TW200533957A - Variable optical element - Google Patents

Variable optical element Download PDF

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Publication number
TW200533957A
TW200533957A TW94106623A TW94106623A TW200533957A TW 200533957 A TW200533957 A TW 200533957A TW 94106623 A TW94106623 A TW 94106623A TW 94106623 A TW94106623 A TW 94106623A TW 200533957 A TW200533957 A TW 200533957A
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Taiwan
Prior art keywords
optical
lens
fluid
optical element
window
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TW94106623A
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Chinese (zh)
Inventor
Bernardus Hendrikus Wilhelmus Hendriks
Stein Kuiper
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Koninkl Philips Electronics Nv
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Publication of TW200533957A publication Critical patent/TW200533957A/en

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    • GPHYSICS
    • G02OPTICS
    • G02BOPTICAL ELEMENTS, SYSTEMS OR APPARATUS
    • G02B3/00Simple or compound lenses
    • G02B3/12Fluid-filled or evacuated lenses
    • G02B3/14Fluid-filled or evacuated lenses of variable focal length
    • GPHYSICS
    • G02OPTICS
    • G02BOPTICAL ELEMENTS, SYSTEMS OR APPARATUS
    • G02B26/00Optical devices or arrangements for the control of light using movable or deformable optical elements
    • G02B26/004Optical devices or arrangements for the control of light using movable or deformable optical elements based on a displacement or a deformation of a fluid
    • G02B26/005Optical devices or arrangements for the control of light using movable or deformable optical elements based on a displacement or a deformation of a fluid based on electrowetting

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  • Physics & Mathematics (AREA)
  • General Physics & Mathematics (AREA)
  • Optics & Photonics (AREA)
  • Lenses (AREA)

Abstract

The invention provides an optical element (204) having a chamber (208) with an entrance window (209), an exit window (210). The chamber comprises two substantially immiscible fluids (212, 213) that are in contact over a meniscus (214). At least one of the entrance window (209) or exit window (210) comprises a surface with a curvature (217,219) that is in contact with one of the fluids. The Abbe-number of the material of this at least one of the entrance and exit windows (209, 210) has a substantial difference with the Abbe-number of the fluid being in contact with the surface having a curvature. By selecting and tuning several optical parameters such as radius, refractive index and Abbe numbers related to these windows and fluids it is possible to design a substantially achromatic optical element or optical lens system.

Description

200533957 九、發明說明: 【电明所屬之技術領域】 本發明係關於一種包括在一彎月面上接觸之一第一流體 與一第二流體之可變光學元件,關於包括此類光學元件之 透鏡系統’關於包括此類光學透鏡系統之成像系統,以及 關於設計此類可變光學元件、透鏡系統及光學成像系統之 方法。 【先前技術】200533957 IX. Description of the invention: [Technical field to which Dianming belongs] The present invention relates to a variable optical element including a first fluid and a second fluid in contact with a meniscus. Lens System 'pertains to imaging systems including such optical lens systems, and to methods of designing such variable optical elements, lens systems, and optical imaging systems. [Prior art]

可變透鏡係一裝置,在該裝置中,能夠以可控方式調整 透鏡之一或多種性質,例如可以改變透鏡之焦距或位置。 相機杈組之影像感測器之一般發展趨勢係其解析度不斷A variable lens is a device in which one or more properties of the lens can be adjusted in a controlled manner, such as changing the focal length or position of the lens. The general development trend of the image sensor of the camera group is its continuous resolution

增加。最初·係低解析度感測器,例如100k像素等級之CIF 影像感測器與300k像素等級之VGA影像感測器,目前則有 高解析度之百萬像素影像感測器。該等較高解析度不僅需 要光學透鏡系統之調焦功能,以便能在整個物距範圍(例 如1〇⑽至無窮遠)内使用高解析度,其還需要包含至少兩 非球面透鏡之透鏡系統,以符合其他光學參數要求,例如 與像差有關之參數。 ^國際專射請案第WC> 娜938G號中,揭示一種 二猎由曲透鏡封閉之電濕透鏡作為可變透鏡系統之相 果組。所施加之電壓控制該電濕透鏡之兩流體之間 面之:狀’並因此得以控制該電濕透鏡之光學功率。 此’猎由在成像系統中使用此電濕透鏡,可變的彎月面 徑能夠滿足含周隹亜本 、, 7弓月面, 求’亚因此可消除影像之散焦。由於, 100130.doc 200533957 濕透鏡之彎月面會w p a & , ^ 、貝上係球形,所以其不會對消除影 光學像差,例如缝开彡德兰 、 羞形像差、變形及球面像差,有明顯increase. Initially, it was a low-resolution sensor, such as a 100k-pixel CIF image sensor and a 300k-pixel VGA image sensor. At present, there are high-resolution megapixel image sensors. These higher resolutions not only require the focusing function of the optical lens system in order to be able to use high resolution over the entire object distance range (for example, 10 ° to infinity), they also require a lens system including at least two aspherical lenses To meet other optical parameter requirements, such as those related to aberrations. ^ International Patent Application No. WC > Na 938G discloses a kind of electrowetting lens enclosed by a curved lens as a result group of a variable lens system. The applied voltage controls the shape of the surface between the two fluids of the electrowet lens and thus the optical power of the electrowet lens can be controlled. This ‘hunting’ uses this electrowetting lens in the imaging system, and the variable meniscus diameter can meet the 7 meniscus including Zhou Yanben, Qiu ’, so it can eliminate the defocus of the image. Since the meniscus of the wet lens 100100.doc 200533957 will be wpa &, ^, the spheroid is spherical, so it will not eliminate aberrations, such as slitting Adeland, shame aberration, deformation and Spherical aberration

用。 、F 由於光學表面之數目有限’該已知電濕透鏡之放大、平 場及像差減小潛力也有限。因此,該模組僅適於低解析度 相機,例如CIF與VGA。對於具有較高解析度感測器之ς 機’例如500 k像素等級之⑻VGA影像感測器、! Μ像素等 鲁⑨之XGA影像感測器及百萬像素裝置,此性能無法滿足需 要。 在美國專利申請案第Us 2〇〇1/〇17985號中,揭示一相機 透鏡堆’其包括具有平坦入口與出口窗之電濕透鏡,並 包括位於該電濕透鏡之前與之後之不同透鏡群組。透過移 動第-透鏡群組執行調焦。該電濕透鏡具有變焦功能。其 對其他光學性能之改善不起作用。 以上該等揭示案無一能解決消除色差問題,而此係達成 • 成像透鏡系統之優良光學色彩校正所需要的。 消除色差係減小光學系統之色散光學功率。色散光學功 率係由於光學元件之材料之折射率〇對光之波長之依賴所 致。py貝數v可表達該波長相依性·· ηΜ-η(λα) ⑴ 此處nU,.)係弋=587.6 nm、心=486」nm及夾=656 3 nm時波 長4.處之折射率。必須良好地校正色散,以獲得較高光學 品質。傳統透鏡系統使用易於模糊之光栅結構或昂貴的雙 合透鏡組件以進行色彩校正。 100130.doc 200533957 〜% %错由將普诵 折射透鏡與衍射透鏡組合在一起實現色差消除。對於雔诉 透鏡,形成透鏡之兩元件通常具有實質上相同之折射二= 及不同之阿貝數。為實現色差消㉟,選擇該等兩元件^ 等式: ΚΙ K2 一 +-= 〇 Vi V2 學功率!〇與〖2以及阿貝數Vmv2,使該等參數滿足以下 式: (2) 消除折射透鏡之色差之另一方法係藉由增加 衍射透鏡之阿貝數僅依賴於廡田+ %仕 、、、°構 只数偟依賴於應用中所使用之波長範圍,. 對於相機模έ且I $夕、士 & 一 m 3 452广、、且要求之波長#圍"可貝數4有固定值 二述用於提供消除色差之透鏡系統之兩種方法都不適於 琶濕透鏡’此係由於在電 私”、、運鏡中先學功率隨兩流體之 ^ ♦月面之半徑之—介而妈:# , 文化而、交化,其中該彎月面之半徑依 賴於所施加之雷厭 品l、丄、 土,上述該等方法僅適用於具有固定光 学功率之透鏡。 未預先公開之歐洲專利申請案第EP 04100100.9號 二:者^考一為PHNLG4GGG8)中,提出—種具有消色差use. Because of the limited number of optical surfaces, the known electrowetting lens has limited potential for magnification, flat field, and aberration reduction. Therefore, this module is only suitable for low-resolution cameras, such as CIF and VGA. For cameras with higher resolution sensors, such as VGA image sensors at 500 k pixels, M pixel and other Lu Xun's XGA image sensor and megapixel device, this performance can not meet the needs. In U.S. Patent Application No. 20001 / 〇17985, a camera lens stack is disclosed that includes an electrowetting lens with flat entrance and exit windows, and includes a difference between before and after the electrowetting lens. Lens group. Focusing is performed by moving the-lens group. The electrowetting lens has a zoom function. It has no effect on the improvement of other optical properties. None of the above disclosures can solve the problem of eliminating chromatic aberration, which is required to achieve excellent optical color correction of the imaging lens system. Eliminating chromatic aberration is to reduce the dispersion optical power of the optical system. Dispersive optical power is due to the dependence of the refractive index of the material of the optical element on the wavelength of light. The py shell number v can express this wavelength dependence. ηΜ-η (λα) ⑴ where nU ,.) is 弋 = 587.6 nm, heart = 486 ″ nm and clip = 656 3 nm at a wavelength of 4. . Dispersion must be well corrected for higher optical quality. Conventional lens systems use grating structures that are easily blurred or expensive double-lens components for color correction. 100130.doc 200533957 ~%% The chromatic aberration can be eliminated by combining a common refraction lens and a diffractive lens. For a complaint lens, the two elements forming the lens usually have substantially the same refractive index = and different Abbe numbers. In order to eliminate chromatic aberration, these two elements are selected ^ Equation: ΚΙ K2-+-= Vi Vi2 Learn power! 〇 2 and Abbe number Vmv2, so that these parameters meet the following formula: (2) Elimination of refraction Another method of chromatic aberration of the lens is to increase the Abbe number of the diffractive lens by only relying on Putian +% ,,, and °. The number depends on the wavelength range used in the application. For camera mode and I $ 夕 , 士 &一; m 3 452 wide, and the required wavelength # circle " Kebei 4 has a fixed value. Second, two methods for providing a lens system to eliminate chromatic aberration are not suitable for a wet lens. This is because in the "electric private", the mirror first learns the power of the two fluids ^ ♦ the radius of the lunar surface-Jie and Ma: #, cultural and cultural, where the radius of the meniscus depends on the applied The above-mentioned methods are only applicable to lenses with fixed optical power. European Patent Application No. EP 04100100.9 No. 2: Unknown (PHNLG4GGG8) is proposed as follows: Achromatic

Mf 透鏡。其揭示,可藉由調整所涉及之液體之光 學性質(例如阿貝教、y r 、)例如在該等液體中混合或溶解精心 遠擇之物質,央斜^么 ^亥不統進行色差消除。基於流體之可變 還鏡構成可實爾#、、 、色差消除之透鏡系統。例如,為使該等流 體之間之介面消^ &圣 ^ a ,, Λ 除色差,流體「i」與「η」之折射率η及 阿貝數V必須遵w 貝遷從以下關係: 100130.doc 200533957 % -1 對於具有平坦入口與出口窗表面之電濕透鏡,此僅僅足 以使流體-流體介面消除色差。對於具有彎曲人口與出口 固表面之電濕透鏡,此會導致非最佳之消色差性質。 本發明之一目的係提供具有實質上之消色差性質之可變 透鏡糸統。 【發明内容】 本發明之目的係藉由一光學元件達成,纟中該光學元件 具有一至,該室具有一入口窗、一出口窗以及縱向延伸穿 :該室之-光軸,|亥室包含一第一流體與一第二流體,該 第〃IL體與该第二流體在橫向延伸穿過該光軸之彎月面上 接觸’該等流體實質上係不互溶流體,該入口窗或出口窗 _已括與5亥苐一或該第二流體中之一流體接觸 之一表面,該表面具有曲率,該入口與出口窗中之該至少 囱之材料之阿貝數與接觸具有該曲率之表面之流體之阿 貝數具有實質之差異。 當該彎曲窗表面與該接觸流體之阿貝數實質上相等時, 則不可能使用該介面使光學元件或整個光學透鏡系統消除 色差。如果該彎曲窗表面與該接觸流體之阿貝數實質上不 同,則可在總體設計中使用該等光學性質來達成實質上消 除色差之光學透鏡系統。 光學透鏡系統之最終整體設計通常係成像之所有方面之 取佳化之結果,以滿足,例如與解析度、視場、最大主光 線角及光學像差(例如變形、球面像差及色差)有關之系統 100130.doc 200533957 規格。 因此’有必要藉由’例如選擇合適之透鏡材料或在流體 中混合或溶解精心選擇之物質,來調整所涉及之流體與透 鏡材料之光學性質,以便可使整個光學透鏡系統實質上消 除色差,並避免使用昂貴的傳統消色差方法。 當電濕透鏡之入口及/或出口窗允許使用彎曲表面時, 也可根據系統之整體光學設計調整該等曲率,以最佳化其 φ 他像差,例如變形、球面像差或場曲率。例如,彎曲表面 可以係球面或非球面。 【實施方式】 圖1概略顯示依據本發明之一光學透鏡系統。該光學透 鏡系統(200)包括兩透鏡群組201與202以及位於第一與第二 透鏡群組之間之光圈203。該第一透鏡群組2〇1包括可變透 鏡,例如電濕透鏡204,並用作可變焦距透鏡。該第二透 鏡群組202使用透鏡220決定光學放大倍數,以使影像之大 • 小與位於該光學透鏡系統之後之影像感測器205之大小相 匹配。另外’其也藉由平場透鏡206減小主光線角。使用 透明覆盍物207,例如平面平行板,覆蓋影像感測器2〇5。 電濕透鏡204具有室208,該室208具有入口窗209與出口 窗210以及縱向延伸穿過該室之光軸211。該室包含在橫向 穿越該光軸之彎月面214上接觸之第一流體21 3與第二流體 212。與第一流體213接觸之入口窗217之表面之曲率半徑 具有與δ亥弟一及弟一^流體之間之彎月面214之曲率相同之 符號。另外,與第二流體212接觸之出口窗21 9之表面之曲 100130.doc 200533957 率半輕具有與該第一及第二流體之間之彎月面214之曲率 相同之符號。如此即可減小高度。該等窗以及該等透鏡可 由玻璃、塑膠或其他合適之材料製造。 所使用之該等兩流體212與213實質上係不互溶流體。第 -流體2"係電絕緣流體,例如矽油或烯烴(此處稱為油), 而第二流體212係導電流體,例如含有鹽溶液之水。該等 兩流體較佳具有相同密度,以便透鏡操作時與其方向無 關,即不依賴於重力對流體之影響。依據光學系统之: 要,也可按以下方法進行設計,即第一流體係電絕緣: 體,而第二流體係導電流體。 該室中之第-電極215通常係具有m2〇贿之間之半徑 之圓柱,但根據該室之形狀與幾何結構,㈣—電極也= 具有其他形狀’例如圓錐形。藉由絕緣塗層,例如可由覆 盍AF-1600疏水頂部塗層之聚對二甲苯_n形成,使電極us 與該等流體電絕緣。第二電極216(通常係環形)配置於該室 之末端,在此例中靠近出口窗。配置此第二電極Η二吏 其至少-部分與第二流體212連接。該連接可能係直接連 接,或者也可能係經由薄絕緣層之電容性耦合。 當未向電極215與216施加電壓時,該等流體在具有曲率 之彎月面214上相接觸。藉由向該等電極施加電壓,可改 變該彎月面,使其具有更小或更大之曲率半徑。另外,依 據該室之組態與該等電極之配置,可實現複數 : 月面形狀。 3 當入口或出口窗之至少一窗使用彎曲表面時,該光學元 100130.doc -10- 200533957 件之該等表面可能參與整體光學設計。該等窗之曲率可能 闕光學設計之額外數目之自由度,以最佳化光學透鏡系 統之光學性能。可能藉由應用非球面表面,以及使電濕透 鏡、使用其之透鏡群組或甚至整個光學透鏡系統消除色差 而調整該等窗之曲率,以進行像差校正。 該光學元件可能用於可包括更多具有光學功率之透鏡之 - A學⑽系統。本發明之目的係,該光學元件不僅用作調 .籲 纟或變焦裝置,而且其還可能用作減小光學透鏡系統中之 其他元件之色差之元件。 彎曲窗與接觸流體之材料之折射率差異向該介面提供一 些$學功率。兩種材料之實質上相等之折射率會導致該介 面實質上不具有光學功率。但是,纟以上兩種情況下,阿 貝數之差異都會因不同波長而導致光學功率之不同。不同 波長所致之光學功率之差異可用於校正系統之色差。 、L #相機透鏡係設計為使用正透鏡,該正透鏡由玻璃 籲《塑膠製造,具有正半徑,並接觸空氣。正常條件下之空 氣具有大約90之高阿貝數。此僅會對色差產生正面影響。 例如,藉由在雙合透鏡中應用具有與設計匹配之合適介面 半徑以及折射率及阿貝數之埋藏式透鏡一透鏡介面,可以 引起對補償之不利影響。可使用之玻璃與塑膠之數目係有 _ 限的’且使用雙合透鏡不具有成本效益。 - 在本發明中,使用流體之光學參數與窗材料之光學性質 之組合來獲得具成本效益並實質上消除色差之光學透鏡系 統。該光學透鏡系統可能僅包括該光學元件,或者包括該 I00i30.doc 200533957 光學元件以及一或多個折射或衍射元件。 通常,依據用作流體之油之選擇,該油之折射率可能在 1·25與1·65之間變化。同樣,依據添加之鹽之類型與數 量,用作另一流體之鹽溶液可能具有在^^與丨·%之間變 化之折射率。類似地,在該油或鹽溶液中使用添加劑可改 變流體之阿貝婁丈。此意味著有可能在較大範圍内調整所應 用之流體之光學參數,以滿足有關色差之設計。Mf lens. It was revealed that by adjusting the optical properties of the liquids involved (eg Abbey, yr, etc.), such as mixing or dissolving carefully selected substances in these liquids, the eccentricity is not uniformly eliminated. The fluid-based variable return lens constitutes a lens system capable of eliminating chromatic aberration. For example, in order to eliminate the interface between these fluids, the refractive indices η and Abbe number V of the fluids "i" and "η" must follow the following relationship: 100130.doc 200533957% -1 For electrowetting lenses with flat entrance and exit window surfaces, this is just enough to make the fluid-fluid interface eliminate chromatic aberration. For electrowetting lenses with curved populations and solid exit surfaces, this can lead to sub-optimal achromatic properties. It is an object of the present invention to provide a variable lens system having substantially achromatic properties. [Summary of the invention] The object of the present invention is achieved by an optical element, wherein the optical element has one to one, the chamber has an entrance window, an exit window, and a longitudinally extending passage: the optical axis of the chamber, A first fluid and a second fluid, the third IL body and the second fluid are in contact on a meniscus extending laterally across the optical axis, 'these fluids are essentially immiscible fluids, the inlet window or outlet The window has included a surface that is in contact with one of the fluids of the second fluid or the second fluid, the surface has a curvature, and the Abbe number of the at least one of the materials in the inlet and outlet windows and the contact has the curvature. The Abbe number of the fluid on the surface is substantially different. When the curved window surface is substantially equal to the Abbe number of the contact fluid, it is impossible to use the interface to eliminate chromatic aberration of the optical element or the entire optical lens system. If the curved window surface is substantially different from the Abbe number of the fluid in contact, the optical properties can be used in the overall design to achieve an optical lens system that substantially eliminates chromatic aberration. The final overall design of an optical lens system is usually the result of optimization of all aspects of imaging to meet, for example, the resolution, field of view, maximum principal ray angle, and optical aberrations (such as distortion, spherical aberration, and chromatic aberration) System 100130.doc 200533957 specifications. Therefore, it is necessary to adjust the optical properties of the fluid and lens materials involved by, for example, selecting appropriate lens materials or mixing or dissolving carefully selected substances in a fluid, so that the entire optical lens system can substantially eliminate chromatic aberration, And avoid using expensive traditional achromatic methods. When the entrance and / or exit window of the electrowetting lens allows the use of curved surfaces, these curvatures can also be adjusted according to the overall optical design of the system to optimize other φ aberrations, such as distortion, spherical aberration, or field curvature . For example, the curved surface can be spherical or aspherical. [Embodiment] FIG. 1 schematically shows an optical lens system according to the present invention. The optical lens system (200) includes two lens groups 201 and 202 and an aperture 203 between the first and second lens groups. The first lens group 201 includes a variable lens, such as an electrowetting lens 204, and functions as a variable focal length lens. The second lens group 202 uses the lens 220 to determine the optical magnification so that the size of the image matches the size of the image sensor 205 located behind the optical lens system. In addition, it also reduces the principal ray angle by the flat field lens 206. A transparent cover 207, such as a flat parallel plate, is used to cover the image sensor 205. The electrowetting lens 204 has a chamber 208 having an entrance window 209 and an exit window 210 and an optical axis 211 extending longitudinally through the chamber. The chamber contains a first fluid 21 3 and a second fluid 212 that are in contact on a meniscus 214 that crosses the optical axis laterally. The radius of curvature of the surface of the entrance window 217 that is in contact with the first fluid 213 has the same sign as the curvature of the meniscus 214 between the? In addition, the curvature of the surface of the outlet window 219 that is in contact with the second fluid 212 has the same sign as the curvature of the meniscus 214 between the first and second fluids. This reduces the height. The windows and the lenses may be made of glass, plastic or other suitable materials. The two fluids 212 and 213 used are essentially immiscible fluids. The first fluid 2 is an electrically insulating fluid, such as silicone oil or olefin (herein referred to as an oil), and the second fluid 212 is a conductive fluid, such as water containing a salt solution. The two fluids preferably have the same density so that the lens is independent of its direction when operating, that is, it does not depend on the effect of gravity on the fluid. According to the requirements of the optical system, it can also be designed according to the following methods, that is, the first stream system is electrically insulated, and the second stream system is conductive fluid. The first-electrode 215 in the chamber is usually a cylinder with a radius of between m2 and 20 mm, but according to the shape and geometry of the chamber, the 电极 -electrode = also has other shapes' such as a conical shape. The electrode us can be electrically insulated from these fluids by an insulating coating, such as poly-xylene_n coated with a hydrophobic top coating of AF-1600. A second electrode 216 (usually ring-shaped) is disposed at the end of the chamber, in this case near the exit window. This second electrode is configured to be at least partially connected to a second fluid 212. The connection may be a direct connection, or it may be a capacitive coupling via a thin insulation layer. When no voltage is applied to the electrodes 215 and 216, the fluids come into contact on the meniscus 214 having a curvature. By applying a voltage to the electrodes, the meniscus can be changed to have a smaller or larger radius of curvature. In addition, according to the configuration of the chamber and the configuration of the electrodes, multiple shapes can be realized: lunar surface. 3 When at least one of the entrance or exit windows uses curved surfaces, the surfaces of the optical element 100130.doc -10- 200533957 may participate in the overall optical design. The curvature of these windows may allow an additional number of degrees of freedom in optical design to optimize the optical performance of the optical lens system. It is possible to adjust the curvature of these windows by applying aspherical surfaces, and eliminating chromatic aberrations by electrowetting lenses, lens groups using them, or even the entire optical lens system to perform aberration correction. This optical element may be used in A-systems that can include more lenses with optical power. It is an object of the present invention that the optical element is used not only as an adjusting or zooming device, but also as an element for reducing chromatic aberration of other elements in an optical lens system. The difference in refractive index between the curved window and the material in contact with the fluid provides the interface with some learning power. A substantially equal refractive index of the two materials results in the interface having substantially no optical power. However, in the above two cases, the difference in Abbe number will result in different optical power due to different wavelengths. The difference in optical power caused by different wavelengths can be used to correct the chromatic aberration of the system. The L # camera lens is designed to use a positive lens, which is made of glass plastic and has a positive radius and contacts the air. Air under normal conditions has a high Abbe number of approximately 90. This only has a positive effect on the color difference. For example, the use of a buried lens-lens interface with a suitable interface radius and refractive index and Abbe number that matches the design in a doublet lens can cause adverse effects on compensation. The number of glasses and plastics that can be used is limited 'and using a doublet lens is not cost effective. -In the present invention, a combination of the optical parameters of the fluid and the optical properties of the window material is used to obtain a cost-effective optical lens system that substantially eliminates chromatic aberration. The optical lens system may include only the optical element, or the I00i30.doc 200533957 optical element and one or more refractive or diffractive elements. Generally, depending on the choice of the oil used as the fluid, the refractive index of the oil may vary between 1.25 and 1.65. Similarly, depending on the type and amount of salt added, a salt solution used as another fluid may have a refractive index that varies between ^^ and 丨 ·%. Similarly, the use of additives in the oil or saline solution can alter the abeloitic of the fluid. This means that it is possible to adjust the optical parameters of the applied fluid within a wide range to meet the design of chromatic aberration.

為了能夠在a光學透鏡系統設計選擇合適之透鏡材料與 流體時有充足之自由,較佳係允許大範圍之折射率。例 如,此可導致用於窗及接觸流體之材料之折射率之實質差 。呈式(3)中對消除色差之要求也可表示為: 此處Δν係材料讀1之阿貝數之差,Δη係材料η與i之折射率 之差。允許折射率之實質差異也要求窗與流體之阿貝數之 實質差異’以最佳化實質上消除色差之電濕透鏡之設計。 還可能選擇最佳化窗、流體及彎曲之材料,以實質上、、肖 除整個光學透鏡系、統之色差。在該情況下,例>,必_ 光學透鏡系統中之所有表面調整方程式⑺中給出之要求。 因Hf鏡之統設計之要求係: y^L, v -ij 如丨 -1) 此處K i係光學功率, 存在於光學系統中之 折射率與阿貝數分別In order to be able to have sufficient freedom in selecting a suitable lens material and fluid in the design of an optical lens system, it is preferable to allow a wide range of refractive indices. For example, this can lead to a substantial difference in refractive index of the materials used for windows and fluids. The requirement for eliminating chromatic aberration in the formula (3) can also be expressed as: Here Δν is the difference between the Abbe number of the material reading 1 and Δη is the difference between the refractive indices of the materials η and i. Allowing a substantial difference in refractive index also requires a substantial difference in the Abbe number of the window and the fluid 'to optimize the design of an electrowetting lens that substantially eliminates chromatic aberration. It is also possible to choose materials that optimize windows, fluids and bends to substantially eliminate the chromatic aberrations of the entire optical lens system. In this case, Example >, the requirements given in all surface adjustment equations in the optical lens system. The requirements for the uniform design of the Hf mirror are: y ^ L, v -ij such as 丨 -1) where K i is the optical power, and the refractive index and Abbe number existing in the optical system are different.

Vi係傳統透鏡元件i之阿貝數,j計算 所有流體彎月面之總和。第一流體之 係Hj與V」,第二流體之折射率與阿貝 100130.doc -12- 200533957 數分別係111 + 1與\^· , ^ α J匕、ν』·Μ,而穹月面之半徑係Ri。 由於具有蠻曲本 表面之與接觸流體之阿貝數之間存在較 大差異戶斤以权正裝置或系統之色差較為容易。其也允許 為具有光學功率之表面使用較小半徑。 因此,呈右縷从* /、蜀弓曲表面之窗與接觸流體之阿貝數之差異較 佳係大於5。 具有4曲表面之窗與接觸流體之阿貝數之差異大於10則 更佳。 圖1顯示依據本發明之設計之範例。其係f/2.8,f=3 97 mm自動聚焦相機透鏡,該透鏡具有66度的視場、⑽_ 的入射光瞳以及6·5 mm的高度,與百萬像素型影像感測器 組合使用。所有的透鏡(2〇9、21〇、22〇及2〇6)都具有非球 面表面,以最佳化影像之光學品質。彎月面214實質上係 球面。電濕透鏡204之封閉塑膠透鏡2〇9與21〇之阿貝數係 55.8,其折射率在56〇 nm波長處大約係1532。導電流體 • 212包括鹽水,其阿貝數為38並在56〇 nm波長處具有1376 之折射率,而第一不導電流體213(其係矽油)之阿貝數係 28,並在560 nm波長處具有!·552之折射率。藉由正確選 擇透鏡之半徑,可使該光學系統實質上消除色差。 圖2顯示依據以上設計之光學透鏡系統之波前像差。圖 中針對490 nm、560 nm& 625 nm三種波長繪出以微米為單 位之波前像差W分別相對於正規化之入射光瞳座標卜與巧 之圖形。在圖2a中,其係針對〇度視場角顯示,在圖几 中’其係針對大約3 3度之視場角顯示。兩圖中垂直方向之 100130.doc -13 - 200533957 最大刻度都係50微米。該等圖式顯示,不同波長之像差具 有同一趨勢,不同波長間之像差差異很小,足以獲得實質 上消除像差之光學透鏡系統。 圖3顯示依據以上設計之光學透鏡系統之多色光學傳遞 函數之計算模數,其係對三個相應波長490 nm、560 nm及 625 nm平均之結果,該等模數與在Px方向與Py方向都最高 達33度之數字視場角之每毫米線數成函數關係。其顯示線 301與302之兩群組。線3〇1之群組係2〇、以及”度之”方 向之多色光學傳遞函數。線3〇2之群組係〇、1〇、2〇、29及 33度之Ρχ方向以及〇與1〇度角度之卜方向之多色光學傳遞 函數。其顯示,高達75線/毫米之調變足以滿足百萬像素 成像應用,例如用於行動電話中的相機。 在以上範例設計中,入口與出口窗兩者之所有表面都具 有表面曲率,以便能夠減少像差,例如變形及球面像差, 以及同度。依據整體系統要求,也可能僅入口或出口窗之 單表面具有曲率,以貫現足夠低之像差層級以及足夠低 之色差。 圖4Α顯示可變焦距影像捕捉裝置421之使用,其中該裝 置42 1使用依據本發明之光學透鏡系統彻。可能從影像感 二杰405獲取測量信號,例如調焦信號,#中該影像感測 。〇5使用之技術在使用影像感測器之相機中廣泛使用。 4測$信號係用作電壓驅動器422之輸入信號。該電壓驅 動器之輸出連接至光學透鏡系統彻之電濕透鏡404之電極 415與416,以控制彎月面414之形狀。圖4Β顯示使用整合 100130.doc 200533957 例。亦可使用其他整合位置。 - 藉由調整所涉及之流體與透鏡材料之光學性質,有可能 使電濕透鏡實質上消除色差並避免使用昂貴的傳統消除色 差方法。例如,可藉由選擇透鏡之合適材料,或者在流體 中混合或溶解精心選擇之物質,達成該調整。 很明顯,料熟悉技術人士,藉由考慮其他光學介面, 本方法還可用於使包括此一電洚 ^濕透鏡之透鏡系統實質上消 除邑差。 該光學元件非常適用於先學类 錢與用於相機應用之 片=Γ例如,該等相機應用可以係電影或靜止照 =式相機,或可拍攝電影或靜止照片之手機相機。尤 學口併且女, 于機口之,對小尺寸、具有高光 〜貝、具有低能量消耗並且耐用之裝置之需求 :二於沒有機械移動零件,例如調焦與變焦零件,使‘ 依據本發明之光學元杜 、 件之光與锈浐 、、。使用依據本發明之光學元 予透鏡錢與成料統可滿足該等需求。 雖然上述說明伟κ、吞 手機之相機… 於小型行動相機系統(例如用於 其他光學系統(例如顯微但本發明還可用於使 減小像差以及減小高度。 ⑺J月I示邑差、 在光學儲存應用中,Vi is the Abbe number of the conventional lens element i, and j calculates the sum of all fluid meniscus. The system of the first fluid is Hj and V ", the refractive index of the second fluid and Abbe's 100130.doc -12- 200533957 are respectively 111 + 1 and \ ^ ·, ^ α Jd, ν ′ · M, and the dome The radius of the face is Ri. Because there is a large difference between the surface with a rough song and the Abbe number in contact with the fluid, it is easier to correct the color difference of the device or system. It also allows the use of smaller radii for surfaces with optical power. Therefore, the difference between the window with a right strand from the surface of Shu Gong curved surface and the Abbe number in contact with the fluid is preferably greater than 5. The difference between a window with a 4-curved surface and an Abbe number in contact with the fluid greater than 10 is more preferable. Figure 1 shows an example of a design according to the invention. It is a f / 2.8, f = 3 97 mm autofocus camera lens with a field of view of 66 degrees, an entrance pupil of 瞳 _, and a height of 6.5 mm. It is used in combination with a megapixel image sensor. All lenses (209, 21, 22, and 20) have aspherical surfaces to optimize the optical quality of the image. The meniscus 214 is essentially spherical. The closed plastic lenses 209 and 21 of the electrowetting lens 204 have an Abbe number of 55.8 and a refractive index of about 1532 at a wavelength of 56 nm. Conductive fluid • 212 includes saline, which has an Abbe number of 38 and a refractive index of 1376 at a wavelength of 56 nm, while the first non-conductive fluid 213 (which is a silicone oil) has an Abbe number of 28 and a wavelength of 560 nm Everywhere! · Refractive index of 552. By properly selecting the lens radius, the optical system can substantially eliminate chromatic aberration. FIG. 2 shows the wavefront aberrations of the optical lens system according to the above design. In the figure, for the three wavelengths of 490 nm, 560 nm & 625 nm, the wavefront aberration W in micrometers is plotted against the normalized entrance pupil coordinates and graphs, respectively. In FIG. 2a, it is displayed for a field angle of 0 degrees, and in FIG. 2 ', it is displayed for a field angle of about 33 degrees. 100130.doc -13-200533957 in the vertical direction of the two figures has a maximum scale of 50 microns. These figures show that the aberrations of different wavelengths have the same trend, and the difference of aberrations between different wavelengths is small enough to obtain an optical lens system that substantially eliminates aberrations. Figure 3 shows the calculated modulus of the polychromatic optical transfer function of the optical lens system based on the above design. It is the result of averaging three corresponding wavelengths of 490 nm, 560 nm, and 625 nm. These modulus and Py and Py The number of lines per millimeter of a digital field angle with a direction up to 33 degrees is a function of function. It shows two groups of lines 301 and 302. The group of lines 30 is 20, and the polychromatic optical transfer function in the direction of "degrees". The group of lines 30 is a multicolored optical transfer function of the Px directions of 0, 10, 20, 29, and 33 degrees and the directions of the angles of 0 and 10 degrees. It shows that modulations up to 75 lines / mm are sufficient for megapixel imaging applications, such as cameras used in mobile phones. In the above example design, all surfaces of both the entrance and exit windows have surface curvatures so that aberrations such as distortion and spherical aberration, and homogeneity can be reduced. Depending on the overall system requirements, it is also possible that only a single surface of the entrance or exit window has curvature to achieve a sufficiently low aberration level and a sufficiently low chromatic aberration. Fig. 4A shows the use of a variable focal length image capturing device 421, which uses the optical lens system according to the present invention. It is possible to obtain measurement signals from the image sensor Erjie 405, such as the focus signal, the image sensor in #. 〇5 The technology used is widely used in cameras using image sensors. The 4 test signal is used as the input signal of the voltage driver 422. The output of this voltage driver is connected to the electrodes 415 and 416 of the electrowetting lens 404 of the optical lens system to control the shape of the meniscus 414. Figure 4B shows an example using integration 100130.doc 200533957. Other integration locations are also available. -By adjusting the optical properties of the fluids and lens materials involved, it is possible to make electrowetting lenses substantially eliminate chromatic aberration and avoid the use of expensive traditional methods of eliminating chromatic aberration. This adjustment can be achieved, for example, by selecting a suitable material for the lens, or by mixing or dissolving a carefully selected substance in a fluid. It is obvious to those skilled in the art that by considering other optical interfaces, this method can also be used to make a lens system including such an electric lens substantially eliminate the difference. This optical element is very suitable for learning money and films for camera applications. For example, these camera applications can be movie or still photo cameras, or mobile phone cameras that can take movies or still photos. You Xuekou and women, at the mouth of the machine, the need for a small size, high light ~ shell, low energy consumption and durable devices: Second, no mechanical moving parts, such as focus and zoom parts, so The invention of the optical element, the light of the piece and the rust. The use of optical elements according to the present invention for lens money and materials can meet these needs. Although the above description is about a camera that swallows a cell phone ... for a small action camera system (such as for other optical systems (such as microscopy), the present invention can also be used to reduce aberrations and heights. In optical storage applications,

u^ , 對夕波長項取與記錄系統之需臾X 辦增加,此係由於4 彳兄之而求不 式,例如⑶、物與5:糸、“取與記錄多種碟片格 例如,所說明之本發明可用於 100130.doc ' 15- 200533957 之光學系統中之其他光學元件所致之波長相依 、、有關可Μ透鏡元件之具體實施例與範例使用電濕原u ^, the need for X-ray wavelength item retrieval and recording systems is increased. This is due to the need of 4 brothers, such as ⑶, Wu and 5: 糸, "take and record a variety of discs. For example, all The invention described can be used in 100130.doc '15- 200533957 for wavelength-dependence caused by other optical elements in optical systems, and specific embodiments and examples of M-lens elements using electrohydrogen

文又弓月面之形狀。當然,將改變兩流體之間之彎 月面开^沿2 + +X 之其他方法視為在本發明之範圍之内Wen bowed the shape of the moon. Of course, other methods of changing the meniscus opening between two fluids along 2 + + X are considered to be within the scope of the present invention

用與配置Α π , J ^ 置為以可控方式改變彎月面之形狀與位置之圓錐狀 电極配合之幫浦。The pump is configured with a conical electrode configured with Α π, J ^ to change the shape and position of the meniscus in a controlled manner.

月=外,本發明可能應用於基於流體之透鏡,藉由調整彎 位置而不係藉由調整形狀而使該透鏡運作。 【圖式簡單說明】 圖1概略顯示依據本發明之一光學透鏡系統。 ° 匕括圖2Α及圖2Β,顯示依據本發明之光學透鏡系 統設計之波前像差。 μ 圖3顯示依據本發明之光學透鏡系統設計之光學傳遞函 數對不同波長之模數。Month, the present invention may be applied to a fluid-based lens, and the lens is operated by adjusting the bending position without adjusting the shape. [Brief Description of the Drawings] FIG. 1 schematically shows an optical lens system according to the present invention. ° Figures 2A and 2B show the wavefront aberrations designed by the optical lens system according to the present invention. Fig. 3 shows the optical transfer function versus the modulus of different wavelengths designed according to the optical lens system of the present invention.

補償由應用 像差。 圖4,包括圖4Α及圖4Β,顯示包括依據本發明之具體實 施例之光學透鏡系統之可變焦距影像捕捉裝置。 【主要元件符號說明】 200 201 202 203 204 205 光學透鏡系統 透鏡群組 透鏡群組 光圈 電濕透鏡 影像感測器 100130.doc -16 - 200533957The compensation is applied by aberrations. Fig. 4, including Figs. 4A and 4B, shows a variable focal length image capturing device including an optical lens system according to a specific embodiment of the present invention. [Description of main component symbols] 200 201 202 203 204 205 Optical lens system Lens group Lens group Aperture Electro-wet lens Image sensor 100130.doc -16-200533957

206 207 208 209 210 211 212 213 214 215 216 217 219 220 400 404 405 414 415 416 421 422 423 平場透鏡 透明覆蓋物 室 入口窗 出口窗 光軸 第二流體 第一流體 彎月面 第一電極 第二電極 曲率 曲率 透鏡 光學透鏡系統 電濕透鏡 影像感測器 彎月面 電極 電極 可變焦距影像捕捉裝置 電壓驅動器 手機 W)〇 130.doc -17-206 207 208 209 210 211 212 213 214 215 216 217 219 220 400 404 405 414 415 416 421 422 423 Flat field lens transparent cover chamber entrance window exit window optical axis second fluid first fluid meniscus first electrode second electrode Curvature curvature lens optical lens system electrowetting lens image sensor meniscus electrode electrode zoom image capture device voltage driver mobile phone W) 〇130.doc -17-

Claims (1)

200533957 十、申請專利範圍: 1. 一種光學元件(204),其具有 -一室(208),其具有一入口窗(209)、一出口窗(210)以 及一縱向延伸穿過該室之光軸(2 π); 該室包括一第一流體(2 13)與一第二流體(212),在一 延伸k穿該光軸之彎月面(214)上接觸,該等流體實質上 係不互溶流體;200533957 10. Scope of patent application: 1. An optical element (204) having a room (208) having an entrance window (209), an exit window (210), and a light extending longitudinally through the room Axis (2 π); the chamber includes a first fluid (2 13) and a second fluid (212) in contact with a meniscus (214) extending through the optical axis, the fluids being essentially Immiscible fluid -忒入口窗或出口窗中之至少一窗包括與該第一或該 第二流體中其一流體接觸之一表面(217、219),該表面 具有一曲率; -亚且該入口窗與出口窗中之該至少一窗之材料之阿 貝數(Abbe-number)與接觸該具有曲率之表面之該流體之 阿貝數具有一實質差異。 2. 如請求们之光學元件,其中該阿魏之差異大於卜 3. 如請求们之光學元件’其中該阿貝數之差異大於1〇。 4. 如請求们之光學元件,其實質上係消色差光學元件。 學元件 5· -種光學透鏡系統,其包括如前述請求項中任—項之光 6. 一種光學透鏡系統,其包括如請求項!之光學元件,复 中該光學透鏡系統實質上係消色差光學透鏡系統。 :種包括如請求項卜2、3或4之光學元件之光學成像裝 8. 一種包括如請求項6之亦學读於么μ 貝6之光子透鏡糸統之光學成 9 · 一種包括如請求項7七sΑ、你 、置 員7或8之^成像裝置之行動電話。 100130.doc-At least one of the entrance or exit window includes a surface (217, 219) in contact with one of the first or second fluids, the surface having a curvature;-and the entrance window and the exit The Abbe-number of the material of the at least one window in the window is substantially different from the Abbe-number of the fluid contacting the surface having curvature. 2. If the optical element of the request, the difference between the ferrites is greater than that of Bu. 3. If the optical element of the request, the difference between the abbe numbers is greater than 10. 4. If requested, the optical element is essentially an achromatic optical element. 5-An optical lens system comprising the light of any one of the preceding claims-an optical lens system comprising an optical element as claimed in the above! The optical lens system is substantially achromatic Optical lens system. : An optical imaging device including an optical element such as item 2, 3, or 4. 8. An optical component including a photon lens system such as item 6, which is also required to be read. 6. An item including, as requested, Item 7 or 7 sΑ, you, or 7 or 8 of ^ imaging device mobile phone. 100130.doc
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