2019
DOI: 10.1016/j.hedp.2019.100711
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Laser experiment for the study of accretion dynamics of Young Stellar Objects: Design and scaling

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Cited by 5 publications
(6 citation statements)
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References 32 publications
(54 reference statements)
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“…The plasma in the experiment was shown to be scalable to acretion events on a young star (Ryutov et al 2000). We verified in particular that our setup is representative of a high plasma β (≥1) Classical T Tauri Stars (CTTSs) accretion case (Revet et al 2019). We experimentally demonstrated the formation of a shell of dense (and optically thick when scaled to astrophysical conditions) plasma that envelopes the core's post-shock region and absorbs the Xrays arising from the central core.…”
Section: Introductionmentioning
confidence: 61%
“…The plasma in the experiment was shown to be scalable to acretion events on a young star (Ryutov et al 2000). We verified in particular that our setup is representative of a high plasma β (≥1) Classical T Tauri Stars (CTTSs) accretion case (Revet et al 2019). We experimentally demonstrated the formation of a shell of dense (and optically thick when scaled to astrophysical conditions) plasma that envelopes the core's post-shock region and absorbs the Xrays arising from the central core.…”
Section: Introductionmentioning
confidence: 61%
“…The value of the laboratory magnetic field (20 T) is chosen such that the laboratory plasma Alfven number is a best compromise match between the Alfven numbers of the YSO and of the solar corona outflows. The indicated velocity ranges correspond to the minimum and maximum speed within the flow; in the laboratory case it corresponds to the ballistic behavior of the expansion 64 . In the astrophysical cases, the material composition (indicated with H) consists in fully ionized hydrogen plus a mixture of heavier elements with abundances of 0.5 compared to the solar values 65 .…”
Section: Resultsmentioning
confidence: 99%
“… is the critical plasma density for optical radiation at the frequency L  and wavelength 2 L c     ). At the same time, this mode requires the use of much stronger magnetic fields, of the order of several tens of tesla [18][19][20]. In a dense plasma, magnetic fields of 10 T or more are required to retain the key dimensionless parameters for modeling of space phenomena [4].…”
Section: Justification Of the Parameters Of The Magnetic System For A...mentioning
confidence: 99%