TW546499B - An optical switch using total internal reflection and a method of switching signals using the same - Google Patents

An optical switch using total internal reflection and a method of switching signals using the same Download PDF

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TW546499B
TW546499B TW091118450A TW91118450A TW546499B TW 546499 B TW546499 B TW 546499B TW 091118450 A TW091118450 A TW 091118450A TW 91118450 A TW91118450 A TW 91118450A TW 546499 B TW546499 B TW 546499B
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Taiwan
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interface
conversion
signal
optical
electric field
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TW091118450A
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Chinese (zh)
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Jingyun Zhang
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Accelight Investments Inc
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Priority claimed from PCT/US2002/005461 external-priority patent/WO2002069008A1/en
Priority claimed from US10/081,911 external-priority patent/US20020136482A1/en
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Abstract

An optical switch is disclosed. The optical switch includes an optical signal transmitting electro-optic crystal having at least one first portion and at least one second portion. At least one of these portions is formed from a material which exhibits a change in index refraction upon the application of an electric field and the first and second portions define a switching interface therebetween. A signal source is provided for emitting a signal along an unguided beam path through the crystal, the unguided beam path intersecting the switching interface at an incident angle. An electric field generator is provided for generating an electrical field in at least one of the first and second portions of the crystal with the electrical field causing a change in an index of refraction for at least one of the first and second portions sufficient to create a critical angle at the interface smaller than the incident angle to reflect the signal off the interface. Thus, by switching the electric field generator off and on, the interface switches between being transparent and reflective to the optical signal to alter the unguided beam path through the crystal. A method of switching using such an electro-optic crystal is also disclosed.

Description

546499 A7 __B7_ 五、發明説明(1 ) 相關技藝之交叉參考 本申請案係請求較早於2001年2月22日提出申請之美 國專利臨時申請案第60/270,824號,標題為“由基於全内反 射之電光晶體所組成的光學開關(Optical Switch Comprised of Electro-Optic Crystal Based on Total Internal Reflection)”之權益0 發明之領域 本發明係有關於電信之領域,並更特定言之係有關於 基於光學之電信領域。更特定言之,本發明係有關於用於 在基於光學之電信網路中轉換光學信號的方法與裝置。 發明之背景 在電信系統中光學信號係變得更為重要。光學信號之 網路操作需要光學開關,以及供作業之光學開關矩陣。近 來重大的研究與發展貢獻係導向光學開關之發展。該研究 與發展之一途徑係研究控制材料之光學特性之方法,具選 擇性地如所需要引導或轉換光學信號。 儘管已完成複數之令人關注的技術發展’但迄今尚無 適當的解決方案。該其中一些發展係利用全内反射(TIR), 相關於該方式一光學信號反射離開一表面於該處在表面之 任一或雙側處材料之折射率具有變化。以下係為利用全内 反射之習知技藝的一些實例。 辑由氣泡產生所控制之全内反射IIIK1 於1991年1月29日授予J.L. Jackel之美國專利第 4,988,157號標題為,,利用氣泡之光學開關(0?以&1^如11 本紙張尺度適用中國國家標準(《s) A4規格(210X297公爱) (請先閲讀背面之注意事項再填寫本頁)546499 A7 __B7_ V. Description of the Invention (1) Cross Reference to Related Techniques This application is a request for US Patent Provisional Application No. 60 / 270,824, filed earlier on February 22, 2001, with the title "Using Rights of the "Optical Switch Comprised of Electro-Optic Crystal Based on Total Internal Reflection" 0 Field of Invention The present invention relates to the field of telecommunications, and more specifically, to optical-based Telecommunications. More specifically, the present invention relates to a method and apparatus for converting optical signals in an optical-based telecommunications network. BACKGROUND OF THE INVENTION Optical signal systems are becoming more important in telecommunication systems. Network operation of optical signals requires optical switches and a matrix of optical switches for operation. Recent significant research and development contributions have led to the development of optical switches. One way of this research and development is to study the methods of controlling the optical properties of materials, selectively directing or converting optical signals as needed. Although a number of interesting technological developments' have been completed, no appropriate solution has been available to date. Some of these developments make use of total internal reflection (TIR), which is related to the way that an optical signal reflects off a surface at either or both sides of the surface where the refractive index of the material changes. The following are some examples of conventional techniques using total internal reflection. US Patent No. 4,988,157 issued to JL Jackel on January 29, 1991 by Total Internal Reflection IIIK1 controlled by bubble generation is titled, Optical Switch Using Bubbles (0? To & 1 ^ such as 11 sheets Standards apply to Chinese national standards ("s) A4 specifications (210X297 public love) (Please read the precautions on the back before filling this page)

546499 A7 ____ —_Β7_ 五、發明説明(2 ) using bubbles)”中講授一種光學開關其係特別有用地作為 一雙穩交叉連接矩陣。平行輸入波導與平行輸出波導係垂 直地構成在基板上俾便交叉。一45度之狹縫係構成橫跨每 一交叉部分’並以具有與波導材料相符之折射率的流體填 注。於狹縫相鄰處配置電極並選擇性地活化以電解方式將 流體轉換成氣泡,從而破壞涵蓋狹缝之相符的折射率並致 使藉由狹縫反射光線而非傳播跨越狹縫。使用催化劑,相 對極性或是足夠尺寸及相同極性之脈衝係可用以破壞氣 泡。 於2000年4月25日授予J.E. Fouquet等人之美國專利第 6,055,344號標題為”製造具有垂直流體填注孔的一種全内 反射光學開關(Fabrication of a total internal reflection optical switch with vertical fluid fill-holes),,中講授一種基 於全内反射(TIR)光學波導轉換技術,係藉由熱量在折射率 相符之液體内產生氣泡所導致,其使光學能量能夠在波導 間轉換。 儘管令人關注的,該等產生氣泡之習知技藝裝置具有 複數之值得注意的限制,其係包括:低反應速度以及包含 流體之需求。流體的減少導致轉換失敗,因而係非令人滿 意的。 藉由折射率相符材料之機械移動而變化全内反射(ΤΠΟ 於1982年12月28日授予Hiroshi Terui等人之美國專利 第4,365,862號標題係為”光學開關(Optical Switch)”。該内 容講授一種波導光學開關其中全内反射(TIR)係藉由一在 6 (請先閲讀背面之注意事項再填寫本頁) 本紙張尺度適用中國國家標準(CNS) A4規格(210X297公釐) 546499 A7 _^_ B7 _ 五、發明説明(3 ) 基板與波導核心之間具有相符之折射率的可移動之電介質 晶片而執行。 於1986年4月15日授予J. Legrand之美國專利第 4,582,391號標題係為”光學開關以及該等開關之矩陣 (Optical switch, and a matrix of such switches)”。該專利内 容中講授一種光學開關,其係基於全内反射(TIR)受電磁控 制之移動構件用以改變水分存在。 於1995年8月22日授予A. Chandonnet等人之美國專利 第5,444,723號標題係為”光學開關以及Q-轉換雷射(Optical switch and Q-switched laser)”。該專利内容中講授一段具有 一核心以及環繞的纖殼之光纖藉由一塊件所支撐,該長度 之一部分於一侧邊上大體上已將纖殼去除而露出,以及一 折射率覆蓋擾動墊係安裝接近該部分並與之平行。一平移 裝置在一第一位置,其中該墊係距該部分夠遠以容許於該 部分中全内反射,與一第二位置,其中該墊係足夠接近該 部分以容許光線自核心散逸,之間將墊移動。 儘管令人關注,但該等機械移動方法無法達到足夠的 轉換速度,並遭受可能的機械故障導致轉換的損失。為了 該等緣故,該等機械移動設計係較不令人滿意的。 藉由半導體變化折射率而控制全内反射(TIR) 於1989年5月23曰授予Kunio Tada之美國專利第 4,832,430號標題係為”光學開關(Optical Switch)’,,該專利 内容中講授將電極配置在一種載子注入式(carrier injection type)光學開關之轉換區域的附近區域中,並且當 7 (請先閲讀背面之注意事項再填寫本頁) 本紙張尺度適用中國國家標準(CNS) A4規格(210X297公釐) 546499 A7 B7 五、發明説明(4 關閉開關時載子係快速移開通過該等電極。全内反射(TIR) 係經由半導體材料而受控制。 於1994年7月12日授予G.W. Taylor等人之美國專利第 5,329,137號標題係為”利用在量子井中的電荷儲存之整體 式全内反射光學開關(Integrated total internal reflection optical switch utilizing charge storage in a quantum well)”。該專利内容中講授一種光學開關其係包括一異質 接面電晶體具有一源極、一閘極、一突丘(mesa)、以及三 自動對準之波導。一光學能之源頭係施用至該其中之一波 導,並藉由從源極所施加之一電荷感應在閘極下折射率的 變化而在開關中產生全内反射。 儘管相對地快速並且無移動元件,但是製造該等開關 係為困難並價昂的,並且限制了轉換的幾何特性。因此, 該等半導體類型的開關係較不令人滿意的。 熱控制全内反射(TIR) 於1992年12月22日授予R.R· Hayes之美國專利第 5,173,956號標題係為”熱驅動光學開關的方法與裝置 (Thermally driven optical switch method and apparatus)’’ 〇 該專利内容中講授在二波導間之光學轉換,其係藉由電流 通過内導區域使其加熱並從而改變其之折射率利用共同之 纖殼内導區域而達成。藉由控制在二波導間電流光學轉 換,而可控制全内反射(TIR)開與關。 儘管令人關注,需花時間產生熱量的瞬間變化並因而 對大部分的應用而言該轉換係為太慢。 本紙張尺度適用中國國家標準(CNS) A4规格(210X297公釐) (請先閲讀背面之注意事項再填寫本頁)546499 A7 ____ —_Β7_ 5. In the description of the invention (2) using bubbles), an optical switch is particularly useful as a bistable cross-connect matrix. Parallel input waveguides and parallel output waveguides are vertically formed on the substrate. Cross. A 45-degree slit is formed across each intersection and is filled with a fluid with a refractive index consistent with the waveguide material. An electrode is placed adjacent to the slit and selectively activated to electrolyze the fluid Converts into bubbles, destroying the matching refractive index covering the slits and causing the slits to reflect light instead of propagating across the slits. With catalysts, pulses of relative polarity or a sufficient size and the same polarity can be used to destroy the bubbles. US Patent No. 6,055,344 issued to JE Fouquet et al. On April 25, 2000 entitled "Fabrication of a total internal reflection optical switch with vertical fluid fill-holes" ,, Teaches a technology based on total internal reflection (TIR) optical waveguide conversion technology, which uses heat to refract The bubble generation liquid inconsistencies caused, which is capable of converting the optical energy between the waveguides. Despite the concerns, these conventional technology devices for generating bubbles have a number of notable limitations, including: low reaction speeds and the need to include fluids. The reduction in fluid caused the conversion to fail and was therefore unsatisfactory. Total internal reflection is changed by mechanical movement of a refractive index conforming material (TIIO, U.S. Patent No. 4,365,862, issued to Hiroshi Terui et al. On December 28, 1982, is titled "Optical Switch". This content teaches a Waveguide optical switch in which the total internal reflection (TIR) is based on a 6 (Please read the precautions on the back before filling in this page) This paper size applies the Chinese National Standard (CNS) A4 specification (210X297 mm) 546499 A7 _ ^ _ B7 _ 5. Description of the invention (3) A movable dielectric wafer with a matching refractive index between the substrate and the waveguide core is executed. The title of US Patent No. 4,582,391 issued to J. Legrand on April 15, 1986 is "Optical switch, and a matrix of such switches". This patent teaches an optical switch, which is based on total internal reflection (TIR) electromagnetically controlled moving members to change moisture Existing. U.S. Patent No. 5,444,723 issued to A. Chandonnet et al. On August 22, 1995 is entitled "Optical Switch and Q-Switched Laser (Optical Switch and Q-switched laser) ". The patent teaches that a section of an optical fiber with a core and a surrounding fiber case is supported by a piece. One part of the length has been substantially removed from the fiber case on one side and exposed. And a refractive index covering disturbance pad is installed near and parallel to the part. A translation device is in a first position, wherein the pad is far enough from the part to allow total internal reflection in the part, and a second position , Where the pad is close enough to the part to allow the light to escape from the core and move the pad between them. Despite the concerns, these mechanical movement methods cannot achieve sufficient conversion speed and suffer from possible mechanical failures resulting in conversion losses For these reasons, these mechanical movement designs are less satisfactory. Controlling total internal reflection (TIR) by changing the refractive index of the semiconductor. US Patent No. 4,832,430, issued to Kunio Tada on May 23, 1989. "Optical Switch", this patent teaches the configuration of electrodes in a carrier injection type optical switch In the vicinity of the conversion area, and when 7 (Please read the precautions on the back before filling this page) This paper size applies to Chinese National Standard (CNS) A4 specifications (210X297 mm) 546499 A7 B7 V. Description of the invention (4 Close When switching, the carrier is quickly removed through these electrodes. Total internal reflection (TIR) is controlled via semiconductor materials. U.S. Patent No. 5,329,137, issued to GW Taylor et al. On July 12, 1994, is entitled "Integrated total internal reflection optical switch utilizing charge storage in quantum wells." a quantum well). " The patent teaches an optical switch including a heterojunction transistor having a source, a gate, a mesa, and three self-aligned waveguides. A source of optical energy is applied to one of the waveguides and generates total internal reflection in the switch by inducing a change in refractive index under the gate by a charge applied from the source. Although relatively fast and free of moving elements, manufacturing such switches is difficult and expensive, and limits the geometry of the transition. Therefore, the open relationship of these semiconductor types is less satisfactory. Thermal Controlled Total Internal Reflection (TIR) US Patent No. 5,173,956 issued to RR Hayes on December 22, 1992 is entitled "Thermally driven optical switch method and apparatus" 〇This patent teaches the optical conversion between the two waveguides, which is achieved by the current passing through the inner conduction region to heat it and thereby change its refractive index using the common fiber shell inner conduction region. By controlling the two waveguides The current can be converted optically, but the total internal reflection (TIR) can be controlled on and off. Despite the concerns, it takes time to generate instantaneous changes in heat and therefore the conversion is too slow for most applications. Applicable to China National Standard (CNS) A4 specification (210X297 mm) (Please read the precautions on the back before filling this page)

•、可I :線丨 546499 A7 B7_ 五、發明説明(5 ) 兔光學功率控制全内反射(TIR) 於1991年5月28日授予W.Chen之美國專利第5,018,842 號標題係為’,光學開關元件(Optical switch device)’’。該專 利内容中講授一種光學功率限制器及開關,在低光強度下 係為透明的而在高強度下係為不透明的,其係由一對由液 體薄膜所分開之直角三角稜鏡所組成,其之折射率係在感 應到開或關全内反射(TIR)之光學能而變化。然而,當網路 之其中之一所欲的設計基準係為涵蓋網路之一平面功率強 度時’強度相關開關並非極為實用。 控制晶體之極化與未極化區域而變化全内反射(ΤΠΟ 於1999年6月8日授予W.K· Bischel等人之美國專利第 5,911,018號標題係為”具有可誘導的折射率範圍與隔開之 輸出標的之低損失光學開關(Low loss optical switch with inducible refractive index boundary and spaced output target)”。該專利内容中講授一種光學波導轉換技術,其係 根據由電光控制針對光學顯示之應用之晶體之極化與未極 化區域所導致之全内反射(TIR)而執行。儘管令人關注,此 所講授之波導受限的方法係限制了實用性。 如上所示:(1)使用全内反射(TIR)的習知技藝主要重 點在於波導開關/應用;(2)複數種與全内反射(TIR)相關的 執行技術;(3)僅有一專利(第5,911,018號)係介紹由電光控 制晶體之極化與未極化區域所導致之全内反射(TIR),但係 針對光學顯示之應用。]Vlichikazu Kondo(於1986年10月21 曰授予其之美國專利第4,618,210號)講授,,當一全内反射 本紙張尺度適用中國國家標準(CNS) A4规格(210X297公釐) 9 (請先閲讀背面之注意事項再填寫本頁)• 、 可 I: Line 丨 546499 A7 B7_ V. Description of the Invention (5) Rabbit Optical Power Control Total Internal Reflection (TIR) No. 5,018,842 of US Patent No. 5,018,842 issued to W.Chen on May 28, 1991, titled ', Optical Switch element (Optical switch device) ''. This patent teaches an optical power limiter and switch. It is transparent at low light intensity and opaque at high intensity. It is composed of a pair of right-angled triangles separated by a liquid film. Its refractive index changes when it senses the optical energy of total internal reflection (TIR) on or off. However, when one of the desired design basis of the network is to cover the power strength of a plane of the network, the 'strength related switch is not very practical. Controlling the polarized and unpolarized regions of the crystal to change the total internal reflection (TiIIO, US Patent No. 5,911,018, issued to WK Bischel et al. On June 8, 1999, is entitled "has an inducible refractive index range and Low loss optical switch with inducible refractive index boundary and spaced output target ". This patent teaches an optical waveguide conversion technology based on electro-optic control for optical display applications. The crystal's polarized and unpolarized regions result in total internal reflection (TIR). Although interesting, the waveguide-limited method taught here has limited practicality. As shown above: (1) using total The main skills of the internal reflection (TIR) technology are waveguide switches / applications; (2) multiple implementation technologies related to total internal reflection (TIR); (3) only one patent (No. 5,911,018) is introduced by Electro-optic controls the total internal reflection (TIR) caused by the polarized and unpolarized regions of crystals, but for optical display applications.] Vlichikazu Kondo (granted on October 21, 1986 US Patent No. 4,618,210) teaches ,, when a total internal reflection within this paper scale applicable Chinese National Standard (CNS) A4 size (210X297 mm) 9 (Please read the back of the precautions to fill out this page)

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發明説明 (TIR)開關需要一相當可觀之交叉角度以獲得足夠低 話時,需要一大體上實用之電壓。因為通常建橋一〜串 及高速驅動電路係為困難的,所以一全内反射(TI汉)0 不適於高速轉換。” 關教 換言之,由電光控制晶體之極化與未極化區域所導敎 之折射率的變化係極小(大小為1〇-5-1〇-4)。因此,電光塊 決方法並無法對光學開關有所助益。 利用折射率之小的變化的一方式係經由電光控制曰 體之極化與未極化區域而產生複數之結構。此方法已用在 基於折射的光束掃描器,如在文獻資料,,利用在鈕酸鐘 (LiTaCh)中域反向的薄膜電光束偏轉器(Thhl film electro-optic beam deflector using domain reversal in LiTa03)’’中所說明,該文獻係由 q. Chen, Y. Chiu,D.N. Lambeth,Τ·Ε· Schlesinger,D.D· Stancil,在美國光學學會 (Optical Society of America)所舉辦之CTuN63, CLEO’93之 會議記錄(第196頁以及下列等)中所發表。並有二專利係說 明在不同的強度下執行該光學掃描器的方法:美國專利第 4,614,408號及美國專利第5,317,446號。在光學開關中使用 基於折射之光束掃描器的主要缺點在於針對一典型的設計 在相鄰頻道間之最大的轉換角度係約為0.6度,並且此轉換 角度係對操作電場之變化敏感。於光學掃描器中,可經由 多重極化與未極化區域選擇性地折射,針對掃描的目的變 化通過電光晶體之一光束的輸出位置。已建議使用折射特 性作為開關的一部分,但通過電光晶體之光學信號的折射 本紙張尺度適用中國國家標準(⑶幻A4規格(210><297公釐) 10 - ................裝…: 6請先聞讀背衙之注意事項再填寫本頁) 訂.................線丨 546499 A7 __B7_ 五、發明説明(7 ) 一般係為偏振相關(polarization dependent)。就其本身而 論,轉換光學信號中的TM及TE成分係在不同的角度下折 射,致使偏振不相關的轉換係為不可能的。可交替地,控 制信號分裂及轉動並將TM及TE成分結合成一偏振係為失 真且價昂。因此,折射並非為令人滿意的一種轉換方法。 一光學開關所需係為具有低插入損耗,能夠轉換不受偏振 與波長之支配,具有快速的轉換速度,較佳地不具有移動 元件並係為一簡單的結構。 發明之概要說明 本發明係提供一種用於光學轉換的裝置與方法。本發 明係包含複數之開關格式包括1 X2、1 X 3、1 X 4、2 X 2、 或4X4、或甚至是NXN。根據本發明,4X4開關格式係 被理解為一非阻塞交叉連接開關矩陣或是其可更為受限 制,並可於一大型光學開關形式中施用。 根據本發明,較佳之開關不具移動元件,並可在極快 速度(10_8〜1(Γ1()秒)下轉換,因為係藉由控制全内反射(TIR) 之狀況而執行轉換。本發明之另一特性在於串話(cross-talk) 係極低並且轉換對於工作電場之變化並不敏感。視開關格 式及設計方法而定,係可根據本發明建構一種具有簡單結 構、提供低插入損耗並且波長與偏振不相關的光學開關。 根據本發明,一構造簡單的1 XN的光學開關包含一輸 入光纖準直儀、一用於光束轉換的電光晶體以及至少二或 更多的輸出光纖準直儀。輸入光纖準直儀將在自由空間(亦 即,未受引導)中傳播的輸入光束準直通過一具有極化與未 本紙張尺度適用中國國家標準(CNS) A4規格(210X297公釐) 11 (請先閱讀背面之注意事項再填寫本頁) — .訂· 囔· 546499 A7 _^__ B7 五、發明説明(8 ) 極化部分的電光轉換晶體。於任何時候,其♦之一輸出光 纖準直儀在自由空間中接收轉換的光束並與相對應的輸出 光纖結合。 本發明同時包含一2 X 2光學開關其係包括二輸入光 纖準直儀、一用於光束轉換的電光晶體以及二輸出光纖準 直儀。該二輸入光纖準直儀將在自由空間中傳播的輸入光 束準直通過一具有簡單之極化與未極化部分的電光晶體。 該二輸出光纖準直儀之每一準直儀接收在自由空間中之任 一輸出光束,並視開關狀態分別地與相對應的光纖結合。 根據本發明之一進一步的觀點,2 X2開關係可包括光束分 離元件其係能夠將開關的整個尺寸顯著地降低。 本發明之轉換技術係利用全内反射(TIR)。超越令人感 興趣的已知光譜,亦即,一所欲轉換者,只要全内反射(TIR) 狀況維持在最長的波長,該開關可在所有的波長下作業, 並且轉換能力並不易受工作電場之變化的影響。再者,一 基於全内反射(TIR)的光學開關針對TM波在相鄰頻道間係 可達成5度至6度的轉換角度,針對TM及TE波在相鄰頻道 間係可達成2度至2.5度的轉換角度,並且該等角度係與工 作電場之變化無關,在複數的方面上係可放寬光學開關設 計之工程限制,並使其之製造更為容易。 參考以下詳細的說明結合伴隨的圖式可對本發明有 更佳的瞭解。 之簡要說明 現僅經由實例如以下之圖式中所示對本發明之較佳 本紙張尺度適用中國國家標準(QJS ) M規格(2〗〇><297公楚) 12 裝…..............tr..................線 (請先閱讀背面之注意事項再填寫本頁) 546499 A7 . B7 五、發明説明(9 ) 具體實施例作成參考資料: 第1(a)、1(b)圖係為本發明之第一具體實施例的概略視 圖,一1 X2開關係由具有簡單之極化與未極化結構的一光 電晶體所組成,根據偏振或未偏振光束之全内反射(TIR) 執行轉換; 第2圖係為本發明之第二具體實施例的概略視圖,一1 X 3開關其係由具有簡單之極化與未極化結構的一光電晶 體所組成,根據偏振或未偏振光束之全内反射(TIR)執行轉 換; 第3圖係為本發明之第三具體實施例的概略視圖,一1 X 4開關其係由具有簡單之極化與未極化結構的一光電晶 體所組成,根據偏振或未偏振光束之全内反射(TIR)執行轉 換; 第4圖係為本發明之第四具體實施例的概略視圖,一2 X 2開關其係由具有簡單之極化與未極化結構的一光電晶 體所組成,根據偏振或未偏振光束之全内反射(TIR)執行轉 換; 第5圖係為本發明之第五具體實施例的概略視圖,與 第4圖之開關類似的一2 X 2開關其係藉由二光束分離稜鏡 具有較短的軸尺寸; 第6圖係為本發明之第六具體實施例的概略視圖,一4 X 4交叉連接開關矩陣其係由具有簡單之極化與未極化結 構的一光電晶體所組成,根據偏振或未偏振光束之全内反 射(TIR)執行轉換; 13 (請先閲讀背面之注意事項再填寫本頁) 本紙張尺度適用中國國家標準(CNS) A4规格(210X297公釐) 546499 A7 _-_ B7 ____________ 五、發明説明(l〇 ) 第7圖係為本發明之第七具體實施例的概略視圖,一 4 X 4開關矩陣其係由具有簡單之極化與未極化結構的一光 電晶體所組成,根據偏振或未偏振光束之全内反射(TIR) 執行轉換;以及 第8圖係為本發明之第八具體實施例的概略視圖,與 第7圖之開關矩陣類似的一4 X 4開關矩陣係由四部分的電 光晶體取代二部分之電光晶體所組成。 K圭具體實施利之詳細說明 於此說明書中,以下的專有名詞具有以下的意義。全 内反射,或TIR思:f曰光學“號當其在一掠射角度(giancing angle)下碰擊具有較低之折射率之材料的一界面時之全反 射返回至#號傳輸材料的一部分。入射角意指介於垂直於 界面的一直線與光學信號之光束路徑間的角度。掠射角度 與入射角之總合等於90度》—準直的信號其中光射線係為 平行的,而一準直儀係為使光射線平行的一光學裝置。自 由空間意指光學信號於其中未受引導的任何環境並因而從 一 X引導的環境發射至一未受引導的環境。光學信號意指 任合形式的光學信號,無論是否為可見光譜,其係經調制 或用以運送資料。於本說明書中光學信號包含所有的電信 頻帶,涵蓋從850 nm至1620 mn,以及DWM與其他形式的 多路傳輸信號。於此說明書中,於複數之内文中使用專有 名詞界面。轉換界面意指一界面可在穿透與反射之間變 化。域界面係為一界面於該處在界面之一侧與另一側間可 將域反向,並係為轉換界面的一較佳形式。輸入/輸出界面 本紙張尺度翻巾闘家鮮(CNS) A4規格(210X297公釐) 14 (請先閲讀背面之注意事項再填寫本頁) /tr :線丨 546499 A7 I----~~^- 五、發明説明(11 ) 係與電光晶體的輸入與輸出表面相關。晶體/空氣界面典型 地係為一非轉換的反射界面。 第1圖係圖示本發明之第一具體實施例,亦即,1 X 2 光學開關(一般係以元件標號1〇〇標示)。開關1〇〇包含一輸 入光纖準直儀202、一電光晶體200、二輸出光纖準直儀 208、210以及位在晶體2〇〇之相對表面上之電極212、214(在 第1a圖中未顯示),在轉換期間係連接至電源208並接地 2 2 0。儘管係以準直儀作為較佳形式之光學裝置,但熟知此 技藝之人士應瞭解本發明包含所有的光學裝置用於將光學 信號發射進入自由空間中。因此,光學信號源可包括一同 調(coherent)的的光源(雷射)、一透鏡系統用於將光學信號 聚焦足以容許其穿過本發明之自由空間的未經引導的信號 路徑部分以及其他類似的結構。包括任何形式光學裝置係 可將光學#號加以處理有效地通過自由空間、通過之後將 說明的轉換結構、並接著返回將信號與波導結合,諸如光 纖。 | 於較佳的形式中,於一準直儀中一信號運送光纖端部 將準直的光學信號發射進入自由空間通過開關,並接著通 過一第二或是輸出準直儀捕捉未受引導的信號並再與另一 光纖結合。例如,準直之光束係較佳地涵蓋收斂的或是發 散的光束,因為準直的光束容許簡單並且容易的開關設計 並使其較易於達成全内反射(TIR)狀況。 電光晶體200係較佳地以鈕酸鋰(LiTa〇3)或是鈮酸鋰 (LiNb〇3)或是其他具有高電光係數的材料製成。僅管厚度 本紙張尺度適用中國國家標準(CNS) A4規格(2〗0χ297公爱) ~77~" (請先閲讀背面之注意事項再填寫本頁)DISCLOSURE OF THE INVENTION When a (TIR) switch requires a considerable cross angle to obtain sufficiently low speech, a substantially practical voltage is required. Because it is usually difficult to build a bridge and a high-speed drive circuit, a total internal reflection (TI Han) 0 is not suitable for high-speed conversion. In other words, Guan Jiao said that the change in the refractive index of the polarized and unpolarized regions induced by the electro-optic control crystal is extremely small (the size is 10-5-1-10). Therefore, the electro-optic block method cannot solve the problem. Optical switches are helpful. One way to take advantage of small changes in refractive index is to use electro-optic to control the polarized and unpolarized regions of the body to produce a complex structure. This method has been used in refraction-based beam scanners such as In the literature, it is described in "Thhl film electro-optic beam deflector using domain reversal in LiTa03", which is described by q. Chen , Y. Chiu, DN Lambeth, T.E. Schlesinger, DD Stancil, published in the conference proceedings of CTuN63, CLEO'93 (p.196 and below), organized by the Optical Society of America There are two patents describing methods of performing the optical scanner at different intensities: US Patent No. 4,614,408 and US Patent No. 5,317,446. The use of a refraction-based beam scanner in an optical switch The main disadvantage is that for a typical design, the maximum conversion angle between adjacent channels is about 0.6 degrees, and this conversion angle is sensitive to changes in the operating electric field. In optical scanners, multiple polarizations and polarities can be used. The selective area is refracted, and changes the output position of a light beam through an electro-optic crystal for the purpose of scanning. It has been suggested to use the refraction characteristic as a part of the switch. Magic A4 specifications (210 > < 297 mm) 10-...... installed ...: 6 Please read the notes on the back before filling this page) Order. ...... Line 丨 546499 A7 __B7_ V. Description of the Invention (7) Generally, it is polarization dependent. For its part, TM in the optical signal is converted And the TE component is refracted at different angles, making the polarization-independent conversion system impossible. Alternately, it is possible to control the signal splitting and rotation and combine the TM and TE components into a polarization system that is distorted and expensive. Therefore, Refraction is not a satisfactory one Conversion method. An optical switch needs to have low insertion loss, be able to convert without being dominated by polarization and wavelength, have a fast conversion speed, preferably have no moving elements, and be a simple structure. Summary of the Invention The present invention provides a device and method for optical conversion. The present invention includes a plurality of switch formats including 1 X2, 1 X 3, 1 X 4, 2 X 2, or 4X4, or even NXN. According to the present invention, the 4X4 switch format is understood as a non-blocking cross-connect switch matrix or it can be more restricted and can be applied in the form of a large optical switch. According to the present invention, the preferred switch does not have a moving element and can be switched at extremely fast speed (10_8 ~ 1 (Γ1 () seconds) because the switching is performed by controlling the condition of total internal reflection (TIR). Another characteristic is that the cross-talk is extremely low and the conversion is not sensitive to changes in the operating electric field. Depending on the switch format and design method, a simple structure, low insertion loss, and An optical switch whose wavelength is not related to polarization. According to the present invention, a simple structured 1 XN optical switch includes an input fiber collimator, an electro-optic crystal for beam conversion, and at least two or more output fiber collimators The input fiber collimator will collimate the input beam propagating in free space (that is, unguided) through a polarized and non-paper size applicable to China National Standard (CNS) A4 (210X297 mm) 11 (Please read the notes on the back before filling in this page) —. Order · 囔 · 546499 A7 _ ^ __ B7 V. Description of the invention (8) Electro-optic conversion crystal of polarized part. At any time One of its output fiber collimators receives the converted light beam in free space and combines it with the corresponding output fiber. The invention also includes a 2 X 2 optical switch, which includes two input fiber collimators, one for Beam-converted electro-optic crystal and two-output fiber collimator. The two-input fiber collimator collimates the input beam propagating in free space through an electro-optic crystal with simple polarized and unpolarized parts. The two-output Each collimator of the fiber optic collimator receives any output beam in free space and combines with the corresponding fiber depending on the switching state. According to a further aspect of the present invention, the 2 × 2 opening relationship may include a beam The separation element can significantly reduce the overall size of the switch. The conversion technology of the present invention utilizes total internal reflection (TIR). Beyond the known spectrum of interest, that is, a person who wants to convert, as long as the total internal The reflection (TIR) condition is maintained at the longest wavelength, the switch can operate at all wavelengths, and the conversion capability is not easily affected by changes in the operating electric field. Furthermore, An optical switch based on total internal reflection (TIR) can achieve a conversion angle of 5 to 6 degrees for TM waves between adjacent channels, and 2 to 2.5 degrees for TM and TE waves between adjacent channels. Conversion angles, and these angles have nothing to do with the changes of the working electric field, in terms of plural aspects, it can relax the engineering restrictions of the optical switch design and make it easier to manufacture. Refer to the following detailed description in conjunction with the accompanying drawings. A better understanding of the present invention. Brief description is now only by way of example, as shown in the following drawings. The preferred paper size of the present invention applies the Chinese National Standard (QJS) M specification (2). ≪ 297 (Chu) 12 packs .............. tr ........ line (please read the precautions on the back before filling in this (Page) 546499 A7. B7 V. Description of the invention (9) References to specific embodiments: Figures 1 (a) and 1 (b) are schematic views of the first specific embodiment of the present invention, with a 1 × 2 opening relationship Consists of a photoelectric crystal with a simple polarized and unpolarized structure, based on the total internal reflection (TIR) of a polarized or unpolarized beam Figure 2 is a schematic view of a second embodiment of the present invention. A 1 X 3 switch is composed of a photoelectric crystal with a simple polarized and unpolarized structure. The total internal reflection (TIR) of the light beam is converted. Figure 3 is a schematic view of a third embodiment of the present invention. A 1 X 4 switch is a photoelectric crystal with a simple polarized and unpolarized structure. The conversion is performed according to the total internal reflection (TIR) of the polarized or unpolarized light beam. Figure 4 is a schematic view of a fourth embodiment of the present invention. A 2 X 2 switch consists of a simple polarized and An unpolarized structure composed of a photoelectric crystal performs conversion based on the total internal reflection (TIR) of a polarized or unpolarized beam; FIG. 5 is a schematic view of a fifth embodiment of the present invention, and the switch of FIG. 4 A similar 2 X 2 switch has a shorter axis size by two beam splitting. Figure 6 is a schematic view of a sixth specific embodiment of the present invention. A 4 X 4 cross-connect switch matrix Simple and unpolarized The structure is composed of a photoelectric crystal, and the conversion is performed according to the total internal reflection (TIR) of the polarized or unpolarized beam; 13 (Please read the precautions on the back before filling this page) This paper size applies to China National Standard (CNS) A4 specifications (210X297 mm) 546499 A7 _-_ B7 ____________ V. Description of the invention (10) Figure 7 is a schematic view of a seventh specific embodiment of the present invention. A 4 X 4 switch matrix has a simple pole And a non-polarized structure composed of a photoelectric crystal, and performs conversion based on the total internal reflection (TIR) of a polarized or unpolarized beam; and FIG. 8 is a schematic view of an eighth specific embodiment of the present invention, and FIG. A 4 X 4 switch matrix similar to the switch matrix in the figure is composed of four parts of electro-optic crystals instead of two parts of electro-optic crystals. Detailed explanation of the specific implementation benefits of K. Kyu In this specification, the following proper nouns have the following meanings. Total internal reflection, or TIR thinking: f "optical" number when it hits an interface of a material with a lower refractive index at a glancing angle, the total reflection returns to a part of the # number transmission material The incident angle means the angle between the straight line perpendicular to the interface and the beam path of the optical signal. The sum of the grazing angle and the incident angle is equal to 90 degrees.—A collimated signal in which the light rays are parallel and one A collimator is an optical device that makes light rays parallel. Free space means any environment in which an optical signal is not guided and thus is emitted from an X-guided environment to an unguided environment. An optical signal means any Optical signals, whether in the visible spectrum or not, are modulated or used to carry data. In this specification, optical signals include all telecommunication frequency bands, covering 850 nm to 1620 mn, as well as DWM and other forms of multiplexing. Transmission signal. In this specification, the proper noun interface is used in the plural. The conversion interface means that an interface can change between penetration and reflection. The domain interface is an interface It can reverse the domain between one side and the other side of the interface, and it is a better form of the conversion interface. Input / output interface This paper size is turned into a paper (CNS) A4 size (210X297 mm) 14 (Please read the precautions on the back before filling this page) / tr: line 丨 546499 A7 I ---- ~~ ^-V. Description of the invention (11) It is related to the input and output surface of the electro-optic crystal. Crystal / The air interface is typically a non-transformed reflective interface. Figure 1 illustrates the first embodiment of the present invention, that is, a 1 X 2 optical switch (generally designated by the component number 100). Switch 1 〇〇 including an input fiber collimator 202, an electro-optic crystal 200, two output fiber collimator 208, 210, and electrodes 212, 214 on the opposite surface of the crystal 200 (not shown in Figure 1a) , Is connected to the power source 208 and grounded 2 2 0 during conversion. Although a collimator is the preferred form of optical device, those skilled in the art should understand that the present invention includes all optical devices for transmitting optical signals Into free space. Therefore, the optical signal source can It includes a coherent light source (laser), an unguided portion of the signal path used to focus the optical signal sufficient to allow it to pass through the free space of the present invention, and other similar structures. In any form The optical device can process the optical #signal effectively through free space, through a conversion structure which will be explained later, and then return to combine the signal with a waveguide, such as an optical fiber. | In a preferred form, in a collimator A signal-carrying fiber end transmits the collimated optical signal into a free space through a switch, and then captures the unguided signal through a second or output collimator and combines it with another fiber. For example, a collimated beam preferably covers a convergent or divergent beam because a collimated beam allows a simple and easy switch design and makes it easier to achieve a TIR condition. The electro-optic crystal 200 is preferably made of lithium button acid (LiTa03) or lithium niobate (LiNb03) or other materials having a high electro-optic coefficient. Regarding thickness only This paper size is applicable to China National Standard (CNS) A4 specification (2〗 0χ297 公 爱) ~ 77 ~ " (Please read the precautions on the back before filling this page)

546499 A7 B7 五、發明説明(l2 可加以變化,但是針對晶體較佳的厚度係約為0.4至0.5厘 米。在晶體的内部,一極化的部分204於一界面205處與一 未極化部分206接合。較佳地,視設計基準而定該一界面205 一般係與矩形形狀晶體的長邊緣平行,或是具有一些微的 角度。根據本發明,構成晶體的材料係為一顯現殘餘偏振 之鐵電的材料5並可精由使材料承受南的電壓場而受到電 氣地感應。應暸解的是全内反射(TIR)所需之電場的強度係 直接地與開關設計之複數之特性有關,包括電光晶體之材 料的選擇、極化/未極化部分之厚度以及在極化/未極化部 分間碰擊界面之光束的入射角。因此,本發明包含使用足 夠的電壓涵蓋於開關元件以獲得於此所說明之開關操作所 需或是所欲之全内反射(TIR)。於說明書中專有名詞”轉換 電場”意指一電場足以在與上述該等設計特性有關的界面 處產生全内反射(TIR)。 於晶體200中,僅有灰與白部分之其中的一部分係經 電氣極化的。因此,二區域204與206之域方向係相對的。 就一線性材料而言,折射率之變化△ η係可以下列之方程式 表示 Δ η = 0.5 X η3 X r X V/t 其中n係為晶體之未受到擾亂的折射率,r係為線性電 光係數,V係為控制電場的大小,以及t係為晶體的厚度。 電光係數r的符號以及△ η的符號係視所施加之電場相對於 極化之方向而定。該等特性可用以在一已知之控制電場下 將△ η之變化的影響最大化。現可對在晶體中使用極化與未 本紙張尺度適用中國國家標準(CNS) Α4規格(210X297公釐) 16 (請先閲讀背面之注意事項再填寫本頁) 裝丨 訂| 546499 A7 ^ B7 五、發明説明(I3 ) 極化結構的優點加以瞭解。 因為電光材料易於成為非等方性的,針對通常的光束 (s波)與特別光束(p波)n及r係可為不同數值。在一已知的工 作狀況下,通常一特別的光束(P波)所顯現之Δη係約為通 常的光束(s波)之Δη的三倍。如此係意味著就工作電壓與 全内反射(TIR)表面之長度而言,特別的光束(ρ波)係易於 達到全内反射(TIR)。再者,當僅針對特別的光束(ρ波)維 持全内反射(TIR)的需求,則本發明之開關係為一維持偏振 的開關。假若施用較高的工作電壓,或是進一步地減小入 射光束的掠角(grazing angle),因此全内反射(TIR)表面變 得較長,不僅針對特別的光束(P波)維持全内反射(TIR)的 需求,同時亦針對通常的光束(s波)維持全内反射(TIR)的需 求。因此,本發明進一步地包含一與偏振不相關的開關。 就熟知此技藝之人士而言,偏振不相關的開關對於光學信 號網路轉換方法係為一重要的優點。 第la圖顯示一準直的光束係由輸入準直儀202發射沿 著一平直的路徑203進入晶體200中。在未施以電場的狀況 下,光束將通過晶體200並自晶體退出,並如圖中所示進入 第一輸出準直儀208。假若具有經由電極212、214所施以之 電場,則以相同之方式施加圖中所示之晶體的白色區域具 有較高的折射率以及圖中所示之晶體的灰色區域具有較低 的折射率,並且一旦符合全内反射(TIR)狀況於是光束會在 界面205處反射,從晶體200退出並沿著路徑207傳播進入第 二準直儀210。因此,該界面係使用作為一供光學信號所用 17 (請先閲讀背面之注意事項再填寫本頁) 本紙張尺度適用中國國家標準(CNS) A4規格(210X297公釐) 546499 A7 、 B7 五、發明説明(l4 ) 的轉換界面。本發明包括施以一電場至界面的任一側,或 是更為理想地施加至界面的雙側,於該處界面的雙侧之域 係反向。以此方式較大的折射率變化係較僅於界面之一側 邊施以電場時更為容易地察覺。 根據本發明,此基於全内反射(TIR)的開關原理係同時 ’ 適用在通常的光束(s波)與特別的光束(p波)。然而,一般而 ^ 言通常的光束(S波)與特別的光束(P波)相較需要較高的電 場電壓或是一較小的掠角(grazing angle)以及較長的全内 反射(TIR)表面。因此,只要針對通常的光束(s波)達到全内 反射(TIR),同時針對特別的光束(p波)建立全内反射 (TIR)。以此方式,於本發明之此具體實施例中提供一偏振 不相關的1 X2光學開關。 折射率η係為波長的函數。就較長的波長而言,無論 是特別的光束或是通常的光束數值η會變得較小。當波長之 光線發射進入開關時,例如整個C及L頻帶從1520至1620 φ nm,只要針對最長的波長維持全内反射(TIR),則同時可 針對所有較短的波長維持全内反射(TIR)。因此,根據本發 明1 X2光學開關的功能係與波長不相關。現可瞭解,針對 在WDM/DWDM網路系統中轉換之應用此係為本發明之另 一引人注目並且重要的特性。第lb圖係為第la圖之具體實 施例的俯視圖。就圖式中可見,電極212、214係配置在相 對的側面上,如上所述地容許施以電場穿過電光晶體200。 第2圖係顯示本發明之第二具體實施例其係包含一 1 X 3光學開關,該開關係基於根據本發明之全内反射(TIR)所 本紙張尺度適用中國國家標準(CNS) A4規格(210X297公釐) 18 -----------------------裝------------------訂------------------線 (請先閲讀背面之注意事項再填寫本頁) 546499 A7 一 一 _ B7_ 五、發明説明(I5 ) 感應的電場。因此,如圖中可見,第2圖具有一輸入光纖準 直儀302、一件電光晶體300或電光晶體300之主體具有四極 化與未極化部分306、308、3 10及3 12以及三輸出光纖準直 儀318、320及322。於此具體實施例中,開關控制電極(未 顯示)具有二分離的部分,一控制左晶體主體而一控制右晶 體主體。如圖所示,一準直的光束係從輸入準直儀3〇2沿著 線304放射並且進入晶體300。於開關位置1,未施以電場並 且光束在晶體300中沿著平直的路徑傳播通過自由空間。信 號光束退出晶體並繼續沿著路徑304傳播直到進入輸出準 直儀318。於開關位置2,施以一控制電場至左電極以致在 晶體之區域306與308之間的界面處達到全内反射(TIR)。因 此,光束304係反射並沿著虛線314傳播並進入一第二輸出 準直儀320。於開關位置3,僅施以一控制電場至右侧電極 以致在光束反射之區域310與3 12之間的界面處達到全内反 射(TIR)。因此,反射的光束沿著路徑3 16退出並進入第三 輸出準直儀322。再者,由前述說明可瞭解,對於通常的光 束(s波)所達成的全内反射(TIR)亦可針對所有特別的光束 (P波)達成全内反射(TIR),使此開關為偏振不相關。同樣 地,針對最長的波長所達到的全内反射(TIR)意指開關係為 波長不相關。 第3圖係顯示本發明之第三具體實施例,再次係為基 於全内反射(TIR)之1 X 4光學開關的形式。如第3圖中所 示’具有一輸入光纖準直儀402、一第一件電光晶體400、 一第二件電光晶體4 01以及電光晶體之5極化與未極化部分 本紙張尺度適用中國國家標準(CNS) A4規格(210X297公釐) 19 (請先閲讀背面之注意事項再填寫本頁) 丨-訂· 囔, 546499 A7 _;_ B7_ 五、發明説明(l6 ) 406、408、410、412及414。同樣地,提供四輸出光纖準直 儀434、436、43 8以及440。與第2圖相似,於此具體實施例 中開關控制電極具有二分離的部分,一用於控制左晶體部 分400而一用於控制右晶體部分4〇i。因此,從準直儀4〇2 退出的一準直的光束沿著平直的路徑404傳播,並進入晶體 400中,接著進入晶體401並沿著線4〇4通過直到進入輸出準 直儀434。於開關位置2,施以一控制電場至電極在晶體4〇〇 中產生一電場以致在區域406與408之間的界面處達到全内 反射(TIR),於該處光束係反射偏離路徑4〇4。反射的光束 沿著路徑416進入一第二輸出準直儀436。於開關位置3,藉 由位在晶體401上的電極(未顯示)施以一控制電場以致在 光束反射之區域412與414之間的界面處達到全内反射 (TIR)。反射的光束自晶體401退出並沿著路徑418傳播進入 第三輸出準直儀438。於開關位置4,於晶體4〇〇及401中產 生電場的二電極上施以一控制電場,以致分別地在區域406 與408及410與414間之二界面處達到全内反射(TIR)。信號 光束在二表面處反射並因而從晶體4〇1退出,並沿著一路徑 420傳播進入第四輸出準直儀440。再者,當對於通常的光 束(s波)所達成的全内反射(TIR)亦可針對特別的光束(p波) 達成全内反射(TIR)。就前述具體實施例而言,同時可達到 波長之不相關性。 第4圖係顯示本發明之第四具體實施例,其係採用2 X 2光學開關的形式。不同於前述的具體實施例,第4圖之開 關具有一對稱的結構。如第4圖中所示,二輸入光纖準直儀 本紙張尺度適用中國國家標準(CNS) A4規格(210X297公釐) 20 (請先閱讀背面之注意事項再填寫本頁) 訂— 546499 A7 _:_____B7_ 五、發明説明(I7 ) 502及504係受引導朝向一電光晶體5〇〇。光學晶體500具有 一極化與未極化部分的夾合結構,其中部分522及520將部 分524夾合於其間。同時配置二輸出光纖準直儀538及540。 於此具體實施例中,一開關控制電極涵蓋部分520、522及 524之整個區域。區域524係較佳地為薄的為了當光束轉換 時將光束離散(walk-off)減至最小。換言之,區域524之厚 度越大則將準直儀53 8及540在個別之最佳的位置針對傳輸 及反射的光束利用最小的結合損耗分別地對準係更加困 難。另一方面,根據本發明區域524係足夠厚用以防止二反 射的表面不致發生該因在全内反射(TIR)模態下逐漸消失 的波所造成之光束洩漏,致使發生不能接受地降低光學信 號。 在開關位置1,未施加電場。於此情況下準直的光束 自輸入準直儀502放射沿著平直路徑506傳播穿過晶體 500,並沿著平直的路徑530傳播進入第一輸出準直儀538。 同樣地,一準直的光束可同時自輸入準直儀504放射沿著一 平直的路徑508傳播通過晶體500,並沿著平直的路徑532 進入第二輸出準直儀540。如圖所示,信號路徑508及506 交叉。然而,只要二輸入光束不具有相同之同調(coherent) 光源,則不會發生干涉否則會使開關性能退化。 於開關位置2,施以一控制電場以致在區域520與524 以及區域522與524之間的界面處達到全内反射(TIR)。於此 狀況下,來自準直儀502的光束係依循路徑506並受反射至 路徑532而進入準直儀540。同樣地,來自準直儀504的光束 本紙張尺度適用中國國家標準(CNS) A4規格(210X297公釐) -21 - (請先閲讀背面之注意事項再填寫本頁)546499 A7 B7 V. Description of the invention (12 can be changed, but the preferred thickness for the crystal is about 0.4 to 0.5 cm. In the crystal, a polarized portion 204 is at an interface 205 and an unpolarized portion 206. Preferably, depending on the design basis, the interface 205 is generally parallel to the long edges of the rectangular-shaped crystal or has some slight angles. According to the present invention, the material constituting the crystal is a material that exhibits residual polarization. The ferroelectric material 5 can be electrically induced by subjecting the material to a voltage field in the south. It should be understood that the strength of the electric field required for total internal reflection (TIR) is directly related to the complex characteristics of the switch design, The choice includes materials for electro-optic crystals, the thickness of the polarized / unpolarized portion, and the angle of incidence of the beam that strikes the interface between the polarized / unpolarized portions. Therefore, the present invention includes the use of sufficient voltage to cover the switching element to The total internal reflection (TIR) required or desired for the switching operation described here is obtained. The proper term "transformed electric field" in the description means that an electric field is sufficient to interact with these design features. A total internal reflection (TIR) occurs at the relevant interface. In the crystal 200, only a portion of the gray and white portions are electrically polarized. Therefore, the directions of the two regions 204 and 206 are opposite. Just one line For materials, the change in refractive index Δ η can be expressed by the following equation: Δ η = 0.5 X η 3 X r XV / t where n is the refractive index of the crystal without being disturbed, r is the linear electro-optic coefficient, and V is the In order to control the size of the electric field, and t is the thickness of the crystal. The sign of the electro-optic coefficient r and the sign of Δ η depend on the applied electric field relative to the direction of polarization. These characteristics can be used to control the electric field in a known The effect of the change of △ η is maximized. The Chinese National Standard (CNS) Α4 specification (210X297 mm) can now be applied to the use of polarization and the paper size in the crystal 16 (Please read the precautions on the back before filling (This page) Binding | 546499 A7 ^ B7 V. Description of the Invention (I3) The advantages of the polarized structure are understood. Because electro-optic materials are prone to become non-isotropic, they are targeted at ordinary light beams (s-waves) and special light beams (p wave ) N and r can be different values. Under a known operating condition, the Δη of a particular light beam (P wave) is usually about three times the Δη of a normal light beam (s wave). It means that in terms of the working voltage and the total internal reflection (TIR) surface length, a special light beam (ρ wave) is easy to reach the total internal reflection (TIR). Furthermore, when only the special light beam (ρ wave) is maintained, The requirement of internal reflection (TIR), the open relationship of the present invention is a switch to maintain polarization. If a higher working voltage is applied, or the grazing angle of the incident beam is further reduced, total internal reflection ( TIR) surface becomes longer, not only the need to maintain total internal reflection (TIR) for a special light beam (P wave), but also the need to maintain total internal reflection (TIR) for a normal light beam (s wave). Therefore, the present invention further includes a polarization-independent switch. For those skilled in the art, polarization-independent switching is an important advantage for optical signal network conversion methods. Figure la shows that a collimated light beam is emitted by the input collimator 202 into a crystal 200 along a straight path 203. Without the application of an electric field, the beam will pass through the crystal 200 and exit from the crystal, and enter the first output collimator 208 as shown in the figure. If there is an electric field applied through the electrodes 212, 214, the white areas of the crystals shown in the figure have the higher refractive index and the gray areas of the crystals shown in the same way have the lower refractive index. Once the TIR condition is met, the light beam will be reflected at the interface 205, exit from the crystal 200 and propagate along the path 207 into the second collimator 210. Therefore, this interface is used as an optical signal. 17 (Please read the precautions on the back before filling out this page.) This paper size applies to China National Standard (CNS) A4 (210X297 mm) 546499 A7, B7 V. Invention Description (l4) of the conversion interface. The invention includes applying an electric field to either side of the interface, or more ideally to both sides of the interface, where the domains of the two sides of the interface are reversed. Larger changes in refractive index in this way are easier to perceive than when an electric field is applied to only one side of the interface. According to the present invention, this switching principle based on total internal reflection (TIR) is applicable to both a normal light beam (s-wave) and a special light beam (p-wave). However, in general, a normal beam (S wave) requires a higher electric field voltage or a smaller grazing angle and a longer total internal reflection (TIR) than a special beam (P wave). )surface. Therefore, as long as total internal reflection (TIR) is achieved for a normal beam (s-wave), total internal reflection (TIR) is established for a special beam (p-wave). In this way, a polarization independent 1 X2 optical switch is provided in this embodiment of the invention. The refractive index η is a function of wavelength. For longer wavelengths, both the particular beam and the usual beam value η become smaller. When light of a wavelength enters the switch, for example, the entire C and L bands are from 1520 to 1620 φ nm, as long as total internal reflection (TIR) is maintained for the longest wavelength, total internal reflection (TIR) can be maintained for all shorter wavelengths at the same time ). Therefore, the functional system of the 1 X2 optical switch according to the present invention is independent of wavelength. It is understood that this is another attractive and important feature of the present invention for applications in WDM / DWDM network systems. Figure lb is a top view of the specific embodiment of Figure la. As can be seen in the figure, the electrodes 212 and 214 are arranged on opposite sides, and an electric field is allowed to pass through the electro-optic crystal 200 as described above. Figure 2 shows a second specific embodiment of the present invention, which includes a 1 X 3 optical switch. The opening relationship is based on the total internal reflection (TIR) according to the present invention. The paper size applies the Chinese National Standard (CNS) A4 specification. (210X297 mm) 18 ----------------------- install ------------------ order- ----------------- line (please read the precautions on the back before filling this page) 546499 A7 -11_ B7_ V. Description of the invention (I5) Electric field induced. Therefore, as can be seen in the figure, the second figure has an input fiber collimator 302, an electro-optic crystal 300, or the main body of the electro-optic crystal 300 having four polarized and unpolarized portions 306, 308, 3 10, and 3 12 and three outputs. Fiber collimators 318, 320, and 322. In this embodiment, the switch control electrode (not shown) has two separate parts, one controlling the left crystal body and one controlling the right crystal body. As shown, a collimated beam is emitted from the input collimator 30 along line 304 and enters crystal 300. At switch position 1, no electric field is applied and the light beam propagates through the free space along the straight path in the crystal 300. The signal beam exits the crystal and continues along path 304 until it enters output collimator 318. At switch position 2, a control electric field is applied to the left electrode so that total internal reflection (TIR) is reached at the interface between the regions 306 and 308 of the crystal. Therefore, the light beam 304 is reflected and propagates along the dotted line 314 and enters a second output collimator 320. At switch position 3, only a control electric field is applied to the right electrode so that total internal reflection (TIR) is reached at the interface between the areas 310 and 3 12 where the beam is reflected. Therefore, the reflected beam exits along path 3 16 and enters the third output collimator 322. Furthermore, as can be understood from the foregoing description, the total internal reflection (TIR) achieved with a normal light beam (s-wave) can also be achieved with respect to all special light beams (P-wave). This makes the switch polarized irrelevant. Similarly, the total internal reflection (TIR) achieved for the longest wavelengths means that the on relationship is that the wavelengths are uncorrelated. Figure 3 shows a third embodiment of the invention, again in the form of a 1 X 4 optical switch based on total internal reflection (TIR). As shown in Figure 3, 'with an input fiber collimator 402, a first electro-optic crystal 400, a second electro-optic crystal 401, and the 5 polarized and unpolarized parts of the electro-optic crystal. This paper is applicable to China National Standard (CNS) A4 Specification (210X297mm) 19 (Please read the notes on the back before filling this page) 丨 -Order · 囔, 546499 A7 _; _ B7_ V. Description of the Invention (l6) 406, 408, 410 , 412 and 414. Similarly, four-output fiber collimators 434, 436, 438, and 440 are provided. Similar to Figure 2, in this embodiment, the switch control electrode has two separate parts, one for controlling the left crystal part 400 and one for controlling the right crystal part 40i. Therefore, a collimated beam exiting from the collimator 402 travels along a straight path 404, and enters the crystal 400, then enters the crystal 401 and passes along the line 400 until it enters the output collimator 434 . At switch position 2, a controlled electric field is applied to the electrode to generate an electric field in the crystal 400 so that total internal reflection (TIR) is reached at the interface between the regions 406 and 408, where the beam reflection deviates from the path 4. 4. The reflected beam enters a second output collimator 436 along path 416. At switch position 3, an electrode (not shown) on the crystal 401 applies a control electric field so that total internal reflection (TIR) is achieved at the interface between the areas 412 and 414 where the beam reflects. The reflected beam exits the crystal 401 and travels along a path 418 into a third output collimator 438. At switch position 4, a control electric field is applied to the two electrodes that generate an electric field in crystals 400 and 401, so that total internal reflection (TIR) is achieved at the interface between areas 406 and 408 and 410 and 414, respectively. The signal beam is reflected at the two surfaces and thus exits from the crystal 401 and propagates along a path 420 into the fourth output collimator 440. Furthermore, when total internal reflection (TIR) is achieved with a normal light beam (s-wave), total internal reflection (TIR) can also be achieved with a special light beam (p-wave). In the foregoing specific embodiment, wavelength independence can be achieved at the same time. FIG. 4 shows a fourth specific embodiment of the present invention, which is in the form of a 2 × 2 optical switch. Unlike the foregoing specific embodiment, the switch of Fig. 4 has a symmetrical structure. As shown in Figure 4, the paper size of the two-input fiber collimator is applicable to the Chinese National Standard (CNS) A4 specification (210X297 mm) 20 (Please read the precautions on the back before filling this page) Order — 546499 A7 _ : _____B7_ 5. Description of the Invention (I7) 502 and 504 are guided toward an electro-optic crystal 500. The optical crystal 500 has a sandwich structure of polarized and unpolarized portions, wherein portions 522 and 520 sandwich a portion 524 therebetween. Configure two output fiber collimators 538 and 540 at the same time. In this embodiment, a switch control electrode covers the entire area of the portions 520, 522, and 524. Region 524 is preferably thin in order to minimize beam walk-off when the beam is switched. In other words, the greater the thickness of the region 524, the more difficult it is to align the collimators 53 8 and 540 at the individual optimal positions with the smallest combined loss for the transmitted and reflected beams, respectively. On the other hand, the region 524 according to the present invention is thick enough to prevent the second reflective surface from causing the beam leakage caused by the wave that gradually disappears in the TIR mode, resulting in an unacceptable reduction in optics. signal. In switch position 1, no electric field is applied. In this case, the collimated light beam is radiated from the input collimator 502 and propagates through the crystal 500 along the straight path 506, and propagates into the first output collimator 538 along the straight path 530. Similarly, a collimated light beam can be simultaneously emitted from the input collimator 504 and propagated through the crystal 500 along a straight path 508, and enter the second output collimator 540 along the straight path 532. As shown, the signal paths 508 and 506 cross. However, as long as the two input beams do not have the same coherent light source, no interference will occur or the switching performance will be degraded. At switch position 2, a control electric field is applied so that total internal reflection (TIR) is achieved at the interface between the regions 520 and 524 and the regions 522 and 524. Under this condition, the light beam from the collimator 502 follows the path 506 and is reflected to the path 532 to enter the collimator 540. Similarly, the light beam from the collimator 504 The paper size applies to the Chinese National Standard (CNS) A4 specification (210X297 mm) -21-(Please read the precautions on the back before filling this page)

546499 A7 -----一__ B7 ’ ^__ 五、發明説明(I8 ) 係依循路徑508係反射偏離介於區域520與524之間的界 面,並係沿著路徑530通過至輸出準直儀538。再者,對於 通常的光束(s波)所達成的全内反射(TIR)亦可針對特別的 光束(P波)建立全内反射(TIR)。同樣地,如之前所論及, 波長的不相關性係為此開關的一特性。 於第5圖中,係顯示本發明之第五具體實施例。於第* || 圖所概略圖示的光學路徑擴大了介於信號與界面間的角 度。如前所示,介於信號路徑與界面間之較佳的角度係約 為1度。該一小的角度係意指輸入準直儀與輸出準直儀需要 隔開遠離晶體部分,因此光束具有足夠的光線分歧性配合 並列的準直儀,或是如第5圖中所示可使用分隔器。因此, 第5圖係顯示一具有對稱的轉換結構的2 X 2光學開關,其 包括二光束分離稜鏡。光束分離稜鏡容許開關之軸向尺寸 減小’因為,不需針對足夠的光束分歧性而提供以配合互 相旁靠的準直儀。如圖所示,第5圖之具體實施例包括二輸 . 入光纖準直儀602及604、一位在輸入端的光束分離稜鏡 610、一具有第4圖之簡單的夾合結構的電光晶體6〇〇,一位 在輸出端的光束分離稜鏡630、以及二輸出光纖準直儀638 及640。於此例中,再一次開關控制電極覆蓋整個晶體區域 620、622以及624。 現可瞭解’於晶體6〇〇之輸入與輸出端處進口與出口 二表面以小的-/+角度加以拋光,該角度等於入射的光束掠 角,以致當光束退出晶體600時不會遭受任何折射。如此將 在通常光束(s波)與特別光束(p波)的另一類型之光束離散 本紙張尺度適用巾目國家標準(CNS) A4規格⑵〇><297公^〇 " -~22~〜546499 A7 ----- __ B7 '^ __ V. Description of the Invention (I8) follows the path 508 and the reflection deviates from the interface between the areas 520 and 524 and passes along the path 530 to the output collimation仪 538。 Instrument 538. Furthermore, the total internal reflection (TIR) achieved for a normal light beam (s-wave) can also be established for a special light beam (P-wave). Likewise, as discussed earlier, the wavelength irrelevance is a characteristic of this switch. FIG. 5 shows a fifth specific embodiment of the present invention. The optical path outlined in Figure * || expands the angle between the signal and the interface. As shown earlier, the preferred angle between the signal path and the interface is about 1 degree. This small angle means that the input collimator and the output collimator need to be separated from the crystal part, so the beam has sufficient light divergence to cooperate with the collimator in parallel, or it can be used as shown in Figure 5. Divider. Therefore, Fig. 5 shows a 2 X 2 optical switch with a symmetrical conversion structure, which includes two beam splitting chirps. Beam splitting allows the axial size of the switch to be reduced 'because there is no need to provide sufficient beam divergence to accommodate collimators that are side-by-side with each other. As shown in the figure, the specific embodiment of FIG. 5 includes two input optical fiber collimators 602 and 604, a beam splitter 610 at the input end, and an electro-optic crystal with a simple clamping structure of FIG. 4 At 600, one beam splitter 稜鏡 630 at the output end, and two output fiber collimators 638 and 640. In this example, the switching control electrodes again cover the entire crystal region 620, 622, and 624. It can now be understood that the surfaces of the inlet and outlet at the input and output ends of the crystal 600 are polished with a small-/ + angle, which is equal to the incident beam sweep angle, so that when the beam exits the crystal 600, it will not suffer any refraction. In this way, the ordinary beam (s-wave) and the special beam (p-wave) of another type of beam are discretized. This paper size applies the national standard (CNS) A4 specification. ⑵〇 > < 297 公 ^ 〇 "-~ 22 ~~

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(請先閱讀背面之注意事項再填窝本頁) t. 546499 A7 一 B7 五、發明説明(l9 ) (walk-off)消除,否則會導致附加的偏振相關損耗(PDL)。 根據本發明,介於二輸出頻道間的光束分離角度可約為1.2 度,該角度太小以致無法在短距離内將二輸出光束分離。 因此,使用二光束分離稜鏡改良分離性。以前述具體實施 例之相同方式執行轉換性能。當然,可以察知的是所示之 稜鏡610係僅為可能發生光束分離的其中一形式。可以使用 任一其他的反射表面,無論是單獨地或是共同地用以達到 所欲之光束路徑。在準直儀602及604係橫向地配置的狀況 下,僅需配置一反射表面。如此類型的稜鏡變化同時施用 在電光晶體600之輸出端上。再者,光束分離稜鏡之構想係 可應用在如第4圖中所示的具體實施例上,該電光晶體不具 有角度圓滑輸入及輸出表面。 第6圖係顯示本發明之一第六具體實施例的一種4 X 4 交叉連接開關矩陣。現由前述可瞭解,第6圖之具體實施例 係以如第一具體實施例之相同的方法操作,但具有稍微更 加複雜的幾何形狀以適合多重輸入與輸出。實質上,所顯 示的係為四光纖輸入準直儀720、722、724以及726,以及 七電光晶體部分702、704、706、708、712、714以及716。 同時所顯示的是四輸出光纖準直儀780、782、784以及786。 每一晶體部分具有極化與未極化部分。具有15對開關控制 電極,每一電極係配置覆蓋每一極化與未極化部分之界 面。因此,當準直的光束自輸入準直儀720、722、724以及 726放射並分別地沿著一平直的光線路徑730、732、734及 736傳播,其在界面處可選擇性地反射,當有需要時選擇性 23 (請先閲讀背面之注意事項再填寫本頁) 本紙張尺度適用中國國家標準(CNS) A4規格(210X297公釐) 546499 A7 B7 五、發明説明(2〇 地反射至每一輸出準直儀。因此,於任何時刻,開關控制 電極可選擇地開啟建立一全内反射(TIR)狀況。現可由第6 圖察知,此具體實施例在四輸入準直儀與四輸出準直儀之 間容許24非多餘的交叉連接結合。此係視為一種非阻塞的4 X 4開關。應注意的是光束730在晶體部分708於晶體空氣界 面處發生反射,導致在光束路徑770上反射至準直儀780。 因此,將所有的在晶體702、704、706中的開關置於關掉的 位置,光束路徑係為730至770。假若在晶體702、704及706 中的任一開關係為開啟,則光束路徑730係分別地反射至路 徑770至774或776 。 第7圖係顯示本發明之第七具體實施例一種4 X 4開關 矩陣,在某種程度上其係根據在第4圖中所揭露的概念。於 此具體實施例中,四輸入準直儀820、822、824及826係針 對電光晶體800、802。同時提供有四輸出光纖準直儀880、 882、884及886。如圖所示,電光晶體800、802係分別地具 有三與二極化及未極化部分,其每一部分之功能為一2X2 開關節點(switch node)。因此,具有五對開關控制電極, 而每一電極係配置涵蓋其中之一2 X 2極化與未極化部 分。於此觀念中,2X2極化與未極化部分如前述所說明係 視為一種夾合的結構。 準直的光束係自每一輸入準直儀820、822、824及826 放射分別地沿著平直的路徑830、832、834及836。沿著該 等光束路徑光線與五2 X 2開關節點交叉,同時通風至晶體 全内反射(TIR)表面。接著,光束沿著四輸出路徑光線870、 本紙張尺度適用中國國家標準(CNS) A4規格(210X297公釐) 24 (請先閲讀背面之注意事項再填寫本頁)------------------------ Install! (Please read the precautions on the back before filling in this page) t. 546499 A7 a B7 5. The invention description (l9) (walk-off) is eliminated, otherwise it will cause additional polarization dependent loss (PDL). According to the present invention, the beam splitting angle between the two output channels may be about 1.2 degrees, which is too small to split the two output beams in a short distance. Therefore, two-beam splitting is used to improve the separability. Conversion performance is performed in the same manner as the foregoing specific embodiment. Of course, it can be seen that the 稜鏡 610 shown is just one of the possible forms of beam splitting. Any other reflective surface can be used, either individually or collectively, to achieve the desired beam path. In the case where the collimators 602 and 604 are arranged laterally, only one reflecting surface is required. This type of chirp change is applied to the output of the electro-optic crystal 600 at the same time. Furthermore, the concept of beam splitting can be applied to the specific embodiment shown in Fig. 4. The electro-optic crystal does not have a smooth input and output surface at an angle. FIG. 6 shows a 4 X 4 cross-connect switch matrix according to a sixth embodiment of the present invention. As can be understood from the foregoing, the specific embodiment of FIG. 6 operates in the same manner as the first specific embodiment, but has a slightly more complex geometry to accommodate multiple inputs and outputs. Essentially, the systems shown are four-fiber input collimators 720, 722, 724, and 726, and seven electro-optic crystal sections 702, 704, 706, 708, 712, 714, and 716. Also shown are four-output fiber collimators 780, 782, 784, and 786. Each crystal portion has a polarized and an unpolarized portion. There are 15 pairs of switch control electrodes, and each electrode system is configured to cover the interface between each polarized and unpolarized part. Therefore, when a collimated beam is emitted from the input collimators 720, 722, 724, and 726 and propagates along a straight ray path 730, 732, 734, and 736, respectively, it can be selectively reflected at the interface, Optional 23 when necessary (please read the notes on the back before filling this page) This paper size applies the Chinese National Standard (CNS) A4 specification (210X297 mm) 546499 A7 B7 V. Description of the invention (20 ° reflection to Each output collimator. Therefore, at any time, the switch control electrode can be selectively turned on to establish a total internal reflection (TIR) condition. It can be seen from Figure 6 that this specific embodiment is a four-input collimator and a four-output collimator. Collimators allow 24 non-redundant cross-connect combinations. This is considered a non-blocking 4 X 4 switch. It should be noted that the beam 730 is reflected at the crystal portion 708 at the crystal-air interface, resulting in a beam path 770 Up reflection to collimator 780. Therefore, set all switches in crystals 702, 704, 706 to the off position, the beam path is 730 to 770. If any of crystals 702, 704, and 706 Open relationship for open On, the beam path 730 is reflected to the paths 770 to 774 or 776, respectively. Figure 7 shows a seventh specific embodiment of the present invention, a 4 X 4 switch matrix, to some extent according to Figure 4 In this specific embodiment, the four-input collimators 820, 822, 824, and 826 are for electro-optic crystals 800, 802. Four-output fiber collimators 880, 882, 884, and 886 are also provided. As shown in the figure, the electro-optic crystals 800 and 802 respectively have three and two polarized and unpolarized parts, each of which functions as a 2X2 switch node. Therefore, there are five pairs of switch control electrodes, and Each electrode system configuration includes one of the 2 X 2 polarized and unpolarized portions. In this concept, the 2X 2 polarized and unpolarized portions are considered as a sandwich structure as described above. Collimated beam Radiation from each input collimator 820, 822, 824, and 826 follows a straight path 830, 832, 834, and 836, respectively. Along these beam paths, the light crosses the five 2 X 2 switch nodes and is ventilated at the same time. To the total internal reflection (TIR) surface of the crystal. Light 870 along the four output paths, this paper size applies Chinese National Standard (CNS) A4 specifications (210X297 mm) 24 (Please read the precautions on the back before filling this page)

546499 A7 _^___ B7____ 五、發明説明(Μ ) 872、874及876退出晶體802,分別地進入四輸出準直儀 880、882、884及886。於任何時間,從零至五對開關控制 電極可開啟建立一全内反射(TIR)狀況。如此導致在四輸入 準直儀與四輸出準直儀之間24非多餘的交叉連接結合。與 前述之具體實施例相較,現可暸解此4X4非阻塞形式具有 較少的元件並因而轉換機構具有較少的多餘物。 第8圖係顯示本發明之第八具體實施例,係為一4 X 4 開關矩陣的形式。如圖所示,四輸入光纖準直儀920、922、 924以及926係受引導朝向電光晶體902、904、906及908之 四部分。同時提供四輸出光纖準直儀980、982、984及986。 晶體902具有一極化與一未極化部分,晶體部分904及908 分別地具有二極化與未極化部分。每一極化與未極化部分 的功能如同前述說明之一2 X 2開關節點。於此具體實施例 中,較佳地具有五對開關控制電極,帶有一電極配置涵蓋 每一2 X 2極化與未極化部分。準直的光束自輸入準直儀 920、922、924、926放射,並分別地沿著一平直的路徑93〇、 932、934及936傳播。沿著該四路徑如圖所示光束與五2 X 2 開關節點及二空氣晶體全内反射(TIR)表面交叉,並沿著四 輸出路徑光線970、972、974及976退出晶體進入四輸出準 直儀980、982、984及986。因此,從零至五對開關控制電 極可開啟導致全内反射(TIR)狀況,致使在四輸入準直儀與 四輸出準直儀之間24非多餘的交叉連接結合。 與第六具體實施例相較,第八具體實施例具有較少件 的電光晶體。另一方面,與第七具體實施例相較,第八且 本紙張尺度適用中國國家標準(CNS) A4規格(210X297公釐) 25 ------------------------ (請先閲讀背面之注意事項再填寫本頁) .-、可| 546499 A7 - ~~ -~^__ 五、發明説明(22 ) — 一- 體實施例具有多於二件的電光晶體。視製造技術與成本而 選擇使用較少或是較多件的電光晶體。例如,儘管在第6 圖之具體實施例中使用較多的晶體部分,但每一部分係為 簡單的結構。應瞭解的是本發明包含具有如圖所示之刀極化/ 未極化形式的整體的晶體結構,以及由—或更多分離的晶 體部分在操作上-個接著一個地配置所製成的組合的晶: 結構。第六、七以及第八具體實施例所有係針對—4 X 4 開關矩陣所提出之設計方法,其係可具有偏振不相關轉換 與波長不相關轉換之特性。 現可進一步地瞭解本發明之開關的製造同時係為簡 單與谷易。可以分開地構成極化/未極化部分,並接著藉由 任何適當的構件,諸如黏著劑或是類似物,以機械方式附 裝。當然,任何該扣件沿著反射與未反射光束路徑不致與 光學特性相干擾。可交替地,一單件電光晶體可加以修改 藉由施以一極化的電極與電場沿著一界面構成極化/未極 化部分。 儘管前述說明已針對本發明之不同的較佳形式與具 體實施例,本發明之範疇並未限制於此並且充分地擴展至 附加之申請專利範圍的範疇。可針對本發明作不同的修改 與變化而不致背離申請專利範圍之廣泛的範疇。已於上述 論及的一些修改以及其他的說明對於熟知此技藝之人士而 言係為顯而易見的。例如,可以具有利用相同之全内反射 (TIR)自由空間轉換原理之不同的幾何形狀。因此,本發明 包含對稱的NXN開關形式以及非對稱的NXM開關形式。 本紙張尺度適用中國國家標準(CNS) Α4規格(210X297公釐) 26 (請先閲讀背面之注意事項再填寫本頁) ------....... :線丨 546499 A7 ___B7 五、發明説明(23 ) 元件標號對照 100··· 1X2光學開關 200···電光晶體 202…輸入光纖準直儀 203…平直的路徑 204···極化的部分 205…界面 206···未極化的部分 207…路徑 208···輸出光鐵準直儀 210…輸出光纖準直儀 212…電極 214…電極 218…電源 220…接地 300···電光晶體 302…輸入光纖準直儀 304…光束 306…極化與未極化部分 308···極化與未極化部分 310…極化與未極化部分 312…極化與未極化部分 314…虛線 316…路徑 318···輸出光纖準直儀 320…輸出光纖準直儀 322…輸出光纖準直儀 400···第一件電光晶體 401···第二件電光晶體 402…輸入光纖準直儀 404…平直的路徑 406…極化與未極化部分 408···極化與未極化部分 410···極化與未極化部分 412···極化與未極化部分 414···極化與未極化部分 416…路徑 420…路徑 434…輸出光纖準直儀 436…輸出光纖準直儀 438···輸出光纖準直儀 440···輸出光纖準直儀 500···電光晶體 502…輸入光纖準直儀 504…輸入光纖準直儀 (請先閲讀背面之注意事項再填寫本頁) 27 本紙張尺度適用中國國家標準(CNS) A4規格(210X297公釐) 546499 A7 B7 五、發明説明(24 506…平直的路徑 714·· •電光晶體部分 508···平直的路徑 716·· •電光晶體部分 520…部分 720.· •光纖輸入準直儀 522…部分 722- •光纖輸入準直儀 524…部分 724·· •光纖輸入準直儀 530…平直的路徑 726" •光纖輸入準直儀 532…路徑 730" •光線路徑 538···輸出光纖準直儀 732·· •光線路徑 540···輸出光纖準直儀 734·· •光線路徑 600···電光晶體 736·· •光線路徑 602…輸入光纖準直儀 770" •路徑 604…輸入光纖準直儀 774·· •路徑 610···光束分離稜鏡 776·· •路徑 620···晶體部分 780" •輸出光纖準直儀 622···晶體部分 782" •輸出光纖準直儀 624···晶體部分 784.· •輸出光纖準直儀 630…光束分離稜鏡 786" •輸出光纖準直儀 638···輸出光纖準直儀 800·· •電光晶體 640···輸出光纖準直儀 802·· •電光晶體 702···電光晶體部分 820" •輸入準直儀 704…電光晶體部分 822·· •輸入準直儀 706···電光晶體部分 824·· •輸入準直儀 708···電光晶體部分 826" •輸入準直儀 712…電光晶體部分 830" •平直的路徑 (請先閲讀背面之注意事項再填寫本頁) 本紙張尺度適用中國國家標準(CNS) A4規格(210X297公釐) 28 546499 A7 B7 五、發明説明(25 ) 832" •平直的路徑 922…輸入光纖準直儀 834- •平直的路徑 924…輸入光纖準直儀 836" •平直的路徑 926…輸入光纖準直儀 870" •輸出路徑光線 930…平直的路徑 872·· •輸出路徑光線 932…平直的路徑 874·· •輸出路徑光線 934…平直的路徑 876" •輸出路徑光線 936…平直的路徑 880" •輸出光纖準直儀 970…輸出路徑光線 882" •輸出光纖準直儀 972…輸出路徑光線 884" •輸出光纖準直儀 974…輸出路徑光線 886" •輸出光纖準直儀 976…輸出路徑光線 902·· •電光晶體 980…輸出光纖準直儀 904" •電光晶體 982…輸出光纖準直儀 906" •電光晶體 984…輸出光纖準直儀 908“ 920·· •電光晶體 •輸入光纖準直儀 986…輸出光纖準直儀 (請先閱讀背面之注意事項再填寫本頁) 本紙張尺度適用中國國家標準(CNS) A4規格(210X297公釐) 29546499 A7 _ ^ ___ B7____ 5. Description of the Invention (M) 872, 874, and 876 exit the crystal 802 and enter the four-output collimators 880, 882, 884, and 886, respectively. At any time, from zero to five pairs of switch control electrodes can be turned on to establish a total internal reflection (TIR) condition. This results in a combination of 24 non-redundant cross-connections between the four-input collimator and the four-output collimator. Compared with the foregoing specific embodiment, it can now be understood that this 4X4 non-blocking version has fewer components and thus the switching mechanism has less excess. FIG. 8 shows an eighth specific embodiment of the present invention, which is in the form of a 4 × 4 switch matrix. As shown, the four-input fiber collimators 920, 922, 924, and 926 are directed toward the four parts of the electro-optic crystals 902, 904, 906, and 908. Four-output fiber collimators 980, 982, 984, and 986 are also available. The crystal 902 has one polarized and one unpolarized portion, and the crystal portions 904 and 908 have two polarized and unpolarized portions, respectively. Each polarized and unpolarized section functions as a 2 X 2 switch node as described previously. In this embodiment, there are preferably five pairs of switch control electrodes with an electrode configuration covering each 2 X 2 polarized and unpolarized portion. The collimated light beams are emitted from the input collimators 920, 922, 924, 926, and propagate along a straight path 930, 932, 934, and 936, respectively. Along the four paths, the light beam intersects with the 5 2 X 2 switch node and the total internal reflection (TIR) surface of the two air crystals, and exits the crystal along the four output paths into the four output standard. Straight instruments 980, 982, 984 and 986. Therefore, from zero to five pairs of switch control electrodes can be turned on resulting in a total internal reflection (TIR) condition, resulting in a combination of 24 non-redundant cross-connections between the four-input collimator and the four-output collimator. Compared with the sixth embodiment, the eighth embodiment has fewer electro-optic crystals. On the other hand, compared with the seventh specific embodiment, the eighth and this paper size applies the Chinese National Standard (CNS) A4 specification (210X297 mm) 25 ---------------- -------- (Please read the notes on the back before filling out this page) .- 、 may | 546499 A7-~~-~ ^ __ 5. Description of the Invention (22) — One-There are many embodiments Two electro-optic crystals. Depending on manufacturing technology and cost, fewer or more electro-optic crystals are used. For example, although a large number of crystal portions are used in the specific embodiment of Fig. 6, each portion has a simple structure. It should be understood that the present invention encompasses a monolithic crystal structure having a knife-polarized / unpolarized form as shown in the figure, and is made of-or more separated crystal portions operatively arranged one after the other Combined crystal: structure. The sixth, seventh, and eighth embodiments are all design methods proposed for the -4 X 4 switch matrix, which can have the characteristics of polarization-independent conversion and wavelength-independent conversion. It can be further understood that the manufacturing of the switch of the present invention is simple and simple. The polarized / unpolarized portions may be separately formed and then mechanically attached by any appropriate member such as an adhesive or the like. Of course, any such fastener along the path of the reflected and unreflected beams does not interfere with the optical characteristics. Alternatively, a single piece of electro-optic crystal can be modified by applying a polarized electrode and an electric field to form a polarized / unpolarized portion along an interface. Although the foregoing description has been directed to different preferred forms and specific embodiments of the present invention, the scope of the present invention is not limited thereto and fully extends to the scope of the appended patent application. Various modifications and changes can be made to the present invention without departing from the broad scope of the scope of patent application. The modifications and other descriptions discussed above are obvious to those skilled in the art. For example, there may be different geometries that utilize the same principle of total internal reflection (TIR) free space conversion. Therefore, the present invention includes a symmetric NXN switch form and an asymmetric NXM switch form. This paper size applies Chinese National Standard (CNS) Α4 specification (210X297 mm) 26 (Please read the precautions on the back before filling this page) ------.......: line 丨 546499 A7 ___B7 V. Description of the invention (23) Component reference number 100 ... 1X2 optical switch 200 ... electro-optic crystal 202 ... input fiber collimator 203 ... straight path 204 ... polarized portion 205 ... interface 206 ... Unpolarized section 207 ... Path 208 ... Output light iron collimator 210 ... Output fiber collimator 212 ... Electrode 214 ... Electrode 218 ... Power supply 220 ... Ground 300 ... Electro-optic crystal 302 ... Input fiber collimation Instrument 304 ... beam 306 ... polarized and unpolarized portion 308 ... polarized and unpolarized portion 310 ... polarized and unpolarized portion 312 ... polarized and unpolarized portion 314 ... dashed line 316 ... path 318 ... ·· Output fiber collimator 320 ... Output fiber collimator 322 ... Output fiber collimator 400 ··· The first electro-optic crystal 401 ··· Second electro-optic crystal 402 ... Input fiber collimator 404 ... Straight Path 406 ... polarized and unpolarized part 408 ... polarized and unpolarized part 410 ... polarized and unpolarized Polarized section 412 ... Polarized and unpolarized section 414 ... Polarized and unpolarized section 416 ... Path 420 ... Path 434 ... Output fiber collimator 436 ... Output fiber collimator 438 ... Output Optical fiber collimator 440 ... Output fiber collimator 500 ... Electro-optic crystal 502 ... Input fiber collimator 504 ... Input fiber collimator (Please read the precautions on the back before filling this page) 27 Paper dimensions Applicable to China National Standard (CNS) A4 specification (210X297 mm) 546499 A7 B7 V. Description of the invention (24 506… Straight path 714 ·· • Electro-optic crystal part 508 ··· Straight path 716 ·· • Electro-optic crystal Part 520 ... Part 720 ... • Fiber Input Collimator 522 ... Part 722- • Fiber Input Collimator 524 ... Part 724 ... • Fiber Input Collimator 530 ... Straight Path 726 " • Fiber Input Collimator 532… path 730 " • ray path 538 ··· output fiber collimator 732 ··· ray path 540 ··· output fiber collimator 734 ··· ray path 600 ··· electro-optic crystal 736 ··· ray path 602… input fiber collimation 770 " • Path 604… input fiber collimator 774 ·· • path 610 ··· beam splitter 稜鏡 776 ··· path 620 ··· crystal part 780 " • output fiber collimator 622 ··· crystal part 782 & quot • Output Fiber Collimator 624 ··· Crystal Part 784. ·· Output Fiber Collimator 630… Beam Splitter 稜鏡 786 " • Output Fiber Collimator 638 ··· Output Fiber Collimator 800 ·· Crystal 640 ·· Output fiber collimator 802 ·· Electro-optic crystal 702 ·· Electro-optic crystal part 820 " • Input collimator 704… Electro-optic crystal part 822 ··· Input collimator 706 ··· Electro-optic crystal part 824 ··· Input collimator 708 ··· Electro-optic crystal section 826 " • Input collimator 712… Electro-optic crystal section 830 " • Straight path (Please read the precautions on the back before filling this page) This paper size Applicable to China National Standard (CNS) A4 specification (210X297 mm) 28 546499 A7 B7 V. Description of the invention (25) 832 " • Straight path 922… Input fiber collimator 834- • Straight path 924… Input Fiber collimator 836 " • Straight path 926… input fiber collimator 870 " • Output path light 930 ... Straight path 872 ·· Output path light 932 ... Straight path 874 ·· • Output path light 934… Straight path 876 " • Output path light 936 ... Straight path 880 " • Output fiber collimator 970 ... Output path light 882 " • Output fiber collimator 972 ... Output path light 884 " • Output fiber collimation Collimator 974… output path light 886 " • output fiber collimator 976… output path light 902 ··· electro-optic crystal 980… output fiber collimator 904 " • electro-optic crystal 982 ... output fiber collimator 906 " • electro-optic crystal 984… output fiber collimator 908 “920 ·· • electro-optic crystal • input fiber collimator 986… output fiber collimator (please read the precautions on the back before filling this page) This paper size is applicable to Chinese national standards (CNS ) A4 size (210X297 mm) 29

Claims (1)

546499 A3 •B8 _ C3 --------____D3_ 六、申請專利範圍 1. 一種光學開關,其包括·· 一光學信號傳輸的電光晶體,其具有至少一第一部 分以及至少一第二部分,構成該等部分之至少其中之一 部分的材料一經施以電場即展現折射率的變化,該第一 與第二部分於其間定出至少一轉換界面;546499 A3 • B8 _ C3 --------____ D3_ VI. Scope of patent application 1. An optical switch comprising: an electro-optic crystal for optical signal transmission, which has at least a first part and at least a second part The material constituting at least one of the parts exhibits a change in refractive index upon application of an electric field, and the first and second parts define at least one transition interface therebetween; 裝 至少一信號源,用於沿著至少一未受引導的光束路 徑放射一信號通過該晶體,該未受引導的光束路徑在一 入射角度下與該至少一轉換界面交叉; 訂 一電場產生器,用於在該晶體之該第一與第二部 分之至少一部分中產生一轉換電場,針對該第一與第二 部分之至少一部分導致折射率變化的該電場在該界面 產生一臨界角小於該入射角,將信號反射離開該界面, 其中藉由將該電場產生器開啟與關掉該界面將光 學信號於穿透與反射之間轉換,改變通過該晶體之該未 受引導的光束路徑。 2. 如申請專利範圍第i項之光學開關,其中該信號源放射 信號係為一或更多之準直的、部分準直的、會聚的或是 分歧的信號。 3. 如申請專利範圍第丨項之光學開關,其中該第一部分之 域的定向相對於該第二部分之域的定向係為反向。 4·如申請專利範圍第3項之光學開關,其中藉由將第—與 第一。P刀之至少一部分構成為—極化的部分而構成該 反向域。 5.如申請專利第3項之光學開關,其中該反向域係藉 本纸張尺度適用中國國家標準dhs ) A4^格(21 Ο X297公-------- -30 - 9 9 64 Asc D 圍 々巳 ΐ-τ利¾丁 ’骨 、-5 ^1•六 由71字一晶體部分以機誠方式結合在一起構成該域界面 而構成’其中該一晶體部分具有與另一部分相對的域定 向0 6·如申請專利範圍第3、4或5項之光學開關,其中該電場 產生器係按適當尺寸與形狀製作,在該第一與第二部分 中產生該轉換電場。 · •如申請專利範圍第3項之光學開關,其中該開關包括二 輸出準直儀並藉由二開關構成為一開關。 8·如申請專利範圍第7項之光學開關,其中該開關係為雙 方向作用的。 9·如申請專利範圍第3項之光學開關,其中該第-與第二 部分係按適當尺寸與形散製作,在該晶體部分間構成至_ 少二域界面。 10·如申請專利範圍第1或3項之光學開關,其中該折射率之 變化係足以反射於該信號中的所有波長,用以提供波長 不相關之轉換。 U·如申請專利範圍第1或3項之光學開關,其中該折射率之 變化係足以反射於該信號中的橫磁(TM)及橫電(TE)偏 振,用以提供偏振不相關之轉換。 . 12·如申請專利範圍第9項之光學開關,其進一步地包括至 少二輸入準直儀其中該晶體按適當尺寸與形狀製作,容 誇至少二未受引導的光學路徑在該入射角度下與該第 '一與第一域界面之每一界面交叉。 13· —種光學開關,其包括: 本纸張尺度適用中國國家標準(CNS) A4規格(21〇乂297公釐) 31 546499Install at least one signal source for emitting a signal through the crystal along at least one unguided beam path, the unguided beam path crossing the at least one conversion interface at an incident angle; and ordering an electric field generator For generating a switching electric field in at least a part of the first and second parts of the crystal, and for the electric field that causes a refractive index change for at least a part of the first and second parts, a critical angle at the interface is smaller than the The angle of incidence reflects the signal away from the interface, where the optical signal is switched between penetration and reflection by turning the electric field generator on and off the interface, changing the unguided beam path through the crystal. 2. The optical switch of item i in the patent application range, wherein the signal emitted by the signal source is one or more collimated, partially collimated, convergent or divergent signals. 3. For the optical switch according to the scope of the patent application, the orientation of the domain of the first part is opposite to the orientation of the domain of the second part. 4. The optical switch according to item 3 of the scope of patent application, in which the first and the first are used. At least a part of the P-knife is constituted as a polarized part to constitute the reverse domain. 5. If the optical switch of item 3 is applied for, the reverse domain is based on the paper standard applicable to the Chinese national standard dhs) A4 ^ grid (21 Ο X297 公 -------- -30-9 9 64 Asc D 々 巳 ΐ々 巳 ΐ-τ 利 ¾ 丁 'bone, -5 ^ 1 • Six is composed of 71-word crystal parts together in a sincere way to form the interface of the domain to form' where the crystal part has another part Relative domain orientation 0 6 · If the optical switch of the patent application is No. 3, 4 or 5, the electric field generator is made in an appropriate size and shape to generate the converted electric field in the first and second parts. • The optical switch of item 3 in the scope of patent application, wherein the switch includes a two-output collimator and is configured as a switch by two switches. 8. The optical switch of item 7 in the scope of patent application, wherein the open relationship is double 9. The optical switch according to item 3 of the scope of patent application, wherein the first and second parts are made with appropriate size and dispersion to form at least two domain interfaces between the crystal parts. 10 · 如The optical switch of the scope of patent application No. 1 or 3, wherein the The change in emissivity is sufficient to reflect all wavelengths in the signal to provide a wavelength-independent conversion. U. For example, the optical switch of the patent application No. 1 or 3, wherein the change in refractive index is sufficient to reflect the The transverse magnetic (TM) and transverse electrical (TE) polarizations in the signal are used to provide polarization-independent conversion. 12. The optical switch according to item 9 of the patent application scope, which further includes at least two input collimators. The crystal is made in an appropriate size and shape, and allows at least two unguided optical paths to intersect each interface of the first and first domain interfaces at the incident angle. 13. An optical switch including: This paper size applies to China National Standard (CNS) A4 (21〇21297mm) 31 546499 申請專利範圍 至少一光學信號之信號源; 一光#仏號傳輸的電光晶體,其係定出二轉換界 面’在每一轉換界面處轉換界面之每一側邊係以一經施 以電療即變化折射率的材料所構成; 該晶體係按適當尺寸與形狀製作,並且該轉換界面 係按適當尺寸並配置容許至少一未受引導的光學路徑 在一入射良度下與該第一與第二轉換界面之一或二界 面交叉; 至少;電場產生器,用於在該轉換界面產生一轉 換電場’該導致折射率變化的該電場足以在該轉換界面 產生一臨界為小於該入射角,將信號反射離開該轉換界 面,以及 至少二年學信號接收器,係供、該光學信號所用; 其中藉声將該電場開啟與關掉,該轉換界面將該 至少一光學、信號於穿透與反射之間轉換,改變通過該晶 體之該未受:弓丨導的光束路徑。 14·如申請專利範圍第13項之光學開關,其包括至少三光學 信號接收器其中該二轉換界面係配置在該電光晶體 中,容許該偉號依循一未受引導、未經反射的光束路徑 通過該轉換界面之第一界面接著通過另一界面,並且未 在該任一轉換界面或是該其中之一轉換界面處選擇性 地轉揍用以構成一 1 X 3開關。 15·如申請專利範圍第13項之光學開關,其中該開關包括至 少二輸入信號產生器,每一產生器定出一未受引導的光 32 本纸張尺度適用中國國家標準(CNS) A4規格(210X297公釐) 546499 經濟部智慧財產局員工消費合作社印製The scope of the patent application is at least one signal source of optical signals; an electro-optic crystal transmitted by a light # 仏, which defines two conversion interfaces. At each conversion interface, each side of the conversion interface changes as soon as electrotherapy is applied. Refractive index material; the crystal system is made in proper size and shape, and the conversion interface is in proper size and configuration to allow at least one unguided optical path to convert with the first and second at an incident goodness One or two interfaces intersect; at least; an electric field generator is used to generate a conversion electric field at the conversion interface. The electric field that causes a change in refractive index is sufficient to generate a threshold at the conversion interface that is less than the incident angle and reflects the signal. Leaving the conversion interface and the signal receiver for at least two years are used for the optical signal; wherein the electric field is turned on and off by sound, and the conversion interface converts at least one optical and signal between transmission and reflection. The conversion changes the path of the unguided beam passing through the crystal. 14. The optical switch according to item 13 of the patent application scope, which includes at least three optical signal receivers, wherein the two conversion interfaces are arranged in the electro-optic crystal, allowing the Weihao to follow an unguided, unreflected beam path The first interface passing through the conversion interface then passes through another interface, and is not selectively switched to form a 1 X 3 switch at any one of the conversion interfaces or one of the conversion interfaces. 15. The optical switch as claimed in item 13 of the scope of patent application, wherein the switch includes at least two input signal generators, each of which sets out an unguided light. 32 This paper standard applies to China National Standard (CNS) A4 specifications. (210X297 mm) 546499 Printed by the Consumer Cooperative of the Intellectual Property Bureau of the Ministry of Economic Affairs 、申諱專利範 束路通過该晶體,該二轉換界面係配置容許該每一光 束路徑在該入射角度下與該每一轉換界面交叉,並延伸 至該其中之一信號接收器,一經施以電場即定出一反射 的光束路徑其中該信號反射離開該轉換界面至該另一 光學信_號接收器,藉此該光學信號可通過或是反射以構 成一2 X 2開關。 M·如申請專利範圍第13項之光學開關,其中該第一與第二 轉換界面係互相電氣地隔離,容許在該每一轉換界面處 獨立地引動該折射率的改變。 17·如申請專利範圍第13項之光學開關,其中該第一與第二 轉換界面並未互相電氣地隔離,而該折射率改變的引動 係一起發生在該二之轉換界面。 18·如申請專利範圍第13項之光學開關,其中該二轉換界面 之其中之一界面針對該光束定出一反射的信號路徑, 轉換元件進一步地包括一與該反射的光束路徑交叉 卓—轉換界面,藉此该彳έ號係可在該;Ξ·轉換界面其中 任一界面處反射以構成一 1 X 4開關。 19. 如申請專利範圍第18項之光學元件,其中該第一轉換界 面係與該第二轉換界面與第三轉換界面電 20. 如申請專利範圍第丨或13項之光學開關,其進一步地包 括一或更多的光學隔離器容許減小開關之轴的尺寸。 21. 如申請專利範圍第20項之光學開關,其中該—或更多的 光學隔離器包含至少一反射表面。22·如申請專利範圍第21項之光學開關,其進一步地包含至 叮 該 的 之 本紙張尺度適用中國國家標準(CNS)A4規格(21〇 χ 297公爱) 33 λ3 Β8 546499The patented patent fan beam passes through the crystal, and the two conversion interface system is configured to allow each beam path to intersect with each conversion interface at the incident angle and extend to one of the signal receivers. The electric field determines a reflected beam path where the signal is reflected off the conversion interface to the other optical signal receiver, whereby the optical signal can pass or reflect to form a 2 X 2 switch. M. The optical switch according to item 13 of the patent application, wherein the first and second conversion interfaces are electrically isolated from each other, allowing the change of the refractive index to be independently induced at each conversion interface. 17. The optical switch according to item 13 of the patent application, wherein the first and second conversion interfaces are not electrically isolated from each other, and the actuation system of the refractive index change occurs at the two conversion interfaces together. 18. The optical switch according to item 13 of the patent application, wherein one of the two conversion interfaces defines a reflected signal path for the light beam, and the conversion element further includes a cross-over conversion with the reflected light beam path. Interface, by which the 号 number can be reflected at this interface; Ξ · conversion interface reflection at any interface to form a 1 X 4 switch. 19. If the optical element of the scope of patent application No. 18, wherein the first conversion interface is electrically connected to the second conversion interface and the third conversion interface 20. If the optical switch of the patent scope No. 丨 or 13 is further applied, Including one or more optical isolators allows reducing the size of the shaft of the switch. 21. The optical switch of claim 20, wherein the-or more optical isolator includes at least one reflective surface. 22. If the optical switch in the scope of application for the patent No. 21, it further contains the paper size of the paper to the Chinese National Standard (CNS) A4 specification (21〇 χ 297 public love) 33 λ3 B8 546499 _'寻利範圍 少一對反射表面,致使該-或更多的每—料信號反射 至-與該未受引導之光束路徑間隔開的光束路徑通過 該晶體。 23·如申請專利範圍第22項之光學„,其中該二反射的表 面包括一稜鏡。 24. —種用於轉換光學信號的光學開關,其係包括·· Ν個輸入信號源,其定出1^個未交又之未受引導的 光束路徑;其中Ν係為二或以上; Ν個輸出信號源; 光學#號傳輸電光晶體,其至少具有足夠的轉 換界面以反射該每一未受引導的光束路徑至該Ν個輸 出準直儀,該轉換界面係配置在一入射角度下與該每 一未受引導的光束路徑交叉,並且其之特徵在於在該 轉換界面處一經施以電場具有折射率之變化產生小於 該入射角的一臨界角,用以將該信號反射離開該轉換 界面;以及 至少足夠的電場產生器,針對該每一轉換界面獨 立地產生轉換電場,構成一非阻塞的ΝχΝ開關。 25.如申請專利範圍第24項之光學開關,其中該電光晶體係 為一單一整體的結構。 26·如申請專利範圍第24項之光學開關,其中該電光晶體係 由晶體之分離的部分所組成,其於操作上係互相接近地 配置。 27· —種用於轉換光學信號的光學開關,該開關包括·· 、尺度適用中國國家標準(CNS) Α4規格(210X297公酱) 34 546499 辱專利麗圍 -〇 Ο_ 'Profit Seeking Range One fewer pair of reflective surfaces causes the-or more per-material signal to reflect-to a beam path spaced from the unguided beam path through the crystal. 23. The optical device according to item 22 of the scope of the patent application, wherein the two-reflective surface includes a frame. 24. An optical switch for converting an optical signal, which includes ... N input signal sources, 1 ^ uncrossed and unguided beam paths; where N is two or more; N output signal sources; optical #transmits electro-optic crystals with at least enough conversion interfaces to reflect each of these unguided The guided beam path to the N output collimators, the conversion interface is configured to intersect each of the unguided beam paths at an incident angle, and is characterized in that once an electric field is applied at the conversion interface, The change in refractive index produces a critical angle less than the incident angle to reflect the signal away from the conversion interface; and at least enough electric field generators to independently generate a conversion electric field for each conversion interface, forming a non-blocking ΝχΝ switch. 25. The optical switch of item 24 in the scope of patent application, wherein the electro-optic crystal system is a single integrated structure. 26. The item of scope of patent application 24 Optical switch, in which the electro-optic crystal system is composed of separate parts of the crystal, which are arranged close to each other in operation. 27 · —An optical switch for converting optical signals, the switch includes ... Standard (CNS) Α4 specification (210X297 male sauce) 34 546499 Dishonored patent Liwei -〇〇 Ο 四輸入準直儀,其定出四交又之未受引導的光束 路徑; 四輸出準直儀; 一光學信號傳輸電光晶體,其至少具有五個轉換 結構係配置與該未受引導的光束路徑交叉,該每一轉換 結構具有二轉換界面,該每一未受引導的光束路徑在一' 2射角度下與該至少-轉換界面交又,該轉換界面之特 徵在於在該界面處-經施以電場具有折射率之變化產 生小於該人射㈣-臨界角,心將該信號反射離開該 轉換界面;以及 至少五電場產生器’針對該每一轉換結構獨立地 產生轉換電場,用於選擇性地反射該光束路徑構成一非 阻塞的4 X 4開關。 28.-種用於轉㈣學信號的光學開關,該開關包括: Ν個輸入信號源’其定出Ν個交叉之未受引導的光 束路徑; Ν個輸出信號源; -光學信號傳輸電光晶體,其至少具有一轉換結 構’其係配置與該任二之未受弓丨導的光束路徑交叉,該 每:轉換結構具有二轉換界面,該每一未受引導的光束 路徑在-入射角度下與該至少_轉換界面交叉,該轉換 界面之特被在於在该界面處一經施以電場具有折射率 之產生小於該人射角的—臨界角’用以將該信號反 射離開該轉換界面;以及 本紙張尺度適用中關家標準⑽S)A4规格⑵0^5^ (請先閱讀背面之注意事項再填寫本頁)〇 Four-input collimator, which determines the four-way unguided beam path; four-output collimator; an optical signal transmission electro-optic crystal, which has at least five conversion structures configured with the unguided beam The paths intersect, each conversion structure has two conversion interfaces, and each unguided beam path intersects the at least-transition interface at a '2' angle, and the conversion interface is characterized by the- Applying a change in the refractive index of the electric field produces less than the person's critical angle, and the heart reflects the signal away from the conversion interface; and at least five electric field generators' independently generate a conversion electric field for each conversion structure for selection Reflecting the beam path by nature constitutes a non-blocking 4 X 4 switch. 28.- An optical switch for transducing scientific signals, the switch comprising: N input signal sources' which define N cross-guided beam paths; N output signal sources;-optical signal transmission electro-optic crystals , Which has at least one conversion structure, whose configuration intersects with the beam path of any of the two unguided beams, the per: conversion structure has two conversion interfaces, and each of the unguided beam paths is at an angle of incidence Crossing the at least _ conversion interface, the conversion interface is characterized in that upon application of an electric field at the interface, a refractive index that is smaller than the human angle of incidence-a critical angle is used to reflect the signal away from the conversion interface; and This paper size applies the Zhongguanjia standard (S) A4 size: 0 ^ 5 ^ (Please read the precautions on the back before filling this page) 35 Jo 546499 至少一電場產生器,針對該每一轉換結構獨立地產 生轉換電場,用於在該光束路徑上選擇性地反射光學信 號’構成一非阻塞的N X N開關。 29·如申请專利範圍第27項之用於轉換光學信號的光學開 關,其為一非阻塞之4 X 4光學開關,其中該四輸入準 直儀一般係佈置成二平行的配對,該每一配對定出未受 引導的光束路徑與另一配對之未受引導的光束路徑交 又而β亥其中之一轉換結構係配置在該等交叉之其中至 少三交又中。 3〇· 一種光學開關,其係包括: 一光學信號傳輸電光晶體,其至少具有第一部分與 至少一第二部分,該等部分之至少一部分係以一經施以 電場即顯現折射率變化的材料所構成,並且按適當的尺 寸與形狀製作在該第一與第二部分之間定出至少二轉 換界面; 至少二信號源,每一信號源沿著一個別的未受引導 的光束路徑放射一信號通過該晶體,該每一未受引導的 光束路徑在個別之入射角度下與該二轉換界面之其中 之一界面交叉; 一電場產生器,用於在該第一與第二部分之至少一 部分中產生一轉換電場,足以在該界面處產生小於該個 別之入射角的一臨界角,用以將該信號反射離開該界 面; 其,中,藉由將該電場產生器開啟與關掉,該界面將 本紙張尺度 —35 Jo 546499 At least one electric field generator generates a conversion electric field independently for each conversion structure, and is used to selectively reflect an optical signal on the beam path to form a non-blocking N X N switch. 29. The optical switch for converting an optical signal according to item 27 of the scope of patent application is a non-blocking 4 X 4 optical switch. The four-input collimator is generally arranged in two parallel pairs. The paired unguided beam path intersects with the other paired unguided beam path, and one of the beta-hailer transition structures is disposed in at least three of the intersections. 30. An optical switch comprising: an optical signal transmission electro-optic crystal having at least a first portion and at least a second portion, at least a portion of which is made of a material that exhibits a change in refractive index upon application of an electric field Structure, and make at least two conversion interfaces between the first and second parts according to the appropriate size and shape; at least two signal sources, each signal source emits a signal along a different unguided beam path Through the crystal, each unguided beam path intersects one of the two conversion interfaces at an individual incident angle; an electric field generator is used in at least a part of the first and second parts Generating a switching electric field is sufficient to generate a critical angle at the interface that is less than the individual incident angle to reflect the signal away from the interface; wherein, by turning the electric field generator on and off, the interface Scale this paper — 36 54649936 546499 j 為光學信號於穿透與反射之間轉換,改變通過該晶體之 該未受引導的光束路徑。 3 1 •如申請專利範圍第30項之光學開關,其中該第一部分至 少部分地圍繞該第二部分。 32.如申請專利範圍第3〇項之光學開關,其中該第二部分係 為一薄帶條的形式。 I. 3·如申凊專利範圍第32項之光學開關,其中該薄帶條係夠 薄以避免不可接受的光束離散,並且夠厚具有二表面反 射’一經施以電場即轉換光學信號。 34·如申請專利範圍第33項之光學開關,其進一步地包括一 第一對一般係為平行的輸入準直儀定出一第一對未受 弓丨導的光束路徑,以及一第二對輸入準直儀定出一第二 對未受引導的光束路徑,並且進一步地包括一第一對輸 出準直儀與一第二對輸出準直儀,其中該第一對未受引 導的光束路徑與該第二對未受引導的光束路徑交叉,並 且該電光晶體包括夠薄的帶條之第;部分用以將信號 從该輸入準直儀轉換至該輸出準直儀。 35. —種光學開關,其係包括·· ^ 一光學信號傳輸電光晶體,其具有二第一部分與一 第一部分,該第二部分係以 '經施以電場即顯現折射率 變化的材料所構成,該第一與第二部分於其間定出二 換界面; 二信號源’用於將信號沿著未受引導的光束抑放 —_射通過該晶體’該每-未受引導的光束路徑在入射角度 本紙張尺度適用中國國家) A4规格(210X297^^一°— -37 - 546499j is the conversion of the optical signal between transmission and reflection, changing the unguided beam path through the crystal. 3 1 • The optical switch according to item 30 of the patent application, wherein the first part at least partially surrounds the second part. 32. The optical switch according to claim 30, wherein the second part is in the form of a thin strip. I. 3. The optical switch according to item 32 of the patent application, wherein the thin strip is thin enough to avoid unacceptable beam dispersion, and thick enough to have two surface reflections' which convert the optical signal upon application of an electric field. 34. The optical switch according to item 33 of the patent application scope, further comprising a first pair of input collimators that are generally parallel to determine a first pair of unguided beam paths, and a second pair The input collimator determines a second pair of unguided beam paths, and further includes a first pair of output collimators and a second pair of output collimators, wherein the first pair of unguided beam paths Intersect the second pair of unguided beam paths, and the electro-optic crystal includes a thin enough band; the portion is used to convert the signal from the input collimator to the output collimator. 35. An optical switch, comprising: an optical signal transmission electro-optic crystal, which has two first parts and a first part, the second part is made of a material that exhibits a change in refractive index upon application of an electric field , The first and second parts define a second interface between them; the two signal sources are used to suppress the signal along the unguided beam—the beam passes through the crystal; the every-unguided beam path is at Incident angle This paper size is applicable to China) A4 size (210X297 ^^ one ° — -37-546499 下與該轉換界面之其中至少一界面交又; 一輸出信號接收器,其係用於接收該信號; 一電場產生器,用於在該晶體之該第二部分中產生 一轉換電場’針對該第二部分導致折射率變化之該電場 足以在该轉換界面處產生小於該入射角的一臨界角,用 以將該信號反射離開該轉換界面; 其中藉由將該電場產生器開啟與關掉,該轉換界面 將該信號於穿透與反射之間轉換,將該信號從一輪出俨 號接收器反射至另一輸出接收器。 36· —種光學開關,其係包括·· 至少一準直的光學信號的光學信號源; 一第一光學信號傳輸電光晶體,其至少具有一第〜 邠分與至少一第二部分,該等部分之至少一部分係以一 經施以電場即顯現折射率變化的材料所構成,該第〜與 第二部分於其間定出一第一轉換界面; >、 一第二光學信號傳輸電光晶體,其至少具有一第一 部分與至少一第四部分,該等部分之至少一部分係以2 經施以電場即顯現折射率變化的材料所構成,該第三邀 第四部分於其間定出一第二轉換界面; 〜 、至少一未受引導的光束路徑通過該晶體,該未爱弓 導的光束路徑在一入射角度下與該第一與第二轉換^ 面交又; 、1 一分開的電場產生器,用於在該晶體之該第 部分以及該第三與第四部分之至少一部分中 本紙^尺度適用^^家標準-(哪)M規格 與第 先 閱 讀 背 面 意 事An interface with at least one of the conversion interfaces; an output signal receiver for receiving the signal; an electric field generator for generating a conversion electric field in the second part of the crystal; The second part of the electric field that causes a change in the refractive index is sufficient to generate a critical angle at the conversion interface that is smaller than the incident angle to reflect the signal away from the conversion interface; wherein, by turning the electric field generator on and off, The conversion interface converts the signal between penetration and reflection, and reflects the signal from a round receiver to another output receiver. 36 · An optical switch, comprising: an optical signal source of at least one collimated optical signal; a first optical signal transmission electro-optic crystal having at least a first to a second component and at least a second portion, etc. At least a part of the part is made of a material that exhibits a change in refractive index upon application of an electric field, and the first to second parts define a first conversion interface therebetween; > a second optical signal transmission electro-optic crystal, It has at least a first part and at least a fourth part, and at least a part of these parts is made of 2 materials that exhibit a change in refractive index upon application of an electric field. The third invites the fourth part to define a second transition therebetween. Interface; ~, at least one unguided beam path passes through the crystal, and the unguided beam path intersects the first and second transition planes at an incident angle; and 1, a separate electric field generator , For the paper in this part of the crystal and at least part of the third and fourth parts ^ standard applicable ^ ^ home standard-(which) M specifications and first reading on the back Order 38 08546499 •3S7 . 屢- 轉換電場,導致折射率變化之該電場足以在該轉換界面 處產生小於該入射角的一臨界角,用以將該信號反射離 開該轉換界面; 三供該準直的光學信號所用的光學信號接收器; 其中藉由將該轉換電場開啟與關掉,該轉換界面將 該至少一光學信號於穿透與反射之間轉換,改變通過該 晶體之該未受引導的光束路徑,從而在該三光學信號接 收器間轉換該光束路徑。 37·如申請專利範圍第13、24或28項之光學開關,其中該信 號源放射該信號,構成一或更多之準直的、部分準直 的、會聚的或是分歧的信號。 38. 如申請專利範圍第13、24或28項之光學開關,其中該開 關係為雙向(bidirectional)的。 39. 如申請專利範圍第13、24或28項之光學開關,其中該至 少一電場產生器係按適當的尺寸與形狀製作,在該轉換 界面之雙側上產生該轉換電場。 · 40·如申請專利範圍第13、24或28項之光學開關,其中該電 光晶體包括一般相對置的輸入/輸出界面,並且該界面 之定向一般係垂直於該未受引導的光束路徑。 41·如申請專利範圍第13、24或28項之光學開關,其中該折 射率之變化係足以於該信號中反射所有的波長,提供波 長不相關的轉換。 42·如申請專利範圍第13、24或28項之光學開關,其中該折 射率之變化係足以於該信號中反射橫磁(TM)及橫電 本纸張尺一~一 39 0354649938 08546499 • 3S7. Repeatedly-converted electric field, the electric field causing a change in refractive index is sufficient to generate a critical angle at the conversion interface that is smaller than the incident angle, to reflect the signal away from the conversion interface; three for the collimation Optical signal receiver for optical signals; wherein by switching the switching electric field on and off, the switching interface changes the at least one optical signal between penetration and reflection to change the unguided light beam passing through the crystal Path, thereby switching the beam path between the three optical signal receivers. 37. The optical switch according to claim 13, 24 or 28, wherein the signal source emits the signal, constituting one or more collimated, partially collimated, convergent or divergent signals. 38. The optical switch of claim 13, 24 or 28, wherein the on-off relationship is bidirectional. 39. In the case of an optical switch with the scope of patent applications No. 13, 24, or 28, wherein the at least one electric field generator is made in an appropriate size and shape, the switching electric field is generated on both sides of the switching interface. · 40. The optical switch of claim 13, 24 or 28, wherein the electro-optic crystal includes a generally opposite input / output interface, and the orientation of the interface is generally perpendicular to the unguided beam path. 41. The optical switch of claim 13, 24 or 28, wherein the change in the refractive index is sufficient to reflect all the wavelengths in the signal, providing a wavelength-independent conversion. 42. If the optical switch with the scope of patent application No. 13, 24 or 28 is applied, the change of the refractive index is sufficient to reflect the transverse magnetic (TM) and transverse electricity in the signal. This paper rule 1 ~ 1 39 03546499 (ΤΕ)偏振,提供偏振不相關的轉換。 43. —種轉換光學信號的方法,其包括: 將一未受引導的光學信號引導進入一電光晶體; 在一入射角度下將該信號通過至少一轉換界面,該 界面係構成在該晶體之極化與未極化部分之間; 選擇性地施以一足夠的電場至該電光晶體改變介 於無轉換界面反射與所具之臨界角小於該入射角之間 的狀態,在該轉換界面處選擇性地通過或反射該信號, 並從而; 在二或更多信號接收器之間轉換該信號。 44· 一種製造電光開關元件的方法,其係包括: 在一電光晶體上構成至少一第一輸入/輸出界面; 在該電光晶體上構成至少一第二輸入/輸出界面, 該第二界面一般係與該第^界面相對置; 修改該晶體之至少一部分,一般地在該第一與第 二輸入/輸出界面之間定出一轉換界面。 45.如申請專利範圍第44項之製造電光開關元件的方法,其 進一步地包括在該電光晶體中構成一第二轉換界面的 步驟。 一 , 尺度適用巾_家標準(CNS) A4规格(210X297公釐)(TE) polarization, providing polarization-independent conversion. 43. A method for converting an optical signal, comprising: directing an unguided optical signal into an electro-optic crystal; passing the signal through at least one conversion interface at an incident angle, the interface being formed at the pole of the crystal Selectively apply a sufficient electric field to the electro-optic crystal to change the state between the reflection-free interface reflection and the critical angle smaller than the incident angle, and select at the conversion interface Pass or reflect the signal, and thereby; convert the signal between two or more signal receivers. 44. A method for manufacturing an electro-optic switching element, comprising: forming at least a first input / output interface on an electro-optic crystal; forming at least a second input / output interface on the electro-optic crystal, the second interface is generally Opposite the third interface; modify at least a part of the crystal, and generally define a conversion interface between the first and second input / output interfaces. 45. The method for manufacturing an electro-optic switching element according to item 44 of the patent application scope, further comprising the step of forming a second conversion interface in the electro-optic crystal. First, the size applies towel _ home standard (CNS) A4 specifications (210X297 mm) 注 意 事Precautions Order 4040
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