CN100401110C - Optical element group for optical read-write head and its manufacturing method - Google Patents
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Abstract
Description
技术领域 technical field
本发明有关一种光学读写装置,且特别是有关一种光学读写头。The invention relates to an optical read-write device, and in particular to an optical read-write head.
背景技术 Background technique
将数据储存在CD及DVD上与通过光学读写装置将储存其上的数据进行存取的技术已熟为人知,通常数据的读写是借由光学读写头的动作而进行;将数据由盘片上取出的原理为先将激光光束聚焦于盘片数据储存表面上,然后将由盘片表面所反射出来而产生的信号光束透过一光探测器,转换成电子信号;实验结果已证实,若入射于光盘片的激光光束为一圆偏振光,则所得的信号光束较佳,因此,使入射于光盘片的光束成为一圆偏振光便成为光学读写头的光学设计条件之一。The technology of storing data on CDs and DVDs and accessing the data stored on them through optical read-write devices is well known. Usually, the reading and writing of data is carried out by the action of optical read-write heads; The principle of taking out the disc is to focus the laser beam on the data storage surface of the disc first, and then pass the signal beam reflected by the disc surface through a photodetector to convert it into an electronic signal; the experimental results have confirmed that if When the laser beam incident on the optical disc is a circularly polarized light, the resulting signal beam is better. Therefore, making the incident beam on the optical disc into a circularly polarized light becomes one of the optical design conditions of the optical pick-up head.
图1A显示了一传统的光学读写头,此光学读写头包括一DVD读写用的激光二极管101、一CD读写用的激光二极管103、一偏极分光镜(polarized beamsplitter)105、一偏极分光镜107、一反射镜(folding mirror)109、一四分之一波板(quarter wavelengh plate;QWP)111以及一光探测器113;激光二极管101与103是用以产生激光光束,激光光束于激光二极管射出后为线偏振状态,亦即其两垂直分量(分别称为S-波、P-波)之间无相位差存在;偏极分光镜105与107是用以对光束中不同的极化分量(S-波与P-波)作反射或透射;反射镜109是用以将光束反射而改变光束的前进方向;而四分之一波板111是用以调整光束的极化态,使光束的S-波、P-波之间产生相位差,当S-波与P-波的相位差达+90度或+270度(亦即-90度)时,便可以使入射于光盘的光束产生九十度的相位差,进而将光束转换成圆偏振光,以产生较佳的信号光束;光探测器113则用于接收由盘片表面所反射出来而产生的信号光束。Fig. 1A has shown a traditional optical read-write head, and this optical read-write head comprises a
此外,CD激光二极管103出光后,有相互垂直的S-波分量与P-波分量,各以IS1与IP1表示其起始强度,假设起始相位差δS-P=0°,如图1B所示,当其入射于偏极分光镜107时,S-波及P-波的穿透效率分别为90%与0%,如图1C的实线所示,若入射于反射镜109时,S-波及P-波的穿透效率分别为70%与20%,如图1D的实线所示,偏极分光镜107与反射镜109的特性如表1所示;In addition, after the
表1Table 1
所以,S-波经偏极分光镜107反射后强度IS成为0,而P-波经偏极分光镜107反射后强度IP=IP1×90%=0.9IP1;接着S-波再经过反射镜109反射后强度IS=0×70%=0,而P-波经反射镜109反射后强度IP=0.9IP1×20%=0.18IP1,则经过偏极分光镜107与反射镜109后,光束的P-波能量IP=0.18IP1,而S-波能量IS则完全不见,且在光束进入光盘前,会再经过四分之一波板111,使之成为圆偏振状态,如图1E所示。由前述可知,虽然最终可以达成使光束成为圆偏振状态,但S-波能量却完全消失,而未被利用到。Therefore, the intensity I S of the S-wave after being reflected by the polarizing
发明内容 Contents of the invention
本发明提供一种用于光学读写头的光学元件组,该光学元件组中不含四分之一波板(quarter wavelength plate;QWP),且此光学元件组包括位于一光程上的数个光学元件,其中至少二光学元件上各具有改变光束极化态的一光学镀膜,使沿该光程行进的一出射光成为一圆偏振光,该圆偏振光入射于一光储存媒体,并最终成为一光探测器所接收的一信号光束。本发明亦提供一种前述光学元件组的制造方法。The present invention provides an optical element group for an optical read-write head, the optical element group does not contain a quarter wave plate (quarter wavelength plate; QWP), and the optical element group includes data located on an optical path An optical element, wherein at least two optical elements each have an optical coating that changes the polarization state of the light beam, so that an outgoing light traveling along the optical path becomes a circularly polarized light, and the circularly polarized light is incident on an optical storage medium, and Finally, it becomes a signal light beam received by a light detector. The invention also provides a manufacturing method of the aforementioned optical element group.
由于本发明所提供的光学元件组中不含四分之一波板,因此,可省去四分之一波板的成本,还可避免四分之一波板品质不良以及组装不良所造成的问题;此外,本发明的相位差是由不同光学元件所组合而产生,因此,可利用各光学元件上的镀膜将光束的极化态调整至各光学元件透射或反射效率较高的极化态,如此,便可得到较佳的信号强度。Since the optical element group provided by the present invention does not contain a quarter-wave plate, the cost of the quarter-wave plate can be saved, and problems caused by poor quality and poor assembly of the quarter-wave plate can also be avoided. Problem; In addition, the phase difference of the present invention is produced by the combination of different optical elements, therefore, the polarization state of the light beam can be adjusted to the polarization state with higher transmission or reflection efficiency of each optical element by using the coating on each optical element , so that better signal strength can be obtained.
附图说明 Description of drawings
图1A-1E为现有光学读写头的光学元件组成及各光学元件特性图。1A-1E are diagrams showing the composition of optical components and the characteristics of each optical component of a conventional optical read-write head.
图2A-2E为依据本发明光学读写头的光学元件组成及各光学元件特性图。2A-2E are diagrams showing the composition of the optical elements and the characteristics of each optical element of the optical read-write head according to the present invention.
图3A-3D为依据本发明的的光学元件组所产生的相位差与光束波长的关系图。3A-3D are graphs showing the relationship between the phase difference generated by the optical element group and the wavelength of the light beam according to the present invention.
图4为依据本发明的光学设计的解说图。Fig. 4 is an illustration of an optical design according to the present invention.
具体实施方式 Detailed ways
图2A为本发明一较佳实施例用于光学读写头的光学元件组的示意图,该光学元件组包括一DVD读写用的激光二极管201、一CD读写用的激光二极管203、一具光学镀膜204的偏极分光镜205、一具光学镀膜206的偏极分光镜207、一具光学镀膜208的反射镜209以及一光探测器211;激光二极管201与203是用以产生分别使用于读写DVD与CD的激光光束,偏极分光镜205与207是用以对光束中不同的极化分量作反射或透射,反射镜209是用以将光束反射而改变光束的前进方向,偏极分光镜205、207与反射镜209上的光学镀膜204、206与208可以使光束的两垂直分量(分别称为S-波、P-波称)之间产生相位差,以调整光束的极化态,当S-波与P-波的相位差达+90度或+270度(亦即-90度)时,便可以使入射于光盘的光束成为圆偏振光;光探测器211则用于接收由盘片表面所反射出来而产生的信号光束,并将之转换成一电子信号。2A is a schematic diagram of an optical element group used for an optical read-write head in a preferred embodiment of the present invention. The optical element group includes a
一般而言,所使用的DVD读写用的激光二极管201的波长为660奈米,则可分别设计具产生相位差的光学镀膜204、206与208的偏极分光镜205、207与反射镜209,使其所产生的相位差与光束波长的关系分别如图3A、3B与3C所示,如此,当激光光束经过具产生相位差的镀膜204、206与208的偏极分光镜205、207与反射镜209时,其相位差总合将如图3D所示,当激光光束的波长为660奈米时,由于光学镀膜204、206与208分别可使激光光束的S-波与P-波产生θ1、θ2及θ3的相位差,并使θ1、θ2及θ3满足下列条件:Generally speaking, the
θ1+θ2+θ3=90°或270°(1)θ 1 +θ 2 +θ 3 = 90° or 270°(1)
因此,依据本发明的光学元件组可以使入射于光盘的光束成为圆偏振光,与四分之一波板所产生的效果相同,所以便可将四分之一波板省去;熟悉本技术的人员可依其需要增减光学元件的数目与种类,通常所使用于光学读写头的光学元件有激光二极管、偏极分光镜(polarized beam splitter)、光栅(grating)、反射镜(folding mirror)、偏光板以及准直器(collimator),以分别使光束产生θ1、θ2...等相位差,并使其总合为+/-90度,以达成产生圆偏振光的目的。Therefore, according to the optical element group of the present invention, the light beam incident on the optical disk can be made into circularly polarized light, which is the same as the effect produced by the quarter-wave plate, so the quarter-wave plate can be omitted; The number and types of optical components can be increased or decreased by the personnel according to their needs. Usually, the optical components used in optical read-write heads include laser diodes, polarized beam splitters, gratings, and folding mirrors. ), a polarizer, and a collimator to generate phase differences such as θ 1 , θ 2 , etc. of the light beams respectively, and make the total of them +/-90 degrees, so as to achieve the purpose of generating circularly polarized light.
此外,本发明还可利用产生相位差的原理,将光束极化态转换到透射或反射效率较高的状态,亦即可利用产生相位差的原理,在对光学元件镀膜的同时,根据所需达成的相位差以及反射/透射率,去一并考虑材料种类的选择、层数以及厚度。在进行光学元件的设计时,如图4所示,可利用下列公式:In addition, the present invention can also use the principle of phase difference to convert the polarization state of the light beam to a state with higher transmission or reflection efficiency, that is, the principle of phase difference can be used to coat the optical element according to the required The achieved phase difference and reflectance/transmittance take into account the selection of material type, number of layers and thickness. When designing optical components, as shown in Figure 4, the following formulas can be used:
Tan2α=[2 IS0IP0Cos(s,p phase shift)]/IS0 2-IP0 2(2)Tan2α=[2 I S0 I P0 Cos(s, p phase shift)]/I S0 2 -I P0 2 (2)
IS0及IP0分别代表具产生相位差的镀膜的光学元件对于光束的反射/透射强度,(s,p phase shift)代表具产生相位差的镀膜的光学元件对于光束的S-波与P-波之间所产生的相位差,夹角α代表椭圆极化光的长轴与S-波坐标轴的夹角。I S0 and I P0 respectively represent the reflection/transmission intensity of the optical element with a coating that produces a phase difference for the beam, and (s, p phase shift) represent the S-wave and P-wave of the optical element with a coating that produces a phase difference for the beam. The phase difference generated between the waves, the angle α represents the angle between the long axis of the elliptically polarized light and the S-wave coordinate axis.
以图2A为例,CD激光二极管203出光后,有相互垂直的S-波分量与P-波分量,各以IS1与IP1表示其起始强度,假设起始相位差δS-P=0°,如图2B所示,当其入射于具产生相位差的镀膜的偏极分光镜207时,S-波及P-波的穿透效率分别为90%与0%,如图2C的实线所示,若入射于具产生相位差的镀膜的反射镜209时,S-波及P-波的穿透效率分别为70%与20%,如图2D的实线所示,然而,依据本发明的实施例中,偏极分光镜207与反射镜209上分别有可产生相位差的光学镀膜206与208,光学镀膜206与208分别可使S-波与P-波之间产生70°与200°的相位差,分别如图2C与2D的虚线椭圆所示,偏极分光镜与反射镜的特性如表2所示;Taking Fig. 2A as an example, after the
表2Table 2
所以,当激光光束入射于偏极分光镜207时,光学镀膜206会对光束能量重新分布,并使S-波与P-波之间产生70°的相位差,使激光光束变为椭圆偏振,并将椭圆长轴调整至接近P-波的方向(因为P-波反射效率较高),如此一来,经过具产生相位差的镀膜的偏极分光镜207时,当δS-P=70°时,Is=0.15IS1,Ip=0.95IP1。Therefore, when the laser beam is incident on the
接下来经过具产生相位差的镀膜的反射镜209时,利用同样的道理,把相位设计大部分的能量集中在偏向P-波方向,原本δS-P=0时,到具产生相位差的镀膜的反射镜209已经没有能量穿过,即使具产生相位差的镀膜的反射镜209的穿透效率很大也是利用不到,不过假如已经经过具产生相位差的镀膜的偏极分光镜207设计使相位差为δS-P=70°,在具产生相位差的镀膜的偏极分光镜207出光时Is=0.15IS1,Ip=0.95IP1,假若设计具产生相位差的镀膜的反射镜209,使其所产生的相位差δS-P=200°,将能量转移集中到P-波方向,如此一来,整体经过具产生相位差的镀膜的反射镜207与209后的能量,会变为Is=0.13IS1,Ip=0.13IP1,一般而言IS1会等于IP1,所以不但光束整体能量会比使用现有技术要强,还可使相位差总合为δS-P=70+200=270°或是-90°,如图2E所示,达到圆偏振的效果,同时增加效率和造成所想要的偏振现象。Next, when passing through the
由于本发明所提供的光学元件组中在光学元件上使用产生相位差的光学镀膜,以达到产生相位差的目的,因此不含四分之一波板,故而,可省去四分之一波板的成本,还可避免四分之一波板品质不良以及组装不良所造成的问题;此外,本发明的相位差是由不同光学元件所组合而产生,因此,可利用各光学元件上的镀膜将光束的极化态调整至各光学元件透射或反射效率较高的极化态,如此,便可得到较佳的信号强度。Since the optical element group provided by the present invention uses an optical coating that produces a phase difference on the optical element to achieve the purpose of producing a phase difference, it does not contain a quarter-wave plate, so a quarter-wave can be omitted The cost of the plate can also avoid the problems caused by the poor quality of the quarter-wave plate and the poor assembly; in addition, the phase difference of the present invention is produced by the combination of different optical elements, so the coating on each optical element can be used The polarization state of the light beam is adjusted to the polarization state with higher transmission or reflection efficiency of each optical element, so that better signal strength can be obtained.
虽然本发明已以较佳实施例揭示如上,然而其并非用以限定本发明,任何熟悉本技术的人员在不脱离本发明的精神和范围内,当可作出种种的等效的改变或替换,因此本发明的保护范围当视后附的本申请权利要求范围所界定的为准。Although the present invention has been disclosed above with preferred embodiments, it is not intended to limit the present invention. Any person familiar with the art may make various equivalent changes or replacements without departing from the spirit and scope of the present invention. Therefore, the scope of protection of the present invention should be defined by the appended claims of the application.
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Citations (4)
Publication number | Priority date | Publication date | Assignee | Title |
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JPS58169351A (en) * | 1982-03-31 | 1983-10-05 | Pioneer Video Corp | Optical information reading device |
CN1195847A (en) * | 1997-02-27 | 1998-10-14 | 三星电子株式会社 | Optical recording/pickup head compatible with compact disk-recordable (CD-R) and digital versatile disk (DVD) using polarization beam splitter |
US20020021494A1 (en) * | 2000-08-18 | 2002-02-21 | Delta Electronics, Inc. | Optical device |
CN1430219A (en) * | 2002-01-04 | 2003-07-16 | 财团法人工业技术研究院 | Multi-wavelength optical read/write head |
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Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS58169351A (en) * | 1982-03-31 | 1983-10-05 | Pioneer Video Corp | Optical information reading device |
CN1195847A (en) * | 1997-02-27 | 1998-10-14 | 三星电子株式会社 | Optical recording/pickup head compatible with compact disk-recordable (CD-R) and digital versatile disk (DVD) using polarization beam splitter |
US20020021494A1 (en) * | 2000-08-18 | 2002-02-21 | Delta Electronics, Inc. | Optical device |
CN1430219A (en) * | 2002-01-04 | 2003-07-16 | 财团法人工业技术研究院 | Multi-wavelength optical read/write head |
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