Electron Imaging in Short-Pulse Strong Field Multiphoton Ionization

Author(s):  
V. Schyja ◽  
T. Lang ◽  
H. Helm
2017 ◽  
Vol 187 (11) ◽  
pp. 1280-1287 ◽  
Author(s):  
Leonid V. Keldysh

Author(s):  
Leonard Doyle ◽  
Pooyan Khademi ◽  
Peter Hilz ◽  
Alexander Sävert ◽  
Georg Schaefer ◽  
...  

Abstract High power short pulse lasers provide a promising route to study the strong field effects of the quantum vacuum, for example by direct photon-photon scattering in the all-optical regime. Theoretical predictions based on realistic laser parameters achievable today or in the near future predict scattering of a few photons with colliding Petawatt laser pulses, requiring single photon sensitive detection schemes and very good spatio-temporal filtering and background suppression. In this article, we present experimental investigations of this photon background by employing only a single high power laser pulse tightly focused in residual gas of a vacuum chamber. The focal region was imaged onto a single-photon sensitive, time gated camera. As no detectable quantum vacuum signature was expected in our case, the setup allowed for characterization and first mitigation of background contributions. For the setup employed, scattering off surfaces of imperfect optics dominated below the residual gas pressures of 1×10-4mbar. Extrapolation of the findings to intensities relevant for photon-photon scattering studies is discussed.


2011 ◽  
Vol 28 (8) ◽  
pp. 083201 ◽  
Author(s):  
Hui-Peng Kang ◽  
Chuan-Liang Wang ◽  
Zhi-Yang Lin ◽  
Yong-Ju Chen ◽  
Ming-Yan Wu ◽  
...  

2012 ◽  
Vol 85 (5) ◽  
Author(s):  
A. K. Kazansky ◽  
A. V. Grigorieva ◽  
N. M. Kabachnik

1999 ◽  
Vol 18 (3) ◽  
pp. 129-142 ◽  
Author(s):  
E. Koudoumas ◽  
R. De Nalda ◽  
C. Fotakis ◽  
S. Couris

The interaction of CS2 with intense short pulse laser radiation is studied, experimentally using time-of-flight mass spectroscopy. Laser pulses of 0.5 and 5 psec at 248 and 496 nm have been used in order to investigate the effect of the wavelength and the pulse duration on the molecular ionization and fragmentation. As shown, for low enough intensities the parent molecular ion is present as the most important peak in all cases. Increasing the intensity results in extensive fragmentation, where the molecular parent ion remains always the more intense mass peak at 496 nm while at 248 nm S+ dominates the mass spectra. Finally, the production of multiply charged fragments is more efficient at the longer wavelength used.


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