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dc.contributor.authorChristopherson, A.R.en_US
dc.contributor.authorBetti, R.en_US
dc.contributor.authorForrest, C.J.en_US
dc.contributor.authorHoward, J.en_US
dc.contributor.authorTheobald, W.en_US
dc.contributor.authorCampbell, E.M.en_US
dc.contributor.authorDelettrez, J.en_US
dc.contributor.authorRosenberg, M.J.en_US
dc.contributor.authorSolodov, A.en_US
dc.contributor.authorStoeckl, C.en_US
dc.contributor.authorPatel, D.en_US
dc.contributor.authorGopalaswamy, V,en_US
dc.contributor.authorCao, D.en_US
dc.contributor.authorPeebles, J.en_US
dc.contributor.authorEdgell, D.en_US
dc.contributor.authorSeka, W.en_US
dc.contributor.authorEpstein, R.en_US
dc.contributor.authorScullin, W.en_US
dc.contributor.authorRadha, P.B.en_US
dc.contributor.authorWei, M.S.en_US
dc.contributor.authorRegan, S.P.en_US
dc.contributor.authorGatu Johnson, Mariaen_US
dc.contributor.authorSimpson, R.en_US
dc.date.accessioned2025-03-21T20:23:08Z
dc.date.available2025-03-21T20:23:08Z
dc.date.issued2022-01
dc.identifier22ja026
dc.identifier.urihttps://hdl.handle.net/1721.1/158735
dc.descriptionSubmitted for publication in Physics of Plasmas
dc.description.abstractHot electrons generated from laser plasma instabilities degrade performance of direct drive implosions by preheating the deuterium and tritium (DT) fuel resulting in early decompression and lower areal densities at stagnation. A technique to quantify the hot electron preheat of the dense DT fuel and connect it to the degradation in areal density is described in detail. Hot electrons are measured primarily from the hard x-rays they emit as they slow down in the target. The DT preheat is inferred from a comparison of the hard x-ray signals between a DT-layered implosion and its mass equivalent ablator only implosion. The preheat energy spatial distribution within the imploding shell is inferred from experiments using high Z payloads of varying thicknesses. It is found that the electrons deposit their energy uniformly throughout the shell material. For typical direct-drive OMEGA implosions driven with an overlapped intensity of ∼9·10^14 W/cm2, approximately ∼0.02%–0.03% of the laser energy is converted into preheat of the stagnated fuel which corresponds to areal density degradations of 10%–20%. The degradations in areal density explain some of the observed discrepancies between the simulated and measured areal densities.
dc.publisherAIPen_US
dc.relation.isversionofdoi.org/10.1063/5.0091220
dc.sourcePlasma Science and Fusion Centeren_US
dc.titleInferences of hot electron preheat and its spatial distribution in OMEGA direct drive implosionsen_US
dc.typeArticleen_US
dc.contributor.departmentMassachusetts Institute of Technology. Plasma Science and Fusion Center
dc.relation.journalPhysics of Plasmas


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