TWI313363B - Multi-focus objective lens - Google Patents
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- TWI313363B TWI313363B TW95145638A TW95145638A TWI313363B TW I313363 B TWI313363 B TW I313363B TW 95145638 A TW95145638 A TW 95145638A TW 95145638 A TW95145638 A TW 95145638A TW I313363 B TWI313363 B TW I313363B
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1313363 九、發明說明: 【發明所屬之技術領域】 本發明係有關於一種多焦物鏡,特別係有關一種較易 製造的多焦物鏡。 【先前技術】 習知的多焦物鏡,如美國專利公開第2006/0201250號 所揭露的,其為一種雙鏡片組成的物鏡,其物鏡重量較重, • 組裝調校的成本較高。並且,由於需使用半導體製程製作 鏡片,因此成本較高,並容易產生雜散光的問題。 美國專利公開第2005/0281172號揭露了 一種單鏡片的 多焦物鏡,該多焦物鏡具有一繞射結構、一第一表面以及 一第二表面,該第一表面相對於該第二表面,該繞射結構 形成於該第一表面之上。美國專利公開第2005/0281172號 之繞射結構的繞射條紋間距需小於3//m,繞射條紋的深度 約為2.24//m,該繞射結構需透過高精密度加工來製作, *其製造成本以及製造難度都偏高。 【發明内容】 本發明即為了欲解決習知技術之問題而提供之多焦物 鏡,包括一第一表面以及一第二表面。第一表面包括一第 一非球面、一第二非球面、一第一繞射結構以及一第二繞 射結構。第一非球面以及第一繞射結構位於一第一區域, 第二非球面以及第二繞射結構位於一第二區域。該第二區 0949-A21811 TWF(N2);P51950098TW;Lemon 6 乜13363 域環繞該第—區域。第二表面包括 :球面::第三繞射結構以及-第二第:= =及弟二繞射結構位於—第三區域,第四非球面以及第 射結構位於—第四區域。該第1313363 IX. DESCRIPTION OF THE INVENTION: TECHNICAL FIELD OF THE INVENTION The present invention relates to a multifocal objective lens, and more particularly to a multifocal objective lens that is relatively easy to manufacture. [Prior Art] A conventional multi-focal objective lens, as disclosed in U.S. Patent Publication No. 2006/0201250, is an objective lens composed of a double lens, the objective lens of which is heavy, and the cost of assembly adjustment is high. Moreover, since a lens is required to be fabricated using a semiconductor process, the cost is high and the problem of stray light is likely to occur. US Patent Publication No. 2005/0281172 discloses a single-lens multi-focus objective lens having a diffraction structure, a first surface and a second surface, the first surface being opposite to the second surface A diffractive structure is formed over the first surface. The diffraction fringe of the diffraction structure of US Patent Publication No. 2005/0281172 needs to be less than 3/m, and the depth of the diffraction fringe is about 2.24/m. The diffraction structure needs to be fabricated by high-precision processing, * Its manufacturing cost and manufacturing difficulty are high. SUMMARY OF THE INVENTION The present invention provides a multifocal objective lens for solving the problems of the prior art, including a first surface and a second surface. The first surface includes a first aspherical surface, a second aspherical surface, a first diffractive structure, and a second diffractive structure. The first aspherical surface and the first diffractive structure are located in a first region, and the second aspherical surface and the second diffractive structure are located in a second region. The second zone 0949-A21811 TWF(N2); P51950098TW; the Lemon 6 乜13363 domain surrounds the first zone. The second surface includes: a spherical surface: a third diffraction structure and - a second: = = and a second diffraction structure is located in the - third region, the fourth aspheric surface and the first radiation structure are located in the - fourth region. The first
域。第二表面為該第一表面的背面。“…“二Q 可以發明之多焦物鏡,各繞射結構的緩射階數搭配 溫度變化及光源中心波長飄移產生的像差。同 結構=之Μ物鏡的第—表面以及第二表面均有繞射 产1卩加大繞射條紋之間隔,而得以降低製造難 二應用本發明,可使該第—光束(hd_dvd雷射 ά以弟—光束(DVD f射光)以及該第三光束(CD雷射光) 的繞射效率全大於—,崎崎低総量;1 【實施方式】 荟知第1圖,其係顯示本發明之多焦物鏡⑽,用以 讀取碟片200,該多焦物鏡100包括一第一表面S1以及一 弟二表面S2。搭配參照第2&圖,第一表面S1包括一第一 ^求面11、一第二非球面12、-第-繞射結構21以及一 第二,射結構22。第—非球面n以及第一繞射結構2“立 於,區域A1,第二非球面12以及第二繞射結構22位 H區域A2。該第二區域A2環繞該第—區域Ai。搭 配芩照第2b圖’第二表面S2包括一第三非球面13、一第 四非球面14、—第二繞射結構23以及-第四繞射結構24。 第二非球面13以及第三繞射結構23位於一第三區域A3 , 0949-Α2Ί 811 TWF(N2);P51950098TW;Lemon 7 I313363 ,=非球面14以及第四繞射結構24位於一第四區域A4。 ^第的區域A4環繞該第三區域A3。第二表面S2為該第 上,面S1的背面,該第—區域A1對應該第三區域A3 , °亥条一區域A2對應該第四區域A4。 ^本發明之多焦物鏡用以對一第一光束(HD-DVD雷射 光第二光束(DVD雷射光)以及一第三光束(CD雷射田光) 進仃聚焦,該第一光束包括一第一波長λι,該第二光束包 括一第二波長λ2 ’該第三光束包括一第三波長λ3。 以下,首先說明該第一繞射結構以及該第三繞射結構 之間的設計關係。 [第一繞射結構以及該第三繞射結構之間的設計關係] 該第一繞射結構以及該第三繞射結構包括一第一設計 波長λ",該第一設計波長與該第一波長^、該第二波 χ 2 (;Λ 0< ΙΝΤφ-φ Λ Λ <0.4 ΙΝΤ 9 Λ·ι ν ^ y % 介於 390 至 420nm 之間; 〇< 之間; 0< ζνΓ(Αΐ)-(Αί)area. The second surface is the back surface of the first surface. "..." Two Q can invent the multi-focus objective lens, the retardation order of each diffraction structure is matched with the temperature variation and the aberration caused by the drift of the center wavelength of the light source. The first surface and the second surface of the objective lens of the same structure have a diffraction of 1 卩 to increase the interval of the diffraction fringes, thereby reducing the manufacturing difficulty. The present invention can be applied to the first beam (hd_dvd laser ά The diffraction efficiency of the light beam (DVD f light) and the third light beam (CD laser light) is all greater than -, and the amount of snagging is low; 1 [Embodiment] The first figure shows the present invention. a focal lens (10) for reading the disc 200, the multi-focus objective lens 100 includes a first surface S1 and a second surface S2. Referring to the second & second embodiment, the first surface S1 includes a first surface 11 a second aspherical surface 12, a first-diffraction structure 21 and a second, radiation structure 22. The first aspheric surface n and the first diffraction structure 2 "stand on, the area A1, the second aspheric surface 12 and the second The second structure A2 surrounds the first region Ai. The second surface A2 includes a third aspheric surface 13, a fourth aspheric surface 14, and a second surface. The diffraction structure 23 and the fourth diffraction structure 24. The second aspheric surface 13 and the third diffraction structure 23 are located in a third area A3. 0949-Α2Ί 811 TWF(N2); P51950098TW; Lemon 7 I313363, = aspherical surface 14 and fourth diffraction structure 24 are located in a fourth area A4. ^The first area A4 surrounds the third area A3. The second surface S2 is In the upper surface of the surface S1, the first region A1 corresponds to the third region A3, and the region A2 corresponds to the fourth region A4. The multifocal objective lens of the present invention is used for a first light beam (HD). a DVD laser light second beam (DVD laser light) and a third light beam (CD laser field light), wherein the first light beam comprises a first wavelength λι and the second light beam comprises a second wavelength λ2 ′ The third light beam includes a third wavelength λ3. Hereinafter, the design relationship between the first diffraction structure and the third diffraction structure will be first described. [Design of the first diffraction structure and the third diffraction structure Relationship] The first diffraction structure and the third diffraction structure include a first design wavelength λ", the first design wavelength and the first wavelength ^, the second wavelength χ 2 (; Λ 0< ΙΝΤ φ-φ Λ Λ <0.4 ΙΝΤ 9 Λ·ι ν ^ y % between 390 and 420 nm; 〇<Room; 0 < ζνΓ (Αΐ) - (Αί)
<0.4 INT /lr\ ιηΊ &介於600至698nm<0.4 INT /lr\ ιηΊ & between 600 and 698 nm
<0.4 INT ^ J^z ^介於700至890nm 之間,以及 0949-A21811TWF(N2);P51950098TW;Lemon 8 1313363 Λ.1 =名 χ(Λ’-1), W其中,dl為該第—繞射結構以及該第三繞射結構之間 的Z木度1N為該第—緩射結構以及該第三繞射結構之折射 率1邊乐一光束包括—第—繞射階數”7"該第二光束包括 7第二繞,數%,該第三光束包括-第三繞射階數, δ亥第―、弟二以及第三繞射階數(Ύ3)係擇自由以下數 ^2;1;0' ;(2;U) ' ' ^3,2,2) ^ (4,3,0). 8,5,Γ) I 、(5,3,3)、(M,G)、(6,4,3)、 以及 ’(10 8’5’4)、(9,6,0)、(9,6,5)、(10,6,0) (,6,5 )所組成之族君夢。 以上所提供之數列’為設計時可收敛的數列。 第-非球面與該第三非球面形成一第一隹距 弟一繞射結構包括一第一繞 ^ 裳一娃私在c 、,几射焦距fD],該第一焦距f】與該 %射^、距fD】滿足以下關係式: ~03<-~~<0.3<0.4 INT ^ J^z ^ is between 700 and 890 nm, and 0949-A21811TWF(N2); P51950098TW; Lemon 8 1313363 Λ.1 = noun (Λ'-1), W where dl is the first - the Z-degree 1N between the diffraction structure and the third diffraction structure is the first-relay structure and the refractive index of the third diffraction structure 1 side beam includes a -th-diffraction order" 7" The second light beam includes 7 second windings, the number of the third light beams, the third light beam includes a third diffraction order, the δHai-, the second two, and the third diffraction order (Ύ3) are selected as follows: 2;1;0' ;(2;U) ' ' ^3,2,2) ^ (4,3,0). 8,5,Γ) I , (5,3,3), (M,G ), (6,4,3), and '(10 8'5'4), (9,6,0), (9,6,5), (10,6,0) (,6,5 ) The group of monarchs is composed. The series provided above is a sequence that can converge when designing. The first aspheric surface forms a first pupil with the third aspheric surface, and the diffraction structure includes a first winding. The baby is privately c, and the focal length fD], the first focal length f] and the % shot and the distance fD satisfy the following relationship: ~03<-~~<0.3
Jm 同日守’该弟一繞射隹距f -Μ- 〇 又 耵…距fD]滿足以下關係式: j D\ =7~~--^___Jm on the same day, the younger brother of a divergence f -Μ- 〇 and 耵...from fD] satisfies the following relationship: j D\ =7~~--^___
(-2x/>xW;x^J ,其中,n=;I、2或3,代表兮笛 係數。 '^弟—、,光射結構的二階相位 同樣的’該第三繞射結構包 〜_ 第-焦距f,與該第三繞射 %射焦距b,該 -0.3<A<0.3 距^滿足以下關係式·· j 03 ,同時’該第三繞射焦距心滿足以下關係式: 0949 A21811TWF(N2);p51g5〇〇98TW:Lern〇n 1313363 fm :7----- (~2χΡ3χ,77η xAj ,其中,ϊι=1、2或3,Ρ3代矣兮窜_ 係數。 代表D亥乐二繞射結構的二階相位 該第一繞射結構與該第三錶身 Ά射、、'°構之所有相位係數 (例如,:階相位錢、三_耗咖絕對值小於0 !。 产该第-繞射結構與該第三繞射結構之第一、第二以及 弟三繞射階數(W),可以相㈤或相異。 ’』以上所提供之數值以及限制ϋ係,透過運算軟體 (例如,鈦思科技所提供之軟體c〇de V),可以得到咳 繞射結構、該第三繞射結構、 以 ^ ΛΑ ^ 及弗—非球面以及該第三非 球面的设計數據,其中,該第一讯 ^ /θ ^ 5又计波長λ,]係以試誤法的 方式5十异取付,其可以為,例如,3264細。 構 之二::說明該第二繞射結構以及該第四繞射結 [第結私及_四繞射結叙_設計關係] 該第二繞射結構以及該第 四繞射結構包括一第二設計 波長λ,,2 ’該第二設計波長X、'…”… 與乐一波長、以及該第波長λ2之間,滿足下列關係式: 〇<之間; 0< 鮮(于)-(&) 乞 0.4 1ΝΤ λ m、 ’ 11 介於 390 至 420nm < 0.4 INT 5 〇949~A21811TWF(N2):P5l95〇〇98TW;Lern〇n Λ, ’ 4介於 600 至 698nm 10 I313363 之間;以及 Λ·2 = Χ (Λ^ - 1), 其中,4為該第二繞射結構以及該第四繞射結構之間的深 度,N為該第二繞射結構以及該第四繞射結構之折射率, 邊第一光束包括一第一繞射階數m,,該第二光束包括—第 —繞射階數%,該第一以及第二繞射階數 下數列 (5’〇)、(5,3)、(6,0)、(6,4)、(8,〇)、(、 (9,〇)、(θ9,6)、〇〇,〇)以及(1〇,6)所組成之族群。 以上所提供之數列,為設計時可㈣的數列。 =第二非球面與該第四非球面形成—第二焦距4,, :::::構包括一第二繞射焦距。該第二焦距^ 弟一%射焦距fD2滿足以下關係式·· 、人 -0-3 <-^<0.3 JD2 ,同時,該第二繞射隹距f p (-2xJ}2xm/1xA„), 4凡町’、、、距tD2滿足以下關係式: 其中,11=1、2 或 3,P /h ± 階相 焦距 位係數。 2㈣第二繞射結構的 該第四繞射結構包括—第四链 6與該第四繞射隹距f # $距圮4,該第_ —。.3<五二 滿足以下關係式:(-2x/>xW;x^J , where n=; I, 2 or 3, representing the whistle coefficient. '^ brother—, the second-order phase of the light-emitting structure is the same as the third diffraction structure package 〜 _ the focal length f, and the third diffraction % focal length b, the -0.3 < A < 0.3 distance ^ satisfies the following relation ·· j 03 , and at the same time 'the third diffraction focal length satisfies the following relationship : 0949 A21811TWF(N2); p51g5〇〇98TW:Lern〇n 1313363 fm :7----- (~2χΡ3χ,77η xAj , where ϊι=1, 2 or 3, Ρ3 矣兮窜 _ coefficient. The second-order phase of the D-Hale two diffraction structure, the first diffraction structure and all the phase coefficients of the third body, and the '° structure (for example, the order phase money, the three-dimensional coffee absolute value is less than 0! The first, second, and third diffraction orders (W) of the first-diffraction structure and the third diffraction structure may be (five) or different. '』 The values provided above and the limit system Through the computing software (for example, the software c〇de V provided by Titans Technology), the cough diffraction structure, the third diffraction structure, the ^ ΛΑ ^ and the aspheric surface, and the third aspheric surface can be obtained. The design data, wherein the first signal ^ / θ ^ 5 is calculated by the wavelength λ,] is taken in a trial and error manner, which may be, for example, 3264 fine. a two-diffraction structure and the fourth diffraction junction [the first and the fourth diffraction structure] the second diffraction structure and the fourth diffraction structure comprise a second design wavelength λ,, 2 ' The second design wavelength X, '...'... and the Le-wavelength, and the first wavelength λ2, satisfy the following relationship: 〇<between;0<鲜(-)-(&) 乞0.4 1ΝΤ λ m, ' 11 between 390 and 420 nm < 0.4 INT 5 〇 949~A21811TWF(N2): P5l95〇〇98TW; Lern〇n Λ, ' 4 between 600 and 698 nm 10 I313363; and Λ·2 = Χ (Λ^ - 1), wherein 4 is the depth between the second diffraction structure and the fourth diffraction structure, and N is the refractive index of the second diffraction structure and the fourth diffraction structure, A light beam includes a first diffraction order m, the second light beam includes a -first diffraction order number, and the first and second diffraction orders are a number of columns (5'〇), (5, 3) , (6,0), (6,4) The group consisting of (8, 〇), (, (9, 〇), (θ9, 6), 〇〇, 〇) and (1〇, 6). The series provided above are the series of (4) at design time. = The second aspherical surface is formed with the fourth aspherical surface - the second focal length 4,, ::::: comprises a second diffraction focal length. The second focal length ^-% of the focal length fD2 satisfies the following relationship: · human -3-3 <-^<0.3 JD2 , and the second diffraction pitch fp (-2xJ}2xm/1xA „ ), 4 Fancho ',,, and tD2 satisfy the following relationship: where 11 = 1, 2, or 3, P / h ± phase focal length coefficient. 2 (d) The fourth diffraction structure of the second diffraction structure includes - the fourth chain 6 and the fourth diffraction pitch f # $ distance 圮 4, the first _ - .. 3 < fifty two meet the following relationship:
1DA (~2xP4xm/lxAll) 麵距一以下關係式: Μ 0949-A2l81iTWF(N2);P51950098TW;Lemon 1313363 其中 數。 2或3,P4代表該第四繞射結 的一階相位係 該第二緩射結構與該第四繞射 該第二繞射結_ f數)的絶對值小於〇.卜 筮- Μ k /、n亥弟四鉍射結構之第一、第-,v菸 弟二繞射階數可以相同或相異。 以及 (例士應^上所提供之數值以及11剛1係,透過運當軟娜 (例如’鈦帥技所提供之軟體Cc>de V),可^ 繞射結構、該第四繞射結構、 )=场到该弟二 球面的設計數據,其中球面以及該第四非 方式計算取得,其可以為:::蝴長、2係以試誤法的 ,、J Μ马,例如,2〇4〇nm。 該多焦物鏡可以由塑膠或破璃等材料製成。 溫度:二:二:例中’利用非球面可消除主要像差與 度义化每成折射率變化所產生的球差 構消剩餘像差與溫度變化產 =、、、σ 移所產生的球差。非域像差以及先源中心波長飄 差,绝傻# :產生正球差’繞射結構產生負球 〜'象可互相平衡達到趨近〇像差的目的。 利用非球面係數與繞射係數和繞射階數最佳的组合, :達到碟片傾斜光學補償設計、碟片厚度誤差光學補償設 \物鏡傾斜光學補償設計、溫度變化光學補償設計、光 源中心波長飄移光學補償設計、物鏡在組裝誤差光學補償 設計、繞射結構高繞射效率光學設計的目的。 亡用本么明之多焦物鏡,各繞射結構的繞射階數搭配 可以補償因溫度變化及光源中心波長飄移產生的像差。同 0949-Α2 彳 S mWF_:P5 〗950〇98TW;Lemon 12 1313363 本發明之多隹物错的楚 . 社雄.. …、物鏡的弟一表面以及第二表面均有繞射 度。同:此岸大繞射條紋之間隔,而得以降低製造難 光)、”'-’::,可使該第—光__雷射 雷射光)以及該第三光束_雷射光) 的繞射效率全大於9〇〇/n LV μ二π m ^ 心;Ϊ 得以降低光能量的損耗。 包括^ 本發明的另—實施例中,該多焦物鏡 - 一第二表面S2。第-表面S1包括 弟非球面π、一第二非球面12、 以及—第二繞射社構22,二】面戈—弟一繞射結構η 繞射結構21二;構環繞該第一 β %紅構21形成於該第—非球面u „ 二、k射結構22形成於該第二非球面12之上。 ::第:二為該第一表面S1的背面,該第二表面S2包 —€球面13以及一第三繞射結構幻,該键 結構23形成於該第三非球面13之上,其中,第三、^钟 構23對應該第一繞射結構21。 一 %,、、、口 包括本發明的又-實施例中,該多焦物鏡 W《-表面81以及一第二表面幻。第—表面 -弟-非球面U、一第二非球叫 =及一第二繞射結構22,該第二繞射結構2 :上,該第二繞射卿形成於該第二非球面d? 弟:表面S2為該第一表面S1的背面,該第二表面Μ包 括一弟四非球面14以及一第四繞射結構Μ,該 結構24形成於該第四非球面M : 具中,弟四繞射結 0949-A21811TWF(N2);P51950098TW;Lemon 13 1313363 構24對應該第二繞射結構22。 雖然本發明已以具體之較佳實施例揭露如上,然其並 非用以限定本發明,任何熟習此項技藝者,在不脫離本發 明之精神和範圍内,仍可作些許的更動與潤飾,因此本發 明之保護範圍當視後附之申請專利範圍所界定者為準。1DA (~2xP4xm/lxAll) The following relationship: Μ 0949-A2l81iTWF(N2); P51950098TW; Lemon 1313363 where number. 2 or 3, P4 represents the first-order phase of the fourth diffraction junction, and the absolute value of the second retardation structure and the fourth diffraction of the second diffraction junction _f is less than 〇. 筮 - Μ k / The first and the first, the first and the second, and the second and second radiant structures of n Haidi may be the same or different. And (the case should be on the value provided and the 11 just 1 series, through the softness of the soft (such as 'software Cc> de V provided by Titanic Technology), can be the diffraction structure, the fourth diffraction structure , ) = field to the design data of the two spheres of the brother, in which the spherical surface and the fourth non-method are calculated, which can be::: butterfly length, 2 series to try the wrong method, J Μ horse, for example, 2〇 4〇nm. The multi-focus objective lens can be made of a material such as plastic or broken glass. Temperature: 2: 2: In the example, 'Using aspherical surface can eliminate the spherical aberration caused by the main aberration and the degree of refractive index change, and the residual aberration and temperature change yield the ball produced by the shift of =, , and σ difference. Non-domain aberrations and pre-source center wavelength drift, absolutely silly #: Produce a positive spherical aberration. The diffraction structure produces a negative sphere. The image can be balanced to achieve the same 〇 aberration. Using the combination of aspheric coefficient and diffraction coefficient and diffraction order: to achieve disc tilt optical compensation design, disc thickness error optical compensation design, objective lens tilt optical compensation design, temperature variation optical compensation design, light source center wavelength The objective of drifting optical compensation design, objective lens optical compensation design in assembly error, and high diffraction efficiency optical design of diffraction structure. The use of the multi-focus objective lens of the Ming Dynasty, the diffraction order of each diffraction structure can compensate for the aberration caused by the temperature change and the drift of the center wavelength of the light source. Same as 0949-Α2 彳 S mWF_:P5 〗 950 〇 98 TW; Lemon 12 1313363 The invention of the invention is a sinister thing. 社雄.. ..., the surface of the objective lens and the second surface have diffraction. Same as: the spacing between the large diffraction stripes of the shore, which can reduce the difficulty of manufacturing), "'-'::, the diffraction of the first-light __ laser" and the diffraction of the third beam_laser light) The efficiency is all greater than 9 〇〇 / n LV μ π m ^ core; 得以 can reduce the loss of optical energy. Including another embodiment of the invention, the multi-focus objective lens - a second surface S2. Surface-surface S1 Including a brother aspherical surface π, a second aspherical surface 12, and a second diffractive structure 22, a second surface, a dih-different structure, a diffraction structure η, a diffraction structure 21, and a structure surrounding the first β% red structure 21 Formed on the first aspheric surface u „ two, the k-ray structure 22 is formed on the second aspheric surface 12. The second surface S2 includes a rear surface of the first surface S1, and the second surface S2 includes a spherical surface 13 and a third diffraction structure. The key structure 23 is formed on the third aspheric surface 13, wherein Third, the clock structure 23 corresponds to the first diffraction structure 21. A %, , , and port include the further embodiment of the present invention, the multi-focus objective lens "- surface 81 and a second surface illusion. a first surface-dipole-aspherical surface U, a second non-spherical surface = and a second diffraction structure 22, the second diffraction structure 2: upper, the second diffraction grating is formed on the second aspherical surface d The surface S2 is the back surface of the first surface S1, the second surface Μ includes a fourth aspherical surface 14 and a fourth diffraction structure Μ, and the structure 24 is formed in the fourth aspherical surface M: The four-diffraction junction 0949-A21811TWF(N2); P51950098TW; the Lemon 13 1313363 structure 24 corresponds to the second diffraction structure 22. Although the present invention has been described above in terms of the preferred embodiments thereof, it is not intended to limit the invention, and those skilled in the art can make some modifications and refinements without departing from the spirit and scope of the invention. Therefore, the scope of the invention is defined by the scope of the appended claims.
0949-A21811TWF(N2);P51950098TW;Lemon 1313363 【圖式簡單說明】 第1圖係顯示本發明之多焦物鏡; 第2a圖係完整顯示本發明之多焦物鏡的第一表面; 第2b圖係完整顯示本發明之多焦物鏡的第二表面; 第3圖係顯示本發明的另一實施例; 第4圖係顯示本發明的又一實施例。 【主要元件符號說明】 鲁 11〜第一非球面 12〜第二非球面 13〜第三非球面 14〜第四非球面 21〜第一繞射結構 22〜第二繞射結構 23〜第三繞射結構 24〜第四繞射結構 ® 100〜多焦物鏡 200〜碟片 A1〜第一區域 A2〜第二區域 A3〜第三區域 A4〜第四區域 S1〜第一表面 S2〜第二表面 0949-A21811TWF(N2);P51950098TW;Lemon 150949-A21811TWF(N2); P51950098TW; Lemon 1313363 [Simplified description of the drawings] Fig. 1 shows the multifocal objective lens of the present invention; Fig. 2a shows the first surface of the multifocal objective lens of the present invention; Fig. 2b The second surface of the multifocal objective lens of the present invention is fully shown; Fig. 3 is a view showing another embodiment of the present invention; and Fig. 4 is a view showing still another embodiment of the present invention. [Description of main component symbols] Lu 11 to first aspherical surface 12 to second aspherical surface 13 to third aspherical surface 14 to fourth aspherical surface 21 to first diffraction structure 22 to second diffraction structure 23 to third winding The radiation structure 24 to the fourth diffraction structure® 100 to the multi-focus objective lens 200 to the disc A1 to the first area A2 to the second area A3 to the third area A4 to the fourth area S1 to the first surface S2 to the second surface 0949 -A21811TWF(N2); P51950098TW; Lemon 15
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| TW95145638A TWI313363B (en) | 2006-12-07 | 2006-12-07 | Multi-focus objective lens |
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