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Laser amplification optical fiber for preventing self-convergence damage

A laser amplification and self-focusing technology, which is applied in cladding optical fiber, optical waveguide and light guide, etc., can solve the problems of pulse peak power and energy gap, optical damage of materials, and light intensity at the focal point, etc., and achieve single pulse energy increase and increase The effect of single fiber power amplification limit capability

Active Publication Date: 2011-10-05
TSINGHUA UNIV
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  • Summary
  • Abstract
  • Description
  • Claims
  • Application Information

AI Technical Summary

Problems solved by technology

Since the fundamental mode light field distribution (approximately Gaussian distribution) is usually used in practical applications, in materials with a positive nonlinear refractive index coefficient, the refraction index experienced by the region with strong central light intensity is relatively large, and the refraction experienced by the surrounding areas with low light intensity When the convergence effect exceeds the diffraction effect of the beam, self-focusing occurs, resulting in a large light intensity at the focal point, which induces photodamage of the material
For fused silica material, for 1 micron laser wavelength, the self-focusing threshold obtained by its typical nonlinear refractive index coefficient is about 4.3MW. In the fiber waveguide structure, although the refractive index guide will have a certain impact on the beam transmission, However, both numerical simulation and experimental results show that the self-focusing threshold power of the optical fiber is basically the same as that of the fused silica bulk material, which limits the pulse energy of at most 43mJ within 10ns pulse width in the fiber laser amplifier, compared with the solid-state laser There is still a considerable gap in the pulse peak power and energy that the system can obtain

Method used

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  • Laser amplification optical fiber for preventing self-convergence damage
  • Laser amplification optical fiber for preventing self-convergence damage
  • Laser amplification optical fiber for preventing self-convergence damage

Examples

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Embodiment 1

[0025] figure 1 It is a structural schematic diagram of a laser amplification fiber for preventing self-focusing damage according to an embodiment of the present invention, including a gain fiber 1 and a section of hollow-core fiber 2, the input end of the hollow-core fiber 2 is welded to the output end of the gain fiber 1 The gain fiber 1 is a fused silica matrix gain fiber.

[0026] The laser amplification fiber structure for preventing self-focusing damage in this embodiment includes two parts: the first part is a fused silica matrix gain fiber. This part amplifies the input pulse to a level where the peak power exceeds its self-focusing threshold power, thereby inducing the self-focusing process, resulting in a contraction of the beam aperture, which is not long enough for self-focusing damage to occur.

[0027] The second part is the hollow core fiber 2 . This part uses the hollow-core fiber 2 to connect with the gain fiber 1 in the previous section. After the contracte...

Embodiment 2

[0029] figure 1 It is a structural schematic diagram of a self-focusing damage-proof laser amplification fiber according to an embodiment of the present invention, including a gain fiber 1 and a section of hollow-core fiber 2, and the two ends of each section of hollow-core fiber 2 are connected to the gain fiber 1, so The aforementioned gain fiber 1 is a fused silica matrix gain fiber.

[0030] The self-focusing damage-proof laser amplification fiber of this embodiment includes three parts: the first part is a fused silica matrix gain fiber. This part amplifies the input pulse to a level where the peak power exceeds its self-focusing threshold power, thereby inducing the self-focusing process, resulting in a contraction of the beam aperture, which is not long enough for self-focusing damage to occur.

[0031] The second part is the hollow core fiber 2 . This part uses the hollow-core fiber 2 to connect with the gain fiber 1 in the previous section. After the contracted beam...

Embodiment 3

[0034] figure 2 It is a structural schematic diagram of a laser amplification fiber for preventing self-focusing damage according to another embodiment of the present invention, including: a gain fiber 1 and two sections of hollow-core fiber 2, and both ends of each section of hollow-core fiber 2 are connected to the gain fiber , with the direction of laser transmission, the length of the gain fiber is shorter as it goes to the rear, and the gain fiber is a fused silica matrix gain fiber.

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Abstract

The invention relates to the technical field of optical fiber laser transmission, and in particular relates to a laser amplification optical fiber for preventing self-convergence damage, which comprises a hollow optical fiber and a gain optical fiber, wherein the rear end of the gain optical fiber is connected with the hollow optical fiber along the laser transmission direction. The gain optical fiber is connected with the hollow optical fiber so as to prevent optical fiber damage caused by optical field convergence due to a self-convergence effect generated during the process of transmitting, amplifying and oscillating the gain optical fiber, so that single fiber power amplification limit performance of the gain optical fiber is improved, and the obtained pulse energy is greatly improved.

Description

technical field [0001] The invention relates to the technical field of optical fiber laser transmission amplification, in particular to a laser amplifying optical fiber that prevents self-focusing damage. Background technique [0002] In the rare earth doped laser gain fiber medium, when the laser intensity exceeds a certain level, the Kerr effect in the medium will be induced, that is, the refractive index of the medium is linearly related to the light intensity, and the linear proportional coefficient is represented by the nonlinear refractive index coefficient . Since the fundamental mode light field distribution (approximately Gaussian distribution) is usually used in practical applications, in materials with a positive nonlinear refractive index coefficient, the refraction index experienced by the region with strong central light intensity is relatively large, and the refraction experienced by the surrounding areas with low light intensity When the convergence effect e...

Claims

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Application Information

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Patent Type & Authority Applications(China)
IPC IPC(8): G02B6/02
Inventor 张海涛巩马理黄志华阎平柳强黄磊
Owner TSINGHUA UNIV
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