WO2000045383A1 - Optical head - Google Patents
Optical head Download PDFInfo
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- WO2000045383A1 WO2000045383A1 PCT/JP2000/000330 JP0000330W WO0045383A1 WO 2000045383 A1 WO2000045383 A1 WO 2000045383A1 JP 0000330 W JP0000330 W JP 0000330W WO 0045383 A1 WO0045383 A1 WO 0045383A1
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- WIPO (PCT)
- Prior art keywords
- light
- light beam
- optical head
- recording medium
- information recording
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- G—PHYSICS
- G11—INFORMATION STORAGE
- G11B—INFORMATION STORAGE BASED ON RELATIVE MOVEMENT BETWEEN RECORD CARRIER AND TRANSDUCER
- G11B7/00—Recording or reproducing by optical means, e.g. recording using a thermal beam of optical radiation by modifying optical properties or the physical structure, reproducing using an optical beam at lower power by sensing optical properties; Record carriers therefor
- G11B7/12—Heads, e.g. forming of the optical beam spot or modulation of the optical beam
- G11B7/135—Means for guiding the beam from the source to the record carrier or from the record carrier to the detector
- G11B7/1353—Diffractive elements, e.g. holograms or gratings
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- G—PHYSICS
- G11—INFORMATION STORAGE
- G11B—INFORMATION STORAGE BASED ON RELATIVE MOVEMENT BETWEEN RECORD CARRIER AND TRANSDUCER
- G11B7/00—Recording or reproducing by optical means, e.g. recording using a thermal beam of optical radiation by modifying optical properties or the physical structure, reproducing using an optical beam at lower power by sensing optical properties; Record carriers therefor
- G11B7/12—Heads, e.g. forming of the optical beam spot or modulation of the optical beam
- G11B7/135—Means for guiding the beam from the source to the record carrier or from the record carrier to the detector
- G11B7/1395—Beam splitters or combiners
Definitions
- the present invention relates to an optical head for optically recording or reproducing information on an information recording medium such as an optical disk.
- FIG. 7 is a conceptual diagram of a conventional optical head.
- 100 (100a, 100Ob) is the optical axis of the optical system
- 101 is a light source such as a semiconductor laser
- 102 is a diffractive element having a uniform diffraction grating
- 103 Is an objective lens
- 104 is an information recording medium
- 105 is a half mirror that transmits and reflects part of light
- 106 is a detection lens formed of a cylindrical lens, etc.
- 107 Is a light receiving element and 110 is a track direction.
- the luminous flux emitted from the light source 101 is converted into three luminous fluxes by the diffractive element 102 as the 0th, + 1st, and-1st-order diffracted light, as represented by the light rays indicated by the arrows in the figure. Branched. These light beams pass through the half mirror 105 and are condensed on the information recording medium 104 by the objective lens 103, and three light spots are generated on the information recording medium 104.
- the 0th-order diffracted light of the three light fluxes becomes a light spot (hereinafter, referred to as “main spot”) used for recording or reproducing information, and has an optical axis of 100 °.
- the first- and first-order diffracted lights are located on the two light spots (hereinafter, “sub-spots”) located at a distance from the optical axis 100 a as shown by the light ray 109 in the figure. It becomes.
- FIG. 8 is a diagram showing three light spots generated on the information track of the information recording medium 104.
- FIG. 8A is a plan view
- FIG. 8B is a cross-sectional view in a direction perpendicular to the track direction 110 of FIG. 8A.
- the two sub-spots 1 1 2 are separated from each other in the direction perpendicular to the track direction 1 1 0 by about 1 Z 4 of the continuous groove cycle, that is, the track cycle, about the main spot 1 1 1 Is located.
- the light reflected by the information recording medium 104 passes through the objective lens 103 again as shown in FIG. 7, is reflected by the half mirror 105, and is received by the light receiving element via the detection lens 106. Guided on 107.
- the detection lens 106 has a function of giving astigmatism to a light beam in order to detect a focus error signal by a known so-called astigmatism method.
- Light reflected from the main spot travels along the optical axes 100a and 100b, and is collected at the intersection of the light receiving element 107 and the optical axis 100b.
- the reflected light from the sub-spot is converged at a position away from the optical axis 100b as shown by a light ray 113.
- the light receiving element 107 has a light detection unit that receives each of these three light beams.
- the luminous flux from the main spot is used to detect the focus error signal and the information signal, and the luminous flux from the two sub-spots is used to detect the tracking error signal by differential calculation of the detection signals.
- FIG. 9 is a diagram illustrating the diffraction element 102.
- a diffraction grating having a uniform period with a stripe pattern is uniformly formed ;
- a circle 108 indicates a range through which light serving as a main beam passes.
- Such a diffraction grating having a uniform period spatially and uniformly divides a passing light beam into 0th, + 1st and 1st order diffracted lights.
- a main beam and two sub beams are generated using such a diffraction element.
- the diffraction efficiency of the diffraction element was generally about 70% for the 0th order, and about 10% for each of the + 1st and 1st orders.
- a main beam and a sub-beam are generated by spatially and uniformly splitting a light beam using a diffraction element having a uniform diffraction grating. Therefore, the transmittance of the main beam in the optical path from the light source to the information recording medium is inevitably reduced by the zero-order diffraction efficiency of the diffraction element.
- the present invention has been made to solve the conventional problems as described above, and an optical head which can improve the transmittance of a main beam in an optical path from a light source to an information recording medium and can obtain a sufficient amount of sub-beams.
- the goal is to realize it.
- an optical head comprises: a light source; a light branching unit that branches light emitted from the light source into a plurality of light beams; and a light beam branched by the light branching unit.
- Focusing means for focusing on a recording medium; A first portion that forms a first light beam that is not substantially diffracted or deflected to the light emitted from the light source; and a second light beam that is diffracted or deflected.
- the second light flux among the light emitted from the light source, passes on the light branching means outside the light that becomes the first light flux. It is characterized by being formed using light.
- the transmittance of the first light flux (for example, the main beam) in the optical path from the light source to the information recording medium can be improved, and the optical head using the light source with low light output can be improved.
- a width of the first portion in the track direction of the information recording medium is substantially equal to a light beam diameter on the light branching device of the light beam limited by the entrance pupil of the light collecting device. It is preferred that they have the same size.
- the first light flux restricted by the entrance pupil of the light condensing means is a light flux that has passed through the first portion, so that the transmittance of the first light flux is increased. Can be improved.
- the first portion is a portion where no diffraction grating is formed
- the second portion is a portion where a diffraction grating is formed.
- the light source and the light source so that the area of the light flux occupying on the entrance pupil of the light focusing means is about half or more of the area of the entrance pupil.
- the light splitting means and the light collecting means are arranged. According to the optical head as described above, the light amount of the second light beam can be made sufficiently large, and the second light beam can be used as a sub-beam having a sufficient light amount necessary for detecting a tracking error signal. Further, it is preferable that the second portion is formed of two diffraction grating forming portions formed on both sides of the first portion in the track direction of the information recording medium with the first portion interposed therebetween. .
- the first light beam is used for recording information on the information recording medium or for recording information on the information recording medium. It is preferable that the second light beam is a light beam for performing tracking control at the time of recording or reproducing information on the information recording medium.
- the second light beam has at least one pair of light beams, and the pair of light beams is collected on the information recording medium by the light condensing means at an interval obtained by multiplying about 1 Z2 of the track pitch by an integer.
- the light is emitted and reflected by the information recording medium and used for detecting a tracking error.
- FIG. 1 is a configuration diagram of an optical head according to an embodiment of the present invention.
- FIG. 2 is a plan view of an optical branching element used for an optical head according to an embodiment of the present invention.
- FIG. 3 is a diagram illustrating an arrangement of a light source, a light splitting element, and an objective lens of an optical head according to an embodiment of the present invention.
- FIG. 4 is a view for explaining a sub beam generated by the optical branching device according to the embodiment of the present invention.
- FIG. 5 is a diagram illustrating a spot formed by the optical head according to one embodiment of the present invention.
- FIG. 6 is a diagram illustrating a spot formed by an optical head according to another embodiment of the present invention.
- Fig. 7 is a block diagram of an example of a conventional optical head.
- FIG. 8 is a diagram illustrating a spot formed by an optical head.
- FIG. 9 is a diagram illustrating an example of a diffraction element of a conventional optical head.
- FIG. 1 is a configuration diagram of an optical system of an optical head according to an embodiment of the present invention.
- 1 is a light source such as a semiconductor laser
- 2 is a diffraction element as a light splitting means
- 3 is an objective lens
- 4 is an information recording medium
- 5a to 5e are light beams split by the diffraction element 2
- 6 is an optical system.
- the optical axis, 8 is a detection lens formed of a cylindrical lens or the like
- 9 is a light receiving element
- 15 is a track direction
- D 1 is the diameter of the aperture (entrance pupil) of the objective lens 3.
- FIG. 2 is a conceptual diagram of a diffraction grating formed on the diffraction element 2.
- the striped regions 2a and 2b indicate the regions where the diffraction grating is formed. No diffraction grating is formed in the portion sandwiched between the regions 2a and 2b in the track direction 15.
- the region 10 is a part of the region where the diffraction grating is not formed.
- the area 10 indicates an area inside the circle 10a, and the main beam passes through the area 10a.
- the diameter D2 of the circle 10a which is the outer periphery of this area 10, is equal to the diameter of the light beam on the light branching means 2 for the light beam limited by the aperture of the diameter D1 corresponding to the entrance pupil of the objective lens 3. .
- the distance d3 between the regions 2a and 2b is approximately equal to the diameter D2 of the circle 10a.
- the light emitted from the light source 1 enters the diffraction element 2 and is split into a plurality of light beams.
- the light beam used as the main beam is the diffraction grating of the diffraction grating 2 like the light beam 5c. This is a light beam that passes through the non-formed portion.
- the luminous flux used as the sub-beam is, for example, the + 1st-order diffracted light in the area 2a as a light beam 5a, the first-order diffracted light as a light beam 5b, and the + 1st-order diffracted light in the area 2b as a light beam 5d.
- the first-order diffracted light is a light beam 5e
- it is two diffracted light beams branched in the directions indicated by the light beams 5b and 5d.
- the main beam and the two sub-beams pass through the half mirror 7 and are focused on the information recording medium 4 by the objective lens 3 to generate three light spots.
- the reflected light from these light spots passes through the objective lens 3 again, is reflected by the half mirror 17, and is guided to the light receiving element 9 via the detection lens 8.
- the position of each light beam guided to the light receiving element 9 and a method of detecting a focus error signal, a tracking error signal, and an information signal using these light beams are the same as in the conventional example, and therefore description thereof is omitted. I do.
- the diffracted lights indicated by the light beams 5a and 5e do not pass through the aperture of the objective lens 3, and thus become unutilized light beams.
- the diffraction grating for generating the sub-beam is located at a position away from the optical axis as in the areas 2a and 2b in Fig. 2, the sub-beam will pass through the aperture of the objective lens sufficiently.
- the distance between the light source 1 and the diffraction element 2 needs to be sufficiently close to satisfy a certain condition. This condition will be described with reference to FIG.
- FIG. 3 is a configuration diagram illustrating an arrangement of a light source, a light splitting element, and an objective lens in an optical head according to an embodiment of the present invention. Elements having the same configurations as those in FIG. 11 is a surface set up at the light source position.
- the conjugate image plane formed by the objective lens 3 is the plane 11.
- the conjugate image height of the objective lens 3 of one of the sub spots generated on the information recording medium 4 is y1, the distance between the boundary between the diffraction grating forming portion and the non-forming portion and the optical axis is y2, yl,
- the condition that the sub-beam passes through more than half of the aperture area of the objective lens 3 is, for example, the following equation (2) when the upper part of FIG.
- Equation (4) y 2> NA * d 1
- FIG. 4 is a diagram showing a state where the sub-beam generated by such a diffraction element passes through the aperture of the objective lens 3 as viewed from the light source 1 side.
- the hatched portion 12 diffracts in the region 2a in FIG. 2 and the sub-beam represented by the light beam 5b in FIG. 1.
- the hatched portion 13 diffracts in the region 2b in FIG. 2 and the light beam in FIG.
- the sub-beam represented by 5d is shown.
- the cross-hatched portion at the center indicates an area where the two sub-beams overlap.
- Circle 14 indicates the aperture (diameter D1) of the objective lens.
- FIG. 4 shows that each of the two sub-beams passes through at least half of the aperture of the objective lens 3. If the area of the passing light beam occupies more than half of the objective lens aperture, the numerical aperture in the direction perpendicular to the track can be secured, so the focused sub-beam is small enough to detect the tracking error signal. It becomes
- Equations (1) to (4) are equations derived from the relationship between the light source, the diffraction element, and the objective lens. However, the equations (1) to (4) are optical systems having other lenses such as a collimated lens. However, it is clear that a similar idea can be applied. is there.
- the transmittance of the main beam is improved by using the diffraction element having the diffraction grating non-forming portion in the area where the main beam passes, and the + 1st-order and 1st-order beams in the diffraction grating forming portion are improved.
- the secondary diffraction efficiency can be set arbitrarily irrespective of the main beam intensity by adjusting the arrangement of the elements, so that a sufficient sub-beam intensity can be obtained.
- the case where a diffraction element having a normal diffraction grating is used as the light branching unit has been described.
- the diffraction grating is blazed, and the light beams 5b and 5d shown in FIG. 1 are used. If a diffraction element with an increased diffraction efficiency of the diffracted light is used, the light amount of the sub-beam can be further increased. As a result, the quality of the tracking error signal can be further improved.
- FIG. 8 shows an example in which two sub-spots are arranged at an interval of 1 Z 2 of the track pitch in a direction perpendicular to the track.
- the present invention is not limited to such a subspot arrangement.
- Figures 5 and 6 show other examples of subspot arrangements.
- FIGS. 5 (a) and 6 (a) are plan views of a part of the information recording medium
- FIGS. 5 (b) and 6 (b) are the tracks of FIGS. 5 (a) and 6 (a), respectively.
- 2 shows a cross-sectional view in a direction perpendicular to the direction.
- the optical system has a structure in which two sub-spots 18 are arranged at an interval of the information track 16's track pitch (1/2 of the track pitch). May be used.
- Such an optical head has a main spot 17 and a sub spot 18 Divides each light beam by the far field to detect a signal
- the two sub-spots 18 are arranged at an interval of twice the track pitch of the information track 16 (four times the track pitch of 1Z2),
- the present invention can also be applied to an optical disc device in which information is recorded and reproduced on three information tracks 16 at the same time by the main spot 17 and the two sub spots 18.
- a light beam other than a light beam used for recording or reproducing information is generated by using a light beam in a range not conventionally used.
- the ratio of using the light emitted from the light source can be improved.
- the present invention can be used for an optical head of a type that operates by condensing a plurality of light beams on an information recording medium, and an optical head using a light source with a smaller light output than before. Can be realized.
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Abstract
Description
明 細 書 光学へッド 技術分野 Description Optical head Technical field
本発明は、 光ディスクなどの情報記録媒体に、 光学的に情報の記録又 は再生を行うための光学ヘッドに関する。 背景技術 The present invention relates to an optical head for optically recording or reproducing information on an information recording medium such as an optical disk. Background art
従来から、 光学へッドの代表的なトラッキングエラ一信号検出方式の 一つとして、 いわゆる 3ビーム方式が知られている。 以下図面を参照し ながら、 この 3ビーム方式の光学ヘッドについて説明しつつ、 従来の技 術を説明する。 Conventionally, a so-called three-beam method has been known as one of the typical tracking error signal detection methods for optical heads. Hereinafter, the conventional technology will be described while describing the three-beam optical head with reference to the drawings.
図 7は、 従来の光学ヘッドの概念図である。 1 0 0 ( 1 0 0 a、 1 0 O b ) は光学系の光軸、 1 0 1は半導体レーザー等の光源、 1 0 2は一 様に回折格子が形成された回折素子、 1 0 3は対物レンズ、 1 0 4は情 報記録媒体、 1 0 5は光の一部を透過して一部を反射するハーフミラー、 1 0 6は円柱レンズ等で形成された検出レンズ、 1 0 7は受光素子、 1 1 0はトラック方向である。 FIG. 7 is a conceptual diagram of a conventional optical head. 100 (100a, 100Ob) is the optical axis of the optical system, 101 is a light source such as a semiconductor laser, 102 is a diffractive element having a uniform diffraction grating, 103 Is an objective lens, 104 is an information recording medium, 105 is a half mirror that transmits and reflects part of light, 106 is a detection lens formed of a cylindrical lens, etc., 107 Is a light receiving element and 110 is a track direction.
光源 1 0 1から発した光束は、 図中の矢印で示した光線で表されるよ うに、 回折素子 1 0 2によって、 0次、 + 1次、 及び— 1次回折光とし て 3つの光束に分岐される。 これら光束は、 ハーフミラ一 1 0 5を透過 し、 対物レンズ 1 0 3により情報記録媒体 1 0 4上に集光され、 3つの 光スポッ卜が情報記録媒体 1 0 4上に生成される。 The luminous flux emitted from the light source 101 is converted into three luminous fluxes by the diffractive element 102 as the 0th, + 1st, and-1st-order diffracted light, as represented by the light rays indicated by the arrows in the figure. Branched. These light beams pass through the half mirror 105 and are condensed on the information recording medium 104 by the objective lens 103, and three light spots are generated on the information recording medium 104.
前記 3つの光束のうち 0次回折光は、 情報の記録又は再生に用いられ る光スポット (以下、 「メインスポット」という。 ) となって光軸 1 0 0 a上に位置し、 + 1次及び— 1次回折光は、 図中の光線 1 0 9が示すよ うに、 光軸 1 0 0 aから離れて位置する 2つの光スポット (以下、 「サ ブスポット」という。 ) となる。 The 0th-order diffracted light of the three light fluxes becomes a light spot (hereinafter, referred to as “main spot”) used for recording or reproducing information, and has an optical axis of 100 °. The first- and first-order diffracted lights are located on the two light spots (hereinafter, “sub-spots”) located at a distance from the optical axis 100 a as shown by the light ray 109 in the figure. It becomes.
図 8は、 情報記録媒体 1 0 4の情報トラック上に生成された、 3つの 光スポットを示す図である。 図 8 ( a ) は平面図を、 図 8 ( b ) は図 8 ( a ) のトラック方向 1 1 0と垂直な方向の断面図を示している。 本図 に示したように、 2つのサブスポット 1 1 2は、 メインスポット 1 1 1 を中心として連続溝周期すなわちトラック周期の約 1 Z 4ずつ、 トラッ ク方向 1 1 0に垂直な方向に離れて位置している。 FIG. 8 is a diagram showing three light spots generated on the information track of the information recording medium 104. As shown in FIG. 8A is a plan view, and FIG. 8B is a cross-sectional view in a direction perpendicular to the track direction 110 of FIG. 8A. As shown in this figure, the two sub-spots 1 1 2 are separated from each other in the direction perpendicular to the track direction 1 1 0 by about 1 Z 4 of the continuous groove cycle, that is, the track cycle, about the main spot 1 1 1 Is located.
情報記録媒体 1 0 4で反射された光はそれぞれ、 図 7に示したように 対物レンズ 1 0 3を再び通過し、 ハーフミラ一 1 0 5で反射され、 検出 レンズ 1 0 6を介して受光素子 1 0 7上に導かれる。 検出レンズ 1 0 6 は、 周知のいわゆる非点収差法によるフォーカスエラ一信号を検出する ために、 光束に非点収差を与える機能を有している。 The light reflected by the information recording medium 104 passes through the objective lens 103 again as shown in FIG. 7, is reflected by the half mirror 105, and is received by the light receiving element via the detection lens 106. Guided on 107. The detection lens 106 has a function of giving astigmatism to a light beam in order to detect a focus error signal by a known so-called astigmatism method.
メインスポットからの反射光は光軸 1 0 0 a、 1 0 O bに沿って進み、 受光素子 1 0 7と光軸 1 0 0 bとの交点に集光される。 サブスポットか らの反射光は、 光線 1 1 3に示すように、 光軸 1 0 0 bから離れた位置 に集光される。 受光素子 1 0 7は、 これら 3つの光束を各々受光する光 検出部を有している。 メインスポットからの光束は、 前記のフォーカス エラー信号の検出と、 情報信号の検出とに用いられ、 2つのサブスポッ 卜からの光束は、 検出信号の差動演算によって、 トラッキングエラー信 号の検出に用いられる。 Light reflected from the main spot travels along the optical axes 100a and 100b, and is collected at the intersection of the light receiving element 107 and the optical axis 100b. The reflected light from the sub-spot is converged at a position away from the optical axis 100b as shown by a light ray 113. The light receiving element 107 has a light detection unit that receives each of these three light beams. The luminous flux from the main spot is used to detect the focus error signal and the information signal, and the luminous flux from the two sub-spots is used to detect the tracking error signal by differential calculation of the detection signals. Can be
ここで、 以下の説明では、 便宜上、 メインスポットを生成する光束を メインビームと呼び、 サブスポットを生成する光束をサブビームと呼ぶ ことにする。 図 9は、 回折素子 1 0 2を説明する図である。 回折素子 1 0 2上には、 縞模様状の均一な周期の回折格子が一様に形成されている ; 円 1 0 8は、 メインビームとなる光が通過する範囲を示している。 この ような均一な周期の回折格子は、 通過する光束を 0次、 + 1次、 及び一 1次回折光として、 空間的に均一に振幅分割する。 Here, in the following description, for convenience, the light beam generating the main spot is referred to as a main beam, and the light beam generating the sub spot is referred to as a sub beam. FIG. 9 is a diagram illustrating the diffraction element 102. On the diffractive element 102, a diffraction grating having a uniform period with a stripe pattern is uniformly formed ; A circle 108 indicates a range through which light serving as a main beam passes. Such a diffraction grating having a uniform period spatially and uniformly divides a passing light beam into 0th, + 1st and 1st order diffracted lights.
従来の光学ヘッドでは、 このような回折素子を用いて、 メインビーム 及び 2つのサブビームを発生させていた。 その回折素子の回折効率は、 0次が 7 0パーセント程度、 + 1次及び一 1次が各々 1 0パーセント程 度が一般的であった。 In a conventional optical head, a main beam and two sub beams are generated using such a diffraction element. The diffraction efficiency of the diffraction element was generally about 70% for the 0th order, and about 10% for each of the + 1st and 1st orders.
しかしながら、 前記のような従来の光学ヘッドの構成では、 均一な回 折格子が形成された回折素子を用いて、 光束を空間的に均一に振幅分割 することによって、 メインビーム及びサブビームを発生させているため、 光源から情報記録媒体に至る光路でのメインビームとしての透過率は、 回折素子の 0次回折効率分だけ低下するのは避けられない。 However, in the configuration of the conventional optical head as described above, a main beam and a sub-beam are generated by spatially and uniformly splitting a light beam using a diffraction element having a uniform diffraction grating. Therefore, the transmittance of the main beam in the optical path from the light source to the information recording medium is inevitably reduced by the zero-order diffraction efficiency of the diffraction element.
また、 0次回折効率の増加は + 1次及び— 1次回折光を減らすことに なるため、 十分なサブビーム光量を得るためには 0次回折効率の増加に は制限がある。 すなわち、 情報の記録のために必要な光量をメインビー ムに確保するためには、 光源として高い光出力を有する半導体レーザー が必要であった。 発明の開示 In addition, since an increase in the 0th-order diffraction efficiency reduces the + 1st-order and −1st-order diffracted light, there is a limit to the increase in the 0th-order diffraction efficiency in order to obtain a sufficient amount of sub-beams. In other words, a semiconductor laser having a high light output was required as a light source in order to secure the amount of light necessary for recording information in the main beam. Disclosure of the invention
本発明は、 前記のような従来の問題を解決するものであり、 光源から 情報記録媒体に至る光路におけるメインビームの透過率を向上させつつ、 しかも十分なサブビーム光量が得られる光学へッドを実現することを目 的とする。 SUMMARY OF THE INVENTION The present invention has been made to solve the conventional problems as described above, and an optical head which can improve the transmittance of a main beam in an optical path from a light source to an information recording medium and can obtain a sufficient amount of sub-beams. The goal is to realize it.
前記目的を達成するために、 本発明の光学ヘッドは、 光源と、 前記光 源から放射される光を複数の光束に分岐させる光分岐手段と、 前記光分 岐手段によって分岐された光束を情報記録媒体に集光させる集光手段と を備え、 前記光分岐手段は前記光源から放射された光に、 実質的に回折 又は偏向を加えていない第 1の光束を形成する第 1の部分と、 回折又は 偏向を加えた第 2の光束を形成する第 2の部分とを有し、 前記第 2の光 束は、 前記光源から放射される光のうち、 前記光分岐手段上において前 記第 1の光束となる光よりも外側を通る光を用いて形成されることを特 徴とする。 前記のような光学ヘッドによれば、 光源から情報記録媒体に 至る光路における第 1の光束 (例えばメインビーム) の透過率を向上さ せることができ、 低い光出力の光源を用いた光学へッドを実現できる。 前記光学へッドにおいては、 前記第 1の部分の前記情報記録媒体の卜 ラック方向における幅は、 前記集光手段の入射瞳で制限される光束の前 記光分岐手段上の光束径とほぼ同一の大きさであることが好ましい。 前 記のような光学へッドによれば、 集光手段の入射瞳で制限される第 1の 光束は、 第 1の部分を通過した光束であるため、 第 1の光束の透過率を より向上させることができる。 In order to achieve the above object, an optical head according to the present invention comprises: a light source; a light branching unit that branches light emitted from the light source into a plurality of light beams; and a light beam branched by the light branching unit. Focusing means for focusing on a recording medium; A first portion that forms a first light beam that is not substantially diffracted or deflected to the light emitted from the light source; and a second light beam that is diffracted or deflected. Wherein the second light flux, among the light emitted from the light source, passes on the light branching means outside the light that becomes the first light flux. It is characterized by being formed using light. According to the optical head as described above, the transmittance of the first light flux (for example, the main beam) in the optical path from the light source to the information recording medium can be improved, and the optical head using the light source with low light output can be improved. Can be realized. In the optical head, a width of the first portion in the track direction of the information recording medium is substantially equal to a light beam diameter on the light branching device of the light beam limited by the entrance pupil of the light collecting device. It is preferred that they have the same size. According to the optical head as described above, the first light flux restricted by the entrance pupil of the light condensing means is a light flux that has passed through the first portion, so that the transmittance of the first light flux is increased. Can be improved.
また、 前記光分岐手段は、 前記第 1の部分が回折格子非形成部で、 前 記第 2の部分が回折格子形成部であることが好ましい。 In the light splitting means, it is preferable that the first portion is a portion where no diffraction grating is formed, and the second portion is a portion where a diffraction grating is formed.
また、 前記第 2の光束が前記集光手段を通過する際に、 前記集光手段 の入射瞳上で占める光束の面積が前記入射瞳の面積の約半分以上となる ように、 前記光源と前記光分岐手段と前記集光手段とが配置されている ことが好ましい。 前記のような光学ヘッドによれば、 第 2の光束の光量 を十分大きくすることができ、 第 2の光束をトラッキングエラー信号検 出に必要な十分な光量を持つサブビームとして用いることができる。 また、 前記第 2の部分は、 前記第 1の部分を挟んで前記第 1の部分の 前記情報記録媒体のトラック方向における両側に形成された 2つの回折 格子形成部で形成されていることが好ましい。 Further, when the second light flux passes through the light focusing means, the light source and the light source so that the area of the light flux occupying on the entrance pupil of the light focusing means is about half or more of the area of the entrance pupil. It is preferable that the light splitting means and the light collecting means are arranged. According to the optical head as described above, the light amount of the second light beam can be made sufficiently large, and the second light beam can be used as a sub-beam having a sufficient light amount necessary for detecting a tracking error signal. Further, it is preferable that the second portion is formed of two diffraction grating forming portions formed on both sides of the first portion in the track direction of the information recording medium with the first portion interposed therebetween. .
また、 前記第 1の光束は、 前記情報記録媒体に対して情報の記録又は 再生を行うための光束で、 前記第 2の光束は、 前記情報記録媒体に対す る情報の記録時又は再生時におけるトラッキング制御のための光束であ ることが好ましい。 Further, the first light beam is used for recording information on the information recording medium or for recording information on the information recording medium. It is preferable that the second light beam is a light beam for performing tracking control at the time of recording or reproducing information on the information recording medium.
また、 前記第 2の光束は、 少なくとも一つの一対の光束を有し、 前記 一対の光束は、 前記集光手段によって前記情報記録媒体にトラックピッ チの約 1 Z 2を整数倍した間隔で集光され、 かつ前記情報記録媒体によ つて反射されてトラッキングエラーの検出に用いられることが好ましい。 図面の簡単な説明 Further, the second light beam has at least one pair of light beams, and the pair of light beams is collected on the information recording medium by the light condensing means at an interval obtained by multiplying about 1 Z2 of the track pitch by an integer. Preferably, the light is emitted and reflected by the information recording medium and used for detecting a tracking error. BRIEF DESCRIPTION OF THE FIGURES
図 1は、 本発明の一実施形態に係る光学ヘッドの構成図 FIG. 1 is a configuration diagram of an optical head according to an embodiment of the present invention.
図 2は、 本発明の一実施形態に係る光学へッドに用いる光分岐素子の 平面図 FIG. 2 is a plan view of an optical branching element used for an optical head according to an embodiment of the present invention.
図 3は、 本発明の一実施形態に係る光学へッドの光源と光分岐素子と 対物レンズとの配置を説明する図 FIG. 3 is a diagram illustrating an arrangement of a light source, a light splitting element, and an objective lens of an optical head according to an embodiment of the present invention.
図 4は、 本発明の一実施形態に係る光分岐素子により発生するサブビ —ムを説明する図 FIG. 4 is a view for explaining a sub beam generated by the optical branching device according to the embodiment of the present invention.
図 5は、 本発明の一実施形態に係る光学へッドによって形成されるス ポットを説明する図 FIG. 5 is a diagram illustrating a spot formed by the optical head according to one embodiment of the present invention.
図 6は、 本発明の別の実施形態に係る光学へッドによって形成される スポットを説明する図 FIG. 6 is a diagram illustrating a spot formed by an optical head according to another embodiment of the present invention.
図 7は、 従来の光学ヘッドの一例の構成図 Fig. 7 is a block diagram of an example of a conventional optical head.
図 8は、 光学へッドによって形成されるスポットを説明する図 図 9は、 従来の光学ヘッドの回折素子の一例を示す図 FIG. 8 is a diagram illustrating a spot formed by an optical head. FIG. 9 is a diagram illustrating an example of a diffraction element of a conventional optical head.
発明を実施するための最良の形態 以下、 本発明の一実施形態について、 図面を用いて説明する。 図 1は、 本発明の一実施形態に係る光学へッドの光学系の構成図を示している。 1は半導体レーザ一等の光源、 2は光分岐手段としての回折素子、 3は 対物レンズ、 4は情報記録媒体、 5 aから 5 eは回折素子 2で分岐され た光線、 6は光学系の光軸、 8は円柱レンズ等で形成された検出レンズ、 9は受光素子であり、 1 5はトラック方向、 D 1は対物レンズ 3の開口 (入射瞳) の直径を示している。 BEST MODE FOR CARRYING OUT THE INVENTION Hereinafter, an embodiment of the present invention will be described with reference to the drawings. FIG. 1 is a configuration diagram of an optical system of an optical head according to an embodiment of the present invention. 1 is a light source such as a semiconductor laser, 2 is a diffraction element as a light splitting means, 3 is an objective lens, 4 is an information recording medium, 5a to 5e are light beams split by the diffraction element 2, and 6 is an optical system. The optical axis, 8 is a detection lens formed of a cylindrical lens or the like, 9 is a light receiving element, 15 is a track direction, and D 1 is the diameter of the aperture (entrance pupil) of the objective lens 3.
図 2は、 回折素子 2に形成された回折格子の概念図である。 縞模様の 領域 2 a、 2 bは、 回折格子が形成されている領域を示している。 トラ ック方向 1 5において領域 2 aと 2 bとで挟まれた部分は、 回折格子が 形成されていない。 領域 1 0は、 この回折格子が形成されていない領域 の一部である。 領域 1 0は円 1 0 aの内側領域を示しており、 領域 1 0 をメインビームが通過する。 この領域 1 0の外周である円 1 0 aの直径 D 2は、 対物レンズ 3の入射瞳に相当する直径 D 1の開口で制限される 光束についての、 光分岐手段 2上の光束径に等しい。 FIG. 2 is a conceptual diagram of a diffraction grating formed on the diffraction element 2. The striped regions 2a and 2b indicate the regions where the diffraction grating is formed. No diffraction grating is formed in the portion sandwiched between the regions 2a and 2b in the track direction 15. The region 10 is a part of the region where the diffraction grating is not formed. The area 10 indicates an area inside the circle 10a, and the main beam passes through the area 10a. The diameter D2 of the circle 10a, which is the outer periphery of this area 10, is equal to the diameter of the light beam on the light branching means 2 for the light beam limited by the aperture of the diameter D1 corresponding to the entrance pupil of the objective lens 3. .
すなわち、 領域 2 aと 2 bとの間の距離 d 3は、 円 1 0 aの直径 D 2 にほぼ等しい。 このことにより、 メインビームに相当する光束は、 回折 素子 2上においては、 回折格子が形成されていない領域を通過すること になる。 That is, the distance d3 between the regions 2a and 2b is approximately equal to the diameter D2 of the circle 10a. As a result, the light beam corresponding to the main beam passes through the region on the diffraction element 2 where no diffraction grating is formed.
光源 1を発した光は、 回折素子 2に入射し、 複数の光束に分岐される これら複数の光束のうち、 メインビームとして利用される光束は、 光線 5 cのように回折格子 2の回折格子非形成部を通過する光束である。 サ ブビームとして利用される光束は、 仮に領域 2 aでの + 1次回折光を光 線 5 a、 一 1次回折光を光線 5 bとし、 領域 2 bでの + 1次回折光を光 線 5 d、 一 1次回折光を光線 5 eとすると、 光線 5 b及び 5 dで示した 方向に分岐された 2つの回折光である。 メインビーム及び 2つのサブビームは、 ハーフミラー 7を透過し、 対 物レンズ 3により情報記録媒体 4に集光され、 3つの光スポッ卜が生成 される。 これら光スポットからの反射光は、 再び対物レンズ 3を通過し、 ハーフミラ一 7で反射され、 検出レンズ 8を介して受光素子 9に導かれ る。 受光素子 9に導かれた各光束の位置と、 これら光束を用いてフォー カスエラ一信号、 トラッキングエラ一信号、 及び情報信号の検出を行う 方法については、 従来例と同様のため、 その説明を省略する。 また、 光 線 5 aと 5 eで示した回折光は、 対物レンズ 3の開口を通過しないため、 利用されない光束となる。 The light emitted from the light source 1 enters the diffraction element 2 and is split into a plurality of light beams. Of these light beams, the light beam used as the main beam is the diffraction grating of the diffraction grating 2 like the light beam 5c. This is a light beam that passes through the non-formed portion. The luminous flux used as the sub-beam is, for example, the + 1st-order diffracted light in the area 2a as a light beam 5a, the first-order diffracted light as a light beam 5b, and the + 1st-order diffracted light in the area 2b as a light beam 5d. If the first-order diffracted light is a light beam 5e, it is two diffracted light beams branched in the directions indicated by the light beams 5b and 5d. The main beam and the two sub-beams pass through the half mirror 7 and are focused on the information recording medium 4 by the objective lens 3 to generate three light spots. The reflected light from these light spots passes through the objective lens 3 again, is reflected by the half mirror 17, and is guided to the light receiving element 9 via the detection lens 8. The position of each light beam guided to the light receiving element 9 and a method of detecting a focus error signal, a tracking error signal, and an information signal using these light beams are the same as in the conventional example, and therefore description thereof is omitted. I do. Further, the diffracted lights indicated by the light beams 5a and 5e do not pass through the aperture of the objective lens 3, and thus become unutilized light beams.
ここで、 図 2の領域 2 a及び 2 bのように、 サブビームを発生させる ための回折格子を、 光軸から離れた位置に配置した場合は、 サブビーム が十分に対物レンズの開口を通過するためには、 光源 1と回折素子 2と の間隔が、 一定条件を満たすように十分に近接している必要がある。 図 3を参照しながら、 この条件について説明する。 Here, if the diffraction grating for generating the sub-beam is located at a position away from the optical axis as in the areas 2a and 2b in Fig. 2, the sub-beam will pass through the aperture of the objective lens sufficiently. In this case, the distance between the light source 1 and the diffraction element 2 needs to be sufficiently close to satisfy a certain condition. This condition will be described with reference to FIG.
図 3は、 本発明の一実施形態に係る光学ヘッドにおける光源と光分岐 素子と対物レンズとの配置を説明する構成図である。 図 1と同一構成の 要素には、 同一番号を付して説明を省略する。 1 1は光源位置に立てた 面である。 情報記録媒体 4を物体面と見ると、 対物レンズ 3による共役 像面が面 1 1である。 FIG. 3 is a configuration diagram illustrating an arrangement of a light source, a light splitting element, and an objective lens in an optical head according to an embodiment of the present invention. Elements having the same configurations as those in FIG. 11 is a surface set up at the light source position. When the information recording medium 4 is regarded as the object plane, the conjugate image plane formed by the objective lens 3 is the plane 11.
情報記録媒体 4上に生成された一方のサブスポッ卜の対物レンズ 3に 関する共役像高を y 1、 回折格子形成部と非形成部の境界と光軸との距 離を y 2とし、 y l、 2の先端でぁる点 1 ' と点 y 2 ' を結ぶ直線 の延長線が対物レンズ 3の開口面と交差する高さを h、 光源 1と回折素 子 2との間隔を d 1、 回折素子 2と対物レンズ 3の開口面との間隔を d 2とし、 紙面上方向を正とすると、 下記の式 ( 1 ) を満足する。 ただし, 回折格子 2の厚み分は、 考慮に入れていない。 式 ( 1) h = y 2 - (y 1— y 2) * d 2Zd 1 The conjugate image height of the objective lens 3 of one of the sub spots generated on the information recording medium 4 is y1, the distance between the boundary between the diffraction grating forming portion and the non-forming portion and the optical axis is y2, yl, The height at which the extension of the straight line connecting the point 1 'and the point y2' at the tip of 2 intersects the aperture of the objective lens 3 is h, the distance between the light source 1 and the diffraction element 2 is d1, and the diffraction is Assuming that the distance between the element 2 and the aperture surface of the objective lens 3 is d2, and the upward direction on the paper is positive, the following expression (1) is satisfied. However, the thickness of the diffraction grating 2 is not taken into account. Equation (1) h = y2-(y1-y2) * d2Zd1
例えば、 サブビームが対物レンズ 3の開口面積の半分以上を通過する 条件は、 たとえば図 3の上方をプラス方向とすると (y>0) 、 下記の 式 (2) である。 For example, the condition that the sub-beam passes through more than half of the aperture area of the objective lens 3 is, for example, the following equation (2) when the upper part of FIG.
式 (2) h<0 Equation (2) h <0
であるから、 式 ( 1 ) から距離 d 1を制限する条件を導くと、 下記の式 (3) で表される。 Therefore, when the condition for limiting the distance d1 is derived from the equation (1), it is expressed by the following equation (3).
式 (3) d l < (y l/y 2 - l) * d 2 Equation (3) d l <(y l / y 2-l) * d 2
さらに、 メインビームが全く回折格子形成領域を通過しないようにす るとすれば、 対物レンズ 3の光源 1側の開口数を NAとすると、 下記の 式 (4) で表される条件を加えて、 d l、 d 2を決めれば良い Further, assuming that the main beam does not pass through the diffraction grating forming area at all, assuming that the numerical aperture on the light source 1 side of the objective lens 3 is NA, the condition expressed by the following equation (4) is added. , Dl, d 2
式 (4) y 2>NA* d 1 Equation (4) y 2> NA * d 1
図 4は、 このような回折素子で発生されたサブビームが、 対物レンズ 3の開口を通過する様子を光源 1側から見た図である。 斜線部 1 2は、 図 2の領域 2 aで回折し、 図 1の光線 5 bで表されるサブビームを、 斜 線部 1 3は、 図 2の領域 2 bで回折し、 図 1の光線 5 dで表されるサブ ビームを示している。 中央部の十字斜線部は、 前記 2つのサブビームが 重なる領域を示している。 円 1 4は、 対物レンズの開口 (直径 D 1) を 示す。 図 4は、 2つのサブビームが、 それぞれ対物レンズ 3の開口の半 分以上を通過していることを表している。 通過する光束の面積が、 対物 レンズ開口の半分以上を占めれば、 トラックに垂直な方向の開口数は確 保できるため、 集光されたサブビームはトラッキングエラ一信号検出に 十分な光量をもつ小さなサブスポットとなる。 FIG. 4 is a diagram showing a state where the sub-beam generated by such a diffraction element passes through the aperture of the objective lens 3 as viewed from the light source 1 side. The hatched portion 12 diffracts in the region 2a in FIG. 2 and the sub-beam represented by the light beam 5b in FIG. 1.The hatched portion 13 diffracts in the region 2b in FIG. 2 and the light beam in FIG. The sub-beam represented by 5d is shown. The cross-hatched portion at the center indicates an area where the two sub-beams overlap. Circle 14 indicates the aperture (diameter D1) of the objective lens. FIG. 4 shows that each of the two sub-beams passes through at least half of the aperture of the objective lens 3. If the area of the passing light beam occupies more than half of the objective lens aperture, the numerical aperture in the direction perpendicular to the track can be secured, so the focused sub-beam is small enough to detect the tracking error signal. It becomes a sub spot.
なお、 式 ( 1 ) から式 (4) は、 光源と、 回折素子と、 対物レンズと の関係から導かれた式であるが、 コリメ一夕レンズ等の他のレンズを有 する光学系であっても、 同様の考え方が適用可能であることは明らかで ある。 Equations (1) to (4) are equations derived from the relationship between the light source, the diffraction element, and the objective lens. However, the equations (1) to (4) are optical systems having other lenses such as a collimated lens. However, it is clear that a similar idea can be applied. is there.
以上のように、 メインビームの通過する領域に回折格子非形成部を設 けた回折素子を用いることにより、 メインビームの透過率が向上し、 か つ回折格子形成部での + 1次および一 1次回折効率は、 各素子の配置を 調節することによりメインビーム光量に関わらずに任意に設定可能とな るため、 十分なサブビーム光量を得ることが可能である。 As described above, the transmittance of the main beam is improved by using the diffraction element having the diffraction grating non-forming portion in the area where the main beam passes, and the + 1st-order and 1st-order beams in the diffraction grating forming portion are improved. The secondary diffraction efficiency can be set arbitrarily irrespective of the main beam intensity by adjusting the arrangement of the elements, so that a sufficient sub-beam intensity can be obtained.
なお、 前記実施形態では、 光分岐手段として通常の回折格子が形成さ れた回折素子を用いた場合を説明したが、 回折格子をブレーズ化して、 図 1に記した光線 5 b及び 5 dで表される回折光の回折効率を増加させ た回折素子を用いれば、 更にサブビームの光量を増加することが可能で ある。 このことにより、 トラッキングエラー信号の品質を一層向上させ ることが出来る。 In the above-described embodiment, the case where a diffraction element having a normal diffraction grating is used as the light branching unit has been described. However, the diffraction grating is blazed, and the light beams 5b and 5d shown in FIG. 1 are used. If a diffraction element with an increased diffraction efficiency of the diffracted light is used, the light amount of the sub-beam can be further increased. As a result, the quality of the tracking error signal can be further improved.
また、 図 2に記した領域 2 a及び 2 bに、 回折格子の代わりにプリズ ム等を形成し、 図 1の光線 5 b及び 5 dの方向に光を偏向させる光学素 子を用いても同様の効果が得られる。 In addition, it is also possible to form a prism or the like in the regions 2a and 2b shown in FIG. 2 instead of the diffraction grating and use an optical element that deflects light in the directions of the light beams 5b and 5d in FIG. Similar effects can be obtained.
また、 前記実施形態では、 図 8に示したように、 2つのサブスポット がトラックと垂直な方向に、 トラックピッチの 1 Z 2の間隔を置いて配 置されている場合を例として示したが、 本発明はこのようなサブスポッ トの配置に限定されるものではない。 図 5 、 6にサブスポットの配置の 別の例を示している。 図 5 ( a ) 、 図 6 ( a ) は、 情報記録媒体の一部 の平面図を、 図 5 ( b ) 、 図 6 ( b ) はそれぞれ図 5 ( a ) 、 図 6 ( a ) のトラック方向と垂直な方向の断面図を示している。 Further, in the above embodiment, as shown in FIG. 8, an example has been described in which two sub-spots are arranged at an interval of 1 Z 2 of the track pitch in a direction perpendicular to the track. However, the present invention is not limited to such a subspot arrangement. Figures 5 and 6 show other examples of subspot arrangements. FIGS. 5 (a) and 6 (a) are plan views of a part of the information recording medium, and FIGS. 5 (b) and 6 (b) are the tracks of FIGS. 5 (a) and 6 (a), respectively. 2 shows a cross-sectional view in a direction perpendicular to the direction.
例えば、 図 5 ( a ) に示したように、 2つのサブスポット 1 8を情報 トラック 1 6のトラックピッチ分 (トラックピッチの 1 / 2の 2倍) の 間隔を置いて配置した構成の光学へッドであってもよい。 For example, as shown in Fig. 5 (a), the optical system has a structure in which two sub-spots 18 are arranged at an interval of the information track 16's track pitch (1/2 of the track pitch). May be used.
このような光学へッドは、 メインスポット 1 7及びサブスポット 1 8 の各々の光束をファーフィールドで分割して信号を検出するいわゆるSuch an optical head has a main spot 17 and a sub spot 18 Divides each light beam by the far field to detect a signal
「差動プッシュフル方式」として知られているトラッキングエラー検出方 式を用いて実現されることは周知である。 It is well known that this is realized using a tracking error detection method known as a “differential push-full method”.
また、 図 6 ( a ) に示したように、 2つのサブスポット 1 8を情報ト ラック 1 6のトラックピッチの 2倍 (トラックピッチの 1 Z 2の 4倍) の間隔をおいて配置し、 メインスポット 1 7及び 2つのサブスポット 1 8により 3本の情報トラック 1 6に対して同時に情報の記録、 再生を行 なうようにした光ディスク装置にも適用できる。 Also, as shown in FIG. 6 (a), the two sub-spots 18 are arranged at an interval of twice the track pitch of the information track 16 (four times the track pitch of 1Z2), The present invention can also be applied to an optical disc device in which information is recorded and reproduced on three information tracks 16 at the same time by the main spot 17 and the two sub spots 18.
以上、 2つのサブスポットが、 トラックピッチの 1 Z 2の整数倍のう ち、 1倍、 2倍、 及び 4倍の間隔をおいて配置された場合について説明 したが、 それ以上大きな整数倍の間隔を置いて配置された場合であって も、 同様に本発明が適用可能である。 The case where the two sub-spots are arranged at intervals of 1, 2, and 4 times the integer multiple of 1 Z 2 of the track pitch has been described above. The present invention can be similarly applied to the case where they are arranged at intervals.
さらに、 サブビームの発生には、 回折素子での + 1次又は— 1次回折 光を用いた例を説明したが、 2次以上の高次の回折光を用いて 2つ以上 のサブビームを発生させる光分岐手段についても、 前記と同様の考え方 で応用可能である。 産業上の利用可能性 Furthermore, the example of using a + 1st- or 1st-order diffracted light from a diffraction element to generate a subbeam has been described. However, two or more subbeams are generated using second- or higher-order diffracted light. The same concept as described above can be applied to the optical branching means. Industrial applicability
以上のように本発明によれば、 光源から発した光束のうち、 従来では 利用していなかった範囲の光束を用いて、 情報の記録又は再生に用いら れる光束以外の光束を発生させることにより、 光源から放射された光を 利用する比率を向上させることができる。 As described above, according to the present invention, of the light beams emitted from a light source, a light beam other than a light beam used for recording or reproducing information is generated by using a light beam in a range not conventionally used. However, the ratio of using the light emitted from the light source can be improved.
このため本発明は、 情報記録媒体上に複数の光束を集光させて動作す る方式の光学へッドに用いることができ、 従来よりも少ない光出力の光 源を用いた光学へッドが実現可能となる。 For this reason, the present invention can be used for an optical head of a type that operates by condensing a plurality of light beams on an information recording medium, and an optical head using a light source with a smaller light output than before. Can be realized.
Claims
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| AU30773/00A AU3077300A (en) | 1999-01-27 | 2000-01-24 | Optical head |
Applications Claiming Priority (2)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP11/18366 | 1999-01-27 | ||
| JP01836699A JP2003022561A (en) | 1999-01-27 | 1999-01-27 | Optical head |
Publications (1)
| Publication Number | Publication Date |
|---|---|
| WO2000045383A1 true WO2000045383A1 (en) | 2000-08-03 |
Family
ID=11969716
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| PCT/JP2000/000330 Ceased WO2000045383A1 (en) | 1999-01-27 | 2000-01-24 | Optical head |
Country Status (3)
| Country | Link |
|---|---|
| JP (1) | JP2003022561A (en) |
| AU (1) | AU3077300A (en) |
| WO (1) | WO2000045383A1 (en) |
Citations (3)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS63138625U (en) * | 1987-03-04 | 1988-09-13 | ||
| EP0475523A1 (en) * | 1990-09-12 | 1992-03-18 | Koninklijke Philips Electronics N.V. | Device for optically scanning an information plane |
| JPH0554415A (en) * | 1991-08-28 | 1993-03-05 | Mitsubishi Electric Corp | Optical recording/reproducing device |
-
1999
- 1999-01-27 JP JP01836699A patent/JP2003022561A/en active Pending
-
2000
- 2000-01-24 WO PCT/JP2000/000330 patent/WO2000045383A1/en not_active Ceased
- 2000-01-24 AU AU30773/00A patent/AU3077300A/en not_active Abandoned
Patent Citations (3)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS63138625U (en) * | 1987-03-04 | 1988-09-13 | ||
| EP0475523A1 (en) * | 1990-09-12 | 1992-03-18 | Koninklijke Philips Electronics N.V. | Device for optically scanning an information plane |
| JPH0554415A (en) * | 1991-08-28 | 1993-03-05 | Mitsubishi Electric Corp | Optical recording/reproducing device |
Also Published As
| Publication number | Publication date |
|---|---|
| AU3077300A (en) | 2000-08-18 |
| JP2003022561A (en) | 2003-01-24 |
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