Abstract

ELI-ALPS, one of the three pillars of the Extreme Light Infrastructure (ELI) project, will be in a unique position to offer dedicated experimental platforms for ultrashort time-resolved investigations of strongly excited dynamical systems. The state-of-the-art surface plasma attosource (SPA) beamlines at ELI-ALPS are being designed and developed to enable new directions in plasma-based attoscience research. The SPA beamlines will be driven by ultrashort, high peak power, high repetition rate lasers based on the latest technology and are aimed to develop previously unavailable attoscience experimental platforms employing surface high-harmonic generation process. This endeavor involves research and development challenges and careful considerations. Here we discuss the physics of plasma attosources and their characteristics under such extreme conditions and the beamline functionalities that would facilitate these objectives. Finally, we delineate the initial research possibilities with these sophisticated instruments.

© 2018 Optical Society of America

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2018 (1)

A. Leblanc and F. Quéré, “In situ ptychographic measurements of high-order harmonic sources from plasma mirrors: a theoretical and numerical study,” Phys. Plasmas 25, 013112 (2018).
[Crossref]

2017 (5)

A. Leblanc, S. Monchocé, H. Vincenti, S. Kahaly, J.-L. Vay, and F. Quéré, “Spatial properties of high-order harmonic beams from plasma mirrors: a ptychographic study,” Phys. Rev. Lett. 119, 155001 (2017).
[Crossref]

S. Kühn, M. Dumergue, S. Kahaly, S. Mondal, M. Füle, T. Csizmadia, B. Farkas, B. Major, Z. Várallyay, F. Calegari, M. Devetta, F. Frassetto, E. Mänsson, L. Poletto, S. Stagira, C. Vozzi, M. Nisoli, P. Rudawski, S. Maclot, F. Campi, H. Wikmark, C. L. Arnold, C. M. Heyl, P. Johnsson, A. L’Huillier, R. Lopez-Martens, S. Haessler, M. Bocoum, F. Boehle, A. Vernier, G. Iaquaniello, E. Skantzakis, N. Papadakis, C. Kalpouzos, P. Tzallas, F. Lépine, D. Charalambidis, K. Varjú, K. Osvay, and G. Sansone, “The ELI-ALPS facility: the next generation of attosecond sources,” J. Phys. B 50, 132002 (2017).
[Crossref]

S. Chatziathanasiou, S. Kahaly, E. Skantzakis, G. Sansone, R. Lopez-Martens, S. Haessler, K. Varju, G. Tsakiris, D. Charalambidis, and P. Tzallas, “Generation of attosecond light pulses from gas and solid state media,” Photonics 4, 26 (2017).
[Crossref]

R. Budriūnas, T. Stanislauskas, J. Adamonis, A. Aleknavičius, G. Veitas, D. Gadonas, S. Balickas, A. Michailovas, and A. Varanavičius, “53  W average power CEP-stabilized OPCPA system delivering 55  TW few cycle pulses at 1  kHz repetition rate,” Opt. Express 25, 5797–5806 (2017).
[Crossref]

S. Mondal, H. A. Hafez, X. Ropagnol, and T. Ozaki, “MV/cm terahertz pulses from relativistic laser-plasma interaction characterized by nonlinear terahertz absorption bleaching in n-doped InGaAs,” Opt. Express 25, 17511–17523 (2017).
[Crossref]

2016 (9)

Z.-Y. Chen and A. Pukhov, “Bright high-order harmonic generation with controllable polarization from a relativistic plasma mirror,” Nat. Commun. 7, 12515 (2016).
[Crossref]

G. Pariente, V. Gallet, A. Borot, O. Gobert, and F. Quéré, “Space-time characterization of ultra-intense femtosecond laser beams,” Nat. Photonics 10, 547–553 (2016).
[Crossref]

N. Tsatrafyllis, B. Bergues, H. Schröder, L. Veisz, E. Skantzakis, D. Gray, B. Bodi, S. Kuhn, G. D. Tsakiris, D. Charalambidis, and P. Tzallas, “The ion microscope as a tool for quantitative measurements in the extreme ultraviolet,” Sci. Rep. 6, 21556 (2016).
[Crossref]

S. V. Bulanov, T. Z. Esirkepov, M. Kando, and J. Koga, “Relativistic mirrors in laser plasmas (analytical methods),” Plasma Sources Sci. Technol. 25, 053001 (2016).
[Crossref]

A. Leblanc, S. Monchocé, C. Bourassin-Bouchet, S. Kahaly, and F. Quéré, “Ptychographic measurements of ultrahigh-intensity laser-plasma interactions,” Nat. Phys. 12, 301–305 (2016).
[Crossref]

M. A. Fareed, N. Thiré, S. Mondal, B. E. Schmidt, F. Légaré, and T. Ozaki, “Efficient generation of sub-100  eV high-order harmonics from carbon molecules using infrared laser pulses,” Appl. Phys. Lett. 108, 124104 (2016).
[Crossref]

M. Thévenet, H. Vincenti, and J. Faure, “On the physics of electron ejection from laser-irradiated overdense plasmas,” Phys. Plasmas 23, 063119 (2016).
[Crossref]

M. Bocoum, M. Thévenet, F. Böhle, B. Beaurepaire, A. Vernier, A. Jullien, J. Faure, and R. Lopez-Martens, “Anticorrelated emission of high harmonics and fast electron beams from plasma mirrors,” Phys. Rev. Lett. 116, 185001 (2016).
[Crossref]

G.-Q. Liao, Y.-T. Li, C. Li, S. Mondal, H. A. Hafez, M. A. Fareed, T. Ozaki, W.-M. Wang, Z.-M. Sheng, and J. Zhang, “Terahertz emission from two-plasmon-decay induced transient currents in laser-solid interactions,” Phys. Plasmas 23, 013104 (2016).
[Crossref]

2015 (10)

M. Thévenet, A. Leblanc, S. Kahaly, H. Vincenti, A. Vernier, F. Quéré, and J. Faure, “Vacuum laser acceleration of relativistic electrons using plasma mirror injectors,” Nat. Phys. 12, 355–360 (2015).
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G. Vampa, T. J. Hammond, N. Thiré, B. E. Schmidt, F. Légaré, C. R. McDonald, T. Brabec, and P. B. Corkum, “Linking high harmonics from gases and solids,” Nature 522, 462–464 (2015).
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M. Reduzzi, P. Carpeggiani, S. Kühn, F. Calegari, M. Nisoli, S. Stagira, C. Vozzi, P. Dombi, S. Kahaly, P. Tzallas, D. Charalambidis, K. Varju, K. Osvay, and G. Sansone, “Advances in high-order harmonic generation sources for time-resolved investigations,” J. Electron Spectrosc. Relat. Phenom. 204, 257–268 (2015).
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P. Heissler, A. Barna, J. M. Mikhailova, G. Ma, K. Khrennikov, S. Karsch, L. Veisz, I. B. Földes, and G. D. Tsakiris, “Multi-μJ harmonic emission energy from laser-driven plasma,” Appl. Phys. B 118, 195–201 (2015).
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A. Flacco, J. Vieira, A. Lifschitz, F. Sylla, S. Kahaly, M. Veltcheva, L. O. Silva, and V. Malka, “Persistence of magnetic field driven by relativistic electrons in a plasma,” Nat. Phys. 11, 409–413 (2015).
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A. Poyé, J.-L. Dubois, F. Lubrano-Lavaderci, E. D’Humières, M. Bardon, S. Hulin, M. Bailly-Grandvaux, J. Ribolzi, D. Raffestin, J. J. Santos, P. Nicolaï, and V. Tikhonchuk, “Dynamic model of target charging by short laser pulse interactions,” Phys. Rev. E 92, 043107 (2015).
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A. Poyé, S. Hulin, M. Bailly-Grandvaux, J. L. Dubois, J. Ribolzi, D. Raffestin, M. Bardon, F. Lubrano-Lavaderci, E. D’Humières, J. J. Santos, P. Nicolaï, and V. Tikhonchuk, “Physics of giant electromagnetic pulse generation in short-pulse laser experiments,” Phys. Rev. E 91, 043106 (2015).
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M. Yeung, J. Bierbach, E. Eckner, S. Rykovanov, S. Kuschel, A. Sävert, M. Förster, C. Rödel, G. G. Paulus, S. Cousens, M. Coughlan, B. Dromey, and M. Zepf, “Noncollinear polarization gating of attosecond pulse trains in the relativistic regime,” Phys. Rev. Lett. 115, 193903 (2015).
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M. Bocoum, F. Böhle, A. Vernier, A. Jullien, J. Faure, and R. Lopez-Martens, “Spatial-domain interferometer for measuring plasma mirror expansion,” Opt. Lett. 40, 3009–3012 (2015).
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M. Lucchini, M. H. Brügmann, A. Ludwig, L. Gallmann, U. Keller, and T. Feurer, “Ptychographic reconstruction of attosecond pulses,” Opt. Express 23, 29502–29513 (2015).
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2014 (8)

G. Kolliopoulos, P. Tzallas, B. Bergues, P. A. Carpeggiani, P. Heissler, H. Schröder, L. Veisz, D. Charalambidis, and G. D. Tsakiris, “Single-shot autocorrelator for extreme-ultraviolet radiation,” J. Opt. Soc. Am. B 31, 926–938 (2014).
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V. Gallet, S. Kahaly, O. Gobert, and F. Quéré, “Dual spectral-band interferometry for spatio-temporal characterization of high-power femtosecond lasers,” Opt. Lett. 39, 4687–4690 (2014).
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F. Quéré, H. Vincenti, A. Borot, S. Monchocé, T. J. Hammond, K. T. Kim, J. A. Wheeler, C. Zhang, T. Ruchon, T. Auguste, J. F. Hergott, D. M. Villeneuve, P. B. Corkum, and R. Lopez-Martens, “Applications of ultrafast wavefront rotation in highly nonlinear optics,” J. Phys. B 47, 124004 (2014).
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W. Helml, A. R. Maier, W. Schweinberger, I. Grguraš, P. Radcliffe, G. Doumy, C. Roedig, J. Gagnon, M. Messerschmidt, S. Schorb, C. Bostedt, F. Grüner, L. F. DiMauro, D. Cubaynes, J. D. Bozek, T. Tschentscher, J. T. Costello, M. Meyer, R. Coffee, S. Düsterer, A. L. Cavalieri, and R. Kienberger, “Measuring the temporal structure of few-femtosecond free-electron laser X-ray pulses directly in the time domain,” Nat. Photonics 8, 950–957 (2014).
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S. Kahaly, S. Monchocé, V. Gallet, O. Gobert, F. Réau, O. Tcherbakoff, P. D’Oliveira, P. Martin, and F. Quéré, “Investigation of amplitude spatio-temporal couplings at the focus of a 100 TW-25  fs laser,” Appl. Phys. Lett. 104, 054103 (2014).
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T. Kluge, C. Gutt, L. G. Huang, J. Metzkes, U. Schramm, M. Bussmann, and T. E. Cowan, “Using X-ray free-electron lasers for probing of complex interaction dynamics of ultra-intense lasers with solid matter,” Phys. Plasmas 21, 033110 (2014).
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S. Monchocé, S. Kahaly, A. Leblanc, L. Videau, P. Combis, F. Réau, D. Garzella, P. D’Oliveira, P. Martin, and F. Quéré, “Optically controlled solid-density transient plasma gratings,” Phys. Rev. Lett. 112, 145008 (2014).
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H. Vincenti, S. Monchocé, S. Kahaly, G. Bonnaud, P. Martin, and F. Quéré, “Optical properties of relativistic plasma mirrors,” Nat. Commun. 5, 3403 (2014).
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2013 (4)

A. Malvache, A. Borot, F. Quéré, and R. Lopez-Martens, “Coherent wake emission spectroscopy as a probe of steep plasma density profiles,” Phys. Rev. E 87, 035101 (2013).
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F. Dollar, P. Cummings, V. Chvykov, L. Willingale, M. Vargas, V. Yanovsky, C. Zulick, A. Maksimchuk, A. G. R. Thomas, and K. Krushelnick, “Scaling high-order harmonic generation from laser-solid interactions to ultrahigh intensity,” Phys. Rev. Lett. 110, 175002 (2013).
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S. Kahaly, S. Monchocé, H. Vincenti, T. Dzelzainis, B. Dromey, M. Zepf, P. Martin, and F. Quéré, “Direct observation of density-gradient effects in harmonic generation from plasma mirrors,” Phys. Rev. Lett. 110, 175001 (2013).
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C. Bourassin-Bouchet, M. M. Mang, F. Delmotte, P. Chavel, and S. de Rossi, “How to focus an attosecond pulse,” Opt. Express 21, 2506–2520 (2013).
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2012 (2)

J. A. Wheeler, A. Borot, S. Monchocé, H. Vincenti, A. Ricci, A. Malvache, R. Lopez-Martens, and F. Quéré, “Attosecond lighthouses from plasma mirrors,” Nat. Photonics 6, 829–833 (2012).
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P. Heissler, R. Hörlein, J. M. Mikhailova, L. Waldecker, P. Tzallas, A. Buck, K. Schmid, C. M. S. Sears, F. Krausz, L. Veisz, M. Zepf, and G. D. Tsakiris, “Few-cycle driven relativistically oscillating plasma mirrors: a source of intense isolated attosecond pulses,” Phys. Rev. Lett. 108, 235003 (2012).
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2011 (1)

2010 (5)

M. Chini, S. Gilbertson, S. D. Khan, and Z. Chang, “Characterizing ultrabroadband attosecond lasers,” Opt. Express 18, 13006–13016 (2010).
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R. Hörlein, Y. Nomura, P. Tzallas, S. G. Rykovanov, B. Dromey, J. Osterhoff, Z. Major, S. Karsch, L. Veisz, M. Zepf, D. Charalambidis, F. Krausz, and G. D. Tsakiris, “Temporal characterization of attosecond pulses emitted from solid-density plasmas,” New J. Phys. 12, 043020 (2010).
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S. Akturk, X. Gu, P. Bowlan, and R. Trebino, “Spatio-temporal couplings in ultrashort laser pulses,” J. Opt. 12, 093001 (2010).
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C. Thaury and F. Quéré, “High-order harmonic and attosecond pulse generation on plasma mirrors: basic mechanisms,” J. Phys. B 43, 213001 (2010).
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S. Ghimire, A. D. DiChiara, E. Sistrunk, P. Agostini, L. F. DiMauro, and D. A. Reis, “Observation of high-order harmonic generation in a bulk crystal,” Nat. Phys. 7, 138–141 (2010).
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2009 (5)

S. Kahaly, S. Mondal, G. R. Kumar, S. Sengupta, A. Das, and P. K. Kaw, “Polarimetric detection of laser induced ultrashort magnetic pulses in overdense plasma,” Phys. Plasmas 16, 043114 (2009).
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F. Krausz and M. Ivanov, “Attosecond physics,” Rev. Mod. Phys. 81, 163–234 (2009).
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U. Teubner and P. Gibbon, “High-order harmonics from laser-irradiated plasma surfaces,” Rev. Mod. Phys. 81, 445–479 (2009).
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U. Frühling, M. Wieland, M. Gensch, T. Gebert, B. Schütte, M. Krikunova, R. Kalms, F. Budzyn, O. Grimm, J. Rossbach, E. Plönjes, and M. Drescher, “Single-shot terahertz-field-driven X-ray streak camera,” Nat. Photonics 3, 523–528 (2009).
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Y. Nomura, R. Hörlein, P. Tzallas, B. Dromey, S. Rykovanov, Z. Major, J. Osterhoff, S. Karsch, L. Veisz, M. Zepf, D. Charalambidis, F. Krausz, and G. D. Tsakiris, “Attosecond phase locking of harmonics emitted from laser-produced plasmas,” Nat. Phys. 5, 124–128 (2009).
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2008 (3)

F. Quéré, C. Thaury, J. P. Geindre, G. Bonnaud, P. Monot, and P. Martin, “Phase properties of laser high-order harmonics generated on plasma mirrors,” Phys. Rev. Lett. 100, 095004 (2008).
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S. G. Rykovanov, M. Geissler, J. Meyer-ter Vehn, and G. D. Tsakiris, “Intense single attosecond pulses from surface harmonics using the polarization gating technique,” New J. Phys. 10, 025025 (2008).
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C. Winterfeldt, C. Spielmann, and G. Gerber, “Colloquium: optimal control of high-harmonic generation,” Rev. Mod. Phys. 80, 117–140 (2008).
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2007 (1)

B. Dromey, S. Kar, C. Bellei, D. C. Carroll, R. J. Clarke, J. S. Green, S. Kneip, K. Markey, S. R. Nagel, P. T. Simpson, L. Willingale, P. McKenna, D. Neely, Z. Najmudin, K. Krushelnick, P. A. Norreys, and M. Zepf, “Bright multi-keV harmonic generation from relativistically oscillating plasma surfaces,” Phys. Rev. Lett. 99, 085001 (2007).
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2006 (4)

G. D. Tsakiris, K. Eidmann, J. Meyer-ter Vehn, and F. Krausz, “Route to intense single attosecond pulses,” New J. Phys. 8, 19 (2006).
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B. Dromey, M. Zepf, A. Gopal, K. Lancaster, M. S. Wei, K. Krushelnick, M. Tatarakis, N. Vakakis, S. Moustaizis, R. Kodama, M. Tampo, C. Stoeckl, R. Clarke, H. Habara, D. Neely, S. Karsch, and P. Norreys, “High harmonic generation in the relativistic limit,” Nat. Phys. 2, 456–459 (2006).
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F. Quéré, C. Thaury, P. Monot, S. Dobosz, P. Martin, J.-P. Geindre, and P. Audebert, “Coherent wake emission of high-order harmonics from overdense plasmas,” Phys. Rev. Lett. 96, 125004 (2006).
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T. Baeva, S. Gordienko, and A. Pukhov, “Theory of high-order harmonic generation in relativistic laser interaction with overdense plasma,” Phys. Rev. E 74, 046404 (2006).
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2005 (1)

F. Quéré, Y. Mairesse, and J. Itatani, “Temporal characterization of attosecond XUV fields,” J. Mod. Opt. 52, 339–360 (2005).
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2004 (1)

M. J. Mead, D. Neely, J. Gauoin, R. Heathcote, and P. Patel, “Electromagnetic pulse generation within a petawatt laser target chamber,” Rev. Sci. Instrum. 75, 4225–4227 (2004).
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2002 (1)

F. Borne, D. Delacroix, J. M. Gel, D. Mass, and F. Amiranoff, “Radiation protection for an ultra-high intensity laser,” Radiat. Prot. Dosimetry 102, 61–70 (2002).
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1996 (2)

D. Von der Linde and K. Rzazewski, “High-order optical harmonic generation from solid surfaces,” Appl. Phys. B 63, 499–506 (1996).
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1993 (2)

P. B. Corkum, “Plasma perspective on strong field multiphoton ionization,” Phys. Rev. Lett. 71, 1994–1997 (1993).
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H. Hamster, A. Sullivan, S. Gordon, W. White, and R. W. Falcone, “Subpicosecond, electromagnetic pulses from intense laser-plasma interaction,” Phys. Rev. Lett. 71, 2725–2728 (1993).
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1983 (1)

A. Bourdier, “Oblique incidence of a strong electromagnetic wave on a cold inhomogeneous electron plasma. Relativistic effects,” Phys. Fluids 26, 1804–1807 (1983).
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Agostini, P.

S. Ghimire, A. D. DiChiara, E. Sistrunk, P. Agostini, L. F. DiMauro, and D. A. Reis, “Observation of high-order harmonic generation in a bulk crystal,” Nat. Phys. 7, 138–141 (2010).
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Akturk, S.

S. Akturk, X. Gu, P. Bowlan, and R. Trebino, “Spatio-temporal couplings in ultrashort laser pulses,” J. Opt. 12, 093001 (2010).
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Aleknavicius, A.

Amiranoff, F.

F. Borne, D. Delacroix, J. M. Gel, D. Mass, and F. Amiranoff, “Radiation protection for an ultra-high intensity laser,” Radiat. Prot. Dosimetry 102, 61–70 (2002).
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Arnold, C. L.

S. Kühn, M. Dumergue, S. Kahaly, S. Mondal, M. Füle, T. Csizmadia, B. Farkas, B. Major, Z. Várallyay, F. Calegari, M. Devetta, F. Frassetto, E. Mänsson, L. Poletto, S. Stagira, C. Vozzi, M. Nisoli, P. Rudawski, S. Maclot, F. Campi, H. Wikmark, C. L. Arnold, C. M. Heyl, P. Johnsson, A. L’Huillier, R. Lopez-Martens, S. Haessler, M. Bocoum, F. Boehle, A. Vernier, G. Iaquaniello, E. Skantzakis, N. Papadakis, C. Kalpouzos, P. Tzallas, F. Lépine, D. Charalambidis, K. Varjú, K. Osvay, and G. Sansone, “The ELI-ALPS facility: the next generation of attosecond sources,” J. Phys. B 50, 132002 (2017).
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Audebert, P.

F. Quéré, C. Thaury, P. Monot, S. Dobosz, P. Martin, J.-P. Geindre, and P. Audebert, “Coherent wake emission of high-order harmonics from overdense plasmas,” Phys. Rev. Lett. 96, 125004 (2006).
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Auguste, T.

F. Quéré, H. Vincenti, A. Borot, S. Monchocé, T. J. Hammond, K. T. Kim, J. A. Wheeler, C. Zhang, T. Ruchon, T. Auguste, J. F. Hergott, D. M. Villeneuve, P. B. Corkum, and R. Lopez-Martens, “Applications of ultrafast wavefront rotation in highly nonlinear optics,” J. Phys. B 47, 124004 (2014).
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Baeva, T.

T. Baeva, S. Gordienko, and A. Pukhov, “Theory of high-order harmonic generation in relativistic laser interaction with overdense plasma,” Phys. Rev. E 74, 046404 (2006).
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Bailly-Grandvaux, M.

A. Poyé, J.-L. Dubois, F. Lubrano-Lavaderci, E. D’Humières, M. Bardon, S. Hulin, M. Bailly-Grandvaux, J. Ribolzi, D. Raffestin, J. J. Santos, P. Nicolaï, and V. Tikhonchuk, “Dynamic model of target charging by short laser pulse interactions,” Phys. Rev. E 92, 043107 (2015).
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A. Poyé, S. Hulin, M. Bailly-Grandvaux, J. L. Dubois, J. Ribolzi, D. Raffestin, M. Bardon, F. Lubrano-Lavaderci, E. D’Humières, J. J. Santos, P. Nicolaï, and V. Tikhonchuk, “Physics of giant electromagnetic pulse generation in short-pulse laser experiments,” Phys. Rev. E 91, 043106 (2015).
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Balickas, S.

Bardon, M.

A. Poyé, S. Hulin, M. Bailly-Grandvaux, J. L. Dubois, J. Ribolzi, D. Raffestin, M. Bardon, F. Lubrano-Lavaderci, E. D’Humières, J. J. Santos, P. Nicolaï, and V. Tikhonchuk, “Physics of giant electromagnetic pulse generation in short-pulse laser experiments,” Phys. Rev. E 91, 043106 (2015).
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A. Poyé, J.-L. Dubois, F. Lubrano-Lavaderci, E. D’Humières, M. Bardon, S. Hulin, M. Bailly-Grandvaux, J. Ribolzi, D. Raffestin, J. J. Santos, P. Nicolaï, and V. Tikhonchuk, “Dynamic model of target charging by short laser pulse interactions,” Phys. Rev. E 92, 043107 (2015).
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Barna, A.

P. Heissler, A. Barna, J. M. Mikhailova, G. Ma, K. Khrennikov, S. Karsch, L. Veisz, I. B. Földes, and G. D. Tsakiris, “Multi-μJ harmonic emission energy from laser-driven plasma,” Appl. Phys. B 118, 195–201 (2015).
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Beaurepaire, B.

M. Bocoum, M. Thévenet, F. Böhle, B. Beaurepaire, A. Vernier, A. Jullien, J. Faure, and R. Lopez-Martens, “Anticorrelated emission of high harmonics and fast electron beams from plasma mirrors,” Phys. Rev. Lett. 116, 185001 (2016).
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Bellei, C.

B. Dromey, S. Kar, C. Bellei, D. C. Carroll, R. J. Clarke, J. S. Green, S. Kneip, K. Markey, S. R. Nagel, P. T. Simpson, L. Willingale, P. McKenna, D. Neely, Z. Najmudin, K. Krushelnick, P. A. Norreys, and M. Zepf, “Bright multi-keV harmonic generation from relativistically oscillating plasma surfaces,” Phys. Rev. Lett. 99, 085001 (2007).
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Bergues, B.

N. Tsatrafyllis, B. Bergues, H. Schröder, L. Veisz, E. Skantzakis, D. Gray, B. Bodi, S. Kuhn, G. D. Tsakiris, D. Charalambidis, and P. Tzallas, “The ion microscope as a tool for quantitative measurements in the extreme ultraviolet,” Sci. Rep. 6, 21556 (2016).
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G. Kolliopoulos, P. Tzallas, B. Bergues, P. A. Carpeggiani, P. Heissler, H. Schröder, L. Veisz, D. Charalambidis, and G. D. Tsakiris, “Single-shot autocorrelator for extreme-ultraviolet radiation,” J. Opt. Soc. Am. B 31, 926–938 (2014).
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Bierbach, J.

M. Yeung, J. Bierbach, E. Eckner, S. Rykovanov, S. Kuschel, A. Sävert, M. Förster, C. Rödel, G. G. Paulus, S. Cousens, M. Coughlan, B. Dromey, and M. Zepf, “Noncollinear polarization gating of attosecond pulse trains in the relativistic regime,” Phys. Rev. Lett. 115, 193903 (2015).
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Bocoum, M.

S. Kühn, M. Dumergue, S. Kahaly, S. Mondal, M. Füle, T. Csizmadia, B. Farkas, B. Major, Z. Várallyay, F. Calegari, M. Devetta, F. Frassetto, E. Mänsson, L. Poletto, S. Stagira, C. Vozzi, M. Nisoli, P. Rudawski, S. Maclot, F. Campi, H. Wikmark, C. L. Arnold, C. M. Heyl, P. Johnsson, A. L’Huillier, R. Lopez-Martens, S. Haessler, M. Bocoum, F. Boehle, A. Vernier, G. Iaquaniello, E. Skantzakis, N. Papadakis, C. Kalpouzos, P. Tzallas, F. Lépine, D. Charalambidis, K. Varjú, K. Osvay, and G. Sansone, “The ELI-ALPS facility: the next generation of attosecond sources,” J. Phys. B 50, 132002 (2017).
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M. Bocoum, M. Thévenet, F. Böhle, B. Beaurepaire, A. Vernier, A. Jullien, J. Faure, and R. Lopez-Martens, “Anticorrelated emission of high harmonics and fast electron beams from plasma mirrors,” Phys. Rev. Lett. 116, 185001 (2016).
[Crossref]

M. Bocoum, F. Böhle, A. Vernier, A. Jullien, J. Faure, and R. Lopez-Martens, “Spatial-domain interferometer for measuring plasma mirror expansion,” Opt. Lett. 40, 3009–3012 (2015).
[Crossref]

Bodi, B.

N. Tsatrafyllis, B. Bergues, H. Schröder, L. Veisz, E. Skantzakis, D. Gray, B. Bodi, S. Kuhn, G. D. Tsakiris, D. Charalambidis, and P. Tzallas, “The ion microscope as a tool for quantitative measurements in the extreme ultraviolet,” Sci. Rep. 6, 21556 (2016).
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Boehle, F.

S. Kühn, M. Dumergue, S. Kahaly, S. Mondal, M. Füle, T. Csizmadia, B. Farkas, B. Major, Z. Várallyay, F. Calegari, M. Devetta, F. Frassetto, E. Mänsson, L. Poletto, S. Stagira, C. Vozzi, M. Nisoli, P. Rudawski, S. Maclot, F. Campi, H. Wikmark, C. L. Arnold, C. M. Heyl, P. Johnsson, A. L’Huillier, R. Lopez-Martens, S. Haessler, M. Bocoum, F. Boehle, A. Vernier, G. Iaquaniello, E. Skantzakis, N. Papadakis, C. Kalpouzos, P. Tzallas, F. Lépine, D. Charalambidis, K. Varjú, K. Osvay, and G. Sansone, “The ELI-ALPS facility: the next generation of attosecond sources,” J. Phys. B 50, 132002 (2017).
[Crossref]

Böhle, F.

M. Bocoum, M. Thévenet, F. Böhle, B. Beaurepaire, A. Vernier, A. Jullien, J. Faure, and R. Lopez-Martens, “Anticorrelated emission of high harmonics and fast electron beams from plasma mirrors,” Phys. Rev. Lett. 116, 185001 (2016).
[Crossref]

M. Bocoum, F. Böhle, A. Vernier, A. Jullien, J. Faure, and R. Lopez-Martens, “Spatial-domain interferometer for measuring plasma mirror expansion,” Opt. Lett. 40, 3009–3012 (2015).
[Crossref]

Bonnaud, G.

H. Vincenti, S. Monchocé, S. Kahaly, G. Bonnaud, P. Martin, and F. Quéré, “Optical properties of relativistic plasma mirrors,” Nat. Commun. 5, 3403 (2014).
[Crossref]

F. Quéré, C. Thaury, J. P. Geindre, G. Bonnaud, P. Monot, and P. Martin, “Phase properties of laser high-order harmonics generated on plasma mirrors,” Phys. Rev. Lett. 100, 095004 (2008).
[Crossref]

Borne, F.

F. Borne, D. Delacroix, J. M. Gel, D. Mass, and F. Amiranoff, “Radiation protection for an ultra-high intensity laser,” Radiat. Prot. Dosimetry 102, 61–70 (2002).
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Borot, A.

G. Pariente, V. Gallet, A. Borot, O. Gobert, and F. Quéré, “Space-time characterization of ultra-intense femtosecond laser beams,” Nat. Photonics 10, 547–553 (2016).
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F. Quéré, H. Vincenti, A. Borot, S. Monchocé, T. J. Hammond, K. T. Kim, J. A. Wheeler, C. Zhang, T. Ruchon, T. Auguste, J. F. Hergott, D. M. Villeneuve, P. B. Corkum, and R. Lopez-Martens, “Applications of ultrafast wavefront rotation in highly nonlinear optics,” J. Phys. B 47, 124004 (2014).
[Crossref]

A. Malvache, A. Borot, F. Quéré, and R. Lopez-Martens, “Coherent wake emission spectroscopy as a probe of steep plasma density profiles,” Phys. Rev. E 87, 035101 (2013).
[Crossref]

J. A. Wheeler, A. Borot, S. Monchocé, H. Vincenti, A. Ricci, A. Malvache, R. Lopez-Martens, and F. Quéré, “Attosecond lighthouses from plasma mirrors,” Nat. Photonics 6, 829–833 (2012).
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Bostedt, C.

W. Helml, A. R. Maier, W. Schweinberger, I. Grguraš, P. Radcliffe, G. Doumy, C. Roedig, J. Gagnon, M. Messerschmidt, S. Schorb, C. Bostedt, F. Grüner, L. F. DiMauro, D. Cubaynes, J. D. Bozek, T. Tschentscher, J. T. Costello, M. Meyer, R. Coffee, S. Düsterer, A. L. Cavalieri, and R. Kienberger, “Measuring the temporal structure of few-femtosecond free-electron laser X-ray pulses directly in the time domain,” Nat. Photonics 8, 950–957 (2014).
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Bourassin-Bouchet, C.

A. Leblanc, S. Monchocé, C. Bourassin-Bouchet, S. Kahaly, and F. Quéré, “Ptychographic measurements of ultrahigh-intensity laser-plasma interactions,” Nat. Phys. 12, 301–305 (2016).
[Crossref]

C. Bourassin-Bouchet, M. M. Mang, F. Delmotte, P. Chavel, and S. de Rossi, “How to focus an attosecond pulse,” Opt. Express 21, 2506–2520 (2013).
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Khan, S. D.

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F. Krausz and M. Ivanov, “Attosecond physics,” Rev. Mod. Phys. 81, 163–234 (2009).
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J. A. Wheeler, A. Borot, S. Monchocé, H. Vincenti, A. Ricci, A. Malvache, R. Lopez-Martens, and F. Quéré, “Attosecond lighthouses from plasma mirrors,” Nat. Photonics 6, 829–833 (2012).
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S. Mondal, H. A. Hafez, X. Ropagnol, and T. Ozaki, “MV/cm terahertz pulses from relativistic laser-plasma interaction characterized by nonlinear terahertz absorption bleaching in n-doped InGaAs,” Opt. Express 25, 17511–17523 (2017).
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Figures (8)

Fig. 1.
Fig. 1. Parameters of the SYLOS and HF primary sources that would drive a complementary set of relativistic laser–plasma experiments in the SPA beamlines. The parameters in red are the values that would be achieved in the final phase.
Fig. 2.
Fig. 2. PIC simulation results for SHHG-SYLOS. (a) Incident and reflected pulses for both S- and P-polarized lasers. (b),(c) Spatiotemporal evolution of plasma electron density for the S- and P-polarized incidences, respectively, showing ultrafast density modulation that is responsible for SHHG. (d) I(ωn) from simulations.
Fig. 3.
Fig. 3. PIC simulation results for SHHG-HF. (a) Incident and reflected pulses for both S- and P-polarized irradiation. (b),(c) Spatiotemporal evolution of the plasma electron density for the S- and P-polarized cases, respectively. Denting in the plasma density profile is observed. (d) I(ωn) from simulations.
Fig. 4.
Fig. 4. Amplitude of the EMP electric field strength at 50 cm distance from the target in various laser facilities versus the laser energy. The data is taken from [54]. The red boxes show the expected electric field strength values for SHHG-SYLOS and SHHG-HF at ELI-ALPS. The red lines indicate linear scaling of the EMP amplitude with the laser pulse energy given a certain pulse duration. The yellow shaded region corresponds to pico-femtosecond scale lasers while the cyan shaded region represents nanosecond class.
Fig. 5.
Fig. 5. Bird’s-eye view of the 3D design of the complete SHHG-SYLOS beamline along with the different functional sub-systems S1–S5. The main driving laser propagates from left to right in the figure.
Fig. 6.
Fig. 6. SHHG SYLOS interaction chamber S4 where the relativistic laser–plasma interaction takes place. The beam path and different constituent elements are demarcated. The red arrow indicates the direction of driving laser entry into S4. The working principle of H5 (Fig. 7) is similar.
Fig. 7.
Fig. 7. Functional schematic of the 3D design of the complete SHHG HF beamline. The beam path and different constituent elements are demarcated. The gray arrow indicates the direction of the driving laser.
Fig. 8.
Fig. 8. Essential phases of research and development activity with SPA beamlines preceding more mature user-based application experiments utilizing SHHG. The violet and orange solid circles correlate the source studies (list boxes) with the location within the beamlines (top left schematic). PG and LH stand for the techniques of polarization gating and light house, respectively.

Tables (1)

Tables Icon

Table 1. Expected Initial Parameters of the SHHG-SYLOS and SHHG-HF Development Beamlinesa

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