CN103594919A - Device capable of improving linear polarization laser output of solid laser - Google Patents

Device capable of improving linear polarization laser output of solid laser Download PDF

Info

Publication number
CN103594919A
CN103594919A CN201310566040.8A CN201310566040A CN103594919A CN 103594919 A CN103594919 A CN 103594919A CN 201310566040 A CN201310566040 A CN 201310566040A CN 103594919 A CN103594919 A CN 103594919A
Authority
CN
China
Prior art keywords
laser
light
reflective mirror
total reflective
polarization state
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
CN201310566040.8A
Other languages
Chinese (zh)
Inventor
王丽荣
林学春
王宝华
郭渭荣
王祥鹏
陈凯
曲研
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.)
Institute of Semiconductors of CAS
Original Assignee
Institute of Semiconductors of CAS
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by Institute of Semiconductors of CAS filed Critical Institute of Semiconductors of CAS
Priority to CN201310566040.8A priority Critical patent/CN103594919A/en
Publication of CN103594919A publication Critical patent/CN103594919A/en
Pending legal-status Critical Current

Links

Images

Landscapes

  • Lasers (AREA)
  • Semiconductor Lasers (AREA)

Abstract

本发明公开了一种提高固体激光器线偏振激光输出的装置,其包括第一全反镜、半导体激光线阵侧泵激光模块、偏振器件、第二全反镜和功率计;其中,所述半导体激光线阵侧泵激光模块发出的激光在第一全反镜、半导体激光线阵侧泵激光模块、偏振器件与第二全反镜之间形成振荡,且在经过偏振器件后呈p偏振态或s偏振态的激光被功率计接收。该装置可使从线偏振输出光中被分离开的另一部分光重新回到谐振腔中得以充分利用,从而使最终的线偏振输出光功率大大提高;不仅如此,该装置还可以灵活调节固体激光器线偏振输出的方向,使其输出的线偏振光既可以呈s偏振态又可以呈p偏振态,进而使固体激光器的应用更加灵活,适用范围更加广泛。

Figure 201310566040

The invention discloses a device for improving the linearly polarized laser output of a solid-state laser, which includes a first total reflection mirror, a semiconductor laser linear array side-pumped laser module, a polarization device, a second total reflection mirror and a power meter; wherein the semiconductor The laser light emitted by the side-pumped laser module of the laser line array oscillates between the first total reflection mirror, the side-pump laser module of the semiconductor laser line array, the polarizer and the second total reflection mirror, and is in a p-polarized state or The s-polarized laser light is received by a power meter. The device can make full use of another part of the light separated from the linearly polarized output light and return to the resonator, so that the final linearly polarized output light power is greatly improved; not only that, but the device can also flexibly adjust the solid-state laser The direction of the linearly polarized output enables the output linearly polarized light to be in either the s-polarized state or the p-polarized state, so that the application of the solid-state laser is more flexible and the scope of application is wider.

Figure 201310566040

Description

A kind of device that improves the output of solid state laser linearly polarized laser
Technical field
The present invention relates to semiconductor laser technique field, relate in particular to a kind of device that combines to improve the output of solid state laser linearly polarized laser with polarizer with L-type resonant cavity.
Background technology
Along with the development of laser technology, people are more and more higher to the requirement of the power output of laser.Yet along with the increase of diode pumped power, the thermal effect of laser medium is more and more obvious, causes the phenomenons such as thermally induced birefringence.The laser that needs linearly polarized light beam for running, as electric-optically Q-switched, frequency translation and light beam external modulation etc., the Depolarization being caused by thermally induced birefringence will obviously increase, and this makes directly from the laser of laser output, can not present single linear polarization characteristic.And in this case on the market the common device that obtains linear polarization output make the linearly polarized laser power loss of final output serious, linear polarization delivery efficiency is generally on the low side.
Summary of the invention
It is serious that the present invention is intended to improve in existing great-power solid laser the hot depolarization phenomenon of laser medium, to such an extent as to the laser of exporting can not present single linear polarization characteristic, has a strong impact on this situation of linear polarization power output of laser.
According to an aspect of the present invention, it provides a kind of device that improves the output of solid state laser linearly polarized laser, and it comprises the first total reflective mirror, semiconductor laser linear array side-pump laser module, polarizer, the second total reflective mirror and power meter; Wherein, the laser that described semiconductor laser linear array side-pump laser module is sent forms vibration between the first total reflective mirror, semiconductor laser linear array side-pump laser module, polarizer and the second total reflective mirror, and is received by power meter at the laser that is p polarization state or s polarization state after polarizer.
Wherein, polarizer surface is coated with polarization beam splitter, when laser beam incidence angle is at a certain angle incident to polarizer, in laser beam the light of p polarization state can be directly through polarizer and along straightline propagation, and the light of s polarization state can reflect.
Wherein, the second total reflective mirror is placed perpendicular to the light that is polarized the s polarization state that device separates or the light of p polarization state is placed.
Wherein, described the first total reflective mirror and the second total reflective mirror form laserresonator, and the second total reflective mirror is also used for residue laser reflection is returned to resonant cavity.
Wherein, when total reflective mirror is placed perpendicular to the light of s polarization state, described power meter is for receiving the light of p polarization state, and total reflective mirror is when place perpendicular to the light of p polarization state, and described power meter is for receiving the light of s polarization state.
Wherein, described certain angle is 56 ° of angles.
The present invention has following beneficial effect:
Polarization laser output device provided by the present invention, can make each part light all be fully utilized, there is the linear polarization delivery efficiency obviously improving than general polarization laser output device, and the laser rays polarization state of its output can change flexibly between p and s, has convenient and practical outstanding characteristic.This device can be applied in all laser production processes to be had in the laser of Depolarization.
Accompanying drawing explanation
Fig. 1 is the structure drawing of device that improves the output of solid state laser linearly polarized laser in first embodiment of the invention;
Fig. 2 is the structure drawing of device that improves the output of solid state laser linearly polarized laser in second embodiment of the invention.
Embodiment
For making the object, technical solutions and advantages of the present invention clearer, below in conjunction with specific embodiment, and with reference to accompanying drawing, the present invention is described in further detail.
Fig. 1 shows a kind of device that improves the output of solid state laser linearly polarized laser proposing in first embodiment of the invention.As shown in Figure 1, this device comprises: total reflective mirror 1, semiconductor laser linear array side-pump laser module 2, polarizer 3, total reflective mirror 4 and power meter 5.
Wherein, total reflective mirror 1 and polarizer 3 are positioned at the both sides of semiconductor laser side-pump laser module 2, described semiconductor laser linear array side-pump laser module 2 is for sending laser, described polarizer 3 surfaces are coated with polarization beam splitter, and the laser that its surface and described semiconductor laser linear array side-pump laser module 2 are sent at an angle, and this angle is preferably 56 °; When described laser beam is incident to polarizer 3 with this certain angle, in laser beam the light of p polarization state can be directly through polarizer 3 and along straightline propagation, and the light of s polarization state is reflected.
Described total reflective mirror 4 is placed perpendicular to the light path of described p polarization state light or s polarization state light, and for reflecting p light or s light, and power meter 5 is placed on the light path of described s polarization state light or p polarization state light, the s polarised light or the p polarised light that for receiving this device of detection, produce.When the s light after total reflective mirror 4 separates perpendicular to quilt is placed, form laserresonator with total reflective mirror 1, the light that semiconductor laser linear array side-pump laser module 2 is sent forms vibration between total reflective mirror 1, semiconductor laser linear array side-pump laser module 2, polarizer 3 and total reflective mirror 4, after polarizer 3, be the directly output of laser of p polarization, by power meter 5, received and survey.
When the p light after total reflective mirror 4 separates perpendicular to quilt is placed, form laserresonator with total reflective mirror 1, the light that semiconductor laser linear array side-pump laser module 2 is sent forms vibration between total reflective mirror 1, semiconductor laser linear array side-pump laser module 2, polarizer 3 and total reflective mirror 4, after polarizer 3, be the directly output of laser of s polarization, by power meter 5, received and survey.Fig. 1 is total reflective mirror 4 perpendicular to the situation of being placed by the s light after separately, and now total reflective mirror 4 forms laserresonator with total reflective mirror 1, and the s polarised light being separated by polarizing device 3 is returned and in resonant cavity, again participates in laser generation by total reflective mirror 4 total reflections.The light that semiconductor laser linear array side-pump laser module 2 is sent forms vibration between total reflective mirror 1, semiconductor laser linear array side-pump laser module 2, polarizer 3 and total reflective mirror 4, after polarizer 3, be the directly output of laser of p polarization, by power meter 5, received and survey.
Fig. 2 is a kind of device that improves the output of solid state laser linearly polarized laser proposing in second embodiment of the invention.As shown in Figure 2, in this embodiment, total reflective mirror 4 is perpendicular to being placed by the p light after separately, and now total reflective mirror 4 and total reflective mirror 1 form laserresonator, and the p polarised light being separated by polarizing device 3 is returned and in resonant cavity, again participates in laser generation by total reflective mirror 4 total reflections.The light that semiconductor laser linear array side-pump laser module 2 is sent forms vibration between total reflective mirror 1, semiconductor laser linear array side-pump laser module 2, polarizer 3 and total reflective mirror 4, after polarizer 3, be the directly output of laser of s polarization, by power meter 5, received and survey
Above-described specific embodiment; object of the present invention, technical scheme and beneficial effect are further described; be understood that; the foregoing is only specific embodiments of the invention; be not limited to the present invention; within the spirit and principles in the present invention all, any modification of making, be equal to replacement, improvement etc., within all should being included in protection scope of the present invention.

Claims (6)

1. a device that improves the output of solid state laser linearly polarized laser, it comprises the first total reflective mirror, semiconductor laser linear array side-pump laser module, polarizer, the second total reflective mirror and power meter; Wherein, the laser that described semiconductor laser linear array side-pump laser module is sent forms vibration between the first total reflective mirror, semiconductor laser linear array side-pump laser module, polarizer and the second total reflective mirror, and is received by power meter at the laser that is p polarization state or s polarization state after polarizer.
2. linearly polarized laser output device according to claim 1, it is characterized in that, polarizer surface is coated with polarization beam splitter, when laser beam incidence angle is at a certain angle incident to polarizer, in laser beam the light of p polarization state can be directly through polarizer and along straightline propagation, and the light of s polarization state can reflect.
3. linearly polarized laser output device according to claim 1, is characterized in that, the second total reflective mirror places perpendicular to the light that is polarized the s polarization state that device separates or the light of p polarization state is placed.
4. linearly polarized laser output device according to claim 1, is characterized in that, described the first total reflective mirror and the second total reflective mirror form laserresonator, and the second total reflective mirror is also used for residue laser reflection is returned to resonant cavity.
5. linearly polarized laser output device as claimed in claim 3, it is characterized in that, when total reflective mirror is placed perpendicular to the light of s polarization state, described power meter is for receiving the light of p polarization state, and total reflective mirror is when place perpendicular to the light of p polarization state, described power meter is for receiving the light of s polarization state.
6. linearly polarized laser output device as claimed in claim 2, is characterized in that, described certain angle is 56 ° of angles.
CN201310566040.8A 2013-11-14 2013-11-14 Device capable of improving linear polarization laser output of solid laser Pending CN103594919A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
CN201310566040.8A CN103594919A (en) 2013-11-14 2013-11-14 Device capable of improving linear polarization laser output of solid laser

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
CN201310566040.8A CN103594919A (en) 2013-11-14 2013-11-14 Device capable of improving linear polarization laser output of solid laser

Publications (1)

Publication Number Publication Date
CN103594919A true CN103594919A (en) 2014-02-19

Family

ID=50084954

Family Applications (1)

Application Number Title Priority Date Filing Date
CN201310566040.8A Pending CN103594919A (en) 2013-11-14 2013-11-14 Device capable of improving linear polarization laser output of solid laser

Country Status (1)

Country Link
CN (1) CN103594919A (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN105140772A (en) * 2015-09-30 2015-12-09 中国科学院合肥物质科学研究院 Electro-optic Q-switch capable of completely compensating for laser thermal depolarization

Citations (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN101106248A (en) * 2006-07-14 2008-01-16 北京国科世纪激光技术有限公司 A permeation rate adjustable laser
CN103217803A (en) * 2013-04-09 2013-07-24 中国科学院半导体研究所 Polarization coupling device for semi-conductor laser device adopting prism

Patent Citations (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN101106248A (en) * 2006-07-14 2008-01-16 北京国科世纪激光技术有限公司 A permeation rate adjustable laser
CN103217803A (en) * 2013-04-09 2013-07-24 中国科学院半导体研究所 Polarization coupling device for semi-conductor laser device adopting prism

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN105140772A (en) * 2015-09-30 2015-12-09 中国科学院合肥物质科学研究院 Electro-optic Q-switch capable of completely compensating for laser thermal depolarization
CN105140772B (en) * 2015-09-30 2018-05-15 中国科学院合肥物质科学研究院 A kind of electro-optical Q-switch that laser heat depolarization is fully compensated

Similar Documents

Publication Publication Date Title
CN103217803A (en) Polarization coupling device for semi-conductor laser device adopting prism
CN102244346B (en) End-pumped laser utilizing half-wave plates
CN105720469B (en) The laser of weak pumping laser efficiency is improved based on light polarization torsion
CN101022203A (en) YAG laser with double electro-optical modulation QNd
CN104184025A (en) Multi-pumping fiber laser structure
CN110034484A (en) A kind of novel Nd:YAG single-frequency loop laser resonance cavity
CN104051949A (en) Efficient compact end-pumped slab laser amplifier device
CN101872076B (en) Optical experiment and method for implementing optical isolation in optical fiber communication system and device thereof
CN102347585B (en) One-way traveling wave annular cavity single-frequency quasi-three-level solid laser
WO2020113743A1 (en) Small integrated free space circulator
CN113285338A (en) Method for improving pump light absorption efficiency of non-polarized absorption gain medium
CN217720243U (en) All-optical device integrated high-efficiency annular cavity optical parametric oscillator
CN107492784A (en) Improve the laser of asymmetric hot spot output
JP2007012981A (en) Laser device with highly reflective coating on the internal total reflection surface of optical element
CN103594919A (en) Device capable of improving linear polarization laser output of solid laser
CN110190492A (en) laser amplifier
CN110492344A (en) Without depolarization loss Nd:YAG annular chamber single-frequency laser
CN102723660B (en) Electro-optic Q-switched pulse laser device with repeat frequency being variable in wide range
CN103401129A (en) LD (laser diode)-pumped single longitudinal mode type continuous wave 1645nm solid laser device
CN103208730A (en) Solid laser with annular pump structure
CN103311794A (en) Solid laser with annular polarization compensation
CN211265957U (en) A Mutual-Injection Solid-State Laser With Embedded Polarization-Maintaining Wave Plates
CN102263364B (en) Transverse plane pump laser capable of high efficiently using pump light
CN102723661B (en) Electro-optic Q-switching and acousto-optic Q-switching pulse laser capable of quickly converting Q-switching modes
CN102157897A (en) Pulse width-adjustable solid laser

Legal Events

Date Code Title Description
C06 Publication
PB01 Publication
SE01 Entry into force of request for substantive examination
SE01 Entry into force of request for substantive examination
C02 Deemed withdrawal of patent application after publication (patent law 2001)
WD01 Invention patent application deemed withdrawn after publication

Application publication date: 20140219