Jul 2 – 6, 2018
Žofín Palace
Europe/Prague timezone

P2.2012 Investigating the influence of the picosecond leading pulse edge on ultra-intense laser heating of solids with 3D PIC simulations

Jul 3, 2018, 2:00 PM
2h
Mánes

Mánes

Speaker

Thomas Kluge

Description

See the full Abstract at http://ocs.ciemat.es/EPS2018ABS/pdf/P2.2012.pdf Investigating the influence of the picosecond leading pulse edge on ultra-intense laser heating of solids with 3D PIC simulations T. Kluge1, M. Garten1,2, A. Huebl1,2, R. Widera1, I. Goethel1, H. Burau1,2, T. Cowan1, U. Schramm1, M. Bussmann1 1 Helmholtz-Zentrum Dresden – Rossendorf, Germany 2 Technische Universität Dresden, Germany With recent improvements in plasma mirror techniques [1] achieving a reproducibly high laser contrast, systematic studies of short-pulse, ultra-high intensity laser-ion acceleration from thin foil targets (~10nm) become experimentally available [2][3]. A deeper understanding of the influence of the pre-pulse phase and ps leading pulse edge of the drive laser could lead to better control and reproducibility of ion cut-off energies which are crucial for using laser-accelerated ions in medical applications. Plasma dynamics accompanying the acceleration are highly non-linear and require precise knowledge about the influence of both ab-initio electromagnetic and atomic evolution of the plasma. Consequently, modelling these processes requires a fully kinetic high resolution treatment and extensive 2D surveys, while comparisons to experiments have shown that a quantitative prediction of proton cut-off energies and evolution of plasma instabilities demand a full 3D approach [4]. We present first results from a 3D PIC simulation campaign, modelling ultra-intense (a0 = 20- 60) laser interaction with up to micrometer thick foils covering the pico-second time span prior to the arrival of the main pulse. Simulations have been performed at the Piz Daint supercomputer at Figure 1: CSCS, Switzerland, using the fully-relativistic 3D3V open-source Longitudinal current density component of particle-in-cell code PIConGPU [5] developed at HZDR. a 300nm Cu target with organic contamination layer. [1] H. B. Shaw, S. Steinke, J. Van Tilborg and W. P. Leemans, Phys. Plasmas 23 (2016) [2] P. L. Poole, L. Obst, G. Cochran et al., New J. Phys. 20 13019 (2018) [3] A. Higginson, R. J. Gray, M. King, et al., Nat. Commun. 9 724 (2018) [4] P. Hilz, T. M. Ostermayr, A. Huebl et al., Nat. Commun. 9 423 (2018) [5] M. Bussmann, A. Huebl, R. Widera et al., Proceedings of SC13, Denver CO USA, Nov 17-21th (2013)

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