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Observations of Multiple Nuclear Reaction Histories and Fuel-Ion Species Dynamics in Shock-Driven Inertial Confinement Fusion Implosions.
Sio, H; Frenje, J A; Le, A; Atzeni, S; Kwan, T J T; Gatu Johnson, M; Kagan, G; Stoeckl, C; Li, C K; Parker, C E; Forrest, C J; Glebov, V; Kabadi, N V; Bose, A; Rinderknecht, H G; Amendt, P; Casey, D T; Mancini, R; Taitano, W T; Keenan, B; Simakov, A N; Chacón, L; Regan, S P; Sangster, T C; Campbell, E M; Seguin, F H; Petrasso, R D.
Afiliación
  • Sio H; Plasma Science and Fusion Center, Massachusetts Institute of Technology, Cambridge, Massachusetts 02139, USA.
  • Frenje JA; Plasma Science and Fusion Center, Massachusetts Institute of Technology, Cambridge, Massachusetts 02139, USA.
  • Le A; Los Alamos National Laboratory, Los Alamos, New Mexico 87545, USA.
  • Atzeni S; Dipartimento SBAI, Università degli Studi di Roma "La Sapienza," Via Antonio Scarpa 14, 00161, Roma, Italy.
  • Kwan TJT; Los Alamos National Laboratory, Los Alamos, New Mexico 87545, USA.
  • Gatu Johnson M; Plasma Science and Fusion Center, Massachusetts Institute of Technology, Cambridge, Massachusetts 02139, USA.
  • Kagan G; Los Alamos National Laboratory, Los Alamos, New Mexico 87545, USA.
  • Stoeckl C; Laboratory for Laser Energetics, Rochester, New York 14623, USA.
  • Li CK; Plasma Science and Fusion Center, Massachusetts Institute of Technology, Cambridge, Massachusetts 02139, USA.
  • Parker CE; Plasma Science and Fusion Center, Massachusetts Institute of Technology, Cambridge, Massachusetts 02139, USA.
  • Forrest CJ; Laboratory for Laser Energetics, Rochester, New York 14623, USA.
  • Glebov V; Laboratory for Laser Energetics, Rochester, New York 14623, USA.
  • Kabadi NV; Plasma Science and Fusion Center, Massachusetts Institute of Technology, Cambridge, Massachusetts 02139, USA.
  • Bose A; Plasma Science and Fusion Center, Massachusetts Institute of Technology, Cambridge, Massachusetts 02139, USA.
  • Rinderknecht HG; Laboratory for Laser Energetics, Rochester, New York 14623, USA.
  • Amendt P; Lawrence Livermore National Laboratory, Livermore, California 94551, USA.
  • Casey DT; Lawrence Livermore National Laboratory, Livermore, California 94551, USA.
  • Mancini R; Physics Department, University of Nevada, Reno, Nevada, 89557, USA.
  • Taitano WT; Los Alamos National Laboratory, Los Alamos, New Mexico 87545, USA.
  • Keenan B; Los Alamos National Laboratory, Los Alamos, New Mexico 87545, USA.
  • Simakov AN; Los Alamos National Laboratory, Los Alamos, New Mexico 87545, USA.
  • Chacón L; Los Alamos National Laboratory, Los Alamos, New Mexico 87545, USA.
  • Regan SP; Laboratory for Laser Energetics, Rochester, New York 14623, USA.
  • Sangster TC; Laboratory for Laser Energetics, Rochester, New York 14623, USA.
  • Campbell EM; Laboratory for Laser Energetics, Rochester, New York 14623, USA.
  • Seguin FH; Plasma Science and Fusion Center, Massachusetts Institute of Technology, Cambridge, Massachusetts 02139, USA.
  • Petrasso RD; Plasma Science and Fusion Center, Massachusetts Institute of Technology, Cambridge, Massachusetts 02139, USA.
Phys Rev Lett ; 122(3): 035001, 2019 Jan 25.
Article en En | MEDLINE | ID: mdl-30735406
Fuel-ion species dynamics in hydrodynamiclike shock-driven DT^{3}He-filled inertial confinement fusion implosion is quantitatively assessed for the first time using simultaneously measured D^{3}He and DT reaction histories. These reaction histories are measured with the particle x-ray temporal diagnostic, which captures the relative timing between different nuclear burns with unprecedented precision (∼10 ps). The observed 50±10 ps earlier D^{3}He reaction history timing (relative to DT) cannot be explained by average-ion hydrodynamic simulations and is attributed to fuel-ion species separation between the D, T, and ^{3}He ions during shock convergence and rebound. At the onset of the shock burn, inferred ^{3}He/T fuel ratio in the burn region using the measured reaction histories is much higher as compared to the initial gas-filled ratio. As T and ^{3}He have the same mass but different charge, these results indicate that the charge-to-mass ratio plays an important role in driving fuel-ion species separation during strong shock propagation even for these hydrodynamiclike plasmas.

Texto completo: 1 Colección: 01-internacional Banco de datos: MEDLINE Idioma: En Revista: Phys Rev Lett Año: 2019 Tipo del documento: Article País de afiliación: Estados Unidos

Texto completo: 1 Colección: 01-internacional Banco de datos: MEDLINE Idioma: En Revista: Phys Rev Lett Año: 2019 Tipo del documento: Article País de afiliación: Estados Unidos