Beam instabilities in laser-plasma interaction: Relevance to preferential ion heating
Physical Review Letters 94:24 (2005)
Abstract:
We propose a new mechanism for anomalous ion heating in ultraintense laser plasmas. This mechanism is based on the excitation of an electron two-stream instability that is driven by the fast electron beam that resonantly decays into ion-acoustic waves. These low frequency waves are then strongly damped by the ion collisions in the dense plasma. The model gives a simple explanation for the preferential heating of the bulk ion population observed in recent laser experiments in the petawatt regime. In particular, this work provides an explanation for the different energy loss in the Au and CD plasmas, in cone-guided fast ignition experiments. © 2005 The American Physical Society.Measurements of Green Laser-Beam Propagation and Backscatter in Long-Scale Length Plasmas
2013 Abstracts IEEE International Conference on Plasma Science (ICOPS) Institute of Electrical and Electronics Engineers (IEEE) (2005) 164-164
Collisional lasers at 41.8 nm in a guided regime
J PHYS IV 127 (2005) 33-37
Laboratory simulations of supernova shockwave propagation
ASTROPHYS SPACE SCI 298:1-2 (2005) 61-67
Abstract:
Supernovae launch spherical shocks into the circumstellar medium (CSM). These shocks have high Mach numbers and may be radiative. We have created similar shocks in the laboratory by focusing laser pulses onto the tip of a solid pin surrounded by ambient gas; ablated material from the pin rapidly expands and launches a shock through the surrounding gas. Laser pulses were typically 5 ns in duration with ablative energies ranging from 1-150 J. Shocks in ambient gas pressures of similar to 1 kPa were observed at spatial scales of up to 5 cm using optical cameras with schlieren. Emission spectroscopy data were obtained to infer electron temperatures (< 10 eV).In this experiment we have observed a new phenomena; at the edge of the radiatively heated gas ahead of the shock, a second shock forms. The two expanding shocks are simultaneously visible for a time, until the original shock stalls from running into the heated gas. The second shock remains visible and continues to expand. A minimum condition for the formation of the second shock is that the original shock is super-critical, i.e., the temperature distribution ahead of the original shock has an inflexion point. In a non-radiative control experiment the second shock does not form. We hypothesize that a second shock could form in the astrophysical case, possibly in radiative supernova remnants such as SN1993J, or in shock-CSM interaction.X-ray line transfer in plasmas with large velocity gradients
ASTROPHYS SPACE SCI 298:1-2 (2005) 171-176