X-ray laser-induced ablation of lead compounds

Proceedings of SPIE--the International Society for Optical Engineering SPIE, the international society for optics and photonics 8077 (2011) 807718-807718-7

Authors:

V Hájková, L Juha, P Boháček, T Burian, J Chalupský, L Vyšín, J Gaudin, PA Heimann, SP Hau-Riege, M Jurek, D Klinger, J Pelka, R Sobierajski, J Krzywinski, M Messerschmidt, SP Moeller, B Nagler, M Rowen, WF Schlotter, ML Swiggers, JJ Turner, SM Vinko, T Whitcher, J Wark, M Matuchová, S Bajt, H Chapman, T Dzelzainis, D Riley, J Andreasson, J Hajdu, B Iwan, N Timneanu, K Saksl, R Fäustlin, A Singer, K Tiedtke, S Toleikis, I Vartaniants, H Wabnitz

K-shell spectroscopy of Au plasma generated with a short-pulse laser

Canadian Journal of Physics 89:5 (2011) 647-651

Authors:

C Zulick, F Dollar, H Chen, K Falk, G Gregori, A Hazi, CD Murphy, J Park, J Seely, CI Szabo, R Tommasini, R Shepherd, K Krushelnick

Abstract:

The production of X-rays from electron transitions into K-shell vacancies (Kα,β) emission) is a well-known process in atomic physics and has been extensively studied as a plasma diagnostic in low-and mid-Z materials. However, X-ray spectra from near neutral high-Z ions are very complex, and their interpretation requires the use of state-of-the-art atomic calculations. In this experiment, the Titan laser system at Lawrence Livermore National Laboratory was used to deliver an approximately 350 J laser pulse, with a 10 ps duration and a wavelength of 1054 nm, to a gold (Au) target. A transparent bent quartz crystal spectrometer with a hard X-ray energy window, ranging from 17 to 102 keV, was used to measure the emission spectrum. Kα1,α2 and Kβ1,γ1 transitions were observed over a range of target sizes. Additionally, a series of shots were conducted with a pre-ionizing long pulse (3 ns, 1-10 J, 527 nm) on the backside of the target. FLYCHK, an atomic non-LTE code, designed to provide ionization and population distributions, was used to model the experiment. K α/Kβ ratios were found to be in good agreement with the predicted value for room temperature Au targets. © 2011 Published by NRC Research Press.

The zero vector potential mechanism of attosecond absorption

Physics of Plasmas 18:5 (2011)

Authors:

T Baeva, S Gordienko, APL Robinson, PA Norreys

Abstract:

A new mechanism for the absorption of energy during the interaction between an ultra-intense laser pulse and a sharp-edged overdense plasma, which we term the zero vector potential (ZVP) mechanism, is presented. The ZVP-mechanism is a nonponderomotive absorption mechanism that should dominate in the interaction of very strong short laser pulses (a0≫1) with overdense plasmas in the case of sharp density gradients. In the ZVP-mechanism the existence of moving zeroes in the vector potential of the relativistic skin layer is crucial to the generation of both fast electron bunches and coherent x-rays. We demonstrate that the laser energy is absorbed from the plasma on the attosecond timescale in the form of electron bunches with unprecedentedly short duration. The numerical simulations are able to validate all qualitative and quantitative aspects of the ZVP-mechanism. © 2011 American Institute of Physics.

In situ x-ray diffraction measurements of the c/a ratio in the high-pressure epsilon phase of shock-compressed polycrystalline iron

PRB American Physical Society 83:14 (2011) 144114

Authors:

JA Hawreliak, B El-Dasher, H Lorenzana, G Kimminau, A Higginbotham, B Nagler, SM Vinko, WJ Murphy, T Whitcher, JS Wark, S Rothman, N Park

Decay of cystalline order and equilibration during the solid-to-plasma transition induced by 20-fs microfocused 92-eV free-electron-laser pulses.

Phys Rev Lett 106:16 (2011) 164801

Authors:

E Galtier, FB Rosmej, T Dzelzainis, D Riley, FY Khattak, P Heimann, RW Lee, AJ Nelson, SM Vinko, T Whitcher, JS Wark, T Tschentscher, S Toleikis, RR Fäustlin, R Sobierajski, M Jurek, L Juha, J Chalupsky, V Hajkova, M Kozlova, J Krzywinski, B Nagler

Abstract:

We have studied a solid-to-plasma transition by irradiating Al foils with the FLASH free electron laser at intensities up to 10(16)  W/cm(2). Intense XUV self-emission shows spectral features that are consistent with emission from regions of high density, which go beyond single inner-shell photoionization of solids. Characteristic features of intrashell transitions allowed us to identify Auger heating of the electrons in the conduction band occurring immediately after the absorption of the XUV laser energy as the dominant mechanism. A simple model of a multicharge state inverse Auger effect is proposed to explain the target emission when the conduction band at solid density becomes more atomiclike as energy is transferred from the electrons to the ions. This allows one to determine, independent of plasma simulations, the electron temperature and density just after the decay of crystalline order and to characterize the early time evolution.