[1] Fedotov S I, Feoktistov L P, Osipov M V. Lasers for ICF with a controllable function of mutual coherence of radiation[J]. Journal of Russian Laser Research, 25, 79-92(2004).

[2] Lindl J D, Amendt P, Berger R L. The physics basis for ignition using indirect-drive targets on the National Ignition Facility[J]. Physics of Plasmas, 11, 339-491(2004).

[3] Smalyuk V A, Shvarts D, Betti R. Role of hot-electron preheating in the compression of direct-drive imploding targets with cryogenic D2 ablators[J]. Physical Review Letters, 100, 1459-1469(2008).

[4] Karasik M, Weaver J L, Aglitskiy Y. Suppression of laser nonuniformity imprinting using a thin high-z coating[J]. Physical Review Letters, 114, 085001(2015).

[5] Eimerl D, Campbell E M, Krupke W F. StarDriver: a flexible laser driver for inertial confinement fusion and high energy density physics[J]. Journal of Fusion Energy, 33, 476-488(2014).

[6] Garanin S G, Derkach V N, Shnyagin R A. Formation of the uniform irradiation of a target in high-power laser facilities[J]. Quantum Electronics, 34, 427-446(2004).

[8] Marozas J A. Fourier transform-based continuous phase-plate design technique: a high-pass phase-plate design as an application for OMEGA and the National Ignition Facility[J]. Journal of The Optical Society of America A-optics Image Science and Vision, 24, 74-83(2007).

[9] Marozas J A, Kelly J H. Angular spectrum representation of pulsed laser beams with two-dimensional smoothing by spectral dispersion[J]. LLE Rev, 78, 62-81(1999).

[10] Regan S, Marozas J A, Kelly J. Experimental investigation of smoothing by spectral dispersion[J]. Journal of The Optical Society of America B-optical Physics, 17, 1483-1489(2000).

[11] Regan S, Marozas J A, Craxton R S. Performance of 1-THz-bandwidth, two-dimensional smoothing by spectral dispersion and polarization smoothing of high-power, solid-state laser beams[J]. Journal of The Optical Society of America B-optical Physics, 22, 998-1002(2005).

[12] Moody J D, Michel P, Divol L. Multistep redirection by cross-beam power transfer of ultrahigh-power lasers in a plasma[J]. Nature Physics, 8, 344-349(2012).

[13] Betti R, Hurricane O A. Inertial-confinement fusion with lasers[J]. Nature Physics, 12, 435-448(2016).

[14] Glenzer S H, Froula D H, Divol L. Experiments and multiscale simulations of laser propagation through ignition-scale plasmas[J]. Nature Physics, 3, 716-719(2007).

[15] Labaune, Christine. Laser-driven fusion: Incoherent light on the road to ignition[J]. Nature Physics, 3, 680-682(2007).

[16] Santos J E, Silva L O, Bingham R. White-light parametric instabilities in plasmas[J]. Physical Review Letters, 98, 235001(2007).

[17] Follett R K, Shaw J G, Myatt J F. Thresholds of absolute instabilities driven by a broadband laser[J]. Physics of Plasmas, 26, 062111(2019).

[18] Palastro J P, Shaw J G, Follett R K. Resonance absorption of a broadband laser pulse[J]. Physics of Plasmas, 25, 123104(2018).

[19] Eimerl D, Skupsky S, Campbell E M. StarDriver: Recent results on beam smoothing and LPI mitigation[J]. Journal of Physics Conference, 717, 012015(2016).

[20] Dorrer C. Statistical analysis of incoherent pulse shaping[J]. Optics Express, 17, 3341-3352(2009).

[21] Spaeth M L, Manes K R, Bowers M. National ignition facility laser system performance[J]. Fusion Science and Technology, 69, 366-394(2016).

[22] Cui Y, Gao Y, Rao D. High-energy low-temporal-coherence instantaneous broadband pulse system[J]. Optics Letters, 44, 2859-2862(2019).

[23] Dorrer C, Hill E M, Zuegel J D. High-energy parametric amplification of spectrally incoherent broadband pulses[J]. Optics Express, 28, 451-471(2020).

[24] Franken P A, Hill A E, Peters C W. Generation of optical harmonics[J]. Physical Review Letters, 7, 118-119(1961).

[25] Bloembergen N, Pershan P S. Light waves at the boundary of nonlinear media[J]. Physical Review, 128, 606-622(1962).

[26] Martinez O E. Achromatic phase matching for second harmonic generation of femtosecond pulses[J]. IEEE Journal Quantum Electronics, 25, 2464-2468(1989).

[27] Richman B A, Bisson S E, Trebino V. Efficient broadband second-harmonic generation by dispersive achromatic nonlinear conversionusing only prisms[J]. Opt Lett, 23, 497(1998).

[28] Ashihara S, Shimura T, Kuroda K. Group-velocity matched second-harmonic generation in tilted quasi-phase-matched gratings[J]. Journal of the Optical Society of America B, 20, 853-856(2003).

[29] Chen B Q, Zhang C, Hu C Y. High-efficiency broadband high-harmonic generation from a single quasi-phase-matching nonlinear crystal[J]. Physical Review Letters, 115, 083902(2015).

[30] Zhang T R, Choo H R, Downer M C. Phase and group velocity matching for second harmonic generation of femtosecond pulses[J]. Applied Optics, 29, 3927-3933(1990).

[31] Brown M. Increased spectral bandwidths in nonlinear conversion processes by use of multicrystal designs[J]. Optics Letters, 23, 1591-1593(1998).

[32] Wang G Y, Garmire E M. High-efficiency generation of ultrashort second-harmonic pulses based on the erenkov geometry[J]. Optics Letters, 19, 254-256(1994).

[33] Pronko M S, Lehmberg R H, Obenschain S P. Efficient second harmonic conversion of broad-band high-peak-power Nd:glass laser radiation using large-aperture KDP crystals in quadrature[J]. IEEE Journal of Quantum Electronics, 26, 337-347(1990).

[34] Ji Lailin, Zhu Baoqiang, Liu Chong. Optimization of quadrature frequency conversion with type-II KDP for second harmonic generation of the nanosecond chirp pulse at 1053 nm[J]. Chinese Optics Letters, 12, 70-74(2014).

[35] Eimerl D, Auerbach J M, Barker C E. Multicrystal designs for efficient third-harmonic generation[J]. Optics Letters, 22, 1208-1210(1997).

[36] Babushkin A, Craxton R S, Oskoui S. Demonstration of the dual-tripler scheme for increased-bandwidth third-harmonic generation[J]. Optics Letters, 23, 927-929(1998).

[37] Short R W, Skupsky S. Frequency conversion of broad-bandwidth laser light[J]. IEEE Journal of Quantum Electronics, 26, 580-588(1990).

[38] Skeldon M D, Craxton R S, Kessler T J. Efficient harmonic generation with a broad-band laser[J]. IEEE Journal of Quantum Electronics, 28, 1389-1399(1992).

[39] [39] Nakatsuka M, Miyanaga N, Kanabe T, et al. Partially coherent light sources f ICF experiment[C] Proc of SPIE. 1993, 1870: 151162.

[40] [40] Videau L, Boscheron A C L, Garnier J C, et al. Recent results of optical smoothing on the Phebus laser[C] Proc of SPIE.1997, 3047: 757762.

[41] Boscheron A C, Sauteret C, Migus A. Efficient broadband sum frequency based on controlled phase-modulated input fields: theory for 351-nm ultrabroadband or ultrashort-pulse generation[J]. Journal of The Optical Society of America B-optical Physics, 13, 818-826(1996).

[42] Raoult F, Boscheron A C, Husson D. Ultrashort, intense ultraviolet pulse generation by efficient frequency tripling and adapted phase matching[J]. Optics Letters, 24, 354-356(1999).

[45] Rozenberg E, Arie A. Broadband and robust adiabatic second-harmonic generation by a temperature gradient in birefringently phase-matched lithium triborate crystal[J]. Optics Letters, 44, 3358-3361(2019).

[46] Zhu H Y, Wang T, Zheng W G. Efficient second harmonic generation of femtosecond laser at 1 μm[J]. Optics Express, 12, 2150-2155(2004).

[47] Zheng Wanguo, Qian LieJia, Yuan Peng. Second harmonic generation of femtosecond laser at one micron in a partially deuterated KDP[J]. Chinese Physics Letters, 23, 139-142(2006).

[48] Dmitriev V G, Osipov M V, Puzyrev V N. Nonlinear optical conversion of Nd:glass laser multimode radiation into the second harmonic in KDP crystal[J]. Journal of Physics B, 45, 165401(2012).

[49] Vasin B L, Korobkin Y V, Osipov M V. Second-harmonic conversion of partially coherent radiation of neodymium glass laser[J]. Bulletin of the Lebedev Physics Institute, 40, 205-209(2013).

[50] Ji L, Zhao X, Liu D. High-efficiency second-harmonic generation of low-temporal-coherent light pulse[J]. Optics Letters, 44, 4359-4362(2019).