TW476947B - Optical pickup - Google Patents
Optical pickup Download PDFInfo
- Publication number
- TW476947B TW476947B TW89122756A TW89122756A TW476947B TW 476947 B TW476947 B TW 476947B TW 89122756 A TW89122756 A TW 89122756A TW 89122756 A TW89122756 A TW 89122756A TW 476947 B TW476947 B TW 476947B
- Authority
- TW
- Taiwan
- Prior art keywords
- lens
- light source
- optical pickup
- light
- laser beam
- Prior art date
Links
Landscapes
- Optical Head (AREA)
- Lenses (AREA)
Abstract
Description
ή|6947Price | 6947
發明說明( 經濟部智慧財產局員工消費合作社印製 【發明背景】 1·發明領域 本發明係有關於一種用於高密度資訊寫入及讀取系統 的拾光’且更特別地,有關於一種可以降低色像差的拾 光器,其係發生在當一藍色光源被使用時。 2·相關技術說明 在光學寫入及讀取系統中,此記錄密度係由聚焦光點 的尺寸大小來決定。一般而言,此聚焦光點的尺寸大小(s) 與波長(λ)成正比,且與口徑(n A)成反比,其可以 方程式(1)來表示: " S 又/NA ......... (1) 對於比在小型碟片(CD s)或數位多用途碟片(d VD s )中所達成之記錄密度更高之一記錄密度而言,此 被聚焦在一光碟上之光點的尺寸大小必須被進一步降低。 ,降低此絲尺寸大小,何被從方程式⑴推論+ 射光束的波長⑴必須被降低,及此接物 ^ 所以,對於如此之高密度資訊記= 有短波長的一雷射光束,舉例而言,一藍先帝 一 2當成一光源,且此接物鏡的口徑必須:維:在 圖1為一圖顯示有關於在此雷射二極體 2輸二倍率方面,一雷射二極體的 ;溫二下 為一圖顯示有關於各種光學材物質 ^化。圖2 」!!!^圖η,倍率:-特別== 冰張尺度適用規格⑵。x 又 --------^---------^ 1^ c請先閱讀背面之注音?事項再填寫本頁} 476947 A7 B7 五、發明說明(>) 下^加’此發射波長成正比地增加,其為雷射二極體的一 個特徵。如同在圖2中所示,各種光學物質之折射的指數 在一短波長區域中突然地變化,舉例而言,接近400 nm, 比較在對於小型碟片(C d s )之780 nm與在對於數位 多用途碟片(DVD s )之650 nm ° 在¥寫入資訊到一光碟時,在此光碟上的一所需位 置,被以寫入能量搜尋,且然後一記錄標號藉由增加寫入 能量而被形成在此被找到的位置上。但是,在輸出能量方 面如此一個突然的變化引起在此光學系統中的色像差,藉 此散焦此光點在此光碟上。另外,其花費不少的時間藉由 一伺服電路的控制去更正此散焦。換句話說,當一高頻(Η F)模組被用來降低由於光束從一光碟反射向一光源而引 起之雜訊,從此光源發射之光束的波長增加,藉此增加了 在此光學系統中的色像差,且特別地,在此接物鏡中,此 問題引起一複製信號之品質的降低。另外,其可進一步被 考慮,如陳圖1巾可見,此發㈣束的波長可隨著在此 拾光器内部之溫度而增加,且因使用不同光源而引起之波 長的變化改變了色像差。 各種不同的拾光器(其具有-光源,此光源具有一 650 的波長及—物鏡)已經被提出以使其可相容於⑽醒 厚度之DVD s及1.2 mm厚度之CD s,在被使用於這 些被提出的拾光器中之技術有-種環狀遮罩技術,用來阻 擋經過在遠軸與近軸區域間之中間區域的 _ -------------% (請先閱讀背面之注意事項再填寫本頁) 訂---------線— 經 濟 部 智 慧 財 產 局 員 工 消 費 合 作 社 印 製 用來藉由使用液晶(LC)快門而控制接物鏡的吨,及Description of the Invention (Printed by the Consumer Cooperative of Intellectual Property Bureau of the Ministry of Economics [Background of the Invention] 1. Field of the Invention The present invention relates to a light pick-up for a high-density information writing and reading system 'and more particularly, to An optical pickup capable of reducing chromatic aberration occurs when a blue light source is used. 2. Description of Related Technology In an optical writing and reading system, the recording density is determined by the size of a focused light spot. In general, the size (s) of this focused spot is proportional to the wavelength (λ) and inversely proportional to the aperture (n A), which can be expressed by equation (1): " S and / NA. ........ (1) This is the focus for a higher recording density than that achieved in compact discs (CD s) or digital versatile discs (d VD s). The size of the light spot on a disc must be further reduced. To reduce the size of this wire, why is it deduced from the equation + + the wavelength of the light beam ⑴ must be reduced, and this object ^ So, for such a high density Information note = a laser beam with a short wavelength, for example In other words, a Lanxiandi 2 is used as a light source, and the aperture of this objective lens must be: Dimensions: In Figure 1 is a diagram showing that in terms of the double power loss of the laser diode 2, a laser diode The figure below Wen Erxia shows a picture of various optical material materials. Figure 2 "!!! ^ 图 η, magnification: -Special == ice sheet scale applicable specifications ⑵. X Again ------- -^ --------- ^ 1 ^ cPlease read the note on the back? Matters before filling out this page} 476947 A7 B7 V. Description of the invention (>) ^ Add 'This emission wavelength increases in proportion to , Which is a feature of laser diodes. As shown in Figure 2, the refractive index of various optical substances changes abruptly in a short wavelength region, for example, close to 400 nm, compared to that for small discs. 780 nm for films (C ds) and 650 nm for digital versatile discs (DVD s) ° When writing information to a disc, a desired position on this disc is searched by writing energy And then a record label is formed at this found position by increasing the writing energy. However, it is so sudden in terms of output energy The change causes chromatic aberration in the optical system, thereby defocusing the light spot on the disc. In addition, it takes a lot of time to correct this defocus by the control of a servo circuit. In other words, when A high frequency (ΗF) module is used to reduce the noise caused by the light beam reflected from a disc to a light source. The wavelength of the light beam emitted from this light source is increased, thereby increasing the chromatic aberration in this optical system. And, in particular, in this objective lens, this problem causes a reduction in the quality of a duplicated signal. In addition, it can be further considered, as seen in Chen Figure 1, the wavelength of the hair bundle can be picked up with the light here The temperature inside the device increases, and the change in wavelength caused by using different light sources changes the chromatic aberration. Various optical pickups (which have a light source with a wavelength of 650 and an objective lens) have been proposed to make them compatible with wake-up DVD s and 1.2 mm CD s. The technology in these proposed optical pickups is a kind of ring mask technology, which is used to block the passing of the middle area between the far axis and the paraxial region. % (Please read the precautions on the back before filling out this page) Order --------- Line — Printed by the Consumer Cooperatives of the Intellectual Property Bureau of the Ministry of Economic Affairs to control the objective lens by using a liquid crystal (LC) shutter Tons, and
476947 A7 五、發明說明(β) 一種全息圖光學元件(Η〇Ε)技術用來使用一全息圖光 學元件(ΗΟΕ)而分光以形成在具有不同厚度的兩磁碟 上之單一焦點。但是,對於一小型可記錄碟片(c D〜R ), 有關此紅色光源的反射率突然地下降,且因此具有78〇nm 之一波長的光源被需求。因為此原因,一DVD不限定/ C D限定光學系統的使用提供在78〇nm& 65〇nm的光束 間之相谷性,或具有一在遠軸與近軸區域間之環狀聚焦區 域的一接物鏡之使用已被提出。特別地,對於—cD限定 光學系統,此接物鏡的口徑被限制且發散光束被投射在此 接物鏡上,藉此更正由於在磁碟與此接物鏡的厚度方面之 差異所引起之像差。 使用一短波長光源的一拾光器,被需求來用於比D V D系統所能達到之更高密度資訊之寫入及讀取。如同一範 例,對於用於H D — D V D s之一拾光器,具有比被d V D s所使用之650 nm更短之一波長之雷射光束,被需求 當成一光源。但是,如同先前所解釋並參考圖2,因為此 磁碟之光學物質的折射指數在比650 nm短的波長上突然 地、艾化,過度的像差發生。因此,存在對於相容於現今之 DVD s,且可以有效地降低色像差的一光學系統之需要。 對於一DVD— R,有關於與紅色光源不同之光源的 反射率降低。因此,對於與DVD —R s之相容性,具有 650 nm的一波長之光源必須被進一步使用。但是,此像差 的問題無法藉由只控制從此650 nm光源發射,且投射在 此接物鏡上之光束的發散而被排除。因此,在發展HD — 本紙張尺度適規格⑵〇 χ 297公釐) 頁 訂 "f/6947 五、發明說明(y) =:容系統方面的關鍵問題為找到-種有效的色像差 述在 =及:J圖】鏡物鏡由兩個透鏡包括-第- ==3’被排列在-磁碟6與用來聚集先東的2 二曰]°顯不在圖3的此結構允許口徑增加到0.7或 因此’如此的—個接物鏡可被使用在用於高密度紀 :的:光學系統中。但是’此接物鏡在兩個透鏡增加此系 光路從長度的使用方面有問題,且光束點的複製,對 關位置方面的一變化高度地敏感。476947 A7 V. Description of the Invention (β) A hologram optical element (ZOE) technology is used to split a light using a holographic optical element (ZOE) to form a single focus on two magnetic disks having different thicknesses. However, for a small recordable disc (c D ~ R), the reflectivity of this red light source suddenly drops, and therefore a light source having a wavelength of 78 nm is required. For this reason, the use of a DVD-unlimited / CD-limited optical system provides a valley between beams of 78nm & 65nm, or a ring-shaped focus region with a far-axis and a paraxial region. The use of objective lenses has been proposed. In particular, for the -cD-limited optical system, the aperture of the objective lens is limited and the divergent beam is projected on the objective lens, thereby correcting aberrations caused by the difference in the thickness of the magnetic disk and the objective lens. An optical pickup using a short-wavelength light source is required for the writing and reading of higher density information than can be achieved by a D V D system. As in the same example, a laser beam with a wavelength shorter than 650 nm used by d V D s is required as a light source for one of the optical pickups used for H D — D V D s. However, as previously explained and referenced to Fig. 2, because the refractive index of the optical substance of this magnetic disk suddenly, aerates at wavelengths shorter than 650 nm, excessive aberrations occur. Therefore, there is a need for an optical system that is compatible with today's DVD s and can effectively reduce chromatic aberration. For a DVD-R, there is a reduction in the reflectance of a light source different from the red light source. Therefore, for compatibility with DVD-R s, a light source with a wavelength of 650 nm must be further used. However, the problem of this aberration cannot be ruled out by controlling only the divergence of the light beam emitted from the 650 nm light source and projected on the objective lens. Therefore, in the development of HD — this paper is suitable for the standard size ⑵ χ 297 mm) page order " f / 6947 V. Description of the invention (y) =: The key problem in the capacity system is to find an effective chromatic aberration description In = and: J]] the lens objective lens consists of two lenses-the first-== 3 'is arranged on-disk 6 and used to focus the first two 2]] This structure is not visible in Figure 3 allows the aperture to increase To 0.7 or so 'such-an objective lens can be used in high-density: optical systems. However, this objective lens has problems in using two lenses to increase the length of the optical path, and the reproduction of the beam spot is highly sensitive to a change in the position.
為解決上述問題,本發明的一個目的為提供一種拾光 器,其使用不同短波長雷射光束當成光源。 D 本發明的另一個目的為提供一種拾光器,其可以有效 地更正由於在光學物質的折射率方面之一個突然的改變而 引起之像差。 本發明仍有另一個目的為提供一種拾光器,其使用一 用於數位多用途碟片(DVD s )之650 nm的雷射光束, 及一用於HD — DVD s之大約400 nm的雷射光束,以 使其能相容於其它光學記錄媒體。 根據本發明的一個觀點,本發明提供一種拾光器包 括··一光源,用來產生500 nm或更短的一雷射光束;— 4/0^/ 4/0^/ 經濟部智慧財產局員工消費合作社印製 A7 五、發明說明(f) 接物鏡,用來將此雷射光束聚焦在 上 此光碟所反射之雷射光束成為一電子二及 且右恭與Γ、.其被排列在此光源與此接物鏡之間,包括— =政:率之散光透鏡及一具有聚焦倍率之聚焦透鏡, i k此對準透鏡的總焦距為f,及此散光透鏡的焦 距為fn,此對準透鏡符合關係一1.5>f/fn。 ,,本,日月的另—觀點’本發明提供—種拾光器包 弟及第—光源,其各別地對應到第一及第二媒體, 生不3波長的雷射光束;—接物鏡,用來各別地將 弟―及第二光源傳來的f射光束聚焦在此第—及第二 t上;第一及第二㈣測器,用來各別地接收從此第-及弟—光源所發射的雷射光束與從此第一及第二媒體所反 $的雷射光束;及-對準透鏡,其被排列在具有一相對短 波長之雷射光束其中之一的光路徑上,此對準透鏡包括一 具有發散倍率之散光透鏡及一具有聚焦倍率之聚焦透鏡, 在其中假設此對準透鏡的總焦距為f,及此散光透鏡的焦 距為fn,此對準透鏡符合關係一 1.5>f/fn。 根據本發明的另一觀點,本發明提供一種拾光器包 括:一接物鏡,其被排列正對第一及笫二媒體;一第一光 源,其被排列在此接物鏡的光路徑上;一分光器,其被排 列^此接物鏡與此第一光源之間;一第二光源,其被排列 在從此分光器所反射之光束的光路徑上;一第一相偵測器 用來接收從此第一光源所發射的雷射光束與從此第一媒體 所反射的雷射光束;一第二相須測器用來接收從此第光源 (請先閱讀背面之注意事項再填寫本頁) ·11111111 1^ A7 A7 經濟部智慧財產局員工消費合作社印製 五、發明說明(& =:射ίΐ與從此第二媒體所反射的雷射光束;及 =—:r散倍率之散光魏及 ^在其中假設此對準透鏡的總焦距為f Ϊ ^焦距為免,此對準透鏡符合關係、—bf/fn 根據本發明的另—觀點,本發明提供_ 括:-接物鏡,其被排列正對第一及第二媒體;二第^ 2皮排列在此接物鏡的光路徑上,用來發射一雷射光 =向i匕第一光碟;第一,第二及第三分光器,其;: ^仗此弟-光源朝向此接物鏡之預定位置的光路徑上.— 苐二光源,其被排列在被此第一 丄 :徑上,用來發射一雷射光東經二=:= 弟一媒體;一第一相偵測器,其被排列在被此第三分光哭 所反射之光束的光路徑上,用來接收從此第一光源所 之雷射光束及從此第一媒體所反射之雷射光束;一第二 ,測為,其被排列在被此第二分光騎反射之光朿的光路 徑上’用來接收從此第二光源所發射之雷射光束及從此 二媒體所反射之雷射光束;及—解透鏡,其被排列在此 接物鏡與此第三分光器之間,此對準透鏡包括一具有發散 =率之散光透鏡及一具有聚焦倍率之聚焦透鏡,在其^叉 δ又此對準透鏡的總焦距為f,及此散光透鏡的焦距為缶, 此對準透鏡符合關係一1.5>f/fn。 藉由詳細的說明本發明的較佳實施例並參考附圖,本 發明的上述目的及優點將變得更顯而易見: 本紙張尺度適用中關家標準(CNS)A4規格⑵Q χ视公f n ϋ · I n I n n I « I I ϋ I ϋ I I II I I ϋ n ϋ ϋ — ϋ ϋ n ϋ n ϋ ϋ n n n ϋ (請先閱讀背面之注意事項再填寫本頁) 476947 A7 、發明說明(^ ) 【發明詳述】 <實施例1> 根據本發明的-種拾光器的一第一較佳實施例被 圖4中。*考si 4 ’ Q 4被定位在正對—媒坪 (光茱)1 〇 〇的一接物鏡1 〇 1之光軸端點上。—又、 4玻璃板1 〇7 ’ -分光器! 〇2及—對準透鏡η 排列在此接物鏡!〇丄與此光源丄〇 4之間。此對準透鏡 10 3包括一具有聚焦倍率之聚焦透鏡i 〇 3 a及= 發散倍率之散光透鏡1 〇 3 b。 ’、 …一相偵測器1 0 6被排列在從此分光器1 〇 2所反射 之光束的光路徑之端點上,及一聚集透鏡1 〇 5用來聚隼 此反射光束,其被定位在分光器丄〇 2與此相侧器^ 6之間。 σ 當此光源1 〇 4發射一 500 nm或更短之雷射光 時二此對準透鏡具有對應的光學特性,其形成本發明的一 特欲。作又没此對準透鏡工0 3的總焦距為f,及 yyb的焦距“,此對準透鏡1〇3符合_ — 1·) > i/fn。 <實施例2 > 5中根的此種拾光器的—第二實施例被顯示在圖 (光禅;二η光源1〇4被定位同軸於正對-媒體 (先業)1()〇的—接物鏡1〇1之光轴。 炉 〇 3,一 λ/4玻填板i 〇 7及-分光哭9透,見 此接物鏡1 0 1與此光源10 4之間。非列在 此對準透鏡1 〇 3 (請先閱讀背面之注意事項再填寫本頁} ,¾In order to solve the above problems, an object of the present invention is to provide an optical pickup that uses different short-wavelength laser beams as a light source. D Another object of the present invention is to provide an optical pickup which can effectively correct aberrations caused by a sudden change in the refractive index of an optical substance. Still another object of the present invention is to provide an optical pickup that uses a laser beam of 650 nm for digital versatile discs (DVD s) and a laser of about 400 nm for HD-DVD s The light beam is made to be compatible with other optical recording media. According to an aspect of the present invention, the present invention provides an optical pickup including a light source for generating a laser beam of 500 nm or less;-4/0 ^ / 4/0 ^ / Intellectual Property Bureau of the Ministry of Economic Affairs Printed by employee consumer cooperative A7 V. Description of the invention (f) An objective lens is used to focus the laser beam on the laser beam reflected on the disc to become an electron two and right and Gong and Γ, which are arranged in Between this light source and the objective lens, it includes: = astigmatism lens and a focusing lens with focusing magnification, ik, the total focal length of this alignment lens is f, and the focal length of this astigmatic lens is fn, this alignment The lens conforms to the relationship 1.5 > f / fn. Another, viewpoint of the sun and the moon. The present invention provides a kind of optical pickup package and a first light source, which respectively correspond to the first and second media, and generate a laser beam of 3 wavelengths; The objective lens is used to separately focus the f-ray beams from the second and second light sources on the first and second t; the first and second detectors are used to separately receive the first and second Brother-the laser beam emitted by the light source and the laser beam reflected from the first and second media; and-an alignment lens arranged in the optical path of one of the laser beams having a relatively short wavelength In the above, the alignment lens includes a astigmatism lens with a divergent magnification and a focus lens with a focus magnification, where it is assumed that the total focal length of the alignment lens is f and the focal length of the astigmatic lens is fn. The alignment lens conforms to Relation one 1.5 > f / fn. According to another aspect of the present invention, the present invention provides an optical pickup including: an objective lens arranged to face the first and second media; a first light source arranged on a light path of the objective lens; A beam splitter arranged between the objective lens and the first light source; a second light source arranged on the light path of the light beam reflected from the beam splitter; a first phase detector for receiving from The laser beam emitted by the first light source and the laser beam reflected from the first medium; a second phase detector is used to receive the first light source (please read the precautions on the back before filling this page) · 11111111 1 ^ A7 A7 Printed by the Consumer Cooperatives of the Intellectual Property Bureau of the Ministry of Economic Affairs. 5. Description of the invention (& =: ΐ ΐ and the laser beam reflected from this second medium; and =-: r astigmatism astigmatism. The total focal length of the alignment lens is f Ϊ ^ The focal length is avoided, and the alignment lens conforms to the relationship, -bf / fn According to another aspect of the present invention, the present invention provides:-an objective lens, which is arranged facing the first 1st and 2nd media; 2nd 2nd skin is arranged at On the light path of the objective lens, it is used to emit a laser light = to the first optical disc; the first, second and third beam splitters, which: ^ by this brother-the light source is directed to the predetermined position of the objective lens On the path. — Twenty-two light sources, which are arranged on this first 丄: path, are used to emit a laser light. East longitude two =: = Diyi media; a first phase detector, which is arranged here. On the light path of the beam reflected by the third beam splitter, it is used to receive the laser beam reflected from the first light source and the laser beam reflected from the first medium; a second, measured as being arranged here On the optical path of the reflected light beam of the second beam splitter, 'for receiving the laser beam emitted from the second light source and the laser beam reflected from the two media; and-a decomposing lens, which is arranged on the objective lens and Between the third beam splitter, the alignment lens includes a astigmatism lens with a divergence ratio and a focusing lens with a focusing magnification, and the total focal length of the alignment lens at f is δ, and the astigmatism lens The focal length is 缶, and this alignment lens conforms to the relationship of 1.5 > f / fn. Description of the preferred embodiments of the present invention and with reference to the accompanying drawings, the above-mentioned objects and advantages of the present invention will become more apparent: This paper size applies the Zhongguan Standard (CNS) A4 specification ⑵Q χ as the public fn ϋ · I n I nn I «II ϋ I ϋ II II II ϋ n ϋ ϋ — ϋ ϋ n ϋ n ϋ ϋ nnn ϋ (Please read the precautions on the back before filling out this page) 476947 A7 、 Invention description (^) [Details of the invention] < Embodiment 1 > A first preferred embodiment of a kind of optical pickup according to the present invention is shown in Fig. 4. * The test si 4 'Q 4 is positioned directly opposite-the medium flat (light jujube) 1 〇〇 An optical lens at the end of the optical axis of 〇1. — Again, 4 glass plates 1 〇 07 ′-Beamsplitter! 〇2 和 —The alignment lens η is arranged on this objective lens! 〇 丄 and this light source 丄 〇 4. The alignment lens 103 includes a focusing lens i 0 3 a having a focusing magnification and a astigmatic lens 1 0 3 b having a diverging magnification. ', ... a phase detector 106 is arranged at the end of the light path of the light beam reflected from the beam splitter 10, and a focusing lens 105 is used to focus the reflected light beam, which is positioned Between the beam splitter 丄 02 and this phase splitter ^ 6. σ When the light source 104 emits laser light of 500 nm or less, the alignment lens has corresponding optical characteristics, which forms a special desire of the present invention. The total focal length of this alignment lens is 0.3, and the focal length of yyb is ". This alignment lens 103 conforms to -1-) > i / fn. ≪ Example 2 > The second embodiment of this kind of optical pickup is shown in the figure (Light Zen; two n light sources 104 are positioned coaxially to the facing-media (first industry) 1 () 〇-connecting the objective lens 101 Optical axis. Furnace 〇3, a λ / 4 glass-filled plate 〇7 and-Spectroscopy 9 through, see this between the objective lens 1 0 1 and the light source 104. The non-column is aligned with the lens 1 〇3 ( Please read the notes on the back before filling out this page}, ¾
訂---------線J 經濟部智慧財產局員工消費合作社印製 [紙張尺度適用中g家標準(CNS)A4 297公, L、發明說明(§ ) 聚焦透鏡1033及-具有發散倍 之«=^^2,”此分光器102所反射 此反射光束,1被集透鏡10 5用來聚集 6之間。/、被疋位在分光器10 2與此相偵測器1〇 田此光源1 〇 4發射-5GG nm或更短之•射弁走 =,此對準魏具有對朗光學雜,其ς明 ==準透鏡103的總焦距為f,及此J透 叙10 3 b的焦距為fn’此對準透鏡1〇3符合關係— 1.5>f/fn 〇 本實施例與第-實施例之間的差異在此對準透鏡的位 置上。在下列貫施例巾’光學結構的設計資料將被顯示。 前兩個實劇的對準透鏡可能具有與下列實施例的對準透 鏡相同之光學特性。 <實施例3 > 根據本發明的此種拾光器的一第三實施例被概略地顯 不在圖6中’且用於此ϋ 6的拾光器之光學資料被表列在 表格1中。 表格1 表面 曲率半徑 ~ ~——-- 厚度 玻璃名稱 物體表面 無限大 0.100000 si 無限大 6.250000 BK7 476947 Α7Β7 經濟部智慧財產局員工消費合作社印製 五、發明說明(7 ) s2 無限大 3.000000 s3 -15.219848 1.000000 FDS1 s4 5.866928 2.000000 TAC8 s5 -4.118685 5.000000 s6 STOP 1.770182 1.802215 BACD5 K:-0.721945 A:0.537259E-02 B:0.183575E-03 C:0.85500E-04 D:-.121341E-04 s7 -179.717593 1.272566 K:-179.717593 A:0.222258E-02 B:-.194835E-03 C:-.172951E-04 D:0.399488E-05 s8 無限大 0.600000 ,CG丨 s9 無限大 〇.〇〇〇〇〇〇 影像表面 無限大 〇.〇〇〇〇〇〇 球形表面的方程式(見在以下之方程式(2)) 折射率/在d線上之Abbe的數目,v BACD5:1.606048/61.3 FDS1:2.012371/20.9 TAC8:1.752798/54.7 BK7:1.530849/64.2 ’CG,:1.623343/31.0 進入孔的直徑(mm) 4.0 波長(nm) 400 (請先閱讀背面之注意事項再填寫本頁) · -—線. 本紙張尺度適用中國國家標準(CNS)A4規格(210 X 297公釐) 經濟部智慧財產局員工消費合作社印製 476947 A7 五、發明說明(β) 此對準透鏡的發散及聚焦元件的焦距 -4.085/3.517 (mm) 整個對準透鏡的焦距(mm) 10.0 接物鏡的焦距(mm) 2.677 Σ1/(/ϊ ·νί) -0.0004 在本實施例中,400 nm的一光源,一具有mm的 一焦距之對準透鏡,及一具有0.75的一口徑之接物鏡被使 用。在此拾光器中的像差被顯示在圖7中。 <實施例4 > 根據本發明的此種拾光器的一第四實施例被概略地顯 示在圖8中,且用於此圖8的拾光器之光學資料被表列在 表格2中。 表格2 表面 曲率半徑 厚度 玻璃名稱 物體表面 無限大 3.680296 si 無限大 6.250000 BK7 s2 無限大 3.000000 s3 -7.765552 1.000000 FDS1 s4 5.998733 2.000000 NBFD12 s5 -4.527848 5.000000. s6 1.770182 1.802215 BACD5 本紙張尺度適用中國國家標準(CNS)A4規格(210 X 297公釐) ,ϋ ϋ ϋ ·ϋ ϋ β-ϋ ·ϋ 口、I I I I ΜΜ I I ϋ ί n l_i Ban 1 -ϋ n ϋ I ϋ n ϋ n ϋ ϋ n- (請先閱讀背面之注意事項再本頁) 476947 A7B7 五、發明說明(丨丨) 經濟部智慧財產局員工消費合作社印製 STOP K>0.721945 A:0.537259E-02 B:0.183575E-03 C:0.85500E-04 D:-.121341E-04 s7 -11.452471 1.272566 K:-179.717593 Α:0·222258Ε-02 B:' D:0.399488E-05 • 194835E-03 C:'172951E-04 s8 無限大 0.600000 ’CG- s9 無限大 〇.〇〇〇〇〇〇 影像表面 無限大 〇.〇〇〇〇〇〇 球形表面的方程式(見在以下之方程式(2)) 折射率/在d線上之Abbe的數目,ν BACD5:1.606048/61.3 FDSl:2.012371/20.9 NAFD12:1.834057/42.3 BK7:1.530849/64.2 ^0^1.623343/31.0 進入孔的直徑(mm) 4.0 波長(nm) 400 對準透鏡的發散及聚焦元件的焦距 (mm) -3.225/3.386 整個對準透鏡的焦距(mm) 10.0 接物鏡的焦距(mm) 2.677 (請先閱讀背面之注意事項再填寫本頁) -%Order --------- Line J Printed by the Consumer Cooperatives of the Intellectual Property Bureau of the Ministry of Economic Affairs [Paper size applicable to Chinese Standard (CNS) A4 297, L, Description of Invention (§) Focusing lens 1033 and -has «= ^^ 2 of the divergence," the reflected light beam reflected by the beam splitter 102 is used by the collection lens 10 5 to collect between 6. /, is located in the beam splitter 10 2 and the phase detector 1 〇 田 This light source 1 〇4 emits -5GG nm or shorter. • Emissions =, this alignment Wei has a long optical hybrid, its brightness = = the total focal length of the quasi lens 103 is f, and this J through The focal length of 10 3 b is fn ', and this alignment lens 10 is in accordance with the relationship — 1.5> f / fn 〇 The difference between this embodiment and the first embodiment lies in the position of the alignment lens. The design information of the example 'optical structure will be displayed. The first two actual alignment lenses may have the same optical characteristics as the alignment lenses of the following embodiments. ≪ Example 3 > A third embodiment of the optical device is schematically shown in Fig. 6 'and the optical data of the optical pickup used for this unit 6 are listed in Table 1. Table 1 Surface curvature Diameter ~~ ——-- thickness glass name object surface infinite 0.100000 si infinite 6.200000 BK7 476947 Α7Β7 printed by the Consumer Cooperative of Intellectual Property Bureau of the Ministry of Economic Affairs 5. Description of invention (7) s2 infinite 3.000000 s3 -15.219848 1.000000 FDS1 s4 5.866928 2.000000 TAC8 s5 -4.118685 5.000000 s6 STOP 1.770182 1.802215 BACD5 K: -0.721945 A: 0.537259E-02 B: 0.183575E-03 C: 0.85500E-04 D:-. 121341E-04 s7 -179.717593 1.272566 K: -179.717593 A: 0.222258E-02 B:-. 194835E-03 C:-. 172951E-04 D: 0.399488E-05 s8 infinite 0.600000, CG 丨 s9 infinite 0.00. The image surface is infinite 0.00. 〇〇〇〇 The equation of the spherical surface (see the following equation (2)) Refractive index / the number of Abbe on the d line, v BACD5: 1.606048 / 61.3 FDS1: 2.012371 / 20.9 TAC8: 1.752798 / 54.7 BK7: 1.530849 / 64.2 'CG ,: 1.623343 / 31.0 The diameter of the entrance hole (mm) 4.0 Wavelength (nm) 400 (Please read the precautions on the back before filling this page) ·-Line. This paper size applies to China National Standard (CNS) A4 specifications (210 X 297 mm) Printed by the Employees ’Cooperative of the Ministry of Economic Affairs and Intellectual Property of the Ministry of Economic Affairs 476947 A7 V. Description of the invention (β) The divergence of this alignment lens and the focal length of the focusing element-4.085 / 3.517 (mm) The focal length of the entire alignment lens (mm) 10.0 Focal length (mm) 2.677 Σ1 / (/ ϊ · νί) -0.0004 In this embodiment, a light source of 400 nm, an alignment lens with a focal length of mm, and an objective lens with a diameter of 0.75 are used . The aberrations in this pickup are shown in FIG. 7. < Embodiment 4 > A fourth embodiment of such an optical pickup according to the present invention is schematically shown in FIG. 8, and optical data for the optical pickup of this FIG. 8 are listed in Table 2 in. Table 2 Surface Curvature Radius Thickness Glass Name Object Surface Infinite 3.680296 si Infinite 6.250000 BK7 s2 Infinite 3.000000 s3 -7.765552 1.000000 FDS1 s4 5.998733 2.000000 NBFD12 s5 -4.527848 5.000000. S6 1.770182 1.802215 BACD5 This paper is in accordance with Chinese national standards (CNS) A4 size (210 X 297 mm), ϋ ϋ ϋ · ϋ ϋ β-ϋ · ϋ 口, IIII ΜΜ II ϋ ί n l_i Ban 1 -ϋ n ϋ I ϋ n ϋ n ϋ ϋ n- (Please read the back first (Notes on this page) 476947 A7B7 V. Description of the invention (丨 丨) Printed by the Consumer Cooperative of the Intellectual Property Bureau of the Ministry of Economic Affairs STOP K > 0.721945 A: 0.537259E-02 B: 0.183575E-03 C: 0.85500E-04 D :-. 121341E-04 s7 -11.452471 1.272566 K: -179.717593 Α: 0 · 222258E-02 B: 'D: 0.399488E-05 • 194835E-03 C:' 172951E-04 s8 infinite 0.600000 'CG- s9 infinite 〇〇〇〇〇〇〇〇 Infinite image surface 0.0000 Sphere equation (see equation (2) below) Refractive index / Number of Abbe on the d line, ν BACD5: 1.606048 / 61.3 FDSl: 2.012371 / 20.9 NAFD12: 1.834057 / 42.3 BK7: 1.530849 / 64.2 ^ 0 ^ 1.623343 / 31.0 diameter of the entrance hole (mm) 4.0 wavelength (nm) 400 divergence of the alignment lens and focal length of the focusing element (mm) -3.225 / 3.386 entire alignment lens Focal length (mm) 10.0 Focal length (mm) of the objective lens 2.677 (Please read the precautions on the back before filling this page)-%
訂---------線J 本紙張尺度適用中國國家標準(CNS)A4規格(210 X 297公釐) 476947 經濟部智慧財產局員工消費合作社印製 A7 B7 五、發明說明(θ)Order --------- Line J This paper size is applicable to China National Standard (CNS) A4 specification (210 X 297 mm) 476947 Printed by A7 B7, Consumer Cooperative of Intellectual Property Bureau of the Ministry of Economic Affairs 5. Description of the invention (θ )
Zl/(fi*v〇 -0.0017 在本實施例中,400 nm的一光源,一具有15 mm的 一焦距之對準透鏡,及一具有0.75的一口徑之接物鏡被使 用。在此拾光器中的像差被顯示在圖9中。 <實施例5> 根據本發明的此種拾光器的一第五實施例被概略地顯 示在圖10中,且用於此圖10的拾光器之光學資料被表 列在表格3中。 表格3 表面 曲率半徑 厚度 玻璃名稱 物體表面 無限大 13.381632 si 無限大 6.250000 BK7 s2 無限大 3.000000 s3 21.6695568 2.000000 BACD5 s4 -7.653445 1.000000 s5 -36.568237 1.000000 FD4 s6 3.690184 2.000000 BACD5 s7 -49.729832 5.000000 s8 STOP 1.770182 1.802215 BACD5 K>0.721945 A:0.537259E-02 B:0.183575E-03 C:0.85500E-04 D:-.121341E-04 s9 -11.452471 1.272566 本紙張尺度適用中國國家標準(CNS)A4規格(210 X 297公釐) --------訂--------I I (請先閱讀背面之注意事項再填寫本頁) 476947 A7 B7 發明說明(/3) 經濟部智慧財產局員工消費合作社印製 K:-179.717593 A:0.222258E-02 B:-. D:0.399488E-05 194835E-03 C:-.172951E-04 slO 無限大 0.600000 ’CG1 s9 無限大 〇.〇〇〇〇〇〇 影像表面 無限大 〇.〇〇〇〇〇〇 球形表面的方程式(見在以下之方程式(2)) 折射率/在d線上之Abbe的數目,v BACD5:1.606048/61.3 FD4:1.808613/27.5 BK7:1.530849/64.2 ,CG’:1.623343/31.0 進入孔的直徑(mm) 4.0 波長(nm) 400 對準透鏡的發散及聚焦元件的焦距 (mm) 9.579/-4.100/5.750 整個對準透鏡的焦距(mrn) 20.0 接物鏡的焦距(mm) 2.677 ΣΙ/Qi >/) 0.0018 一焦距之對準透鏡,及一具有〇·75的一口徑之接物鏡被使 用。在此拾光器中的像差被顯示在圖1 1中。一球形表面的方程式,其先前在表格1到表格3中祐 本紙張尺度適用中國國家標準(CNS)A4規格(210 X 297公爱) (請先閱讀背面之注意事項再填寫本頁) % 訂---------線 476947 A7 發明說明(丨^) 提及’藉由方程式(2)而被表示 Ch2 經濟部智慧財產局員工消費合作社印製 zsTrT^^r'Ah'+BhSChS+Dh^El^+Fh14·..··(2) ,其中z為從此表面算㈣深度’ h為從此光軸算起的距 離’c為曲率,k為一圓錐曲線參數,及A,b,c及 球形曲線參數。 、對於貫施例3 ’ 4及5,因為從此光源所發射之光束 的波長在± 1〇職的誤差範圍之内,此散焦的角度可被表 不成在焦點深度方面之± 〇.36 _的不確定性。 圖12描述使用-傳統對準透鏡之—拾光器的光路 徑’及圖13描述在圖12的此傳統拾光器中的像差。相 對地’圖14描述使用根據本發明的一對準透鏡之一拾光 器的光路徑,及圖i 5描述在圖工4的此拾光器中的像σ差。 如同在圖12及圖13中所示,因為此傳統對準 被設計成使其可適用於500腿或更長的一波長’碎散 倍率不足以更正具有比500 nm更短之一波長的光束利 =色像差。對於圖i 2的拾光器,每—透鏡的焦距各別 地為-^秦㈣及綱,此Abbe的數目各別地 為 43.0 53.9 及 62.3,且2 1/(/丨”丨)=〇 〇〇67。如同在 圖1 3中所示’400 nm光束的像差對於此拾光器是可以,勿、 略的’但是對於405 nm’此像差的角度突然地增加。因此, 此傳統對準透鏡無法被使用於短波長光束。 ’ 同時,如同在圖1 4及圖1 5中所示,在400 nm與 405 nm發射光束之間,像差之角度的變化較小。因為根據 Μ氏張尺度適用中國國家標準(CNS)A4規格(210 X 297公爱 (請先閱讀背面之注意事項再填寫本頁) -------訂---------線| •ΓZl / (fi * v0-0.0017 In this embodiment, a light source at 400 nm, an alignment lens with a focal length of 15 mm, and an objective lens with a diameter of 0.75 are used. The light is picked up here The aberrations in the filter are shown in Fig. 9. < Embodiment 5 > A fifth embodiment of such an optical pickup according to the present invention is schematically shown in Fig. 10 and is used for the pickup of Fig. 10. The optical data of the optical device are listed in Table 3. Table 3 Surface curvature radius thickness Glass name Object surface infinite 13.381632 si infinite 6.200000 BK7 s2 infinite 3.000000 s3 21.6695568 2.000000 BACD5 s4 -7.653445 1.000000 s5 -36.568237 1.000000 FD4 s6 3.690184 2.000000 BACD5 s7 -49.729832 5.000000 s8 STOP 1.770182 1.802215 BACD5 K > 0.721945 A: 0.537259E-02 B: 0.183575E-03 C: 0.85500E-04 D:-. 121341E-04 s9 -11.452471 1.272566 This paper is applicable to Chinese national standards (CNS) A4 specification (210 X 297 mm) -------- Order -------- II (Please read the precautions on the back before filling this page) 476947 A7 B7 Invention Description (/ 3) Employees of Intellectual Property Bureau, Ministry of Economic Affairs Printed by Fei Cooperative K: -179.717593 A: 0.222258E-02 B:-. D: 0.399488E-05 194835E-03 C:-. 172951E-04 slO Infinity 0.600000 'CG1 s9 Infinity 0.000.00.00 〇The image surface is infinitely large. The equation of the spherical surface (see equation (2) below) Refractive index / the number of Abbe on the d line, v BACD5: 1.606048 / 61.3 FD4: 1.808613 / 27.5 BK7 : 1.530849 / 64.2, CG ': 1.623343 / 31.0 diameter of the entrance hole (mm) 4.0 wavelength (nm) 400 divergence of the alignment lens and focal length of the focusing element (mm) 9.579 / -4.100 / 5.750 focal length of the entire alignment lens ( mrn) 20.0 Focal length of the objective lens (mm) 2.677 ΣΙ / Qi > /) 0.0018 An alignment lens with a focal length and an objective lens with a diameter of 0.75 are used. The aberrations in this pickup are shown in FIG. 11. An equation for a spherical surface, which was previously used in Forms 1 to 3. The paper size applies the Chinese National Standard (CNS) A4 (210 X 297 public love) (Please read the precautions on the back before filling this page).% Order --------- Line 476947 A7 Description of Invention (丨 ^) Mention 'Ch2 is printed by equation (2) Ch2 Printed by the Consumers ’Cooperative of the Intellectual Property Bureau of the Ministry of Economic Affairs ^^ r'Ah' + BhSChS + Dh ^ El ^ + Fh14 ····· (2), where z is the depth from the surface, h is the distance from the optical axis, c is the curvature, k is a conic curve parameter, and A, b , C and spherical curve parameters. For the implementation examples 3'4 and 5, because the wavelength of the light beam emitted from this light source is within the error range of ± 10 °, this defocus angle can be expressed as ± 0.36 in the depth of focus. Uncertainty. FIG. 12 illustrates the optical path 'of an optical pickup using a conventional alignment lens and FIG. 13 illustrates aberrations in this conventional optical pickup of FIG. Relative to the ground 'FIG. 14 depicts the light path using an optical pickup of one of the alignment lenses according to the present invention, and FIG. 5 depicts the aberration σ in this optical pickup of FIG. 4. As shown in Figures 12 and 13, because this traditional alignment is designed to make it suitable for a wavelength of 500 legs or longer, the fragmentation magnification is not sufficient to correct a beam with a wavelength shorter than 500 nm Profit = chromatic aberration. For the optical pickup of Fig. I 2, the focal length of each lens is-^ Qin Wei and Gang, respectively, and the number of Abbe is 43.0 53.9 and 62.3, respectively, and 2 1 / (/ 丨 "丨) = 〇 〇〇67. As shown in Figure 13 '400 nm beam aberration is possible for this pickup, please, slightly' but for 405 nm 'the angle of this aberration suddenly increases. Therefore, this tradition Alignment lenses cannot be used for short-wavelength beams. 'At the same time, as shown in Figures 14 and 15, the change in the angle of aberration is smaller between 400 nm and 405 nm emission beams. The Zhang scale is applicable to China National Standard (CNS) A4 specifications (210 X 297 public love (please read the precautions on the back before filling this page) ------- Order --------- Line | • Γ
(請先閱讀背面之注意事項再填寫本頁) 訂---------線J 經濟部智慧財產局員工消費合作社印製 47⑽4/ A7 -------------------- 五、發明說明(丨/) 本么明的對準透鏡具有高聚焦倍率,像差可被有效地更 正。結果,一光點可被以在對應到此發射光束之波長的變 化之-焦點深度的範圍内,被聚焦在此媒體上。 對於有關於如此短波長光束方面之色像差的有效降 低假4此整個對準透鏡的焦距為f且此散光透鏡的焦距 為fn,此對準透鏡符合關係—15>f/fn是必須的。 、較佳地,假設透鏡組(其構成此拾光器)的前焦距, 為f 1 f2 ··,及fn,其被從此光源朝向此媒體排列,且 對於此透鏡組之光學物f的d _線上之A b b e數目為 v:l ’ v2 ’ ···,及vn,此拾光器符合關係—〇 〇〇5<i/(fi · vl)+ 1/(Ω · v2)+ …+ 1/(fn · vn)<〇 〇〇〇5。 -種使用兩個光社拾光H,將在下列實施例中被描 述。 <實施例6 > . 芩考圖1 6,一第一光源1 〇 4 a被定位在一接物鏡 10 1 (其正對-媒體1 Q 〇)之光軸的端點上。用來控 制此接物鏡1 〇 1的口徑之一波長選擇過渡器3 〇 〇,— 對準透叙1 0 3 (其為本發明的一特徵),及一分光器1 〇 2被排列在此接物鏡χ 〇丄與此第一光源丄〇4a之間。 此分光器1〇 2傳輸從此第-光源工〇 4 3所發射之 雷射光束,且反射從-第二光源丄〇 4 W發射之雷射光 束。如同在圖1 6中所示,此第二光源工〇 4 b被排列在 從此分光為1 〇 2所反射之光束的光路徑上。 此波長選擇過遽器3 0 〇的使用是任意的。換句話 本紙張尺度適用中國國家標準(CNS)A4規格(210 X 297公复) 476947 A7 B7 五、發明說明(K ) ,,此波長選擇過絲、3 〇 〇在#存在對於相控制 第一及第一光源1 〇 4 a及1 〇 4b之口徑的一需长日士; 被合併到此拾光器。舉例而言,如果此第一光源1 〇| 發射一 400 nm藍光雷射及需要一 〇·7的口徑,且此第一、a 源1 0 4 b發射一 650 nm紅光雷射及需要一 〇6的口/一光 此波長選擇賴器3 0 Q被使用來在當傳輸所有的= nm雷射光束時,允許接物鏡的口徑降低到用於咖聰帝 射光束之0.6。 田 一傳統光束發射/偵測裝置,其包括一像偵測器及— 田射'極體,可能被用來當成第-及第二光源工〇 4 3及 1 〇4b,因此-雷射光束可被相同的裝置發射及接收。 所扩Πί叙10 3 ’其形成本發明的一個特徵如先前 =田述’包括—具有聚焦倍率之聚焦透鏡1 0 3 a及-罝 =散倍率之散光透鏡i 〇 3 b。假設此整個對準透鏡工 準透此散光透鏡1 ◦ 3 b的焦距為出,此對 及弟一先源1 〇 4 a及1 0 4 b傳來之雷射光 束,且同步地助其更正色像差。 <實施例7 > 1 ο 1 7 ’ 一第一光源1 0 4 a被定位在一接物鏡 制此i上正對—媒體1。Q)之光軸的端點上。用來控 竟101的口徑之-波長選細器300, - 第一八2 03 (其為本發明的—特徵)’及第-,第二及 弟二刀先器102a,1〇2m1〇2c被排列在此接 ^ 紙張尺 --------^--------- (請先閱讀背面之注意事項再填寫本頁} 濟 部 智 慧 財 產 局 員 工 消 費 合 作 社 印 製 476947 A7 _ B7 五、發明說明(丨p 物鏡1 0 1與此第一光源1 0 4 a之間的預定位置上。 此第三分光器1 0 2 c傳輸從此第一光源1 〇 4 a來 的雷射光束’及將從一第一光源1 Q 4 b來的雷射光束反 射向此媒體100。如同在圖17中所示,此第二光源1 0 4 b被排列在從此第三分光器1 〇 2 c所反射之光束的 光路徑上。 此第二分光器1 0 2 b傳輸從此第一及第二光源丄〇 4a及l〇4b來的雷射光束,且反射從此媒體反射之光 束,其係從此第二光源1 〇 4 b所起源。被此媒體1 〇 〇 所反射且被此第二分光器1 〇 2 b轉向之光束,被一第二 聚集透鏡8 0 2聚集到一第二相偵測器7 〇 2上。 此第一分光器1〇 2 a將從此第一及第二光〇 4 a及1 〇4b來的雷射光束傳向此媒體丄〇〇。相同地, 此第一分器1 0 2 a反射從此媒體X 〇 〇反射之光束,其 係從此第一光源1 〇 4 a所起源,且傳輸從此媒體1 〇◦ 反射之光束,其係從此第二光源i 〇4b所起源。被此媒 體1 0 0所反射且被此第一分光器i 〇 2 a轉向之光束, 被一第一?κ集透鏡8 0 1聚集到一第一相债測器6 〇 2 上。 、’ 此波長選擇過濾器3 〇 〇的使用是任意的。換句話 說,此波長選擇過濾器3 〇 〇當其存在對於分開控制用於 第一及第二光源1 〇 4 a及1 0 4 b之口徑的一需求時, 被合併到此拾光器。舉例而言,如果此第一光 發射一 雷射及需要一 〇.7的口 = = ^ I ·ϋ n n I n ϋ 一· MM w W W _ I - (請先閱讀背面之注意事項再填寫本頁) -(Please read the precautions on the back before filling this page) Order --------- Line J Printed by the Consumer Cooperatives of the Intellectual Property Bureau of the Ministry of Economic Affairs 47⑽4 / A7 ------------ -------- V. Explanation of the invention (丨 /) The alignment lens of this Meming has a high focusing magnification, and the aberration can be effectively corrected. As a result, a light spot can be focused on the medium within a range corresponding to the change in the wavelength of the emitted light beam-the depth of focus. For the effective reduction of chromatic aberrations in such short-wavelength beams, the focal length of the entire alignment lens is f and the focal length of this astigmatic lens is fn. This alignment lens conforms to the relationship—15> f / fn is necessary . Preferably, it is assumed that the front focal length of the lens group (which constitutes the optical pickup) is f 1 f2 ··, and fn, which are arranged from the light source toward the medium, and d for the optical object f of the lens group _ The number of A bbe on the line is v: l 'v2' ···, and vn. This pickup conforms to the relationship—〇〇〇5 < i / (fi · vl) + 1 / (Ω · v2) +… + 1 / (fn · vn) < 0.00005. A light pickup H using two optical companies will be described in the following examples. < Embodiment 6 > Considering FIG. 16, a first light source 10a is positioned at the end of the optical axis of an objective lens 101 (which is directly opposite to the medium 1Qo). One of the apertures used to control the objective lens 101 is a wavelength-selective transition device 300, which is aligned with the lens 103 (which is a feature of the present invention), and a beam splitter 100 is arranged here. The objective lens χ 〇 丄 and this first light source 丄 04a. This beam splitter 102 transmits the laser beam emitted from the first light source 403, and reflects the laser beam emitted from the second light source 〇4 W. As shown in FIG. 16, the second light source module 0 4 b is arranged on the light path of the light beam reflected from this split to 102. The use of this wavelength selection filter 300 is arbitrary. In other words, this paper size applies the Chinese National Standard (CNS) A4 specification (210 X 297 public copy) 476947 A7 B7 V. Description of the invention (K), this wavelength is selected over the wire, 3 〇〇 在 # exists for phase control No. One and the first light source 1 04a and 1 104b caliber need a long day; are incorporated into this optical pickup. For example, if the first light source 1 〇 | emits a 400 nm blue laser and requires a caliber of 10.7, and the first and a source 1 0 4 b emits a 650 nm red laser and requires one 〇6 口 / 一 光 This wavelength selection device 3 0 Q is used to allow the aperture of the objective lens to be reduced to 0.6 for the Congdi laser beam when transmitting all = nm laser beams. Tian Yi's traditional beam emission / detection device, which includes an image detector and-Tian She 'polar body, may be used as the first and second light source workers 043 and 104b, so-laser beam Can be transmitted and received by the same device. The expanded 10 3 ′, which forms a feature of the present invention, is as described previously. The field lens includes a focusing lens 1 0 3 a and a astigmatic lens i 0 3 b with astigmatic magnification. Assume that the entire alignment lens is transmitted through the astigmatic lens 1 ◦ 3 b. The focal length of the astigmatism lens 1 is 3, and the pair of laser beams from the first source 10 4 a and 10 4 b will be synchronized to help correct it. Chromatic aberration. < Embodiment 7 > 1 ο 1 7 ′ A first light source 1 0 4 a is positioned on an objective lens so as to face i—media 1. Q) at the end of the optical axis. Wavelength selector 300 used to control the aperture of 101,-the first eight 2 03 (which is a feature of the present invention) and the second, second and second two-knife precursors 102a, 102m1〇2c Arranged here ^ Paper rule -------- ^ --------- (Please read the precautions on the back before filling out this page} Printed by the Employee Consumer Cooperative of the Ministry of Economic Affairs and Intellectual Property of the Ministry of Education 476947 A7 _ B7 V. Description of the invention (p) The objective lens 1 0 1 and the first light source 1 0 4 a are at a predetermined position. The third beam splitter 1 0 2 c transmits the light from the first light source 1 0 4 a. The laser beam 'and the laser beam from a first light source 1 Q 4 b are reflected toward the medium 100. As shown in FIG. 17, the second light source 1 0 4 b is arranged at the third beam splitter 1 〇2 c on the optical path of the light beam reflected. The second beam splitter 10 2 b transmits the laser light beams from the first and second light sources 丄 04a and 104b, and reflects the light beam reflected from the medium. , Which originates from this second light source 104b. The light beam reflected by this medium 1000 and steered by this second beam splitter 102b is directed by a second focusing lens 8202 Set to a second phase detector 7 〇. The first beam splitter 10 2 a transmits the laser beams from the first and second light 04 a and 104 b to the medium 丄 〇〇 Similarly, the first splitter 10 2 a reflects the light beam reflected from the medium X 〇〇, which originates from the first light source 104 A, and transmits the light beam reflected from the medium 1 0. The origin of the second light source i 〇4b. The light beam reflected by this medium 100 and turned by this first beam splitter i 〇2 a is collected by a first? Κ set lens 801 to a first phase debt The use of this wavelength selection filter 3 is optional. In other words, this wavelength selection filter 3 is used for the first and second light sources 1 for separate control. 〇4 a and 10 4 b are required to be incorporated into the optical pickup when required. For example, if the first light emits a laser and requires a port of 0.7 = = ^ I · ϋ nn I n ϋ I · MM w WW _ I-(Please read the notes on the back before filling this page)-
A7 五、發明說明() 源1 0 4 b發射一 650nm紅光雷射及需要一 〇.6 口句, 過滤器3 0 0被使用來當傳輸所有的400請 田射先束守,允許接物鏡的口徑降低到用於65〇 光束之0.6。 、 nm μ射 所二對t透鏡10 3 ’其形成本發明的-個特徵如先前 斤心处’包括—具有聚焦倍率之聚焦透鏡丨◦ =散倍率之散光透鏡丄〇 3 b。假設此整個對準透鏡: 〇 3的焦距為f’且此散光透鏡丄Q 3 對準透鏡1 〇 3符八關# 1 '、、、巨為fn ’此 ?健二 /fn。此對準透鏡1 〇 m弟一及第二光源i 〇 4 a及丄〇 4 b傳來之雷射 光束’且同步地助其更正色像差。 訂 <實施例8 > 線 -ιοΠ】18丄一第一光源104a被定位在-接物鏡 G、正對—媒體1 Q Q)之光軸的端點上。用來抑 ,接物鏡! 〇工的口徑之一波長選擇過濾器3 〇 〇,: 弟-,第二及第三分光器102a,1〇2b及i〇2c 被排列在此接物鏡i 0 i與此第一光源工〇 4 3之間的預 ^置上。相同地’-對準透鏡i Q 3 (其為本發明的」 特徵),被定位在此第一及第二分光器 之間。 此第二分光器1〇 2 C傳輸從此第—光源工〇 4 a來 的雷射光束’及將從-第二光源i 〇 4 b來的雷射光束反 射向此媒體10 0。如同在圖i 8中所示,此第二光源丄 〇 4 b被排列在從此第三分光器丄〇 2 c所反射之光束的 本紙張尺度適用中國國家標準(CNS)A4規格(21G X 297公复― 476947 經濟部智慧財產局員工消費合作社印製 A7 B7 五、發明說明(丨Ο 光路徑上。 此第二分光器102b傳輸從此第一及第二光源工〇 4 a及1 0 4b來的所有雷射光束,且反射從此媒體反射 之光束,其係從此第二光源i 04b所起源。被此媒體工 〇 0所反射且被此第一分光器1 〇 2 b轉向之光束被一第 二聚集透鏡8 0 2聚集到一第二相偵測器7 〇 2上。 此第一分光器1 0 2 a將從此第一及第二光源丄〇4 a及104b來的所有雷射光束傳向此媒體1 〇 〇。相同 地,此第一分器1 0 2 a反射從此媒體i 〇 〇反射之光 束,其係從此第二光源1 〇 4 a所起源,且傳輸從此媒體 1 0 0反射之光束,其係從此第二光源i 〇 4㈣起源。 被此媒體1 0 0所反射且被此第一分光器1〇 2 a轉向之 光束被一第一聚集透鏡8 〇1聚集到一第—相偵測〇 2 ° - 此波長選擇過濾器3 Q 0的使収任意的。 說’此波長選擇過瀘、器3 〇 0當其存在對於分開控制用於 第一及第二光源1 0“及1 〇4b之口徑的_需求日士,、 被合併到此拾光器。舉例而言,如果此第—光源 : 發射一 40〇nm藍光雷射及需要一 〇7的口徑,=此μ 一 = 源1 0 4 b發射一 050 nm紅光雷射及需要— 弟—光 . 乂 的口 和·, 此波長選擇過濾器3〇〇被使用來在傳輪所有的二 雷射光束時,允許接物鏡的口徑降低到 nm 光束之0.6。 · 以5〇聰雷射 此對準透鏡103,其形成本發明的一個特徵如先前 I紙張尺度適用中國國家標準(CNS)A4規格⑵Q χ 297公爱「 --------訂---------線» (請先閱讀背面之注意事項再填寫本頁) 476947 經濟部智慧財產局員工消費合作社印製 A7 --------BL________ 五、發明說明0 ) 所描述’包括一具有聚焦倍率之聚焦透鏡1 Ο 3 a及一具 有發散倍率之散光透鏡1 〇 3 b。假設此整個對準透鏡1 〇 3的焦距為f ’且此散光透鏡1 〇 3 b的焦距為fn,此 對準透鏡1 〇 3符合關係一 1.5>f/fn。此對準透鏡1 〇 3對準從第一及第二光源i〇4a及i〇4b傳來之雷射 光束,且同步地助其更正色像差。 <實施例9 > 芩考圖1 9,一第一光源1 〇 4 a被定位在一接物鏡 101 (其正對一媒體10 0)之光軸的端點上。用來控 制此接物鏡1〇1的口徑之一波長選擇過濾器3 0 0,及 第一,第二及第三分光器,1〇2上及1〇2^ 被排列在此接物鏡1 〇 1與此第一光源1 〇 4 a之間的預 定位置上。相同地,一對準透鏡丄〇 3 (其為本發明的一 特徵),被定位在此第二及第三分光器丄〇21^及1 〇2 C 之間。 此第二分光器1 0 2 C傳輸從此第一光源1〇 4 a來 的雷射光束,及將從-第二光源丄〇 4]3來的雷射光束反 射向此媒體100。如同在圖19中所示,此第二光源丄 04b被排列在從此第三分光器1〇2c所反射之光束的 光路徑上。 此第二分光器1〇 2 b傳輸從此第一及第二光源工〇 4 a及1〇 4 b來的所有雷射光束,且反射從此媒體反射 之光束’其係從此第二光源丄〇4b所起源。被此媒體丄 0 0所反射且被此第二分光器丄〇 2 b轉向之光束,被一 本紙張尺度適用中國國家標準(CNS)A4規格(210 X 297公爱)----- ^---------^ 1^ (請先閱讀背面之注意事項再填寫本頁) H ϋ ϋ ϋ 476947 經濟部智慧財產局員工消費合作社印製 A7 五、發明說明(>\) 第二聚集透鏡8 〇 2聚集到一第二相偵測器7 0 2上。 此第一分光器1 〇 2 a將從此第一及第二光源1 〇 4 a及104b來的所有雷射光束傳向此媒體1 〇 〇。相同 地,此第一分器1 〇 2 a反射從此媒體1 〇 〇反射之光 束’其係從此第二光源1 〇 4 a所起源,且傳輸從此媒體 1 0 0反射之光束,其係從此第二光源1 〇 4 b所起源。 被此媒體1 0 〇所反射且被此第一分光器^ 〇 2 a轉向之 光束,被一第一聚集透鏡8 〇丄聚集到一第一相偵測器6 0 2上。 此波長選擇過濾器3 〇 0的使用是任意的。換句話 ,,此,長選擇過濾器3 〇 〇當其存在對於分開控制用於 第一及第二光源1 0 4 3及1 〇 4 b之口徑的一需求時, 被合併到此拾光器。舉例而言,如果此第一光源丄〇 4 a 發射一 4〇〇nm藍光雷射及需要一 〇·7的口徑,且'此第二光 源1 0 4b發射一 650 nm紅光雷射及需要一 〇·6的口押, 此波長選擇過遽器3 〇〇被使用來在傳輪所有的 =光束時,允許接物鏡的口徑降低到用於 光束之0.6。 ^ nm田射 此對準透鏡1〇 3,其形成本發明的 所描述,包括一具有聚焦倍率之聚焦透鏡i 所 有發散倍率之散光透鏡1 (3 3 b。麟轉1具 〇 3的焦距為f,且此散光透鏡】〇 3 b的 广兄1 對準透鏡i〇3^_—15〉f/fnm4fm (請先閱讀背面之注意事項再填寫本頁) --線· 3對準從第-及第二光源1043及1〇4=== _ 尺度適用 297 公髮丁 476947 經濟部智慧財產局員工消費合作社印製 A7 B7_ 五、發明說明(>>) 光束,且同步地助其更正色像差。 〈實施例10 > 根據本發明之此拾光器的一第十實施例被概略地顯示 在圖20及圖22中,且用於圖20及圖2 2之拾光器的 光學資料被表列在表格4中。 表格4 表面 曲率半徑 厚度 玻璃名稱 物體表面 無限大 0.100000 si 無限大 0.250000 BK7 s2 無限大 5.929508z 2.122789z s3 無限大 6.000000 BK71 s4 無限大 3.000000 s5 -4.081133 1.000000 FDS1 s6 30.164147 2.000000 BACD5 s7 -3.467121 5.000000 K:-0.2007701 Α:0.445555Ε-03 Β:-0.119205Ε-03 C:0.316310Ε-04 D:-.267022E-05 s8 STOP 1.770182 1.802215 BACD5 K:-0.721945 A:0.537259E-02 B:0.183575E-03 C:0.855000E-04 D:-.121341E-04 本紙張尺度適用中國國家標準(CNS)A4規格(210 X 297公釐) (請先閱讀背面之注意事項再填寫本頁)A7 V. Explanation of the invention () Source 1 0 4 b emits a 650nm red laser and requires a sentence of 10.6. The filter 3 0 0 is used to transmit all 400, please be protected by Tian She, allowing access. The aperture of the objective lens is reduced to 0.6 for a 65 ° beam. The two pairs of t-lenses 10 3 ′, which form a characteristic of the present invention, include the focusing lens with focus magnification, and the astigmatism lens with astigmatism 丄 03b. Assume that the entire alignment lens: θ 3 has a focal length of f ′ and this astigmatism lens 丄 Q 3 is aligned with the lens 1 〇 3 符 八 关 # 1 ′,,, and is fn ′, which is Kenji / fn. The laser beams ′ from the first and second light sources i 〇 4 a and 丄 〇 4 b of the alignment lens 100 m and synchronously help them correct chromatic aberration. ≪ Example 8 > Line-ιοΠ] 18: A first light source 104a is positioned at the end of the optical axis of the objective lens G, facing the media 1QQ). Used to suppress the objective lens! The wavelength selection filter 3, which is one of the apertures, is: the second, third, and third beam splitters 102a, 102b, and 〇2c are arranged on the objective lens i 0 i and the first light source. Pre-placement between 4 and 3. Similarly, the '-alignment lens i Q 3 (which is a "feature" of the present invention) is positioned between the first and second beam splitters. The second beam splitter 10 2C transmits a laser beam ' from the first light source worker 04a and a laser beam from the second light source i 04b to the medium 100. As shown in Fig. I 8, this second light source 丄 〇4 b is arranged on the light beam reflected from the third beam splitter 丄 02 c. The paper size of this paper applies the Chinese National Standard (CNS) A4 specification (21G X 297). Public reply-476947 Printed by A7 B7, Consumer Cooperative of Intellectual Property Bureau of the Ministry of Economic Affairs 5. Description of the invention (On the light path. The second beam splitter 102b transmits the light from the first and second light source workers 04a and 104b. All the laser beams reflected by this medium originate from this second light source i 04b. The light beam reflected by this media worker 00 and steered by this first beam splitter 1 02b is first The two focusing lenses 8 0 2 are focused on a second phase detector 7 0 2. The first beam splitter 1 0 2 a transmits all the laser beams from the first and second light sources 10 4 a and 104 b. To the medium 100. Similarly, the first splitter 10 2a reflects the light beam reflected from the medium i 00, which originates from the second light source 104, and the transmission is reflected from the medium 100 The light beam originates from this second light source i 04. It is reflected by the medium 100 The light beam turned by this first beam splitter 10 2 a is focused by a first focusing lens 8 0 1 to a first phase detection 0 2 °-the selection of this wavelength selection filter 3 Q 0 is arbitrary. Say ' This wavelength selection filter, 300, is incorporated into this pickup when it exists for separately controlling the apertures of the first and second light sources 10 "and 104b, which are required by Japan. For example, In other words, if this first-light source: emits a 40nm blue laser and requires a caliber of 107, = this μ a = source 1 0 4 b emits a 050 nm red laser and needs-brother-light. 乂The wavelength selection filter 300 is used to allow the aperture of the objective lens to be reduced to 0.6 nm when all the two laser beams of the transmission wheel are passed. 103, which forms a feature of the present invention, such as the previous I paper size applicable to the Chinese National Standard (CNS) A4 specification ⑵Q χ 297 public love "-------- order --------- line» ( (Please read the precautions on the back before filling this page) 476947 Printed by the Consumer Cooperatives of the Intellectual Property Bureau of the Ministry of Economic Affairs A7 -------- BL________ V. Invention Description 0 ) The description 'includes a focusing lens 1 0 3 a with focusing magnification and a astigmatic lens 1 0 3 b with diverging magnification. It is assumed that the focal length of the entire alignment lens 1 0 3 is f' and this astigmatic lens 1 〇 3 The focal length of b is fn, and this alignment lens 1 03 conforms to the relationship 1.5 > f / fn. This alignment lens 1 03 is aimed at the thunder from the first and second light sources i04a and i04b. The light beam is emitted and synchronously helps it correct chromatic aberration. < Embodiment 9 > Consider Fig. 19, a first light source 104a is positioned at the end of the optical axis of an objective lens 101 (which is directly opposite a medium 100). One wavelength selection filter 300, which is used to control the aperture of the objective lens 101, and the first, second, and third beam splitters, 102 and 102 are arranged on the objective lens 10. 1 at a predetermined position between this and the first light source 104a. Similarly, an alignment lens 丄 03 (which is a feature of the present invention) is positioned between the second and third beam splitters 丄 2121 and 〇2 C. The second beam splitter 10 2C transmits a laser beam from the first light source 104a, and reflects the laser beam from the second light source 104a toward the medium 100. As shown in Fig. 19, the second light source 丄 04b is arranged on the light path of the light beam reflected from the third beam splitter 102c. The second beam splitter 10b transmits all the laser beams from the first and second light sources 0a and 104b, and reflects the light beams reflected from the medium, which is from the second light source 0b. The origin. The light beam reflected by this media 丄 0 0 and steered by this second beam splitter 丄 〇2 b is adapted to a Chinese paper standard (CNS) A4 (210 X 297) by a paper size ----- ^ --------- ^ 1 ^ (Please read the precautions on the back before filling out this page) H ϋ ϋ ϋ 476947 Printed by the Consumers ’Cooperative of the Intellectual Property Bureau of the Ministry of Economic Affairs A7 V. Invention Description (> \) The second focusing lens 802 is focused on a second phase detector 702. The first beam splitter 10 2 a transmits all the laser beams from the first and second light sources 104 a and 104 b to the medium 100. Similarly, the first splitter 102a reflects the light beam reflected from the medium 100, which originates from the second light source 104a, and transmits the light beam reflected from the medium 100, which is from the first Origin of the two light sources 104b. The light beam reflected by the medium 100 and turned by the first beam splitter ^ 〇 2 a is collected by a first focusing lens 80 丄 onto a first phase detector 602. The use of this wavelength selection filter 300 is arbitrary. In other words, this, the long selection filter 300 is incorporated into this pickup when there is a need to separately control the apertures for the first and second light sources 1043 and 104b. Device. For example, if this first light source 〇 04 a emits a 400 nm blue laser and requires a calibre of 10.7, and 'this second light source 10 4 b emits a 650 nm red laser and requires In the mouth of 10.6, this wavelength selection filter 300 is used to allow the aperture of the objective lens to be reduced to 0.6 for the beam when all the = beams of the transmission wheel. ^ nm field-aligning this alignment lens 103, which forms the description of the present invention, includes a focusing lens i with a focusing power i, an astigmatism lens 1 (3 3 b with all divergent powers). f, and this astigmatism lens] 〇3 b's wide brother 1 aligning lens i〇3 ^ _- 15> f / fnm4fm (Please read the precautions on the back before filling in this page)-Line · 3 alignment from the first -And the second light source 1043 and 104. === _ The scale is applicable 297 Gong Ding 476947 Printed by the Consumer Cooperative of the Intellectual Property Bureau of the Ministry of Economic Affairs A7 B7_ 5. Description of the invention (> >) light beam, and synchronously Correction of chromatic aberration. <Embodiment 10> An tenth embodiment of the optical pickup according to the present invention is schematically shown in Figs. 20 and 22, and is used in the optical pickup of Figs. 20 and 22. The optical data are listed in Table 4. Table 4 Surface curvature radius Thickness Glass name Object surface Infinity 0.100000 si Infinity 0.20000 BK7 s2 Infinity 5.929508z 2.122789z s3 Infinity 6.0000 BK71 s4 Infinity 3.000000 s5 -4.081133 1.000000 FDS1 s6 30.164147 2.000000 BACD5 s7 -3.467121 5. 000000 K: -0.2007701 A: 0.445555E-03 B: -0.119205E-03 C: 0.316310E-04 D:-. 267022E-05 s8 STOP 1.770182 1.802215 BACD5 K: -0.721945 A: 0.537259E-02 B: 0.183575E -03 C: 0.855000E-04 D:-. 121341E-04 This paper size applies to China National Standard (CNS) A4 (210 X 297 mm) (Please read the precautions on the back before filling this page)
訂---------線J 476947 A7 B7 五、發明說明(〉〉) 經濟部智慧財產局員工消費合作社印製 s9 -11.452471 1.272566 K:-179.717593 A:0.222258E-02 B:-.194835E-03 C:-.172951E-04 D:0.399488E-05 slO 無限大 0.600000 ,CG, s9 無限大 〇.〇〇〇〇〇〇 影像表面 無限大 〇.〇〇〇〇〇〇 球形表面的方程式(見在以上之方程式 ⑵) 折射率/在d線上之Abbe的數目,v BK7:1.514520 在 650 nm/l.530849 在 400 nm/64.2 FDS1:1. 911294 在 650 nm/2.012371 在 400 nm/20.9 TAC8:1.725425 在 650 nm/1.752798 在 400 nm/54.7 BACD5:1.586422 在 650 nm/1. 606048 在 400 nm/61.3 ’CG’ :1.581922 在 650 nm/1. 623343 在 400 nm/31.0 進入孔的直徑(nun) 4.0 波長(nm) 400,650 (請先閱讀背面之注意事項再填寫本頁)Order --------- line J 476947 A7 B7 V. Description of invention (〉〉) Printed by the Consumer Cooperatives of the Intellectual Property Bureau of the Ministry of Economic Affairs s9 -11.452471 1.272566 K: -179.717593 A: 0.222258E-02 B:- .194835E-03 C:-. 172951E-04 D: 0.399488E-05 slO Infinite 0.600000, CG, s9 Infinite 0.000.00.00 The surface of the image is Infinite. 0.0000.00 Equation (see equation ⑵ above) Refractive index / number of Abbes on the d-line, v BK7: 1.514520 at 650 nm / l.530849 at 400 nm / 64.2 FDS1: 1. 911294 at 650 nm / 2.012371 at 400 nm / 20.9 TAC8: 1.725425 at 650 nm / 1.752798 at 400 nm / 54.7 BACD5: 1.586422 at 650 nm / 1. 606048 at 400 nm / 61.3 'CG': 1.581922 at 650 nm / 1. 623343 at 400 nm / 31.0 diameter of the hole (Nun) 4.0 Wavelength (nm) 400,650 (Please read the precautions on the back before filling this page)
訂---------線J 本紙張尺度適用中國國家標準(CNS)A4規格(210 X 297公釐) 476947 A7 五 、發明說明 對準透鏡的發散 -3.499/4.239 在 400 nm (mm) 整個對準透鏡的焦距 19.995 在 400 nm 接物鏡的焦距(πιπ〇 ΣίΤαΓΤο ~~' ' Ρ 1 - "" '----- 2.677 在 400 nm -0.0032 經濟部智慧財產局員工消費合作社印製 本 —* wv /u η '' V 丄iJULii 之一焦距的對準透鏡,及-具有〇·75之-口徑的接物鏡被 使,。因為從此光源所發射之光束的波長在土 5 nm的誤 差範圍之内’此散焦的角度可被表示成在焦點深度方面之 一 0.36 // m的不確疋性。相同地,在nm的光學距離 為 0.012 λ 〇 圖2 0描述在根據本發明之拾光器中,具有4〇5 nm 的一波長之光束的光路徑,及圖2丄描述在圖2 〇之拾光 為中的像差。圖2 2描述在根據本發明之拾光器中,具有 605 nm的一波長之光束的光路徑,及圖2 3描述在圖2 2 之拾光器中的像差。特別地,圖2 4比較地描述在圖2 〇 之拾光器中,40〇nm光束與4〇1及405 11〇1光束的像差。 如同在圖24中所示,在400 nm光束與405 nm光束 的像至方面的差異,在根據本發明之拾光器中幾乎無法被 偵測。因為根據本發明之對準透鏡具有高聚焦倍率,像差 可被有效地更正。結果,一光點可以在對應到發射光束之 波長的變化之-焦點深度的範圍内,而被聚焦在一媒體上。 對於更多有關於如此短波長光束方面之色像差的有效 紙張尺度適用中國國家標準(CNS)A4規格⑽X 297公髮y (請先閱讀背面之注意事項再填寫本頁) % . --線- 476947 A7 五、發明說明(><) 降低,假設此整個對準透鏡的焦距為f,及此散光透鏡的 焦距為fn,此對準透鏡符合關係一0.5>f/fn是必須的。 較佳地,假設透鏡組(其構成此拾光器)的前焦距, 為fl,f2 ’…,及fn,其被從此光源朝向此媒體排列,且 對於此透鏡組之光學物質的d —線上之A b b e數目為 vl,V2,…,及vn,此拾光器符合關係_〇 005<1/(fl · vl)+ · v2)H-----l· l/(fn · vn)<0·⑻05。 根據本發明之拾光器相容於現今的DVDs,及HD —D VD s兩者,其需要一接近405 nm的藍色光源及一 具有0.6的口徑之接物鏡,但此規格尚未標準化。根據本 發明之拾光器,使用一具有一高口徑的接物鏡及一具有 500 nm或更短的一短波長之光源,而確保了高密度資訊的 讀取及記錄。特別地,具有此組態的對準透鏡解釋了上述 之有利於,密度資訊的讀取及記錄,藉由有效地更正有關 於=長藍光雷射光束方面之色像差。在當本發明已被特 並參考其較佳實施例時,藉由這些在此技 :能被達成:Ϊ;未=:= = == 疋義之本發明的精神及範圍。 規格(210 x 297公爱) 476947 Α7 Β7 經濟部智慧財產局員工消費合作社印製 五、發明說明(>έ) 【圖式之Μ早說明】 圖1一圖顯示有關於在一雷射一極體的各種不同溫度 情形下之輸出倍率方面’此雷射一極體的發射波長之變化; 圖2為一圖顯示有關於各種光學物質之波長方面,折 射指數的變化; 圖3為一用於色像差更正之一傳統接物鏡的概略視 圖; 圖4顯示根據本發明之一種拾光器的一第一實施例之 光學排列; 圖5顯示根據本發明之此拾光器的一第二實施例之光 學排列; 圖6顯示根據本發明之此拾光器的一第三實施例之光 路徑; 圖7描述在圖6的拾光器中之像差; 圖8描述根據本發明之此拾光器的一第四實施例之光 路徑; 圖9描述在圖8的拾光器中之像差; 圖10顯示根據本發明之此拾光器的一第四實施例之 光路徑; 圖1 1描述在圖10的拾光器中之像差; 圖12描述使用一傳統對準透鏡之一拾光器的光路 徑; 圖13描述在圖12的傳統拾光器中之像差; 圖14描述使用根據本發明之一對準透鏡的一拾光器 (請先閱讀背面之注意事項再填寫本頁) ¾ 二IT、· .線· 本紙張尺度適用中國國家標準(CNS)A4規格(210 X 297公爱) 476947 經濟部智慧財產局員工消費合作社印製 A7 發明說明( 的光路徑; 圖1 5描述在圖14的拾光器中之像差; 圖16顯不根據本發明之一種拾光器的一第六實施例 之光學排列; ' 圖17顯示根據本發明之一種拾光器的一第七實施例 之光學排列; 圖18顯示根據本發明之一種拾光器的_第八實施例 之光學排列; ' 圖19顯示根據本發明之一種拾光器的一第九實施例 之光學排列; 圖2 0描述在根據本發明之拾光器中具有々os nm的 一波長之光束的光路徑; 圖2 1描述在圖2 〇的拾光器中之像差; 圖2 2描述在根據本發明之拾光器中具有65〇 ηηι的 一波長之光束的光路徑; 圖2 3描述在圖2 2的拾光器中之像差;及 圖2 4描述在圖2 0的拾光器中,對於400 nm光束 及對於401及405 nm光束之像差。 【參考標號對照表】 10 0媒體(光碟) 101接物鏡 10 2分光器 102a第一分光器 1 0 2 b第二分光器 本紙張尺度適用中國國家標準(CNS)A4規格(210 X 297公爱) (請先間讀背面之注意事項再填寫本頁) 訂---------ί 476947 A7 _ B7 五、發明說明(>?) 1 ◦2 C第三分光器 1 0 3對準透鏡 1 0 3 a聚焦透鏡 1 0 3 b散光透鏡 1 0 4光源 1 0 4 a第一光源 1 0 4 b第二光源 1 0 5聚集透鏡 1 0 6相偵測器 1 0 7又/4玻璃板 3 0 0波長選擇過濾器 6 0 2第一相偵測器 7 0 2第二相偵測器 8 0 1第一對準透鏡 8 0 2第二對準透鏡 (請先閱讀背面之注意事項再填寫本頁)Order --------- Line J This paper size is applicable to China National Standard (CNS) A4 specification (210 X 297 mm) 476947 A7 V. Description of the invention Divergence of the alignment lens-3.499 / 4.239 at 400 nm ( mm) Focal length of the entire alignment lens 19.995 at 400 nm Focal length of the objective lens (πιπ〇ΣίΤαΓΤο ~~ '' Ρ 1-" " '----- 2.677 at 400 nm -0.0032 Employees of Intellectual Property Bureau, Ministry of Economic Affairs Cooperative print— * wv / u η ”V 丄 iJULii, one of the focal lengths of the alignment lens, and an objective lens with a diameter of 0.75 is used, because the wavelength of the light beam emitted from this light source is in the soil Within an error range of 5 nm, this defocused angle can be expressed as an uncertainty of 0.36 // m in terms of focal depth. Similarly, the optical distance in nm is 0.012 λ 〇 Figure 2 0 is described in In the optical pickup according to the present invention, the optical path of a light beam having a wavelength of 4.05 nm, and the aberration in FIG. 2 described in the optical pickup of FIG. 20 are described in FIG. In the optical pickup, the optical path of a light beam having a wavelength of 605 nm, and FIG. 2 3 is described in FIG. 2 2 Aberrations in the lens. In particular, FIG. 24 is a comparative description of the aberrations of the 400 nm beam and the 401 and 405 1101 beams in the optical pickup of FIG. 20. As shown in FIG. 24 The difference between the image of the 400 nm beam and the 405 nm beam can hardly be detected in the optical pickup according to the present invention. Because the alignment lens according to the present invention has a high focusing magnification, the aberration can be effectively Correction. As a result, a light spot can be focused on a medium within the range of the focal depth corresponding to the change in the wavelength of the emitted beam. For more effective paper on chromatic aberrations with respect to such short wavelength beams Standards are applicable to China National Standard (CNS) A4 specifications ⑽ X 297 public y (please read the precautions on the back before filling out this page)%. --Line-476947 A7 V. Description of invention (> <) Decrease, assuming this The focal length of the entire alignment lens is f, and the focal length of this astigmatism lens is fn. It is necessary that the alignment lens conforms to the relationship of 0.5> f / fn. Preferably, it is assumed that the lens group (which constitutes the optical pickup) The front focal length is fl, f2 '..., and fn, which are determined from this light source Aligned to this medium, and the number of A bbe on the d — line of the optical substance of the lens group is vl, V2, ..., and vn, and this optical pickup conforms to the relationship _0055 < 1 / (fl · vl) + · v2) H ----- l·l / (fn · vn) < 0 · ⑻05. The optical pickup according to the present invention is compatible with both today's DVDs and HD-D VD s. It requires a blue light source near 405 nm and an objective lens with a diameter of 0.6, but this specification has not been standardized. According to the optical pickup of the present invention, an objective lens having a high aperture and a light source having a short wavelength of 500 nm or less are used to ensure the reading and recording of high-density information. In particular, the alignment lens having this configuration explains the above-mentioned advantage, the reading and recording of density information, by effectively correcting the chromatic aberration related to the = long blue laser beam. When the present invention has been specifically described with reference to its preferred embodiments, with these techniques: can be achieved: Ϊ; not =: = = == meaning of the spirit and scope of the present invention. Specifications (210 x 297 public love) 476947 Α7 Β7 Printed by the Consumer Cooperatives of the Intellectual Property Bureau of the Ministry of Economic Affairs. 5. Description of the invention (>) [Early description of the pattern] Figure 1 shows a picture about a laser In terms of the output magnification of the polar body under different temperature conditions, the change of the emission wavelength of this laser-polar body; Figure 2 is a graph showing the change of the refractive index with respect to the wavelength of various optical substances; Figure 3 is a A schematic view of a conventional objective lens for chromatic aberration correction; FIG. 4 shows an optical arrangement of a first embodiment of an optical pickup according to the present invention; FIG. 5 shows a second optical pickup according to the present invention. Optical arrangement of the embodiment; Fig. 6 shows a light path of a third embodiment of the optical pickup according to the present invention; Fig. 7 illustrates aberrations in the optical pickup of Fig. 6; A light path of a fourth embodiment of the optical pickup; FIG. 9 illustrates aberrations in the light pickup of FIG. 8; FIG. 10 shows a light path of a fourth embodiment of the optical pickup according to the present invention; 11 describes aberrations in the optical pickup of FIG. 10; 12 depicts the light path of an optical pickup using one of the conventional alignment lenses; FIG. 13 depicts the aberrations in the conventional optical pickup of FIG. 12; FIG. 14 depicts an optical pickup using an alignment lens according to the present invention (Please read the precautions on the back before filling out this page) ¾ IT, ··················· This paper size applies to China National Standard (CNS) A4 specifications (210 X 297 public love) FIG. 15 illustrates the light path of the invention; FIG. 15 depicts the aberrations in the optical pickup of FIG. 14; FIG. 16 shows an optical arrangement of a sixth embodiment of an optical pickup according to the present invention; An optical arrangement of a seventh embodiment of an optical pickup according to the present invention is shown; FIG. 18 shows an optical arrangement of an eighth embodiment of an optical pickup according to the present invention; FIG. 19 shows an optical arrangement according to the present invention Optical arrangement of a ninth embodiment of an optical device; Fig. 20 depicts the optical path of a light beam with a wavelength of 々os nm in an optical pickup according to the invention; Fig. 21 depicts the optical pickup in Fig. 20 Aberrations; Figure 2 2 depicts the The optical path of a light beam with a wavelength of 65 nm in the optical pickup; FIG. 23 depicts the aberrations in the optical pickup of FIG. 22; and FIG. 24 describes the aberration in the optical pickup of FIG. 400 nm beam and aberration for 401 and 405 nm beams. [Reference Table] 10 0 Media (Disc) 101 Receiver 10 2 Beamsplitter 102a First Beamsplitter 1 0 2 b Second Beamsplitter Applicable to this paper size China National Standard (CNS) A4 Specification (210 X 297 Public Love) (Please read the precautions on the back before filling this page) Order --------- ί 476947 A7 _ B7 V. Description of the Invention (>?) 1 ◦ 2 C Third beam splitter 1 0 3 Alignment lens 1 0 3 a Focusing lens 1 0 3 b Astigmatic lens 1 0 4 Light source 1 0 4 a First light source 1 0 4 b Second light source 1 0 5 Focusing lens 1 0 6-phase detector 1 0 7/4 glass plate 3 0 0 Wavelength selection filter 6 0 2 First-phase detector 7 0 2 Second-phase detector 8 0 1 First alignment lens 8 0 2 Second alignment lens (Please read the precautions on the back before filling this page)
訂---------線J 經濟部智慧財產局員工湞費合作社印製 本紙張尺度適用中國國家標準(CNS)A4規格(210 X 297公釐)Order --------- Line J Printed by the Employees' Cooperative of Intellectual Property Bureau of the Ministry of Economic Affairs This paper size applies to China National Standard (CNS) A4 (210 X 297 mm)
Claims (1)
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
TW89122756A TW476947B (en) | 2000-10-27 | 2000-10-27 | Optical pickup |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
TW89122756A TW476947B (en) | 2000-10-27 | 2000-10-27 | Optical pickup |
Publications (1)
Publication Number | Publication Date |
---|---|
TW476947B true TW476947B (en) | 2002-02-21 |
Family
ID=21661715
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
TW89122756A TW476947B (en) | 2000-10-27 | 2000-10-27 | Optical pickup |
Country Status (1)
Country | Link |
---|---|
TW (1) | TW476947B (en) |
-
2000
- 2000-10-27 TW TW89122756A patent/TW476947B/en not_active IP Right Cessation
Similar Documents
Publication | Publication Date | Title |
---|---|---|
TW561473B (en) | Objective lens, light converging optical system, optical pickup apparatus, and recording/reproducing apparatus | |
TW556178B (en) | Optical pickup apparatus and objective lens | |
EP1359574A2 (en) | Recording reproducing optical system, objective lens and aberration correcting optical element | |
TW526339B (en) | Compatible optical pickup | |
EP1096483A2 (en) | Optical pickup | |
US7656774B2 (en) | Objective lens, optical head, and optical pickup apparatus | |
TWI237819B (en) | Optical pick-up device and objective lens used therein | |
TW539869B (en) | Objective lens for optical pickup apparatus and optical pickup apparatus | |
JP2009093785A (en) | Lens system for holographic storage medium | |
US20040042084A1 (en) | Optical pickup device and optical element used for the same | |
TW476947B (en) | Optical pickup | |
JP2001194581A (en) | Objective lens and optical pickup device | |
EP1538613A2 (en) | Optical pickup apparatus and optical information recording and/or reproducing apparatus | |
TW563109B (en) | Objective lens device capable of correcting chromatic aberration and optical pickup employing the same | |
Braat | Influence of substrate thickness on optical disk readout | |
JP2002237078A (en) | Object lens and optical pickup device | |
JP2006244656A (en) | Objective lens, optical pickup device, and optical disk device | |
JP4294460B2 (en) | Objective lens, optical pickup device and optical disk device | |
US7990831B2 (en) | Optical pickup device | |
JP2794816B2 (en) | Recording / playback optical system | |
US20060164967A1 (en) | Objective lens and optical pickup device | |
JP2001337269A (en) | Optical device for compensating chromatic aberration and optical pickup device | |
JP2004326868A (en) | Objective optical element and optical pickup device | |
US7710847B2 (en) | Optical pickup apparatus | |
JP2001108894A (en) | Optical system for optical pickup, optical pickup device, coupling optical system, lens for coupling optical system, and recording and reproducing device |
Legal Events
Date | Code | Title | Description |
---|---|---|---|
GD4A | Issue of patent certificate for granted invention patent | ||
MM4A | Annulment or lapse of patent due to non-payment of fees |