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Cascaded pumping module and laser of a kind of resonant cavity

A cascaded pump and resonant cavity technology, applied in the field of optoelectronics, can solve the problems of no way for pump light to enter the optical fiber, poor beam quality, low brightness, etc., to achieve the improvement of light-to-light conversion efficiency, increase output power, and increase brightness Effect

Active Publication Date: 2019-03-05
HUAZHONG UNIV OF SCI & TECH
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  • Summary
  • Abstract
  • Description
  • Claims
  • Application Information

AI Technical Summary

Problems solved by technology

[0005] (1) After the pump light passes through the optical fiber, the spherical reflector is reflected and returns to the optical fiber again; when the pump light emerges from the optical fiber, it is in a ring shape, and some light will be missed through the spherical reflector, causing loss;
[0006] (2) The pump source uses semiconductor pumping, the beam quality is very poor, the brightness is very low, there is no way to let more pump light enter the fiber, so that its output power has an upper limit

Method used

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  • Cascaded pumping module and laser of a kind of resonant cavity
  • Cascaded pumping module and laser of a kind of resonant cavity
  • Cascaded pumping module and laser of a kind of resonant cavity

Examples

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Embodiment 1

[0035] figure 2 It is a schematic diagram of a pumping device coupled with a disk and a spherical lens group involved in a cascaded pumping module of a resonant cavity according to an embodiment of the present invention. Such as figure 1 As shown, the optical device includes a disc 1 , a reflector 2 , a second dichroic mirror 6 , a focusing mirror 7 , a gain fiber 5 and a reflector 8 .

[0036] The material of disc 1 is Yb:YAG crystal, which has a diameter of 15mm and a thickness of 200um. The back of the disc is coated with a high-reflection film. Mirror 2 is a 1030nm high-reflection mirror with a reflectivity of 99.9% and a radius of curvature of 2m; the dichroic mirror 6 is a 1030nm high-reflection and 1080nm high-transmission plane mirror with a reflectivity of 99.9% and a transmittance of 99.9%; the focusing mirror 7 has a diameter of 15mm , a focusing lens with an effective focal length of 17mm; the gain fiber 5 is a Yb-doped double-clad silica fiber, the core diamete...

Embodiment 2

[0047] image 3 It is a schematic diagram of a pumping device coupled with two disks and a spherical lens group involved in a cascaded pumping module of a resonant cavity according to an embodiment of the present invention. Such as image 3 As shown, the pump module includes 2 discs 1 , 2 mirrors 2 , a first dichroic mirror 3 and a first dichroic mirror 6 , two focusing mirrors 7 , a gain fiber 5 , and a mirror 8 .

[0048] Among them, the material of disc 1 is Yb:YAG crystal with a diameter of 15mm and a thickness of 200um. The back of the disc is coated with a high-reflection film. The corresponding wavelengths of the film system are 940nm and 1030nm, and the reflectivity is 99.9% and 99.9% respectively. Reflector 2 is a 1030nm high-reflection mirror with a reflectivity of 99.9% and a radius of curvature of 2m; the dichroic mirror 6 is a 1030nm high-reflection and 1080nm high-transmission flat mirror with a reflectivity of 99.9% and a transmittance of 99.9%; focusing mirror...

Embodiment 3

[0053] Figure 4 It is a schematic diagram of a pumping device coupled with a disc and a parabolic mirror involved in a cascaded pumping module of a resonant cavity according to an embodiment of the present invention. Such as Figure 4 As shown, the pump module includes a disc 1 , a reflector 2 , a first dichroic mirror 3 , a parabolic reflector 4 , a gain fiber 5 , and a reflector 8 .

[0054] Among them, the material of disc 1 is Yb:YAG crystal with a diameter of 15mm and a thickness of 200um. The back of the disc is coated with a high-reflection film. The corresponding wavelengths of the film system are 940nm and 1030nm, and the reflectivity is 99.9% and 99.9% respectively. Reflector 2 is a 1030nm high reflection mirror with a reflectivity of 99.9% and a radius of curvature of 2m; the dichroic mirror 3 is a plane mirror with 1030nm high transparency and 1080nm high reflection, with a transmittance of 99.9% and a reflectivity of 99.9%; The focal length of the mirror is 50m...

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Abstract

The invention discloses a resonant cavity shared cascading pump module and a laser. The pump module comprises a disc laser, a beam splitting system, a coupling system (7), a gain material and a reflection system (8) which are arranged in sequence along a direction of a light path. The disc laser comprises a pump light source, a cavity mirror (2) and an active gain mirror (1). The pump light source is used for pumping the active gain mirror (1), thereby generating laser. The laser is reflected by the beam splitting system, is coupled into the gain material through focusing of the coupling system and is reflected by the reflection system (8). The laser is returned according to the original light path. The beam splitting system is used for transmitting required laser and reflecting undesired laser. The invention also discloses the laser with the pump module. According to the resonant cavity shared cascading pump module, the laser generated in the cavity of the disc laser passes through a gain optical fiber repeatedly, so the pump light absorbed by the optical fiber is increased, and the light conversion efficiency is greatly improved.

Description

technical field [0001] The invention belongs to the technical field of optoelectronics, and more specifically relates to a cascaded pumping module of a resonant cavity and a laser. Background technique [0002] Same-band pumping, also known as resonant pumping, is a pumping method that can greatly increase the pumping power, reduce the quantum deficit of the laser system, and reduce the thermal effect. At present, the 10kw fundamental mode fiber laser produced by IPG adopts the same-band pumping scheme. [0003] The biggest problem of the existing in-band pumping scheme is that the pump wavelength is not on the absorption peak of the gain material, resulting in a very low absorption coefficient of the gain material for the pump light. For fiber lasers, the current solutions to this problem are: (1) increase the doping concentration; (2) increase the core area; (3) reduce the inner cladding area. But the ensuing problem is that increasing the doping concentration will easil...

Claims

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Application Information

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Patent Type & Authority Patents(China)
IPC IPC(8): H01S3/067H01S3/08H01S3/081H01S3/101
CPCH01S3/067H01S3/08059H01S3/0816H01S3/101
Inventor 朱广志陈永骞朱晓王海林齐丽君赵文广曹登
Owner HUAZHONG UNIV OF SCI & TECH
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