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1.
我们在实验中演示了520nm单频绿光泵浦的基于周期极化磷酸钛氧钾(PPKTP)晶体的780nm+1560nm双共振光参量振荡器,高效制备780nm+1 560nm连续可调谐双色下转换光场。该参量振荡器可输出93.3 mW的1 560nm单频激光和44.6mW的780nm单频激光。通过改变PPKTP晶体的温度所得到的波长粗调范围为:信号光1 529.81nm~1 573.83nm(~44nm),闲置光788.26nm~777.20nm(~11nm);通过连续调谐520nm泵浦激光频率初步得到的闲置光在780.24nm(铷原子D2线)处频率连续调谐范围约1.6GHz。 相似文献
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介绍了以Nd:YAG激光器的三倍频光作泵浦源,BBO作非线性光学晶体,在410一2200nm波段可连续调谐的光参量振荡器(OPO)的工作原理和实验装置,测定了其调谐曲线的输出能量,并对实验结果做了分析。 相似文献
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提出一种基于交叉泵浦实现受激电磁耦子散射的非共线相位匹配的方法,获得频率可调谐的窄带Stokes光输出。根据参量放大理论,推导出交叉泵浦受激电磁耦子散射的单程放大增益效率表达式,揭示了交叉泵浦实现受激电磁耦子非共线相位匹配的物理机制。实验上采用泵浦光在晶体侧面全反射的方式构建交叉泵浦,通过旋转晶体改变泵浦光全反射角,实现相位匹配条件的改变和输出Stokes光频率的调谐。输出Stokes光线宽为0.17 nm,波长调谐范围为1 068~1 076 nm。在15 mJ的泵浦能量下的输出能量为1.07 mJ,能量转化效率为6.8%。本研究为非线性参量转换过程中的相位匹配方法提供一种方案参考,尤其适用于泵浦光脉宽小于纳秒量级的短脉冲情况。 相似文献
5.
报道了一台高重复频率2 mm光学参量振荡器泵浦的磷锗锌光学参量振荡器。磷锗锌晶体(ZnGeP2,简称ZGP)采用Ⅰ类相位匹配方式,切割角度q为55°,f为0°,尺寸5.5 mm×6 mm×18 mm,在4.0 kHz重复频率下,当注入5.2 W的2 mm圆偏振光时,获得310 mW中红外输出,p偏振态2 mm到3~5 mm光-光转换效率12%。通过调节晶体的角度,实验获得ZGP光学参量振荡器的波长调谐曲线,在误差范围内与理论变化规律相符。 相似文献
6.
利用半导体激光泵浦输出1064 nm波长的全固态连续Nd:YVO4激光器作为泵浦源,采用周期调谐和温度调谐组合调谐技术,对基于掺氧化镁周期性极化铌酸锂晶体(MgO:LiNbO3, PPMgLN)准相位匹配(QPM)的全固态连续波(CW)光学参量振荡器(OPO)宽波段无分立连续调谐输出特性进行研究。实验采用连续工作模式和外腔结构,基于多周期PPMgLN晶体的30.2,30.4和30.6 m周期,在改变晶体的极化周期的基础上,同时在30~100 ℃范围内调节晶体工作温度。实验结果表明:CW PPMgLN OPO的泵浦阈值仅为0.22 W;不同极化周期需要的温度调谐范围不同;信号光在1 559.8~1 597.2 nm近红外波段和闲频光在3 187.3~3 347.3 nm中红外波段连续调谐输出。实现了外腔式全固态CW OPO在信号光和闲频光波段的无分立连续调谐输出。 相似文献
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采用调Q Nd:YAG激光倍频光(0.532μm)泵浦温度调谐MgO:LiNbO_3晶体单、双谐振光参量振荡器(OPO包括DRO、SRO)的实验结果.双谐振(DRO)调谐范围达844.1~1411.3nm,最低泵浦阈值0.22mJ/pulse;单谐振(SRO)调谐范围达738.9~1032.2nm,最低泵浦阈值0.66mJ/pulse.最大能量转换效率为10.4%. 相似文献
9.
基于掺MgO周期极化铌酸锂晶体的光学参量振荡器是一种全固态中红外可调谐相干光源.泵浦源为1064 nm声光调Q Nd:YAG激光器.通过温度调谐实现了中红外可调谐参量光的输出,当晶体的温度从40°C升高到200°C时,获得信号光的输出范围为1.561 μm~1.670μm,空闲光的调谐范围为3.342 μm~2.932 μm.当泵浦源脉宽为70 ns,重复频率为10 kHz,平均功率为.161 W,获得波长为1631μm.当泵浦源脉宽为70 ns,重复频率为10 kHz,平均功率为1.61 W,获得波长为1631 nm信号光的输出功率为21 1 mW. 相似文献
10.
本文采用折射率面来描述光参量振荡过程的物理图象,获得了光参量振荡过程的相位匹配图象和频率调谐的简单的数学表达式,直观简洁地说明了光参量振荡器频率调谐曲线的调谐行为.我们用1.06μm和0.532μm激光泵浦β-BaB2O4(BBO)晶体,获得了角度调谐的BBO光参量振荡器的调谐范围分别为1.7~2.35μm及0.72~2.1μm,最大能量转换效率为15%,还讨论了输出能量与腔长的关系. 相似文献
11.
T. Andres P. Haag S. Zelt J.-P. Meyn A. Borsutzky R. Beigang R. Wallenstein 《Applied physics. B, Lasers and optics》2003,76(3):241-244
A synchronously pumped femtosecond optical parametric oscillator based on congruent MgO-doped periodically poled lithium niobate
(c-MgO:PPLN) is reported. The system, operating at room temperature, was pumped by a mode-locked Ti:sapphire laser. The wavelengths
of the signal and idler waves were tuned from 870 nm to 1.54 μm and 1.58 to 5.67 μm, respectively, by changing the pump wavelength,
the grating period or the cavity length. Pumped by 1.1 W of 755 nm laser radiation, the OPO generated 310 mW of 1080 nm radiation.
This signal output corresponds to a total conversion efficiency of 50%. Without dispersion compensation the OPO generated
phase-modulated signal pulses of 200 fs duration. Besides the OPO of c-MgO:PPLN, an OPO of stoichiometric (s) MgO:PPLN was
investigated. Because of the reduced sensitivity to photorefractive damage, both crystals allowed efficient OPO operation
at room temperature.
Received: 19 August 2002 / Revised version: 11 December 2002 / Published online: 19 March 2003
RID="*"
ID="*"Corresponding author. Fax: +49-631/205-3906, E-mail: andres@physik.uni-kl.de 相似文献
12.
Suddapalli Chaitanya Kumar Adolfo Esteban‐Martin Takuro Ideguchi Ming Yan Simon Holzner Theodor W. Hnsch Nathalie Picqu Majid Ebrahim‐Zadeh 《Laser \u0026amp; Photonics Reviews》2014,8(5):L86-L91
A few‐cycle, broadband, singly‐resonant optical parametric oscillator (OPO) for the mid‐infrared based on MgO‐doped periodically‐poled LiNbO3 (MgO:PPLN), synchronously pumped by a 20‐fs Ti:sapphire laser is reported. By using crystal interaction lengths as short as 250 µm, and careful dispersion management of input pump pulses and the OPO resonator, near‐transform‐limited, few‐cycle idler pulses tunable across the mid‐infrared have been generated, with as few as 3.7 optical cycles at 2682 nm. The OPO can be continuously tuned over 2179‐3732 nm (4589‐2680 cm‐1) by cavity delay tuning, providing up to 33 mW of output power at 3723 nm. The idler spectra exhibit stable broadband profiles with bandwidths spanning over 422 nm (FWHM) recorded at 3732 nm. The effect of crystal length on spectral bandwidth and pulse duration is investigated at a fixed wavelength, confirming near‐transform‐limited idler pulses for all grating interaction lengths. By locking the repetition frequency of the pump laser to a radio‐frequency reference, and without active stabilization of the OPO cavity length, an idler power stability better than 1.6% rms over >2.75 hours is obtained when operating at maximum output power, in excellent spatial beam quality with TEM00 mode profile. Photograph shows a multigrating MgO:PPLN crystal used as a nonlinear gain medium in the few‐cycle femtosecond mid‐IR OPO. The visible light is the result of non‐phase‐matched sum‐frequency mixing between the interacting beams. 相似文献
13.
Synchronously Pumped Femtosecond Optical Parametric Oscillator Based on MgO-Doped Periodically Poled LiNbO3
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We report a femtosecond optical parametric oscillator based on MgO-doped PPLN synchronously pumped by a mode-locked Ti:sapphire laser. The wavelengths of the signal and idler are continuously tuned from 1100 to 1300hm and from 2080 to 2930nm, respectively, by changing the pump wavelength and the OPO cavity length. The maximum signal output power of 130mW at the wavelength of 1225nm is obtained, pumped by 900roW of 800hm laser radiation. This corresponds to a total conversion efficiency of 22.1%. The signal pulse duration is measured to be 167fs by intensity autocorrelation with chirped mirrors for intracavity dispersion compensation. 相似文献
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We present a period-continuously-tunable optical parametric oscillator based on a fan-out MgO:PPLN with a grating period range
from 26.9 to 29.5 μm. The OPO was pumped by a Q-switched Nd:YAG laser with a repetition of 10 kHz. With a grating period of
29.3 μm and 22.0 W pump power, the idler output power at 3.78 μm arrived at 3.40 W. With a period of 27.1 μm and 13.5 W pump,
the idler output at 4.58 μm arrived at 0.36 W. This is, to our best knowledge, the highest average power for pulsed OPO operating
near 4.5 μm based on PPLN or MgO:PPLN. By translating the fan-out MgO:PPLN, the idler wavelength was tuned continuously from
3.78 to 4.62 μm. 相似文献
16.
We report on a self-guided operation of a green-pumped singly resonant continuous-wave optical parametric oscillator with
a bulk MgO-doped PPLN crystal. It is achieved by increasing the OPO cavity length beyond the stability boundary so that the
OPO can only oscillate with formation of a thermally induced waveguide inside the crystal. The effects of the thermal waveguide
on the OPO performance are studied by measuring output power characteristics at different cavity lengths. Improvement of spatial
mode quality and stability of output power by self-guiding is demonstrated. Measurement of temporal characteristics proves
that formation of the waveguide originates from the photo-thermal effect in the nonlinear crystal by absorption of pump power. 相似文献
17.
I.-H. Bae H. S. Moon S. Zaske C. Becher S. K. Kim S.-N. Park D.-H. Lee 《Applied physics. B, Lasers and optics》2011,103(2):311-319
We present a 532 nm-pumped singly-resonant cw optical parametric oscillator based on MgO-doped PPLN with a minimum threshold
pump power of 0.3 W. The OPO with a two-mirror standing-wave cavity is optimized by using a tunable diode laser on the path
of the resonant signal beam. The maximum output power is 200 mW at an idler wavelength near 1330 nm at a pump power of 2 W.
We report the degradation of the output power and beam characteristics at high pump power indicating a strong thermal lensing
in the crystal. The continuous tuning range of the OPO is measured to be 800 MHz which is close to 90% of the free spectral
range of the OPO cavity. 相似文献
18.
Optical parametric oscillation in periodically poled lithium niobate driven by a diode-pumped Q-switched erbium fiber laser 总被引:2,自引:0,他引:2
Britton PE Taverner D Puech K Richardson DJ Smith PG Ross GW Hanna DC 《Optics letters》1998,23(8):582-584
We describe what is to our knowledge the first nanosecond periodically poled lithium niobate (PPLN) optical parametric oscillator (OPO) driven by a fiber laser. The source was frequency doubled by a PPLN sample before pumping a second, 20-mm-long, PPLN crystal. The OPO threshold was <10muJ, with pump depletions of as much as 45% and a tunable signal range of 945-1450 nm (1690-4450-nm idler range). We demonstrated 130-nm signal tuning by varying the pump wavelength and doubling crystal's temperature. Also, we achieved 15-nm tuning with all crystals at a constant temperature. The results demonstrate the potential of the fiber laser:PPLN combination for practical, versatile, and tunable sources. 相似文献
19.
Tuning and stability of a continuous-wave mid-infrared high-power single resonant optical parametric oscillator 总被引:1,自引:0,他引:1
M.M.J.W. van Herpen S. Li S.E. Bisson S. te Lintel Hekkert F.J.M. Harren 《Applied physics. B, Lasers and optics》2002,75(2-3):329-333
A 2.2-W continuous-wave, continuously tunable, single-frequency OPO has been developed in the 3.0–3.8 μm wavelength range
for the detection of molecular trace gasses. The oscillation threshold, output power and stability of the single resonant
OPO were improved by optimizing pump beam waist and OPO cavity length. Both air-spaced and solid etalons were tested to frequency
stabilize and tune the OPO, from which the solid etalon gave a better performance. Temperature oscillations in the PPLN crystal
caused oscillations in the idler wavelength of less than 200 MHz over 300 s; the short-term stability was less than 3 MHz
over 1 s. The high laser power, in combination with photoacoustic spectroscopy, achieved a detection limit of 10 parts-per-trillion
for ethane in nitrogen.
Received: 9 April 2002 / Revised version: 14 June 2002 / Published online: 2 September 2002
RID="*"
ID="*"Corresponding author. Fax:+31-24/3653311, E-Mail: maartenh@sci.kun.nl 相似文献
20.
An optical parametric oscillator (OPO) based on periodically-poled lithium niobate (PPLN) and pumped by 1064.2-nm laser is demonstrated, which can be conveniently tuned by the means of changing its operating temperature. The parameters of the set-up and experimental results are introduced in this paper. We adjusted the operating temperature from 80 to 250 ℃, the output wavelength shifted from 1485.4 to 1540.7 nm. The average of the shifts is 0.33 nm/℃. 相似文献