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LHD Bootstrap Current Coefficient Calculations with the VENUS+δ f code

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Figure

Fig. 1The magnetic axis position dependence of the experimen-
Fig. 3VENUS+δ f bootstrap current coefficients D31* versusthe normalized plasma radius r/a for the LHD configura-tions with different magnetic axes positions Rax = 3.90 m(diamonds), 3.95 m (circles), 4.00 m (squares), 4.05 m(crosses), 4.1 m (triangles) for the collisional regime withν/V = 0.003 [1/m] (a) and ν/V = 0.010 [1/m] (b).
Fig. 4SPBSC bootstrap current coefficients D31* versus thenormalized plasmas radius r/a for the LHD configura-tions with different magnetic axes positions Rax = 3.90 m(diamonds), 3.95 m (circles), 4.00 m (squares), 4.05 m(crosses), 4.10 m (triangles) for the collisional regimewith νth/Vth = 0.003 [1/m].
Fig. 6DKESbootstrapcurrentcoefficients(squares),VENUS+δ fbootstrapcurrentcoefficients(linewith circles) and Shaing-Callen limit (dotted line) for thetest LHD configuration at r/a = 0.5 with Rax = 3.75 m asa function of the inverse mean free path ν/V [1/m] withzero radial electric field.
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