Simulation of the interaction of intense ultrashort X-ray laser pulses with micro-sized Al targets
We study the interaction of extremely short and high-intensity X-ray pulses with a 1.0μm thick Al foil. Four pulse lengths – 100 fs, 200 fs, 300 fs, and 400 fs – are considered. The photon energy is 1830 eV and the pulse intensity is 1017W/cm2. The interaction dynamics are calculated via a radiation...
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doaj-d2eccb11618746de891bdd2fb0c834272021-05-06T04:23:33ZengElsevierResults in Physics2211-37972021-05-0124104097Simulation of the interaction of intense ultrashort X-ray laser pulses with micro-sized Al targetsMohammed Shihab0Yasmine Adel1Nabil M. El-Siragy2Tanta University, Faculty of Science, Physics Department, Tanta 31527, Egypt; Academy of Scientific Research and Technology (ASRT), Cairo, EgyptTanta University, Faculty of Science, Physics Department, Tanta 31527, EgyptTanta University, Faculty of Science, Physics Department, Tanta 31527, EgyptWe study the interaction of extremely short and high-intensity X-ray pulses with a 1.0μm thick Al foil. Four pulse lengths – 100 fs, 200 fs, 300 fs, and 400 fs – are considered. The photon energy is 1830 eV and the pulse intensity is 1017W/cm2. The interaction dynamics are calculated via a radiation hydrodynamic code. The X-ray laser pulse heats the target isochorically. It generates a homogeneous hot dense matter; electrons are hotter than ions. The simulation of the interaction of pump and probe pulses with a delay time in the fs scale provides that the probe pulse heats the target significantly. A Monte-Carlo method is used to provide a microscopic description; the electron distribution function shows a two-temperature system. The electron distribution has spikes at the energy difference between the k-edges of Al ions and the energy of incident photons. The energies of these spikes depend on the considered ionization depression model. The Chihara formula and the non-equilibrium random phase approximation are utilized to calculate the X-ray Thomson scattering spectrum (XRTS). For collective scattering, the plasmon peaks are a function of the pulse lengths and the electron distribution function. Therefore, when XRTS is fitted to a measured spectrum may give the target density, the target temperature, and the microscopic electron distribution function.http://www.sciencedirect.com/science/article/pii/S2211379721002540 |
collection |
DOAJ |
language |
English |
format |
Article |
sources |
DOAJ |
author |
Mohammed Shihab Yasmine Adel Nabil M. El-Siragy |
spellingShingle |
Mohammed Shihab Yasmine Adel Nabil M. El-Siragy Simulation of the interaction of intense ultrashort X-ray laser pulses with micro-sized Al targets Results in Physics |
author_facet |
Mohammed Shihab Yasmine Adel Nabil M. El-Siragy |
author_sort |
Mohammed Shihab |
title |
Simulation of the interaction of intense ultrashort X-ray laser pulses with micro-sized Al targets |
title_short |
Simulation of the interaction of intense ultrashort X-ray laser pulses with micro-sized Al targets |
title_full |
Simulation of the interaction of intense ultrashort X-ray laser pulses with micro-sized Al targets |
title_fullStr |
Simulation of the interaction of intense ultrashort X-ray laser pulses with micro-sized Al targets |
title_full_unstemmed |
Simulation of the interaction of intense ultrashort X-ray laser pulses with micro-sized Al targets |
title_sort |
simulation of the interaction of intense ultrashort x-ray laser pulses with micro-sized al targets |
publisher |
Elsevier |
series |
Results in Physics |
issn |
2211-3797 |
publishDate |
2021-05-01 |
description |
We study the interaction of extremely short and high-intensity X-ray pulses with a 1.0μm thick Al foil. Four pulse lengths – 100 fs, 200 fs, 300 fs, and 400 fs – are considered. The photon energy is 1830 eV and the pulse intensity is 1017W/cm2. The interaction dynamics are calculated via a radiation hydrodynamic code. The X-ray laser pulse heats the target isochorically. It generates a homogeneous hot dense matter; electrons are hotter than ions. The simulation of the interaction of pump and probe pulses with a delay time in the fs scale provides that the probe pulse heats the target significantly. A Monte-Carlo method is used to provide a microscopic description; the electron distribution function shows a two-temperature system. The electron distribution has spikes at the energy difference between the k-edges of Al ions and the energy of incident photons. The energies of these spikes depend on the considered ionization depression model. The Chihara formula and the non-equilibrium random phase approximation are utilized to calculate the X-ray Thomson scattering spectrum (XRTS). For collective scattering, the plasmon peaks are a function of the pulse lengths and the electron distribution function. Therefore, when XRTS is fitted to a measured spectrum may give the target density, the target temperature, and the microscopic electron distribution function. |
url |
http://www.sciencedirect.com/science/article/pii/S2211379721002540 |
work_keys_str_mv |
AT mohammedshihab simulationoftheinteractionofintenseultrashortxraylaserpulseswithmicrosizedaltargets AT yasmineadel simulationoftheinteractionofintenseultrashortxraylaserpulseswithmicrosizedaltargets AT nabilmelsiragy simulationoftheinteractionofintenseultrashortxraylaserpulseswithmicrosizedaltargets |
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