摘要Frequency modulation to amplitude modulation (FM-to-AM) conversion is important for controlling temporal shapes of high-power Nd:glass lasers in the application of fusion ignition. To suppress this FM-to-AM conversion effect in the process of broadband third-harmonic generation of Nd:glass laser, we report an efficient frequency-tripling scheme based on mixing narrowband and broadband pulses. Numerical results show that the FM-to-AM conversion in frequency conversion process can be suppressed effectively. For a required third-harmonic bandwidth of 1 THz, the defined relative modulation α in pulse intensity is as large as 180% in the conventional baseline design, while it will be reduced to only about 20% by using our proposed scheme.
Abstract:Frequency modulation to amplitude modulation (FM-to-AM) conversion is important for controlling temporal shapes of high-power Nd:glass lasers in the application of fusion ignition. To suppress this FM-to-AM conversion effect in the process of broadband third-harmonic generation of Nd:glass laser, we report an efficient frequency-tripling scheme based on mixing narrowband and broadband pulses. Numerical results show that the FM-to-AM conversion in frequency conversion process can be suppressed effectively. For a required third-harmonic bandwidth of 1 THz, the defined relative modulation α in pulse intensity is as large as 180% in the conventional baseline design, while it will be reduced to only about 20% by using our proposed scheme.
[1] Murray J R et al 1989 J. Opt. Soc. Am . B 6 2402
[2] Skupsky S et al 1989 J. Appl. Phys. 66 3456
[3] Boehly T R et al 2001 Phys. Plasmas 8 2331
[4] Rothenberg J E et al 1999 Proc. SPIE 3492 51
[5] Hocquet S et al 2008 App. Opt. 47 3338
[6] Qiu Z R, Cai X J and Wang Z J 1991 Acta Opt. Sin. 11 208 (in Chinese)
[7] Eimerl D et al 1997 Opt. Lett. 22 1208
[8] Li K, Zhang B, Yuan X D and Wei X F 2005 High Power Laser and Particle Beams 17 995 (in Chinese)
[9] Qian L J 1995 Acta Opt. Sin. 15 662 (in Chinese)
[10] Yang Y S et al 2007 Acta Phys. Sin. 56 6468 (in Chinese)
[11] Yang Y S et al 2009 Opt. Lett. 24 3848
[12] Zheng W G, Qian L J, Yuan P, Luo H and Zhu H Y 2006 Chin. Phys. Lett. 23 139
[13] Han W et al 2008 Chin. Phys. Lett. 25 4003
[14] Wu Y C et al 2005 Chin. Phys. Lett. 22 1426
[15] Babushkin A et al 1998 Opt. Lett. 23 927
[16] Zhao K et al 2010 J. Opt. 12 035206
[17] Shi S X, Chen G F, Zhao W and Liu J F 2003 Nonliear Optics (Xian: Xidian University Press) p 375
[18] Boscheron A C L, Sauteret C J and Migus A 1996 J. Opt. Soc. Am . B 13 818
[19] Hocquet S et al 2008 J. Phys.: Conf. Ser. 112 032016