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TWI696806B - Fiber interferometer and method for manufacturing the same - Google Patents

Fiber interferometer and method for manufacturing the same Download PDF

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TWI696806B
TWI696806B TW108117716A TW108117716A TWI696806B TW I696806 B TWI696806 B TW I696806B TW 108117716 A TW108117716 A TW 108117716A TW 108117716 A TW108117716 A TW 108117716A TW I696806 B TWI696806 B TW I696806B
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fiber
core
optical fiber
interferometer
light guide
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TW108117716A
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Chinese (zh)
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TW202043695A (en
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于欽平
王賀年
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國立中山大學
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Abstract

A fiber interferometer includes a sensing unit having a case, a resonating chamber and a first fiber core, and two light guide units respectively connected to two ends of the sensing unit. The case delimits a resonating chamber. The first fiber core is located at a central axis of the resonating chamber. Each light guide unit includes an outer case and a second fiber core. The second fiber core is located at a central axis of the outer case of the light guide unit. The first and second fiber cores are connected in series along the same axis. One of the two light guide units includes an opening portion located on the interconnected part of the sensing unit and the light guide unit. The resonating chamber intercommunicates with the outside through the opening portion. A method for manufacturing the fiber interferometer is also provided.

Description

光纖干涉儀及其製造方法 Optical fiber interferometer and its manufacturing method

本發明係關於一種測量儀器,尤其是一種用於測量微小位移、折射率、環境溫度及壓力變化等精密研究的光纖干涉儀及其製造方法。 The invention relates to a measuring instrument, in particular to an optical fiber interferometer and its manufacturing method used for precise research on measuring small displacement, refractive index, environmental temperature and pressure change.

光纖干涉儀係可以用於測量溫度、張力、壓力、濃度、折射率等環境參數,並結合光纖通訊技術,係能夠實現遠端即時監控及提高檢測密度,符合資訊大量且快速流通的現代產業需求,另外,光纖干涉儀係藉由解讀光訊號在環境中的變化已取得量測資料,因此具有抵抗電磁干擾、反應快速、耐高溫高壓等優點,係可以廣泛應用於各種系統及領域。 The optical fiber interferometer system can be used to measure environmental parameters such as temperature, tension, pressure, concentration, refractive index, etc., and combined with optical fiber communication technology, it can realize remote real-time monitoring and increase detection density, which meets the needs of modern industries with large amounts of information and rapid circulation In addition, the optical fiber interferometer has obtained measurement data by interpreting the changes of the optical signal in the environment, so it has the advantages of resisting electromagnetic interference, fast response, high temperature and high pressure resistance, and can be widely used in various systems and fields.

習知的光纖干涉儀的原理係利用兩道光通過不同的光學路徑(Optical Path),其中一道光受環境影響作為感測訊號,另一道光則未受影響作為參考訊號,使兩道光之間產生相位差(Phase Difference)並在輸出端產生干涉頻譜(Interference Spectrum),藉由分析頻譜位移可推算環境參數之變化。 The principle of the conventional optical fiber interferometer is to use two lights to pass through different optical paths. One of the lights is affected by the environment as a sensing signal, and the other light is not affected as a reference signal. The difference (Phase Difference) and the interference spectrum (Interference Spectrum) at the output end, by analyzing the spectrum shift can be estimated changes in environmental parameters.

習知的光纖干涉儀係利用酸腐蝕、高溫拉伸、飛秒雷射蝕刻等方式,縮減感測區段的光纖直徑,使進入光纖的光線可以在感測區段分光再耦合形成干涉,又,為了使光纖干涉儀的尺寸小至微米等級,以便更靈活運用於感測裝置,係導致製造光纖干涉儀的技術難度升高,例如:高溫拉伸及 酸蝕處理所提升的感測靈敏度有限,並且降低元件的機械強度而影響實際感測應用;飛秒雷射加工的成本高、損耗大,且加工表面粗糙而容易殘留環境介質,導致感測精確度降低。 The conventional optical fiber interferometer system uses acid corrosion, high temperature stretching, femtosecond laser etching, etc. to reduce the diameter of the optical fiber in the sensing section, so that the light entering the optical fiber can be split in the sensing section and then coupled to form interference, and In order to make the size of the optical fiber interferometer as small as the micron level, so as to be more flexibly used in the sensing device, it causes the technical difficulty of manufacturing the optical fiber interferometer to increase, such as: high temperature stretching The increased sensitivity of the etching process is limited, and the mechanical strength of the component is reduced to affect the actual sensing application; femtosecond laser processing has high cost and large loss, and the processing surface is rough and easy to leave environmental media, resulting in accurate sensing Degree is reduced.

有鑑於此,習知的光纖干涉儀及其製造方法確實仍有加以改善之必要。 In view of this, the conventional optical fiber interferometer and its manufacturing method still need to be improved.

為解決上述問題,本發明的目的是提供一種光纖干涉儀,具有結構簡單的開放式共振腔,係可以增加感測應用範圍。 In order to solve the above problems, the object of the present invention is to provide an optical fiber interferometer with an open resonant cavity with a simple structure, which can increase the sensing application range.

本發明的次一目的是提供一種光纖干涉儀,材料成本低且結構簡單,係可以降低生產成本。 The next object of the present invention is to provide an optical fiber interferometer with low material cost and simple structure, which can reduce production costs.

本發明的又一目的是提供一種光纖干涉儀製造方法,具有可調整的製程參數,係可以提高感測準確度及提升產品良率。 Another object of the present invention is to provide a method for manufacturing an optical fiber interferometer with adjustable process parameters, which can improve sensing accuracy and product yield.

本發明的再一目的是提供一種光纖干涉儀製造方法,係可以提升元件的機械強度及減少元件損耗。 Still another object of the present invention is to provide a method for manufacturing an optical fiber interferometer, which can improve the mechanical strength of components and reduce component losses.

本發明全文所記載的元件及構件使用「一」或「一個」之量詞,僅是為了方便使用且提供本發明範圍的通常意義;於本發明中應被解讀為包括一個或至少一個,且單一的概念也包括複數的情況,除非其明顯意指其他意思。 The use of the quantifier "a" or "one" in the elements and components described throughout the present invention is for convenience and provides the usual meaning of the scope of the present invention; in the present invention, it should be interpreted as including one or at least one, and single The concept of also includes the plural case unless it clearly means something else.

本發明的光纖干涉儀,包含:一感測單元,具有一外殼層、由該外殼層包圍環繞之一共振腔,及位於該共振腔之中心軸線上的一第一纖芯;及二導光單元,各該導光單元具有一纖殼,及位於該纖殼之中心軸線上的一第二纖芯,該二導光單元係以軸向分別結合於該感測單元之二端,該第一纖芯與該二第二纖芯串接於同一軸線上,其中一該導光單元具有一開口部,該 開口部位於該導光單元與該感測單元之接合處,該共振腔透過該開口部連通外部環境。 The optical fiber interferometer of the present invention includes: a sensing unit having an outer shell layer, a resonant cavity surrounded by the outer shell layer, and a first fiber core located on the central axis of the resonant cavity; and two light guides Unit, each of the light guide units has a fiber shell, and a second fiber core located on the central axis of the fiber shell, the two light guide units are axially coupled to the two ends of the sensing unit, respectively A fiber core and the two second fiber cores are connected in series on the same axis, one of the light guide units has an opening, the The opening is located at the junction of the light guide unit and the sensing unit, and the resonant cavity communicates with the external environment through the opening.

本發明的光纖干涉儀製造方法,包含:將一晶體光纖之一第一連接面接合一單模光纖之一對接面,並裁切該晶體光纖形成一第二連接面;將該晶體光纖由該第二連接面一端浸入一蝕刻溶液,並靜置一蝕刻時間後,清洗及風乾該晶體光纖,使該晶體光纖形成軸向之一共振腔及一蝕刻纖芯;將一斜角光纖之一端面與一拋光片之間維持一傾斜角度進行研磨,研磨後之該端面形成一熔接面及一研磨面;及將該晶體光纖之該第二連接面接合該斜角光纖之該熔接面,該第二連接面與該研磨面之間係該共振腔之開口。 The method for manufacturing an optical fiber interferometer of the present invention includes: joining a first connection surface of a crystal fiber to a butt surface of a single-mode fiber, and cutting the crystal fiber to form a second connection surface; One end of the second connection surface is immersed in an etching solution, and after standing for an etching time, the crystal fiber is cleaned and air-dried to form a resonant cavity and an etched core in the axial direction of the crystal fiber; Grinding at a tilt angle with a polishing sheet, the end surface after grinding forms a fusion surface and a grinding surface; and the second connection surface of the crystal fiber is joined to the fusion surface of the oblique angle fiber, the first Between the two connecting surfaces and the polishing surface is the opening of the resonance cavity.

據此,本發明的光纖干涉儀及其製造方法,藉由蝕刻、研磨、熔接等製程方法,使不同粗細之纖芯結合共振腔,所生產的光纖干涉儀,係具有高折射率靈敏度、簡化製程難度及降低加工成本等功效;另外,藉由控制研磨角度、蝕刻時間等製程參數,係可以控制光纖干涉儀的尺寸結構,能夠配合感測需求調整共振腔及纖芯的規格,具有提升感測準確度及增加感測應用範圍等功效。 Accordingly, the optical fiber interferometer and its manufacturing method of the present invention, by etching, grinding, welding and other process methods, combine cores of different thicknesses with the resonant cavity, the produced optical fiber interferometer has high refractive index sensitivity and simplification The process is difficult and the processing cost is reduced. In addition, by controlling the process parameters such as grinding angle and etching time, the size and structure of the fiber interferometer can be controlled, and the specifications of the resonant cavity and core can be adjusted to meet the sensing needs, with a sense of improvement Effectiveness of measuring accuracy and increasing sensing application range.

其中,該感測單元係蝕刻加工後的光子晶體光纖,該光子晶體光纖具有一纖芯區域及一纖衣區域,該第一纖芯及該共振腔分別為被侵蝕之該纖芯區域及該纖衣區域。如此,係可以藉由蝕刻調整共振腔及纖芯之結構,具有簡化製程難度及降低加工成本的功效。 The sensing unit is an etched photonic crystal fiber. The photonic crystal fiber has a core region and a fiber jacket region. The first core and the resonant cavity are the eroded core region and the resonant cavity, respectively. Slim coat area. In this way, the structure of the resonant cavity and the fiber core can be adjusted by etching, which has the effects of simplifying the difficulty of the manufacturing process and reducing the processing cost.

其中,各該導光單元之該纖殼的直徑等於該感測單元之該外殼層的直徑。如此,該纖殼及該外殼層係可以平整對接,具有保護內部光通道及提升元件機械強度的功效。 Wherein, the diameter of the fiber shell of each light guide unit is equal to the diameter of the outer shell layer of the sensing unit. In this way, the fiber shell and the outer shell layer can be smoothly butted, and have the effects of protecting the internal optical channel and enhancing the mechanical strength of the component.

其中,各該導光單元之該第二纖芯的直徑大於該感測單元之該第一纖芯的直徑。如此,光線通過係可以產生分光,具有感測環境介質的功 效。 Wherein, the diameter of the second core of each light guide unit is larger than the diameter of the first core of the sensing unit. In this way, light passing through the system can produce split light, which has the function of sensing environmental media effect.

其中,該第一連接面及該第二連接面與該晶體光纖之橫切面的夾角小於1度,該對接面與該單模光纖之橫切面的夾角小於1度,該熔接面與該斜角光纖之橫切面的夾角小於1度。如此,該晶體光纖與該單模光纖及該斜角光纖可以平整連接,具有避免熔接時發生結構損壞的功效。 Wherein, the angle between the first connection surface and the second connection surface and the cross-section of the crystal fiber is less than 1 degree, the angle between the butt connection surface and the cross-section of the single-mode fiber is less than 1 degree, the fusion splice and the bevel angle The angle of the cross section of the optical fiber is less than 1 degree. In this way, the crystal fiber, the single-mode fiber and the oblique angle fiber can be connected smoothly, which has the effect of avoiding structural damage during welding.

其中,該晶體光纖浸入該蝕刻溶液之深度係該共振腔長度。如此,係可以製造出不同長度之共振腔,具有配合感測需求調整規格的功效。 Wherein, the depth of the crystal fiber immersed in the etching solution is the length of the resonant cavity. In this way, resonant cavities of different lengths can be manufactured, which has the effect of adjusting the specifications to meet the sensing needs.

其中,該蝕刻纖芯之直徑係與該蝕刻時間呈負相關。如此,係可以藉由蝕刻調整分光的強度比,具有調整干涉條紋之深淺對比的功效。 Wherein, the diameter of the etched core is inversely related to the etching time. In this way, it is possible to adjust the intensity ratio of the spectroscope by etching, which has the effect of adjusting the contrast of the depth of interference fringes.

其中,該斜角光纖之該端面係由一割線分隔為該熔接面及該研磨面,該熔接面與該研磨面之夾角係該傾斜角度之補角,該傾斜角度為45度。如此,係可以形成共振腔之開口且盡可能減少結構破壞,具有維持元件機械強度及提升製程良率的功效。 Wherein, the end surface of the oblique optical fiber is divided into the welding surface and the polishing surface by a secant line, and the angle between the welding surface and the polishing surface is the supplementary angle of the inclination angle, and the inclination angle is 45 degrees. In this way, the opening of the resonant cavity can be formed and structural damage can be reduced as much as possible, which has the effect of maintaining the mechanical strength of the device and improving the yield of the process.

其中,該割線與該熔接面之周緣的最大垂直距離係一端面高度,該端面高度是66.6微米至86微米。如此,係可以提供介質通過之空間且盡可能減少結構破壞,具有維持元件機械強度及提升製程良率的功效。 Wherein, the maximum vertical distance between the cutting line and the periphery of the welding surface is the height of one end surface, and the height of the end surface is 66.6 microns to 86 microns. In this way, it can provide space for the medium to pass through and minimize structural damage, which has the effect of maintaining the mechanical strength of the device and improving the yield of the process.

其中,接合該晶體光纖與該斜角光纖時,在該單模光纖連接該晶體光纖之另一端,及該斜角光纖位於該端面之另一端,分別連接一光源及一光功率計,當該晶體光纖之該蝕刻纖芯與該斜角光纖之纖芯完全對齊時,該光功率計能夠偵側到最大讀值。如此,係可以輔助纖芯熔接,具有提升干涉頻譜的清晰度及減少元件損耗的功效。 Where, when splicing the crystal fiber and the beveled fiber, the single-mode fiber is connected to the other end of the crystal fiber, and the beveled fiber is located at the other end of the end face, respectively connected to a light source and an optical power meter, when the When the etched core of the crystal fiber is completely aligned with the core of the beveled fiber, the optical power meter can detect the maximum reading. In this way, it can assist the fusion of the core, which has the effect of improving the clarity of the interference spectrum and reducing component losses.

1‧‧‧感測單元 1‧‧‧sensing unit

11‧‧‧外殼層 11‧‧‧Shell

12‧‧‧共振腔 12‧‧‧Resonant cavity

13‧‧‧第一纖芯 13‧‧‧First core

2‧‧‧導光單元 2‧‧‧Light guide unit

21‧‧‧纖殼 21‧‧‧ Fiber Shell

22‧‧‧第二纖芯 22‧‧‧second core

23‧‧‧開口部 23‧‧‧ opening

3‧‧‧晶體光纖 3‧‧‧Crystal fiber

4‧‧‧單模光纖 4‧‧‧Single-mode fiber

5‧‧‧斜角光纖 5‧‧‧Bevel fiber

C‧‧‧纖芯區域 C‧‧‧Core area

D‧‧‧纖衣區域 D‧‧‧fiber clothing area

L1‧‧‧輸入光 L1‧‧‧ input light

M‧‧‧測量光 M‧‧‧ measuring light

R‧‧‧參考光 R‧‧‧Reference light

L2‧‧‧輸出光 L2‧‧‧ output light

S1‧‧‧第一連接面 S1‧‧‧First connection surface

A‧‧‧對接面 A‧‧‧ Docking

S2‧‧‧第二連接面 S2‧‧‧Second connection surface

Q‧‧‧蝕刻溶液 Q‧‧‧Etching solution

E‧‧‧端面 E‧‧‧End

P‧‧‧拋光片 P‧‧‧Polishing tablets

θ‧‧‧傾斜角度 θ‧‧‧Tilt angle

F‧‧‧熔接面 F‧‧‧welding surface

G‧‧‧研磨面 G‧‧‧Grinded surface

T‧‧‧割線 T‧‧‧cutting line

H‧‧‧端面高度 H‧‧‧Height

X‧‧‧光源 X‧‧‧Light source

W‧‧‧光功率計 W‧‧‧ Optical Power Meter

〔第1圖〕本發明一較佳實施例的分解立體圖。 [Figure 1] An exploded perspective view of a preferred embodiment of the present invention.

〔第2圖〕本發明的感測單元之加工前後對照的正視圖。 [Figure 2] Front view of the sensor unit of the present invention before and after processing.

〔第3圖〕本發明一較佳實施例進行感測的光線通過情形圖。 [Figure 3] A diagram of the light passing state of a preferred embodiment of the invention.

〔第4a圖〕本發明一較佳實施例的裁切製程的動作情形圖。 [Figure 4a] A diagram of the operation of the cutting process according to a preferred embodiment of the present invention.

〔第4b圖〕本發明一較佳實施例的蝕刻製程的動作情形圖。 [Figure 4b] A diagram of the operation of the etching process according to a preferred embodiment of the present invention.

〔第4c圖〕本發明一較佳實施例的研磨製程的動作情形圖。 [Figure 4c] A diagram of the operation of the polishing process according to a preferred embodiment of the present invention.

〔第4d圖〕本發明一較佳實施例的熔接製程的動作情形圖。 [Figure 4d] A diagram of the operation of the welding process according to a preferred embodiment of the present invention.

為讓本發明之上述及其他目的、特徵及優點能更明顯易懂,下文特舉本發明之較佳實施例,並配合所附圖式,作詳細說明如下:請參照第1圖所示,其係本發明光纖干涉儀的較佳實施例,係包含一感測單元1及二導光單元2,該二導光單元2係以軸向分別結合於該感測單元1之二端,形成同軸之結構。 In order to make the above and other objects, features and advantages of the present invention more obvious and understandable, the preferred embodiments of the present invention are described below in conjunction with the attached drawings, which are described in detail as follows: Please refer to FIG. 1, It is a preferred embodiment of the optical fiber interferometer of the present invention, which includes a sensing unit 1 and two light guide units 2, the two light guide units 2 are axially coupled to the two ends of the sensing unit 1 to form Coaxial structure.

請參照第1及2圖所示,該感測單元1具有一外殼層11、由該外殼層11包圍環繞之一共振腔12,及一第一纖芯13,該第一纖芯13係位於該共振腔12之中心軸線上。該感測單元1可以是光子晶體光纖(Photonic Crystal Fiber,PCF)經由裁切、蝕刻等製程所產生,如第2圖所示,光子晶體光纖係由二氧化矽(Silica,SiO2)組成,包含中央實心的纖芯(Core)區域C,及圍繞纖芯的纖衣(Cladding)區域D,該纖衣區域D係由複數個不相連且平行該纖芯區域C的空氣孔洞排列而成,在蝕刻製程中,由蝕刻液進入該複數個空氣孔洞,係可以侵蝕該纖衣區域D形成該共振腔12,及縮減該纖芯區域C的直徑,係形成可藉由蝕刻時間長短控制直徑大小的該第一纖芯13。 Please refer to FIGS. 1 and 2, the sensing unit 1 has an outer shell layer 11, a resonant cavity 12 surrounded by the outer shell layer 11, and a first core 13, the first core 13 is located in The central axis of the resonant cavity 12. The sensing unit 1 may be a photonic crystal fiber (Photonic Crystal Fiber, PCF) produced through cutting, etching and other processes. As shown in FIG. 2, the photonic crystal fiber is composed of silicon dioxide (Silica, SiO 2 ). Contains a central solid core region C and a cladding region D surrounding the core. The clad region D is formed by a plurality of unconnected air holes parallel to the core region C. In the etching process, the etching solution enters the plurality of air holes, which can erode the fiber-coating area D to form the resonant cavity 12, and reduce the diameter of the core area C. The diameter can be controlled by the length of the etching time.的第一纤芯13.

請參照第1圖所示,該二導光單元2分別具有一纖殼21,及 位於該纖殼21內的一第二纖芯22,該第二纖芯22係軸向通過該纖殼21之中心,該纖殼21之直徑較佳等於該感測單元1之該外殼層11的直徑,該第二纖芯22之直徑較佳大於該感測單元1之該第一纖芯13的直徑。該二導光單元2係可以是由同一條單模光纖(Single Mode Fiber,SMF)裁切為二。 Please refer to FIG. 1, the two light guide units 2 have a fiber shell 21, and A second core 22 located in the core 21, the second core 22 passing axially through the center of the core 21, the diameter of the core 21 is preferably equal to the outer shell layer 11 of the sensing unit 1 The diameter of the second core 22 is preferably larger than the diameter of the first core 13 of the sensing unit 1. The two light guide unit 2 series may be cut into two by the same single mode fiber (SMF).

該二導光單元2係可以藉由熔接製程分別結合於該感測單元1之二端,使該第一纖芯13與該二第二纖芯22串接形成同軸結構之光路,且該外殼層11與該纖殼21較佳以軸向平整對接,係可以保護內部之纖芯結構。又,在其中一該導光單元2與該感測單元1之接合處,移除部分之該纖殼21以形成一開口部23,該共振腔12係藉由該開口部23連通外部環境,使環境中的流體通過該開口部23進入該共振腔12,係可以用以測量各種環境參數。 The two light guide units 2 can be respectively connected to the two ends of the sensing unit 1 through a welding process, so that the first core 13 and the two second cores 22 are connected in series to form a coaxial structure optical path, and the housing The layer 11 and the fiber shell 21 are preferably flatly and axially butted to protect the inner core structure. Moreover, at one of the junctions of the light guide unit 2 and the sensing unit 1, part of the fiber shell 21 is removed to form an opening 23, and the resonance cavity 12 communicates with the external environment through the opening 23. Allowing fluid in the environment to enter the resonance cavity 12 through the opening 23 can be used to measure various environmental parameters.

請參照第3圖所示,據由前述結構,一輸入光L1由任一該導光單元2往該感測單元1的方向進入該第二纖芯22,當該輸入光L1抵達該第一纖芯13與該第二纖芯22之交界處時,由於光路直徑縮減而導致分光,係產生一測量光M行經該共振腔12內的流體介質,及一參考光R沿同軸之該第一纖芯13前進,當該測量光M及該參考光R抵達該感測單元1與另一該導光單元2之接合處時,該測量光M及該參考光R耦合為一輸出光L2,由於行經不同的光路使該測量光M與該參考光R之間產生相位差,導致該輸出光L2經由另一該導光單元2之該第二纖芯22輸出後,可以形成干涉頻譜。 Referring to FIG. 3, according to the foregoing structure, an input light L1 enters the second core 22 from any of the light guide units 2 toward the sensing unit 1 when the input light L1 reaches the first At the junction of the fiber core 13 and the second fiber core 22, the optical path is reduced due to the reduced diameter of the optical path, which generates a measurement light M traveling through the fluid medium in the resonant cavity 12, and a reference light R along the first axis coaxial The core 13 advances, and when the measurement light M and the reference light R reach the junction of the sensing unit 1 and the other light guide unit 2, the measurement light M and the reference light R are coupled into an output light L2, Since the phase difference between the measurement light M and the reference light R is caused by traveling through different optical paths, the output light L2 can be output through the second core 22 of the other light guide unit 2 to form an interference spectrum.

請參照第4a~4d圖所示,其係本發明光纖干涉儀製造方法之較佳實施例的製程步驟,係包含將一晶體光纖3之一第一連接面S1接合一單模光纖4之一對接面A,並裁切該晶體光纖3形成一第二連接面S2;將該晶體光纖3由該第二連接面S2一端浸入一蝕刻溶液Q,並靜置一蝕刻時間後,清洗及風乾該晶體光纖3,使該晶體光纖3形成軸向之一共振腔及一蝕刻纖芯;將一斜角光纖5之一端面E與一拋光片P之間維持一傾斜角度θ進行研磨, 研磨後該端面E形成為一熔接面F及一研磨面G;將該晶體光纖3之該第二連接面S2接合該斜角光纖5之該熔接面F,該第二連接面S2與該研磨面G之間係該共振腔之開口。 Please refer to FIGS. 4a to 4d, which are the process steps of the preferred embodiment of the method for manufacturing an optical fiber interferometer of the present invention, which includes joining a first connection surface S1 of a crystal fiber 3 to one of a single-mode fiber 4 Butt surface A, and cut the crystal fiber 3 to form a second connection surface S2; immerse the crystal fiber 3 from an end of the second connection surface S2 into an etching solution Q, and after standing for an etching time, clean and air-dry the The crystal fiber 3 makes the crystal fiber 3 form a resonant cavity and an etched core in the axial direction; maintain an inclined angle θ between an end face E of a beveled fiber 5 and a polishing sheet P to grind, After polishing, the end surface E is formed into a fusion surface F and a polishing surface G; the second connection surface S2 of the crystal fiber 3 is joined to the fusion surface F of the oblique optical fiber 5, the second connection surface S2 and the polishing Between the faces G is the opening of the resonant cavity.

請參照第4a圖所示,該晶體光纖3之該第一連接面S1、該第二連接面S2及該單模光纖4之該對接面A,較佳為表面平整且無碎片殘留;又,該第一連接面S1及該第二連接面S2與該晶體光纖3之橫切面的夾角較佳小於1度,該對接面A與該單模光纖4之橫切面的夾角較佳小於1度,係可以避免該晶體光纖3與該單模光纖4熔接時發生結構損壞,而影響光路的暢通性。 Referring to FIG. 4a, the first connection surface S1, the second connection surface S2 of the crystal fiber 3 and the butt surface A of the single-mode fiber 4 preferably have a flat surface and no debris remains; The angle between the first connection surface S1 and the second connection surface S2 and the cross-sectional surface of the crystal fiber 3 is preferably less than 1 degree, and the angle between the butt surface A and the single-mode optical fiber 4 is preferably less than 1 degree. It is possible to avoid structural damage when the crystal fiber 3 and the single-mode fiber 4 are fused, which affects the smoothness of the optical path.

請參照第4b圖所示,該晶體光纖3較佳以傾斜方式浸入該蝕刻溶液Q,係可以使該蝕刻溶液Q容易進入該晶體光纖3之空氣孔洞,以提升蝕刻的效率。另外,該晶體光纖3浸入液面下之深度係該共振腔之長度;又,該蝕刻纖芯之直徑係與該蝕刻時間呈負相關,即該蝕刻時間愈長將導致該蝕刻纖芯之直徑愈短,因此,藉由控制該蝕刻長度及該蝕刻時間等製程參數,係可以調整該光纖干涉儀之結構而改變干涉頻譜之特性(例如:共振腔長度與干涉頻譜之條紋密集度呈正相關;該晶體光纖3之纖芯直徑係影響干涉條紋之深淺對比),能夠提升分析干涉頻譜的準確性。 Referring to FIG. 4b, the crystal fiber 3 is preferably immersed in the etching solution Q in an inclined manner, so that the etching solution Q can easily enter the air hole of the crystal fiber 3 to improve the etching efficiency. In addition, the depth of the crystal fiber 3 immersed under the liquid surface is the length of the resonant cavity; in addition, the diameter of the etched core is inversely related to the etching time, that is, the longer the etching time will result in the diameter of the etched core The shorter, therefore, by controlling the etching length and the etching time and other process parameters, the structure of the fiber interferometer can be adjusted to change the characteristics of the interference spectrum (for example: the length of the resonant cavity is positively correlated with the fringe density of the interference spectrum; The core diameter of the crystal fiber 3 affects the contrast of the interference fringes), which can improve the accuracy of analyzing the interference spectrum.

請參照第4c圖所示,該斜角光纖5之該端面E在研磨後係由一割線T分隔為該熔接面F及該研磨面G,該熔接面F與該研磨面G之夾角係該傾斜角度θ之補角,該傾斜角度θ較佳為45度,該熔接面F與該斜角光纖5之橫切面的夾角較佳小於1度;又,該割線T與該熔接面F之周緣的最大垂直距離係一端面高度H,該端面高度H可以是66.6微米至86微米,係可以確保共振腔之開口可供介質流通,同時減少對該斜角光纖5之結構破壞,能夠維持光纖干涉儀之機械強度及提升製程良率。 Please refer to FIG. 4c, the end surface E of the oblique optical fiber 5 is divided by a cutting line T into the welding surface F and the grinding surface G after grinding, and the angle between the welding surface F and the grinding surface G is the Complementary angle of the inclination angle θ, the inclination angle θ is preferably 45 degrees, and the angle between the fusion surface F and the cross-section of the oblique optical fiber 5 is preferably less than 1 degree; in addition, the cut line T and the periphery of the fusion surface F The maximum vertical distance is the height H of the end face. The height H of the end face can be 66.6 microns to 86 microns. It can ensure that the opening of the resonant cavity can be used for medium circulation, and at the same time reduce the structural damage to the oblique fiber 5 and maintain fiber interference. The mechanical strength of the instrument and improve the process yield.

請參照第4d圖所示,接合該晶體光纖3與該斜角光纖5時,係可以在該單模光纖4連接該晶體光纖3之另一端,及該斜角光纖5位於該端面E之另一端,分別連接一光源X及一光功率計W,使該光功率計W透過該晶體光纖3、該單模光纖4及該斜角光纖5測量該光源X之光強度,當該晶體光纖3之該蝕刻纖芯與該斜角光纖5之纖芯完全對齊時,使串連各纖芯而形成之光路暢通,則該光功率計W能夠偵側到最大讀值,係可以輔助該晶體光纖3與該斜角光纖5在進行熔接過程中,避免纖芯接合發生些微錯位,能夠提升干涉頻譜的清晰度及減少元件損耗。 Referring to FIG. 4d, when the crystal fiber 3 and the oblique angle fiber 5 are spliced, the other end of the crystal fiber 3 can be connected to the single-mode fiber 4 and the oblique angle fiber 5 is located at the other end of the end face E One end is connected to a light source X and an optical power meter W, respectively, so that the optical power meter W passes through the crystal fiber 3, the single mode fiber 4 and the oblique fiber 5 to measure the light intensity of the light source X, when the crystal fiber 3 When the etched core and the core of the oblique optical fiber 5 are completely aligned, the optical path formed by connecting the cores is clear, the optical power meter W can detect the maximum reading, which can assist the crystal fiber 3. During the fusion splicing process with the oblique optical fiber 5, a slight misalignment of the core joint can be avoided, which can improve the clarity of the interference spectrum and reduce component losses.

綜上所述,本發明的光纖干涉儀及其製造方法,藉由蝕刻、研磨、熔接等製程方法,使不同粗細之纖芯結合共振腔,所生產的光纖干涉儀,係具有高折射率靈敏度、簡化製程難度及降低加工成本等功效;另外,藉由控制研磨角度、蝕刻時間等製程參數,係可以控制光纖干涉儀的尺寸結構,能夠配合感測需求調整共振腔及纖芯的規格,具有提升感測準確度及增加感測應用範圍等功效。 In summary, the optical fiber interferometer and its manufacturing method of the present invention, by etching, grinding, welding and other manufacturing methods, combine cores of different thicknesses with the resonant cavity, and the produced optical fiber interferometer has high refractive index sensitivity 、Simplify the process difficulty and reduce the processing cost. In addition, by controlling the process parameters such as grinding angle and etching time, the size and structure of the optical fiber interferometer can be controlled, and the specifications of the resonant cavity and the core can be adjusted according to the sensing needs. Improve the accuracy of sensing and increase the scope of sensing applications.

雖然本發明已利用上述較佳實施例揭示,然其並非用以限定本發明,任何熟習此技藝者在不脫離本發明之精神和範圍之內,相對上述實施例進行各種更動與修改仍屬本發明所保護之技術範疇,因此本發明之保護範圍當視後附之申請專利範圍所界定者為準。 Although the present invention has been disclosed using the above-mentioned preferred embodiments, it is not intended to limit the present invention. Any person skilled in the art without departing from the spirit and scope of the present invention, making various changes and modifications relative to the above-mentioned embodiments still belongs to this The technical scope of the invention is protected, so the scope of protection of the present invention shall be subject to the scope defined in the appended patent application.

1‧‧‧感測單元 1‧‧‧sensing unit

11‧‧‧外殼層 11‧‧‧Shell

12‧‧‧共振腔 12‧‧‧Resonant cavity

13‧‧‧第一纖芯 13‧‧‧First core

2‧‧‧導光單元 2‧‧‧Light guide unit

21‧‧‧纖殼 21‧‧‧ Fiber Shell

22‧‧‧第二纖芯 22‧‧‧second core

23‧‧‧開口部 23‧‧‧ opening

Claims (11)

一種光纖干涉儀,包含:一感測單元,具有一外殼層、由該外殼層包圍環繞之一共振腔,及位於該共振腔之中心軸線上的一第一纖芯;及二導光單元,各該導光單元具有一纖殼,及位於該纖殼之中心軸線上的一第二纖芯,該二導光單元係以軸向分別結合於該感測單元之二端,該第一纖芯與該二第二纖芯串接於同一軸線上,其中一該導光單元具有一開口部,該開口部位於該導光單元與該感測單元之接合處,該共振腔透過該開口部連通外部環境。 An optical fiber interferometer includes: a sensing unit having a shell layer, a resonance cavity surrounded by the shell layer, and a first fiber core located on a central axis of the resonance cavity; and two light guide units, Each of the light guide units has a fiber shell and a second fiber core located on the central axis of the fiber shell, the two light guide units are axially coupled to the two ends of the sensing unit, the first fiber The core and the two second fiber cores are connected in series on the same axis, one of the light guide units has an opening, the opening is located at the junction of the light guide unit and the sensing unit, and the resonant cavity passes through the opening Connect the external environment. 如申請專利範圍第1項所述之光纖干涉儀,其中,該感測單元係蝕刻加工後的光子晶體光纖,該光子晶體光纖具有一纖芯區域及一纖衣區域,該第一纖芯及該共振腔分別為被侵蝕之該纖芯區域及該纖衣區域。 The optical fiber interferometer as described in item 1 of the patent application scope, wherein the sensing unit is an etched photonic crystal fiber, the photonic crystal fiber has a core area and a fiber coat area, and the first core and The resonant cavity is the eroded core region and the fiber jacket region, respectively. 如申請專利範圍第1項所述之光纖干涉儀,其中,各該導光單元之該纖殼的直徑等於該感測單元之該外殼層的直徑。 An optical fiber interferometer as described in item 1 of the patent application range, wherein the diameter of the fiber shell of each light guide unit is equal to the diameter of the outer shell layer of the sensing unit. 如申請專利範圍第1項所述之光纖干涉儀,其中,各該導光單元之該第二纖芯的直徑大於該感測單元之該第一纖芯的直徑。 The optical fiber interferometer according to item 1 of the patent application scope, wherein the diameter of the second core of each light guide unit is larger than the diameter of the first core of the sensing unit. 一種光纖干涉儀製造方法,包含:將一晶體光纖之一第一連接面接合一單模光纖之一對接面,並裁切該晶體光纖形成一第二連接面;將該晶體光纖由該第二連接面一端浸入一蝕刻溶液,並靜置一蝕刻時間後,清洗及風乾該晶體光纖,使該晶體光纖形成軸向之一共振腔及一蝕刻纖芯;將一斜角光纖之一端面與一拋光片之間維持一傾斜角度進行研磨,研磨後之該端面形成一熔接面及一研磨面;及將該晶體光纖之該第二連接面接合該斜角光纖之該熔接面,該第二連接面 與該研磨面之間係該共振腔之開口。 A method for manufacturing an optical fiber interferometer, comprising: joining a first connection surface of a crystal fiber to a butt surface of a single-mode fiber, and cutting the crystal fiber to form a second connection surface; switching the crystal fiber from the second One end of the connection surface is immersed in an etching solution, and after standing for an etching time, the crystal fiber is cleaned and air-dried to form a resonant cavity and an etched core in the axial direction of the crystal fiber; Polishing discs are maintained at an inclined angle for grinding, and the end surface after grinding forms a fusion surface and a grinding surface; and the second connection surface of the crystal fiber is joined to the fusion surface of the oblique angle fiber, the second connection surface Between the grinding surface and the opening of the resonant cavity. 如申請專利範圍第5項所述之光纖干涉儀製造方法,其中,該第一連接面及該第二連接面與該晶體光纖之橫切面的夾角小於1度,該對接面與該單模光纖之橫切面的夾角小於1度,該熔接面與該斜角光纖之橫切面的夾角小於1度。 The method for manufacturing an optical fiber interferometer as described in item 5 of the patent application range, wherein the angle between the first connection surface and the second connection surface and the cross section of the crystal fiber is less than 1 degree, and the butting surface and the single-mode fiber The angle between the cross-sectional plane is less than 1 degree, and the angle between the fusion plane and the cross-sectional plane of the oblique optical fiber is less than 1 degree. 如申請專利範圍第5項所述之光纖干涉儀製造方法,其中,該晶體光纖浸入該蝕刻溶液之深度係該共振腔長度。 The method for manufacturing an optical fiber interferometer as described in item 5 of the patent application range, wherein the depth of the crystal fiber immersed in the etching solution is the length of the resonant cavity. 如申請專利範圍第5項所述之光纖干涉儀製造方法,其中,該蝕刻纖芯之直徑係與該蝕刻時間呈負相關。 The method for manufacturing an optical fiber interferometer as described in item 5 of the patent application scope, wherein the diameter of the etched core is inversely related to the etching time. 如申請專利範圍第5項所述之光纖干涉儀製造方法,其中,該斜角光纖之該端面係由一割線分隔為該熔接面及該研磨面,該熔接面與該研磨面之夾角係該傾斜角度之補角,該傾斜角度為45度。 The method for manufacturing an optical fiber interferometer as described in item 5 of the patent application range, wherein the end surface of the beveled optical fiber is divided by a secant into the welding surface and the polishing surface, and the angle between the welding surface and the polishing surface is the The supplementary angle of the tilt angle is 45 degrees. 如申請專利範圍第9項所述之光纖干涉儀製造方法,其中,該割線與該熔接面之周緣的最大垂直距離係一端面高度,該端面高度是66.6微米至86微米。 The method for manufacturing an optical fiber interferometer as described in item 9 of the patent application range, wherein the maximum vertical distance between the cutting line and the periphery of the welding surface is the height of one end surface, and the height of the end surface is 66.6 microns to 86 microns. 如申請專利範圍第5項所述之光纖干涉儀製造方法,其中,接合該晶體光纖與該斜角光纖時,在該單模光纖連接該晶體光纖之另一端,及該斜角光纖位於該端面之另一端,分別連接一光源及一光功率計,當該晶體光纖之該蝕刻纖芯與該斜角光纖之纖芯完全對齊時,該光功率計能夠偵側到最大讀值。 The method for manufacturing an optical fiber interferometer as described in item 5 of the patent application scope, wherein when splicing the crystal fiber and the beveled fiber, the other end of the crystal fiber is connected to the single-mode fiber, and the beveled fiber is located at the end face At the other end, a light source and an optical power meter are respectively connected. When the etched core of the crystal fiber is completely aligned with the core of the beveled fiber, the optical power meter can detect the maximum reading.
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Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN114184119A (en) * 2021-12-30 2022-03-15 台州安奇灵智能科技有限公司 Low-cost repeatedly-produced polarization-maintaining optical fiber end surface Michelson interference sensor

Citations (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US20060109477A1 (en) * 2004-11-19 2006-05-25 Yan Zhou High efficiency balanced detection interferometer
CN203894161U (en) * 2014-04-18 2014-10-22 深圳大学 All-fiber refractometer based on michelson interferometer and system
TWI458939B (en) * 2012-07-02 2014-11-01 Univ Nat United Highly sensitive optical interferometer and its making method
TWI545360B (en) * 2015-05-26 2016-08-11 國立中山大學 A method of producing optical fiber resonant cavity

Patent Citations (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US20060109477A1 (en) * 2004-11-19 2006-05-25 Yan Zhou High efficiency balanced detection interferometer
TWI458939B (en) * 2012-07-02 2014-11-01 Univ Nat United Highly sensitive optical interferometer and its making method
CN203894161U (en) * 2014-04-18 2014-10-22 深圳大学 All-fiber refractometer based on michelson interferometer and system
TWI545360B (en) * 2015-05-26 2016-08-11 國立中山大學 A method of producing optical fiber resonant cavity

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN114184119A (en) * 2021-12-30 2022-03-15 台州安奇灵智能科技有限公司 Low-cost repeatedly-produced polarization-maintaining optical fiber end surface Michelson interference sensor

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