Abstract

Recent progresses in femtosecond ytterbium-doped fiber laser technology are opening new perspectives in strong field physics and attosecond science. High-order harmonic generation from these systems is particularly interesting because it provides high flux beams of ultrashort extreme ultraviolet radiation. A great deal of effort has been devoted to optimize the macroscopic generation parameters. Here we investigate the possibility of enhancing the single-atom response by producing high-order harmonics from the second, third and fourth harmonics of a turnkey 50 W, 166 kHz femtosecond Yb-fiber laser providing 135 fs pulses at 1030 nm. We show that the harmonic efficiency is optimal when the process is driven by the third harmonic, producing 6.6 ± 1.3 × 1014 photons/s at 18 eV in argon, which corresponds to 1.9 ± 0.4 mW average power.

© 2019 Optical Society of America under the terms of the OSA Open Access Publishing Agreement

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2019 (1)

M. Puppin, Y. Deng, C. W. Nicholson, J. Feldl, N. B. M. Schröter, H. Vita, P. S. Kirchmann, C. Monney, L. Rettig, M. Wolf, and R. Ernstorfer, “Time- and angle-resolved photoemission spectroscopy of solids in the extreme ultraviolet at 500 kHz repetition rate,” Rev. Sci. Instruments 90, 023104 (2019).
[Crossref]

2018 (5)

2017 (6)

M. Müller, A. Klenke, T. Gottschall, R. Klas, C. Rothhardt, S. Demmler, J. Rothhardt, J. Limpert, and A. Tünnermann, “High-average-power femtosecond laser at 258 nm,” Opt. Lett. 42, 2826–2829 (2017).
[Crossref]

D. A. Horke, N. Roth, L. Worbs, and J. Küpper, “Characterizing gas flow from aerosol particle injectors,” J. Appl. Phys. 121, 123106 (2017).
[Crossref]

A. Harth, C. Guo, Y.-C. Cheng, A. Losquin, M. Miranda, S. Mikaelsson, C. M. Heyl, O. Prochnow, J. Ahrens, U. Morgner, A. L’Huillier, and C. L. Arnold, “Compact 200 kHz HHG source driven by a few-cycle OPCPA,” J. Opt. 20, 014007 (2017).
[Crossref]

L. Lavenu, M. Natile, F. Guichard, Y. Zaouter, M. Hanna, E. Mottay, and P. Georges, “High-energy few-cycle Yb-doped fiber amplifier source based on a single nonlinear compression stage,” Opt. Express 25, 7530 (2017).
[Crossref] [PubMed]

C. Marceau, T. J. Hammond, A. Y. Naumov, P. B. Corkum, and D. M. Villeneuve, “Wavelength scaling of high harmonic generation for 267 nm, 400 nm and 800 nm driving laser pulses,” J. Phys. Commun. 1, 015009 (2017).
[Crossref]

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: At. Mol. Opt. Phys. 50, 013001 (2017).
[Crossref]

2016 (8)

F. Calegari, G. Sansone, S. Stagira, C. Vozzi, and M. Nisoli, “Advances in attosecond science,” J. Phys. B: At. Mol. Opt. Phys. 49, 062001 (2016).
[Crossref]

S. Hädrich, Jan Rothhardt, M. Krebs, S. Demmler, A. Klenke, A. Tünnermann, and J. Limpert, “Single-pass high harmonic generation at high repetition rate and photon flux,” J. Phys. B: At. Mol. Opt. Phys. 49, 172002 (2016).
[Crossref]

J. Rothhardt, S. Hädrich, Y. Shamir, M. Tschnernajew, R. Klas, A. Hoffmann, G. K. Tadesse, A. Klenke, T. Gottschall, T. Eidam, J. Limpert, A. Tünnermann, R. Boll, C. Bomme, H. Dachraoui, B. Erk, M. Di Fraia, D. A. Horke, T. Kierspel, T. Mullins, A. Przystawik, E. Savelyev, J. Wiese, T. Laarmann, J. Küpper, and D. Rolles, “High-repetition-rate and high-photon-flux 70 eV high-harmonic source for coincidence ion imaging of gas-phase molecules,” Opt. Express 24, 18133 (2016).
[Crossref] [PubMed]

C. M. Heyl, H. Coudert-Alteirac, M. Miranda, M. Louisy, K. Kovacs, V. Tosa, E. Balogh, K. Varjú, A. L’Huillier, A. Couairon, and C. L. Arnold, “Scale-invariant nonlinear optics in gases,” Optica 3, 75 (2016).
[Crossref]

R. Klas, S. Demmler, M. Tschernajew, S. Hädrich, Y. Shamir, A. Tünnermann, J. Rothhardt, and J. Limpert, “Table-top milliwatt-class extreme ultraviolet high harmonic light source,” Optica 3, 1167 (2016).
[Crossref]

S. Hädrich, M. Kienel, M. Müller, A. Klenke, J. Rothhardt, R. Klas, T. Gottschall, T. Eidam, A. Drozdy, P. Jójárt, Z. Várallyay, E. Cormier, K. Osvay, A. Tünnermann, and J. Limpert, “Energetic sub-2-cycle laser with 216 W average power,” Opt. Lett. 41, 4332–4335 (2016).
[Crossref]

G. H. Kim, J. Yang, B. Lee, E. G. Sall’, S. A. Chizhov, A. G. Kalintsev, V. E. Yashin, and U. Kang, “Efficient generation of the second and third harmonics of high-power femtosecond Yb:KGW-laser radiation in nonlinear-optical BBO crystals,” J. Opt. Technol. 83, 463–467 (2016).
[Crossref]

J. Rothhardt, C. Rothhardt, M. Müller, A. Klenke, M. Kienel, S. Demmler, T. Elsmann, M. Rothhardt, J. Limpert, and A. Tünnermann, “100 W average power femtosecond laser at 343 nm,” Opt. Lett. 41, 1885–1888 (2016).
[Crossref] [PubMed]

2015 (2)

H. Wang, Y. Xu, S. Ulonska, J. S. Robinson, P. Ranitovic, and R. A. Kaindl, “Bright high-repetition-rate source of narrowband extreme-ultraviolet harmonics beyond 22 eV,” Nat. Commun. 6, 7459 (2015).
[Crossref]

D. Popmintchev, C. Hernández-García, F. Dollar, C. Mancuso, J. A. Pérez-Hernández, M.-C. Chen, A. Hankla, X. Gao, B. Shim, A. L. Gaeta, M. Tarazkar, D. A. Romanov, R. J. Levis, J. A. Gaffney, M. Foord, S. B. Libby, A. Jaron-Becker, A. Becker, L. Plaja, M. M. Murnane, H. C. Kapteyn, and T. Popmintchev, “Ultraviolet surprise: efficient soft x-ray high-harmonic generation in multiply ionized plasmas,” Science 350, 1225–1231 (2015).
[Crossref]

2014 (2)

J. Rothhardt, S. Hädrich, A. Klenke, S. Demmler, A. Hoffmann, T. Gotschall, T. Eidam, M. Krebs, J. Limpert, and A. Tünnermann, “53 W average power few-cycle fiber laser system generating soft x rays up to the water window,” Opt. Lett. 39, 5224–5227 (2014).
[Crossref] [PubMed]

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).
[Crossref]

2013 (1)

C.-J. Lai, G. Cirmi, K.-H. Hong, J. Moses, S.-W. Huang, E. Granados, P. Keathley, S. Bhardwaj, and F. X. Kärtner, “Wavelength Scaling of High Harmonic Generation Close to the Multiphoton Ionization Regime,” Phys. Rev. Lett. 111, 073901 (2013).
[Crossref] [PubMed]

2012 (3)

C. M. Heyl, J. Güdde, A. L’Huillier, and U. Höfer, “High-order harmonic generation with uJ laser pulses at high repetition rates,” J. Phys. B: At. Mol. Opt. Phys. 45, 074020 (2012).
[Crossref]

A. Cabasse, G. Machinet, A. Dubrouil, E. Cormier, and E. Constant, “Optimization and phase matching of fiber-laser-driven high-order harmonic generation at high repetition rate,” Opt. Lett. 37, 4618–4620 (2012).
[Crossref] [PubMed]

A. Cingöz, D. C. Yost, T. K. Allison, A. Ruehl, M. E. Fermann, I. Hartl, and J. Ye, “Direct frequency comb spectroscopy in the extreme ultraviolet,” Nature 482, 68–71 (2012).
[Crossref] [PubMed]

2011 (2)

S. Kazamias, S. Daboussi, O. Guilbaud, K. Cassou, D. Ros, B. Cros, and G. Maynard, “Pressure-induced phase matching in high-order harmonic generation,” Phys. Rev. A 83, 063405 (2011).
[Crossref]

J. Higuet, H. Ruf, N. Thiré, R. Cireasa, E. Constant, E. Cormier, D. Descamps, E. Mével, S. Petit, B. Pons, Y. Mairesse, and B. Fabre, “High-order harmonic spectroscopy of the Cooper minimum in argon: experimental and theoretical study,” Phys. Rev. A 83, 053401 (2011).
[Crossref]

2009 (2)

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).
[Crossref] [PubMed]

J. Boullet, Y. Zaouter, J. Limpert, S. Petit, Y. Mairesse, B. Fabre, J. Higuet, E. Mével, E. Constant, and E. Cormier, “High-order harmonic generation at a megahertz-level repetition rate directly driven by an ytterbium-doped-fiber chirped-pulse amplification system,” Opt. Lett. 34, 1489–1491 (2009).
[Crossref] [PubMed]

2008 (2)

E. Gagnon, A. S. Sandhu, A. Paul, K. Hagen, A. Czasch, T. Jahnke, P. Ranitovic, C. Lewis Cocke, B. Walker, M. M. Murnane, and H. C. Kapteyn, “Time-resolved momentum imaging system for molecular dynamics studies using a tabletop ultrafast extreme-ultraviolet light source,” Rev. Sci. Instruments 79, 063102 (2008).
[Crossref]

P. Colosimo, G. Doumy, C. I. Blaga, J. Wheeler, C. Hauri, F. Catoire, J. Tate, R. Chirla, A. M. March, G. G. Paulus, H. G. Muller, P. Agostini, and L. F. DiMauro, “Scaling strong-field interactions towards the classical limit,” Nat. Phys. 4, 386–389 (2008).
[Crossref]

2006 (1)

A. Paul, E. Gibson, X. Zhang, A. Lytle, T. Popmintchev, X. Zhou, M. Murnane, I. Christov, and H. Kapteyn, “Phase-Matching Techniques for Coherent Soft X-Ray Generation,” IEEE J. Quantum Electron. 42, 14–26 (2006).
[Crossref]

2005 (2)

C. Gohle, T. Udem, M. Herrmann, J. Rauschenberger, R. Holzwarth, H. A. Schuessler, F. Krausz, and T. W. Hänsch, “A frequency comb in the extreme ultraviolet,” Nature 436, 234 (2005).
[Crossref] [PubMed]

R. J. Jones, K. D. Moll, M. J. Thorpe, and J. Ye, “Phase-Coherent Frequency Combs in the Vacuum Ultraviolet via High-Harmonic Generation inside a Femtosecond Enhancement Cavity,” Phys. Rev. Lett. 94, 193201 (2005).
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2001 (2)

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 garmonic generation,” Science 292, 1689–1692 (2001).
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2000 (2)

R. Dörner, V. Mergel, O. Jagutzki, L. Spielberger, J. Ullrich, R. Moshammer, and H. Schmidt-Böcking, “Cold target recoil ion momentum spectroscopy: a ‘momentum microscope’ to view atomic collision dynamics,” Phys. Reports 330, 95–192 (2000).
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A. Dubietis, G. Tamošauskas, A. Varanavičius, and G. Valiulis, “Two-photon absorbing properties of ultraviolet phase-matchable crystals at 264 and 211 nm,” Appl. Opt. 39, 2437 (2000).
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1999 (1)

E. Constant, D. Garzella, P. Breger, E. Mével, C. Dorrer, C. Le Blanc, F. Salin, and P. Agostini, “Optimizing High Harmonic Generation in Absorbing Gases: Model and Experiment,” Phys. Rev. Lett. 82, 1668–1671 (1999).
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1994 (1)

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).
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1993 (2)

P. B. Corkum, “Plasma perspective on strong field multiphoton ionization,” Phys. Rev. Lett. 71, 1994 (1993).
[Crossref] [PubMed]

B. Henke, E. Gullikson, and J. Davis, “X-ray interactions: photoabsorption, scattering, transmission, and reflection at E=50–30000 eV, Z=1–92,”; At. Data Nucl. Data Tables 54, 181–342 (1993).
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1992 (1)

P. Balcou, C. Cornaggia, A. S. L. Gomes, L. A. Lompre, and A. L’Huillier, “Optimizing high-order harmonic generation in strong fields,” J. Phys. B: At. Mol. Opt. Phys. 25, 4467–4485 (1992).
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1962 (1)

J. W. Cooper, “Photoionization from Outer Atomic Subshells. A Model Study,” Phys. Rev. 128, 681–693 (1962).
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Agostini, P.

P. Colosimo, G. Doumy, C. I. Blaga, J. Wheeler, C. Hauri, F. Catoire, J. Tate, R. Chirla, A. M. March, G. G. Paulus, H. G. Muller, P. Agostini, and L. F. DiMauro, “Scaling strong-field interactions towards the classical limit,” Nat. Phys. 4, 386–389 (2008).
[Crossref]

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 garmonic generation,” Science 292, 1689–1692 (2001).
[Crossref] [PubMed]

E. Constant, D. Garzella, P. Breger, E. Mével, C. Dorrer, C. Le Blanc, F. Salin, and P. Agostini, “Optimizing High Harmonic Generation in Absorbing Gases: Model and Experiment,” Phys. Rev. Lett. 82, 1668–1671 (1999).
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Ahrens, J.

A. Harth, C. Guo, Y.-C. Cheng, A. Losquin, M. Miranda, S. Mikaelsson, C. M. Heyl, O. Prochnow, J. Ahrens, U. Morgner, A. L’Huillier, and C. L. Arnold, “Compact 200 kHz HHG source driven by a few-cycle OPCPA,” J. Opt. 20, 014007 (2017).
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Allison, T. K.

A. Cingöz, D. C. Yost, T. K. Allison, A. Ruehl, M. E. Fermann, I. Hartl, and J. Ye, “Direct frequency comb spectroscopy in the extreme ultraviolet,” Nature 482, 68–71 (2012).
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Arnold, C. L.

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: At. Mol. Opt. Phys. 50, 013001 (2017).
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A. Harth, C. Guo, Y.-C. Cheng, A. Losquin, M. Miranda, S. Mikaelsson, C. M. Heyl, O. Prochnow, J. Ahrens, U. Morgner, A. L’Huillier, and C. L. Arnold, “Compact 200 kHz HHG source driven by a few-cycle OPCPA,” J. Opt. 20, 014007 (2017).
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C. M. Heyl, H. Coudert-Alteirac, M. Miranda, M. Louisy, K. Kovacs, V. Tosa, E. Balogh, K. Varjú, A. L’Huillier, A. Couairon, and C. L. Arnold, “Scale-invariant nonlinear optics in gases,” Optica 3, 75 (2016).
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Augé, F.

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 garmonic generation,” Science 292, 1689–1692 (2001).
[Crossref] [PubMed]

Balcou, P.

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 garmonic generation,” Science 292, 1689–1692 (2001).
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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).
[Crossref] [PubMed]

P. Balcou, C. Cornaggia, A. S. L. Gomes, L. A. Lompre, and A. L’Huillier, “Optimizing high-order harmonic generation in strong fields,” J. Phys. B: At. Mol. Opt. Phys. 25, 4467–4485 (1992).
[Crossref]

Balogh, E.

Bandulet, H.-C.

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).
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Beaulieu, S.

Becker, A.

D. Popmintchev, C. Hernández-García, F. Dollar, C. Mancuso, J. A. Pérez-Hernández, M.-C. Chen, A. Hankla, X. Gao, B. Shim, A. L. Gaeta, M. Tarazkar, D. A. Romanov, R. J. Levis, J. A. Gaffney, M. Foord, S. B. Libby, A. Jaron-Becker, A. Becker, L. Plaja, M. M. Murnane, H. C. Kapteyn, and T. Popmintchev, “Ultraviolet surprise: efficient soft x-ray high-harmonic generation in multiply ionized plasmas,” Science 350, 1225–1231 (2015).
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Benko, C.

G. Porat, C. M. Heyl, S. B. Schoun, C. Benko, N. Dörre, K. L. Corwin, and J. Ye, “Phase-matched extreme-ultraviolet frequency-comb generation,” Nat. Photonics 12, 387–391 (2018).
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Bhardwaj, S.

C.-J. Lai, G. Cirmi, K.-H. Hong, J. Moses, S.-W. Huang, E. Granados, P. Keathley, S. Bhardwaj, and F. X. Kärtner, “Wavelength Scaling of High Harmonic Generation Close to the Multiphoton Ionization Regime,” Phys. Rev. Lett. 111, 073901 (2013).
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Blaga, C. I.

P. Colosimo, G. Doumy, C. I. Blaga, J. Wheeler, C. Hauri, F. Catoire, J. Tate, R. Chirla, A. M. March, G. G. Paulus, H. G. Muller, P. Agostini, and L. F. DiMauro, “Scaling strong-field interactions towards the classical limit,” Nat. Phys. 4, 386–389 (2008).
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Blanc, C. Le

E. Constant, D. Garzella, P. Breger, E. Mével, C. Dorrer, C. Le Blanc, F. Salin, and P. Agostini, “Optimizing High Harmonic Generation in Absorbing Gases: Model and Experiment,” Phys. Rev. Lett. 82, 1668–1671 (1999).
[Crossref]

Boll, R.

Bomme, C.

Boullet, J.

Breger, P.

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 garmonic generation,” Science 292, 1689–1692 (2001).
[Crossref] [PubMed]

E. Constant, D. Garzella, P. Breger, E. Mével, C. Dorrer, C. Le Blanc, F. Salin, and P. Agostini, “Optimizing High Harmonic Generation in Absorbing Gases: Model and Experiment,” Phys. Rev. Lett. 82, 1668–1671 (1999).
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Cabasse, A.

Calegari, F.

F. Calegari, G. Sansone, S. Stagira, C. Vozzi, and M. Nisoli, “Advances in attosecond science,” J. Phys. B: At. Mol. Opt. Phys. 49, 062001 (2016).
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Cassou, K.

S. Kazamias, S. Daboussi, O. Guilbaud, K. Cassou, D. Ros, B. Cros, and G. Maynard, “Pressure-induced phase matching in high-order harmonic generation,” Phys. Rev. A 83, 063405 (2011).
[Crossref]

Catoire, F.

P. Colosimo, G. Doumy, C. I. Blaga, J. Wheeler, C. Hauri, F. Catoire, J. Tate, R. Chirla, A. M. March, G. G. Paulus, H. G. Muller, P. Agostini, and L. F. DiMauro, “Scaling strong-field interactions towards the classical limit,” Nat. Phys. 4, 386–389 (2008).
[Crossref]

Chen, M.-C.

D. Popmintchev, C. Hernández-García, F. Dollar, C. Mancuso, J. A. Pérez-Hernández, M.-C. Chen, A. Hankla, X. Gao, B. Shim, A. L. Gaeta, M. Tarazkar, D. A. Romanov, R. J. Levis, J. A. Gaffney, M. Foord, S. B. Libby, A. Jaron-Becker, A. Becker, L. Plaja, M. M. Murnane, H. C. Kapteyn, and T. Popmintchev, “Ultraviolet surprise: efficient soft x-ray high-harmonic generation in multiply ionized plasmas,” Science 350, 1225–1231 (2015).
[Crossref]

Chen, Y.

Cheng, Y.-C.

A. Harth, C. Guo, Y.-C. Cheng, A. Losquin, M. Miranda, S. Mikaelsson, C. M. Heyl, O. Prochnow, J. Ahrens, U. Morgner, A. L’Huillier, and C. L. Arnold, “Compact 200 kHz HHG source driven by a few-cycle OPCPA,” J. Opt. 20, 014007 (2017).
[Crossref]

Chirla, R.

P. Colosimo, G. Doumy, C. I. Blaga, J. Wheeler, C. Hauri, F. Catoire, J. Tate, R. Chirla, A. M. March, G. G. Paulus, H. G. Muller, P. Agostini, and L. F. DiMauro, “Scaling strong-field interactions towards the classical limit,” Nat. Phys. 4, 386–389 (2008).
[Crossref]

Chizhov, S. A.

Christov, I.

A. Paul, E. Gibson, X. Zhang, A. Lytle, T. Popmintchev, X. Zhou, M. Murnane, I. Christov, and H. Kapteyn, “Phase-Matching Techniques for Coherent Soft X-Ray Generation,” IEEE J. Quantum Electron. 42, 14–26 (2006).
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Cingöz, A.

A. Cingöz, D. C. Yost, T. K. Allison, A. Ruehl, M. E. Fermann, I. Hartl, and J. Ye, “Direct frequency comb spectroscopy in the extreme ultraviolet,” Nature 482, 68–71 (2012).
[Crossref] [PubMed]

Cireasa, R.

J. Higuet, H. Ruf, N. Thiré, R. Cireasa, E. Constant, E. Cormier, D. Descamps, E. Mével, S. Petit, B. Pons, Y. Mairesse, and B. Fabre, “High-order harmonic spectroscopy of the Cooper minimum in argon: experimental and theoretical study,” Phys. Rev. A 83, 053401 (2011).
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Cirmi, G.

C.-J. Lai, G. Cirmi, K.-H. Hong, J. Moses, S.-W. Huang, E. Granados, P. Keathley, S. Bhardwaj, and F. X. Kärtner, “Wavelength Scaling of High Harmonic Generation Close to the Multiphoton Ionization Regime,” Phys. Rev. Lett. 111, 073901 (2013).
[Crossref] [PubMed]

Colosimo, P.

P. Colosimo, G. Doumy, C. I. Blaga, J. Wheeler, C. Hauri, F. Catoire, J. Tate, R. Chirla, A. M. March, G. G. Paulus, H. G. Muller, P. Agostini, and L. F. DiMauro, “Scaling strong-field interactions towards the classical limit,” Nat. Phys. 4, 386–389 (2008).
[Crossref]

Comby, A.

Comtois, D.

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).
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Constant, E.

Cooper, J. W.

J. W. Cooper, “Photoionization from Outer Atomic Subshells. A Model Study,” Phys. Rev. 128, 681–693 (1962).
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Corkum, P. B.

C. Marceau, T. J. Hammond, A. Y. Naumov, P. B. Corkum, and D. M. Villeneuve, “Wavelength scaling of high harmonic generation for 267 nm, 400 nm and 800 nm driving laser pulses,” J. Phys. Commun. 1, 015009 (2017).
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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).
[Crossref] [PubMed]

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).
[Crossref] [PubMed]

P. B. Corkum, “Plasma perspective on strong field multiphoton ionization,” Phys. Rev. Lett. 71, 1994 (1993).
[Crossref] [PubMed]

Cormier, E.

Cornaggia, C.

P. Balcou, C. Cornaggia, A. S. L. Gomes, L. A. Lompre, and A. L’Huillier, “Optimizing high-order harmonic generation in strong fields,” J. Phys. B: At. Mol. Opt. Phys. 25, 4467–4485 (1992).
[Crossref]

Corwin, K. L.

G. Porat, C. M. Heyl, S. B. Schoun, C. Benko, N. Dörre, K. L. Corwin, and J. Ye, “Phase-matched extreme-ultraviolet frequency-comb generation,” Nat. Photonics 12, 387–391 (2018).
[Crossref]

Couairon, A.

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: At. Mol. Opt. Phys. 50, 013001 (2017).
[Crossref]

C. M. Heyl, H. Coudert-Alteirac, M. Miranda, M. Louisy, K. Kovacs, V. Tosa, E. Balogh, K. Varjú, A. L’Huillier, A. Couairon, and C. L. Arnold, “Scale-invariant nonlinear optics in gases,” Optica 3, 75 (2016).
[Crossref]

Coudert-Alteirac, H.

Cros, B.

S. Kazamias, S. Daboussi, O. Guilbaud, K. Cassou, D. Ros, B. Cros, and G. Maynard, “Pressure-induced phase matching in high-order harmonic generation,” Phys. Rev. A 83, 063405 (2011).
[Crossref]

Czasch, A.

E. Gagnon, A. S. Sandhu, A. Paul, K. Hagen, A. Czasch, T. Jahnke, P. Ranitovic, C. Lewis Cocke, B. Walker, M. M. Murnane, and H. C. Kapteyn, “Time-resolved momentum imaging system for molecular dynamics studies using a tabletop ultrafast extreme-ultraviolet light source,” Rev. Sci. Instruments 79, 063102 (2008).
[Crossref]

Daboussi, S.

S. Kazamias, S. Daboussi, O. Guilbaud, K. Cassou, D. Ros, B. Cros, and G. Maynard, “Pressure-induced phase matching in high-order harmonic generation,” Phys. Rev. A 83, 063405 (2011).
[Crossref]

Dachraoui, H.

Davis, J.

B. Henke, E. Gullikson, and J. Davis, “X-ray interactions: photoabsorption, scattering, transmission, and reflection at E=50–30000 eV, Z=1–92,”; At. Data Nucl. Data Tables 54, 181–342 (1993).
[Crossref]

Delen, X.

Demmler, S.

Deng, Y.

M. Puppin, Y. Deng, C. W. Nicholson, J. Feldl, N. B. M. Schröter, H. Vita, P. S. Kirchmann, C. Monney, L. Rettig, M. Wolf, and R. Ernstorfer, “Time- and angle-resolved photoemission spectroscopy of solids in the extreme ultraviolet at 500 kHz repetition rate,” Rev. Sci. Instruments 90, 023104 (2019).
[Crossref]

Descamps, D.

A. Comby, S. Beaulieu, E. Constant, D. Descamps, S. Petit, and Y. Mairesse, “Absolute gas density profiling in high-order harmonic generation,” Opt. Express 26, 6001–6009 (2018).
[Crossref] [PubMed]

J. Higuet, H. Ruf, N. Thiré, R. Cireasa, E. Constant, E. Cormier, D. Descamps, E. Mével, S. Petit, B. Pons, Y. Mairesse, and B. Fabre, “High-order harmonic spectroscopy of the Cooper minimum in argon: experimental and theoretical study,” Phys. Rev. A 83, 053401 (2011).
[Crossref]

DiMauro, L. F.

P. Colosimo, G. Doumy, C. I. Blaga, J. Wheeler, C. Hauri, F. Catoire, J. Tate, R. Chirla, A. M. March, G. G. Paulus, H. G. Muller, P. Agostini, and L. F. DiMauro, “Scaling strong-field interactions towards the classical limit,” Nat. Phys. 4, 386–389 (2008).
[Crossref]

Dollar, F.

D. Popmintchev, C. Hernández-García, F. Dollar, C. Mancuso, J. A. Pérez-Hernández, M.-C. Chen, A. Hankla, X. Gao, B. Shim, A. L. Gaeta, M. Tarazkar, D. A. Romanov, R. J. Levis, J. A. Gaffney, M. Foord, S. B. Libby, A. Jaron-Becker, A. Becker, L. Plaja, M. M. Murnane, H. C. Kapteyn, and T. Popmintchev, “Ultraviolet surprise: efficient soft x-ray high-harmonic generation in multiply ionized plasmas,” Science 350, 1225–1231 (2015).
[Crossref]

Dörner, R.

R. Dörner, V. Mergel, O. Jagutzki, L. Spielberger, J. Ullrich, R. Moshammer, and H. Schmidt-Böcking, “Cold target recoil ion momentum spectroscopy: a ‘momentum microscope’ to view atomic collision dynamics,” Phys. Reports 330, 95–192 (2000).
[Crossref]

Dörre, N.

G. Porat, C. M. Heyl, S. B. Schoun, C. Benko, N. Dörre, K. L. Corwin, and J. Ye, “Phase-matched extreme-ultraviolet frequency-comb generation,” Nat. Photonics 12, 387–391 (2018).
[Crossref]

Dorrer, C.

E. Constant, D. Garzella, P. Breger, E. Mével, C. Dorrer, C. Le Blanc, F. Salin, and P. Agostini, “Optimizing High Harmonic Generation in Absorbing Gases: Model and Experiment,” Phys. Rev. Lett. 82, 1668–1671 (1999).
[Crossref]

Doumy, G.

P. Colosimo, G. Doumy, C. I. Blaga, J. Wheeler, C. Hauri, F. Catoire, J. Tate, R. Chirla, A. M. March, G. G. Paulus, H. G. Muller, P. Agostini, and L. F. DiMauro, “Scaling strong-field interactions towards the classical limit,” Nat. Phys. 4, 386–389 (2008).
[Crossref]

Drozdy, A.

Dubietis, A.

Dubrouil, A.

Eidam, T.

Elsmann, T.

Erk, B.

Ernstorfer, R.

M. Puppin, Y. Deng, C. W. Nicholson, J. Feldl, N. B. M. Schröter, H. Vita, P. S. Kirchmann, C. Monney, L. Rettig, M. Wolf, and R. Ernstorfer, “Time- and angle-resolved photoemission spectroscopy of solids in the extreme ultraviolet at 500 kHz repetition rate,” Rev. Sci. Instruments 90, 023104 (2019).
[Crossref]

Fabre, B.

J. Higuet, H. Ruf, N. Thiré, R. Cireasa, E. Constant, E. Cormier, D. Descamps, E. Mével, S. Petit, B. Pons, Y. Mairesse, and B. Fabre, “High-order harmonic spectroscopy of the Cooper minimum in argon: experimental and theoretical study,” Phys. Rev. A 83, 053401 (2011).
[Crossref]

J. Boullet, Y. Zaouter, J. Limpert, S. Petit, Y. Mairesse, B. Fabre, J. Higuet, E. Mével, E. Constant, and E. Cormier, “High-order harmonic generation at a megahertz-level repetition rate directly driven by an ytterbium-doped-fiber chirped-pulse amplification system,” Opt. Lett. 34, 1489–1491 (2009).
[Crossref] [PubMed]

Feldl, J.

M. Puppin, Y. Deng, C. W. Nicholson, J. Feldl, N. B. M. Schröter, H. Vita, P. S. Kirchmann, C. Monney, L. Rettig, M. Wolf, and R. Ernstorfer, “Time- and angle-resolved photoemission spectroscopy of solids in the extreme ultraviolet at 500 kHz repetition rate,” Rev. Sci. Instruments 90, 023104 (2019).
[Crossref]

Fermann, M. E.

A. Cingöz, D. C. Yost, T. K. Allison, A. Ruehl, M. E. Fermann, I. Hartl, and J. Ye, “Direct frequency comb spectroscopy in the extreme ultraviolet,” Nature 482, 68–71 (2012).
[Crossref] [PubMed]

Foord, M.

D. Popmintchev, C. Hernández-García, F. Dollar, C. Mancuso, J. A. Pérez-Hernández, M.-C. Chen, A. Hankla, X. Gao, B. Shim, A. L. Gaeta, M. Tarazkar, D. A. Romanov, R. J. Levis, J. A. Gaffney, M. Foord, S. B. Libby, A. Jaron-Becker, A. Becker, L. Plaja, M. M. Murnane, H. C. Kapteyn, and T. Popmintchev, “Ultraviolet surprise: efficient soft x-ray high-harmonic generation in multiply ionized plasmas,” Science 350, 1225–1231 (2015).
[Crossref]

Fraia, M. Di

Gaeta, A. L.

D. Popmintchev, C. Hernández-García, F. Dollar, C. Mancuso, J. A. Pérez-Hernández, M.-C. Chen, A. Hankla, X. Gao, B. Shim, A. L. Gaeta, M. Tarazkar, D. A. Romanov, R. J. Levis, J. A. Gaffney, M. Foord, S. B. Libby, A. Jaron-Becker, A. Becker, L. Plaja, M. M. Murnane, H. C. Kapteyn, and T. Popmintchev, “Ultraviolet surprise: efficient soft x-ray high-harmonic generation in multiply ionized plasmas,” Science 350, 1225–1231 (2015).
[Crossref]

Gaffney, J. A.

D. Popmintchev, C. Hernández-García, F. Dollar, C. Mancuso, J. A. Pérez-Hernández, M.-C. Chen, A. Hankla, X. Gao, B. Shim, A. L. Gaeta, M. Tarazkar, D. A. Romanov, R. J. Levis, J. A. Gaffney, M. Foord, S. B. Libby, A. Jaron-Becker, A. Becker, L. Plaja, M. M. Murnane, H. C. Kapteyn, and T. Popmintchev, “Ultraviolet surprise: efficient soft x-ray high-harmonic generation in multiply ionized plasmas,” Science 350, 1225–1231 (2015).
[Crossref]

Gagnon, E.

E. Gagnon, A. S. Sandhu, A. Paul, K. Hagen, A. Czasch, T. Jahnke, P. Ranitovic, C. Lewis Cocke, B. Walker, M. M. Murnane, and H. C. Kapteyn, “Time-resolved momentum imaging system for molecular dynamics studies using a tabletop ultrafast extreme-ultraviolet light source,” Rev. Sci. Instruments 79, 063102 (2008).
[Crossref]

Gao, X.

D. Popmintchev, C. Hernández-García, F. Dollar, C. Mancuso, J. A. Pérez-Hernández, M.-C. Chen, A. Hankla, X. Gao, B. Shim, A. L. Gaeta, M. Tarazkar, D. A. Romanov, R. J. Levis, J. A. Gaffney, M. Foord, S. B. Libby, A. Jaron-Becker, A. Becker, L. Plaja, M. M. Murnane, H. C. Kapteyn, and T. Popmintchev, “Ultraviolet surprise: efficient soft x-ray high-harmonic generation in multiply ionized plasmas,” Science 350, 1225–1231 (2015).
[Crossref]

Garzella, D.

E. Constant, D. Garzella, P. Breger, E. Mével, C. Dorrer, C. Le Blanc, F. Salin, and P. Agostini, “Optimizing High Harmonic Generation in Absorbing Gases: Model and Experiment,” Phys. Rev. Lett. 82, 1668–1671 (1999).
[Crossref]

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Other (1)

“SNLO nonlinear optics code available from A. V. Smith, AS-Photonics, Albuquerque, NM,”.

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Figures (6)

Fig. 1
Fig. 1 Scheme of the experimental setup. We generate the harmonics (2nd, 3rd and 4th) of the YDFA fundamental laser in BBO crystals. The upconverted beam is filtered by dichroic mirrors, magnified by a telescope, and focused in an argon gas jet. The spatially-resolved XUV spectrum is measured by an imaging spectrometer, and the absolute XUV flux is measured by a calibrated photodiode.
Fig. 2
Fig. 2 Measurement of the laser beam spatial profiles. (a) Focus of the ωL beam at 50 W average power, after a -100 mm/300 mm telescope and f=300 mm lens. (b) Focus of the 2ωL beam at 19 W after a -100 mm/300 mm telescope and f=300 mm lens. (c) Focus of the 3ωL beam at 7 W after a -100 mm/500 mm telescope and f=300 mm lens. (d) Near-Field of the 4ωL beam at 1.75 W after a -100 mm/500 mm telescope. (e) Beam waist measurement versus average power at 3ωL after a -100 mm/500 mm telescope (w1) and at focus (w0) with f=300 mm. (f) Beam waist measurement versus average power at 4ωL after a -100 mm/500 mm telescope (w1) and its projection on the x (wx) and y axis (wy).
Fig. 3
Fig. 3 (a)-(d) Spatially resolved high-harmonic spectrum generated in argon using a driving laser at 1,2,3 and 4ωL, with respective intensities of 1.5, 2.8, 3.4 and 1.6 × 1014 W.cm−2. The peak density in the generating medium is 4.5 × 1018 at./cm3 at ωL and 3.5 × 1018 at./cm3 at 2,3 and 4 ωL. The spectra at 1 and 2 ωL are recorded after reflection on two Nb2O5 plates. The spectra at 3 and 4 ωL are recorded after transmission through an Al filter.
Fig. 4
Fig. 4 (a) Transmission of the 157 nm Al filters used at different driving wavelengths. The filters used in each configuration are different. (b) XUV reflectivity after two Nb2O5 plates in s- and p- polarization at ~ 70° incidence angle.
Fig. 5
Fig. 5 (a) Intensity dependency of the total HHG efficiency at 1030 nm in two focusing conditions. The intensity was tuned by changing the laser energy. (b) Efficiency per harmonic at the highest power in the two focusing conditions.
Fig. 6
Fig. 6 (a) Intensity dependency of the total HHG efficiency at 1,2,3 and 4 ωL. The intensity was tuned by changing the laser energy at 1 and 2ωL, and was changed by setting different pinhole diameters at 3 and 4ωL. (b) Maximal flux at each harmonic generated from 1,2,3 and 4ωL beams. (c) Total efficiency for the detected harmonics as a function of generating frequency, at the interpolated intensity of 1.5 × 1014 W.cm−2. The dashed line is a power fit of the efficiency made from 1 to 3 ωL.

Tables (1)

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Table 1 Most Relevant XUV Photon Flux in Ar.

Equations (1)

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d P M = d 0 λ L 2 2 π 2 w 0 2 Δ δ ( 1 η / η c r i t )