When actually driving and controlling the bimorph piezoelectric element 61, the drive circuit 68 controls the drive voltage V based on the distance signal H as described above, and keeps the distance between the magnetic head 16 and the optical disk 10 constant. At this time, since the piezoelectric element 61a outputs a voltage corresponding to the motion acceleration at that time, the notch 6
Third electrical terminal 6 connected to piezoelectric element 61a through
7 outputs an acceleration voltage C indicating the vibration state of the bimorph piezoelectric element 61. The drive circuit 68 detects the frequency of the bimorph-type piezoelectric element 61 based on the acceleration voltage C, and if the secondary and tertiary resonance frequencies f ₁ and f ₂ or near the same, the drive voltage V according to a preset coefficient. Decrease. Thus, unnecessary resonance is suppressed, the bimorph piezoelectric element 61 is appropriately driven, and the distance between the magnetic head 16 and the optical disk 10 is controlled to be constant. At this time, the surface of the piezoelectric element 61a exposed in the notch 64 acts as an acceleration sensor and directly outputs the acceleration voltage C. Therefore, the vibration state of the bimorph type piezoelectric element 61 can be detected with a simple structure without increasing the cost. can do. In the above embodiment, the case where the magnetic head 16 for generating the bias magnetic field is driven has been described as an example. However, as another embodiment, as shown in FIG. 41, it is used for driving control of the objective lens for light beam irradiation. Is also good. in this case,
In order to displace the objective lens 56 in the direction of arrow B while maintaining the parallelism, a bimorph-type piezoelectric element 70 without a notch is provided in parallel with the bimorph-type piezoelectric element 61, and the bimorph-type piezoelectric elements 61 and 70 A holder 59 for holding the objective lens 56 is fixed to the vibrating end. Although not shown, the present invention is not limited to an optical disk recording / reproducing apparatus, and may be applied to an actuator of a magnetic head for tracking control of a VTR. Here, as shown in FIG. 42, the bimorph type piezoelectric elements 61 and 70 are composed of piezoelectric elements 61a and 61b polarized in the same thickness direction and an elastic shim 61c and an electric terminal, which also serve as a conductive plate made of a metal material such as copper. 65, 66a and 66b. When a voltage is applied so that the electric terminals 66a and 66b have the same polarity and the terminals 65 have different polarities, one of the piezoelectric elements 61a and 61b extends in the length direction of the arrow, and the other extends in the length direction of the arrow. Shrink to An elastic shim 61c is adhered to opposing sides of the respective piezoelectric elements 61a and 61b, and the length of the elastic shim 61c does not change. As a result, the bimorph type piezoelectric element bends and deforms in the (α) direction in the figure. Therefore, a focus shift is detected by a known method, and a voltage corresponding to the shift amount is applied to the bimorph type piezoelectric element to drive the objective lens holder 69 and eventually the objective lens 56 to perform focus control.

Looking at the frequency characteristics in the above operation,
As shown in FIG. 43, the relatively low frequencies f ₂ , f ₃ , f ₄
In this case, the second, third and fourth resonances occur, and the vibration level is high, so that there is a problem that the control band cannot be widened. If two bimorph-type piezoelectric elements 61a and 61b are arranged in parallel as shown in FIG. 41 so that no tilt occurs when the objective lens 56 is displaced, the assemblability is poor or the amount of displacement is reduced. There was a problem that it could not be large. The invention of claim 3 has been made to solve the above-mentioned problem, and embodies an actuator for a recording / reproducing apparatus which has a simple structure, good assemblability, a wide control band, and a large movable amount. I do.

An embodiment of the third aspect of the present invention will now be described with reference to FIG.
47 will be described. In the figure, a bimorph piezoelectric element 61 is an elastic shim 71 that is a conductive metal plate that also serves as a piezoelectric element 61a, 61b polarized in the same thickness direction and a conductive plate sandwiched between the piezoelectric elements 61a, 61b.
Consists of The elastic shim 71 is formed in such a shape that its width is substantially inversely proportional to the value of the first-order reference function of the fixed-roll supported beam. That is, in FIG. 45, if the width of the elastic shim 71 is b, the length is 1, the x-axis is taken in the length direction, and the elastic shim 71 is supported at x = 0

[0031]

B∝ 1 / {cos βl-cosβl) (coshβx-cosβx) + (sinβl + sinβl) (sinβx-sinβx)｝ βl = 2.365

The shape is as follows. The piezoelectric elements 61a and 61b are bonded to both surfaces of the elastic shim 71. With the above configuration, by applying a desired voltage to the piezoelectric element 61, the objective lens holder 6 can be driven in the same manner as in the prior art.
9. The objective lens 56 is driven in the direction of the arrow (B) to control the defocus of the light spot collected by the objective lens 56. At this time, the elastic shim 71 of the piezoelectric element 61 is used.
Has a shape as described above. Generally, the bending displacement is inversely proportional to the second moment of area, that is, when the thickness is constant, the bending displacement is inversely proportional to the width. Therefore, the piezoelectric element 61 is displaced in the vibration mode of fixed-roll support. As shown at 46, the objective lens holder 69 is displaced in the direction of the arrow (B) without always tilting. The frequency characteristics of this actuator are shown in FIG.
As shown in (2), since the second or higher order vibration mode is suppressed, the control band can be expanded. In the above embodiment, the shape of the elastic shim 71 is formed such that its width is inversely proportional to the value of the primary reference function of the fixed-roll supported beam.
As shown in FIG. 48, similarly, it may be formed so as to be inversely proportional to the value of the quadratic reference function. The principle of operation is exactly the same as described above. The frequency characteristics at that time are shown in FIG.
As shown in second order resonance frequency f ₂ is excited, the other oscillation modes are suppressed, it is possible to set the resonance frequency f ₀ as a so-called system to a higher frequency. Further, the shape of the elastic shim 71 may be set based on a cubic or quaternary reference function depending on the application,
It may be based on the superposition of multiple order reference functions. Also,
The reference function is not limited to the fixed-roll support condition, but may be a reference function based on a fixed-free or free-free support condition. Although the above embodiment has been described with respect to an example in which the focus control is performed, as shown in FIG. 50, the focus control may be performed in the tracking control direction orthogonal to the optical axis of the objective lens 56, that is, in the direction of the arrow (B). Obviously, a similar effect is achieved. Further, it can be easily estimated that a combination of the focus control shown in FIG. 44 and the tracking control shown in FIG. FIG. 51 shows another embodiment for performing the tracking operation of the magnetic head. The magnetic head chip 16a is mounted on the free end of the piezoelectric element 61, and drives the magnetic head chip 16a according to the same principle as described above, so that the track recorded on the magnetic tape and the magnetic head chip 16a are moved.
Control is performed so as to correct the deviation from “a”.

FIG. 52 shows an external magnetic field applying device in an optical disk recording / reproducing device as still another embodiment.
A magnetic head 16 is provided at a free end of the piezoelectric element 61. The distance between the optical disk 10 and the magnetic head 16 is detected by an appropriate method, and the same as described above is used to eliminate a deviation from a predetermined distance. The magnetic head 16 is driven on the principle. In each of the above embodiments, the bimorph piezoelectric element 61 is formed by providing the piezoelectric elements 61a and 61b on both surfaces of the elastic shim 71. However, the bimorph piezoelectric element may be formed by bonding the piezoelectric element to only one side of the elastic shim.

[0034]

As described above, according to the optical disk recording / reproducing apparatus of the first aspect of the present invention, the displacement between the magnetic head and the optical disk recording surface is detected, and the detection signal is
Since the magnetic head is driven by the piezoelectric element actuator, the optical disk surface and the magnetic head surface can be brought close to each other, and the magnetic field fluctuation on the optical disk recording surface due to the optical disk surface deflection can be reduced, thereby improving the efficiency. In addition, the characteristics can be improved, and the arrangement accuracy of each part can be reduced. According to the second aspect of the present invention, a notch for exposing the piezoelectric element is provided at a part of the vibrating end of the bimorph type piezoelectric element, and the third electric terminal connected to the notch is connected to the drive circuit. In addition, since the drive voltage is set based on the acceleration voltage obtained from the third electric terminal, unnecessary resonance vibration can be attenuated to a level that does not hinder control, and the control band of the bimorph piezoelectric element actuator is widened. Has an effect. According to the third aspect of the present invention, since the conductive metal plate of the bimorph type piezoelectric element is determined based on the vibration reference function of the beam, it is possible to suppress a second-order or higher-order resonance level in the frequency characteristics. In addition to being able to set the resonance frequency relatively freely, the control band can be expanded. Further, the displacement position can be made large. As a result, the control performance of the actuator can be improved with a simple structure.

[Brief description of the drawings]

FIG. 1 is a light intensity-distance characteristic diagram in a distance detecting unit according to an example of an optical disk recording / reproducing apparatus.

FIG. 2 is a characteristic diagram showing a distribution of light intensity with respect to a position on an alternate long and short dash line j-j in FIG.

FIG. 3 is a plan view of an optical element arrangement of a distance detecting unit.

FIG. 4 is an output-distance characteristic diagram of both photodetectors.

FIG. 5 is a circuit diagram for obtaining a differential output.

FIG. 6 is a differential output-distance characteristic diagram.

FIG. 7 is an optical element arrangement plan view in consideration of a light intensity distribution of a light source.

FIG. 8 is a plan view of another example of optical element arrangement in consideration of the light intensity distribution of the light source.

9A is a side view and FIG. 9B is a plan view of a main part of the optical disk recording / reproducing apparatus.

FIG. 10 is a plan view of the printed wiring board in FIG. 9;

FIG. 11 is an explanatory diagram of an optical path in FIG.

12A is a plan view of still another example, and FIG. 12B is a cross-sectional view taken along a line kk in FIG.

FIG. 13 is a plan view of another example and a cross-sectional view taken on a plane along line l-l in FIG.

14 is a plan view showing patterning of each wiring to a spacer in FIG.

FIG. 15 is a plan view showing another example of patterning each wiring to the spacer in FIG. 13;

FIG. 16 is an explanatory diagram showing a light state and a light intensity distribution of FIG.

FIG. 17 is an explanatory diagram showing a light state and a light intensity distribution of FIG.

18A is a plan view of still another example, and FIG. 18B is a cross-sectional view taken along a line MM in FIG.

19A is a side view of the spacer in FIG. 18, and FIG.

20 is a plan view showing patterning of each wiring on a printed wiring board of FIG.

FIG. 21 is a side sectional view of still another example.

FIG. 22 is an exploded perspective view of FIG. 21.

FIG. 23 is a connection diagram of the drive circuit of FIG. 21;

FIG. 24 is a side sectional view of a main part of an example of an optical disk recording / reproducing apparatus.

FIG. 25 is an exploded perspective view of the electromagnetic actuator in FIG. 24.

FIG. 26 is a side sectional view of a main part of another example.

FIG. 27 is a sectional side view of a main part of still another embodiment.

FIG. 28 is a side view of a main part of an embodiment of the optical disk recording / reproducing apparatus of claim 1;

FIG. 29 is a perspective view of the piezoelectric actuator in FIG. 28.

FIG. 30 is a partial side view for explaining the operation.

FIG. 31 is a perspective view of a main part of another embodiment.

FIG. 32 is a partial side view for explaining the operation of FIG. 31;

FIG. 33 is a partial side view for explaining the operation of FIG. 31;

FIG. 34 is a diagram of a magnetic field intensity variation on the disk recording surface.

FIG. 35 is a perspective view of a main part of still another embodiment.

FIG. 36 is a side view of the position detection sensor of FIG.

FIG. 37 is an output characteristic diagram of the position detection sensor.

FIG. 38 is a displacement amount-frequency characteristic diagram.

FIG. 39 is a perspective view of a main part of an embodiment of the optical disk recording / reproducing apparatus of claim 2;

FIG. 40 is a diagram showing a displacement position-frequency characteristic diagram of the bimorph type piezoelectric element in FIG. 39.

FIG. 41 is a perspective view of a main part of another embodiment.

FIG. 42 is a side view of the bimorph piezoelectric element shown in FIG. 41.

FIG. 43 is a gain-frequency characteristic diagram of FIG. 42.

FIG. 44 is a perspective view of a main part of an embodiment of an optical disk recording / reproducing apparatus according to claim 3;

FIG. 45 is a plan view of that of FIG. 44.

FIG. 46 is a side view showing the same operation.

FIG. 47 is a frequency characteristic diagram.

FIG. 48 is a plan view of another embodiment.

FIG. 49 is a frequency characteristic line of FIG.

FIG. 50 is a perspective view of still another embodiment.

FIG. 51 is a perspective view of still another embodiment.

FIG. 52 is a perspective view of still another embodiment.

FIG. 53 is a side sectional view of the distance detecting means.

54 is a light intensity-distance characteristic diagram of FIG. 53.

FIG. 55 is a schematic side view of a main part of an optical disk recording / reproducing apparatus.

FIG. 56 is a partial side view for explaining the operation.

FIG. 57 is a graph showing magnetic field strength fluctuation characteristics on the recording surface of the optical disc.

[Explanation of symbols]

Reference Signs List 10 optical disk, 15 optical head, 16 magnetic head, 20 light emitting diode (light source), 21a, 21b
Photodetector, 49 magnetic member (shielding means), 56 objective lens, 61 bimorph piezoelectric element (piezoelectric element actuator), 61a, 61b piezoelectric element, 64 notch,
65, 66, 67 first, second, third electric terminals, 71
Elastic shim (conductive metal plate).

 ──────────────────────────────────────────────────続 き Continuation of the front page (31) Priority claim number Japanese Patent Application No. 63-1778025 (32) Priority date July 19, 1988 (33) (33) Priority claim country Japan (JP) (31) Priority Claim Number Japanese Patent Application No. 1-28597 (32) Priority Date Hei 1 (1989) February 9 (33) Priority Country Japan (JP) (72) Inventor Kazu Nakajima 8-1-1 Honcho Tsukaguchi, Amagasaki City (56) References JP-A-62-264420 (JP, A) JP-A-62-1155 (JP, A) JP-A-52-145011 (JP, A) JP 56-83983 (JP, A) JP-A-62-1131 (JP, A) JP-A-54-70003 (JP, A) Japanese utility model application Sho 61-130017 (JP, U)

Claims (3)

(57) [Claims] 1. A bias magnetic field is provided in the recording portion on the optical disk, and, by irradiating a light spot to record, during reproduction in the optical disk recording and reproducing apparatus for reading information by receiving the reflected light of the recording surface, light Optical head that records and reproduces signals by irradiating the optical disc with light
When, of moving in a radial direction of the optical head integrally with the optical disk
Is, the magnetic head for generating a bias magnetic field consists of a said magnetic head and integrally movable emitting element and a light detector mounted <br/> on the same base, the said magnetic head recording Distance detecting means for detecting the distance between the recording surface and outputting the distance information, and movably supported in a direction substantially perpendicular to the recording surface;
An optical disc recording / reproducing apparatus, comprising: a bimorph-type piezoelectric element actuator that drives the magnetic head so that the distance becomes constant according to the distance detection information. 2. A bimorph-type piezoelectric element having a first electric terminal and a second electric terminal connected thereto, and a driving voltage applied between the first electric terminal and the second electric terminal, the piezoelectric element actuator being adapted to apply a driving voltage to the bimorph piezoelectric element. A driving circuit for displacing the piezoelectric element by a predetermined amount, wherein a part of the vibrating end of the bimorph piezoelectric element is different from a part to which the first electric terminal and the second electric terminal are connected.
A notch for exposing the piezoelectric element is provided, a third electric terminal connected to the notch is connected to the drive circuit, and the drive voltage is set based on an acceleration voltage input from the third electric terminal. 2. The optical disk recording / reproducing apparatus according to claim 1, further comprising the driving circuit. 3. The bimorph comprising: a conductive metal plate whose width is determined based on a vibration reference function of a beam; and a piezoelectric element joined to at least one surface of the conductive metal plate and polarized in a thickness direction. 2. The optical disk recording / reproducing apparatus according to claim 1, wherein a piezoelectric element actuator is formed by the piezoelectric element.