CN108493756B - YVO based on Nd4/Nd:GdVO4Double-frequency laser of combined crystal - Google Patents

YVO based on Nd4/Nd:GdVO4Double-frequency laser of combined crystal Download PDF

Info

Publication number
CN108493756B
CN108493756B CN201810122328.9A CN201810122328A CN108493756B CN 108493756 B CN108493756 B CN 108493756B CN 201810122328 A CN201810122328 A CN 201810122328A CN 108493756 B CN108493756 B CN 108493756B
Authority
CN
China
Prior art keywords
crystal
laser
yvo4
gdvo4
temperature control
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
CN201810122328.9A
Other languages
Chinese (zh)
Other versions
CN108493756A (en
Inventor
胡淼
金涛
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.)
Inno Laser Technology Corp ltd
Original Assignee
Hangzhou Dianzi 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 Hangzhou Dianzi University filed Critical Hangzhou Dianzi University
Priority to CN201810122328.9A priority Critical patent/CN108493756B/en
Publication of CN108493756A publication Critical patent/CN108493756A/en
Application granted granted Critical
Publication of CN108493756B publication Critical patent/CN108493756B/en
Active legal-status Critical Current
Anticipated expiration legal-status Critical

Links

Images

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
    • H01S3/14Lasers, i.e. devices using stimulated emission of electromagnetic radiation in the infrared, visible or ultraviolet wave range characterised by the material used as the active medium
    • H01S3/16Solid materials
    • H01S3/163Solid materials characterised by a crystal matrix
    • H01S3/1671Solid materials characterised by a crystal matrix vanadate, niobate, tantalate
    • H01S3/1673YVO4 [YVO]
    • 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
    • H01S3/102Controlling the intensity, frequency, phase, polarisation or direction of the emitted radiation, e.g. switching, gating, modulating or demodulating by controlling the active medium, e.g. by controlling the processes or apparatus for excitation
    • H01S3/1028Controlling the intensity, frequency, phase, polarisation or direction of the emitted radiation, e.g. switching, gating, modulating or demodulating by controlling the active medium, e.g. by controlling the processes or apparatus for excitation by controlling the temperature
    • 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
    • H01S3/14Lasers, i.e. devices using stimulated emission of electromagnetic radiation in the infrared, visible or ultraviolet wave range characterised by the material used as the active medium
    • H01S3/16Solid materials
    • H01S3/163Solid materials characterised by a crystal matrix
    • H01S3/1671Solid materials characterised by a crystal matrix vanadate, niobate, tantalate

Landscapes

  • Physics & Mathematics (AREA)
  • Electromagnetism (AREA)
  • Engineering & Computer Science (AREA)
  • Plasma & Fusion (AREA)
  • Optics & Photonics (AREA)
  • Chemical & Material Sciences (AREA)
  • Crystallography & Structural Chemistry (AREA)
  • Lasers (AREA)

Abstract

The invention discloses a Nd-YVO-based optical fiber4/Nd:GdVO4A dual-frequency laser of composite crystal comprising Nd-YVO4/Nd:GdVO4The device comprises a combined crystal, a heat sink temperature control module, a pumping module, a laser resonant cavity and an output module; the pump module emits pump light, Nd: YVO4/Nd:GdVO4The combined crystal receives the pump light, the pump light is stimulated and amplified to form double-frequency laser after passing through the laser resonant cavity, and the output module receives and outputs the double-frequency laser adjusted by the laser resonant cavity; nd: YVO4/Nd:GdVO4The combined crystal is arranged in a heat sink temperature control module which is used for controlling Nd: YVO4/Nd:GdVO4The temperature of the combined crystals. The invention adopts Nd-YVO4/Nd:GdVO4The combined crystal is used as a gain medium, can generate a double-frequency laser beam with large frequency difference when receiving the radiation of the pump light, and adjusts the beam quality of the double-frequency laser through the laser resonant cavity and the output module. In addition, the temperature of the combined crystal can be adjusted in real time through the heat sink temperature control module, so that the adjustment of the power balance degree of the dual-frequency laser is realized.

Description

YVO based on Nd4/Nd:GdVO4Double-frequency laser of combined crystal
Technical Field
The invention relates to the technical field of double-frequency lasers and photoproduction millimeter waves, in particular to a laser based on Nd: YVO4/Nd:GdVO4A dual frequency laser incorporating a crystal.
Background
In recent years, with the rapid development of the mobile internet, various new wireless communication services are overlaid, the amount of network data is exponentially increased, and limited spectrum resources become more and more scarce. Compared with the traditional microwave signals, the millimeter wave and sub-millimeter wave signals with higher frequency have the advantages of larger bandwidth, narrower wave beam, stronger anti-interference capability and the like. Recent 5G networks have begun to use millimeter waves as their frequency band for ultra-high speed communications.
At present, in a plurality of methods for generating millimeter wave and submillimeter wave signals, heterodyne beat frequency of a double-frequency laser signal is an effective scheme for acquiring low-noise and high-frequency electric signals. In the heterodyne beat frequency process, the frequency of the output electric signal depends on the frequency difference of the double-frequency laser signal; the photoelectric conversion efficiency depends on the power product of the dual-frequency laser signal. When the total power of the output double-frequency laser is constant, the beat frequency efficiency is higher when the power balance is higher. To date, many studies on dual-frequency lasers have been conducted around both improving the output frequency difference and improving the power balance. In the early stage of research, a research group has used a single crystal dual-frequency laser to obtain a dual-frequency laser signal with a frequency difference of 80GHz, but has suffered from a dilemma on the way of further improving the frequency difference.
The frequency difference of double-frequency laser signals output by the existing single crystal double-frequency laser is generally less than 100GHz, and high-frequency millimeter wave signals above 100GHz cannot be obtained by direct beat frequency. With the progress of research, different laser crystals can be organically combined by utilizing the emission spectrum difference among the laser crystals, and the combined crystal can be used as a laser gain medium to obtain dual-frequency laser output with higher frequency difference.
Disclosure of Invention
The invention aims to provide a double-frequency laser for outputting high-frequency difference laser signals, and simultaneously, the power of double-frequency laser can be balanced and tuned.
Aiming at the purpose, the invention discloses a Nd-YVO-based material4/Nd:GdVO4A dual-frequency laser of composite crystal comprising Nd-YVO4/Nd:GdVO4The device comprises a combined crystal, a heat sink temperature control module, a pumping module, a laser resonant cavity and an output module; the pump module emits pump light, Nd: YVO4/Nd:GdVO4The combined crystal receives the pump light, the pump light is stimulated and amplified to form double-frequency laser after passing through the laser resonant cavity, and the output module receives and outputs the double-frequency laser adjusted by the laser resonant cavity; nd: YVO4/Nd:GdVO4The combined crystal is arranged in a heat sink temperature control module which is used for controlling Nd: YVO4/Nd:GdVO4The temperature of the crystal is combined to realize the power balance adjustment of the dual-frequency laser. Wherein, Nd is YVO4/Nd:GdVO4The composite crystal is neodymium-doped yttrium vanadate/neodymium-doped gadolinium vanadate composite crystal.
Further, Nd: YVO4/Nd:GdVO4YVO (YVO) with thickness of the combined crystal close to one end of the pumping module lower than that of Nd4/Nd:GdVO4The thickness of the combined crystal at the end away from the pumping module.
Further, Nd: YVO4/Nd:GdVO4The composite crystal comprises Nd: YVO4Laser crystal, Nd: GdVO4Laser crystal, Nd: YVO4/Nd:GdVO4The composite crystal is prepared by mixing Nd: YVO4(Neodymium-doped yttrium vanadate) laser crystal and Nd: GdVO4Carrying out crystal bonding on the (neodymium-doped gadolinium vanadate) laser crystal to obtain the crystal; nd: YVO4/Nd:GdVO4YVO (Nd: YVO) of composite crystal4One side of the laser crystal is arranged at one side close to the pumping module. Nd: YVO4/Nd:GdVO4The combined crystal is a gain medium in the laser resonant cavity and is used for realizing the stimulated radiation amplification of the dual-frequency laser signal. YVO is due to Nd4/Nd:GdVO4The wavelengths of the excited radiation of the composite crystal are respectively in Nd and YVO4Crystal and Nd: GdVO4The crystal emission spectrum (as shown in FIG. 1) is within the range, so that at 20 ℃, Nd: YVO4Excited radiation wavelength of crystal and Nd: GdVO4The difference of the excited radiation wavelength of the crystal exceeds 1.2nm, and the theoretical frequency difference is more than 300 GHz; on the other hand, when Nd: YVO4/Nd:GdVO4When the temperature of the combined crystal changes, the existence of different crystal emission spectrum peaks is cancelled, and the power balance of the output dual-frequency laser signal shows corresponding change.
Further, the heat sink temperature control module comprises a clamp holder, a water-cooling base, a semiconductor refrigerating piece, a temperature control probe, a front end controller and a PC control end, wherein the clamp holder clamps the combined crystal; the semiconductor refrigerating piece is arranged at the bottom of the holder; the water-cooling base is arranged at the bottom of the semiconductor refrigerating piece; the temperature control probe is arranged on the clamper; the front-end controller is electrically connected with the temperature control probe; the PC control end is electrically connected with the front-end controller.
Furthermore, the front-end controller is electrically connected with the temperature control probe through a lead, and the lead is a double-core copper lead.
Furthermore, the pumping module comprises a pumping source, an optical fiber and an input coupling mirror, wherein the pumping source is communicated with the optical fiber, and the optical fiber is communicated with the input coupling mirror. The pump source is used for emitting pump light, and the optical fiber and the input coupling mirror are used for transmitting and converging the pump light so as to improve the utilization rate of the pump light.
Furthermore, the laser resonant cavity comprises a front-end coating film and a reflector, the front-end coating film is coated on one side of the combined crystal close to the pumping module, and the reflector and the front-end coating film are arranged in parallel relatively so as to provide positive feedback for laser amplification.
Furthermore, the output module comprises an output coupling mirror and a tail fiber, the output coupling mirror and the reflecting mirror are arranged in parallel relatively, and the tail fiber is connected with the output coupling mirror. The output coupling mirror is used for improving the output coupling efficiency of the double-frequency laser and improving the output power.
Further, the temperature control range of the front-end controller is-10 ℃ to 100 ℃.
Further, the output frequency difference of the output module is not lower than 300 GHz.
The invention has the beneficial effects that:
the invention adopts Nd-YVO4/Nd:GdVO4The combined crystal is used as a gain medium and can generate a dual-frequency laser beam with the frequency difference larger than 300GHz when receiving the optical radiation of the pump. In addition, the temperature of the combined crystal can be adjusted in real time through the heat sink temperature control module, so that the adjustment of the power balance degree of the dual-frequency laser is realized. YVO based on Nd4/Nd:GdVO4The output frequency difference of the double-frequency laser output by the double-frequency laser of the combined crystal is not lower than 300GHz, and meanwhile, the heterodyne beat frequency efficiency can be improved by adjusting the power balance of the output double-frequency laser, so that the combined crystal has better applicability.
Drawings
YVO shown in figure 1 as Nd4/Nd:GdVO4YVO as Nd component in composite crystal4Crystal emission spectrum (a) and Nd: GdVO4Crystal emission spectrum (b);
FIG. 2 shows Nd: YVO4/Nd:GdVO4Designing a structure diagram of the combined crystal;
FIG. 3 shows YVO based on Nd in example 14/Nd:GdVO4The composition structure diagram of the dual-frequency laser of the combined crystal;
FIG. 4 shows YVO based on Nd in example 14/Nd:GdVO4The system output power temperature control tuning chart of the dual-frequency laser of the combined crystal.
Detailed Description
The following are specific embodiments of the present invention and are further described with reference to the drawings, but the present invention is not limited to these embodiments.
Example 1
The purpose of this embodiment is to provide a dual-frequency laser that can output high frequency difference, can carry out power balance tuning to the dual-frequency laser that outputs simultaneously in time. To achieve the object, referring to FIG. 3, this embodiment discloses a Nd: YVO based optical film4/Nd:GdVO4A dual-frequency laser of composite crystal comprising Nd-YVO4/Nd:GdVO4The device comprises a combined crystal 4, a heat sink temperature control module, a pumping module, a laser resonant cavity and an output module; the pump module emits pump light, Nd: YVO4/Nd:GdVO4The combined crystal 4 receives the pump light, is stimulated and amplified after passing through the laser resonant cavity to form dual-frequency laser, and the output module receives and outputs the dual-frequency laser adjusted by the laser resonant cavity; nd: YVO4/Nd:GdVO4The combined crystal 4 is arranged in a heat sink temperature control module which is used for controlling Nd: YVO4/Nd:GdVO4The temperature of the combined crystals 4.
Nd:YVO4/Nd:GdVO4YVO is smaller than Nd in thickness at one end of the combined crystal 4 close to the pumping module4/Nd:GdVO4The thickness of the combined crystal at the end away from the pumping module. Nd: YVO4/Nd:GdVO4The composite crystal is composed of Nd: YVO4Crystal 17 and Nd: GdVO4The crystal 18 is composed of Nd YVO4/Nd:GdVO4YVO (Nd: YVO) of composite crystal4One side of the laser crystal is arranged at one side close to the pumping module. The axial cross section dimension is 3mm multiplied by 3mm, all the axial cross section dimensions are a-axis cutting, each end face is coated with a film, and the optical axis is vertically arranged, as shown in figure 2.
Wherein, Nd is YVO4/Nd:GdVO4The combined crystal is a gain medium in the laser resonant cavity and is used for realizing the stimulated radiation amplification of the double-frequency laser. YVO is due to Nd4/Nd:GdVO4The wavelengths of the excited radiation of the composite crystal are respectively in Nd and YVO4Crystal and Nd: GdVO4CrystalEmission spectrum range (as shown in FIG. 1), therefore at 20 deg.C, Nd: YVO4Excited radiation wavelength of crystal and Nd: GdVO4The difference of the excited radiation wavelength of the crystal exceeds 1.2nm, and the theoretical frequency difference is more than 300 GHz; on the other hand, when Nd: YVO4/Nd:GdVO4When the temperature of the combined crystal changes, the existence of different crystal emission spectrum peaks cancels the long phenomenon, and the power balance of the output dual-frequency laser signal shows corresponding change.
The heat sink temperature control module comprises a clamp holder 7, a water-cooling base 9, a semiconductor refrigerating piece 8, a temperature control probe 11, a front end controller 10 and a PC control end 12, wherein the clamp holder 7 clamps the combined crystal 4; the semiconductor refrigerating piece 8 is arranged at the bottom of the clamping device 7; the water-cooling base 9 is arranged at the bottom of the semiconductor refrigerating piece 8; the temperature control probe 11 is arranged on the clamper 7; the front-end controller 10 is electrically connected with the temperature control probe 11; the PC control terminal 12 is electrically connected to the front-end controller 10. The water-cooling base 9 is used for realizing heat exchange, the temperature control probe 11 is used for detecting the temperature of the combined crystal, the front-end controller 10 is used for automatically adjusting the direction and the magnitude of the power supply current of the semiconductor refrigerating piece 8, and the PC control end 12 is used for setting the temperature control temperature and checking the real-time temperature of the combined crystal detected by the temperature control probe.
The holder 7 is a metal holder made of aluminum alloy material and is composed of an upper triangular prism and a lower triangular prism which are connected by screws, a square groove with the diameter of 3.5mm multiplied by 3.5mm is arranged at the splicing center and is used for placing indium foil wrapped Nd: YVO4/Nd:GdVO4The crystals are combined.
The semiconductor refrigerating piece 8 is a semiconductor refrigerating piece with the model number of TEC1-12708, and the maximum refrigerating power is 68.9W.
The water-cooling base 9 is a hollow aluminum alloy box body which is provided with a water outlet and a water inlet and is used for fixing the holder 7 and the semiconductor refrigerating piece 8 and improving the stability of temperature control in the heat exchange process.
The front-end controller 10 is a model TCB-NA semiconductor refrigeration chip temperature control board, and is based on a PID control algorithm to further realize temperature regulation and control from-10 ℃ to 100 ℃, and the temperature control precision can reach 0.1 ℃.
The temperature control probe 11 is a thermistor (NTC) having a resistance of 10K Ω, and its B value is 3950 (the B value is a parameter describing physical characteristics of the thermistor material, i.e., a thermal sensitivity index, and the larger the B value, the higher the sensitivity of the thermistor).
The PC control end 12 is a computer with serial port debugging software. The PC control end 12 is electrically connected with the front-end controller 10 through a data line 16, and the data line 16 is a serial port line from USB to RS-232.
The front-end controller 10 is electrically connected with the temperature control probe 11 through a lead 15, and the lead 15 is a double-core copper lead.
The pumping module comprises a pumping source 1, an optical fiber 2 and an input coupling mirror 3, wherein the pumping source 1 is communicated with the optical fiber 2, and the optical fiber 2 is communicated with the input coupling mirror 3. The pump source 1 is used for emitting pump light, and the optical fiber 2 and the input coupling mirror 3 are used for transmitting and converging the pump light, so that the utilization rate of the pump light is improved. The pumping source 1 is a semiconductor laser with the output center wavelength of 808nm, and the output power of the semiconductor laser is adjustable; the optical fiber 2 is a multimode optical fiber, and the core diameter thereof is 100 mu m; the input coupling mirror 3 is a self-focusing lens.
The laser resonant cavity comprises a front-end coating 5 and a reflector 6, wherein the front-end coating 5 is coated on the combined crystal, and the reflector 6 and the front-end coating 5 are arranged in parallel relatively so as to provide positive feedback for laser amplification. Wherein, the front end coating film 5 comprises a total reflection film 19 and an antireflection film 20; the reflecting mirror 6 is a plane reflecting mirror, and the mirror surface of the plane reflecting mirror close to the combined crystal side is plated with a part of high reflecting film (R ═ 90% @1064nm) and high reflecting film (HR @808 nm).
Referring to FIG. 2, Nd: YVO4/Nd:GdVO4One end of the composite crystal 4 is Nd: YVO4The other end of the laser crystal 17 is Nd: GdVO with larger thickness4And a laser crystal 18 having both end faces of the combined crystal coated with a film. Wherein, Nd is YVO4One side of the laser crystal close to the coupling input mirror is plated with a total reflection film (HR @1064nm)19 and an antireflection film (AR @808nm)20, Nd is YVO4Laser crystal and Nd: GdVO4The end face of the middle combination of the laser crystal is plated with an antireflection film (AR @808nm)&1064nm)21,Nd:GdVO4The end face of the laser crystal close to one side of the reflector is coated with an antireflection film (AR @1064nm) 22.
The output module comprises an output coupling mirror 13 and a tail fiber 14, wherein the output coupling mirror 13 is arranged opposite to and parallel to the reflecting mirror 6, and the tail fiber 14 is connected with the output coupling mirror 13. The output coupling mirror 13 is used to improve the coupling efficiency of the dual-frequency laser and improve the output power. The tail fiber 14 is a multimode fiber with a core diameter of 100 μm; the output coupling mirror 13 is an aspheric lens, and the coupling efficiency can reach 85%.
The temperature control range of the front-end controller 10 is-10 ℃ to 100 ℃.
The output frequency difference of the output module is not lower than 300 GHz.
In addition, the dual-frequency laser disclosed by the embodiment also needs auxiliary devices such as a base, a lens support and a screw to stabilize the whole dual-frequency laser device and keep the consistency of the central height of the optical path, and then the dual-frequency laser signal is smoothly output by adjusting the position of the pumping source and working parameters such as the position and the angle of the reflector. Finally, the dual-frequency laser in the embodiment can realize the output of the dual-frequency laser with the central wavelength of about 1060nm, the frequency difference of not less than 300GHz and the tunable power balance degree, and the temperature control characteristic of the dual-frequency laser at 5-40 ℃ is shown in fig. 4.
YVO based on Nd provided in the embodiment4/Nd:GdVO4The working principle of the dual-frequency laser of the combined crystal is as follows: YVO (Nd: YVO) cut under the action of 808nm laser pumping source4Crystal and Nd: GdVO4Due to the difference of emission cross-section spectrums in frequency, the output wavelengths of the crystal also show obvious difference, namely the output of the dual-frequency laser can be realized. YVO (Nd: YVO) obtained by cutting an a axis4Crystal and Nd: GdVO4YVO (Nd: YVO) formed by mutually and vertically combining crystal optical axes4/Nd:GdVO4The combined crystal is used as a gain medium of the laser and placed on the central line of pump light, the pump module is adjusted to select proper pump power, the heat sink temperature control module is used for adjusting the power balance degree of the double-frequency laser, the laser resonant cavity and the output module are used for controlling the beam quality of the double-frequency laser, and finally the large-frequency-difference double-frequency laser output with balanced power is obtained. It can also be adjusted in real time by presetting the temperature of temperature control through the PC control endThe temperature of the whole crystal realizes the purpose of balanced tuning of the power of the double-frequency laser.
The dual-frequency laser provided in the embodiment adopts Nd: YVO4/Nd:GdVO4The combined crystal is used as a gain medium, can generate a double-frequency laser beam with large frequency difference when receiving the radiation of the pump light, and adjusts the beam quality of the double-frequency laser through the laser resonant cavity and the output module. In addition, the temperature of the combined crystal can be adjusted in real time through the heat sink temperature control module, so that the adjustment of the power balance degree of the dual-frequency laser is realized. YVO based on Nd4/Nd:GdVO4The output frequency difference of the double-frequency laser output by the double-frequency laser of the combined crystal is not lower than 300GHz, and meanwhile, the heterodyne beat frequency efficiency can be improved by adjusting the power balance of the output double-frequency laser, so that the combined crystal has better applicability.
The specific embodiments described herein are merely illustrative of the spirit of the invention. Various modifications or additions may be made to the described embodiments or alternatives may be employed by those skilled in the art without departing from the spirit or ambit of the invention as defined in the appended claims.

Claims (7)

1. A double-frequency laser based on Nd, YVO4/Nd, GdVO4 composite crystal is characterized by comprising Nd, YVO4/Nd, GdVO4 composite crystal, a heat sink temperature control module, a pumping module, a laser resonant cavity and an output module; the pump module emits pump light, the combined crystal of YVO4/Nd GdVO4 receives the pump light, the pump light is stimulated and amplified to form double-frequency laser after passing through the laser resonant cavity, and the output module receives and outputs the double-frequency laser adjusted by the laser resonant cavity; the Nd is YVO4/Nd is GdVO4 composite crystal is arranged on the heat sink temperature control module, and the heat sink temperature control module is used for controlling the temperature of the Nd is YVO4/Nd is GdVO4 composite crystal;
the heat sink temperature control module comprises a clamp holder, a water-cooling base, a semiconductor refrigerating piece, a temperature control probe, a front end controller and a PC control end, wherein the clamp holder clamps the combined crystal; the semiconductor refrigerating piece is arranged at the bottom of the holder; the water-cooling base is arranged at the bottom of the semiconductor refrigerating piece; the temperature control probe is arranged on the clamper; the front-end controller is electrically connected with the temperature control probe; the PC control end is electrically connected with the front-end controller; the water-cooling base is used for realizing heat exchange, the temperature control probe is used for detecting the temperature of the combined crystal, the front-end controller is used for automatically adjusting the direction and the magnitude of the power supply current of the semiconductor refrigerating element, and the PC control end is used for setting the temperature control temperature and checking the real-time temperature of the combined crystal detected by the temperature control probe;
the output module comprises an output coupling mirror and a tail fiber, the output coupling mirror and the reflecting mirror are arranged in parallel relatively, and the tail fiber is connected with the output coupling mirror;
the thickness of the Nd: YVO4/Nd: GdVO4 combined crystal close to one end of the pumping module is lower than that of the Nd: YVO4/Nd: GdVO4 combined crystal far away from one end of the pumping module.
2. The dual-frequency laser of claim 1, which is based on a Nd: YVO4/Nd: GdVO4 composite crystal, wherein the Nd: YVO4/Nd: GdVO4 composite crystal comprises Nd: YVO4 laser crystal, Nd: GdVO4 laser crystal, and the Nd: YVO4/Nd: GdVO4 composite crystal is obtained by crystal-bonding Nd: YVO4 laser crystal and Nd: GdVO4 laser crystal; the Nd: YVO4 laser crystal side of the Nd: YVO4/Nd: GdVO4 combined crystal is arranged at the side close to the pumping module.
3. The Nd: YVO4/Nd: GdVO4 composite crystal-based dual-frequency laser of claim 1, wherein the front-end controller is electrically connected with the temperature control probe through a lead wire, and the lead wire is a dual-core copper lead wire.
4. The Nd: YVO4/Nd: GdVO4 composite crystal-based two-frequency laser of claim 1, wherein the pump module comprises a pump source, an optical fiber and an input coupling mirror, the pump source is communicated with the optical fiber, and the optical fiber is communicated with the input coupling mirror.
5. The dual-frequency laser of claim 4, based on a Nd: YVO4/Nd: GdVO4 composite crystal, wherein the laser resonant cavity comprises a front-end coating and a reflector, the front-end coating is coated on one side of the composite crystal close to the pumping module, and the reflector and the front-end coating are arranged in parallel relatively.
6. The dual-frequency laser based on Nd: YVO4/Nd: GdVO4 composite crystal as claimed in claim 1, wherein the temperature of the front-end controller is controlled in a range of-10 ℃ to 100 ℃.
7. The two-frequency laser based on Nd: YVO4/Nd: GdVO4 composite crystal as claimed in any one of claims 1-6, wherein the output frequency difference of the output module is not lower than 300 GHz.
CN201810122328.9A 2018-02-07 2018-02-07 YVO based on Nd4/Nd:GdVO4Double-frequency laser of combined crystal Active CN108493756B (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
CN201810122328.9A CN108493756B (en) 2018-02-07 2018-02-07 YVO based on Nd4/Nd:GdVO4Double-frequency laser of combined crystal

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
CN201810122328.9A CN108493756B (en) 2018-02-07 2018-02-07 YVO based on Nd4/Nd:GdVO4Double-frequency laser of combined crystal

Publications (2)

Publication Number Publication Date
CN108493756A CN108493756A (en) 2018-09-04
CN108493756B true CN108493756B (en) 2020-06-12

Family

ID=63344651

Family Applications (1)

Application Number Title Priority Date Filing Date
CN201810122328.9A Active CN108493756B (en) 2018-02-07 2018-02-07 YVO based on Nd4/Nd:GdVO4Double-frequency laser of combined crystal

Country Status (1)

Country Link
CN (1) CN108493756B (en)

Families Citing this family (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN114204383B (en) * 2021-11-24 2024-01-16 北京大学 Quantum thermometer based on active lasing and implementation method thereof

Citations (5)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN101071932A (en) * 2007-05-22 2007-11-14 南昌航空大学 Semiconductor laser precision tune-up and tempeature control device
CN101572384A (en) * 2009-03-13 2009-11-04 中国科学院福建物质结构研究所 Combined continuous full-solid state Raman laser
US7742509B2 (en) * 2008-09-25 2010-06-22 Photop Technologies Single-longitudinal mode laser with orthogonal-polarization traveling-wave mode
CN102891422A (en) * 2011-12-22 2013-01-23 清华大学 Nonlinear crystal temperature control device
CN105071217A (en) * 2015-08-27 2015-11-18 山东大学 Self-frequency-doubling all-solid-state yellow-light laser

Family Cites Families (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN104682196A (en) * 2013-11-29 2015-06-03 福州高意通讯有限公司 Direct semiconductor laser

Patent Citations (5)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN101071932A (en) * 2007-05-22 2007-11-14 南昌航空大学 Semiconductor laser precision tune-up and tempeature control device
US7742509B2 (en) * 2008-09-25 2010-06-22 Photop Technologies Single-longitudinal mode laser with orthogonal-polarization traveling-wave mode
CN101572384A (en) * 2009-03-13 2009-11-04 中国科学院福建物质结构研究所 Combined continuous full-solid state Raman laser
CN102891422A (en) * 2011-12-22 2013-01-23 清华大学 Nonlinear crystal temperature control device
CN105071217A (en) * 2015-08-27 2015-11-18 山东大学 Self-frequency-doubling all-solid-state yellow-light laser

Non-Patent Citations (1)

* Cited by examiner, † Cited by third party
Title
"Efficient dual-wavelength diode-end-pumped laser with a diffusion-bonded Nd:YVO4/Nd:GdVO4 crystal";Y.J.Huang等;《OPTICAL MATERIALS EXPRESS》;20150930;正文第2节、第3节、附图1a、1b *

Also Published As

Publication number Publication date
CN108493756A (en) 2018-09-04

Similar Documents

Publication Publication Date Title
CN107565352B (en) A kind of laser exporting the tunable Laguerre Gaussian beam of 1064nm
CN101950918B (en) Self-frequency-doubling green light solid laser suitable for laser display
CN103618205A (en) Full-solid-state single longitudinal mode yellow light laser
CN107086430B (en) A kind of third harmonic generation ultraviolet laser
CN103036139A (en) Narrow-linewidth tunable semiconductor longitudinal single-ended pump rubidium steam laser optical path system
CN112421353A (en) Device for inhibiting gain narrowing and obtaining ultrashort pulse amplification output and adjusting method
CN102005694B (en) Single-end pumped intra-cavity frequency doubled ultraviolet solid laser
WO2019028679A1 (en) Frequency-doubling laser and harmonic laser light generating method
CN108493756B (en) YVO based on Nd4/Nd:GdVO4Double-frequency laser of combined crystal
CN205790929U (en) A kind of dye laser
CN216648854U (en) Orthogonal polarization dual-wavelength laser with adjustable proportion
CN102299464A (en) Microchip solid state laser
CN112886377A (en) Emerald gemstone continuous tunable laser pumped by 590nm waveband Raman frequency doubling light source
CN204103239U (en) A kind of all solid state single frequency tunable red laser
CN105470795A (en) All-solid-state yellow laser for medicine
CN106785854B (en) A kind of hydrogen fluoride optical maser wavelength selection output Foldaway unstable resonator
CN115498492A (en) Single-frequency diamond single crystal ultraviolet laser
CN114883896A (en) 2 mu m laser
CN104269731B (en) Sum frequency sodium beacon laser
CN208508230U (en) A kind of end face uniform pumping solid state laser
CN110632805B (en) Solid single-laser dual-wavelength pumping optical difference frequency terahertz wave generating device
CN113839294B (en) Y-shaped cavity tunable synchronous pulse dual-wavelength laser based on double crystals
CN111244734A (en) Mid-infrared single-mode laser
CN205319504U (en) Medical all -solid yellow laser
CN207183794U (en) Short cavity sticking-type 532nm semiconductor pump lasers

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
GR01 Patent grant
GR01 Patent grant
TR01 Transfer of patent right
TR01 Transfer of patent right

Effective date of registration: 20210603

Address after: 310018 room 2725, building 5, Fred Plaza, Baiyang street, Hangzhou Economic and Technological Development Zone, Zhejiang Province

Patentee after: HANGZHOU BOCHANG PHOTOELECTRIC TECHNOLOGY Co.,Ltd.

Address before: 310018 no.1158, No.2 street, Baiyang street, Hangzhou Economic and Technological Development Zone, Hangzhou, Zhejiang Province

Patentee before: HANGZHOU DIANZI University

TR01 Transfer of patent right
TR01 Transfer of patent right

Effective date of registration: 20220601

Address after: 518000 Guangdong Shenzhen Nanshan District science and Technology Park North area two long road 8, 305 building (305).

Patentee after: INNO LASER TECHNOLOGY Corp.,Ltd.

Address before: 310018 room 2725, building 5, Fred Plaza, Baiyang street, Hangzhou Economic and Technological Development Zone, Zhejiang Province

Patentee before: HANGZHOU BOCHANG PHOTOELECTRIC TECHNOLOGY CO.,LTD.