抄録
Comparison of the mechanisms of the Weibel instability and the field generating thermal instability is made on the basis of the Boltzmann equation. The case k⊥∇T0⁄⁄∇n0 is investigated, where k is the wave vector, T0 and n0 are the zeroth order temperature and the number density. In the collisional plasma (klm<<1, where lm is the electron mean free path), the thermal instability is unstable, but the Weibel instability is stable. In the collisionless case (klm>>1), the situation is vice versa. When the equilibrium velocity distribution function is expanded by the Legendre polynomials Pl with the polar axis along ∇T0, l=2 and l=1 components are essential, respectively, for the Weibel instability and the thermal instability.