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 PP12: Poster Session VI:
MFE Analytical, Computational and Data Science Techniques and Machine Learning
MFE Active Control and Whole Device Modelings
MFE MHD and Stability
DIII-D and Conventional Tokamaks II
Warm Dense Matter
Particle acceleration, beams and relativistic plasmas: Laser-plasma wakefield or direct laser accelerators
2:00 PM - 5:00 PM
Wednesday, October 9, 2024
Hyatt Regency
Room: Grand Hall West
Abstract: PP12.00124 : Probing the conductivity of compressed plastic using THz time-domain spectroscopy*
Presenter:
Eric R Sung
(SLAC National Accelerator Laboratory)
Authors:
Eric R Sung
(SLAC National Accelerator Laboratory)
Edna Rebeca R Toro Garza
(Stanford University)
Suzanne J Ali
(Lawrence Livermore Natl Lab)
Trevor M Hutchinson
(Lawrence Livermore National Laboratory)
Luke B Fletcher
(SLAC - Natl Accelerator Lab)
Philipp T May
(University of Rostock)
Gaia Righi
(LLNL)
Dominik Kraus
(University of Rostock)
Siegfried H Glenzer
(SLAC National Accelerator Laboratory)
Benjamin K Ofori-Okai
(SLAC - Natl Accelerator Lab)
We present single-shot THz time-domain spectroscopy measurements of shock compressed plastic. THz time-domain spectroscopy is a useful tool for determining electrical conductivity [3]. Because THz frequencies are much slower than electron-electron and electron-ion interactions, the THz field probes the quasi-DC electric response of the plastic. Furthermore, single-shot THz detection enables the probing of material properties during irreversible processes, making it an appealing tool for interrogating matter driven to extreme conditions. By observing changes in the THz signal reflected off the sample, we infer changes in the electrical properties of the plastics under shock compression.
[1] D. Kraus et al., Nat. Astron., 1, 606-611 (2017).
[2] D. Kraus et al, Phys. Rev. Res., 5, L022023 (2023).
[3] B. K. Ofori-Okai et al, Phys. Plasmas, 31, 042711 (2024).
*This work is supported by the DOE Office of Science, Fusion Energy Science under FWP 100182, FWP 100866, and by the DOE LDRD program at SLAC National Accelerator Laboratory, under contract DE-AC02-76SF00515 as part of the Panofsky Fellowship awarded to BKOO. The use of the Jupiter Laser Facility was supported by the U.S. Department of Energy, Lawrence Livermore National Laboratory, under Contract No. DE-AC52-07NA27344.
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