[1] [1] C. A. Haynam, P. J. Wegner, and J. M. Auerbach, “National ignition facility laser performance status,” Appl. Opt. 46, 3276–3303 (2007).

[2] [2] M. L. Spaeth, K. R. Manes, M. Bowers, P. Celliers, J.-M. Di Nicola, P. Di Nicola, S. Dixit, G. Erbert, J. Heebner, D. Kalantar, O. Landen, B. MacGowan, B. Van Wonterghem, P. Wegner, C. Widmayer, and S. Yang, “National ignition facility laser system performance,” Fusion Sci. Technol. 69, 366–394 (2016).

[3] [3] V. Supradeepa, “Stimulated Brillouin scattering thresholds in optical fibers for lasers linewidth broadened with noise,” Opt. Express 21, 4677–4687 (2013).

[4] [4] J. R. Murray, J. R. Smith, R. B. Ehrlich, D. T. Kyrazis, C. E. Thompson, T. L. Weiland, and R. B. Wilcox, “Experimental observation and suppression of transverse stimulated Brillouin scattering in large optical components,” J. Opt. Soc. Am. B 6, 2402–2411 (1989).

[5] [5] S. Weber and C. Riconda, “Temperature dependence of parametric instabilities in the context of the shock-ignition approach to inertial confinement fusion,” High Power Laser Sci. Eng. 3, e6 (2015).

[6] [6] D. F. Browning, J. E. Rothenberg, and R. B. Wilcox, The Issue of FM to AM Conversion on the National Ignition Facility (Lawrence Livermore National Laboratory (LLNL), 1998).

[7] [7] C. Dorrer, “Spectral and temporal properties of optical signals with multiple sinusoidal phase modulations,” Appl. Opt. 53, 1007–1019 (2014).

[8] [8] C. Dorrer, R. Roides, R. Cuffney, A. V. Okishev, W. A. Bittle, G. Balonek, A. Consentino, E. Hill, and J. D. Zuegel, “Fiber front end with multiple phase modulations and high-bandwidth pulse shaping for high-energy laser-beam smoothing,” IEEE J. Sel. Top. Quantum Electron. 19, 219–230 (2013).

[9] [9] M. Temporal, B. Canaud, W. J. Garbett, R. Ramis, and S. Weber, “Irradiation uniformity at the Laser MegaJoule facility in the context of the shock ignition scheme,” High Power Laser Sci. Eng. 2, e8 (2014).

[10] [10] S. Vidal, J. Luce, and D. Penninckx, “Experimental demonstration of linear precompensation of a nonlinear transfer function due to second-harmonic generation,” Opt. Lett. 36, 88–90 (2011).

[11] [11] S. Hocquet, G. Lacroix, and D. Penninckx, “Compensation of frequency modulation to amplitude modulation conversion in frequency conversion systems,” Appl. Opt. 48, 2515–2521 (2009).

[12] [12] S. Hocquet, D. Penninckx, E. Bordenave, C. Gouédard, and Y. Jaoun, “FM-to-AM conversion in high-power lasers,” Appl. Opt. 47, 3338–3349 (2008).

[13] [13] D. Penninckx, N. Beck, J.-F. Gleyze, and L. Videau, “Signal propagation over polarization-maintaining fibers: problem and solutions,” J. Lightwave Technol. 24, 4197–4207 (2006).

[14] [14] J. R. Simpson, R. H. Stolen, F. M. Sears, W. Pleibel, J. B. Macchesney, and R. E. Howard, “A single-polarization fiber,” J. Lightwave Technol. 1, 370–374 (1983).

[15] [15] D. Nolan, G. Berkey, M.-J. Li, X. Chen, W. Wood, and L. Zenteno, “Single-polarization fiber with a high extinction ratio,” Opt. Lett. 29, 1855–1857 (2004).

[16] [16] D. Penninckx and N. Beck, “Definition, meaning, and measurement of the polarization extinction ratio of fiber-based devices,” Appl. Opt. 44, 7773–7779 (2005).

[17] [17] Z. Qiao, X. Wang, W. Fan, and Z. Lin, “Demonstration of a highenergy, narrow-bandwidth, and temporally shaped fiber regenerative amplifier,” Opt. Lett. 40, 4214–4217 (2015).