CN103944049A - Miniature three-endoscope ring cavity mid-infrared optical parametric oscillator - Google Patents

Miniature three-endoscope ring cavity mid-infrared optical parametric oscillator Download PDF

Info

Publication number
CN103944049A
CN103944049A CN201410114460.7A CN201410114460A CN103944049A CN 103944049 A CN103944049 A CN 103944049A CN 201410114460 A CN201410114460 A CN 201410114460A CN 103944049 A CN103944049 A CN 103944049A
Authority
CN
China
Prior art keywords
opo
coupled lens
mirror
annular chamber
laser
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.)
Granted
Application number
CN201410114460.7A
Other languages
Chinese (zh)
Other versions
CN103944049B (en
Inventor
张凯
彭跃峰
魏星斌
罗兴旺
彭珏
高剑蓉
李德明
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.)
Beijing Huayu Dexin Photoelectric Technology Co Ltd
Original Assignee
Institute of Applied Electronics of CAEP
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 Institute of Applied Electronics of CAEP filed Critical Institute of Applied Electronics of CAEP
Priority to CN201410114460.7A priority Critical patent/CN103944049B/en
Publication of CN103944049A publication Critical patent/CN103944049A/en
Application granted granted Critical
Publication of CN103944049B publication Critical patent/CN103944049B/en
Active legal-status Critical Current
Anticipated expiration legal-status Critical

Links

Landscapes

  • Optical Modulation, Optical Deflection, Nonlinear Optics, Optical Demodulation, Optical Logic Elements (AREA)
  • Lasers (AREA)

Abstract

The invention provides a miniature three-endoscope ring cavity mid-infrared optical parametric oscillator. According to the technical scheme, the three- endoscope ring cavity structure is adopted, the inverse transformation effect is reduced, transformation efficiency is improved, system isolation is avoided, and the size of an OPO system is reduced. Compared with a four-endoscope ring cavity OPO, the three-endoscope ring cavity OPO reduces the light outlet threshold of a laser device, transformation efficiency is improved, the complexity of a ring cavity is reduced, reliability of the OPO system is improved, and the size and the weight of the OPO system are reduced at the same time.

Description

A kind of miniaturization three chamber mirror annular chamber mid-infrared parameter oscillator
Technical field
What the present invention relates to is laser technique, especially a kind of miniaturization three chamber mirror annular chamber mid-infrared parameter oscillator.
Background technology
In the prior art, known technology is that the mid-infrared laser of 3-5 μ m is widely used in national defence, scientific research and the civil areas such as electrooptical countermeasures, atmospheric monitoring, Molecular Spectroscopy, laser medicine.Along with the continuous expansion of application and deeply, having infrared solid laser in certain power level, tunable, miniaturization receives much concern in recent years.Optical parametric oscillator (OPO) based on frequency translation is one of effective way producing high power, tunable mid-infrared laser.
OPO system is mainly made up of pump laser, coupling shielding system, nonlinear crystal resonant cavity mirror.And OPO is only made up of nonlinear crystal and chamber mirror, it is simple in structure, compact, is very beneficial for developing to miniaturization.But its pump laser is relative complex and huge but, be difficult to and OPO integration realization integral miniaturization.Along with the development of 1 μ m and 2 μ m Fiber laser technologies, in the miniaturization of infrared OPO another kind of thinking is provided, be about to separate with OPO as the fiber laser of pumping source integrated, thereby realize the miniaturization of OPO.
In line chamber OPO, in order to reduce the conversion efficiency of threshold value, raising pump light, outgoing mirror, conventionally to pumping laser reflection, comes and goes pumping laser and passes through nonlinear crystal.But in order to prevent the impact of light echo on pump laser, must between pump laser and OPO, add shielding system.This will increase the weight and volume of OPO, and the complexity of system.Especially, in the time that OPO is near degeneracy wavelength, will there is serious inverse conversion effect in line chamber OPO, reduces the conversion efficiency of pump light.
In order to reduce inverse conversion effect, avoid the impact of light echo on pumping laser, proposed to adopt the mentality of designing of annular chamber in miniaturization OPO.And the proposition of miniaturization OPO to volume, weight and reliability aspect strict demand, four common chamber mirror annular chambers (rectangle or X-type) are also not exclusively suitable for, and need be optimized design for miniaturization specially, this is the existing weak point of prior art.
Summary of the invention
Object of the present invention, be exactly for the existing deficiency of prior art, and provide a kind of technical scheme of miniaturization three chamber mirror annular chamber mid-infrared parameter oscillator, this scheme can realize OPO miniaturization, the photo threshold that goes out that has reduced laser, has improved conversion efficiency, has reduced the complexity of annular chamber, improve the reliability of OPO system, reduced the volume and weight of OPO system simultaneously.
This programme is achieved by the following technical measures: a kind of miniaturization three chamber mirror annular chamber mid-infrared parameter oscillator, include fiber laser and OPO system shell as OPO pumping source, in OPO system shell, include pumping coupling system and OPO annular chamber; In pumping coupling system, be provided with front coupled lens and rear coupled lens; In OPO annular chamber, be provided with OPO speculum, OPO total reflective mirror, OPO outgoing mirror and nonlinear crystal; The laser beam that fiber laser sends is successively through entering OPO annular chamber after front coupled lens and rear coupled lens; Laser beam penetrates through after OPO total reflective mirror, nonlinear crystal and OPO outgoing mirror after entering OPO annular chamber successively; When laser beam passes OPO outgoing mirror, a part of laser beam is reflexed to OPO speculum by OPO outgoing mirror and after OPO speculum reflexes to OPO total reflective mirror, reflexes to nonlinear crystal through OPO total reflective mirror again.
As this programme preferably: the fibre core size that front coupled lens and the ratio of rear coupled lens focal length are laser beam and expect the ratio of waist spot size.
As this programme preferably: the distance between front coupled lens and fiber laser equals the focal length of front coupled lens.
As this programme preferably: front coupled lens and rear coupled lens are coaxially placed, and described nonlinear crystal is placed in the focal position of rear coupled lens.
As this programme preferably: by adjusting distance energy coarse adjustment laser between front coupled lens and fiber-optic output by waist spot position and size after pumping coupling system; Can finely tune waist spot position and size by the relative distance of adjusting between front coupled lens and rear coupled lens.
As this programme preferably: front coupled lens and rear coupled lens select the convex lens of two short focal lengths to combine.
This programme is according to parameters such as the numerical aperture of fiber laser and fibre core sizes, multiple different short focal length lens combinations are carried out to simulation calculation and optimization design, under the prerequisite that meets the condition of debuging, shorten as far as possible the distance of two eyeglass spacing and rear coupled lens and waist spot position, and obtain suitable waist spot size to optimize pump power density, in avoiding lens lesion, improve conversion efficiency.In specific implementation process, the ratio of selecting two lump coke distances is actual fibre core size and expect the short focal length lens of ratio of waist spot size, when distance between front coupled lens and fiber-optic output is its focal length size, change two lens relative distances less on the waist spot size and location impact by after coupled system, therefore by compact as far as possible two lens coaxial placement, nonlinear crystal is placed in rear coupled lens focal position, should be noted that the chamber mirror that rear coupled lens focal length is greater than an angled placement debugs Len req.When dwindling distance between front coupled lens and fiber-optic output while making it be less than front coupled lens focal length, by the waist spot position after coupled system from lens more away from, waist spot is larger; When distance between current coupled lens and fiber-optic output is greater than its focal length, by the waist spot position after coupled system from lens more close to, waist spot is less, by adjusting two lens relative distance fine-tuning waist spot positions and size.
The beneficial effect of this programme can be learnt according to the narration to such scheme, owing in this scheme, the fiber laser as pumping source being separated with OPO, realized the miniaturization of OPO, the OPO system after integrated vanning only includes coupled system and the OPO annular chamber of lens composition; Optimize pumping coupling system, adopt two short focus lens combinations, by optimizing focal length and the relative distance of two lens, the spot size of pumping laser, beam waist position, the angle of divergence etc. are realized to optimum Match in OPO annular chamber, then realize modularization clamping, improve the reliability of OPO system; Adopt three chamber mirror ring cavity structures, reduce inverse conversion effect, improve conversion efficiency, avoid shielding system, reduce the volume of OPO system.Compared with four chamber mirror OPO annular chambers, three chamber mirror OPO annular chambers have reduced the photo threshold that of laser, have improved conversion efficiency, have reduced the complexity of annular chamber, have improved the reliability of OPO system, have reduced the volume and weight of OPO system simultaneously.
As can be seen here, the present invention compared with prior art, has outstanding substantive distinguishing features and progressive significantly, and the beneficial effect of its enforcement is also apparent.
Brief description of the drawings
Fig. 1 is the structural representation of the specific embodiment of the invention.
In figure, 1 is fiber laser, and 2 is front coupled lens, and 3 is rear coupled lens, and 4 is OPO speculum, and 5 is OPO annular chamber, and 6 is OPO system shell, and 7 is OPO outgoing mirror, and 8 is nonlinear crystal, and 9 is OPO total reflective mirror, and 10 is pumping coupling system.
Embodiment
For clearly demonstrating the technical characterstic of this programme, below by an embodiment, and in conjunction with its accompanying drawing, this programme is set forth.
Miniaturization three chamber mirror annular chamber mid-infrared parameter oscillator provided by the invention comprise: as the fiber laser 1 of pumping source, front coupled lens 2, rear coupled lens 3, OPO speculum 4, OPO total reflective mirror 9, OPO outgoing mirror 7, nonlinear crystal 8, pumping coupling system 10, annular chamber OPO5, OPO system shell 6.Pumping coupling system 10 is by front coupled lens 2, and rear coupled lens 3 forms, and their focal length and relative position all pass through strict setting, and in order to reduce system bulk, the length of pumping coupling system 10 reduces as far as possible.Annular chamber OPO5 is by OPO speculum 4, OPO total reflective mirror 9, and OPO outgoing mirror 7, nonlinear crystal 8 forms, OPO speculum 4, OPO total reflective mirror 9, the relative position of OPO outgoing mirror 7 and angle will be adjusted according to concrete execution mode.
Embodiment one:
Fiber laser 1 as pumping source adopts 2mm pulse optical fiber, and repetition rate is that 1-100kHz is adjustable, and pulse duration hundred nanosecond adopt polarization maintaining optical fibre to realize linear polarization output, to reach the phase-matching condition of OPO.
Pumping coupling system 10 is realized the 2mm pulse laser of fiber laser output is collimated and expanded, front coupled lens 2, the two-sided anti-reflection film that is all coated with 2mm of rear coupled lens 3.
Nonlinear crystal 8 in annular chamber OPO5 adopts two ZGP crystal (ZnGeP2 that optical axis direction is staggered relatively, phosphorus germanium zinc), with walking from compensation under compensated birefringence phase matched, increase the gain length of optical parameter conversion simultaneously, reduce and photo threshold, improve conversion efficiency.OPO total reflective mirror 9 has high-transmission rate to 2mm laser, and near laser 4mm is had to high reflectance, angled placement.OPO speculum 4 has high reflectance near laser 4mm, becomes level angle to place.OPO outgoing mirror 7 has high-transmission rate to 2mm laser, and near laser 4mm is had to partial reflectance, angled placement.By adjusting OPO speculum 4, OPO total reflective mirror 9, the relative position of OPO outgoing mirror 7 and angle, realize the high-efficiency operation of three chamber mirror annular chamber OPO.By changing angle and the working temperature of ZGP crystal, can realize the tuning of 3 ~ 5mm wave band.In the laser of annular chamber OPO5 output, comprise near the laser of 4mm that optical parameter conversion produces, and remaining non-switched 2 pumping lasers.
After the system integration, the volume of OPO system shell 6 can be controlled in 80mm × 80mm × 220mm, and weight is less than 2.5kg, and two waveband power output reaches tens of watts.
Embodiment two:
In conjunction with Fig. 1, present embodiment is described, difference described in present embodiment and execution mode one is, nonlinear crystal adopts PPLN crystal (Periodically Poled Lithium Niobate, periodically poled lithium niobate), two logical light faces of crystal are coated with the anti-reflection film of pumping laser and parameter laser.Because PPLN crystal is based on accurate phase matched, there is not walk-off effect, therefore do not need bicrystal to walk from compensation.By polarization cycle (monocycle, multicycle, fan-shaped cycle, mixing cycle), incident angle and the working temperature (room temperature to 200 DEG C conventionally) etc. of design PPLN crystal, absorb in cut-off wave band meeting phase-matching condition and PPLN, can realize near the continuous precise of 1 ~ 4mm tuning, and be expected to realize the even mid-infrared laser output of super continuous spectrums of multiband (>=2).
Embodiment three:
In conjunction with Fig. 1, present embodiment is described, difference described in present embodiment and execution mode two is, fiber laser 1 as pumping source adopts 1mm pulse optical fiber, similar in the parameters such as repetition rate, pulse duration, beam quality and execution mode one.Front coupled lens 2 in pumping coupling system 10, the two-sided anti-reflection film that is all coated with 1mm of rear coupled lens 3.OPO total reflective mirror 9 has high-transmission rate to 1mm laser, near infrared signal light and in infrared ideler frequency light there is high reflectance, angled placement.OPO speculum 4 near infrared signal light and in infrared ideler frequency light there is high reflectance, become level angle place.OPO outgoing mirror 7 has high-transmission rate to 1mm laser, near infrared signal light and in wherein a kind of laser of infrared ideler frequency light there is high-transmission rate, another kind of laser has part reflection, or two kinds of laser are all had to part reflection, angled placement.By adjusting OPO speculum 4, OPO total reflective mirror 9, the relative position of OPO outgoing mirror 7 and angle, realize the high-efficiency operation of three chamber mirror annular chamber OPO.
Embodiment four:
In conjunction with Fig. 1, present embodiment is described, difference described in present embodiment and execution mode one, execution mode two be as pumping source ~ 2mm laser adopts the Tm of technology maturation, the solid state laser of Ho doping, enters pumping coupling system 10 by the Transmission Fibers of 2mm.
Embodiment five:
In conjunction with Fig. 1, present embodiment is described, difference described in present embodiment and execution mode three is to adopt into the 1mm laser of pumping source the solid state laser (as Nd:YAG, Nd:YVO4, Nd:YLF etc.) of the Nd doping of technology maturation, enters pumping coupling system 10 by the Transmission Fibers of 1mm.
Embodiment five:
In conjunction with Fig. 1, present embodiment is described, the difference described in present embodiment and execution mode five is to adopt into the 1.319mm laser of pumping source the solid state laser of the Nd doping of technology maturation, enters pumping coupling system 10 by the Transmission Fibers of 1.319mm.Front coupled lens 2 in pumping coupling system 10, the two-sided anti-reflection film that is all coated with 1.319mm of rear coupled lens 3.OPO total reflective mirror 9 has high-transmission rate to 1.319mm laser, near infrared signal light and in infrared ideler frequency light there is high reflectance, angled placement.OPO speculum 4 near infrared signal light and in infrared ideler frequency light there is high reflectance, become level angle place.OPO outgoing mirror 7 has high-transmission rate to 1.319mm laser, near infrared signal light and in wherein a kind of laser of infrared ideler frequency light there is high-transmission rate, another kind of laser has part reflection, or two kinds of laser are all had to part reflection, angled placement.

Claims (5)

1. miniaturization three chamber mirror annular chamber mid-infrared parameter oscillator, include fiber laser and OPO system shell as OPO pumping source, it is characterized in that: in described OPO system shell, include pumping coupling system and OPO annular chamber; In described pumping coupling system, be provided with front coupled lens and rear coupled lens; In described OPO annular chamber, be provided with OPO speculum, OPO total reflective mirror, OPO outgoing mirror and nonlinear crystal; The laser beam that described fiber laser sends is successively through entering OPO annular chamber after front coupled lens and rear coupled lens; Described laser beam penetrates through after OPO total reflective mirror, nonlinear crystal and OPO outgoing mirror after entering OPO annular chamber successively; When described laser beam passes OPO outgoing mirror, a part of laser beam is reflexed to OPO speculum by OPO outgoing mirror and after OPO speculum reflexes to OPO total reflective mirror, reflexes to nonlinear crystal through OPO total reflective mirror again.
2. a kind of miniaturization three chamber mirror annular chamber mid-infrared parameter oscillator according to claim 1, is characterized in that: described front coupled lens and the ratio of rear coupled lens focal length the fibre core size that is laser beam and the ratio of expecting waist spot size.
3. a kind of miniaturization three chamber mirror annular chamber mid-infrared parameter oscillator according to claim 1, is characterized in that: the distance between described front coupled lens and fiber laser equals the focal length of front coupled lens.
4. a kind of miniaturization three chamber mirror annular chamber mid-infrared parameter oscillator according to claim 1, is characterized in that: described front coupled lens and rear coupled lens are coaxially placed, and described nonlinear crystal is placed in the focal position of rear coupled lens.
5. a kind of miniaturization three chamber mirror annular chamber mid-infrared parameter oscillator according to claim 1, is characterized in that: pass through waist spot position and the size after pumping coupling system by the distance energy coarse adjustment laser of adjusting between front coupled lens and fiber-optic output; Can finely tune waist spot position and size by the relative distance of adjusting between front coupled lens and rear coupled lens.
CN201410114460.7A 2014-03-26 2014-03-26 A kind of three hysteroscope annular chamber mid-infrared parameter oscillator of miniaturization Active CN103944049B (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
CN201410114460.7A CN103944049B (en) 2014-03-26 2014-03-26 A kind of three hysteroscope annular chamber mid-infrared parameter oscillator of miniaturization

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
CN201410114460.7A CN103944049B (en) 2014-03-26 2014-03-26 A kind of three hysteroscope annular chamber mid-infrared parameter oscillator of miniaturization

Publications (2)

Publication Number Publication Date
CN103944049A true CN103944049A (en) 2014-07-23
CN103944049B CN103944049B (en) 2017-03-15

Family

ID=51191601

Family Applications (1)

Application Number Title Priority Date Filing Date
CN201410114460.7A Active CN103944049B (en) 2014-03-26 2014-03-26 A kind of three hysteroscope annular chamber mid-infrared parameter oscillator of miniaturization

Country Status (1)

Country Link
CN (1) CN103944049B (en)

Cited By (5)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN105119137A (en) * 2015-08-24 2015-12-02 哈尔滨工业大学 High power far infrared 8 mu m laser beam generator based on ZnGeP2 circular cavity OPO
CN107611762A (en) * 2017-10-16 2018-01-19 中国科学院合肥物质科学研究院 A kind of broad tuning, narrow linewidth, efficient mid-infrared parameter oscillator
CN109326950A (en) * 2018-12-11 2019-02-12 中国科学院上海光学精密机械研究所 Ring cavity structure optically erasing device
JP2020516961A (en) * 2017-04-17 2020-06-11 ユニバーシティ・オブ・セントラル・フロリダ・リサーチ・ファウンデーション,インコーポレイテッドUniversity Of Central Florida Research Foundation, Inc. Optical parametric device based on random phase matching in polycrystalline media
CN111417249A (en) * 2019-01-07 2020-07-14 中国科学院大连化学物理研究所 Method for preparing molecular beam by excitation of molecule broad-band vibration-inversion state

Citations (5)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH06132594A (en) * 1992-03-09 1994-05-13 Tech Res & Dev Inst Of Japan Def Agency Wide band wavelength variable 90× phase matching ktp optical parametric oscillator
CN1309445A (en) * 2000-12-20 2001-08-22 中国科学院上海光学精密机械研究所 Frequency multiplier with triangular ring cavity
US6647034B1 (en) * 2001-04-30 2003-11-11 Sandia Corporation Method to improve optical parametric oscillator beam quality
CN102088158A (en) * 2010-12-22 2011-06-08 北京中科思远光电科技有限公司 Method and device for obtaining high-power ultraviolet laser light
CN103259177A (en) * 2013-04-26 2013-08-21 哈尔滨工业大学 Intermediate infrared optical parametric oscillator based on four-mirror ring-shaped resonant cavity

Patent Citations (5)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH06132594A (en) * 1992-03-09 1994-05-13 Tech Res & Dev Inst Of Japan Def Agency Wide band wavelength variable 90× phase matching ktp optical parametric oscillator
CN1309445A (en) * 2000-12-20 2001-08-22 中国科学院上海光学精密机械研究所 Frequency multiplier with triangular ring cavity
US6647034B1 (en) * 2001-04-30 2003-11-11 Sandia Corporation Method to improve optical parametric oscillator beam quality
CN102088158A (en) * 2010-12-22 2011-06-08 北京中科思远光电科技有限公司 Method and device for obtaining high-power ultraviolet laser light
CN103259177A (en) * 2013-04-26 2013-08-21 哈尔滨工业大学 Intermediate infrared optical parametric oscillator based on four-mirror ring-shaped resonant cavity

Cited By (6)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN105119137A (en) * 2015-08-24 2015-12-02 哈尔滨工业大学 High power far infrared 8 mu m laser beam generator based on ZnGeP2 circular cavity OPO
JP2020516961A (en) * 2017-04-17 2020-06-11 ユニバーシティ・オブ・セントラル・フロリダ・リサーチ・ファウンデーション,インコーポレイテッドUniversity Of Central Florida Research Foundation, Inc. Optical parametric device based on random phase matching in polycrystalline media
JP7225204B2 (en) 2017-04-17 2023-02-20 ユニバーシティ・オブ・セントラル・フロリダ・リサーチ・ファウンデーション,インコーポレイテッド Optical parametric device based on random phase matching in polycrystalline media
CN107611762A (en) * 2017-10-16 2018-01-19 中国科学院合肥物质科学研究院 A kind of broad tuning, narrow linewidth, efficient mid-infrared parameter oscillator
CN109326950A (en) * 2018-12-11 2019-02-12 中国科学院上海光学精密机械研究所 Ring cavity structure optically erasing device
CN111417249A (en) * 2019-01-07 2020-07-14 中国科学院大连化学物理研究所 Method for preparing molecular beam by excitation of molecule broad-band vibration-inversion state

Also Published As

Publication number Publication date
CN103944049B (en) 2017-03-15

Similar Documents

Publication Publication Date Title
CN100358192C (en) Generator of terahertz by oscillator with acyclic polarized crystal and double-wavelength optical parameter
CN103944049A (en) Miniature three-endoscope ring cavity mid-infrared optical parametric oscillator
US20170018904A1 (en) Optical parametric oscillation laser based on i-type quasi-phase matching
CN107528197B (en) Two-chamber compound unsteady cavity modeling pumping from optical parametric oscillation mid-infrared laser device
CN108666862B (en) A kind of infrared double-wave length is tunable from optical parametric oscillator
CN101924318A (en) Device for outputting dual wavelength laser and terahertz wave based on single periodical and polarized crystal
CN104868354A (en) Optical parameter laser apparatus
CN104503183B (en) Self frequency-changing's tera-hertz parametric oscillator
CN203326348U (en) Tunable-wavelength deep ultraviolet light laser
CN101777724B (en) End-pumped dual-wavelength coaxial switching output Q-switched base-frequency and double-frequency laser
CN101677173B (en) Generation method and device of intermediate infrared femtosecond laser pulse with self-stabilized carrier phase
CN101986484A (en) Laser triple frequency system
CN102868080A (en) Device capable of generating high terahertz pulse through external cavity resonance enhancement
CN206498081U (en) A kind of tunable ultrashort pulse Fiber-optic parameter oscillator
CN204290022U (en) Infrared two-chamber optical parametric oscillator in a kind of narrow linewidth high light beam quality
CN204290023U (en) Infrared intra-cavity optical parametric oscillator during a kind of miniaturized wide spectral is tunable
CN204290024U (en) Infrared ring light parametric oscillator in a kind of compact three chamber mirrors
CN102354897B (en) External secondary cascading difference frequency terahertz light source generation device and implementation method
CN201226412Y (en) Whole solid-state intermediate infrared light parameter frequency difference laser
Wang et al. Wide-tunable mid infrared intra-cavity optical parametric oscillator based on multi-period MgO: PPLN
CN108155553B (en) Fine adjustable optical parametric oscillator with fast gain band switching
CN103368044A (en) Synchronous double-frequency pulse microchip laser based on temperature control mechanism
CN203690698U (en) Single-frequency intermediate infrared light source system of 2 [mu]m fiber laser pump
CN106340797B (en) 2 μm of tunable laser of annular chamber optical parametric oscillator are constituted based on body grating
CN105790045A (en) High-energy few-cycle ultra-high-signal to noise ratio femtosecond seed pulse generation 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
C14 Grant of patent or utility model
GR01 Patent grant
TR01 Transfer of patent right
TR01 Transfer of patent right

Effective date of registration: 20170522

Address after: 100192, A207, building two, building B-2, Zhongguancun Dongsheng science and Technology Park, No. 66 Xiao Dong Road, Beijing, Haidian District

Patentee after: Beijing Huayu Dexin Photoelectric Technology Co Ltd

Address before: 621000 Mianyang, Sichuan, box 1013, box of 919

Patentee before: Applied Electronics Inst., Chinese Engineering Physics Inst.