TW200912425A - Multifocal lens having a progressive optical power region and a discontinuity - Google Patents

Multifocal lens having a progressive optical power region and a discontinuity Download PDF

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Publication number
TW200912425A
TW200912425A TW97111800A TW97111800A TW200912425A TW 200912425 A TW200912425 A TW 200912425A TW 97111800 A TW97111800 A TW 97111800A TW 97111800 A TW97111800 A TW 97111800A TW 200912425 A TW200912425 A TW 200912425A
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TW
Taiwan
Prior art keywords
lens
optical power
region
power
optical
Prior art date
Application number
TW97111800A
Other languages
Chinese (zh)
Inventor
Ronald D Blum
William Kokonaski
Venkatramani S Iyer
Joshua N Haddock
Mark Mattison-Shupnick
Original Assignee
Pixeloptics Inc
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by Pixeloptics Inc filed Critical Pixeloptics Inc
Publication of TW200912425A publication Critical patent/TW200912425A/en

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Classifications

    • GPHYSICS
    • G02OPTICS
    • G02CSPECTACLES; SUNGLASSES OR GOGGLES INSOFAR AS THEY HAVE THE SAME FEATURES AS SPECTACLES; CONTACT LENSES
    • G02C7/00Optical parts
    • G02C7/02Lenses; Lens systems ; Methods of designing lenses
    • G02C7/06Lenses; Lens systems ; Methods of designing lenses bifocal; multifocal ; progressive
    • G02C7/061Spectacle lenses with progressively varying focal power
    • G02C7/063Shape of the progressive surface
    • GPHYSICS
    • G02OPTICS
    • G02CSPECTACLES; SUNGLASSES OR GOGGLES INSOFAR AS THEY HAVE THE SAME FEATURES AS SPECTACLES; CONTACT LENSES
    • G02C7/00Optical parts
    • G02C7/02Lenses; Lens systems ; Methods of designing lenses
    • G02C7/06Lenses; Lens systems ; Methods of designing lenses bifocal; multifocal ; progressive
    • G02C7/061Spectacle lenses with progressively varying focal power
    • GPHYSICS
    • G02OPTICS
    • G02CSPECTACLES; SUNGLASSES OR GOGGLES INSOFAR AS THEY HAVE THE SAME FEATURES AS SPECTACLES; CONTACT LENSES
    • G02C7/00Optical parts
    • G02C7/02Lenses; Lens systems ; Methods of designing lenses
    • G02C7/06Lenses; Lens systems ; Methods of designing lenses bifocal; multifocal ; progressive
    • G02C7/061Spectacle lenses with progressively varying focal power
    • G02C7/063Shape of the progressive surface
    • G02C7/066Shape, location or size of the viewing zones
    • GPHYSICS
    • G02OPTICS
    • G02CSPECTACLES; SUNGLASSES OR GOGGLES INSOFAR AS THEY HAVE THE SAME FEATURES AS SPECTACLES; CONTACT LENSES
    • G02C2202/00Generic optical aspects applicable to one or more of the subgroups of G02C7/00
    • G02C2202/16Laminated or compound lenses
    • GPHYSICS
    • G02OPTICS
    • G02CSPECTACLES; SUNGLASSES OR GOGGLES INSOFAR AS THEY HAVE THE SAME FEATURES AS SPECTACLES; CONTACT LENSES
    • G02C2202/00Generic optical aspects applicable to one or more of the subgroups of G02C7/00
    • G02C2202/20Diffractive and Fresnel lenses or lens portions

Abstract

Embodiments of the present invention relate to a multifocal lens having a diffractive optical power region and a progressive optical power region. Embodiments of the present invention provide for the proper alignment and positioning of each of these regions, the amount of optical power provided by each of the regions, the optical design of the progressive optical power region, and the size and shape of each of the regions. The combination of these design parameters allows for an optical design having less unwanted astigmatism and distortion as well as both a wider channel width and a shorter channel length compared to conventional PALs. Embodiments of the present invention may also provide a new, inventive far-intermediate distance zone and may further provide for increased vertical stability of vision within a zone of the lens.

Description

200912425 九、發明說明: 【發明所屬之技術領域】 本發明係關於多焦點眼科透鏡、透鏡設計、透鏡系統及 用於眼睛上、眼睛中或眼睛周圍的眼鏡產品或裝置。特定 言之,本發明係關於在多數情況下將與漸進多焦點鏡片相 關聯之不當失真、不當散光及視力損害減小至佩戴者非常 可接受之範圍的多焦點眼科透鏡、透鏡設計、透鏡系統及 眼鏡產品。 本申請案為2007年12月25曰申請且名為"具有一漸進之 光功率區域及一不連續性之多焦點鏡片(Multifocal Lens Having a Progressive Optical Power Region and a Discontinuity)" 之美國第11/964,030號的部份接續申請案,其全部内容以 引用之方式併入本文中。 本申請案主張來自以下臨時申請案之全部内容的優先權 且全部内容以引用之方式併入: 2007年3月29日申請且名為"具有一不連續性之複合增強 型漸進多焦點鏡片(Composite Advanced Progressive Addition Lens having a Discontinuity)”之美國第 60/907,367號; 2007年7月7日申請之且名為"與供應漸進之透鏡區域之 低附加功率相關聯的改進環面及球面曲率(Refined Toric & Spherical Curvatures Associated with a Low Add Power Contributing Progressive Lens Region)” 的美國第 60/924,975號; 2007年8月1日申請且名為”用於近視力及中間視力之校 正的組合光學器件(Combined Optics for Correction of Near 130295.doc 200912425 and Intermediate Vision)"的美國第 60/935,226號; 2007年8月16曰申請且名為”用以產生增強型多焦點眼鏡 片之加工的金剛石車削(Diamond Turning of Tooling to Generate Enhanced Multi-Focal Spectacle Lenses)”的美國 第 60/935,492號:· 2007年8月17日申請且名為"具有連續光功率之增強型透 鏡(Advanced Lens with Continuous Optical power)"的美國 第 60/935,573號; Ο200912425 IX. DESCRIPTION OF THE INVENTION: FIELD OF THE INVENTION The present invention relates to multifocal ophthalmic lenses, lens designs, lens systems, and eyewear products or devices for use on, in or around the eyes. In particular, the present invention relates to multifocal ophthalmic lenses, lens designs, lens systems that, in most cases, reduce inappropriate distortion, improper astigmatism, and visual impairment associated with progressive multifocal lenses to a very acceptable range for the wearer. And eyewear products. This application is filed on December 25, 2007, and is entitled "Multifocal Lens Having a Progressive Optical Power Region and a Discontinuity" Part of the continuation application of 11/964,030, the entire contents of which is incorporated herein by reference. The present application claims priority from the entire content of the following provisional application, the entire content of which is hereby incorporated by reference: Composite Advanced Progressive Addition Lens having a Discontinuity)" US 60/907,367; and July 7, 2007, entitled "" Improved toroidal and spherical curvature associated with the low additional power supplied to the progressive lens area (Refined Toric & Spherical Curvatures Associated with a Low Add Power Contributing Progressive Lens Region)" US 60/924,975; Applied on August 1, 2007 and named "Combined Optics for Correction of Near Vision and Intermediate Vision" U.S. Patent Application Serial No. 60/935,226, filed on Jan. 16, 2007, entitled,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,, The beauty of turning (Diamond Turning of Tooling to Generate Enhanced Multi-Focal Spectacle Lenses) No. 60 / 935,492: · August 17, 2007 application and entitled " has enhanced continuous optical power of the lens (Advanced Lens with Continuous Optical power) " US No. 60 / 935,573; Ο

2007年8月20日申請且名為”具有連續光功率之增強型多 焦點鏡片(Advanced Multifocal Lens with c〇ntimj〇us 〇ptical p〇wer)" 的美國第60/956,813號;及 2007年9月5日申請且名為”改進之增強型多焦點(汉^^^ Enhanced Multi-Focal)” 的美國第 6〇/97〇,〇24號。 【先前技術】 老花眼為常常伴隨變老之人眼晶狀體的調節喪失。此調 節喪失首先導致不能夠聚焦於近距離物件上且後來導致不 能夠聚焦於中間距離物件上。用於校正老花眼之標準工具 為多焦點眼科透鏡。多焦點透鏡為用於校正一距離範圍: 之聚焦問題的具有一個以上焦距(亦即,光功率)之透鏡。 多焦點眼科透鏡借助於料鏡之區劃分為不同光功率之區 域來工作。通常,位於透鏡之上部部分中之相對大區校正 遠距離視力誤差(若存在)。位於透鏡之底部部分中之較小 =提供額外光功率以用於校正由老花眼所引起的近距離視 力誤差。多焦點透鏡亦可含有位於透鏡之中間部分附近的 130295.doc 200912425 區域,其提供額外光功率以用於校正中間距離視力誤差。 多焦點透鏡可由形成連續或不連續光功率之連續或不連續 表面組成。 不同光功率之區域之間的過渡可為突變的(如在具有雙 焦點及三焦點透鏡的情況下)或為平滑及連續的(如在具有 漸進多焦點鏡片的情況下)。漸進多焦點鏡片為包含自透 鏡之遠距離區至透鏡之下部部分中之近距離區的連續增加 之正屈光光功率之梯度的 · 〜 "丁〜JHJ /干US Patent No. 60/956,813, filed on August 20, 2007, entitled "Advanced Multifocal Lens with c〇ntimj〇us 〇ptical p〇wer"; and 2007 The US 6th/97〇, 〇24, which was filed on September 5th and named "Improved Multi-Focal". [Prior Art] Presbyopia is often accompanied by aging. Loss of adjustment of the lens of the human eye. This loss of adjustment first leads to inability to focus on close objects and later to focus on objects at intermediate distances. The standard tool for correcting presbyopia is a multifocal ophthalmic lens. A lens with more than one focal length (ie, optical power) for correcting a range of distances: A multifocal ophthalmic lens works by dividing the area of the mirror into regions of different optical power. Typically, it is located above the lens. The relative large area in the section corrects the distance vision error (if any). The smaller in the bottom portion of the lens = provides additional optical power for correction caused by presbyopia Close-range visual error. The multifocal lens may also contain a 130295.doc 200912425 region located near the middle portion of the lens that provides additional optical power for correcting intermediate distance vision errors. Multifocal lenses may form continuous or discontinuous optical power Continuous or discontinuous surface composition. Transitions between regions of different optical power can be abrupt (as in the case of bifocal and trifocal lenses) or smooth and continuous (as in progressively multifocal lenses) In the case of a progressive multifocal lens, the gradient of the positive refractive power from the distance from the long distance zone of the lens to the short distance zone in the lower part of the lens is ~··"Ding~JHJ/Dry

進通常起始於被稱為透鏡之配合十字或配合點者處或附近 且繼續漸進直至在透鏡之近距離區中實現全附加功率為 止。習知及技術現狀之漸進多焦點鏡片利用經成形以形成 光功率之此漸進的透鏡之一個或兩個外表面上之一表面構 形在光學工業内漸進多焦點鏡片在複數時被稱為PALs或 在單數時被稱為PAL。PAL優於傳統之雙焦點及三隹點透 鏡,由於PAL向使用者提供一無線紋、外觀合意的多焦點 透鏡,該多焦點透鏡在使用者之焦點自遠距離處之物件過 渡旦至近距離處之物件時具有連續視力校正且並無感覺得到 之影像中斷,或反之亦然。 然PAL現在作為老花眼之校正在美國 虞4枝 < 穴啤久题汉亡世界被 ^ =及正在流行’但其亦具有嚴重視力損害。 害包括(但不限於)不當散光、失真及眼花 貝 可影響使用者之水平觀察寬度,其為在使用者聚隹二^ 距離時左右觀看時可清楚看到之視户 、,。疋The progression typically begins at or near the point of the mating cross or mating point known as the lens and continues to progress until full additional power is achieved in the close range of the lens. Conventional and state of the art progressive progressive multifocal lenses utilize one of the surface configurations of one or both of the outer surfaces of the progressive lens that is shaped to form optical power. In the optical industry, progressive multifocal lenses are referred to as PALs at complex times. Or in the singular is called PAL. PAL is superior to traditional bifocal and three-point lens. Because PAL provides users with a wireless pattern and a multi-focal lens with appropriate appearance, the multifocal lens is at the user's focal point from a long distance to a close distance. The object has continuous vision correction and no perceived image interruption, or vice versa. However, PAL is now being corrected as a presbyopia in the United States. The 穴 啤 啤 久 久 久 汉 汉 汉 汉 汉 汉 汉 汉 汉 汉 汉 汉 汉 汉 汉 汉 汉 汉 汉 汉 汉 汉 但 但 但 但 但Harm includes, but is not limited to, improper astigmatism, distortion, and scalp, which can affect the user's horizontal viewing width, which is a viewable household that can be clearly seen when viewing the user's distance.疋

可在聚焦於中間距離時且有窄豕&。因此,PAL 叶-有乍的切觀察寬度,此情形可 I30295.doc 200912425 使付難以觀察到電腦螢幕之大部分。類似地,pAL可在聚 焦於近距離時具有窄的水平觀察寬度,此情形可使得難以 觀察到書本或報紙之完整頁。遠距離視力可類似地受影 響。PAL亦可使得佩戴者歸因於透鏡之失真而難以進行運 動°除此等限制以外’冑因於存在於透鏡中之每-者中的 失真’ PAL之許多佩戴者經受被稱為視覺運動(常常稱為 ”眼花”)之不愉快效應。事實上,許多人由於此效應之不舒 適而拒絕佩戴此等透鏡。 當考慮老花眼個人之近距離光功率需要時,所需之近距 離光功率之量與個人眼睛中所留有的調節幅度(近距離聚 之量成反比。通常’隨著個人變老,調節幅度之 里降低。調節幅度亦可由於各種健康原因而降低。因此, 在某人變老且變得更老花時,用以校正某人在近距離及中 =離二聚焦之能力所需的光功率(稱為所需的屈光光功 °近距離及中間距離光功率通常陳述為”附加 加成光功率”。附加功率為對遠距離視力校正之 t功率的量。附加功率通常指代添加至遠距離視力校正以 達成適當近距離視力校正的光功率。相而言若某人且 有-1.00D之用於遠距離觀察之光功率校正及+1嶋之用^ 近距離觀察之^功率校正,則據信此個人具有+2細之近 距離附加功率。 藉由比較兩個個人之不同近距離附加功率需要,有可能 直接比較每一個人之近點聚焦需 b 徊又T处兩 戈僅舉例而言,45歲的 可月b而要+i.〇〇d之近距離附加功率 刀千I在一近點距離處 130295.doc 200912425 清楚地看見’而80歲的個人可能需要+2 _75D至+3.5 0D之近 距離附加功率來在同一近點距離處清楚地看見。由於pAL 中視力損害之程度隨著屈光附加功率而增加,所以老花程 度愈高的個人將經受愈大的視力損害。在以上實例中,45 歲的個人與80歲的個人相比將具有與其透鏡相關聯之較低 紅度之失真以及較寬中間距離及近距離視力區。如顯而易 見’此與在存在與變老相關聯之生活品質問題(諸如,虛 弱或靈活性喪失)的情況下所需的完全相反。給視力功能 添加損害且抑制安全性之處方多焦點透鏡與使生活較簡 單、較安全及較不複雜的透鏡成明顯對照。 僅舉例而言,具有+1 ·〇〇D近距離附加功率之習知pAL可 具有大約1.00D或更少不當散光。然而,具有+25〇D近距 離附加功率之習知PAL可具有大約2 75D或更多不當散光, 而具有+3.25D近距離附加功率之習知pAL可具有大約3.75d 或更多不當散光。因此,隨著PAL之近距離附加功率增加 (舉例而言,與+l,0〇D pAL相比之+2_5〇d PAL),PAL内所 發現之不當散光以大於線性之速率增加。 更近,已開發出一種雙面PAL,其具有置放於透鏡之每 外表面上之漸進多焦點表面構形。兩個漸進多焦點表面 相對於彼此對準及旋轉以不僅給出所需的適當之總加成近 距離附加功率,而且使由透鏡之一個表面上之pAL所形成 的不§散光抵消透鏡之另一表面上之pAL所形成的不當散 光中之一些。儘管與傳統pAL相比,對於給定近距離附加 功率而言,此設計減小了不當散光及失真,但上文所列出 130295.doc 200912425 之不當散光、失真及其他視力損害的程度仍對某些佩戴者 引起嚴重視力問題。 已開發出其他多焦點透鏡,其提供彼此光通信之連續及/ 或不連續光學元件的置放。然而,此等透鏡尚未實現連續 及/或不連續元件之最佳置放及對準。此等透鏡亦未能實 現光通信中所置放之光學元件的最佳光功率分布。因此, 此等透鏡通常具有一或多個感覺得到之影像中斷、稜鏡影 像跳躍、外觀問題、表面不連續性、不良視力人體工學, 1 及/或過陡之光功率梯度。此等問題通常轉換成此等透鏡 之佩戴者之視覺疲勞、眼睛疲勞及頭痛。此等透鏡亦未能 實現上部遠-中間距離區、具有光功率之平台之遠-中間 區’及具有光功率之平台之中間區。 因此’迫切需要提供一種眼鏡片及/或眼鏡系統,該系 統滿足老花眼個人之無用需要且同時以一方式校正其老花 眼,該方式在進行運動、在電腦上工作及閱讀書本或報紙 時減小失真及模糊、加寬水平觀察寬度、允許改良之安全 性’及允許改良之視覺能力。 【發明内容】 - 在本發明之一實施例中,一種眼科透鏡具有一遠距離區 ' 及一配合點。該眼科透鏡可包括一大致球面功率區域,其 用於提供加成光功率至該遠距離區以便提供該透鏡之一中 間距離區。該眼科透鏡可進一步包括一位於該遠距離區與 該大致球面功率區域之間的不連續性。該眼科透鏡可進一 步包括一漸進之光功率區域,其起始於該大致球面功率區 130295.doc -11 - 200912425 域之一部分處以用於提供加成光功率至該大致球面功率區 域以便提供該透鏡之一近距離區。 在本發明之一實施例中,一種眼科透鏡具有一遠距離區 及一配合點。該眼科透鏡可包括一大致球面功率區域,其 用於提供加成光功率至該遠距離區以便提供該透鏡之一上 部遠-中間距離區。該眼科透鏡可進一步包括一位於該遠 距離區與該大致球面功率區域之間的不連續性。該眼科透 鏡可進步包括—漸進之光功率區域,其起始於該大致球 面功率區域之一部分處以用於提供加成光功率至該大致球 面功率區域以便提供該透鏡之一中間距離區及該透鏡之一 近距離區。 在本發明之一實施例中,一種眼科透鏡具有一遠距離區 及一配合點。該眼科透鏡可包括一大致球面功率區域,其 用於提供加成光功率至該遠距離區。該眼科透鏡可進一步 包括一位於該遠距離區與該大致球面功率區域之間的不連 續丨生該眼科透鏡可進一步包括一漸進之光功率區域,其 用於提供加成光功率至該大致球面功率區域以便提供該透 鏡之一中間距離區及該透鏡之一近距離區,該眼科透鏡可 進一步包括位於該漸進之光功率區域之一部分中的光功率 之一平台,其用於在該透鏡之一區中提供視力之垂直穩定 性。 。在本發明之一實施例中,一種眼科透鏡具有一遠距離 區、一中間距離區及一近距離區。該眼科透鏡可包括一大 求面力率區域,其用於提供加成光功率至該遠距離區。 130295.doc -12- 200912425 該眼科透鏡可進-步包括一位於該遠距離區與該大致球面 功率區域之間的不連續性。該眼科透鏡可進一步包括一漸 枝光功率區域,其中該漸進之光功率區域之-部分供應 一負光功率至該大致球面功率區域。 在本發明之一實旛你丨φ 口 頁例中種眼科透鏡具有一遠距離 區、-上部遠_中間區、_中間距離區及一近距離區。該 眼科透鏡可包括一漸進$也.右π 祈進之先功率區域。該眼科透鏡可進一 步^括位於該漸進之光功率區域之一部分中的光功率之一 第平口,其用於在該上部遠_中間距離區中提供視力之 垂直穩定性。 。在本發明之—實施例中,—種眼科透鏡具有—遠距離 區、-中間距離區及一近距離區。該眼科透鏡可包括一大 致球面功率區域,其用於提供加成光功率至該遠距離區。 該眼科透鏡可進-步包括一位於該遠距離區與該大致球面 功率區域之間的不連續性。該眼科透鏡可進一步包括一漸 Ο 進之光功率區域,其與該不連續性間隔開且在該不連續性 下方以用於提供加成光功率至該大致球面功率區域。 【實施方式】 本發明之實施例將結合諸圖之以下實施方式更完整理解 及瞭解,該等圖並未按比例,其中相同參考編號指示對 應、類似或相似元件。 許夕眼科、驗光及光學術語用於本申請案中。為了清楚 起見,下文列出其定義: 附加功率·•附加功率表示近距離視力及/或中間距離視 130295.doc 13 200912425 二斤:的額外正光功率。當眼睛之正常調節功率不再足以 聚‘、、、於近距離或中間距離物件上 眼而開處方。附加功率被稱為"附力/j心破針對老花It can be narrowed & when focusing on the intermediate distance. Therefore, the PAL leaf - has a slanting observation width, which can be difficult to observe most of the computer screen in the case of I30295.doc 200912425. Similarly, pAL can have a narrow horizontal viewing width when focused at close distances, which can make it difficult to observe a complete page of a book or newspaper. Long-distance vision can be similarly affected. PAL can also make it difficult for the wearer to move due to lens distortion. In addition to these limitations, 'there are distortions in each of the lenses'. Many wearers of PAL experience what is called visual motion ( The unpleasant effect often referred to as "eyes". In fact, many people refuse to wear these lenses because of the uncomfortable effect of this effect. When considering the short-distance optical power requirements of the presbyopic individual, the amount of close-range optical power required is inversely proportional to the amount of adjustment left in the individual's eyes (the amount of close-up convergence is usually proportional. Usually, as the individual ages, the adjustment range The reduction can also be reduced for various health reasons. Therefore, when someone ages and becomes older, the light needed to correct a person's ability to be in close and medium=two focus is needed. Power (referred to as the required refractive power) close-range and intermediate-distance optical power is usually stated as "additional additive optical power." The additional power is the amount of t-power corrected for long-range vision. Additional power is usually referred to as added to the far Distance vision correction to achieve appropriate near vision correction of optical power. If one has a -1.00D optical power correction for long-distance observation and +1 ^ ^ close-range observation of power correction, It is believed that this individual has a +2 fine close-range additional power. By comparing the different close-range additional power requirements of the two individuals, it is possible to directly compare each individual's near-point focus to b 徊 and T at the two points only For example, the 45-year-old can be the monthly b and the +i.〇〇d close-range additional power knife thousand I is at a close distance 130295.doc 200912425 clearly sees '80-year-old individuals may need +2 _75D The close-range additional power to +3.5 0D is clearly seen at the same near-point distance. Since the degree of visual impairment in pAL increases with the additional power of refraction, the higher the presbyopia, the more vision the individual will experience. Damage. In the above example, a 45-year-old individual will have a lower redness distortion associated with his lens and a wider intermediate and near vision area than the 80-year-old. As is evident, this is in existence and The opposite is true in the case of ageing associated quality of life issues (such as weakness or loss of flexibility). Adding damage to the vision function and suppressing safety where the multifocal lens makes life simpler, safer and more Uncomplicated lenses are in sharp contrast. By way of example only, conventional pALs with +1 · 〇〇 D close range additional power may have approximately 1.00 D or less improper astigmatism. However, with a close range of +25 〇D The conventional PAL of power may have about 2 75D or more improper astigmatism, while the conventional pAL with +3.25D close range additional power may have about 3.75d or more improper astigmatism. Therefore, with the close power of PAL Increasing (for example, +2_5〇d PAL compared to +l,0〇D pAL), the improper astigmatism found in PAL increases at a rate greater than linear. More recently, a double-sided PAL has been developed. Having a progressive multifocal surface configuration placed on each outer surface of the lens. The two progressive multifocal surfaces are aligned and rotated relative to each other to give not only the appropriate total additive close-range additional power required, but also The astigmatism formed by the pAL on one surface of the lens cancels some of the improper astigmatism formed by the pAL on the other surface of the lens. Although this design reduces improper astigmatism and distortion for a given close-range additional power compared to conventional pAL, the degree of improper astigmatism, distortion, and other visual impairments listed above for 130295.doc 200912425 remains Some wearers cause serious vision problems. Other multifocal lenses have been developed that provide for the placement of continuous and/or discontinuous optical elements in optical communication with one another. However, such lenses have not achieved optimal placement and alignment of continuous and/or discontinuous components. These lenses also fail to achieve optimal optical power distribution of the optical components placed in the optical communication. Thus, such lenses typically have one or more perceived image interruptions, artifacts, appearance problems, surface discontinuities, poor vision ergonomics, and/or steep power gradients. These problems are often translated into visual fatigue, eye strain and headache of the wearer of such lenses. These lenses also failed to achieve the upper far-intermediate distance zone, the far-middle zone of the platform with optical power, and the intermediate zone of the platform with optical power. Therefore, there is an urgent need to provide an ophthalmic lens and/or eyeglass system that satisfies the useless needs of presbyopic individuals while simultaneously correcting their presbyopia in a manner that reduces movement, working on a computer, and reading books or newspapers. Distortion and blurring, widening the horizontal viewing width, allowing for improved safety' and allowing improved visual capabilities. SUMMARY OF THE INVENTION - In one embodiment of the invention, an ophthalmic lens has a remote zone ' and a mating point. The ophthalmic lens can include a substantially spherical power region for providing additive optical power to the remote region to provide an intermediate distance region of the lens. The ophthalmic lens can further include a discontinuity between the remote region and the substantially spherical power region. The ophthalmic lens can further include a progressive optical power region that begins at a portion of the substantially spherical power region 130295.doc -11 - 200912425 for providing additive optical power to the substantially spherical power region to provide the lens One of the close range areas. In one embodiment of the invention, an ophthalmic lens has a distal zone and a mating point. The ophthalmic lens can include a substantially spherical power region for providing additive optical power to the remote region to provide an upper-middle distance region of the lens. The ophthalmic lens can further include a discontinuity between the remote region and the substantially spherical power region. The ophthalmic lens can be advanced to include a progressive optical power region starting at a portion of the substantially spherical power region for providing additive optical power to the substantially spherical power region to provide an intermediate distance region of the lens and the lens One of the close range areas. In one embodiment of the invention, an ophthalmic lens has a distal zone and a mating point. The ophthalmic lens can include a substantially spherical power region for providing additive optical power to the remote region. The ophthalmic lens can further include a discontinuity between the remote region and the substantially spherical power region. The ophthalmic lens can further include a progressive optical power region for providing additive optical power to the substantially spherical surface a power region for providing an intermediate distance region of the lens and a close distance region of the lens, the ophthalmic lens further comprising a platform of optical power in a portion of the progressive optical power region for use in the lens The vertical stability of vision is provided in one zone. . In one embodiment of the invention, an ophthalmic lens has a remote zone, an intermediate zone, and a close zone. The ophthalmic lens can include a large area of force ratio for providing additive optical power to the remote area. 130295.doc -12- 200912425 The ophthalmic lens can further include a discontinuity between the remote region and the substantially spherical power region. The ophthalmic lens can further include a tapered optical power region, wherein a portion of the progressive optical power region supplies a negative optical power to the substantially spherical power region. In the case of the present invention, the ophthalmic lens has a long distance zone, an upper far_intermediate zone, a middle intermediate zone and a close distance zone. The ophthalmic lens may include a progressive $., right π, initial power region. The ophthalmic lens can further include one of the optical powers located in a portion of the progressive optical power region for providing vertical stability of vision in the upper distal-intermediate distance region. . In an embodiment of the invention, the ophthalmic lens has a long distance zone, a middle distance zone and a close range zone. The ophthalmic lens can include a substantially spherical power region for providing additive optical power to the remote region. The ophthalmic lens can further include a discontinuity between the remote region and the substantially spherical power region. The ophthalmic lens can further include an progressive optical power region spaced apart from the discontinuity and below the discontinuity for providing additive optical power to the substantially spherical power region. The embodiments of the present invention are more fully understood and understood from the following description of the accompanying drawings, wherein the claims Xu Xi ophthalmology, optometry and optical terminology are used in this application. For the sake of clarity, the definitions are listed below: Additional power • Additional power indicates near vision and/or intermediate distance 130295.doc 13 200912425 Two pounds: extra positive light power. When the normal adjustment power of the eye is no longer enough to gather ‘, ,, close to the eye or the middle of the object to prescribe. Additional power is called "with force/j heartbreak for presbyopia

透鏡之遠距離光功率。舉例而言,若個人具有_3_M :巨離觀察處方及用於近距離觀察之+2〇〇d附加功率,則多 …點透鏡之近距離部分令之實際光功率為兩個功率之和, 附加功率有時被稱為正光功率或加成光功率。 二,功率亦可指代透鏡之中間距離部分中的附加功率且被 ::+間距離附加功率"。通常,t間距離附加功率為近 距離附加功率之大約5〇 四此在以上實例中,個人可 間距_察之附加功率且多焦點透鏡 之中間距離部分中的實際總光功率可能為·2嶋。 混合區··跨越透鏡之光功率不連續性之至少一部分而過 :光功率差的區,其中該不連續性定位於一第一光功率與 一第二光功率之間。可(例如)藉由不同表面構形或藉由不 同折射率來引起第-光功率與第二光功率之間的差。光功 :跨越混合區而自第—光功率連續地過渡至第二光功率。 當使用繞射光學器件時,混合區可包括混合繞射光學器件 之周邊區域的光效率。混合區用於外觀增強原因。混合區 通㊉歸因於其不良光學特性而不認為其為透鏡之有用部 为。混合區亦被稱為過渡區。 通道.透鏡之藉由増加正光功率而界定之區域,其以透 鏡之中〜為中心’其自遠距離區延伸至近距離區且並無大 於1.00D之不當散光。對於漸進多焦點鏡片而言,此光功 130295.doc 200912425 率漸進大約起始於稱為配合點之透鏡之一區中且結束於近 距離區中。然而,具有漸進之光功率區域之本發明之實施 例中,通道可起始於配合點下方大約4 mm與大約1〇 間處。通道有時被稱為過道。 通道長度:通道長度為自光功率首先開始增加的通道之 界定起始處至附加功率在透鏡之指定近距離觀察功率的大 約85。/。内的通道中之位置所量測的距離。通道通常起始於 配合點處或配合點附近。 通道寬度:由高於大約L00D之不當散光所限定的通道 之最窄部分。此定義在比較透鏡時有用,因為較寬通道寬 度通常與對於佩戴者而言的較少模糊、較少失真、較好視 覺效能、增加之視覺舒適度,及對通道之較易適應性相 關。 連續光功率:大體上恆定或以不會形成感覺得到之影像 中斷之方式改變的光功率。 連續表面:不會引起感覺得到之影像中斷之折射表面。 連續表面可在透鏡之外部或内部。若在内部,則其可能具 有與相鄰於其之材料不同的折射率。連續表面之一實例為 大體上球面透鏡或漸進多焦點鏡片的表面。 等高線圖:藉由量測及繪製透鏡之光功率改變及/或不 當散光光功率而產生的曲線。等高線曲線可用散光光功率 之各種篮敏度來產生,從而提供透鏡在哪些情況下擁有作 為歸因於其光學設計之效應的不當散光及其擁有程度之視 覺圖像。此等圖之分析可用於量化透鏡之通道長度、通道 130295.doc •15- 200912425 寬度、讀取寬度及遠距離寬度。等高線圖可被稱為不當散 光功率圖、球面功率圖、平均功率圖、附加功率圖,或功 率誤差圖。此等圖亦可用於量測及描繪透鏡之各種部分中 的光功率。 習知通道長度:歸因於眼鏡款式之美學關注或傾向,可 能歸因於框架式樣而需要使被垂直縮短之透鏡配合框架。 在此等透鏡中,為了傳遞足夠近距離視力,亦自然地縮短 . 通道。習知通道長度指代非縮短透鏡中之通道的長度。此 〇 等通道長度通常(但並非總是)大約15 mm或更長。通常, 較長通道長度意謂與具有較短通道長度之pAL相比而言的 較寬通道寬度及較少不當散光。 不連續ft . +連續性為產生對於使用纟而言感覺得到之 影像中斷的光功4改變或表面改變。不連續性可由透鏡之 兩個區域之間的光功率之步升或步降而引起。舉例而言, 0· 1 0D之不連續性指代透鏡之兩個區域之間的〇 1 之步升 或步降。 I’ 不連續光功率:以形成感覺得到之影像中斷之方式改變 的光功率。 不連續表面:引起感覺得到之影像中斷之表面。不連續 - 4面可在透鏡之外部或内部。若在内部,則其可能具有與 相鄰於其之材料不同的折射率。僅舉例而言,不連續表面 為表面自it鏡之遠距離區改變至近距離區之具線紋之雙焦 點透鏡的表面。 動態透鏡I有隨著電能、機械能或力的施力口而可改變 130295.doc 200912425 •;“的透鏡。動態透鏡之光功率在無f額外研磨或抛 光的情況下可改變。整個透鏡可具有可改變之光功率,或 透鏡之僅-部分、區域或區可具有可改變之光功率。此透 鏡之光功率為動態的或可㈣的,使得可在兩個或兩個以 上光功率之間切換光功率。光功率中之一者可大體上無光 功率。動態透鏡之實例包括電活性透鏡、電凹凸透鏡、具 有一或多個機械移動零件之透鏡,或由適型隔膜製成之透 鏡(諸如,氣體透鏡或流體透鏡)。動態透鏡亦可被稱為動 態光學n件或動態光學元件。動態透鏡亦可被稱為透射性 自適應光學器件或透鏡。 遠-中間距離區:含有允許使用者在遠_中間距離處清楚 地看見之光功率之透鏡的部分或區域。遠·中間距離區可 定位於透鏡之遠距離區與中間距離區之間,在此情況下其 被稱為"上部遠-中間距離區”。遠-中間距離區亦可定位於 透鏡之近距離區下方,在此情況下其亦被稱為"下部遠-中 間距離區"。遠-中間距離區亦可被稱為遠-中間視力區。 遠-中間距離:僅舉例而言,吾人在觀察吾人之辦公桌 之遠邊緣時觀看到的距離。此距離通常(但並非總是)被認 為距眼睛介於大約29吋與大約5呎之間,且在一些情況下 可在距眼睛大約29吋與大約10呎之間。遠-中間距離亦可 被稱為遠-中間觀察距離或遠-中間距離點。 遠距離參考點:位於配合十字上方大約4至8 mm的參考 點’在該參考點處可容易地量測PAL之遠距離處方或遠距 離光功率。 130295.doc -17- 200912425 遠距離區:含有允許使用者在遠距離處清楚地看見之光 功率之透鏡的部分或區域。遠距離區亦可被稱為遠視力 區。 遠距離寬度:透鏡之遠距離觀察部分内之最窄水平寬 度,在配合點上方大約4至8 mm,其藉由佩戴者之〇 25D遠 距離光功率校正内之光功率提供清楚、大致無模糊之校 正。 遠距離:僅舉例而言,吾人在觀察超出吾人之辦公桌之 邊緣時、在駕駛一汽車時、在觀看遠處山脈時或在看電影 時觀看到的距離。此距離通常(但並非總是)被認為距眼睛 大於大約5呎,且在一些情況下可距眼睛大於大約1〇呎。 "遠距離’,不會與距眼睛大約2〇呎或更遠的無窮遠混淆。在 無窮遠處,眼睛之調節系統完全放鬆。提供於吾人之光學 處方中以校正距眼睛大約5呎(或1〇呎)或更大的光功率通常 並不與校正距眼睛大約20呎所需的光功率顯著不同。因 此,如本文中所使用,遠距離指代距眼睛大約5呎(或1〇呎) G 及更大的距離。遠距離亦可被稱為遠觀察距離及遠距離 點。 一 配合十字/配合點:透鏡上之參考點,其表示一旦將透 - 鏡安裝於眼鏡框架中且定位於佩戴者之臉上,透過透鏡一 直向前看時佩戴者之瞳孔之近似位置。配合十字/配合點 通常(但並非總是)位於通道之起始處垂直上方大約2 mm至 5 mm處。配合十字可具有在僅超過+〇 〇〇D至大約+〇 i2d 之範圍内的非常微小量之正光功率。此點或十字通常用墨 130295.doc 200912425 水標記於透鏡表面上以提供簡單參考點以用於量測及/或 複核透鏡相對於佩戴者之瞳孔的配合。標記易於在分配透 鏡給佩戴者時移除。 硬式或軟式漸進多焦點區域•具有快或慢速率之光功率 改變或散光功率改變的漸進多焦點區分別被稱為硬式或軟 式漸進多焦點區域。主要含有快速率之改變的透鏡可被稱 為"硬式漸進多焦點鏡片"。主要含有慢速率之改變的透鏡 可被稱為"軟式漸進多焦點鏡片"。視所選擇之過道長度、The long distance optical power of the lens. For example, if an individual has _3_M: a large deviation observation prescription and an additional power of +2 〇〇d for close-up observation, the close-range portion of the multi-point lens causes the actual optical power to be the sum of the two powers, Additional power is sometimes referred to as positive optical power or additive optical power. Second, power can also refer to additional power in the middle distance portion of the lens and additional power by ::+ distance. In general, the additional power between the distances t is approximately 5 近 of the close-range additional power. In the above example, the individual can be spaced to see the additional power and the actual total optical power in the intermediate distance portion of the multifocal lens may be . . The mixing zone comprises: at least a portion of the optical power discontinuity across the lens: a region of poor optical power, wherein the discontinuity is positioned between a first optical power and a second optical power. The difference between the first optical power and the second optical power can be caused, for example, by different surface configurations or by different refractive indices. Optical power: continuously transitions from the first-optical power to the second optical power across the mixing zone. When diffractive optics are used, the mixing zone can include the light efficiency of the peripheral regions of the hybrid diffractive optics. The mixing zone is used for appearance enhancement reasons. The mixing zone is not considered to be a useful part of the lens due to its poor optical properties. The mixing zone is also known as the transition zone. A region of a lens that is defined by the addition of positive optical power, which is centered in the lens. It extends from a long range to a close range and has no astigmatism greater than 1.00D. For progressive multifocal lenses, this optical power progressively begins approximately in a region of the lens known as the mating point and ends in the close region. However, in embodiments of the invention having a progressive optical power region, the channel may begin between about 4 mm and about 1 turn below the mating point. Channels are sometimes referred to as aisles. Channel length: The channel length is approximately 85 from the beginning of the definition of the channel from which the optical power first begins to increase to the additional power observed at a specified close distance of the lens. /. The distance measured by the position in the inner channel. The channel usually starts at or near the mating point. Channel Width: The narrowest portion of the channel defined by improper astigmatism above about L00D. This definition is useful when comparing lenses because wider channel widths are generally associated with less blurring, less distortion, better visual performance, increased visual comfort, and easier adaptability to the wearer. Continuous optical power: optical power that is substantially constant or that changes in a manner that does not create a perceived image interruption. Continuous surface: A refractive surface that does not cause a perceived image interruption. The continuous surface can be external or internal to the lens. If inside, it may have a different refractive index than the material adjacent to it. An example of a continuous surface is the surface of a substantially spherical lens or a progressive addition lens. Contour map: A curve produced by measuring and plotting the optical power of the lens and/or the power of the astigmatic light. The contour curve can be generated by various basket sensitivities of the astigmatic light power to provide a visual image of the lens with under-accurate astigmatism and its degree of possession as a result of its optical design. The analysis of these figures can be used to quantify the channel length of the lens, the width of the channel 130295.doc •15- 200912425, the read width and the long distance. The contour map can be referred to as an improper astigmatism power map, a spherical power map, an average power map, an additional power map, or a power error map. These figures can also be used to measure and depict the optical power in various parts of the lens. Conventional channel length: Due to the aesthetic focus or tendency of the eyeglass style, it may be necessary to have the lens that is vertically shortened to fit the frame due to the frame style. In these lenses, in order to transmit sufficient near vision, it is also naturally shortened. The known channel length refers to the length of the channel in the non-shortened lens. This 〇 equal channel length is usually (but not always) about 15 mm or longer. Generally, a longer channel length means a wider channel width and less improper astigmatism than a pAL having a shorter channel length. Discontinuous ft. + Continuity is the generation of light work 4 changes or surface changes that are interrupted by the use of 纟. The discontinuity can be caused by a step-up or step-down of the optical power between the two regions of the lens. For example, a discontinuity of 0·1 0D refers to a step-up or step-down of 〇 1 between two regions of the lens. I' Discontinuous optical power: The optical power that is changed in such a way as to form a perceived image interruption. Discontinuous surface: The surface that causes the perceived image to be interrupted. Discontinuous - 4 faces can be outside or inside the lens. If inside, it may have a different refractive index than the material adjacent to it. By way of example only, the discontinuous surface is the surface of the surface of the bifocal point lens that changes from a long range of the mirror to a close range. The dynamic lens I can be changed with the application of electric energy, mechanical energy or force 130295.doc 200912425 • "The lens. The optical power of the dynamic lens can be changed without additional grinding or polishing. The entire lens can be Having a changeable optical power, or only a portion, region or region of the lens may have a changeable optical power. The optical power of the lens is dynamic or (four) such that it can be in two or more optical powers Switching optical power. One of the optical powers may be substantially free of optical power. Examples of dynamic lenses include electroactive lenses, electrical meniscus lenses, lenses with one or more mechanically moving parts, or made of a suitable diaphragm. A lens (such as a gas lens or a fluid lens). A dynamic lens may also be referred to as a dynamic optical n-piece or a dynamic optical element. A dynamic lens may also be referred to as a transmissive adaptive optic or lens. A portion or region of the lens that allows the user to clearly see the optical power at a far-intermediate distance. The far-middle distance region can be positioned between the far distance zone and the intermediate distance zone of the lens In this case, it is called the "upper far-middle distance zone." The far-middle distance zone can also be positioned below the close range of the lens, which in this case is also referred to as "lower far-intermediate distance zone". The far-middle distance zone may also be referred to as the far-middle vision zone. Far-middle distance: For example only, the distance we see when observing the far edge of our desk. This distance is usually (but not always) considered to be between about 29 inches and about 5 inches from the eye, and in some cases between about 29 inches and about 10 inches from the eye. The far-middle distance can also be referred to as a far-middle viewing distance or a far-middle distance point. Remote reference point: A reference point of approximately 4 to 8 mm above the mating cross. At this reference point, the long distance prescription or remote optical power of the PAL can be easily measured. 130295.doc -17- 200912425 Remote Zone: A section or area containing a lens that allows the user to clearly see the power of light at a distance. The long distance zone can also be referred to as the far vision zone. Long-distance width: The narrowest horizontal width in the long-distance viewing portion of the lens, approximately 4 to 8 mm above the mating point, which provides clear, substantially blur-free power by the wearer's 25D long-range optical power correction Correction. Long distance: For example, the distance we watch when we look beyond the edge of our desk, when driving a car, when watching a distant mountain range, or while watching a movie. This distance is usually (but not always) considered to be greater than about 5 inches from the eye, and in some cases greater than about 1 inch from the eye. "remote distance' will not be confused with infinity that is about 2 inches or more from the eye. At infinity, the eye's conditioning system is completely relaxed. The optical power provided in our optical prescription to correct about 5 呎 (or 1 〇呎) or more from the eye is usually not significantly different from the optical power required to correct about 20 距 from the eye. Thus, as used herein, the distance refers to a distance of about 5 呎 (or 1 〇呎) G and greater from the eye. Long distances can also be referred to as far viewing distances and long distance points. A mating cross/fit point: a reference point on the lens that represents the approximate position of the wearer's pupil when the lens is mounted in the spectacle frame and positioned on the wearer's face through the lens. The mating cross/fit point is usually (but not always) located approximately 2 mm to 5 mm vertically above the beginning of the channel. The mating cross can have a very small amount of positive optical power in the range of only + 〇 〇〇D to about + 〇 i2d. This point or cross is typically marked with ink 130295.doc 200912425 water on the lens surface to provide a simple reference point for measuring and/or recombining the lens with respect to the wearer's pupil. The marking is easy to remove when dispensing the lens to the wearer. Hard or soft progressive multifocal zones • Progressive multifocal zones with fast or slow rate optical power changes or astigmatic power changes are referred to as hard or soft progressive multifocal zones, respectively. A lens that mainly contains a change in the rate of rapidity can be referred to as a "hard progressive multifocal lens". A lens that mainly contains a change in slow rate can be called a "soft progressive multifocal lens". Depending on the length of the aisle selected,

所需的附加功率,及設計者之數學工具而定,PAL可含有 硬區及軟區兩者。 硬式漸進多焦點鏡片.具有遠距離校正與近距離校正之 間的較不平緩、較陡過渡之漸進多焦點鏡片。在硬式PAL 中’不t失真可在配合點下方且並不&開至透鏡之遠距離 區域之周邊中。在一些情況下’硬式pAL亦可具有較短通 道長度及較窄通道寬度。"經修改之硬式漸進多焦點鏡片” 為一包含經稍微修改之硬式PAL光學設計的pAL,該設計 具有軟式PAL之-或多個特徵,諸如:較平緩之光功率過 渡車乂長通道、杈寬通道、展開至透鏡之周邊中之較多不 當散光,及配合點下方之較少不當散光。 光功率之水平穩定性:具有跨越區域或區之水平寬度之 大致值疋光功率的透錄^^ p 千的边鏡之Q域或區。或者,光功率改變可 為跨越區域或區之水平寬度的每毫米大約0.05D或更少的 := 料另帛代,光功率改變可為跨越區域或區之 水平寬度的每毫米大―或更少的平均值。作為最終 130295.doc -19· 200912425 替代,光功率改變可為跨越區域或區之水平寬度的每毫米 大約0.20D或更少的平均值。區域或區可具有大約】麵或 更大的水平寬度。作為一替代,區域或區可具有大約一 至大約3 mm或更大的水平寬度。作為最終替代,區域或區 可具有大約2 mm至大約6 mm或更大的水平寬度。區域或 ; 區可為透鏡之遠距離區、上部遠-中間距離區、中間距離 區、近距離區、下部遠-中間距離區,或任何其他區域。 視力之水平穩定性··據信透鏡之一區域或區在該區域或 區在使用者跨越該區域或區左右觀看時具有大致恆定清楚 視力的情況下具有視力之水平穩定性。區域或區可具有大 約1 mm或更大的水平寬度。作為一替代,區域或區可具有 大約1 mm至大約3 mm或更大的水平寬度。作為最終替 代,區域或區可具有大約2 mm至大約6 mm或更大的水平 寬度。區域或區可為透鏡之遠距離區、上部遠-中間距離 區、中間距離區、近距離區、下部遠-中間距離區,或任 何其他區域。 ^ %像中斷.影像中斷為在透過透鏡觀看時影像中感覺得 &中斷。當影像中斷發生時,透過透鏡„得^ = 不再無縫。影像中斷可為跨越影像中斷之影像的稜鏡移 &、跨越影像中斷之影像的放大率改變、在影像中斷處或 周圍的衫像之犬然模糊,或所有三者之組合。一種判定透 鏡是否具有一影像中斷之方法係將透鏡置放於距一組垂直 線、水平線或栅格一固定距離處。圖1A至圖1〇B展示具 有-1.25D遠距離校正及+2.25D附加功率且保持為距膝上型螢 130295.doc -20- 200912425 幕6"的不同透鏡,該等圖顯示距膝上型螢幕19·5"所拍攝之 垂直線或柵格。圖1Α及圖1Β展示根據本發明之一實施例 之透鏡。圖2Α及圖2Β展示根據本發明之另一實施例之透 鏡。圖3Α及圖3Β展示根據本發明之另一實施例之透鏡。 圖4Α及圖4Β展示根據本發明之另—實施例之透鏡。圖5八 及圖5Β展示平頂多透鏡。圖6Α及圖6Β展示具有層狀剖切 (slab-off)稜鏡之緩斜頂透鏡。圖7Α及圖7Β展示緩斜頂透 鏡。圖8Α及圖8Β展示混合雙焦點透鏡。圖9Α及圖9Β展示 平頂三焦點透鏡。圖1〇Α及圖1〇Β展示執行透鏡。圖UA及 圖11Β展示由Sola Optical登記商標之s〇la SmartSegTM透 鏡,其具有-2.25D遠距離校正及+2〇〇D附加功率且保持為 距膝上型螢幕6",該圖顯示距膝上型螢幕丨9.5 "所拍攝之垂 直線或柵格。圖12A至圖13B展示具有·丨25D遠距離校正及 + 2.25D附加功率且保持為距膝上型螢幕6”的不同透鏡,該 等圖顯示距膝上型螢幕19.5”所拍攝之垂直線或柵格。圖 12A及圖 12B展示由 Essilor登記商標之 Variiux Physi〇 36〇tm 透鏡。圖13A及圖13B展示由Carl Zeiss Visi〇n登記商標之 Sola Compact Ultra™透鏡。圖1A至圖11B展示產生感覺得 到之影像中斷之透鏡。圖12A至圖13B展示不產生感覺得 到之影像中斷之透鏡。 中間距離區:含有允許使用者在中間距離處清楚地看見 之光功率之透鏡的部分或區域。中間距離區亦可被稱為中 間視力區。 中間距離:僅舉例而言,吾人在閱讀報紙時、在電觸上 130295.doc 21 200912425 工作時、在清洗水槽中之盤時或在熨燙衣服時觀看到的距 離。此距離通常(但並非總是)被認為距眼睛介於大約16对 與大約29时之間。中間距離亦可被稱為中間觀察距離及中 間距離點。應指出,"中間距離"亦可被稱為"近_中間距離", 因為近距離”為距眼睛介於大約丨〇叶至大約丨6时。或者, 大約16吋之"中間距離"之僅一部分可被稱為”近·中間距離"。 "遠-中間距離"不會與”中間距離”混淆。„遠-中間距離,,代 替地距眼睛大約29吋至大約5呎(或1 〇呎)。 1.- 透鏡.引起光收斂或發散的任何裝置或一裝置之部分。 透鏡可為折射或繞射的。透鏡可在一個或兩個表面上為凹 的、凸的或平的。透鏡可為球面的、圓柱的、稜鏡的,或 其組合。透鏡可由光學玻璃、塑膠、熱塑性樹脂、熱固性 樹脂、玻璃與樹脂之複合物,或不同光學等級之樹脂或塑 勝之複合物製成°透鏡可被稱為光學元件、光學預成型 坯 '光學晶圓、經修整之透鏡毛坯,或光學器件。應指 出,在光學工業範圍内,一裝置可甚至在其具有零光功率 (被稱為平的或無光功率)的情況下被稱為透鏡。透鏡通常 在可^佩戴透鏡時經定向,使得透鏡之遠距離區在頂部 且近距離部分在底部。術語,,上部,'、”下部”、”上方”、"下 方"垂直"、"水平"、"上” '"下"、”左,,、”右,,、”頂部” 及底部"在用於參考透鏡時可相對於此定向而獲得。 .毛坯•由可成形為透鏡之光學材料製成的裝置。透 二毛培可4經修整的",其意謂透鏡毛喊其兩個外表面 成形為折射外表面。經修整之透鏡毛述具有一可為包括零 130295.doc -22- 200912425 或平的光功率之任何光功率的光功率。透鏡毛注可為 修整之"透鏡毛堪,其音臂携错主α , 再思明透鏡毛坯已經成形以具有僅一 個經修整之折射外表面。透鏡㈣可為"未修整之"透鏡毛 述,其意謂透鏡毛述之任-外表面均未成形為折射表:。 未修整之或半修整之透鏡毛坯之未修整 正表面可借助於稱為Depending on the additional power required and the designer's mathematical tools, the PAL can contain both hard and soft zones. Hard progressive multifocal lens. A progressive, multi-focal lens with a less gradual, steeper transition between long range correction and close distance correction. In hard PAL, 'no t distortion can be below the fit point and not & open to the periphery of the far distance region of the lens. In some cases the 'hard pAL' may also have a shorter channel length and a narrower channel width. "Modified Hard Progressive Multifocal Lens" is a pAL that includes a slightly modified hard PAL optical design that has soft PAL- or features such as a flatter optical power transition vehicular long channel,杈 Wide channel, more improper astigmatism spread out to the periphery of the lens, and less improper astigmatism below the fit point. Horizontal stability of optical power: Pervasive power with an approximate value of the horizontal width across the area or zone ^^ p Q domain or region of the side mirror. Alternatively, the optical power change can be about 0.05D or less per millimeter across the horizontal width of the region or region: = another generation, the optical power change can be crossed The average of the horizontal width of the area or zone is greater than or equal to the average of the millimeters. As an alternative 130295.doc -19. 200912425, the optical power change can be about 0.20D or less per millimeter across the horizontal width of the zone or zone. The average value. The area or zone may have a horizontal width of about 面 or greater. As an alternative, the zone or zone may have a horizontal width of from about one to about 3 mm or more. As a final alternative, the zone The or region may have a horizontal width of from about 2 mm to about 6 mm or more. The region or region may be a long distance zone of the lens, an upper far-middle distance zone, a middle distance zone, a close range zone, and a lower far-middle distance Zone, or any other zone. Horizontal stability of vision · It is believed that a region or zone of a lens has a level of vision in the region or zone with substantially constant clear vision when viewed by the user across the zone or zone. Stability. The zone or zone may have a horizontal width of about 1 mm or more. As an alternative, the zone or zone may have a horizontal width of from about 1 mm to about 3 mm or more. As a final alternative, the zone or zone may have A horizontal width of from about 2 mm to about 6 mm or more. The area or zone may be a long distance zone of the lens, an upper far-middle distance zone, a middle distance zone, a close range zone, a lower far-middle zone zone, or any other Area. ^ % is like interruption. The image interruption is an interruption in the image when viewed through the lens. When the image interruption occurs, the lens „ ^^ = no longer seamless. The image interruption can be a shift of the image that is interrupted by the image, a change in the magnification of the image that is interrupted by the image, a dog-like blurring of the image at the interruption of the image, or a combination of all three. One method of determining whether a lens has an image interruption is to position the lens at a fixed distance from a set of vertical lines, horizontal lines, or grids. 1A through 1B show different lenses with a -1.25D remote correction and +2.25D additional power and remain at a distance of 130295.doc -20-200912425 Curtain 6" Type screen 19·5" The vertical line or grid taken. 1A and 1B show a lens in accordance with an embodiment of the present invention. 2A and 2B show a lens in accordance with another embodiment of the present invention. 3A and 3B show a lens in accordance with another embodiment of the present invention. 4A and 4B show a lens according to another embodiment of the present invention. Figure 5 and Figure 5 show a flat-top multi-lens. Figure 6A and Figure 6B show a slow-sloping top lens with a layered slab-off. Figure 7A and Figure 7 show the slow-sloping top lens. Figures 8A and 8B show a hybrid bifocal lens. Fig. 9A and Fig. 9B show a flat top triple focus lens. Figure 1A and Figure 1 show the execution lens. Figure UA and Figure 11 show the s〇la SmartSegTM lens registered by Sola Optical with 2.25D remote correction and +2〇〇D additional power and kept at 6" from the laptop screen. The vertical line or grid of the upper screen 丨 9.5 ". Figures 12A-13B show different lenses with 丨25D remote correction and + 2.25D additional power and held at 6" from the laptop screen, which shows a vertical line taken from the laptop screen 19.5" Grid. Figures 12A and 12B show a Variiux Physi〇 36〇tm lens registered by Essilor. Figures 13A and 13B show a Sola Compact UltraTM lens registered by Carl Zeiss Visi〇n. Figures 1A through 11B show lenses that produce a perceived image interruption. Figures 12A-13B show lenses that do not produce a perceived image break. Intermediate distance zone: A portion or region containing a lens that allows the user to clearly see the optical power at an intermediate distance. The intermediate distance zone can also be referred to as the intermediate vision zone. Intermediate distance: For example, the distance we watched when reading newspapers, when working on electricity, 130295.doc 21 200912425, when cleaning the dishes in the sink, or when ironing clothes. This distance is usually (but not always) considered to be between about 16 pairs and about 29 hours from the eye. The intermediate distance can also be referred to as the intermediate viewing distance and the intermediate distance point. It should be noted that "intermediate distance" can also be referred to as "near_intermediate distance", because the close distance is from about 丨〇 to about 6 o'clock from the eye. Or, about 16 &" Only a part of the intermediate distance " can be called "near intermediate distance". " far-intermediate distance" will not be confused with "middle distance". „ far-intermediate distance, instead of about 29吋 to about 5呎 (or 1〇呎) from the eye. 1.- Lens. Any device or part of a device that causes light to converge or diver. The lens can be refracted or wound. The lens may be concave, convex or flat on one or both surfaces. The lens may be spherical, cylindrical, meandered, or a combination thereof. The lens may be made of optical glass, plastic, thermoplastic resin, thermoset. Resin, a composite of glass and resin, or a composite of different optical grades of resin or plastic. The lens can be referred to as an optical component, an optical preform 'optical wafer, a finished lens blank, or an optical device. It should be noted that within the optical industry, a device may be referred to as a lens even when it has zero optical power (referred to as flat or no optical power). Lenses are typically oriented when the lens is wearable, such that The long range of the lens is at the top and the close part is at the bottom. Terms, upper, ', 'lower', 'above', "lower "vertical", "level", "upper"'"under&Quot;, "Left,", "Right,", "Top", and Bottom " can be obtained relative to this orientation when used with a reference lens. . Blank • A device made of an optical material that can be shaped into a lens. Translucent ", which means that the lens screams its two outer surfaces to form a refractive outer surface. The trimmed lens representation has an optical power that can be any optical power including zero 130295.doc -22-200912425 or flat optical power. The lens can be trimmed and the lens arm carries the wrong master a, and the lens blank has been shaped to have only one trimmed refractive outer surface. The lens (4) may be an "unfinished" lens, which means that none of the outer surface of the lens is formed into a refractive table: Untrimmed or semi-finished lens blank untrimmed

Ο 自由成型(free-forming)之製造製程或藉由更傳統之表面口 工及拋光來修整。經修整之透鏡毛柱尚未使其周邊邊= 形、整邊或修改以配合至眼鏡框架中。為了此定義之目 的,經修整之透鏡毛链為—透鏡。然而,—旦透鏡毛柱經 成形、整邊或修改以配合眼鏡框架,則其不再被稱為透鏡 毛述。 具線紋之多焦點透鏡:具有不同光功率之兩個或兩個以 上相鄰區域的多焦點透鏡,其具有—可由觀看透鏡之佩戴 者之某人看見的可見不連續性。該不連續性引起兩個或兩 個以上區域之間的感覺得到之影像中斷。具線紋之多焦點 透鏡之實例為具線紋之(非混合)雙交點或三焦點透鏡。 無線紋之多焦點透鏡··具有不同光功率之兩個或兩個以 上相鄰區域的多焦點透鏡,其在諸如漸進多焦點鏡片中之 兩個或兩個以上區域之間不具有不連續性或在兩個或兩個 以上區域之間具有不可由觀看透鏡之佩戴者之某人看見的 不可見不連續性。該不連續性引起兩個或兩個以上區域之 間的感覺得到之影像中斷。具有不連續性之無線紋之多焦 點透鏡之一實例為混合雙焦點透鏡^ PAL亦可被稱為無線 紋之多焦點透鏡,但PAL不具有不連續性。 130295.doc -23- 200912425 低附加功率PAL :具有小於侃截I + t _ 、佩戴者在近觀察距離處清楚 地看見之必要近附加光功率的漸進多焦點鏡片。 低附加功率漸進之光功率區 察距離處清楚地看見之必要近 區域。 、多焦點透鏡:具有一個以上焦點或光功率的透鏡。此等 透鏡可為靜態的或動態的多焦點透鏡之實例包括雙Ο Free-forming manufacturing process or trimming with more traditional surface work and polishing. The trimmed lens stub has not been shaped, trimmed, or modified to fit into the eyeglass frame. For the purposes of this definition, the finished lens strand is a lens. However, once the lens column is shaped, trimmed, or modified to fit the eyeglass frame, it is no longer referred to as a lens. A multi-focal lens with a line: a multifocal lens having two or more adjacent regions of different optical power, having a visible discontinuity that can be seen by someone viewing the wearer of the lens. This discontinuity causes a perceived interruption in the image between two or more regions. Examples of multi-focal lenses with lines are lined (non-mixed) double intersection or triple focus lenses. Wireless multifocal lens · Multifocal lens with two or more adjacent regions of different optical power, without discontinuity between two or more regions, such as progressive multifocal lenses Or between two or more regions having invisible discontinuities that are not visible to someone wearing the wearer of the viewing lens. This discontinuity causes a perceived interruption in the image between two or more regions. An example of a multifocal point lens having a discontinuous wireless pattern is a hybrid bifocal lens. PAL may also be referred to as a wireless multifocal lens, but PAL does not have discontinuities. 130295.doc -23- 200912425 Low additional power PAL: A progressive multifocal lens with less than the interception I + t _ and the necessary near-additional optical power that the wearer clearly sees at a near viewing distance. The low-power-advanced progressive optical power zone clearly sees the necessary near-area at the distance. Multifocal lens: A lens with more than one focus or optical power. Examples of such lenses that can be static or dynamic multifocal lenses include dual

焦點透鏡、三焦點透鏡或漸進多焦點鏡片。動態多隹點透 鏡包括(僅舉例而言)電活性透鏡。視所用電極之類型‘、施 加至電極之電μ ’及在液晶之薄層内改變的折射率而定, 可將各種光功率形成於電活性透鏡中。動態多焦點透鏡亦 包括(僅舉例而言)包含適型光學部件之透鏡,諸如,玻璃 透鏡及流體透鏡、兩個或兩個以上可移動部件調整光功率 的機械可調整透鏡’或電凹凸透鏡。多焦點透鏡亦可為靜 態及動態之組合。舉例而言,一電活性元件可用於與以下Focus lens, trifocal lens or progressive multifocal lens. Dynamic multi-point lenses include, by way of example only, electroactive lenses. Depending on the type of electrode used, the electrical μ applied to the electrode, and the refractive index that changes within the thin layer of liquid crystal, various optical powers can be formed in the electroactive lens. Dynamic multifocal lenses also include, by way of example only, lenses comprising suitable optical components, such as glass lenses and fluid lenses, mechanically adjustable lenses that adjust the optical power of two or more movable components, or electrical meniscus lenses. . Multifocal lenses can also be a combination of static and dynamic. For example, an electroactive element can be used with the following

U 域:具有小於佩戴者在近觀 附加光功率的漸進之光功率 透鏡光通信:一靜態球面透鏡、一靜態單視力透鏡、—靜 態多焦點透鏡(諸如’僅舉例而言’一漸進多焦點鏡片)、 一平頂28雙焦點透鏡,或一平頂7χ28三焦點透鏡。在多數 (但並非所有)情況下,多焦點透鏡為折射性透鏡。在某些 情況下,多焦點透鏡可包含繞射光學器件及/或繞射與折 射光學器件之組合。 、 離區·3有允許使用者在近距離處清楚地看見之光 功率之透鏡的部分或區域。近距離區亦可被稱為近視力 區0 130295.doc 24- 200912425 近距離:僅舉例而言,吾人在閱讀書本時、在穿針引線 時或在讀取藥瓶上之說明時觀看到的距離。此距離通常 (但並非總是)被認為距眼睛介於大約1〇吋與大約16吋之 間。近距離亦可被稱為近觀察距離及近距離點。 辦公室透鏡/辦公室PAL:-種特定設計之職業漸進多焦 點鏡片,其以主要中間距離視力區取代遠距離視力區且通 常在近距離區提供近距離視力及在中間距離區提供中間距 離視力。光功率自近距離區遞減至中間距離區。總光功率 〇 遞減為相比佩戴者之典型近距離附加功率而言的較小光功 率改變。因此,較寬中間距離視力得、藉由較寬通道寬度及 亦由較寬閱讀寬度來提供。此係借助於通常允許配合十字 上方的較大值之不當散光的光學設計來完成。由於此等特 徵,此類PAL良好地適用於辦公桌工作,但吾人不能駕駛 汽車或使用此類PAL在辦公室或家周圍散步,因為該透鏡 含有很少(若存在)遠距離觀察區。 目艮科透鏡:-適用於視力校正之透鏡,其包括(僅舉例 U 而言)眼鏡片、隱形眼鏡、眼内透鏡(intra-ocuiar lens)、角 膜甘欠體’及角膜覆蓋體(corneal on-lay)。 光通信:兩個或兩個以上光功率區域以某一方式對準使 -- 得光通過經對準之區域且經受等於光通過之點處之每一個 別區域的光功率之和的組合光功率的狀態。該等區域可嵌 入在透鏡内或相同透鏡或不同透鏡之相對表面上。 光功率區域:具有光功率之透鏡的區域。 光功率之平台:具有跨越區域或區之水平寬度及/或垂 130295.doc -25- 200912425 直長度之大致怪定光功率的透鏡之區域或區。或者,光功 率改變可為跨越區域或區之水平寬度及/或垂直長度的每 毫米大約0.05D或更少的平均值。作為另一替代,光功率 改變可為跨越區域或區之水平寬度及/或垂直長度的每毫 米大約0.10D或更少的平均值。作為最終替代,光功率改 變可為跨越區域或區之水平寬度及/或垂直長度的每毫米 大約0.20D或更少的平均值。區域或區可具有大約】爪爪或 更大的水平寬度及/或垂直長度。作為一替代’區域或區 可具有大約1 mm至大約3 mm或更大的水平寬度及/或垂直 長度。作為一最終替代,區域或區可具有大約2 至大約 6 mm或更大的水平寬度及/或垂直長度。光功率之平台允 許區域内之光功率的垂直穩定性及/或水平穩定性。可由 透鏡之佩戴者藉由上下移動其頦或藉由左右觀看來視覺地 識別光功率之平台。若區域具有光功率之平台,則佩戴者 將注意到,在給定距離處之物件貫穿該區域而大致保持聚 焦。區域或區可為透鏡之遠距離區、上部遠-中間距離 區、中間距離區、近距離區、下部遠_中間距離區,或任 何其他區域。 漸進多焦點區域:PAL之-連續區域,其供應pAL之遠 距離區與PAL之近距離區之間的一連續、增加之光功率。 在該區域之起始處之遠距離區中《附加功率為大約+〇遍 或更小。在一些情況下,該區域可在於透鏡之近距離區中 達到全附加功率之後供應一降低之光功率。 漸進多焦點表面:PAL之一連續表面,其供應pAL之遠 130295.doc -26- 200912425 距離區與PAL之近距離區之間的一連續、增加之光功率。 在該表面之起始處之遠距離區中之附加功率為大約 或更小。在一些情況下,該表面可在於透鏡之近距離區中 達到全附加功率之後供應一降低之光功率。 漸進之光功率區域•·透鏡之一區域,其通常在該區域之 上部部分中具有第一光功率及通常在該區域之下部部分中 具有第二光功率,其中該兩者之間存在光功率之連續改 變。漸進之光功_區域可在透鏡之一纟面上或礙人在透鏡 内。漸進之光功率區域可包含被稱為”漸進之光功率表面” 之一或多個表面構形。漸進之光功率表面可在透鏡之任一 表面上或埋入於透鏡内。據信漸進之光功率區域在光功率 增加到超過相鄰視力區之光功率時,,開始•,或"起始"。通 常’此增加為+〇.12D或更大之正光功率。漸進之光功率區 域之起始處的增加之光功率可由正光功率之大致連續增加 引起。或者’漸進之光功率區域之起始處的附加功率可由 為漸進之光功率區域之部分或不同光功率區域之部分的光 力率之步級引起。光功率之步級可由不連續性引起。漸進 之光功率區域之光功率可在達到其最大附加功率之後降 低。漸進之光功率區域可如在習知漸進多焦點鏡片中開始 於配合點處或附近或可如在本發明之實施例中開始於配合 點之下方。 閱讀寬度:透鏡之近距離觀察部分内之最窄水平寬度, 其藉由佩戴者之0.25D近距離觀察光功率校正内之光功率 提供清楚、大致無失真之校正。 130295.doc •27· 200912425 短通道長度:歸因於眼鏡款式之美學關注或傾向,可能 需要使被垂直縮短之透鏡配合至具有窄、垂直高度的框架 式樣中。在此透鏡中,亦自然地縮短通道。短通道長度指 代縮短透鏡中之通道的長度。此等通道長度通常(但並非 總是)介於大約9 mm與大約13 mm之間。通常,較短通道 長度意謂較窄通道寬度及更多不當散光。較短通道設計有 時被稱為具有與硬"漸進多焦點鏡片設計相關聯的某些特 徵,因為遠距離校正與近距離校正之間的過渡歸因於由較 短垂直通道長度所引起的光功率之較陡增加而較硬。 軟式漸進多焦點鏡片:具有遠距離校正與近距離校正之 間的較平緩過渡之漸進多焦點鏡片。此較平緩過渡引起增 加里之不虽政光。在軟式pAL中,增加量之不當散光可侵 入穿過配合點定位之跨越透鏡而延伸的假想水平線上方。 軟式PAL亦可具有較長通道長度及較寬通道寬度。"經修改 之軟式漸進多焦點鏡片”為一具有經修改之光學設計的軟 式pal,該設計具有硬式PAL之特徵中之一或多者,諸 如·較陡之光功率過渡、較短通道、較窄通道、推進至透 鏡之觀察部分中之較多不當散光,及配合點下方之較多不 當散光。 ' 靜態透鏡:具有不可隨著電能、機械能或力的施加而改 變之光功率的透鏡。靜態透鏡之實例包括球面透鏡、圓柱 透鏡、漸進多焦點鏡片、雙焦點透鏡及三焦點透鏡。靜態 透鏡亦可被稱為固定透鏡。 光功率之步級.可導致光功率不連續性之兩個光學區或 130295.doc -28- 200912425 區域之間的光功率差。光功率 刀十差可為光功率 光功率在透鏡之上部部分與下部部分之間增加Γ光功^差 =先功率之步降,其中光功率在透鏡之上部部分盘下部 邛刀之間降低。舉例而言,若U-domain: progressive optical power lens communication with less than the wearer's close-up additional optical power: a static spherical lens, a static single vision lens, a static multifocal lens (such as 'only for example' a progressive multifocal Lens), a flat top 28 bifocal lens, or a flat top 7χ28 trifocal lens. In most, but not all, cases, the multifocal lens is a refractive lens. In some cases, the multifocal lens may comprise a combination of diffractive optics and/or diffractive and refractive optics. The detachment area 3 has a portion or region of the lens that allows the user to clearly see the power of the light at a close distance. The close range can also be referred to as the near vision zone. 0 130295.doc 24- 200912425 Close range: For example only, the distance we see when reading a book, when threading a needle, or when reading a description on a vial. . This distance is usually (but not always) considered to be between about 1 〇吋 and about 16 距 from the eye. Close range can also be referred to as near observation distance and close distance point. Office Lens/Office PAL: A specially designed professional progressive multifocal point lens that replaces the long range vision zone with a primary intermediate distance vision zone and typically provides near vision in the close range and mid-range vision in the intermediate zone. The optical power is reduced from the close range to the intermediate distance zone. The total optical power 〇 is reduced to a smaller optical power change than the typical close-range additional power of the wearer. Therefore, a wider intermediate distance vision is provided by a wider channel width and also by a wider reading width. This is done by means of an optical design that generally allows for improper astigmatism that fits a larger value above the cross. Because of these characteristics, such PALs are well suited for desk work, but we cannot drive a car or use such PALs to walk around the office or home because the lens contains little, if any, remote viewing area. Target lenses: - lenses for vision correction, including (for example only U) ophthalmic lenses, contact lenses, intra-ocuiar lenses, corneal bodies, and corneal on -lay). Optical communication: a combination of two or more optical power regions aligned in such a way that light passes through the aligned regions and undergoes a sum of optical power equal to each individual region at the point at which the light passes. The state of power. These regions can be embedded in the lens or on the opposite surface of the same lens or different lenses. Optical power area: The area of the lens with optical power. Platform for optical power: A region or region of a lens that has a horizontal width across a region or region and/or a straightforward length of the lens. Alternatively, the change in optical power may be an average of about 0.05 D or less per millimeter across the horizontal width and/or vertical length of the region or zone. As a further alternative, the optical power change can be an average of about 0.10 D or less per millimeter across the horizontal width and/or vertical length of the region or zone. As a final alternative, the optical power change can be an average of about 0.20 D or less per millimeter across the horizontal width and/or vertical length of the zone or zone. The area or zone may have approximately a claw or a greater horizontal width and/or vertical length. As an alternative 'area or zone may have a horizontal width and/or a vertical length of from about 1 mm to about 3 mm or more. As a final alternative, the regions or zones may have a horizontal width and/or a vertical length of from about 2 to about 6 mm or greater. The optical power platform allows vertical stability and/or horizontal stability of the optical power in the area. The platform of the optical power can be visually identified by the wearer of the lens by moving it up and down or by viewing left and right. If the area has a platform for optical power, the wearer will notice that the object at a given distance extends through the area to substantially maintain focus. The area or zone may be the long range of the lens, the upper far-middle distance zone, the intermediate zone zone, the close range zone, the lower far-middle zone zone, or any other zone. Progressive multifocal area: PAL-continuous area that supplies a continuous, increasing optical power between the remote area of the pAL and the close range of the PAL. The additional power is about +〇 or less in the long range at the beginning of the area. In some cases, the region may supply a reduced optical power after reaching full additional power in the close range of the lens. Progressive multifocal surface: One continuous surface of PAL, which supplies the distance of pAL 130295.doc -26- 200912425 A continuous, increasing optical power between the distance zone and the PAL close range. The additional power in the remote zone at the beginning of the surface is about or less. In some cases, the surface may be supplied with a reduced optical power after reaching full additional power in the close range of the lens. Progressive optical power region • a region of a lens that typically has a first optical power in an upper portion of the region and typically a second optical power in a lower portion of the region, wherein optical power exists between the two Continuous change. The progressive optical work _ region can be on one of the lenses or in the lens. The progressive optical power region may comprise one or more surface configurations referred to as "progressive optical power surfaces." The progressive optical power surface can be on either surface of the lens or embedded in the lens. It is believed that the progressive optical power region begins with •, or "start" when the optical power increases beyond the optical power of the adjacent vision zone. Usually, this increase is positive light power of +〇.12D or more. The increased optical power at the beginning of the progressive optical power region can be caused by a substantially continuous increase in positive optical power. Alternatively, the additional power at the beginning of the 'gradual optical power region' may be caused by a step of the optical power rate of a portion of the progressive optical power region or a portion of the different optical power regions. The step of optical power can be caused by discontinuity. The optical power of the progressive optical power region can be reduced after reaching its maximum additional power. The progressive optical power region can begin at or near the mating point as in a conventional progressive multifocal lens or can begin below the mating point as in embodiments of the invention. Reading Width: The narrowest horizontal width in the close-view portion of the lens, which provides a clear, substantially distortion-free correction by observing the optical power within the optical power correction by the wearer's 0.25D close range. 130295.doc •27· 200912425 Short channel length: Due to the aesthetic focus or tendency of the eyewear style, it may be necessary to fit the vertically shortened lens into a frame pattern with a narrow, vertical height. In this lens, the passage is also naturally shortened. The short channel length refers to shortening the length of the channel in the lens. These channel lengths are usually (but not always) between about 9 mm and about 13 mm. Generally, a shorter channel length means a narrower channel width and more improper astigmatism. Shorter channel designs are sometimes referred to as having certain features associated with hard " progressive multifocal lens designs because the transition between distance correction and close distance correction is due to the length of the shorter vertical channel The optical power is steeper and harder. Soft progressive multifocal lens: A progressively multifocal lens with a gentle transition between long range correction and close distance correction. This relatively flat transition caused an increase in the political light. In soft pAL, an increased amount of improper astigmatism can invade an imaginary horizontal line extending across the lens through the mating point. Soft PALs can also have longer channel lengths and wider channel widths. "Modified Soft Progressive Multifocal Lens" is a soft pal with a modified optical design that has one or more of the features of a hard PAL, such as a steeper optical power transition, a shorter channel, Narrow channels, more improper astigmatism propelled into the viewing portion of the lens, and more improper astigmatism below the fit point. 'Static lens: A lens with optical power that cannot be changed with the application of electrical energy, mechanical energy or force. Examples of static lenses include spherical lenses, cylindrical lenses, progressive multifocal lenses, bifocal lenses, and trifocal lenses. Static lenses can also be referred to as fixed lenses. The step of optical power can cause two optical power discontinuities. Optical zone or optical power difference between 130295.doc -28- 200912425. The optical power knife difference can be the optical power optical power between the upper part and the lower part of the lens to increase the light power difference = first power Step down, where the optical power is reduced between the lower part of the upper part of the lens. For example, if

之# #奎曰丨λ 、兄之上部部分具有+1.00D 之先功率’則+〇.5〇D之光 步升”將在光功率步升(或 不連續性)之後立即產生具有+1 〆 ’D之光功率的透鏡之下 部部分。下部區域中之光功率 據稱係由光功率之步級,,形 攻 0 不當散光:在透鏡内找到的不告 .u 士、日^ J +田散先,其並非患者之處 方視力校正之部分,而為歸因於 口听口於結合兩個光功率區的光功 率之平滑梯度的透鏡之光學設叶 予又寸之甽產物。儘管一透鏡可 具有跨越各種屈光度之透鏡之不同區的變化之不當散光, 但術語’’不當散光”通常係指在透鏡中找到的最大不當散 光。不當散光亦可進-步特徵化為相對於整個透鏡定位於 透鏡之特定部分内的不當散光。在此情況下,使用修飾語 於指示僅考慮透鏡之特定部分内之不當散光。透鏡之佩戴 者將感覺不當散光為由透鏡引起之模糊及/或《真。在光 學工業内眾所周知且被接受的,只要透鏡之不當散光及失 真為大約1.00D或更小,則透鏡之使用者在多數情況下將 幾乎不會注意到。 光功率之垂直穩定性:具有跨越區域或區之垂直長度之 大致良疋光功率的透鏡之區域或區。或者,光功率改變可 為跨越區域或區之垂直長度的每毫米大約0.05D或更少的 平均值。作為另一替代’光功率改變可為跨越區域或區之 130295.doc -29- 200912425 垂直長度的每毫米大約〇.1〇D或更少的平均值。作為最終 替代,光功率改變可為跨越區域或區之垂直長度的每毫米 大約0.20D或更少的平均值。區域或區可具有大約】匪或 更大的垂直長度。作為-替代,區域或區可具有大約imm 至大約3 mm或更大的垂直長度。作為最終替代區域或區 可具有大約2 mm至大約6 mm或更大的垂直長度。區域或 區可為透鏡之遠距離區、上部遠-中間距離區、中間距離 區、近距離區、下部遠-中間距離區,或任何其他區域。 視力之垂直穩定性:據信透鏡之一區域或區在該區域或 區在使用者跨越該區域或區上下觀看時具有大致恆定清楚 視力的情況下具有視力之垂直穩定性。然而,應指出,雖 然PAL具有自遠距離區至近距離區之清楚視力,但此等區 之間的光功率被混合。因此,PAL具有遠距離區與近距離 區之間的視力之混合穩定性。因此,卩^^^具有遠距離區與 近距離區之間的光功率之非常有限的垂直穩定性。區域或 區可具有大約1 mm或更大的垂直長度。作為一替代,區域 或區可具有大約1 mm至大約3 mm或更大的垂直長度。作 為最終替代,區域或區可具有大約2 mm至大約6 mm或更 大的垂直長度。區域或區可為透鏡之遠距離區、上部遠一 中間距離區、中間距離區、近距離區、下部遠-中間距離 區,或任何其他區域。 本文所揭示之本發明係關於解決與PAL相關聯之問題中 之許多(若並非多數)的光學設計、透鏡及眼鏡系統之實施 例。此外’本文所揭示之本發明顯著消除與pal相關聯之 130295.doc •30- 200912425 視力損害中的多數。本發明提供一種為佩戴者達成適當遠 距離、中間距離及近距離光功率同時提供用於各種距離之 大致連續聚焦能力的構件。本發明亦可提供一種為佩戴者 達成適當上部遠-中間距離及/或下部遠_中間距離光功率同 時提供用於各種距離之大致連續聚焦能力的構件。本文所 揭不之本發明具有遠小於PAL的不當散光。本文所揭示之 本發明允許藉由以+0.12D步級或+〇 25D步級之自+1 〇〇〇至 +3.50D之附加功率的全範圍之老花校正。對於+3 〇〇d以下 〇 t附加功率處方而言,本發明通常將不當散光保持為大約 1.00D或更小的最大值。對於某些高附加功率處方(諸如, 〇D +3.2 5D ’及+3.50D)而言,本發明通常將不當散 光保持為大約1.50D的最大值。 本文所揭示之發明性透鏡及透鏡設計之實施例允許將兩 個離散光學元件光學地組合成一個多焦點透鏡。第一光學 70件可具有一供應一大致球面光功率的大致球面功率區 . 4。第二光學元件可具有-供應-漸進之光功率的漸進之 ^ 《功率區域°供應漸進之光功率之第二光學元件並不提供 用於使用者在近距離處清楚地觀看的足夠附加功率。供應 — Μ球面光功率之第—光學元件提供—除由第二光學㈣ ' 賴供之光功率以外的光功率’以允許制者在近距離處 清楚地觀看。由於附加功率之部分係由供應大致球面光功 率之第-光學TG件提供,因此多焦點透鏡具有比具有相同 總附加功率之PAL少的不當散光。 在本發明之-實施例中,第―光學元件可為具有與透鏡 130295.doc •31 - 200912425 之周圍材料不同的折射率之埋入式繞射光學器件。在另— 實施例中’第_光學元件可為具有與透鏡之周圍材料不同 的折射率之埋入式折射光學器件。在另一實施例中,第— 光學7C件可為埋入式電活性元件。在另一實施例中,第一 光予7〇件可在透鏡之一個或兩個表面上且可(例如)藉由研 磨板製、表面鑄造、衝壓,或自由成型發明性透鏡之一 外表面來提供。 在本發明之一實施例中,第二光學元件可在透鏡之一個 或兩個表面上且可(例如)藉由研磨、模製、表面鑄造、衝 壓,或自由成型本發明之透鏡之一外表面來提供。在另— 實施例十,第二光學元件可埋入於透鏡内且具有不同於透 鏡之周圍材料之折射率的折射率之梯度。通常(但並非總 疋)若光學元件中之一者埋入於透鏡内,則另一光學元件 疋位於透鏡之一個或兩個外表面上。 在本發明之一實施例中,供應大致球面光功率之第一光 學7L件與供應漸進之光功率的第二光學元件之至少一部分 光通信。在另一實施例中,供應大致球面光功率之第一光 子元件及供應漸進之光功率的第二光學元件經數學地組人 成單一光學元件,該單一光學元件可在透鏡之一外部折射 表面上或埋入於透鏡内。 本發明之實施例提供:供應大致球面光功率之第一光學 7G件及供應漸進之光功率的第二光學元件的適當對準及定 位。本發明之實施例亦提供:由大致球面功率區域所提供 之光功率的量、由漸進之光功率區域所提供之光功率的 130295.doc •32- 200912425 量,及漸進之光功率區域之光學設計。本發明之實施例亦 k供·大致球面功率區域的大小及形狀及漸進之光功率區 域的大小及形狀。此等設計參數之組合允許很高級之光學 没汁’與當今市售之技術現狀PAL相比,該設計具有較少 不當散光及失真以及較寬通道寬度及較短通道長度。 應指出’諸圖及在諸圖中所展示之任何特徵並未按比例 繪製。圖14A展示根據本發明之一實施例之透鏡之前表面 的視圖。圖14B展示本發明之一不同實施例之前表面的視 圖。圖14A至圖14B展示發明性透鏡之前凸表面具有兩個 光功率區域。第一光功率區域為透鏡之上部部分中之遠距 離區1410。第一光功率區域為透鏡之下部部分中供應加成 光功率的大致球面功率區域1420。在圖14A中,大致球面 功率區域呈透鏡之弓形區段之形狀。可將該弓形區段想為 具有遠大於透鏡之直徑的直徑之圓形區域。由於該圓形區 域對於透鏡而言過大,因此僅其圓周之頂部弓形配合在透 鏡内。在圖14B中,大致球面功率區域為圓形形狀。大致 球面功率區域定位於配合點1430下方。或者,大致球面功 率區域可定位於配合點處或上方。光功率之不連續性存在 於遠距離區與大致球面功率區域之間。不連續性之至少一 部分可由定位於兩個光功率區域之間的混合區144〇混合。 混合區可為大約2.0 mm寬或更小或大約〇 5 mm寬或更小。 圖14C展示透鏡之背表面的視圖。圖uc展示透鏡之背凹 表面具有供應加成光功率的漸進之光功率區域145〇。應指 出,當在透鏡之背凹表面上發現漸進之光功率區域時,^ 130295.doc -33- 200912425##奎曰丨λ, the upper part of the brother has a power of +1.00D, then +〇.5〇D of the light step will be generated immediately after the optical power step (or discontinuity).之下'D light power of the lower part of the lens. The optical power in the lower area is said to be the step of light power, shape attack 0 improper astigmatism: not found in the lens. u, Shi, ^ J + Tian Sanxian, which is not part of the patient's vision correction, is the product of the lens that is attributed to the smoothing gradient of the optical power combining the optical power of the two optical power zones. The lens may have a variation of improper astigmatism across different regions of the lens of various diopter, but the term ''inappropriate astigmatism') generally refers to the largest improper astigmatism found in the lens. Improper astigmatism can also be characterized as improper astigmatism that is positioned within a particular portion of the lens relative to the entire lens. In this case, the modifier is used to indicate that only improper astigmatism within a particular portion of the lens is considered. The wearer of the lens will feel that the astigmatism is blurred by the lens and/or "true." It is well known and accepted in the optical industry that as long as the improper astigmatism and distortion of the lens is about 1.00 D or less, the user of the lens will hardly notice in most cases. Vertical stability of optical power: A region or region of a lens having substantially good optical power that spans the vertical length of the region or region. Alternatively, the optical power change can be an average of about 0.05 D or less per millimeter across the vertical length of the region or zone. As an alternative, the optical power change can be an average of about 〇.1〇D or less per millimeter of the vertical length of the region or zone 130295.doc -29-200912425. As a final alternative, the optical power change can be an average of about 0.20 D or less per millimeter across the vertical length of the zone or zone. The area or zone may have a vertical length of about 匪 or greater. As an alternative, the region or zone may have a vertical length of from about imm to about 3 mm or more. The final replacement area or zone may have a vertical length of from about 2 mm to about 6 mm or more. The area or zone may be the long range of the lens, the upper far-middle distance zone, the intermediate zone zone, the close zone zone, the lower far-middle zone zone, or any other zone. Vertical Stability of Vision: It is believed that a region or region of the lens has vertical stability of vision in the region or region with substantially constant clear vision when viewed by the user across the region or region. However, it should be noted that although PAL has clear vision from a long range to a close range, the optical power between such areas is mixed. Therefore, PAL has a mixed stability of vision between a distant area and a close range. Therefore, 卩^^^ has a very limited vertical stability of optical power between the distant zone and the close zone. The area or zone may have a vertical length of about 1 mm or more. As an alternative, the regions or zones may have a vertical length of from about 1 mm to about 3 mm or more. As a final alternative, the zones or zones may have a vertical length of from about 2 mm to about 6 mm or more. The area or zone may be a long range of lenses, an upper far intermediate distance zone, a middle distance zone, a close range zone, a lower far-middle zone zone, or any other zone. The invention disclosed herein relates to embodiments of optical design, lens and eyeglass systems that address many, if not most, of the problems associated with PAL. Furthermore, the invention disclosed herein significantly eliminates the majority of the visual impairment associated with pal 130295.doc • 30- 200912425. SUMMARY OF THE INVENTION The present invention provides a means for achieving a suitable long range, intermediate distance and close range optical power for a wearer while providing substantially continuous focusing capabilities for various distances. The present invention may also provide a means for providing the wearer with an appropriate upper far-middle distance and/or lower far-intermediate distance optical power while providing substantially continuous focusing capabilities for various distances. The invention disclosed herein has an improper astigmatism that is much smaller than PAL. The invention disclosed herein allows for full range of presbyopia corrections with additional power from +1 〇〇〇 to +3.50 D in steps of +0.12D or +〇 25D. For additional power prescriptions of +3 〇〇d 〇 t, the present invention typically maintains improper astigmatism at a maximum of about 1.00 D or less. For certain high additional power prescriptions (such as 〇D +3.2 5D ' and +3.50D), the present invention typically maintains improper astigmatism at a maximum of about 1.50D. Embodiments of the inventive lens and lens designs disclosed herein allow for the optical combination of two discrete optical elements into one multifocal lens. The first optical member 70 can have a substantially spherical power region that supplies a substantially spherical optical power. The second optical element can have a progressive supply of - supply-progressive optical power. ^ Power Zone ° The second optical component that supplies progressive optical power does not provide sufficient additional power for the user to clearly view at close range. Supply - the first part of the Μ spherical power - the optical element provides - in addition to the optical power other than the optical power supplied by the second optical (4) to allow the producer to clearly see at close range. Since the portion of the additional power is provided by the first optical TG member that supplies substantially spherical optical power, the multifocal lens has less astigmatism than the PAL having the same total additional power. In an embodiment of the invention, the first optical element may be a buried diffractive optic having a refractive index different from that of the surrounding material of the lens 130295.doc • 31 - 200912425. In another embodiment, the 'optical optical element can be a buried refractive optical device having a refractive index different from the material surrounding the lens. In another embodiment, the first optical 7C member can be a buried electroactive element. In another embodiment, the first light can be on one or both surfaces of the lens and can be formed, for example, by grinding, surface casting, stamping, or free forming one of the outer surfaces of the inventive lens. Come on. In an embodiment of the invention, the second optical element may be on one or both surfaces of the lens and may be, for example, by grinding, molding, surface casting, stamping, or free forming one of the lenses of the present invention. The surface is provided. In another embodiment 10, the second optical element can be embedded within the lens and have a gradient of refractive index that is different from the refractive index of the material surrounding the lens. Typically (but not always), if one of the optical components is embedded in the lens, the other optical component is located on one or both outer surfaces of the lens. In one embodiment of the invention, the first optical 7L member that supplies substantially spherical optical power is in optical communication with at least a portion of the second optical component that supplies progressive optical power. In another embodiment, a first photonic element that supplies substantially spherical optical power and a second optical element that supplies progressive optical power are mathematically grouped into a single optical element that can refract surface outside of one of the lenses Upper or buried in the lens. Embodiments of the present invention provide for proper alignment and positioning of a first optical 7G component that supplies substantially spherical optical power and a second optical component that supplies progressive optical power. Embodiments of the present invention also provide for the amount of optical power provided by the substantially spherical power region, the amount of optical power provided by the progressive optical power region, 130295.doc • 32-200912425, and the optical power of the progressive optical power region. design. Embodiments of the present invention also provide for the size and shape of the substantially spherical power region and the size and shape of the progressive optical power region. The combination of these design parameters allows for a very advanced optical immersion' which has less improper astigmatism and distortion and a wider channel width and shorter channel length than the current state of the art PAL. It should be noted that the drawings and any features shown in the figures are not drawn to scale. Figure 14A shows a view of a front surface of a lens in accordance with an embodiment of the present invention. Figure 14B shows a view of the front surface of a different embodiment of the present invention. Figures 14A-14B show the convex surface of the inventive lens having two regions of optical power. The first optical power region is a remote separation region 1410 in the upper portion of the lens. The first optical power region is a substantially spherical power region 1420 that supplies additive optical power in the lower portion of the lens. In Fig. 14A, the substantially spherical power region is in the shape of an arcuate segment of the lens. The arcuate segment can be thought of as a circular region having a diameter that is much larger than the diameter of the lens. Since the circular area is too large for the lens, only the top of its circumference is arcuately fitted within the lens. In Fig. 14B, the substantially spherical power region has a circular shape. The approximate spherical power region is positioned below the mating point 1430. Alternatively, the approximate spherical power region can be positioned at or above the mating point. The discontinuity of optical power exists between the long range and the substantially spherical power area. At least a portion of the discontinuity may be mixed by a mixing zone 144 that is positioned between the two optical power regions. The mixing zone can be about 2.0 mm wide or less or about 〇 5 mm wide or smaller. Figure 14C shows a view of the back surface of the lens. Figure uc shows the back concave surface of the lens with a progressive optical power region 145 供应 that supplies the added light power. It should be noted that when a progressive optical power region is found on the concave surface of the lens, ^ 130295.doc -33- 200912425

多數(但並非所有)情況下,背凹表面亦包含環面曲線以校 正患者之散光折射誤差。漸進之光功率區域起始於透鏡之 配合點下方。或者,圖14D展示起始於透鏡之配合點處或 附近的漸進之光功率區域。當漸進之光功率區域起始於大 致球面功率區域之上部邊緣處時,如在圖14D中,提供光 功率之步級(Step)1470,其附加至提供於漸進之光功率之 起始處的光功率。當漸進之光功率區域開始於大致球面功 率區域上方(未圖示)時,大致球面功率區域之上部邊緣引 起跨越漸進之光功率區域之通道的不連續性。 圖14E展示穿過透鏡之中心垂直線所截取的圖i4A及圖 14C之透鏡的橫截面圖。如在圖14E中可見,一遠距離光 功率1415提供於遠距離區中。大致球面功率區域及漸進之 光功率區域經對準以與彼此光通信,使得由每一區域所供 應之光功率在近距離區146〇中組合以為使用者提供總近距 離附加功率1465。漸進之光功率區域開始於配合點下方且 結束於透鏡之底部處或上方。圖14F自前面展示發明性透 鏡,其展示在透鏡之前|面及背表面上圖l4A及圖之 光功率區域的置放及光學對準。圖UG自前面展示發明性 透鏡,其展示在透鏡之前表面及背表面上圖14B及圖Μ 之光功率區域的置放及光學對準。如在圖"f及圖“G中 均可見’漸進之光功率區域起始於大致球面功率區域之至 少一部分處且被間隔開且在不連續性下方。 如上文所提及’在本發明之—些實施例中,大致球面功 率區域、混合區,及漸推夕土丄* 久研進之先功率區域可經數學地組合及 130295.doc -34- 200912425 定位於透鏡之單—表面上。在此實施例之一實例中,透鏡 之佩戴者無需遠距離校正且需要+2 25D之近距離校正。圖 Isa說m立於透鏡之一表面之底部部分中的大致球面 功=區域1510。該透鏡具有一混合區㈣,該混合區㈣ 在遠距離區中之光功率與大致球面功率區域之光功率之間 . 過渡。僅舉例而言,在圖15A之透鏡令,大致球面功率區 - 域具有+1.25D之光功率且遠距離區具有一平的光功率。圖 广 说說明定位於透鏡之—表面上的漸進之光功率區域 ” 刪。如已指此區域可能在前凸表面、背凹表面,或 在前凸表面與背凹表面兩者上。僅舉例 透鏡中,漸進之光功率區域具有+1,_之附加功圖率 15= ⑽明發明性透鏡之單一表面,該單一表面為圖“a中 所展示之透鏡之表面與圖15B中所展示之透鏡之表面的組 合。僅舉例而言’在圖15C中之發明性透鏡中,近距離區 光功率為+2.25"為由大致球面功率區域所供應之 + 1.2扣之光功率與由漸進之光功率區域所供應之+ 1.咖之 ^ 4功率的組合。應注意,在圖況中,漸進之光功率區域 ㉟光學對準以起始於大致球面功率區域之—部分處,且被 ' 間隔開且在混合區下方。 在本發明之-些實施例中’兩個表面可藉由將兩個表面 之幾何形狀數學地添加在-起進而形成一新的單一表面來 組合。此新的單-表面可接著由_模具來製造該模具可 由自由成型或由金剛石車削來生產。該模具可用於生產可 由任何光學實驗室來表面加工的半修整之透鏡毛述。 130295.doc -35- 200912425 藉由以笛卡兒(Cartesian)座標中之幾何函數來描述兩個 表面中之母一者,可將圖15A中之表面與圖15B中所描述 之表面數學地組合以形成圖15C中所展示的新表面,該新 表面為兩個表面之組合。 可將界定或產生大致球面功率區域及混合區之表面劃分 為同等大小的離散區段。可將每一區段分別描述為相對於 固定表面或固定曲率的區域化高度或區域化曲線。此表面 • 可由以下等式來描述: Ζι(χ,β=£|>(Ά) /'=0 y=〇 類似地,可將界定或產生漸進之光功率區域之表面劃分 為同等大小的離散區段,該等區段與上文所提及之區段具 同大】、可將每一區段分別描述為相對於固定表面或 固定曲率的區域化高度或區域化曲線。此表面可由以下等 式來描述: U " /'=0 y=〇 若兩個表面之區段為相同大小,則組合來自每-表面之 區段係直接的。接著可藉由兩個表面之簡單疊加或下式來 描述經組合之表面: Ζ,{χ,γ)=Ζλ(χ,γ)+Ζ2{χ,γ) 130295.doc -36- 200912425 在圖15D中說明此過程。 區段之大小應儘可能小以達成每—表面之料表示。此 外,可在組合兩個表面之後進行漸進之光功率區域的最佳 化,或可預先最佳化漸進之光功率區域以用於更好地組合 大致球面功率區域與混合區。必要時,可不組合混合區且 僅組合大致球面功率區域與漸進之光功率區域。 亦可藉由Menezes之美國專利第M83,9l6號及w〇〇iey等 人之美國專利第6,955,433號中所描述之方法來組合兩個表 面,其全部内容均以引用之方式併入本文中。 發明者已發現在眼科技術中迄今從未以相同方式校正之 一距離範圍的重要性。該距離範圍位於大約29吋與大約5 呎之間,且已發現該距離範圍對於諸如聚焦於吾人之辦公 桌之遠邊緣的任務尤其重要。在先前技術中’此距離範圍 已在很大程度上被忽略,且在先前技術定義中此距離範圍 遠距離或中間距離之類別混在一起。因此,此距離範 圍已作為此等類別中之一者之部分而校正。發明者將此距 離範圍稱為”遠-中間距離"。已發明被稱為"遠_中間距離區,, 之新視力區來提供用於此發明性遠-中間距離之適當聚焦 食b力。本發明之實施例可包括此遠-中間距離區且可最佳 化此區中之光功率來提供遠—中間距離之適當聚焦能力。 本發明之實施例可包括此遠-中間距離區且可最佳化透鏡 中之此區的位置來提供透鏡之適當人體工學使用。當此區 定位於遠距離區與中間距離區之間時,將其稱為"上部遠· 中間距離區”。當此區定位於近距離區下方時,將其稱為 130295.doc -37- 200912425 ”下部遠-中間距離區”。 通常’先前技術多焦點透鏡並不提供遠-中間距離處之 適當聚焦能力或提供遠_中間距離處之僅有限之聚焦能 力舉例而s,雙焦點透鏡之遠距離區域或區經針對個別 佩戴者而開處方以允許在遠觀察距離(諸如,大約2〇呎或 更大的光學無窮遠)處之聚焦能力。然而,應注意,在多 數情況下,相同遠距離光功率將在大約5呎或更大之觀察 距離時對於佩戴者而言足夠。雙焦點透鏡之近距離區域或 p 11經開處方以允許大約1㈣至大約16时之近觀察距離處的 聚焦此力二焦點透鏡允許在遠觀察距離處、近觀察距離 處及中間觀察距離處(自大約16吋至大約29吋)的適當聚 焦忐力。PAL提供遠觀察距離與近觀察距離之間的清楚連 續視力然、而’由於PAL令之光功率自遠距離區連續過渡 至近距離區,因此在PAL之此過渡區中之垂直穩定性非常 有限。 {㈤於PAL ’本文所揭示之發明性透鏡可提供透鏡之特 《區或;^個區中的垂直穩定性…區中之垂直穩定性可由 可引起不連續性的光功率之步級來提供。此外,發明性透 兄可提仏最不刀散至佩戴者之視力的步級或多個步級的位 4。又,發明性透鏡可提供形成步級或多個步級,因此在 吾人觀看透鏡之佩戴者之臉時,通常看*見此等步級。 又發明性透鏡可提供形成步級或多個步級,使得佩戴者 之眼睛可在區之間觀看時(例如,在自遠距離區觀看至近 距離區時)在步級或多個步級之間舒適地平移。最終,在 130295.doc •38· 200912425 本發明之某些實施例中,發日日叫、乐μ , i明性透鏡提供在距佩戴者之眼 睛大約4至5叹與大約叫至12奴間的連續不間斷之聚焦 能力’且具有在佩戴者㈣於遠輯物件與處於距佩戴者 之眼睛小於4至5叹處的物件之間時經舒適過渡的僅單一不 ㈣生。在本發明之其他實施例中,光功率之步級出現於 遠距離區與中間距離區之問,益n 再L弋間,藉此發明性透鏡允許在距佩 戴者之眼睛大約29忖與大約1〇对至12时之間的連續不間斷 之聚焦能力,且具有在佩戴者聚焦於遠距離物件與處於距 佩戴者之«大約29叶處的物件之間時經舒適過渡的僅單 一不連續性。 在本發明之實施例中’可能有必要對準大致球面功率區 域與漸進之光功率區域以確保在遠-中間區中及在中間距 離區中提供正確之總光功率。遠_中間距離區通常具有在 近距離附加功率之大約2〇%與大約44%之間的附加功率。 中間距離區通常具有在近距離附加功率之大約桃與大約 55%之間的附加功率。可能亦有必要對準及定位此等區域 以形成-可用及人體工學上靈活之透鏡以用於在佩戴者之 視線在各種區(遠距離區、遠_中間距離區' 中間距離區, 及近距離區)之間過渡時。最後,亦可能有必要設計存在 於遠距離視力校正與近距離視力校正之間的光功率之梯度 以確保最佳中間距離校正及/或遠-中間距離校正。 在本發明之一實施例中,大致球面功率區域定位於配合 點下方大約0 mm與大約7 mm之間處。在本發明之另一實 施例中,大致球面功率區域定位於配合點下方大約2 mm與 130295.doc •39- 200912425 ^約5咖之間處。在本發明之-實施例中,漸進之光功率 起始於大致球面功率區域之頂部邊緣下方大約2_至 大約議處的大致球面功率區域之一部分處。在本發明 之另一實施例中,漸進之光功率區_始於大致球面功率 區域之頂部邊緣下方大約4酿至大約8顧處的大致球面 功率區域之-部分處。在本發明之—實施例中,遠·中間 距離功率應起始於配合點下方大約3麵與大約4随之間 處且沿通道向下延伸大約4mm。在本發明之一實施例中,In most (but not all) cases, the concave surface also contains a torus curve to correct the astigmatic refractive error of the patient. The progressive optical power region begins below the mating point of the lens. Alternatively, Figure 14D shows a progressive optical power region starting at or near the mating point of the lens. When the progressive optical power region begins at an upper edge of the substantially spherical power region, as in Figure 14D, an optical power step 1470 is provided that is added to the beginning of the progressive optical power. Optical power. When the progressive optical power region begins above the substantially spherical power region (not shown), the upper edge of the substantially spherical power region causes discontinuities in the channel across the progressive optical power region. Figure 14E shows a cross-sectional view of the lenses of Figures i4A and 14C taken through the center vertical line of the lens. As can be seen in Figure 14E, a long range optical power 1415 is provided in the remote zone. The substantially spherical power region and the progressive optical power region are aligned to optically communicate with each other such that the optical power supplied by each region is combined in the close range 146A to provide the user with a total near-field additional power 1465. The progressive light power region begins below the mating point and ends at or above the bottom of the lens. Figure 14F shows the inventive lens from the front showing the placement and optical alignment of the optical power regions of Figure 14A and Figure on the front and back surfaces of the lens. Figure UG shows the inventive lens from the front showing the placement and optical alignment of the optical power regions of Figure 14B and Figure on the front and back surfaces of the lens. As can be seen in both the graph "f and the graph "G, the 'gradual light power region starts at at least a portion of the substantially spherical power region and is spaced apart and below the discontinuity. As mentioned above' in the present invention In some embodiments, the approximate spherical power region, the mixing region, and the progressive power zone can be mathematically combined and 130295.doc -34- 200912425 located on the single-surface of the lens. In one example of this embodiment, the wearer of the lens does not require remote correction and requires close proximity correction of +2 25D. Figure Isa shows the approximate spherical work = area 1510 in the bottom portion of one of the surfaces of the lens. The lens has a mixing zone (four) that transitions between the optical power in the remote zone and the optical power of the substantially spherical power zone. By way of example only, in the lens of Figure 15A, the substantially spherical power zone - The domain has an optical power of +1.25 D and the remote zone has a flat optical power. The figure illustrates the progressive optical power region located on the surface of the lens. This area may be referred to as being on the convex surface, the concave surface, or both the convex surface and the concave surface. In the example lens alone, the progressive optical power region has a +1, _ additional work rate 15 = (10) a single surface of the inventive lens, which is the surface of the lens shown in Figure a and in Figure 15B. A combination of the surfaces of the lenses shown. By way of example only, in the inventive lens of Figure 15C, the optical power at the close range is +2.25" for the optical power of +1.2 buckles supplied by the substantially spherical power region The combination of the power supplied by the progressive optical power region + 1. The combination of the power of the 4 powers. It should be noted that in the picture, the progressive optical power region 35 is optically aligned to start at the portion of the substantially spherical power region, and They are 'spaced apart' and below the mixing zone. In some embodiments of the invention 'two surfaces can be combined by mathematically adding the geometry of the two surfaces to form a new single surface. The new single-surface can then be fabricated from a mold. The mold can be produced by freeform or by diamond turning. The mold can be used to produce semi-trimmed lens representations that can be surfaced by any optical laboratory. 130295.doc -35 - 2009124 25 By describing the parent of the two surfaces as a geometric function in the Cartesian coordinates, the surface in Figure 15A can be mathematically combined with the surface depicted in Figure 15B to form Figure 15C. The new surface is shown, the new surface is a combination of two surfaces. The surface defining or generating the approximate spherical power region and the mixing region can be divided into discrete segments of equal size. Each segment can be described as being relatively fixed Regionalized height or regionalized curve of surface or fixed curvature. This surface can be described by the following equation: Ζι(χ,β=£|>(Ά) /'=0 y=〇 Similarly, it can be defined or The surface that produces the progressive optical power region is divided into discrete segments of equal size, which segments are as large as the segments mentioned above, and each segment can be described as being relative to a fixed surface or fixed The regionalized height or regionalization curve of curvature. This surface can be described by the following equation: U " /'=0 y=〇If the sections of the two surfaces are the same size, combine the sections from each surface Directly. Then by two surfaces A simple superposition or a formula is used to describe the combined surface: Ζ, {χ, γ) = Ζ λ (χ, γ) + Ζ 2 {χ, γ) 130295.doc -36- 200912425 This process is illustrated in Figure 15D. The size should be as small as possible to achieve a per-surface representation. In addition, the progressive optical power region can be optimized after combining the two surfaces, or the progressive optical power region can be optimized in advance for more It is good to combine the approximate spherical power region and the mixed region. If necessary, the mixed region and the combination of the approximate spherical power region and the progressive optical power region may be combined. The US Patent Nos. M83, 9l6 and w〇〇iey of Menezes may also be used. The two surfaces are combined by the method described in U.S. Patent No. 6,955,433, the disclosure of which is incorporated herein by reference. The inventors have found that the importance of a range of distances has never been corrected in the same way in ophthalmic technology. This range of distances is between about 29 吋 and about 5 , and has been found to be particularly important for tasks such as focusing on the far edge of my office table. In the prior art, this range of distances has been largely ignored, and in the prior art definitions this distance range is mixed with the categories of long distances or intermediate distances. Therefore, this range of distances has been corrected as part of one of these categories. The inventor referred to this range of distances as "far-intermediate distance". The invention has been invented as the "far-intermediate distance zone, a new visual zone to provide an appropriate focus for this inventive far-intermediate distance b Embodiments of the invention may include this far-intermediate distance zone and may optimize the optical power in this zone to provide an appropriate focus capability for the far-intermediate distance. Embodiments of the invention may include this far-intermediate distance zone The position of this region in the lens can be optimized to provide proper ergonomic use of the lens. When this region is positioned between the remote zone and the intermediate zone, it is referred to as "upper and middle distance zone ". When this zone is located below the close range, it is called 130295.doc -37- 200912425 "lower far-middle distance zone". Often the 'pre-technical multifocal lens does not provide the proper focus capability at the far-intermediate distance or provides only a limited focus capability at the far-intermediate distance. s, the far-distance region or region of the bifocal lens is for individual wearers. The prescription is prescribed to allow for focusing at a far viewing distance (such as an optical infinity of about 2 〇呎 or greater). However, it should be noted that in most cases, the same long range optical power will be sufficient for the wearer at an observation distance of about 5 Torr or greater. The close range of the bifocal lens or p 11 is pre-specified to allow for focusing at a near viewing distance of about 1 (four) to about 16 o'clock. This force is at the far viewing distance, near the viewing distance, and at the intermediate viewing distance ( Appropriate focus pressure from approximately 16 吋 to approximately 29 吋). PAL provides a clear continuous visual power between the far viewing distance and the near viewing distance, and the vertical stability in the transition zone of PAL is very limited due to the continuous transition of the PAL light power from the long range to the close range. {(5) In PAL' The inventive lens disclosed herein can provide a special "region or a vertical stability in a region". The vertical stability in the region can be provided by the step of optical power that can cause discontinuities. . In addition, the inventive transvestite may provide a step 4 or a plurality of steps that are least smeared to the wearer's vision. Moreover, the inventive lens can provide a step or a plurality of steps, so that when we look at the wearer's face of the lens, it is generally seen to see such steps. The inventive lens can also provide a step or steps such that the wearer's eyes can be viewed between zones (eg, when viewed from a remote zone to a close zone) in steps or steps Panning comfortably. Finally, in some embodiments of the invention, 130295.doc • 38· 200912425, the day of the day, the music, the illuminating lens provides about 4 to 5 sighs from the wearer's eyes and about 12 to slaves. The continuous uninterrupted focus ability' has only a single (four) birth that is comfortably transitioned between the wearer (four) between the object and the object that is less than 4 to 5 sag from the wearer's eye. In other embodiments of the invention, the step of optical power occurs between the remote zone and the intermediate zone, whereby the inventive lens allows for about 29 inches from the wearer's eye. 1 〇 continuous uninterrupted focusing ability between 12 o'clock and with only a single discontinuity through the comfort transition between the wearer focusing on a distant object and the object at about 29 leaves from the wearer Sex. In embodiments of the invention, it may be necessary to align the substantially spherical power region with the progressive optical power region to ensure that the correct total optical power is provided in the far-middle region and in the mid-space separation region. The far-intermediate distance zone typically has an additional power between approximately 2% and approximately 44% of the additional power at close range. The intermediate distance zone typically has an additional power between approximately peach and approximately 55% of the additional power at close range. It may also be necessary to align and position such areas to form an available and ergonomically flexible lens for use in the wearer's line of sight in various zones (distance zone, far_intermediate zone zone intermediate distance zone, and When the transition between the close range). Finally, it may also be necessary to design a gradient of optical power that exists between distance vision correction and near vision correction to ensure optimal intermediate distance correction and/or far-intermediate distance correction. In one embodiment of the invention, the substantially spherical power region is positioned between about 0 mm and about 7 mm below the mating point. In another embodiment of the invention, the substantially spherical power region is positioned between about 2 mm below the mating point and 130295.doc • 39-200912425^ about 5 coffee. In an embodiment of the invention, the progressive optical power begins at about one of the approximately spherical power regions below the top edge of the substantially spherical power region. In another embodiment of the invention, the progressive optical power zone begins at a portion of the substantially spherical power region of about 4 to about 8 points below the top edge of the substantially spherical power region. In an embodiment of the invention, the far-intermediate distance power should originate between about 3 and about 4 below the mating point and about 4 mm down the channel. In an embodiment of the invention,

中間距離功率應起始於遠·中間距離區之後且沿通道向下 延伸大約3 mm至大約4_。前述量測僅為例示性的,且不 意欲限制本發明。 Ο 若大致球面功率區域及漸進之光功率區域未經適當對準 及定位,則透鏡之使用者將不具有透鏡之可用部分中的適 當視力校正。舉例而言’若大致球面功率區域定位為遠高 於配合點,則佩戴者可在直線向前觀看時具有過多用於遠 距離觀察之光功帛。作為另一實{列,若⑯附加功率漸進之 光功率區域在透鏡中定位過高,則由大致球面功率區域及 漸進之光功率區域所提供之中間距離區中的組合光功率可 能對於佩戴者而言過高。 圖16及圖17展示具有+1.25D之近距離附加功率的三個習 知PAL設計(由Essilor登記商標之Essilor Physio™透鏡、由 Essllor 登記商標之 Essilor Ellipse™ 透鏡,及由 Shamir Optical登記商標之Shamir Piccolo™透鏡)。圖16展示由 Rotlex Class P1ustm所量測之關於三個透鏡的附加功率梯 130295.doc -40- 200912425 度。圖17展示如由RoUex登記商標之Rotlex Class PIustm所 量測之三個透鏡中自配合點沿附加功率之通道向下每3 mm 所獲得之量測。 圖18展示在本發明之三個實施例中自配合點沿附加功率 之通道向下每3 mm所獲得之量測。在此等實施例中,圖16 • 及圖17之三個透鏡與具有+1,〇〇D之光功率的大致球面功率 • 區域進行光通信。在此等實施例中,漸進之光功率區域起 . 始於配合點處,且大致球面功率區域之頂部邊緣恰置放在 f) 配合點下方。如自圖Μ可見’在配合點下方9 mm處之透鏡 之附加功率過強。配合點下方9 mm處之透鏡之區域可能通 常為中間距離區之部分。對於+2.25D之近距離附加功率而 言’中間距離附加功率應為+1,12D。然而,Essilor Physio™實施例在距配合點9 mm處具有+1.63〇之附加功 率,Essilor Ellipse™實施例在距配合點9 mm處具有 + 1.82D之附加功率,且shamir Piccolo·™實施例在距配合點 9 mm處具有+1.68D之附加功率。由於在中間距離區中存 〇 在過多附加功率,所以透鏡之使用者可能感覺其眼睛好像 在拉動或橫越。此情形可引起頭痛且使用者將必須將物件 固持為距其眼睛更近來經由此區適當聚焦。因此,若未最 佳化大致球面功率區域及漸進之光功率區域之光功率、置 放及對準’則所得透鏡將具有以下各項中之一或多者:不 良視力人體工學、不良視力舒適度,及不良視力清晰度。 作為另一實例,圖19展示如由R〇tlex Class Plus™所量 測之關於左側發明性透鏡之一實施例及右側Essil〇r 130295.doc • 41 - 200912425The intermediate distance power should start after the far middle distance zone and extend down the channel by about 3 mm to about 4 mm. The foregoing measurements are illustrative only and are not intended to limit the invention. Ο If the approximate spherical power area and the progressive optical power area are not properly aligned and positioned, the user of the lens will not have the proper vision correction in the available portion of the lens. For example, if the approximate spherical power region is positioned much higher than the mating point, the wearer can have too much optical power for long-distance viewing when viewed in a straight line. As another real {column, if the 16 additional power progressive optical power region is positioned too high in the lens, the combined optical power in the intermediate distance region provided by the substantially spherical power region and the progressive optical power region may be for the wearer. Too high. Figures 16 and 17 show three conventional PAL designs with a close range of additional power of +1.25D (Essilor PhysioTM lens by Essilor, Essilor EllipseTM lens by Essllor, and trademarked by Shamir Optical) Shamir PiccoloTM lens). Figure 16 shows an additional power ladder for three lenses measured by Rotlex Class P1ustm 130295.doc -40 - 200912425 degrees. Figure 17 shows the measurement obtained from the mating point of the three lenses in the three lenses as measured by RoRox Class PIustm of the RoUex registered trademark along the additional power channel down every 3 mm. Figure 18 shows the measurements obtained from the mating point along the additional power channel down every 3 mm in three embodiments of the invention. In these embodiments, the three lenses of Figures 16 and 17 are in optical communication with a substantially spherical power • region having optical power of +1, 〇〇D. In these embodiments, the progressive optical power region begins at the mating point and the top edge of the substantially spherical power region is placed just below the f) mating point. As can be seen from the figure, the additional power of the lens at 9 mm below the mating point is too strong. The area of the lens at 9 mm below the fit point may be part of the intermediate distance zone. For the close-range additional power of +2.25D, the intermediate distance additional power should be +1, 12D. However, the Essilor PhysioTM embodiment has an additional power of +1.63 9 9 mm from the mating point, and the Essilor EllipseTM embodiment has an additional power of +1.82 D at 9 mm from the mating point, and the shamir PiccoloTM example is Additional power of +1.68D from 9 mm from the mating point. Since there is too much additional power in the intermediate distance zone, the user of the lens may feel that his or her eyes are pulling or traversing. This situation can cause headaches and the user will have to hold the object closer to his eye to properly focus through this area. Therefore, if the optical power, placement, and alignment of the approximate spherical power region and the progressive optical power region are not optimized, the resulting lens will have one or more of the following: poor vision ergonomics, poor vision Comfort, and poor vision clarity. As another example, Figure 19 shows an embodiment of the left-hand inventive lens as measured by R〇tlex Class PlusTM and the right Essil® 130295.doc • 41 - 200912425

Physio-透鏡兩者的附加功率梯度。發明性透鏡及 Physi。™透鏡兩者具有+2.25D之附加功率。發日月性透鏡具 有一具有+1.25D之光功率的大致球面功率區域及一具有 + 1._之光功率的漸進之光功率區域。漸進之光功率區域 之頂部恰起始於配合點下方,且大致球面功率區域之頂部 定位於配合點下方4 mm處。因此,在大致球面功率區域開 始添加光功率至透鏡之前,存在僅漸進之光功率區域供應 增加之光功率的透鏡之一區域。圖2〇展示如由R〇Uex Class P1US™所量測之兩個透鏡中,自配合點沿附加功率之 通道向下每3 mm所獲得之量測。與在距配合點9瓜⑴處具 有+1.I0D之附加功率的—physi〇TM之實施例相比,發 明性透鏡之此實施例在距配合點9 mm處具有+1 6〇1)之: 加功率。如前所述,絲最佳化大致球面功率區域及漸進 之光功率區域之光功率、置放及對準,則所得透鏡將具有 不良視力人體工學、不良視力舒適度^良視力清晰度。 在由透鏡如在圖18及圖20中之配合點下方15 111111處提供正 確之全附加功率時更為如此。 因此’儘管發明性透鏡之此等實施例與技術現狀隱相 比具有各種優良屬性’但應顯而易見’此等透鏡可被使用 者拒絕。發明性透鏡之實施例在中間距離區中具有過多附 加功率且自配合點至透鏡之底部的光功率梯度過陡。 藉由針對Essilor Physi0™透鏡比較圖j 8及圖2〇中所展示 之附加功率量測,應顯而易見,吾人不能將+1⑽D球面功 率區域添加至圖17之Essilor Physi〇™透鏡且進而接近圖2〇 130295.doc • 42- 200912425 之Essilor Physi〇™透鏡。因此,應顯而易見,大致球面功 率區域及/或漸進之光功率區域必須經特定設計以考慮遠 距離區與近距離區之間的光功率之梯度來提供適當中間距 離校正及/或遠-中間距離校正。 圖21展示發明性透鏡之四個區域:一遠距離區一 上部遠-中間距離區2120、一中間距離區213〇及一近距離 區2140。此等區域並未按比例展示。上部遠-中間距離區 可具有自點Η至點I的高度及自點a至點β的寬度。中間距 離區可具有自點〗至點j的高度及自點c至點D的寬度。近距 離區可具有自點J至點G的高度及自點e至點f的寬度。在本 發明之某些實施例中,發明性透鏡可向佩戴者提供用於遠 距離區及近距離區之適當校正且提供允許佩戴者在遠-中 間距離及中間距離處適當觀看的光功率之最佳化梯度。在 本發明之某些實施例中,透鏡可具有在上部遠-中間距離 區中的視力之垂直穩定性及/或在中間區中的視力之垂直 穩定性。在不具有遠-中間區之本發明之實施例中,中間 距離區可具有增加之視力之垂直穩定性。 額外遠-中間距離區域可提供於近距離區下方。在此實 施例中,此區域可被稱為"下部”遠中間距離區,且在遠距 離區域與中間距離區域之間的遠-中間距離區域可被稱為 "上部”遠-中間距離區域。上部及下部遠-中間區可具有相 同光功率。下部遠-中間區可包括在發明性透鏡設計中以 允許老花佩戴者在向下看時更容易地看見其腳或地板。此 情形在上下樓梯時可提供額外安全性。 130295.doc -43· 200912425 本發明之實施例可包括在透鏡之區域之間的一或多個不 連續性。可藉由不連續表面或藉由透鏡之兩個不同區域之 間的不連續光功率來引起不連續性。可藉由光功率之步升 或步降來引起不連續性。不連續性定義為在透過透鏡觀看 時產生感覺得到之影像中斷的透鏡之表面或透鏡之光功率 - 的任何改變。僅舉例而言,發明者已製造多種發明性透 • 鏡,且已發現當透鏡具有小於大約(MOD之光功率不連續 'ί·生時且當與通常佩戴眼鏡片之方式―致地將透鏡定位於距 〇 目艮睛—距離處時難以感覺到影像中斷、然而,在多數情況 下,可視覺上偵測到大於大約〇 1〇〇至〇 12D之光功率不連 續性。此外,透鏡之佩戴者可感覺得到之此光功率不連續 生可在某些視覺任務(例如,觀察電腦螢幕)期間干擾佩戴 者之視力。應注意,上文關於不連續性所陳述之光功率僅 為實例’且不連續性為在透過透鏡觀看時產生感覺到影像 中斷之能力的透鏡之表面或光功率的任何改變。 ( 發明者已進—步證實,某些不連續性比其他更顯著及/ J $干擾更多。因此,本發明之實施例可包括較不顯著及/ $干擾較少的一或多個不連續性。發明者已發現,與位於 中間距離區、近距離區内的不連續性或中間距離區與近距 • 冑區之間的不連續性相比,使用者在視覺上更好地忍受透 鏡之遠距離區與上部遠_中間距離區之間的不連續性。此 外,發明者已證實,歸因於眼睛在由混合區所形成之任何 影像中斷或模糊上過渡較快,混合不連續性之至少一部分 的混合區之寬度愈窄,眼睛在不連續性上過渡愈好。儘管 130295.doc -44 - 200912425 此情形可能看似指示不連續性因此不應被混合,但此情形 必須由混合不連續性之有利外觀效應來平衡以形成幾乎不 可見之不連續性。 本文所揭示之發明性透鏡之實施例由一或多個不連續性 組成,其中一不連續性可由+0.12D或更大的光功率之步升 來引起。本文所揭示之發明性實施例可具有單一不連續 性,其由一具有小於大約2.0 mm或在大約丨〇爪〇1與〇 5 之間的寬度之混合區至少部分地混合。此寬度之混合區可 由金剛石車削來產生。然而,在本發明之其他實施例中, 並未混合不連續性。在本發明之實施例中,不連續性可由 超過大約+0.25D及在多數情況下超過大約+〇 5〇D的光功率 之步升來引S °光功率之步升及因此不連續性通常(但並 非總是)定位於發明性透鏡之遠距離區與遠_中間距離區之 間。或者,當發明性透鏡不具有遠·中間距離區時,不連 續性通常定位於透鏡之遠距離區與中間距離區之間。圖Μ 及圖26展示在漸進之光功率區域之起始之前的光功率之此 步升。 本發明之所有實施例允許具有光功率之三個可用區的能 力:-遠距離區、—中間距離區,及一近距離區。本發明 之實施例亦可提供具有第四區(上部遠_中間距離區)的能 力,及在一些實施例中亦可提供具有第五區(下部遠-中間 距離區)的能力。本發明之實施例可: a)增加通道之長度以允許光功率之額外2 _至3匪平 M U上部遠_中間㈣校正。此光功率區可在使 130295.doc -45- 200912425 用吾人之電腦或觀看吾人之辦公桌的邊緣時有用。應 注意,增加通道長度可視將容納透鏡之眼鏡框架之垂 直尺寸而為不可能的。 b)增加通道之長度以允許光功率之額外2爪瓜至3爪爪平 台以提供下部遠-中間距離校正。此光功率區可在向 ; 上或向下爬樓梯時觀看吾人之腳或地板時有用。應注 • 意,增加通道長度可視將容納透鏡之眼鏡框架之垂直 尺寸而為不可能的。 p G)利用—或多個不連續性。該或該等不連續性可由光功 率之-或多個步級來引起,其中步級為光功率之步升 或步降。由於不連續性使用非常少(若存在)的透鏡不 動產來步升或步降光功率,所以通道可經設計以允許 2功率之平台而無需延伸通道之長度。重要的係應注 意,光功率之步級愈大,透鏡中可提供給光功率平台 的不動產愈多。在本發明之實施例中,光功率之平台 冑供於不連續性之後且提供遠_中間距離校正。此在 《需添加通道之長度的情況下完成。圖22展示具有光 料之兩個平台223G及2240之本發明之—實施例;且 ® 23展示具有光功率之三個平台233G、測及2350之 - 本發明之一實施例。 d) 保持通道之長度相同,但使光功率在光功率之各種區 之間較快傾斜。應注意,此通常產生伴隨佩戴者之視 力舒適度及眼睛疲勞的問題。 e) 在近距離區下方立即使用光功率之步降以允許下部 130295.doc -46 * 200912425 退-中間距離區。應注意,下部遠-中間距離區可僅在 透鏡之近距離部分下方存在足夠透鏡不動產的情況下 為可能的。 圖22展不沿本發明之一實施例之中心垂直中線的光功 率,該實施例包括將遠距離區連接至近距離區的漸進之光 功率區域。該圖並未按比例繪製。遠距離區中之光功率展 示為平的且因此由父軸2210表示。漸進之光功率區域開始 於透鏡之配合點2220處。或者,漸進之光功率區域可開始 於配合點下方^儘管漸進之光功率區域之光功率在通道之 長度上曰加,但漸進之光功率區域可將光功率之兩個平台 提供於通道内。第一平台2230提供上部遠_中間距離校正 且第二平台2240提供中間距離校正。或者,漸進之光功率 區域提供光功率之單一平台,其提供中間距離校正或遠_ 中間距離校正。光功率之第一平台可具有沿通道之在大約 1 mm與大約6 mm之間或在大約2 mm與大約3 mm之間的垂 直長度。然而,在所有情況下,光功率之平台具有至少大 約1 mm之垂直長度。在光功率之第一平台之後,由漸進之 光功率區域所供應之光功率增加直至光功率之第二平台為 止。光功率之第二平台可具有沿通道之在大約1 mm與大約 6 mm之間或在大約2 mm與大約3 mm之間的垂直長度。在 光功率之第二平台之後’由漸進多焦點區域所供應之光功 率增加直至總近距離光功率達到2250處為止。在達成近距 離光功率之後,由漸進之光功率區域所供應之光功率可開 始降低。若光功率降低至近距離區中之附加功率之大約 130295.doc •47· 200912425 20%至大約44%之間,則可提供一下部遠-中間區。 圖23展不/σ本發明之一實施例之中心垂直中線的光功 率,該實施例包括將遠距離區連接至近距離區的漸進之光 功率區域。該圖並未按比例繪製。遠距離區中之光功率展 不為平的且因此由\軸2310表示。漸進之光功率區域開始 於透鏡2320之配合點處。或者,漸進之光功率區域可開始 於配合點下方。儘管漸進之光功率區域之光功率在通道之 長度上增加,但漸進之光功率區域可將光功率之三個平台 提供於通道内。第一平台2330提供上部遠-中間距離校 正,第二平台2340提供中間距離校正,且第三平台235〇提 供近距離校正。光功率之第一平台可具有沿通道之在大約 1 mm與大約6 mm之間或在大約2 mm與大約3 mm之間的垂 直長度。然而,在所有情況下,光功率之平台具有至少大 約1 mm之垂直長度。在光功率之第一平台之後,由漸進之 光功率區域所供應之光功率增加直至光功率之第二平台為 止。光功率之第二平台可具有沿通道之在大約丨mm與大約 6 mm之間或在大約2 mm與大約3 mm之間的垂直長度。在 光功率之第二平台之後,由漸進之光功率區域所供應之光 功率增加直至光功率之第三平台為止。光功率之第三平台 可具有沿通道之在大約1 mm與大約6 min之間或在大約2 mm與大約3 mm之間的垂直長度。在2360處達成近距離光 功率之後’由漸進之光功率區域所供應之光功率可開始降 低。若光功率降低至近距離區中之附加功率之大約2〇%至 大約44%之間,則可提供一下部遠中間區。 130295.doc -48- 200912425 圖24展示沿本發明之—實施例之中心垂直中線的光功 率該實施例包括一大致球面功率區域…不連續性及— 將遠距離區連接至近距離區的漸進之光功率區域。該圖並 未按比例繪製。遠距離區中之光功率展示為平的且因此由 軸10表示。漸進之光功率區域開始於透鏡之配合點 2420處或附近。不連續性期可由大致球面功率區域引 起,其引起光功率之步級,且供應光功率244〇。漸進之光 功率區域可起始於不連續性上方。在此情況下,漸進之光 功率區域之起始可藉由量測遠距離區中之光功率及接著將 透鏡之-區或區域定位於不連續性上方來定位,在不連續 性上方’透鏡之光功率開始逐漸以正光功率增加或以負光 功率減小。恰在不連續性之前的光功率與恰在不連續性之 後的光功率之間的差被稱為"光功率之步級"。"光功率之 步升”在光功#自不連續性之前増#至不連續性之後的情 況下發生。”光功率之步降"在光功率自不連續性之前降低 至不連續性之後的情況下發生。因此,若漸進之光功率區 域起始於不連續性上方,則緊接在不連續性之前,透鏡中 之總光功率為漸進之光功率區域及遠距離區的光功率,且 緊接在不連續性之後,透鏡中之總光功率為由光功率之步 級所引起的光功率以及漸進多焦點區域及遠距離區之光功 率。或者,漸進之光功率區域可起始於不連續性下方,使 侍緊接在不連續性之前,透鏡中之總光功率為遠距離光功 率,且在不連續性之後,一旦漸進之光功率區域起始,則 透鏡中之總光功率為由光功率之步級所引起的光功率以及 130295.doc -49- 200912425 漸進多焦點區域及遠距離區之光功率。漸進之光功率區域 可緊接在不連續性之後開始。或者,漸進之光功率區域可 在距不連續性1或更多毫米處開始,進而形成光功率之平 台2450,該平台2450可對於中間距離觀察或上部遠-中間 距離觀察有用。在本發明之一些實施例申,漸進之光功率 區域可具有負光功率2460使得該區域在具有增加透鏡中之 總光功率的正光功率之前降低透鏡中之總功率。舉例而 言,由光功率之步級所引起的光功率可高於適當遠-中間 距離觀察所需的光功率。在此情況下,在不連續性處及緊 接在不連續性之後的漸進之光功率區域之一部分可降低透 鏡之光功率以提供適當上部遠-中間距離校正。漸進之光 功率區域可接著增加光功率以提供適當中間距離校正 2470。漸進之光功率區域之光功率可進—步增加直至全近 距離光功率2480為止,在全近距離光功率248〇之後漸進之 光功率區域之光功率可再次開始降低。若光功率降低至近 距離區中之附加功率之太約2〇%至大約44%之間,則可提 供一下部遠-中間區。 在漸進之光功率區域開始於不連續性上方的本發明之實 施例中,由漸進之光功率區域所供應之光功率可最初為零 或負。不連續性可由光功率之步級引起。由光功率之步級 所引起的光功率可大約等於適當中間距離校正或遠-中間 距離校正所需的光功率。因此,若由漸進之光功率區域所 供應之初始光功率為零,則不連續性之後的組合光功率將 為適當中間距離校正或遠_中間距離校正。類似地,由光 130295.doc -50- 200912425 Γ 功率之步級所引起的光功率可大於適當中間距離校正或 遠-中間距離校正所需的光功率。因a,若由漸進之光功 率區域所供應之初始光功率為負,則不連續性之後的組合 光2率將為適當中間距離校正或遠·中間距離校正。在任 ί月況下,右渐進之光功率區域初始土也提供一正光功率, 不連續性之後的組合光功率將過強。此情形經證實為圖16 至圖20中的情況。此外,應注意,若光功率之步級引起比 適當中間距離校正或遠_中間距離校正高的光功率,則可 使用下部附加功率漸進之光功率區域,進而改良透鏡之光 學特徵。應注意’漸進之光功率區域之光功率愈低,愈少 不μ散光及失真將添加至最終透鏡。 或者,在漸進之光功率區域開始於不連續性上方的本發 明之實施例中’由漸進之光功率區域所供應之光功率可最 初為正。在此等實施例中,由光功率之步級所引起的光功 率可減小為小於適當中間距離校正或適當遠-中間距離校 正所需的光功率。因此’若由漸進之光功率區域所供應之 初始光功率為正,則不連續性之後的組合光功率將為適當 中間距離校正或遠-中間距離校正、然而,應注意,與大 致球面區域之光功率等於或大於由漸進之光功率區域所供 應之光功率的實施例相比’此實施例中之不當散光及失真 在最終透鏡中較大。 圖25展示沿本發明之一實施例之中心垂直中線的光功 率’該實施例包括-大致球面功率區域、—不連續性及一 將遠距離區連接至近距離區的漸進之光功率區域。該圖並 130295.doc 200912425 未按比例繪製。遠距離區中之光功率展示為平的且因此由 X軸2510表示。不連續性2520可定位於配合點2530下方, 例如’在配合點下方大約3 mm處。不連續性可由大致球面 功率區域引起’其引起光功率之步級,且供應光功率 2540。漸進之光功率區域可起始於大致球面功率區域之一 • 部分處’例如’緊接在不連續性之後或立即在2550之後。 大致球面功率區域可具有在不連續性之大約3 mm至5 mm 内的”非球面部分"2560。在此部分之後,大致球面功率區 域可大體上為球面。漸進之光功率區域的光功率與大致球 面功率區域之非球面部分的光功率之組合可形成一組合的 漸進之光功率區域,該區域具有以與光功率之急劇步升相 反的大致連續方式緊接在不連續性之後增加的光功率。淨 光學效應在於光功率之步級小於由大致球面功率區域所提 供之全光功率2570。非球面部分及漸進之光功率區域允許 大致球面功率區域之全光功率在不連續性之後逐漸達成。 非球面部分可提供適當上部遠-中間距離校正258〇。或 〇 者,漸進之光功率區域可供應額外光功率以提供適當上部 遠-中間距離校正。漸進之光功率區域可接著增加光功率 以提供適當中間距離校正2585。或者,可能不提供僅適當 ' 遠-中間距離校正。漸進之光功率區域之光功率可進一步 增加直至全近距離光功率2590為止,在全近距離光功率 2590之後漸進之光功率區域之光功率可再次開始降低。在 本發明之實施例中,下部遠-中間距離校正2595可由在近 距離區之後的光功率之步降來提供。或者,下部遠-中間 130295.doc -52· 200912425 距離區可由供應降低透鏡中之光功率之負光功率的漸進之 光功率區域來提供。 圖26展示沿本發明之一實施例之中心垂直中“ W 率,該實施例包括-大致球面功率區域、一不連續性及一 將遠距離區連接至近距離區的漸進之光功率區域。該圖並 . 隸比例繪製。遠距離區中之光功率展示為平的且因此由 X軸2610表示。不連續性262〇可在遠距離區與上部遠-中間 距離區2640之間定位於配合點⑽下方。或者,不連續性 可在遠距離區與中間距離區2650之間定位於配合點下方。 不連續性可由大致球面功率區域引起,其引起光功率之步 級,且供應光功率2660。光功率之步升可等於遠_中間距 離校正所需的光功率。或者’光功率之步升可等於中間距 離校正所需的光功率。漸進之光功率區域可起始於大致球 面功率區域之一部分處,例如,緊接在不連續性之後或立 即在2670之後。若漸進之光功率區域開始於不連續性下 方’則可接著提供光功率之平台以用於上部遠-中間距離 八 區或用於中間距離區。漸進之光功率區域繼續直至全近距 離光功率2680為止,在全近距離光功率268〇之後,漸進之 光功率區域可供應降低透鏡中之光功率的負光功率。若光 ' 功率降低至近距離區中之附加功率之大約20%至大約44% 之間,則可提供一下部遠_中間區。在本發明之一些實施例 中透鏡可包括用於該等距離區之任一者的光功率之平台。 在本發明之實施例中,透鏡可提供+2 〇〇Ε)近附加功率。 透鏡可包括一具有+1.00D之光功率的埋入式大致球面功率 130295.doc -53· 200912425Physio-additional power gradient for both lenses. Inventive lens and Physi. Both TM lenses have an additional power of +2.25D. The diurnal lens has a substantially spherical power region having an optical power of +1.25 D and a progressive optical power region having an optical power of + 1. The top of the progressive optical power region starts just below the mating point and the top of the approximate spherical power region is located 4 mm below the mating point. Thus, prior to the initial addition of optical power to the lens in the substantially spherical power region, there is one region of the lens in which only the progressive optical power region supplies increased optical power. Figure 2 shows the measurement obtained from the mating point along the additional power channel down every 3 mm of the two lenses as measured by the R〇Uex Class P1USTM. This embodiment of the inventive lens has +1 6 〇 1) 9 mm from the mating point compared to the embodiment of the physi 〇 TM having an additional power of +1.I0D from the mating point 9 melon (1). : Add power. As previously mentioned, the silk optimizes the optical power, placement, and alignment of the approximate spherical power region and the progressive optical power region, and the resulting lens will have poor vision ergonomics, poor visual comfort, and good vision clarity. This is especially true when the lens provides the correct full additional power at 15 111111 below the mating point in Figures 18 and 20. Thus, although such embodiments of the inventive lens have various excellent properties as compared to the state of the art, it should be apparent that such lenses can be rejected by the user. Embodiments of the inventive lens have too much additional power in the intermediate distance zone and the optical power gradient from the mating point to the bottom of the lens is too steep. By comparing the additional power measurements shown in Figure j 8 and Figure 2 for the Essilor Physi0TM lens, it should be apparent that we cannot add the +1 (10) D spherical power region to the Essilor Physi® lens of Figure 17 and thus to Figure 2 〇130295.doc • 42-200912425 Essilor Physi〇TM lens. Therefore, it should be apparent that the substantially spherical power region and/or the progressive optical power region must be specifically designed to provide an appropriate intermediate distance correction and/or far-intermediate distance in consideration of the gradient of optical power between the remote and close regions. Correction. Figure 21 shows four regions of the inventive lens: a remote zone - an upper far-intermediate zone 2120, an intermediate zone 213 and a close zone 2140. These areas are not shown to scale. The upper far-middle distance zone may have a height from the point Η to the point I and a width from the point a to the point β. The mid-range separation area may have a height from a point to a point j and a width from a point c to a point D. The close-up area may have a height from the point J to the point G and a width from the point e to the point f. In certain embodiments of the invention, the inventive lens provides the wearer with appropriate corrections for the remote and close regions and provides optical power that allows the wearer to properly view at the far-intermediate and intermediate distances. Optimize the gradient. In some embodiments of the invention, the lens may have vertical stability of vision in the upper distal-middle distance zone and/or vertical stability of vision in the intermediate zone. In embodiments of the invention that do not have a far-intermediate zone, the intermediate distance zone may have increased vertical stability of vision. An additional far-middle distance zone can be provided below the close range. In this embodiment, this region may be referred to as the "lower" far intermediate distance zone, and the far-middle distance zone between the far zone and the intermediate zone may be referred to as "upper" region. The upper and lower far-middle zones can have the same optical power. The lower far-middle zone can be included in the inventive lens design to allow the presbyopic wearer to more easily see his or her feet when looking down. This situation provides additional safety when going up and down the stairs. 130295.doc -43. 200912425 Embodiments of the invention may include one or more discontinuities between regions of the lens. The discontinuity can be caused by a discontinuous surface or by discontinuous optical power between two different regions of the lens. The discontinuity can be caused by the stepping or stepping of the optical power. Discontinuity is defined as any change in the surface of the lens or the optical power of the lens that produces a perceived image break when viewed through the lens. By way of example only, the inventors have made a variety of inventive transmissive lenses, and have found that when the lens has less than about (the optical power of the MOD is not continuous, and when the lens is worn with the lens typically used) It is difficult to feel the interruption of the image when it is located at a distance from the eye-catching distance. However, in most cases, optical power discontinuities greater than about 〇〇1〇〇 to 〇12D can be visually detected. In addition, the lens is This optical power discontinuity that the wearer can feel can interfere with the wearer's vision during certain visual tasks (eg, viewing a computer screen). It should be noted that the optical power stated above for discontinuity is only an example' And discontinuity is any change in the surface or optical power of the lens that produces the ability to sense image discontinuities when viewed through the lens. (The inventors have further confirmed that some discontinuities are more pronounced than others and / J $ There is more interference. Accordingly, embodiments of the present invention may include one or more discontinuities that are less noticeable and/or less interfered. The inventors have discovered that the intermediate distance zone, the close distance zone The discontinuity of the discontinuity or intermediate distance zone is closer to the discontinuity between the close and the squat zone, and the user visually better endures the discontinuity between the far distance zone of the lens and the upper distance zone Furthermore, the inventors have demonstrated that due to the faster transition of the eye in any image interruption or blur formed by the mixing zone, the narrower the width of the mixing zone of at least a portion of the mixing discontinuity, the eye is in discontinuity The better the transition. Although 130295.doc -44 - 200912425 this situation may seem to indicate discontinuity and therefore should not be mixed, but this situation must be balanced by the favorable appearance effect of the mixing discontinuity to form an almost invisible discontinuity. Embodiments of the inventive lenses disclosed herein consist of one or more discontinuities, wherein a discontinuity can be caused by a step of optical power of +0.12 D or greater. The inventive implementation disclosed herein. An example may have a single discontinuity that is at least partially mixed by a mixing zone having a width of less than about 2.0 mm or between about 丨〇1 and 〇5. The mixing zone of this width may be Diamond turning is produced. However, in other embodiments of the invention, discontinuities are not mixed. In embodiments of the invention, the discontinuity may be more than about +0.25 D and in most cases more than about +〇5 The step of the optical power of 〇D rises to induce a step-up of the S° optical power and thus the discontinuity is usually (but not always) positioned between the far-distance zone of the inventive lens and the far-intermediate distance zone. When the inventive lens does not have a far/intermediate distance zone, the discontinuity is typically located between the far distance zone and the intermediate zone zone of the lens. Figure 26 and Figure 26 show the optical power before the start of the progressive optical power zone. This embodiment of the invention allows for the ability to have three usable zones of optical power: a long range zone, an intermediate zone zone, and a close range zone. Embodiments of the invention may also provide a fourth zone. The ability of the upper zone (intermediate distance zone) and, in some embodiments, the ability to have a fifth zone (lower far-intermediate distance zone). Embodiments of the invention may: a) increase the length of the channel to allow for an additional 2 _ to 3 光 of the optical power M U upper _ middle (four) correction. This optical power zone can be used when using 130295.doc -45- 200912425 on our computer or on the edge of our desk. It should be noted that it is not possible to increase the length of the channel as it would be to accommodate the vertical dimensions of the lens frame of the lens. b) Increase the length of the channel to allow an additional 2 paws to the 3 pawl platform for optical power to provide a lower far-intermediate distance correction. This optical power zone can be useful when viewing the feet or floors of the person while climbing up or down the stairs. Note • It is not possible to increase the length of the channel as it would accommodate the vertical dimension of the lens frame of the lens. p G) Utilization - or multiple discontinuities. The or discontinuity may be caused by - or a plurality of steps of optical power, wherein the step is a step-up or step-down of optical power. Since the discontinuity uses very little (if any) lens immobility to step up or step down the optical power, the channel can be designed to allow a 2 power platform without the need to extend the length of the channel. It is important to note that the greater the step of optical power, the more real estate that can be supplied to the optical power platform in the lens. In an embodiment of the invention, the platform of optical power is supplied after the discontinuity and provides a far-intermediate distance correction. This is done in the case where you need to add the length of the channel. Figure 22 shows an embodiment of the invention with two platforms 223G and 2240 of light; and <23> shows three platforms 233G, measured and 2350 having optical power - an embodiment of the invention. d) Keep the length of the channel the same, but make the optical power tilt faster between the various areas of optical power. It should be noted that this often creates problems with the wearer's visual comfort and eye strain. e) Immediately use the optical power step below the close range to allow the lower 130295.doc -46 * 200912425 back-intermediate distance zone. It should be noted that the lower far-middle distance zone may be possible only if there is sufficient lens real estate below the close proximity portion of the lens. Figure 22 shows the optical power of a central vertical centerline not in accordance with an embodiment of the present invention. This embodiment includes a progressive optical power region that connects the remote zone to the close zone. The figure is not drawn to scale. The optical power in the long range is shown to be flat and thus represented by the parent axis 2210. The progressive optical power region begins at the mating point 2220 of the lens. Alternatively, the progressive optical power region may begin below the mating point. ^ Although the optical power of the progressive optical power region is increased over the length of the channel, the progressive optical power region provides both platforms of optical power within the channel. The first platform 2230 provides an upper far-intermediate distance correction and the second platform 2240 provides an intermediate distance correction. Alternatively, the progressive optical power region provides a single platform of optical power that provides intermediate distance correction or far-intermediate distance correction. The first platform of optical power may have a vertical length of between about 1 mm and about 6 mm or between about 2 mm and about 3 mm along the channel. However, in all cases, the platform of optical power has a vertical length of at least about 1 mm. After the first platform of optical power, the optical power supplied by the progressive optical power region increases until the second platform of optical power. The second platform of optical power may have a vertical length of between about 1 mm and about 6 mm or between about 2 mm and about 3 mm along the channel. After the second platform of optical power, the optical power supplied by the progressive multifocal region increases until the total near-field optical power reaches 2250. After the near-optical power is reached, the optical power supplied by the progressive optical power region can begin to decrease. If the optical power is reduced to approximately 130295.doc •47·200912425 20% to approximately 44% of the additional power in the close range, a lower far-middle zone may be provided. Figure 23 shows the optical power of the center vertical centerline of one embodiment of the invention. This embodiment includes a progressive optical power region that connects the remote zone to the close zone. The figure is not drawn to scale. The optical power spread in the long range is not flat and is therefore represented by the \ axis 2310. The progressive optical power region begins at the mating point of the lens 2320. Alternatively, the progressive optical power region can begin below the mating point. Although the optical power of the progressive optical power region increases over the length of the channel, the progressive optical power region provides three platforms of optical power within the channel. The first platform 2330 provides an upper far-intermediate distance correction, the second platform 2340 provides an intermediate distance correction, and the third platform 235 provides a close distance correction. The first platform of optical power may have a vertical length of between about 1 mm and about 6 mm or between about 2 mm and about 3 mm along the channel. However, in all cases, the platform of optical power has a vertical length of at least about 1 mm. After the first platform of optical power, the optical power supplied by the progressive optical power region increases until the second platform of optical power. The second platform of optical power may have a vertical length along the channel of between about 丨mm and about 6 mm or between about 2 mm and about 3 mm. After the second platform of optical power, the optical power supplied by the progressive optical power region is increased until the third platform of optical power. The third platform of optical power may have a vertical length of between about 1 mm and about 6 min or between about 2 mm and about 3 mm along the channel. After the near-field optical power is reached at 2360, the optical power supplied by the progressive optical power region can begin to decrease. If the optical power is reduced to between about 2% and about 44% of the additional power in the close range, a lower intermediate zone can be provided. 130295.doc -48- 200912425 Figure 24 shows optical power along a central vertical centerline of an embodiment of the present invention. This embodiment includes a substantially spherical power region... discontinuity and - progressive connection of the remote zone to the close zone Light power area. The figure is not drawn to scale. The optical power in the long range is shown to be flat and thus represented by the axis 10. The progressive optical power region begins at or near the mating point 2420 of the lens. The discontinuity period can be caused by a substantially spherical power region that causes a step of optical power and supplies optical power 244 〇. Progressive light The power zone can start above the discontinuity. In this case, the initial phase of the progressive optical power region can be located by measuring the optical power in the remote region and then positioning the region or region of the lens above the discontinuity, above the discontinuity 'lens The optical power begins to gradually increase with positive optical power or with negative optical power. The difference between the optical power just before the discontinuity and the optical power just after the discontinuity is called the "step of optical power". "stepping of optical power" occurs in the case of optical power before the discontinuity 増# to discontinuity.” The step of optical power drops" decreases to discontinuity before the optical power is discontinuous After the situation occurs. Therefore, if the progressive optical power region starts above the discontinuity, the total optical power in the lens is the progressive optical power region and the optical power of the remote region immediately before the discontinuity, and immediately after After continuity, the total optical power in the lens is the optical power caused by the step of optical power and the optical power of the progressive multifocal region and the far range. Alternatively, the progressive optical power region may begin below the discontinuity such that the contact is before the discontinuity, the total optical power in the lens is the long-range optical power, and after the discontinuity, once the progressive optical power At the beginning of the region, the total optical power in the lens is the optical power caused by the step of optical power and the optical power of the progressive multifocal region and the remote region of 130295.doc -49-200912425. The progressive light power area can begin immediately after the discontinuity. Alternatively, the progressive optical power region can begin at a distance of 1 or more millimeters from the discontinuity, thereby forming a platform 2450 of optical power that can be useful for intermediate distance viewing or upper far-intermediate distance viewing. In some embodiments of the invention, the progressive optical power region may have a negative optical power 2460 such that the region reduces the total power in the lens prior to having positive optical power that increases the total optical power in the lens. For example, the optical power caused by the step of optical power can be higher than the optical power required to observe the appropriate far-intermediate distance. In this case, the optical power of the lens can be reduced at the discontinuity and in a portion of the progressive optical power region immediately after the discontinuity to provide proper upper far-intermediate distance correction. The progressive light power zone can then be increased in optical power to provide an appropriate intermediate distance correction 2470. The optical power of the progressive optical power region can be increased step by step until the full-field optical power is 2480, and the optical power of the progressive optical power region can start to decrease again after the full-field optical power of 248 。. If the optical power is reduced to between about 2% and about 44% of the additional power in the close range, a lower far-middle zone may be provided. In embodiments of the invention where the progressive optical power region begins above the discontinuity, the optical power supplied by the progressive optical power region may initially be zero or negative. The discontinuity can be caused by the step of optical power. The optical power caused by the step of optical power can be approximately equal to the optical power required for proper intermediate distance correction or far-intermediate distance correction. Therefore, if the initial optical power supplied by the progressive optical power region is zero, the combined optical power after the discontinuity will be an appropriate intermediate distance correction or a far-intermediate distance correction. Similarly, the optical power caused by the step of light 130295.doc -50- 200912425 Γ power can be greater than the optical power required for proper intermediate distance correction or far-intermediate distance correction. Since a, if the initial optical power supplied by the progressive optical power region is negative, the combined light 2 rate after the discontinuity will be an appropriate intermediate distance correction or a far intermediate distance correction. In any case, the initial gradual optical power region initial soil also provides a positive optical power, and the combined optical power after discontinuity will be too strong. This case has been confirmed as the case in Figs. 16 to 20. In addition, it should be noted that if the step of optical power causes an optical power that is higher than the appropriate intermediate distance correction or the far-intermediate distance correction, the lower additional power progressive optical power region can be used, thereby improving the optical characteristics of the lens. It should be noted that the lower the optical power in the progressive light power region, the less the astigmatism and distortion will be added to the final lens. Alternatively, the optical power supplied by the progressive optical power region may be initially positive in embodiments of the invention where the progressive optical power region begins above the discontinuity. In such embodiments, the optical power caused by the step of optical power can be reduced to less than the optical power required for proper intermediate distance correction or proper far-intermediate distance correction. Therefore, if the initial optical power supplied by the progressive optical power region is positive, the combined optical power after the discontinuity will be the appropriate intermediate distance correction or the far-intermediate distance correction, however, it should be noted that with the substantially spherical region The optical power is equal to or greater than the embodiment of the optical power supplied by the progressive optical power region. The improper astigmatism and distortion in this embodiment are larger in the final lens. Figure 25 shows the optical power of a central vertical centerline along an embodiment of the invention. This embodiment includes a - substantially spherical power region, - discontinuity, and a progressive optical power region connecting the remote region to the close region. The figure is not drawn to scale. 130295.doc 200912425. The optical power in the long range is shown to be flat and thus represented by the X-axis 2510. The discontinuity 2520 can be positioned below the mating point 2530, such as 'about 3 mm below the mating point. The discontinuity can be caused by the substantially spherical power region, which causes the step of optical power, and supplies optical power 2540. The progressive optical power region may originate from one of the substantially spherical power regions. • The portion 'e.g.' immediately after the discontinuity or immediately after 2550. The substantially spherical power region may have an aspherical portion "2560 within about 3 mm to 5 mm of discontinuity. After this portion, the substantially spherical power region may be substantially spherical. The optical power of the progressive optical power region The combination of the optical power of the aspherical portion of the substantially spherical power region can form a combined progressive optical power region having a substantially continuous manner opposite the sharp rise in optical power immediately following the discontinuity. Optical power. The net optical effect is that the optical power step is less than the total optical power 2570 provided by the substantially spherical power region. The aspherical portion and the progressive optical power region allow the total optical power of the substantially spherical power region to gradually evolve after discontinuity. The aspherical portion may provide an appropriate upper far-intermediate distance correction 258. Or, the progressive optical power region may supply additional optical power to provide an appropriate upper far-intermediate distance correction. The progressive optical power region may then add light. Power to provide proper intermediate distance correction 2585. Or, may not provide only proper 'far-intermediate distance calibration The optical power of the progressive optical power region may be further increased until the full close optical power 2590, and the optical power of the progressive optical power region may begin to decrease again after the full close optical power 2590. In an embodiment of the invention, The lower far-intermediate distance correction 2595 may be provided by a step of optical power after the close range. Alternatively, the lower far-middle 130295.doc -52· 200912425 distance zone may be supplied by a negative optical power that reduces the optical power in the lens. A progressive optical power region is provided. Figure 26 shows a "W rate in the center of the center along an embodiment of the invention. This embodiment includes - a substantially spherical power region, a discontinuity, and a remote region connected to the close region. The progressive light power area. The figure is drawn by the scale. The optical power in the long range is shown to be flat and thus represented by the X-axis 2610. The discontinuity 262 定位 can be positioned below the mating point (10) between the remote zone and the upper far-middle distance zone 2640. Alternatively, the discontinuity may be positioned below the mating point between the remote zone and the intermediate zone 2650. The discontinuity can be caused by a substantially spherical power region that causes a step of optical power and supplies optical power 2660. The step-up of the optical power can be equal to the optical power required for the far-neutral distance correction. Or the step of the optical power step can be equal to the optical power required for the mid-range separation correction. The progressive optical power region may originate at a portion of the approximate spherical power region, e.g., immediately after the discontinuity or immediately after 2670. If the progressive optical power region begins below the discontinuity, then a platform of optical power can be provided for the upper far-intermediate distance eight zone or for the intermediate distance zone. The progressive optical power region continues until the full-close optical power is 2680. After the full-field optical power is 268 ,, the progressive optical power region can supply negative optical power that reduces the optical power in the lens. If the light' power is reduced to between about 20% and about 44% of the additional power in the close range, a lower far-middle zone may be provided. In some embodiments of the invention the lens may comprise a platform for optical power of any of the equidistant zones. In an embodiment of the invention, the lens can provide +2 〇〇Ε) near additional power. The lens may comprise a buried substantially spherical power having an optical power of +1.00 D. 130295.doc -53· 200912425

區域該區域、㉟對準使得大致球面功率區域之頂部邊緣在 透鏡之配合點下方大約3 mm處對準。透鏡可具有一漸進之 光功率表面’該表面具有一定位於透鏡之凸外表面上的漸 進之光功率區域。或者,漸進之光功率表面可定位於透鏡 之凹表面上、分裂於透鏡之兩個外表面之間,或埋入於透 鏡内。漸進之光功率區域具有為零之初始光功率,其增加 至+ 1.00D之最大光功率。漸進之光功率區域經對準使得呈 有零光功率之其通道的起始在透鏡之配合點下方大約10 mm 處開始。換言之’漸進之光功率區域經對準使得其通道的 起始在由埋入式球面功率區域所引起之光功率的步升所引 起之不連續性下方大約7_處。在此發明性實施例中,在 發明,透鏡中不存在遠.中間距離區。然而,中間距離區 具有遠大於市售之任何PAL透鏡的最小大約7 之視力之 垂直穩定性。如可易於理解,漸進之光功率與大致球面功 率區域的組合光功率在大致球面功率區域之頂部邊緣下方 大約7 rnm之後才開始。因此,自配合下方大約3麵處至 配合點下方大約1G mm處的光功率為由大致球面功率區域 所提供的+1細光功率。此光功率為近距離附加功率之 50¾且因此提供適當的_間距離校正。 在本發明之又-實施例中,透鏡可提供+2 5〇d近附加功 率。透鏡可具有-具有+1.25D之光功率的大致球面功率區 域,該區域係自由成型於透鏡之凹的背環面/散光校正外 表面上其經對準使知大致球面功率區域之頂部邊緣係在 透鏡之配合點下方大約4 mm處。透鏡可具有一定位於透鏡 130295.doc -54- 200912425 之岫凸表面上且具有為零之初始光功率(其增加至+125D 最大光功率)的漸進之光功率區域。漸進之光功率區域 經對準使得其通道的起始在透鏡之配合點下方大約10 mm 處開始。換言之,漸進之光功率區域係經對準使得其通道 的起始在由埋入式球面功率區域所引起之光功率的步升所 引起之不連續性下方大約6職處。在此發明性實施例中, 在發明性透鏡中不存在遠-中間距離區。然而,中間距離 區具有遠大於市售之任何PAL透鏡的最小大約6 之視力The region, 35, is aligned such that the top edge of the substantially spherical power region is aligned approximately 3 mm below the mating point of the lens. The lens can have a progressive optical power surface' that has a progressive optical power region that is located on the convex outer surface of the lens. Alternatively, the progressive optical power surface can be positioned on the concave surface of the lens, split between the two outer surfaces of the lens, or embedded in the lens. The progressive optical power region has an initial optical power of zero, which increases to a maximum optical power of +1.00D. The progressive optical power region is aligned such that the beginning of its channel with zero optical power begins approximately 10 mm below the mating point of the lens. In other words, the 'gradual optical power region is aligned such that its channel starts at about 7_ below the discontinuity caused by the step-up of the optical power caused by the buried spherical power region. In this inventive embodiment, in the invention, there is no far intermediate distance zone in the lens. However, the intermediate distance zone has a vertical stability that is much greater than the minimum of about 7 of any commercially available PAL lens. As can be readily appreciated, the combined optical power of the progressive optical power and the approximate spherical power region begins approximately 7 rnm below the top edge of the substantially spherical power region. Therefore, the optical power from about 3 faces below the fit to about 1 Gmm below the fit point is the +1 fine light power provided by the approximate spherical power region. This optical power is 503⁄4 of the close-range additional power and thus provides an appropriate _ distance correction. In still further embodiments of the invention, the lens provides a near additional power of +25 〇d. The lens may have a substantially spherical power region having an optical power of +1.25 D which is freely formed on the concave back annulus/astigmatism correcting outer surface of the lens which is aligned such that the top edge of the substantially spherical power region is aligned Approximately 4 mm below the mating point of the lens. The lens may have a progressive optical power region that is located on the convex surface of the lens 130295.doc -54 - 200912425 and has an initial optical power of zero (which is increased to +125D maximum optical power). The progressive optical power region is aligned such that the beginning of its channel begins approximately 10 mm below the mating point of the lens. In other words, the progressive optical power region is aligned such that the beginning of its channel is approximately six degrees below the discontinuity caused by the step-up of the optical power caused by the buried spherical power region. In this inventive embodiment, there is no far-intermediate distance zone in the inventive lens. However, the intermediate distance zone has a visual power that is much greater than approximately 6 of any commercially available PAL lens.

漸進之光功率與大致球面 之垂直穩定性。如可易於理解 力率區,域的合光功率在大致球面功率區域之頂部邊緣 (大致球面功率區域之頂部邊緣為不連續性之位置)下方大 =6職之後才開始。因此,自配合下方大約4顏處至配 合點下方大約10 mm處的光功率為由大致球面功率區域所 提供的+U5D光功率。此光功率為近距離附加功率之5〇% 且因此提供適當的中間距離校正。 在本發明之實施例中’透鏡可提供+2.25D近附加功率。 透鏡可包括-具有+〇.75D之光功率的埋入式大致球面功率 區域’該區域經對準使得大致球面功率區域之頂部邊緣在 透鏡之配合點下方大約3 mm處對準。透鏡可具有一漸進之 光功率表面,該表面具有—定位於透鏡之凸外表面上的漸 進之光功率區域。或者,漸進之光功率表面可定位於透鏡 之凹表面上、分裂於透鏡之兩個外表面之間,或埋入於透 鏡内。漸進之光功率區域具有為零之初始光功率,其增加 至+1.50D之最大光功率。漸進之光功率區域經對準使得具 130295.doc -55- 200912425 有零光功率之其通道的起始在透鏡之配合點下方大約7 mm 處開始。換言之,漸進之光功率區域經對準使得其通道的 起始在由埋入式球面功率區域所引起之光功率的步升所引 起之不連續性下方大約4 mm處。在此發明性實施例中,存 在在發明性透鏡中找到的遠_中間距離區。該遠-中間距離 區具有最小大約4 mm之視力之垂直穩定性。並無市售pAL 具有一遠-中間距離區或一具有如此長的視力之垂直穩定 性的遠_中間距離區。如可易於理解,漸進之光功率與大 致球面功率區域的組合光功率在大致球面功率區域之頂部 邊緣下方大約4 mm之後才開始。因此,自配合下方大約 3 mm處至配合點下方大約7 mm處的光功率為由大致球面 功率區域所提供的+0.75D光功率。此光功率為近距離附加 功率之33,33%且因此提供適當遠-中間距離校正。 應指出’以上實施例僅作為實例而提供且不意謂限制用 於漸進之光功率區域或大致球面功率區域之對準的距配合 點之距離。此外,在實例中所給出之光功率亦不意謂限 制。此外,不應將在透鏡之表面上、分裂於透鏡之表面之 間’或埋入於透鏡内的區域之位置解釋為限制。最後,雖 然以上某些實施例可教示遠-中間距離區的缺乏,但可藉 由改變由每一區域所提供的對準及光功率來包括遠_中間 距離區。 在本發明之實施例中,球面功率區域可在眼科透鏡之— 表面上或埋入於眼科透鏡内。球面功率區域可為折射功率 區域且可以折射方式產生光功率。或者,球面功率區域可 130295.doc -56- 200912425 功率區域且可以繞射方式產生光功率。對於折射 光功率區域兩者而言,光功率係由具有不同折射率 光學材料與第二光學材料之間的光學界面來產生。 ==率區域可為球面之一表面之一區段,其甲光功率由 下式來疋義十(n2.ni)/R,其中伞為以折射功率區域之屈 =為Μ的光㈣’n2為第—光學材料之折射率,^為 第二光學材料之折射率,且R為球面之半徑。繞射光功率 &域可為由適當炫耀分布(blaze pr〇f叫之同心環組成的 相位環繞、表面起伏的繞射結構。此結構在此項技術中 眾所周知。此繞射光功率區域之光功率由下式定義: η=[(2α)/Φ]"2,其中ri為第丨環〇=1,2, 3,之半徑 繞射光功率區域之設計波長,且 ^ 仗且為以繞射光功率區域之 屈光度為單位的光功率。雖然環之半徑確定繞射光功率區 域之光功率,但表面起伏繞射結構之高“確定入射光得 以聚焦之份額(亦βρ ’繞射光功率區域之繞射效率最大 繞射效率在繞射光功率區域之相位延遲為如下式所定義之 波長的整數倍時達成:(η2_η1)(Ηπιλ,其中h為第—光學材 料=折射率’ η,為第二光學材料之折射率,d為繞射結構 之高度,λ為繞射光功率區域之設計波長,且爪為一整數 (m=l,2, 3,...)。 在本發明之一實施例中,在方法之第—操作中,可提供 具有漸進之光功率區域之第一多焦點光學器件。漸進之光 功率區域可具有+1.00D之附加功率,儘管任何附加功率為 可能的。僅舉例而言,第一多焦點光學器件可由cr39樹 130295.doc 57· 200912425 脂(由㈣登記商標)組成且具有15〇之折射率。在方法之 第二操作令’第一多焦點光學器件可(僅舉例而言,藉由 熱鱗造)固化至第二多焦點光學器件之表面上_^ Ο 合透鏡。第二多焦點光學器件可具有至少一球面功率區 域。第二多焦點光學器件可為透鏡、透鏡晶圓、經修整之 透鏡毛迷,或半修整之透鏡毛述。僅舉例而言,第二多焦 點光學器件可由一固化聚合物組成,諸如,購自Mitsui: 具有1.67之折射率的聚合物。第二多焦點光學器件可且有 能夠產生一個以上光功率之至少一多焦點表面。多焦點表 面可在由第一多焦點光學器件覆蓋之前在第二多焦點光學 器件之外部上。多焦點光學器件可為以下各項中之一者: 執行雙焦點透鏡 '具線紋之FT 28、FT 35、曲頂^、曲頂 35 ' 7x35三焦點透鏡、整塊雙焦點透鏡、圓形^雙焦點透 鏡、具有經設計以提供特定正屈光度光功率之表面:伏繞 射圖案之繞射光功率區域,或具有球面功率區域之任何其 他多焦點光學器件。第二多焦點光學器件可具有光功率之 任何組σ。若利用繞射光功率區域,則其可提供+1 〇〇D之 光功率,儘管任何光功率為可能的。熟習此項技術者可容 易地設計此繞射光學器件。應進一步指出,繞射光功率區 域或球面功率區域之具線紋之邊界的周邊外部邊緣處或附 近的光功率可經混合以便將第二多焦點光學器件之周邊邊 緣不連續性隱藏在複合透鏡内。 在本發明之某些實施例中,第二多焦點光學器件可提供 為具有一繞射光功率區域的半修整之透鏡毛坯,該繞射光 130295.doc -58- 200912425 功率區域在光學器件之一表面上供應+】〇〇d之光功率且在 另-表面(光學器件之相反表面)上未修整。第一多焦點光 學器件可經鑄造及固化至具有繞射光功率區域之第二多焦 點光學器件之表面上以便形成複合光學器件。在此實施例 中,複合透鏡可具有一具有一漸進之光功率區域的外部前 表面 1人式繞射光功率區域,及-能夠在猶後日期進 行:由成型或表面加工及拋光的未修整之外部背表面。應 注意,埋入式繞射光功率區域將歸因於第一多焦點光學器 件與第—多焦點光學器件之間的折射率差而供應光功率至 複合透鏡。 理解’雖然在本發明之此特定實施例中,第一多焦點 光予器件包含具有150之折射率的材料且第二多焦點光學 ,件匕3具有1 ·67之折射率的材料,但用於每一光學器件 之材料可顛倒。 °° 本發明之t施例可根據Α致球面功_區域來描述。然 而,應理解,由於繞射光功率區域為一類大致球面功率區 日斤χ此等實把例亦描述包括一繞射光功率區域的本發 ^之實施例。因此,繞射光功率區域之大小、形狀及光學 、° 如由本發明之實施例所描述之大致球面功率區域 ' 形狀及光學設計相同。類似地,繞射光功率區域 相對於却進之光功率區域的對準可與如由本發明之實施例 所描述之大τ占 亡 尺致球面功率區域相對於漸進之光學區域的 相同。 于 發明之另一實施例中,一具線紋之雙焦點透鏡可為 130295.doc -59- 200912425 第二多焦點光學器件。該具線紋之雙焦點透鏡之多焦點表 面可埋入於複合透鏡内。在此實施例中,具 ^ 又展、黑占The progressive optical power is approximately perpendicular to the spherical stability. As can be easily understood, the combined power of the field begins after the top edge of the approximate spherical power region (the position at which the top edge of the approximate spherical power region is discontinuous) is greater than the 6th position. Therefore, the optical power at approximately 10 mm from the underside of the fit to approximately 10 mm below the mating point is the +U5D optical power provided by the substantially spherical power region. This optical power is 5〇% of the close-range additional power and thus provides an appropriate intermediate distance correction. The lens can provide +2.25D near additional power in embodiments of the invention. The lens may comprise a buried substantially spherical power region having an optical power of + 〇.75D. The region is aligned such that the top edge of the substantially spherical power region is aligned about 3 mm below the mating point of the lens. The lens can have a progressive optical power surface having a progressive optical power region positioned on the convex outer surface of the lens. Alternatively, the progressive optical power surface can be positioned on the concave surface of the lens, split between the two outer surfaces of the lens, or embedded in the lens. The progressive optical power region has an initial optical power of zero, which increases to a maximum optical power of +1.50 D. The progressive optical power region is aligned such that the beginning of its channel with zero optical power 130295.doc -55-200912425 begins approximately 7 mm below the mating point of the lens. In other words, the progressive optical power region is aligned such that the beginning of its channel is about 4 mm below the discontinuity caused by the step-up of the optical power caused by the buried spherical power region. In this inventive embodiment, there is a far-intermediate distance zone found in the inventive lens. The far-middle distance zone has a vertical stability of vision of a minimum of about 4 mm. There is no commercially available pAL with a far-intermediate distance zone or a far-intermediate distance zone with such long vertical stability. As can be readily appreciated, the combined optical power of the progressive optical power and the substantially spherical power region begins approximately 4 mm below the top edge of the substantially spherical power region. Therefore, the optical power from approximately 3 mm below the fit to approximately 7 mm below the mating point is the +0.75 D optical power provided by the substantially spherical power region. This optical power is 33,33% of the close-range additional power and thus provides proper far-intermediate distance correction. It should be noted that the above embodiments are provided by way of example only and are not meant to limit the distance from the mating point for the alignment of the progressive optical power region or the substantially spherical power region. Moreover, the optical power given in the examples is not meant to be limiting. Further, the position of the region on the surface of the lens, split between the surfaces of the lens, or the region buried in the lens should not be construed as a limitation. Finally, while some of the above embodiments may teach a lack of far-intermediate distance zones, the far-intermediate distance zone may be included by varying the alignment and optical power provided by each zone. In an embodiment of the invention, the spherical power region may be on the surface of the ophthalmic lens or embedded in the ophthalmic lens. The spherical power region can be a refractive power region and can produce optical power in a refractive manner. Alternatively, the spherical power region can be 130295.doc -56- 200912425 power region and can generate optical power in a diffractive manner. For both refractive optical power regions, the optical power is produced by an optical interface between the optical material having a different refractive index and the second optical material. The == rate region can be a segment of one surface of the spherical surface, and its optical power is expressed by the following formula: n2.ni/R, where the umbrella is the light of the refractive power region = Μ (four)' N2 is the refractive index of the first optical material, ^ is the refractive index of the second optical material, and R is the radius of the spherical surface. The diffracted optical power & field can be a circumscribed, surface undulating diffraction structure consisting of a blaze pr〇f concentric ring. This structure is well known in the art. The optical power of this diffracted optical power region It is defined by: η=[(2α)/Φ]"2, where ri is the design wavelength of the diffracted optical power region of the radius 丨 ring 〇=1, 2, 3, and ^ 仗 is diffracted light The power of the power region is the unit of optical power. Although the radius of the ring determines the optical power of the diffracted optical power region, the surface relief diffraction structure is high "determining the fraction of incident light that is focused (also βp' diffracted by the optical power region) The maximum efficiency diffraction efficiency is achieved when the phase retardation of the diffracted optical power region is an integer multiple of the wavelength defined by the equation: (η2_η1) (Ηπιλ, where h is the first optical material = refractive index 'η), which is the second optical material The refractive index, d is the height of the diffraction structure, λ is the design wavelength of the diffracted optical power region, and the claws are an integer (m = 1, 2, 3, ...). In one embodiment of the invention, In the first method of operation, For a first multifocal optic having a progressive optical power region. The progressive optical power region may have an additional power of +1.00 D, although any additional power is possible. By way of example only, the first multifocal optic may be from cr39 The tree 130295.doc 57· 200912425 is composed of (4) registered trademark and has a refractive index of 15 。. In the second operation of the method, the first multifocal optic can (for example, by hot scale) Curing onto the surface of the second multifocal optic. The second multifocal optic may have at least one spherical power region. The second multifocal optic may be a lens, a lens wafer, a trimmed lens hair By way of example, the second multifocal optic may consist of a solid polymer, such as that available from Mitsui: a polymer having a refractive index of 1.67. The second multifocal optic may And having at least one multifocal surface capable of producing more than one optical power. The multifocal surface may be external to the second multifocal optic prior to being covered by the first multifocal optic Multifocal optics can be one of the following: Performing a bifocal lens 'lined FT 28, FT 35, curved top ^, curved top 35 ' 7x35 trifocal lens, monolithic bifocal lens, circle a bifocal lens having a surface designed to provide a particular positive diopter optical power: a diffracted optical power region of a volt diffraction pattern, or any other multifocal optic having a spherical power region. The second multifocal optic may have Any set of optical powers σ. If a diffracted optical power region is utilized, it can provide optical power of +1 〇〇 D, although any optical power is possible. This diffractive optic can be readily designed by those skilled in the art. It should be further noted that the optical power at or near the peripheral outer edge of the diffractive optical power region or the spherical power region may be mixed to hide the peripheral edge discontinuity of the second multifocal optic within the composite lens. . In some embodiments of the invention, the second multifocal optic may be provided as a semi-trimmed lens blank having a diffracted optical power region, the diffracted light 130295.doc -58- 200912425 power region on one surface of the optical device The optical power of + 〇〇d is supplied and is not trimmed on the other surface (opposite surface of the optical device). The first multifocal optical device can be cast and cured onto the surface of the second multifocal optic having a diffractive optical power region to form a composite optical device. In this embodiment, the composite lens can have an outer front surface 1 human diffracted optical power region having a progressive optical power region, and - can be performed on a later date: unfinished by molding or surface processing and polishing External back surface. It should be noted that the buried diffracted optical power region will supply optical power to the composite lens due to the difference in refractive index between the first multifocal optic and the first multifocal optic. Understand that although in this particular embodiment of the invention the first multifocal photo-presence device comprises a material having a refractive index of 150 and a second multifocal optics, the member 匕3 has a refractive index of 1.67, but The material for each optics can be reversed. °° The t embodiment of the present invention can be described in terms of the 球 spherical work_region. However, it should be understood that since the diffractive optical power region is a type of substantially spherical power region, such an embodiment also describes an embodiment of the present invention including a diffractive optical power region. Thus, the size, shape, and optics of the diffracted optical power region are the same as the substantially spherical power region 'shape and optical design as described by embodiments of the present invention. Similarly, the alignment of the diffracted optical power region relative to the progressive optical power region can be the same as the large τ occupying spherical power region as described by embodiments of the present invention with respect to the progressive optical region. In another embodiment of the invention, a line of bifocal lenses may be 130295.doc -59 - 200912425 second multifocal optics. The multifocal surface of the lined bifocal lens can be embedded in the composite lens. In this embodiment,

’兄之折射曲線可經設計以在給定用於第二多焦點光學器 件之材料的折射率及用於第一多焦點光學器件之材料的= 射率的情況下允許所需之適當加成功率。此類計算在此項 技術中眾所周知且可順利地及容易地計算。在多數(但並 非所有)情況下,第二多焦點光學器件之附加光功率供鹿 :為峨75D、+1.贿、+125D及一些情況下的+1划中: f °在多數(但並非所有)情況下,第二多焦點光學器件 之遠距離光功率為零光功率1 —多焦點光學器件上之漸 =之光學區域的光功率供應可向佩戴者提供遠距離光功率 +又正且在多數(但並非所有)情況下為乃D、+i 〇〇d及 1.25D中之一者的附加功率供應。 在本發明之其他實施例巾,可修整複合透鏡之外部背表 之後2整,合透鏡之外部背表面時,背表面可提供所需 1提供佩戴者之遠距離、中間距離及/或近距離視 之折射誤:至^ ^。因此’複合透鏡可能夠校正佩戴者 折射誤差’諸如,佩戴者之散光、遠 眼。當背表面未經修整(例如,第”隹…及成老化 ^ 第一多焦點光學器件為半修 =毛述)時,複合透鏡將不具有最終經修整之光功率。 曰圓發月之$ #把例中’具有-多焦點表面之薄光學 二::於填充有未固化樹脂的空腔内以在樹腊固化時 透鏡之鏡。因此’―旦樹月旨固化,樹月旨可形成複合 夕表面。多焦點表面可折射地或繞射地產生光 I30295.doc •60- 200912425 功率。樹脂可具有不同於薄光學晶圓之折射率的折射率。 一旦未固化樹脂之表面中之一者固化,其可形成具有一外 表面曲率的漸進之光功率區域。舉例而言,樹脂可藉由熱 固化、光固化(可見或不可見)或光固化與熱固化之組合來 固化。僅舉例而言,可藉由在鑄造過程中所使用的墊圈來 將光學晶圓固持於適當位置中。 在本發明之另一實施例中,薄光學器件可在其表面上具 有漸進之光功率區域。薄光學器件可具有已知折射率。薄 光學器件可形成於具有與薄光學器件不同之折射率之預製 光學材料之薄層的頂部上以形成一複合光學器件。預製光 學材料可具有一折射地或繞射地產生光功率的大致球面功 率區域。新近形成之複合光學器件可黏著性地接合至較厚 之未修整之透鏡毛坯以形成一複合透鏡,該複合透鏡具 有:一具有漸進之光功率區域的外部前表面、一埋入式大 致球面功率區域,及一能夠由此項技術中已知之製造技術 來修整的未修整之外表面。 在本發明之多數(但並非所有)實施例十,當製造複合透 鏡τ具有大致球面功率區域之透鏡或光學器件可用作一 整體可消耗背部模具,該模具置放於用於鑄造眼科透鏡之 光學墊圈之背部中。術語"整體可消耗"用於指示透鏡或光 干器件用作模具來形成複合透鏡之背部,而且透鏡或光學 器件經消耗且變成接合至固化於模具内的複合透鏡之部 分,從而變成最終複合透鏡之整體部分。可經由用於鑄造 眼科透鏡之玻璃或金屬模具來提供前部模具。形成於前部 J30295.doc •61 - 200912425 模具與背部可消耗模具之間的 光學樹脂來填充且固化。舉例 固化之材料而定’固化可為熱 中之一者。 空腔可用具有適當折射率之 而言,視所需之引發劑及待 固化、光固化或兩者之組合 在本發明之實施例中,剛才所描述之模製技術可允許半 修整或經修整之透错· & 、 之透鏡毛坯的製造。當鑄造複合透鏡為經修 整之透鏡毛柱時,可用1 &立口 ± 用”外邛月表面上之適當環面曲線來'The refractive curve of the brother can be designed to allow the appropriate success to be achieved given the refractive index of the material for the second multifocal optic and the = radiance of the material used for the first multifocal optic. rate. Such calculations are well known in the art and can be calculated smoothly and easily. In most (but not all) cases, the additional optical power of the second multifocal optic is for the deer: 峨75D, +1. bribe, +125D and in some cases +1 stroke: f ° in the majority (but In all cases), the far-distance optical power of the second multifocal optic is zero optical power 1 - the optical power supply of the optical region on the multi-focus optics provides the far-distance optical power to the wearer + And in most (but not all) cases, the additional power supply is one of D, +i 〇〇d, and 1.25D. In other embodiments of the present invention, the outer surface of the composite lens can be trimmed after the outer back surface of the composite lens. When the outer back surface of the lens is closed, the back surface can provide the required distance to provide the wearer's long distance, intermediate distance and/or close range. Refraction error: to ^ ^. Thus the 'composite lens may be capable of correcting the wearer's refractive error' such as the astigmatism of the wearer, the far eye. When the back surface is untrimmed (for example, the first 隹... and the aging ^ the first multifocal optic is half repaired), the composite lens will not have the final trimmed optical power. #例中的薄的光光的光光二:: In the cavity filled with uncured resin, the lens of the lens is cured when the wax is cured. Therefore, the tree can be formed. Composite eve surface. Multifocal surface can produce light refracting or diffracting. I30295.doc •60- 200912425 Power. Resin can have a refractive index different from that of a thin optical wafer. Once one of the surfaces of the uncured resin Curing, which can form a progressive optical power region with an outer surface curvature. For example, the resin can be cured by heat curing, photocuring (visible or invisible) or a combination of photocuring and thermal curing. In this regard, the optical wafer can be held in place by a gasket used in the casting process. In another embodiment of the invention, the thin optical device can have a progressive optical power region on its surface. thin The device may have a known refractive index. A thin optical device may be formed on top of a thin layer of pre-formed optical material having a different refractive index than the thin optical device to form a composite optical device. The preformed optical material may have a refractive or A substantially spherical power region that produces optical power diffracted. The newly formed composite optic can be adhesively bonded to a thicker untrimmed lens blank to form a composite lens having: a progressive optical power region The outer front surface, a buried substantially spherical power region, and an untrimmed outer surface that can be trimmed by fabrication techniques known in the art. In most, but not all, embodiments of the present invention, A lens or optic that produces a composite lens τ having a substantially spherical power region can be used as a unitary consumable back mold that is placed in the back of an optical gasket used to cast an ophthalmic lens. The term "wholely consumable" The indicator lens or the optical dry device is used as a mold to form the back of the composite lens, and the lens or optical device Consumed and become bonded to the portion of the composite lens that is cured within the mold, thereby becoming an integral part of the final composite lens. The front mold can be provided via a glass or metal mold used to cast the ophthalmic lens. Formed in the front J30295.doc • 61 - 200912425 The optical resin between the mold and the back consumable mold is filled and cured. For example, the curing material can be one of the heats. The cavity can be used with the appropriate refractive index, depending on the desired Agents and to be cured, photocured, or a combination of the two In embodiments of the present invention, the molding techniques just described may allow for the fabrication of semi-trimmed or finished transmissive lens blanks. When the lens is a trimmed lens column, the 1 & port can be used ± with the appropriate torus curve on the outer moon surface

預製可消耗背部模具以便校正佩戴者之散光折射誤差。接 著可在塾圈内旋轉可消耗背部模具以允許相對於在複合透 鏡中形成漸進之光功率區域之曲率的前表面模具來對準散 光軸。叹疋散光校正之軸的技術在經修整之眼科透鏡禱造 的技術中眾所周知。 在本發明之又一實施例中,可使用前部整體可消耗模 具。可預成型前部整體可消耗模具,其具有在其外表面上 之漸進之光功率區域曲率及在其内部背表面上折射地或繞 射地產生光功率的球面功率區域。在此情況下,破璃或金 屬模具可用於f部上以形成待用樹脂填充及接著經固化以 形成複合透鏡的空腔。在此情況下,前部可消耗模且可變 成與形成之經固化之樹脂光學器件一體。在此之後,複合 透鏡之背部可經自由成型或研磨及拋光。X,如先前所論 述,複合透鏡之背表面可在固化成經修整之表面時模製, 該經修整之表面提供校正所欲佩戴者之散光所需的必要環 面曲率及/或提供佩戴者之遠距離光功率校正以及佩戴者 之近距離光功率校正所需的適當球面功率。 130295.doc •62- 200912425 圖29A至圖29D展示根據本發明之實施例製造一複合透 鏡之方法。圖29A展示一製造方法,其包括:鑄造一具有 繞射光功率區域的平坦繞射多焦點光學器件,繼之以在繞 射多焦點光學器件之頂部上鑄造漸進之光功率區域之曲 率。圖29B展示與圖29A相同的製造方法,除使用不同前 - 部鑄造眼科材料以外。圖29C展示一製造方法,其包括: . 在眼科材料之前部漸進之光功率區域與背部額外層之間囊 ' 封一具有繞射光功率區域的繞射多焦點光學器件,藉此前 f) 部漸進之光功率區域之材料與背部額外層相同,然而,繞 射多焦點光學器件之材料不同。圖29D展示與圖29D相同的 製造方法,除繞射多焦點光學器件材料由與圖29C中之繞射 多焦點光學器件之眼科材料不同的眼科材料鑄造以外。 表I為各種眼科材料之清單,其中之任何兩者可用於製 造複合透鏡,只要兩種材料相容且將接合至彼此或使用一 塗層來促進兩種材料之間的黏著。Prefabrication can consume the back mold to correct the wearer's astigmatic refractive error. The back mold can then be rotated within the loop to allow alignment of the astigmatism axis with respect to the front surface mold that forms the curvature of the progressive optical power region in the composite lens. The technique of sighing the axis of astigmatism correction is well known in the art of trimmed ophthalmic lens prayer. In yet another embodiment of the invention, a front integral consumable mold can be used. The front portion of the overall consumable mold can be preformed having a progressive optical power region curvature on its outer surface and a spherical power region that refracts or circulates optical power on its inner back surface. In this case, a glass or metal mold can be used on the f portion to form a cavity to be filled with a resin and then cured to form a composite lens. In this case, the front portion can be consumed and can be integrated with the formed cured resin optical device. After that, the back of the composite lens can be freely formed or ground and polished. X, as previously discussed, the back surface of the composite lens can be molded as it is cured into a finished surface that provides the necessary toroidal curvature required to correct the astigmatism of the intended wearer and/or provides the wearer The long-distance optical power correction and the appropriate spherical power required for the wearer's close-range optical power correction. 130295.doc • 62- 200912425 Figures 29A-29D show a method of fabricating a composite lens in accordance with an embodiment of the present invention. Figure 29A shows a method of fabrication comprising: casting a flat diffractive multifocal optic having a region of diffracted optical power followed by casting a curvature of a progressive optical power region on top of the diffractive multifocal optic. Figure 29B shows the same manufacturing method as Figure 29A, except that different front-part cast ophthalmic materials are used. Figure 29C shows a method of fabrication comprising: - a diffuse multifocal optic having a region of diffracted optical power between the progressively progressive optical power region of the ophthalmic material and the additional layer of the back, whereby the front f) is progressive The material of the optical power region is the same as the additional layer of the back, however, the material of the diffractive multifocal optics is different. Figure 29D shows the same fabrication method as Figure 29D except that the diffractive multifocal optic material is cast from an ophthalmic material that is different from the ophthalmic material of the diffractive multifocal optic of Figure 29C. Table I is a list of various ophthalmic materials, any of which can be used to make a composite lens as long as the two materials are compatible and will join to each other or use a coating to promote adhesion between the two materials.

材料 折射率 Abbe 值 供應商 CR39 1.498 55 PPG Nouryset 200 1.498 55 Great Lakes Rav-7 1.50 58 Evergreen/Great Lakes Co. Trivex 1.53 44 PPG MR-8 1.597 41 Mitsui MR-7 1.665 31 Mitsui MR-10 1.668 31 Mitsui MR-20 1.594 43 Mitsui Brite-5 1.548 38 Doosan Corp·(韓國) Brite-60 1.60 35 Doosan Corp.(韓國) Brite-Super 1.553 42 Doosan Corp.(韓國) TS216 1.59 32 Tokuyama 聚碳酸酯 1.598 31 GEMaterial Refractive Index Abbe Value Supplier CR39 1.498 55 PPG Nouryset 200 1.498 55 Great Lakes Rav-7 1.50 58 Evergreen/Great Lakes Co. Trivex 1.53 44 PPG MR-8 1.597 41 Mitsui MR-7 1.665 31 Mitsui MR-10 1.668 31 Mitsui MR-20 1.594 43 Mitsui Brite-5 1.548 38 Doosan Corp. (Korea) Brite-60 1.60 35 Doosan Corp. (Korea) Brite-Super 1.553 42 Doosan Corp. (Korea) TS216 1.59 32 Tokuyama Polycarbonate 1.598 31 GE

表I 130295.doc •63- 200912425 在本發明之某些實施例中,混合區在大致球面功率區域 之至少一部分與遠距離區之間過渡光功率。圖27A至27C 展示具有一混合區2710之本發明之實施例,該混合區具有 位於配合點2720處或下方的大體上恆定寬度。圖28A至 28C展示具有一混合區2810之本發明之實施例,該混合區 - 包括一具有位於配合點2820處或下方之大體上0 mm之寬度 的部分(進而類似於具線紋之雙焦點透鏡在此部分中提供 • 過渡)。圖27A及圖28A展示位於配合點處的混合區之頂部 (') 邊緣。圖27B及圖28B展示位於配合點下方3 mm處的混合 區之頂部邊緣。圖27C及圖28C展示位於配合點下方6 mm 處的混合區之頂部邊緣。混合區2710及2810之部分可小於 大約2.0 mm寬且可在大約0.5 mm寬與大約1.0 mm寬之間。 應注意,本發明預期使用具有在大約0.1 mm與大約1.0 mm 之間的寬度之混合區。圖28A進一步展示對應於配合點之 位置的混合區之中心區域具有在大約0.1 mm與大約0.5 mm 之間的寬度。圖28C展示寬度減小以在混合區之中心區域 li 中不具有混合的混合2810。 大致球面功率區域及遠距離區各自具有可由特定光學相 " 位分布所界定的光功率。為了形成給定寬度之混合區,產 • 生相位分布,其在本發明之某些實施例中在混合區之起始 處匹配第一光功率區域的相位分布之值及第一空間導數且 在混合區之結束處匹配第二光功率區域的相位分布之值及 第二空間導數。在本發明之其他實施例中,混合區相位分 布之起始及結束分別匹配第一及第二光功率區域之相位分 130295.doc -64- 200912425 布的值以及第一及第二空間導數。在任一情況下,混合區 之相位分布可由一或多個數學函數及/或表達式來描述, 其可包括(但不限於)二階或更高階多項式、指數函數、三 角函數及對數函數。在本發明之某些實施例中,混合區為 繞射的’在本發明之其他實施例中,混合區為折射的,且 ; 在本發明之其他實施例中,混合區具有折射及繞射子區。 在本發明之一些實施例中,為了使透鏡提供高品質視 力,犯合區之寬度必須非常窄。混合區必須窄以允許佩戴 〇 者之眼睛在佩戴者之視線在遠距離焦點與中間距離或近距 離焦點之間切換時快速地橫越混合區。舉例而言,混合區 之寬度必須小於大約2.0 mm,小於大約丨〇 mm,或小於大 、、勺0 ’ 5 mm。使用習知眼科透鏡製造技術來製造此窄混合區 非常困難。舉例而言,當前技術現狀之單點、自由成型眼 科表面產生僅卉可具有超過大約〇5 之寬度的混合區。 此外,此等方法提供很少或不提供對混合區輪廓之精確形 的控制用於由液體單體樹脂來轉造透鏡之習知玻璃模 / 具加工的產生亦有限,因為玻璃不能單點加工且必須與所 有精細表面特徵可能丟失的研磨過程一起工作。 、田刖,可用於產生具有一具有已知且以經濟可行方式良 好又控之輪廓之窄混合區的透鏡之唯一方法係金屬透鏡模 八,單沾金剛石車削。在此方法中,金剛石力口工設備配備 有緩It或快速工具伺服能力,兩者在此項技術中眾所周 知僅舉例而言,此等模具可以諸如電解州或〜州之材料 可用於液體單體樹脂鑄造過程或熱塑性射出成型過 130295.doc -65- 200912425 程。 、以上發明性實施例中之每一者可使用金剛石車削、自由 成型、表面鑄造、完整透鏡鑄造、層壓或模製(包括射出 成型)來製造。已發現,在無混合區之實施例中,金剛石 車削提供最陡不連續性及最佳保真度。在多數(但並非所 有)it况下,由金屬(諸如,僅舉例而言,塗有錄之鋁戈 鋼,或銅鎳合金)來金剛石車削模具。用以產生光功率之 步級所需之製造方法或技術在工業中已知且由㈠堇舉例而 言)金剛石車削模具或嵌入物及接著鑷造或射出成型透 鏡、金剛石車削實際透鏡,及自由成型組成。 在本發明之一實施例中,藉由利用技術現狀之自由成型 製造技術,有可能將校正佩戴者之散光折射誤差的環面表 面置放於與大致球面功率區域相同的透鏡之表面上。當此 兩個不同表面曲線係藉由自由成型產生時,接著有可能將 漸進之光功率區域置放於透鏡之相反表面上。在此情況 下’漸進之光功率區域經模製及預成型於半修整之毛坯的 一個表面上,且組合之散光校正及球面功率區域係經由自 由成型半修整之毛坯的相反未修整之表面來提供。 在本發明之一些實施例中,大致球面功率區域寬於由高 於大約1.00D之不當散光所限制之通道的最窄部分。在本 發明之其他實施例中,大致球面功率區域寬於由高於大約 0.75D之不當散光所限制之通道的最窄部分。 在本發明之一些實施例中,大致球面功率區域可大體上 為球面或可亦為非球面;舉例而言,以便校正散光。大致 130295.doc -66- 200912425 球面功率區域亦可具有經置放以改良透鏡之美觀性或以減 小失真之一非球面曲線或多個曲線。在本發明之一些實施 例中’發明性多焦點透鏡為靜態的。在本發明之其㈣施 例中,發明性多焦點透鏡為動態的,且大致球面功率區域 由(例如)電活性元件動態地產生。在本發明之一些實施例 中,大致球面功率區域為嵌入式繞射元件,諸如,表面起 伏繞射元件。 本發明預期如下半修整之透鏡毛坯的生產,其中一個經 修整之表面包含大致球面功率區域、遠距離區及混合區, 且另一表面未經修整。本發明預期如下半修整之透鏡毛坯 的生產,其中一個經修整之表面包含漸進之光功率區域, 且另一表面未經修整。本發明亦預期針對某些處方而產生 、、至〇整之透鏡毛坯。亦應注意,本發明預期相對於大致球 面功率區域最佳化漸進之光功率區域以最佳化不當散光之 程度、通道長度及通道寬度。此外,本發明預期在必要時 最佳化混合區以減小在混合區中找到的不當散光。此外, 本發明允許使用任何透鏡材料,不管為塑料、玻璃、樹脂 還是複合物。本發明亦預期使用任何光學有用折射率。本 發明亦允許可能通常用於眼科透鏡上的所有塗層及透鏡處 理,諸如,僅舉例而言,耐硬擦傷之塗層、抗折射塗層、 緩衝塗層,及自我清潔鐵氟龍(Tefl〇n)塗層。最後,本發 明提供藉由此項技術中已知的技術來製造,包括(但不限 於)表面加工、自由成型、金剛石車削、銑削、衝壓、射 出成型、表面鑄造、層壓、整邊、研磨及鑽孔。 130295.doc •67· 200912425 應進一步注意,本發明預期與隱形眼鏡及眼鏡片一起使 用。 為了更清楚地展示發明性多焦點透鏡優於習知技術現狀 PAL之優越性,將本發明之一實施例與兩個技術現狀PAL 進行比較。透鏡之量測係由Visionix登記商標之Visionix VM-2500TM透鏡繪圖儀來獲得。技術現狀PAL中之一者為 由Varilux登記商標的Varilux Physio™透鏡,其具有大約 + 2.00D附加功率。技術現狀PAL中之另一者為由Varilux登 記商標的Varilux Ellipse™透鏡,其具有短通道設計及大約 + 2.00D附加功率。如在表II中可見,Physio透鏡具有1.68D 之最大不當散光,10.5 mm之通道寬度及1 7.0 mm之通道長 度。Ellipse透鏡具有2.00D之最大不當散光,8.5 mm之通 道寬度及1 3.5 mm之通道長度。發明性透鏡亦具有大約 + 2.00之附加功率。然而,相比而言,發明性透鏡具有小 於1.00D之最大不當散光。由於最大不當散光低於1.00D, 所以對於所有意圖及目的而言,通道寬度與透鏡自身一樣 寬。最後,通道長度為14.5 mm。亦應指出,Visionix VM-2500™透鏡繪圖儀與Rotlex Class Plus™透鏡繪圖儀均歸因 於其小寬度而不能夠偵測發明性透鏡中之不連續性處的不 當散光。Table I 130295.doc • 63- 200912425 In some embodiments of the invention, the mixing zone transitions optical power between at least a portion of the substantially spherical power region and the remote region. Figures 27A through 27C show an embodiment of the invention having a mixing zone 2710 having a substantially constant width at or below the mating point 2720. Figures 28A through 28C show an embodiment of the invention having a mixing zone 2810 that includes a portion having a width of substantially 0 mm at or below the mating point 2820 (and thus resembling a double focus with a line) The lens is provided in this section • Transition). Figures 27A and 28A show the top (') edge of the mixing zone at the mating point. Figures 27B and 28B show the top edge of the mixing zone located 3 mm below the mating point. Figures 27C and 28C show the top edge of the mixing zone 6 mm below the mating point. Portions of mixing zones 2710 and 2810 can be less than about 2.0 mm wide and can be between about 0.5 mm wide and about 1.0 mm wide. It should be noted that the present invention contemplates the use of a mixing zone having a width of between about 0.1 mm and about 1.0 mm. Figure 28A further shows that the central region of the mixing zone corresponding to the location of the mating point has a width of between about 0.1 mm and about 0.5 mm. Figure 28C shows a blend 2810 having a reduced width to have no mixing in the central region li of the mixing zone. The substantially spherical power region and the remote region each have an optical power that can be defined by a particular optical phase " bit distribution. In order to form a mixing zone of a given width, a phase distribution is produced which, in some embodiments of the invention, matches the value of the phase distribution of the first optical power region and the first spatial derivative at the beginning of the mixing zone and The end of the mixing zone matches the value of the phase distribution of the second optical power zone and the second spatial derivative. In other embodiments of the invention, the start and end of the mixing zone phase distribution respectively match the values of the phase scores 130295.doc -64 - 200912425 of the first and second optical power zones and the first and second spatial derivatives. In either case, the phase distribution of the mixing zone can be described by one or more mathematical functions and/or expressions, which can include, but are not limited to, second-order or higher order polynomials, exponential functions, trigonometric functions, and logarithmic functions. In some embodiments of the invention, the mixing zone is diffractive. In other embodiments of the invention, the mixing zone is refractive, and in other embodiments of the invention, the mixing zone has refraction and diffraction. Sub-area. In some embodiments of the invention, in order for the lens to provide high quality vision, the width of the compromise zone must be very narrow. The mixing zone must be narrow to allow the wearer's eyes to quickly traverse the mixing zone as the wearer's line of sight switches between a distant focus and an intermediate or near focus. For example, the width of the mixing zone must be less than about 2.0 mm, less than about 丨〇 mm, or less than a large, spoon 0' 5 mm. It is very difficult to fabricate this narrow mixing zone using conventional ophthalmic lens manufacturing techniques. For example, the single point, freeform ophthalmic surface of the current state of the art produces a mixing zone that can only have a width greater than about 〇5. In addition, these methods provide little or no control over the precise shape of the contour of the mixing zone. The use of conventional glass molds for the conversion of lenses from liquid monomer resins is also limited because glass cannot be processed at a single point. It must work with all grinding processes where fine surface features may be lost. The only method that can be used to produce a lens having a narrow mixing zone with a known and economically viable and well-controlled profile is a metal lens mold, single-dip diamond turning. In this method, the diamond force oral equipment is equipped with a slow It or fast tool servo capability, both of which are well known in the art by way of example only, such molds may be used for materials such as electrolysis or statistic for liquid monomers Resin casting process or thermoplastic injection molding has passed 130295.doc -65- 200912425. Each of the above inventive examples can be fabricated using diamond turning, free forming, surface casting, full lens casting, lamination or molding (including injection molding). It has been found that in the embodiment without the mixing zone, diamond turning provides the steepest discontinuity and the best fidelity. In most (but not all) conditions, the metal is turned by a metal (such as, for example, a coated aluminum steel, or a copper-nickel alloy). The manufacturing methods or techniques required to produce the steps of optical power are known in the industry and, by way of example, diamond turning dies or inserts and subsequent fabrication or injection molding lenses, diamond turning actual lenses, and freedom Molding composition. In one embodiment of the present invention, it is possible to place a toroidal surface correcting the astigmatism refractive error of the wearer on the surface of the same lens as the substantially spherical power region by utilizing the state of the art free-form manufacturing technique. When the two different surface curves are produced by freeform formation, it is then possible to place the progressive optical power region on the opposite surface of the lens. In this case, the 'gradual optical power region is molded and preformed onto one surface of the semi-trimmed blank, and the combined astigmatism correction and spherical power regions are via the opposite untrimmed surface of the freeform semi-trimmed blank. provide. In some embodiments of the invention, the substantially spherical power region is wider than the narrowest portion of the channel bound by improper astigmatism above about 1.00D. In other embodiments of the invention, the substantially spherical power region is wider than the narrowest portion of the channel bound by improper astigmatism above about 0.75D. In some embodiments of the invention, the substantially spherical power region may be substantially spherical or may be aspheric; for example, to correct for astigmatism. Approximate 130295.doc -66- 200912425 The spherical power zone may also have an aspherical curve or curves that are placed to improve the aesthetics of the lens or to reduce distortion. In some embodiments of the invention, the inventive multifocal lens is static. In its (iv) embodiment of the invention, the inventive multifocal lens is dynamic and the substantially spherical power region is dynamically generated by, for example, an electroactive element. In some embodiments of the invention, the substantially spherical power region is a built-in diffractive element, such as a surface undulating diffractive element. The present invention contemplates the production of a semi-trimmed lens blank wherein one of the finished surfaces comprises a substantially spherical power zone, a remote zone and a mixing zone, and the other surface is untrimmed. The present invention contemplates the production of a semi-trimmed lens blank wherein one of the finished surfaces contains a progressive optical power region and the other surface is untrimmed. The present invention also contemplates lens blanks that are produced for certain prescriptions. It should also be noted that the present invention contemplates optimizing the progressive optical power region relative to the approximate spherical power region to optimize the extent of improper astigmatism, channel length, and channel width. Moreover, the present invention contemplates optimizing the mixing zone as necessary to reduce improper astigmatism found in the mixing zone. Furthermore, the invention allows the use of any lens material, whether plastic, glass, resin or composite. The invention also contemplates the use of any optically useful refractive index. The present invention also allows for all coatings and lens treatments that may be commonly used on ophthalmic lenses, such as, by way of example only, hard abrasion resistant coatings, anti-refracting coatings, buffer coatings, and self-cleaning Teflon (Tefl) 〇n) Coating. Finally, the invention is made by techniques known in the art including, but not limited to, surface machining, free forming, diamond turning, milling, stamping, injection molding, surface casting, lamination, trimming, grinding And drilling. 130295.doc •67· 200912425 It should be further noted that the present invention is contemplated for use with contact lenses and ophthalmic lenses. In order to more clearly demonstrate the superiority of the inventive multifocal lens over the state of the art PAL, one embodiment of the present invention is compared to two state of the art PAL. The measurement of the lens is obtained by the Visionix VM-2500TM Lens Plotter, a registered trademark of Visionix. One of the state of the art PAL is the Varilux PhysioTM lens, a trademark registered by Varilux, which has an additional power of approximately + 2.00D. State of the Art The other in PAL is the Varilux EllipseTM lens, registered by Varilux, which has a short channel design and approximately + 2.00 D additional power. As can be seen in Table II, the Physio lens has a maximum improper astigmatism of 1.68D, a channel width of 10.5 mm and a channel length of 1 7.0 mm. The Ellipse lens has a maximum improper astigmatism of 2.00D, a channel width of 8.5 mm and a channel length of 1 3.5 mm. The inventive lens also has an additional power of about + 2.00. However, in contrast, the inventive lens has a maximum improper astigmatism of less than 1.00D. Since the maximum improper astigmatism is less than 1.00D, the channel width is as wide as the lens itself for all intents and purposes. Finally, the channel length is 14.5 mm. It should also be noted that both the Visionix VM-2500TM Lens Plotter and the Rotlex Class PlusTM Lens Plotter are due to their small width and are not capable of detecting inappropriate astigmatism at discontinuities in the inventive lens.

屬性 VARILUX ELLIPSE VARILUX PHYSIO 發明性實施例 (2.00D附加功率) (2.00D附加功率) (10球面透鏡+10附加 PHYSIO) 距離功率 0.12D .08D -0.11D 近總功率 2.11D 2.17D 1.90D 130295.doc -68- 200912425Attribute VARILUX ELLIPSE VARILUX PHYSIO Inventive embodiment (2.00D additional power) (2.00D additional power) (10 spherical lens + 10 additional PHYSIO) Distance power 0.12D .08D -0.11D Near total power 2.11D 2.17D 1.90D 130295. Doc -68- 200912425

總附加功率 1.99D 2.11D 2.02D 通道長度 13.5MM 17.0MM 14.5MM 通道寬度 8.5MM 10.5MM 23.5MM 最大不當散光 2.05D 1.68D 0.90D (中線下方) 最大不當散光 0.98D 0.95D 0.5D (中線上方) 表II 【圖式簡單說明】 圖1A至圖13B展示具有感覺得到之影像中斷或不具有感 覺得到之影像中斷的不同透鏡; 圖14A展示根據本發明之實施例的具有兩個光功率區域 及一混合區之一透鏡之前表面的視圖; 圖14B展示根據本發明之實施例的具有兩個光功率區域 及一混合區之一透鏡之前表面的視圖; 圖14C展示圖14A或圖14B之透鏡之背表面的視圖,其具 有在透鏡之配合點下方的漸進之光功率區域; 圖14D展示圖14A或圖14B之透鏡之背表面的視圖,其具 有在透鏡之配合點處或附近的漸進之光功率區域; 圖14E展示穿過透鏡之中心垂直線所截取的圖14A及圖 14C之透鏡的橫截面圖; 圖14F自前面展示圖14A及圖14C之發明性透鏡,其展示 在透鏡之前表面及背表面上之光功率區域的置放及光學對 準; 130295.doc -69- 200912425 圖14G自前面來展示圖14B及圖14c之發明性透鏡,其展 示在透鏡之前表面及背表面上之光功率區域的置放及光學 對準; 圖15A展示根據本發明之實施例具有兩個光功率區域及 一混合區之一透鏡之前表面的視圖; 圖15B展示圖15A之透鏡之背表面的視圖,其具有在透 鏡之配合點下方的漸進之光功率區域; 圖15C展示一具有一表面之發明性透鏡,該表面為圖 15人之表面與圖158之表面的數學組合; 圖15D展示用插圖解釋圖1SA及圖1SB之表面如何組合以 形成圖15C之表面的圖; 圖16展示由Rotlex登記商標之R〇Uex aass piusTM所量測 之關於具有+1.25D之近距離附加功率之以下透鏡的附加功 率梯度:由Essilor登記商標之EssU〇r physi〇TM透鏡、由 Essilor登記商標之Essil〇r miipseTM透鏡,及由处咖卜 Optical 登記商標之 Shamir Picc〇i〇TM透鏡; 圖17展示在如由R0tlex登記商標之R〇Uex Class plusTM所 量測之圖16的三個透鏡中找到的自西己合點沿附加功率之通 道向下所獲得之量測; 圖18展示在本發明之實施例中找到的自配合點沿附加功 率之通道向下所獲得之量測,其中具有+1.00D之光功率之 一大致球面功率區域置放為與圖16之透鏡光通信; 圖19展示如由R〇tlex登記商標之R〇Uex class plusTM所量 測之關於左側發明性透鏡之—實施例及右側由Essilor登記 130295.doc 200912425 商標之Essilor Physio™透鏡兩者的附加功率梯度; 圖20展示自如由Rotlex登記商標之Rotlex Class Plus™所 量測之圖19的兩個透鏡中找到的附加功率之通道下方的配 合點處所獲得之量測; 圖21展示發明性透鏡之四個區域:一遠距離區、一上部 遠-中間距離區、一中間距離區及一近距離區; 圖2 2至圖2 3展示沿本發明之實施例之中心垂直中線的光 功率’該等實施例包括將遠距離區連接至近距離區的漸進 之光功率區域; 圖2 4至圖2 6展示沿本發明之實施例之中心垂直中線的光 功率’該等實施例包括一大致球面功率區域、一不連續性 及一將遠距離區連接至近距離區的漸進之光功率區域; 圖27A至圖27C展示具有一混合區之本發明之實施例, 該混合區具有位於透鏡之配合點處或下方的大體上恆定寬 度; 圖28A至圖28C展示具有一混合區之本發明之實施例, 該混合區包括一具有位於透鏡之配合點處或下方之大體上 〇 mm之寬度的部分(進而類似於具線紋之雙焦點透鏡在此 部分中提供過渡);及 圖29A至圖29D展示根據本發明之實施例製造一複合透 鏡之方法。 【主要元件符號說明】 1410 距離區 1415 距離光功率 130295.doc 200912425Total additional power 1.99D 2.11D 2.02D channel length 13.5MM 17.0MM 14.5MM channel width 8.5MM 10.5MM 23.5MM maximum improper astigmatism 2.05D 1.68D 0.90D (below the midline) maximum improper astigmatism 0.98D 0.95D 0.5D (medium Above the line) Table II [Simple Description of the Drawings] Figures 1A-13B show different lenses with perceived image interruption or no perceived image interruption; Figure 14A shows two optical powers in accordance with an embodiment of the present invention. A view of the front surface of the lens of one of the regions and a mixing zone; Figure 14B shows a view of the front surface of the lens having two optical power regions and a mixing region in accordance with an embodiment of the present invention; Figure 14C shows Figure 14A or Figure 14B a view of the back surface of the lens with a progressive optical power region below the mating point of the lens; Figure 14D shows a view of the back surface of the lens of Figure 14A or Figure 14B with a progressive at or near the mating point of the lens Figure 14E shows a cross-sectional view of the lens of Figures 14A and 14C taken through the centerline of the lens; Figure 14F The inventive lenses of Figures 14A and 14C are shown above, showing the placement and optical alignment of the optical power regions on the front and back surfaces of the lens; 130295.doc -69- 200912425 Figure 14G shows Figure 14B from the front and The inventive lens of Figure 14c, which shows the placement and optical alignment of the optical power regions on the front and back surfaces of the lens; Figure 15A shows one of two optical power regions and one mixing region in accordance with an embodiment of the present invention. Figure 15B shows a view of the back surface of the lens of Figure 15A with a progressive optical power region below the mating point of the lens; Figure 15C shows an inventive lens having a surface, the surface being a Figure 15D shows a diagram explaining how the surfaces of Figures 1SA and 1SB are combined to form the surface of Figure 15C; Figure 16 shows the R〇Uex aass piusTM registered by Rotlex. Additional power gradients for the following lenses with close-range additional power of +1.25D: EssU〇r physi〇TM lens registered by Essilor, registered by Essilor The Essil〇r miipseTM lens, and the Shamir Picc〇i® lens from the officially registered trademark; Figure 17 shows the three lenses of Figure 16 as measured by the R〇Uex Class plusTM registered by R0tlex. The measurement obtained from the west self-combination point along the channel of additional power is shown; Figure 18 shows the measurement obtained by the self-mating point found in the embodiment of the invention along the channel of additional power, wherein One of the optical powers of +1.00 D is placed in a substantially spherical power area for optical communication with the lens of Figure 16; Figure 19 shows the left inventive lens as measured by the R〇Uex class plusTM registered trademark of R〇tlex. Additional power gradients for both the embodiment and the Essilor Registered 130295.doc 200912425 trademark Essilor PhysioTM lens; Figure 20 shows the two lenses of Figure 19 as measured by the Rotlex Class PlusTM of the Rotlex registered trademark. The measurement obtained at the matching point below the channel of the additional power; Figure 21 shows four regions of the inventive lens: a long distance zone, an upper far-middle distance zone, a middle distance zone and a Close range; Figure 2 2 to 2 3 show optical power along a central vertical centerline of an embodiment of the invention. These embodiments include a progressive optical power region that connects the remote zone to the close zone; Figure 2 4 26 shows the optical power along the center vertical centerline of an embodiment of the invention. The embodiments include a substantially spherical power region, a discontinuity, and a progressive optical power that connects the remote region to the close region. Figure 27A-27C shows an embodiment of the invention having a mixing zone having a substantially constant width at or below the mating point of the lens; Figures 28A-28C show the invention having a mixing zone In an embodiment, the mixing zone includes a portion having a width of substantially 〇mm at or below the mating point of the lens (and thus a line-like bifocal lens providing a transition in this portion); and FIG. 29A to 29D shows a method of fabricating a composite lens in accordance with an embodiment of the present invention. [Main component symbol description] 1410 Distance zone 1415 Distance optical power 130295.doc 200912425

1420 致球面功率區域 1430 合點 1440 合區 1450 進之光功率區域 1465 近距離附加功率 1470 功率之步級 1510 致球面功率區域 1520 合區 1530 進之光功率區域 2110 距離區 2120 部遠-中間距離區 2130 間距離區 2140 距離區 2210 轴 2220 合點 2230 台 2240 台 2310 軸 2320 鏡 2330 台 2340 台 2350 台 2410 轴 2420 合點 130295.doc -72- 200912425 2430 連續 2440 功率 2450 台 2460 光功 2470 間距 2480 近距 2510 轴 2520 連續 2530 合點 2540 功率 2560 球面 2570 光功 2580 部遠 2585 間距 2590 近距 2595 部遠 2610 軸 2620 連續 2630 合點 2640 部遠 2650 間距 2660 功率 2680 近距 2710 合區1420 Spherical power zone 1430 Junction 1440 Junction 1450 Into the optical power zone 1465 Close-range additional power 1470 Power step 1510 Spherical power zone 1520 Junction 1530 Into the optical power zone 2110 Distance zone 2120 Far-middle distance Zone 2130 Distance zone 2140 Distance zone 2210 Axis 2220 Coupling 2230 Taiwan 2240 Taiwan 2310 Axis 2320 Mirror 2330 Taiwan 2340 2350 Taiwan 2410 Axis 2420 Coupling 130295.doc -72- 200912425 2430 Continuous 2440 Power 2450 Taiwan 2460 Optical work 2470 Spacing 2480 Close range 2510 Axis 2520 Continuous 2530 Coupling 2540 Power 2560 Spherical 2570 Optical work 2580 Part 2585 Pitch 2590 Close distance 2595 Part far 2610 Axis 2620 Continuous 2630 Joint 2640 Part 2650 Pitch 2660 Power 2680 Close range 2710

性 率 離校正 離光功率 性 部分 率 -中間距離校正 離校正 離光功率 -中間距離校正 性 -中間距離區 離區 離光功率 130295.doc •73- 200912425 2720 合點 2810 合區 2820 合點Saturation Rate Offset Power Offset Power Rate Partial Rate - Intermediate Distance Correction Offset Offset Power Offset - Intermediate Distance Correction - Intermediate Distance Zone Offset Power Offset Power 130295.doc •73- 200912425 2720 Joint 2810 Junction 2820 Joint

C 130295.doc -74-C 130295.doc -74-

Claims (1)

200912425 十、申請專利範圍: 1. 一種具有一遠距離區之眼科透鏡,其包含. 一用於提供第一遞增附加光功率之繞射光功率區 域,; 一位於該遠距離區與該繞射光功率區域之間之不連續 性;及 一用於提供第二遞增附加光功率之漸進光功率區域, 其中該繞射光功率區域之至少一部分係與該冑進之光功 率區域處於光通信中,因此該第—遞增附加光功率及該 第二遞增附加光功率一起提供使用者一近距離附加功 率〇 2·如請求項1之眼科透鏡,其進一步包含: 一光功率之平台,其位於該漸進之光功率區域之一部 分中,以用於在該眼科透鏡之中間距離區中提供視力之 垂直穩定性。 3.如請求項2之眼科透鏡,其令該光功率之平台具有大約】 毫米至大約3毫米或更大的垂直長度。 4·如請求項2之眼科透鏡,其中該光功率之平台具有大約2 毫米至大約6毫米或更大的垂直長度。 5.如請求項1之眼科透鏡’其進一步包含: 犯σ區其用於跨越該不連續性之至少一部分而混 合該光功率。 6·如請求項5之眼科透鏡,其中該混合區之至少一部分具 有大約2.0毫米或更小的寬度。 130295.doc 200912425 7. 如請求項1之眼科透鏡,其中該眼科透鏡具有—中間距 離區’且該中間距離區具有一在該近距離附加功率之大 約45%與大約55%之間的附加功率。 8. 如請求項!之眼科透鏡,其中該透鏡具有—配合點,且 其中該繞射光功率區域之頂部邊緣係定位於該配合點下 方大約3毫米與大約4毫米之間處,且其中該漸進之光功 率區域係起始於距該繞射光功率區域之該頂部邊緣大約 4毫米與大約8毫米之間處。 9. 如請求項1之眼科透鐘,1由y π 打慫筑其中该不連續性係由光功率之 一步級所引起。 至少大 10.如請求項9之眼科透鏡,其中該光功率之步級為 約+ 0.12 D之光功率的一步升。 U.如請求項1之眼科透鏡’其中該繞射光功率區域係定位 於該透鏡之一表面上或埋入於該透鏡内。 A如請求机眼科透鏡’其中該漸進之光功率區域係定 位於該透鏡之一表面上或埋入於該透鏡内。 13.如請求項!之眼科透鏡,其中該漸進之光功率區域包含 -漸進之光功率表面,且其中該漸進之光功率表面係藉 由自由成型、模製或表面澆鑄中之一者來產生。 Μ.如請求W之眼科透鏡,丨中該繞射光功率區域係藉由 自由成型該透鏡之-表面、模製該透鏡之—表面、或將 一表面埋入於該透鏡内中之一者來產生。 15. 如請求項1之眼科透鏡,其中該透鏡包含一上部遠-中間 距離區,且其中該上部遠_中間距離區具有—在該近距離 130295.doc 200912425 附加功率的大約2〇%與大約44%之間的附加功率。 16.如凊求項1之眼科透鏡,其中該透鏡具有一配合點,且 其中該繞射光功率區域之頂部邊緣係定位於該配合點下 n 9 2毛米與大約5毫米之間處,且其中該漸進之光功 率區域係起始於距該繞射光功率區域之該頂部邊緣大約 4毫米與大約8毫米之間處。 17·如請求項!之眼科透鏡,其中該透鏡具有—近距離區, 中由該漸進之光功率區域所貢獻之該光功率在該近 距離區之後降低以便提供一下部遠_中間區。 18. —種透鏡,其包含: 具有第一折射率之第一層,其中該第一層具有第 一曲率及第二曲率,其中該第二曲率提供一單一光功 率;及 一具有不同於該第一折射率之第二折射率之第二層, 其中該第二層具有第—曲率及第二曲率,其中該第二層 之第二曲率提供一漸進之光功率且係與該第—層之第二 曲率處於光通信中,並藉此提供一組合光功率以校正近 距離視力。 19. 如請求項18之透鏡,其中該單—光功率係—球面光功 〇 20. 如請求項18之透鏡,其中該第二層之第二曲率係於 透鏡之外表面上。 ' 21_如請求項18之透鏡,其中該第一層之第二曲率係自透鏡 之配合點下方4毫米處開始。 兄 130295.doc 200912425 —及弟二曲率 間 22.如請求項18之透鏡’其中該第一層之第 之透鏡光功率具有不連續性。 23_ —種透鏡,其包含: -具有第-折射率之第一層,其中該第一層包含一遠 距離區及一第一光學元件;及 -具有不同於該第一折射率之第二折射率之第二層, 其中該第二層包含一遠距離區及一第二光學元件, 其中該第一光學元件包含一訾皙 ^ s 貫買上球面之光功率區 域,該實質上球面之光功率區域供應透鏡之總近距離附 加功率之第一部份, 其中由於該第一層之該第一光學元件及該遠距離區之 間之光功率步升’在該第一層之該第一光學元件及該遠 距離區之邊界上產生一光學不連續性, 其中s亥第一光學凡件係位於透鏡之配合點下方*毫米 處, 其中該第二光學元件包含一漸進之光功率區域,該漸 進之光功率區域供應透鏡之總近距離附加功率之第二部 份,且 其中β亥第一及第二光學元件係處於光通信中,因此該 透鏡之總近距離附加功率之第一部份與該透鏡之總近距 離附加功率之第二部份係組合以供應該透鏡之總近距離 附加功率。 24.如請求項23之透鏡,其中該第—及第二光學元件係經對 準以形成一遠-中間距離區及一中間距離區。 130295.doc 200912425 2 5.如請求項2 4之透鏡5其中該达-中間距離區具有一在該透 鏡之總近距離附加功率之大約20%與大約44%之間的附 加功率,且該中間距離區具有一在該透鏡之總近距離附 加功率之大約45%與大約55%之間的附加功率。 130295.doc200912425 X. Patent Application Range: 1. An ophthalmic lens having a long distance zone, comprising: a diffractive optical power region for providing a first incremental additional optical power; and a diverging optical power at the remote distance region a discontinuity between the regions; and a progressive optical power region for providing a second incremental additional optical power, wherein at least a portion of the diffracted optical power region is in optical communication with the advanced optical power region, such The first-incremental additional optical power and the second incremental additional optical power together provide a near-field additional power of the user. The ophthalmic lens of claim 1, further comprising: a platform of optical power located in the progressive light In one portion of the power region, for providing vertical stability of vision in the intermediate distance region of the ophthalmic lens. 3. The ophthalmic lens of claim 2, wherein the platform of optical power has a vertical length of from about [mm] to about 3 mm or more. 4. The ophthalmic lens of claim 2, wherein the platform of optical power has a vertical length of from about 2 mm to about 6 mm or more. 5. The ophthalmic lens of claim 1 further comprising: a sigma zone for mixing the optical power across at least a portion of the discontinuity. 6. The ophthalmic lens of claim 5, wherein at least a portion of the mixing zone has a width of about 2.0 mm or less. The method of claim 1 , wherein the ophthalmic lens has an intermediate distance zone and the intermediate distance zone has an additional power between about 45% and about 55% of the approximate additional power. . 8. As requested! An ophthalmic lens, wherein the lens has a mating point, and wherein a top edge of the diffracted optical power region is positioned between about 3 mm and about 4 mm below the mating point, and wherein the progressive optical power region is Starting between about 4 mm and about 8 mm from the top edge of the diffracted optical power region. 9. In the ophthalmic clock of claim 1, 1 is constructed by y π, wherein the discontinuity is caused by a step of optical power. At least 10. The ophthalmic lens of claim 9 wherein the step of optical power is one step liter of optical power of about + 0.12 D. U. The ophthalmic lens of claim 1, wherein the diffractive optical power region is located on or embedded in a surface of the lens. A, such as a requesting ophthalmic lens, wherein the progressive optical power region is located on or embedded in one of the lenses. 13. The ophthalmic lens of claim 3, wherein the progressive optical power region comprises a progressive optical power surface, and wherein the progressive optical power surface is produced by one of free forming, molding, or surface casting. . In the case of an ophthalmic lens of claim W, the diffractive optical power region is formed by freely molding the surface of the lens, molding the surface of the lens, or embedding a surface in the lens. produce. 15. The ophthalmic lens of claim 1, wherein the lens comprises an upper distal-intermediate distance region, and wherein the upper distal-intermediate distance region has - about 2% and about approximately 30% of the additional power at the close distance 130295.doc 200912425 Additional power between 44%. 16. The ophthalmic lens of claim 1, wherein the lens has a mating point, and wherein a top edge of the diffracted optical power region is positioned between n 9 2 m and about 5 mm below the mating point, and Wherein the progressive optical power region begins at between about 4 mm and about 8 mm from the top edge of the diffracted optical power region. 17. If requested! An ophthalmic lens, wherein the lens has a close-range region in which the optical power contributed by the progressive optical power region is reduced after the near-field to provide a lower-intermediate region. 18. A lens comprising: a first layer having a first index of refraction, wherein the first layer has a first curvature and a second curvature, wherein the second curvature provides a single optical power; and one has a different a second layer of a second index of refraction of the first index of refraction, wherein the second layer has a first curvature and a second curvature, wherein the second curvature of the second layer provides a progressive optical power and is coupled to the first layer The second curvature is in optical communication and thereby provides a combined optical power to correct for close vision. 19. The lens of claim 18, wherein the single-optical power system - spherical optical work 〇 20. The lens of claim 18, wherein the second curvature of the second layer is on the outer surface of the lens. The lens of claim 18, wherein the second curvature of the first layer begins at 4 mm below the mating point of the lens. Brother 130295.doc 200912425 - The second curvature of the 22. The lens of claim 18 wherein the lens optical power of the first layer has a discontinuity. a lens comprising: - a first layer having a first refractive index, wherein the first layer comprises a long distance region and a first optical element; and - having a second refractive index different from the first refractive index a second layer, wherein the second layer comprises a remote region and a second optical component, wherein the first optical component comprises an optical power region of the spherical surface, the substantially spherical optical power The first portion of the total short-range additional power of the lens is supplied to the lens, wherein the first optical component of the first layer and the optical power between the remote regions step up 'the first optical in the first layer An optical discontinuity is generated at a boundary between the component and the remote region, wherein the first optical component is located at *mm below the mating point of the lens, wherein the second optical component includes a progressive optical power region, The progressive optical power region supplies a second portion of the total near-distance additional power of the lens, and wherein the first and second optical components are in optical communication, so the total near-distance additional power of the lens A second portion of the total power close to the total power of the lens is combined to supply the total near-field additional power of the lens. 24. The lens of claim 23, wherein the first and second optical elements are aligned to form a far-intermediate distance zone and an intermediate distance zone. 130295.doc 200912425 2 5. The lens 5 of claim 2, wherein the intermediate-intermediate distance zone has an additional power between about 20% and about 44% of the total power of the total close proximity of the lens, and the intermediate The distance zone has an additional power between about 45% and about 55% of the total power of the lens. 130295.doc
TW97111800A 2007-03-29 2008-03-31 Multifocal lens having a progressive optical power region and a discontinuity TW200912425A (en)

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Families Citing this family (7)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
EP2365380A3 (en) * 2007-12-14 2012-05-02 Pixeloptics Inc. Multiple layer multifocal composite lens
US8922723B2 (en) 2010-06-30 2014-12-30 Panasonic Corporation Optical device
CN102893619A (en) 2010-06-30 2013-01-23 松下电器产业株式会社 Optical device
EP2780759B1 (en) * 2011-11-16 2016-03-02 Essilor International (Compagnie Générale D'Optique) Method for providing an optical system of an ophthalmic spectacle lens and method for manufacturing an ophthalmic spectacle lens
US9618774B2 (en) 2014-02-10 2017-04-11 Shamir Optical Industry Ltd. Quasi progressive lenses for eyewear
EP3105634A4 (en) * 2014-02-10 2017-11-29 Shamir Optical Industry Ltd Quasi progressive lenses for eyewear
DE102014004381B4 (en) * 2014-03-26 2023-08-10 Rodenstock Gmbh Improved ophthalmic lens for presbyopia correction and method of manufacture and apparatus

Family Cites Families (24)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US4576623A (en) * 1984-03-23 1986-03-18 Corning Glass Works Method for making multifocal ophthalmic lens
US4881804A (en) * 1987-11-12 1989-11-21 Cohen Allen L Multifocal phase plate with a pure refractive portion
CA1316728C (en) * 1988-04-01 1993-04-27 Michael J. Simpson Multi-focal diffractive ophthalmic lenses
JP2899296B2 (en) * 1988-11-10 1999-06-02 アレン・エル・コーエン Manufacturing method of multifocal phase plate
US5152788A (en) * 1989-12-27 1992-10-06 Minnesota Mining And Manufacturing Company Multifocal diffractive ophthalmic lens and method of manufacture
US5223862A (en) * 1991-04-08 1993-06-29 Corning Incorporated High-index, organic lens member
JPH0749471A (en) * 1993-08-06 1995-02-21 Kuraray Co Ltd Spectacles
US5861934A (en) 1996-05-06 1999-01-19 Innotech, Inc. Refractive index gradient lens
IL123574A0 (en) * 1998-03-05 1998-10-30 Holo Or Ltd Progressive multifocal lens construction for eyeglasses
IL124991A (en) * 1998-06-18 2002-12-01 Rotlex 1994 Ltd Multifocal lens combining the advantages of progressive addition lenses and diffractive lenses
US6086203A (en) 1998-09-03 2000-07-11 Johnson & Johnson Vision Care, Inc. Progressive addition lenses
AU3365200A (en) * 1999-03-16 2000-10-04 Johnson & Johnson Vision Care, Inc. Method of manufacturing spectacle lenses
FR2793038B1 (en) * 1999-04-29 2002-01-25 Essilor Int COMPOSITE OPHTHALMIC LENS AND METHOD FOR OBTAINING SUCH A LENS
US6619799B1 (en) * 1999-07-02 2003-09-16 E-Vision, Llc Optical lens system with electro-active lens having alterably different focal lengths
US6871951B2 (en) * 2000-06-23 2005-03-29 E-Vision, Llc Electro-optic lens with integrated components
US7178918B2 (en) * 2000-09-08 2007-02-20 Griffin Richard A Ophthalmic lenses with induced aperture and redundant power regions
BR0213012A (en) * 2001-10-05 2004-12-28 E Vision Llc Hybrid Electroactive Lenses
WO2003107076A1 (en) * 2002-06-14 2003-12-24 株式会社メニコン Lens for eye
US7377638B2 (en) * 2003-05-19 2008-05-27 Essilor International (Compagnie Generale D'optique) Four zone multifocal lenses
CN100472278C (en) * 2003-06-09 2009-03-25 株式会社朝日光学 Bifocal plastic lens
US6951391B2 (en) * 2003-06-16 2005-10-04 Apollo Optical Systems Llc Bifocal multiorder diffractive lenses for vision correction
US7156516B2 (en) * 2004-08-20 2007-01-02 Apollo Optical Systems Llc Diffractive lenses for vision correction
US20060066808A1 (en) * 2004-09-27 2006-03-30 Blum Ronald D Ophthalmic lenses incorporating a diffractive element
FR2884622B1 (en) * 2005-04-19 2007-08-10 Essilor Int OPHTHALMIC GLASS COMPRISING A VARIABLE REFRACTION INDEX LAYER

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