Modeling of XFEL induced ionization and atomic displacement in protein nanocrystals

X-ray free-electron lasers enable high-resolution imaging of biological materials by using short enough pulses to outrun many of the effects of radiation damage. Experiments conducted at the LCLS have obtained diffraction data from single particles and protein nanocrystals at doses to the sample over 3 GGy. The details of the interaction of the X-ray FEL pulse with the sample determine the limits of this new paradigm for imaging. Recent studies suggest that in the case of crystalline samples, such as protein nanocrystals, the atomic displacements and loss of bound electrons in the crystal (due to the high X- ray intensity) has the effect of gating the diffraction signal, and hence making the experiment less radiation sensitive. Only the incident photon intensity in the first part of the pulse, before the Bragg diffraction has died out, is relevant to acquiring signal and the rest of the pulse will mainly contribute to a diffuse background. In this work we use a plasma based non-local thermodynamic equilibrium code to explore the displacement and the ionization of a protein nanocrystal at various X-ray wavelengths and intensities.

[1]  L. Spitzer Physics of fully ionized gases , 1956 .

[2]  Bob Nagler,et al.  TOF-OFF: A method for determining focal positions in tightly focused free-electron laser experiments by measurement of ejected ions , 2011 .

[3]  W. H. Benner,et al.  Femtosecond diffractive imaging with a soft-X-ray free-electron laser , 2006, physics/0610044.

[4]  M. Murillo,et al.  Dense plasma temperature equilibration in the binary collision approximation. , 2002, Physical review. E, Statistical, nonlinear, and soft matter physics.

[5]  Yuri Ralchenko,et al.  Review of the 9th NLTE code comparison workshop. , 2007, High energy density physics.

[6]  R. Henderson The potential and limitations of neutrons, electrons and X-rays for atomic resolution microscopy of unstained biological molecules , 1995, Quarterly Reviews of Biophysics.

[7]  Petra Fromme,et al.  Three-dimensional structure of cyanobacterial photosystem I at 2.5 Å resolution , 2001, Nature.

[8]  D Rolles,et al.  Ultrafast transitions from solid to liquid and plasma states of graphite induced by x-ray free-electron laser pulses. , 2012, Physical review letters.

[9]  Georg Weidenspointner,et al.  Self-terminating diffraction gates femtosecond X-ray nanocrystallography measurements , 2011, Nature Photonics.

[10]  Ryszard S. Romaniuk,et al.  Operation of a free-electron laser from the extreme ultraviolet to the water window , 2007 .

[11]  R. London,et al.  Large-scale molecular dynamics simulations of dense plasmas: The Cimarron Project , 2012 .

[12]  Carl Caleman,et al.  Auger electron cascades in water and ice , 2004 .

[13]  E. Abreu,et al.  Modeling of soft x-ray induced ablation in solids , 2011, Optics + Optoelectronics.

[14]  J. Hajdu,et al.  Potential for biomolecular imaging with femtosecond X-ray pulses , 2000, Nature.

[15]  M. Klintenberg,et al.  Radiation damage in biological material: Electronic properties and electron impact ionization in urea , 2008, 0808.1197.

[16]  D. Book,et al.  NRL (Naval Research Laboratory) Plasma Formulary. Revised. , 1983 .

[17]  Town,et al.  Fokker-Planck simulations of short-pulse-laser-solid experiments. , 1994, Physical review. E, Statistical physics, plasmas, fluids, and related interdisciplinary topics.

[18]  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.

[19]  Mark A Hill,et al.  Will reduced radiation damage occur with very small crystals? , 2005, Journal of synchrotron radiation.

[20]  Keith A. Nugent,et al.  Biomolecular imaging and electronic damage using X-ray free-electron lasers , 2011 .

[21]  Henry N. Chapman,et al.  Femtosecond X-ray protein nanocrystallography , 2010 .

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

[23]  S. Hau-Riege,et al.  Photoelectron dynamics in x-ray free-electron-laser diffractive imaging of biological samples. , 2012, Physical review letters.

[24]  Carl Caleman,et al.  Simulations of radiation damage in biomolecular nanocrystals induced by femtosecond X-ray pulses , 2011 .

[25]  D. Ratner,et al.  First lasing and operation of an ångstrom-wavelength free-electron laser , 2010 .

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

[27]  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.

[28]  John M. Dawson,et al.  High‐Frequency Conductivity and the Emission and Absorption Coefficients of a Fully Ionized Plasma , 1962 .

[29]  Georg Weidenspointner,et al.  Lipidic phase membrane protein serial femtosecond crystallography , 2012, Nature Methods.

[30]  James M. Holton,et al.  A beginner’s guide to radiation damage , 2009, Journal of synchrotron radiation.

[31]  Carl Caleman,et al.  Nanocrystal imaging using intense and ultrashort X-ray pulses , 2009 .

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

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

[34]  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.

[35]  Richard A. London,et al.  Unified model of secondary electron cascades in diamond , 2004 .

[36]  Yuri Ralchenko,et al.  Review of the NLTE-5 kinetics workshop , 2009 .

[37]  H. Scott,et al.  GLF - A simulation code for X-ray lasers , 1994 .

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

[39]  Colin Nave,et al.  The optimum conditions to collect X-ray data from very small samples. , 2008, Journal of synchrotron radiation.

[40]  Garth J. Williams,et al.  High-Resolution Protein Structure Determination by Serial Femtosecond Crystallography , 2012, Science.

[41]  Sébastien Boutet,et al.  Room temperature femtosecond X-ray diffraction of photosystem II microcrystals , 2012, Proceedings of the National Academy of Sciences.

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

[43]  Benjamin G Davis,et al.  Glyco- and peptidomimetics from three-component Joullié-Ugi coupling show selective antiviral activity. , 2005, Journal of the American Chemical Society.

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

[45]  Elspeth F Garman,et al.  Experimental determination of the radiation dose limit for cryocooled protein crystals. , 2006, Proceedings of the National Academy of Sciences of the United States of America.

[46]  Georg Weidenspointner,et al.  Time-resolved protein nanocrystallography using an X-ray free-electron laser , 2012, Optics express.

[47]  Georg Weidenspointner,et al.  Radiation damage in protein serial femtosecond crystallography using an x-ray free-electron laser. , 2011, Physical review. B, Condensed matter and materials physics.

[48]  Stefan P. Hau-Riege,et al.  X-ray atomic scattering factors of low- Z ions with a core hole , 2007 .