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Raman laser based on crystalline in fresnoite structure

A technology of Raman laser and barite, applied in the field of Raman laser

Active Publication Date: 2014-11-19
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 Raman crystals for extracavity single-pass Raman lasers.

[0056] structured as figure 1 As shown, the laser consists of a pulsed laser 1 and a Raman crystal 2. Pulse laser 1 is a picosecond pulse laser pumped by a flash lamp, double-modulated by an acousto-optic modulator and a dye saturable absorbing material, and its output wavelength is 532nm, a pulse width of 30ps, and a repetition frequency of 10Hz; 2 TiSi 2 o 8 Raman crystals generate stimulated Raman light. Figure 8 It is the output Raman laser spectrum diagram of the laser. From the figure, we can clearly see the output of the 558nm primary Raman laser and the 587nm secondary Raman laser.

[0057] The Raman crystal 2 is Ba 2 TiSi 2 o 8 Crystal, the size of which is 5 x 5 x 25mm 3 , the transparent surface is 5×5mm 2 , which are polished and uncoated on both sides.

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

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

Embodiment 2

[0061] Example 2: Ca 2 TiSi 2 o 8 Extracavity double-pass Raman lasers for crystals.

[0062] structured as 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 pulsed laser 1 outputs laser light with a wavelength of 532 nm, a pulse width of 30 ps, ​​and a repetition rate of 10 Hz. The input mirror 3 is coated with a dielectric film with a transmittance of more than 99% for incident light at 532nm and a reflectivity of more than 99% for Raman laser at 558nm. The output mirror 4 is coated with a dielectric film with a reflectivity greater than 99% for incident light at 532nm and a transmittance greater than 99% for Raman light at 558nm.

[0063] The pulsed laser 1 is the same as that in Embodiment 1.

[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 circular surfac...

Embodiment 3

[0067] Example 3: Sr 2 TiSi 2 o 8 Crystalline extracavity multiple-pass Raman lasers.

[0068] structured as 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 pulsed laser 1 , and its plane forms an included 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 rate of 10 Hz. The input mirror 3 is coated with a dielectric film with a transmittance of more than 99% for fundamental frequency light and a reflectivity of more than 99% for Raman light (558nm). A dielectric film with a transmittance greater than 99% for Raman light (558nm). The radius of curvature of the concave surfa...

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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 barite structure crystal, in particular to a Raman laser using a barite structure crystal as a Raman gain crystal, and belongs to the field of laser technology. Background technique [0002] The stimulated Raman scattering (SRS) effect of Raman crystals can be used to obtain lasers with wavelengths that cannot be directly emitted by solid-state lasers. The existing Raman crystals can be used to obtain laser output from the ultraviolet band to the near-infrared band, including new yellow lasers. Light, orange laser, and 1.5μm eye-safe laser are widely used in astronomy, military, medical, electronic display, remote sensing, ocean exploration, chemistry and other fields. Therefore, exploring new Raman crystals has become the focus of material research One of the hot spots. [0003] The performance of Raman laser depends on the characteristics of Raman crystal. Raman crystals currently entering the pract...

Claims

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Application Information

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Patent Type & Authority Patents(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