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

A Brillouin gain spectrum, non-scanning technology is applied in the field of devices for measuring Brillouin gain spectrum, which 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: 2013-03-13
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

Method used

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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 implementation mode one: combine figure 1 Describe this embodiment, the pump-detection method described in this embodiment non-scanning device for measuring the Brillouin gain spectrum, it consists of a fiber laser 1, a fiber circulator 2, a polarization controller 3, an optical fiber to be tested 4, and an optical fiber isolation device 5 and ASE light source 6;

[0019] The laser output end of the fiber laser 1 communicates with the first port 2-1 of the fiber circulator 2, the second port 2-2 of the fiber circulator 2 communicates with the first port of the polarization controller 3, and the second port of the polarization controller 3 The port is communicated with one end of the optical fiber 4 to be tested; the laser output end of the ASE light source 6 is communicated with the optical input end of the fiber isolator 5, and the optical output end of the optical fiber isolator 5 is communicated with the other end of the optical fiber 4 to be tested, and the...

specific Embodiment approach 2

[0021] Embodiment 2: The difference between this embodiment and the device for non-scanning measurement of the Brillouin gain spectrum by the pump-probe method in Embodiment 1 is that the laser output by the fiber laser 1 is a C-band narrow-band laser, The wavelength is 1550nm, and the linewidth 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 by the pump-probe method in Embodiment 1 is that the laser output by the ASE light source 6 is a C-band broadband laser, The spectrum is flat around 1550nm, and the range of spectral flatness 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] Brillouin gain spectrum contains important information such as Brillouin frequency shift, linewidth 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 scattered Stokes light is called the Brillouin gain spectrum of nonlinear media; the second is the double-ended method, that is, the pump-probe method, "-" represents that this method uses two paths of light, one for pump light and the other for To detect light, a tunable laser or microwave generator is used to control th...

Claims

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Application Information

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Patent Type & Authority Applications(China)
IPC IPC(8): G01J3/45G01J3/28
Inventor 高玮毕雅凤刘胜男胡小博孙培敬熊燕玲
Owner HARBIN UNIV OF SCI & TECH
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