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Phys. Rev. A 72, 023409 (2005) [8 pages]

  Photoionization of helium atoms irradiated with intense vacuum ultraviolet free-electron laser light. Part I. Experimental study of multiphoton and single-photon processes

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T. Laarmann1,*, A. R. B. de Castro2, P. Gürtler1, W. Laasch1, J. Schulz1,†, H. Wabnitz1,‡, and T. Möller1,§
1Hamburger Synchrotronstrahlungslabor HASYLAB at Deutsches Elektronen Synchrotron DESY, Notkestr. 85, 22607 Hamburg, Germany
2Laboratorio Nacional de Luz Sincrotron LNLS 13084-971 Campinas SP, Brazil and Instituto de Fisica Gleb Wataghin, Universidade Estadual de Campinas IFGW-UNICAMP 13083-970 Campinas SP, Brazil

Received 30 August 2004; published 15 August 2005

The interaction of He atoms with intense vacuum-ultraviolet light of a free-electron laser is investigated using time-of-flight mass spectroscopy and photoelectron spectroscopy. The atoms were irradiated with 100 fs pulses at 95 nm wavelength, which corresponds to ∼13 eV photon energy. The ionization of He atoms is observed at a peak intensity of 1010–1013 W∕cm2, which is due both to nonlinear multiphoton ionization with the fundamental wavelength and single-photon ionization with third harmonic radiation of the free-electron laser. The observation of two sharp photoelectron peaks in the kinetic energy spectra, that are separated by the photon energy, is in agreement with the numerical solution of the time-dependent Schrödinger equation. The calculation was done using the fully quantized field and a limited but representative set of basis states. The ionization rate dependence on the laser peak intensity indicates that: (a) The low-energy peak in the photoelectron spectra is mainly due to two-photon absorption of the fundamental, but (b) the high-energy peak at 15.4 eV is probably due to third harmonic FEL radiation. The theoretically predicted contribution from three-photon absorption of the fundamental is of about the same order of magnitude and could not be separated from the third harmonic background signal. Particularly, the photoelectron spectra and He+ time-of-flight data give evidence that the intensity of third harmonic light is high enough to perform single-shot spectroscopy on gas phase samples.

© 2005 The American Physical Society

URL:
http://link.aps.org/doi/10.1103/PhysRevA.72.023409
DOI:
10.1103/PhysRevA.72.023409
PACS:
42.50.Hz, 33.60.Cv, 32.80.Rm

*Present address: Max-Born-Institute, Max-Born Str. 2a, D-12489 Berlin, Germany. Electronic address: tim.laarmann@desy.de

†Present address: MAX-lab, Box 118, 22100 Lund, Sweden.

‡Present address: CEA-SPAM, Bât. 522, Centre d’Etudes de Saclay, 91191 Gif-sur-Yvette, France.

§Present address: Technische Universität Berlin, Hardenbergstr. 36, D-10623 Berlin, Germany.

See Also

Comment: T. Laarmann, A. R. de Castro, P. Gürtler, W. Laasch, J. Schulz, H. Wabnitz, and T. Möller, Reply to “Comment on ‘Photoionization of helium atoms irradiated with intense vacuum ultraviolet free-electron laser light. Part I. Experimental study of multiphoton and single-photon processes’ ”, Phys. Rev. A 74, 037402 (2006).

Comment: Dimitrios Charalambidis, P. Tzallas, N. A. Papadogiannis, L. A. Nikolopoulos, E. P. Benis, and G. D. Tsakiris, Comment on “Photoionization of helium atoms irradiated with intense vacuum ultraviolet free-electron laser light. Part I. Experimental study of multiphoton and single-photon processes”, Phys. Rev. A 74, 037401 (2006).

 
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