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All fiber Q-switch

An all-fiber, switching technology, applied in the field of Q-switching, can solve the problems of Q-switched fiber lasers not working normally, device performance can not be guaranteed, center wavelength drift, etc., to achieve stable and reliable laser output, improve laser output power and efficiency, Effect of stabilizing the center wavelength of the grating

Active Publication Date: 2012-07-04
浙江合波光学科技有限公司
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  • Abstract
  • Description
  • Claims
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AI Technical Summary

Problems solved by technology

[0007] However, there are obvious deficiencies in this technology, which limit its application range
First of all, it is necessary to write long-period fiber gratings on the optical fiber in advance, which requires expensive special writing equipment, and requires the optical fiber to be photosensitive, that is, to be able to write gratings
Secondly, because the phase shift of the phase-shifted long-period fiber grating is different, its transmission spectrum will be very different, so it is necessary to precisely tune the local phase of the long-period fiber grating, otherwise the performance of the device will not be guaranteed
Finally, the central wavelength of the long-period fiber grating is very sensitive to temperature. If no temperature control technology is added, the ambient temperature changes, and the central wavelength of the grating will drift, which will cause the Q-switched fiber laser to fail to work normally.

Method used

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Embodiment

[0076] Figure 3a , Figure 3b It is a schematic diagram of the axial and transverse sections of the all-fiber Q-switch embodiment of the present invention. In this embodiment, the all-fiber Q-switch is composed of long-period grating pressing template 306, V-groove 310, optical fiber, piezoelectric ceramic 305, semiconductor cooling chip 312, thermistor 311, metal shell 304 and other components.

[0077] In this embodiment, the cross section of the V-shaped groove is as attached Figure 4 As shown, there is a V-shaped groove 402 in the center of the upper surface of the V-shaped groove base material 401, which has a cross section like the letter "V". The length of the V-groove is 3 cm, and the depth of the V-groove is 100 μm. The axial section of the long-period grating pressing template is attached Figure 5 As shown, the lower surface of the LPFG pressing template base material 501 has a tooth-like surface feature 502 with a period of 206 microns in the lateral directio...

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Abstract

The invention relates to an all fiber Q-switch, which comprises a fiber, a V-shaped groove, a long-period grating pressed template, piezoelectric ceramics, a semiconductor chilling plate, a thermistor and a metal shell, wherein the fiber passes through the metal shell, and one section of the fiber is a bare fiber; the long-period grating pressed template, the bare fiber and the V-shaped groove are arranged from top to bottom in the metal shell to form a sandwich-like structure; optical cement is coated on the outer surface of the bare fiber; the piezoelectric ceramics is arranged between the inner top of the metal shell and the long-period grating pressed template; the semiconductor chilling plate closely attaches to the outer bottom of the metal shell; and the lateral surface of the V-shaped groove is closely provided with the thermistor for inducing the temperature of the V-shaped groove. The all fiber Q-switch has the characteristic of zero insertion loss. When the all fiber Q-switch is applied to a Q-switched fiber laser, the all fiber Q-switch can improve the output power and efficiency of the laser under the same conditions.

Description

technical field [0001] The invention relates to a Q switch, in particular to an all-fiber Q switch based on a long-period fiber grating. Background technique [0002] In some applications such as industrial laser marking and laser cutting, laser pulses with high peak power are required, which can usually be achieved using Q modulation technology. The basic principle of Q modulation technology is to make the loss (or Q value) in the laser resonator cavity change according to a preset program through a certain method. At the beginning of the pump excitation, the resonator has high loss (low Q value), and the laser cannot generate laser oscillation due to the high threshold, so the number of particles in the metastable state can accumulate to a higher level. Then at the set moment, the loss of the resonant cavity is suddenly reduced to a very low value (high Q value), and the laser threshold is immediately lowered. At this time, the number of inversion particles greatly exceed...

Claims

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Application Information

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Patent Type & Authority Patents(China)
IPC IPC(8): H01S3/115H01S3/067
Inventor 周金龙李传文赵浩
Owner 浙江合波光学科技有限公司
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