Strong Field Multiple Ionization as a Route to Electron Dynamics in a van der Waals Cluster

2013 ◽  
Vol 111 (8) ◽  
Author(s):  
J. Wu ◽  
X. Gong ◽  
M. Kunitski ◽  
F. K. Amankona-Diawuo ◽  
L. Ph. H. Schmidt ◽  
...  
2008 ◽  
Vol 10 (2) ◽  
pp. 025007 ◽  
Author(s):  
O Herrwerth ◽  
A Rudenko ◽  
M Kremer ◽  
V L B de Jesus ◽  
B Fischer ◽  
...  

2013 ◽  
Vol 139 (18) ◽  
pp. 184309 ◽  
Author(s):  
Vladimir S. Petrovic ◽  
Sebastian Schorb ◽  
Jaehee Kim ◽  
James White ◽  
James P. Cryan ◽  
...  

2019 ◽  
Vol 205 ◽  
pp. 04013
Author(s):  
Stanislav Yu. Kruchinin ◽  
Ferenc Krausz ◽  
Vladislav S. Yakovlev

We study the characteristic energy and time scales describing the coherent electron dynamics and decoherence phenomena in solids interacting with ultrashort laser pulses. Our analysis resulted in the derivation system of dimensionless adiabaticity parameters and derivation of the non-Markovian density-matrix equations applicable on arbitrary short timescales.


2002 ◽  
Vol 351 (1-2) ◽  
pp. 121-127 ◽  
Author(s):  
Susanne Ullrich ◽  
György Tarczay ◽  
Xin Tong ◽  
Mark S Ford ◽  
Caroline E.H Dessent ◽  
...  

2006 ◽  
Vol 125 (1) ◽  
pp. 014313 ◽  
Author(s):  
Álvaro Valdés ◽  
Rita Prosmiti ◽  
Pablo Villarreal ◽  
Gerardo Delgado-Barrio

2019 ◽  
Vol 205 ◽  
pp. 05002
Author(s):  
Christian Heide ◽  
Takuya Higuchi ◽  
Konrad Ullmann ◽  
Heiko B. Weber ◽  
Peter Hommelhoff

We demonstrate that currents induced in graphene by ultrashort laser pulses are sensitive to the exact shape of the electric-field waveform. By increasing the field strength, we found a transition of the light–matter interaction from the weak-field to the strong-field regime at around 2 V/nm, where intraband dynamics influence interband transitions. In this strong-field regime, the light-matter interaction can be described by the wavenumber trajectories of electrons in the reciprocal space. For linearly polarized light the electron dynamics are governed by repeated sub-optical-cycle Landau-Zener transitions between the valence- and conduction band, resulting in Landau-Zener-Stuckelberg interference, whereas for circular polarized light this interference is supressed.


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