KR100300379B1 - Actuating device for optical pick-up - Google Patents

Abstract

An object of the present invention is to prevent a rotational movement when the movable portion is driven in the tracking direction and to realize a normal tracking servo.

The yoke 3 is attached to the lens holder 1 supporting the objective lens 2, and permanently attached to one inner wall surface 3a of the mutually opposing inner wall surfaces 3a and 3b of the yoke 3. While fixing the magnet 5, the auxiliary yoke 12 is formed so as to cover both end surfaces of the permanent magnet 5. A pair of tracking coils 10, 11 wound on the base 7 in a direction orthogonal to the optical axis of the objective lens 2 and wound in a reverse direction to a part of the focus coil 9. Are bonded to each other and the two tracking coils 10 and 11 are arranged in a direction orthogonal to the focus coil 9. The joining portions of these focus coils 9 and both tracking coils 10 and 11 are inserted into the gap between the permanent magnet 5 and the inner wall surface 3b of the yoke 3 opposite thereto, and the both tracking coils ( When the lens holder 1 is driven in the tracking direction of the objective lens 2 by the current flowing through the 10 and 11, the magnetic flux density at both sides with both tracking coils 10 and 11 interposed between the auxiliary yoke By homogenizing by (12), generation of a rotation moment is suppressed and normal tracking servo is made.

Description

Actuator device of optical pickup {ACTUATING DEVICE FOR OPTICAL PICK-UP}

The present invention relates to an optical pickup actuator device for recording or reproducing information on a medium such as a compact disc or a mini disc.

Fig. 6 is a perspective view showing an actuator device of a conventional optical pickup, Fig. 7 is a plan sectional view showing a magnetic circuit of the actuator device, and Fig. 8 is an explanatory view of a tracking coil provided in the actuator device, in which reference numerals are used in these drawings. 1 denotes a lens holder, and an objective lens 2 and a yoke 3 are attached to the lens holder 1. The yoke 3 is a demagnetized magnetic body having an open top, and the top yoke 4 is joined to the open end to form a closed path. Permanent magnets 5 are attached to one of the inner wall surfaces 3a and 3b of the yoke 3 which are opposed to each other, and the magnetic circuit is formed by the yoke 3 and the permanent magnets 5. Is composed. The component on the lens holder 1 side including this magnetic circuit forms a movable portion. The lens holder 1 is movable by attaching the lens holder 1 to the standing portion 7a of the base 7 via four wires 6. The part is elastically supported by the standing part 7a of the base 7 which forms the fixed part.

The focus coil 9 is attached to the base 7 via the bobbin 8, and the focus coil 9 is wound in a frame shape in a direction orthogonal to the optical axis of the objective lens 2. A pair of tracking coils 10 and 11 are adhered to a part of the focus coil 9, and both tracking coils 10 and 11 are arranged side by side in a direction orthogonal to the focus coil 9. As shown in Fig. 8, both tracking coils 10 and 11 are wound in opposite directions so that when current is supplied in a direction indicated by a solid line or broken line in the same figure, current in the same direction flows to adjacent effective portions 10a and 11a. It is wired so that As in FIG. 7, the junction of the focus coil 9 and both tracking coils 10, 11 is inserted in the gap between the permanent magnet 5 and the inner wall surface 3b of the yoke 3 opposite thereto, The magnetic flux from the permanent magnet 5 to the inner wall surface 3b, that is, the magnetic flux in the Y direction of the coordinate axis as shown in Fig. 6, intersects the current flowing through each of the coils 9, 10, 11. Therefore, the force in the Z direction of the coordinate axis acts by the current flowing through the focus coil 9, and the lens holder 1 acts in the focus direction of the objective lens 2, that is, in the Z direction. Similarly, a force in the X direction of the coordinate axis also acts by the current flowing in the adjacent effective portions 10a and 11a between the two tracking coils 10 and 11 so that the lens holder 1 moves in the tracking direction of the objective lens 2. do.

By the way, in the actuator device of the above-mentioned conventional optical pickup actuator device, as shown in Fig. 7, besides the magnetic flux directed from the permanent magnet 5 to the inner wall surface 3b of the yoke 3, Since both magnetic fluxes are directed to the tracking coils 10 and 11 in the inclined direction and the like, the magnetic flux density distributions on both sides between the tracking coils 10 and 11 are close to the permanent magnets 5 side, and the inner wall surface is inclined. The side (3b) is in a slight unbalanced state. Here, when both tracking coils 10 and 11 are caught with elemental stones, the direction in which both tracking coils 10 and 11 are wound in the reverse direction, for example, in the solid line of FIG. 8 to both tracking coils 10 and 11. When current flows in the direction shown, the permanent magnet 5 side of one tracking coil 10 becomes the N pole, and the permanent magnet 5 side of the other tracking coil 11 becomes the S pole. Therefore, as indicated by the black arrows in FIG. 7, due to the imbalance of the distribution state of the magnetic flux density, the force attracted to the permanent magnet 5 side acts on the one tracking coil 10, and the other With respect to the tracking coil 11, the force repulsed by the permanent magnet 5 acts, and a rotation moment is generated by these forces. As a result, there was a problem that an unnecessary rotational motion was caused in the movable portion including the lens holder 1 and the dynamic characteristics of the high frequency region were shaken (see Fig. 9).

In addition, this problem is not limited to a moving magnet (MM) actuator device having a magnetic circuit attached to the movable part side, but also to a moving coil (MC) actuator device having a focus coil and a tracking coil attached to the movable part side. Occurs.

1 is a perspective view showing an actuator device of an optical pickup according to an embodiment;

2 is a plan sectional view showing a main portion of the actuator device;

3 is a perspective view showing components of a magnetic circuit;

4 is a plan sectional view of the magnetic circuit;

5 is an explanatory diagram showing frequency characteristics of the actuator device;

6 is a perspective view showing an actuator device of a conventional optical pickup;

7 is a plan sectional view showing a magnetic circuit of the actuator device;

8 is an explanatory diagram of a tracking coil provided in the actuator device;

9 is an explanatory diagram showing a frequency characteristic of a conventional actuator device.

* Description of the symbols for the main parts of the drawings *

1: Lens holder 2: Objective lens

3: yoke 3a, 3b: inner wall surface

5: permanent magnet 6: wire

7: base 9: focus coil

10, 11: tracking coil 12: auxiliary yoke

The present invention forms an auxiliary yoke for reducing the magnetic flux on the side of the magnet, and the winding direction is reversed so that the magnetic flux does not face the oblique direction with respect to the pair of tracking coils provided in parallel. Forming such an auxiliary yoke eliminates the imbalance of the magnetic flux density on both sides of the tracking coil, so that unnecessary rotational movement can be prevented from being caused in the movable portion.

In the optical pickup actuator device according to the present invention, a lens holder holding an objective lens, a focus coil wound in a direction orthogonal to the optical axis of the objective lens, and a direction in which the winding coil is arranged in a direction orthogonal to the focus coil are reversed. Magnets and yokes having a pair of tracking coils and opposing surfaces facing each other with the focusing coil and tracking coils interposed therebetween and generating magnetic fluxes directed from one opposing surface to the other opposing surface; An auxiliary yoke disposed at both cross-sections along the parallel direction of the tracking coil, wherein the lens holder is moved in the focus direction and by the interaction of the current flowing through the focus coil and the tracking coil with the magnetic flux from the magnet. It was configured to drive in the tracking direction.

In this configuration, since the magnetic flux from both end faces of the magnet is reduced by the auxiliary yoke, the magnetic flux in the oblique direction with respect to the pair of tracking coils in both end faces of the magnet decreases, so that the magnetic flux density on both sides of the tracking coil is reduced. Roughness can be made uniform. As a result, unnecessary rotational motion is not induced in the movable portion including the lens holder, thereby maintaining the dynamic characteristics of the normal high frequency region (see FIG. 5).

The above configuration can be applied to an actuator device of a moving coil method, but is particularly effective when applied to a moving magnet method in which a component of a magnetic circuit is attached to the movable part side.

In addition, although two magnets may be disposed on opposite surfaces of the yoke opposite to each other with the tracking coil interposed therebetween, the magnets may be disposed on one opposite surface of the yoke to reduce the movable portion. Since the imbalance of magnetic flux density in both sides of a tracking coil becomes remarkable, it is also effective to apply it to the actuator apparatus of a moving magnet system also in this point.

In addition, the auxiliary yoke may be post-attached to a separate component to the yoke, but by forming the auxiliary yoke integrally bent to the side of the yoke can reduce the number of parts can simplify the assembly work. .

EXAMPLE

1 is a perspective view showing an actuator device of an optical pickup, FIG. 2 is a plan sectional view showing the main part of the actuator device, FIG. 3 is a perspective view showing components of a magnetic circuit, and FIG. It is a flat sectional view of the said magnetic circuit, and the same code | symbol is attached | subjected to the part corresponding to FIGS.

The optical pickup actuator according to the present embodiment differs from the above-described conventional example in that the auxiliary yoke 12 is provided at both ends along the parallel direction of the tracking coils 10 and 11 in the permanent magnet 5. ), And the other configurations are basically the same. That is, the auxiliary yoke 12 bent at an almost right angle with respect to one inner wall surface 3a is integrally formed in the both side parts of the depressed yoke 3 which opened the upper end, and these auxiliary yoke ( 12 extends toward the other inner wall surface 3a so as to cover both end surfaces of the permanent magnet 5 attached to one inner wall surface 3b. These auxiliary yokes 12 reduce the magnetic flux in the oblique direction with respect to both tracking coils 10 and 11 in the permanent magnets 5, so that the yoke 3 in the permanent magnets 5 as shown in FIG. Only the magnetic flux directed to the inner wall surface 3b of the cross section is generated, and the magnetic flux density distributions on both the left and right sides of the same figure with the tracking coils 10 and 11 are almost similar.

In the optical pick-up actuator device configured as described above, the movable portion including the lens holder 1 is driven in the focusing direction of the objective lens 2 by the current flowing through the focus coil 9, so that both tracking coils 10 and 11 are operated. The point in which the movable part including the lens holder 1 is driven in the tracking direction of the objective lens 2 by the current flowing in the same manner as in the conventional example, but when the movable part is driven in the tracking direction, both tracking coils 10 and 11 The magnetic flux densities on both the right and left sides between the two sides are equalized by the auxiliary yoke 12 so that the generation of the rotation moment is suppressed. Therefore, unnecessary rotational motion is not induced in the movable portion including the lens holder 1, so that the dynamic characteristics of the normal high frequency region can be maintained.

In the above embodiment, the case where the auxiliary yoke 12 is integrally bent and formed on both side portions of the yoke 3 has been described, but the auxiliary yoke 12 formed separately from the yoke 3 is described. May be post-attached and integrated. Conventionally, the auxiliary yoke 12 does not necessarily cover all of the side cross-sections of the permanent magnets 5, but causes the imbalance of the magnetic flux density distribution on both sides with the tracking coils 10 and 11 interposed therebetween. If the magnetic flux can be reduced, the auxiliary yoke 12 may be arranged so as to cover a part of the side cross section of the permanent magnet 5.

This invention is implemented by the form as demonstrated above, and the effect described below is acquired.

A lens holder for holding an objective lens, a focus coil wound in a direction orthogonal to the optical axis of the objective lens, a pair of tracking coils arranged in parallel with and wound in a direction orthogonal to the focus coil, and the focus coil And magnets and yokes having opposing surfaces facing each other with the tracking coils interposed therebetween, generating magnetic fluxes from one opposing surface to the other opposing surface, and both end surfaces along the parallel direction of the tracking coils in the magnets. When the lens holder is configured to drive the lens holder in the focusing direction and the tracking direction by an interaction between the current flowing through the focusing coil and the tracking coil and the magnetic flux from the magnet, the auxiliary yoke is disposed at both sides of the magnet. Since the magnetic flux from the cross section is reduced by the auxiliary yoke, a pair of traces The magnetic flux toward the coil in the oblique direction decreases, so that the density of the magnetic flux density on both sides of the tracking coil can be equalized, and as a result, unnecessary rotational movement is not caused in the movable part including the lens holder. The dynamic characteristics of a normal high frequency region can be maintained.

While preferred embodiments of the present invention have been described using specific terms, such descriptions are for illustrative purposes only and various changes and modifications may be made without departing from the spirit and scope of the following claims. It must be understood.

Claims (2)

A lens holder for holding an objective lens, a focus coil wound in a direction orthogonal to the optical axis of the objective lens, a pair of tracking coils arranged in parallel with and wound in a direction orthogonal to the focus coil, and the focus coil And generating a magnetic flux directed to the other opposite surface across the part of the yoke having opposing surfaces facing each other with the tracking coil interposed therebetween, and a portion of the focus coil and the tracking coil disposed on one opposite surface of the yoke. And a lens holder connected to the other opposite surface side of the yoke, and the lens holder moves in the focusing direction or the tracking direction together with the yoke by energizing the focus coil or the tracking coil. In the actuator apparatus of the present invention, the magnet is located on one opposite surface side of the yoke. Standing along the juxtaposition direction of the tracking coil and the secondary yoke are installed on both sides, the actuator of the optical pickup device, comprising a step of reducing the magnetic flux generated obliquely towards each tracking coil from the side end portion of the magnet. The optical pickup actuator device according to claim 1, wherein the auxiliary yoke is formed integrally bent at the side of the yoke.