Nothing Special   »   [go: up one dir, main page]

CN105811227B - A kind of super flat super continuous spectrums laser acquisition methods of femtosecond - Google Patents

A kind of super flat super continuous spectrums laser acquisition methods of femtosecond Download PDF

Info

Publication number
CN105811227B
CN105811227B CN201610307174.1A CN201610307174A CN105811227B CN 105811227 B CN105811227 B CN 105811227B CN 201610307174 A CN201610307174 A CN 201610307174A CN 105811227 B CN105811227 B CN 105811227B
Authority
CN
China
Prior art keywords
laser
pulse
optical fiber
wavelength
mould group
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Active
Application number
CN201610307174.1A
Other languages
Chinese (zh)
Other versions
CN105811227A (en
Inventor
万雄
刘鹏希
章婷婷
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Shanghai Institute of Technical Physics of CAS
Original Assignee
Shanghai Institute of Technical Physics of CAS
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by Shanghai Institute of Technical Physics of CAS filed Critical Shanghai Institute of Technical Physics of CAS
Priority to CN201610307174.1A priority Critical patent/CN105811227B/en
Publication of CN105811227A publication Critical patent/CN105811227A/en
Application granted granted Critical
Publication of CN105811227B publication Critical patent/CN105811227B/en
Active legal-status Critical Current
Anticipated expiration legal-status Critical

Links

Classifications

    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01SDEVICES USING THE PROCESS OF LIGHT AMPLIFICATION BY STIMULATED EMISSION OF RADIATION [LASER] TO AMPLIFY OR GENERATE LIGHT; DEVICES USING STIMULATED EMISSION OF ELECTROMAGNETIC RADIATION IN WAVE RANGES OTHER THAN OPTICAL
    • H01S3/00Lasers, i.e. devices using stimulated emission of electromagnetic radiation in the infrared, visible or ultraviolet wave range
    • H01S3/05Construction or shape of optical resonators; Accommodation of active medium therein; Shape of active medium
    • H01S3/06Construction or shape of active medium
    • H01S3/063Waveguide lasers, i.e. whereby the dimensions of the waveguide are of the order of the light wavelength
    • H01S3/067Fibre lasers
    • H01S3/06708Constructional details of the fibre, e.g. compositions, cross-section, shape or tapering
    • H01S3/06716Fibre compositions or doping with active elements
    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01SDEVICES USING THE PROCESS OF LIGHT AMPLIFICATION BY STIMULATED EMISSION OF RADIATION [LASER] TO AMPLIFY OR GENERATE LIGHT; DEVICES USING STIMULATED EMISSION OF ELECTROMAGNETIC RADIATION IN WAVE RANGES OTHER THAN OPTICAL
    • H01S3/00Lasers, i.e. devices using stimulated emission of electromagnetic radiation in the infrared, visible or ultraviolet wave range
    • H01S3/05Construction or shape of optical resonators; Accommodation of active medium therein; Shape of active medium
    • H01S3/06Construction or shape of active medium
    • H01S3/063Waveguide lasers, i.e. whereby the dimensions of the waveguide are of the order of the light wavelength
    • H01S3/067Fibre lasers
    • H01S3/06754Fibre amplifiers
    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01SDEVICES USING THE PROCESS OF LIGHT AMPLIFICATION BY STIMULATED EMISSION OF RADIATION [LASER] TO AMPLIFY OR GENERATE LIGHT; DEVICES USING STIMULATED EMISSION OF ELECTROMAGNETIC RADIATION IN WAVE RANGES OTHER THAN OPTICAL
    • H01S3/00Lasers, i.e. devices using stimulated emission of electromagnetic radiation in the infrared, visible or ultraviolet wave range
    • H01S3/09Processes or apparatus for excitation, e.g. pumping
    • H01S3/091Processes or apparatus for excitation, e.g. pumping using optical pumping
    • H01S3/094Processes or apparatus for excitation, e.g. pumping using optical pumping by coherent light
    • H01S3/0941Processes or apparatus for excitation, e.g. pumping using optical pumping by coherent light of a laser diode
    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01SDEVICES USING THE PROCESS OF LIGHT AMPLIFICATION BY STIMULATED EMISSION OF RADIATION [LASER] TO AMPLIFY OR GENERATE LIGHT; DEVICES USING STIMULATED EMISSION OF ELECTROMAGNETIC RADIATION IN WAVE RANGES OTHER THAN OPTICAL
    • H01S3/00Lasers, i.e. devices using stimulated emission of electromagnetic radiation in the infrared, visible or ultraviolet wave range
    • H01S3/10Controlling the intensity, frequency, phase, polarisation or direction of the emitted radiation, e.g. switching, gating, modulating or demodulating
    • H01S3/10007Controlling the intensity, frequency, phase, polarisation or direction of the emitted radiation, e.g. switching, gating, modulating or demodulating in optical amplifiers
    • H01S3/10015Controlling the intensity, frequency, phase, polarisation or direction of the emitted radiation, e.g. switching, gating, modulating or demodulating in optical amplifiers by monitoring or controlling, e.g. attenuating, the input signal
    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01SDEVICES USING THE PROCESS OF LIGHT AMPLIFICATION BY STIMULATED EMISSION OF RADIATION [LASER] TO AMPLIFY OR GENERATE LIGHT; DEVICES USING STIMULATED EMISSION OF ELECTROMAGNETIC RADIATION IN WAVE RANGES OTHER THAN OPTICAL
    • H01S3/00Lasers, i.e. devices using stimulated emission of electromagnetic radiation in the infrared, visible or ultraviolet wave range
    • H01S3/10Controlling the intensity, frequency, phase, polarisation or direction of the emitted radiation, e.g. switching, gating, modulating or demodulating
    • H01S3/13Stabilisation of laser output parameters, e.g. frequency or amplitude
    • H01S3/1305Feedback control systems

Landscapes

  • Physics & Mathematics (AREA)
  • Electromagnetism (AREA)
  • Engineering & Computer Science (AREA)
  • Plasma & Fusion (AREA)
  • Optics & Photonics (AREA)
  • Automation & Control Theory (AREA)
  • Lasers (AREA)

Abstract

The invention discloses a kind of super flat super continuous spectrums laser acquisition methods of femtosecond, this method is realized on the super continuous spectrums laser of super flat spectrum output.This method include wavelength selection, seed laser generate, seed laser power amplification, laser compression and amplify again, super continuous spectrums generate and monitoring, seed laser power automatic adjusument.The beneficial effects of the invention are as follows, by the way of a kind of pumping of reaction type amplitude modulation multiwavelength laser, in conjunction with wide spectrum spectrum monitoring, the intensity of multi wavelength pumping laser is adaptively adjusted, the super continuous spectrums laser output that high output spectrum flatness and stability are realized by superposition, meets the needs of precision wide spectrum quantitative analysis.

Description

A kind of super flat super continuous spectrums laser acquisition methods of femtosecond
Technical field
The present invention relates to a kind of pulse laser generation methods, more particularly to a kind of reaction type amplitude modulation multiwavelength laser that is based on to pump The super flat super continuous spectrums laser acquisition methods of the femtosecond at Pu.
Background technique
Super continuous spectrums laser refer to when pumping laser pass through special optical waveguide when, a series of nonlinear effect causes incidence The spectrum widening of laser beam, to export wide spectrum laser beam-title super continuous spectrums.Especially as ultrafast laser and photonic crystal The development of optical fiber (Photonic crystal fibers, abbreviation PCF) technology, is produced using propagation of the ultrashort pulse in PCF Raw super continuum light has become the noticeable project in the whole world.This technology only needs low-down pulse energy (about Super continuum light can 1nJ) be generated, and obtained super continuum light is relevant and brightness is high --- this makes it ideal White light source.
Super continuous spectrums laser has been rapidly developed since birth, especially in terms of spectral region, is covered substantially Infrared spectral coverage has been covered from ultraviolet in.In addition, also achieving huge progress in terms of high-power and device miniaturization.
However, current super continuous laser source can not in some applications for needing to refine wide spectrum quantitative analysis It is competent, because existing super continuous spectrums laser source is asked in the technical indicators such as output spectrum flatness and stability there are some Topic can not adapt to the requirement of wide range accurate quantification analysis.Therefore, the super company of high output spectrum flatness and stability how is realized Continuous spectrum laser is a urgent need to solve the problem.
Summary of the invention
The purpose of the present invention is to provide a kind of realities of the super continuous spectrums laser of high output spectrum flatness and stability Existing method, its mode based on the pumping of reaction type amplitude modulation multiwavelength laser can meet the needs of precision wide spectrum quantitative analysis.
The technical scheme is that be achieved in, high output spectrum flatness and stability proposed by the present invention Super continuous spectrums laser is made of controller, pumping source mould group, ring laser mould group and supercontinuum generation and monitoring mould group.
Pumping source mould group is used to generate the multi-Wavelength Pulses seed laser of loop laser device assembly.It includes power regulation Device, the first impulse generator, the first shaping amplifier, first laser tube drive circuit, the second impulse generator, the second shaping are put Big device, second laser tube drive circuit, third impulse generator, third shaping amplifier, third laser tube drive circuit, three close One optical fiber, the first Polarization Controller and optoisolator;Wherein first laser tube drive circuit by the first field-effect tube driving circuit, First field-effect tube and first laser diode and its discharge loop composition;Similarly, second laser tube drive circuit is by second Field-effect tube driving circuit, the second field-effect tube and second laser diode and its discharge loop composition;The driving of third laser tube Circuit is made of third field-effect tube driving circuit, third field-effect tube and third laser diode and its discharge loop;Power Adjuster is used to amplify the first shaping amplifier, the second shaping amplifier, third shaping amplifier the adjusting of multiple.
Ring laser mould group include the first semiconductor laser, the second semiconductor laser, third semiconductor laser, Four-in-one photo-coupler, annular chamber, the first negative GVD optical fiber, the first wavelength division multiplexer, ytterbium doped optical fiber amplifier, the second wavelength-division are multiple With device, the second negative GVD optical fiber, the second Polarization Controller, third Polarization Controller, Faraday isolator and the 4th Polarization Control Device, the multi-Wavelength Pulses seed laser for sending to pumping source mould group carry out power amplification and pulse mode-locked compression.
Supercontinuum generation and monitoring mould group include PCF coupler, PCF, one-in-and-two-out optical fiber, output interface and wide range Section spectrometer carries out real-time monitoring for generating super continuous spectrums pulse laser, while to its spectral characteristic, and monitoring result is anti- It feeds controller.
Controller contains the hardware circuit and software systems for executing control with data analysis, swashs for controlling the first semiconductor Light device, the second semiconductor laser, third semiconductor laser, the first impulse generator, the second impulse generator, third pulse Generator, power governor and wide spectrum spectrometer, and the output spectrum signal for receiving wide spectrum spectrometer carries out spectroscopic data Analysis.
The super flat spectrum of super continuous spectrums laser exports and high stable characteristic is realized according to the following steps:
(1) according to the zero-dispersion wavelength λ of PCF0, find out its corresponding frequency f0;Setpoint frequency difference Δ f, setpoint frequency f1= f0+ Δ f finds out its corresponding wavelength X1;Similarly, setpoint frequency f2=f0Δ f finds out its corresponding wavelength X2
(2) select the operation wavelength of first laser diode and the first semiconductor laser for λ0;Select second laser two Pole pipe and the operation wavelength of the second semiconductor laser are λ1;Select the work of third laser diode and third semiconductor laser Making wavelength is λ2
(3) controller sending control instruction gives the first impulse generator, the second impulse generator and third impulse generator, The pulse frequency of three is set as identical value and is allowed to start work;
(4) controller issues control instruction starting the first semiconductor laser, the second semiconductor laser, third semiconductor Laser, wide spectrum spectrometer;
(5) controller issues control instruction to power governor, and power governor is by the first shaping amplifier, the second shaping One identical initial value A of amplification factor setting of amplifier, third shaping amplifier1=A2=A3
The high frequency electric pulse that (6) first impulse generators issue carries out shaping pulse through the first shaping amplifier first, adjusts High level duty ratio is saved, the high frequency electric pulse of nanosecond is formed, then presses A1After multiple carries out power amplification, it is sent into first laser The control pin of the field-effect tube driving chip in the first field-effect tube driving circuit in tube drive circuit, field-effect tube driving The nanosecond pulse signal that the output pin of chip generates high frequency be used to control the first field-effect tube of high-speed high-power conducting and Cut-off makes first laser diode generate the nanosecond of high frequency for controlling the charge and discharge in first laser diode discharge circuit Pulse seed laser;
Similarly, it is whole that the high frequency electric pulse that the second impulse generator issues carries out pulse through the second shaping amplifier first Shape adjusts high level duty ratio, forms the high frequency electric pulse of nanosecond, then presses A2After multiple carries out power amplification, it is sent into the The control pin of the field-effect tube driving chip in the second field-effect tube driving circuit in dual-laser tube drive circuit, field-effect The output pin of pipe driving chip generates high frequency nanosecond pulse signal for controlling leading for the second field-effect tube of high-speed high-power Logical and cut-off makes second laser diode generate high frequency nanosecond for controlling the charge and discharge in second laser diode discharge circuit Grade pulse seed laser;
Similarly, it is whole that the high frequency electric pulse that third impulse generator issues carries out pulse through third shaping amplifier first Shape adjusts high level duty ratio, forms the high frequency electric pulse of nanosecond, then presses A3After multiple carries out power amplification, it is sent into the The control pin of the field-effect tube driving chip in third field-effect tube driving circuit in three laser tube drive circuits, field-effect The output pin of pipe driving chip generates the nanosecond pulse signal of high frequency for controlling high-speed high-power third field-effect tube On and off makes third laser diode generate high frequency for controlling the charge and discharge of third laser diode discharge loop Nanosecond pulse seed laser;
(7) three beams wavelength is respectively λ0、λ1、λ2Pulse seed laser through in three-in-one fiber coupling entering light fibre, then through the One Polarization Controller and optoisolator are transferred into ring laser mould group.The effect of first Polarization Controller and optoisolator is Eliminate the issuable echo interference of ring laser mould group;
(8) the first semiconductor laser in ring laser mould group, the wavelength of transmitting are λ0Continuous pump laser beam warp It crosses after two equal part of four-in-one photo-coupler and annular chamber is entered with both direction, pass through the first wavelength division multiplexer and the second wavelength-division respectively After multiplexer, ytterbium doped optical fiber amplifier is pumped from both direction.The wavelength of pumping source mould group output is λ0Nanosecond pulse Seed laser carries out power amplification by ytterbium doped optical fiber amplifier, while the nanosecond pulse laser first passes through the first negative GVD light Fibre, pulse are compressed, since ytterbium doped optical fiber amplifier has positive GVD, so the nanosecond pulse have passed through stretching, using After second negative GVD optical fiber, pulse has obtained second compression again, and chirp (chirp) compensation is carried out in annular chamber.Third Polarization Control Device, Faraday isolator and the 4th Polarization Controller form a resonator, using nonlinear polarization rotation, formed etc. Saturable absorber is imitated, the nonlinear birefringence effect in optical fiber is recycled, based on the self-locking mode in nonlinear birefringence optical fiber Mechanism generates ultrashort femtosecond laser pulse, and makes the laser in annular chamber along one-way transmission, defeated by the second Polarization Controller High-power wavelength is λ out0Femtosecond pulsed laser to supercontinuum generation and monitoring mould group;
Meanwhile the second semiconductor laser in ring laser mould group, the wavelength of transmitting are λ1Continuous pump laser beam Annular chamber is entered with both direction after two equal part of four-in-one photo-coupler, passes through the first wavelength division multiplexer and the second wave respectively After division multiplexer, ytterbium doped optical fiber amplifier is pumped from both direction.The wavelength of pumping source mould group output is λ1Nanosecond arteries and veins It rushes seed laser and carries out power amplification by ytterbium doped optical fiber amplifier, while the nanosecond pulse laser first passes through the first negative GVD Optical fiber, pulse are compressed, and since ytterbium doped optical fiber amplifier has positive GVD, so the nanosecond pulse have passed through stretching, then are passed through After crossing the second negative GVD optical fiber, pulse has obtained second compression again, and chirp (chirp) compensation is carried out in annular chamber.Based on non-linear Self-locking mode mechanism in birefringence fiber generates ultrashort femtosecond laser pulse, and makes laser in annular chamber along one-way transmission, Exporting high-power wavelength by the second Polarization Controller is λ0Femtosecond pulsed laser to supercontinuum generation and monitoring mould group;
Similarly, the third semiconductor laser in same time, ring laser mould group, the wavelength of transmitting are λ2Even Continuous pump laser beam enters annular chamber after two equal part of four-in-one photo-coupler with both direction, multiple by the first wavelength-division respectively After device and the second wavelength division multiplexer, ytterbium doped optical fiber amplifier is pumped from both direction.Pumping source mould group output wavelength be λ2Nanosecond pulse seed laser carry out power amplification by ytterbium doped optical fiber amplifier, while the nanosecond pulse laser first passes through The first negative GVD optical fiber is crossed, pulse is compressed, since ytterbium doped optical fiber amplifier has positive GVD, so the nanosecond pulse is passed through It stretches, after the second negative GVD optical fiber, pulse has obtained second compression again, and chirp (chirp) is carried out in annular chamber and is mended It repays.Using the nonlinear birefringence effect in optical fiber, ultrashort fly is generated based on the self-locking mode mechanism in nonlinear birefringence optical fiber Second grade laser pulse, and make the laser in annular chamber along one-way transmission, exporting high-power wavelength by the second Polarization Controller is λ2Femtosecond pulsed laser to supercontinuum generation and monitoring mould group;
(9) wavelength of ring laser mould group output is respectively λ0、λ1、λ2Femtosecond pulsed laser enter continuous spectrum production In raw and monitoring mould group, after entering PCF by PCF coupler, due to the nonlinear effect that each rank is all types of in PCF, formed Respectively with λ0、λ1、λ2Centered on spectrum widening, the width and intensity and λ of broadening0、λ1、λ2Femtosecond pulsed laser power Directly proportional, the spectrum of three broadenings is overlapped mutually, and forms femtosecond super continuous spectrums pulse laser;
(10) femtosecond super continuous spectrums pulse laser passes through output interface by being divided into two-way after one-in-and-two-out optical fiber all the way Output;Another way enters wide spectrum spectrometer and is monitored, and super continuous spectrums monitoring result is sent to controller;
(11) controller analyzes super continuous spectrums monitoring result, evaluates its spectrum flatness, while generating new needle To the first shaping amplifier, the second shaping amplifier, third shaping amplifier amplification factor A1、A2、A3
(12) (5) to (11) constantly are repeated, until super continuous spectrums monitoring result meets flatness requirement.It so far, will be newest A1、A2、A3It is fixed, finally realize the super continuous spectrums laser of high output spectrum flatness and stability.
The invention has the advantages that by the way of a kind of pumping of reaction type amplitude modulation multiwavelength laser, in conjunction with wide light Spectrum monitoring is composed, the intensity of multi wavelength pumping laser is adaptively adjusted, by the high output spectrum flatness of superposition realization and surely Qualitative super continuous spectrums laser output, meets the needs of precision wide spectrum quantitative analysis.
Detailed description of the invention
Fig. 1 is the principle of the present invention figure, in figure: 1 --- controller;2 --- pumping source mould group;3 --- power governor; 4 --- the first impulse generator;5 --- the first shaping amplifier;6 --- first laser diode;7 --- the first field-effect Pipe;8 --- the first field-effect tube driving circuit;9 --- the second impulse generator;10 --- the second shaping amplifier;11—— Second laser diode;12 --- the second field-effect tube;13 --- the second field-effect tube driving circuit;14 --- third pulse hair Raw device;15 --- third shaping amplifier;16 --- third field-effect tube driving circuit;17 --- third field-effect tube; 18 --- third laser diode;19 --- three-in-one optical fiber;20 --- the first Polarization Controller;21 --- optoisolator; 22 --- ring laser mould group;23 --- the first negative GVD optical fiber;24 --- the first wavelength division multiplexer;25 --- the 4th polarization Controller;26 --- Faraday isolator;27 --- third Polarization Controller;28 --- ytterbium doped optical fiber amplifier;29—— Second wavelength division multiplexer;30 --- the second negative GVD optical fiber;31 --- the second Polarization Controller;32 --- supercontinuum generation and Monitor mould group;33 --- PCF coupler;34——PCF;35 --- one-in-and-two-out optical fiber;36 --- output interface;37 --- it is wide Spectral coverage spectrometer;38 --- four-in-one photo-coupler;39 --- the first semiconductor laser;40 --- the second semiconductor laser Device;41 --- third semiconductor laser;42 --- first laser tube drive circuit;43 --- second laser tube drive circuit; 44 --- third laser tube drive circuit;45 --- annular chamber.
Note: GVD, that is, group velocity dispersion, group velocity dispersion;PCF, that is, photonic crystal Fiber, photonic crystal fiber.
Specific embodiment
The specific embodiment of the invention is as shown in Figure 1.
The structure of the super continuous spectrums laser of high output spectrum flatness and stability proposed by the present invention is as shown in Figure 1, The super continuous spectrums laser is by controller 1, pumping source mould group 2, ring laser mould group 22 and supercontinuum generation and monitoring mould 32 composition of group.
Pumping source mould group 2 is used to generate the multi-Wavelength Pulses seed laser of loop laser device assembly 22.It includes power tune Save device 3, the first impulse generator 4, the first shaping amplifier 5, first laser tube drive circuit 42, the second impulse generator 9, the Two shaping amplifiers 10, second laser tube drive circuit 43, third impulse generator 14, third shaping amplifier 15, third swash Light pipe driving circuit 44, three-in-one optical fiber 19, the first Polarization Controller 20 and optoisolator 21;Wherein first laser pipe driving electricity Road 42 is made of the first field-effect tube driving circuit 8, the first field-effect tube 7 and first laser diode 6 and its discharge loop;Class As, second laser tube drive circuit 43 is by the second field-effect tube driving circuit 13, the second field-effect tube 12 and second laser two Pole pipe 11 and its discharge loop composition;Third laser tube drive circuit 44 is imitated by third field-effect tube driving circuit 16, third field It should pipe 17 and third laser diode 18 and its discharge loop composition;Power governor 3 is used for the first shaping amplifier 5, the Two shaping amplifiers 10, third shaping amplifier 15 amplify the adjusting of multiple.
Ring laser mould group 22 includes the first semiconductor laser 39, the second semiconductor laser 40, third semiconductor Laser 41, four-in-one photo-coupler 38, annular chamber 45, the first negative GVD optical fiber 23, the first wavelength division multiplexer 24, Yb dosed optical fiber Amplifier 28, the second wavelength division multiplexer 29, the second negative GVD optical fiber 30, the second Polarization Controller 31, third Polarization Controller 27, Faraday isolator 26 and the 4th Polarization Controller 25, the multi-Wavelength Pulses seed for being sent to pumping source mould group 2 Laser carries out power amplification and pulse mode-locked compression.
Supercontinuum generation and monitoring mould group 32 include PCF coupler 33, PCF34, one-in-and-two-out optical fiber 35, output interface 36 and wide spectrum spectrometer 37, real-time monitoring is carried out for generating super continuous spectrums pulse laser, while to its spectral characteristic, and Monitoring result is fed back into controller 1.
Controller 1 is containing the hardware circuit and software systems for executing control with data analysis, for controlling the first semiconductor Laser 39, the second semiconductor laser 40, third semiconductor laser 41, the first impulse generator 4, the second impulse generator 9, third impulse generator 14, power governor 3 and wide spectrum spectrometer 37, and receive the output spectrum of wide spectrum spectrometer 37 Signal carries out spectral data analysis.
The super flat spectrum of super continuous spectrums laser exports and high stable characteristic is realized according to the following steps:
(1) according to the zero-dispersion wavelength λ of PCF340, find out its corresponding frequency f0;Setpoint frequency difference Δ f, setpoint frequency f1 =f0+ Δ f finds out its corresponding wavelength X1;Similarly, setpoint frequency f2=f0Δ f finds out its corresponding wavelength X2;(at this λ in embodiment0=780nm, f0=3.85 × 1014Hz;Δ f=2 × 1014Hz;f1=5.85 × 1014Hz, λ1=513nm;f2= 1.85×1014Hz, λ2=1247nm)
(2) selecting the operation wavelength of first laser diode 6 and the first semiconductor laser 39 is λ0;Select second laser The operation wavelength of diode 11 and the second semiconductor laser 40 is λ1;Third laser diode 18 and third semiconductor is selected to swash The operation wavelength of light device 41 is λ2
(3) controller 1 issues control instruction to the first impulse generator 4, the second impulse generator 9 and third pulse generation The pulse frequency of three is set as identical value and is allowed to start work by device 14;(pulse frequency is in the present embodiment 100MHz)
(4) controller 1 issues control instruction starting the first semiconductor laser 39, the second semiconductor laser 40, third Semiconductor laser 41, wide spectrum spectrometer 37;
(5) controller 1 issues control instruction to power governor 3, and power governor 3 is by the first shaping amplifier 5, second One identical initial value A of amplification factor setting of shaping amplifier 10, third shaping amplifier 151=A2=A3
The frequency that (6) first impulse generators 4 issue is that the electric pulse of 100MHz carries out first through the first shaping amplifier 5 Shaping pulse adjusts high level duty ratio, and the frequency for forming nanosecond is the electric pulse of 100MHz, then presses A1Multiple carries out function After rate amplification, the field-effect tube being sent into the first field-effect tube driving circuit 8 in first laser tube drive circuit 42 drives core The control pin of piece, the output pin of field-effect tube driving chip generate the nanosecond pulse signal that frequency is 100MHz and are used to control The on and off of the first field-effect tube of high-speed high-power 7 processed, for controlling the charge and discharge of 6 discharge loop of first laser diode Electricity makes first laser diode 6 generate the nanosecond pulse seed laser of repetition 100MHz;
Similarly, the electric pulse that the frequency that the second impulse generator 9 issues is 100MHz is first through the second shaping amplifier 10 Shaping pulse is first carried out, high level duty ratio is adjusted, the frequency for forming nanosecond is the electric pulse of 100MHz, then presses A2Multiple The field-effect tube in the second field-effect tube driving circuit 13 after carrying out power amplification, in feeding second laser tube drive circuit 43 The control pin of driving chip, the output pin of field-effect tube driving chip generate the nanosecond pulse signal that frequency is 100MHz For controlling the on and off of the second field-effect tube of high-speed high-power 12, for controlling 11 discharge loop of second laser diode Charge and discharge, make second laser diode 11 generate repetition 100MHz nanosecond pulse seed laser;
Similarly, the electric pulse that the frequency that third impulse generator 14 issues is 100MHz is first through third shaping amplifier 15 Shaping pulse is first carried out, high level duty ratio is adjusted, the frequency for forming nanosecond is the electric pulse of 100MHz, then presses A3Multiple The field-effect tube in third field-effect tube driving circuit 16 after carrying out power amplification, in feeding third laser tube drive circuit 44 The control pin of driving chip, the output pin of field-effect tube driving chip generate the nanosecond pulse signal that frequency is 100MHz For controlling the on and off of high-speed high-power third field-effect tube 17, for controlling 18 discharge loop of third laser diode Charge and discharge, make third laser diode 18 generate repetition 100MHz nanosecond pulse seed laser;
(7) three beams wavelength is respectively λ0、λ1、λ2Pulse seed laser through in three-in-one 19 coupled into optical fibres of optical fiber, then pass through First Polarization Controller 20 and optoisolator 21 are transferred into ring laser mould group 22.First Polarization Controller 20 and optical isolation The effect of device 21 is to eliminate the issuable echo interference of ring laser mould group 22;
(8) the first semiconductor laser 39 in ring laser mould group 22, the wavelength of transmitting are λ0Continuous pumping laser Beam enters annular chamber 45 after 41 liang of equal parts of four-in-one photo-coupler with both direction, passes through the first wavelength division multiplexer 24 respectively After the second wavelength division multiplexer 29, ytterbium doped optical fiber amplifier 28 is pumped from both direction.Pumping source mould group 2 export wavelength be λ0Nanosecond pulse seed laser carry out power amplification by ytterbium doped optical fiber amplifier 28, while nanosecond pulse laser is first By the first negative GVD optical fiber 10, pulse is compressed, since ytterbium doped optical fiber amplifier 28 has positive GVD, so nanosecond arteries and veins Punching have passed through stretching, and after the second negative GVD optical fiber 23, pulse has obtained second compression again, and chirp is carried out in annular chamber 45 (chirp) it compensates.Third Polarization Controller 27, Faraday isolator 26 and the 4th Polarization Controller 25 form a resonance Device forms equivalent saturable absorber using nonlinear polarization rotation, recycles the nonlinear birefringence effect in optical fiber It answers, ultrashort femtosecond laser pulse is generated based on the self-locking mode mechanism in nonlinear birefringence optical fiber, and make in annular chamber 45 For laser along one-way transmission, exporting high-power wavelength by the second Polarization Controller 31 is λ0Femtosecond pulsed laser to super continuous Spectrum generates and monitoring mould group 32;
Meanwhile the second semiconductor laser 40 in ring laser mould group 22, the wavelength of transmitting are λ1Continuous pumping swashs Light beam enters annular chamber 45 after 41 liang of equal parts of four-in-one photo-coupler with both direction, passes through the first wavelength division multiplexer respectively 24 and second after wavelength division multiplexer 29, pumps ytterbium doped optical fiber amplifier 28 from both direction.The wavelength that pumping source mould group 2 exports For λ1Nanosecond pulse seed laser carry out power amplification, while the nanosecond pulse laser by ytterbium doped optical fiber amplifier 28 The first negative GVD optical fiber 10 is first passed through, pulse is compressed, since ytterbium doped optical fiber amplifier 28 has positive GVD, so the nanosecond Pulse have passed through stretching, and after the second negative GVD optical fiber 23, pulse has obtained second compression again, and Zhou is carried out in annular chamber 45 Sing (chirp) compensation.Ultrashort femtosecond laser pulse is generated based on the self-locking mode mechanism in nonlinear birefringence optical fiber, and makes ring For laser in shape chamber 45 along one-way transmission, exporting high-power wavelength by the second Polarization Controller 31 is λ0Femtosecond pulse swash Light is to supercontinuum generation and monitors mould group 32;
Similarly, the third semiconductor laser 41 in same time, ring laser mould group 22, the wavelength of transmitting are λ2Continuous pump laser beam enters annular chamber 45 after 41 liang of equal parts of four-in-one photo-coupler with both direction, respectively by the After one wavelength division multiplexer 24 and the second wavelength division multiplexer 29, ytterbium doped optical fiber amplifier 28 is pumped from both direction.Pumping source mould The wavelength of 2 output of group is λ2Nanosecond pulse seed laser by ytterbium doped optical fiber amplifier 28 carry out power amplification, simultaneously should Nanosecond pulse laser first passes through the first negative GVD optical fiber 10, and pulse is compressed, since ytterbium doped optical fiber amplifier 28 has just GVD, so the nanosecond pulse have passed through stretching, after the second negative GVD optical fiber 23, pulse has obtained second compression again, in ring Chirp (chirp) compensation is carried out in shape chamber 45.Using the nonlinear birefringence effect in optical fiber, it is based on nonlinear birefringence optical fiber In self-locking mode mechanism generate ultrashort femtosecond laser pulse, and make the laser in annular chamber 45 along one-way transmission, pass through second It is λ that Polarization Controller 31, which exports high-power wavelength,2Femtosecond pulsed laser to supercontinuum generation and monitoring mould group 32;
(9) wavelength that ring laser mould group 22 exports is respectively λ0、λ1、λ2Femtosecond pulsed laser enter continuous spectrum Generate and monitoring mould group 32 in, after entering PCF 34 by PCF coupler 33, due to all types of non-thread of each rank in PCF34 Property effect, formed respectively with λ0、λ1、λ2Centered on spectrum widening, the width and intensity and λ of broadening0、λ1、λ2Femtosecond Pulsed laser power is directly proportional, and the spectrum of three broadenings is overlapped mutually, and forms femtosecond super continuous spectrums pulse laser, the present embodiment Middle super continuous spectrums range is 400nm-2500nm;
(10) femtosecond super continuous spectrums pulse laser is connect by output all the way by being divided into two-way after one-in-and-two-out optical fiber 35 Mouth 36 exports;Another way enters wide spectrum spectrometer 37 and is monitored, and super continuous spectrums monitoring result is sent to controller 1;
(11) controller 1 analyzes super continuous spectrums monitoring result, evaluates its spectrum flatness, while generating new needle To the first shaping amplifier 5, the second shaping amplifier 10, third shaping amplifier 15 amplification factor A1、A2、A3
(12) (5) to (11) constantly are repeated, until super continuous spectrums monitoring result meets flatness requirement.It so far, will be newest A1、A2、A3It is fixed, finally realize the super continuous spectrums laser of high output spectrum flatness and stability.

Claims (1)

1. a kind of super flat super continuous spectrums laser acquisition methods of femtosecond, this method is the super continuous spectrums in the output of super flat spectrum Realized on laser, the super continuous spectrums laser include controller (1), pumping source mould group (2), power governor (3), First impulse generator (4), the first shaping amplifier (5), first laser diode (6), the first field-effect tube (7), first Effect tube drive circuit (8), the second impulse generator (9), the second shaping amplifier (10), second laser diode (11);The Two field-effect tube (12), the second field-effect tube driving circuit (13), third impulse generator (14), third shaping amplifier (15), third field-effect tube driving circuit (16), third field-effect tube (17), third laser diode (18), three-in-one optical fiber (19), the first Polarization Controller (20), optoisolator (21), ring laser mould group (22), the first negative GVD optical fiber (23), One wavelength division multiplexer (24), Faraday isolator (26), third Polarization Controller (27), is mixed the 4th Polarization Controller (25) Ytterbium optical fiber amplifier (28), the second wavelength division multiplexer (29), the second negative GVD optical fiber (30), the second Polarization Controller (31), super company Continuous spectrum generates and monitoring mould group (32), PCF coupler (33), PCF (34), one-in-and-two-out optical fiber (35), output interface (36), width Spectral coverage spectrometer (37), four-in-one photo-coupler (38), the first semiconductor laser (39), the second semiconductor laser (40), Third semiconductor laser (41), first laser tube drive circuit (42), second laser tube drive circuit (43), third laser tube Driving circuit (44), annular chamber (45);It is characterized in that the super flat super continuous spectrums laser acquisition methods of femtosecond are as follows:
1) according to the zero-dispersion wavelength λ of PCF0, find out its corresponding frequency f0;Setpoint frequency difference Δ f, setpoint frequency f1=f0+Δ F finds out its corresponding wavelength X1;Similarly, setpoint frequency f2=f0Δ f finds out its corresponding wavelength X2
2) select the operation wavelength of first laser diode and the first semiconductor laser for λ0;Select second laser diode and The operation wavelength of second semiconductor laser is λ1;Select the operation wavelength of third laser diode and third semiconductor laser For λ2
3) controller issues control instruction to the first impulse generator, the second impulse generator and third impulse generator, by three The pulse frequency of person is set as identical value and is allowed to start work;
4) controller issues control instruction starting the first semiconductor laser, the second semiconductor laser, third semiconductor laser Device, wide spectrum spectrometer;
5) controller issues control instruction to power governor, and power governor amplifies the first shaping amplifier, the second shaping One identical initial value A of amplification factor setting of device, third shaping amplifier1=A2=A3
6) high frequency electric pulse that the first impulse generator issues carries out shaping pulse through the first shaping amplifier first, adjusts high electricity Flat duty ratio forms the high frequency electric pulse of nanosecond, then presses A1After multiple carries out power amplification, it is sent into the driving of first laser pipe The control pin of the field-effect tube driving chip in the first field-effect tube driving circuit in circuit, field-effect tube driving chip The nanosecond pulse signal that output pin generates high frequency is used to control the on and off of the first field-effect tube of high-speed high-power, uses Charge and discharge in control first laser diode discharge circuit make first laser diode generate the nanosecond pulse seed of high frequency Laser;
Similarly, the high frequency electric pulse that the second impulse generator issues carries out shaping pulse through the second shaping amplifier first, adjusts High level duty ratio is saved, the high frequency electric pulse of nanosecond is formed, then presses A2After multiple carries out power amplification, it is sent into second laser The control pin of the field-effect tube driving chip in the second field-effect tube driving circuit in tube drive circuit, field-effect tube driving The output pin of chip generates high frequency nanosecond pulse signal and is used to control the conducting of the second field-effect tube of high-speed high-power and cuts Only, for controlling the charge and discharge in second laser diode discharge circuit, second laser diode is made to generate high frequency nanosecond pulse Seed laser;
Similarly, the high frequency electric pulse that third impulse generator issues carries out shaping pulse through third shaping amplifier first, adjusts High level duty ratio is saved, the high frequency electric pulse of nanosecond is formed, then presses A3After multiple carries out power amplification, it is sent into third laser The control pin of the field-effect tube driving chip in third field-effect tube driving circuit in tube drive circuit, field-effect tube driving The nanosecond pulse signal that the output pin of chip generates high frequency be used to control high-speed high-power third field-effect tube conducting and Cut-off makes third laser diode generate the nanosecond of high frequency for controlling the charge and discharge of third laser diode discharge loop Pulse seed laser;
7) three beams wavelength is respectively λ0、λ1、λ2Pulse seed laser through in three-in-one fiber coupling entering light fibre, then partially through first Vibration controller and optoisolator are transferred into ring laser mould group;The effect of first Polarization Controller and optoisolator is to eliminate The issuable echo interference of ring laser mould group;
8) the first semiconductor laser in ring laser mould group, the wavelength of transmitting are λ0Continuous pump laser beam is closed by four Annular chamber is entered with both direction after one photo-coupler, two equal part, passes through the first wavelength division multiplexer and the second wavelength division multiplexer respectively Later, ytterbium doped optical fiber amplifier is pumped from both direction;The wavelength of pumping source mould group output is λ0Nanosecond pulse seed swash Light carries out power amplification by ytterbium doped optical fiber amplifier, while the nanosecond pulse laser first passes through the first negative GVD optical fiber, pulse It is compressed, since ytterbium doped optical fiber amplifier has positive GVD, so the nanosecond pulse have passed through stretching, it is negative using second After GVD optical fiber, pulse has obtained second compression again, and chirp (chirp) compensation is carried out in annular chamber;Third Polarization Controller, method Optoisolator and the 4th Polarization Controller is drawn to form a resonator, using nonlinear polarization rotation, formation is equivalent can Saturated absorbing body recycles the nonlinear birefringence effect in optical fiber, based on the self-locking mode mechanism in nonlinear birefringence optical fiber Ultrashort femtosecond laser pulse is generated, and makes the laser in annular chamber along one-way transmission, is exported by the second Polarization Controller big The a length of λ of power waves0Femtosecond pulsed laser to supercontinuum generation and monitoring mould group;
Meanwhile the second semiconductor laser in ring laser mould group, the wavelength of transmitting are λ1Continuous pump laser beam passes through four Annular chamber is entered with both direction after unification two equal part of photo-coupler, passes through the first wavelength division multiplexer and the second wavelength-division multiplex respectively After device, ytterbium doped optical fiber amplifier is pumped from both direction;The wavelength of pumping source mould group output is λ1Nanosecond pulse seed Laser carries out power amplification by ytterbium doped optical fiber amplifier, while the nanosecond pulse laser first passes through the first negative GVD optical fiber, arteries and veins Punching is compressed, since ytterbium doped optical fiber amplifier has positive GVD, so the nanosecond pulse have passed through stretching, using second After negative GVD optical fiber, pulse has obtained second compression again, and chirp compensation is carried out in annular chamber;Based in nonlinear birefringence optical fiber Self-locking mode mechanism generate ultrashort femtosecond laser pulse, and make the laser in annular chamber along one-way transmission, pass through the second polarization It is λ that controller, which exports high-power wavelength,1Femtosecond pulsed laser to supercontinuum generation and monitoring mould group;
Similarly, the third semiconductor laser in same time, ring laser mould group, the wavelength of transmitting are λ2Continuous pump Pu laser beam enters annular chamber after two equal part of four-in-one photo-coupler with both direction, passes through the first wavelength division multiplexer respectively After the second wavelength division multiplexer, ytterbium doped optical fiber amplifier is pumped from both direction;The wavelength of pumping source mould group output is λ2's Nanosecond pulse seed laser carries out power amplification by ytterbium doped optical fiber amplifier, while the nanosecond pulse laser first passes through the One negative GVD optical fiber, pulse are compressed, since ytterbium doped optical fiber amplifier has positive GVD, so the nanosecond pulse have passed through drawing It stretches, after the second negative GVD optical fiber, pulse has obtained second compression again, and chirp compensation is carried out in annular chamber;Using in optical fiber Nonlinear birefringence effect, ultrashort femtosecond laser pulse is generated based on the self-locking mode mechanism in nonlinear birefringence optical fiber, And make the laser in annular chamber along one-way transmission, exporting high-power wavelength by the second Polarization Controller is λ2Femtosecond pulse Laser is to supercontinuum generation and monitors mould group;
9) wavelength of ring laser mould group output is respectively λ0、λ1、λ2Femtosecond pulsed laser enter continuous spectrum generate and prison Survey in mould group, after entering PCF by PCF coupler, due to the nonlinear effect that each rank is all types of in PCF, formed respectively with λ0、λ1、λ2Centered on spectrum widening, the width and intensity and λ of broadening0、λ1、λ2Femtosecond pulsed laser power at just Than the spectrum of three broadenings is overlapped mutually, and forms femtosecond super continuous spectrums pulse laser;
10) femtosecond super continuous spectrums pulse laser is exported by output interface all the way by being divided into two-way after one-in-and-two-out optical fiber; Another way enters wide spectrum spectrometer and is monitored, and super continuous spectrums monitoring result is sent to controller;
11) controller analyzes super continuous spectrums monitoring result, evaluates its spectrum flatness, while generating and new being directed to first Shaping amplifier, the second shaping amplifier, third shaping amplifier amplification factor A1、A2、A3
12) step 5) is constantly repeated to 11), until super continuous spectrums monitoring result meets flatness requirement, so far, by newest A1、 A2、A3It is fixed, finally realize the super continuous spectrums laser of high output spectrum flatness and stability.
CN201610307174.1A 2016-05-11 2016-05-11 A kind of super flat super continuous spectrums laser acquisition methods of femtosecond Active CN105811227B (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
CN201610307174.1A CN105811227B (en) 2016-05-11 2016-05-11 A kind of super flat super continuous spectrums laser acquisition methods of femtosecond

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
CN201610307174.1A CN105811227B (en) 2016-05-11 2016-05-11 A kind of super flat super continuous spectrums laser acquisition methods of femtosecond

Publications (2)

Publication Number Publication Date
CN105811227A CN105811227A (en) 2016-07-27
CN105811227B true CN105811227B (en) 2019-04-02

Family

ID=56456606

Family Applications (1)

Application Number Title Priority Date Filing Date
CN201610307174.1A Active CN105811227B (en) 2016-05-11 2016-05-11 A kind of super flat super continuous spectrums laser acquisition methods of femtosecond

Country Status (1)

Country Link
CN (1) CN105811227B (en)

Families Citing this family (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN107248689B (en) * 2017-08-10 2018-05-25 珠海光恒科技有限公司 A kind of full multimode pumping double-cladding fiber amplifier of high-power narrow line width
CN117477329B (en) * 2023-12-20 2024-03-19 吉林省科英医疗激光有限责任公司 High-power semiconductor pumping fiber laser parallel driving power supply and control method thereof

Citations (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US20040032887A1 (en) * 2001-12-17 2004-02-19 Nima Ahmadvand system and method for generating multi-wavelength laser source using highly nonlinear fiber
CN103296569A (en) * 2013-06-25 2013-09-11 中国人民解放军国防科学技术大学 Super-continuum spectrum light source based on dual-band seed source Er-Yb co-doped optical fiber amplifier
CN104849257A (en) * 2015-06-02 2015-08-19 中国科学院上海技术物理研究所 Small ultraviolet frequency sweeping laser-based resonance Raman spectrum detection system and method
CN105048267A (en) * 2015-09-10 2015-11-11 电子科技大学 Intermediate infrared super-continuum spectrum laser light source

Family Cites Families (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP5029180B2 (en) * 2007-07-12 2012-09-19 住友電気工業株式会社 SC light source device

Patent Citations (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US20040032887A1 (en) * 2001-12-17 2004-02-19 Nima Ahmadvand system and method for generating multi-wavelength laser source using highly nonlinear fiber
CN103296569A (en) * 2013-06-25 2013-09-11 中国人民解放军国防科学技术大学 Super-continuum spectrum light source based on dual-band seed source Er-Yb co-doped optical fiber amplifier
CN104849257A (en) * 2015-06-02 2015-08-19 中国科学院上海技术物理研究所 Small ultraviolet frequency sweeping laser-based resonance Raman spectrum detection system and method
CN105048267A (en) * 2015-09-10 2015-11-11 电子科技大学 Intermediate infrared super-continuum spectrum laser light source

Non-Patent Citations (1)

* Cited by examiner, † Cited by third party
Title
基于双波长相干超短脉冲光源的超连续谱产生;李旻等;《光学学报》;20150430;第35卷(第4期);第0406001-1~7页 *

Also Published As

Publication number Publication date
CN105811227A (en) 2016-07-27

Similar Documents

Publication Publication Date Title
CN106716749B (en) Passive modelocked fiber ring generators
CN102545042B (en) Production method of optical microwave signal with tunable broadband frequency
CN107069410B (en) A kind of multipurpose bidirectional passive mode-locking full optical fiber laser system
CN102510001B (en) Frequency-doubling green light laser
CN103022873B (en) Ultrashort pulse generator based on double pump parametric process
CN103545703B (en) Light-operated trigger laser
CN101330191A (en) SF pulse optical fibre laser and method for generating SF pulse seeds laser
CN109713562A (en) Random fiber laser based on random Brillouin's dynamic raster
CN105811227B (en) A kind of super flat super continuous spectrums laser acquisition methods of femtosecond
CN102237633A (en) High-power narrow-pulse laser light source
CN106877121B (en) Pulse width tuning laser based on light-operated graphene Chirp Bragg grating
CN105759531B (en) A kind of super continuum source
CN105790073B (en) A kind of super continuous spectrums laser of flat spectrum output
CN102130413B (en) Full optical fiber type supercontinuum laser source based on multi-component-doped silica optical fiber
CN103904534B (en) All -fiber actively Qswitched laser based on saturable absorption optical fiber
CN105790053B (en) Infrared super continuous spectrums laser implementation method in a kind of output of flat spectrum
CN105762649B (en) Infrared super continuous spectrums laser in a kind of output of flat spectrum
CN102508388A (en) Optical fiber parameter amplifier
CN108923234B (en) Supercontinuum generating device
CN206412627U (en) Annular resonance intonation Q pulse MOPA optical fiber lasers
CN110061408A (en) It mixes the preparation of chromium selenizing zinc nanoparticles saturable absorber and its constitutes full optical fiber Q-switched laser
CN206412629U (en) The MOPA optical fiber lasers of adjustable pulse width
CN209200364U (en) Three colour synchronisation mode locked fiber lasers
CN109510057B (en) Method for generating 1-micron-waveband high-peak-power nanosecond pulse laser
CN102694577B (en) Method for generating pulse signal for ultra-wideband pulse signal device

Legal Events

Date Code Title Description
C06 Publication
PB01 Publication
C10 Entry into substantive examination
SE01 Entry into force of request for substantive examination
GR01 Patent grant
GR01 Patent grant