TW200807055A - Static progressive surface region in optical communication with a dynamic optic - Google Patents

Static progressive surface region in optical communication with a dynamic optic Download PDF

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Publication number
TW200807055A
TW200807055A TW096121255A TW96121255A TW200807055A TW 200807055 A TW200807055 A TW 200807055A TW 096121255 A TW096121255 A TW 096121255A TW 96121255 A TW96121255 A TW 96121255A TW 200807055 A TW200807055 A TW 200807055A
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lens
power
dynamic
optics
ophthalmic lens
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TW096121255A
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Chinese (zh)
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TWI435139B (en
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Ronald D Blum
William Kokonaski
Venkatramani S Iyer
Joshua N Haddock
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Pixeloptics Inc
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    • 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
    • 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
    • AHUMAN NECESSITIES
    • A61MEDICAL OR VETERINARY SCIENCE; HYGIENE
    • A61FFILTERS IMPLANTABLE INTO BLOOD VESSELS; PROSTHESES; DEVICES PROVIDING PATENCY TO, OR PREVENTING COLLAPSING OF, TUBULAR STRUCTURES OF THE BODY, e.g. STENTS; ORTHOPAEDIC, NURSING OR CONTRACEPTIVE DEVICES; FOMENTATION; TREATMENT OR PROTECTION OF EYES OR EARS; BANDAGES, DRESSINGS OR ABSORBENT PADS; FIRST-AID KITS
    • A61F9/00Methods or devices for treatment of the eyes; Devices for putting-in contact lenses; Devices to correct squinting; Apparatus to guide the blind; Protective devices for the eyes, carried on the body or in the hand
    • 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
    • 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
    • G02C7/068Special properties achieved by the combination of the front and back surfaces
    • 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
    • G02C7/08Auxiliary lenses; Arrangements for varying focal length
    • 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
    • G02C7/08Auxiliary lenses; Arrangements for varying focal length
    • G02C7/081Ophthalmic lenses with variable focal length
    • G02C7/083Electrooptic 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

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  • Health & Medical Sciences (AREA)
  • Ophthalmology & Optometry (AREA)
  • Physics & Mathematics (AREA)
  • General Health & Medical Sciences (AREA)
  • General Physics & Mathematics (AREA)
  • Optics & Photonics (AREA)
  • Heart & Thoracic Surgery (AREA)
  • Biomedical Technology (AREA)
  • Engineering & Computer Science (AREA)
  • Vascular Medicine (AREA)
  • Life Sciences & Earth Sciences (AREA)
  • Animal Behavior & Ethology (AREA)
  • Public Health (AREA)
  • Veterinary Medicine (AREA)
  • Eyeglasses (AREA)
  • Liquid Crystal (AREA)

Abstract

An ophthalmic lens is presented in which the lens includes a progressive addition region and a dynamic optic. The dynamic optic and the progressive addition region are in optical communication. The progressive addition region has an add power which is less than a user's near viewing distance add power. The dynamic optic, when activated, provides the additional needed optical power for the wearer to see clearly at a near distance. This combination leads to the unexpected result that not only does the wearer have the ability to see clearly at intermediate and near distances, but the level of unwanted astigmatism, distortion, and vision compromise are reduced significantly.

Description

200807055 九、發明說明: 【發明所屬之技術領域】 本發明係關於在眼睛上、眼睛内或眼睛周圍利用之多焦 點眼用透鏡、透鏡設計、透鏡系統及眼鏡產品或設備。更 具體言之,本發明係關於多焦點眼用透鏡、透鏡設計、透 鏡系統及眼鏡產品,其提供在多數情況下減小與增進透鏡 相關聯之無用失真、無用散光及視力損害至配戴者完全能 夠接受的範圍之光學效應/最終結果。 【先前技術】 老lb眼為常伴隨著衰老之人眼晶狀體之調節性的損失。 此調節性損失導致不能夠聚焦於近距離物件上。校正老花 眼之標準工具為多焦點眼用透鏡。多焦點透鏡為一種具有 一個以上焦距(亦即,光焦度)以用於在一距離範圍上校正 聚焦問題之透鏡。多焦點眼用透鏡藉由將透鏡區域分成不 同光焦度之區域而工作。通常,位於透鏡上部之相對較大 的區域校正遠距離視力誤差(若存在)。位於透鏡底部之較 小區域提供額外光焦度用於校正由老花眼所造成之近距離 視力誤差。多焦點透鏡亦可含有位於靠近透鏡中部處之較 小區域’其提供額外光焦度用於校正中距離視力誤差。 不同光焦度之區域之間的過渡可為突然的(如在雙焦點 與二焦點透鏡的情況下),或為平緩且連續的(如在增進透 鏡的情況下)。增進透鏡為一種類型之多焦點透鏡,其包 含自透鏡之遠距離觀察區開始至透鏡下部之近距離觀察區 持續增加的正屈光光焦度的梯度。光焦度之此增進大體始 121818.doc 200807055 於接近透鏡之所謂配合十字或配合點且持續增$直至在近 距離觀察區中實現全添加焦度且接著達到平穩狀態。習知 與當前技術狀態之增進透鏡在透鏡之一或兩個外表面上利 用經成形以形成光焦度之此增進之表面構形。增進透鏡在 光學工業内被稱作PAL (複數形式為PALs或單數形式為 PAL)。PAL透鏡優於傳統雙焦點與三焦點透鏡之有利之處 在於其可向使用者提供無冑、在美容上合意的多焦點透 鏡,當聚焦於遠距離之物件上至近距離之物件或當聚焦於 近距離之物件上至遠距離之物件時其具有連續的視力校 正。 雖然PAL現已在美國及遍及世界作為對老花眼之校正而 被廣泛地接受且流行,但其亦具有嚴重的視力損害。此等 損害包括(但不限於)無用散光、失真及知覺模糊。此等視 力損害可影響使用者之水平觀察寬度,其為當使用者在給 定距離聚焦時自一側至另一侧所清楚看到的視場寬度。因 此’當在中距離聚焦時,PAL透鏡可具有較窄的水平觀察 寬度’此可使觀察電腦螢幕之較大部分變得困難。類似 地,當在近距離聚焦時,PAL透鏡可具有較窄的水平觀察 寬度’此可使觀察書或報紙之完整頁面變得困難。遠距離 視力可類似地受到影響。歸因於透鏡的失真,pAL透鏡亦 可在配戴者在進行體育運動時造成困難。另外,由於光學 添加焦度置於APL透鏡底部區域’因此當配戴者觀寧在t 頭部上方位於近距離或中距離之物件時,其必須向後傾斜 其頭部來使用此區域。相反’當配戴者下樓梯且假設向下 121818.doc 200807055 看時’由透鏡提供近距離焦點,而非清楚地看到其腳盘樓 梯所必需的遠距離焦點。因&,配戴者之腳將為離焦的且 表:為模糊的。除了此等限制之外,歸因於存在於透鏡中 之每-者中之不平衡失真’許多PAL配戴者經歷被稱作視 覺運動(常被稱作"眼花")之不舒適的效應。實際上,由於 此效應,許多人拒絕佩戴該等透鏡。 旦當考慮老花眼個人之近光焦度需要時,所需近光焦度的 量與個人在其眼睛中留有的調節幅度的量(近距離聚焦能 力)直接相關。大體而t,隨著個人衰老,調節幅度的量 ,小。調節幅度亦可由於各種健康原因而減小。因此,隨 著個人衰老且變得更加老花眼,校正該人在近觀察距離 與中觀察距離聚焦的能力所需之光焦度依據所需屈光光學 添加焦度而變得更強。僅舉例而言,一個45歲的人可需要 L00屈光度之近觀察距離光焦度來在近點距離看清楚, 而一個80歲的人可需要+2·75屈光度至+3 〇〇屈光度之近觀 察距離光焦度來在同一近點距離看清楚。由於在PAL透鏡 中視力損害程度隨著屈光光學添加焦度而增加,因此一個 更高度老花眼的人將經受更大的視力損害。在上述實例 中,與80歲的人相比,45歲的人將具有與其透鏡相關聯之 更低程度之失真。顯而易見,考慮到與年老相關聯之生活 ⑽質問題(諸如虛弱或失去靈巧性),此與所需要的完全相 反。向視力功能增加損害且抑制安全性之處方多焦點透鏡 與使生活更容易、更安全且複雜性更低的透鏡截然相反。 僅舉例而言,具有+1〇〇D近光焦度之習知ΡΑ[可具有大 121818.doc 200807055 約+1.00D或更少的無用散光。然而,具有+2.50D近光焦度 之習知PAL可具有大約+2.75D或更多的無用散光,而具有 +3.25D近點光焦度之習知PAL可具有大約+3.75D或更多的 無用散光。因此,隨著PAL近距離添加焦度增加(例如與 + 1.00D PAL相比為+2.50D PAL),在該pAL内發現的無用 散光相對於近距離添加焦度以大於線性速率之速率增加。 近來,已研製雙側PAL,其具有置於透鏡每一侧上之增 進表面構形。兩個增進表面經對準且相對於彼此旋轉不僅 提供所需的適當總添加近距離添加焦度,且亦使由pal在 透鏡之一個表面上所形成之無用散光與由pal在透鏡之 另一表面上所形成之無用散光中之某些無用散光抵消。即 使此没计與傳統PAL透鏡相比略微減小給定近距離添加焦 度之無用散光與失真,上文所列出之無用散光、失真及其 他視力損害之程度仍對配戴者造成嚴重的視力問題。 因此’迫切需要提供滿足老花眼個人的虛榮需要且同時 以在進行體育運動、操作電腦及閱讀書或報紙時減小失真 與模糊、開闊水平觀察寬度、允許改良安全性且允許改良 視覺能力之方式校正其老花眼的眼鏡片及/或眼鏡系統。 【發明内容】 在本發明之一實施-例中,具有一配合點用於一使用者之 眼用透鏡可包括具有一通道之增進區域,其中該增進區域 内具有一添加焦度。眼用透鏡可進一步包括一動態光學, 其在啟動時可與具有一光焦度之增進區域進行光學傳遞。 在本發明之一實施例中,具有一配合點用於一使用者之 121818.doc 200807055 艮用透鏡可包括具有一通道之增進區域,其中該增進區域 内/、有添加焦度。眼用透鏡可進一步包括一動態光學, 其在啟動時與具有光焦度之增進區域進行光學傳遞,其中 該動態光學具有位於配合點之大約15 mm内之頂部周邊邊 緣。 【實施方式】 在本申印案中使用許多眼科、驗光及光學術語。為了清 楚起見,其定義在下文中列出: 添加焦度··添加至遠距離觀察光焦度之光焦i,其為在 多焦點透鏡中近距離看清楚所需的光焦度。舉例而言,若 個人具有-3.00D之遠距離觀察處方與+2 〇〇D近距離觀察 添加焦度,則在多焦點透鏡之近距離部分中之實際光焦度 為].00D。添加焦度有時被稱作正焦度。添加焦度可進一 步藉由被稱作”近觀察距離添加焦度"(其指在透鏡之近觀察 距離部分中之添加焦度)與"中觀察距離添加焦度”(其指在 透鏡之中觀察距離部分中之添加焦度)來進行區分。通 常,中觀察距離添加焦度為近觀察距離添加焦度之大約 50〇/。。因此,在上述實例中,個人將具有+1〇〇1)之中距離 觀察添加焦度且在多焦點透鏡之中觀察距離部分中之實際 總光焦度為-2.00D。 大約:在士 10%内(包括土10%)。因此,短語"大約1〇 mm,r 可被理解為意謂自9 mn^U mm(包括9 111111與11 mm)。 摻合區:沿透鏡周邊邊緣之光焦度過渡,藉此光焦度在 摻合區上自第一杈正焦度持續過渡至第二校正焦度或自第 121818.doc -10- 200807055 一校正焦度持續過渡至第一校正焦度。大體而言,掺合區 經設計為具有盡可能小的寬度。動態光學之周邊邊緣可包 括一摻合區以減小動態光學之可見度。利用摻合區係出於 美谷增強原因且亦為了增強視力功能性。歸因於摻合區之 南無用散光,其通常不被視作透鏡之可用部分。摻合區亦 被稱作過渡區。 通道:藉由增加正光焦度所界定之增進透鏡之區域,其 自运距離光焦度區域或區延伸至近距離光焦度區域或區。 此光焦度增進始於被稱作配合點之PAL之區域且結束於近 距離觀察區。通道有時被稱作過道。 通道長度:通道長度為自配合點至通道中添加焦度在所 指定近距離觀察焦度之大約85%内之位置所量測之距離。 通道寬度:藉由高於大約+1.00D的無用散光所限定之通 道的最窄部分。當比較PAL透鏡時,此定義可用,此歸因 於更寬的通道寬度大體與更小的失真、更佳的視覺效能、 增加的視覺舒適性及配戴者更容易的適應性相關之事實。 等值線囷:自量測與繪製增進透鏡之無用散光光焦度所 產生之曲線。等值線圖可產生有各種散光光焦度敏感性, 因此提供在何處與以何種程度增進透鏡具有無用散光作為 其光學設計之部分的視覺圖。該等圖之分析通常用於量化 PAL之通道長度、通道寬度、讀取寬度及遠距離寬产。等 值線圖亦可被稱作無用散光焦度圖。此等圖亦可用_I_ 及描繪在透鏡之各部分中的光焦度。 習知通道長度:歸因於眼鏡樣式之審美方法或趨勢,可 121818.doc • 11 · 200807055 而要具有垂直縮短的透鏡。在該透鏡中,通道自然亦較 短。1知通道長度係指非縮短PAL透鏡中通道的長度。此 等通道長度通常為(但並非總是為)大約15 mm或更長。大 體而言,較長的通道長度意謂較寬的通道寬度與較少的無 用散光。較長通道設計常與"軟”增進相關聯,因為歸因於 光焦度更緩慢地增加,遠距離校正與近距離校正之間的過 渡更軟。 動態透鏡:-種光焦度可隨著電能、機械能或力的施加 而改變之透鏡。整個透鏡可具有可變光焦度,或僅透鏡之 -部分'區域或區可具有可變的光焦度。該透鏡之光焦度 係動態的或可調整的’使得光焦度可在兩個或兩個以上光 焦度之間切換。該等光焦度中之—者可為大體上無光焦度 之光焦度。動態透鏡之實例包括電活性透鏡、凹凸透鏡、 流體透鏡、具有-或多個組件之可移動動態光學、氣體透 鏡及具有能夠變形之部件的薄膜透鏡。動態透鏡亦可被稱 作動態光學、動態光學元件、動態光學區或動態光學區 域。 遠距離參考點:位於配合十字上方大約3至4 _處之參 考點’在此處可容易地量測透鏡之遠距離處方或遠距離光 焦度。 遠距離觀察區··含有允許使用者在遠觀察距離校正地觀 看之光焦度之透鏡的部分。 遠距離寬度:透鏡之遠距離觀察部分内最窄的水平寬 度〃提供/月楚、基本上無失真之校正,且光焦度在配戴 121818.doc 12 200807055 者之遠距離觀察光焦度校正之0.25D内。 遠觀察距離:僅舉例而言,當某人超過其桌子邊緣觀察 時’開汽車時’觀看遠山或看電影時,其所看到之距離。 此距離通常(但並非總是)被視作距眼睛大約以英吋或更 多。遠觀察距離亦可被稱作遠距離與遠距離點。 配合十字/配合點:在PAL上之參考點,其表示一旦透鏡 安裝於眼鏡框内且定位於配戴者面部當配戴者透過透鏡直 視時其瞳孔之近似位置。配合十字/配合點通常(但並非總 疋)位於通道開始處垂直上方2至5 mm。配合十字通常具有 自稍微超過+0·00屈光度至大約+012屈光度之範圍的極少 量之正光焦度。此點或十字標記於透鏡表面上,使得其可 提供一簡易參考點來相對於配戴者的瞳孔進行量測及/或 復核透鏡的配合。在將透鏡分配至患者/配戴者後即容易 地移除該標記。 硬增進透鏡·在遠距離校正與近距離校正之間具有較不 緩慢的較陡峭過渡之增進透鏡。在硬PAL中,無用失真可 在配合點下方且並不向外擴展至透鏡的周邊内。硬pAL亦 可具有更短的通道長度與更窄的通道寬度。一"經修改的 硬增進透鏡”為一硬PAL,其經修改以具有有限數目的軟 PAL特徵,諸如更緩慢的光焦度過渡,更長的通道、更寬 的通道、更多的無用散光擴展至透鏡周邊内,及更少的無 用散光在配合點下方。 .中距離觀察區:含有允許使用者在中觀察距離校正地觀 看之光焦度之透鏡的部分。 1218IS.doc -13· 200807055 中觀察距離··僅舉例而言,當某人閱讀報紙時,操作電 腦時’在水槽中刷盤子時,或熨燙衣服時,其所看到的距 離。此距離通常(但並非總是)被視作在距眼睛大約16英吋 與大約32英吋之間。中觀察距離亦可被稱作中距離與中距 離點。 透鏡:使光會聚或發散的任何設備或設備的部分。該設 備可為靜態的或動態的。透鏡可為折射的或繞射的。透鏡 可在一個表面或兩個表面上為凹面、凸面或平的。透鏡可 為球形、圓柱形、稜形或其組合。透鏡可由光學玻璃、塑 料或樹脂製成。透鏡亦可被稱作光學元件、光學區、光學 區域、光焦度區域或光學。應指出的是,在光學工業内, 一透鏡即使具有零光焦度,其亦可被稱作透鏡。 透鏡毛坯:由可成形為透鏡的光學材料製成之設備。透 鏡毛述可被修整意谓透鏡毛链經成形以在兩個外表面上具 有光焦度。透鏡毛坯可被半修整意謂透鏡毛坯經成形以在 僅一個外表面上具有光焦度。透鏡毛坯可不被修整意謂透 鏡毛坯可不成形為在任一外表面上具有光焦度。未被修整 或半修整透鏡毛坯的表面可藉由被稱作自由成形的製造方 法或藉由更傳統的表面加工與研磨來進行修整。 低添加焦度PAL · —種具有小於配戴者在近距離看清楚 所必而之近添加焦度之近添加焦度的增進透鏡。 多焦點透鏡:一種具有一個以上焦點i光焦I的透鏡。 該等透鏡可為靜態的或動態的。靜態多焦點透鏡之實例包 括雙焦點透鏡、三焦點透鏡或增進透鏡。動態多焦點透鏡 121818.doc -14- 200807055 的實例包括電活性透鏡,藉此各種光焦度可視所用電極類 型、施加至電極之電壓及在液晶薄層内改變的折射率而在 透鏡中形成。多焦點透鏡亦可為靜態與動態之組合。舉例 而言,電活性元件可用於與靜態球形透鏡、靜態單光透 鏡、靜態多焦點透鏡(諸如,僅舉例而言,增進透鏡)進行 光學傳遞。在大多數情況下(但非所有情況下),多焦點透 鏡為折射透鏡。200807055 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 that are utilized on, in or around the eye. More particularly, the present invention relates to multifocal ophthalmic lenses, lens designs, lens systems, and eyewear products that provide for reducing, in most cases, unwanted distortion associated with enhanced lenses, unwanted astigmatism, and visual impairment to the wearer. A fully acceptable range of optical effects / end results. [Prior Art] The old lb eye is often accompanied by the modulating loss of the lens of the aging person. This accommodative loss results in the inability to focus on close objects. The standard tool for correcting presbyopia is a multifocal ophthalmic lens. A multifocal lens is a lens that has more than one focal length (i.e., power) for correcting focus problems over a range of distances. Multifocal ophthalmic lenses work by dividing the lens area into regions of different power. Typically, a relatively large area located above the lens corrects for remote vision errors, if any. The smaller area at the bottom of the lens provides additional power for correcting near vision errors caused by presbyopia. The multifocal lens may also contain a smaller area located near the middle of the lens, which provides additional power for correcting the mid-range vision error. The transition between regions of different powers can be abrupt (as in the case of bifocal and bifocal lenses), or gentle and continuous (as in the case of enhanced lenses). The enhanced lens is a type of multifocal lens that includes a gradient of positive refractive power that continues to increase from the distance viewing zone of the lens to the close viewing zone of the lower portion of the lens. This increase in power generally begins with the so-called mating cross or mating point of the lens and continues to increase until the full add power is achieved in the close viewing zone and then reaches a plateau. Conventional and current state of the art lenses utilize shaped surfaces formed on one or both of the lenses to form the enhanced power of the power. Promotional lenses are referred to as PAL in the optical industry (plural form is PALs or singular form is PAL). PAL lenses are superior to conventional bifocal and trifocal lenses in that they provide a flawless, cosmetically pleasing multifocal lens to the user when focusing on objects at a distance to close objects or when focusing on It has continuous vision correction when the object is close to the object at a distance. Although PAL is now widely accepted and popular in the United States and throughout the world as a correction for presbyopia, it also has severe visual impairment. Such damage includes, but is not limited to, unwanted astigmatism, distortion, and perceptual blurring. Such visual impairment can affect the horizontal viewing width of the user, which is the field of view width that is clearly seen from side to side when the user is focusing at a given distance. Therefore, when focusing at a medium distance, the PAL lens can have a narrower horizontal viewing width' which makes it difficult to observe a larger portion of the computer screen. Similarly, a PAL lens can have a narrower horizontal viewing width when focusing at close distances. This can make it difficult to view a complete page of a book or newspaper. Long-distance vision can be similarly affected. Due to the distortion of the lens, the pAL lens can also cause difficulties for the wearer while performing sports. In addition, since the optical add power is placed in the bottom area of the APL lens, when the wearer is looking at a close or intermediate distance object above the t head, it must tilt its head backward to use this area. Conversely, 'when the wearer goes down the stairs and assumes downwards, the lens provides a close focus, rather than clearly seeing the long-distance focus necessary for its foot ladder. Because of &, the wearer's feet will be out of focus and the table: blurred. In addition to these limitations, due to the unbalanced distortions that exist in each of the lenses' many PAL wearers experience an uncomfortable experience called visual motion (often referred to as "eyes") effect. In fact, many people refuse to wear these lenses due to this effect. When considering the near-power requirement of presbyopia, the amount of near-power required is directly related to the amount of adjustment (close-range focus) that the individual has in his or her eye. In general, t, as the individual ages, the amount of adjustment is small. The magnitude of the adjustment can also be reduced for various health reasons. Thus, as the individual ages and becomes more presbytic, the power required to correct the person's ability to focus at near and intermediate viewing distances becomes stronger depending on the desired refractive optical add power. For example only, a 45-year-old person may need a near-observation distance power of L00 diopter to see at a near-point distance, while an 80-year-old person may need +2·75 diopters to +3 〇〇 diopters. Observe the distance power to see clearly at the same near point. Since the degree of visual impairment in the PAL lens increases with the refractive power of the refractive optics, a person with a higher degree of presbyopia will experience greater visual impairment. In the above example, a 45 year old would have a lower degree of distortion associated with their lens than a 80 year old. Obviously, considering the life associated with old age (10) quality issues (such as weakness or loss of dexterity), this is exactly the opposite of what is needed. A multifocal lens that adds damage to the vision function and suppresses safety is the opposite of a lens that makes life easier, safer, and less complex. By way of example only, conventional 具有 having a +1 〇〇 D near power [can have a large opaque astigmatism of about 121818.doc 200807055 or about +1.00D or less. However, conventional PALs with +2.50D near-power can have unwanted astigmatism of about +2.75D or more, while conventional PALs with +3.25D near-point power can have about +3.75D or more. Useless astigmatism. Thus, as the PAL gains an increase in close proximity (e.g., +2.50 D PAL compared to + 1.00 D PAL), the unwanted astigmatism found within the pAL increases at a rate greater than the linear rate relative to the close distance. Recently, two-sided PALs have been developed which have an enhanced surface configuration placed on each side of the lens. The two enhanced surfaces are aligned and rotated relative to each other not only provides the appropriate total added close-in addition power required, but also the unwanted astigmatism formed by pal on one surface of the lens and the other by the pal in the lens Some of the unwanted astigmatism formed on the surface is offset by some unwanted astigmatism. Even if this does not reduce the useless astigmatism and distortion of a given close-range add power compared to a conventional PAL lens, the degree of unwanted astigmatism, distortion, and other visual impairments listed above is still severe for the wearer. Vision problems. Therefore, there is an urgent need to provide a vanity need to satisfy the presbyopia and at the same time to correct distortions and blurring while exercising, operating computers and reading books or newspapers, widening the viewing width, allowing improved safety and allowing improved visual ability. Its presbyopic spectacle lenses and / or glasses system. SUMMARY OF THE INVENTION In one embodiment of the invention, an ophthalmic lens having a mating point for a user can include a promotional region having a channel, wherein the enhancing region has an added power. The ophthalmic lens can further include a dynamic optics that can be optically transmitted with an enhanced area having a power at startup. In one embodiment of the invention, a mating point is provided for a user. 121818.doc 200807055 The lens can include a raised area having a channel, wherein the boosting area has/with added power. The ophthalmic lens can further include a dynamic optics that optically transmits upon activation with a region of enhanced power having a top peripheral edge within about 15 mm of the mating point. [Embodiment] Many ophthalmology, optometry and optical terms are used in this application. For the sake of clarity, the definitions are listed below: Adding the power added to the optical power i of the far-sighted power, which is the power required to see at a close distance in the multifocal lens. For example, if an individual has a long-range observation prescription of -3.00D and a close-up observation of +2 〇〇D, the actual power in the close-range portion of the multifocal lens is .00D. Adding power is sometimes referred to as positive power. The addition of power can be further referred to by the "close-to-view distance plus power" (which refers to the added power in the near-observation distance portion of the lens) and the "in-view distance plus the power" (which refers to the lens) The degree of addition in the distance portion is observed to distinguish. Typically, the medium viewing distance add power is approximately 50 〇/ of the near observation distance. . Therefore, in the above example, the individual will have a distance of +1 〇〇 1) to observe the add power and the actual total power in the distance portion observed in the multifocal lens is -2.00D. Approx.: Within 10% of the staff (including 10% of the soil). Therefore, the phrase "about 1 〇 mm, r can be understood to mean from 9 mn^U mm (including 9 111111 and 11 mm). Blending zone: a power conversion along the peripheral edge of the lens, whereby the power is continuously transitioned from the first positive power to the second corrected power on the blending zone or from 121818.doc -10- 200807055 The corrected power continues to transition to the first corrected power. In general, the blending zone is designed to have as small a width as possible. The peripheral edge of the dynamic optics can include a blending zone to reduce the visibility of dynamic optics. The use of blending zones is due to the enhancement of the US Valley and also to enhance visual function. Due to the southern unwanted astigmatism of the blending zone, it is generally not considered a usable part of the lens. The blending zone is also referred to as the transition zone. Channel: A region of the enhanced lens defined by increasing the positive power, the self-traveling power range or region extending to the close power region or region. This power enhancement begins at the area of the PAL referred to as the mating point and ends at the close viewing area. Channels are sometimes referred to as aisles. Channel length: The channel length is the distance measured from the mating point to the position where the added power in the channel is within approximately 85% of the specified close-range viewing power. Channel Width: The narrowest portion of the channel defined by unwanted astigmatism above about +1.00D. This definition is available when comparing PAL lenses due to the fact that wider channel widths are generally associated with less distortion, better visual performance, increased visual comfort, and easier adaptability of the wearer. Contours: Self-measurement and plotting the curves produced by the unwanted astigmatic power of the lens. Contour maps can produce a variety of astigmatic power sensitivities, thus providing a visual map of where and to what extent the lens has unwanted astigmatism as part of its optical design. The analysis of these figures is typically used to quantify PAL channel length, channel width, read width, and wide range yield. The contour map can also be referred to as a astigmatic astigmatism map. These figures can also use _I_ and the power drawn in the various parts of the lens. Conventional channel length: An aesthetic approach or trend due to the style of the eyewear. 121818.doc • 11 · 200807055 A lens with a vertical shortening is required. In this lens, the passage is naturally shorter. 1 Knowing the channel length refers to the length of the channel in the non-shortened PAL lens. These channel lengths are usually (but not always) about 15 mm or longer. In general, a longer channel length means a wider channel width and less unwanted astigmatism. Longer channel designs are often associated with "soft" enhancements because the transition between distance correction and close distance correction is softer due to the slower increase in power. Dynamic lens: - Spectral power can be used A lens that changes with the application of electrical energy, mechanical energy, or force. The entire lens may have a variable power, or only a portion-area or region of the lens may have a variable power. The power of the lens is Dynamic or adjustable 'allows the power to be switched between two or more powers. Among these powers, the power can be substantially absorptive. Dynamic lens Examples include electroactive lenses, meniscus lenses, fluid lenses, movable dynamic optics with or without multiple components, gas lenses, and thin film lenses with deformable components. Dynamic lenses may also be referred to as dynamic optics, dynamic optics. , dynamic optics zone or dynamic optics zone. Remote reference point: a reference point located approximately 3 to 4 _ above the mating cross. Here, the far-distance prescription or long-range power of the lens can be easily measured. The area containing the lens that allows the user to view the power of the power at a distance from the distance. The long-distance width: the narrowest horizontal width in the long-distance observation portion of the lens 〃 provides / month, basically no distortion Correction, and the power is within 0.25D of the long-distance viewing power correction of 121818.doc 12 200807055. Far viewing distance: For example, when someone exceeds the edge of their table to observe 'drive the car When you watch a distant mountain or watch a movie, the distance it sees. This distance is usually (but not always) considered to be about mile or more from the eye. The far viewing distance can also be called far and far. Distance point. Matching cross/fit point: A reference point on the PAL that indicates the approximate position of the pupil when the lens is mounted in the eyeglass frame and positioned on the wearer's face when the wearer looks through the lens. The points are usually (but not always) 2 to 5 mm vertically above the beginning of the channel. The mating cross typically has a very small amount of positive power ranging from slightly above +0·00 diopters to about +012 diopters. This point or cross is marked on the surface of the lens such that it provides a simple reference point for measuring and/or recombining the lens relative to the wearer's pupil. It is easy to assign the lens to the patient/wearer. Ground removal of the mark. Hard enhancement lens · A slower, steeper transition between the distance correction and the close distance correction. In hard PAL, unwanted distortion can be below the fit point and not scale out Within the perimeter of the lens, the hard pAL can also have a shorter channel length and a narrower channel width. A "modified hard enhancement lens" is a hard PAL modified to have a finite number of soft PAL features, Such as slower power transitions, longer channels, wider channels, more unwanted astigmatism extending into the perimeter of the lens, and less unwanted astigmatism below the fit point. Medium distance observation zone: A portion containing a lens that allows the user to observe the distance of the power of the viewing angle. 1218IS.doc -13· 200807055 Observed distance··For example only, when someone reads a newspaper, when they operate the computer, when they brush the dishes in the sink, or when they iron the clothes, they see the distance. This distance is usually (but not always) considered to be between about 16 inches and about 32 inches from the eye. The medium viewing distance can also be referred to as the medium distance and the medium distance. Lens: Any part of a device or device that converges or diverges light. The device can be static or dynamic. The lens can be refracting or diffractive. The lens may be concave, convex or flat on one or both surfaces. The lens can be spherical, cylindrical, prismatic or a combination thereof. The lens can be made of optical glass, plastic or resin. A lens can also be referred to as an optical element, an optical zone, an optical zone, a power zone, or an optics. It should be noted that in the optical industry, a lens can be referred to as a lens even if it has zero power. Lens blank: A device made of an optical material that can be shaped into a lens. The lens can be trimmed to mean that the lens strands are shaped to have power on both outer surfaces. The fact that the lens blank can be half-finished means that the lens blank is shaped to have power on only one outer surface. The fact that the lens blank may not be trimmed means that the lens blank may not be shaped to have power on either outer surface. The surface of the unfinished or semi-trimmed lens blank can be trimmed by a process known as freeform or by more conventional surface processing and grinding. Low add power PAL - A type of enhanced lens with a near add power that is less than the wearer's near-added power at close range. Multifocal lens: A lens having more than one focus i-focus I. The lenses can be static or dynamic. Examples of static multifocal lenses include bifocal lenses, trifocal lenses, or promotional lenses. Examples of dynamic multifocal lenses 121818.doc -14-200807055 include electroactive lenses whereby various optical powers are formed in the lens depending on the type of electrode used, the voltage applied to the electrodes, and the refractive index that changes within the thin layer of liquid crystal. Multifocal lenses can also be a combination of static and dynamic. For example, an electroactive element can be used for optical transmission with a static spherical lens, a static single light lens, a static multifocal lens such as, for example, a promotional lens. In most cases (but not all cases), the multifocal lens is a refractive lens.

近距離觀察區:含有允許使用者在近觀察距離校正地觀 看之光焦度之透鏡的部分。 近觀察距離:僅舉例而言,當某人讀書時,穿針時,或 閱凟藥瓶上的說明時,其所看到的距離。此距離通常(但 並非總是)被視作在距眼睛大約12英吋與大約16英忖之 間。近觀察距離亦可被稱作近距離與近距離點。 辦公用透鏡/辦公用pal ·· —種特殊設計的增進透鏡, 其提供在配合十字上方的中距離視力,更寬的通道寬度以 及更寬的讀取寬度。此藉由一種光學設計而實現,該設計 在配合十字上方擴展無用散光且其利用主要為中距離視力 區之視力區更換遠距離視力區。由於此等特徵,此種類型 的PAL特別適於科室工作,但由於透鏡並不含有遠距離觀 察區,因此配戴者不能在開車或在辦公室或家周圍散步時 使用此種類型的PAL。 眼用透鏡:一種適用於視力校正的讀於 、仅此的迓鏡,其包括眼鏡 片、隱形眼鏡、人工晶狀體、角膜嵌體及角膜覆體。 光學傳遞:以一方式對準給定光隹辩 4卞口心71□焦度之兩個或兩個以上 121818.doc -】5- 200807055 的光學使得穿過所對準光學的光經歷等於個別元件之光焦 度總和的組合光焦度的情況。 囷案化電極:在電活性透鏡中利用的電極,其使得藉由 向電極施加適當電壓,由液晶所形成的光焦度繞射地形 • 成,而與電極的大小、形狀與配置無關。舉例而言,可藉 由使用同心環形電極在液晶内動態地產生繞射光學效應。 像素化電極:在電活性透鏡中利用之電極,其可與電極 的大小、形狀及配置無關地個別定址。此外,由於電極可 _ 個別定址,因此可向電極施加任何隨意模式的電壓。舉例 而言,像素化電極可為在笛卡兒陣列中排列的正方形或矩 形或在六邊形陣列中排列的六邊形。像素化電極無需為符 合格栅的規則形狀。舉例而言,若每一環可個別定址,則 像素化電極可為同心環。同心像素化電極可經個別定址以 形成繞射光學效應。 增進區域:一個透鏡區域,其在該區域的第一部分中具 鲁 有第一光焦度且在該區域的第二部分中具有第二光焦度, 其中第一部分與第二部分之間存在連續的光焦度變化。舉 例而言’透鏡的一區域可在該區域的一端具有遠觀察距離 • 光焦度。該光焦度可在該區域上以正焦度持續增加至中觀 察距離光焦度且接者至該區域之相對端的近觀察距離光焦 度。在光焦度到達近觀察距離光焦度之後,光焦度可以使 得此增進區域之光焦度過渡回遠觀察距離光焦度内的方式 減小。增進區域可在透鏡的表面上或嵌於透鏡内。當增進 區域在表面上且包含一表面構形時,其被稱作增進表面。 121818.doc -16 - 200807055 讀取寬度:透鏡之近距離觀察部分内最窄的水平寬度, 其提供清楚基本上無失真之校正’且光焦度在配戴者近距 離觀察光焦度校正之0.25D内。 短通道長度:歸因於眼鏡樣式之審美關係或趨勢,可需 要具有垂直縮短的透鏡。在該透鏡中,通道自然亦較短。 短通道長度係指縮短的PAL透鏡中通道的長度。此等通道 長度通常(但並非總是)在大約11 mm與大約15 mm之間。大 體而言,較短的通道長度意謂較窄的通道寬度與較多的無 _ 用散光。較短通道設計常與"硬n增進相關聯,因為歸因於 光焦度更陡峭地增加,遠距離校正與近距離校正之間的過 渡更硬。 軟增進透鏡:在遠距離校正與近距離校正之間具有更緩 慢的過渡的增進透鏡。在軟PAL中,無用失真可在配合點 上方並向外擴展到透鏡的周邊内。軟PAL亦可具有更長的 通道長度與更寬的通道寬度。一 ’’經修改的軟增進透鏡,,為 一軟PAL,其經修改以具有有限數目的硬PAL特徵,諸如 ® 更陡峭的光焦度過渡,更短的通道、更窄的通道、更多無 用散光推進至透鏡觀察部分内,及更多的無用散光在配合 點下方。 靜態透鏡:一種具有不可隨著電能、機械能或力的施加 而改變之光焦度之透鏡。靜態透鏡的實例包括球形透鏡、 圓柱形透鏡,增進透鏡、雙焦點透鏡及三焦點透鏡。靜態 透鏡亦可被稱作固定透鏡。 無用散光:增進透鏡内發現的無用的像差、失真或散 121818.doc •17· 200807055 光’其不為患者指定視力校正之部分,而是P AL的光學設 計中固有的,此歸因於觀察區之間光焦度的平緩梯度。雖 然透鏡可在各種屈光度透鏡的不同區域上具有無用散光, 但透鏡中之無用散光大體上指代發現於透鏡中之最大無用 散光。無用散光亦可指代位於透鏡的特定部分(與整個透 鏡相對)内的無用散光。在此情況下,使用量化語言來表 示僅考慮在透鏡的特定部分内的無用散光。 當描述動態透鏡時,本發明涵蓋(僅舉例而言)電活性透 鏡、流體透鏡、氣體透鏡、薄膜透鏡及可機械移動透鏡 專。該等透鏡之實例可發現於Blum等人之美國專利第 6,517,2035虎、弟 6,491,394號、第 6,619,799號,Epstein與 Kiirtin的美國專利第7,008,054號、第6,040,947號、第 5,668,620 號、第 5,999,328 號、第 5,956,183 號、第 6,893,124號,Silver的美國專利第4,890,903號、第 6,〇69,742 號、第 7,085,065 號、第 6,188,525 號、第 6,618,208號,Stoner的美國專利第 5,182,585 號及 Quaglia 的 美國專利第5,229,885號。 在光學工業中熟知且接受的是,只要透鏡的無用散光與 失真在大約1.00D或更小,則透鏡的使用者(在大多數情況 下)很難對其有所覺察。本文所揭示之本發明係關於光學 設計、透鏡及眼鏡系統的實施例,其解決許多(若非大多 數)與P AL相關聯的問題。另外,本文所揭示的本發明顯著 地排除與PAL相關聯的大多數視力損害。本發明提供一種 達成配戴者之適當遠、中及近距離光焦度的構件,同時提 121818.doc -18- 200807055 供各種距離之連續聚焦能力,類似於PAL之聚焦能力。但 對於諸如+3.00D、+3.25D及+3_5〇D之特定高添加焦度處 方,本發明同時保持無用散光為最大值大約l 5〇D。然 而,在多數情況下,本發明保持無用散光為最大值大約 1.00D或更小。 本發明係基於使低添加焦度PAL與動態透鏡對準使得動 態透鏡與低添加焦度PAL進行光學傳遞,藉此動態透鏡向 配戴者提供在近距離看清楚額外需要的光焦度。此組合產 生意想不到的結果:不僅配戴者能夠在中距離與近距離看 /月楚,而且無用散光、失真及視力損害的程度被顯著降 低。 動態透鏡可為電活性元件。在電活性透鏡中,電活性光 學嵌於光學基板之表面内或可附著至其。光學基板可為一 經修整的、半修整的或未修整的透鏡毛坯。當使用半修整 或未修整的毛坯時,透鏡毛坯可在將透鏡製造為具有一或 夕個光焦度期間被修整。電活性光學亦可嵌於習知光學透 鏡之表面内或附著至其。習知光學透鏡可為單焦點透鏡或 多焦點透鏡,諸如增進透鏡或雙焦點或三焦點透鏡。電活 性光學可位於電活性透鏡的整個觀察區域中或在其僅一部 为中。電活性光學可與光學基板的周邊邊緣間隔以將電活 性透鏡磨邊為眼鏡。電活性元件可位於靠近透鏡的頂部、 中部或底部處。當大體上不施加電壓時,電活性光學可處 於禁用狀態,其中其大體上不提供光焦度。換言之,當大 體上不施加電壓時,電活性光學可具有與其中其被嵌入或 121818.doc -19- 200807055 附著的光學基板或習知透鏡大體 ^ ^ 八殿上相同的折射率。當施加 電壓時,電活性光學可處於其提供 他 攸伢九學添加焦度的啟動狀 悲。換言之,當施加電廢時’電活性光學可且有録中立 被歲入或附著的光學基板或習知透鏡不同的折射率。 電活性透鏡可用於校正眼睛的習知或非習知誤差。可藉 由電活性元件、光學基板或習知光學透鏡或藉由兩者之組 合形成此校正。眼睛的f知誤差包括低階像差,諸如近 視、、遠視、老花眼及散光。眼睛的非f知誤差包括較高階 像差,其可由眼睛層不規則性造成。 —液晶可用作電活性光學的—部分,因為液晶的折射率可 藉由在液晶上產生電場而改變。可藉由向位於液晶兩側上 的電極施加一或多個電壓來產生該電場。電極可為大體上 透月的且由大體上透明導電材料(諸如氧化銦錫(叮〇)或在 此項技術中熟知的其他該等材料)製造。基於液晶之電活 性光學可尤其適料電活性光學的一部|,因&液晶可提 供所需範圍的折射率變化以提供平的至+3 〇〇D的光學添加 焦度。此光學添加焦度範圍可能能夠校正多數患者之老花 眼。 液晶薄層(小於10 μπι)可用於建構電活性光學。該液晶 薄層可夾於兩個透明基板之間。兩個基板亦可沿其周邊邊 緣密封,使得以大體上氣密的方式在基板内密封液晶。透 明導電材料層可沈積於兩個基本上平坦的透明基板的内表 面上。導電材料可接著用作電極。當採用薄層時,電極的 形狀與大小可用於在透鏡内誘發特定光學效應。待施加至 121818.doc •20- 200807055 液晶之該等薄層之此等電極 極之所需刼作電壓可為 的,通常小於5伏。電極可被 〜目田低 π j破圖案化。舉例而言, 使用在該等基板中之至少_者 曰 可上况積的同心環形電極來在 ,晶内動態地產生繞射光學效應。該光學效應可基於環半 徑、核寬度及分別施加至不同環的電屢範圍而產生光學添 加焦度。電極可被像素化。舉例而言,像素化電極可為在 笛卡兒陣列中排列的正方形或矩形或在六邊形陣列中排列 的六邊形。該像素化電極陣列Close-range viewing area: A portion containing a lens that allows the user to view the power of the power at a near viewing distance. Near viewing distance: For example, when someone is reading a book, when they are wearing a needle, or when reading the instructions on the vial, the distance they see. This distance is usually (but not always) considered to be between about 12 inches and about 16 inches from the eye. The near viewing distance can also be referred to as a close distance and a close distance point. Office lens/office pal · A specially designed promotional lens that provides mid-range vision above the cross, wider channel width, and wider read width. This is achieved by an optical design that expands unwanted astigmatism above the mating cross and that replaces the far vision zone with a field of vision that is primarily a mid-range vision zone. Due to these characteristics, this type of PAL is particularly suitable for departmental work, but since the lens does not contain a remote viewing area, the wearer cannot use this type of PAL while driving or walking around the office or home. Ophthalmic lens: A type of frogscope that is suitable for vision correction, including spectacle lenses, contact lenses, intraocular lenses, corneal inlays, and keratoplasts. Optical transmission: aligning a given light with a method of 卞 卞 卞 卞 71 71 71 71 71 71 818 818 818 818 818 818 818 818 818 818 818 818 818 818 818 818 818 818 818 818 818 818 818 818 818 818 818 818 818 818 818 818 818 The case of the combined power of the sum of the powers. A pad electrode: an electrode utilized in an electroactive lens that allows the refractive power formed by the liquid crystal to be diffracted by applying an appropriate voltage to the electrode regardless of the size, shape, and configuration of the electrode. For example, a diffractive optical effect can be dynamically generated within a liquid crystal by using a concentric ring electrode. Pixelated electrode: An electrode utilized in an electroactive lens that can be individually addressed regardless of the size, shape, and configuration of the electrodes. Furthermore, since the electrodes can be individually addressed, any random mode voltage can be applied to the electrodes. For example, the pixelated electrodes can be squares or rectangles arranged in a Cartesian array or hexagons arranged in a hexagonal array. The pixelated electrodes need not be in a regular shape that conforms to the grid. For example, if each ring is individually addressable, the pixelated electrodes can be concentric rings. The concentric pixelated electrodes can be individually addressed to form a diffractive optical effect. Enhancement region: a lens region having a first power in a first portion of the region and a second power in a second portion of the region, wherein there is a continuity between the first portion and the second portion The power of the power changes. For example, a region of the lens may have a far viewing distance at one end of the region. The power can be continuously increased in positive power on the area to a medium viewing distance power and a near viewing distance power to the opposite end of the area. After the power reaches the near-observation distance power, the power can be reduced in such a way that the power of the enhanced region transitions back into the far-view distance. The enhancement zone can be on the surface of the lens or embedded in the lens. When the enhancement zone is on the surface and contains a surface configuration, it is referred to as a promotional surface. 121818.doc -16 - 200807055 Read Width: The narrowest horizontal width in the close-up portion of the lens, which provides a clear, virtually distortion-free correction' and the power is corrected by the wearer at close range. Within 0.25D. Short channel length: Due to the aesthetic relationship or trend of the style of the glasses, a lens with a vertical shortening may be required. In this lens, the passage is naturally shorter. The short channel length refers to the length of the channel in the shortened PAL lens. These channel lengths are usually (but not always) between about 11 mm and about 15 mm. In general, a shorter channel length means a narrower channel width and more astigmatism. Shorter channel designs are often associated with "hard n enhancements because the transition between remote and close correction is harder due to a steeper increase in power. Soft enhancement lens: A progressive lens with a slower transition between long range correction and close distance correction. In soft PAL, unwanted distortion can be spread over the mating point and outward into the perimeter of the lens. Soft PALs can also have longer channel lengths and wider channel widths. A ''modified soft enhancement lens, a soft PAL modified to have a finite number of hard PAL features, such as ® steeper power transitions, shorter channels, narrower channels, more The unwanted astigmatism advances into the lens viewing portion, and more unwanted astigmatism is below the mating point. Static lens: A lens that has a power that cannot be changed with the application of electrical energy, mechanical energy, or force. Examples of static lenses include spherical lenses, cylindrical lenses, promotional lenses, bifocal lenses, and trifocal lenses. Static lenses can also be referred to as fixed lenses. Useless astigmatism: Improves the useless aberrations, distortions, or distractions found in the lens. 121818.doc •17· 200807055 Light 'It does not specify the part of the vision correction for the patient, but is inherent in the optical design of the P AL, due to A gentle gradient of power between the observation zones. Although the lens can have unwanted astigmatism over different regions of the various diopter lenses, the unwanted astigmatism in the lens generally refers to the largest unwanted astigmatism found in the lens. Useless astigmatism can also refer to unwanted astigmatism located in a particular portion of the lens (as opposed to the entire lens). In this case, a quantization language is used to indicate that only unwanted astigmatism within a particular portion of the lens is considered. When describing dynamic lenses, the present invention encompasses, by way of example only, electroactive lenses, fluid lenses, gas lenses, film lenses, and mechanically movable lenses. Examples of such lenses can be found in U.S. Patent Nos. 6,517, 2035 to Blum et al., U.S. Patent Nos. 6,491,394, 6,619,799, Epstein and Kiirtin, U.S. Patent Nos. 7,008,054, 6,040,947, 5,668,620, 5,999,328. No. 5,956,183, 6,893,124, U.S. Patent Nos. 4,890,903, 6, 6, 69,742, 7,085,065, 6,188,525, 6, 618, 208, Stoner, U.S. Patent No. 5, U.S. Patent No. 5,229,885 to Qua. It is well known and accepted in the optical industry that the user of the lens (in most cases) is difficult to perceive as long as the unwanted astigmatism and distortion of the lens is at about 1.00 D or less. 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 P AL. Additionally, the invention disclosed herein significantly excludes most of the visual impairment associated with PAL. The present invention provides a means for achieving the appropriate far, medium and close power of the wearer, while providing a continuous focusing capability for various distances, similar to the focusing power of PAL, 121818.doc -18-200807055. However, for certain high add powers such as +3.00D, +3.25D, and +3_5〇D, the present invention simultaneously maintains unwanted astigmatism to a maximum of about 15 〇D. However, in most cases, the present invention maintains unwanted astigmatism to a maximum of about 1.00 D or less. The present invention is based on aligning the low add power PAL with the dynamic lens such that the dynamic lens is optically transmitted with the low add power PAL, whereby the dynamic lens provides the wearer with a clear view of the additional required power at close range. This combination produces unexpected results: not only can the wearer see the mid-range and close-up, but the degree of unwanted astigmatism, distortion, and visual impairment is significantly reduced. The dynamic lens can be an electroactive element. In an electroactive lens, electroactive light is embedded in or attached to the surface of the optical substrate. The optical substrate can be a trimmed, semi-trimmed or unfinished lens blank. When a semi-trimmed or untrimmed blank is used, the lens blank can be trimmed during the manufacture of the lens to have one or a single power. Electroactive optics can also be embedded in or attached to the surface of conventional optical lenses. Conventional optical lenses can be single focus lenses or multifocal lenses, such as promotional lenses or bifocal or trifocal lenses. The electroactive optics can be located throughout the viewing area of the electroactive lens or in only one of it. Electroactive optics can be spaced from the peripheral edge of the optical substrate to educe the electroactive lens into spectacles. The electroactive element can be located near the top, middle or bottom of the lens. When substantially no voltage is applied, the electroactive optics can be in a disabled state, wherein it generally does not provide power. In other words, when substantially no voltage is applied, the electroactive optics can have the same refractive index as the optical substrate or the conventional lens in which it is embedded or attached to 121818.doc -19-200807055. When a voltage is applied, the electroactive optics can be in a state of turbulence that provides him with the added power of the nine. In other words, when electrical waste is applied, the electroactive optics can have a refractive index that is different from that of an optical substrate or a conventional lens that is aged or attached. Electroactive lenses can be used to correct for conventional or non-conventional errors in the eye. This correction can be formed by an electroactive element, an optical substrate or a conventional optical lens or by a combination of the two. Eye misunderstandings include low-order aberrations such as myopia, hyperopia, presbyopia, and astigmatism. Non-fognitive errors in the eye include higher order aberrations, which can be caused by eye layer irregularities. - Liquid crystal can be used as part of electroactive optics because the refractive index of liquid crystal can be changed by generating an electric field on the liquid crystal. The electric field can be generated by applying one or more voltages to electrodes located on both sides of the liquid crystal. The electrodes can be substantially moon-permeable and fabricated from a substantially transparent conductive material such as indium tin oxide (iridium tin oxide) or other such materials well known in the art. Liquid-based electro-optical optics can be especially suitable for electroactive optics. The & liquid crystal provides a range of refractive index changes to provide an optical add power of flat to +3 〇〇D. This optical add power range may be able to correct the presbyopia of most patients. A thin layer of liquid crystal (less than 10 μm) can be used to construct electroactive optics. The liquid crystal layer can be sandwiched between two transparent substrates. The two substrates may also be sealed along their peripheral edges to seal the liquid crystal within the substrate in a substantially airtight manner. A layer of transparent conductive material can be deposited on the inner surface of two substantially planar transparent substrates. A conductive material can then be used as the electrode. When a thin layer is employed, the shape and size of the electrodes can be used to induce specific optical effects within the lens. The required operating voltage of these electrodes to be applied to the 121818.doc • 20-200807055 liquid crystal layer may be, typically less than 5 volts. The electrode can be patterned by ~ 目田低 π j broken. For example, a diffractive ring effect can be dynamically generated within the crystal using concentric ring electrodes at least in the substrate. The optical effect can be optically additive based on the ring radius, the core width, and the electrical range applied to the different rings, respectively. The electrodes can be pixelated. For example, the pixelated electrodes can be squares or rectangles arranged in a Cartesian array or hexagons arranged in a hexagonal array. The pixelated electrode array

〜』用於猎由椟仿繞射同心環 電極結構來產生光學添加焦度。 彳豕京化電極亦可用於以類 似於用於校正基於地面之天文學中大氣亂流的方式來校正 眼睛的較高階像差。 當前製造方法限制最小像素大小,且同樣限制最大動離 電活性光學直徑。僅舉例而厂當使用形成繞射圖案之;; 心像素化方法時,最大動態電活性光學直徑經估計對於 + 1.50D為20 mm,對於+ 1.25D為24 _,且對於+ ι _為 30 mm。當使用像素化繞射方法時,當前製造方法限制最 大動態電活性光學直徑。同#,本發明的實施例可具有動 態電活性光學,其在較大的直徑處具有較小光焦度。 或者,電活性光學包含兩個透明基板與一液晶層,其中 第一基板基本上為平坦的且塗佈有透明導電層,而第二基 板具有目案化表面,該表面具有表面凸凹繞射圖案且亦 塗佈有透明導電層。表面凸凹繞射光學為—實體基板,其 在/、上具有餘刻或形成的繞射格柵。表面凸凹繞射圖案可 藉由金剛石切削、射出成形、模鑄、熱成形及衝壓成形而 121818.doc • 21 - 200807055 形成。該光學可經設計具有固定光焦度及/或像差校正。 藉由經由電極施加電塵至液晶,光焦度/像差校正可分別 藉由折射率失配與匹配來接通與斷開。當大體上無電麼施 加時’液晶可具有與表面凸凹繞射光學大體上相同的折射 率。此抵消通常由表面凸凹繞射元件所提供的光焦度。當 施加電壓時’液晶可具有不同於表面凸凹繞射元件之折射 率,使得表面凸凹繞射元件現提供光學添加焦度。藉由使 用表面凸凹繞射圖案方法,可製造具有較大直徑或水平寬 度之動態電活性光學。可使此等光學的寬度高達或大於4〇 mm ° 亦"T使用較尽的液晶層(通常>5〇 μιη)來建構電活性多焦 點光學。舉例而言,可採用模態透鏡來形成折射光學。在 此項技術中已知,模悲透鏡併有單一連續低傳導性圓形電 極,該電極由單一高傳導性環形電極圍繞並與其電接觸。 在她加單一電壓至咼傳導性環電極後,低傳導性電極、基 本上徑向對稱電阻網路在液晶層上產生電壓梯度,其隨後 在液晶中誘發折射率梯度^具有折射率梯度之⑸層將充 當電活性透鏡且將使入射至其上的光聚焦。 在本發明的"實施例中,動態光學與增進透鏡組合使用 以形成-組合透鏡1進透鏡可為低添加焦度增進透鏡。 增進透鏡包含增進區域。動態光學可經定位,使得其與增 進區域進行光學傳遞。動態光學與增進區域間帛,但其間 進行光學傳遞。 在本發明之一實施例巾,增進區域可具有+0.50D、 I21818.doc • 22 - 200807055 + 0.75D、+1.00D、+1.12D、+1.25D、+1.37D及+ 1.50D 中之 一者的添加焦度。在本發明之一實施例中,動態光學在啟 動狀態可具有 +0.50D、+0.75D、+1.00D、+1.12D、 + 1.25D、+1.37D、+1.50D、+1.62D、+1.75D、+2.00D 及 +2.25D中之一者之光焦度。增進區域之添加焦度與動態光 學的光焦度可經製造或指定用於+0.125D(其大約為+0.12或 + 0.13)屈光等級或+0.25D屈光等級的患者。 應指出的是,本發明涵蓋在遠、中及近觀察距離適當地 校正配戴者視力所需的任何及所有可能焦度組合(動態與 靜態)。在本揭示内容中所提供之本發明之實例與實施例 僅為說明性的且不欲以任何方式而為限制性的。相反,其 意欲展示當低添加焦度增進區域與動態光學進行光學傳遞 時之添加光焦度關係。 動態光學可具有一摻合區,使得沿元件周邊邊緣之光焦 度被摻合以當元件啟動時減小周邊邊緣的可見度。在多數 (但非所有)情況下,動態光學之光焦度可在摻合區中自由 啟動時的動態光學所形成的最大光焦度過渡至增進透鏡中 發現的光焦度。在本發明的一實施例中,摻合區沿動態光 學周邊邊緣可為1 mm至4 mm寬。在本發明的另一實施例 中,摻合區沿動態光學周邊邊緣可為1 mm至2 mm寬。 當動態光學禁用時,動態光學將大體上不提供光學添加 焦度。因此,當動態光學禁用時,增進透鏡可提供組合透 鏡之所有添加焦度(亦即,組合光學之總添加焦度等於PAL 的添加焦度)。若動態光學包括摻合區,則在禁用狀態, 121818.doc -23- 200807055 歸因於禁用狀態中的折射率匹配,摻合區大體上不形成光 焦度且大體上無無用散光。在本發明的實施例中,當動雜 光學禁用時,在組合透鏡内的總無用散光大體上等於由增 進透鏡所造成的無用散光。在本發明的一實施例中,當動 態光學被禁用時,組合光學之總添加焦度可大約為+1〇〇D 且在組合透鏡内的總無用散光可為大約i .⑽D或更少。在 本發明的另一實施例中,當動態光學被禁用時,組合光學 之、’、“添加焦度可大約為+1 25D且在組合透鏡内的總無用散 光可為大約1.25D或更少。在本發明的另一實施例中,當 動悲光學被禁用時,組合光學之總添加焦度可大約為 +1.5 0D且在組合透鏡内的總無用散光可為大約15〇d或更 少〇 當動態光學啟動時,動態光學將提供額外光焦度。因為 動L光學與增進透鏡進行光學傳遞,組合光學的總添加焦 度等於PAL的添加焦度與動態光學的添加光焦度。若動態 光學包括一摻合區,則在啟動狀態中,歸因於在啟動狀態 中折射率失配,摻合區形成光焦度與無用散光,且很大程 度上不可用於視力聚焦。因此,當動態光學包括摻合區 時,組合光學的無用散光僅在動態光學不包括摻合區的可 用部分内經量測。在本發明的一實施例中,當動態光學被 啟動時,如經由該透鏡的可用部分所量測,組合透鏡内之 總無用散光可大體上等於增進透鏡内的無用散光。在本發 的具&例中’當動態光學被啟動且組合光學的總添加 焦度在大約+〇.75D與大約+2·25〇之間時,在組合透鏡之可 I21818.doc •24- 200807055 用部分内的總無用散光可為1.00D或更少。在本發明的另 一實施例中,當動態光學被啟動且組合光學的總添加焦度 在大約+2.50D與大約+2.75D之間時,在組合透鏡之可用部 分内的總無用散光可為L25D或更少。在本發明的另一實 施例中,當動態光學被啟動且組合光學之總添加焦度在大 約+3.00D與大約+3.50D之間時,在組合透鏡之可用部分内 的總無用散光可為1.50D或更少。因此,本發明允許形成 一具有顯著高於透鏡之無用散光之總添加焦度(如經由透 鏡的可用部分所量測)的透鏡。或以另一種方式說明,對 於本發明之組合透鏡的給定總添加焦度,大體上減小無用 散光程度。關於在文獻中所教示的透鏡或市售透鏡,此為 很大程度的改良。此改良轉換為更高的適配率、更小的失 真、配戴者更少的失誤或失向及由配戴者所觀察的更寬的 清楚的中距離與近距離視場。 在本發明的一實施例中,動態光學可形成使用者近距離 視力處方所需之總添加焦度的大約3〇〇/❶與大約。之間。 低添加焦度PAL之增進區域可形成使用者近距離視力處方 所而之添加焦度之其餘部分,亦即,分別在大約與大 約30 /。之間。在本發明的另_實施例中,冑態光學與增進 區域可各形成使㈣近距離視力處方所需之總添加焦度的 大約50%。右動態光學形成過多的總添加焦度,則當動態 透鏡禁用時’使用者可能不能在中距離看清楚。另外,當 動=光干啟動時’使用者在中距離觀察區中可能具有過多 的光焦度且同樣可能不能夠在中距離看清楚。若動態光學 121818.doc -25- 200807055 形成過少的總添加焦冑,則组合透鏡可具有過多的無用散 光。 當動態光學包括摻合區時,可需要動態光學足夠寬以確 保摻合區的至少一部分位於組合光學的周邊中。在本發明 之一實施例中,動態光學之水平寬度可為大約26 mm或更 大。在本發明的另—實施例中,動態光學之水平寬度可在 大約24 mm與大約4〇 mm之間。在本發明的另一實施例 中,動態光學的水平寬度在大約30 mm與大約34 mm之 _ 間。若動光學在寬度上小於大約24咖,則當動態光學 啟動時,可忐摻合區可與使用者視力建立介面且對使用者 形成過多的失真且使其眼花。若動態光學在寬度上大於大 約40 mm,則可能難以將組合透鏡磨邊為眼鏡框形狀。在 多數情況下(但非所有情況下),當動態光學經定位使得其 摻合區在組合透鏡的配合點處或在組合透鏡的配合點下方 時,動悲光學可具有一橢圓形狀,其水平寬度尺寸大於其 0 垂直高度尺寸。當動態光學經定位使得其摻合區在配合點 上方時,動態光學通常(但非總是)經定位,使得動態光學 的頂部周邊邊緣在配合點上方最少8 mm處。應注意,非電 活性之動態光學可置放至組合透鏡的周邊邊緣。另外,該 非電活性動態光學可在寬度上小於2 4 m m。 在本發明的一實施例中,動態光學位於配合點處或配合 點上方。動態光學之頂部周邊邊緣可在配合點上方大約〇 mm與15 mm之間。動態光學當啟動時能夠提供當配戴者在 中距離、近距離或在中距離與近距離之間的某距離(近_中 121818.doc -26- 200807055 距離)觀看時所需的光焦度。此係由於動態光學位於配合 點處或配合點上方。此將允許使用者在直視時具有校正中 距離處方。另外,由於增進區域,光焦度自配合點向下經 過通道持續增加。當透過該通道觀察時,使用者將具有校 正近中距離與近距離處方校正。因此,使用者可在許多 情形中無需向下觀看直至或必須提高其下頜直至透過透鏡 的中距離觀察區觀看。若動態光學與組合透鏡的頂部垂直 間隔,則使用者亦可能夠藉由利用啟動的動態光學上方的 組合透鏡之一部分來在遠距離觀察。當動態光學禁用時, 在配合點處或靠近配合點的透鏡區域將返回至透鏡的遠距 離光焦度。 在動悲光學具有摻合區之實施例中,在配合點上方定位 该動態光學可為較佳的。在該實施例中,當動態光學啟動 時,使甩者可透過配合點且透過通道向下直視而無需透過 摻合區觀察。如上文所提及,摻合區可引入高度的無用散 光,透過其觀察可為不舒服的。因此,使用者可使用在啟 動狀態的組合光學而不經歷高度的無用散光,因為使用者 無需越過動態光學的邊緣或摻合區。 在本發明的一實施例中,動態光學位於配合點下方。動 悲光學之頂部周邊邊緣可在配合點下方大約〇瓜瓜與15瓜瓜 之間。备使用者透過配合點直視時,藉由組合光學提供遠 距離處方权正’因為動態光學並不與組合透鏡的此部分進 仃光學傳遞。然肩,當使用者自配合點向下透過通道轉移 其凝視時’隨著使用者眼睛越過動態光學的摻合區,使用 121818.doc -27- 200807055 者可經歷高度的無用散光。此可以下文所詳細描述的多種 方式矯正。 本發明組合眼用透鏡包含一光學設計,其考慮: 1)本發明眼用透鏡滿足配戴者近視力校正所需的總近距 離添加焦度; ^ 2)處於組合透鏡的可用部分中之無用散光或失真程度; • 3)部分由增進區域形成的光學添加焦度的量; 4)當啟動時由動態光學形成的光焦度的量; _ 5)增進區域的通道長度; 6) 關於其是否為(僅舉例而言)軟PAL設計、硬PAL設 計、修改的軟PAL設計或修改的硬PAL設計之增進區域的 設計; 7) 動態光學之寬度與長度;及 8) 動態光學相對於增進區域之位置。 圖1A展示具有配合點110與增進區域120之增進透鏡100 的一實施例。圖1A中的增進透鏡為低添加焦度增進透鏡, ^ 其經設計以向配戴者提供小於配戴者所需近距離光焦度校 正之所要光焦度。舉例而言,PAL之添加焦度可為近距離 光焦度校正之50%。沿透鏡軸線AA自配合點至透鏡上光焦 度在所要添加光焦度之85%内的點之距離被稱作通道長 度。通道長度在圖1A中表示為距離D。距離D之值可視許 多因素而變化,諸如鏡框風格(透鏡將被磨邊以符合該鏡 框)、所需光焦度之量及所需通道寬度之大小。在本發明 之一實施例中,距離D在大約11 mm與大約20 mm之間。在 121818.doc -28 - 200807055 本發明之另一實施例中,距離D在大約14mm與大約i8 mm 之間。 圖1B展不沿圖以之透鏡之橫截面沿軸線aa所截取的光 焦度130之曲線圖。曲線圖之χ軸表示沿透鏡中軸線aa之 距離。曲線圖之y軸表示在透鏡内光焦度的量。在曲線圖 中所展示的光焦度始於配合點。在配合點之前或配合點處 之光焦度可為大約+0.00D至大約+〇12D(亦即,近似無光 焦度)或可視使用者之遠距離處方需要而具有正屈光度或 負屈光度。圖1B展示在配合點之前或在配合點處不具有光 焦度之透鏡。在配合點之後,光焦度持續增加至最大焦 度。對於沿軸線AA之透鏡的某長度,可持續存在最大焦 度。圖1B展示最大焦度持續存在,其表現為光焦度之平穩 狀恶。圖1B亦展示在最大焦度之前出現的距離D。在最大 焦度平穩狀態之後,光焦度可接著持續降低直至所要光焦 度。所要光焦度可為小於最大焦度的任何焦度且可等於在 配合點處的光焦度。圖1B展示光焦度在最大焦度之後持續 降低。 在本發明之一實施例中,增進區域可為位於透鏡之前表 面上的增進表面且動態光學可嵌埋於透鏡内部。在本發明 之另一實施例中,增進區域可為位於透鏡的後表面上的增 進表面且動態光學可嵌埋於透鏡内部。在本發明的另一實 施例中,増進區域可為兩個增進表面,其中一個表面位於 透鏡之前表面上且第二表面位於透鏡之後表面上(如雙表 面增進透鏡之表面)且動態光學可嵌埋於透鏡内部。在其 121818.doc •29- 200807055 他本發明實施例中,增進區域可不由幾何表面產生,而是 可由折射率梯度產生。該實施例將允許透鏡之兩個表面類 似於在單焦點透鏡上使用之表面。提供增進區域之該折射 率梯度可位於透鏡内部或在透鏡表面上。 如上文所述之本發明之一個重要優勢在於,即使當動態 光學處於禁用狀態時,配戴者總是具有校正中距離與遠距 離視力光焦度。因此,可需要的唯一控制機制為用於當配 戴者需要適當近距離光焦度時選擇性地啟動動態光學之構 件。藉由低添加焦度PAL提供此效應,該低添加焦度PAL 具有在近距離提供小於使用者處方近距離需要之光焦度的 添加焦度,且此外,此低添加焦度接近配戴者中距離觀察 需要之校正處方光焦度。當動態光學啟動時,將滿足配戴 者之近距離光焦度聚焦需要。 此可大大地簡化控制透鏡所需的感應器組。實際上,所 有可需要的是-種感應設備,其可偵測使用者是否超過中 距離而聚焦。若使用者比遠距離近而聚焦,則可啟動動態 光學。若使用者並不比遠距離近而聚焦,則可禁用動態光 學。該設備可為一簡單的傾斜開關、手動開關或測距儀。 在本:明的實施例中,可將少量暫態延遲置於控制系統 I ’使侍在動態光學啟動之前患者眼睛越過動態光學之周 。此允許配戴者避免任何討厭的無用失真效應, 該等失真效應可藉由播i 透匕動悲光學之周邊邊緣觀察而造 態光學包括摻合區時,該實施例可為有益的。僅 牛歹•而"’當觀察者之視線自觀察一遠距離物件至-近距 121818.doc •30- 200807055 離物件移動時,配戴者的眼睛將在動態光學之周邊邊緣上 轉至近距離觀察區内。在此情況下,動態光學將直至配戴 者之視線已越過動態光學周邊邊緣且至近距離觀察區内才 啟動。藉由延遲啟動動態光學之時間以允許配戴者視線越 .過周邊邊緣而發生此種情況。若動態光學之啟動並不暫時 地延遲且相反在配戴者之視線越過周邊邊緣之前啟動,則 配戴者在透過周邊邊緣觀察時可經歷高度的無用散光。通 常當動態光學之周邊邊緣位於組合透鏡之配合點處或下方 時利用此本發明實施例。在其他本發明實施例中,動態光 學之周邊邊緣可位於組合透鏡的配合點上方且因此,在許 多情況下,可無需該延遲,因為當在中距離與近距離之間 觀察時’配戴者視線從不越過動態光學之周邊邊緣。 在其他本發明實施例中,動態光學之增進透鏡與摻合區 可經設計,使得在兩者重疊之區域中,在摻合區中之無用 散光至少部分抵消在PAL中之無用散光中之某些。此效應 可與雙侧PAL相當,在雙側PAL中,一個表面之無用散光 經設計以抵消另一表面之無用散光中之某些。 在本發明之一實施例中,可需要增加動態光學之大小並 定位動態光學使得動態光學之頂部周邊邊緣在透鏡之配合 點上方。圖2A展示與更大動態光學22〇組合之低添加焦度 增進透鏡200的一實施例,該動態光學22〇經置放使得動態 光學之頂部周邊邊緣250位於透鏡之配合點21〇上方。在本 發明的一實施例中,較大動態光學之直徑在大約24 1^11與 大約40 mm之間。動態光學相對於透鏡配合點之垂直移位 121818.doc •31- 200807055 由距離d表示。在本發明之一實施例中,距離d在大約〇mm 至等於動態光學之直徑的大約一半之距離的範圍内。在本 發明之另一實施例中,距離d為在動態光學之大約八分之 一與動態光學之直徑之八分之三之間的距離。圖2B展示具 有一組合光焦度230之一實施例,由於動態光學與增進區 域240進行光學傳遞,因此形成此組合光焦度23〇。透鏡 200可具有減小的通道長度。在本發明之一實施例中,通 道長度在大約11 mm與大約20 mm之間。在本發明之另一 實施例中,通道長度在大約14 mm與大約18 mm之間。 在圖2A與圖2B所說明之本發明實施例中,當動態光學 啟動時,因為透鏡為低添加焦度PAL且動態光學位於配合 點上方’因此配戴者在直視時具有校正中距離視力。隨著 配戴者眼睛移動至通道下方,配戴者亦具有校正近-中距 離。最終,配戴者在組合透鏡之區域内具有校正近距離視 力’在該組合透鏡區域内,動態光學與增進區域之焦度經 組曰以形成所需要的近觀察距離校正。此為一種組合動態 光學與增進區域之有利方法,因為電腦使用主要為中觀察 距離任務且為一種許多人以直視或稍微向下的觀察姿勢觀 察電細螢幕之中觀察距離任務。在禁用狀態,透鏡在配合 點上方且靠近配合點之區域允許利用在配合點下方之弱增 進焦度而用於距離視力觀察校正。增進區域之最大光焦度 形成配戴者所需近距離光焦度之大約一半且動態光學形成 清楚近距離視力所需之光焦度的其餘部分。 圖3A-3C說明本發明之一實施例,其中動態光學32〇置 121818.doc •32- 200807055 於透鏡300内,且增進區域31〇置於透鏡後表面上。在藉由 被稱作自由成形之製造方法加工具有整合動態光學之半修 整透鏡毛述期間,可將此後增進表面置於透鏡上。在本發 明之另一實施例中,增進區域位於半修整透鏡毛坯之前表 面上半修整透鏡毛链併有動態光學,使得動態光學與增 進表面彎曲適當對準。接著藉由習知表面加工、研磨、磨 邊及女裝至眼鏡框内來加工半修整透鏡毛迷。 如圖3A所說明,當動態光學禁用時,沿配戴·者眼睛34〇 透過配合點之視線所得到的光焦度向配戴者提供校正遠距 離視力330。如圖3B所說明,當動態光學啟動時,沿配戴 者眼睛透過配合點之視線所得到的光焦度向配戴者提供校 正中距離聚焦焦度331。隨著配戴者向通道下方移動其凝 視(如在圖3B-3C中所示),動態光學與增進表面之組合光 學提供自中距離焦點至近距離焦點之一基本上連續的焦度 過渡。因此,如圖3C所說明,當動態光學啟動時,沿自配 戴者眼睛透過近距離觀察區之視線所取得之光焦度向配戴 者提供校正近距離聚焦焦度332。本發明之此實施例的一 個主要優勢可為控制系統僅需要決定配戴者是否向遠距離 觀察。在此距離觀察之情況下,動態光學可保持為禁用狀 態。在使用測距設備的實施例中,測距系統僅需要決定物 件是否比配戴者之中距離更靠近眼睛。在此情況下,動態 光學將被啟動以提供組合光焦度,從而允許同時中距離與 近距離光焦度校正。本發明之此實施例之另一主要優勢在 於,當動悲光學啟動時,諸如當使用者自透鏡之遠距離部 121818.doc -33- 200807055 分至透鏡之近距離部分觀察及使用者自透鏡之近距離部分 至透鏡之遠距離部分觀察時,眼睛無需越過或穿過動態光 學之上邊緣。若動態光學使其最上邊緣位於配合點下方, 則&自遠距離至近距離觀察或自近距離至遠距離觀察時, 眼睛必須越過或穿過此上邊緣。然而,本發明之實施例可 允許在配合點下方定位該動態光學,使得眼睛並不越過動 怨光學之最上邊緣。該實施例可允許關於視覺效能與人體 工學之其他優勢。 雖然圖3A-3C說明在後表面上之增進表面區域,但當動 悲光學可位於透鏡内時其亦可置於透鏡之前表面上或位於 透鏡之前表面與後表面上。另外,雖然說明動態光學位於 透鏡内部,但若其由彎曲基板製成且由眼用覆蓋材料覆 蓋’則其亦可置於透鏡表面上。藉由使用與各具有不同添 加焦度之不同PAL透鏡組合的具有已知光焦度之一個動態 光學’可能大體上減小動態光學半修整毛坯SKU之數目。 舉例而言,+0.75D動態光學可與+0.50D、+0.75D或+1.00D 增進區域或表面組合以分別產生+125D、+1.50D或+1.75D 之添加焦度。或+1.00D動態光學可與+0.75D或+1.00D增進 區域或表面組合以產生+1.75或+2.00D之添加焦度。此 外’增進區域可經最佳化以說明配戴者特徵,諸如患者遠 距離焦度及透過透鏡之眼睛路徑,以及增進區域被添加至 提供大約一半所需讀取校正之動態電活性光學之事實。同 樣,與之相反者亦可良好運作。舉例而言,+1 .〇〇D增進區 域或表面可與+0.75D、+1.00D、+1.25D或+1.50D動態光學 121818.doc -34- 200807055 組合以產生+1.75D、+2.00D、+2.25D或+2.50D之組合添加 焦度。 圖4 A說明本發明之另一實施例,藉此低添加焦度增進透 鏡400與大於增進區域及/或通道430之動態光學420組合。 在此實施例中,來自動態光學之摻合區之無用失真450處 _ 於配合點410與增進通道430與讀取區440外部。圖4B-4D展 _ 示沿圖4A之透鏡橫截面沿轴線AA所取得之光焦度的曲線 圖。每一曲線圖之X軸表示沿透鏡中轴線AA之距離。每一 _ 曲線圖之y軸表示在透鏡内光焦度的量。在配合點之前或 配合點處之光焦度可為大約+0.00D至大約+0.12D(亦即, 近似無光焦度)或可視使用者之遠距離處方需要而具有正 屈光度或負屈光度。圖4B展示在配合點之前或在配合點處 不具有光焦度之透鏡。圖4B展示沿圖4A之軸線AA所取得 的由固定增進表面或區域所提供之光焦度460。圖4C展示 沿圖4A之軸線AA所取得的由動態光學啟動時所提供之光 焦度470。最後,圖4D展示沿圖4A之軸線AA所取得的動態 ^ 電活性光學與固定增進區域之組合焦度。自圖式清楚可 見,動態電活性光學之頂部與底部失真摻合區450在配合 點410與增進讀取區440及通道430外部。 圖5A與5B說明動態光學520位於低添加焦度增進透鏡 500之配合點510下方之實施例。在圖5A中,動態電活性光 學之掺合區之位置隨著配戴者之眼睛向下追蹤增進過道 530而導致顯著的總失真550。在本發明之某些實施例中, 此藉由延遲動態光學之啟動直至配戴者之眼睛越過動態光 121818.doc -35- 200807055 學之摻合區之上邊緣而解決。圖5B展示沿圖5A之軸線AA 之光焦度。可見失真區域550在配合點正下方與透鏡之添 加焦度重疊且進一步展示延遲動態光學之啟動直至眼睛越 過此區域之需要。一旦眼睛越過此區域且進入(例如)讀取 區54❹,則不再有顯著光學失真。在本發明之一實施例 中,可提供1 mm至2 mm之極窄的摻合區以允許眼睛快速 ^ 越過此區域。在本發明的一實施例中,動態光學之水平寬 度可在大約24 mm與大約40 mm之間。在本發明的另一實 Φ 施例中,動態光學之水平寬度可在大約30 mm與大約34 mm之間。在本發明之另一實施例中,動態光學的水平寬 度可為大約32 mm。因此,在某些本發明實施例中,動態 光學之形狀更類似橢圓形,其中水平量測比垂直量測更 寬。 圖6A-6C展示動態光學之實施例。在所示實施例中,動 態光學具有橢圓形狀且寬度在大約26 mm與大約32 mm之 間。展示動態光學之各種高度。圖6A展示高度為大約14 • mm之動態光學。圖6B展示高度為大約19 mm之動態光 學。圖6C展示高度為大約24 mm之動態光學。~ 』 used for hunting by the 椟-like diffraction concentric ring electrode structure to produce optical add power. The phlegm electrode can also be used to correct higher order aberrations of the eye in a manner similar to that used to correct atmospheric turbulence in ground-based astronomy. Current manufacturing methods limit the minimum pixel size and also limit the maximum moving electrical active optical diameter. By way of example only, when using a diffraction pattern; the maximum dynamic electroactive optical diameter is estimated to be 20 mm for + 1.50D, 24 _ for +1.25D, and 30 for + ι _ Mm. Current manufacturing methods limit the maximum dynamic electroactive optical diameter when using pixelated diffraction methods. In the same manner, embodiments of the present invention may have dynamic electroactive optics having a smaller power at a larger diameter. Alternatively, the electroactive optics comprise two transparent substrates and a liquid crystal layer, wherein the first substrate is substantially flat and coated with a transparent conductive layer, and the second substrate has a meshed surface having a surface convex and concave diffraction pattern It is also coated with a transparent conductive layer. The surface convex-concave diffractive optics is a solid substrate having a residual or formed diffraction grating on /. The surface relief pattern can be formed by diamond cutting, injection molding, die casting, thermoforming, and stamping. 121818.doc • 21 - 200807055. The optics can be designed to have fixed power and/or aberration correction. By applying electric dust to the liquid crystal via the electrodes, the power/disparity correction can be turned on and off by refractive index mismatch and matching, respectively. The liquid crystal may have substantially the same refractive index as the surface convex-concave diffractive optics when applied substantially without electricity. This cancellation is typically the power provided by the surface convex and concave diffractive elements. The liquid crystal may have a refractive index different from that of the surface convex and concave diffractive elements when a voltage is applied, such that the surface convex and concave diffractive elements now provide optical add power. Dynamic electroactive optics having a larger diameter or horizontal width can be fabricated by using a surface convex and concave diffraction pattern method. The width of these optics can be as high as or greater than 4 〇 mm ° and also use a more liquid crystal layer (usually > 5 〇 μιη) to construct electroactive multifocal point optics. For example, a modal lens can be employed to form refractive optics. It is known in the art to model a lens with a single continuous low conductivity circular electrode that is surrounded by and in electrical contact with a single highly conductive ring electrode. After she applies a single voltage to the 咼 conductive ring electrode, the low-conductivity electrode, the substantially radial symmetrical resistance network creates a voltage gradient across the liquid crystal layer, which then induces a refractive index gradient in the liquid crystal with a refractive index gradient (5) The layer will act as an electroactive lens and will focus the light incident thereon. In the "embodiment of the invention, the combination of dynamic optics and enhancement lenses to form a combination lens 1 into the lens may be a low add power enhancement lens. The promotional lens contains a promotional area. Dynamic optics can be positioned such that it is optically transmitted to the enhanced region. Dynamic optics and enhanced inter-regional enthalpy, but optical transmission between them. In an embodiment of the invention, the enhancement zone may have one of +0.50D, I21818.doc • 22 - 200807055 + 0.75D, +1.00D, +1.12D, +1.25D, +1.37D, and + 1.50D. The added power of the person. In an embodiment of the invention, the dynamic optics may have +0.50D, +0.75D, +1.00D, +1.12D, +1.25D, +1.37D, +1.50D, +1.62D, + 1.75 in the startup state. The power of one of D, +2.00D and +2.25D. The add power and dynamic optical power of the enhanced region can be manufactured or specified for patients with a +0.125D (which is approximately +0.12 or +0.13) refractive index or a +0.25D refractive index. It should be noted that the present invention encompasses any and all possible power combinations (dynamic and static) required to properly correct the wearer's vision at the far, middle and near viewing distances. The examples and embodiments of the invention are provided by way of illustration only and are not intended to be limiting. Rather, it is intended to show the add power relationship when the low add power enhancement region is optically transmitted with dynamic optics. Dynamic optics can have a blending zone such that the power along the perimeter edge of the component is blended to reduce the visibility of the peripheral edge when the component is activated. In most, but not all, cases, the power of the dynamic optics can be maximized by the dynamic power of the dynamic optics when freely activated in the blending zone to enhance the power found in the lens. In an embodiment of the invention, the blending zone may be from 1 mm to 4 mm wide along the dynamic optical peripheral edge. In another embodiment of the invention, the blending zone may be 1 mm to 2 mm wide along the dynamic optical peripheral edge. When dynamic optics is disabled, dynamic optics will generally not provide optical add power. Thus, when dynamic optics is disabled, the enhancement lens provides all of the added power of the combined lens (i.e., the total add power of the combined optics is equal to the added power of the PAL). If the dynamic optics include a blending zone, then in the disabled state, 121818.doc -23-200807055 due to index matching in the disabled state, the blending zone generally does not form a power and is substantially free of unwanted astigmatism. In an embodiment of the invention, when the moving optics are disabled, the total unwanted astigmatism in the combined lens is substantially equal to the unwanted astigmatism caused by the progressive lens. In an embodiment of the invention, when dynamic optics is disabled, the combined add power of the combined optics may be approximately +1 〇〇 D and the total unwanted astigmatism within the combined lens may be approximately i. (10) D or less. In another embodiment of the invention, when dynamic optics is disabled, the combined optical, ',' add power may be approximately +1 25D and the total unwanted astigmatism within the combined lens may be approximately 1.25D or less. In another embodiment of the invention, when dynamic optics is disabled, the combined add power of the combined optics may be approximately +1.5 0D and the total unwanted astigmatism within the combined lens may be approximately 15 〇 d or less. When dynamic optical start-up, dynamic optics will provide additional power. Because the L-optical and the enhanced lens are optically transmitted, the total add power of the combined optics is equal to the add power of the PAL and the add power of the dynamic optics. Dynamic optics includes a blending zone, and in the activated state, the blending zone forms power and unwanted astigmatism due to refractive index mismatch in the activated state, and is largely unusable for vision focusing. When dynamic optics includes a blending zone, the unwanted astigmatism of the combined optics is only measured within the available portion of the dynamic optics that does not include the blending zone. In an embodiment of the invention, when dynamic optics is initiated, such as via Measured by the available portion of the lens, the total unwanted astigmatism in the combined lens can be substantially equal to the useless astigmatism within the enhanced lens. In the & examples of the present invention, 'when dynamic optics is activated and combined optical total add power Between about +〇.75D and about +2·25〇, the total unwanted astigmatism in the portion of the combined lens I21818.doc •24-200807055 can be 1.00D or less. Another in the present invention In embodiments, when dynamic optics is activated and the total add power of the combined optics is between about +2.50D and about +2.75D, the total unwanted astigmatism in the available portion of the combined lens can be L25D or less. In another embodiment of the invention, when dynamic optics is initiated and the total add power of the combined optics is between about +3.00D and about +3.50D, the total unwanted astigmatism in the available portion of the combined lens can be 1.50. D or less. Thus, the present invention allows for the formation of a lens having a total additive power that is significantly higher than the unwanted astigmatism of the lens (as measured by the available portion of the lens). Or alternatively, for the present invention Combined lens Total addition of power generally reduces the degree of unwanted astigmatism. This is a significant improvement with respect to lenses or commercially available lenses taught in the literature. This improvement translates to higher fit rates, less distortion, The wearer has fewer errors or misalignments and a wider clear mid-range and close-range field of view as observed by the wearer. In one embodiment of the invention, dynamic optics can form a user's near vision prescription The required total add power is between about 3 〇〇/❶ and about 。. The low add power PAL enhancement area can form the rest of the user's close vision prescription, ie, respectively Between about and about 30. In another embodiment of the invention, the xenon optics and enhancement regions can each form about 50% of the total add power required to prescribe (4) a close vision. The right dynamic optics creates too much total add power, so when the dynamic lens is disabled, the user may not be able to see it at a medium distance. In addition, when the motion = light dry start, the user may have too much power in the mid-range viewing zone and may also not be able to see it at a medium distance. If dynamic optics 121818.doc -25- 200807055 forms too little total added eschar, the combined lens can have excessive unwanted astigmatism. When the dynamic optics include a blending zone, dynamic optics may be required to be wide enough to ensure that at least a portion of the blending zone is in the perimeter of the combined optics. In one embodiment of the invention, the dynamic optics may have a horizontal width of about 26 mm or greater. In other embodiments of the invention, the horizontal width of the dynamic optics may be between about 24 mm and about 4 mm. In another embodiment of the invention, the horizontal width of the dynamic optics is between about 30 mm and about 34 mm. If the moving optics is less than about 24 ga in width, the erbium blending region can create an interface with the user's vision and create excessive distortion to the user and cause dazzling when dynamic optical activation. If the dynamic optics is greater than about 40 mm in width, it may be difficult to sharpen the combined lens into a spectacle frame shape. In most cases (but not in all cases), the dynamic optics may have an elliptical shape when the dynamic optics are positioned such that the blending zone is at the mating point of the combined lens or below the mating point of the combined lens. The width dimension is greater than its 0 vertical height dimension. When the dynamic optics is positioned such that its blending zone is above the mating point, the dynamic optics is typically (but not always) positioned such that the top perimeter edge of the dynamic optics is at least 8 mm above the mating point. It should be noted that non-electroactive dynamic optics can be placed to the peripheral edge of the combined lens. Additionally, the non-electroactive dynamic optics can be less than 2 4 m in width. In an embodiment of the invention, the dynamic optics are located at or above the mating point. The top edge of the dynamic optics can be between approximately 〇 mm and 15 mm above the mating point. Dynamic optics, when activated, provides the power required to be viewed by the wearer at medium distances, close distances, or some distance between the medium and close distances (near _121818.doc -26-200807055 distance) . This is due to the dynamic optics being located at or above the mating point. This will allow the user to have a corrected mid-range prescription when looking directly. In addition, due to the enhanced area, the power continues to increase from the mating point through the passage. When viewed through this channel, the user will have a correction for near-middle distance and close-range prescription corrections. Thus, the user may not need to look down in many situations until or must raise their lower jaw until viewed through the mid-range viewing area of the lens. If the dynamic optics are vertically spaced from the top of the combined lens, the user can also view at a distance by utilizing a portion of the combined lens above the activated dynamic optics. When dynamic optics is disabled, the lens area at or near the mating point will return to the distant power of the lens. In embodiments where the sinister optics have a blending zone, positioning the dynamic optics above the mating point may be preferred. In this embodiment, when dynamic optical activation is enabled, the latter can be made to pass through the mating point and through the channel to look straight down without observing through the blending zone. As mentioned above, the blending zone can introduce a high degree of unwanted astigmatism through which viewing can be uncomfortable. Thus, the user can use the combined optics in the activated state without experiencing a high degree of unwanted astigmatism because the user does not have to cross the edge or blending area of the dynamic optics. In an embodiment of the invention, the dynamic optics are located below the mating point. The top edge of the sorrowful optics can be placed between the melon and the melon below the fit point. When the user is looking directly through the mating point, the remote prescription is provided by the combined optics because the dynamic optics does not optically transmit to this portion of the combined lens. However, when the user shifts their gaze through the channel from the point of fit, the user can experience a high degree of unwanted astigmatism as the user's eyes pass over the dynamic optical blending zone. This can be corrected in a number of ways as described in detail below. The combination ophthalmic lens of the present invention comprises an optical design which considers: 1) the ophthalmic lens of the present invention satisfies the total near-distance addition power required for the wearer's near vision correction; ^ 2) is useless in the usable portion of the combined lens The degree of astigmatism or distortion; • 3) the amount of optical add-on that is partially formed by the enhanced region; 4) the amount of power formed by dynamic optics when activated; _ 5) the length of the channel in the enhanced region; 6) Whether it is (for example only) soft PAL design, hard PAL design, modified soft PAL design or modified hard PAL design enhancement area design; 7) dynamic optics width and length; and 8) dynamic optics relative to enhancement The location of the area. FIG. 1A shows an embodiment of a progressive lens 100 having a mating point 110 and a boosting region 120. The progressive lens of Figure 1A is a low add power enhancement lens, which is designed to provide the wearer with the desired power less than the wearer's required close power power correction. For example, the added power of PAL can be 50% of the proximity power correction. The distance from the mating point along the lens axis AA to the point at which the optical power on the lens is within 85% of the power to be added is referred to as the channel length. The channel length is represented as distance D in Figure 1A. The value of the distance D can vary depending on many factors, such as the frame style (the lens will be edged to conform to the frame), the amount of power required, and the desired channel width. In one embodiment of the invention, the distance D is between about 11 mm and about 20 mm. In another embodiment of the invention, 121818.doc -28 - 200807055, the distance D is between about 14 mm and about i8 mm. Fig. 1B is a graph showing the power of 130 taken along the axis aa of the cross section of the lens. The axis of the graph represents the distance along the central axis aa of the lens. The y-axis of the graph represents the amount of power in the lens. The power shown in the graph begins at the mating point. The power at or before the mating point may be from about +0.00D to about +〇12D (i.e., approximately no optical power) or may have positive or negative diopter as desired by the user's long distance prescription. Figure 1B shows a lens that does not have a power before the mating point or at the mating point. After the mating point, the power continues to increase to the maximum power. For a certain length of the lens along the axis AA, the maximum power can continue to exist. Figure 1B shows that the maximum power persists, which is manifested by the smoothness of the power. Figure 1B also shows the distance D that occurs before the maximum power. After the maximum power steady state, the power can then continue to decrease until the desired power. The desired power may be any power less than the maximum power and may be equal to the power at the mating point. Figure 1B shows that the power is continuously reduced after the maximum power. In one embodiment of the invention, the enhancement region can be a raised surface on the front surface of the lens and the dynamic optics can be embedded within the lens. In another embodiment of the invention, the enhancement region can be an elevation surface on the rear surface of the lens and the dynamic optics can be embedded within the lens. In another embodiment of the invention, the snagging region can be two enhancing surfaces, one of which is on the front surface of the lens and the second surface is on the rear surface of the lens (such as the surface of the dual surface enhancing lens) and is dynamically optically embeddable. Buried inside the lens. In its embodiment of the invention, 121818.doc • 29-200807055, the enhancement region may be produced by a geometric surface, but may be produced by a refractive index gradient. This embodiment will allow the two surfaces of the lens to resemble the surface used on a single focus lens. The refractive index gradient providing the enhancement region can be located inside the lens or on the lens surface. An important advantage of the present invention as described above is that the wearer always has a corrected intermediate distance and a distant visual power even when dynamic optics is in a disabled state. Thus, the only control mechanism that may be required is a component for selectively activating dynamic optics when the wearer requires proper proximity power. This effect is provided by a low add power PAL having an add power that provides a power less than the user's prescription close distance at a close distance, and further, this low add power is close to the wearer The medium distance observation requires correction of the prescription power. When dynamic optics is activated, the wearer's close-range power focusing needs to be met. This greatly simplifies the sensor set required to control the lens. In fact, all that is needed is a sensing device that detects if the user is out of focus and is in focus. Dynamic optics can be activated if the user is focusing closer than a long distance. Dynamic optics can be disabled if the user is not focusing closer than the distance. The device can be a simple tilt switch, manual switch or range finder. In this embodiment, a small amount of transient delay can be placed in the control system I' to allow the patient's eyes to cross the perimeter of the dynamic optics before the dynamic optical activation. This allows the wearer to avoid any annoying useless distortion effects that may be beneficial when the optical includes the blending zone by the observation of the peripheral edge of the sorrowful optics. Only the calf • and "' when the observer's line of sight observes a distant object to - close to 121818.doc • 30- 200807055 When the object moves, the wearer's eyes will turn to the near edge of the dynamic optics Distance to the observation area. In this case, dynamic optics will not start until the wearer's line of sight has crossed the dynamic optical peripheral edge and into the close viewing zone. This occurs by delaying the activation of the dynamic optics to allow the wearer's line of sight to pass over the perimeter edge. If the activation of the dynamic optics is not temporarily delayed and instead is initiated before the wearer's line of sight crosses the peripheral edge, the wearer can experience a high degree of unwanted astigmatism as viewed through the peripheral edge. This embodiment of the invention is typically utilized when the peripheral edge of the dynamic optics is at or below the mating point of the combined lens. In other embodiments of the invention, the peripheral edge of the dynamic optics may be located above the mating point of the combined lens and, therefore, in many cases, the delay may not be needed because the wearer is viewed between mid and close distances. The line of sight never crosses the peripheral edge of the dynamic optics. In other embodiments of the present invention, the dynamic optical enhancement lens and blending region can be designed such that in the region where the two overlap, the unwanted astigmatism in the blending region at least partially offsets some of the unwanted astigmatism in the PAL. some. This effect is comparable to a two-sided PAL where the unwanted astigmatism of one surface is designed to counteract some of the unwanted astigmatism of the other surface. In one embodiment of the invention, it may be desirable to increase the size of the dynamic optics and position the dynamic optics such that the top perimeter edge of the dynamic optics is above the mating point of the lens. 2A shows an embodiment of a low add power enhancement lens 200 in combination with a larger dynamic optics 22 that is placed such that the top perimeter edge 250 of the dynamic optics is above the mating point 21〇 of the lens. In one embodiment of the invention, the larger dynamic optics have a diameter between about 24 1^11 and about 40 mm. Vertical shift of dynamic optics relative to the mating point of the lens 121818.doc •31- 200807055 is represented by the distance d. In one embodiment of the invention, the distance d is in the range of from about 〇mm to about half the diameter of the dynamic optics. In another embodiment of the invention, the distance d is the distance between about one-eighth of the dynamic optics and three-eighths of the diameter of the dynamic optics. 2B shows an embodiment having a combined power 230 that is formed by optical transmission of the dynamic optics and enhancement region 240. Lens 200 can have a reduced channel length. In one embodiment of the invention, the channel length is between about 11 mm and about 20 mm. In another embodiment of the invention, the channel length is between about 14 mm and about 18 mm. In the embodiment of the invention illustrated in Figures 2A and 2B, when dynamic optical activation, the lens has a low add power PAL and dynamic optics are located above the mating point' so the wearer has corrected mid-range vision when looking directly at the eye. As the wearer's eyes move below the channel, the wearer also has a corrected near-to-middle distance. Finally, the wearer has corrected near vision in the area of the combined lens. In the combined lens area, the dynamic optics and the enhanced area are grouped to form the desired near viewing distance correction. This is an advantageous method of combining dynamic optics and enhanced areas because the computer uses primarily the medium-observation distance task and observes the observation distance task in the electric screen for a large number of people viewing in a direct or slightly downward viewing position. In the disabled state, the area of the lens above the mating point and close to the mating point allows for the use of weak gain enhancement below the mating point for distance vision observation correction. The maximum power of the enhanced region forms approximately half of the close power required by the wearer and the dynamic optics form the remainder of the power required for clear near vision. 3A-3C illustrate an embodiment of the invention in which dynamic optics 32 is disposed 121818.doc • 32-200807055 within lens 300 and enhancement region 31 is placed on the rear surface of the lens. This post-enhancement surface can be placed on the lens during processing of a semi-trimmed lens having integrated dynamic optics by a manufacturing process known as freeform. In another embodiment of the invention, the enhancement zone is located on the surface of the semi-trimmed lens blank before the semi-trimmed lens blank and has dynamic optics such that the dynamic optics are properly aligned with the elevation surface curvature. The semi-finished lens fan is then processed by conventional surface processing, grinding, edge grinding, and women's clothing into the eyeglass frame. As illustrated in Figure 3A, when dynamic optics is disabled, the optical power obtained by the wearer's eye 34 透过 through the line of sight of the mating point provides the wearer with corrected distance vision 330. As illustrated in Figure 3B, when dynamic optical activation is initiated, the optical power obtained by the wearer's eye through the line of sight of the mating point provides the wearer with a corrected mid-range focus power 331. As the wearer moves its gaze below the channel (as shown in Figures 3B-3C), the combined optics of the dynamic optics and the enhanced surface provides a substantially continuous power transition from one of the mid-range focus to the close focus. Thus, as illustrated in Figure 3C, upon dynamic optical activation, the wearer is provided with a corrected close focus power 332 along the power taken from the wearer's eye through the line of sight of the close viewing area. A major advantage of this embodiment of the invention may be that the control system only needs to determine if the wearer is looking at a distance. In this case of distance observation, dynamic optics can remain disabled. In an embodiment using a ranging device, the ranging system only needs to determine if the object is closer to the eye than the wearer. In this case, dynamic optics will be activated to provide combined power, allowing simultaneous mid-range and close-range power correction. Another major advantage of this embodiment of the present invention is that when the sinus optical is activated, such as when the user is from the remote portion of the lens 121818.doc -33 - 200807055 to the close portion of the lens and the user from the lens The eye does not need to cross or pass through the upper edge of the dynamic optics when viewed from a close distance portion to a remote portion of the lens. If dynamic optics have its uppermost edge below the fit point, & the eye must cross or pass through the upper edge when viewed from a long distance to a close distance or from a close distance to a long distance. However, embodiments of the present invention may allow the dynamic optics to be positioned below the mating point such that the eye does not cross the uppermost edge of the tamper optical. This embodiment may allow for other advantages regarding visual performance and ergonomics. Although Figures 3A-3C illustrate enhanced surface areas on the back surface, they may also be placed on the front surface of the lens or on the front and back surfaces of the lens when the dynamic optics are within the lens. Further, although the dynamic optics are illustrated as being located inside the lens, they may also be placed on the surface of the lens if they are made of a curved substrate and covered by an ophthalmic cover material. The number of dynamic optical half-trimmed blank SKUs may be substantially reduced by using a dynamic optical having known powers combined with different PAL lenses each having a different added power. For example, +0.75D dynamic optics can be combined with a +0.50D, +0.75D, or +1.00D enhancement region or surface to produce an add power of +125D, +1.50D, or +1.75D, respectively. Or +1.00D dynamic optics can be combined with a +0.75D or +1.00D enhancement region or surface to produce an add power of +1.75 or +2.00D. In addition, the 'enhanced area can be optimized to account for wearer characteristics, such as the patient's long-range power and the eye path through the lens, and the fact that the enhanced area is added to provide dynamic electroactive optics that provide approximately half of the read correction required. . Similarly, the opposite can work well. For example, a +1.〇〇D enhancement region or surface can be combined with +0.75D, +1.00D, +1.25D, or +1.50D dynamic optics 121818.doc -34-200807055 to produce +1.75D, +2.00D Add a power of +2.25D or +2.50D. 4A illustrates another embodiment of the present invention whereby the low add power enhancement lens 400 is combined with dynamic optics 420 that is larger than the enhancement region and/or channel 430. In this embodiment, the unwanted distortion 450 from the dynamic optical blending region is at the mating point 410 and the enhancement channel 430 and the read region 440. 4B-4D are graphs showing the power taken along the axis AA of the lens cross section of Fig. 4A. The X-axis of each graph represents the distance along the central axis AA of the lens. The y-axis of each _ graph represents the amount of power in the lens. The power at or before the mating point may be from about +0.00D to about +0.12D (i.e., approximately no power) or may have positive or negative diopter as desired by the user's long distance prescription. Figure 4B shows a lens that does not have power before the mating point or at the mating point. Figure 4B shows the power 460 provided by the fixed promotional surface or region taken along axis AA of Figure 4A. Figure 4C shows the power 470 provided by dynamic optical actuation taken along axis AA of Figure 4A. Finally, Figure 4D shows the combined power of the dynamic electro-active optics and the fixed enhancement regions taken along axis AA of Figure 4A. As is clear from the figure, the top and bottom distortion blending regions 450 of the dynamic electroactive optics are external to the mating point 410 and the enhanced read zone 440 and channel 430. 5A and 5B illustrate an embodiment in which dynamic optics 520 are positioned below mating point 510 of low add power enhancement lens 500. In Figure 5A, the position of the dynamic electroactive optical blending zone is traced down along the wearer's eye to enhance the aisle 530 resulting in significant total distortion 550. In some embodiments of the invention, this is resolved by delaying the activation of dynamic optics until the wearer's eye passes over the upper edge of the blending zone of dynamic light 121818.doc-35-200807055. Figure 5B shows the power along axis AA of Figure 5A. The visible distortion region 550 overlaps the add power of the lens directly below the mating point and further exhibits the need to delay the activation of dynamic optics until the eye passes over the region. Once the eye passes over this area and enters, for example, the read area 54, there is no significant optical distortion. In one embodiment of the invention, an extremely narrow blending zone of 1 mm to 2 mm can be provided to allow the eye to quickly pass over this zone. In an embodiment of the invention, the horizontal width of the dynamic optics can be between about 24 mm and about 40 mm. In another embodiment of the invention, the horizontal width of the dynamic optics may be between about 30 mm and about 34 mm. In another embodiment of the invention, the horizontal width of the dynamic optics can be about 32 mm. Thus, in some embodiments of the invention, the shape of the dynamic optics is more similar to an ellipse, wherein the horizontal measurement is wider than the vertical measurement. Figures 6A-6C show an embodiment of dynamic optics. In the illustrated embodiment, the dynamic optics have an elliptical shape and a width of between about 26 mm and about 32 mm. Showcase the various heights of dynamic optics. Figure 6A shows dynamic optics with a height of approximately 14 • mm. Figure 6B shows dynamic optics at a height of about 19 mm. Figure 6C shows dynamic optics with a height of approximately 24 mm.

圖7A-7K展示比較現有當前技術狀態之增進透鏡與包括 低添加焦度增進透鏡與動態光學之本發明之實施例的無用 散光等值線圖。藉由Visionix當前技術狀態PowerMapVM 2000™” 高精度透鏡分析器(High Precision Lens Analyzer)" 量測並產生無用散光焦度圖,該高精度透鏡分析器為在製 造或設計PAL時由透鏡製造商用於量測並檢驗其自身PAL 121818,doc -36- 200807055 之品質控制與市場營銷規範目的之同一設備。使用低添加 焦度PAL與球形透鏡來模仿本發明之實施例。球形透鏡具 有等於延伸至透鏡周邊之給定光焦度之啟動的動態光學之 光焦度的光焦度。Figures 7A-7K show unwanted astigmatism contour plots comparing prior art progressive lenses with embodiments of the present invention including low add power enhancement lenses and dynamic optics. Visionix's current state of the art PowerMapVM 2000TM High Precision Lens Analyzer" measures and produces a map of unwanted astigmatism, which is used by lens manufacturers when manufacturing or designing PAL The same device for measuring and verifying the quality control and marketing specifications of its own PAL 121818, doc-36-200807055. A low add power PAL and a spherical lens are used to mimic an embodiment of the invention. The spherical lens has an extension to The power of the dynamic optical power of the activation of a given power around the lens.

圖 7A 比較 Essilor Varilux Physio™ +1.25D PAL 與包括 Essilor Varilux Physio™ +1.00D PAL與+0.25D動態光學以 形成+1.25D之總添加焦度的本發明實施例。圖7B比較 Essilor Varilux Physio™ +1.50D PAL與包括 Essilor Varilux Physio™ +0.75D PAL與+0.75D動態光學以形成+ 1.50D之總 添加焦度的本發明實施例。圖7C比較Essilor Vadlux Physio™ +1.75D PAL 與包括 Essilor Varilux Physio™ + 1.00D PAL與+0.75D動態光學以形成+1.75D之總添加焦度 的本發明實施例。圖7D比較Essilor Varilux Physio™ +2.00D PAL 與包括 Essilor Varilux Physio™ +1.00D PAL 與 + 1.00D動態光學以形成+2.00D之總添加焦度的本發明實施 例。圖 7E比較Essilor Varilux Physio™ +2.00D PAL與包括 Essilor Varilux Physio™ +0.75D PAL與+ 1.25D動態光學以 形成+2.00D之總添加焦度的本發明實施例。圖7F比較 Essilor Varilux Physio™ +2.25D PAL與包括 Essilor Varilux Physio™ +1.00D PAL與+ 1.25D動態光學以形成+2.25D之總 添加焦度的本發明實施例。圖7G比較Essilor Varilux Physio™ +2.25D PAL 與包括 Essilor Varilux Physio™ + 0.75D PAL與+1.5 0D動態光學以形成+2.25D之總添加焦度 的本發明實施例。圖7H比較Essilor Varilux Physio™ 121818.doc -37- 200807055 +2.50D PAL與包括 Essilor Varilux Physio™ +1.25D PAL與 + 1.25D動態光學以形成+2.50D之總添加焦度的本發明實施 例。圖71 比較Essilor Varilux Physio™ +2.50D PAL與包括 Essilor Varilux Physio™ +1.00D PAL與+1_50D動態光學以 形成+2.50D之總添加焦度的本發明實施例。圖7J比較 Essilor Varilux Physio™ +2.75D PAL與包括 Essilor Varilux - Physio™ +1.25D PAL與+1.50D動態光學以形成+2.75D之總 添加焦度的本發明實施例。圖7K比較Essilor Varilux _ Physio™ +3.00D PAL 與包括 Essilor Varilux Physio™ + 1.50D PAL與+1.50D動態光學以形成+3.00D之總添加焦度 的本發明實施例。 圖7A-7K清楚地展示本發明之方法所做出的優於當前技 術狀態之增進透鏡之顯著改良。當與當前技術狀態之PAL 透鏡相比時,在圖7A-7K中所展示之本發明實施例具有顯 著較小的失真、顯著較少的無用散光、更寬的通道寬度及 對於更低添加焦度與更高添加焦度略微更短的通道長度。 ® 本發明之方法能夠提供此等顯著改良同時允許使用者如利 用習知PAL透鏡在遠距離、中距離及近距離看清楚。 本發明另外涵蓋,視配戴者之瞳孔距離、配合點及所切 割的鏡框邊尺寸而定,動態光學可需要相對於增進區域偏 心垂直且在某些情況下水平。然而,在所有情況下,當動 態光學相對於增進區域偏心時,當動態光學啟動時,其保 持與該區域進行光學傳遞。應注意的是,鏡框邊或邊緣之 垂直尺寸在許多情況下(但非所有情況下)確定此偏心量。 121818.doc -38- 200807055 本發明之眼用透鏡允許88%或更高之光學透射。若在眼 用透鏡之兩個表面上利用抗反射塗層,則光學透射率將超 過90%。本發明之眼用透鏡之光學效率為9〇%或更佳。本 發明之眼用透鏡能夠以多種熟知透鏡處理(僅舉例而言, 諸如抗反射塗層、防刮塗層、緩衝塗層、疏水性塗層及紫 外線塗層)來被塗佈。紫外線塗層可塗覆至眼用透鏡或動 態光學。在動態光學為基於液晶之電活性光學之實施例 中’紫外線塗層可防止液晶免於紫外光損害,紫外光可能 隨著時間損害液晶。本發明之眼用透鏡亦能夠被磨邊為眼 鏡框所需形狀,或在其周邊鑽孔以便於(僅舉例而言)在無 邊緣眼鏡框中被安裝。 另外應注意的是,本發明涵蓋所有眼用透鏡;隱形眼 睛、人工晶狀體、角膜覆體、角膜嵌體及眼鏡片。 【圖式簡單說明】 圖1A展示一具有一配合點與一增進區域之低添加焦度增 進透鏡的一實施例; 圖1B展示沿圖1A之透鏡之橫截面沿轴線aa所截取之光 焦度13 0的曲線圖; 圖2 A展示具有與更大動態光學組合之低添加焦度增進透 鏡之本發明的一實施例,該更大動態光學經置放使得動態 光學之一部分位於透鏡之一配合點上方; 圖2B展示具有一由於動態光學與增進區域進行光學傳遞 而產生的組合光焦度之圖2 A之組合透鏡; 圖3 A展示具有一低添加焦度增進透鏡與一動態光學之本 121818.doc •39、 200807055 發明之一實施例,動態光學經放置使得動態光學之一部分 位於透鏡之配合點上方。圖3 A展示當動態光學禁用時,沿 自配戴者眼睛透過配合點之視線所取得的光焦度向配戴者 提供板正遂距離視力, 圖3B展示圖3A之透鏡。圖3B展示當動態光學啟動時, 沿自配戴者眼睛透過配合點之視線所取得的光焦度向配戴 者提供校正中距離聚焦焦度; 圖3C展示圖3A之透鏡。圖3C展示當動態光學啟動時, 沿自配戴者眼睛透過近距離觀察區之視線所取得的光焦度 向配戴者提供校正近距離聚焦焦度; 圖4 A展示具有與動態光學組合之低添加焦度增進透鏡之 本發明的一實施例,動態光學大於增進區域及/或通道且 位於透鏡之配合點上方; 圖4B展示沿圖4A之軸線AA所取得之藉由固定增進表面 或區域所提供之光焦度; 圖4C展示沿圖4A之軸線AA所取得之藉由動態光學在啟 動時所提供之光焦度; 圖4D展示沿圖4A之軸線AA所取得之動態電活性光學與 固定增進區域之組合焦度。圖4D展示動態電活性光學之頂 部與底部失真摻合區在配合點與增進讀取區與通道外部; 圖5 A展示本發明之一實施例,其中動態光學位於低添加 焦度增進透鏡之配合點下方; 圖5B展示沿圖5A之軸線AA所取得之光焦度; 圖6A至圖6C展示動態光學之大小之各種實施例;及 121818.doc -40· 200807055 圖7A至圖7K展示比較現有當前技術狀態之增進透鏡與 包括低添加焦度增進透鏡及動態光學之本發明之實施例的 無用散光等值線圖。 【主要元件符號說明】Figure 7A compares an Essilor Varilux PhysioTM + 1.25D PAL with an embodiment of the invention comprising Essilor Varilux PhysioTM + 1.00D PAL and +0.25D dynamic optics to form a total add power of +1.25D. Figure 7B compares an Essilor Varilux PhysioTM + 1.50D PAL with an embodiment of the invention comprising Essilor Varilux PhysioTM + 0.75D PAL and +0.75D dynamic optics to form a total add power of + 1.50D. Figure 7C compares an embodiment of the invention with Essilor Vadlux PhysioTM + 1.75D PAL and including Essilor Varilux PhysioTM + 1.00D PAL and +0.75D dynamic optics to form a total add power of +1.75D. Figure 7D compares an embodiment of the invention with Essilor Varilux PhysioTM + 2.00D PAL and including Essilor Varilux PhysioTM + 1.00D PAL and + 1.00D dynamic optics to form a total add power of +2.00D. Figure 7E compares an Essilor Varilux PhysioTM + 2.00D PAL with an embodiment of the invention comprising Essilor Varilux PhysioTM + 0.75D PAL and + 1.25D dynamic optics to form a total add power of +2.00D. Figure 7F compares an Essilor Varilux PhysioTM + 2.25D PAL with an embodiment of the invention comprising Essilor Varilux PhysioTM + 1.00D PAL and + 1.25D dynamic optics to form a total add power of +2.25D. Figure 7G compares an Essilor Varilux PhysioTM + 2.25D PAL with an embodiment of the invention comprising Essilor Varilux PhysioTM + 0.75D PAL and +1.5 0D dynamic optics to form a total add power of +2.25D. Figure 7H compares an embodiment of the invention with Essilor Varilux PhysioTM 121818.doc -37-200807055 +2.50D PAL and including Essilor Varilux PhysioTM + 1.25D PAL and + 1.25D dynamic optics to form a total add power of +2.50D. Figure 71 compares an Essilor Varilux PhysioTM + 2.50D PAL with an embodiment of the invention comprising Essilor Varilux PhysioTM + 1.00D PAL and +1/50D dynamic optics to form a total add power of +2.50D. Figure 7J compares an Essilor Varilux PhysioTM + 2.75D PAL with an embodiment of the invention comprising Essilor Varilux - PhysioTM + 1.25D PAL and +1.50D dynamic optics to form a total add power of +2.75D. Figure 7K compares an Essilor Varilux _ PhysioTM + 3.00D PAL with an embodiment of the invention comprising Essilor Varilux PhysioTM + 1.50D PAL and +1.50D dynamic optics to form a total add power of +3.00D. Figures 7A-7K clearly show a significant improvement in the enhanced lens made by the method of the present invention over the current state of the art. Embodiments of the invention shown in Figures 7A-7K have significantly less distortion, significantly less unwanted astigmatism, wider channel width, and lower add focus when compared to current state of the art PAL lenses. Degrees and higher added focal lengths are slightly shorter. The method of the present invention can provide such significant improvements while allowing the user to see at a distance, at a medium distance, and at a close distance, using conventional PAL lenses. The invention further encompasses that depending on the wearer's pupil distance, the fit point, and the size of the cut frame edge, dynamic optics may need to be eccentric with respect to the enhanced region and, in some cases, horizontal. However, in all cases, when the dynamic optics is eccentric with respect to the enhancement region, it remains optically transferred to the region when the dynamic optics are activated. It should be noted that the vertical dimension of the edge or edge of the frame determines this amount of eccentricity in many cases (but not in all cases). 121818.doc -38- 200807055 The ophthalmic lens of the present invention allows optical transmission of 88% or higher. If an anti-reflective coating is applied to both surfaces of the ophthalmic lens, the optical transmission will exceed 90%. The optical efficiency of the ophthalmic lens of the present invention is 9% or better. The ophthalmic lens of the present invention can be coated by a variety of well known lens treatments, such as, for example, antireflective coatings, scratch resistant coatings, cushioning coatings, hydrophobic coatings, and ultraviolet coatings. The UV coating can be applied to an ophthalmic lens or dynamic optics. In embodiments where dynamic optics is liquid crystal based electroactive optics, the UV coating prevents the liquid crystal from being damaged by ultraviolet light, which may damage the liquid crystal over time. The ophthalmic lens of the present invention can also be edged to the desired shape of the eyeglass frame or drilled around its periphery to facilitate (by way of example only) installation in an edgeless spectacle frame. Additionally, it should be noted that the present invention encompasses all ophthalmic lenses; invisible eyes, intraocular lenses, corneal coverings, corneal inlays, and ophthalmic lenses. BRIEF DESCRIPTION OF THE DRAWINGS Figure 1A shows an embodiment of a low add power enhancement lens having a mating point and a enhancement area; Figure 1B shows the optical focus taken along the axis aa of the cross section of the lens of Figure 1A. Graph of degree 130; Figure 2A shows an embodiment of the invention having a low add power enhancement lens combined with greater dynamic optics, such that one of the dynamic optics is located in one of the lenses Figure 2B shows the combined lens of Figure 2A with a combined power produced by optical transmission of the dynamic optics and the enhanced area; Figure 3A shows a low add power enhancement lens and a dynamic optics In one embodiment of the invention, 121818.doc • 39, 200807055, the dynamic optics are placed such that a portion of the dynamic optics is above the mating point of the lens. Figure 3A shows that when dynamic optics is disabled, the power taken along the line of sight of the wearer's eye through the mating point provides the wearer with positive slanting distance vision, and Figure 3B shows the lens of Figure 3A. Figure 3B shows the corrected mid-range focus power provided to the wearer along the power taken from the wearer's eye through the line of sight of the mating point when the dynamic optics is activated; Figure 3C shows the lens of Figure 3A. Figure 3C shows that when dynamic optical activation is initiated, the power taken along the line of sight of the wearer's eye through the close-range viewing zone provides the wearer with corrected near-focus focus; Figure 4A shows the combination with dynamic optics. In an embodiment of the invention with a low add power enhancing lens, the dynamic optics is larger than the enhancement region and/or the channel and above the mating point of the lens; Figure 4B shows the fixed surface or region obtained by fixing along the axis AA of Figure 4A. Figure 4C shows the power provided by dynamic optics at startup along axis AA of Figure 4A; Figure 4D shows the dynamic electroactive optics taken along axis AA of Figure 4A The combined power of the fixed enhancement zone. Figure 4D shows the top and bottom distortion blending regions of the dynamic electroactive optics at the mating point and the enhanced read zone and the exterior of the channel; Figure 5A shows an embodiment of the invention in which dynamic optics are positioned in a low add power enhancing lens Figure 5B shows the power taken along axis AA of Figure 5A; Figures 6A-6C show various embodiments of the size of dynamic optics; and 121818.doc -40· 200807055 Figure 7A to Figure 7K show comparisons of existing A progressive astigmatism contour map of a progressive lens of the present state of the art and an embodiment of the invention comprising a low add power enhancement lens and dynamic optics. [Main component symbol description]

100 增進透鏡 110 配合點 120 增進區域 130 光焦度 200 低添加焦度增進透鏡 210 配合點 220 動態光學 230 組合光焦度 240 增進區域 250 頂部周邊邊緣 300 透鏡 310 增進區域 320 動態光學 330 校正遠距離視力 331 校正中距離聚焦焦度 332 校正近距離聚焦焦度 340 配戴者眼睛 400 低添加焦度增進透鏡 410 配合點 420 動態光學 121818.doc -41- 200807055100 Enhancement lens 110 Mating point 120 Enhancement area 130 Power 200 Low add power Enhancement lens 210 Mating point 220 Dynamic optics 230 Combining power 240 Enhancement area 250 Top peripheral edge 300 Lens 310 Enhancement area 320 Dynamic optics 330 Correcting long range 331 vision correction medium distance focus power 332 correction close focus focus 340 wearer eye 400 low add power enhancement lens 410 mating point 420 dynamic optics 121818.doc -41- 200807055

430 440 450 460 470 AA d D 增進區域及/或通道 讀取區 無用失真/頂部與底部失真摻合區 光焦度 光焦度 透鏡轴線 距離 距離430 440 450 460 470 AA d D Enhancement area and / or channel Reading area Unwanted distortion / top and bottom distortion blending area Power Power Power Lens Axis Distance Distance

121818.doc -42-121818.doc -42-

Claims (1)

200807055 十、申請專利範圍: L 種具有一配合點的用於一使用者之眼用透鏡,其包 含: ~ 一具有一通道之增進區域,其中該增進區域内具有一 添加焦度;及 一與該增進區域進行光學傳遞之動態光學,當該動態 、光學啟動時,該動態光學具有一光焦度, 其中該動悲光學具有一位於該配合點大約i 5 mm内之 頂部周邊邊緣。 2.如請求項丨之眼用透鏡,其中該添加焦度小於該使用者 之近觀察距離添加焦度。 3·如請求項1之眼用透鏡,其中該添加焦度為該近觀察距 離添加焦度之大約50%。 4.如請求項1之眼用透鏡,其中該添加焦度在該近觀察距 離添加焦度之大約30%與大約70%之間。 5·如請求項1之眼用透鏡,其中當加上該添加焦度時,該 _ 光焦度大體上等於該使用者之近觀察距離添加焦度。 6·如請求項1之眼用透鏡,其中該增進區域位於該透鏡之 一前表面上。 7·如請求項1之眼用透鏡,其中該增進區域位於該透鏡之 一後表面上。 8·如請求項1之眼用透鏡,其中該增進區域嵌於該透鏡 内。 9·如請求項1之眼用透鏡,其中該動態光學位於該透鏡之 121818.doc 200807055 一前表面上。 夏〇·如請求項1之眼用透鏡,其中該動態光學位於該透鏡之 一後表面上。 11 ·如請求項1之眼用透鏡,其中該動態光學嵌於該透鏡 内。 12.如請求項1之眼用透鏡,其中該動態光學係一電活性光 13 ·如請求項1之眼用透鏡,其中該動態光學係一凹凸透 ⑩ 鏡。 14·如請求項i之眼用透鏡,其中該動態光學係一流體透 鏡。 15 ·如請求項1之眼用透鏡,其中該動態光學係一具有至少 一個移動組件之可移動動態光學。 16·如請求項1之眼用透鏡,其中該動態光學係一氣體透 17·如清求項1之眼用透鏡’其中該動態光學係一具有一能 ® 夠變形之薄膜之薄膜透鏡。 18.如請求項1之眼用透鏡,其中該添加焦度在大約+0.50屈 光度與大約+1.50屈光度之間。 19·如請求項1之眼用透鏡,其中該光焦度在大約+0.50屈光 度與大約+2.25屈光度之間。 20·如請求項1之眼用透鏡,其中該動態光學具有一在大約 24 mm與大約40 mm之間的寬度。 21·如請求項1之眼用透鏡,其中該增進區域之該通道具有 121818.doc 200807055 一在大約11 mm與大約20 mm之間的長度。 22·如請求項1之眼用透鏡,其中該動態光學之一頂部周邊 邊緣之至少一部分位於該透鏡之該配合點上方。 23·如請求項1之眼用透鏡,其中該動態光學之一頂部周邊 邊緣位於該透鏡之該配合點上方大約0 mm與該動態光學 之垂直長度之大約一半之間。 24·如請求項1之眼用透鏡,其中該動態光學之一頂部周邊 邊緣位於該透鏡之該配合點上方該動態光學之該垂直長 度之大約八分之一與該動態光學之該垂直長度之大約八 刀之二之間0 25·如請求項1之眼用透鏡,其中該動態透鏡直至該使用者 之眼睛越過該動態光學之一頂部周邊邊緣才被啟動。 26·如請求項丨之眼用透鏡,其進一步包含一與該動態光學 相關聯之摻合區。 27如請求項1之眼用透鏡,其中該光焦度包含兩個或兩個 以上光焦度。 28·如請求項i之眼用透鏡,其中該光焦度包含一正焦度與 大體上無光焦度。 29·如請求項丨之眼用透鏡,其中該光焦度係可改變的。 3〇·如請求項1之眼用透鏡,其中該動態光學可被啟動與禁 用。 3 1 ·如請求項1之眼用透鏡,其中該動態光學與該增進區域 間隔。 / 32·如請求項1之眼用透鏡,其進一步包含一用於控制該光 121818.doc 200807055 焦度的感應器。 33·如請求項32之眼用透鏡,其中當該使用者超過一中距離 觀察時,該感應器禁用該動態光學。 34·如請求項32之眼用透鏡,其中當該使用者比一遠距離近 而觀察時,該感應器啟動該動態光學。 35.如請求項1之眼用透鏡,其中當該動態光學啟動時,當 * 該使用者透過該配合點觀察時,一中距離視力校正向該 使用者提供。 _ 36·如請求項1之眼用透鏡,其中當該動態光學禁用時,當 該使用者透過該配合點觀察時,一遠距離視力校正向該 使用者提供。 37·如請求項丨之眼用透鏡,其中該動態光學相對於該增進 區域偏心。 38·如請求項丨之眼用透鏡,其中該透鏡由一半修整毛达形 成0200807055 X. Patent Application Range: L types of ophthalmic lenses for a user having a matching point, comprising: ~ a promotion area having a channel, wherein the enhancement area has an added power; and The enhanced region is optically optically optically optically having a power when the dynamic, optically activated, wherein the dynamic optical has a top peripheral edge within about 5 mm of the mating point. 2. The ophthalmic lens of claim 3, wherein the added power is less than the proximity of the user to add power. 3. The ophthalmic lens of claim 1, wherein the added power is about 50% of the added power of the near viewing distance. 4. The ophthalmic lens of claim 1, wherein the add power is between about 30% and about 70% of the near-view distance add power. 5. The ophthalmic lens of claim 1, wherein when the added power is added, the _ power is substantially equal to the proximity of the user to add power. 6. The ophthalmic lens of claim 1, wherein the enhancement region is located on a front surface of the lens. 7. The ophthalmic lens of claim 1, wherein the enhancement region is located on a rear surface of the lens. 8. The ophthalmic lens of claim 1, wherein the enhancement region is embedded in the lens. 9. The ophthalmic lens of claim 1 wherein the dynamic optics is located on a front surface of the lens 121818.doc 200807055. The eye lens of claim 1, wherein the dynamic optics is located on a rear surface of the lens. 11. The ophthalmic lens of claim 1 wherein the dynamic optics are embedded within the lens. 12. The ophthalmic lens of claim 1, wherein the dynamic optical system is an electroactive light, such as the ophthalmic lens of claim 1, wherein the dynamic optical system is a concave-convex lens. 14. The ophthalmic lens of claim i, wherein the dynamic optics is a fluid lens. The ophthalmic lens of claim 1, wherein the dynamic optical system has movable dynamic optics of at least one moving component. The ophthalmic lens of claim 1, wherein the dynamic optical system is a gas lens of the invention, wherein the dynamic optical system has a thin film lens of a film capable of deforming. 18. The ophthalmic lens of claim 1 wherein the additive power is between about +0.50 diopters and about +1.50 diopters. 19. The ophthalmic lens of claim 1 wherein the power is between about +0.50 diopters and about +2.25 diopters. 20. The ophthalmic lens of claim 1 wherein the dynamic optics has a width of between about 24 mm and about 40 mm. 21. The ophthalmic lens of claim 1, wherein the channel of the enhancement zone has a length of between 12111.doc 200807055 and between about 11 mm and about 20 mm. 22. The ophthalmic lens of claim 1 wherein at least a portion of one of the top peripheral edges of the dynamic optics is above the mating point of the lens. The ophthalmic lens of claim 1, wherein a top peripheral edge of the dynamic optics is between about 0 mm above the mating point of the lens and about half of the vertical length of the dynamic optics. The ophthalmic lens of claim 1, wherein a top peripheral edge of the dynamic optics is located above the mating point of the lens by about one eighth of the vertical length of the dynamic optics and the vertical length of the dynamic optics Between approximately eight and eight knives, the ophthalmic lens of claim 1, wherein the dynamic lens is activated until the user's eye passes over a top peripheral edge of the dynamic optics. 26. The ophthalmic lens of claim 3, further comprising a blending zone associated with the dynamic optics. The ophthalmic lens of claim 1, wherein the power comprises two or more optical powers. 28. The ophthalmic lens of claim i, wherein the power comprises a positive power and substantially no power. 29. An ophthalmic lens as claimed in claim 1, wherein the power is changeable. 3. The ophthalmic lens of claim 1, wherein the dynamic optics can be activated and disabled. The ophthalmic lens of claim 1, wherein the dynamic optics are spaced apart from the enhancement region. / 32. The ophthalmic lens of claim 1, further comprising a sensor for controlling the power of the light 121818.doc 200807055. 33. The ophthalmic lens of claim 32, wherein the sensor disables the dynamic optics when the user observes over a medium distance. 34. The ophthalmic lens of claim 32, wherein the sensor activates the dynamic optics when the user is viewed closer than a distance. 35. The ophthalmic lens of claim 1, wherein when the dynamic optics is activated, a mid-range vision correction is provided to the user when the user views through the mating point. The ophthalmic lens of claim 1, wherein when the dynamic optics is disabled, a distance vision correction is provided to the user when the user views through the mating point. 37. The ophthalmic lens of claim 3, wherein the dynamic optics is eccentric with respect to the enhancement region. 38. The ophthalmic lens of claim ,, wherein the lens is formed by half trimming the hair 121818.doc121818.doc
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Families Citing this family (15)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US8523354B2 (en) * 2008-04-11 2013-09-03 Pixeloptics Inc. Electro-active diffractive lens and method for making the same
EP2577387A1 (en) * 2010-05-24 2013-04-10 Pixeloptics, Inc. Reduction of image jump
KR101385347B1 (en) 2010-06-30 2014-04-14 파나소닉 주식회사 Optical device
US9256077B2 (en) 2010-06-30 2016-02-09 Panasonic Intellectual Property Management Co., Ltd. Optical device
JP2012103312A (en) * 2010-11-08 2012-05-31 Seiko Epson Corp Progressive refractive power lens and design method thereof
DE102010055185B4 (en) 2010-12-20 2019-09-05 Carl Zeiss Vision International Gmbh Device with a spectacle lens with variable action and method for adjusting the effect of a spectacle lens
US20120212696A1 (en) * 2011-01-27 2012-08-23 Pixeloptics, Inc. Variable optical element comprising a liquid crystal alignment layer
JP2015513691A (en) 2012-02-07 2015-05-14 三井化学株式会社 Laser patterning of conductive films for electrically driven lenses
EP2642332B1 (en) * 2012-03-23 2015-05-06 Essilor International (Compagnie Générale d'Optique) A progressive addition lens for a wearer
US10690945B2 (en) * 2014-02-18 2020-06-23 Essilor International Method for optimizing an optical lens equipment for a wearer
DE102015219482B4 (en) * 2015-10-08 2017-07-13 Carl Zeiss Vision International Gmbh Spectacles with a spectacle lens with a movable lens segment
US20200026098A1 (en) * 2016-09-29 2020-01-23 Mitsui Chemicals, Inc. Lens, lens blank, and eyewear
CN115697249A (en) 2020-06-01 2023-02-03 应用奈米医材科技股份有限公司 Bifacial aspheric diffractive multifocal lenses and their manufacture and use
WO2022138060A1 (en) * 2020-12-25 2022-06-30 株式会社ニコン・エシロール Spectacle lens, method for designing spectacle lens, method for manufacturing spectacle lens, and device for designing spectacle lens
TWI813083B (en) * 2021-12-01 2023-08-21 長庚醫療財團法人基隆長庚紀念醫院 Method and lens for enhancing myopia control and method of manufacturing lens

Family Cites Families (19)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
GB2146791B (en) * 1983-09-16 1987-01-28 Suwa Seikosha Kk Progressive multifocal ophthalmic lens
JPS6338915A (en) * 1986-08-05 1988-02-19 Canon Inc Auto-focusing spectacles
US5124734A (en) * 1987-07-14 1992-06-23 Daniel Barnea Opthalmic lens
JP2665341B2 (en) * 1988-01-11 1997-10-22 オリンパス光学工業株式会社 Liquid crystal lens
JP2998233B2 (en) * 1991-02-28 2000-01-11 トヨタ自動車株式会社 Variable focus glasses
US5644374A (en) * 1992-02-03 1997-07-01 Seiko Epson Corporation Variable focus type eyesight correcting apparatus
US5359444A (en) * 1992-12-24 1994-10-25 Motorola, Inc. Auto-focusing optical apparatus
JP3196877B2 (en) * 1995-04-18 2001-08-06 ホーヤ株式会社 Progressive multifocal lens
US5774274A (en) * 1995-05-12 1998-06-30 Schachar; Ronald A. Variable focus lens by small changes of the equatorial lens diameter
US6540354B2 (en) * 1997-10-16 2003-04-01 Essilor International Multifocal ophthalmic 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
FR2807169B1 (en) * 2000-03-31 2002-06-07 Essilor Int METHOD OF MOUNTING OPHTHALMIC LENSES
US7019890B2 (en) * 2001-10-05 2006-03-28 E-Vision, Llc Hybrid electro-active lens
CN1653374A (en) * 2002-03-13 2005-08-10 E-视觉有限公司 Electro-optic lens with integrated components
DK1947501T3 (en) * 2002-08-09 2012-08-06 E Vision Llc Electroactive contact lens system
EP1654566B1 (en) * 2003-08-15 2015-02-25 E-Vision LLC Enhanced electro-active lens system
US7090348B2 (en) * 2003-10-28 2006-08-15 Essilor International (Compagnie Generale D'optique) Method for designing spectacle lenses taking into account an individual's head and eye movement
EP1735644A4 (en) * 2004-03-31 2010-01-27 Univ California Fluidic adaptive lens

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