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Raman laser based on crystalline in fresnoite structure

A technology of Raman laser and titanite, applied in the field of Raman lasers

Active Publication Date: 2013-02-27
SHANDONG UNIV
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  • Summary
  • Abstract
  • Description
  • Claims
  • Application Information

AI Technical Summary

Problems solved by technology

[0004] Aiming at the problems existing in the existing Raman lasers, the present invention provides a laser based on a barite structure Raman crystal and its working method

Method used

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  • Raman laser based on crystalline in fresnoite structure
  • Raman laser based on crystalline in fresnoite structure
  • Raman laser based on crystalline in fresnoite structure

Examples

Experimental program
Comparison scheme
Effect test

Embodiment 1

[0055] Example 1: Ba 2 TiSi 2 O 8 Single pass Raman laser outside the cavity of Raman crystal.

[0056] Structure like figure 1 As shown, the laser is composed of a pulsed laser 1 and a Raman crystal 2. The pulsed laser 1 is a picosecond pulsed laser pumped by a flash lamp and dual-modulated with an acousto-optic modulator and dye saturable absorption material. Its output wavelength is 532nm, pulse width 30ps, and repetition frequency is 10Hz pulsed laser; 2 TiSi 2 O 8 Raman crystals generate stimulated Raman light. Figure 8 This is the output Raman laser spectrogram of the laser. It is obvious from the figure that the output of the first-level Raman laser at 558nm and the second-level Raman laser at 587nm can be seen.

[0057] The Raman crystal 2 is Ba 2 TiSi 2 O 8 Crystal, its size is 5×5×25mm 3 , The clear surface is 5×5mm 2 , Its double-sided polishing is not coated.

[0058] Ba 2 TiSi 2 O 8 Crystal preparation method:

[0059] Reaction equation: 2BaCO 3 +TiO 2 +2SiO 2 =Ba 2 Ti...

Embodiment 2

[0061] Example 2: Ca 2 TiSi 2 O 8 Crystal double-pass Raman laser outside the cavity.

[0062] Structure like figure 2 As shown, the laser consists of a pulsed laser 1, an input mirror 3, a Raman crystal 2 and a concave output mirror 4 arranged in sequence along the optical path. The pulse laser 1 outputs laser light with a wavelength of 532 nm, a pulse width of 30 ps, ​​and a repetition frequency of 10 Hz. The input mirror 3 is coated with a dielectric film with a transmittance of more than 99% for incident light at 532 nm and a reflectance of more than 99% for Raman laser at 558 nm. The output mirror 4 is coated with a dielectric film with a reflectivity of more than 99% for incident light at 532 nm and a transmittance of more than 99% for Raman light at 558 nm.

[0063] The pulse laser 1 is the same as that in the first embodiment.

[0064] The Raman crystal 3 is Ca 2 TiSi 2 O 8 The crystal is a cylinder with a length of 35mm. The light-transmitting surface is a round surface,...

Embodiment 3

[0067] Example 3: Sr 2 TiSi 2 O 8 Multi-pass Raman laser outside the crystal cavity.

[0068] Structure like image 3 As shown, the laser is composed of a pulsed laser 1, an input mirror 3, a Raman crystal 2 and an output mirror 5 arranged in sequence along the optical path. The concave surface of the input mirror 3 faces the pulse laser 1 and its plane forms an angle of 45° with the laser direction. The Raman crystal 2 and the output mirror 5 are located on the optical path of the light reflected by the input mirror 3.

[0069] The pulsed laser 1 outputs a pulsed laser with a wavelength of 532 nm, a pulse width of 30 ps, ​​and a repetition frequency of 10 Hz. The input mirror 3 is coated with a dielectric film with a transmittance greater than 99% for the fundamental frequency light and a Raman light (558nm) reflectivity greater than 99%. The output mirror 5 is a flat mirror, and both sides are coated with a reflectance greater than 99% for the fundamental frequency light. Dielec...

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Abstract

The invention relates to a Raman laser based on a crystalline in a fresnoite structure. The laser comprises a pump source, a laser resonant cavity and a Raman crystalline. The Raman crystalline in the fresnoite structure adjusts the laser wavelength and generates laser output provided with fixed frequency shift, the Raman crystalline in the fresnoite structure is obtained through a czochralski method, the general formula is A2RM2O8, wherein A=Ca, Sr or BA; R=Ti or V; and M=Si or Ge. The Raman crystalline is placed outside the laser resonant cavity to form an external cavity type Raman frequency shift laser and placed inside the laser resonant cavity to form an internal cavity type Raman frequency shift laser. The laser has the advantages of being stable in output, simple in structure, high in environmental adaptability and the like.

Description

Technical field [0001] The invention relates to a Raman laser based on a barium barium silicate structure crystal, in particular to a Raman laser using barium barium silicate structure crystal as a Raman gain crystal, and belongs to the technical field of lasers. Background technique [0002] Using the stimulated Raman scattering (SRS) effect of Raman crystals can obtain lasers with wavelengths that cannot be directly emitted by solid-state lasers. Using existing Raman crystals, laser output from ultraviolet to near-infrared can be obtained, including new yellows. Light, orange laser, and 1.5μm human eye safety laser, have a wide range of applications in astronomy, military, medical, electronic display, remote sensing, ocean exploration, chemistry and other fields. Therefore, the exploration of new Raman crystals has become the field of materials research. One of the hot spots. [0003] The performance of the Raman laser depends on the characteristics of the Raman crystal. The Ra...

Claims

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Application Information

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Patent Type & Authority Applications(China)
IPC IPC(8): H01S3/30H01S3/16C30B15/00C30B29/22C30B29/32C30B29/34
Inventor 张怀金王继扬申传英赵显王正平赵永光于浩海
Owner SHANDONG UNIV