Collection Of theses on high power laser and plasma physics, Volume. 10, Issue 1, 75202(2010)
Laser-produced plasma helium-like titanium Kα x-ray source and its application to Rayleigh-Taylor instability study
Several experiments are performed on the ShenGuang-II laser facility to investigate an x-ray source and test radiography concepts. X-ray lines emitted from laser-produced plasmas are the most practical means of generating these high intensity sources. By using a time-integrated space-resolved keV spectroscope and pinhole camera, potential helium-like titanium Kα x-ray backlighting (radiography) line source is studied as a function of laser wavelength, ratio of pre-pulse intensity to main pulse intensity, and laser intensity (from 7.25 to ~ 11.3×1015 W/cm2). One-dimensional radiography using a grid consisting of 5 μm Au wires on 16 μm period and the pinhole-assisted point projection is tested. The measurements show that the size of the helium-like titanium Kα source from a simple foil target is larger than 100 μm, and relative x-ray line emission conversion efficiency ξx from the incident laser light energy to heliumlike titanium K-shell spectrum increases significantly with pre-pulse intensity increasing, increases rapidly with laser wavelength decreasing, and increases moderately with main laser intensity increasing. It is also found that a gold gird foils can reach an imaging resolution better than 5-μm featured with high contrast. It is further demonstrated that the pinhole-assisted point projection at such a level will be a novel two-dimensional imaging diagnostic technique for inertial confinement fusion experiments.
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Wang Rui-Rong, Chen Wei-Min, Wang Wei, Dong Jia-Qin, Xiao Sha-Li. Laser-produced plasma helium-like titanium Kα x-ray source and its application to Rayleigh-Taylor instability study[J]. Collection Of theses on high power laser and plasma physics, 2010, 10(1): 75202
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Received: Oct. 5, 2009
Accepted: --
Published Online: Jun. 2, 2017
The Author Email: Rui-Rong Wang (wangrr59@citiz.net)
CSTR:32186.14.