CN212323401U - Miniaturized human eye safety laser - Google Patents

Miniaturized human eye safety laser Download PDF

Info

Publication number
CN212323401U
CN212323401U CN201922269092.4U CN201922269092U CN212323401U CN 212323401 U CN212323401 U CN 212323401U CN 201922269092 U CN201922269092 U CN 201922269092U CN 212323401 U CN212323401 U CN 212323401U
Authority
CN
China
Prior art keywords
laser
human eye
miniaturized
cavity
crystal
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
CN201922269092.4U
Other languages
Chinese (zh)
Inventor
王万祎
赵子竣
王杰
丁戗
曾璞
胡少沛
温锋
余吉庆
张治旭
孙子泰
刘乙洁
张祎景
公丕华
黄颖全
陈方军
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.)
South West Institute of Technical Physics
Original Assignee
South West Institute of Technical Physics
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 South West Institute of Technical Physics filed Critical South West Institute of Technical Physics
Priority to CN201922269092.4U priority Critical patent/CN212323401U/en
Application granted granted Critical
Publication of CN212323401U publication Critical patent/CN212323401U/en
Active legal-status Critical Current
Anticipated expiration legal-status Critical

Links

Images

Abstract

The utility model discloses a be applied to laser rangefinder's miniaturized people's eye safety laser instrument, the utility model discloses a following technical scheme realizes: adopts the glass and crystal composite technology to add the gain medium Er3+/Yb3+Co-doped phosphate glass and passively Q-switched saturable Co2+:MgAl2O4The crystal is subjected to optical thermal recombination, and the composite material is reducedThe temperature gradient in the medium can be increased, so that the thermal focal length is lengthened, the mode volume is increased, and the quality of laser beams is improved; in addition, the composite material reduces the loss in the cavity, improves the particle number density in the cavity, narrows the pulse width and increases the output energy, thereby improving the performance of the laser. The utility model discloses a natural passive refrigerated mode makes the structure of whole laser more simple, compact, adopts the LD single tube laser terminal surface pumping of central wavelength 940nm, is adapted to wide temperature application range.

Description

Miniaturized human eye safety laser
Technical Field
The utility model belongs to the technical field of energy photoelectron and solid laser, a miniaturized human eye safety laser is related to.
Background
1.5 μm wavelength laser is in the communication window, and has wide application in the field of optical communication; meanwhile, laser with the wavelength of 1.5 mu m is positioned in a wave band insensitive to human eyes, and the smoke penetration capability is strong, so that the laser has great application potential. In particular to a 1.5 mu m wave band micro pulse laser with small volume, low power consumption, wide temperature adaptation range, high stability and low cost, and has wide application prospect in the laser ranging field of unmanned aerial vehicles, ranging telescopes, military affairs and the like.
At present, three technical methods for outputting 1.5-micron wavelength eye-safe laser are available: optical Parametric Oscillation (OPO), Stimulated Raman Scattering (SRS), and direct output. The OPO and SRS are usually obtained by converting a laser beam of 1.06 μm to a frequency, which results in a complicated system structure, is not suitable for military applications such as individual combat, and is also relatively expensive, which is not suitable for mass production. The direct output 1.5 μm laser is easy to be miniaturized compared with OPO and SRS, so that the method is the most ideal method for mass production and application. The direct output of 1.5 μm laser includes two modes, one is direct output of a semiconductor laser, and the other is obtained by pumping a gain medium through the semiconductor laser. The laser diode has poor beam quality, the semiconductor material is easily affected by temperature, and the stability is not high. The most common way to obtain the eye safety laser with 1.5 μm direct output is the LD pumped erbium glass, because the erbium-ytterbium co-doped phosphate glass has the characteristics of long upper energy level lifetime, high erbium-ytterbium energy transfer efficiency, difficult generation of fluorescence quenching, and the like, and the production condition is mature, and the LD pumped erbium glass is the most commonly used gain medium for directly outputting the eye safety laser with 1.5 μm low repetition frequency at present.
Currently, there are two main ways of LD-pumped erbium glass lasers, end-pumped and side-pumped. According to research, the side pumping mode mostly adopts an LD double-side pumping erbium glass plate strip mode, the mode can obtain single-pulse energy millifocal level laser output with the pulse width of about 10ns and the output of 1.5 mu m laser, but the mode of large-area conduction cooling is adopted, and very large temperature gradient exists in the thickness direction, so that wave front distortion, thermal birefringence and thermal lens effect are easily generated, therefore, the light beam quality is poor, and an external circulating water cooling system is required, so that the laser is huge in size and is very inconvenient to carry and use.
SUMMERY OF THE UTILITY MODEL
Objects of the invention
The utility model aims at: on the basis of an LD end-pumped erbium glass laser, a miniaturized eye-safe laser with better beam quality and higher light-light conversion efficiency is provided.
(II) technical scheme
In order to solve the technical problem, the utility model provides a miniature people's eye safety laser instrument, it includes by preceding pumping source 2 to the coaxial arrangement in back, focusing lens 3, transfer Q crystal 4, gain medium 5, transfer Q crystal 4 and gain medium 5 to pass through the light beam thermal recombination and form the combined material module, the front side of pumping source 2 arranges totally reflecting mirror 1, and the output mirror is arranged to the combined material module rear side.
The pumping source 2 is a TO-3 packaged LD, and the central wavelength is 940 nm.
The diameter of a waist spot on the light emitting surface of the pump source 2 is 250 micrometers, the fast axis divergence angle is smaller than 35 degrees, the slow axis divergence angle is 10 degrees, and the fast axis adopts an optical fiber fast axis collimating mirror with a 940nm antireflection film plated on the surface to compress the divergence angle.
Wherein, the total reflection mirror 1 is anti-reflection at 940nm and total reflection at 1535 nm.
Wherein the output mirror 6 has a transmittance of 10% at a wavelength of 1535 nm.
Wherein, the Q-switched crystal 4 is Co2 +: MgAl2O4 crystal with length of 1.6 mm; the gain medium 5 is Er3+/Yb3 +: glass, 3.0mm in length; the size after compounding is phi 1mm multiplied by 4.6 mm.
The composite material module is characterized in that one surface, close to the total reflection mirror, of the composite material module is plated with anti-reflection films with wavelengths of 940nm and 1535nm, one surface, close to the output mirror, of the composite material module is plated with anti-reflection films with wavelengths of 940nm and 1535nm, the cavity length is 4.6mm, the pumping pulse width is 7ms, and the repetition frequency is 10 Hz.
Wherein the laser cavity type is a flat-flat cavity.
(III) advantageous effects
The miniaturized eye safety laser provided by the technical scheme adopts a diode laser end with the central wavelength of 940nmThe laser output of 1.5 μm is obtained by surface pumping erbium glass, passively adjusting Q, and naturally and passively cooling, and the gain medium Er is used3+/Yb3+: /glass and passively Q-switched crystal Co2+:MgAl2O4The optical thermal compounding is carried out, the loss in the cavity is reduced, the particle number density in the cavity is improved, the single pulse output energy is increased, the output pulse width is reduced, the beam quality of output laser is improved, meanwhile, a natural cooling mode is adopted, the traditional huge cooling system is avoided, and the size of the whole laser is reduced by a large degree.
Drawings
Fig. 1 is a schematic diagram of a miniature eye-safe laser.
Fig. 2 is a schematic diagram of a micro eye-safe laser structure.
Detailed Description
In order to make the objects, contents, and advantages of the present invention clearer, the following description of the embodiments of the present invention will be made in detail with reference to the accompanying drawings and examples.
As shown in fig. 1 and 2, the utility model discloses miniature people's eye safety laser includes by preceding pumping source 2 to back coaxial arrangement, focusing lens 3, transfer Q crystal 4, gain medium 5, transfers Q crystal 4 and gain medium 5 to pass through the compound composite material module of light beam thermal recombination formation, the front side arrangement total reflection mirror 1 of pumping source 2, the output mirror is arranged to the composite material module rear side.
The laser of the embodiment adopts an end-face pumping mode, the pumping source 2 is a TO-3 packaged LD with a center wavelength of 940nm, compared with a wavelength of 976nm, Yb3+The absorption cross section around 940nm wavelength has small change with temperature, when the wavelength of the pump light is shifted, the laser output does not change too much, which is beneficial to the stability of the ultrahigh laser; the diameter of a waist spot on a light emitting surface of the LD is 250um, the fast axis divergence angle is smaller than 35 degrees, the slow axis divergence angle is 10 degrees, the fast axis adopts an optical fiber fast axis collimating mirror with a 940nm antireflection film plated on the surface to compress the divergence angle, a focusing lens 3 with the focal length of 5mm is adopted for focusing, and the beam waist of the focused light spot is about 80 um.
The laser cavity type is flat-flat cavity, total reflection mirror 1 is anti-reflection to 940nm and total reflection to 1535nm, and output mirror 6 has a transmittance of 10% to 1535nm wavelength.
In the composite material module, the Q-switched crystal 4 is Co2+:MgAl2O4A crystal having a length of 1.6 mm; the gain medium 5 is Er3+/Yb3+: glass, 3.0mm in length; the size after compounding is phi 1mm multiplied by 4.6 mm. One surface of the composite material module close to the total reflection mirror is plated with anti-reflection films with the wavelengths of 940nm and 1535nm, one surface of the composite material module close to the output mirror is plated with a total reflection film with the wavelengths of 940nm and an anti-reflection film with the wavelengths of 1535nm, the cavity length is 4.6mm, the pumping pulse width is 7ms, and the repetition frequency is 10 Hz.
According to the above technical scheme, the utility model has the following characteristics of showing:
(1) the end-face pumping of the LD single-tube laser with the central wavelength of 940nm is adopted, so that the wide temperature use range is adapted;
(2) the gain medium and the passive Q-switched crystal are subjected to optical thermal compounding, and compared with a traditional structure that the gain medium and the passive Q-switched crystal are separated, the thermal deposition of erbium glass can be reduced by adopting a compounding technology, the thermal depolarization and the end face deformation are reduced, the loss in a cavity is reduced, and the particle number density in the cavity is improved, so that the single-pulse output energy is increased, the output pulse width is reduced, and the beam quality of output laser is improved;
(3) the laser adopts a natural passive cooling mode, so that the structure of the whole laser is simpler and more compact.
The foregoing is only a preferred embodiment of the present invention, and it should be noted that, for those skilled in the art, a plurality of modifications and variations can be made without departing from the technical principle of the present invention, and these modifications and variations should also be considered as the protection scope of the present invention.

Claims (8)

1. The miniaturized human eye safety laser is characterized by comprising a pumping source (2), a focusing lens (3), a Q-switched crystal (4) and a gain medium (5) which are coaxially arranged from front to back, wherein the Q-switched crystal (4) and the gain medium (5) are thermally compounded through light beams to form a composite material module, a total reflection mirror (1) is arranged on the front side of the pumping source (2), and an output mirror is arranged on the rear side of the composite material module.
2. Miniaturized human eye safe laser according TO claim 1, characterized in that the pump source (2) is a TO-3 package LD with a center wavelength of 940 nm.
3. The miniaturized human eye safe laser device according to claim 2, wherein the diameter of the waist spot of the light emitting surface of the pump source (2) is 250um, the fast axis divergence angle is less than 35 degrees, the slow axis divergence angle is 10 degrees, and the fast axis adopts the compression divergence angle of the optical fiber fast axis collimating mirror with the surface plated with 940nm antireflection film.
4. A miniaturized human eye safe laser according to claim 3, characterized in that the total reflection mirror (1) is anti-reflective at 940nm and totally reflective at 1535 nm.
5. A miniaturized human eye-safe laser according to claim 4, characterized in that the output mirror (6) has a transmission of 10% at a wavelength of 1535 nm.
6. Miniaturized human eye safe laser according to claim 5, characterized in that the Q-switched crystal (4) is Co2 +: MgAl2O4 crystal with length of 1.6 mm; the gain medium (5) is Er3+/Yb3 +: glass, 3.0mm in length; the size after compounding is phi 1mm multiplied by 4.6 mm.
7. The miniaturized human eye safe laser of claim 6, wherein the surface of the composite module near the total reflection mirror is plated with anti-reflection films with wavelengths of 940nm and 1535nm, the surface near the output mirror is plated with anti-reflection films with wavelengths of 940nm and 1535nm, the cavity length is 4.6mm, the pumping pulse width is 7ms, and the repetition frequency is 10 Hz.
8. The miniaturized eye-safe laser of claim 1, wherein the laser cavity type is a plano-plano cavity.
CN201922269092.4U 2019-12-17 2019-12-17 Miniaturized human eye safety laser Active CN212323401U (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
CN201922269092.4U CN212323401U (en) 2019-12-17 2019-12-17 Miniaturized human eye safety laser

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
CN201922269092.4U CN212323401U (en) 2019-12-17 2019-12-17 Miniaturized human eye safety laser

Publications (1)

Publication Number Publication Date
CN212323401U true CN212323401U (en) 2021-01-08

Family

ID=74029617

Family Applications (1)

Application Number Title Priority Date Filing Date
CN201922269092.4U Active CN212323401U (en) 2019-12-17 2019-12-17 Miniaturized human eye safety laser

Country Status (1)

Country Link
CN (1) CN212323401U (en)

Similar Documents

Publication Publication Date Title
Lü et al. Dual-wavelength laser operation at 1064 and 914 nm in two Nd: YVO 4 crystals
CN111653926A (en) Miniaturized human eye safety pulse laser
CN210201151U (en) All-solid-state green laser
CN100428587C (en) Laser diode side pumped thulium/holmium double doped lithium lutetium fluoride crystal laser
CN111769427A (en) Erbium-doped wedge waveguide amplifier capable of realizing high efficiency, large energy and small volume
CN101807774B (en) Self-stimulated Raman scattering laser of In-Band pump
CN101814695B (en) Directly-pumping self-stimulated Raman scattering human eye safe waveband laser
CN103050870B (en) Novel microchip laser supporting optical fiber output
CN102208745A (en) Miniaturized passive Q-switching eye-safe Raman laser
CN106058632B (en) A kind of adjustable passive Q-adjusted raman laser system of pulse energy based on bonded crystals
Burns et al. CW diode-pumped microlaser operation at 1.5-1.6 μm in Er, Yb: YCOB
CN111106517A (en) Erbium-doped fiber laser with same pump for random Raman fiber laser
CN203645130U (en) High-power glass-doped laser device
CN113594842A (en) Device and method for generating ultrashort pulse of erbium-doped laser
CN111370988B (en) 1.55 mu m wave band Q-switched pulse laser
CN212323401U (en) Miniaturized human eye safety laser
CN106532422A (en) Six-wavelength output passively Q-switched c-cut Nd:YVO4 self-Raman all-solid-state laser
CN201243158Y (en) Medium-infrared thulium doped optical fiber laser amplifier
US7003011B2 (en) Thin disk laser with large numerical aperture pumping
US20220209491A1 (en) Structure and configuration of the passively q-switched diode end-pumped solid-state laser
Zhang et al. A compact high power laser-diode side-pumped Tm, Ho: YAG laser nearly at room temperature with intracavity Tm: YAG laser
Lü et al. 1064 nm Nd: YAG laser intracavity pumped at 946 nm
CN201001003Y (en) Laser diode side pumped thulium/holmium double doped lithium lutetium fluoride crystal laser
CN211859139U (en) All-solid-state femtosecond laser of Kerr mode-locked ytterbium-doped lanthanum gadolinium silicate crystal
CN209544812U (en) A kind of big energy femto-second laser of high power

Legal Events

Date Code Title Description
GR01 Patent grant
GR01 Patent grant