Single-fiber-type CARS excitation source device and realization method based on two-stage non-linear tuning

A technology of nonlinear tuning and realization method, which is applied in the direction of nonlinear optics, measuring devices, material excitation analysis, etc., can solve the problems that hinder the wide application of CARS, slow wavelength tuning speed, huge system, etc., and achieve the expansion of molecular vibration wave number range, The effect of fast tuning speed and reduced implementation difficulty

Active Publication Date: 2015-08-12
TIANJIN UNIV
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  • Summary
  • Abstract
  • Description
  • Claims
  • Application Information

AI Technical Summary

Problems solved by technology

At present, CARS systems usually use two Ti-doped sapphire lasers with feedback control or two optical parametric oscillators pumped by the same pump source as the excitation source. The pump light and the Stokes light need to be synchronized,...

Method used

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  • Single-fiber-type CARS excitation source device and realization method based on two-stage non-linear tuning
  • Single-fiber-type CARS excitation source device and realization method based on two-stage non-linear tuning
  • Single-fiber-type CARS excitation source device and realization method based on two-stage non-linear tuning

Examples

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Embodiment 1

[0033] Implementation example 1: A single-fiber CARS excitation source device based on dual-stage nonlinear tuning

[0034] Such as figure 1 As shown, the device includes a femtosecond fiber laser source 1, an electronically controlled optical power attenuator 2, a voltage controller 3, a primary tuner 4, a pulse stretcher 5, a pump laser source 6, a wavelength division multiplexer 7, Gain fiber 8, secondary tuner 9, optical filter 10 and output port 11.

[0035] The femtosecond linearly polarized pulsed light output by the femtosecond fiber laser source 1 enters the electronically controlled optical power attenuator 2 as a Stokes optical pulse seed source, and the optical power attenuation value is controlled by the voltage controller 3, and the optical pulse after optical power attenuation Entering the primary tuner 4 to realize power-controlled optical pulse wavelength tuning, the output pulsed light is stretched by the pulse stretcher 5, and then combined with the pumped ...

Embodiment 2

[0036] Implementation example 2: A method for realizing a single-fiber CARS excitation source based on dual-stage nonlinear tuning

[0037] Using femtosecond fiber laser light source to provide femtosecond level linearly polarized pulse light, used as the Stokes light pulse seed source of CARS source, the pulse width range is 50-200fs, the center wavelength is 1030-1064nm, and the repetition frequency is 10MHz-100MHz. Pulse energy greater than 1nJ. The voltage controller outputs the control voltage to control the attenuation value of the electronically controlled optical power attenuator composed of the phase retarder and the polarizer to realize the optical power attenuation adjustment. The primary tuner is composed of photonic crystal fiber. By controlling the injected light power, the soliton self-frequency shift nonlinear effect of photonic crystal fiber is used to realize the tuning of Stokes optical pulse, and the tuning wavelength range is 10-40nm. The pulse stretcher ...

Embodiment 3

[0040] Implementation Example 3: Application Example

[0041] The CARS source outputs a signal light pulse and a Stokes light pulse, wherein the signal light pulse is used as a pump light pulse of the CARS source. Under the action of the pump light pulse of the CARS source and the two light pulses of the Stokes light pulse, the molecular vibration in the analyte that resonates with the frequency difference between the pump light pulse and the Stokes light pulse is first excited, so that It generates resonance, and then the resonant molecular vibration converts a large amount of pump light output by the CARS source into anti-Stokes light to realize the detection of specific molecules. Through two-stage tuning, the pump light pulse and Stokes light pulse of the CARS source cover a wavenumber of 400-4000cm -1 Molecular vibration, so as to meet the measurement of molecular vibration spectrum and excitation imaging of specific molecules in biochemistry.

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Abstract

The invention discloses a single-fiber-type CARS excitation source device and realization method based on two-stage non-linear tuning. The device comprises a femtosecond fiber laser light source, an electric control light power attenuator, a first-stage tuner, a pulse broadening device, a second-stage tuner, a pump laser, a wavelength division multiplexer, a gain fiber, an optical filter and an output port. The femtosecond fiber laser light source outputs femtosecond pulses serving as Stokes optical pulses which enter the electric control light power attenuator; power control optical pulse wavelength tuning is realized in the first-stage tuner; the pulses are broadened to be femtosecond pulses through the pulse broadening device, and the femtosecond pulses then enter the gain fiber for amplification; signal optical pulses and idler frequency optical pulses are generated in the second-stage tuner, wherein the signal optical pulses serve as pump optical pulses of a CARS source; the optical filter filters the idler frequency optical pulses and the residual pump continuous light; and the rest optical pulses are output from the output port. Compared with the prior art, the device adopts a single-fiber light path structure and electric control tuning, and has the advantages of compact structure, anti-interference, high reliability and fast tuning speed; and CARS rapid imaging requirement is met.

Description

technical field [0001] The invention relates to the technical field of optical nonlinear microscopic imaging, in particular to an excitation source device of a CARS microscopic imaging system. Background technique [0002] CARS microscopy utilizes coherent anti-Stokes Raman scattering to detect molecules. When the frequency difference between the pump light and the Stokes light is equal to the vibration frequency of the molecule to be detected, strong anti-Stokes scattered light will be generated, thereby enabling the detection of the molecule to be detected. Due to the high signal-to-noise ratio of CARS microscopic imaging technology, its three-dimensional tomographic capability, and the need for fluorescent labeling and confocal systems, it has attracted widespread attention in recent years and has developed rapidly. The CARS microscopy imaging system requires two wavelengths of laser light, at least one of which is wavelength tunable. At present, CARS systems usually us...

Claims

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Application Information

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IPC IPC(8): G02F1/35G01N21/65
CPCG01N21/65G01N2021/655G02F1/35
Inventor 江俊峰刘铁根刘琨王双王辉吴航
Owner TIANJIN UNIV
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