Volume 87, Number 5, September 2009
|Number of page(s)||6|
|Section||Atomic, Molecular and Optical Physics|
|Published online||24 September 2009|
Femtosecond laser pulse shaping for enhanced ionization
Fritz Haber Institute of the Max Planck Society - Faradayweg 4-6, D-14195 Berlin, Germany, EU
2 Institut für Theoretische Physik and European Theoretical Spectroscopy Facility (ETSF), Freie Universität Berlin Arnimallee 14, D-14195 Berlin, Germany, EU
3 Instituto de Biocomputación y Física de Sistemas Complejos (BIFI) - Corona de Aragón 42, E-50009 Zaragoza, Spain, EU
4 Nanoscience Center, Department of Physics, University of Jyväskylä - FI-40014 Jyväskylä, Finland, EU
5 Nano-Bio Spectroscopy group and ETSF Scientific Development Centre, Departamento de Física de Materiales, Universidad del País Vasco, Centro de Física de Materiales CSIC-UPV/EHU-MPC and DIPC E-20018 San Sebastián, Spain, EU
6 Max Planck Institute of Microstructure Physics - Weinberg 2, D-06120 Halle, Germany, EU
Corresponding authors: email@example.com firstname.lastname@example.org
Accepted: 2 September 2009
We demonstrate how the shape of femtosecond laser pulses can be tailored in order to obtain maximal ionization of atoms or molecules. For that purpose, we have overlayed a direct-optimization scheme on top of a fully unconstrained computation of the three-dimensional time-dependent Schrödinger equation. The procedure looks for pulses that maintain the same total length and integrated intensity or fluence as a given pulse that serves as an initial guess. It allows, however, for changes in frequencies —within a certain, predefined range— and overall shape, leading to enhanced ionization. We illustrate the scheme by calculating ionization yields for the molecule when irradiated with short ( fs), high-intensity laser pulses. The magnitude of the obtained enhancement, as well as the shape of the solution optimal field depend strongly on the constrains imposed on the search space. In particular, when only small frequencies are allowed, the solution merely increases the peak intensity through temporal compression, as expected from a simple tunneling picture. If larger frequencies are allowed the structure of the solution field is more complicated.
PACS: 32.80.Qk – Coherent control of atomic interactions with photons / 32.80.Fb – Photoionization of atoms and ions / 31.15.ac – High-precision calculations for few-electron (or few-body) atomic systems
© EPLA, 2009
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