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Table 2 The peak time of the energy partition for the three modes

From: Dispersion relation as a channel of plasma turbulence evolution

Mode

β i =0 . 05

β i =0 . 1

β i =0 . 2

IB1

\(500\, \Omega _{\mathrm {p}}^{-1}\)

\(1000\, \Omega _{\mathrm {p}}^{-1}\)

\(1400\, \Omega _{\mathrm {p}}^{-1}\)

IB2

\(700\, \Omega _{\mathrm {p}}^{-1}\)

\(1000\, \Omega _{\mathrm {p}}^{-1}\)

\(1400\, \Omega _{\mathrm {p}}^{-1}\)

IC

\(700\, \Omega _{\mathrm {p}}^{-1}\)

\(1000\, \Omega _{\mathrm {p}}^{-1}\)

\(1600\, \Omega _{\mathrm {p}}^{-1}\)

  1. Peak time (in units of inverse proton cyclotron frequency) of the energy partition for the fundamental ion Bernstein mode (IB1), the second-harmonic of the ion Bernstein mode (IB2), and the oblique ion cyclotron mode (IC) as functions of ion beta.