Multi-wavelength non-atomic resonance Faraday semiconductor laser

A technology of atomic optical filters and semiconductors, which is applied in the direction of lasers, phonon exciters, laser components, etc., can solve the problems of inability to set different magnetic fields for beams, and inability to achieve non-interference light output, etc., to eliminate competition and achieve sustainable tuning effect

Active Publication Date: 2020-12-01
PEKING UNIV
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  • Summary
  • Abstract
  • Description
  • Claims
  • Application Information

AI Technical Summary

Problems solved by technology

It follows that, due to figure 2 The beams of the two wavelengths are always under the same magnetic field conditions, no matter whether the atomic gas chamber is filled with buffer gas, in this structure, different magnetic fields cannot be set for the beams of different wavelengths, so figure 2 The structure shown cannot achieve 852nm and 780nm output without disturbing light
That is to say, in the above two methods, the dual-wavelength laser is completed under the condition of uniform magnetic field, and each wavelength is subjected to the same magnetic field condition for frequency selection, and the output achieved shows limitations.

Method used

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  • Multi-wavelength non-atomic resonance Faraday semiconductor laser
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  • Multi-wavelength non-atomic resonance Faraday semiconductor laser

Examples

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Embodiment 1

[0041] Non-atomic resonant Faraday semiconductor lasers with dual-wavelength output such as Figure 4 As shown, it includes a laser source, a collimating lens, a first polarizing beam splitting prism 3, an atomic gas chamber 4, a permanent magnet 5 for applying an axial static magnetic field to the atomic gas chamber 4, and a second polarizing beam splitting prism arranged on the optical path in sequence. 3a and reflector 6, wherein the placement angles of the first polarizing beam splitting prism 3 and the second polarizing beam splitting prism 3a are adjusted so that their positional relationship is orthogonal.

[0042] In order to achieve 780nm and 852nm output, the laser is provided with two optical paths, corresponding to the first laser light source 1 and the second laser light source 1a respectively, and their outgoing light is two coherent beams polarized in the vertical direction, the first collimator lens 2 and The second collimating lenses 2a are respectively arrang...

Embodiment 2

[0052] A non-atomic resonant Faraday semiconductor laser that achieves three-wavelength output such as Figure 5 As shown, similarly, it includes a laser source, a collimator lens, a first polarizing beam splitter prism 3, an atomic gas chamber 4 and a permanent magnet 5 for applying an axial static magnetic field to the atomic gas chamber 4, the second The polarizing beam splitting prism 3a and the reflecting mirror 6, wherein the placement angles of the first polarizing beam splitting prism 3 and the second polarizing beam splitting prism 3a are adjusted so that their positional relationship is orthogonal.

[0053] In order to achieve 780nm, 852nm and 766nm output, the laser is equipped with three optical paths, corresponding to the first laser light source 1, the second laser light source 1a, and the third laser light source 1b, and their outputs are three vertically polarized coherent beams, The first collimating lens 2, the second collimating lens 2a and the third collima...

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Abstract

The invention provides a multi-wavelength non-atomic resonance Faraday semiconductor laser. The laser comprises a laser source, a collimating lens, a Faraday atom optical filter and a reflector (6) which are sequentially arranged on an optical path; the laser source comprises a first laser light source (1) and a second laser light source (1a); an atom air chamber (4) contains a first alkali metalatom and a second alkali metal atom; a permanent magnet (5) applies a static magnetic field to the atom air chamber (4), and therefore, the magnetic field intensity in the atomic gas chamber (4) is uniformly distributed in the axial direction and non-uniformly distributed in the radial direction, and the magnetic field intensity on each emergent light path corresponds to the magnetic field intensity which is required by a corresponding wavelength transmission spectrum of a Faraday atomic filter only contains one non-atomic resonance transmission peak. According to the laser of the invention, through the optical filter with the non-uniform magnetic field, multiple beams of light respectively pass through corresponding magnetic field areas on respective optical paths, so that different magnetic field intensities can be obtained, and multi-wavelength laser output without interference light is realized.

Description

【Technical field】 [0001] The invention belongs to the technical field of semiconductor lasers, in particular to a multi-wavelength non-atomic resonance Faraday semiconductor laser with a gas chamber mixed with two kinds of alkali metal atoms. 【Background technique】 [0002] In the field of lasers, the concept of multiwavelength lasers has been around since the early days of lasers, but its status is still rather vague. Realizing multiple wavelength laser outputs on the same device can improve the application efficiency of devices, reduce system complexity, and reduce costs. As more and more applications find new laser devices, multi-wavelength laser devices are also getting more attention. [0003] Multi-wavelength lasers can be applied in fields such as optical communication, wavelength division multiplexing, and quantum frequency standards. Traditional multi-wavelength lasers are mainly based on fiber lasers and solid-state lasers. Fiber lasers typically consist of rela...

Claims

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Application Information

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Patent Type & Authority Applications(China)
IPC IPC(8): H01S3/08H01S3/104H01S3/0941
CPCH01S3/08086H01S3/0941H01S3/104
Inventor 陈景标常鹏媛罗斌郭弘
Owner PEKING UNIV
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