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With respect to, in Fig. 2 we have used 100 energy modes (instead of 60) and a 250 km radial range (instead of 200 km); the resulting differences with the analogous Fig. 5 of are, however, negligible.
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With respect to, in Fig. 2 we have used 100 energy modes (instead of 60) and a 250 km radial range (instead of 200 km); the resulting differences with the analogous Fig. 5 of are, however, negligible.
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Note that, for no ν̄ spectral split (J̄l=0), one recovers from Eq. 11 the "sum rule" Jh=J̄.
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Note that, for no ν̄ spectral split (J̄l=0), one recovers from Eq. 11 the "sum rule" Jh=J̄.
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Multiangle simulations appear to suppress nonadiabatic features emerging at single-angle, such as the bipolar oscillations (see) and the ν̄ split (see and this work).
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Multiangle simulations appear to suppress nonadiabatic features emerging at single-angle, such as the bipolar oscillations (see) and the ν̄ split (see and this work).
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