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CN112666649A - Solid core anti-resonance optical fiber for realizing medium infrared band cut-off-free single mode transmission - Google Patents

Solid core anti-resonance optical fiber for realizing medium infrared band cut-off-free single mode transmission Download PDF

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CN112666649A
CN112666649A CN202011464239.6A CN202011464239A CN112666649A CN 112666649 A CN112666649 A CN 112666649A CN 202011464239 A CN202011464239 A CN 202011464239A CN 112666649 A CN112666649 A CN 112666649A
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core
solid
fiber
optical fiber
tubular
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史伟
张帅
孙帅
盛泉
姚建铨
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Tianjin University
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Tianjin University
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Abstract

本发明提供一种实现中红外波段无截止单模传输的实芯反谐振光纤,其特征在于,包括实芯纤芯,包覆在实芯纤芯外部的管状外包层,在实芯纤芯内分布有六个外部包覆有管状内包层的圆形实芯小管,各个圆形实芯小管相互之间无接触、均匀地环绕分布在实芯纤芯中,形成无节点式结构;实芯纤芯和各个圆形实芯小管采用折射率较低的材料制作而成,管状外包层和管状内包层采用折射率较高的材料制作而成,从而形成完全实芯的光纤结构。

Figure 202011464239

The invention provides a solid-core anti-resonant fiber for realizing single-mode transmission without cut-off in the mid-infrared band, which is characterized in that it comprises a solid-core fiber core, a tubular outer cladding covering the outside of the solid-core fiber core, and a tubular outer cladding covering the outside of the solid-core fiber core. There are six circular solid core tubules covered with a tubular inner cladding, and each circular solid core tubule is evenly distributed in the solid core fiber core without contact with each other, forming a nodeless structure; the solid core fiber The core and each round solid core tube are made of materials with lower refractive index, and the outer tubular cladding and inner tubular cladding are made of materials with higher refractive index, thereby forming a completely solid fiber structure.

Figure 202011464239

Description

Solid core anti-resonance optical fiber for realizing medium infrared band cut-off-free single mode transmission
Technical Field
The invention relates to a single-mode solid-core optical fiber based on an anti-resonance characteristic, belonging to the field of special optical fiber design and simultaneously belonging to the field of mid-infrared laser transmission design.
Background
The common solid-core silica fiber is used as a traditional medium for transmitting light waves, and has a great number of intrinsic defects in practical application, such as nonlinear effect, dispersion effect, photo-induced damage effect, ultraviolet and mid-infrared band light-blocking effect and the like. These intrinsic physical problems are difficult to solve effectively in the framework of conventional optical fibers, and thus become fundamental obstacles that greatly restrict the forward development of optical fiber transmission technology. Therefore, it is necessary to design a new optical fiber with excellent transmission performance and stable material and structural properties.
The first generation of hollow core optical fibers based on the photonic band gap effect made great progress both experimentally and theoretically in the early 21 st century. But the structure of the optical fiber is complex, and the transmission loss of the transmission optical fiber can not break through the limit of the surface scattering loss, so that the transmission bandwidth is narrow, and the laser damage threshold is not high enough. With the development of the hollow-core anti-resonant fiber, many researchers optimize and design the hollow-core anti-resonant fiber with wide transmission bandwidth and low transmission loss. However, the design and drawing process of the hollow-core optical fiber structure are complicated, and the hollow-core structure is easy to collapse and has no good structural stability, so that the real large-scale batch production is difficult to realize.
Therefore, based on the design concept of the anti-resonance optical fiber, the invention provides the solid anti-resonance optical fiber with good non-cutoff single-mode transmission characteristic, which can be used for excellent single-mode transmission of middle-infrared band laser, provides a new method and thought for the design of a large-core-diameter single-mode active optical fiber and the research of the nonlinear characteristics of the large-core-diameter single-mode active optical fiber, and also expands the design field of the anti-resonance optical fiber and promotes the further development of the solid optical fiber in the laser transmission field.
Disclosure of Invention
The invention aims to provide a design method of a solid anti-resonance optical fiber, which realizes the non-cutoff single-mode transmission of mid-infrared band laser by filling materials with different refractive indexes and controlling the size of structural parameters of the optical fiber. The technical scheme of the invention is as follows:
a solid core anti-resonance optical fiber for realizing medium infrared band cut-off-free single mode transmission is characterized by comprising a solid core fiber core and a tubular outer cladding layer covering the outside of the solid core fiber core, wherein six round solid core small tubes with tubular inner cladding layers covering the outside are distributed in the solid core fiber core, and the round solid core small tubes are uniformly distributed in the solid core fiber core in a surrounding way without contact with each other to form a node-free structure; the solid core fiber core and each round solid small tube are made of materials with lower refractive indexes, and the tubular outer cladding layer and the tubular inner cladding layer are made of materials with higher refractive indexes, so that a completely solid optical fiber structure is formed.
Furthermore, the round solid small tubes are uniformly distributed in the solid fiber core in a surrounding way.
Further, according to the wavelength of the mid-infrared band to be transmitted and the refractive index of the two selected materials, the length L of the anti-resonance period is determined, and the thickness of the tubular inner cladding is determined through optimized design.
Further, the refractive index of the solid core and the round solid small tube is n22.4158; the refractive index of the tubular outer cladding and the tubular inner cladding is n12.8034, the thickness of the tubular inner cladding is 0.52 μm.
Further, the central diameter of the solid core of the solid core anti-resonance optical fiber is 20 μm, and the minimum gap between the tubular inner cladding and the tubular outer cladding of the solid core anti-resonance optical fiber is 2 μm. The thickness of the tubular outer cladding is 5 μm. The diameter of the round solid small tube is 13.6 mu m.
The solid anti-resonance optical fiber is characterized in that when laser is transmitted in the structure, the laser and the tubular inner cladding generate anti-resonance action, so that a laser field is limited in the solid fiber core and transmitted in a single-mode, and the solid anti-resonance optical fiber has excellent laser single-mode transmission characteristics; compared with a hollow fiber, the solid anti-resonance fiber is very stable in overall structure and not easy to collapse, and the structure can be easily processed and manufactured by drilling and filling materials on a common solid fiber base material, so that large-scale batch production can be performed by industrialized drawing, the market prospect is good, the function realization mode is simple, and a good technical conversion foundation is achieved.
Drawings
FIG. 1 is a schematic structural diagram of a solid core antiresonant optical fiber for implementing cut-off-free single mode transmission according to the present invention;
FIG. 2 is a schematic diagram illustrating the variation of the antiresonance period of the solid antiresonant fiber in the embodiment of FIG. 1;
FIG. 3 shows the fundamental mode HE of the embodiment of FIG. 1 when the optical fiber structure has different diameter d of the round solid-core small tube 311And higher order mode TE01Schematic diagram of the variation of the transmission loss of (1);
FIG. 4 shows a fundamental mode HE of the optical fiber structure of the embodiment of FIG. 1 when transmitting laser beams with different wavelengths11And higher order mode TE01Schematic diagram of the transmission loss variation.
Fig. 5 is a schematic diagram of field intensity distribution when the optical fiber structure in the embodiment of fig. 1 realizes very good single-mode transmission.
Reference numerals: 1-solid core, 2-tubular outer cladding, 3-round solid core small tube, 4-tubular inner cladding
Detailed Description
The invention is described in further detail below with reference to the figures and specific examples. It should be understood that the specific embodiments described herein are merely illustrative of the invention and are not intended to limit the invention.
Fig. 1 is a schematic structural diagram of a solid core antiresonant optical fiber for implementing non-cutoff single-mode transmission according to the embodiment of the present invention. The fiber core structure comprises a tubular outer cladding layer 2, a solid fiber core 1, six round solid small tubes 3 embedded in the solid fiber core 1 and a tubular inner cladding layer 4 wrapping the round solid small tubes 3, wherein the six round solid small tubes 3 are uniformly distributed in the solid fiber core 1 in a surrounding mode without contact, and a node-free structure is formed. Laser with the wavelength of lambda being 3 mu m is led into the structural optical fiber, and the non-cutoff single-mode transmission characteristic of the designed optical fiber structure in the middle infrared band is proved by a software simulation mode.
Wherein the solid core 1 and the round solid small tube 3 are made of material As with lower refractive index2S3Filling with a refractive index n22.4158; the tubular outer cladding 2 and the tubular inner cladding 4 are made of a material As having a high refractive index2Se3Filling with a refractive index n12.8034, thereby forming an optical fiber structure that is entirely filled with solid core material.
As shown in FIG. 1, the solid core 1 has a large central diameterSmall DcoreSet to 20 μm; the distance G between the tubular inner cladding 4 and the tubular outer cladding 2 is set to be 2 μm; thickness T of the tubular envelope 2exSet to 5 μm. The anti-resonance period length L of the solid core anti-resonance fiber structure can be obtained as 1.055 μm according to the formula (1):
Figure BDA0002832472470000031
whereby the thickness T of the tubular inner cladding 4 is set to
Figure BDA0002832472470000032
The transmission loss of the laser light in this fiber is at a minimum.
FIG. 2 is a schematic diagram of an antiresonance period of a solid antiresonant fiber obtained by simulation in the example. It can be found that the solid core antiresonant fiber designed by the invention has obvious antiresonant characteristic, the antiresonant period L is 1.05546 μm, the first antiresonant point is located at 0.5277 μm, and the result is consistent with the theoretical value calculated by the formula (1).
FIG. 3 shows a fundamental mode HE of the solid-core antiresonant optical fiber structure of the embodiment with different diameter d of the circular solid-core small tube 311And higher order mode TE01The respective transmission losses are illustrated schematically. It can be seen that the fiber structure designed by the present invention has very good non-cutoff single-mode transmission characteristics, especially when d is 13.6 μm, the transmission loss of the fundamental mode is about three orders of magnitude lower than that of the high-order mode, and even if the diameter size of the circular solid small tube 3 changes, the transmission loss of the fundamental mode remains substantially unchanged, thereby achieving excellent single-mode transmission.
FIG. 4 is a diagram illustrating a fundamental mode HE of a solid-core anti-resonant fiber structure in an embodiment when transmitting laser beams with different wavelengths11And higher order mode TE01Schematic diagram of the variation of the transmission loss of (1). As can be seen, in the intermediate infrared band of 2.5-3.5 μm, the solid core anti-resonance optical fiber with the structure has better transmission characteristics, the transmission loss of the fundamental mode is about two orders of magnitude lower than that of the high-order mode, and therefore, the solid core anti-resonance optical fiber can be used for transmitting laser in the intermediate infrared band in a good single-modeAnd (6) inputting.
Fig. 5 is a schematic diagram of field intensity distribution when the solid core antiresonant fiber structure in the embodiment realizes excellent single-mode transmission. Under the influence of the anti-resonance characteristic, the solid core optical fiber structure designed by the invention well limits laser inside the optical fiber core, and realizes excellent single-mode transmission.
The present invention is not limited to the above-described embodiments. The foregoing description of the specific embodiments is intended to describe and illustrate the technical solutions of the present invention, and the above specific embodiments are merely illustrative and not restrictive. Those skilled in the art, having the benefit of this disclosure, may effect numerous modifications thereto and changes may be made without departing from the scope of the invention as defined by the claims and their equivalents.

Claims (7)

1.一种实现中红外波段无截止单模传输的实芯反谐振光纤,其特征在于,包括实芯纤芯,包覆在实芯纤芯外部的管状外包层,在实芯纤芯内分布有六个外部包覆有管状内包层的圆形实芯小管,各个圆形实芯小管相互之间无接触、均匀地环绕分布在实芯纤芯中,形成无节点式结构;实芯纤芯和各个圆形实芯小管采用折射率较低的材料制作而成,管状外包层和管状内包层采用折射率较高的材料制作而成,从而形成完全实芯的光纤结构。1. a solid-core anti-resonant optical fiber that realizes mid-infrared band without cut-off single-mode transmission, is characterized in that, comprises a solid-core fiber core, and is wrapped in a tubular outer cladding outside the solid-core fiber core, distributed in the solid-core fiber core There are six circular solid-core tubules covered with a tubular inner cladding, and each circular solid-core tubule is evenly distributed in the solid-core fiber core without contact with each other, forming a node-free structure; the solid-core fiber core And each round solid core tube is made of materials with lower refractive index, and the tubular outer cladding and the tubular inner cladding are made of materials with higher refractive index, thereby forming a completely solid core optical fiber structure. 2.根据权利要求1所述的无截止单模传输的实芯反谐振光纤,其特征在于,各个圆形实芯小管相互之间均匀地环绕分布在实芯纤芯中。2 . The solid-core anti-resonant optical fiber for single-mode transmission without cutoff according to claim 1 , wherein the circular solid-core small tubes are evenly distributed in the solid-core fiber core around each other. 3 . 3.根据权利要求1所述的无截止单模传输的实芯反谐振光纤,其特征在于,根据所要传输的中红外波段波长,所选用的两种材料的折射率大小,确定反谐振周期长度L,经过优化设计,确定管状内包层的厚度。3. The solid-core anti-resonant optical fiber without cut-off single-mode transmission according to claim 1, is characterized in that, according to the mid-infrared wavelength to be transmitted, the size of the refractive index of the selected two materials determines the anti-resonance period length L, The thickness of the tubular inner cladding is determined by the optimized design. 4.根据权利要求1所述的无截止单模传输的实芯反谐振光纤,其特征在于,实芯纤芯和圆形实芯小管折射率为n2=2.4158;管状外包层和管状内包层折射率为n1=2.8034,所述管状内包层的厚度为0.52μm。4 . The solid-core anti-resonant fiber with no cut-off single-mode transmission according to claim 1 , wherein the refractive index of the solid-core fiber core and the circular solid-core small tube is n 2 =2.4158; the tubular outer cladding and the tubular inner cladding The refractive index was n 1 =2.8034, and the thickness of the tubular inner cladding was 0.52 μm. 5.根据权利要求1-4任意一项所述的无截止单模传输的实芯反谐振光纤,其特征在于,所述实芯反谐振光纤的实芯纤芯的中心直径为20μm,所述实芯反谐振光纤的管状内包层与管状外包层之间的最小间隙为2μm。5 . The solid-core anti-resonant fiber for single-mode transmission without cutoff according to any one of claims 1 to 4, wherein the center diameter of the solid core of the solid-core anti-resonant fiber is 20 μm, and the The minimum gap between the inner tubular cladding and outer tubular cladding of solid core anti-resonant fibers is 2 μm. 6.根据权利要求1-5任意一项所述的无截止单模传输的实芯反谐振光纤,所述管状外包层的厚度为5μm。6 . The solid-core anti-resonant fiber for single-mode transmission without cutoff according to any one of claims 1 to 5 , wherein the thickness of the tubular outer cladding is 5 μm. 7 . 7.根据权利要求1-6任意一项所述的无截止单模传输的实芯反谐振光纤,所述圆形实芯小管的直径为13.6μm。7 . The solid-core anti-resonant optical fiber for single-mode transmission without cutoff according to any one of claims 1 to 6 , wherein the diameter of the circular solid-core small tube is 13.6 μm. 8 .
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Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN113325509A (en) * 2021-06-04 2021-08-31 浙江师范大学 Optical fiber multi-pass cell based on microstructure optical fiber

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* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN107621670A (en) * 2017-10-13 2018-01-23 北京工业大学 All solid state antiresonant fiber
CN108549128A (en) * 2018-05-15 2018-09-18 复旦大学 Hollow antiresonance photonic crystal optical fiber coupler and its application
CN110208901A (en) * 2019-05-15 2019-09-06 武汉长盈通光电技术有限公司 A kind of hollow antiresonance optical fiber
CN110501777A (en) * 2019-07-28 2019-11-26 复旦大学 A Hollow-Core Anti-Resonance Fiber Polarization Filter

Patent Citations (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN107621670A (en) * 2017-10-13 2018-01-23 北京工业大学 All solid state antiresonant fiber
CN108549128A (en) * 2018-05-15 2018-09-18 复旦大学 Hollow antiresonance photonic crystal optical fiber coupler and its application
CN110208901A (en) * 2019-05-15 2019-09-06 武汉长盈通光电技术有限公司 A kind of hollow antiresonance optical fiber
CN110501777A (en) * 2019-07-28 2019-11-26 复旦大学 A Hollow-Core Anti-Resonance Fiber Polarization Filter

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN113325509A (en) * 2021-06-04 2021-08-31 浙江师范大学 Optical fiber multi-pass cell based on microstructure optical fiber
CN113325509B (en) * 2021-06-04 2022-08-16 浙江师范大学 Optical fiber multi-pass cell based on microstructure optical fiber

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Application publication date: 20210416