共查询到20条相似文献,搜索用时 31 毫秒
1.
Y. F. Lü X. H. Zhang X. D. Yin J. Xia A. F. Zhang J. Q. Lin 《Applied physics. B, Lasers and optics》2010,99(1-2):115-119
The continuous-wave high efficiency laser emission of Nd:YVO4 at the fundamental wavelength of 914 nm and its 457 nm second harmonic obtained by intracavity frequency doubling with an LBO nonlinear crystal is investigated under pumping by diode laser at 880 nm into emitting level 4F3/2. 6.5 W at 457 nm with M 2=1.8 was obtained from a 5-mm-thick 0.4 at.% Nd:YVO4 laser medium and a 15-mm-long LBO nonlinear crystal in a Z-type cavity for 18.6 W absorbed pump power. An optical-to-optical efficiency with respect to the absorbed pump power was 0.35. Comparative results obtained for the pump with diode laser at 808 nm, into the highly-absorbing level 4F5/2, are given in order to prove the advantages of the 880 nm wavelength pumping. 相似文献
2.
We report for the first time a continuous-wave (CW) coherent radiation at 500.5 nm by intracavity sum-frequency generation
of 1063 nm Nd:GdVO4 laser and 946 nm Nd:YAG laser. Blue-green laser is obtained by using a doubly cavity, type-II critical phase matching KTiOPO4 (KTP) crystal sum-frequency mixing. With total pump power of 27.8 W, TEM00 mode blue-green laser at 500.5 nm of 421 mW is obtained. At the output power level of 421 mW, the blue-green power stability
is better than 2.8% and laser beam quality M
2 factor is 1.37. 相似文献
3.
A sum-frequency yellow-green laser at 554.9 nm is reported by this paper, 946 nm wavelength is obtained from 4F3/2-4I9/2 transition in Nd:YAG and 1342 nm wavelength is obtained from 4F3/2-4I13/2 transition in Nd:YVO4. Using a doubly folded-cavity type-II critical phase matching KTP crystal intra cavity to make 946 nm laser from Nd:YAG and 1342 nm laser from Nd:YVO4 frequency summed, with incident pumped power of 30 W in Nd:YAG and 20 W in Nd:YVO4, TEM00 mode yellow-green laser at 554.9 nm at 1.15 W is obtained and its M2 factor is less than 1.22. The experimental results show that the Nd:YAG and Nd:YVO4 crystals intra-cavity sum-frequency mixing is an effective method for yellow-green laser and it can be applied to other two laser crystals to obtain more all-solid-state lasers with different wavelengths. 相似文献
4.
An efficient 2 μm room temperature Ho:YVO(4) laser resonantly pumped by a 1.94 μm Tm:YAP laser is demonstrated, for the first time to our knowledge, in this Letter. Up to 8.58 W of laser output at 2053 nm is obtained with the optical-to-optical conversion efficiency as much as 41.2%. The output beam had quality of M2 factor with Mx(2) of 3.58 and My(2) of 1.76 at 8 W output level. In addition, we also obtained 4.18 W laser output at 2066 nm and 7.04 W at 2040 nm from the Ho:YVO(4) laser with conversion efficiency of 27.8% and 33.8%, respectively. 相似文献
5.
6.
It is reported that efficient continuous-wave (CW) self-frequency-doubling green laser at 530 nm performed with a diode-pumped
Nd3+:YCa4O(BO3)3 (Nd:YCOB) laser. With a diode pump power of 14.3 W, TEM00 mode green laser at 530 nm of 1.07 W is obtained. At the output power level of 1.07 mW, the output stability is better than
5%. The beam quality M2 value is about 1.37. To the best of our knowledge, this is the highest power laser at 530 nm generated by self-frequency
doubling of a diode pumped Nd:YCOB laser. 相似文献
7.
It is reported that efficient continuous-wave (CW) self-frequency-doubling red laser at 666 nm performed with a diode-pumped
Nd3+:YCa4O(BO3)3 (Nd:YCOB) laser. With a diode pump power of 14.3 W, TEM00 mode red laser at 666 nm of 570 mW is obtained. At the output power level of 570 mW, the output stability is better than
3.5%. The beam quality M2 value is about 1.25. To the best of our knowledge, this is the highest power laser at 666 nm generated by self-frequency
doubling of a diode pumped Nd:YCOB laser. 相似文献
8.
We report for the first time a continuous-wave (CW) coherent radiation at 480 nm by intracavity sum-frequency generation of
900 nm Neodymium Doped Strontium and Lanthanum Aluminate (Nd:ASL) laser and 1030 nm Yb:Y3Al5O12 (Yb:YAG) laser. Blue laser is obtained by using a doubly cavity, type-I critical phase matching LiB3O5 (LBO) crystal sum-frequency mixing. With total pump power of 28.6 W, the blue laser at 480 nm of 170 mW is obtained. At the
output power level of 170 mW, the blue power stability is better than 4.7% and laser beam quality M
2 factor is 1.43. 相似文献
9.
Near-infrared laser action of nitrogen atoms was obtained in a hollow cathode discharge. Four laser lines at wavelengths of 1358.2, 939.3, 938.7, and 862.9 nm were observed in the cw mode. In addition, the laser line at 904.6 nm was observed in quasi-cw operation in the afterglow for the first time. It is supposed that resonant charge exchange between He+ and N2 followed by predissociation of N
2
+
is an important way of populating the upper laser levels. 相似文献
10.
We report for the first time a efficient compact red laser at 671.5 nm generation by intracavity frequency doubling of a continuous
wave laser operation of a diode direct pumped Nd:LuVO4 laser on the 4
F
3/2 → 4
I
13/2 transition at 1343 nm. An LBO crystal, cut for critical type I phase matching at room temperature is used for second harmonic
generation of the laser. At an absorbed pump power of 16.2 W, as high as 4.3 W of continuous wave output power at 671.5 nm
is achieved with 10-mm-long LBO. Comparative results obtained for the pump with diode laser at 808 nm, into the highly-absorbing
4
F
5/2 level, are given in order to prove the advantages of the 880 nm wavelength pumping. 相似文献
11.
We report for the first time a continuous-wave (CW) blue-green radiation at 504 nm by intracavity sum-frequency generation
of 946 nm Nd:YAG laser and 1080 nm Nd:YAlO3 (Nd:YAP) laser. Using type-I critical phase matching LiB3O5 (LBO) crystal, 504 nm blue-green laser was obtained by 946 and 1080 nm intra-cavity sum-frequency mixing, and output power
of 215 mW was demonstrated. At the output power level of 215 mW, the output power stability is better than 4.7% and laser
beam quality M2 factor is 1.21. 相似文献
12.
13.
L. S. Ma Ph. Courteille G. Ritter W. Neuhauser R. Blatt 《Applied physics. B, Lasers and optics》1993,57(3):159-162
Modulation-transfer spectroscopy is used to observe resonances in 130Te2 near 467 nm. A signal-to-noise ratio of 500 is obtained with 1 mW laser power and with a time constant of 10 ms; the lineshapes are investigated in detail for different demodulation phases. The signal can be used to servolock a blue dye ring laser at 467 nm on a 130Te2 resonance which serves as reference line for precision spectroscopy on single, trapped Yb+ ions at 467 nm. 相似文献
14.
We report for the first time a continuous-wave (CW) blue-green laser emission by sum-frequency mixing in Nd:CNGG crystal.
Using type-I critical phase-matching LBO crystal, a blue-green laser at 497 nm is obtained by 1061 and 935 nm intracavity
sum-frequency mixing. The maximum laser output power of 232 mW is obtained when an incident pump laser of 18.2 W is used.
At the output power level of 232 mW, the output stability is better than 3.67%. The beam quality M
2 value is are about 1.26 and 1.38 in both horizontal and vertical dimensions respectively. 相似文献
15.
The continuous-wave high-efficiency laser emission of Nd:GdVO4 at the second-harmonic of 456 nm obtained by intracavity frequency doubling with an BiB3O6(BiBO) nonlinear crystal is investigated under pumping by diode laser at 880 nm into emitting level 4F3/2. About 3.8 W at 456 nm with M2 = 1.4 was obtained from a 5 mm-thick 0.4 at.% Nd:GdVO4 laser medium and a 12 mm-long BiBO nonlinear crystal in a Z-type cavity for 13.9 W absorbed pump power. An optical-to-optical efficiency with respect to the absorbed pump power was 0.274. Comparative results obtained for the pump with diode laser at 808 nm, into the highly-absorbing 4F5/2 level, are given in order to prove the advantages of the 880 nm wavelength pumping. 相似文献
16.
The continuous-wave high efficiency laser emission of Nd:YAG at the fundamental wavelength of 1319 nm and its 659.5-nm second
harmonic obtained by intracavity frequency doubling with an LBO nonlinear crystal is investigated under pumping by diode laser
at 885 nm (on the 4
F
3/2 → 4
I
13/2 transition). An end-pumped Nd:YAG crystal yielded 9.1 W at 1319 nm of continuous-wave output power for 18.2 W of absorbed
pump power. The slope efficiency with respect to the absorbed pump power is 0.55. Furthermore, 5.2 W 659.5 nm red light is
acquired by frequency doubling, resulting in an optical-to-optical efficiency with respect to the absorbed pump power of 0.286.
Comparative results obtained for the pump with diode laser at 808 nm (on the 4
F
5/2 → 4
I
13/2 transition) are given in order to prove the advantages of the 885 nm wavelength pumping. 相似文献
17.
H. B. Shen Q. P. Wang Y. X. Zhang Z. J. Liu F. Bai X. X. Chen Z. H. Cong L. Gao W. X. Lan C. Wang Y. G. Zhang Z. G. Wu W. T. Wang 《Applied physics. B, Lasers and optics》2012,109(4):643-648
A high-power diode-side-pumped 1,105?nm Nd:GGG laser and a laser at 552?nm based on intracavity frequency doubling of 1,105?nm laser are demonstrated for the first time. A 26.8-W 1,105?nm laser continuous wave output was achieved under the incident pump power of 170?W. A LiB3O5 crystal is used for second harmonic generation of 1,105?nm laser. When the pump power was 170?W, the average output power at 552?nm of 7.3?W was obtained, corresponding to the optical conversion efficiency of 4.3?%. And the minimum pulse width is 181?ns with the pulse repetition rate of 10?kHz. The M 2 factors are measured to be 19.8 and 17.6 in the horizontal and vertical directions, respectively. 相似文献
18.
Y. F. Lü X. H. Zhang J. Xia X. D. Yin A. F. Zhang L. Bao D. Wang H. Quan 《Laser Physics》2009,19(12):2174-2178
We report the efficient compact red laser at 670 nm generation by intracavity frequency doubling of a continuous wave laser
operation of a diode direct pumped Nd:GdVO4 laser on the 4
F
3/2 → 4
I
13/2 transition at 1340 nm. An LBO crystal, cut for critical type I phase matching at room temperature is used for second harmonic
generation of the laser. At an absorbed pump power of 16.2 W, as high as 5.1 W of continuous wave output power at 670 nm is
achieved with 15-mm-long LBO. The optical-to-optical conversion efficiency is up to 0.31, and the fluctuation of the red output
power was better than 3.0% in the given 30 min. Comparative results obtained for the pump with diode laser at 808 nm, into
the highly-absorbing 4
F
5/2 level, are given in order to prove the advantages of the 880 nm wavelength pumping. 相似文献
19.
Nilesh J. Vasa Kouki Morishita Husayin Parhat Tatsuo Okada Mitsuo Maeda Osamu Uchino 《Optical Review》1997,4(1):A176-A179
Spectrally pure high-power tunable single-mode operation of a pulsed Ti3+:sapphire laser by a tunable injection-seeding is reported. The injection laser was a cw diode laser pumped, spectrally narrowed
tunable Cr3+:LiSrAlF6 (Cr3+:LiSAF) laser with a grating in the auxiliary cavity. Single-mode tunable operation of a pulsed Ti3+: sapphire ring oscillator was obtained at different wavelengths in the range between 818 nm and 848 nm with a typical linewidth
of 0.006 cm-1. To extend the applicability of this operation to a differential absorption lidar system, the single-mode Ti3+:sapphire oscillator output was amplified and a high energy output of 38 mJ was obtained with the same linewidth. 相似文献
20.
S. Xie Y. Bo J. Xu Y. Shen P. Wang Z. Wang F. Yang Q. Peng D. Cui J. Zhang Z. Xu 《Applied physics. B, Lasers and optics》2011,102(4):781-787
We report a high-power, narrow linewidth and tunable quasi-continuous-wave (QCW) yellow laser system at 589.159?nm. The system is of a design employing single-pass sum-frequency generation (SFG) in a LBO crystal by mixing the 1064?nm with 1319?nm lines from a two diode-side-pumped Nd:YAG master oscillator-power amplifier (MOPA) laser system. With the pump power of 35?W at 1064?nm and 25?W at 1319?nm, a 7.5?W QCW output of the SFG yellow laser at 589.159?nm, which is the vacuum wavelength of a general sodium D2 line, is obtained with a linewidth less than 0.7?GHz and a beam-quality factor M 2=1.2. The wavelength of the laser can be precisely step-tuned from 589.148 to 589.167?nm with an increment of 0.13?pm by means of a temperature-controlled etalon. 相似文献