Photoelectron holography of atomic targets
We study the spatial interference effects appearing during the ionization of atoms (H, He, Ne, and Ar) by few-cycle laser pulses using single-electron ab initio calculations. The spatial interference is the result of the coherent superposition of the electronic wave packets created during one half c...
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American Physical Society
2019
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Acceso en línea: | Registro en Scopus DOI Handle Registro en la Biblioteca Digital |
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LEADER | 09585caa a22011417a 4500 | ||
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001 | PAPER-25763 | ||
003 | AR-BaUEN | ||
005 | 20240930121104.0 | ||
008 | 190410s2019 xx ||||fo|||| 00| 0 eng|d | ||
024 | 7 | |2 scopus |a 2-s2.0-85060141185 | |
040 | |a Scopus |b spa |c AR-BaUEN |d AR-BaUEN | ||
100 | 1 | |a Borbély, S. | |
245 | 1 | 0 | |a Photoelectron holography of atomic targets |
260 | |b American Physical Society |c 2019 | ||
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506 | |2 openaire |e Política editorial | ||
520 | 3 | |a We study the spatial interference effects appearing during the ionization of atoms (H, He, Ne, and Ar) by few-cycle laser pulses using single-electron ab initio calculations. The spatial interference is the result of the coherent superposition of the electronic wave packets created during one half cycle of the driving field following different spatial paths. This spatial interference pattern may be interpreted as the hologram of the target atom. With the help of a wave-function analysis (splitting) technique and approximate (strong-field and Coulomb-Volkov) calculations, we directly show that the hologram is the result of the electronic-wave-packet scattering on the parent ion. On the He target we demonstrate the usefulness of the wave-function splitting technique in the disentanglement of different interference patterns. Further, by performing calculations for the different targets, we show that the pattern of the hologram does not depend on the angular symmetry of the initial state and it is strongly influenced by the atomic species of the target: A deeper bounding potential leads to a denser pattern. © 2019 American Physical Society. |l eng | |
536 | |a Detalles de la financiación: Office of Research, Innovation and Economic Development, California State Polytechnic University, Pomona | ||
536 | |a Detalles de la financiación: Nemzeti Kutatási Fejlesztési és Innovációs Hivatal | ||
536 | |a Detalles de la financiación: D.G.A. acknowledges Grant No. PICT-2016-2096 of ANPCyT (Argentina). K.T. and L.N. acknowledge support from the National Research, Development and Innovation Office (NKFIH) Grant No. KH 126886. The numerical calculations were performed using the high performance computing resources of Babeş-Bolyai University. | ||
593 | |a Faculty of Physics, Babeş-Bolyai University, Cluj-Napoca, 400084, Romania | ||
593 | |a ELI-ALPS, ELI-HU Nonprofit Ltd., Dugonics tér 13, Szeged, H-6720, Hungary | ||
593 | |a Institute for Astronomy and Space Physics IAFE (CONICET-UBA), Buenos Aires, 1428, Argentina | ||
593 | |a Institute for Nuclear Research, Hungarian Academy of Sciences (ATOMKI), P.O. Box 51, Debrecen, H-4001, Hungary | ||
690 | 1 | 0 | |a ARGON LASERS |
690 | 1 | 0 | |a ATOM LASERS |
690 | 1 | 0 | |a ATOMS |
690 | 1 | 0 | |a CALCULATIONS |
690 | 1 | 0 | |a WAVE FUNCTIONS |
690 | 1 | 0 | |a WAVE PACKETS |
690 | 1 | 0 | |a AB INITIO CALCULATIONS |
690 | 1 | 0 | |a COHERENT SUPERPOSITIONS |
690 | 1 | 0 | |a ELECTRONIC WAVE PACKETS |
690 | 1 | 0 | |a FEW-CYCLE LASER PULSE |
690 | 1 | 0 | |a INTERFERENCE PATTERNS |
690 | 1 | 0 | |a PHOTOELECTRON HOLOGRAPHIES |
690 | 1 | 0 | |a SPATIAL INTERFERENCE |
690 | 1 | 0 | |a SPATIAL INTERFERENCE PATTERNS |
690 | 1 | 0 | |a HOLOGRAMS |
700 | 1 | |a Tóth, A. | |
700 | 1 | |a Arbó, Diego Gabriel | |
700 | 1 | |a Tokési, K. | |
700 | 1 | |a Nagy, L. | |
773 | 0 | |d American Physical Society, 2019 |g v. 99 |k n. 1 |p Phys. Rev. A |x 24699926 |t Physical Review A | |
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