Turbulent amplification of magnetic fields in laboratory laser-produced shock waves by Meinecke, J, Doyle, H, Miniati, F, Bell, A, Bingham, R, Crowston, R, Drake, R, Fatenejad, M, Koenig, M, Kuramitsu, Y, Kuranz, C, Lamb, D, Lee, D, Macdonald, M, Murphy, C, Park, H, Pelka, A, Ravasio, A, Sakawa, Y, Schekochihin, A, Scopatz, A, Tzeferacos, P, Wan, W, Woolsey, N, Yurchak, R

Turbulent amplification of magnetic fields in laboratory laser-produced shock waves by Meinecke, J, Doyle, H, Miniati, F, Bell, A, Bingham, R, Crowston, R, Drake, R, Fatenejad, M, Koenig, M, Kuramitsu, Y, Kuranz, C, Lamb, D, Lee, D, MacDonald, M, Murphy, C, Park, H, Pelka, A, Ravasio, A, Sakawa, Y, Schekochihin, A, Scopatz, A, Tzeferacos, P, Wan, W, Woolsey, N, Yurchak, R

FLASH magnetohydrodynamic simulations of shock-generated magnetic field experiments by Tzeferacos, P, Fatenejad, M, Flocke, N, Gregori, G, Lamb, D, Lee, D, Meinecke, J, Scopatz, A, Weide, K

“…In these experiments, a long-pulse laser illuminates a target in a chamber filled with Argon gas, producing shock waves that generate magnetic fields via the Biermann battery mechanism. …”

FLASH hydrodynamic simulations of experiments to explore the generation of cosmological magnetic fields by Scopatz, A, Fatenejad, M, Flocke, N, Gregori, G, Koenig, M, Lamb, D, Lee, D, Meinecke, J, Ravasio, A, Tzeferacos, P, Weide, K, Yurchak, R

“…In these experiments, a long-pulse laser illuminates a target in a chamber filled with Argon gas, producing shock waves that generate magnetic fields via the Biermann battery mechanism. …”

Modeling HEDLA magnetic field generation experiments on laser facilities by Fatenejad, M, Bell, A, Benuzzi-Mounaix, A, Crowston, R, Drake, R, Flocke, N, Gregori, G, Koenig, M, Krauland, C, Lamb, D, Lee, D, Marques, JR, Meinecke, J, Miniati, F, Murphy, C, Park, H, Pelka, A, Ravasio, A, Remington, B, Reville, B, Scopatz, A, Tzeferacos, P, Weide, K, Woolsey, N, Young, R

“…Attempts to perform simulations of these experiments using the FLASH code have uncovered previously unreported numerical difficulties in modeling the Biermann battery mechanism near shock waves which can lead to the production of large non-physical magnetic fields. …”

Time evolution and asymmetry of a laser produced blast wave by Tubman, E, Scott, R, Doyle, H, Meinecke, J, Ahmed, H, Alraddadi, R, Bolis, R, Cross, J, Crowston, R, Doria, D, Lamb, D, Reville, B, Robinson, A, Tzeferacos, P, Borghesi, M, Gregori, G, Woolsey, N

“…The emission front is asymmetrical in shape and tends to a more symmetrical shape as it progresses due to the production of a second shock wave later in time, which pushes out the front of the blast wave. …”

Experimental platform for the investigation of magnetized-reverse-shock dynamics in the context of POLAR by Gregori, G, Albertazzi, B, Falize, E, Falize, E, Pelka, A, Brack, F, Kroll, F, Yurchak, R, Brambrink, E, Mabey, P, Ozaki, N, Pikuz, S, Van Box Som, L, Bonnet-Bidaud, J, Cross, J, Filippov, E, Kodama, R, Mouchet, M, Morita, T, Sakawa, Y, Drake, R, Kuranz, C, Manuel, M, Li, C, Tzeferacos, P, Lamb, D, Schramm, U, Koenig, M

“…The laser irradiation (I ∼ 2 × 1014 W · cm−2 ) of a multilayer target generates a shock wave that produces a rear side plasma expanding flow. …”