第一章 参考文献
[1.1] T. H. Maiman, “Stimulated optical radiation in Ruby,” Nature 187, 493 (1960).
[1.2] E. Hoover and J. Squier, “Advances in multiphoton microscopy technology,” Nat. Photon. 7, 93 (2013).
[1.3] T. Yajima, F. Shimizu, and K. Shimoda, “High-speed photography using a ruby optical maser,” Appl. Opt. 1, 770 (1962).
[1.4] D. E. Spence, P. N. Kean, and W. Sibbett, “60-fsec pulse generation from a self-mode- locked Ti:sapphire laser,” Opt. Lett. 16, 42 (1991).
[1.5] A. H. Zewail, “Femtochemistry: Atomic-scale dynamics of the chemical bond,” J. Phys. Chem. A 104, 5660 (2000).
[1.6] Y. C. Lin, Y. Nabekawa, and K. Midorikawa, “Optical parametric amplification of sub- cycle shortwave infrared pulses,” Nat. Commun. 11, 3413 (2020).
[1.7] K. Midorikawa, “High-order harmonic generation and attosecond science,” Jpn. J. Appl. Phys. 50, 090001 (2011).
[1.8] T. Gaumnitz, A. Jain, Y. Pertot, M. Huppert, I. Jordan, F. Ardana-Lamas, and H. J. Wörner, “Streaking of 43-attosecond soft-X-ray pulses generated by a passively CEP- stable mid-infrared driver,” Opt. Express 25, 27506 (2017).
[1.9] M. Chini, H. Mashiko, H. Wang, S. Chen, C. Yun, S. Scott, S. Gilbertson, and Z. Chang, “Delay control in attosecond pump-probe experiments,” Opt. Express 17, 21459 (2009).
[1.10] E. Goulielmakis, M. Uiberacker, R. Kienberger, A. Baltuska, V. Yakovlev, A. Scrinzi, T. Westerwalbesloh, U. Kleineberg, U. Heinzmann, M. Drescher, and F. Krausz, “Direct measurement of light waves,” Science 305, 1267 (2004).
[1.11] M. Hentschel, R. Kienberger, C. Spielmann, G. A. Reider, N. Milosevic, T. Brabec, P. Corkum, U. Heinzmann, M. Drescher, and F. Krausz, “Attosecond metrology,” Nature 414, 509 (2001).
[1.12] P. M. Paul, E. S. Toma, P. Breger, G. Mullot, F. Augé, P. Balcou, H. G. Muller, and P. Agostini, “Observation of a train of attosecond pulses from high harmonic generation,” Science 292, 1689 (2001).
[1.13] M. Drescher, M. Hentschel, R. Kienberger, M. Uiberacker, V. Yakovlev, A. Scrinzi, T. Westerwalbesloh, U. Kleineberg, U. Heinzmann, and F. Krausz, “Time-resolved atomic inner-shell spectroscopy,” Nature 419, 803 (2002).
[1.14] M. Uiberacker, T. Uphues, M. Schultze, A. J. Verhoef, V. Yakovlev, M. F. Kling, J. Rauschenberger, N. M. Kabachnik, H. Schroder, M. Lezius, K. L. Kompa, H.-G. Muller, M. J. J. Vrakking, S. Hendel, U. Kleineberg, U. Heinzmann, M. Drescher, and F. Krausz, “Attosecond real-time observation of electron tunnelling in atoms,” Nature 446, 627 (2007).
[1.15] M. Schultze, M. Fieß, N. Karpowicz, J. Gagnon, M. Korbman, M. Hofstetter, S. Neppl, A. L. Cavalieri, Y. Komninos, T. Mercouris, C. A. Nicolaides, R. Pazourek, S. Nagele, J. Feist, J. Burgdörfer, A. M. Azzeer, R. Ernstorfer, R. Kienberger, U. Kleineberg, E. Goulielmakis, F. Krausz, and V. S. Yakovlev, “Delay in photoemission,” Science 328, 1658 (2010).
[1.16] A. Wirth, M. T. Hassan, I. Grguraš, J. Gagnon, A. Moulet, T. T. Luu, S. Pabst, R. Santra, Z. A. Alahmed, A. M. Azzeer, V. S. Yakovlev, V. Pervak, F. Krausz, and E. Goulielmakis, “Synthesized light transients,” Science 334, 195 (2011).
[1.17] Y. Nabekawa, Y. Furukawa, T. Okino, A. A. Eilanlou, E. J. Takahashi, K. Yamanouchi, and K. Midorikawa, “Settling time of a vibrational wavepacket in ionization,” Nat. Commun. 6, 8197 (2015).
[1.18] M. Sabbar, H. Timmers, Y.-J. Chen, A. K. Pymer, Z.-H. Loh, S. Sayres, S. Pabst, R. Santra, and S. R. Leone, “State-resolved attosecond reversible and irreversible dynamics in strong optical fields,” Nat. Phys. 13, 472 (2017).
[1.19] F. Calegari, D. Ayuso, A. Trabattoni, L. Belshaw, S. De Camillis, S. Anumula, F. Frassetto, L. Poletto, A. Palacios, P. Decleva, J. B. Greenwood, F. Martín, and M. Nisoli, “Ultrafast electron dynamics in phenylalanine initiated by attosecond pulses,” Science 346, 336 (2014).
[1.20] C. Ott, A. Kaldun, L. Argenti, P. Raith, K. Meyer, M. Laux, Y. Zhang, A. Blattermann, S. Hagstotz, T. Ding, R. Heck, J. Madronero, F. Martin, and T. Pfeifer, “Reconstruction and control of a time-dependent two-electron wave packet,” Nature 516, 374 (2014).
[1.21] M. Schultze, E. M. Bothschafter, A. Sommer, S. Holzner, W. Schweinberger, M. Fiess, M. Hofstetter, R. Kienberger, V. Apalkov, V. S. Yakovlev, M. I. Stockman, and F. Krausz, “Controlling dielectrics with the electric field of light,” Nature 493, 75 (2013).
[1.22] M. Schultze, K. Ramasesha, C. Pemmaraju, S. Sato, D. Whitmore, A. Gandman, J. S. Prell, L. J. Borja, D. Prendergast, K. Yabana, D. M. Neumark, and S. R. Leone, “Attosecond band-gap dynamics in silicon,” Science 346, 1348 (2014).
[1.23] H. Mashiko, K. Oguri, T. Yamaguchi, A. Suda, and H. Gotoh, “Petahertz optical drive with wide-bandgap semiconductor,” Nat. Phys. 12, 741 (2016).
[1.24] M. Lucchini, S. A. Sato, A. Ludwig, J. Herrmann, M. Volkov, L. Kasmi, Y. Shinohara, K. Yabana, L. Gallmann, and U. Keller, “Attosecond dynamical Franz-Keldysh effect in polycrystalline diamond,” Science 353, 916 (2016).
[1.25] M. Volkov, S. A. Sato, F. Schlaepfer, L. Kasmi, N. Hartmann, M. Lucchini, L. Gallmann, A. Rubio, and U. Keller, “Attosecond screening dynamics mediated by electron localization in transition metals,” Nat. Phys. 15, 1145 (2019).
[1.26] F. Krausz and M. Ivanov, “Attosecond physics,” Rev. Mod. Phys. 81, 163 (2009). [1.27] J. Puebla, J. Kim, K. Kondou, and Y. Otani, “Spintronic devices for energy-efficient data storage and energy harvesting,” Commun. Mater. 1, 24 (2020).
[1.28] S. A. Wolf, D. D. Awschalom, R. A. Buhrman, J. M. Daughton, S. von Molnar, M. L. Roukes, A. Y. Chtchelkanova, and D. M. Treger, “Spintronics: A spin-based electronics vision for the future,” Sicence 294, 1488 (2001).
[1.29] A. Kirilyuk, A. V. Kimel, and T. Rasing, “Ultrafast optical manipulation of magnetic order,” Rev. Mod. Phys. 88, 039904 (2016).
[1.30] F. Siegrist, J. A. Gessner, M. Ossiander, C. Denker, Y.-P. Chang, M. C. Schröder, A. Guggenmos, Y. Cui, J. Walowski, U. Martens, J. K. Dewhurst, U. Kleineberg, M. Münzenberg, S. Sharma, and M. Schultze, “Light-wave dynamic control of magnetism,” Nature 571, 240 (2019).
[1.31] J. K. Dewhurst, P. Elliott, S. Shallcross, E. K. U. Gross, and S. Sharma, “Laser-induced intersite spin transfer,” Nano Lett. 18, 1842 (2018).
[1.32] H. Höchst, R. Patel, and F. Middleton, “Multiple-refection λ4 phase shifter: a viable alternative to generate circular-polarized synchrotron radiation,” Nucl. Instrum. Meth. A 347, 107 (1994).
[1.33] F. Willems, C. T. L. Smeenk, N. Zhavoronkov, O. Kornilov, I. Radu, M. Schmidbauer, M. Hanke, C. von Korff Schmising, M. J. J. Vrakking, and S. Eisebitt, “Probing ultrafast spin dynamics with high-harmonic magnetic circular dichroism spectroscopy,” Phys. Rev. B 92, 220405 (2015).
[1.34] A. Fleischer, O. Kfir, T. Diskin, P. Sidorenko, and O. Cohen, “pin angular momentum and tunable polarization in high-harmonic generation,” Nat. Photon. 8, 543 (2014).
[1.35] T. Fan, P. Grychtol, R. Knut, C. Hernández-García, D. D. Hickstein, D. Zusin, C. Gentry, F. J. Dollar, C. A. Mancuso, C. W. Hogle, O. Kfir, D. Legut, K. Carva, J. L. Ellis, K. M. Dorney, C. Chen, O. G. Shpyrko, E. E. Fullerton, O. Cohen, P. M. Oppeneer, D. B. Milošević, A. Becker, A. A. Jaroń-Becker, T. Popmintchev, M. M. Murnane, and H. C. Kapteyn, “Bright circularly polarized soft X-ray high harmonics for X-ray magnetic circular dichroism,” Proc. Natl. Acad. Sci. USA 112, 14206 (2015).
[1.36] O. Kfir, S. Zayko, C. Nolte, M. Sivis, M. Möller, B. Hebler, S. S. P. K. Arekapudi, D. Steil, S. Schäfer, M. Albrecht, O. Cohen, S. Mathias, and C. Ropers, “Nanoscale magnetic imaging using circularly polarized high-harmonic radiation,” Sci. Adv. 3, 4641 (2017).
[1.37] J. F. Ward and C. H. C. New, “Optical third harmonic generation in gases by a focused laser beam,” Phys. Rev. A 185, 57 (1969).
[1.38] J. Reintjes, C-Y. She, and R. Eckardt, “Generation of coherent radiation in XUV by fifth- and seventh-order frequency conversion in rare gases,” IEEE J. Quantum Electron. 14, 581 (1978).
[1.39] J. Bokor, P. H. Bucksbaum, and R. R. Freeman, “Generation of 35.5-nm coherent radiation,” Opt. Lett. 8, 217 (1983).
[1.40] A. McPherson, G. Gibson, H. Jara, U. Johann, T. S. Luk, I. A. McIntyre, K. Boyer, and C. K. Rhodes, “Studies of multiphoton production of vacuum-ultraviolet radiation in the rare gases,” J. Opt. Soc. Am. B 4, 595 (1987).
[1.41] M. Ferray, A. L’Huillier, X. F. Li, L. A. Lompre, G. Mainfray, and C. Manus, “Multiple-harmonic conversion of 1064 nm radiation in rare gases,” J. Phys. B 21, 1669 (1991).
[1.42] N. Sarukura, K. Hata, T. Adachi, R. Nodomi, M. Watanabe, and S. Watanabe, “Coherent soft x-ray generation by the harmonics of an ultrahigh-power KrF laser,” Phys. Rev. A 43, 1669 (1991).
[1.43] P. B. Corkum, “Plasma perspective on strong-field multiphoton ionization,” Phys. Rev. Lett. 71, 1994 (1993).
[1.44] M. V. Ammosov, N. B. Delone, and V. P. Krainov, “Tunnel ionization of complex atoms and of atomic ions in an alternating electromagnetic field,” Sov. Phys. JETP 64, 1191 (1986).
[1.45] J. J. Macklin, J. D. Kmetec, and C. L. Gordon, “High-order harmonic generation using intense femtosecond pulses,” Phys. Rev. Lett. 70, 766 (1993).
[1.46] M. Nisoli, S. D. Silvestri, and O. Svelto, “Generation of high-energy 10-fs pulses by a new pulse compression technique,” Appl. Phys. Lett. 68, 2793 (1996).
[1.47] C. Spielmann, N. H. Burnett, S. Sartania, R. Koppitsch, M. Schnürer, C. Kan, M. Lenzner, P. Wobrauschek, and F. Krausz, “Generation of coherent X-rays in the water window using 5-femtosecond laser pulses,” Science 278, 661 (1997).
[1.48] E. J. Takahashi, T. Kanai, and K. Midorikawa, “High-order harmonic generation by an ultrafast infrared pulse,” Appl. Phys. B 100, 29 (2010).
[1.49] T. Popmintchev, M.-C. Chen, D. Popmintchev, P. Arpin, S. Brown, S. Alisauskas, G. Andiukaitis, T. Balciunas, O. D. Mücke, A. Pugzlys, A. Baltuska, B. Shim, S. E. Schrauth, A. Garta, C. Hernández-García, L. Plaja, A. Becker, A. Jaron-Becker, M. M. Murnane, and H. C. Kapteyn, “Bright coherent ultrahigh harmonics in the keV X-ray regime from mid-infrared femtosecond lasers,” Science 336, 1287 (2012).
[1.50] E. J. Takahashi, T. Kanai, K. L. Ishikawa, Y. Nabekawa, and K. Midorikawa, “Coherent water window x ray by phase-matched high-order harmonic generation in neutral media,” Phys. Rev. Lett. 101, 253901 (2008).
[1.51] V. Cardin, B. E. Schimdt, N. Thiré, S. Beaulieu, V. Wanie, M. Negro, C. Vozzi, V. Tosa, and F. Légaré, “Self-channelled high harmonic generation of water window soft x- rays,” J. Phys. B 51, 174004 (2018).
[1.52] J. Pupeikis, P.-A. Chevreuil, N. Bigler, L. Gallmann, C. R. Phillips, and U. Keller, “Water window soft x-ray source enabled by a 25 W few-cycle 2.2 µm OPCPA at 100 kHz,” Optica 7, 168 (2020).
[1.53] T. Popmintchev, M.-C. Chen, A. Bahabad, M. Gerrity, P. Sidorenko, O. Cohen, I. P. Christov, M. M. Murnane, and H. C. Kapteyn, “Phase matching of high harmonic generation in the soft and hard x-ray regions of the spectrum,” Proc. Natl. Acad. Sci. USA 106 10516 (2009).
[1.54] H. Xiong, H. Xu, Y. Fu, J. Yao, B. Zeng, W. Chu, Y. Cheng, Z. Xu, E. J. Takahashi, K. Midorikawa, X. Liu, and J. Chen, “Generation of a coherent x ray in the water window region at 1 kHz repetition rate using a mid-infrared pump source,” Opt. Lett. 34, 1747 (2009).
[1.55] M.-C. Chen, P. Arpin, T. Popmintchev, M. Gerrity, B. Zhang, M. Seaberg, D. Popmintchev, M. M. Murnane, and H. C. Kapteyn, “Bright, coherent, ultrafast soft x- ray harmonics spanning the water window from a tabletop light source,” Phys. Rev. Lett. 105, 173901 (2010).
[1.56] N. Ishii, K. Kaneshima, K. Kitano, T. Kanai, S. Watanabe, and J. Itatani, “Carrier- envelope phase-dependent high harmonic generation in the water window using few- cycle infrared pulses,” Nat. Commun. 5, 3331 (2014).
[1.57] S. L. Cousin, F. Silva, S. Teichmann, M. Hemmer, B. Buades, and J. Biegert, “High- flux table-top soft x-ray source driven by sub-2-cycle, CEP stable, 1.85-µm 1-kHz pulses for carbon K-edge spectroscopy,” Opt. Lett. 39, 5383 (2014).
[1.58] F. Silva, S. M. Teichmann, S. L. Cousin, M. Hemmer, and J. Biegert, “Spatiotemporal isolation of attosecond soft X-ray pulses in the water window,” Nat. Commun. 6, 6611 (2015).
[1.59] S. M. Teichmann, F. Silva, S. L. Cousin, M. Hemmer, and J. Biegert, “0.5-keV soft x- ray attosecond continua,” Nat. Commun. 7, 11493 (2016).
[1.60] G. J. Stein, P. D. Keathley, P. Krogen, H. Liang, J. P. Siqueira, C.-L. Chang, C.-J. Lai, K.-H. Hong, G. M. Laurent, and F. X. Kärtner, “Water-window soft x-ray high- harmonic generation up to the nitrogen K-edge driven by a kHz, 2.1 µm OPCPA source,” J. Phys. B 49, 155601 (2016).
[1.61] J. Li, X. Ren, Y. Yin, K. Zhao, A. Chew, Y. Cheng, E. Cunningham, Y. Wang, S. Hu, Y. Wu, M. Chini, and Z. Chang, “53-attosecond X-ray pulses reach the carbon K-edge,” Nat. Commun. 8, 186 (2017).
[1.62] A. S. Johnson, D. R. Austin, D. A. Wood, C. Brahms, A. Gregory, K. B. Holzner, S. Jarosch, E. W. Larsen, S. Parker, C. S. Strüber, P. Ye, W. John, G. Tisch, and J. P. Marangos, “High-flux soft x-ray harmonic generation from ionization-shaped few- cycle laser pulses,” Sci. Adv. 4, 3761 (2018).
[1.63] C. Schmidt, Y. Pertot, T. Balciunas, K. Zinchenko, M. Matthews, H. J. Wörner, and J.- P. Wolf, “High-order harmonic source spanning up to the oxygen K-edge based on filamentation pulse compression,” Opt. Express 26, 11834 (2018).
[1.64] C. Kleine, M. Ekimova, G. Goldsztejn, S. Raabe, C. Strüber, J. Ludwig, S. Yarlagadda, S. Eisebitt, M. J. J. Vrakking, T. Elsaesser, E. T. J. Nibbering, and A. Rouzée, “Soft x- ray absorption spectroscopy of aqueous solutions using a table-top femtosecond soft x-ray source,” J. Phys. Chem. Lett. 10, 52 (2019).
[1.65] J. Li, A. Chew, S. Hu, J. White, X. Ren, S. Han, Y. Yin, Y. Wang, Y. Wu, and Z. Chang, “Double optical gating for generating high flux isolated attosecond pulses in the soft X-ray regime,” Opt. Express 27, 30280 (2019).
[1.66] L. Barreau, A. D. Ross, S. Garg, P. M. Kraus, D. M. Neumark, and S. R. Leone, “Efficient table-top dual-wavelength beamline for ultrafast transient absorption spectroscopy in the soft X-ray region,” Sci. Rep. 10, 5773 (2020).
[1.67] M. Gebhardt, T. Heuermann, R. Klas, C. Liu, A. Kirsche, M. Lenski, Z. Wang, C. Gaida, J. E. Antonio-Lopez, A. Schülzgen, R. Amezcua-Correa, J. Rothhardt, and J. Limpert, “Bright, high repetition rate water window soft X-ray source enabled by nonlinear pulse self-compression in antiresonant hollow-core fibre,” Light: Sci. Appl. 10, 36 (2020).
[1.68] Y. Pertot, C. Schmidt, M. Matthews, A. Chauvet, M. Huppert, V. Svoboda, A. von Conta, A. Tehlar, D. Baykusheva, J.-P. Wolf, and H. J. Wörner, “Time resolved x-ray absorption spectroscopy with a water window high-harmonic source,” Science 355, 264 (2017).
[1.69] A. R. Attar, A. Bhattacherjee, C. D. Pemmaraju, K. Schnorr, K. D. Closser, D. Prendergast, and S. R. Leone, “Femtosecond x-ray spectroscopy of an electrocyclic ring-opening reaction,” Science 356, 54 (2017).
[1.70] A. D. Smith, T. Balciunas, Y.-P. Chang, C. Schmidt, K. Zinchenko, F. B. Nunes, E. Rossi, V. Svoboda, Z. Yin, J.-P. Wolf, and H. J. Wörner, “Femtosecond soft x-ray absorption spectroscopy of liquids with a water-window high-harmonic source,” J. Phys. Chem. Lett. 11, 1981 (2020).
[1.71] Y. Wang, T. Guo, J. Li, J. Zhao, Y. Yin, X. Ren, J. Li, Y. Wu, M. Weidman, Z. Chang, M. F. Jager, C. J. Kaplan, R. Geneaux, C. Ott, D. M. Neumark, and S. R. Leone, “Enhanced high-order harmonic generation driven by a wavefront corrected high- energy laser,” J. Phys. B 51, 134005 (2018).
[1.72] M. Nisoli, S. De Silvestri, V. Magni, O. Svelto, R. Danielius, A. Piskarskas, G. Valiulis, and A. Varanavicius, “Highly efficient parametric conversion of femtosecond Ti:sapphire laser pulses at 1 kHz,” Opt. Lett. 19, 1973 (1994).
[1.73] G. Cerullo and S. De Silvestri, “Ultrafast optical parametric amplifiers,” Rev. Sci. Instrum. 74, 1 (2003).
[1.74] I. N. Ross, P. Matousek, G. H. C. New, and K. Osvay, “Analysis and optimization of optical parametric chirped pulse amplification,” J. Opt. Soc. Am. B 19, 2945 (2002).
[1.75] O. D. Mücke, S. Ališauskas, A. J. Verhoef, A. Pugžlys, A. Baltuška, V. Smilgevičius, J. Pocius, L. Giniūnas, R. Danielius, and N. Forget, “Self-compression of millijoule 1.5 µm pulses,” Opt. Lett. 34, 2498 (2009).
[1.76] A. Vaupel, N. Bodnar, B. Webb, L. Shah, and M. C. Richardson, “Concepts, performance review, and prospects of table-top, few-cycle optical parametric chirped- pulse amplification,” Opt. Eng. 53, 051507 (2013).
[1.77] Q. Zhang, E. J. Takahashi, O. D. Mücke, P. Lu, and K. Midorikawa, “Dual-chirped optical parametric amplification for generating few hundred mJ infrared pulses,” Opt. Express 19, 7190 (2011).
[1.78] A. S. Johnson, D. Wood, D. R. Austin, C. Brahms, A. Gregory, K. B. Holzner, S. Jarosch, E. W. Larsen, S. Parker, C. Strüber, P. Ye, J. W. G. Tisch, and J. P. Marangos, “Apparatus for soft x-ray table-top high harmonic generation,” Rev. Sci. Instrum. 89, 083110 (2018).
[1.79] J. Tate, T. Auguste, H. G. Muller, P. Salières, P. Agostini, and L. F. DiMauro, “Scaling of wave-packet dynamics in an intense midinfrared field,” Phys. Rev. Lett. 98, 013901 (2007).
[1.80] A. D. Shiner, C. Trallero-Herrero, N. Kajumba, H.-C. Bandulet, D. Comtois, F. Légaré, M. Giguère, J-C. Kieffer, P. B. Corkum, and D. M. Villeneuve, “Wavelength scaling of high harmonic generation efficiency,” Phys. Rev. Lett. 103, 073902 (2009).
[1.81] A. Rundquist, C. G. Durfee III, Z. Chang, C. Herne, S. Backus, M. M. Murnane, and H. C. Kapteyn, “Phase-Matched Generation of Coherent Soft X-rays,” Science 280, 1412 (1998).
[1.82] D. Strickland and G. Mourou, “Compression of amplified chirped optical pulses,” Opt. Commun. 56, 219 (1985).
[1.83] S. Backus, C. G. Durfee, M. M. Murnane, and H. C. Kapteyn, “High power ultrafast lasers,” Rev. Sci. Instrum. 69, 1207 (1998).
[1.84] E. Takahashi, Y. Nabekawa, and K. Midorikawa, “Generation of 10-µJ coherent extreme-ultraviolet light by use of high-order harmonics,” Opt. Lett. 27, 1920 (2002).
[1.85] W. Boutu, T. Auguste, J. P. Caumes, H. Merdji, and B. Carré, “Scaling of the generation of high-order harmonics in large gas media with focal length,” Phys. Rev. A 84, 053819 (2011).
[1.86] C. M. Heyl, J. Güdde, A. L’Huillier, and U. Höfer, “High-order harmonic generation with µJ laser pulses at high repetition rates,” J. Phys. B 45, 074020 (2012).
[1.87] P. Rudawski, C. M. Heyl, F. Brizuela, J. Schwenke, A. Persson, E. Mansten, R. Rakowski, L. Rading, F. Campi, B. Kim, P. Johnsson, and A. L’Huillier, “A highflux high-order harmonic source,” Rev. Sci. Instrum. 84, 073103 (2013).
[1.88] C. M. Heyl, C. L. Arnold, A. Couairon, and A. L’Huillier, “Introduction to macroscopic power scaling principles for high-order harmonic generation,” J. Phys. B 50, 013001 (2016).
[1.89] A. Nayak, I. Orfanos, I. Makos, M. Dumergue, S. Kühn, E. Skantzakis, B. Bodi, K. Varju, C. Kalpouzos, H. I. B. Banks, A. Emmanouilidou, D. Charalambidis, and P. Tzallas, “Multiple ionization of argon via multi-XUV-photon absorption induced by 20-GW high-order harmonic laser pulses,” Phys. Rev. A 98, 023426 (2018).
[1.90] K. Kovács, B. Major, E. Balogh, C. P. Korös, P. Rudawski, C. M. Heyl, P. Johnsson, C. L. Arnold, A. L’Huillier, V. Tosa, and K. Varjú, “Multi-parameter optimization of a loose focusing high flux high-harmonic beamline,” J. Phys. B 52, 055402 (2019).
[1.91] J. Rothhardt, M. Krebs, S. Hädrich, S. Demmler, J. Limpert, and A. Tünnermann, “Absorption-limited and phase-matched high harmonic generation in the tight focusing regime,” New J. Phys. 16, 033022 (2014).
[1.92] D. Rupp, N. Monserud, L. Bruno, M. Sauppe, J. Zimmermann, Y. Ovcharenko, T. Möller, F. Frassetto, L. Poletto, A. Trabattoni, F. Calegari, M. Nisoli, K. Sander, C. Peltz, M. J. Vrakking, T. Fennel, and A. Rouzée, “Coherent diffractive imaging of single helium nanodroplets with a high harmonic generation source,” Nat. Commun. 8, 493 (2017).
[1.93] D. D. Hickstein, F. J. Dollar, P. Grychtol, J. L. Ellis, R. Knut, C. Hernández-García, D. Zusin, C. Gentry, J. M. Shaw, T. Fan, K. M. Dorney, A. Becker, A. Jaroń-Becker, H. C. Kapteyn, M. M. Murnane, and C. G. Durfee, “Non-collinear generation of angularly isolated circularly polarized high harmonics,” Nat. Photon. 9, 743 (2015).
[1.94] P.-C. Huang, C. Hernández-García, J.-T. Huang, P.-Y. Huang, C.-H. Lu, L. Rego, D. D. Hickstein, J. L. Ellis, A. Jaron-Becker, A. Becker, S.-Da Yang, C. G. Durfee, L. Plaja, H. C. Kapteyn, M. M. Murnane, A. H. Kung, and M.-C. Chen, “Polarization control of isolated high-harmonic pulses,” Nat. Photon. 12, 349 (2018).
[1.95] W. Komatsubara, F. Kong, C. Zhang, and P. B. Corkum, “High harmonics diffraction caused by an ellipticity grating,” J. Phys. B 53, 094002 (2020).
[1.96] O. Kfir, P. Grychtol, E. Turgut, R. Knut, D. Zusin, D. Popmintchev, T. Popmintchev, H. Nembach, J. M. Shaw, A. Fleischer, H. Kapteyn, M. Murnane and O. Cohen, “Generation of bright phase-matched circularly-polarized extreme ultraviolet high harmonics,” Nat. Photon. 9, 99 (2015).
第二章 参考文献
[2.1] P. B. Corkum, “Plasma perspective on strong-field multiphoton ionization,” Phys. Rev. Lett. 71, 1994 (1993).
[2.2] F. Lureau, G. Matras, O. Chalus, C. Derycke, T. Morbieu, C. Radier, O. Casagrande, S. Laux, S. Ricaud, G. Rey, A. Pellegrina, C. Richard, L. Boudjemaa, C. S.-Boisson, A. Baleanu, R. Banici, A. Gradinariu, C. Caldararu, B. De Boisdeffre, P. Ghenuche, A. Naziru, G. Kolliopoulos, L. Neagu, R. Dabu, I. Dancus, and D. Ursescu, “High-energy hybrid femtosecond laser system demonstrating 2 × 10 PW capability,” High Power Laser Sci. Eng. 8, 43 (2020).
[2.3] A. M. Perelomov, V. S. Popov, and M. V. Terentev, “Ionization of atoms in an alternating electric field,” Sov. Phys. JETP 23, 924 (1966).
[2.4] M. V. Ammosov, N. B. Delone, and V. P. Krainov, “Tunnel ionization of complex atoms and of atomic ions in an alternating electromagnetic field,” Sov. Phys. JETP 64, 1191 (1986).
[2.5] Z. Chang, Fundamentals of Attosecond Optics (CRC Press, 2011).
[2.6] M. Lewenstein, P. Balcou, M. Y. Ivanov, A. L’Huillier, and P. B. Corkum, “Theory of high-harmonic generation by low-frequency laser fields,” Phys. Rev. A 49, 2117 (1994).
[2.7] D. B. Milošević, W. Becker, and R. Kopold, “Generation of circularly polarized high- order harmonics by two-color coplanar field mixing,” Phys. Rev. A 61, 063403 (2000).
[2.8] O. Neufeld, E. Bordo, A. Fleischer, and O. Cohen, “High harmonic generation with fully tunable polarization by train of linearly polarized pulses,” New J. Phys. 19, 023051 (2017).
[2.9] O. Neufeld, D. Podolsky, and O. Cohen, “Floquet group theory and its application to selection rules in harmonic generation,” Nat. Commun. 10, 405 (2019).
[2.10] P. Salières, B. Carré, L. Le Déroff, F. Grasbon, G. G. Paulus, H. Walther, R. Kopold, W. Becker, D. B. Milošević, A. Sanpera, and M. Lewenstein, “Feynman's path-integral approach for intense-laser-atom interactions,” Science 292, 902 (2001).
[2.11] D. B. Milošević, “Circularly polarized high harmonics generated by a bicircular field from inert atomic gases in the p state: A tool for exploring chirality-sensitive processes,” Phys. Rev. A 92, 043827 (2015).
[2.12] D. B. Milošević and W. Becker, “Improved strong-field approximation and quantum- orbit theory: Application to ionization by a bicircular laser field,” Phys. Rev. A 93, 063418 (2016).
[2.13] J. Heslar, D. A. Telnov, and S.-I Chu, “Conditions for perfect circular polarization of high-order harmonics driven by bichromatic counter-rotating laser fields,” Phys. Rev. A 99, 023419 (2019).
[2.14] D. B. Milošević and W. Becker, “High-order harmonic generation by bi-elliptical orthogonally polarized two-color fields,” Phys. Rev. A 102, 023107 (2020).
[2.15] Y. Su, K. Fang, and J. Zhang, “Shortcut to study angular momentum transfer of harmonic generation in intense laser fields,” Opt. Express 29, 22679 (2021).
[2.16] E. Pisanty, S. Sukiasyan, and M. Ivanov, “Spin conservation in high-order-harmonic generation using bicircular fields,” Phys. Rev. A 90, 043829 (2014).
[2.17] T. Fan, P. Grychtol, R. Knut, C. Hernández-García, D. D. Hickstein, D. Zusin, C. Gentry, F. J. Dollar, C. A. Mancuso, C. W. Hogle, O. Kfir, D. Legut, K. Carva, J. L. Ellis, K. M. Dorney, C. Chen, O. G. Shpyrko, E. E. Fullerton, O. Cohen, P. M. Oppeneer, D. B. Milošević, A. Becker, A. A. Jaroń-Becker, T. Popmintchev, M. M. Murnane, and H. C. Kapteyn, “Bright circularly polarized soft X-ray high harmonics for X-ray magnetic circular dichroism,” Proc. Natl. Acad. Sci. USA 112, 14206 (2015).
[2.18] C. R. Mansfield and E. R. Peck, “Dispersion of Helium,” J. Opt. Soc. Am. 59, 199 (1969).
[2.19] A. Börzsönyi, Z. Heiner, M. P. Kalashnikov, A. P. Kovács, and K. Osvay, “Dispersion measurement of inert gases and gas mixtures at 800 nm,” Appl. Opt. 47, 4856 (2008).
[2.20] E. R. Peck and D. J. Fisher, “Dispersion of Argon,” J. Opt. Soc. Am. 54, 1362 (1964).
[2.21] B. L. Henke, E. M. Gullikson, and J. C. Davis, “X-ray interactions: photoabsorption, scattering, transmission, and reflection at E = 50-30,000 eV, Z = 1-92,” At. Data Nucl. Data Tables 54, 181 (1993).
[2.22] M.-C. Chen, P. Arpin, T. Popmintchev, M. Gerrity, B. Zhang, M. Seaberg, D. Popmintchev, M. M. Murnane, and H. C. Kapteyn, “Bright, coherent, ultrafast soft x- ray harmonics spanning the water window from a tabletop light source,” Phys. Rev. Lett. 105, 173901 (2010).
[2.23] E. Constant, D. Garzella, P. Breger, M. Mevel, C. Dorrer, C. L. Blanc, F. Salin, and P. Agostini, “Optimizing high harmonic generation in absorbing gases: model and experiment,” Phys. Rev. Lett. 82, 1668 (1999).
[2.24] Y. Wang, T. Guo, J. Li, J. Zhao, Y. Yin, X. Ren, J. Li, Y. Wu, M. Weidman, Z. Chang, M. F. Jager, C. J. Kaplan, R. Geneaux, C. Ott, D. M. Neumark, and S. R. Leone, “Enhanced high-order harmonic generation driven by a wavefront corrected high- energy laser,” J. Phys. B 51, 134005 (2018).
[2.25] E. Takahashi, Y. Nabekawa, and K. Midorikawa, “Generation of 10-µJ coherent extreme-ultraviolet light by use of high-order harmonics,” Opt. Lett. 27, 1920 (2002).
[2.26] W. Boutu, T. Auguste, J. P. Caumes, H. Merdji, and B. Carré, “Scaling of the generation of high-order harmonics in large gas media with focal length,” Phys. Rev. A 84, 053819 (2011).
[2.27] C. M. Heyl, J. Güdde, A. L’Huillier, and U. Höfer, “High-order harmonic generation with µJ laser pulses at high repetition rates,” J. Phys. B 45, 074020 (2012).
[2.28] P. Rudawski, C. M. Heyl, F. Brizuela, J. Schwenke, A. Persson, E. Mansten, R. Rakowski, L. Rading, F. Campi, B. Kim, P. Johnsson, and A. L’Huillier, “A highflux high-order harmonic source,” Rev. Sci. Instrum. 84, 073103 (2013).
[2.29] C. M. Heyl, C. L. Arnold, A. Couairon, and A. L’Huillier, “Introduction to macroscopic power scaling principles for high-order harmonic generation,” J. Phys. B 50, 013001 (2016).
[2.30] A. Nayak, I. Orfanos, I. Makos, M. Dumergue, S. Kühn, E. Skantzakis, B. Bodi, K. Varju, C. Kalpouzos, H. I. B. Banks, A. Emmanouilidou, D. Charalambidis, and P. Tzallas, “Multiple ionization of argon via multi-XUV-photon absorption induced by 20-GW high-order harmonic laser pulses,” Phys. Rev. A 98, 023426 (2018).
[2.31] K. Kovács, B. Major, E. Balogh, C. P. Korös, P. Rudawski, C. M. Heyl, P. Johnsson, C. L. Arnold, A. L’Huillier, V. Tosa, and K. Varjú, “Multi-parameter optimization of a loose focusing high flux high-harmonic beamline,” J. Phys. B 52, 055402 (2019).
[2.32] J. Rothhardt, M. Krebs, S. Hädrich, S. Demmler, J. Limpert, and A. Tünnermann, “Absorption-limited and phase-matched high harmonic generation in the tight focusing regime,” New J. Phys. 16, 033022 (2014).
[2.33] C.-J. Lai and F. X. Kärtner, “The influence of plasma defocusing in high harmonic generation,” Opt. Express 19, 22377 (2011).
第三章 参考文献
[3.1] L. Xu, K. Nishimura, A. Suda, K. Midorikawa, Y. Fu, and E. J. Takahashi, “Optimization of a multi-TW few-cycle 1.7-μm source based on type-I BBO dual- chirped optical parametric amplification,” Opt. Express 28, 15138 (2020).
[3.2] D. Strickland and G. Mourou, “Compression of amplified chirped optical pulses,” Opt. Commun. 56, 219 (1985).
[3.3] N. Thiré, S. Beaulieu, V. Cardin, A. Laramée, V. Wanie, B. E. Schmidt, and F. Légaré, “10 mJ 5-cycle pulses at 1.8 μm through optical parametric amplification,” Appl. Phys. Lett. 106, 091110 (2015).
[3.4] I. N. Ross, P. Matousek, G. H. C. New, and K. Osvay, “Analysis and optimization of optical parametric chirped pulse amplification,” J. Opt. Soc. Am. B 19, 2945 (2002).
[3.5] J. V. Rudd, R. J. Law, T. S. Luk, and S. M. Cameron, “High-power optical parametric chirped-pulse amplifier system with a 1.55 µm signal and a 1.064 µm pump,” Opt. Lett. 30, 1974 (2005).
[3.6] Q. Zhang, E. J. Takahashi, O. D. Mücke, P. Lu, and K. Midorikawa, “Dual-chirped optical parametric amplification for generating few hundred mJ infrared pulses,” Opt. Express 19, 7190 (2011).
[3.7] Y. Fu, K. Midorikawa, and E. J. Takahashi, “Towards a petawatt-class few- cycleinfrared laser system via dual-chirped optical parametric amplification,” Sci. Rep. 8, 7692 (2018).
[3.8] E. B. Treacy, “Optical pulse compression with diffraction gratings”, IEEE J. Quantum Electron. 5, 454 (1969).
[3.9] R. L. Fork, O. E. Martinez, and J. P. Gordon, “Negative dispersion using pairs of prisms,” Opt. Lett. 9, 150 (1984).
[3.10] R. Trebino, K. W. DeLong, D. N. Fittinghoff, J. N. Sweetser, M. A. Krumbugel, B. A. Richman, and D. J. Kane, “Measuring ultrashort laser pulses in the time-frequency domain using frequency-resolved optical gating,” Rev. Sci. Instrum. 68, 3277 (1997).
[3.11] Y. Fu, B. Xue, K. Midorikawa, and E. J. Takahashi, “TW-scale mid-infrared pulses near 3.3 μm directly generated by dual-chirped optical parametric amplification,” Appl. Phys. Lett. 112, 241105 (2018).
[3.12] S. Semushin and V. Malka, “High density gas jet nozzle design for laser target production,” Rev. Sci. Instrum. 72, 2961 (2001).
[3.13] V. E. Leshchenko, B. K. Talbert, Y. H. Lai, S. Li, Y. Tang, S. J. Hageman, G. Smith, P. Agostini, L. F. DiMauro, and C. I. Blaga, “High-power few-cycle Cr:ZnSe mid- infrared source for attosecond soft x-ray physics,” Optica 7, 981 (2020).
[3.14] H. Xiong, H. Xu, Y. Fu, J. Yao, B. Zeng, W. Chu, Y. Cheng, Z. Xu, E. J. Takahashi, K. Midorikawa, X. Liu, and J. Chen, “Generation of a coherent x ray in the water window region at 1 kHz repetition rate using a mid-infrared pump source,” Opt. Lett. 34, 1747 (2009).
[3.15] S. M. Teichmann, F. Silva, S. L. Cousin, M. Hemmer, and J. Biegert, “0.5-keV soft x- ray attosecond continua,” Nat. Commun. 7, 11493 (2016).
[3.16] C. Schmidt, Y. Pertot, T. Balciunas, K. Zinchenko, M. Matthews, H. J. Wörner, and J.- P. Wolf, “High-order harmonic source spanning up to the oxygen K-edge based on filamentation pulse compression,” Opt. Express 26, 11834 (2018).
[3.17] A. S. Johnson, D. Wood, D. R. Austin, C. Brahms, A. Gregory, K. B. Holzner, S. Jarosch, E. W. Larsen, S. Parker, C. Strüber, P. Ye, J. W. G. Tisch, and J. P. Marangos, “Apparatus for soft x-ray table-top high harmonic generation,” Rev. Sci. Instrum. 89, 083110 (2018).
[3.18] N. Ishii, K. Kaneshima, K. Kitano, T. Kanai, S. Watanabe, and J. Itatani, “Carrier- envelope phase-dependent high harmonic generation in the water window using few- cycle infrared pulses,” Nat. Commun. 5, 3331 (2014).
[3.19] N. Saito, Ultrafast transient absorption spectroscopy using attosecond soft X-ray pulses in the water window (PhD thesis, The University of Tokyo, 2019).
[3.20] C. Schmidt, Y. Pertot, T. Balciunas, K. Zinchenko, M. Matthews, H. J. Wörner, and J.- P. Wolf, “High-order harmonic source spanning up to the oxygen K-edge based on filamentation pulse compression,” Opt. Express 26, 11834 (2018).
[3.21] J. Li, X. Ren, Y. Yin, K. Zhao, A. Chew, Y. Cheng, E. Cunningham, Y. Wang, S. Hu, Y. Wu, M. Chini, and Z. Chang, “53-attosecond X-ray pulses reach the carbon K-edge,” Nat. Commun. 8, 186 (2017).
[3.22] G. J. Stein, P. D. Keathley, P. Krogen, H. Liang, J. P. Siqueira, C.-L. Chang, C.-J. Lai, K.-H. Hong, G. M. Laurent, and F. X. Kärtner, “Water-window soft x-ray high- harmonic generation up to the nitrogen K-edge driven by a kHz, 2.1 µm OPCPA source,” J. Phys. B 49, 155601 (2016).
[3.23] V. Cardin, B. E. Schimdt, N. Thiré, S. Beaulieu, V. Wanie, M. Negro, C. Vozzi, V. Tosa, and F. Légaré, “Self-channelled high harmonic generation of water window soft x- rays,” J. Phys. B 51, 174004 (2018).
[3.24] E. Takahashi, Y. Nabekawa, and K. Midorikawa, “Generation of 10-µJ coherent extreme-ultraviolet light by use of high-order harmonics,” Opt. Lett. 27, 1920 (2002).
[3.25] Opto Diode Corporation, “Data sheet,” https://optodiode.com/pdf/AXUV100GDS. pdf.
[3.26] N. Nakano, H. Kuroda, T. Kita, and T. Harada, “Development of a flat-field grazing- incidence XUV spectrometer and its application in picosecond XUV spectroscopy,” Appl. Opt. 23, 2386 (1984).
[3.27] National Institute of Standards and Technology, “NIST Atomic Spectra Database Lines Form,” https://physics.nist.gov/PhysRefData/ASD/lines_form.html.
第四章 参考文献
[4.1] R. H. Garvey, C. H. Jackman, and A. E. S. Green, “Independent-particle-model potentials for atoms and ions with 36 < Z < 54 and a modified Thomas-Fermi atomic energy formula,” Phys. Rev. A 12, 1144 (1975).
[4.2] S. Minemoto, T. Umegaki, Y. Oguchi, T. Morishita, A.-T. Le, S. Watanabe, and H. Sakai, “Retrieving photorecombination cross sections of atoms from high-order harmonic spectra,” Phys. Rev. A 78, 061402(R) (2008).
[4.3] A. D. Shiner, B. E. Schmidt, C. Trallero-Herrero, H. J. Wörner, S. Patchkovskii, P. B. Corkum, J-C. Kieffer, F. Légaré, and D. M. Villeneuve, “Probing collective multi- electron dynamics in xenon with high-harmonic spectroscopy,” Nat. Phys. 7, 464 (2011).
[4.4] A. S. Johnson, D. R. Austin, D. A. Wood, C. Brahms, A. Gregory, K. B. Holzner, S. Jarosch, E. W. Larsen, S. Parker, C. S. Strüber, P. Ye, W. John, G. Tisch, and J. P. Marangos, “High-flux soft x-ray harmonic generation from ionization-shaped few- cycle laser pulses,” Sci. Adv. 4, 3761 (2018).
[4.5] V. Cardin, B. E. Schimdt, N. Thiré, S. Beaulieu, V. Wanie, M. Negro, C. Vozzi, V. Tosa, and F. Légaré, “Self-channelled high harmonic generation of water window soft x- rays,” J. Phys. B 51, 174004 (2018).
[4.6] S. P. Le Blanc, R. Sauerbrey, S. C. Rae, and K. Burnett, “Spectral blue shifting of a femtosecond laser pulse propagating through a high-pressure gas,” J. Opt. Soc. Am. B 10, 1801 (1993).
[4.7] A. M. Perelomov, V. S. Popov, and M. V. Terentev, “Ionization of atoms in an alternating electric field,” Sov. Phys. JETP 23, 924 (1966).
[4.8] C.-J. Lai and F. X. Kärtner, “The influence of plasma defocusing in high harmonic generation,” Opt. Express 19, 22377 (2011).
[4.9] E. J. Takahashi, T. Kanai, and K. Midorikawa, “High-order harmonic generation by an ultrafast infrared pulse,” Appl. Phys. B 100, 29 (2010).
[4.10] E. J. Takahashi, T. Kanai, K. L. Ishikawa, Y. Nabekawa, and K. Midorikawa, “Coherent water window x ray by phase-matched high-order harmonic generation in neutral media,” Phys. Rev. Lett. 101, 253901 (2008).
[4.11] J. Pupeikis, P.-A. Chevreuil, N. Bigler, L. Gallmann, C. R. Phillips, and U. Keller, “Water window soft x-ray source enabled by a 25 W few-cycle 2.2 µm OPCPA at 100 kHz,” Optica 7, 168 (2020).
[4.12] T. Popmintchev, M.-C. Chen, A. Bahabad, M. Gerrity, P. Sidorenko, O. Cohen, I. P. Christov, M. M. Murnane, and H. C. Kapteyn, “Phase matching of high harmonic generation in the soft and hard x-ray regions of the spectrum,” Proc. Natl. Acad. Sci. USA 106 10516 (2009).
[4.13] H. Xiong, H. Xu, Y. Fu, J. Yao, B. Zeng, W. Chu, Y. Cheng, Z. Xu, E. J. Takahashi, K. Midorikawa, X. Liu, and J. Chen, “Generation of a coherent x ray in the water window region at 1 kHz repetition rate using a mid-infrared pump source,” Opt. Lett. 34, 1747 (2009).
[4.14] M.-C. Chen, P. Arpin, T. Popmintchev, M. Gerrity, B. Zhang, M. Seaberg, D. Popmintchev, M. M. Murnane, and H. C. Kapteyn, “Bright, coherent, ultrafast soft x- ray harmonics spanning the water window from a tabletop light source,” Phys. Rev. Lett. 105, 173901 (2010).
[4.15] N. Ishii, K. Kaneshima, K. Kitano, T. Kanai, S. Watanabe, and J. Itatani, “Carrier- envelope phase-dependent high harmonic generation in the water window using few- cycle infrared pulses,” Nat. Commun. 5, 3331 (2014).
[4.16] S. L. Cousin, F. Silva, S. Teichmann, M. Hemmer, B. Buades, and J. Biegert, “High- flux table-top soft x-ray source driven by sub-2-cycle, CEP stable, 1.85-µm 1-kHz pulses for carbon K-edge spectroscopy,” Opt. Lett. 39, 5383 (2014).
[4.17] F. Silva, S. M. Teichmann, S. L. Cousin, M. Hemmer, and J. Biegert, “Spatiotemporal isolation of attosecond soft X-ray pulses in the water window,” Nat. Commun. 6, 6611 (2015).
[4.18] S. M. Teichmann, F. Silva, S. L. Cousin, M. Hemmer, and J. Biegert, “0.5-keV soft x- ray attosecond continua,” Nat. Commun. 7, 11493 (2016).
[4.19] G. J. Stein, P. D. Keathley, P. Krogen, H. Liang, J. P. Siqueira, C.-L. Chang, C.-J. Lai, K.-H. Hong, G. M. Laurent, and F. X. Kärtner, “Water-window soft x-ray high- harmonic generation up to the nitrogen K-edge driven by a kHz, 2.1 µm OPCPA source,” J. Phys. B 49, 155601 (2016).
[4.20] J. Li, X. Ren, Y. Yin, K. Zhao, A. Chew, Y. Cheng, E. Cunningham, Y. Wang, S. Hu, Y. Wu, M. Chini, and Z. Chang, “53-attosecond X-ray pulses reach the carbon K-edge,” Nat. Commun. 8, 186 (2017).
[4.21] C. Schmidt, Y. Pertot, T. Balciunas, K. Zinchenko, M. Matthews, H. J. Wörner, and J.- P. Wolf, “High-order harmonic source spanning up to the oxygen K-edge based on filamentation pulse compression,” Opt. Express 26, 11834 (2018).
[4.22] C. Kleine, M. Ekimova, G. Goldsztejn, S. Raabe, C. Strüber, J. Ludwig, S. Yarlagadda, S. Eisebitt, M. J. J. Vrakking, T. Elsaesser, E. T. J. Nibbering, and A. Rouzée, “Soft x- ray absorption spectroscopy of aqueous solutions using a table-top femtosecond soft x-ray source,” J. Phys. Chem. Lett. 10, 52 (2019).
[4.23] L. Barreau, A. D. Ross, S. Garg, P. M. Kraus, D. M. Neumark, and S. R. Leone, “Efficient table-top dual-wavelength beamline for ultrafast transient absorption spectroscopy in the soft X-ray region,” Sci. Rep. 10, 5773 (2020).
[4.24] M. Gebhardt, T. Heuermann, R. Klas, C. Liu, A. Kirsche, M. Lenski, Z. Wang, C. Gaida, J. E. Antonio-Lopez, A. Schülzgen, R. Amezcua-Correa, J. Rothhardt, and J. Limpert, “Bright, high repetition rate water window soft X-ray source enabled by nonlinear pulse self-compression in antiresonant hollow-core fibre,” Light: Sci. Appl. 10, 36 (2020).
第五章 参考文献
[5.1] B. Xue, Y. Tamaru, Y. Fu, H. Yuan, P. Lan, O. D. Mücke, A. Suda, K. Midorikawa, and E. J. Takahashi, “Fully stabilized multi-TW optical waveform synthesizer: Toward gigawatt isolated attosecond pulses,” Sci. Adv. 6, 2802 (2020).
[5.2] S. Minemoto, T. Umegaki, Y. Oguchi, T. Morishita, A.-T. Le, S. Watanabe, and H. Sakai, “Retrieving photorecombination cross sections of atoms from high-order harmonic spectra,” Phys. Rev. A 78, 061402(R) (2008).
[5.3] H. Mashiko, M. J. Bell, A. R. Beck, M. J. Abel, P. M. Nagel, C. P. Steiner, J. Robinson, D. M. Neumark, and S. R. Leone, "Tunable frequency-controlled isolated attosecond pulses characterized by either 750 nm or 400 nm wavelength streak fields," Opt. Express 18, 25887 (2010).
[5.4] E. J. Takahashi, P. Lan, O. D. Mücke, Y. Nabekawa, and K. Midorikawa, “Attosecond nonlinear optics using gigawatt-scale isolated attosecond pulses,” Nat. Commun. 4, 2691 (2013).
[5.5] J. Li, Andrew Chew, S. Hu, J. White, X. Ren, S. Han, Y. Yin, Y. Wang, Y. Wu, and Z. Chang, “Double optical gating for generating high flux isolated attosecond pulses in the soft X-ray regime,” Opt. Express 27, 30280 (2019).
[5.6] T. Fan, P. Grychtol, R. Knut, C. Hernández-García, D. D. Hickstein, D. Zusin, C. Gentry, F. J. Dollar, C. A. Mancuso, C. W. Hogle, O. Kfir, D. Legut, K. Carva, J. L. Ellis, K. M. Dorney, C. Chen, O. G. Shpyrko, E. E. Fullerton, O. Cohen, P. M. Oppeneer, D. B. Milošević, A. Becker, A. A. Jaroń-Becker, T. Popmintchev, M. M. Murnane, and H. C. Kapteyn, “Bright circularly polarized soft X-ray high harmonics for X-ray magnetic circular dichroism,” Proc. Natl. Acad. Sci. USA 112, 14206 (2015).
[5.7] O. Kfir, P. Grychtol, E. Turgut, R. Knut, D. Zusin, D. Popmintchev, T. Popmintchev, H. Nembach, J. M. Shaw, A. Fleischer, H. Kapteyn, M. Murnane and O. Cohen, “Generation of bright phase-matched circularly-polarized extreme ultraviolet high harmonics,” Nat. Photon. 9, 99 (2015).
[5.8] The Center for X-ray Optics, “X-Ray Interactions with Matter,” https://henke.lbl. gov/optical_constants/.
[5.9] E. J. Takahashi, Y. Nabekawa, and K. Midorikawa, “Low-divergence coherent soft x- ray source at 13 nm by high-order harmonics,” Appl. Phys. Lett. 84, 4 (2004).
[5.10] E.J. Takahashi, T. Kanai, and K. Midorikawa, “High-order harmonic generation by an ultrafast infrared pulse,” Appl. Phys. B 100, 29 (2010).
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