[1] Dudley J M, Genty G R, Coen S. Supercontinuum generation in photonic crystal fiber [J]. Rev. Mod. Phys., 2006, 78(4): 1135-1184.

[2] Alfano R R, Shapiro S L. Emission in the Region 4000 to 7 000  Via Four-Photon Coupling in Glass [J]. Phys. Rev. Lett., 1970, 24(11): 584-587.

[3] Ranka J K, Windeler R S, Stentz A J. Visible continuum generation in air-silica microstructure optical fibers with anomalous dispersion at 800 nm [J]. Opt. Lett., 2000, 25(1): 25-27.

[4] Nisoli M, De Silvestri S, Svelto O. Generation of high energy 10 fs pulses by a new pulse compression technique [J]. Appl. Phys. Lett., 1996, 68(20): 2793-2795.

[5] Durfee C G, Backus S, Murnane M M, et al. Ultrabroadband phase-matched optical parametric generation in the ultraviolet by use of guided waves [J]. Opt. Lett., 1997, 22(20): 1565.

[6] Popmintchev T, Chen M, Arpin P, et al. The attosecond nonlinear optics of bright coherent X-ray generation [J]. Nat. Photonics., 2010, 4(12): 822-832.

[7] Welch M G, Cook K, Correa R A, et al. Solitons in Hollow Core Photonic Crystal Fiber: Engineering Nonlinearity and Compressing Pulses [J]. J. Lightwave Technol., 2009, 27(11): 1644-1652.

[8] Ouzounov D G. Generation of megawatt optical solitons in hollow-core photonic band-gap fibers [J]. Science, 2003, 301(5640): 1702-1704.

[9] Russell P S J, H lzer P, Chang W, et al. Hollow-core photonic crystal fibres for gas-based nonlinear optics [J]. Nat. Photonics., 2014, 8(4): 278-286.

[10] Travers J C, Chang W, Nold J, et al. Ultrafast nonlinear optics in gas-filled hollow-core photonic crystal fibers [Invited][J]. J. Opt. Soc. Am. B., 2011, 28(12): A11-A26.

[11] Benabid F. Stimulated Raman scattering in hydrogen-filled hollow-core photonic crystal fiber [J]. Science, 2002, 298(5592): 399-402.

[12] Pearce G J, Wiederhecker G S, Poulton C G, et al. Models for guidance in kagome-structured hollow-core photonic crystal fibres [J]. Opt. Express, 2007, 15(20): 12680-12685.

[13] Couny F, Benabid F, Roberts P J, et al. Generation and Photonic Guidance of Multi-Octave Optical-Frequency Combs [J]. Science, 2007, 318(5853): 1118-1121.

[14] Février S, Beaudou B T, Viale P. Understanding origin of loss in large pitch hollow-core photonic crystal fibers and their design simplification [J]. Opt. Express, 2010, 18(5): 5142-5150.

[15] Wang Y Y, Wheeler N V, Couny F, et al. Low loss broadband transmission in hypocycloid-core Kagome hollow-core photonic crystal fiber [J]. Opt Lett., 2011, 36(5): 669-671.

[16] Yu F, Knight J C. Negative curvature hollow-core optical fiber [J]. IEEE J. Sel. Top. Quantum Electron., 2016, 22(2): 146-155.

[17] Meng F, Gao S, Wang Y, et al. Efficient dispersive waves generation from argon-filled anti-resonant nodeless fiber [C]. CLEO_SI.2017.STu3K.4., 2017.

[18] Debord B, Alharbi M, Vincetti L, et al. Multi-meter fiber-delivery and pulse self-compression of milli-Joule femtosecond laser and fiber-aided laser-micromachining [J]. Opt. Express, 2014, 22(9):10735-10746.

[19] Guichard F, Giree A, Zaouter Y, et al. Nonlinear compression of high energy fiber amplifier pulses in air-filled hypocycloid-core Kagome fiber [J]. Opt. Express, 2015, 23(6):7416-7423.

[20] Mak K F, Seidel M, Pronin O, et al. Compressing μJ-level pulses from 250 fs to sub-10 fs at 38-MHz repetition rate using two gas-filled hollow-core photonic crystal fiber stages [J]. Opt Lett., 2015, 40(7): 1238-1241.

[21] Joly N Y, Nold J, Chang W, et al. Bright spatially coherent wavelength-tunable deep-UV laser source using an Ar-filled photonic crystal fiber [J]. Phys. Rev. Lett., 2011, 106(20): 203901.

[22] ZHOU Y Z, HUANG L L, Chai L, et al. The beam combination of multi-core photonic crystal fiber by using the Kagome fiber [J]. Acta Phys. Sin.,(周雨竹,黄莉莉,柴路,等. 利用Kagome光纤实现多芯光子晶体光纤的输出合束. 物理学报)2016, 65(2): 024206.

[23] Litchinitser N M, Dunn S C, Usner B, et al. Resonances in microstructured optical waveguides [J]. Opt Express, 2003, 11(10): 1243-1251.

[24] Chang W, Nazarkin A, Travers J C, et al. Influence of ionization on ultrafast gas-based nonlinear fiber optics [J]. Opt. Express, 2011, 19(21): 21018-21027.

[25] Couairon A, Brambilla E, Corti T, et al. Practitioner’s guide to laser pulse propagation models and simulation [J]. Eur. Phys. J. Spec. Top., 2011, 199(1): 5-76.

[26] Kolesik M, Moloney J V. Modeling and simulation techniques in extreme nonlinear optics of gaseous and condensed media [J]. Rep. Prog. Phys., 2014, 77(1): 016401.

[27] Sinkin O V, Holzlohner R, Zweck J, et al. Optimization of the split-step fourier method in modeling optical-fiber communications systems [J]. J. Lightwave Technol., 2003, 21(1): 61-68.

[28] Husakou A V, Herrmann J. Supercontinuum generation of higher-order solitons by fission in photonic crystal fibers [J]. Phys. Rev. Lett., 2001, 87(20): 203901.

[29] Archambault J L, Black R J, Lacroix S, et al. Loss calculations for antiresonant waveguides [J]. J. Lightwave Technol., 1993, 11(3): 416-423.

[30] Vincetti L, Setti V. Waveguiding mechanism in tube lattice fibers [J]. Opt. Express, 2010, 18(22): 23133-23146.

[31] Borzsonyi A, Heiner Z, Kalashnikov M P, et al. Dispersion measurement of inert gases and gas mixtures at 800 nm [J]. Appl. Opt., 2008, 47(27): 4856-4863.

[32] Agrawal G P. Nonlinear fiber optics [M]. Amsterdam: Elsevier/Academic Press, 2013.

[33] Balciunas T, Fourcade-Dutin C, Fan G, et al. A strong-field driver in the single-cycle regime based on self-compression in a kagome fibre [J]. Nat. Communications, 2015, 6: 6117.

[34] Nazarkin A, Korn G. Pulse self-compression in the subcarrier cycle regime [J]. Phys. Rev. Lett., 1999, 83(23): 4748-4751.