共查询到20条相似文献,搜索用时 46 毫秒
1.
G. Durry N. Amarouche L. Joly X. Liu B. Parvitte V. Zéninari 《Applied physics. B, Lasers and optics》2008,90(3-4):573-580
The 2.7 μm spectral range is highly suitable for the in situ monitoring of atmospheric H2O using compact balloonborne laser diode spectrometers. Water vapour spectroscopic parameters of the 202
101 and the 413
414 transitions of the ν3 band are revisited in this spectral region using a new distributed-feedback InGaAsSb laser diode emitting at 2.63 μm. Accurate
line strengths are provided which are well adapted for the in situ probing of the middle atmosphere. Our measurements are
thoroughly compared to an existing molecular database, laboratory measurements and ab-initio calculations. A laser hygrometer
was developed for operation from small stratospheric balloons using this new laser diode technology, with emission at 2.6 μm.
The realized sensor is described and results from a recent test-flight are reported.
PACS 07.57.Ty; 92.60 Jq 相似文献
2.
E. A. Arbabzadah C. C. Phillips M. J. Damzen 《Applied physics. B, Lasers and optics》2013,111(2):333-339
A study is made of a diode pumped Er3+:YSGG laser crystal operating at 2.797 μm. Lasers were constructed in the bounce geometry, using a transversely cooled 50 at.% Er:YSGG slab and a face-cooled 38 at.% Er:YSGG slab. Results from these are compared with those from a 50 at.% Er3+:YAG laser, also in the bounce geometry. With quasi-continuous wave diode pumping, free-running pulse energies of up to ~55 mJ and a slope efficiency of 20.5% are obtained from 50 at.% Er:YSGG. Better thermal performance is obtained from the face-cooled 38 at.% Er:YSGG slab, allowing average power of ~2 W to be obtained at a repetition rate and pump pulse duration of 140 Hz and 500 μs, respectively. Both Er:YSGG systems perform better than Er:YAG. Numerical modelling of the free-running 50 at.% Er:YSGG and Er:YAG systems is undertaken with good qualitative agreement with experimental results. Electro-optic Q-switching of the 50 at.% Er:YSGG laser using a LiNbO3 crystal yields ~0.5 mJ pulses with ~77 ns duration. 相似文献
3.
Ersen Beyatl? Solmaz Naghizadeh Adnan Kurt Alphan Sennaroglu 《Applied physics. B, Lasers and optics》2012,109(2):221-225
We report a low-threshold continuous-wave Tm:YAG laser that can be excited near 785?nm with low-cost, single-mode AlGaAs laser diodes. Low-threshold operation was achieved using a tightly focused, astigmatically compensated x-cavity containing a 2-mm-thick Tm:YAG crystal with 5?% Tm3+ concentration. Two linearly polarized single-mode diodes operating at 785.8?nm were polarization coupled to end pump the resonator. With a 6?% output coupler, as high as 32?mW of output power could be obtained at 2016?nm with 184?mW of incident pump power. The output could be further tuned in the 1935?C2035?nm range. Slope efficiency measurements indicated that cross-relaxation was very effective at this doping level. With a 2?% output coupler, lasing could be obtained with as low as 32.3?mW of pump power. In the limit of vanishing output coupling, the incident threshold pump power could be reduced to as low as 25?mW. To our knowledge, this is among the lowest lasing thresholds reported to date for continuous-wave, room-temperature thulium lasers. 相似文献
4.
C. Corsi M. Inguscio S. Chudzynski K. Ernst F. D’Amato M. De Rosa 《Applied physics. B, Lasers and optics》1999,68(2):267-269
Sensitivity studies are also performed, to evaluate the minimum detectable concentration of HCl in air.
Received: 7 August 1998/Revised version: 5 October 1998 相似文献
5.
A.V. Podlipensky K.V. Yumashev N.V. Kuleshov H.M. Kretschmann G. Huber 《Applied physics. B, Lasers and optics》2003,76(3):245-247
Spectroscopic data of a V3+:YAG passive Q-switch crystal were measured. The absorption recovery time was determined to be of 37±7 ns and the ground state
absorption cross section was estimated to be 0.7×10-18 cm2 at 1.44 μm and 3.5×10-18 cm2 at 1.34 μm. Passively Q-switched operation of diode pumped 1.44 μm and 1.3 μm Nd:YAG lasers was demonstrated using this crystal
as saturable absorber. Average output powers of 1.42 W (1.44 μm) and 1.56 W (1.34 μm) and pulse energies of 24 μJ (1.44 μm)
and 25 μJ (1.34 μm) were observed, respectively.
Received: 19 August 2002 / Published online: 12 February 2003
RID="*"
ID="*"Corresponding author. Fax: +49-40/42838-6281, E-mail: kretschmann@physnet.uni-hamburg.de 相似文献
6.
G. Galzerano A. Gambetta E. Fasci A. Castrillo M. Marangoni P. Laporta L. Gianfrani 《Applied physics. B, Lasers and optics》2011,102(4):725-729
We report on the absolute frequency measurement of an extended-cavity diode laser stabilized against a Doppler-free vibration?Crotation transition of the H2 18O isotopologue near 1.384???m. Absolute determination is performed by comparing the water-stabilized laser frequency with respect to a GPS-disciplined Rb microwave standard by means of a self-referenced fiber-based optical frequency comb. The line center frequency of the 22,1??22,0 transition of the H2 18O ??1+??3 combination band is found to be 216?519?045?955(13)?kHz. 相似文献
7.
Performance of a diode end-pumped Cr,Er:YSGG laser at 2.79 μm 总被引:1,自引:0,他引:1
We present a diode end-pumped Cr,Er:YSGG laser at 2.79 μm operated in the continuous-wave (CW) and pulsed modes. Er3+ ions are directly pumped into the upper laser state 4 I 11/2 using a 967-nm diode laser, which avoids various nonradiative losses. The laser produces 50.2 mW of power in the CW mode. An average power of 169 mW is obtained at a repetition rate of 100 Hz and a pulse duration of 2 ms. The maximum laser energy achieved is 1.95 mJ at a repetition rate of 50 Hz, corresponding to a peak power of 970 mW and a slope efficiency is 7.6%. The far-field divergence angle of the laser is measured to be 8 mrad. 相似文献
8.
The static laser performance of a-growth Nd:GdVO4 crystal (a-cut, 4×4×25 (mm)) at 1.34μm pumped by flash-lamp is investigated with different transmissions of output couplers. With the output coupler transmission of T = 30%, the static output energy of 148 mJ is obtained when the pump energy is 35.2 J, and the corresponding electric-optical conversion efficiency is 0.42%. The Q-switched output of lasers with the output wavelength ranging from 1.3 to 1.6μm can be realized by using Co2 :LaMgAl11O19 (Co:LMA) as saturable absorber. A flash-lamp-pumped, passively Q-switched Nd:GdVO4 laser with Co:LMA as saturable absorber is demonstrated in plano-concave laser cavity. With the cavity length of 16.3 cm and pump energy of 19.8 J, the single-pulse output energy, pulse width, and peak power are obtained to be 4 mJ, 80 ns, and 5×104 W, respectively. 相似文献
9.
P. Kluczynski S. Lundqvist S. Belahsene Y. Rouillard L. Nähle M. Fischer J. Koeth 《Applied physics. B, Lasers and optics》2012,108(1):183-188
We report Tunable Diode Laser Spectroscopy measurements of propane using a recently developed 3.37 μm GaInAsSb/AlGaInAsSb DFB laser. We have demonstrated that Wavelength Modulation Spectroscopy can be utilized to enhance a sharp feature in the broader propane spectrum around 3370.4 nm. A minimum detectable concentration of 30 ppb×m was obtained at a response time of 0.5 s. This corresponded to a minimum detectable absorption of 8 × 10?5 which is why an improvement of the sensitivity by an order of magnitude is possible using this laser and a more optimized optical setup. 相似文献
10.
《光学学报》2010,30(9)
报道了采用1064nm激光抽运周期极化掺杂氧化镁的铌酸锂(PPMgO…CLN)晶体光参变振荡器(OPO)实现高效率2.7μm可调谐激光输出的实验结果,理论计算了PPMgO…CLN晶体准相位匹配(QPM)温度调谐曲线。在1064nm激光抽运功率为182W,声光Q开关工作频率为10kHz和PPMgO:CLN晶体工作温度为150℃条件下,获得了平均功率为36.7W、波长为2.73μm中红外激光输出,斜率效率为23.7%。通过改变周期为31.3μmPPMgO…CLN晶体的工作温度30℃~200℃,获得了中红外波长3.0~2.6μm激光输出,波长温度调谐实验结果与理论分析结果有大约10℃的差异。 相似文献
11.
Efficient 2.7-μm emission in Er3+-doped bismuth germanate glass pumped by 980-nm laser diode 总被引:2,自引:0,他引:2
An Er 3+-doped lead-free bismuth germanate glass is synthesized. Its 2.7-μm emission property is analyzed, and the efficient 2.7-μm emission from the glass is observed under 980-nm laser diode excitation. The prepared glass possesses high spontaneous transition probability (64.8 s 1 ) and a large calculated emission cross section (6.61×10 21 cm 2 ) corresponding to the 4I11/2→4I13/2 transition. The multiphonon relaxation rate for the excited state 4I11/2 is only 236 s 1 . Therefore, the excellent spectroscopic properties and outstanding thermal stability suggest that this glass is a suitable host for developing solid-state lasers operating in the mid-infrared. 相似文献
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14.
We employed tunable diode laser absorption spectroscopy to measure the line strength, the methane (CH4), ethane (C2H6) and the propane (C3H8) broadening coefficients for the 523–422 H2O transition at 3619.61 cm?1. Water amount fractions generated by a stable and accurate humidity transfer standard, traceable to the SI units via the German national humidity standard, were used to calibrate the spectroscopic line strength measurements. We focus on the traceability of the measured line data to the SI and on uncertainty assessments following the guidelines of the Guide to the Expression of Uncertainty in Measurement. We determined the line strength to be (8.42 ± 0.07)×10?20 cm?1/(cm?2 molecule) corresponding to a relative uncertainty of ±0.8%. To the best of our knowledge, we report the first methane, ethane and propane broadening coefficients of (8.037 ± 0.056)×10?5 cm?1/hPa, (9.077 ± 0.064)×10?5 cm?1/hPa and (10.469 ± 0.073)×10?5 cm?1/hPa for the 523–422 H2O transition at 3619.61 cm?1, respectively. The relative combined uncertainties of the stated CH4, C2H6 and C3H8 broadening coefficients are in the ±0.7% range. 相似文献
15.
16.
Nai Zhang Weizai Zhang Gaoting Chen Jianhua Xu Zhiwu Liu Zujie Fang 《Chinese Journal of Lasers》1992,(6)
The experimental study of compression of picosecond optical pulses from a gainswitched InGaAsP DFB laser at 1.5μm wavelength range using a Gires-Tournois interferome-ter has been reported. Ultrashort optical pulses with pulsewidths of 6.6 ps, repetition rate of2.4GHz, and peak power in excess of 200 mW are obtained. The characteristics of a Gires-Tournois interferometer as a pulse compressor are also discussed. 相似文献
17.
High-power operation of uncoated 22μm-wide quantum cascade lasers (QCLs) emitting at λ~ 4.8μm is reported. The emitting region of the QCL structure consists of a 30-period strain-compensated Ino.68 Gao.32 As/In0.37 Alo.63 As superlattice. For a 4-mm-long laser in pulsed mode, a peak output power is achieved in excess of 2240mW per facet at 81K with a threshold current density of 0.64 kA/cm^2. The effects of varying the cavity lengths from 1 to 4 mm on the performances of the QCLs are analysed in detail and the low waveguide loss of only about 1.4 cm^-1 is extracted. 相似文献
18.
A mid-infrared optical communication experiment using a lead-salt diode laser emitting at 3.5 m is reported. Bit-error rate measurements have been performed for pulse code modulated data at 100 Mbits–1 using a fluoride glass fibre as a transmission channel. A bit-error rate better than 10–10 was achieved at a signal-to-noise ratio of 20 dB.S. T. Eng has a joint appointment with the Jet Propulsion Laboratory, Pasadena, California 91109, USA. 相似文献
19.
中红外激光领域广泛使用高性能高反射光学元件,高反射率高精度测试技术是制备高性能反射光学元件的基础。针对2.7~3.0μm波段光学元件高反射率测量的实际需求,基于量子级联激光器建立了连续光腔衰荡反射率测试实验装置,通过优选2.7~3.0μm波段反射带内水汽吸收较弱的测试波长,分析空气中水汽吸收对衰荡时间和反射率测量的影响,并比较空气和氮气环境下反射率测量结果,实现了2.7~3.0μm波段高反镜反射率的准确测量,在反射率约99.95%时绝对测量精度优于2×10-5。实验结果显示,采用测试波长2.9μm并在测量时保证初始腔和测试腔腔长相同,无需使用氮气环境,直接在实验室空气环境可实现高反射率的精确测量。 相似文献
20.
Cheng Li Yonggang Zhang Kai Wang Yi Gu Haosibaiyin Li YaoYao Li 《Infrared Physics & Technology》2010,53(3):173-176
Using double heterojunction structure with linearly graded InxAl1–xAs as buffer layer and In0.9Al0.1As as cap layer, wavelength extended In0.9Ga0.1As detectors with cutoff wavelength of 2.88 μm at room temperature have been grown by using gas source molecular beam epitaxy, their characteristics have been investigated in detail and compared with the detectors cutoff at 2.4 μm with similar structure as well as commercial InAs detectors. Typical resistance area product R0A of the detectors reaches 3.2 Ω cm2 at 290 K. Measured peak detectivity reaches 6.6E9 cm Hz1/2/W at room temperature. 相似文献