WO2021120487A1 - 一种电光调q腔内倍频亚纳秒脉冲绿光激光器 - Google Patents

一种电光调q腔内倍频亚纳秒脉冲绿光激光器 Download PDF

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WO2021120487A1
WO2021120487A1 PCT/CN2020/087510 CN2020087510W WO2021120487A1 WO 2021120487 A1 WO2021120487 A1 WO 2021120487A1 CN 2020087510 W CN2020087510 W CN 2020087510W WO 2021120487 A1 WO2021120487 A1 WO 2021120487A1
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electro
frequency
optical
sub
switched
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PCT/CN2020/087510
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French (fr)
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于广礼
丁建永
肖湖福
郭忠纪
周军
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南京先进激光技术研究院
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    • H—ELECTRICITY
    • H01—ELECTRIC ELEMENTS
    • H01S—DEVICES 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
    • H01S5/00—Semiconductor lasers
    • H01S5/06—Arrangements for controlling the laser output parameters, e.g. by operating on the active medium
    • H01S5/0615—Q-switching, i.e. in which the quality factor of the optical resonator is rapidly changed
    • H—ELECTRICITY
    • H01—ELECTRIC ELEMENTS
    • H01S—DEVICES 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
    • H01S5/00—Semiconductor lasers
    • H01S5/02—Structural details or components not essential to laser action
    • H01S5/022—Mountings; Housings
    • H01S5/0225—Out-coupling of light
    • H01S5/02253—Out-coupling of light using lenses
    • H—ELECTRICITY
    • H01—ELECTRIC ELEMENTS
    • H01S—DEVICES 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
    • H01S5/00—Semiconductor lasers
    • H01S5/06—Arrangements for controlling the laser output parameters, e.g. by operating on the active medium
    • H01S5/062—Arrangements for controlling the laser output parameters, e.g. by operating on the active medium by varying the potential of the electrodes
    • H01S5/06233—Controlling other output parameters than intensity or frequency
    • H01S5/06236—Controlling other output parameters than intensity or frequency controlling the polarisation, e.g. TM/TE polarisation switching

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  • the invention relates to the field of laser technology, in particular to an electro-optic Q-switched intracavity frequency-doubled sub-nanosecond pulsed green laser.
  • Sub-nanosecond pulsed green laser refers to a green laser with a pulse width of less than 1ns. Compared with the traditional Q-switched nanosecond pulse laser (10 ⁇ 100ns pulse width), it has the advantages of narrow pulse width and high peak power. For nano-processing applications, it can reduce the heat-affected zone of processing and improve processing efficiency; corresponding to laser ranging applications, under the same energy, sub-nanosecond pulse width lasers have a better ranging accuracy than a few nanosecond pulse width lasers and tens of seconds pulse width lasers. Ranging distance can be increased several times to dozens of times.
  • sub-nanosecond pulse lasers Compared with infrared pulsed lasers, it has the advantages of short wavelength, etc., and has a wide range of applications in laser ocean radar, laser fine processing, laser medical treatment, and nonlinear optics.
  • Commonly used methods for generating sub-nanosecond pulse lasers include passively Q-switched microchip lasers, short-cavity electro-optic Q-switched lasers, mode-locked lasers, cavity emptying, SBS compressed pulse width, and electrically modulated semiconductor lasers.
  • the traditional sub-nanosecond pulsed green lasers are generally realized by extra-cavity frequency doubling. Since the frequency doubling efficiency is directly proportional to the peak power density of the fundamental frequency light, some applications are used to improve the frequency doubling efficiency. Shaping optical elements are added between the devices, so the entire optical path has disadvantages such as complex structure, low light-to-light conversion efficiency, and large size.
  • the technical problem to be solved by the present invention is to provide an electro-optical Q-switched intracavity frequency-doubled sub-nanosecond pulsed green laser, which can achieve high-efficiency and compact structure of sub-nanosecond pulsed green laser output, thereby satisfying laser micromachining, Applications in the fields of laser ranging, laser medical treatment, scientific research, etc.
  • the present invention provides an electro-optical Q-switched intracavity frequency-doubled sub-nanosecond pulsed green laser, including: a pump source, a pump coupling element, a polarization beam splitter, a laser gain medium, and a ⁇ /4 wave plate , Electro-optical switch, fundamental frequency resonator mirror, harmonic separation, frequency doubling crystal and fundamental frequency/frequency doubling resonator mirror; the pump light emitted by the pump source is focused into the gain medium by the pump coupling element, and is polarized
  • the beam splitting prism, the fundamental frequency resonator mirror, and the fundamental frequency/frequency doubling cavity reflector form an L-shaped folded resonator.
  • the ⁇ /4 wave plate and the electro-optical switch are on one arm of the folded cavity, and the harmonic separation and frequency doubling crystal On the other arm of the cavity.
  • the pump source output mode is spatial light output or fiber coupled output, and the pump mode is pulse pumping or continuous pumping.
  • the pump coupling element adopts a single lens or a lens group structure to couple the pump light into the laser gain medium with a certain spot size.
  • the resonant cavity of the laser adopts an L-shaped folded cavity structure
  • a polarization beam splitting prism is used as a folding mirror of the resonant cavity
  • the polarization beam splitting prism simultaneously functions as a polarizer and a resonant cavity folding mirror in the resonant cavity.
  • the glossy surface also needs to be coated with a pump light anti-reflection coating.
  • the laser gain medium is Nd:YVO 4 crystal, Nd:GdVO 4 crystal, Nd:YAG crystal, Nd:YLF crystal, and can output a laser crystal with a wavelength of 1 ⁇ m.
  • the laser gain medium and the ⁇ /4 wave plate laser electro-optical switch are placed on one arm of the folded cavity, and work together with the polarization splitting prism to realize electro-optical Q-switching; the harmonic separator and the frequency doubling crystal are placed on the other side of the resonant cavity.
  • the polarization output of the fundamental frequency light is matched with the polarization of the frequency doubling crystal to achieve the maximum frequency doubling efficiency.
  • the laser adopts electro-optical Q-switching mode to work, and the Q-switching mode can be pressurized electro-optical Q-switching or decompression electro-optical Q-switching.
  • the electro-optical switch may be an RTP electro-optical switch, BBO electro-optical switch, LGS electro-optical switch, LN electro-optical switch or KD*P electro-optical switch.
  • the frequency doubling mode adopts intracavity frequency doubling.
  • the phase matching mode of the frequency doubling crystal can be critical phase matching or non-critical phase matching;
  • the output mode of the frequency doubling light is to insert harmonics between the polarization beam splitting prism and the frequency doubling crystal. Separating mirror, the incident angle of the harmonic separator is 45° or other angles, which can realize the fundamental frequency light passing through and the frequency-doubled light output;
  • the frequency-doubled crystals are LBO crystal, KTP crystal, PPLN crystal, BBO crystal.
  • the present invention realizes the sub-nanosecond pulsed green laser output with high frequency doubling efficiency through the short cavity structure, intracavity frequency doubling, and electro-optic Q-switching mode, which can be directly used for sub-nanosecond pulsed green light.
  • the sub-nanosecond pulse output is realized through intracavity frequency doubling, which has the advantages of compact structure, high efficiency, stability and reliability, and low cost.
  • Figure 1 is a schematic diagram of the laser structure of the present invention.
  • an electro-optical Q-switched intracavity frequency-doubled sub-nanosecond pulsed green laser includes: pump source, pump coupling element, polarization beam splitter, laser gain medium, ⁇ /4 wave plate, electro-optical switch , Fundamental frequency resonator mirror, harmonic separation environment, frequency doubling crystal and fundamental frequency/frequency doubling resonator mirror; the pump light emitted by the pump source is focused into the gain medium by the pump coupling element, and the polarization beam splitting prism and The fundamental frequency resonant cavity mirror and the fundamental frequency/frequency doubled resonant cavity reflector constitute an L-shaped folded resonator.
  • the ⁇ /4 wave plate and the electro-optical switch are on one arm of the folded cavity, and the harmonic separation and frequency doubling crystal are in the resonant cavity. On the other arm.
  • the laser of the present invention is a semiconductor laser end-pumped, pressurized electro-optical Q-switching, and the resonance adopts a three-mirror folded cavity structure, and can realize sub-nanosecond pulsed green light output through intracavity frequency doubling.
  • the pump source 1 is used to generate laser light with a certain spectral line width and is used to pump the laser gain medium 2. In order to achieve higher conversion efficiency, the output spectral line should match the absorption spectral line of the laser gain medium 2.
  • the output mode of the middle pump source can be a semiconductor laser with spatial light output, or a semiconductor laser with fiber coupled output, and the pump mode is continuous pumping or pulse pumping.
  • the pump coupling element 2 is used to couple the laser light generated by the pump source 1 into the laser gain medium 2 with a specific spot diameter to realize the mode matching of the pump light and the oscillating light in the resonance. It can be a single lens or a lens composed of multiple lenses. Group, the surface of the lens is plated with an anti-reflection coating for the pump source 1.
  • the polarization beam splitting prism 3 mainly plays two roles in resonance. First, as a folding mirror of the resonant cavity, it plays the role of turning the light path. Second, as the polarizer in the resonant cavity, the gain medium is generated. The laser light becomes linearly polarized light.
  • the right-angled surface of the polarization beam splitting prism of this embodiment is coated with an anti-reflection coating for the pump light and the fundamental frequency laser, and the inclined surface is coated with an anti-reflection coating for the pump light and a polarization coating for the fundamental frequency light.
  • the polarization beam splitting prism 3 may also be a polarizing plate in the form of a dielectric film.
  • the laser gain medium 4 realizes population inversion after absorbing the pump light of the pump source 1.
  • the gain in the gain medium is greater than the loss of the resonant cavity, laser oscillation can be established, which is a necessary element for laser generation.
  • the laser gain medium is Nd:YVO 4 crystal.
  • the ⁇ /4 wave plate 5 and the electro-optical switch 6 play the role of polarization conversion in the resonant cavity to realize Q-switched pulse output.
  • the laser is a pressurized electro-optic Q-switch.
  • the fast axis direction of the ⁇ /4 wave plate 5 and the direction of the linearly polarized light generated by the laser gain medium 4 and the polarization beam splitting prism 3 form an angle of 45°, which transforms the linearly polarized light into Into circularly polarized light.
  • the electro-optical switch 6 is not applied with the ⁇ /4 voltage, the circularly polarized light is reflected by the fundamental frequency optical resonator mirror 7, and then becomes linearly polarized light after passing through the ⁇ /4 wave plate 5.
  • the electro-optical switch 6 in this embodiment is an RTP electro-optical switch.
  • the fundamental frequency resonant cavity mirror 7 is mainly a mirror that realizes fundamental frequency light.
  • the resonant cavity mirror 7 is a 0° reflector, and the surface can be a flat surface, a concave surface, or a convex surface.
  • the harmonic separator 8 is mainly used to separate the fundamental frequency light from the frequency doubled light.
  • the surface of the reflector is coated with a coating for fundamental frequency light enhancement and frequency doubled light reflection to output the frequency doubled light outside the resonance.
  • the incident angle of the harmonic separator in this embodiment is 45°.
  • the frequency doubling crystal 9 mainly converts the wavelength of the fundamental frequency light into the frequency-doubled green light output through nonlinear frequency conversion.
  • the frequency doubling crystal is an LBO crystal.
  • the fundamental frequency/frequency doubling resonator mirror 10 mainly realizes the simultaneous reflection of the fundamental frequency light and the frequency doubling light. In this way, the fundamental frequency light can be double-passed and doubled in the frequency doubling crystal to improve the frequency doubling efficiency.
  • the fundamental frequency/frequency doubling resonant cavity mirror 10 is a 0° mirror, and the surface can be a flat surface, a concave surface, or a convex surface.

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  • Physics & Mathematics (AREA)
  • Condensed Matter Physics & Semiconductors (AREA)
  • General Physics & Mathematics (AREA)
  • Electromagnetism (AREA)
  • Optics & Photonics (AREA)
  • Optical Modulation, Optical Deflection, Nonlinear Optics, Optical Demodulation, Optical Logic Elements (AREA)
  • Lasers (AREA)

Abstract

一种电光调Q腔内倍频亚纳秒脉冲绿光激光器，包括：泵浦源(1)、泵浦耦合元件(2)、偏振分光棱镜(3)、激光增益介质(4)、λ/4波片(5)、电光开关(6)、基频谐振腔反射镜(7)、谐波分离镜(8)、倍频晶体(9)和基频/倍频谐振腔反射镜(10)。通过短腔结构、腔内倍频、电光调Q方式，实现了高倍频效率的亚纳秒脉冲绿光激光输出，可以直接用于需要亚纳秒脉冲绿光激光器的场合；通过腔内倍频的方式，实现亚纳秒脉冲输出，具有结构紧凑、效率高、稳定可靠、成本低等优点。

Description

一种电光调Q腔内倍频亚纳秒脉冲绿光激光器 技术领域
本发明涉及激光技术领域，尤其是一种电光调Q腔内倍频亚纳秒脉冲绿光激光器。
背景技术
亚纳秒脉冲绿光激光器是指脉冲宽度小于1ns的绿光激光器，与传统的调Q纳秒脉冲激光(10～100ns脉宽)相比，具有脉宽窄，峰值功率高等优点，对于激光微纳加工应用来说可以减小加工的热影响区，改善加工效率；对应激光测距应用，在相同能量下，亚纳秒脉宽激光比几纳、几十秒脉宽激光的测距精度及测距距离可以提高几倍至几十倍。相比于红外脉冲激光器，具有波长短等优点，在激光海洋雷达、激光精细加工、激光医疗、非线性光学等方面都有广泛的应用。常用的亚纳秒脉冲激光器的产生方法有被动调Q微片激光器、短腔电光调Q激光器、锁模激光器、腔倒空、SBS压缩脉宽、电调制半导体激光器等。而传统亚纳秒脉冲绿光激光器一般是通过腔外倍频来实现的，由于倍频效率与基频光的峰值功率密度有成正比，有些应用为了提升倍频效率，在基频及倍频装置之间加入整形光学元件，因此整个光路存在结构复杂，光光转换效率低，尺寸大等缺点。
发明内容
本发明所要解决的技术问题在于，提供一种电光调Q腔内倍频亚纳秒脉冲绿光激光器，能够实现高效率、结构紧凑的亚纳秒脉冲绿光激光输出，从而满足激光微加工、激光测距、激光医疗、科研等领域的应用。
为解决上述技术问题，本发明提供一种电光调Q腔内倍频亚纳秒脉冲绿光激光器，包括：泵浦源、泵浦耦合元件、偏振分光棱镜、激光增益介质、λ/4波片、电光开关、基频谐振腔反射镜、谐波分离境、倍频晶体和基频/倍频谐振腔反射镜；泵浦源发射的泵浦光经泵浦耦合元件聚焦到增益介质内，偏振分光棱镜与基频谐振腔反射镜、基频/倍频谐振腔反射镜构成L型折叠谐振腔，λ/4波片与电光开关在折叠腔的一个臂上，谐波分离境和倍频晶体在谐振腔的另一个臂上。
优选的，泵浦源输出方式为空间光输出或光纤耦合输出，泵浦方式为脉冲泵浦或连续泵浦。
优选的，泵浦耦合元件采用单透镜或透镜组结构，将泵浦光以一定光斑尺寸耦合到激光增益介质内。
优选的，激光器的谐振腔采用L型折叠腔结构，偏振分光棱镜作为谐振腔的折叠镜，偏振分光棱镜在谐振腔内同时起到偏振片及谐振腔折叠镜的作用，此偏振分光棱镜的通光面同时需要镀有泵浦光增透膜。
优选的，激光增益介质为Nd:YVO 4晶体、Nd:GdVO 4晶体、Nd:YAG晶体、Nd:YLF晶体，能够输出1μm波长的激光晶体。
优选的，激光增益介质、λ/4波片激光电光开关放在折叠腔的一个臂上，与偏振分光棱镜共同作用实现电光调Q；谐波分离镜及倍频晶体放在谐振腔的另一臂上，实现基频光线偏振输出与倍频晶体倍频的偏振匹配，实现最大倍频效率。
优选的，激光器采用电光调Q方式工作，调Q方式可以是加压式电光调Q或退压式电光调Q。
优选的，电光开光可以为RTP电光开关、BBO电光开关、LGS电光开关、LN电光开关或KD*P电光开关。
优选的，倍频方式采用腔内倍频，倍频晶体的相位匹配方式可以是临界相位匹配或非临界相位匹配；倍频光的输出方式为在偏振分光棱镜与倍频晶体之间插入谐波分离镜，谐波分离镜的入射角度为45°或其他角度，可以实现基频光通过，倍频光输出；倍频晶体为LBO晶体、KTP晶体、PPLN晶体、BBO晶体。
本发明的有益效果为：本发明通过短腔结构、腔内倍频、电光调Q方式，实现了高倍频效率的亚纳秒脉冲绿光激光输出，可以直接用于需要亚纳秒脉冲绿光激光器的场合；通过腔内倍频的方式，实现亚纳秒脉冲输出，具有结构紧凑、效率高、稳定可靠、成本低等优点。
附图说明
图1为本发明的激光器结构示意图。
具体实施方式
如图1所示，一种电光调Q腔内倍频亚纳秒脉冲绿光激光器，包括：泵浦源、泵浦耦合元件、偏振分光棱镜、激光增益介质、λ/4波片、电光开关、基频谐振腔反射镜、谐波分离境、倍频晶体和基频/倍频谐振腔反射镜；泵浦源发射的泵浦光经泵浦耦合元件聚焦到增益介质内，偏振分光棱镜与基频谐振腔反射镜、基频/倍频谐振腔反射镜构成L型折叠谐振腔，λ/4波片与电光开关在折叠腔的一个臂上，谐波分离境和倍频晶体在谐振腔的另一个臂上。
本发明的激光器为半导体激光器端面泵浦、加压式电光调Q，谐振采用三镜折叠腔结构，通过腔内倍频、可以实现亚纳秒脉冲绿光输出。
泵浦源1用于产生一定谱线宽度的激光，用于泵浦激光增益介质2，为达到较高的转换效率，输出光谱线应与激光增益介质2的吸收谱线相匹配，本实施例中泵浦源的输出方式可以为空间光输出的半导体激光器，也可以为光纤耦合输出的半导体激光器，泵浦方式为连续泵浦或脉冲泵浦。
泵浦耦合元件2用于将泵浦源1产生的激光以特定光斑直径耦合进激光增益介质2，实现泵浦光与谐振内振荡光的模式匹配，可以为单透镜或多个透镜组成的透镜组，透镜表面镀有对泵浦源1的增透膜。
偏振分光棱镜3是在谐振中主要起到两个作用，第一，作为谐振腔的一个折叠镜，起到转折光路的作用，第二，作为谐振腔内起偏器的，将增益介质产生的激光变成线偏振光。本实施例的偏振分光棱镜的直角面镀有对泵浦光与基频激光的增透膜，斜面镀有对泵浦光增透膜，同时对基频光的偏振膜，本实施例中的偏振分光棱镜3也可以是介质膜形式的偏振片。
激光增益介质4在吸收泵浦源1的泵浦光后，实现粒子数反转，当增益介质内的增益大于谐振腔的损耗后，就可以建立起激光振荡，是产生激光的一个必要元件，本实施例中激光增益介质为Nd:YVO 4晶体。
λ/4波片5和电光开关6在谐振腔内起到偏振转换的作用，实现调Q脉冲输出。本实施例中激光器为加压式电光调Q，λ/4波片5的快轴方向与激光增益介质4与偏振分光棱镜3产生的线偏振光方向成45°夹角，将线偏振光变成圆偏振光。在电光开关6未加λ/4电压时，圆偏振光经基频光谐振腔反射镜7反射，再次通过λ/4波片5后变成线偏振光，此时偏振方向旋转90°，反射光经偏振分光棱镜3反射，谐振腔不能输出激光，实现“关门”效果；当给电光开关6加上λ/4波电压后，谐振实现“开门”效果，输出一调Q脉冲。本实施例中的电光开关6为RTP电光开关。
基频谐振腔反射镜7主要是实现基频光的反射镜，本实施例中谐振腔反射镜7为0°反射镜，表面可以为平面、凹面、或凸面。
谐波分离镜为8主要是实现将基频光与倍频光分开，通过将反射镜的一个表面镀有基频光增透、倍频光反射的镀膜，将倍频光输出到谐振外。本实施例中谐波分离镜的入射角为45°。
倍频晶体9主要是通过非线性频率变换将基频光波长转换为倍频的绿光输出，本实施例中倍频晶体为LBO晶体。
基频/倍频谐振腔反射镜10主要是实现基频光与倍频光的同时反射，通过此种方式可以实现基频光在倍频晶体内双通倍频，提高倍频效率。本实施例中基频/倍频谐振腔反射镜10为0°反射镜，表面可以为平面、凹面、或凸面。

Claims (9)

  1. 一种电光调Q腔内倍频亚纳秒脉冲绿光激光器，其特征在于，包括：泵浦源、泵浦耦合元件、偏振分光棱镜、激光增益介质、λ/4波片、电光开关、基频谐振腔反射镜、谐波分离境、倍频晶体和基频/倍频谐振腔反射镜；泵浦源发射的泵浦光经泵浦耦合元件聚焦到增益介质内，偏振分光棱镜与基频谐振腔反射镜、基频/倍频谐振腔反射镜构成L型折叠谐振腔，λ/4波片与电光开关在折叠腔的一个臂上，谐波分离境和倍频晶体在谐振腔的另一个臂上。
  2. 如权利要求1所述的电光调Q腔内倍频亚纳秒脉冲绿光激光器，其特征在于，泵浦源输出方式为空间光输出或光纤耦合输出，泵浦方式为脉冲泵浦或连续泵浦。
  3. 如权利要求1所述的电光调Q腔内倍频亚纳秒脉冲绿光激光器，其特征在于，泵浦耦合元件采用单透镜或透镜组结构，将泵浦光以一定光斑尺寸耦合到激光增益介质内。
  4. 如权利要求1所述的电光调Q腔内倍频亚纳秒脉冲绿光激光器，其特征在于，激光器的谐振腔采用L型折叠腔结构，偏振分光棱镜作为谐振腔的折叠镜，偏振分光棱镜在谐振腔内同时起到偏振片及谐振腔折叠镜的作用，此偏振分光棱镜的通光面同时需要镀有泵浦光增透膜。
  5. 如权利要求1所述的电光调Q腔内倍频亚纳秒脉冲绿光激光器，其特征在于，激光增益介质为Nd:YVO 4晶体、Nd:GdVO 4晶体、Nd:YAG晶体、Nd:YLF晶体，能够输出1μm波长的激光晶体。
  6. 如权利要求1所述的电光调Q腔内倍频亚纳秒脉冲绿光激光器，其特征在于，激光增益介质、λ/4波片激光电光开关放在折叠腔的一个臂上，与偏振分光棱镜共同作用实现电光调Q；谐波分离镜及倍频晶体放在谐振腔的另一臂上，实现基频光线偏振输出与倍频晶体倍频的偏振匹配，实现最大倍频效率。
  7. 如权利要求1所述的电光调Q腔内倍频亚纳秒脉冲绿光激光器，其特征在于，激光器采用电光调Q方式工作，调Q方式是加压式电光调Q或退压式电光调Q。
  8. 如权利要求1所述的电光调Q腔内倍频亚纳秒脉冲绿光激光器，其特征在于，电光开光为RTP电光开关、BBO电光开关、LGS电光开关、LN电光开关或KD*P电光开关。
  9. 如权利要求1所述的电光调Q腔内倍频亚纳秒脉冲绿光激光器，其特征在于，倍频方式采用腔内倍频，倍频晶体的相位匹配方式可以是临界相位匹配或非临界相位匹 配；倍频光的输出方式为在偏振分光棱镜与倍频晶体之间插入谐波分离镜，谐波分离镜的入射角度为45°或其他角度，可以实现基频光通过，倍频光输出；倍频晶体为LBO晶体、KTP晶体、PPLN晶体、BBO晶体。
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CN112467511B (zh) * 2020-11-25 2022-03-22 中国工程物理研究院上海激光等离子体研究所 一种基于非线性频率转换的近场滤波和激光器横模控制系统及控制方法
CN114665359A (zh) * 2022-02-24 2022-06-24 南京邮电大学 一种高稳定性风冷绿光激光器
CN117277038A (zh) * 2023-11-21 2023-12-22 武汉光谷航天三江激光产业技术研究院有限公司 基于双晶体串接的单端泵浦机载脉冲激光器及控制方法

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