CN109687274A - A kind of all solid laser for lasing 350nm laser - Google Patents

A kind of all solid laser for lasing 350nm laser Download PDF

Info

Publication number
CN109687274A
CN109687274A CN201910047752.6A CN201910047752A CN109687274A CN 109687274 A CN109687274 A CN 109687274A CN 201910047752 A CN201910047752 A CN 201910047752A CN 109687274 A CN109687274 A CN 109687274A
Authority
CN
China
Prior art keywords
laser
mirror
wavelength
plano
concave mirror
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.)
Pending
Application number
CN201910047752.6A
Other languages
Chinese (zh)
Inventor
沈建平
王巍
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.)
Nanjing Post and Telecommunication University
Nanjing University of Posts and Telecommunications
Original Assignee
Nanjing Post and Telecommunication University
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 Nanjing Post and Telecommunication University filed Critical Nanjing Post and Telecommunication University
Priority to CN201910047752.6A priority Critical patent/CN109687274A/en
Publication of CN109687274A publication Critical patent/CN109687274A/en
Pending legal-status Critical Current

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
    • H01S3/08Construction or shape of optical resonators or components thereof
    • 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
    • H01S3/08Construction or shape of optical resonators or components thereof
    • H01S3/08059Constructional details of the reflector, e.g. shape
    • 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
    • H01S3/11Mode locking; Q-switching; Other giant-pulse techniques, e.g. cavity dumping

Landscapes

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

Abstract

The invention discloses a kind of all solid lasers for lasing 350nm laser, including the 966nmLD laser pump (ing) and fibre-coupled mirrors for generating laser source, fibre-coupled mirrors are used to integrate the hot spot that 966nmLD laser pump (ing) generates laser, laser further includes average mirror, plano-concave mirror and filter, and the YSGG crystal according to designated ratio mixed with Er is provided between average mirror and plano-concave mirror, average mirror, plano-concave mirror, YSGG crystal and filter are set gradually on the same axis;Average mirror peace concave mirror combines the resonant cavity to form laser, the plating film coefficient of average mirror are as follows: the transmitance that 350nm, 540nm~558nm, 650nm~675nm wavelength laser reflectivity are greater than 99.9% and 966nm wavelength laser is greater than 95%;Different plating film coefficients is arranged according to continuous and pulse output condition in plano-concave mirror;YSGG crystal is used as the gain media of laser;Filter is used to filter out all light emitted from laser outside 350nm wavelength laser;Overall structure of the present invention is simple, directly lasing can go out the laser of 350nm, and have good hot spot beam quality.

Description

A kind of all solid laser for lasing 350nm laser
Technical field
The invention belongs to optical device field more particularly to laser devices, and in particular to one kind swashs for lasing 350nm The all solid laser of light.
Background technique
Solid ultraviolet laser by pump mode be divided into xenon flash lamp pumping ultraviolet laser, krypton flashlamp-pumped ultraviolet laser and Novel laser diode pumping full-solid laser.But the outer laser optical photoelectric transformation efficiency of solid violet is generally lower, purple light two When pole pipe develops to shorter wavelength, new difficulty can be brought in terms of photon limitation, non-radiative processes, maintenance Topic.There are two types of the method that full solid state ultraviolet laser spectral line generates is general, first is that directly being carried out to infrared all solid laser intracavitary Or outer 3 frequencys multiplication of chamber or 4 frequencys multiplication obtain ultraviolet laser spectral line;It is then recycled second is that obtaining second harmonic first with frequency doubling technology Ultraviolet laser spectral line is obtained with frequency technology.
Gas laser includes the excimer laser to work in a pulsed fashion, the ion laser to work in a continuous manner With He-Cd and metal vapors ultraviolet laser.The wavelength of gas ultraviolet laser is mixed dependent on used gas Polymer type.Metal vapors ultraviolet laser refers mainly to copper steam ultraviolet laser, its generation wavelength is 511nm's and 578nm Light then can produce the ultraviolet radioactive that wavelength is 255nm, 271nm and 289nm using mixing and frequency multiplication.Laser beam distribution clothes From Gaussian Profile.Outstanding problem in gas laser application is that occupation area of equipment big, limited reliability, service life be short, high energy Consumption and high cost.Moreover, excimer pulsed laser beam is of poor quality, exposure mask loss is big.There are light for ion laser and He-Cd The disadvantage of beam directional stability difference.
Middle ultraviolet band is the emphasis direction of ALGaN laser diode development;Because the excitation of the wave band ultraviolet radioactive is imitated Rate highest, delivery efficiency are also relatively high.In order to keep UV ray radiation source more practical, the ultraviolet diode development of semiconductor One direction is the volume and power consumption for substantially reducing existing ultraviolet laser and its power supply, another direction is exploitation launch wavelength For 280nm, power consumption less than 10mW light emitting diode and launch wavelength be 340nm, power consumption be less than 25mW laser diode
In summary, existing ultraviolet wavelength solid state laser or gas laser have that the device is complicated degree are higher, Sufficiently bulky, expensive problem;But with the development of technology, for the heterogeneous of the semiconductor laser complexity of ultraviolet wavelength Junction structure and very high current density propose very high requirement to semiconductor material, and current ultraviolet semiconductor laser can only Reach 370nm and power be not it is especially high, be unable to satisfy requirement.
Summary of the invention
The high, body for the above-mentioned solid state laser of ultraviolet wavelength in the prior art and gas laser integral device complexity Product is big, expensive, and the optical maser wavelength the problem of being unable to satisfy existing generation demand generated, and the present invention is in proposing one kind All solid laser for lasing 350nm laser;The all solid laser is gone out using the very simple direct lasing of device 350nm in turn avoids swashing as current solid state laser and gas with the preferable hot spot beam quality that solid state laser possesses Light device the device is complicated the high and sufficiently bulky problem of degree, specific technical solution are as follows:
A kind of all solid laser for lasing 350nm laser, the laser include for generating laser source 966nmLD laser pump (ing) and the 966nmLD laser pump (ing) output end and coaxial fibre-coupled mirrors are installed in, the optical fiber coupling Close mirror and be used to integrate the hot spot that the 966nmLD laser pump (ing) generates laser, the laser further include average mirror, plano-concave mirror and Filter, and it is provided between the average mirror and the plano-concave mirror YSGG crystal according to designated ratio mixed with Er, it is described flat Flat mirror, plano-concave mirror, YSGG crystal and filter are set gradually on the same axis;Wherein, the average mirror peace concave mirror combines shape At the resonant cavity of laser, the plating film coefficient of the average mirror are as follows: 350nm, 540nm~558nm, 650nm~675nm wavelength swash The transmitance that light reflectivity is greater than 99.9% and 966nm wavelength laser is greater than 95%;The plating film coefficient of the plano-concave mirror are as follows: 350nm wavelength laser transmitance is 20%, the transmitance of 558nm wavelength laser is 3% and the transmitance of 675nm wavelength laser is 2%;The YSGG crystal is used as the gain media of laser;The filter be used for filter out outside 350nm wavelength laser it is all from The light that laser emits.
Further, under pulse output condition, the laser is arranged between the average mirror and the plano-concave mirror There are an aperture and passive Q-switch, the average mirror, aperture, passive Q-switch and the plano-concave mirror are coaxially disposed, and The passive Q-switch is between the aperture and the plano-concave mirror, wherein the average mirror peace concave mirror combines to be formed The resonant cavity of laser, to provide feedback energy and specified wavelength and the light of frequency selected to penetrate, the plated film of the average mirror Coefficient are as follows: 350nm, 540nm~558nm, 650nm~675nm wavelength laser reflectivity swash greater than 99.9% and 966nm wavelength The transmitance of light is greater than 95%, the plating film coefficient of the plano-concave mirror are as follows: 350nm wavelength laser transmitance is 50%, 558nm wavelength The transmitance of laser is 3% and the transmitance of 675nm wavelength laser is 2% and the transmitance of 966nm wavelength laser is greater than 95%, the aperture for filtering in the resonant cavity high-order mode of light beam and to beam shaping, use by the passive Q-switch The peak work of the light beam is promoted in the quality factor Q for controlling the resonant cavity to realize the compression to the beam energy Rate.
Further, the passive Q-switch include one with BK7 material preparation substrate and be covered on the substrate by MoS2The film of composition forms, wherein the film is arranged close to the aperture.
Further, the Er that the YSGG crystal is mixed is Er3+Ion, and the Er3+The concentration of ion is 35%.
Further, the output end of the 966nmLD laser pump (ing) is additionally provided with an optical-fiber coupling connector, for described Being flexibly connected between laser and the fibre-coupled mirrors occurs for 966nmLD laser pump (ing).
Further, the average mirror and the plano-concave mirror are the setting of two sides plated film.
Compared with prior art, all solid laser for lasing 350nm laser of the invention have the beneficial effect that it is whole Body structure is simple, avoids current solid state laser and gas laser the device is complicated that degree is high and sufficiently bulky problem, and Higher power output can be used;Meanwhile directly lasing can go out the laser of 350nm, there is good hot spot beam quality.
Detailed description of the invention
Fig. 1 is the structure composition figure signal described in present example for all solid laser of lasing 350nm laser.
Identifier declaration: 1-966nmLD laser pump (ing), 2- optical-fiber coupling connector, 3- fibre-coupled mirrors, the average mirror of 4-, 5- First plano-concave mirror, 6- filter, 7- thin plate, 8- passive Q-switch, 9- the second plano-concave mirror.
Specific embodiment
In order to enable those skilled in the art to better understand the solution of the present invention, below in conjunction in the embodiment of the present invention Attached drawing, technical scheme in the embodiment of the invention is clearly and completely described.
In embodiments of the present invention, a kind of all solid laser for lasing 350nm laser is provided, can be used for realizing Continuous and pulse 350nm laser output;Specifically, the part a in refering to fig. 1, the laser for the output of continuous 350nm laser Including the 966nmLD laser pump (ing) 1 for generating laser source and it is installed in 1 output end of 966nmLD laser pump (ing) and coaxial light Fine coupling mirror 3, fibre-coupled mirrors 3 are used to integrate the hot spot that 966nmLD laser pump (ing) 1 generates laser, and laser further includes average Mirror 4, the first plano-concave mirror 5 and filter 6, and be provided with according to designated ratio between average mirror 4 and the first plano-concave mirror 5 mixed with 35% Er3+YSGG crystal, average mirror 4, YSGG crystal, the first plano-concave mirror 5 and filter 6 are set gradually on the same axis;Wherein, just In the case where normal continuous-wave lasing laser, the plating film coefficient of average mirror are as follows: 350nm, 540nm~558nm and 650nm~675nm wave The reflectivity of long laser is greater than 99.9%, and 966nm wavelength laser transmitance is greater than 95% setting, the plating film coefficient of plano-concave mirror Are as follows: 350nm wavelength laser transmitance is 20%, the transmitance of 558nm wavelength laser is 3% and the transmission of 675nm wavelength laser Rate is that 2% and 966nm wavelength laser transmitance is greater than 95% setting.
Referring again to the part b in Fig. 1, in the specific embodiment of the invention, using laser of the invention when in impulsive condition When lower generation 350nm laser exports, plating film coefficient is used are as follows: 350nm wavelength laser transmitance is 50%, 558nm wavelength laser Transmitance be 3% and the transmitance of 675nm wavelength laser is 2% and 966nm wavelength transmitance is 95% the second plano-concave Mirror 9 is realized, wherein is provided with an aperture 7 and passive Q-switch 8 between average mirror 4 and the second plano-concave mirror 9, wherein Aperture 7, passive Q-switch 9 and the second plano-concave mirror 9 are coaxially disposed, and passive Q-switch 8 is located at aperture 7 and the second plano-concave Between mirror 9;Meanwhile passive Q-switch 8 include one with BK7 material preparation substrate and be covered on substrate by with a thickness of 1.8nm- The few layer of MoS of 3.7nm2The film of composition forms, and film is located between aperture 7 and the second plano-concave mirror 9 and close to aperture Diaphragm 7 is arranged.
In embodiments of the present invention, in the case where 966nmLD laser pump (ing) continuously exports laser, 540nm~558nm wave Long laser is issued by YSGG crystal;Likewise, 975nm~1000nm wavelength laser is also obtained by YSGG crystal lasing;And 340nm ~350nm light occur in crystal and frequency generate, and wavelength be 350nm be most strong light;And average mirror peace concave mirror is as sharp The resonant cavity of light device, gain media of the present invention by the YSGG crystal mixed with Er as laser, to realize population inversion With the necessary condition for manufacturing the output of 350nm laser with frequency, emit energy and the choosing of light beam come feedback laser by resonant cavity The wave for selecting permeable wavelength and frequency filters out the light emitted other than 350nm from laser finally by filter, realizes The continuous output of 350nm laser.
Under 966nmLD laser pump (ing) pulse output condition, the high-order of resonance intracavity beam is filtered out by aperture Mould simultaneously carries out shaping to light beam, meanwhile, in conjunction with passive Q-switch;Specifically, passive Q-switch is because of MoS2Film possesses can be " full With " and " bleaching " saturated absorbing body characteristic as influence laser cavity quality factor Q value can make it is continuous by what is generally exported Laser energy, which is compressed in the extremely narrow pulse of width, to be emitted, to make the peak power of light source that several orders of magnitude can be improved;Finally The continuous output of 350nm laser is realized by plano-concave mirror and filter, wherein filter is 350nm laser filter, last real to guarantee Now the light beam in addition to 350nm wavelength laser without other wavelength is penetrated from filter 6.
Preferably, under pulse output condition, in order to allow intracavitary 350nm light to generate oscillation and the arteries and veins exported will not be made Punching causes to export pulse energy decline because transmitance is too low, and the transmitance to plano-concave mirror in 350nm wavelength laser is arranged It is 50%.
In addition, in the present invention, the output end of 966nmLD laser pump (ing) 1 is additionally provided with an optical-fiber coupling connector 2, use Being flexibly connected between laser and fibre-coupled mirrors 3 occurs in 966nmLD laser pump (ing);Preferably, average 4 He of mirror in the present invention First plano-concave mirror 5 and the second plano-concave mirror 9 are the setting of two sides plated film.
Compared with prior art, all solid laser for lasing 350nm laser of the invention have the beneficial effect that it is whole Body structure is simple, avoids current solid state laser and gas laser the device is complicated that degree is high and sufficiently bulky problem, and Higher power output can be used;Meanwhile directly lasing can go out the laser of 350nm, there is good hot spot beam quality.
The foregoing is merely a prefered embodiment of the invention, is not intended to limit the scope of the patents of the invention, although referring to aforementioned reality Applying example, invention is explained in detail, still can be to aforementioned each tool for coming for those skilled in the art Technical solution documented by body embodiment is modified, or carries out equivalence replacement to part of technical characteristic.All benefits The equivalent structure made of description of the invention and accompanying drawing content is directly or indirectly used in other related technical areas, Similarly within the invention patent protection scope.

Claims (6)

1. a kind of all solid laser for lasing 350nm laser, the laser include for generating laser source 966nmLD laser pump (ing) and the 966nmLD laser pump (ing) output end and coaxial fibre-coupled mirrors are installed in, the optical fiber coupling It closes mirror and is used to integrate the hot spot that the 966nmLD laser pump (ing) generates laser, which is characterized in that the laser further includes average Mirror, plano-concave mirror and filter, and it is provided between the average mirror and the plano-concave mirror YSGG according to designated ratio mixed with Er Crystal, the average mirror, plano-concave mirror, YSGG crystal and filter are set gradually on the same axis;Wherein, the average mirror peace Concave mirror combines the resonant cavity to form laser, the plating film coefficient of the average mirror are as follows: and 350nm, 540nm~558nm, 650nm~ The transmitance that 675nm wavelength laser reflectivity is greater than 99.9% and 966nm wavelength laser is greater than 95%;The plano-concave mirror Plate film coefficient are as follows: 350nm wavelength laser transmitance is 20%, the transmitance of 558nm wavelength laser is 3% and 675nm wavelength swashs The transmitance of light is 2%;The YSGG crystal is used as the gain media of laser;The filter swashs for filtering out 350nm wavelength All light emitted from laser outside light.
2. being used for all solid laser of lasing 350nm laser as described in claim 1, which is characterized in that exported in pulse Under the conditions of, the laser is provided with an aperture and passive Q-switch between the average mirror and the plano-concave mirror, described Average mirror, aperture, passive Q-switch and the plano-concave mirror are coaxially disposed, and the passive Q-switch is located at the aperture Between the plano-concave mirror, wherein the average mirror peace concave mirror combines the resonant cavity to form laser, to provide feedback energy Measure and select specified wavelength and the light of frequency to penetrate, the plating film coefficient of the average mirror are as follows: 350nm, 540nm~558nm, The transmitance that 650nm~675nm wavelength laser reflectivity is greater than 99.9% and 966nm wavelength laser is greater than 95%, described flat The plating film coefficient of concave mirror are as follows: 350nm wavelength laser transmitance is 50%, the transmitance of 558nm wavelength laser is 3% and 675nm The transmitance of wavelength laser is that the transmitance of 2% and 966nm wavelength laser is greater than 95%, and the aperture is for filtering The high-order mode of light beam and to beam shaping in the resonant cavity, the passive Q-switch be used to control the quality of the resonant cavity because Plain Q promotes the peak power of the light beam to realize the compression to the beam energy.
3. being used for all solid laser of lasing 350nm laser as claimed in claim 2, which is characterized in that the passive Q is opened Close include one with BK7 material preparation substrate and be covered on the substrate by MoS2The film of composition forms, wherein described thin Film is arranged close to the aperture.
4. being used for all solid laser of lasing 350nm laser as described in claim 1, which is characterized in that the YSGG is brilliant The Er that body is mixed is Er3+Ion, and the Er3+The concentration of ion is 35%.
5. being used for all solid laser of lasing 350nm laser as described in claim 1, which is characterized in that the 966nmLD The output end of laser pump (ing) is additionally provided with an optical-fiber coupling connector, and laser and institute occurs for the 966nmLD laser pump (ing) State the flexible connection between fibre-coupled mirrors.
6. all solid laser as claimed in any one of claims 1 to 5 for lasing 350nm laser, which is characterized in that institute It states average mirror and the plano-concave mirror is the setting of two sides plated film.
CN201910047752.6A 2019-01-18 2019-01-18 A kind of all solid laser for lasing 350nm laser Pending CN109687274A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
CN201910047752.6A CN109687274A (en) 2019-01-18 2019-01-18 A kind of all solid laser for lasing 350nm laser

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
CN201910047752.6A CN109687274A (en) 2019-01-18 2019-01-18 A kind of all solid laser for lasing 350nm laser

Publications (1)

Publication Number Publication Date
CN109687274A true CN109687274A (en) 2019-04-26

Family

ID=66193717

Family Applications (1)

Application Number Title Priority Date Filing Date
CN201910047752.6A Pending CN109687274A (en) 2019-01-18 2019-01-18 A kind of all solid laser for lasing 350nm laser

Country Status (1)

Country Link
CN (1) CN109687274A (en)

Citations (5)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US5276695A (en) * 1992-10-26 1994-01-04 The United States Of America As Represented By The Secretary Of The Navy Multifrequency, rapidly sequenced or simultaneous tunable laser
CN1754290A (en) * 2003-05-02 2006-03-29 光波电子公司 Laser resistant to internal ir-induced damage
CN106816807A (en) * 2017-03-30 2017-06-09 华中科技大学 Optical fiber laser as pumping source intracavity pump optical parametric oscillator
CN107394577A (en) * 2017-08-16 2017-11-24 中国科学院福建物质结构研究所 Infrared all solid state laser in one kind
CN107419334A (en) * 2017-08-10 2017-12-01 中国科学院福建物质结构研究所 A kind of crystalline material, its preparation method and the application as laser crystal

Patent Citations (5)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US5276695A (en) * 1992-10-26 1994-01-04 The United States Of America As Represented By The Secretary Of The Navy Multifrequency, rapidly sequenced or simultaneous tunable laser
CN1754290A (en) * 2003-05-02 2006-03-29 光波电子公司 Laser resistant to internal ir-induced damage
CN106816807A (en) * 2017-03-30 2017-06-09 华中科技大学 Optical fiber laser as pumping source intracavity pump optical parametric oscillator
CN107419334A (en) * 2017-08-10 2017-12-01 中国科学院福建物质结构研究所 A kind of crystalline material, its preparation method and the application as laser crystal
CN107394577A (en) * 2017-08-16 2017-11-24 中国科学院福建物质结构研究所 Infrared all solid state laser in one kind

Non-Patent Citations (2)

* Cited by examiner, † Cited by third party
Title
HONGKUN NIE等: ""Highly Efficient Continuous-Wave and Passively Q-Switching 2.8 um Er:YSGG Laser"", 《IEEE PHOTONICS TECHNOLOGY LETTERS》 *
P.A.LOIKO等: ""Judd-Ofelt analysis and stimulated-emission cross-sections for highly doed(38 at%) Er:YSGG laser cystal"", 《JOUNAL OF LUMINESCENCE》 *

Similar Documents

Publication Publication Date Title
JPH01502309A (en) Fixed wavelength laser light source
CN107482425A (en) A kind of Gao Zhongying, single longitudinal mode, narrow spaces 2.79um laser pumping source
CN110061412A (en) A kind of ultraviolet solid-state laser apparatus suitable for optic communication
CN103346472A (en) 100MHz high repetition frequency, 1ns narrow pulse width narrow line width laser mixing amplifying device and method
CN102299475B (en) Narrow-linewidth single-transverse mode hundred watt level 2 micron thulium doped fiber laser with all-fiber structure
CN110165528B (en) Multi-wavelength same-repetition-frequency and repetition-frequency-controllable mid-infrared all-fiber laser
CN110474228A (en) A kind of perovskite quantum dot devitrified glass is the laser of gain media
CA1297935C (en) Wavelength locked dye lazer with transverse pumping
CN206412627U (en) Annular resonance intonation Q pulse MOPA optical fiber lasers
CN106058632B (en) A kind of adjustable passive Q-adjusted raman laser system of pulse energy based on bonded crystals
CN111313216A (en) Method for suppressing intensity noise of high-power continuous wave single-frequency laser
CN109687274A (en) A kind of all solid laser for lasing 350nm laser
CN115764544B (en) High side mode rejection ratio narrow linewidth external cavity laser and optical equipment
CN116435863A (en) Sodium guide star laser
CN109687276A (en) The gain switch laser of thulium-doped fiber laser pumping
CN211238802U (en) Final amplifier and optical fiber laser output device
CN209133829U (en) A kind of optical fiber laser
CN113270785A (en) Continuous wave 1.5 mu m human eye safety all-solid-state self-Raman laser
CN108988115B (en) Novel same-threshold equivalent dual-waveband intermediate infrared pulse laser and laser output method
CN109494556A (en) A kind of all solid laser of dichromatism visible light red for lasing, green
CN105305218A (en) All solid state laser
CN102185237A (en) High-power and 1,319 nm single-wavelength continuous laser device
CN106941239B (en) Laser-doubled efficiency-adjusted method
CN213989551U (en) Q-switched microchip laser using light-operated switch
CN2711952Y (en) Three-mirror resonant cavity laser for sum-frequency in semiconductor laser pump cavity

Legal Events

Date Code Title Description
PB01 Publication
PB01 Publication
SE01 Entry into force of request for substantive examination
SE01 Entry into force of request for substantive examination
RJ01 Rejection of invention patent application after publication
RJ01 Rejection of invention patent application after publication

Application publication date: 20190426