Diffraction at a time grating in above-threshold ionization: The influence of the Coulomb potential

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We analyze the photoelectron emission spectrum in atomic above-threshold ionization by a linearly polarized short-laser pulse. Direct electrons can be characterized by both intracycle and intercycle interferences. The former results from the coherent superposition of two different electron trajector...

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Autor principal: Arbó, Diego Gabriel
Otros Autores: Ishikawa, K.L, Schiessl, K., Persson, E., Burgdörfer, J.
Formato: Capítulo de libro
Lenguaje:Inglés
Publicado: 2010
Acceso en línea:Registro en Scopus
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Biblioteca Central Dr. Luis F. Leloir (FCEN) de Universidad de Buenos Aires
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100 1 |a Arbó, Diego Gabriel 
245 1 0 |a Diffraction at a time grating in above-threshold ionization: The influence of the Coulomb potential 
260 |c 2010 
270 1 0 |m Arbó, D. G.; Institute for Astronomy and Space Physics, IAFE (CONICET-UBA), CC 67, Suc. 28 (1428) Buenos Aires, Argentina 
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506 |2 openaire  |e Política editorial 
520 3 |a We analyze the photoelectron emission spectrum in atomic above-threshold ionization by a linearly polarized short-laser pulse. Direct electrons can be characterized by both intracycle and intercycle interferences. The former results from the coherent superposition of two different electron trajectories released in the same optical cycle, whereas the latter is the consequence of the superposition of multiple trajectories released in different cycles. In the present article, a semiclassical analytical expression for the complete (both intracycle and intercycle) interference pattern is derived. We show that the recently proposed semiclassical description in terms of a diffraction process at a time grating remains qualitatively unchanged in the presence of the long-range Coulomb potential. The latter causes only a phase shift of the intracycle interference pattern. We verify the predictions of the semiclassical model by comparison with full three-dimensional (3D) time-dependent Schrödinger equation (TDSE) solutions. One key finding is that the subcycle interference structures originating from trajectories launched within a time interval of less than 1 femtosecond should be experimentally observable also in low-resolution spectra for longer multicycle pulses. © 2010 The American Physical Society.  |l eng 
593 |a Institute for Astronomy and Space Physics, IAFE (CONICET-UBA), CC 67, Suc. 28 (1428) Buenos Aires, Argentina 
593 |a Department of Physics, FCEN, University of Buenos Aires, Argentina 
593 |a Photon Science Center, Graduate School of Engineering, University of Tokyo, Hongo 7-3-1, Bunkyo-ku, Tokyo 113-8656, Japan 
593 |a Institute for Theoretical Physics, Vienna University of Technology, Wiedner Hauptstraße 8-10/136, A-1040 Vienna, Austria 
690 1 0 |a ABOVE-THRESHOLD IONIZATION 
690 1 0 |a ANALYTICAL EXPRESSIONS 
690 1 0 |a COHERENT SUPERPOSITIONS 
690 1 0 |a COULOMB POTENTIAL 
690 1 0 |a DIFFRACTION PROCESS 
690 1 0 |a DINGER EQUATION 
690 1 0 |a ELECTRON TRAJECTORIES 
690 1 0 |a FEMTOSECONDS 
690 1 0 |a INTERFERENCE PATTERNS 
690 1 0 |a INTERFERENCE STRUCTURES 
690 1 0 |a LINEARLY POLARIZED 
690 1 0 |a MULTI-CYCLE PULSE 
690 1 0 |a OPTICAL CYCLES 
690 1 0 |a PHOTO-ELECTRON EMISSION 
690 1 0 |a RESOLUTION SPECTRA 
690 1 0 |a SEMICLASSICAL MODEL 
690 1 0 |a SHORT LASER PULSE 
690 1 0 |a SUB-CYCLE 
690 1 0 |a THREE-DIMENSIONAL (3D) 
690 1 0 |a TIME INTERVAL 
690 1 0 |a TIME-DEPENDENT 
690 1 0 |a ATOMIC SPECTROSCOPY 
690 1 0 |a COULOMB BLOCKADE 
690 1 0 |a DIFFRACTION 
690 1 0 |a ELECTRIC FIELDS 
690 1 0 |a EMISSION SPECTROSCOPY 
690 1 0 |a IONIZATION POTENTIAL 
690 1 0 |a PHOTOELECTRON SPECTROSCOPY 
690 1 0 |a PHOTOIONIZATION 
690 1 0 |a TRAJECTORIES 
690 1 0 |a THREE DIMENSIONAL 
700 1 |a Ishikawa, K.L. 
700 1 |a Schiessl, K. 
700 1 |a Persson, E. 
700 1 |a Burgdörfer, J. 
773 0 |d 2010  |g v. 82  |k n. 4  |p Phys Rev A  |x 10502947  |t Physical Review A - Atomic, Molecular, and Optical Physics 
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