Ionization of the hydrogen atom by short half-cycle pulses: Dependence on the pulse duration

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A theoretical study of the ionization of hydrogen atoms by short external half-cycle pulses (HCPs) as a function of the pulse duration, using different quantum and classical approaches, is presented. Total ionization probability and energy distributions of ejected electrons are calculated in the fra...

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Detalles Bibliográficos
Autor principal: Arbó, Diego Gabriel
Otros Autores: Gravielle, M.S, Dimitriou, K.I, Tókési, K., Borbély, S., Miraglia, J.E
Formato: Capítulo de libro
Lenguaje:Inglés
Publicado: 2010
Acceso en línea:Registro en Scopus
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Aporte de:Registro referencial: Solicitar el recurso aquí
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100 1 |a Arbó, Diego Gabriel 
245 1 0 |a Ionization of the hydrogen atom by short half-cycle pulses: Dependence on the pulse duration 
260 |c 2010 
270 1 0 |m Arbó, D. G.; Institute for Astronomy and Space Physics, IAFE, CC 67, Suc. 28 (1428), Buenos Aires, Argentina 
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506 |2 openaire  |e Política editorial 
520 3 |a A theoretical study of the ionization of hydrogen atoms by short external half-cycle pulses (HCPs) as a function of the pulse duration, using different quantum and classical approaches, is presented. Total ionization probability and energy distributions of ejected electrons are calculated in the framework of the singly-distorted Coulomb-Volkov (SDCV) and the doubly-distorted Coulomb-Volkov (DDCV) approximations. We also performed quasiclassical calculations based on a classical trajectory Monte Carlo method which includes the possibility of tunneling (CTMC-T). Quantum and classical results are compared to the numerical solution of the time-dependent Schrödinger equation (TDSE). We find that for high momentum transfers the DDCV shows an improvement compared to the SDCV, especially in the low-energy region of the electron emission spectra, where SDCV fails. In addition, DDCV reproduces successfully the TDSE electron energy distributions at weak momentum transfers. CTMC-T results reveal the importance of tunneling in the ionization process for relative long pulses and strong momentum transfers but fails to overcome the well-known classical suppression observed for weak electric fields. © EDP Sciences, Societá Italiana di Fisica, Springer-Verlag 2010.  |l eng 
593 |a Institute for Astronomy and Space Physics, IAFE, CC 67, Suc. 28 (1428), Buenos Aires, Argentina 
593 |a Department of Physics, FCEN, University of Buenos Aires, Argentina 
593 |a Department of Physical Science and Applications, Hellenic Army Academy, Vari, Greece 
593 |a Department of Informatics, Technological Educational Institution, Lamia, Greece 
593 |a Institute of Theoretical and Chemical Physics, National Hellenic Research Foundation, Athens, Greece 
593 |a Institute of Nuclear Research of the Hungarian Academy of Science, ATOMKI, PO Box 51, 4001 Debrecen, Hungary 
593 |a Faculty of Physics, Babes-Bolyai University, Cluj-Napoca, Romania 
700 1 |a Gravielle, M.S. 
700 1 |a Dimitriou, K.I. 
700 1 |a Tókési, K. 
700 1 |a Borbély, S. 
700 1 |a Miraglia, J.E. 
773 0 |d 2010  |g v. 59  |h pp. 193-200  |k n. 2  |p Eur. Phys. J. D  |x 14346060  |t European Physical Journal D 
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