Strong-field short-pulse ionization of the molecular hydrogen ion
β Scribed by C.R. Mendez; J.R. Vazquez de Aldana; L. Plaja; L. Roso; A.M. Popov; O.V. Tikhonova; P.A. Volkov; E.A. Volkova
- Publisher
- John Wiley and Sons
- Year
- 2004
- Tongue
- English
- Weight
- 174 KB
- Volume
- 1
- Category
- Article
- ISSN
- 1612-2011
No coin nor oath required. For personal study only.
β¦ Synopsis
The strong-field molecular dynamics is studied by direct numerical integration of the non-stationary Schroedinger equation for laser pulses of femtosecond duration. The calculations are performed beyond the Born-Oppenheimer approximation with both electronic and rotational degrees of freedom being taken into account. The rotational dynamics is confirmed to play a significant role during molecular ionization. Nevertheless, a range of parameters is found that provide molecular ionization to be correctly described under assumption of "frozen" molecular axis orientation. Using this model the results of 3D electron dynamics of a molecule are obtained. For ultrashort pulses a 3D account of the electronic degrees of freedom is proved to provide a full description of the strong-field molecular behavior.
π SIMILAR VOLUMES
The Coulomb-repulsion compensation of classical nonrelativistic hydrogen ions in the beam in crossover in the presence of a strong pulsed laser field with an intensity of about 10^15^W/cm^2^is theoretically studied. It is demonstrated that the average effective interaction force can fundamentally di
Outside the framework of the dipole approximation (with an accuracy of about v/c) the effective interaction force between hydrogen ions, moving as paraxial beam in a pulsed field of two opposite laser waves directed parallel to beam, is theoretically studied. In the region of medial fields, when the
The liquid secondary ion mass spectrometry and electron impact ionization fragmentation pathways of 1,9bis(dimethylamino)-2,8-dimethoxy-dibenzofuran (l), a new proton-sponge base with increased steric compression (buttressing) and much higher basicity (pK, = 14.3), and of its monoprotonated (2) and