TWI227471B - Optical member and optical device which uses the same - Google Patents

Optical member and optical device which uses the same Download PDF

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Publication number
TWI227471B
TWI227471B TW091104405A TW91104405A TWI227471B TW I227471 B TWI227471 B TW I227471B TW 091104405 A TW091104405 A TW 091104405A TW 91104405 A TW91104405 A TW 91104405A TW I227471 B TWI227471 B TW I227471B
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Taiwan
Prior art keywords
light
wavelength
laser
grating
optical
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TW091104405A
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Chinese (zh)
Inventor
Shoichi Kyotani
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Alps Electric Co Ltd
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    • GPHYSICS
    • G11INFORMATION STORAGE
    • G11BINFORMATION STORAGE BASED ON RELATIVE MOVEMENT BETWEEN RECORD CARRIER AND TRANSDUCER
    • G11B7/00Recording 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
    • G11B7/12Heads, e.g. forming of the optical beam spot or modulation of the optical beam
    • G11B7/135Means for guiding the beam from the source to the record carrier or from the record carrier to the detector
    • G11B7/1353Diffractive elements, e.g. holograms or gratings
    • GPHYSICS
    • G11INFORMATION STORAGE
    • G11BINFORMATION STORAGE BASED ON RELATIVE MOVEMENT BETWEEN RECORD CARRIER AND TRANSDUCER
    • G11B7/00Recording 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
    • G11B7/12Heads, e.g. forming of the optical beam spot or modulation of the optical beam
    • G11B7/125Optical beam sources therefor, e.g. laser control circuitry specially adapted for optical storage devices; Modulators, e.g. means for controlling the size or intensity of optical spots or optical traces
    • G11B7/127Lasers; Multiple laser arrays
    • G11B7/1275Two or more lasers having different wavelengths
    • GPHYSICS
    • G11INFORMATION STORAGE
    • G11BINFORMATION STORAGE BASED ON RELATIVE MOVEMENT BETWEEN RECORD CARRIER AND TRANSDUCER
    • G11B2220/00Record carriers by type
    • G11B2220/20Disc-shaped record carriers
    • G11B2220/25Disc-shaped record carriers characterised in that the disc is based on a specific recording technology
    • G11B2220/2537Optical discs
    • G11B2220/2545CDs
    • GPHYSICS
    • G11INFORMATION STORAGE
    • G11BINFORMATION STORAGE BASED ON RELATIVE MOVEMENT BETWEEN RECORD CARRIER AND TRANSDUCER
    • G11B2220/00Record carriers by type
    • G11B2220/20Disc-shaped record carriers
    • G11B2220/25Disc-shaped record carriers characterised in that the disc is based on a specific recording technology
    • G11B2220/2537Optical discs
    • G11B2220/2562DVDs [digital versatile discs]; Digital video discs; MMCDs; HDCDs

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  • Physics & Mathematics (AREA)
  • Optics & Photonics (AREA)
  • Optical Head (AREA)
  • Diffracting Gratings Or Hologram Optical Elements (AREA)

Abstract

To avoid problems that a conventional diffraction grating shows large fluctuation in the wavelength by the changes in the temperature and causes a large shift of the light-accepting position in the light-accepting part for laser light. Projections 11a as a first grating are formed on a transparent resin substrate and steps 11b as a second grating are formed as superposed on the inclined faces of the projections 11a. The depth dimension h of each step in the steps 11b is determined in such a manner that (n-1)h, wherein n is the refractive index, is equal to an positive integral multiple of the wavelength. The optimum number of steps is determined by the depth h and the period p. When the wavelength is 658 nm or 785 nm, the optimum number of steps is 6.

Description

五、發明説明(u 【技術領域】 經濟部智慈財產局員工消費合作社印製 本發明涉及一*種2種不同波長的雷射入射的光學構件 ,特別是涉及一種用受光部接收彼此光軸錯開的雷射的光 學構件和使用該光學構件的光學裝置。 【先行技術】 在搭載在CD和DVD雙方都能使用的光碟裝置中的 光拾波器中,爲了簡化結構,搭載有把兩個不同波長的雷 射光源設置爲一體的發光部。在所述發光部中,因爲隔開 微小的間隔配置了所述光源,所以在雷射的光軸錯開的狀 態下形成光路。在光軸錯開的狀態下,因爲受光部的受光 位置産生了偏差,所以有必要在受光部使雙方的雷射的受 光位置一致。 第7圖是表示爲了消除所述偏差而設置的以往的光學 構件30的俯視圖。所述光學構件30在板狀的透明構件的 一側的面上形成有凹凸形狀的繞射光柵30a,設置在與受 光部相對的位置上。 所述光學構件30搭載在CD和DVD兼用的光碟裝置 上,在該光碟裝置中,設置有發出作爲CD用的7 8 5 nm波 長(人1 )的雷射和作爲DVD用的65 8nm的波長(又2 ) 的雷射的發光部。如第7圖所示,在盤上反射的返回光的 光軸錯開的狀態下返回到光學構件30,用所述光學構件 30的繞射光柵30a使雙方的雷射繞射,在到達受光部3 1 的位置,使受光位置變爲相互一致。另外,根據波長的長 (請先閲讀背面之注意事項再填寫本頁) 本紙張尺度適用中國國家標準(CNS ) A4規格(210X297公釐) - 4- 1227471 更 if·, ea 1 π |Β7 五、發明説明(2) 度繞射角度不同,在第7圖所示的情況下,λ 1的繞射角 度(0 1 )比λ 2的繞射角度(0 2 )大。 【本發明所欲解決之課題】 但是,因爲在發出所述雷射的發光部中,具有隨著溫 度變化波長發生變動的特性,所以在所述以往的光學構件 3 0中,隨著溫度變化,繞射角度變動,結果使在雷射的 受光部的受光位置變得彼此不一致,産生了偏移問題。例 如,如果受光部的受光位置大幅度地偏移,則高於1次繞 射光的高次繞射光漏入受光部,産生偏移。 鑒於以上所述問題的存在,本發明的目的在於:提供 一種能使相互錯開的雷射的光軸在受光部上一致,並能降 低由溫度變化造成的波長變動的影響的光學構件和使用該 光學構件的光學裝置。 【用以解決課題之手段】 爲了實現以上所述目的,本發明的光學構件,入射不 同波長λ 1和λ 2的雷射,其特徵在於:設置有使第一波 長λ 1的雷射繞射,使第二波長;I 2的雷射不繞射地透射 的繞射光柵。 在這種情況下,能使所述繞射光柵的結構爲:對於所 述第一波長λ 1的雷射,對1次繞射光具有選擇性,對於 所述第二波長λ 2的雷射,具有對〇次繞射光的選擇性。 所述繞射光柵具有形成凹凸狀的第一光柵部和在所述 本紙張尺度適用中國國家標準(CNS ) A4規格(210X297公釐) (請先閲讀背面之注意事項再填寫本頁) 訂 經濟部智慧財產局員工消費合作社印製 -5- 1227471 厂了 A7 B7 五、發明説明(3) 第一光柵部的傾斜面上呈臺階狀形成的第二光柵部,呈所 述臺階狀形成的第二光柵部的每一級臺階的深度(h ), 相對於所述第二波長λ 2的雷射爲(n-1 ) h = m λ 2 (但是 ’ η爲折射率,m爲正整數),最好把所述第二光柵部的 臺階狀的臺階數設置爲:能使所述第二波長;I 2的雷射不 繞射而透射,使所述第一波長λ 1的雷射以給定的角度繞 射。 另外,所述第二光柵部的各級在寬度方向和深度方向 都是形成等距離爲最佳。 在所述本發明中,因爲使一方波長的雷射不繞射,所 以能使另一方雷射的繞射角度變小,從而能降低因溫度變 化導致的波長變動的影響,能減小受光部的受光位置的偏 差。 另外,通過使所述第一波長λ 1爲785 nm,所述第一 波長λ 2爲65 8nm,就能適用於CD和DVD兼用的光拾波 器。 另外,在所述情況下,通過把所述第二光柵部的臺階 狀的臺階數設置爲6級,就能對雙方的雷射進行維持其在 受光位置上的高效率的設計。 另外,最好在所述第二光柵部的表面上形成凹凸狀的 第三光柵部,形成所述凹凸,使在所述第二光柵部的一個 臺階上形成的第三光柵部的周期在所述雷射的波長以下。 因爲利用該凹凸能起到防止反射的效果,所以能降低由光 的反射造成的損失。 本纸張尺度適用中國國家標準(CNS ) A4規格(210X297公釐) (讀先閱讀背面之注意事項再填寫本頁)V. Description of the invention (u [Technical Field] Printed by the Consumer Cooperative of the Intellectual Property Office of the Ministry of Economics The present invention relates to an optical component of laser light incident with two kinds of different wavelengths, and more particularly to a light receiving unit that receives the optical axes of each other Staggered laser optical components and optical devices using the optical components. [Preceding technology] In order to simplify the structure, an optical pickup mounted in an optical disc device that can be used by both CDs and DVDs is equipped with two Laser light sources of different wavelengths are provided as an integrated light emitting section. In the light emitting section, the light sources are arranged at minute intervals, so that the optical path is formed in a state where the optical axes of the lasers are staggered. The optical axes are staggered Since the light receiving position of the light receiving unit is deviated in the state, it is necessary to make the light receiving positions of both lasers coincide in the light receiving unit. FIG. 7 is a plan view showing a conventional optical member 30 provided to eliminate the deviation. The optical member 30 has a concave and convex diffraction grating 30a formed on one surface of a plate-shaped transparent member, and is provided at a position facing the light receiving portion. The optical member 30 is mounted on an optical disc device for both CD and DVD, and the optical disc device is provided with a laser emitting a wavelength of 7 8 5 nm (CD 1) for CD and 65 8 nm for DVD The light emitting part of the laser with a wavelength of (2). As shown in FIG. 7, the optical axis of the returned light reflected on the disc is staggered and returned to the optical member 30, and the diffraction grating of the optical member 30 is used. 30a makes the laser diffraction of both sides reach the position of the light receiving part 31, so that the light receiving positions are consistent with each other. In addition, according to the length of the wavelength (please read the precautions on the back before filling this page) This paper size is applicable to China National Standard (CNS) A4 Specification (210X297 mm)-4- 1227471 More if ·, ea 1 π | B7 V. Description of the Invention (2) The angle of diffraction is different. In the case shown in Figure 7, λ 1 The diffraction angle (0 1) is larger than the diffraction angle (0 2) of λ 2. [Problems to be Solved by the Invention] However, the light emitting part emitting the laser has a wavelength that changes with temperature. Due to the changing characteristics, in the conventional optical member 30 described above, As the temperature changes and the diffraction angle changes, the light receiving positions of the laser light receiving section become inconsistent with each other, which causes a problem of shifting. For example, if the light receiving position of the light receiving section is greatly shifted, it is higher than the first winding. The high-order diffracted light of the emitted light leaks into the light-receiving part and is shifted. In view of the above-mentioned problems, an object of the present invention is to provide a light-receiving part whose laser light axes can be aligned with each other and can be reduced. Optical member affected by wavelength variation caused by temperature change and optical device using the optical member. [Means to Solve the Problem] In order to achieve the above-mentioned object, the optical member of the present invention is incident at different wavelengths λ 1 and λ 2 The laser is characterized in that: a diffraction grating is provided to diffract the laser of the first wavelength λ 1 and make the second wavelength; the laser of I 2 transmits without diffraction. In this case, the structure of the diffraction grating can be such that: for a laser of the first wavelength λ 1, it is selective for a single diffraction light, and for a laser of the second wavelength λ 2, It has selectivity to zero diffraction light. The diffraction grating has a first grating portion forming a concave and convex shape, and the Chinese National Standard (CNS) A4 specification (210X297 mm) is applied to the paper size (please read the precautions on the back before filling this page). Printed by the Ministry of Intellectual Property Bureau's Consumer Cooperative -5- 1227471 Factory A7 B7 V. Description of the invention (3) The second grating portion formed in a step shape on the inclined surface of the first grating portion, and the first grating portion formed in the step shape. The depth (h) of each step of the two grating portions with respect to the second wavelength λ 2 is (n-1) h = m λ 2 (but 'η is a refractive index and m is a positive integer), Preferably, the number of step-like steps of the second grating portion is set to enable the second wavelength; the laser of I 2 is transmitted without diffraction, and the laser of the first wavelength λ 1 is given to Diffraction at a fixed angle. In addition, it is preferable that the respective stages of the second grating portion are formed at equal distances in the width direction and the depth direction. In the present invention, since the laser beam of one wavelength is not diffracted, the diffraction angle of the other laser beam can be made smaller, thereby reducing the influence of wavelength variation due to temperature changes and reducing the light receiving portion. Deviation of the light receiving position. In addition, by setting the first wavelength λ 1 to 785 nm and the first wavelength λ 2 to 65 8 nm, the present invention can be applied to an optical pickup for both CD and DVD. In addition, in this case, by setting the number of step-like steps of the second grating portion to six steps, it is possible to design the laser beams of both sides with high efficiency while maintaining their light receiving positions. In addition, it is preferable that a concave-convex third grating portion is formed on a surface of the second grating portion, and the concave-convex is formed so that a period of the third grating portion formed on one step of the second grating portion is at The laser wavelength is below. Since the effect of preventing the reflection is obtained by using the unevenness, the loss caused by the reflection of light can be reduced. This paper size is applicable to China National Standard (CNS) A4 specification (210X297 mm) (Read the precautions on the back before filling this page)

'1T 經濟部智慧財產局員工消費合作社印製 -6 -'1T Printed by the Consumer Cooperative of the Intellectual Property Bureau of the Ministry of Economic Affairs -6-

五、發明説明(4) 另外,因爲所述第一光柵部和第二光柵部都是用樹脂 來〜體形成的,所以能降低製造成本。 另外,本發明的光學裝置其特徵在於:設置有使發出 第一波長λ 1的雷射的發光點與發出第二波長;I 2的雷射 的發光點向與光軸正交的方向錯開置位的發光部和使來自 所述發光部的光透射的所述光學構件,使所述第一波長又 1的雷射的光軸與第二波長λ 2的雷射的光軸在給定位置 上一致。 在所述本發明中,因爲設置有把兩個波長的雷射的光 源設置爲一體的發光部,和能使兩個波長的雷射獨立地繞 射的單一光學構件,所以能減少零部件數量,簡化結構, 從而能降低成本。 【本發明之最佳實施形態】 第1圖是表示搭載了本發明的光學構件的光學裝置的 一個例子的槪要圖,第2圖是表示光學構件及其光軸的模 式圖’弟3圖是表不光學構件的一部分的俯視圖,第4圖 是表示相對於臺階數爲6的光柵深度的光的效率的線圖, 第5圖是表示相對於臺階數爲5的光柵深度的光的效率的 線圖。 第1圖所示的作爲光學裝置的光拾波器1 〇具有:內 置了半導體雷射二極體的發光部1 2 ;使該發光部1 2發射 的雷射變爲平行光的視准透鏡1 3 ;在使入射的雷射反射 的同時,使從所述反射方向入射的光透射的分光鏡1 4 ; 本紙張尺度適用中國國家標準(CNS ) Α4規格(210X297公釐) — - (請先閲讀背面之注意事項再填寫本頁) 、1Τ 經濟部智慧財產局員工消費合作社印製 1227471 Α7 Β7 五、發明説明(—5 物鏡1 5 ;受光部1 6 ;配置在所述受光部1 6和分光鏡i 4 之間的本發明的光學構件1 1。 (請先閱讀背面之注意事項再填寫本頁) 所述發光部12中,形成了用於CD的波長7 8 5 nm ( λ 1 )的雷射發光點的發光元件1 2 a和形成了用於D V D的波 長65 8nm (又2 )的雷射發光點的發光元件12b,在單一的 框體內以分開微小間隔(S )的狀態配置。 如果從所述發光部1 2發射的波長;I 1、λ 2的雷射入 射到分光鏡14,則在分光鏡14向盤D1的方向反射,由 視准透鏡1 3變爲平行光後入射到物鏡1 5。由物鏡1 5聚 光的雷射在盤D1上形成光點,在盤D1上反射的返回光 在彼此的光軸錯開的狀態下通過物鏡1 5、視准透鏡1 3, 透射分光鏡1 4,到達所述光學構件。 經濟部智慧財產局員工消費合作社印製 如第2圖所示,所述光學構件1 1是用光透射性的樹 脂構件、玻璃構件或樹脂和玻璃的複合材料形成的板狀構 件。在該光學構件1 1中,DVD用波長λ 2的雷射不繞射 ,直接透射,導入受光部16,使CD用波長λ 1的雷射繞 射後,導入受光部16。另外,如第1圖所示,可以在光 學構件1 1和受光部1 6之間配置凹透鏡1 7,使在受光部 1 6上形成的雷射光束的形狀擴大。 所述受光部1 6由光電二極體形成,具有分割爲四份 的感測器A、Β、C、D組合而成的感光元件和在所述感光 元件的兩側部設置的感測器E和F構成的側部感光元件 。例如,作爲CD和DVD的跟蹤伺服機構,分別適用三 光束法、相位差法,作爲聚焦伺服機構適用象散法。在 本纸張尺度適用中國國家標準(CNS ) A4規格(2】0X 297公釐) -8- 1227471 A7 B7 ---— 五、發明説明(6) CD和DVD的聚焦伺服機構中,使用所述感光元件作爲公 共元件。 (請先閱讀背面之注意事項再填寫本頁) 在所述受光部1 6中’由於波長隨著溫度變化而變化 ,雷射的光點在與感測器E和感測器F連接成的EF方向 正交的方向上偏移,其結果’更高次的繞射光漏入感光元 件,從而導致産生偏移這一問題。在此’在下面表示改善 了所述偏差後的光學構件1 1 ° 在所述光學構件1 1的射出面一側’形成有連續形成 多個凸部1 1 a的第一光柵部,各凸部1 1 a的傾斜面上形成 有臺階狀的臺階部1 1 b (第2光柵部)。由所述凸部1 1 a 和臺階部1 1 b構成繞射光柵11 A。 所述第一光柵部近乎爲鋸齒狀,各凸部11a都是同一 形狀,是由垂直面和傾斜面形成的直角三角形。另外,所 述臺階部lib中,平坦面S1〜S6漸漸改變高度,形成的臺 階數爲6級,各級在X方向的寬度尺寸w和y方向深度 尺寸h都是等間隔的(h = d/5,w = p/6 )。但是,p爲周期 ,該周期是凸部1 1 a的寬度尺寸。 經濟部智慧財產局員工消費合作社印製 在第3圖所示的光學構件1 1上形成的繞射光柵1 ! A 中,如果各級的深度尺寸爲h,樹脂的折射率爲n,雷射 的波長爲λ,則關係式(n -1 ) h = m λ成立。但是,m爲正 整數。通過由所述關係式決定h,使(η -1 ) h爲波長的正 整數倍,對於所述波長λ的雷射,能使它不繞射而直接進 行透射。 由所述關係式,對於λ 2 ( 6 5 8nm )的雷射設置h,使 本紙張尺度適用中國國家標準(CNS ) A4規格(2丨OX297公釐) -9-5. Description of the Invention (4) In addition, since the first grating portion and the second grating portion are both formed of resin, the manufacturing cost can be reduced. In addition, the optical device of the present invention is characterized in that the light emitting point of the laser emitting the first wavelength λ 1 and the second wavelength are provided; the light emitting point of the laser emitting I 2 is staggered in a direction orthogonal to the optical axis. And the optical member that transmits the light from the light emitting portion so that the optical axis of the laser having the first wavelength of 1 and the optical axis of the laser having the second wavelength λ 2 are at predetermined positions. Consistent. In the present invention, since a light emitting unit in which two-wavelength laser light sources are integrated and a single optical member capable of independently diffracting two-wavelength lasers is provided, the number of parts can be reduced. , Simplifying the structure, which can reduce costs. [Best Embodiment of the Present Invention] FIG. 1 is a schematic diagram showing an example of an optical device equipped with the optical member of the present invention, and FIG. 2 is a schematic diagram showing the optical member and its optical axis. FIG. 4 is a plan view showing a part of the optical member, FIG. 4 is a line graph showing the efficiency of light with respect to a grating depth of 6 steps, and FIG. 5 is a graph showing the efficiency of light with respect to a grating depth of 5 steps Line illustration. The optical pickup 10 shown in FIG. 1 as an optical device includes: a light emitting section 12 in which a semiconductor laser diode is built in; and a collimating lens for converting the laser emitted by the light emitting section 12 into parallel light. 13; Beamsplitters that transmit incident light from the direction of reflection while reflecting incident lasers 1 4; This paper size applies Chinese National Standard (CNS) A4 specifications (210X297 mm) —-(Please Read the notes on the back before filling out this page), printed by the Consumer Cooperative of the Intellectual Property Bureau of the Ministry of Economic Affairs 1227471 Α7 Β7 V. Description of the invention (-5 objective lens 15; light receiving unit 16; arranged in the light receiving unit 16 The optical member 1 1 of the present invention between the dichroic mirror i 4 and the beam splitter i 4. (Please read the precautions on the back before filling this page.) In the light emitting section 12, a wavelength 7 8 5 nm (λ 1 for CD) is formed. The light emitting element 1 2 a of the laser light emitting point) and the light emitting element 12 b formed with a laser light emitting point having a wavelength of 65 8 nm (also 2) for a DVD are in a state of being separated by a minute interval (S) in a single frame. Configuration: if the wavelength emitted from the light emitting part 12; the laser of I1, λ2 When it hits the beam splitter 14, the beam splitter 14 reflects in the direction of the disc D1, changes from collimating lens 13 to parallel light, and then enters the objective lens 15. The laser beam condensed by the objective lens 15 forms light on the disc D1. Point, the return light reflected on the disk D1 passes through the objective lens 15, the collimator lens 13, and the transmission beam splitter 14 to the optical member in a state where the optical axes of the disks are staggered from each other. As shown in FIG. 2, the optical member 11 is a plate-shaped member made of a light-transmitting resin member, a glass member, or a composite material of resin and glass. In this optical member 11, a wavelength for DVD is used. The laser of λ 2 is transmitted directly without being diffracted, and is introduced into the light receiving unit 16. After the laser of wavelength λ 1 is diffracted to the CD, the laser is introduced into the light receiving unit 16. In addition, as shown in FIG. A concave lens 17 is arranged between the light receiving part 16 and the shape of the laser beam formed on the light receiving part 16 to enlarge the light receiving part 16 formed of a photodiode and having a sensor divided into four parts. A, B, C, D combined photosensitive element and on both sides of the photosensitive element The side photosensitive elements constituted by sensors E and F. For example, as the tracking servo mechanism for CD and DVD, the three-beam method and the phase difference method are applicable, and the astigmatism method is used as the focusing servo mechanism. In this paper The standard is applicable to the Chinese National Standard (CNS) A4 specification (2) 0X 297 mm. -8- 1227471 A7 B7 ----- 5. Description of the invention (6) In the focus servo mechanism of CD and DVD, the photosensitive element is used as Common components. (Please read the precautions on the back before filling in this page.) In the light receiving unit 16, 'the wavelength of the laser varies with the temperature, and the light point of the laser is between sensor E and sensor F. The connected EF directions are shifted in a direction orthogonal to each other, and as a result, higher-order diffracted light leaks into the photosensitive element, causing a problem of shift. Herein, "the optical member 1 1 after the deviation is improved is shown below. On the side of the exit surface of the optical member 11", a first grating portion in which a plurality of convex portions 1 1a are continuously formed is formed. A stepped step portion 1 1 b (a second grating portion) is formed on the inclined surface of the portion 1 1 a. The convex portion 1 1 a and the step portion 1 1 b constitute a diffraction grating 11 A. The first grating portion is almost sawtooth-shaped, and each of the convex portions 11a has the same shape, and is a right-angled triangle formed by a vertical surface and an inclined surface. In addition, in the stepped portion lib, the flat surfaces S1 to S6 gradually change in height, and the number of steps formed is six. The width dimension w in each direction in the X direction and the depth dimension h in the y direction are equally spaced (h = d / 5, w = p / 6). However, p is a period, and this period is a width dimension of the convex portion 1 1 a. The diffraction grating 1! A formed on the optical member 11 shown in Figure 3 by the Consumer Cooperative of the Intellectual Property Bureau of the Ministry of Economic Affairs, if the depth dimension of each stage is h, the refractive index of the resin is n, and the laser The wavelength of λ is λ, then the relationship (n -1) h = m λ holds. However, m is a positive integer. By determining h from the relational expression so that (η -1) h is a positive integer multiple of the wavelength, a laser of the wavelength λ can be transmitted directly without diffraction. From the relationship, set h for a laser of λ 2 (658 nm) so that the paper size applies the Chinese National Standard (CNS) A4 specification (2 丨 OX297 mm) -9-

經濟部智慧財產局員工消費合作社印製 五、發明説明(7) (m ) h爲λ 2的正整數倍,當λ 2的雷射入射到繞射光 W 1 1 Α時,能不繞射,而是以0次繞射光直接透射。 根據以上所述,決定凸部1 1 a的光柵深度尺寸d ( =5h ),周期P也例如預先設置在從30到50 // m的範圍 @ ’決定剩下的臺階部的級數,據此就能決定光學構件 1 1的形狀。在此,通過一級一級地改變臺階數,證明第3 β所示的臺階數爲6級的形狀爲最佳。下面,參照第4圖 就其理由加以說明。 第4圖是表示相對於波長λ 1和波長λ 2的各繞射光 的光柵深度和效率的關係的線圖。但是,周期(ρ )爲20 V m,折射率爲1.54。另外,第4圖的縱軸的效率表示當 雷射通過繞射光柵1 1 A時的、通過前的雷射光量爲1時 ’通過後的0次繞射光(0T ) 、± 1次繞射光(:b 1T )和 ± 2次繞射光(土 2T )的光量的比率。 如第4圖(a )所示,通過把繞射光柵的光柵深度尺 寸d設置爲6// m附近,能得到高效率的65 8nm ( 2)的0 次繞射光和7 85 nm ( λ 1 )的1次繞射光。 如以上所述,通過形成光學構件1 1,對於λ 1的雷射 ,具有選擇1次繞射光的選擇性,對於λ 2的雷射,具有 選擇0次繞射光的選擇性。並且都能以高效率得到λ 1的 1次繞射光和λ 2的0次繞射光。 另外,在第4圖(b)和(c)所示光栅深度尺寸下, 無法取得高效率的7 85nm ( λ 1 )的1次繞射光和65 8nm (λ 2 )的0次繞射光。如果深度尺寸d變大,對應波長 本纸張尺度適用中國國家標準(CNS ) A4規格(210X297公釐) (請先閱讀背面之注意事項再填寫本頁)Printed by the Consumer Cooperatives of the Intellectual Property Bureau of the Ministry of Economic Affairs. 5. Description of the Invention (7) (m) h is a positive integer multiple of λ 2. When a laser of λ 2 is incident on the diffracted light W 1 1 Α, it can be undiffracted. Instead, it is directly transmitted with 0 times of diffracted light. According to the above, the grating depth dimension d (= 5h) of the convex portion 1 1 a is determined, and the period P is also set in advance, for example, in a range from 30 to 50 // m @ 'to determine the number of steps of the remaining step portion, according to This can determine the shape of the optical member 11. Here, by changing the number of steps one step at a time, it has been proved that the shape with the number of steps indicated by 3 β being 6 steps is optimal. The reason will be described below with reference to FIG. 4. Fig. 4 is a graph showing the relationship between the grating depth and the efficiency of each diffracted light with respect to the wavelength? 1 and the wavelength? 2. However, the period (ρ) was 20 V m and the refractive index was 1.54. In addition, the efficiency of the vertical axis in FIG. 4 indicates that when the laser passes through the diffraction grating 1 1 A, the amount of laser light before passing is 1 ', and the diffraction light is 0 times (0T) after passing and ± 1 time. (: B 1T) and the ratio of the light quantity of ± 2nd-order diffracted light (soil 2T). As shown in Fig. 4 (a), by setting the grating depth dimension d of the diffraction grating to around 6 // m, it is possible to obtain highly efficient 0x diffraction light of 65 8nm (2) and 7 85 nm (λ 1 ) 1st diffracted light. As described above, by forming the optical member 1 1, for the laser of λ 1, there is a selectivity of selecting the first diffraction light, and for the laser of λ 2, it has the selectivity of selecting the 0 diffraction light. In addition, it is possible to obtain the first diffraction light of λ 1 and the zero diffraction light of λ 2 with high efficiency. In addition, at the grating depth dimensions shown in Figs. 4 (b) and (c), high-efficiency 1st diffracted light of 7 85nm (λ 1) and 0th diffracted light of 65 8nm (λ 2) cannot be obtained. If the depth dimension d becomes larger, the corresponding wavelength This paper size applies the Chinese National Standard (CNS) A4 specification (210X297 mm) (Please read the precautions on the back before filling this page)

-10- 1227471-10- 1227471

五、發明説明(8) 變化的變動就變大,所以不好。並且,雖然在(b )的深 度下’能得到7 8 5 n m的2次繞射光,但是效率變差,所 以不好。 因此’光柵深度尺寸d爲6 // m附近(更確切地說, 應爲6· 1 // m附近),通過以等距離形成臺階部丨丨b的各 級的寬度尺寸和深度尺寸,就能得到維持了高效率的繞射 光柵1 1 A。 另外’第5圖所示的線圖是把第3圖所示繞射光栅 1 1 A的臺階數由6級改爲5級。但是,在這種情況下也如 以上所述,以等距離形成各級的寬度尺寸和深度尺寸。 在第5圖所示的繞射光柵1 1 A中,通過把繞射光柵 的光柵深度尺寸d設置爲5 · 8 // m附近(e ),據此就能得 到商效率的6 5 8 n m的-1次繞射光和7 8 5 n m的0次繞射光 。在這種情況下,也可以把λ 1和λ 2顛倒,使65 8nm爲 λ 1,7 85nm 爲 λ 2。 如以上所述,通過採用由第4圖的(a )或第5圖(e )決定的繞射光柵的光柵深度尺寸d的形狀,只使65 8nm 的雷射的0次繞射光透射,並且只使7 8 5 nm的雷射的1 次繞射光繞射,或只使65 8nm的雷射的-1次繞射光繞射 ,只使785nm的雷射的0次繞射光透射,能使7 8 5 nm的 光軸和65 8nm的光軸在受光部1 6上一致。 因此,因爲一方的雷射不繞射,所以不受波長變動的 影響,因爲另一方的雷射雖然繞射,但是繞射角度比以往 小,所以作爲整體能降低波長變動導致的影響。並且’在 本纸張尺度適用中國國家標準(CNS) A4規格(210x297公釐) (請先閱讀背面之注意事項再填寫本頁) 訂 經濟部智慧財產局員工消費合作社印製 -11 - :227471 五、發明説明(9) 所述的光學構件1 1中,在臺階數爲6級和5級中,採取 6級的形狀在光的效率方面更好。 另外,在本實施例中,雖然說明了波長65 8nm和 7 8 5 n m的組合,但是也可以是其他波長的組合。波長的組 合不同,最佳的臺階部的級數和深度尺寸也就不同。 另外,^通過用樹脂一體形成構成所述第一光柵部的凸 部1 la和構成第二光柵部的臺階部1 lb,就能降低成本。 第6圖所示的繞射光柵1 1 B是表示所述繞射光柵1 i a 的變形例的一部分的俯視圖。 該繞射光柵1 1 B在所述繞射光柵1 1 A的臺階部1 1 b 的各平坦面S 1〜S 6上重疊形成由鋸齒狀的的凹凸構成的微 小繞射光柵(第三光柵部)1 1 c。在該微小光柵部1 1 c中 ,當把從凸部到相鄰的凸部作爲1個周期時,該1周期最 好比所述雷射的波長λ 1和λ 2短。據此,就能起到與形 成高價防止反射膜時同樣的防止反射的作用。 綜上所述,本發明能使錯開的光軸在給定的位置上一 致,並且能僅使一方波長的雷射繞射,而使另一方的雷射 的繞射角度比以往的繞射角度更小,因此,與使雙方的雷 射都繞射的情況相比,更能降低由於溫度的變化而導致的 波長變動所造成的影響。 另外,因爲本發明的光學裝置具有發射兩個波長的雷 射的發光部和使各雷射的光軸一致的單一光學構件,所以 能減少零部件數量,簡化結構,從而能降低成本。 本紙張尺度適用中國國家標準(CNS ) Α4規格(2Ι0Χ297公釐) (請先閱讀背面之注意事項再填寫本頁) 訂 經濟部智慧財產局員工消費合作社印製 -12- 1227471 經濟部智慧財產局員工消費合作社印製 f VP ' > a 7I dHr B7 五、發明説明(id 【圖面之簡單說明】 第1圖是表示搭載了本發明的光學構件的光學裝置的 一個例子的槪要圖。 第2圖是表示光學構件及其光軸的模式圖。 第3圖是表示光學構件的一部分的俯視圖。 第4圖是表示相對於臺階數爲6的光柵深度的光的效 率的線圖。 第5圖是表示相對於臺階數爲5的光柵深度的光的效 率的線圖。 第6圖是表示本發明的光學構件的變形例的一部分的 俯視圖。 第7圖是表示以往的光學構件及其光軸的模式圖。 【符號說明】 10—光拾波器; 11一光學構件; 11a —凸邰(第一光柵部); Π b —臺階部(第二光栅部); 11c一微小光栅部(第三光柵部); 12—發光部; 12a、12b —發光元件; 1 3 —視准透鏡; 1 4 —分光鏡 ; 15 —物鏡; (請先閱讀背面之注意事項再填寫本頁) 本紙張尺度適用中國國家標準(CNS ) A4規格(210X 297公釐) -13- 1227471V. Description of the invention (8) The change becomes larger, so it is not good. In addition, although the second-order diffracted light of 7 8 5 n m can be obtained at the depth of (b), the efficiency is deteriorated, which is not good. Therefore, the grating depth dimension d is around 6 // m (more precisely, it should be around 6 · 1 // m). By forming the width and depth dimensions of the steps 丨 丨 b at equal distances, It is possible to obtain a diffraction grating 1 1 A which maintains a high efficiency. In addition, the line diagram shown in FIG. 5 is a step number of the diffraction grating 1 1 A shown in FIG. 3 changed from 6 steps to 5 steps. However, in this case, as described above, the width and depth dimensions of each stage are formed at equal distances. In the diffraction grating 1 1 A shown in FIG. 5, by setting the grating depth dimension d of the diffraction grating to the vicinity of 5 · 8 // m (e), the quotient efficiency of 6 5 8 nm can be obtained. -1 diffraction light and 0 8 diffraction light at 7 8 5 nm. In this case, it is also possible to reverse λ 1 and λ 2 so that 65 8 nm is λ 1 and 7 85 nm is λ 2. As described above, by adopting the shape of the grating depth dimension d of the diffraction grating determined by (a) in FIG. 4 or (e) in FIG. 5, only the 0th order diffraction light of the 65 8 nm laser is transmitted, and Diffracting only 1 diffraction light of a laser of 7 8 5 nm, or -1 diffraction light of a 65 8 nm laser, and transmitting only 0 diffraction light of a 785 nm laser, can make 7 The optical axis of 8 5 nm and the optical axis of 65 8 nm are aligned on the light receiving portion 16. Therefore, since one laser is not diffracted, it is not affected by the wavelength variation, and although the other laser is diffracted, the diffraction angle is smaller than in the past, so the effect of wavelength variation can be reduced as a whole. And 'The Chinese standard (CNS) A4 size (210x297 mm) applies to this paper size (Please read the precautions on the back before filling this page) Order printed by the Intellectual Property Bureau Staff Consumer Cooperatives of the Ministry of Economic Affairs -11-: 227471 5. Invention Description (9) In the optical member 11 according to (9), the shape of the 6th step in the number of steps of 6th and 5th steps is better in terms of light efficiency. In addition, in this embodiment, although the combination of the wavelengths of 65 8 nm and 7 8 5 nm is described, a combination of other wavelengths may be used. Depending on the combination of wavelengths, the number of steps and depth dimensions of the optimal stepped portion will vary. In addition, by integrally forming the convex portion 11a constituting the first grating portion and the step portion 1lb constituting the second grating portion with resin, the cost can be reduced. The diffraction grating 1 1 B shown in FIG. 6 is a plan view showing a part of a modification of the diffraction grating 1 i a. This diffraction grating 1 1 B is superposed on each of the flat surfaces S 1 to S 6 of the stepped portion 1 1 b of the diffraction grating 1 1 A to form a minute diffraction grating (a third grating) composed of jagged irregularities. Part) 1 1 c. In the micro grating portion 1 1 c, when one period is taken from the convex portion to the adjacent convex portion, the one period is preferably shorter than the wavelengths λ 1 and λ 2 of the laser. This makes it possible to prevent reflection in the same manner as when forming an expensive antireflection film. To sum up, the present invention can make the staggered optical axes consistent at a given position, and can only diffract the laser of one wavelength, and make the diffraction angle of the other laser more than the conventional diffraction angle. It is smaller, and therefore, it is possible to reduce the influence of the wavelength variation due to the temperature change more than in the case where both the lasers are diffracted. In addition, since the optical device of the present invention has a light emitting portion that emits lasers of two wavelengths and a single optical member that aligns the optical axes of the lasers, the number of parts can be reduced, the structure can be simplified, and the cost can be reduced. This paper size applies the Chinese National Standard (CNS) Α4 specification (2Ι0 × 297 mm) (Please read the precautions on the back before filling this page) Order printed by the Intellectual Property Bureau of the Ministry of Economic Affairs and Consumer Cooperatives-12- 1227471 Printed by employee consumer cooperative f VP '> a 7I dHr B7 V. Description of the invention (id [Simplified description of drawing] Figure 1 is a schematic diagram showing an example of an optical device equipped with the optical member of the present invention. Fig. 2 is a schematic view showing an optical member and its optical axis. Fig. 3 is a plan view showing a part of the optical member. Fig. 4 is a line chart showing the efficiency of light with respect to a grating depth of 6 steps. Fig. 5 is a line diagram showing the efficiency of light with respect to a grating depth of 5 steps. Fig. 6 is a plan view showing a part of a modification of the optical member of the present invention. Fig. 7 is a view showing a conventional optical member and its Schematic diagram of the optical axis. [Description of symbols] 10—optical pickup; 11—optical component; 11a—convex (first grating portion); Π b—step portion (second grating portion); 11c—micro Grid section (third grating section); 12—light emitting section; 12a, 12b—light emitting element; 1 3—collimator lens; 1 4—beamsplitter lens; 15—objective lens; (please read the precautions on the back before filling this page ) This paper size applies to China National Standard (CNS) A4 (210X 297 mm) -13- 1227471

五、發明説明(J 1 6 —受光部。 (請先閱讀背面之注意事項再填寫本頁)V. Description of the invention (J 1 6-Light receiving section. (Please read the precautions on the back before filling this page)

、1T 經濟部智慧財產局8工消費合作社印製 本紙張尺度適用中國國家標準(CNS ) Α4規格(210Χ 297公釐) -14-Printed by 8T Consumer Cooperatives, Bureau of Intellectual Property, Ministry of Economic Affairs, 1T This paper is sized to the Chinese National Standard (CNS) A4 (210 × 297 mm) -14-

Claims (1)

1227471 -if- A8 B8 C8 D8 申請專利範圍 .一種光學構 之光學構件, 置有使第一波 射光不繞射而 .如申請專利 述繞射光柵, 次繞射光的選 有對0次繞射 .如申請專利 雷射光 設 2的雷 2 所 有對1 光,具 3 所 階狀形 所述臺 ,相對 m λ 2 把 述第二 λ 1的 述繞射 成在所 階狀形 於所述 (η爲 所述第 波長λ 雷射光 光柵具 述第一 成的第 第二波 折射率 二光柵 2的雷 以規定 件,屬 其特徵 長入1 透射的 範圍第 對於所 擇性, 光的選 範圍第 有呈凹 光柵部 一 aU. tint 一尤W 長;I 2 ,m爲 部的臺 射光不 角度繞 於入射 在於: 的雷射 繞射光 對於所 擇性。 2項所 凸狀形 的傾斜 部的每 的雷射 正的整 階狀的 繞射而 射0 不同波長λ 1和λ 2的 光繞射,使第二波長λ 柵。 1項所述的光學構件,其中: 述第一波長λ 1的雷射光,具 述第二波長λ 2的雷身寸 述的光學構件,其中: 成的第一光柵部和呈臺 面上的第二光柵部,以 一級臺階的深度(h ) 爲 -1 h 數); 臺階數設置爲:能使所 透射,使所述第一波長 (請先閲讀背面之注意事項再填寫本頁) 訂 經濟部智慧財產局員工消費合作社印製 :是 : 2 : 中都 中 λ 中 其向 其長 其 , 方 ,波 , 件度 件二 件 構深 構第 構 學和 學述 學 光向 光所 光 的方 的, 的 述度 述1T1述 所寬 所 η 所 項在 項 5 項 3 階 3 8 5 第臺 第 7 第 圍各 圍爲 圍 範的 範 1 範 利部。利 λ 利 專柵的專長 專 請光成請波。請 申二形申一1T1申 如第來如第 η 如 •述距 ·述 8 · 4 所間 5 所 5 6 等 6 以 爲 本紙張尺度適用中國國家標準(CNS ) Α4規格(210X297公釐) -15 - 1227471 (修更 ABCD 頁VI '4 1Β替Φ 六、申請專利範圍 2 所述第二光柵部的臺階狀的臺階數爲6級。 7 ·如申請專利範圍第3項所述的光學構件,其中: 在所述第二光柵部的表面上形成有凹凸狀的第三光柵 部,把所述凹凸形成爲:使形成在所述第二光柵部的1個 臺階上的第三光柵部的周期在所述雷射光的波長以下。 8 ·如申請專利範圍第7項所述的光學構件,其中: 所述第一光柵部和第二光柵部都是用樹脂一體形成的 〇 9 · 一種光學裝置,其特徵在於: 設置有使發出第一波長λ 1的雷射光的發光點與發出 第二波長λ 2的雷射光的發光點向與光軸正交的方向錯開 置位的發光部,和使來自所述發光部的光進行透射的申請 專利範圍第1〜8項中任意1項所述的光學構件,使所述 第一波長λ 1的雷射光的光軸與第二波長λ 2的雷射光之 光軸在規定位置上一致。 (請先閱讀背面之注意事項再填寫本頁) 、11 經濟部智慧財產局員工消費合作社印製 -16- 本紙張尺度適用中國國家標準(CNS ) Α4規格(2Ι0Χ297公釐)1227471 -if- A8 B8 C8 D8 Patent application scope. An optical structure of an optical component, which is provided to prevent the first wave of light from being diffracted. For example, the diffraction grating is applied for the application. For example, for the patented laser light set 2 of the laser 2 all pair 1 light, the stage has a step shape of 3, and relative to m λ 2 the diffraction of the second λ 1 is formed in the step shape in the ( η is the predetermined wavelength of the second wavelength λ laser light grating with the second component of the second wavelength refractive index two gratings, which is a feature whose length is 1 and the range of transmission. For the selectivity, the selection range of light The first part has a concave grating part, aU. Tint, especially W length; I 2, m is a part of the table light does not angle around the incident on: the laser diffraction light for the selectivity. 2 convex shape of the inclined part Each of the lasers is diffracted in a positive order and diffracts light of different wavelengths λ 1 and λ 2 to make the second wavelength λ grid. The optical component according to item 1, wherein: the first wavelength λ Laser light of 1 with laser body of the second wavelength λ 2 The optical component described above, wherein: the first grating portion formed and the second grating portion on the table, the depth of the first step (h) is -1 h number); the number of steps is set to: The first wavelength (please read the precautions on the back before filling out this page) Printed by the Consumer Cooperatives of the Intellectual Property Bureau of the Ministry of Economic Affairs: Yes: 2: Zhongdu Zhong λ Zhong Qi Zhong Chang Long, Fang, Wave, Pieces The two parts of the structure are the deep structure of the structure and the theory of the light. The description of the light, the light, the light, the light, the light, the light, the light, the light, the light, the light, the light, the light, the light, the light, the light, the light, the light or the light, the light, the light, the light, the light, the light, the light, the light, the light, the light, the light, the light, the light, the light, the light, the light, the light, the light, the light, the light, the light, the light, the light, the light, the light, the light, the light, the light, the light, the light, the light, light Each circle is the Fan 1 Fan Li Department of the Fan. Lee's expertise Please apply for two-form application, 1T1 application as the first item, such as item η, such as • distance, description 8 · 4 between 5 places 5 6 etc. 6 The Chinese paper standard (CNS) Α4 specification (210X297 mm) applies to this paper size- 15-1227471 (revised ABCD page VI '4 1B instead of Φ VI. Patent application scope 2 The number of steps of the second grating portion of the second grating portion is six. 7 · The optical member according to item 3 of the patent application scope , Wherein: a concave-convex third grating portion is formed on a surface of the second grating portion, and the concave-convex is formed so that a third grating portion formed on a step of the second grating portion The period is below the wavelength of the laser light. 8 · The optical member according to item 7 of the patent application scope, wherein: the first grating portion and the second grating portion are both integrally formed of resin. 9 · An optical The device is characterized in that: a light-emitting portion is provided in which the light-emitting point emitting laser light of a first wavelength λ 1 and the light-emitting point emitting laser light of a second wavelength λ 2 are staggered in a direction orthogonal to the optical axis, and Transmitting light from the light-emitting part The optical member according to any one of the items 1 to 8 of the patent scope, please make the optical axis of the laser light of the first wavelength λ 1 and the optical axis of the laser light of the second wavelength λ 2 coincide at a predetermined position. (Please read the precautions on the back before filling out this page), 11 Printed by the Consumer Cooperatives of the Intellectual Property Bureau of the Ministry of Economic Affairs -16- This paper size applies to China National Standard (CNS) Α4 specification (2Ι0 × 297 mm)
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