Steering Attosecond Electron Wave Packets with Light

Author:

Kienberger R.1,Hentschel M.1,Uiberacker M.1,Spielmann Ch.12,Kitzler M.1,Scrinzi A.1,Wieland M.3,Westerwalbesloh Th.4,Kleineberg U.4,Heinzmann U.4,Drescher M.4,Krausz F.1

Affiliation:

1. Institut für Photonik, Technische Universität Wien, Gusshausstr. 27, A-1040 Wien, Austria.

2. Physikalisches Institut EP1, Universität Würzburg, Am Hubland, D-97074 Würzburg, Germany.

3. Fachhochschule Koblenz, RheinAhrCampus Remagen, Südallee 2, D-53424 Remagen, Germany.

4. Fakultät für Physik, Universität Bielefeld, D-33615 Bielefeld, Germany.

Abstract

Photoelectrons excited by extreme ultraviolet or x-ray photons in the presence of a strong laser field generally suffer a spread of their energies due to the absorption and emission of laser photons. We demonstrate that if the emitted electron wave packet is temporally confined to a small fraction of the oscillation period of the interacting light wave, its energy spectrum can be up- or downshifted by many times the laser photon energy without substantial broadening. The light wave can accelerate or decelerate the electron's drift velocity, i.e., steer the electron wave packet like a classical particle. This capability strictly relies on a sub-femtosecond duration of the ionizing x-ray pulse and on its timing to the phase of the light wave with a similar accuracy, offering a simple and potentially single-shot diagnostic tool for attosecond pump-probe spectroscopy.

Publisher

American Association for the Advancement of Science (AAAS)

Subject

Multidisciplinary

Reference33 articles.

1. Direct Observation of Multiphoton Processes in Laser-Induced Free-Free Transitions

2. Investigations of above-threshold ionization using subpicosecond laser pulses

3. Observation of Laser-Assisted Auger Decay in Argon

4. Observation of Laser Assisted Photoelectric Effect and Femtosecond High Order Harmonic Radiation

5. This applies in the nonrelativistic limit for interaction times short enough to prevent the electron from traveling distances comparable to or larger than the light wavelength during the interaction (dipole approximation). These conditions are fulfilled by femtosecond pulses of visible light at intensities below 10 18 W/cm 2 . In this intensity regime of interactions ponderomotive effects provide the only means of affecting electron motion by light. For ultrashort (<1 ps) pulse durations electrons released into a strong field lose energy equal to the ponderomotive potential of the laser which is transferred into a blue shift of the radiation (6). The ponderomotive potential of long pulses on the other hand is capable of modifying the momentum of free electrons (7).

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