Modeling the gain of inner-shell X-ray laser transitions in neon, argon, and copper driven by X-ray free electron laser radiation using photo-ionization and photo-excitation processes  

作　　者：Joseph Nilsen 

机构地区：[1]Lawrence Livermore National Laboratory,Livermore,CA 94551,USA

出　　处：《Matter and Radiation at Extremes》2016年第1期76-81,共6页极端条件下的物质与辐射（英文）

基　　金：performed under the auspices of the U.S.Department of Energy by Lawrence Livermore National Laboratory under Contract DE-AC52-07NA27344。

摘　　要：Using an X-ray free electron laser(XFEL)at 960 eV to photo-ionize the 1s electron in neutral neon followed by lasing on the 2p-1s transition in singly-ionized neon,an inner-shell X-ray laser was demonstrated at 849 eV in singly-ionized neon gas several years ago.It took decades to demonstrate this scheme,because it required a very strong X-ray source that could photo-ionize the 1s(K shell)electron in neon on a timescale comparable to the intrinsic Auger lifetime in neon of 2 fs.In this paper,we model the neon inner shell X-ray laser under similar conditions to those used in the XFEL experiments at the SLAC Linac Coherent Light Source(LCLS),and show how we can improve the efficiency of the neon laser and reduce the drive requirements by tuning the XFEL to the 1s-3p transition in neutral neon in order to create gain on the 2p-1s line in neutral neon.We also show how the XFEL could be used to photo-ionize L-shell electrons to drive gain on n=3-2 transitions in singlyionized Ar and Cu plasmas.These bright,coherent,and monochromatic X-ray lasers may prove very useful for doing high-resolution spectroscopy and for studying non-linear process in the X-ray regime.

关 键 词：Photo-pumping X-ray free-electron laser X-ray laser 

分 类 号：TN2[电子电信—物理电子学]