Paper | Title | Page |
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TUXD4 | Analysis Methods for Electron Radiography Based on Laser-Plasma Accelerators | 274 |
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Funding: DOE National Nuclear Security Administration under Award Number DE-NA0003856 DOE under Awards DE-SC00215057 University of Rochester New York State Energy Research and Development Authority Analysis methods are presented for determining the res-olution of both contact and projected electron radiography based on a laser-plasma accelerator. A means to determine the field strength of the electric/magnetic fields generated when a laser is incident on an object of interest is also outlined. Broad radiography results are reported and future plans for the diagnostic technique are outlined. |
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Slides TUXD4 [12.157 MB] | ||
DOI • | reference for this paper ※ doi:10.18429/JACoW-NAPAC2022-TUXD4 | |
About • | Received ※ 02 August 2022 — Revised ※ 04 August 2022 — Accepted ※ 06 August 2022 — Issue date ※ 03 September 2022 | |
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TUXD5 |
Development of Achromatic Imaging Capabilities for pRad at LANSCE | |
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Funding: The research presented is supported by the Laboratory Directed Research and Development program of Los Alamos National Laboratory under project number 20220343ER. Proton radiography is a powerful diagnostics technique that is capable of resolving ultra-fast processes on the ns scale in dense matter with micrometer spatial resolution. This unique performance is realized by the use of a chromatic imaging system, which consists of four quadrupole lenses [1]. Chromatic imaging systems have a mono-energetic focal length. That means, if a target with areas of different energy losses is to be investigated, it is only possible to focus on one proton energy leaving other areas of interest blurred. A simple method of focusing multiple energies at once and thus increasing the depth-of-field is the use of multiple detector stations along the beam axis. Proton images captured at downstream detector positions can be combined into a single image using a method called ’focus stacking’. A complete cancellation of the position- and energy dependent 2nd order chromatic aberrations that mostly affect the current image quality of pRad [2] is only possible by using an achromatic imaging system. Following the proposals in early design studies at LANSCE [3] a new prototype achromatic system is currently being developed for a 25 MeV S-band electron accelerator. *LA-UR-22-24725 [1] N. King, et al., Nucl. Instr. and Meth. in Phys. Res. A, Vol 424, 1999 [2] F.E. Merrill, Rev. of Acc. Sci. and Tech. Vol 8, 2015 [3] B. Blind, A.J. Jason, Proc. of PAC, 2005 |
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Slides TUXD5 [4.745 MB] | ||
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