Device and method for measuring brillouin gain spectrum in non-scanning manner based on pumping-detection method

A Brillouin gain spectrum, non-scanning technology, applied in the field of devices for measuring Brillouin gain spectrum, can solve the problems of long measurement time, low signal-to-noise ratio, and complicated device, and achieves simple device, huge application potential, high power stable effect

Inactive Publication Date: 2015-04-22
HARBIN UNIV OF SCI & TECH
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  • Summary
  • Abstract
  • Description
  • Claims
  • Application Information

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Problems solved by technology

[0003] The purpose of the present invention is to solve the problems of low signal-to-noise ratio, long measurement time and complex devices for measuring the Brillouin gain spectrum in the existing devices and methods, and provides a pump-detection method for non-scanning measurement of the Brillouin gain Apparatus and method for spectroscopy

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  • Device and method for measuring brillouin gain spectrum in non-scanning manner based on pumping-detection method
  • Device and method for measuring brillouin gain spectrum in non-scanning manner based on pumping-detection method
  • Device and method for measuring brillouin gain spectrum in non-scanning manner based on pumping-detection method

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specific Embodiment approach 1

[0018] Specific embodiment one: combination figure 1 In this embodiment, the pump-probe method of non-scanning measurement of Brillouin gain spectrum in this embodiment is composed of fiber laser 1, fiber circulator 2, polarization controller 3, fiber under test 4, and fiber isolation The device 5 and the ASE light source 6 are composed;

[0019] The laser output end of the fiber laser 1 is connected to the first port 2-1 of the fiber circulator 2, the second port 2-2 of the fiber circulator 2 is connected to the first port of the polarization controller 3, and the second port of the polarization controller 3 is connected. The port is connected with one end of the fiber under test 4; the laser output end of the ASE light source 6 is connected with the light input end of the fiber isolator 5, the light output end of the fiber isolator 5 is connected with the other end of the fiber under test 4, and the fiber circulator 2 The third port 2-3 of is the light output end of the device ...

specific Embodiment approach 2

[0021] Embodiment 2: The difference between this embodiment and the device for non-scanning Brillouin gain spectrum measurement of the pump-probe method described in Embodiment 1 is that the laser light output by the fiber laser 1 is a C-band narrowband laser. The wavelength is 1550nm and the line width range is 1KHz-10MHz.

specific Embodiment approach 3

[0022] Embodiment 3: The difference between this embodiment and the device for non-scanning Brillouin gain spectrum measurement of the pump-probe method described in Embodiment 1 is that the laser output from the ASE light source 6 is a C-band broadband laser. The spectrum is flat around 1550nm, and the flat range of the spectrum is 1nm-40nm.

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Abstract

A device and a method for measuring a brillouin gain spectrum in a non-scanning manner based on a pumping-detection method relate to a device and a method for measuring the brillouin gain spectrum and aim to solve the problems of low signal-to-noise ratio, long measurement time and complex device of the conventional device and method in brillouin gain spectrum measurement. In the device for measuring the brillouin gain spectrum in the non-scanning manner based on the pumping-detection method, the laser output end of an optical fiber laser is communicated with the first port of an optical fiber circulator; the second port of the optical fiber circulator is communicated with the first port of a polarization controller, and the second port of the polarization controller is communicated with one end of an optical fiber to be measured; the laser output end of an ASE (Amplified Spontaneous Emission) light source is communicated with the light input end of an optical fiber isolator; the light output end of the optical fiber isolator is communicated with the other end of the optical fiber to be measured; and the third port of the optical fiber circulator serves as the light output end of the device for measuring the brillouin gain spectrum in the non-scanning manner based on the pumping-detection method; and besides, the connection is optical fiber connection. The device and the method provided by the invention are suitable for measuring the brillouin gain spectrum.

Description

Technical field [0001] The invention relates to a device and method for measuring Brillouin gain spectrum. Background technique [0002] The Brillouin gain spectrum contains important information such as Brillouin frequency shift, line width, and gain envelope, and is widely used in distributed optical fiber sensing, filtering and amplification of weak signals, and Brillouin lidar detection. At present, there are two main types of devices and methods for measuring the Brillouin gain spectrum: One is the single-ended method, that is, only the pump light is input into the nonlinear medium (such as optical fiber, water, etc.), and then the Brillouin The spectrum of the scattered Stokes light is called the Brillouin gain spectrum of the nonlinear medium; the second is the double-ended method, that is, the pump-detection method. "-" means that the method uses two paths of light, one is pump light, and the other To detect the light, a tunable laser or microwave generator is used to co...

Claims

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Application Information

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Patent Type & Authority Patents(China)
IPC IPC(8): G01J3/45G01J3/28
Inventor 高玮史光耀李宏伟刘胜男杨玉强张洪英
Owner HARBIN UNIV OF SCI & TECH
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