Intra- and intercycle interference of angle-resolved electron emission in laser-assisted XUV atomic ionization
A theoretical study of ionization of the hydrogen atom due to an XUV pulse in the presence of an infrared (IR) laser is presented. Well-established theories are usually used to describe the laser-assisted photoelectron effect: the well-known soft-photon approximation firstly posed by Maquet et al (2...
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Institute of Physics Publishing
2018
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001 | PAPER-25246 | ||
003 | AR-BaUEN | ||
005 | 20240930121420.0 | ||
008 | 190410s2018 xx ||||fo|||| 00| 0 eng|d | ||
024 | 7 | |2 scopus |a 2-s2.0-85045672149 | |
030 | |a JPAPE | ||
040 | |a Scopus |b spa |c AR-BaUEN |d AR-BaUEN | ||
100 | 1 | |a Gramajo, A.A. | |
245 | 1 | 0 | |a Intra- and intercycle interference of angle-resolved electron emission in laser-assisted XUV atomic ionization |
260 | |b Institute of Physics Publishing |c 2018 | ||
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506 | |2 openaire |e Política editorial | ||
520 | 3 | |a A theoretical study of ionization of the hydrogen atom due to an XUV pulse in the presence of an infrared (IR) laser is presented. Well-established theories are usually used to describe the laser-assisted photoelectron effect: the well-known soft-photon approximation firstly posed by Maquet et al (2007 J. Mod. Opt. 54 1847) and Kazansky's theory in (2010 Phys. Rev. A 82, 033420). However, these theories completely fail to predict the electron emission perpendicularly to the polarization direction. Making use of a semiclassical model (SCM), we study the angle-resolved energy distribution of PEs for the case that both fields are linearly polarized in the same direction. We thoroughly analyze and characterize two different emission regions in the angle-energy domain: (i) the parallel-like region with contribution of two classical trajectories per optical cycle and (ii) the perpendicular-like region with contribution of four classical trajectories per optical cycle. We show that our SCM is able to assess the interference patterns of the angle-resolved PE spectrum in the two different mentioned regions. Electron trajectories stemming from different optical laser cycles give rise to angle-independent intercycle interferences known as sidebands. These sidebands are modulated by an angle-dependent coarse-grained structure coming from the intracycle interference of the electron trajectories born during the same optical cycle. We show the accuracy of our SCM as a function of the time delay between the IR and the XUV pulses and also as a function of the laser intensity by comparing the semiclassical predictions of the angle-resolved PE spectrum with the continuum-distorted wave strong field approximation and the ab initio solution of the time-dependent Schrödinger equation. © 2018 IOP Publishing Ltd. |l eng | |
536 | |a Detalles de la financiación: Universidad de Buenos Aires, UBACyT 20020130100617BA | ||
536 | |a Detalles de la financiación: UNCuyo 06/C487 | ||
536 | |a Detalles de la financiación: PIP0386, PIP0513, PICT-2014-2363, PICT 2016-0296 | ||
536 | |a Detalles de la financiación: Agencia Nacional de Promoción Científica y Tecnológica | ||
536 | |a Detalles de la financiación: Work supported by CONICET PIP0386 and PIP0513, PICT-2014-2363 and PICT 2016-0296 of ANPCyT (Argentina), the University of Cuyo (UNCuyo 06/C487) and the University of Buenos Aires (UBACyT 20020130100617BA). | ||
593 | |a CONICET, Centro Atómico Bariloche (CNEA), Bariloche, 8400, Argentina | ||
593 | |a Institute of Astronomy and Space Physics IAFE (CONICET-UBA), CC 67, Suc. 28, Buenos Aires, C1428ZAA, Argentina | ||
690 | 1 | 0 | |a ANGLE-RESOLVED PHOTOELECTRON SPECTRA |
690 | 1 | 0 | |a INTRA- AND INTERCYCLE INTERFERENCES |
690 | 1 | 0 | |a LASER-ASSITED PHOTOELECTRIC EFFECT |
690 | 1 | 0 | |a SEMICLASSICAL MODEL |
690 | 1 | 0 | |a XUV+IR MULTIPHOTON IONIZATION |
690 | 1 | 0 | |a ATOM LASERS |
690 | 1 | 0 | |a ATOMS |
690 | 1 | 0 | |a DISTORTION (WAVES) |
690 | 1 | 0 | |a PHOTOELECTRICITY |
690 | 1 | 0 | |a PHOTOELECTRON SPECTROSCOPY |
690 | 1 | 0 | |a PHOTOELECTRONS |
690 | 1 | 0 | |a PHOTOIONIZATION |
690 | 1 | 0 | |a PHOTONS |
690 | 1 | 0 | |a POLARIZATION |
690 | 1 | 0 | |a TRAJECTORIES |
690 | 1 | 0 | |a ANGLE-RESOLVED PHOTOELECTRON SPECTRA |
690 | 1 | 0 | |a COARSE-GRAINED STRUCTURE |
690 | 1 | 0 | |a CONTINUUM DISTORTED WAVES |
690 | 1 | 0 | |a INTRA- AND INTERCYCLE INTERFERENCES |
690 | 1 | 0 | |a INTRACYCLE INTERFERENCES |
690 | 1 | 0 | |a MULTIPHOTON IONIZATION |
690 | 1 | 0 | |a SEMICLASSICAL MODEL |
690 | 1 | 0 | |a STRONG-FIELD APPROXIMATIONS |
690 | 1 | 0 | |a ELECTRON EMISSION |
700 | 1 | |a Picca, R.D. | |
700 | 1 | |a López, S.D. | |
700 | 1 | |a Arbó, Diego Gabriel | |
773 | 0 | |d Institute of Physics Publishing, 2018 |g v. 51 |k n. 5 |p J Phys B At Mol Opt Phys |x 09534075 |w (AR-BaUEN)CENRE-332 |t Journal of Physics B: Atomic, Molecular and Optical Physics | |
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963 | |a VARI |