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Dive into the research topics where C. H. Huang is active.

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Featured researches published by C. H. Huang.


Applied Physics Letters | 1990

Comparison of simultaneous multiple wavelength lasing in various neodymium host crystals at transitions from 4F3/2–4I11/2 and 4F3/2–4I13/2

Hongyuan Shen; R.R. Zeng; Y. P. Zhou; Guanghui Yu; C. H. Huang; Z.D. Zeng; Wenbin Zhang; Q. J. Ye

The possibility of simultaneous multiple wavelength lasing in various neodymium host crystals such as Nd:YAG, Nd:YLF, Nd:BEL, and Nd:YAP has been analyzed by the ‘‘oscillation condition.’’ It is shown that this kind of laser can be realized in all the described crystals in pulsed state, but only achieved in the Nd:YAP crystal in continuous‐wave state. On the basis of the analyzed results, we have achieved cw simultaneous multiple wavelength lasing in Nd:YAP crystal for the first time at both 1.0795 and 1.3414 μm.


IEEE Journal of Quantum Electronics | 1991

Simultaneous multiple wavelength laser action in various neodymium host crystals

Hongyuan Shen; R.R. Zeng; Y. P. Zhou; Gui Fang Yu; C. H. Huang; Z.D. Zeng; W.J. Zhang; Q.J. Ye

The oscillation condition of a simultaneous multiple wavelength laser has been established and used to analyze the possibility of simultaneous oscillation in various neodymium host crystals, such as Nd:YAG, Nd:YLF, Nd:BEL, and Nd:YAP crystals at the transitions from /sup 4/F/sub 3/2/-/sup 4/I/sub 13/2/ and /sup 4/F/sub 3/2/-/sup 4/I/sub 11/2/. It is shown that this kind of laser can be realized in all the described crystals in a pulsed state. In general, continuous wave (CW) operation, however, can only be achieved for Nd:YAP. On the basis of these results, CW simultaneous double wavelength lasing has been achieved in a Nd:YAP crystal for the first time at both 1.0795 mu m and 1.314 mu m. >


Applied Optics | 1993

1079.5- and 1341.4-nm: larger energy from a dual-wavelength Nd:YAlO 3 pulsed laser

Huan Shen; Weiran Lin; R.R. Zeng; Y. P. Zhou; G. F. Yu; C. H. Huang; Zhige Zeng; W. J. Zhang; R. F. Wu; Qixiang Ye

On the basis of oscillation conditions of simultaneous multiple-wavelength lasing that we have established, a larger-energy (1079.5 and 1341.4 nm) dual-wavelength Nd:YAlO(3) pulsed laser has been developed. Output energies of 3.71 and 1.39 J with efficiencies of 1.29% and 0.48% for the 1341.4-and 1079.5-nm wavelengths, respectively, have been achieved. To our knowledge, this is the best result among simultaneous dual-wavelength solid-state lasers to date. The temporal and spatial distributions of these beams obtained from a free-running dual-wavelength Nd:YAlO3 pulsed laser have also been measured. Experimental results show that the temporal and spatial overlap of the two beams is quite good for this type of laser.


IEEE Journal of Quantum Electronics | 1992

Second harmonic generation and sum frequency mixing of dual wavelength Nd:YAlO/sub 3/ laser in flux grown KTiOPO/sub 4/ crystal

Huan Shen; Y. P. Zhou; Weiran Lin; Z.D. Zeng; R.R. Zeng; G. F. Yu; C. H. Huang; A.D. Jiang; S.Q. Jia; D.Z. Shen

On the basis of accurately measured refractive indexes, the authors have obtained the Sellmeiers equations for flux grown KTiOPO/sub 4/ (KTP) crystal and used them to calculate the phase matched angles ( theta /sub m/, phi /sub m/) and effective nonlinear coefficients (d/sub eff/) for type I and III second harmonic generation (SHG) and sum frequency mixing (SFM) of radiations at 1.0795 and 1.3414 mu m. The optimum phase matching conditions for 1.0795 and 1.3414 mu m SHG are that theta /sub m/=86.88 and 58.88 degrees , respectively, in an XZ plane ( phi =0) and for SMF of 1.0795 and 1.3414 mu m in the same plane 76.02 degrees . The corresponding d/sub eff/ values calculated from theta /sub m/s are 18.07*10/sup -9/ and 17.42*10/sup -9/ esu. >


Applied Optics | 1990

Measurement of the refractive index and thermal refractive index coefficients of Nd:YAP crystal

Z.D. Zeng; Hongyuan Shen; Miaoliang Huang; Hao Xu; R.R. Zeng; Y. P. Zhou; Guifang Yu; C. H. Huang

The principal refractive indices of yttrium aluminate crystal doping with 1-wt.% neodymium (Nd:YAP) have been measured by a minimum deviation method for the wavelengths 0.5398, 0.6328, and 1.0795 microm in the temperature range of 289-435 K. The thermal refractive index coefficients have been obtained at these wavelengths, and they are all positive and slightly decrease with increased wavelength. The constants of the single term Sellmeier equation are also given for the 273-420 K temperature range. These constants are in linear relationship with temperature in the 4 x 10(-3) error range.


IEEE Journal of Quantum Electronics | 1989

Measurement of the stimulated emission cross section for the /sup 4/F/sub 3/2/-/sup 4/I/sub 13/2/ transition of Nd/sup 3+/ in YAlO/sub 3/ crystal

Hongyuan Shen; Tianguan Lian; Ruirong Zheng; Y. P. Zhou; Guijang Yu; C. H. Huang; Hong Liao; Zhengdong Zheng

A method for the simultaneous measurement of the stimulated emission cross section and fluorescence lifetime by studying the relation between laser parameters and the laser relaxation oscillation frequency is discussed. The stimulated emission cross section for the /sup 4/F/sub 3/2/-/sup 4/I/sub 13/2/ transition of Nd/sup 3+/ ion in YAP crystal was measured to be (22+or-1)*10/sup -20/ cm/sup 2/. >


Journal of Applied Physics | 1998

Computational model of Q-switch Nd:YAlO3 dual-wavelength laser

Hua Su; Huan Shen; Weiran Lin; R.R. Zeng; C. H. Huang; G. Zhang

A rate equation model with spatial hole-burning effect is built to calculate the Q-switch Nd:YAlO3(Nd:YAP) simultaneous dual wavelength laser. We find that 1341.4 and 1079.5 nm lasers can be simultaneously generated in a linear cavity by controlling the output coupling rates of the two coherent radiations. In contrast, a Y cavity and devices to control relative Q-switch delay were necessary for the dual wavelength Nd:YAG laser in previous work. Also with this model, some optimum parameters’ relationships to pump energy are investigated.


Journal of Applied Physics | 1991

Laser action of Nd:YAlO3 at 1300 nm

Hongyuan Shen; Y. P. Zhou; R.R. Zeng; G. F. Yu; C. H. Huang; Z.D. Zeng; Wenwu Zhang; W. X. Lin; Qixiang Ye

From our measured value of the stimulated emission cross section for 4F3/2–4I13/2 transition of Nd3+ ion in YAlO3 crystal as well as the results of continuous wave (cw) and pulsed 1341.4 nm Nd:YAP lasers, it can be seen that Nd:YAP is an excellent 1300 nm laser crystal. In our laboratory cw output power of 195.8 W at 1341.4 nm with an overall efficiency of 1.43% and pulsed output energy of 5.1 J at 1341.4 nm with an overall efficiency of 2.02% have been achieved by using this kind of crystal.


Optics Communications | 2000

The study of 1341.4 nm Nd:YAlO3 laser intracavity frequency doubling by LiB3O5

Ge Zhang; Hongyuan Shen; R.R. Zeng; C. H. Huang; Wenxion Lin; Jianhong Huang

Abstract The study of 1341.4 nm Nd:YAlO 3 laser intracavity frequency doubling by nonlinear optical crystal LiB 3 O 5 is reported in this paper. Based on the calculation and analysis on the beam parameter inside the cavity, a 1.2 W 670 nm output power was achieved at an average pumping electrical power of 1664 W.


Journal of Applied Physics | 1992

Second‐harmonic generation and sum‐frequency mixing of double‐wavelength Nd:YALO3 laser to 413.7‐nm violet coherent radiation in LiIO3 crystal

Huan Shen; Weiran Lin; R.R. Zeng; Y. P. Zhou; G. F. Yu; C. H. Huang; Z.D. Zeng; Zhang Wj

A new method to get 413.7‐nm violet coherent radiation by using second‐harmonic generation and sum‐frequency mixing of radiation from a 1341.4‐ and 1079.5‐nm dual‐wavelength Nd:YALO3 laser in a LiIO3 crystal is reported in this communication. First, the 670.7‐nm red coherent radiation is obtained by second‐harmonic generation of 1341.4‐nm radiations in a LiIO3 crystal, and then the 670.7‐ and 1079.5‐nm radiations are mixed again in a second LiIO3 crystal to get 413.7‐nm radiation. The phase‐matching angles are obtained for both nonlinear optical processes. The experimental results agree well with calculated results.

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R.R. Zeng

Chinese Academy of Sciences

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Y. P. Zhou

Chinese Academy of Sciences

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Z.D. Zeng

Chinese Academy of Sciences

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Hongyuan Shen

Chinese Academy of Sciences

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Huan Shen

Chinese Academy of Sciences

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Weiran Lin

Chinese Academy of Sciences

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G. F. Yu

Chinese Academy of Sciences

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G. Zhang

Chinese Academy of Sciences

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Ge Zhang

Chinese Academy of Sciences

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