Диссертация (1102749), страница 22
Текст из файла (страница 22)
Panov, and A. Shkurinov, “Simultaneousgeneration of nonlinear optical harmonics and terahertz radiation in air: polarizationdiscrimination of various nonlinear contributions,” Front. Optoelectron., vol. 8, no. 1, pp. 73–80,2014.[89] А. А. Ушаков, П. А. Чижов, Р. В. Волков, В. В. Букин, and С. В. Гарнов, “Зависимостьэффективности генерации терагерцового излучения от состояния поляризации полейдвуцветной накачки про оптическом пробое воздуха,” Краткие сообщения по физикеФИАН, vol.
7, pp. 31–37, 2014.[90] T.-J. Wang, S. Yuan, Y. Chen, and S. L. Chin, “Intense broadband THz generation fromfemtosecond laser filamentation,” Chin. Opt. Lett., vol. 11, no. 1, p. 11401, 2013.[91] Y. You, T. Oh, and K. Kim, “Mechanism of elliptically polarized terahertz generation intwo-color laser filamentation,” Opt. Lett., vol. 38, no. 7, pp. 1034–6, 2013.[92] N. V. Vvedenskii, A. I.
Korytin, V. A. Kostin, A. A. Murzanev, A. A. Silaev, and A. N.Stepanov, “Two-Color Laser-Plasma Generation of Terahertz Radiation Using a FrequencyTunable Half Harmonic of a Femtosecond Pulse,” Phys. Rev. Lett., vol. 112, no. 5, p. 055004,2014.[93] A. Houard, Y. Liu, B. Prade, and A. Mysyrowicz, “Polarization analysis of terahertzradiation generated by four-wave mixing in air.,” Opt. Lett., vol. 33, no. 11, pp.
1195–1197,2008.93[94] J. Wu, Y. Tong, M. Li, H. Pan, and H. Zeng, “THz generation by a two-color pulse inprealigned molecules,” Phys. Rev. A - At. Mol. Opt. Phys., vol. 82, no. 5, pp. 1–15, 2010.[95] J.-M. Manceau, M. Massaouti, and S. Tzortzakis, “Coherent control of THz pulsespolarization from femtosecond laser filaments in gases.,” Opt. Express, vol. 18, no. 18, pp.18894–9, 2010.[96] M.
Li, W. Li, Y. Shi, P. Lu, H. Pan, and H. Zeng, “Verification of the physical mechanismof THz generation by dual-color ultrashort laser pulses,” Appl. Phys. Lett., vol. 101, no. 16, p.161104, 2012.[97] T. I. Oh, Y. S. You, and K. Y. Kim, “Two-dimensional plasma current and optimizedterahertz generation in two-color photoionization,” Opt. Express, vol. 20, no. 18, pp. 19778–19786, 2012.[98] T. I. Oh, Y. S. You, N. Jhajj, E. W. Rosenthal, H. M. Milchberg, and K. Y. Kim, “Scalingand saturation of high-power terahertz radiation generation in two-color laser filamentation,”Appl.
Phys. Lett., vol. 102, no. 20, pp. 10–13, 2013.[99] T. I. Oh, Y. S. You, N. Jhajj, E. W. Rosenthal, H. M. Milchberg, and K. Y. Kim, “Intenseterahertz generation in two-color laser filamentation: Energy scaling with terawatt lasersystems,” New J. Phys., vol. 15, 2013.[100] P. B. Petersen and A. Tokmakoff, “Source for ultrafast continuum infrared and terahertzradiation.,” Opt. Lett., vol.
35, no. 12, pp. 1962–1964, 2010.[101] M. Kress, T. Loffler, M. D. Thomson, R. Dorner, H. Gimpel, K. Zrost, T. Ergler, R.Moshammer, U. Morgner, J. Ullrich, and H. G. Roskos, “Determination of the carrier-envelopephase of few-cycle laser pulses with terahertz-emission spectroscopy,” Nat. Phys., vol. 2, p. 327,2006.[102] Y. Bai, L.
Song, R. Xu, C. Li, P. Liu, Z. Zeng, Z. Zhang, H. Lu, R. Li, and Z. Xu,“Waveform-controlled terahertz radiation from the air filament produced by few-cycle laserpulses,” Phys. Rev. Lett., vol. 108, no. 25, pp. 1–5, 2012.[103] Y. Bai, P. Liu, L. Song, R. Li, and Z. Xu, “Intense THz radiation from laser plasma withcontrollable waveform and polarization,” Proc. SPIE, vol.
9361, no. 21, p. 93611Y, 2015.[104] K.S. Yee, K. S. "Numerical solution of initial boundary value problems involvingMaxwell’s equations in isotropic media", IEEE Trans. Antennas Propag. 14(3), 302-307, 1966.[105] Ghosh, S. K., & Pal, T. (2007). Interparticle coupling effect on the surface plasmonresonance of gold nanoparticles: from theory to applications.
Chemical reviews, 107(11), 47974862, 2007.[106] Taflove, A., & Brodwin, M. E. (1975). Numerical solution of steady-state electromagneticscattering problems using the time-dependent Maxwell's equations. IEEE transactions onmicrowave theory and techniques, 23(8), 623-630.[107] Couairon, A., Brambilla, E., Corti, T. et al. Eur.
Phys. J. Spec. Top. (2011) 199: 5.[108] M. Geissler, G. Tempea, A. Scrinzi, M. Schnurer, F. Krausz, T. Brabec, Phys. Rev. Lett.83, 2930 (1999)[109] H.S. Chakraborty, M.B. Gaarde, A. Couairon, Opt. Lett. 31, 3662 (2006), M.B. Gaarde, A.Couairon, Phys. Rev. Lett.103, 043901 (2009)94[110] A.V. Husakou, J. Herrmann, Phys. Rev. Lett. 87, 203901 (2001).[111] M. Kress, T.
Löffler, S. Eden, M. Thomson, and H. G. Roskos, “Terahertz-pulsegeneration by photoionization of air with laser pulses composed of both fundamental andsecond-harmonic waves,” Opt. Lett., vol. 29, no. 10, pp. 1120–1122, 2004.[112] A.V. Borodin, N.A. Panov, O.G. Kosareva, V.A. Andreeva, M.N. Esaulkov, V.A.Makarov, A.P.
Shkurinov, S.L. Chin, and X.-C. Zhang, “Transformation of THz spectra emittedfrom dual-frequency femtosecond pulse interaction in gases,” Opt. Lett., vol. 38, no. 11, pp.1906–1908, 2013.[113] C.C. Cheng, E.M. Wright, and J.V. Moloney, “Generation of electromagnetic pulses fromplasma channels induced by femtosecond light strings,” Phys. Rev. Lett., vol. 87, no. 21, p.213001, 2001.[114] G.
Shvets, I. Kadanovich, and E. Startsev, “Comment on ‘“Generation of ElectromagneticPulses from Plasma Channels Induced by Femtosecond Light Strings,”’” Phys. Rev. Lett., vol.89, no. 13, p. 139301, 2002.[115] V. T. Tikhonchuk, “Comment on ‘“Generation of Electromagnetic Pulses from PlasmaChannels Induced by Femtosecond Light Strings,”” Phys. Rev. Lett., vol.
89, no. 20, p. 209301,2002.[ 116 ] W. Hoyer, a. Knorr, J. V. Moloney, E. M. Wright, M. Kira, and S. W. Koch,“Photoluminescence and terahertz emission from femtosecond laser-induced plasma channels,”Phys. Rev. Lett., vol. 94, no. 11, pp. 1–4, 2005.[117] C. D. Amico, A. Houard, S. Akturk, Y. Liu, J. Le Bloas, M.
Franco, B. Prade, A.Couairon, V. T. Tikhonchuk, and A. Mysyrowicz, “Forward THz radiation emission byfemtosecond filamentation in gases: Theory and experiment,” New J. Phys., vol. 10, p. 013015,2008.[118] A. Gorodetsky, A. D. Koulouklidis, M. Massaouti, and S. Tzortzakis, “Physics of theconical broadband terahertz emission from two-color laser-induced plasma filaments,” Phys.Rev.
A - At. Mol. Opt. Phys., vol. 89, no. 3, pp. 1–6, 2014.[119] J. Peñano, P. Sprangle, D. Gordon, B. Hafizi, and P. Serafim, “THz generation in plasmasusing two-color laser pulses,” Phys. Rev. E, vol. 81, pp. 1–8, 2010.[120] K. Y. Kim, J. H. Glownia, A. J. Taylor, and G.
Rodriguez, “High-power broadbandterahertz generation via two-color photoionization in gases,” IEEE J. Quantum Electron., vol. 48,no. 6, pp. 797–805, 2012.[121] J. Peñano, P. Sprangle, D. Gordon, B. Hafizi, and P. Serafim, “THz generation in plasmasusing two-color laser pulses,” Phys. Rev.
E, vol. 81, pp. 1–8, 2010.[ 122] А. А. Ушаков, П. А. Чижов, Р. В. Волков, В. В. Букин, and С. В. Гарнов,“Зависимость эффективности генерации терагерцового излучения от состоянияполяризации полей двуцветной накачки про оптическом пробое воздуха,” Краткиесообщения по физике ФИАН, vol. 7, pp. 31–37, 2014.[123] A. A.
Silaev and N. V. Vvedenskii, “Residual-current excitation in plasmas produced byfew-cycle laser pulses,” Phys. Rev. Lett., vol. 102, no. 11, pp. 1–4, 2009.[124] H.G. Muller, “An efficient propagation scheme for the time-dependent Schr ̈odingerequation in the velocity gauge,” Laser Phys., vol. 9, p. 138, 1999.95[125] N. Karpowicz, X. Lu, and X.-C.
Zhang, “Terahertz gas photonics,” J. Mod. Opt., vol. 56,no. 10, pp. 1137–1150, 2009.[126] A. V Andreev and S. Y. Stremoukhov, “Terahertz-radiation generation in the ionizationfree regime of light-atom interaction,” Phys. Rev. A, vol. 87, p. 053416, 2013.[127] S. Y. Stremoukhov and A. V Andreev, “Spatial variations of the intensity of THz radiationemitted by extended media in two-color laser fields,” Laser Phys. Lett., vol. 12, no. 1, p. 015402,2015.[128] M. Kolesik and J. V. Moloney, “Nonlinear optical pulse propagation simulation: FromMaxwell’s to unidirectional equations,” Phys. Rev. E - Stat.
Nonlinear, Soft Matter Phys., vol.70, no. 3 2, pp. 1–11, 2004.[129] I. Babushkin, W. Kuehn, C. Köhler, S. Skupin, L. Bergé, K. Reimann, M. Woerner, J.Herrmann, and T. Elsaesser, “Ultrafast spatiotemporal dynamics of terahertz generation byionizing two-color femtosecond pulses in gases,” Phys. Rev. Lett., vol. 105, no. 5, pp. 1–4, 2010.[130] L. Bergé, S.
Skupin, C. Köhler, I. Babushkin, and J. Herrmann, “3D numerical simulationsof THz generation by two-color laser filaments,” Phys. Rev. Lett., vol. 110, no. 7, pp. 1–5, 2013.[131] I. Babushkin, S. Skupin, A. Husakou, C. Kohler, E. Cabrera-Granado, L. Berge, and J.Herrmann, “Tailoring terahertz radiation by controlling tunnel photoionization events in gases,”New J. Phys., vol. 13, p. 123029, 2011.[132] Marburger, J.
H. (1975). Self-focusing: theory. Progress in Quantum Electronics, 4, 35110.[133] Couairon, A. (2003). Dynamics of femtosecond filamentation from saturation of selffocusing laser pulses. Physical Review A, 68(1), 015801.[134] J. Kasparian, R. Sauerbrey, and S. L. Chin, Appl. Phys. B 71, 877 (2000)[135] L. V. Keldysh, “Ionization in the field of a strong electromagnetic wave”, Sov.
Phys.JETP, vol. 20, pp. 1307, 1965.[136] J. Muth-Böhm, A. Becker, and F. H. M. Faisal, “Suppressed molecular ionization for aclass of diatomics in intense femtosecond laser fields”, Phys. Rev. Lett., vol. 85, pp. 2280, 2000.[137] Thomas Kim Kjeldsen and Lars Bojer Madsen, “Strong-field ionization of N2: length andvelocity gauge strong-field approximation and tunnelling theory”, J. Phys. B, vol.
37, pp. 2033,2004.[138] M. V. Ammosov, N. B. Delone, and V. P. Krainov, “Tunnel ionization of complex atomsand of atomic ions in an alternating electromagnetic field”, Sov. Phys. JETP, vol. 64, pp. 1191,1986.[139] X. M. Tong, Z. X. Zhao, and C. D. Lin, “Theory of molecular tunneling ionization”, Phys.Rev. A, vol. 66, pp. 033402, 2002.[140] X. M. Tong and C.D. Lin, “Empirical formula for static field ionization rates of atoms andmolecules by lasers in the barrier-suppression regime”, J.
![](https://s.studizba.com/z.php?f=/templates/si/i/noavatar.png&w=100&h=100&t=1"){kind=avatar}
