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Modelling and numerical methods for the study of particle transport in a hot plasma

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Academic year: 2021

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Figure

Figure 1: Irradiation scheme of a target by intense laser light in the case of the direct drive approach (left) and the indirect drive approach (right).
Figure 2: International Thermonuclear Experiment Reactor project (ITER - -Cadarache) for the magnetic connement fusion (left) and the laser installation Laser MegaJoule (LMJ - Bordeaux) for Inertial Connement Fusion (right).
Figure 2.2: Representation of the dissipation coecient as a function of k for the Vlasov equation and for the M 1 , two populations M 1 and M 2 models.
Figure 2.3: Representation of the modulus integrand of the impedance (2.41) as a function of k in the limit ω/k << v th in the case ω/ω pe = 0.1 and v th /c = 0.8
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