[1] D. J. Binks,L. A. W. Gloster,T. A. King et al.. Frequency locking of a pulsed single-longitudinal-mode laser in a coupled-cavity resonator[J]. Appl. Opt.,1997,36(36):9371-9377
[2] C. T. Gross,J. Kiess,F. Keilmann. Pulsed high-power far-infrared gas lasers:performance and spectral survey[J]. IEEE J. Quantu. Electron.,1987,QE-23(4):377-384
[3] O. A. Romanovskii. Applicability of airborne lidars based on middle IR gas lasers for gas analysis of the atmosphere[C]. SPIE,2007,6594:65940C-1
[4] G. Kovar,D. Larouche,M. Piche et al.. Single-longitudinal-mode operation of a TEA CO2 laser with a modified Fabry-Perot interferometer[J]. Appl. Opt.,1985,24(21):3584-3590
[5] K. Silakhori,A. Behjat,F. Soltanmoradi et al.. A compact injection locked single longitudinal mode TEA CO2 laser[C]. SPIE,2005,5777:433-437
[6] A. K. Kar,D. M. Tratt,J. H. Mathew et al.. Status and prospects of hybrid and injection-locked TEA CO2 lasers for lidar and nonlinear optics applications[J]. IEEE J. Quant. Electron.,1985,QE-21(4):359-364
[7] A. Kumar,J. P. Nilaya,D. J. Biswas. Improved efficiency of a hybrid CO2 laser as a result of increased TEM00 mode filling factor[J]. Rev. Sci. Instrum.,2004,75(12):5203-5204
[8] N. P. Barnes,J. C. Barnes. Injection seeding. I. Theory[J]. IEEE J. Quant. Electron.,1993,29(10):2670-2683
[9] S. Y. Tochitsky,R. Narang,C. Filip et al.. Generation of 160-ps terawatt-power CO2 laser pulses[J]. Opt. Lett.,1999,24:1717-1719
[10] E. Palange,G. Salvetti. Control of intrapulse frequency chirping in long-pulse CO2 lasers employing perturbation-insensitive optical cavities[J]. Appl. Opt.,1991,30(27):3832-3841
[11] J. M. Boon-Engering,L. A. W. Gloster,W.E. van derVeer et al.. Highly efficient single-longitudinal-mode β-BaB2O4 optical parametric oscillator with a new cavity design[J]. Opt. Lett.,1995,20:2087-2089
[12] G. Salvetti,E. Palange,G. Salvetti. Multipass-prism interferometer for fine-frequency-tuning,single-mode operation of TEA CO2 lasers[J]. Opt. Lett.,1984,9:393-395
[13] Y. H. Wang,Y. C. Qu,W. J. Zhao et al.. Single longitudinal mode pulse from a TEA CO2 laser by using a three-mirror resonator with a Fabry-Pérot etalon[J]. Appl. Phys. B.,2008,92:237-241
[14] J. R. Izatt,M. A. Rob,Wen-sen Zhu. Two and three-grating resonators for high-power pulsed CO2 lasers[J]. Appl. Opt.,1991,30:4319-4329
[15] J. M. Vaughan. The Fabry-Prot Interferometer:History,Theory,Practice,and Applications[M]. Taylor & Francis(1989)
[16] Lü Yanfei,Tan Huiming,Miao Tongqun et al.. All-solid-state CW doubly resonant all-intracavity sum-frequency mixing 593 nm laser[J]. Chinese J. Lasers,2005,32(6):730-732