Modeling of soft x-ray induced ablation in solids

Powerful free electron lasers (FELs) operating in the soft X-ray regime are offering new possibilities for creating and probing materials under extreme conditions. We describe here simulations to model the interaction of a focused FEL pulse with metallic solids (niobium, vanadium, and their deuterides) at 13.5 nm wavelength (92 eV) with peak intensities between 1015 to 1018 W/cm2 and a fixed pulse length of 15 femtoseconds (full width at half maximum). The interaction of the pulse with the metallic solids was modeled with a non-local thermodynamic equilibrium code that included radiation transfer. The calculations also made use of a self-similar isothermal fluid model for plasma expansion into vacuum. We find that the time-evolution of the simulated critical charge density in the sample results in a critical depth that approaches the observed crater depths in an earlier experiment performed at the FLASH free electron laser in Hamburg. The results show saturation in the ablation process at intensities exceeding 1016 W/cm2. Furthermore, protons and deuterons with kinetic energies of several keV have been measured, and these concur with predictions from the plasma expansion model. The results indicate that the temperature of the plasma reached almost 5 million K after the pulse has passed.

[1]  Marta Fajardo,et al.  Hydrodynamic simulation of XUV laser-produced plasmas , 2004 .

[2]  H. Chapman,et al.  Soft x-ray free electron laser microfocus for exploring matter under extreme conditions. , 2009, Optics express.

[3]  J. Chalupský,et al.  Sub-micron focusing of soft x-ray free electron laser beam , 2009, Optics + Optoelectronics.

[4]  J Gautier,et al.  Non-thermal desorption/ablation of molecular solids induced by ultra-short soft x-ray pulses. , 2009, Optics express.

[5]  C. Caleman,et al.  Studies of resolidification of non-thermally molten InSb using time-resolved X-ray diffraction , 2005 .

[6]  Richard A. London,et al.  Femtosecond time-delay X-ray holography , 2007, Nature.

[7]  B. L. Henke,et al.  X-Ray Interactions: Photoabsorption, Scattering, Transmission, and Reflection at E = 50-30,000 eV, Z = 1-92 , 1993 .

[8]  John C. Stewart,et al.  Lowering of Ionization Potentials in Plasmas , 1966 .

[9]  Richard M. More,et al.  Electronic energy-levels in dense plasmas , 1982 .

[10]  J. Feldhaus,et al.  FLASH—the first soft x-ray free electron laser (FEL) user facility , 2010 .

[11]  H. Wabnitz,et al.  The soft x-ray free-electron laser FLASH at DESY: beamlines, diagnostics and end-stations , 2009 .

[12]  P. Audebert,et al.  Laser-driven proton scaling laws and new paths towards energy increase , 2006 .

[13]  Richard A. London,et al.  Damage threshold of inorganic solids under free-electron-laser irradiation at 32.5 nm wavelength , 2007 .

[14]  Howard A. Scott,et al.  Cretin—a radiative transfer capability for laboratory plasmas , 2001 .

[15]  F. Maia,et al.  Feasibilityof imaging living cells at subnanometer resolutionsbyultrafastX-raydiffraction , 2008 .

[16]  J. C. Slater Atomic Shielding Constants , 1930 .

[17]  S. Hau-Riege,et al.  Interaction of ultrashort x-ray pulses with B4C , SiC, and Si. , 2007, Physical review. E, Statistical, nonlinear, and soft matter physics.

[18]  H N Chapman,et al.  Saturated ablation in metal hydrides and acceleration of protons and deuterons to keV energies with a soft-x-ray laser. , 2011, Physical review. E, Statistical, nonlinear, and soft matter physics.

[19]  P. Mora,et al.  Plasma expansion into a vacuum. , 2003, Physical review letters.

[20]  Stephanie B. Hansen,et al.  Advances in NLTE modeling for integrated simulations , 2009 .

[21]  J. Itatani,et al.  Pressure Ionization and Line Merging in Strongly Coupled Plasmas Produced by 100-fs Laser Pulses , 1998 .

[22]  J. Meyer-ter-Vehn,et al.  Hydrodynamic simulation of subpicosecond laser interaction with solid-density matter , 2000, Physical review. E, Statistical physics, plasmas, fluids, and related interdisciplinary topics.