The proton resonant firehose instability may arise in collisionless plasmas in which the proton velocity distribution is approximately bi‐Maxwellian with T ∥ p / T ⊥ p > 1, where ⊥ and ∥ denote directions relative to the background magnetic field B ○ . Linear theory and one‐dimensional simulations predict that enhanced field fluctuations from the proton resonant firehose instability impose a constraint on proton temperature anisotropies of the form 1 − T ⊥ p / T ∥ p = S p /β ∥ p α p where β ∥ p ≡ 8π n p k B T ∥ p / B ○ 2 , and the fitting parameters S p ∼ 1 and α p ≃ 0.7. Observations from the Wind spacecraft are reported here. These measurements show for the first time with a comprehensive plasma and magnetic field data set that this constraint is statistically satisfied in the solar wind near 1 AU, with best‐fit values of S p = 1.21 ± 0.26 and α p = 0.76 ± 0.14.
No takes yet. Share an insight, caveat, or question.
Kasper et al. (2002) studied this question.
Synapse has enriched 5 closely related papers on similar clinical questions. Consider them for comparative context: