Bulletin of the American Physical Society
66th Annual Meeting of the APS Division of Plasma Physics
Monday–Friday, October 7–11, 2024; Atlanta, Georgia
Session GO09: High Energy Density Science: Hydrodynamics
9:30 AM–12:18 PM,
Tuesday, October 8, 2024
Hyatt Regency
Room: Regency V
Chair: J. Levesque, Los Alamos National Laboratory
Abstract: GO09.00004 : Development of a scintillator-based x-ray imager for high resolution backlit x-ray radiography experiments*
10:06 AM–10:18 AM
Presenter:
Nobuhiko Izumi
(Lawrence Livermore Natl Lab)
Authors:
Nobuhiko Izumi
(Lawrence Livermore Natl Lab)
Jeremy Huckins
(Lawrence Livermore National Laboratory)
Jason Prince
(Lawrence Livermore National Laboratory)
Joshua A Tabimina
(Lawrence Livermore National Laboratory)
Justin Buscho
(Lawrence Livermore National Laboratory)
Mai S Beach
(Lawrence Livermore National Laboratory)
Mary T Burkey
(Lawrence Livermore National Laboratory)
Sara Y Cheng
(Lawrence Livermore National Laboratory)
Kumar S. Raman
(Lawrence Livermore National Laboratory)
Gareth N Hall
(Lawrence Livermore National Laboratory)
David K. Bradley
(Lawrence Livermore Natl Lab)
Tina Ebert
(Lawrence Livermore National Laboratory)
Alexandre Do
(Lawrence Livermore National Laboratory)
Shon T. Prisbrey
(Lawrence Livermore National Laboratory)
Sabrina R Nagel
(Lawrence Livermore Natl Lab)
To satisfy these requirements, we designed a new imaging setup which is a combination of a pulsed laser driven x-ray backlit source (hν ~ 7.2 KeV), a bent crystal x-ray imager (x-ray image magnification 10x), and a newly developed scintillator-based x-ray imager. The scintillator-based x-ray imager consists of a scintillator screen (LuAG:Ce, 100 μm thick) and an industrial lens (image magnification: 3.33x, NA 0.158), and a CMOS imager. To satisfy the required SNR with a given intensity of the x-ray source, we need a new imaging detector with spatial resolution better than 20 μm at the scintillator while having DQE better than 10%.
We assembled a proof-of-principle setup of the imager and evaluated basic performance parameters. We will discuss the obtained performance and compare it to an analytical model of the system.
**This work was performed under the auspices of the Lawrence Livermore National Security, LLC, (LLNS) under Contract No. DE-AC52-07NA27344LLNL-ABS-866026
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