TWI442114B - A fabrication method of few-mode double-clad crystal fibers and a processing method of double-clad crystal fibers - Google Patents

A fabrication method of few-mode double-clad crystal fibers and a processing method of double-clad crystal fibers Download PDF

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TWI442114B
TWI442114B TW100128990A TW100128990A TWI442114B TW I442114 B TWI442114 B TW I442114B TW 100128990 A TW100128990 A TW 100128990A TW 100128990 A TW100128990 A TW 100128990A TW I442114 B TWI442114 B TW I442114B
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fiber
double
crystal
diffusion
crystal fiber
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TW201307922A (en
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Jau Sheng Wang
Wood Hi Cheng
wei lun Wang
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Univ Nat Sun Yat Sen
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近單模態雙纖衣晶纖之製造方法及雙纖衣晶纖之加工方法Method for manufacturing near single mode double fiber clothing crystal fiber and processing method of double fiber clothing crystal fiber

本發明係關於一種光纖製造方法,尤其是一種藉由調整雙纖衣晶纖之纖心直徑,而形成近單模態雙纖衣晶纖之方法。The present invention relates to a method for fabricating an optical fiber, and more particularly to a method for forming a near-monomodal double-fiber crystal fiber by adjusting the core diameter of the double-fiber crystal fiber.

習知光纖製造方法(例如:抽絲塔技術或雷射基座加熱生長法(LHPG)等),係用以將一纖衣(Cladding)包覆於一纖心(Core),而形成一光纖(Optical Fibers),其中,採用「抽絲塔技術」得以由不同折射率之非晶矽材料形成該纖心及該纖衣,惟,該纖心之材料為非晶矽,而非具有良好光學、熱及機械特性之釔鋁石榴石(YAG)晶體。而採用「雷射基座加熱生長法」(LHPG)得以將釔鋁石榴石晶體製成一晶體光纖(Crystal Fibers,或稱晶纖)之纖心,且該纖心可以摻雜鎳離子(Ni2+ )及鉻離子(Cr4+ )等過渡材料,而使該晶纖具有1.3至1.6微米(μm)的寬頻發光頻譜,惟,該纖心之直徑很難縮至10微米以下,且該纖心直徑大小會隨長度而變化,造成傳輸時的插入損耗(Insertion Loss)提高。為克服上述問題,乃發展出以雷射基座加熱生長法為基礎的改良式方法。Conventional fiber manufacturing methods (for example, wire drawing tower technology or laser pedestal heating growth method (LHPG), etc.) are used to coat a fiber (Cladding) on a core to form an optical fiber. (Optical Fibers), wherein the "spinning tower technology" is used to form the core and the fiber by an amorphous germanium material having different refractive indices, but the material of the core is amorphous, rather than having good optics. , yttrium aluminum garnet (YAG) crystals with thermal and mechanical properties. The "laser radiant heating growth method" (LHPG) is used to form the yttrium aluminum garnet crystal into the core of a crystal fiber (Crystal Fibers, or crystal fiber), and the core can be doped with nickel ions (Ni a transition material such as 2+ ) and chromium ion (Cr 4+ ), such that the crystal fiber has a broad-band emission spectrum of 1.3 to 1.6 micrometers (μm), but the diameter of the core is difficult to be reduced to less than 10 micrometers, and The diameter of the core varies with length, resulting in increased insertion loss (Insertion Loss). In order to overcome the above problems, an improved method based on the laser pedestal heating growth method has been developed.

請參閱第1圖所示,如中華民國公告第I318305號「間接加熱之雙纖衣晶體光纖製造方法」發明專利案,揭示一種習知雙纖衣晶纖製造方法,其係進行一晶纖製備程序,以製造一雙纖衣晶纖(Double-Clad Crystal Fibers)9。詳言之,該晶纖製備程序係先製備一晶體光纖91,並將該晶體光纖91插入一玻璃毛細管(Fused Silica Capillary Tube)92中,然後在該玻璃毛細管92要加熱之熔區外圍設置一管狀晶體93,再以雷射R照射於該管狀晶體93而進行加熱,使該管狀晶體93逐漸升高溫度,而產生熱輻射加熱該玻璃毛細管92,使該玻璃毛細管92因高溫而包覆於該晶體光纖91,進而形成矽熔融式(Fused-Silica)包覆之雙纖衣晶纖9。其中,當該管狀晶體93逐漸升高溫度,而達到一擴散互融溫度(例如:1600℃)時,該管狀晶體93所產生的熱輻射促使該晶體光纖91及該玻璃毛細管92之間開始產生交互擴散現象,即該晶體光纖91及該玻璃毛細管92開始進行一「擴散互融過程」(Collapsing Process),待一段時間後,降低雷射R之功率,使該管狀晶體93之溫度低於該擴散互融溫度,使該晶體光纖91及該玻璃毛細管92之間停止產生交互擴散現象,即該晶體光纖91及該玻璃毛細管92結束進行該「擴散互融過程」,完成該雙纖衣晶纖9之製造過程(即該晶纖製備程序),且該雙纖衣晶纖9之纖心直徑小於10微米且纖心直徑均勻。Please refer to FIG. 1 , for example, the invention patent of "Indirect Heating Double Fiber Crystal Optical Fiber Manufacturing Method" of the Republic of China Announcement No. I318305, discloses a conventional method for manufacturing a double fiber clothing crystal fiber, which is prepared by a crystal fiber. Procedure to make a Double-Clad Crystal Fibers 9. In detail, the crystal fiber preparation process first prepares a crystal fiber 91, and inserts the crystal fiber 91 into a glass capillary (Fused Silica Capillary Tube) 92, and then sets a periphery of the melting zone where the glass capillary 92 is to be heated. The tubular crystal 93 is further heated by irradiating the tubular crystal 93 with a laser R to gradually raise the temperature of the tubular crystal 93, and heat radiation is generated to heat the glass capillary 92, so that the glass capillary 92 is coated with high temperature. The crystal fiber 91 further forms a Fused-Silica coated double-fiber crystal fiber 9. Wherein, when the tubular crystal 93 is gradually raised in temperature to reach a diffusion and fusion temperature (for example, 1600 ° C), the heat radiation generated by the tubular crystal 93 causes the crystal fiber 91 and the glass capillary 92 to start to be generated. The phenomenon of mutual diffusion, that is, the crystal fiber 91 and the glass capillary 92 begin a "collapsing process", and after a period of time, the power of the laser R is lowered, so that the temperature of the tubular crystal 93 is lower than the Diffusion and fusion temperature, the inter-diffusion phenomenon is stopped between the crystal optical fiber 91 and the glass capillary 92, that is, the crystal optical fiber 91 and the glass capillary 92 complete the "diffusion and integration process", and the double-fiber crystal fiber is completed. The manufacturing process of 9 (i.e., the crystal fiber preparation procedure), and the fiber diameter of the double-fiber crystal fiber 9 is less than 10 μm and the core diameter is uniform.

請參閱第2圖所示,其係習知雙纖衣晶纖製造方法之纖心直徑變化曲線圖,其中,當該「擴散互融過程」開始進行後(即時間值≧0),隨著雷射強度增加,則纖心尺寸(即纖心直徑)有縮小的趨勢;反之,則纖心尺寸有增大的趨勢。因此,長期以來,若欲製造纖心直徑較小的雙纖衣晶纖9,則須於該晶纖製備程序中,將雷射強度提高,使得該晶纖製備程序完成後,可以形成該纖心直徑較小之雙纖衣晶纖9。Please refer to FIG. 2, which is a graph of the core diameter change of the conventional method for manufacturing a double-fiber crystal fiber, wherein when the "diffusion and integration process" starts (ie, the time value ≧0), As the laser intensity increases, the core size (ie, the core diameter) tends to decrease; otherwise, the core size tends to increase. Therefore, for a long time, if a double-fiber crystal fiber 9 having a small core diameter is to be produced, the laser intensity must be increased in the crystal fiber preparation process, so that the fiber can be formed after the crystal fiber preparation process is completed. Double-fiber crystal fiber 9 with a small heart diameter.

此外,由於近單模態光纖(Few-Mode Fibers)之能量輸出分佈接近單模光纖,因此具有可以提高「增益離子吸收幫浦光源功率」及降低「雷射閥值功率」等優點,其中,近單模態光纖之纖心直徑≦2微米,若採用習知雙纖衣晶纖製造方法製造「近單模態雙纖衣晶纖」,則需於該「擴散互融過程」中增加雷射強度,以縮小該雙纖衣晶纖9之纖心直徑。惟,習知雙纖衣晶纖製造方法僅能使該纖心直徑縮至5±0.25μm,(請詳見中華民國公告第I318305號之說明書第8頁),若再進一步提高雷射強度,則會因為加熱溫度過高,使得玻璃材質的黏滯性降低,而容易造成纖心不連續或纖心直徑不均勻等現象,因此,習知雙纖衣晶纖製造方法無法製造「近單模態雙纖衣晶纖」。In addition, since the energy output distribution of the near-mode optical fiber (Few-Mode Fibers) is close to that of the single-mode fiber, it has the advantages of improving the "gain ion absorption pump source power" and lowering the "laser threshold power". Near-single-mode fiber has a core diameter of 微米2 μm. If a conventional double-fiber crystal fiber manufacturing method is used to manufacture "near-mode uni-fiber double-fiber crystal fiber", it is necessary to add a thunder to the "diffusion and integration process". The intensity of the shot is used to reduce the core diameter of the double-fiber crystal fiber 9. However, the conventional method for manufacturing a double-fiber crystal fiber can only reduce the diameter of the core to 5±0.25 μm (please refer to page 8 of the specification of the Republic of China Announcement No. I318305), and if the laser intensity is further increased, However, because the heating temperature is too high, the viscosity of the glass material is lowered, and the core discontinuity or the core diameter is not uniform. Therefore, the conventional double-fiber crystal fiber manufacturing method cannot manufacture the near-single mode. State double fiber clothing crystal fiber."

除此之外,目前尚無其他文獻提及有關近單模態雙纖衣晶纖之製造方法或雙纖衣晶纖之加工方法,用以將雙纖衣晶纖之纖心直徑縮至近單模態光纖之纖心直徑。因此,長期以來,產業界存在無法製造近單模態雙纖衣晶纖的問題,當通訊光波段的光訊號於雙纖衣晶纖傳遞時,能量輸出分佈無法接近單模光纖,因此,不僅「增益離子吸收幫浦光源功率」無法提高,而且「雷射閥值功率」無法降低。In addition, there is no other literature mentioning the manufacturing method of the near-monomodal double-fiber crystal fiber or the processing method of the double-fiber crystal fiber to reduce the core diameter of the double-fiber crystal fiber to the near single The core diameter of the modal fiber. Therefore, for a long time, there is a problem in the industry that it is impossible to manufacture near-single-mode double-fiber crystal fiber. When the optical signal of the communication optical band is transmitted in the double-fiber crystal fiber, the energy output distribution cannot be close to the single-mode fiber, and therefore, not only The "gain ion absorption pump source power" cannot be increased, and the "laser threshold power" cannot be lowered.

綜上所述,有必要提供一種近單模態雙纖衣晶纖之製造方法,以製造一種纖心直徑縮至近單模態光纖之纖心直徑、纖心直徑均勻及纖心材料為釔鋁石榴石晶體之雙纖衣晶纖,以及一種雙纖衣晶纖之加工方法,用以將該雙纖衣晶纖9之纖心直徑縮至近單模態光纖之纖心直徑。In summary, it is necessary to provide a method for manufacturing a near-monomodal double-fiber crystal fiber to produce a fiber core diameter reduced to a near-monomodal fiber core diameter, a uniform core diameter, and a core material of bismuth aluminum. A double-fiber crystal fiber of garnet crystals, and a method for processing a double-fiber crystal fiber to reduce the core diameter of the double-fiber crystal fiber 9 to the core diameter of the near-mono-mode fiber.

本發明的目的乃改良上述之缺點,以提供一種近單模態雙纖衣晶纖之製造方法,藉由多次調整纖心直徑之過程,而製造一種纖心直徑縮至近單模態光纖之纖心直徑、纖心直徑均勻及纖心材料為釔鋁石榴石晶體之近單模態雙纖衣晶纖。The object of the present invention is to improve the above disadvantages, and to provide a method for manufacturing a near-monomodal double-fiber crystal fiber, which is manufactured by repeatedly adjusting the diameter of the core to reduce the core diameter to the near-simular fiber. The core diameter, the core diameter are uniform, and the core material is a near-unimodal double-fiber crystal fiber of yttrium aluminum garnet crystal.

本發明之次一目的,係提供一種雙纖衣晶纖之加工方法,藉由對雙纖衣晶纖進行至少一次纖心調整程序,使雙纖衣晶纖之纖心直徑可以縮至近單模態光纖之纖心直徑,而形成近單模態雙纖衣晶纖。A second object of the present invention is to provide a method for processing a double-fiber crystal fiber, wherein the core diameter of the double-fiber crystal fiber can be reduced to a near single mode by performing at least one core adjustment procedure on the double-fiber crystal fiber. The core diameter of the fiber is formed to form a near-unimodal double-fiber crystal fiber.

一種近單模態雙纖衣晶纖之製造方法,係包含:一晶纖製備程序,係進行一擴散互融過程一次而製備一雙纖衣晶纖;及一纖心調整程序,係將該雙纖衣晶纖重新進行該擴散互融過程至少一次,直到該雙纖衣晶纖之纖心直徑值縮至一近單模態纖心直徑值,而形成一近單模態雙纖衣晶纖;其中,各該擴散互融過程之雷射功率值逐次降低。A method for manufacturing a near-single-mode double-fiber crystal fiber comprises: a crystal fiber preparation process for performing a diffusion and mutual fusion process to prepare a double-fiber crystal fiber; and a core adjustment program The double-fiber crystal fiber re-does the diffusion and fusion process at least once until the core diameter value of the double-fiber crystal fiber is reduced to a near-unimodal core diameter value to form a near-monomodal double-fiber crystal Fiber; wherein the laser power value of each of the diffusion and mutual fusion processes is successively decreased.

其中,該纖心調整程序進行該擴散互融過程之雷射功率值低於該晶纖製備程序進行該擴散互融過程之雷射功率值。The laser power value of the diffusion adjustment process is lower than the laser power value of the diffusion process.

其中,該纖心調整程序之擴散互融過程重新進行的次數若為數次,則各該擴散互融過程之雷射功率值逐次降低。Wherein, if the number of times of the diffusion and integration process of the core adjustment procedure is repeated several times, the laser power value of each of the diffusion and integration processes is successively decreased.

其中,該晶纖製備程序係由一雷射照射於一管狀晶體而產生熱輻射,使一晶體光纖及一玻璃毛細管開始進行該擴散互融過程,待該擴散互融過程結束後形成該雙纖衣晶纖。Wherein, the crystal fiber preparation process is irradiated to a tubular crystal by a laser to generate heat radiation, so that a crystal fiber and a glass capillary tube start the diffusion and mutual fusion process, and the double fiber is formed after the diffusion and integration process is completed. Clothing crystal fiber.

其中,該纖心調整程序係包含:一調整步驟,係由該雙纖衣晶纖再次開始進行該擴散互融過程,使該雙纖衣晶纖之纖心直徑縮小,其中,該調整步驟之擴散互融過程的雷射功率值低於上一次進行該擴散互融過程之雷射功率值;及一判斷步驟,係判斷該雙纖衣晶纖之纖心直徑值是否縮至該近單模態纖心直徑值,若判斷為是,則結束進行該擴散互融過程,以形成該近單模態雙纖衣晶纖,若判斷為否,則待結束進行該擴散互融過程後,再進行該調整步驟。Wherein, the core adjustment program comprises: an adjusting step, wherein the diffusion and mutual fusion process is started again by the double-fiber crystal fiber, and the core diameter of the double-fiber crystal fiber is reduced, wherein the adjusting step is The laser power value of the diffusion and integration process is lower than the laser power value of the previous diffusion and integration process; and a judging step is to determine whether the core diameter value of the fiberglass fiber is reduced to the near single mode If the value is determined to be YES, the diffusion and mutual fusion process is terminated to form the near-monomodal double-fiber crystal fiber. If the determination is negative, the diffusion and mutual fusion process is to be completed. Perform this adjustment step.

一種雙纖衣晶纖之加工方法,係包含:一調整步驟,係由一雙纖衣晶纖開始進行一擴散互融過程,使該雙纖衣晶纖之纖心直徑縮小,其中,該調整步驟之雷射功率值低於該雙纖衣晶纖製造時之擴散互融過程的雷射功率值,且該調整步驟若非第一次進行,則該擴散互融過程之雷射功率值低於上一次進行該擴散互融過程之雷射功率值;及一判斷步驟,係判斷該雙纖衣晶纖之纖心直徑值是否縮至一預定直徑值,若判斷為是,則結束進行該擴散互融過程,以形成一近單模態雙纖衣晶纖,若判斷為否,則待結束進行該擴散互融過程後,再進行該調整步驟。A method for processing a double-fiber crystal fiber comprises: an adjusting step of performing a diffusion and mutual fusion process by a pair of fiber-optic crystal fibers, thereby reducing a core diameter of the fiber-optic fiber, wherein the adjusting The laser power value of the step is lower than the laser power value of the diffusion and fusion process during the manufacturing of the double fiber crystal fiber, and if the adjustment step is not performed for the first time, the laser power value of the diffusion and integration process is lower than a laser power value of the last diffusion process; and a determining step of determining whether the core diameter value of the fiberglass fiber is reduced to a predetermined diameter value, and if the determination is yes, ending the diffusion The mutual fusion process is performed to form a near-monomodal double-fiber crystal fiber. If the determination is negative, the adjustment step is performed after the diffusion and mutual integration process is completed.

其中,該預定直徑值等於一近單模態纖心直徑值。Wherein the predetermined diameter value is equal to a near single mode core diameter value.

其中,該預定直徑值大於一近單模態纖心直徑值。Wherein the predetermined diameter value is greater than a near single mode core diameter value.

其中,該雙纖衣晶纖之纖心材料為釔鋁石榴石晶體。Wherein, the core material of the double-fiber crystal fiber is yttrium aluminum garnet crystal.

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:本發明全文所述之「晶纖」(Crystal Fibers),係指晶體光纖,其纖心材料為晶體,例如:釔鋁石榴石晶體,一般石榴石之空間群(space group)屬於Ia-3d(Oh 10 ),其化學通式可寫成Y3Al5Ol2(YAG),其係本發明所屬技術領域中具有通常知識者可以理解。The above and other objects, features and advantages of the present invention will become more <RTIgt;"CrystalFibers" refers to a crystalline fiber whose core material is a crystal, such as yttrium aluminum garnet crystal. The space group of garnet belongs to Ia-3d (O h 10 ). The formula can be written as Y3Al5Ol2 (YAG), which is understood by those of ordinary skill in the art to which the present invention pertains.

本發明全文所述之「雙纖衣」(Double-Clad),係指晶纖於主要傳輸光能量之纖心外,另包覆兩層玻璃為主材質,其係本發明所屬技術領域中具有通常知識者可以理解。"Double-Clad" as used throughout the present invention refers to a crystal fiber which is mainly composed of a core material which mainly transmits light energy, and is coated with two layers of glass as a main material, which has the technical field of the present invention. Usually the knowledge person can understand.

本發明全文所述之「摻鉻」(Cr-Doped),係指將鉻離子掺入YAG材料中,其係本發明所屬技術領域中具有通常知識者可以理解。"Cr-Doped" as used throughout the present invention refers to the incorporation of chromium ions into a YAG material, as will be understood by those of ordinary skill in the art to which the present invention pertains.

本發明全文所述之「近單模態」(Few-Mode),係指當通訊光波段的光訊號於光纖中傳遞時,能量輸出分佈接近單模光纖之光纖狀態,其中,當光纖結構的纖心直徑越做越小時,較高階的模態就會隨著縮小的纖心直徑而截止,能存在於光纖中的模態數目就越來越少,一旦纖心直徑尺寸小於某一特定值,所有高階模態便會截止,只存在最低階基礎模態。以Corning公司所生產的單模矽光纖SMF28為例,入射光波長用1.55微米計算,其纖心折射率n1=1.465、纖衣折射率n2=1.46,則纖心半徑需小於9微米時,所有高階模態才會全部截止。這個觀念可以簡單地用V-number來計算,給定光纖結構尺寸與折射率以及入射光波長,若V≦2.405,則該光纖只存在最低階的基礎模態。本發明之V-number在1.4微米為3.8,相當接近理論值(V=2.405),故稱之為近單模態(Few-Mode),其係本發明所屬技術領域中具有通常知識者可以理解。The "Few-Mode" as described in the full text of the present invention means that when the optical signal of the communication optical band is transmitted in the optical fiber, the energy output distribution is close to the optical fiber state of the single-mode optical fiber, wherein when the optical fiber structure is As the core diameter becomes smaller, the higher order mode is cut off with the reduced core diameter, and the number of modes that can exist in the fiber is less and less, once the core diameter size is less than a certain value. All high-order modes will be cut off, and only the lowest-order basic modes exist. Taking the single-mode 矽 fiber SMF28 produced by Corning as an example, the incident light wavelength is calculated by 1.55 micrometer, and the core refractive index n1=1.465, the fiber refractive index n2=1.46, and the core radius is less than 9 micrometers, all The higher order modes will all be cut off. This concept can be simply calculated using V-number, given the fiber structure size and refractive index and the wavelength of the incident light. If V≦2.405, then the fiber has only the lowest order fundamental mode. The V-number of the present invention is 3.8 at 1.4 micrometers, which is quite close to the theoretical value (V=2.405), so it is called near-unimodal (Few-Mode), which can be understood by those having ordinary knowledge in the technical field to which the present invention pertains. .

本發明所述之「雷射基座加熱生長法」(LHPG),或稱LHPG生長法,係屬於浮動熔區法的一種,最早由Burrus和Stone所開發,LHPG生長法是以連續式CO2雷射為加熱源,CO2雷射光源經衰減器將功率衰減後,藉由兩個凸透鏡將雷射光束擴束,使原來直徑為5毫米之雷射光束擴增為3公分,然後再進入生長腔中,當3公分的CO2雷射進入生長腔中後,會經過一組內外圓錐的反射鏡,此時圓形光束會轉變成環形光束,然後再經一傾角45°之平面反射鏡將雷射反射進入頂端之拋物面反射鏡,最後由拋物面反射鏡將CO2雷射光聚焦於原始晶棒之頂端,使原始晶棒頂端熔融,藉由適當的控制CO2雷射的功率,使原始晶棒頂端形成一熔融之半球,由電腦介面的控制使得子晶緩慢地下移與熔區接觸,然後調整熔區的形狀,使上下兩個固定介面呈水平,再緩慢地將子晶往上拉,藉由功率衰減器微調CO2雷射的功率,以調整熔區的大小,使得熔區的高度與原始晶棒直徑相近,此時一面將子晶往上拉,一面將原始晶棒往上推送,便可成長出晶體光纖,其係本發明所屬技術領域中具有通常知識者可以理解。The "Lray Base Heating Growth Method" (LHPG), or LHPG growth method, of the present invention belongs to the floating melting zone method, which was first developed by Burrus and Stone, and the LHPG growth method is a continuous CO2 mine. As a heating source, the CO2 laser light source attenuates the power through the attenuator, and the laser beam is expanded by two convex lenses, so that the original laser beam with a diameter of 5 mm is amplified to 3 cm, and then enters the growth chamber. When a 3 cm CO2 laser enters the growth chamber, it passes through a set of mirrors inside and outside the cone. At this time, the circular beam is converted into a ring beam, and then the laser is irradiated through a plane mirror with an inclination of 45°. Reflecting the parabolic mirror into the top, the parabolic mirror focuses the CO2 laser light on the top of the original ingot to fuse the top of the original ingot. By properly controlling the power of the CO2 laser, the top of the original ingot is formed. The molten hemisphere is controlled by the computer interface to slowly move the subcrystals into contact with the melting zone, then adjust the shape of the melting zone so that the upper and lower fixed interfaces are horizontal, and then slowly pull the subcrystals upwards, with power attenuation. Fine-tune the power of the CO2 laser to adjust the size of the melt zone so that the height of the melt zone is close to the diameter of the original ingot. At this time, the seed crystal is pulled up and the original crystal bar is pushed up to grow the crystal. Optical fibers are understood by those of ordinary skill in the art to which the present invention pertains.

本發明所述之「擴散互融過程」(Collapsing Process),係指一管狀藍寶石晶體(Sapphire Tube)經由加熱而大於或等於一擴散互融溫度(例如:1600℃)時,該管狀藍寶石晶體所產生熱輻射,使得形成雙纖衣晶纖之晶體光纖及玻璃毛細管之間溫度提高製玻璃軟化溫度,而開始產生交互擴散(interdiffusion)現象(即開始進行擴散互融過程),直到該管狀晶體之溫度小於該擴散互融溫度時,晶體光纖及玻璃毛細管之間溫度降低,而停止產生交互擴散現象(即停止進行擴散互融過程),其係本發明所屬技術領域中具有通常知識者可以理解。The "collapsing process" in the present invention refers to a tubular sapphire crystal when a tubular sapphire crystal is heated to be greater than or equal to a diffusion and fusion temperature (for example, 1600 ° C). Producing heat radiation, such that the temperature between the crystal fiber forming the double-fiber crystal fiber and the glass capillary increases the glass softening temperature, and begins to generate an interdiffusion phenomenon (ie, begins the diffusion and mutual fusion process) until the tubular crystal When the temperature is less than the diffusion and fusion temperature, the temperature between the crystal fiber and the glass capillary is lowered, and the occurrence of the interdiffusion phenomenon (i.e., stopping the diffusion and mutual fusion process) is stopped, which is understood by those skilled in the art to which the present invention pertains.

本發明所述之「增益離子吸收幫浦光源功率」(Gain Medium Absorbed Pumping Power),係指當鎳離子(Ni2+ )及鉻離子(Cr4+ )等過渡金屬材料摻雜於纖心時,該過渡金屬材料中的離子吸收雷射激發光源之能量,其係本發明所屬技術領域中具有通常知識者可以理解。The "Gain Medium Absorbed Pumping Power" in the present invention refers to when a transition metal material such as nickel ions (Ni 2+ ) and chromium ions (Cr 4+ ) is doped into the core. The ions in the transition metal material absorb the energy of the laser excitation source, as will be understood by those of ordinary skill in the art to which the present invention pertains.

本發明所述之「雷射閥值功率」(Pumping Threshold Power),係指在雷射泵浦功率增加達一臨界值時,使得雷射增益介質的粒子數達到居量數反轉,而使受激輻射大於自發輻射產生雷射輸出,此時的臨界值稱為雷射閥值功率,其係本發明所屬技術領域中具有通常知識者可以理解。The "Pumping Threshold Power" in the present invention means that when the laser pump power increases by a critical value, the number of particles of the laser gain medium is reversed, and The stimulated radiation is greater than the spontaneous radiation to produce a laser output, and the critical value at this time is referred to as the laser threshold power, as will be understood by those of ordinary skill in the art to which the present invention pertains.

本發明所述之「近單模態纖心直徑值」(a diameter value of the core of the few-mode double-clad crystal fiber),係指若晶體光纖之纖心折射率n1=1.82且內層纖衣折射率n2=1.64,則當纖心半徑需≦2微米時,高階模態才會截止,因此,近單模態晶體光纖之纖心直徑值係≦2微米,其係本發明所屬技術領域中具有通常知識者可以理解。The "a diameter value of the core of the few-mode double-clad crystal fiber" refers to a core fiber refractive index n1=1.82 and an inner layer. When the refractive index of the fiber is n2=1.64, the high-order mode is cut off when the core radius needs to be 2 μm. Therefore, the core diameter value of the near-monomorphic crystal fiber is 微米2 μm, which is the technology of the present invention. Those with ordinary knowledge in the field can understand.

請參閱第3圖所示,其係本發明之近單模態雙纖衣晶纖之製造方法較佳實施例之系統示意圖,其係藉由一晶纖製造裝置A製造一雙纖衣晶纖1(例如:纖心直徑值≧5微米),再使該雙纖衣晶纖1之纖心直徑值縮至一預定直徑值(例如:一近單模態纖心直徑值),而形成一近單模態雙纖衣晶纖2。在此實施例中,該晶纖製造裝置A為習知雷射基座加熱生長(LHPG)裝置,惟不以此為限;該晶纖製造裝置A係包含一雷射R及一管狀晶體T,該雷射R可以照射該管狀晶體T進行加熱,其中,該晶纖製造裝置A還可以執行一製造程式及/或顯示該雙纖衣晶纖1之即時影像,用以觀測及調整該雙纖衣晶纖1之纖心直徑;該雙纖衣晶纖1為習知雙纖衣晶纖,例如:摻鉻雙纖衣晶纖(Cr-Doped Double-Clad Crystal Fibers)等,惟不以此為限。Please refer to FIG. 3 , which is a schematic diagram of a system for manufacturing a near-single-mode double-fiber crystal fiber according to a preferred embodiment of the present invention, which is manufactured by a crystal fiber manufacturing device A to produce a double fiber crystal fiber. 1 (for example, a core diameter value of ≧ 5 μm), and then reducing the core diameter value of the double-fiber crystal fiber 1 to a predetermined diameter value (for example, a near-monomodal core diameter value) to form a Near monomodal double fiber clothing crystal fiber 2. In this embodiment, the crystal fiber manufacturing device A is a conventional laser pedestal heating growth (LHPG) device, which is not limited thereto; the crystal fiber manufacturing device A includes a laser R and a tubular crystal T The laser R can be irradiated to the tubular crystal T for heating, wherein the crystal fiber manufacturing apparatus A can also execute a manufacturing program and/or display an instant image of the double-fiber crystal fiber 1 for observing and adjusting the double The core diameter of the fiber-optic crystal fiber 1; the double-fiber crystal fiber 1 is a conventional double-fiber crystal fiber, for example, Cr-Doped Double-Clad Crystal Fibers, etc., but This is limited.

請參閱第4圖所示,其係本發明之近單模態雙纖衣晶纖之製造方法較佳實施例之流程圖,本發明之近單模態雙纖衣晶纖之製造方法係包含一晶纖製備程序S1及一纖心調整程序S2,該晶纖製備程序S1係進行一擴散互融過程(Collapsing Process)一次,以製備該雙纖衣晶纖1,之後,再進行該纖心調整程序S2。詳言之,該晶纖製備程序S1係如習知雙纖衣晶纖製造方法,由該雷射R照射於該管狀晶體T而產生熱輻射,使一晶體光纖(Crystal Fiber)11及一玻璃毛細管(Fused Silica Capillary Tube)12開始進行一擴散互融過程,待該擴散互融過程結束後形成該雙纖衣晶纖1,在此容不贅述。其中,該雙纖衣晶纖1之纖心直徑值大於該近單模態纖心直徑值;該雷射R之雷射功率值可以為一常數值或一變數值(例如:功率與時間之關係曲線等)。Referring to FIG. 4, which is a flow chart of a preferred embodiment of a method for manufacturing a near-simular dual-fiber crystal fiber of the present invention, the method for manufacturing a near-simular double-fiber crystal fiber of the present invention comprises a crystal fiber preparation program S1 and a core adjustment program S2, the crystal fiber preparation program S1 is subjected to a diffusion process (Collapsing Process) once to prepare the double fiber clothing crystal fiber 1, and then the core fiber is further processed. Adjust program S2. In detail, the crystal fiber preparation program S1 is a conventional method for manufacturing a double-fiber crystal fiber, and the laser light is irradiated onto the tubular crystal T to generate heat radiation, so that a crystal fiber 11 and a glass are produced. The capillary (Fused Silica Capillary Tube) 12 begins a diffusion and mutual fusion process, and the double-fiber crystal fiber 1 is formed after the diffusion and fusion process is completed, and is not described herein. The core diameter value of the double-fiber crystal fiber 1 is greater than the near-unimodal core diameter value; the laser power value of the laser R may be a constant value or a variable value (for example, power and time) Relationship curve, etc.).

該纖心調整程序S2係將該雙纖衣晶纖1重新進行該擴散互融過程至少一次,直到該雙纖衣晶纖1之纖心直徑值縮至該預定直徑值,其中,若該預定直徑值為該近單模態纖心直徑值,則可以形成該近單模態雙纖衣晶纖2。其中,該纖心調整程序S2進行該擴散互融過程之雷射功率值低於該晶纖製備程序S1進行該擴散互融過程之雷射功率值,且該纖心調整程序S2之擴散互融過程重新進行的次數若為數次,則各該擴散互融過程之雷射功率值逐次降低,換言之,該晶纖製備程序S1及該纖心調整程序S2之各該擴散互融過程的雷射功率值逐次降低。在此實施例中,該近單模態纖心直徑值係以2微米作為實施態樣說明,惟不以此為限。The core adjustment procedure S2 is to perform the diffusion and mutual fusion process at least once until the core diameter value of the double-fiber crystal fiber 1 is reduced to the predetermined diameter value, wherein, if the predetermined The diameter value is the near-monomodal core diameter value, and the near-monomodal double-fiber crystal fiber 2 can be formed. The laser power value of the diffusion adjustment process is lower than the laser power value of the diffusion preparation process, and the diffusion adjustment of the core adjustment program S2 is performed. If the number of times the process is re-executed is several times, the laser power values of the diffusion and mutual integration processes are successively decreased, in other words, the laser power of the diffusion process of the crystal fiber preparation program S1 and the core adjustment program S2 The value is gradually reduced. In this embodiment, the near-unimodal core diameter value is described by using 2 micrometers as an implementation example, but not limited thereto.

詳言之,該纖心調整程序S2係包含一調整步驟S21及一判斷步驟S22,該調整步驟S21係由該雙纖衣晶纖1再次開始進行該擴散互融過程,使該雙纖衣晶纖1之纖心直徑縮小,其中,該調整步驟S21之雷射功率值低於該雙纖衣晶纖製造時之擴散互融過程的雷射功率值,且該調整步驟S21若非第一次進行,則該擴散互融過程之雷射功率值低於上一次進行該擴散互融過程之雷射功率值。之後,再進行該判斷步驟S22。更詳言之,該調整步驟S21係將該雙纖衣晶纖1穿入該管狀晶體T,並由該雷射R加熱該管狀晶體T,該管狀晶體T產生熱輻射加熱該雙纖衣晶纖1,使該雙纖衣晶纖1再次開始進行該擴散互融過程,其中,藉由降低雷射功率值,可以弱化該雙纖衣晶纖1之離子擴散效應(Ions Diffusion),而減緩該晶體光纖11與該玻璃毛細管12之間交互擴散的程度,使該雙纖衣晶纖1之纖心直徑縮小,因此可以增加該雙纖衣晶纖1之纖心直徑值的可調性,之後,再進行該判斷步驟S22。其中,藉由功率控制技術可以將該雷射功率值進行回授計算,使該雷射功率值之變動量維持於±0.1%。In detail, the core adjustment program S2 includes an adjustment step S21 and a determination step S22. The adjustment step S21 is performed again by the double-fiber crystal fiber 1 to perform the diffusion and mutual fusion process to make the double-fiber crystal The core diameter of the fiber 1 is reduced, wherein the laser power value of the adjusting step S21 is lower than the laser power value of the diffusion and fusion process during the manufacturing of the fiber-optic fiber, and the adjusting step S21 is not performed for the first time. The laser power value of the diffusion and integration process is lower than the laser power value of the previous diffusion and integration process. Thereafter, the determining step S22 is performed again. More specifically, the adjusting step S21 penetrates the double-fiber crystal fiber 1 into the tubular crystal T, and the tubular crystal T is heated by the laser R, and the tubular crystal T generates heat radiation to heat the double-fiber crystal. Fiber 1 causes the double-fiber crystal fiber 1 to start the diffusion and mutual fusion process again, wherein by reducing the laser power value, the ion diffusion effect (Ions Diffusion) of the double-fiber crystal fiber 1 can be weakened and slowed down. The degree of inter-diffusion between the crystal optical fiber 11 and the glass capillary tube 12 reduces the core diameter of the double-fiber crystal fiber 1, thereby increasing the adjustability of the core diameter value of the double-fiber crystal fiber 1. Thereafter, the determining step S22 is performed again. The power control technology can perform the feedback calculation on the laser power value to maintain the variation of the laser power value at ±0.1%.

該判斷步驟S22係判斷該雙纖衣晶纖1之纖心直徑值是否縮至該預定直徑值,例如:該近單模態纖心直徑值,惟不以此為限,若判斷為「是」,則結束進行該擴散互融過程,形成該近單模態雙纖衣晶纖2;若判斷為「否」,則待結束進行該擴散互融過程後,再進行該調整步驟S21。更詳言之,該判斷步驟S22係藉由即時影像監測技術,例如:以電荷耦合元件(CCD)搭配電腦程式形成影像等方式,而由該晶纖製造裝置A或一顯示裝置(圖未繪示)觀測該雙纖衣晶纖1之即時影像,並將該即時影像供一使用者或一製造程式監測該雙纖衣晶纖1之纖心直徑值,以判斷是否於結束進行該擴散互融過程後,再次進行該調整步驟S21。其中,若該纖心直徑值尚未縮至該預定直徑值,則可於該雙纖衣晶纖1之纖心直徑保持均勻時,先結束進行該擴散互融過程,使得該雙纖衣晶纖1可以在纖心直徑保持均勻先冷卻凝固,以便再次進行該調整步驟S21,以小幅修整該雙纖衣晶纖1之纖心直徑;反之,若該纖心直徑值已縮至該預定直徑值(例如:該近單模態纖心直徑值),則直接結束進行該擴散互融過程,而形成該近單模態雙纖衣晶纖2。在此實施例中,係以進行三次該擴散互融過程,並將該預定直徑值設為2微米作為實施態樣說明如後,惟不以此為限。The determining step S22 is to determine whether the core diameter value of the double-fiber crystal fiber 1 is reduced to the predetermined diameter value, for example, the near-unimodal core diameter value, but not limited thereto. Then, the diffusion and mutual fusion process is completed to form the near-unimodal double-fiber crystal fiber 2; if the determination is "NO", the adjustment step S21 is performed after the diffusion and mutual integration process is completed. More specifically, the determining step S22 is performed by the instant image monitoring technology, for example, by forming a video with a charge coupled device (CCD) and a computer program, and the crystal fiber manufacturing device A or a display device (not shown) Observing the real-time image of the double-fiber crystal 1 and monitoring the core diameter value of the double-fiber crystal 1 by a user or a manufacturing program to determine whether the diffusion is completed at the end After the melting process, the adjustment step S21 is performed again. Wherein, if the core diameter value has not been reduced to the predetermined diameter value, the diffusion and mutual fusion process may be ended first when the core diameter of the double-fiber crystal fiber 1 is kept uniform, so that the double-fiber crystal fiber 1 can be cooled and solidified while maintaining the core diameter uniformly, so as to perform the adjusting step S21 again to slightly trim the core diameter of the double-fiber crystal fiber 1; conversely, if the core diameter value has been reduced to the predetermined diameter value (for example, the near-monomodal core diameter value), the diffusion and mutual fusion process is directly ended, and the near-monomodal double-fiber crystal fiber 2 is formed. In this embodiment, the diffusion and mutual fusion process is performed three times, and the predetermined diameter value is set to 2 micrometers as an embodiment, but is not limited thereto.

舉例而言,該晶纖製備程序S1係先備妥該晶體光纖11,例如:摻鉻釔鋁石榴石(Cr:YAG)晶棒,其直徑值及長度值各為0.5毫米(mm)及3公分(cm);待該晶體光纖11進行雷射基座加熱生長法(LHPG Method)兩次後,該晶體光纖11之直徑降低至70±2微米;接著,將該晶體光纖11置入該玻璃毛細管12,例如:內徑為76微米、外徑為320微米之玻璃毛細管12;之後,將該晶體光纖11及該玻璃毛細管12以一穿越速度(例如:3至5毫米/分鐘)穿入該管狀晶體T(例如:藍寶石晶體管等),同時,由該雷射R(例如:CO2 雷射等)照射於該管狀晶體T進行加熱,其中,該雷射R之功率曲線為該第一功率曲線P1(如第5圖所示),使該管狀晶體T逐漸升高溫度,而產生熱輻射加熱該玻璃毛細管12,該晶體光纖11及該玻璃毛細管12因為開始進行該擴散互融過程,使該晶體光纖11及該玻璃毛細管12之間產生交互擴散(interdiffusion)現象,待結束進行該擴散互融過程後,形成一內纖衣層(inner cladding layer),使得該晶體光纖11及該玻璃毛細管12共同形成矽熔融式包覆之雙纖衣晶纖1。For example, the crystal fiber preparation program S1 is prepared by preparing the crystal optical fiber 11, for example, a chrome-doped yttrium aluminum garnet (Cr:YAG) ingot having a diameter value and a length value of 0.5 mm (mm) and 3, respectively. Dimensions (cm); after the crystal fiber 11 is subjected to the LHPG Method twice, the diameter of the crystal fiber 11 is reduced to 70 ± 2 μm; then, the crystal fiber 11 is placed in the glass. The capillary 12, for example, a glass capillary 12 having an inner diameter of 76 μm and an outer diameter of 320 μm; thereafter, the crystal optical fiber 11 and the glass capillary 12 are penetrated at a crossing speed (for example, 3 to 5 mm/min). a tubular crystal T (for example, a sapphire transistor or the like), and simultaneously irradiated to the tubular crystal T by the laser R (for example, a CO 2 laser or the like) for heating, wherein a power curve of the laser R is the first power Curve P1 (as shown in Fig. 5) causes the tubular crystal T to gradually increase in temperature, and heat radiation is generated to heat the glass capillary tube 12. The crystal optical fiber 11 and the glass capillary tube 12 are subjected to the diffusion and mutual fusion process. Interacting between the crystal fiber 11 and the glass capillary 12 (interdif) a fusion phenomenon, after the diffusion and mutual fusion process is completed, an inner cladding layer is formed, so that the crystal optical fiber 11 and the glass capillary 12 together form a double-coated crystal fiber 1 which is melt-coated. .

該纖心調整程序S2係先進行該調整步驟S21,由該雷射R加熱該管狀晶體T,使該雙纖衣晶纖1再次開始進行該擴散互融過程,其中,該雷射R之功率曲線為該第二功率曲線P2(如第5圖所示),該第二功率曲線P2之值低於該第一功率曲線P1之值,使該晶體光纖11及該玻璃毛細管12之間產生小幅度的交互擴散,用以縮小該雙纖衣晶纖1之纖心直徑值,並且,使該雙纖衣晶纖1之纖心保持均勻及連續。接著,進行該判斷步驟S22,由該晶纖製造裝置A取得該雙纖衣晶纖1之即時影像,該使用者及該製造程式可以由該即時影像判讀該雙纖衣晶纖1之纖心直徑值,此時,由於該纖心直徑值尚未縮至2微米,因此,於結束該擴散互融過程後,再進行該調整步驟S21,以再次開始進行該擴散互融過程,其中,該雷射R之功率曲線為該第三功率曲線P3(如第5圖所示),該第三功率曲線P3之值低於該第二功率曲線P2之值,使該雙纖衣晶纖1之纖心直徑可以進一步縮小;接著進行該判斷步驟S22,若該纖心直徑值已縮至2微米,則結束該擴散互融過程,形成該近單模態雙纖衣晶纖2。The core adjustment program S2 first performs the adjusting step S21, and the tubular crystal T is heated by the laser R, so that the double-fiber crystal fiber 1 starts the diffusion and integration process again, wherein the power of the laser R The curve is the second power curve P2 (as shown in FIG. 5), and the value of the second power curve P2 is lower than the value of the first power curve P1, so that the crystal fiber 11 and the glass capillary 12 are small. The mutual diffusion of the amplitude is used to reduce the core diameter value of the double-fiber crystal fiber 1, and the core of the double-fiber crystal fiber 1 is kept uniform and continuous. Then, the determining step S22 is performed, and the instant image of the double-fiber crystal fiber 1 is obtained by the crystal fiber manufacturing device A, and the user and the manufacturing program can interpret the core of the double-fiber crystal fiber 1 from the instant image. The diameter value, at this time, since the core diameter value has not been reduced to 2 micrometers, after the diffusion and mutual integration process is finished, the adjusting step S21 is performed to start the diffusion and mutual fusion process again, wherein the lightning The power curve of the R is the third power curve P3 (as shown in FIG. 5), and the value of the third power curve P3 is lower than the value of the second power curve P2, so that the fiber of the double fiber clothing crystal fiber 1 The core diameter can be further reduced; then the determining step S22 is performed, and if the core diameter value has been reduced to 2 micrometers, the diffusion and mutual fusion process is terminated to form the near-monomodal double-fiber crystal fiber 2.

綜上所述,本發明之近單模態雙纖衣晶纖之製造方法係由該晶纖製備程序S1先形成該纖心直徑較大之雙纖衣晶纖1,再由該纖心調整程序S2將該雙纖衣晶纖1重複進行該擴散互融過程,且該纖心調整程序S2之雷射功率值低於該晶纖製備程序S1之雷射功率值,且該纖心調整程序S2之雷射功率值逐次降低,直到該雙纖衣晶纖1之纖心直徑縮至該近單模態纖心直徑值,以形成該近單模態雙纖衣晶纖2。因此,本發明之近單模態雙纖衣晶纖之製造方法可以成功製造該近單模態雙纖衣晶纖2,其中,該近單模態雙纖衣晶纖2之纖心材料為釔鋁石榴石晶體、該近單模態雙纖衣晶纖2之纖心直徑值可縮至該近單模態纖心直徑值且纖心直徑均勻。In summary, the method for manufacturing the near-unimodal double-fiber crystal fiber of the present invention first forms the double-fiber crystal fiber 1 having a larger core diameter by the crystal fiber preparation program S1, and then the core is adjusted. The process S2 repeats the diffusion and fusion process of the double-fiber crystal fiber 1 , and the laser power value of the core adjustment program S2 is lower than the laser power value of the crystal fiber preparation program S1, and the core adjustment program The laser power value of S2 is successively decreased until the core diameter of the double-fiber crystal fiber 1 is reduced to the near-monomodal core diameter value to form the near-monomodal double-fiber crystal fiber 2. Therefore, the method for manufacturing the near-monomodal double-fiber crystal fiber of the present invention can successfully manufacture the near-monomodal double-fiber crystal fiber 2, wherein the core material of the near-monomodal double-fiber crystal fiber 2 is The yttrium aluminum garnet crystal, the core diameter value of the near-monomorphic double-fiber crystal fiber 2 can be reduced to the near-unimodal core diameter value and the core diameter is uniform.

再者,本發明之纖心調整程序S2可以調整現有雙纖衣晶纖的纖心直徑值,而形成一種雙纖衣晶纖之加工方法,藉由該調整步驟S21再次開始進行該擴散互融過程,並逐次降低雷射功率值,使該雙纖衣晶纖1之離子擴散效應降低,不僅可縮小該雙纖衣晶纖1之纖心直徑值,並使該雙纖衣晶纖1之纖心直徑值更具可調性。再藉由該判斷步驟S22判斷該雙纖衣晶纖1之纖心直徑是否縮至該預定直徑值,其中,該預定直徑值可以大於或等於該近單模態纖心直徑值,在此以「該預定直徑值等於該近單模態纖心直徑值」為例,若判斷為「是」,則結束進行該擴散互融過程,形成該近單模態雙纖衣晶纖2;若判斷為「否」,則待結束進行該擴散互融過程後,先降低雷射功率值,再進行該調整步驟S21。因此,本發明之雙纖衣晶纖之加工方法可以使現有雙纖衣晶纖之纖心直徑值縮至該近單模態纖心直徑值,而形成近單模態雙纖衣晶纖。Furthermore, the core adjustment program S2 of the present invention can adjust the core diameter value of the existing double-fiber crystal fiber to form a processing method of the double-fiber crystal fiber, and the diffusion integration is started again by the adjusting step S21. Process, and successively reducing the laser power value, so that the ion diffusion effect of the double-fiber crystal fiber 1 is reduced, not only reducing the core diameter value of the double-fiber crystal fiber 1, but also making the fiber-optic fiber 1 The core diameter value is more adjustable. And determining, by the determining step S22, whether the core diameter of the double-fiber crystal fiber 1 is reduced to the predetermined diameter value, wherein the predetermined diameter value may be greater than or equal to the near-unimodal core diameter value, where "The predetermined diameter value is equal to the near-unimodal core diameter value" as an example. If the determination is "Yes", the diffusion and mutual fusion process is terminated to form the near-monomodal double-fiber crystal fiber 2; If the value is NO, the laser power value is first lowered after the diffusion and mutual integration process is completed, and the adjustment step S21 is performed. Therefore, the method for processing the double-fiber crystal fiber of the present invention can reduce the core diameter value of the existing double-fiber crystal fiber to the near-monomodal core diameter value to form a near-monomodal double-fiber crystal fiber.

藉由前揭之技術手段,本發明所揭示之方法的主要特點列舉如下:The main features of the method disclosed by the present invention are listed below by the technical means disclosed above:

其一:由於該雙纖衣晶纖1之纖心直徑值可縮至該近單模態纖心直徑值,且進行該擴散互融過程之雷射功率值逐次降低,因此,本發明具有「增益離子吸收幫浦光源功率」提升及「雷射閥值功率」降低之功效。First, since the core diameter value of the double-fiber crystal fiber 1 can be reduced to the near-unimodal core diameter value, and the laser power value of the diffusion and mutual fusion process is successively decreased, the present invention has " The gain ion absorption boosts the power of the pump source and the "laser threshold power" is reduced.

其二:由於近單模態摻鉻雙纖衣晶纖之纖心直徑值可縮至該近單模態纖心直徑值,減少光在晶纖裡傳輸的模態數,使得光的能量輸出分佈接近單模光纖,因此,本發明具有模態傳輸損耗(Transmission Loss)降低之功效。Secondly, since the core diameter value of the near-monomorphic chromium-doped double-fiber crystal fiber can be reduced to the near-unimodal core diameter value, the number of modes of light transmitted in the crystal fiber is reduced, so that the energy output of the light is made. The distribution is close to a single mode fiber, and therefore, the present invention has the effect of reducing modal transmission loss (Transmission Loss).

其三:由於近單模態摻鉻雙纖衣晶纖之纖心直徑值可縮至該近單模態纖心直徑值,因此,針對摻鉻晶纖而言,本發明不僅可以將通訊波段維持於1.3至1.6微米,且具有提升自發輻射放大光源的轉換效率(Transform Efficiency)之功效。Thirdly, since the core diameter value of the near-monomorphic chromium-doped double-fiber crystal fiber can be reduced to the near-unimodal core diameter value, the present invention can not only communicate the communication band for the chromium-doped crystal fiber. It is maintained at 1.3 to 1.6 microns and has the effect of improving the conversion efficiency of the spontaneous emission amplification source.

其四:由於該纖心直徑值可縮至該近單模態纖心直徑值且纖心直徑均勻,使得纖心截面積不同所造成的插入損耗(Insertion Loss)降低,因此,本發明具有插入損耗降低之功效。Fourthly, since the core diameter value can be reduced to the near-monomodal core diameter value and the core diameter is uniform, the insertion loss (Insertion Loss) caused by the different core cross-sectional areas is reduced, and therefore, the present invention has an insertion The effect of reduced loss.

其五:僅需藉由重複進行該擴散互融過程,並將雷射功率值逐次降低,即可提高雙纖衣晶纖之增益並維持超寬頻特性,因此,本發明具有容易實行及成本低廉之功效。Fifth, by repeating the diffusion and integration process and decreasing the laser power value successively, the gain of the double-fiber crystal fiber can be improved and the ultra-wideband characteristic can be maintained. Therefore, the invention is easy to implement and low in cost. The effect.

綜上所述,本發明所揭示之製造方法或加工方法可以解決長期以來無法將該纖心直徑值縮至該近單模態纖心直徑值的問題,進一步將近單模態摻鉻雙纖衣晶纖開發為高效率、低傳輸損耗及全光網域之自發輻射放大光源、光纖雷射或超寬頻放大器。In summary, the manufacturing method or the processing method disclosed by the present invention can solve the problem that the core diameter value cannot be reduced to the near-unimodal core diameter value for a long time, and the near-monomorphic chromium-doped double-fiber garment is further reduced. Crystal fiber is developed as a high-efficiency, low transmission loss and self-generated radiation amplification source for all-optical domains, fiber laser or ultra-wideband amplifier.

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。While the invention has been described in connection with the preferred embodiments described above, it is not intended to limit the scope of the invention. The technical scope of the invention is protected, and therefore the scope of the invention is defined by the scope of the appended claims.

[本發明][this invention]

1...雙纖衣晶纖1. . . Double fiber clothing crystal fiber

11...晶體光纖11. . . Crystal fiber

12...玻璃毛細管12. . . Glass capillary

2...近單模態雙纖衣晶纖2. . . Near-unimodal double-fiber crystal fiber

A...晶纖製造裝置A. . . Crystal fiber manufacturing device

R...雷射R. . . Laser

T...管狀晶體T. . . Tubular crystal

P1...第一功率曲線P1. . . First power curve

P2...第二功率曲線P2. . . Second power curve

P3...第三功率曲線P3. . . Third power curve

S1...晶纖製備程序S1. . . Crystal fiber preparation program

S2...纖心調整程序S2. . . Core adjustment program

S21...調整步驟S21. . . Adjustment steps

S22...判斷步驟S22. . . Judgment step

[習知][知知]

9...雙纖衣晶纖9. . . Double fiber clothing crystal fiber

91...晶體光纖91. . . Crystal fiber

92...玻璃毛細管92. . . Glass capillary

93...管狀晶體93. . . Tubular crystal

R...雷射R. . . Laser

第1圖:習知雙纖衣晶纖製造方法之示意圖。Figure 1: Schematic diagram of a conventional method for producing a double-fiber crystal fiber.

第2圖:習知雙纖衣晶纖製造方法之纖心直徑變化曲線圖。Fig. 2 is a graph showing the core diameter change of the conventional method for manufacturing a double fiber clothing crystal fiber.

第3圖:本發明之近單模態雙纖衣晶纖之製造方法較佳實施例之系統示意圖。Fig. 3 is a schematic view showing the system of the preferred embodiment of the method for producing a near-simultane double-fiber crystal fiber of the present invention.

第4圖:本發明之近單模態雙纖衣晶纖之製造方法較佳實施例之流程圖。Fig. 4 is a flow chart showing a preferred embodiment of the method for producing a near-simular dual-fiber crystal fiber of the present invention.

第5圖:本發明之近單模態雙纖衣晶纖之製造方法較佳實施例之功率曲線圖。Fig. 5 is a graph showing the power curve of a preferred embodiment of the method for producing a near-simultane double-fiber crystal fiber of the present invention.

S1...晶纖製備程序S1. . . Crystal fiber preparation program

S2...纖心調整程序S2. . . Core adjustment program

S21...調整步驟S21. . . Adjustment steps

S22...判斷步驟S22. . . Judgment step

Claims (14)

一種近單模態雙纖衣晶纖之製造方法,係包含:一晶纖製備程序,係進行一擴散互融過程一次而製備一雙纖衣晶纖;及一纖心調整程序,係將該雙纖衣晶纖重新進行該擴散互融過程至少一次,直到該雙纖衣晶纖之纖心直徑值縮至一近單模態纖心直徑值,而形成一近單模態雙纖衣晶纖;其中,各該擴散互融過程之雷射功率值逐次降低。A method for manufacturing a near-single-mode double-fiber crystal fiber comprises: a crystal fiber preparation process for performing a diffusion and mutual fusion process to prepare a double-fiber crystal fiber; and a core adjustment program The double-fiber crystal fiber re-does the diffusion and fusion process at least once until the core diameter value of the double-fiber crystal fiber is reduced to a near-unimodal core diameter value to form a near-monomodal double-fiber crystal Fiber; wherein the laser power value of each of the diffusion and mutual fusion processes is successively decreased. 依申請專利範圍第1項所述之近單模態雙纖衣晶纖之製造方法,其中該纖心調整程序進行該擴散互融過程之雷射功率值低於該晶纖製備程序進行該擴散互融過程之雷射功率值。According to the manufacturing method of the near-single-mode double-fiber crystal fiber according to the first aspect of the patent application, wherein the laser power adjustment process performs the diffusion power conversion process, and the laser power value is lower than the crystal fiber preparation program for the diffusion. The laser power value of the integration process. 依申請專利範圍第1項所述之近單模態雙纖衣晶纖之製造方法,其中該纖心調整程序之擴散互融過程重新進行的次數若為數次,則各該擴散互融過程之雷射功率值逐次降低。According to the manufacturing method of the near-single-mode double-fiber crystal fiber according to the first aspect of the patent application, wherein the diffusion and integration process of the core adjustment program is repeated several times, the diffusion and integration process is performed. The laser power value is successively reduced. 依申請專利範圍第1項所述之近單模態雙纖衣晶纖之製造方法,其中該晶纖製備程序係由一雷射照射於一管狀晶體而產生熱輻射,使一晶體光纖及一玻璃毛細管開始進行該擴散互融過程,待該擴散互融過程結束後形成該雙纖衣晶纖。The method for manufacturing a near-unimodal double-fiber crystal fiber according to claim 1, wherein the crystal fiber preparation process is irradiated by a laser to a tubular crystal to generate heat radiation, and a crystal fiber and a crystal fiber are used. The glass capillary begins the diffusion and mutual fusion process, and the double-fiber crystal fiber is formed after the diffusion and mutual fusion process is completed. 依申請專利範圍第1項所述之近單模態雙纖衣晶纖之製造方法,其中該纖心調整程序係包含:一調整步驟,係由該雙纖衣晶纖再次開始進行該擴散互融過程,使該雙纖衣晶纖之纖心直徑縮小,其中,該調整步驟之擴散互融過程的雷射功率值低於上一次進行該擴散互融過程之雷射功率值;及一判斷步驟,係判斷該雙纖衣晶纖之纖心直徑值是否縮至該近單模態纖心直徑值,若判斷為是,則結束進行該擴散互融過程,以形成該近單模態雙纖衣晶纖,若判斷為否,則待結束進行該擴散互融過程後,再進行該調整步驟。The method for manufacturing a near-unimodal double-fiber crystal fiber according to claim 1, wherein the core adjustment program comprises: an adjusting step of restarting the diffusion from the double-fiber crystal fiber again The melting process reduces the core diameter of the double-fiber crystal fiber, wherein the laser power value of the diffusion and fusion process of the adjusting step is lower than the laser power value of the previous diffusion and integration process; and a judgment a step of determining whether the core diameter value of the double-fiber crystal fiber is reduced to the near-unimodal core diameter value, and if the determination is yes, ending the diffusion and mutual fusion process to form the near-simple mode double If the fiber-optic crystal fiber is judged to be no, the adjustment step is performed after the diffusion and mutual fusion process is completed. 依申請專利範圍第1項所述之近單模態雙纖衣晶纖之製造方法,其中該雙纖衣晶纖之纖心材料為釔鋁石榴石晶體。The method for manufacturing a near-monomodal double-fiber crystal fiber according to the first aspect of the patent application, wherein the core material of the double-fiber crystal fiber is a yttrium aluminum garnet crystal. 依申請專利範圍第1、2、3、4、5或6項所述之近單模態雙纖衣晶纖之製造方法,其中該雷射功率值之變動量維持於±0.1%。The method for manufacturing a near-unimodal double-fiber crystal fiber according to the first, second, third, fourth, fifth or sixth aspect of the patent application, wherein the variation of the laser power value is maintained at ±0.1%. 依申請專利範圍第1、2、3、4、5或6項所述之近單模態雙纖衣晶纖之製造方法,其中該判斷步驟係由即時影像監測技術觀測該雙纖衣晶纖之即時影像,供一使用者或一製造程式監測該雙纖衣晶纖之纖心直徑值,以判斷是否再進行該調整步驟。According to the manufacturing method of the near-single-mode double-fiber crystal fiber according to the first, second, third, fourth, fifth or sixth aspect of the patent application, wherein the judging step is to observe the double-fiber crystal fiber by the instant image monitoring technology. The instant image is for a user or a manufacturing program to monitor the core diameter value of the fiberglass fiber to determine whether to perform the adjustment step. 一種雙纖衣晶纖之加工方法,係包含:一調整步驟,係由一雙纖衣晶纖開始進行一擴散互融過程,使該雙纖衣晶纖之纖心直徑縮小,其中,該調整步驟之雷射功率值低於該雙纖衣晶纖製造時之擴散互融過程的雷射功率值,且該調整步驟若非第一次進行,則該擴散互融過程之雷射功率值低於上一次進行該擴散互融過程之雷射功率值;及一判斷步驟,係判斷該雙纖衣晶纖之纖心直徑值是否縮至一預定直徑值,若判斷為是,則結束進行該擴散互融過程,以形成一近單模態雙纖衣晶纖,若判斷為否,則待結束進行該擴散互融過程後,再進行該調整步驟。A method for processing a double-fiber crystal fiber comprises: an adjusting step of performing a diffusion and mutual fusion process by a pair of fiber-optic crystal fibers, thereby reducing a core diameter of the fiber-optic fiber, wherein the adjusting The laser power value of the step is lower than the laser power value of the diffusion and fusion process during the manufacturing of the double fiber crystal fiber, and if the adjustment step is not performed for the first time, the laser power value of the diffusion and integration process is lower than a laser power value of the last diffusion process; and a determining step of determining whether the core diameter value of the fiberglass fiber is reduced to a predetermined diameter value, and if the determination is yes, ending the diffusion The mutual fusion process is performed to form a near-monomodal double-fiber crystal fiber. If the determination is negative, the adjustment step is performed after the diffusion and mutual integration process is completed. 依申請專利範圍第9項所述之雙纖衣晶纖之加工方法,其中該預定直徑值等於一近單模態纖心直徑值。The method for processing a double-fiber crystal fiber according to claim 9, wherein the predetermined diameter value is equal to a near-monomodal core diameter value. 依申請專利範圍第9項所述之雙纖衣晶纖之加工方法,其中該預定直徑值大於一近單模態纖心直徑值。The method for processing a double-fiber crystal fiber according to claim 9, wherein the predetermined diameter value is greater than a near-monomodal core diameter value. 依申請專利範圍第9項所述之雙纖衣晶纖之加工方法,其中該雙纖衣晶纖之纖心材料為釔鋁石榴石晶體。According to the processing method of the double-fiber crystal fiber according to claim 9, wherein the core material of the double-fiber crystal fiber is yttrium aluminum garnet crystal. 依申請專利範圍第9、10、11或12項所述之雙纖衣晶纖之加工方法,其中該雷射功率值之變動量維持於±0.1%。The method for processing a double-fiber crystal fiber according to claim 9, 10, 11 or 12, wherein the variation of the laser power value is maintained at ±0.1%. 依申請專利範圍第9、10、11或12項所述之雙纖衣晶纖之加工方法,其中該判斷步驟係由即時影像監測技術觀測該雙纖衣晶纖之即時影像,供一使用者或一製造程式監測該雙纖衣晶纖之纖心直徑值,以判斷是否於結束進行該擴散互融過程後,再次進行該調整步驟。According to the processing method of the double-fiber crystal fiber according to claim 9, 10, 11 or 12, wherein the judging step is to observe an instant image of the double-fiber crystal fiber by a real-time image monitoring technology for a user. Or a manufacturing program monitors the core diameter value of the double-fiber crystal fiber to determine whether the adjustment step is performed again after the diffusion and mutual integration process is finished.
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