2011
DOI: 10.1016/j.hedp.2011.04.001
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Two-color Thomson scattering at FLASH

Abstract: We propose a two-color pump-probe Thomson scattering experiment at the FLASH facility in Hamburg to characterize warm dense matter states. The fundamental free electron laser wavelength of 40.5 nm is used to pump a liquid hydrogen jet that is subsequently probed with the third harmonic at 13.5 nm. We have considered the laser-target interaction in the pump and probe phase by using the radiation hydrodynamics code HELIOS. The calculation of the Thomson scattering spectrum is based on the Chihara formula which i… Show more

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Cited by 13 publications
(8 citation statements)
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“…Leaving the static ion structure factor S ii (k) as a free fit parameter, an ionization degree Ion feature (brown) in warm dense lithium at T = 4.5 eV and ρ = 0.6 g/cm 3 with the total form factor N (k) (blue), atomic form factor f (k) (red), and the form factor of screening electrons q(k) (green) from DFT-MD simulations (solid line) compared with the values from [27] (boxes) and analytical calculations. The influence of the ionization degree, assuming Z f = 1.0 (dashed line) and Z f = 1.35 (dotted line) is shown within the analytical results using Debye-Hückel theory [55] for q(k) and hydrogen-like wave functions [56] for f (k). We compare also with f (k) for Li + from HartreeFock [57] (dash-dotted).…”
Section: Comparison With Xrts Experiments On Wdmmentioning
confidence: 78%
“…Leaving the static ion structure factor S ii (k) as a free fit parameter, an ionization degree Ion feature (brown) in warm dense lithium at T = 4.5 eV and ρ = 0.6 g/cm 3 with the total form factor N (k) (blue), atomic form factor f (k) (red), and the form factor of screening electrons q(k) (green) from DFT-MD simulations (solid line) compared with the values from [27] (boxes) and analytical calculations. The influence of the ionization degree, assuming Z f = 1.0 (dashed line) and Z f = 1.35 (dotted line) is shown within the analytical results using Debye-Hückel theory [55] for q(k) and hydrogen-like wave functions [56] for f (k). We compare also with f (k) for Li + from HartreeFock [57] (dash-dotted).…”
Section: Comparison With Xrts Experiments On Wdmmentioning
confidence: 78%
“…The contribution of bound electrons is given by the ion structure factor S ii weighted by the form factor f i (k) of tightly bound electrons and the screening function q(k) of weakly bound electrons. The screening cloud and the ion structure factor are evaluated via the Debye-Hückel theory, whereas the form factor is approximated using hydrogenic wave functions [40]. Finally, electron ionization during the scattering event is given by the bound-free structure factor S c (k, ω) which is modulated by the ion movement S s [41].…”
Section: Theory Of the Dynamic Structure Factormentioning
confidence: 99%
“…For the calculation of the second term in the Chihara formula (2) which characterizes the scattering on bound electrons, we use the atomic form factor f i (k) [24] and the simple Debye-Hückel ion-ion structure factor for point charges [25] S ii (k) = k 2 + κ 2 e k 2 + κ 2 i + κ 2 e (5) with the inverse screening length κ c = e 2 c n c /( 0 k B T c ) for species c = e (electrons) and c = i (ions). In the Debye-Hückel picture, the screening cloud can be given with the electron-ion structure factor by q…”
Section: Theory For the Dynamic Structure Factormentioning
confidence: 99%