Abstract:This Letter presents a novel approach to study electron transport in warm dense matter. It also includes the first x-ray Thomson scattering (XRTS) measurement from low-density CH foams compressed by a strong laser-driven shock at the OMEGA laser facility. The XRTS measurement is combined with velocity interferometry (VISAR) and optical pyrometry (SOP) providing a robust measurement of thermodynamic conditions in the shock. Evidence of significant preheat contributing to elevated temperatures reaching 17.5-35 e… Show more
“…Figure 3 shows the temperature profile of 3 separate simulations at 2 ns with a 1, 5, and 10 eV preheat. The 10 eV preheat (larger than expected from past studies [5]), produces only a small (∼ 1 − 2 eV) difference in the profile temperature. Our analysis supports the practice in most radiation transport experiments that this heating is unimportant because both the amount of high-energy emission (electrons and photons) is small compared to the total emission and most of this emission streams through the target.…”
Section: Drivementioning
confidence: 54%
“…Non-thermal electrons produced in the hohlraum can stream into the target, preheating the target material prior to the launch of the radiation front. For low-drive experiments, a few eV pre-heat can alter the evolution of the shock front [5]. But, for the COAX experiment, even a 10 eV pre-heat does not significantly alter the flow of the much more powerful COAX drive.…”
One of the difficulties in developing accurate numerical models of radiation flow in a coupled radiation-hydrodynamics setting is accurately modeling the transmission across a boundary layer. The COAX experiment is a platform design to test this transmission including standard radiograph and flux diagnostics as well as a temperature diagnostic measuring the population of excitation levels and ionization states of a dopant embedded within the target material. Using a broad range of simulations, we study the experimental errors in this temperature diagnostic. We conclude with proposed physics experiments that show features that are much stronger than the experimental errors and provide the means to study transport models.
“…Figure 3 shows the temperature profile of 3 separate simulations at 2 ns with a 1, 5, and 10 eV preheat. The 10 eV preheat (larger than expected from past studies [5]), produces only a small (∼ 1 − 2 eV) difference in the profile temperature. Our analysis supports the practice in most radiation transport experiments that this heating is unimportant because both the amount of high-energy emission (electrons and photons) is small compared to the total emission and most of this emission streams through the target.…”
Section: Drivementioning
confidence: 54%
“…Non-thermal electrons produced in the hohlraum can stream into the target, preheating the target material prior to the launch of the radiation front. For low-drive experiments, a few eV pre-heat can alter the evolution of the shock front [5]. But, for the COAX experiment, even a 10 eV pre-heat does not significantly alter the flow of the much more powerful COAX drive.…”
One of the difficulties in developing accurate numerical models of radiation flow in a coupled radiation-hydrodynamics setting is accurately modeling the transmission across a boundary layer. The COAX experiment is a platform design to test this transmission including standard radiograph and flux diagnostics as well as a temperature diagnostic measuring the population of excitation levels and ionization states of a dopant embedded within the target material. Using a broad range of simulations, we study the experimental errors in this temperature diagnostic. We conclude with proposed physics experiments that show features that are much stronger than the experimental errors and provide the means to study transport models.
“…Theimportance of thenonlocal electron transport has been recently observed experimentally, where it was demonstrated that theclassical diffusive hydrodynamics fails to model thereal behavior of the plasma. In contrast, theNTH model succeeds to predict acomplex plasma behavior [12].…”
Section: Nth Model Of Laser-heated Plasmamentioning
confidence: 84%
“…The plasma profile and the temperature are strongly affected by these nonlocal processes[7], which may also lead to asignificant effect on thehigh-power laser interaction as demonstrated in this work. A correct treatment of the ablation process requires anaccurate nonlocal radiation-hydrodynamics, which has been demonstrated in[8][9][10][11][12] during last several decades.Ablation physics under nonlocal transport conditions is of importance for two main applications:…”
Interaction of high-power lasers with solid targets is in general strongly affected by the limited contrast available. The laser pre-pulse ionizes the target and produces a pre-plasma which can strongly modify the interaction of the main part of the laser pulse with the target. This is of particular importance for future experiments which will use laser intensities above 10 21 W cm −2 and which are subject to the limited contrast. As a consequence the main part of the laser pulse will be modified while traversing the pre-plasma, interacting with it partially. A further complication arises from the fact that the interaction of a high-power pre-pulse with solid targets very often takes place under nonlocal transport conditions, i.e. the characteristic mean-free-path of the particles and photons is larger than the characteristic scale-lengths of density and temperature. The classical diffusion treatment of radiation and heat transport in the hydrodynamic model is then insufficient for the description of the pre-pulse physics. These phenomena also strongly modify the formation of the pre-plasma which in turn affects the propagation of the main laser pulse. In this paper nonlocal radiation-hydrodynamic simulations are carried out and serve as input for subsequent kinetic simulations of ultra-high intensity laser pulses interacting with the plasma in the ultra-relativistic regime. It is shown that the results of the kinetic simulations differ considerably whether a diffusive or nonlocal transport is used for the radiation-hydrodynamic simulations.
“…In dense plasmas, DSF, usually probed in x-ray Thomson scattering experiments, is considered as an important, and sometimes irreplaceable, diagnostic tool to probe thermal properties, such as temperature and density, in the internal regime of dense plasmas. [5,[38][39][40][41][42] It is a common practice to calculate DSF in the framework of time-dependent density functional theory (TDDFT), [43,44] which avoids the cumbersome calculation of the Bethe-Salpeter equation [1,45] of the many-body perturbation theory (MBPT) approach, owing to the less important contribution of long-range exchange and correlation effect in the DSF. [1] It was shown [16,25,35,46,47] as a rule of the thumb that for |𝑞| smaller than twice of the plasmon cutoff wave vector 𝑞c, the method reproduced the experimental DSF well with lifetime broadening effects included semi-empirically.…”
We propose an ansatz without adjustable parameters for the calculation of dynamical structure factor. The ansatz combines quasi-particle Green’s function, especially the contribution from the renormalization factor, and the exchange-correlation kernel from time-dependent density functional theory together, verified for typical metals and semiconductors from plasmon excitation regime to Compton scattering regime. It has the capability to reconcile both small-angle and large-angle inelastic x-ray scattering (IXS) signals with much improved accuracy, which can be used, as the theoretical base model, in inversely inferring electronic structures of condensed matter from IXS experimental signals directly. It may also be used to diagnose thermal parameters, such as temperature and density, of dense plasmas in x-ray Thomson scattering experiments.
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