TW454099B - Multicore and multimode dispersion managed fibers - Google Patents
Multicore and multimode dispersion managed fibers Download PDFInfo
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- TW454099B TW454099B TW088116554A TW88116554A TW454099B TW 454099 B TW454099 B TW 454099B TW 088116554 A TW088116554 A TW 088116554A TW 88116554 A TW88116554 A TW 88116554A TW 454099 B TW454099 B TW 454099B
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- G—PHYSICS
- G02—OPTICS
- G02B—OPTICAL ELEMENTS, SYSTEMS OR APPARATUS
- G02B6/00—Light guides; Structural details of arrangements comprising light guides and other optical elements, e.g. couplings
- G02B6/02—Optical fibres with cladding with or without a coating
- G02B6/02214—Optical fibres with cladding with or without a coating tailored to obtain the desired dispersion, e.g. dispersion shifted, dispersion flattened
- G02B6/02219—Characterised by the wavelength dispersion properties in the silica low loss window around 1550 nm, i.e. S, C, L and U bands from 1460-1675 nm
- G02B6/02247—Dispersion varying along the longitudinal direction, e.g. dispersion managed fibre
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- G—PHYSICS
- G02—OPTICS
- G02B—OPTICAL ELEMENTS, SYSTEMS OR APPARATUS
- G02B6/00—Light guides; Structural details of arrangements comprising light guides and other optical elements, e.g. couplings
- G02B6/02—Optical fibres with cladding with or without a coating
- G02B6/028—Optical fibres with cladding with or without a coating with core or cladding having graded refractive index
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- C—CHEMISTRY; METALLURGY
- C03—GLASS; MINERAL OR SLAG WOOL
- C03B—MANUFACTURE, SHAPING, OR SUPPLEMENTARY PROCESSES
- C03B37/00—Manufacture or treatment of flakes, fibres, or filaments from softened glass, minerals, or slags
- C03B37/01—Manufacture of glass fibres or filaments
- C03B37/012—Manufacture of preforms for drawing fibres or filaments
- C03B37/01205—Manufacture of preforms for drawing fibres or filaments starting from tubes, rods, fibres or filaments
- C03B37/01211—Manufacture of preforms for drawing fibres or filaments starting from tubes, rods, fibres or filaments by inserting one or more rods or tubes into a tube
- C03B37/01222—Manufacture of preforms for drawing fibres or filaments starting from tubes, rods, fibres or filaments by inserting one or more rods or tubes into a tube for making preforms of multiple core optical fibres
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- G—PHYSICS
- G02—OPTICS
- G02B—OPTICAL ELEMENTS, SYSTEMS OR APPARATUS
- G02B6/00—Light guides; Structural details of arrangements comprising light guides and other optical elements, e.g. couplings
- G02B6/02—Optical fibres with cladding with or without a coating
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- G—PHYSICS
- G02—OPTICS
- G02B—OPTICAL ELEMENTS, SYSTEMS OR APPARATUS
- G02B6/00—Light guides; Structural details of arrangements comprising light guides and other optical elements, e.g. couplings
- G02B6/02—Optical fibres with cladding with or without a coating
- G02B6/02042—Multicore optical fibres
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- G—PHYSICS
- G02—OPTICS
- G02B—OPTICAL ELEMENTS, SYSTEMS OR APPARATUS
- G02B6/00—Light guides; Structural details of arrangements comprising light guides and other optical elements, e.g. couplings
- G02B6/24—Coupling light guides
- G02B6/26—Optical coupling means
- G02B6/28—Optical coupling means having data bus means, i.e. plural waveguides interconnected and providing an inherently bidirectional system by mixing and splitting signals
- G02B6/293—Optical coupling means having data bus means, i.e. plural waveguides interconnected and providing an inherently bidirectional system by mixing and splitting signals with wavelength selective means
- G02B6/29371—Optical coupling means having data bus means, i.e. plural waveguides interconnected and providing an inherently bidirectional system by mixing and splitting signals with wavelength selective means operating principle based on material dispersion
- G02B6/29374—Optical coupling means having data bus means, i.e. plural waveguides interconnected and providing an inherently bidirectional system by mixing and splitting signals with wavelength selective means operating principle based on material dispersion in an optical light guide
- G02B6/29376—Optical coupling means having data bus means, i.e. plural waveguides interconnected and providing an inherently bidirectional system by mixing and splitting signals with wavelength selective means operating principle based on material dispersion in an optical light guide coupling light guides for controlling wavelength dispersion, e.g. by concatenation of two light guides having different dispersion properties
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- C—CHEMISTRY; METALLURGY
- C03—GLASS; MINERAL OR SLAG WOOL
- C03B—MANUFACTURE, SHAPING, OR SUPPLEMENTARY PROCESSES
- C03B2203/00—Fibre product details, e.g. structure, shape
- C03B2203/10—Internal structure or shape details
- C03B2203/22—Radial profile of refractive index, composition or softening point
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- C—CHEMISTRY; METALLURGY
- C03—GLASS; MINERAL OR SLAG WOOL
- C03B—MANUFACTURE, SHAPING, OR SUPPLEMENTARY PROCESSES
- C03B2203/00—Fibre product details, e.g. structure, shape
- C03B2203/32—Eccentric core or cladding
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- C—CHEMISTRY; METALLURGY
- C03—GLASS; MINERAL OR SLAG WOOL
- C03B—MANUFACTURE, SHAPING, OR SUPPLEMENTARY PROCESSES
- C03B2203/00—Fibre product details, e.g. structure, shape
- C03B2203/34—Plural core other than bundles, e.g. double core
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- G—PHYSICS
- G02—OPTICS
- G02B—OPTICAL ELEMENTS, SYSTEMS OR APPARATUS
- G02B6/00—Light guides; Structural details of arrangements comprising light guides and other optical elements, e.g. couplings
- G02B6/02—Optical fibres with cladding with or without a coating
- G02B6/028—Optical fibres with cladding with or without a coating with core or cladding having graded refractive index
- G02B6/0281—Graded index region forming part of the central core segment, e.g. alpha profile, triangular, trapezoidal core
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- G—PHYSICS
- G02—OPTICS
- G02B—OPTICAL ELEMENTS, SYSTEMS OR APPARATUS
- G02B6/00—Light guides; Structural details of arrangements comprising light guides and other optical elements, e.g. couplings
- G02B6/02—Optical fibres with cladding with or without a coating
- G02B6/036—Optical fibres with cladding with or without a coating core or cladding comprising multiple layers
- G02B6/03605—Highest refractive index not on central axis
- G02B6/03611—Highest index adjacent to central axis region, e.g. annular core, coaxial ring, centreline depression affecting waveguiding
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- G—PHYSICS
- G02—OPTICS
- G02B—OPTICAL ELEMENTS, SYSTEMS OR APPARATUS
- G02B6/00—Light guides; Structural details of arrangements comprising light guides and other optical elements, e.g. couplings
- G02B6/02—Optical fibres with cladding with or without a coating
- G02B6/036—Optical fibres with cladding with or without a coating core or cladding comprising multiple layers
- G02B6/03616—Optical fibres characterised both by the number of different refractive index layers around the central core segment, i.e. around the innermost high index core layer, and their relative refractive index difference
- G02B6/03622—Optical fibres characterised both by the number of different refractive index layers around the central core segment, i.e. around the innermost high index core layer, and their relative refractive index difference having 2 layers only
- G02B6/03627—Optical fibres characterised both by the number of different refractive index layers around the central core segment, i.e. around the innermost high index core layer, and their relative refractive index difference having 2 layers only arranged - +
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- G—PHYSICS
- G02—OPTICS
- G02B—OPTICAL ELEMENTS, SYSTEMS OR APPARATUS
- G02B6/00—Light guides; Structural details of arrangements comprising light guides and other optical elements, e.g. couplings
- G02B6/02—Optical fibres with cladding with or without a coating
- G02B6/036—Optical fibres with cladding with or without a coating core or cladding comprising multiple layers
- G02B6/03616—Optical fibres characterised both by the number of different refractive index layers around the central core segment, i.e. around the innermost high index core layer, and their relative refractive index difference
- G02B6/03638—Optical fibres characterised both by the number of different refractive index layers around the central core segment, i.e. around the innermost high index core layer, and their relative refractive index difference having 3 layers only
- G02B6/03644—Optical fibres characterised both by the number of different refractive index layers around the central core segment, i.e. around the innermost high index core layer, and their relative refractive index difference having 3 layers only arranged - + -
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- G—PHYSICS
- G02—OPTICS
- G02B—OPTICAL ELEMENTS, SYSTEMS OR APPARATUS
- G02B6/00—Light guides; Structural details of arrangements comprising light guides and other optical elements, e.g. couplings
- G02B6/02—Optical fibres with cladding with or without a coating
- G02B6/036—Optical fibres with cladding with or without a coating core or cladding comprising multiple layers
- G02B6/03616—Optical fibres characterised both by the number of different refractive index layers around the central core segment, i.e. around the innermost high index core layer, and their relative refractive index difference
- G02B6/03661—Optical fibres characterised both by the number of different refractive index layers around the central core segment, i.e. around the innermost high index core layer, and their relative refractive index difference having 4 layers only
- G02B6/03666—Optical fibres characterised both by the number of different refractive index layers around the central core segment, i.e. around the innermost high index core layer, and their relative refractive index difference having 4 layers only arranged - + - +
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- G—PHYSICS
- G02—OPTICS
- G02B—OPTICAL ELEMENTS, SYSTEMS OR APPARATUS
- G02B6/00—Light guides; Structural details of arrangements comprising light guides and other optical elements, e.g. couplings
- G02B6/02—Optical fibres with cladding with or without a coating
- G02B6/036—Optical fibres with cladding with or without a coating core or cladding comprising multiple layers
- G02B6/03616—Optical fibres characterised both by the number of different refractive index layers around the central core segment, i.e. around the innermost high index core layer, and their relative refractive index difference
- G02B6/03661—Optical fibres characterised both by the number of different refractive index layers around the central core segment, i.e. around the innermost high index core layer, and their relative refractive index difference having 4 layers only
- G02B6/03683—Optical fibres characterised both by the number of different refractive index layers around the central core segment, i.e. around the innermost high index core layer, and their relative refractive index difference having 4 layers only arranged - - + +
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- G—PHYSICS
- G02—OPTICS
- G02B—OPTICAL ELEMENTS, SYSTEMS OR APPARATUS
- G02B6/00—Light guides; Structural details of arrangements comprising light guides and other optical elements, e.g. couplings
- G02B6/24—Coupling light guides
- G02B6/26—Optical coupling means
- G02B6/268—Optical coupling means for modal dispersion control, e.g. concatenation of light guides having different modal dispersion properties
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- G—PHYSICS
- G02—OPTICS
- G02B—OPTICAL ELEMENTS, SYSTEMS OR APPARATUS
- G02B6/00—Light guides; Structural details of arrangements comprising light guides and other optical elements, e.g. couplings
- G02B6/24—Coupling light guides
- G02B6/26—Optical coupling means
- G02B6/28—Optical coupling means having data bus means, i.e. plural waveguides interconnected and providing an inherently bidirectional system by mixing and splitting signals
- G02B6/293—Optical coupling means having data bus means, i.e. plural waveguides interconnected and providing an inherently bidirectional system by mixing and splitting signals with wavelength selective means
- G02B6/29304—Optical coupling means having data bus means, i.e. plural waveguides interconnected and providing an inherently bidirectional system by mixing and splitting signals with wavelength selective means operating by diffraction, e.g. grating
- G02B6/29316—Light guides comprising a diffractive element, e.g. grating in or on the light guide such that diffracted light is confined in the light guide
- G02B6/29317—Light guides of the optical fibre type
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- Physics & Mathematics (AREA)
- Chemical & Material Sciences (AREA)
- General Physics & Mathematics (AREA)
- Optics & Photonics (AREA)
- Dispersion Chemistry (AREA)
- Engineering & Computer Science (AREA)
- Life Sciences & Earth Sciences (AREA)
- General Life Sciences & Earth Sciences (AREA)
- Geochemistry & Mineralogy (AREA)
- Manufacturing & Machinery (AREA)
- Materials Engineering (AREA)
- Organic Chemistry (AREA)
- Optical Communication System (AREA)
- Optical Fibers, Optical Fiber Cores, And Optical Fiber Bundles (AREA)
- Optical Couplings Of Light Guides (AREA)
Abstract
Description
45 4 09 945 4 09 9
經濟部中央德荜局月工:^-;!;.;4:-;>:,;·-·!·^,:;? 發明領域: 。本發明係關於1998年9月.16日申誚·之美國第60/100495 號專利申清案,該專利曰期作為本案之優先申請日期。 運行於標準光纖介質中之光學訊號產生相當小之變化 ,在距雄内光學訊號將產生顯著之損失。—項變化包含光 色散。色散管理光纖具有正值以及負值色散特性,其長度 與平均色散乘積接近零色散。發明背景: 光色散沿著波導變化為波導材料以及結構之函數。在 j寺定波長下零色散為可能的,但是零色散係關於"四波相混 現水,其在相鄰波長頻道產生串音。四波相混在零色散情 况下最為顯著,但是隨著光學功率以及減小頻道間距而提 南。 光色散以及四波相混能夠藉由色散管理光纖而避免, 其結合正值及負值色散光纖(於所預傳送波長情況下)。因 為只有使用零色散光纖將避免四波相混。 —項使用正值色散光纖以傳送光學訊號通過長距離方 去以及色散補償模组含有捲狀物負值色散光纖以週期性地 插入色散光纖以減小合併光學路徑之平均色散。不過,補 仿模組將減小訊號功率而不會使訊號朝著預期目的前進。 正值以及負值色散光纖之長度端部對著端部拼接在一 起以更有效地傳送光學訊號而減小光色散。不過,需要計 劃保持追蹤組合光纖之色散特性,以及必需庫存兩條不同 之光纖。Monthly work of the Central German Bureau of the Ministry of Economic Affairs: ^-;!;.; 4:-; >:,; ...- !! ^,:;? Invention Field:. The present invention relates to the US Patent Application No. 60/100495 filed on September 16, 1998. The date of the patent is the priority application date of this case. The optical signal running in the standard optical fiber medium has a relatively small change, and the optical signal will cause significant losses in the distance. —The term change includes light dispersion. The dispersion management fiber has positive and negative dispersion characteristics, and its length and average dispersion product are close to zero dispersion. Background of the invention: Light dispersion changes along the waveguide as a function of waveguide material and structure. Zero dispersion is possible at a fixed wavelength, but zero dispersion is about "four-wave mixed water, which produces crosstalk in adjacent wavelength channels." Four-wave mixing is most significant in the case of zero dispersion, but it increases with optical power and reduced channel spacing. Optical dispersion and four-wave mixing can be avoided by the dispersion management fiber, which combines positive and negative dispersion fibers (at the pre-transmitted wavelength). Because only using zero-dispersion fiber will avoid four-wave mixing. The term uses positive dispersion fibers to transmit optical signals through long distances and the dispersion compensation module contains roll-shaped negative dispersion fibers to periodically insert the dispersion fibers to reduce the average dispersion of the combined optical path. However, the imitation module will reduce the signal power without moving the signal towards its intended purpose. The ends of the positive and negative dispersion fibers are spliced together to transmit optical signals more efficiently and reduce optical dispersion. However, it is necessary to plan to keep track of the dispersion characteristics of the combined fibers, and to keep two different fibers in stock.
人通用中國國家標準(CNS ) Λ4規格(_ 210X m公釐) (讀先閱讀背面之注意事項再填寫本頁) .^. --5 線 454 09 954 09 9五、發明説明(2- A7 B7 經滴部中央#-局負工消带合: 色散管理光纖亦製造為連續性地長度,其具有交替性 區段,其在欲傳送波長下具有相反之色散符號。只需要庫 存一種光纖,但是色散週期在製造時(即,在重複兩個區段 之長度)必需加以選擇以及在往後並不能加以改變。在區 段間之界面處污染亦可能進入光纖,其在抽拉為最終形式· 也必品各別地加以拇光以及組合。 色散管理線纜包含一對或多對光纖,其色散符號為相 反的。線欖區段拼接在一起,使得一個區段之正值色散光 纖連接至相鄰區段之負值色散光纖。再次地,需要追縱區 段長度之色散計劃,以及各別光纖設計受到限制,因為相反 符號色散在傳送波長下必需為相等大小。 發明大要: 本發明包含光學系統各種實施例,其補償光色散以及 避免四波相混,同時減小光纖之庫存以及在設計提供更加 彈性以及光纖特性。同時可能為較短色散週期(即重複在 色散變化内之長度)而在製造後不會使製造以及其他色散 參數選擇變為複雜。 一項.實施例為色散補償光纖系統,其包含單模光纖,該 光纖具有一組多個連續性光學路徑,其具有不同色散特性 以傳輸光學訊號。一條光學路徑在光學訊號之中央波長下 呈現出正值色散,以及另外一條光學路徑在光學訊號之中 央波長下呈現出負值色散。耦合機制偏移光學訊號於兩條 路徑前進部份之間,在光學訊號之中央波長下該路徑長度 乘以平均色散值接近零。優先地,色散以及色散斜率在中 (CNS ) Λ4規格(210X 297公斧) r (請先閱讀背而之注意事項再填寫本頁) •装'GM China National Standard (CNS) Λ4 specification (_ 210X m mm) (read the precautions on the back before filling this page). ^. --5 Line 454 09 954 09 9 V. Description of the invention (2- A7 B7 via the central part of the drop section # -offset elimination: Dispersion management fiber is also manufactured as a continuous length, which has alternating sections, which have the opposite dispersion sign at the wavelength to be transmitted. Only one fiber is required to be stocked, However, the dispersion period must be selected at the time of manufacture (ie, repeating the length of the two sections) and cannot be changed later. Contamination may also enter the fiber at the interface between the sections, which is drawn into the final form · It is also necessary to add the light and combination separately. The dispersion management cable contains one or more pairs of optical fibers, and the dispersion symbols are opposite. The segments of the cables are spliced together so that a segment of positive dispersion fiber is connected. Negative dispersion fibers to adjacent sections. Again, the dispersion plan that needs to track the length of the section and the design of the individual fibers are limited because the opposite sign dispersion must be equal in size at the transmission wavelength. Important: The present invention includes various embodiments of optical systems that compensate for optical dispersion and avoid four-wave mixing, while reducing the fiber inventory and providing more flexibility and fiber characteristics in the design. At the same time, it may be a shorter dispersion period (that is, repeating in The length within the dispersion variation) does not complicate manufacturing and other dispersion parameter selection after manufacturing. One. An embodiment is a dispersion-compensated fiber system that includes a single-mode fiber that has a set of multiple continuous optics Path, which has different dispersion characteristics to transmit optical signals. One optical path exhibits positive dispersion at the central wavelength of the optical signal and the other optical path exhibits negative dispersion at the central wavelength of the optical signal. Coupling mechanism shift The optical signal is between the two forward parts of the path. At the central wavelength of the optical signal, the path length multiplied by the average dispersion value is close to zero. Preferentially, the dispersion and dispersion slope are in the middle (CNS) Λ4 specification (210X 297 male axe). r (please read the precautions before filling this page)
、-J ------.I 1 1-:11 • mu t ....... - - mt · ίκΊ Β7 五、發明説明 ίΐίΓ為相匹配的,使得整個波長範圍内平均色散接近 (請先閱讀背面之注意事項再填寫本頁) 連、纟胃性光學路麵触此平行或目心地延伸,以及越 =何干频合辆,路彳㈣鱗訊號偏移並不會干擾任 !一甘條路經。例如,單—光纖能夠製造出具有-組多條心 =、f包繞著。每1蕊形成—條光學路徑,其具有 不同的色散特性。 ^號此夠藉她合機制成為—條或多條長職光拇而 =心為間正值地偏移。_合機制能夠藉由心蕊之間距使心 '為放置相當靠近在—起以維持訊號轉移而產生作用。後者 耦合模在心蕊間需要對稱性色散之特性以及具有色散週期 寺於心蕊間之1¾合長度。前綠合模能_由在不相等間 距處偏移職心蕊間使心蕊之色散躲產生更大彈性。 她合模錢,正似及貞值色散4之色散斜率優先地 相匹配(例如為低數值或相反符號)使得形成平均色散保持 為接近零。. ’、 ^另外-個實施爿包含光纖區段,其具有一對或多對相 反付號色.散特性之心為。區段端部對著端部拼接為一扭 其具有-個區段正值色散心蕊與另外—個色^ 心蕊對準。區段長度之選擇使長度與平均紐值乘積接近 零。每-對心蕊能夠平行地傳送訊號,其藉由正值與負值 色散之絕飽直相t以及藉由S -個區段中對準相鄰區段之 心蕊達成,該相鄰區段為相反符號之正值與負值色散。多 對正值及負值色散心蕊能夠獨立地排列以保持大於一個位 度適用中國囡家標準(CNS )八4規格(210 X m公釐) 454 09 9 八7 B7 五、發明説明(屮)、 -J ------. I 1 1-: 11 • mu t .......--mt · ίκΊ Β7 V. Description of the invention ίΐίΓ is matched so that the average dispersion in the entire wavelength range is close to (Please read the precautions on the back before filling in this page) Even if the optical pavement of the stomach and the stomach extend in parallel or intently, and the frequency is equal to the number of cars, the signal deviation of the road scale will not interfere with it! A sweet road. For example, a single-fiber can be manufactured with -groups of multiple cores =, f wrapped around. Each core forms an optical path, which has different dispersion characteristics. The ^ number is enough to be a combination of one or more long-term jobs and = a positive shift in heart. The _he mechanism can make the heart's place quite close to each other by the distance between the cores and cores to maintain the signal transfer. The latter coupling mode requires symmetrical dispersion characteristics between the cores and a length of 1¾ between the cores. Anterior green mold clamping energy_By shifting between the cores and cores at unequal distances, the dispersion of the cores will be more flexible. For the mold coin, the dispersion slopes of the positive value and the positive value dispersion 4 are matched preferentially (for example, with low values or opposite signs) so that the average dispersion is kept close to zero. ′, ^ Another implementation includes a fiber section that has one or more pairs of opposite sign dispersion and dispersion characteristics. The end of the segment is spliced into a twist opposite the end. It has one segment positive dispersion core and the other color ^ core. The length of the segment is chosen so that the product of the length and the average button value approaches zero. Each pair of cores can transmit signals in parallel, which is achieved by the absolute saturation t of positive and negative dispersion t and by the cores of the S-segment aligned to the adjacent segment, the adjacent area Segments are positive and negative dispersion with opposite signs. Many pairs of positive and negative dispersive cores can be independently arranged to maintain greater than one degree. Applicable to China National Standard (CNS) 8 4 specifications (210 X m mm) 454 09 9 8 7 B7 5. Description of the invention (屮)
I -¾ 辑率或顧之傳送。色料tj級大雜絲夠藉由控 制相鄰區段間角度性刻痕變為可能的以對準多心猱不同 之組合,該心蕊具有不同的色散特性。 單一光纖亦能夠製造為,多模光纖,其具有基模路徑以 及較尚階模路徑,其具有不同的色散值以形成具有不同色 散特性之同心圓光學路徑。該更進一步實施例耦合機制包 备個或多個模輕合器,其亦能夠形成為逐漸變化耗合或 長週期光栅以偏務光學訊號於基模與較高模路徑之間。.. 基模能夠排列為呈現出正值色散,以及較高階模能夠 加以排列以呈現出為較小數值之負值色散。因而,該排列 之模耦合器放置作為偏移光學訊號進入基模以作為較長間 距而大於較咼階模。不過,具有適當心蕊分佈以及選擇標 準化頻率,基模以及第二階模之色散以及色散斜率能夠為 相專大小但是符號相反。同時,較佳訊號限制有可能在標 準化頻率值而遠離模截止數值。 不同的連接器能夠在多心蕊或多模光纖中加以使用以 傳送通過訊號進入單模單心蕊光纖内。例如,能夠使用光 柵以偏移光學訊號由一條心蕊g移至另外一條心蕊,其對 準於單模單一心蕊光纖或由較高階至基模以藉由單模單一 心蕊光纖作更進一步傳送。逐漸變化耦合亦能夠使用來促 使訊號進入單一心蕊或進入基模。除此,分離單模單一心 ‘黑光纖能夠連接至多心蕊光纖之不同心蕊,以及一個切換 器能夠使用來更進一步傳送訊號由一條連結光纖至共同單 模單一心蕊光纖。 '(請先Μ讀背面之注意事項再填寫本頁) -裝·I-¾ edit rate or transfer. The large jigsaws of the pigment tj level can be made possible by controlling the angular notches between adjacent sections to align different combinations of multiple cores, which have different dispersion characteristics. A single optical fiber can also be manufactured as a multimode fiber with a fundamental mode path and a higher order mode path with different dispersion values to form concentric circular optical paths with different dispersion characteristics. The coupling mechanism of this further embodiment includes one or more mode light couplers, which can also be formed as gradually changing consumable or long-period gratings to bias optical signals between the fundamental mode and the higher mode path. .. Fundamental modes can be arranged to exhibit positive dispersion, and higher order modes can be arranged to exhibit negative dispersion with smaller values. Thus, the arrayed mode couplers are placed as offset optical signals into the fundamental mode as longer distances than the higher order modes. However, with proper core distribution and selection of the normalized frequency, the dispersion and dispersion slope of the fundamental and second-order modes can be phase-specific, but with opposite signs. At the same time, it is possible that the better signal limit is far away from the mode cutoff value at the standardized frequency value. Different connectors can be used in multi-core or multi-mode fibers to transmit signals into single-mode single-core fibers. For example, a grating can be used to shift the optical signal from one core to another core, which is aligned with a single-mode single core fiber or from a higher order to the fundamental mode for further transmission through a single-mode single core fiber . Gradual coupling can also be used to force the signal into a single stamen or into the fundamental mode. In addition, the separated single-mode single-core ‘black fiber can be connected to different cores of a multi-core fiber, and a switch can be used to further transmit signals from a link fiber to a common single-mode single-core fiber. '(Please read the precautions on the back before filling in this page)
、1T 線 .氏張尺度通用中國固家標準 (CNS ) Λ4規格(210X297公釐) ^54 09 9 A7 ——_ B7 五、發明説明(.f ) (請先閲讀背面之注意事項再填寫本頁) 能夠利用傳統的處理過程製造多模光纖,其具有模色 散特性。多心蕊光纖能夠藉由組合兩條或多條心蕊桿件在 預製件内於傳統抽拉光纖之前。能夠使用不同排列之管件 或桿件以對準以及分隔心蕊桿件,以及粉塵外包層能夠加 以固結於心蕊結;^四週以密閉結構體於預製件内。 附圖簡單說明: 第一曱圖(圖1A)為多心蕊光纖放大圖,.其具有兩個不 同色散特性之偏移心蕊。 第一乙圖(圖1B)為另外一個多心蕊光纖之類似;^大圖 ,其具有一個位於中央之心蕊以及一個偏移心蕊,其具有不 同的色散特性。 第一丙圖(圖1C)為另外一個多心蕊光纖之類似放大圖 ,_其具有兩條不同色散特性之同心圓心蕊。. 第二圖為較小之放大側視圖,其顯示出兩個相對旋轉 以及拼接在一起多心蕊光纖之區段長度。 第‘·三甲圖(圖3A)及第三乙圖(圖3B)包含兩個心蕊之多 心.游光纖折射率分佈,其折射率為心蕊半徑"r"之函數。 笫二.丙圖(獨.3C)至第三,已圖(圖3F)包含相互交替折射 率分佈,其特別適合達成負值色散。 第四圖(圖4)為另外一個示意性改變之多心蕊光纖側 視圖,其包含長週期光栅以光學地耦合兩條心蕊。 第五圖(圖5)為具有四心蕊之多心蕊光纖放大端視圖, 其中兩個心蕊為正值色散特性以及兩個為負值色散特性。 第六圖(圖6)為逐漸變化耦合之側視圖以連接圖1A多 本紙張尺度適用中國國家標华(CNS ) Λ4規格(210 X 297公芨) 一09 9 .心蕊光纖之兩條心蕊至傳統單一心蕊光纖。 第=圖(圖7)為輕合側視圖,其偏移訊號於多心蕊光纖 兩,^與連接◎之間,該連接器連結多^蕊光纖之兩條 心蕊之-至傳統單—心蕊光纖之心蕊。 第八圖(圖8)為多模光纖之側視圖,其具有連續性長週 期光柵以偏觀號祕有不㈣鋪性模間。 —第,九圖(圖9)為以階躍分佈心蕊設計為例之標準化傳 .播苇参bn與多模光纖標準化頻率"之曲線圖。 第十圖(圖10)為相同階躍分饰心蕊詨計之標準化波導 色散dn與波導標準化頻率,,.ν”曲線圖。 第十圖(圖11)為支撐兩個心蕊桿件於開孔桿件内之 放大端視圖。 第十-圖(圖12)為支撐兩個心蕊桿件於管件内之相同 大小端視圖。 、第十二圖(圖13)騎由特卿狀桿件將兩個心蕊桿件 黏附在一起之相同大小端視圖。 第卞四圖(®14)糾—個相同大小端棚,其顯示出 :個心蕊桿件_在—起於融合織件於兩條心蕊週圍之 前。 . . 附圖簡單說明: 光纖10,10’,10";光纖區段1〇Α,1〇β;心蕊12,12 f ’14,14’,14'’;心蕊风機14&刚;包層.16,16’ 中心軸18,18’;中心轴18A,⑽;刻痕%光糖冰光 3〇;心蕊32, 34, 36, 38;包層40;心蕊44;中心軸邮、 1T line. The scale of Zhang ’s scale is in accordance with the general Chinese solid standard (CNS) Λ4 specification (210X297 mm) ^ 54 09 9 A7 ——_ B7 V. Description of the invention (.f) (Please read the notes on the back before filling in this Page) Multimode fiber can be manufactured using traditional processing, which has modal dispersion characteristics. Multi-core fiber can be combined in a preform before traditionally pulling fiber by combining two or more core rods. Different arrangement of pipes or rods can be used to align and separate the core core members, and the dust cover can be consolidated to the core core; ^ surrounded by a closed structure in the preform. Brief description of the drawings: The first diagram (Figure 1A) is an enlarged view of a multi-core fiber, which has two offset cores with different dispersion characteristics. Figure 1B (Figure 1B) is similar to another multi-core fiber; ^ large figure, which has a central core and an offset core, which have different dispersion characteristics. The first C figure (Figure 1C) is a similar enlarged view of another multi-core fiber, which has two concentric cores with different dispersion characteristics. The second image is a smaller enlarged side view showing the lengths of two segments that are relatively rotated and spliced together. The first three graphs (Fig. 3A) and the third graph (Fig. 3B) contain the refractive index distribution of the two cores of the core. The refractive index is a function of the radius of the cores " r ". Figures II.C (Single. 3C) to third. Figures (Figure 3F) contain alternate refractive index distributions, which are particularly suitable for achieving negative dispersion. The fourth figure (Figure 4) is another schematic view of a multi-core fiber that includes a long-period grating to optically couple the two cores. The fifth figure (FIG. 5) is an enlarged end view of a multi-core fiber with four cores, in which two cores have positive dispersion characteristics and two have negative dispersion characteristics. The sixth figure (Figure 6) is a side view of gradually changing coupling to connect multiple paper sizes in Figure 1A. It is applicable to China National Standards (CNS) Λ4 specification (210 X 297 cm)-09 9. The two cores of the core fiber Core to traditional single core fiber. Figure = (Figure 7) is a side view of the light closing, the offset signal is between the two core fiber ^ and the connection ◎, this connector connects the two core fiber of the multi core fiber-to the traditional single- Heart Core of Heart Fiber. The eighth figure (Figure 8) is a side view of a multimode optical fiber, which has a continuous long-period grating with a non-patterning mode and a non-patterning mode. —The ninth figure (Figure 9) is the standardization transmission using the step-distribution core design as an example. The curve diagram of the sowing reed bn and the standardized frequency of multimode fiber ". The tenth figure (Fig. 10) is a graph showing the normalized waveguide dispersion dn and the waveguide normalized frequency, .ν "of the same step-separated heart core meter. The tenth figure (Fig. 11) is to support two core members An enlarged end view of the hole-shaped member. The tenth-figure (fig. 12) is an end view of the same size that supports the two core rods in the tube. An end view of the same size where two core rods are glued together. Figure 24 (®14) corrects an end shelf of the same size, which shows: a core rod_ 在 —starts from the fusion fabric Before the two cores are around... Brief description of the drawings: Optical fiber 10, 10 ', 10 " Optical fiber section 10A, 1〇β; Heart core 12, 12 f '14, 14', 14 '' Cardiac fan 14 &rigid; cladding. 16, 16 'central axis 18, 18'; central axis 18A, ⑽; score% light sugar ice light 30; core 32, 34, 36, 38; package Layer 40; heart 44; central axis post
454 09 9 ‘ . A7 ___ B7五、發明説明(7) 經濟部中央標毕局一只工消泞合作社印製 變孝禺合區域60;波導62, 64;心蕊66;光纖7q.基板π. 光纖80;心‘品82,包層84;光拇86;中心軸88 v預擊件 90;桿件92,心'孤'木?·件94, 96;玻璃粉塵⑽;預.事件ίο。. 玻璃桿件102,104;填充桿件1〇6,108;管件11〇;粉塵’ 112;桿件114;心蕊桿件116,118;預製件12〇;包^^22; 預製件130;心蕊桿件132,134;粉塵136。 詳細說明: 圖1A所顯示多心蕊光纖10具有正值色散心蕊12以及負 值色散心蕊14並由共同包層1帽繞著。相反符號色散之兩 個心說'12及14係指對一個波長範圍(通常相當於飼^之放大 頻窗)之中央波長而言,其由光纖10所傳送。對於由丨53〇nm 至1560·錄内4鮮理,設収值心蕊能夠類似 於SMF 1528光纖,以及設計負值心蕊能夠類似於1585 LS之 產物。兩種光纖可由本公司提供。對於其他波長範圍,能 夠使用不同形式之已知心蕊設計,其簡單地制如下。:雨條减取1镇光纖戦學巾心贿平行延伸以及 分隔,離"S",該距離能夠加以調整以防止或促使自動柄合 於心蕊12及14之間。如圖所示,距離"s"假設相當大足以防 止自動,合。在製造過程中,心蕊_桿件比值約為〇· 4或更 大之心蕊桿件通常分隔相#聰以產生所需要之隔離。在 ,纖10=邊中附加性刻痕2(3提供光纖1()角度性指標區段長 度之參考點。 在圖2<兩個最初為連續性先_之區段長度舰與 10B軸向地對準以及相對地繞著,其解中心轴碰及⑽ 本纸狀度適用中囡國家樣 (請先閱讀背而之注意事項再填寫本页) •装- 訂 線 10 4 5 4 099 A7 B7 五、發明説明(g·) 經濟部中央福舉局負工消費合作社印¾ 旋轉於拼接在一起之前,其利用例如拼接器以設計作為保 持偏極性光纖。選擇旋轉大小將使光纖區段1〇A之正值色 政心遂12A與光纖區段10B負值色散心蕊14B對準。除此,設 計之對稱性亦能夠使光纖區段10A之負值色散心蕊14A與光 纖區段12B正值色散心蕊12B對準。區段l〇A及10B長度能夠 加以調整而異於沿著兩個區段丨0A與丨〇β合併長度,以及沿 著任何後續一對區段之平均色散接近零色散。 假如在每一區段10Α及10Β中兩條心蕊12Α, 14Α以及12Β ,14Β使用來傳輪不同的訊號,兩條心蕊正值及負值色散大 小相同以及兩個區段10Α以及10B在長度上應該為相等的。 不過,假如每一區段只有一條心蕊傳輪訊號(例如為區段1〇 Α之心蕊12Α以及區段1 〇Β之心蕊14Β),則兩條心蕊色散能夠 在不同大小處能夠加以最佳化以及不同長度區段能夠結合 以得到平均色散為接近零。兩條心蕊色散斜率優先地相匹 配以保持在整個傳送波長範圍内保持平均色散接近零。 並不拼接區段化長度之光纖以交替光學路徑於正值與 負值色散心蕊12與14之間,被動性或主動性耦合能夠產生 於心蕊12與14向前長度之間。被動性耦合能夠藉由減小心 蕊間分離"S11使得功率轉移以所需要色散週期在心蕊之間 發生該週期等於耦合長度。心蕊12及14正值及負值色散 應該為對稱於中央波長(其大小相等),因為訊號在每一心 洛.12及14中佔用一半時間。視為隔離之兩條心蕊12與丨4之 傳播係數應該儘可能地相同以保持更完全之功率轉移。耦 合長度由複合波導兩個最低階超模之傳播係數差值所決定 泰纸张尺度適用中囡國家榇準(CNS )以規格(2丨〇><297公犮) (锖先閱讀背面之注意事項再填寫本頁) -裝 訂 線 以及能夠設計作為消色性或光色性。 圖3A以及3B顯示出正值與負值色散心蕊12及14之折射 率分伟,其肖^列加以變使兩條心蕊12與14間之有效折射 率為相等的。正值色散心蕊12具有簡單階躍分佈(Ge〇2—454 09 9 '. A7 ___ B7 V. Description of the invention (7) Printed by the Industrial Standards Bureau of the Ministry of Economic Affairs of the Central Government Bureau of the Industrial Cooperatives Co., Ltd. 60; waveguide 62, 64; core 66; optical fiber 7q. Substrate π Optical fiber 80; heart 82, cladding 84; light thumb 86; center axis 88 v pre-strike 90; rod 92, heart 'solitary' wood? · Pieces 94, 96; glass dust 预; pre.event ίο . Glass rods 102,104; filled rods 106, 108; tube members 11; dust '112; rods 114; core rods 116, 118; preforms 12; packs ^^ 22; preforms 130; core rods Pieces 132,134; dust 136. Detailed description: The multi-core fiber 10 shown in FIG. 1A has a positive dispersion core 12 and a negative dispersion core 14 and is surrounded by a common cladding 1 cap. The two symbols of opposite sign dispersion, '12 and 14 ', refer to the central wavelength of a wavelength range (usually equivalent to the amplification window of the feedband), which is transmitted by the optical fiber 10. For the range from 530nm to 1560nm, the set core value can be similar to the SMF 1528 fiber, and the design negative core value can be similar to the product of 1585 LS. Two kinds of fiber can be provided by our company. For other wavelength ranges, different forms of known cardiac designs can be used, which are simply made as follows. : The rain bar is reduced by 1 parallel extension and separation of the heart fiber of the fiber optic school towel, and the distance from "S" can be adjusted to prevent or promote the automatic handle to fit between the heart cores 12 and 14. As shown in the figure, the distance " s " is assumed to be quite large enough to prevent automatic closing. In the manufacturing process, a core-bar member with a core-to-bar ratio of about 0.4 or greater is usually separated by a phase #sat to produce the required isolation. In the fiber 10 = additional nick 2 in the side (3 provides the reference point for the optical fiber 1 () angle index section length. In Figure 2 < the two initial section length continuity ship and 10B axis Ground alignment and relative rotation, the solution center axis hits ⑽ This paper is suitable for China and the country (please read the precautions on the back first and then fill out this page) • Binding-Thread 10 4 5 4 099 A7 B7 V. Description of the invention (g ·) Printed by the Central Consumers' Bureau of the Ministry of Economic Affairs, the Consumer Cooperatives of the Ministry of Economic Affairs ¾ Rotating before splicing together, it uses, for example, a splicer to design it as a polarized maintaining fiber. Choosing the size of the rotation will make fiber section 1 〇A's positive value 12A is aligned with the negative dispersion core 14B of the optical fiber section 10B. In addition, the design symmetry can also make the negative dispersion core 14A of the optical fiber section 10A and the optical fiber section 12B Positive dispersion center alignment 12B. The lengths of the segments 10A and 10B can be adjusted to differ from the combined length of the two segments 丨 0A and 〇β, and the average dispersion along any subsequent pair of segments Close to zero dispersion. Suppose that the two cores 12A, 14A and 12B in each segment 10A and 10B. 14B is used to transmit different signals. The positive and negative dispersion values of the two cores are the same and the two segments 10A and 10B should be equal in length. However, if there is only one cardiac transmission signal in each segment (For example, the heart core 12A of segment 10A and the heart core 14B of segment 1 〇B), the dispersion of the two cores can be optimized at different sizes and the segments of different lengths can be combined to obtain an average The dispersion is close to zero. The dispersion slopes of the two cores are preferentially matched to keep the average dispersion close to zero over the entire transmission wavelength range. Fibers without segmented lengths are spliced with alternating optical paths at positive and negative dispersion centers. Between cores 12 and 14, passive or active coupling can occur between the forward lengths of the cores 12 and 14. Passive coupling can reduce the separation between the cores " S11 so that the power transfer is centered on the required dispersion period The period between cores is equal to the coupling length. The positive and negative dispersion of cores 12 and 14 should be symmetrical to the central wavelength (which is equal in size), because the signal is occupied in each core. 12 and 14. Half-time. The propagation coefficients of the two cores 12 and 4 regarded as isolated should be as same as possible to maintain more complete power transfer. The coupling length is determined by the difference between the propagation coefficients of the two lowest-order supermodes of the composite waveguide. Paper size applies to China National Standards (CNS) to specifications (2 丨 〇 > < 297g) (锖 Read the precautions on the back before filling this page)-Gutter and can be designed as achromatic or light Figures 3A and 3B show the positive and negative dispersion of the refractive indices of the cores 12 and 14, respectively, and the difference is changed so that the effective refractive indices between the two cores 12 and 14 are equal. Positive The value dispersion core 12 has a simple step distribution (Ge〇2—
Si 〇2心蕊具有Si 〇2包層)以及有效折射率” n(奶)"在心蕊 與包層值之間。負值色散心蕊丨4具有"w形式"或區段化心 :分饰之3又计,其具有些微提高包層折射率之摻雜劑以與 正值色散心為12有效折射率"neff"相匹配。例如,含有摻 雜劑包層能夠由Ge〇2-Si〇2或Ti〇2-SiO//f構成。(注意:圖 3B虛線代表圍繞著石夕石包層16之折射率大小。) 通常,較為複雜分佈形狀需要形成負值色散以及色散 斜率異於具有正值色散心蕊之情況。另外四個範例描繪於 圖3C-3F中,每一情況能夠維持負值色散而不會過度地損及 其他光學特性例如為有效面積,模場直徑,彎曲,以及微彎 曲。與分佈線相交之箭頭表示設計之彈性以改變分佈之各 個線段。 使用圖3C分佈達成具有正值或負值色散斜率之正值或 負值色散.。圖3D設計特別使用作為達成具有相當大有效面 積之正值或負值色散。後者兩個設計圖3£及邡能夠考慮作 為色散控制,其製造時為低耗損。 在心:12與14間有效輕合能夠在如圖4所示之心蕊間 ,由形成一個或多個長週期光柵24而達成。耦合功能為局 部的,因而兩條心蕊12及14能夠獨立地設計。例如,心蕊12 與14間傳播係數以及心蕊色散本小能夠加以改變。光柵24 木紙張尺^TfSii 準(CNSy^M 210x-^^y D4〇99 .A7 ~~---· ‘_B7五.、發明説明(P) 1 ΊΛ 經濟部中央標毕局员二ίίίφί合作.,-ΐ-t.: 間之間距能夠加以調整以補償心蕊色散之不同大小,因而 與長度相乘之平均值仍然接近零色散。能夠使用逐漸變化 部份以及長週期光栅24以放大耦合功能。 - 長週期光栅24能夠由光色敏心蕊材料形成,其暴露於 化學線放射圖案以在光纖1〇中產生刻痕擾動。心茂} 14間之包層區域亦能夠製造為光學刻痕以提昇耦合功能 。長週期光栅24能夠藉由高功率準分子雷射劃記於光纖抽 拉操作過程中。色散週期能夠為十分小以及多種,因為耦 合機制不能對光纖10增加污染物。 _光栅精確性為非常嚴格的,因為所需要頻譜效應頻帶 為十分見廣以及長週期光柵,其通常週期約為數百微米。 同時刻痕擾動大小為十分低(避免氫氣加載之需要),因為 長週期光柵24會沿著光纖1〇佔據相當大的距離(例如為一 米或二米)而不會有負面之影響。刻度擾動能夠一次劃記 一點或立即劃記數點,特別是在高度抽拉速度。刻痕或曲 率之擾動亦能夠使用高功率C〇2雷射劃記於抽拉操作過程 中以完成類似的耦合功能。能夠使用其他擾動以形成類似 的光柵包含藉由週期地擠壓光纖或路徑長度變化或藉由週 期性微彎油路徑長度變化產生之壓力變化。 長週期光柵以及模麵合器其他資訊能夠在VengSarkar 專人之 Long-Period Fiber Gratings, as Band-Rejection Filters,發表於Journal of Ligthwave Technology, Vol, 14,No. 1,JanuaiT 1996,pages 58-65文獻中,及P〇〇le 等人之"HelicaJL-Grating Two-Mode Fiber Spatial-Mode ★纸張尺度適用中國國家梂準(..CNS)以現格(2丨0><297公釐) 13 ' (請先Μ讀背面之注意事項再填寫本頁) .裝Si 〇2 core has Si 〇2 cladding) and effective refractive index "n (milk)" between the core and cladding value. Negative value dispersion core 丨 4 has "w form" or segmentation Mind: The third decoration is added, and the dopant with a slight increase in the refractive index of the cladding layer matches the positive refractive index of 12 effective refractive index " neff ". For example, the cladding containing the dopant can be made of Ge 〇2-Si〇2 or Ti〇2-SiO // f. (Note: the dashed line in Figure 3B represents the refractive index of the stone cladding layer 16.) Generally, more complex distribution shapes need to form negative dispersion and The dispersion slope is different from the case with positive dispersion cores. The other four examples are depicted in Figures 3C-3F. Each case can maintain negative dispersion without unduly compromising other optical characteristics such as effective area, mode field Diameter, bend, and microbend. The arrows that intersect the distribution line indicate the flexibility of the design to change the various line segments of the distribution. Use the distribution of Figure 3C to achieve positive or negative dispersion with a positive or negative dispersion slope. Figure 3D design Specially used as reaching with a considerable effective area Positive or negative dispersion. The latter two design diagrams 3 £ and 邡 can be considered as dispersion control, which has low loss during manufacture. Attention: Effective light coupling between 12 and 14 can be between the cores as shown in Figure 4. Is achieved by forming one or more long-period gratings 24. The coupling function is local, so the two cores 12 and 14 can be independently designed. For example, the propagation coefficients between the cores 12 and 14 and the core dispersion can be small. Change it. Grating 24 wooden paper ruler ^ TfSii standard (CNSy ^ M 210x-^^ y D4〇99 .A7 ~~ --- '' _B7 V. Description of the invention (P) 1 ΊΛ Member of the Central Bureau of the Ministry of Economic Affairs Two ίίίφί cooperation.,-Ϊ́-t .: The interval can be adjusted to compensate for the different sizes of cardioid dispersion, so the average value multiplied by the length is still close to zero dispersion. Gradual changes can be used and long-period gratings24 Coupling function for magnification.-The long-period grating 24 can be formed of a light-color sensitive core material, which is exposed to a chemical radiation pattern to create a scoring disturbance in the optical fiber 10. The cladding region between 14 and 14 can also be manufactured Optical scoring to improve coupling function. Long period light 24 can be marked by the high-power excimer laser during the drawing operation of the fiber. The dispersion period can be very small and various, because the coupling mechanism cannot add contaminants to the fiber 10. The accuracy of the grating is very strict because The required spectrum effect frequency band is a very common and long-period grating, which usually has a period of about several hundred microns. At the same time, the size of the scratch disturbance is very low (to avoid the need for hydrogen loading), because the long-period grating 24 will run along the fiber 10. Occupies a considerable distance (for example, one or two meters) without negative effects. Scale disturbances can mark one point at a time or immediately count the number, especially at the height pull speed. The scoring or curvature disturbance can also be marked with a high-power CO2 laser during the drawing operation to accomplish a similar coupling function. The ability to use other perturbations to form similar gratings includes pressure changes generated by periodically extruding fiber or path length changes or by periodic microbend path length changes. Other information about long period gratings and die face combiners can be found in Long-Period Fiber Gratings, as Band-Rejection Filters by VengSarkar, published in Journal of Ligthwave Technology, Vol, 14, No. 1, JanuaiT 1996, pages 58-65. Medium, and Pohl and others, " HelicaJL-Grating Two-Mode Fiber Spatial-Mode ★ The paper size is applicable to China National Standards (..CNS) to present (2 丨 0 > < 297 mm) 13 '(Please read the precautions on the back before filling this page).
、1T 454099 、’ A7 —--;--B7五、發明說明(丨丨) 2 1 經濟部中央摞準-^貝工消货合汴仕印製 C〇uple:r 亦發表於Joumal _〇f Ligthwave Technology, '_〇* 5,May 1991,pages..598-604文獻中。兩篇 文章在此加入作為參考之用。 ; 大於兩條心蕊能夠形成於單一光纖中,如圖5所示。兩 條正值色散心蕊32及34以及光纖之兩條負值色散心蕊36及 38能夠由共同包層_繞著。心蕊32-38能夠以正值及負 值色散心蕊分組地配對(例如為32,36以及34,38),以及成 對心蕊能夠對各別位元速率或應用加以最佳化。可加以變 化,在光纖30相鄰區段間藉由改變角度地標記配對能夠加 =變化以對色散計劃產生更,大彈性。換言之,相同光纖30 能夠使用來維持-組多個不同的色散計劃。虛擬心蕊44提 供角度地標記光纖3〇之參考點於光學中心軸46週圍。 類似光纖10之心蕊12及14,光纖30心蕊32, 34, 36及38 偏移光學巾^滅,其錢產生雛模色制題。能夠使 用週期性扭轉或連續磕旋轉光纖1〇或3〇以減小該問題。光 纖10之心蕊12以及14或光纖3〇之心蕊32, 34,36及38能夠藉 由各別包層區域圍繞著以使通過光纖1〇及3〇之分離光學路 徑性能最佳化。 當連接至傳統單模光纖或類似波導結構例如為即時放 大器工作站或連接端部處,每一對兩條心蕊係關於傳統波 導之單一心蕊。圖6描繪出漸變耦合區域6〇,其連接色散管 理光纖10至傳統單模光纖7〇。兩條波導62與64對準於光纖 10之正值以及負值色散心蕊12及14,但是只有波導64對準 於傳統光纖70之單一心蕊66。在耗合區域内,兩條波導62 本纸张尺度適用中國囤家標準(CNS )六4規格(2丨0X 297公费)\ψ I---------裝-- (請先閱讀背而之注意事項再填寫本頁) 、1Τ 線 4 5 4 09 9 A7 B7, 1T 454099, 'A7 —--; --B7 V. Description of the invention (丨 丨) 2 1 Printed by the Central Government of the Ministry of Economic Affairs ^ Printed by Bei Gong Consumer Goods Couple: r Also published in Joumal _〇 f Ligthwave Technology, '_〇 * 5, May 1991, pages .. 598-604 literature. Two articles are included here for reference. ; More than two cores can be formed in a single fiber, as shown in Figure 5. The two positive dispersion cores 32 and 34 and the two negative dispersion cores 36 and 38 of the optical fiber can be surrounded by a common cladding. Cortex 32-38 can be paired with positive and negative dispersive cortex groups (for example, 32, 36 and 34, 38), and the paired cortex can be optimized for individual bit rates or applications. It can be changed, and the pairing can be changed by changing the angle between adjacent sections of the optical fiber 30 to increase the flexibility of the dispersion plan. In other words, the same fiber 30 can be used to maintain-set multiple different dispersion plans. The virtual core 44 provides a reference point for optically marking the optical fiber 30 around the optical central axis 46. Similar to the cores 12 and 14 of the optical fiber 10, and the cores 32, 34, 36, and 38 of the optical fiber 30 are offset, and the money generates a prototype color problem. This problem can be reduced by periodically twisting or continuously chirping the fiber 10 or 30. The cores 12 and 14 of the optical fiber 10 or the cores 32, 34, 36, and 38 of the optical fiber 30 can be surrounded by respective cladding regions to optimize the separation optical path performance through the optical fibers 10 and 30. When connected to a conventional single-mode fiber or similar waveguide structure, such as an instant amplifier workstation or a connection end, each pair of two cores is a single core of a conventional waveguide. Figure 6 depicts a gradual coupling region 60, which connects the dispersion management fiber 10 to a conventional single-mode fiber 70. The two waveguides 62 and 64 are aligned with the positive and negative dispersion cores 12 and 14 of the optical fiber 10, but only the waveguide 64 is aligned with the single core 66 of the conventional optical fiber 70. Within the consumable area, two waveguides of 62 paper sizes are applicable to the Chinese storehouse standard (CNS) six 4 specifications (2 丨 0X 297 public fee) \ ψ I --------- install-(Please read first Note from the back, please fill out this page), 1T line 4 5 4 09 9 A7 B7
五、發明説明(丨tJ 及64漸變地耦合在一起以傳移功率至波導以。 能夠使用長週期光柵24以替代漸變輕合區域6〇如圖? 所示以導引光學訊號進入適當心蕊(例如為心蕊12)於傳統 光纖70界面之前。傳統光纖7〇之心蕊66對準於色散管理光 纖10之心蕊融接絲學職沿耗鮮理光賴傳播。 V溝槽基板72保持光纖1 〇與70間所需要之對準。 、^傳統光卿能崎雜色散管理光、_之心、蕊12或14 ’或每㉟12及14能觸特分離之傳統规。在後者 f月况下,光纖切換器(並未顯示出)能夠使用來交替地連接 各別傳統光纖至單-傳統賴。切換器能夠藉由感測器加 以控制,錢測靖^飾在於各轉絲纖中。 圖w田繪出另外—個光纖1〇,,其具有兩條類似心蕊12, 以及1‘埋歲於共同包層以,内。與光纖1〇之心蕊比較(顯 不於圖ία中),心蕊〇央沿著另外—條光卿,之光學中 心軸。其他心蕊14,偏移中心軸18,。 ^中央心凝12較容易對準於標準光纖之心蕊。不過,區 段交替,纖1〇’端部對著端部之拼接以偏移中央心蕊12,與 偏離〜凝14間之訊號較為困難。因而,心蕊12,與14,間之 二號轉f優先地勤側向—發生。在任何端部對著端 部連接前,職優絲藉蝴如逐漸變化先_’或藉由使 甩逐漸變蝴合_偏移至中央减12,,如_所示。 __亚不集中只有一條心蕊12,於光學中心轴18,,圖1C顯 不出另外一條具有兩條心蕊12”與14"之光纖10”,以同心圓 圖案集令於光學中心㈣"。能夠使用侧邊麵合器以偏移V. Description of the invention (tJ and 64 are gradually coupled together to transfer power to the waveguide. A long-period grating 24 can be used instead of the gradual light closing region 60. As shown in the figure? To guide the optical signal into the appropriate heart (For example, the core core 12) Before the interface of the traditional optical fiber 70. The core core 66 of the conventional optical fiber 70 is aligned with the core fusion wire of the dispersion management optical fiber 10 and the optical fiber spreads along the fresh fiber. The V-groove substrate 72 is maintained The required alignment between the optical fiber 10 and 70. ^ Traditional Guang Qing Nozaki hybrid dispersion management light, _Heart, core 12 or 14 'or the traditional rule that each twelve and 14 can touch the separation. In the latter f month In this case, the optical fiber switcher (not shown) can be used to alternately connect the traditional optical fibers to the single-traditional Lai. The switcher can be controlled by the sensor. Figure W depicts another optical fiber 10, which has two similar cores 12, and 1 'buried under the common cladding. Compared with the core of fiber 10 (not shown in the figure) (Middle), the core of the heart is along the center of the optical axis of the other Guangqing, the other core is 14, The central axis 18, ^ The central core 12 is easier to align with the core of the standard fiber. However, the segments are alternated, and the end of the fiber 10 'is facing the end to splice to offset the central core 12 and deviate ~ It is more difficult to condense the signal of the 14th. Therefore, the heart cores 12 and 14 and the second of the 2nd turn f are preferentially laterally-occurring. Before any end is connected to the end, Yeyou Silk will gradually change first. _ 'Or by gradually shifting it to _ offset to the center minus 12, as shown in _. __Asian concentration has only one stamen 12, on the optical central axis 18, Figure 1C shows that the other has Two cores 12 "and 14" fiber 10 "are set in the center of the optical fiber in a concentric circle pattern. The side face coupler can be used to offset
ir 4 5 4 09 9 五、發明_ir 4 5 4 09 9 V. Invention_
.14. 經 濟 部 rb 局 令 A's^ 訊唬於同心心蕊121'與14"之間。具有同心心蕊12”與14"之 光纖10"顯現ϋ較小雙折射性以及較為容易仙傳統技術 製造。亦能夠使用其他同心心蕊或與偏離心蕊合併之同心 心蕊。.. 在光纖中色散管理之另外一項方法描繪於圖8中。所 顯不多模光纖80具有中.心心蕊82以及圍繞著之包層料設計 作為維持大於-個絲傳雖。—健例如為基模顯示出 正值色散;以及另外-健例如為第二階模呈現出負值色 散。長週期光栅86沿著光學中心軸88以重複圖案劃記在光 纖80上’該圖案調整每一模中光學訊號相對耐久 度與平均色散乘積和接近零。 " 參考圖8,第二階模負值色散具有較大值而大於基模之 負值色散。因而,量測基模中光柵86間運行距離長度之間 距LF大於第二階模中光柵86間運行距離長度之間距曰其 他組合為可能的,包含兩個操作模間相等大小之相反符號、 之色散。能夠使用相等間隔之光柵以均勻地分配兩個不^ 拉間之光學運行距離。同時能夠使用高於第二模之模以作 為该用途以減彳、偏極模色散。光柵㈣岭 高 偏移訊1«移至仏續高階模,但是對加人模之非預、 期損耗對會限制較高階模之使用。 圖8及9曲線圖列舉出具有階躍折射率心 ί之性能。在圖8中,標準化傳播係數‘對標i 化頻率V"繪製出,其能夠以數學定義如下: bnK/5/k-n2)/(n「n2) 一请先閲讀背面之注意事項#填寫本育〕 -装· 線 4 d 4 uy y M B7 5 1—_ 五、發明説明(叶) 部 τ.!? i 消.14. The Ministry of Economic Affairs rb ordered A's ^ to fool between the concentric cores 121 'and 14 ". Optical fiber 10 with concentric cores 12 "and 14 " shows a smaller birefringence and is easier to manufacture with traditional techniques. It is also possible to use other concentric cores or concentric cores that merge with off-center cores .. In fiber Another method for medium dispersion management is depicted in Figure 8. The shown multimode fiber 80 has a center core 82 and a cladding material surrounding it designed to maintain greater than one silk pass though. For example, a basic mode Showing positive value dispersion; and in addition, for example, showing negative value dispersion for the second-order mode. The long-period grating 86 is marked on the optical fiber 80 in a repeating pattern along the optical center axis 88 'This pattern adjusts the optical in each mode The sum of the signal's relative durability and the average dispersion product is close to zero. &Quot; Referring to Figure 8, the second-order mode negative value dispersion has a larger value and is larger than the negative value of the fundamental mode. Therefore, the running distance between the gratings 86 in the fundamental mode is measured The distance between the lengths LF is greater than the running distance between the gratings 86 in the second-order mode. The other distances are possible, including the opposite sign of the same size between the two operating modes, and the dispersion. Equally spaced light can be used. In order to evenly distribute the optical running distance between two non-drags. At the same time, a die higher than the second mode can be used for this purpose to reduce chirp and polar mode dispersion. Grating ridge height offset 1 «moved to 仏Continuing higher-order modes, but the unpredicted and expected loss pairs for adding modes will limit the use of higher-order modes. Figures 8 and 9 plot the performance with a step index. In Figure 8, the normalized propagation coefficient 'The benchmarking frequency V " is drawn, and it can be defined mathematically as follows: bnK / 5 / k-n2) / (n 「n2) Please read the notes on the back first # fill in this education]-equipment · line 4 d 4 uy y M B7 5 1—_ 5. Description of the invention (leaf) τ.!? i 消
i'J V二 2;τ—2-η22)0·55/λ 其中"点"為傳播係數,X'為心蕊折射率,'v為包層折射 率,"又"為一個範圍之中央波長,以及"k”為係數2ττ/λ,以 及"a"為波導心蕊半徑。棵準化傳播係數以"n(eff>"表示, 其在"〇"與111”間變化,"〇"表示整個在包層中傳播以及” Γ 表示整個在心蕊中傳播。在心蕊中發生較多傳播更嚴格地 受到限制大於在包層中發生較多傳播之情況。標準化頻率 值”V1'具有與中央波長"λ"之反比關係。 曲線LPq!,LPU,以及LP02分別地表示基模,第二,以及 第三模。依據圖9範例性曲線圖9,需要大於2.4之標準化頻 率以維持一個模,但是需要甚至於在3. 5附近之較大值以適 當地界定最常應用之訊號。, 如圖10所示,約為3. 5標準化頻率亦提供操作區域,其 具有與標準化波導色散"Dn 11之相反符號,其經驗公式如下: Dn=Vd2Vbn/(dV2) 雖然小於3. 5標準化頻率產生較高色散之可能,第二階 模訊號限制將減小。遠離第二階模截止波長之操作(即顯 然地高於4)將減小彎曲以及為彎曲損耗以及偏極分裂 。光纖80週期性或連續性扭轉亦能夠加以使用以減小偏極 模色散。 以ps/km為測量單位之波導色散"D"能夠以下列公式計Dn(-niA)/(cA) 其中△為相對折射率差值。波導色散"D"符號與標準化波 導色散”Dn"相反,因而基模” LPqi"波導色散為正值以及第 本紙张尺度適用中1司固各標华(CNS ) /\4現格(21〇_X 297公资)1*7… (請先閲讀背面之注意事項再填寫本頁). 裝. 訂 線 4 54 09 9 、發明説明(\f) A7 B7 6 1 合 二階模.LPn"波導色散為負值。 大於2. 4之標準化頻率下,階躍折射率光纖之基模Lp θΐ 之波導色散” D"相當低因而任何顯著光色散最主要歸諸於 材料色散。在1550nm頻窗中,,階躍折射率光纖之基模考色 散受限於17-20ps/km。不過,較複雜心蕊分佈設計包含區 段化心蕊以及環狀分佈能夠加以使用產生較高色散值。正 值與負值色散心蕊間之心蕊設計亦能夠加以選擇為適當相 關色散斜率使得平均色散保持為接近零於整個訊號波長之 範圍。例如,色散斜率大小為相等地,但是符號為相反的或 絕對值為較低。 多模及多心蕊設計能夠合併於各個光纖内以對色散產 生更進一步控制同時其他設計標準值亦為最佳化。例如 描缯'於圖1A中光纖10之心蕊12及14或描繪於圖ΐβ及π中其 他心蕊能夠形成為多模心蕊,以及色散規格亦能夠在模及' 心蕊間加以區分。 ' 月&夠使用傳統製造技術以製造出多模光纖8〇,以及類 似於先前對多心蕊光纖所說明之光折射性技術能夠加以使 用以劃記光柵。雖然長週期光柵86優先地作為模耦合其 他圖案以及變化形式包含直徑變化亦能夠使用來偏訊' 於不同模之間。 其餘圖11-14,顯示出各種預製件(亦稱為毛肱)以較容 易製造先前所說明多心蕊光纖,其使用不同桿件於管件中' 以及形成保持偏極光纖之OVD(光學汽相沉積法)技術。 在圖11所顯示光纖預製件90具有鑽孔桿件92以承典兩 (請先閲讀背面之注意事項再填寫本頁.}i'J V 2 2; τ—2-η22) 0 · 55 / λ where " point " is the propagation coefficient, X 'is the refractive index of the core,' v is the refractive index of the cladding, and " is The central wavelength of a range, and " k "is the coefficient 2ττ / λ, and " a " is the core radius of the waveguide. The normalized propagation coefficient is expressed as " n (eff > ", which is in " 〇 " And 111 ", " 〇 " means the entire spread in the cladding and" Γ means the entire spread in the heart core. More transmission in the heart core is more strictly restricted than in the cladding. The normalized frequency value "V1 'has an inverse relationship with the central wavelength " λ ". The curves LPq !, LPU, and LP02 represent the fundamental mode, the second, and the third mode, respectively. According to the exemplary curve diagram of FIG. 9, a normalized frequency greater than 2.4 is required to maintain a mode, but a large value even around 3.5 is required to properly define the most commonly used signals. As shown in Figure 10, about 3.5 standardized frequencies An operating area is also provided, which has the opposite sign to the normalized waveguide dispersion " Dn 11 Its empirical formula is as follows: Dn = Vd2Vbn / (dV2) Although less than 3.5 normalized frequency may produce higher dispersion, the second-order mode signal limit will be reduced. Operations far away from the second-order mode cutoff wavelength (that is obviously high) 4) will reduce bending and bending loss and polarization splitting. Periodic or continuous twisting of optical fiber 80 can also be used to reduce polarization mode dispersion. Waveguide dispersion measured in ps / km " D " Dn (-niA) / (cA) can be calculated by the following formula, where △ is the relative refractive index difference. The waveguide dispersion " D " sign is opposite to the normalized waveguide dispersion "Dn", so the fundamental mode "LPqi" waveguide dispersion is positive And the 1st paper standard is applicable in the first paper standard (CNS) / \ 4 present grid (21〇_X 297 public capital) 1 * 7 ... (Please read the precautions on the back before filling this page). Order line 4 54 09 9 、 Instruction of the invention (\ f) A7 B7 6 1 Combined second-order mode. LPn " Waveguide dispersion is negative. At a standardized frequency greater than 2.4, the waveguide of the fundamental mode Lp θΐ of the step-index fiber Dispersion "D " is quite low so any significant light dispersion is mainly attributed to Material dispersion. In the 1550nm frequency window, the fundamental mode dispersion of a step-index fiber is limited to 17-20ps / km. However, more complex stamen distribution designs that include segmented stamens and annular distribution can be used Produces higher dispersion values. The core design between positive and negative dispersion cores can also be selected to properly correlate the dispersion slope so that the average dispersion remains near zero over the entire signal wavelength range. For example, the dispersion slopes are equal in magnitude, but the signs are reversed or the absolute value is low. Multimode and multicore designs can be incorporated into each fiber to further control dispersion, while other design criteria are optimized. For example, the cores 12 and 14 of the optical fiber 10 depicted in Figure 1A or the other cores depicted in Figures ΐβ and π can be formed into multimode cores, and the dispersion specifications can be distinguished between the modes and the cores. 'Member & can use conventional manufacturing techniques to make multimode fiber 80, and light refraction techniques similar to those previously described for multicore fibers can be used to mark gratings. Although the long-period grating 86 preferentially acts as a mode coupling to other patterns and variations including diameter changes, it can also be used to bias signals between different modes. The remaining Figures 11-14 show various prefabricated parts (also known as bristles) to make it easier to manufacture the previously described multicore fiber, which uses different rods in the tube 'and to form an OVD (optical vapor Phase deposition) technology. The optical fiber preform 90 shown in FIG. 11 has a drilled rod member 92 to support the two (please read the precautions on the back before filling this page.)
、1T 線—— 454099 A7 「 ---—. _ B7 五、發明説明((ς ) 條玻璃心忠'桿件94及96。桿件92以包層材料製造出,以及 兩條玻埚心為桿件94及96包含心蕊及包層材料,其依次地 藉由光學汽相沉積法以產生不同色散特性折射率分佈地加 以塗覆。亦由包層材料製造出玻璃粉塵98塗覆於桿件外側 以及加以固結以完成預製件9〇。由預製件抽拉出多心蕊光 纖具有至少兩條彼此平行延伸之心蕊以及呈現出不同的 散特性。 圖11所顯示之光纖預製件100具有兩條玻璃桿件1〇2以 及104以及兩條裝置於管件11〇内之填充桿件1〇6及1〇8,以 及固結粉塵112圍繞著管件i1G。兩條心蕊捍件取及1〇4具 有心蕊及包層分佈,其维持不同的色散特性。填充桿件106 及108, f件11〇,以及粉塵H2均由包層材料製造出,其與心 蕊桿件102與104融合在一起以完成預製件。 ^ 圖12描繪出預製件120,其包含特別形狀包層材料之桿 件114,該桿件維持兩條具有不同色散特性之心蕊桿件ιΐ6 及118。兩條心蕊桿件丨16及118能夠黏附至桿件114以維持 兩條心蕊桿件於所需要之相對位置持續到預製件12〇被固 結。 如圖13所示預製件13〇 έ含兩條黏附在一起心蕊桿件 132以及134以及由固結粉塵136圍繞著。心蕊桿件][32以及 134具有不同的色散特性以及折射率分怖,其能夠促使或防 止由預製件13 0抽拉出最終心蕊間之自動耦合。 粉塵外包層98’112, 122,及136在固結過程中產生轴向 以及徑向力量收縮,其密封組件於預製件9〇, 1〇〇, 12〇,以及 本纸很尺度適财IS ,¾家桮準(CNS ) 210X2^^7 4 Λ7 Β7 8 It· 五、發明説明 (Η 130内。在下一抽拉處理過程 在心荐間產生熬合作用以及能^用折射性技術 償圍繞著心㈣物她術以補 1方、可觀额置以產生肖紐參考點。 乂 在四條顏件内之賴心蕊桿倾_96,勝1{}4, ιΐ6— ,以及132-134具杨等或不相等絕對翻號 =大小色散之職性或連續性輕二 ^成長度與平均色散積接近零。不過,需要不同大小色散 ,期性满合,其在不同色散心蕊中產生不同運 達成相關長额平桃㈣接赫。 . ' '〜..... ----1 n I— n ----- I - ·! --- (請先閲.讀背面之注意事項再填寫本頁} ---訂---1 線 卜乂尺^。)7國国家標準(CNS ) Λ4现格(210 X 297公疫) *2^0、 1T line—— 454099 A7 "-----. _ B7 V. Description of the invention (() glass heart loyalty 'rods 94 and 96. The rod 92 is made of cladding material, and two glass pot cores The rods 94 and 96 include a core and a cladding material, which are sequentially coated by optical vapor deposition to produce refractive index distributions with different dispersion characteristics. Glass dust 98 is also manufactured from the cladding material and coated on The outside of the rod is consolidated to complete the preform 90. The multi-core fiber drawn from the preform has at least two cores extending parallel to each other and exhibits different scattering characteristics. The optical fiber preform shown in Figure 11 100 has two glass rods 102 and 104, two filling rods 106 and 108 installed in the tube 110, and a consolidation dust 112 surrounding the tube i1G. The two heart cores take And 104 have core and cladding distributions, which maintain different dispersion characteristics. Filled rods 106 and 108, f 11 and dust H2 are all made of cladding material, which is related to the core rod 102 and 104 is fused together to complete the preform. ^ Figure 12 depicts the preform 120, which contains a special shape Rod-like cladding member 114, which maintains two core members 6 and 118 with different dispersion characteristics. The two core members 16 and 118 can be adhered to the rod 114 to maintain the two core members. The rods continue to be fixed at the required relative position until the preform 12o is consolidated. As shown in FIG. 13, the preform 13o contains two core rods 132 and 134 adhered together and is surrounded by consolidation dust 136. Cardiac rods] [32 and 134 have different dispersion characteristics and refractive index distributions, which can promote or prevent the automatic coupling between the final cores drawn from the preform 130. Dust coating 98'112, 122, And 136 shrink in the axial and radial forces during the consolidation process, and its sealing components are in the prefab 90, 100, 120, and the paper is very suitable for IS, ¾ Jia Cupquan (CNS) 210X2 ^ ^ 7 4 Λ7 Β7 8 It · V. Description of the invention (Η130). In the next drawing process, there is co-operation between the heart and the heart, and refraction technology can be used to compensate the heart around the heart, and to supplement one side, The considerable amount is set to generate the Xiao Niu reference point. 赖 In the four faces, Lai Xinrui leans _96, wins 1 {} 4, ιΐ6—, and 132-134 with Yang et al. or unequal absolute numbers = size or dispersion of continuity or continuity. The length and average dispersion product are close to zero. However, different sizes of dispersion are required, and the period is full. In different dispersive cores, different operations are performed to achieve the relevant long-term flat peach blossoms.. '' ~ ..... ---- 1 n I— n ----- I-·! --- ( Please read it first. Read the precautions on the back before filling out this page} --- Order --- 1 Line 乂 乂 乂. ) National Standards of 7 Countries (CNS) Λ4 is now available (210 X 297 public epidemic) * 2 ^ 0
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US10049598P | 1998-09-16 | 1998-09-16 |
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TW454099B true TW454099B (en) | 2001-09-11 |
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TW088116554A TW454099B (en) | 1998-09-16 | 1999-09-26 | Multicore and multimode dispersion managed fibers |
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EP (1) | EP1114337A2 (en) |
JP (1) | JP2002525645A (en) |
KR (1) | KR20010088804A (en) |
CN (1) | CN1359474A (en) |
AU (1) | AU1439900A (en) |
BR (1) | BR9913334A (en) |
CA (1) | CA2344200A1 (en) |
ID (1) | ID30554A (en) |
TW (1) | TW454099B (en) |
WO (1) | WO2000016131A2 (en) |
ZA (1) | ZA995927B (en) |
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US6611648B2 (en) | 2001-05-09 | 2003-08-26 | Corning Incorporated | Optical fibers having cores with different propagation constants, and methods of manufacturing same |
AU2002356179A1 (en) | 2001-08-22 | 2003-03-10 | Corning Incorporated | Controlled dispersion optical fiber |
FR2864254B1 (en) | 2003-12-23 | 2006-03-03 | Cit Alcatel | HOM MULTIMODE OPTICAL FIBER WITH DISPERSION MANAGEMENT |
KR101050885B1 (en) * | 2003-12-26 | 2011-07-20 | 주식회사 케이티 | Dispersion compensation device in optical transmission system |
CN100495093C (en) * | 2007-09-14 | 2009-06-03 | 中国科学院上海光学精密机械研究所 | Strongly coupled multi-core optical fiber |
US8123400B2 (en) * | 2008-04-16 | 2012-02-28 | Ofs Fitel, Llc | Multi-core fiber grating sensor |
JP5168702B2 (en) * | 2008-10-03 | 2013-03-27 | 国立大学法人横浜国立大学 | Multi-core fiber core placement method |
JP5367726B2 (en) * | 2008-12-24 | 2013-12-11 | 古河電気工業株式会社 | Multi-core optical fiber |
JP5267481B2 (en) * | 2010-02-18 | 2013-08-21 | 住友電気工業株式会社 | Multi-core optical fiber |
CN103403591A (en) * | 2011-03-04 | 2013-11-20 | 株式会社藤仓 | Multi-core fiber, and multi-core fiber connection method using the same |
JP2012203036A (en) * | 2011-03-23 | 2012-10-22 | Mitsubishi Cable Ind Ltd | Optical transmission line |
JP5351938B2 (en) * | 2011-08-17 | 2013-11-27 | 株式会社フジクラ | Coupled multi-core fiber |
JP5867076B2 (en) * | 2011-12-28 | 2016-02-24 | 住友電気工業株式会社 | Multi-core optical fiber |
JP6039700B2 (en) * | 2012-03-07 | 2016-12-07 | オーエフエス ファイテル,エルエルシー | Grating based sensor |
JP2014052410A (en) * | 2012-09-05 | 2014-03-20 | Mitsubishi Cable Ind Ltd | Multi-core optical fiber |
JP6192442B2 (en) * | 2013-05-16 | 2017-09-06 | 株式会社フジクラ | Coupled multi-core fiber |
CN106575014B (en) * | 2014-08-22 | 2019-12-17 | 住友电气工业株式会社 | Optical fiber |
WO2016035883A1 (en) | 2014-09-05 | 2016-03-10 | 古河電気工業株式会社 | Multicore fiber and manufacturing method therefor |
CN105091920A (en) * | 2015-09-02 | 2015-11-25 | 中国电子科技集团公司第八研究所 | Clustered fiber Bragg grating sensor |
US10001597B2 (en) | 2015-09-22 | 2018-06-19 | Corning Incorporated | Multicore optical fibers and interconnection methods for the same |
JP2017072818A (en) * | 2015-10-08 | 2017-04-13 | 住友電気工業株式会社 | Multicore optical fiber, multicore optical fiber cable, and optical fiber transmission system |
JP6879300B2 (en) * | 2016-05-12 | 2021-06-02 | 住友電気工業株式会社 | Manufacturing methods for multi-core optical fibers, fiber bragg gratings and fiber bragg gratings |
KR101941020B1 (en) * | 2016-06-14 | 2019-01-22 | 광주과학기술원 | Voltage Sensor based on Optical Fiber |
CN109613646B (en) * | 2019-01-18 | 2020-07-03 | 厦门大学 | Different-core double-core optical fiber with characteristic wavelength in transmission spectrum |
US20230244025A1 (en) * | 2020-06-29 | 2023-08-03 | Nippon Telegraph And Telephone Corporation | Multi-core fiber, optical transmission system, and optical transmission method |
JP7520145B2 (en) * | 2020-12-04 | 2024-07-22 | 株式会社フジクラ | Fiber connection, optical communication system, optical device, and method for manufacturing fiber connection |
FR3123912B1 (en) * | 2021-06-15 | 2023-06-16 | Draka Comteq France | Method of manufacturing a preform for a multi-core optical fiber and method of manufacturing multi-core optical fibers. |
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US4478488A (en) * | 1980-11-03 | 1984-10-23 | At&T Bell Laboratories | Information transmission using dispersive optical fibers |
US5087108A (en) * | 1989-08-11 | 1992-02-11 | Societa' Cavi Pirelli S.P.A. | Double-core active-fiber optical amplifier having a wide-band signal wavelength |
FR2728693B1 (en) * | 1994-12-21 | 1997-01-31 | Alcatel Cable | METHOD FOR MANUFACTURING A MULTIFIBER OPTICAL DISTRIBUTOR AND OPTICAL DISTRIBUTOR OBTAINED ACCORDING TO THIS METHOD |
US5894537A (en) * | 1996-01-11 | 1999-04-13 | Corning Incorporated | Dispersion managed optical waveguide |
-
1999
- 1999-08-10 WO PCT/US1999/018090 patent/WO2000016131A2/en not_active Application Discontinuation
- 1999-08-10 BR BR9913334-2A patent/BR9913334A/en not_active Application Discontinuation
- 1999-08-10 ID IDW20010838A patent/ID30554A/en unknown
- 1999-08-10 KR KR1020017003356A patent/KR20010088804A/en not_active Application Discontinuation
- 1999-08-10 EP EP99969152A patent/EP1114337A2/en not_active Withdrawn
- 1999-08-10 CN CN99810832A patent/CN1359474A/en active Pending
- 1999-08-10 AU AU14399/00A patent/AU1439900A/en not_active Abandoned
- 1999-08-10 CA CA002344200A patent/CA2344200A1/en not_active Abandoned
- 1999-08-10 JP JP2000570612A patent/JP2002525645A/en active Pending
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WO2000016131A2 (en) | 2000-03-23 |
CA2344200A1 (en) | 2000-03-23 |
AU1439900A (en) | 2000-04-03 |
WO2000016131A9 (en) | 2000-11-16 |
ID30554A (en) | 2001-12-20 |
EP1114337A2 (en) | 2001-07-11 |
KR20010088804A (en) | 2001-09-28 |
WO2000016131A3 (en) | 2000-05-25 |
BR9913334A (en) | 2002-06-18 |
ZA995927B (en) | 2000-04-04 |
CN1359474A (en) | 2002-07-17 |
JP2002525645A (en) | 2002-08-13 |
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