Tohru Hada | Kyushu University (original) (raw)
Papers by Tohru Hada
Bulletin of the American Physical Society, Nov 16, 2015
Physics of Plasmas, May 1, 2019
Japanese Journal of Applied Physics, Sep 1, 2012
Physics of Plasmas, Feb 1, 2019
Physics of Plasmas, Jun 1, 2016
Japan Geoscience Union, May 1, 2015
Japan Geoscience Union, Mar 10, 2017
Japan Geoscience Union, Mar 10, 2017
Earth, Planets and Space, Jul 13, 2020
Journal of Geophysical Research, Jul 1, 2009
The proton velocity distribution functions (VDFs) observed in the solar wind often show beam comp... more The proton velocity distribution functions (VDFs) observed in the solar wind often show beam components. In this study, by means of one-dimensional hybrid simulation, parametric instabilities of circularly polarized Alfvén waves in core proton-electron-beam proton plasmas are discussed. Numerical results show that nonlinear evolution of parametric instabilities in core proton-electron-beam proton plasmas are different from those in core proton-electron plasmas. Furthermore, numerical solutions of the linear dispersion relations suggest the importance of the proton kinetic effects, which agrees with the past studies. In the case that the beams are stable, according to the excitation of the broadband Alfvén waves by the parametric instabilities, protons are diffused in the velocity space, resulting in the scattering and broadening of the beam components. Such time evolution of the proton VDFs changes the wave dispersion relation and affects the properties of the parametric instabilities, in agreement with the past theoretical studies. As a result, even if a decay instability is dominant at the linear stage, the parent wave can mainly be dissipated by the modulational instability at the nonlinear stage. Phase coherent turbulence is generated corresponding to the occurrence of the modulational instability. Parametric instabilities are also observed in plasmas with unstable beams. When left-hand polarized (LH-) Alfvén wave is initially given, both backward propagating right-hand polarized (RH-) and LH- Alfvén waves are excited by the decay instabilities in our runs. As time elapses, phase coherent turbulence is generated by the modulational instabilities, as in the case of stable beams. Some of the beam protons are perpendicularly accelerated by cyclotron resonance with the primary wave.
Nonlinear Processes in Geophysics, Feb 14, 2014
Journal of Geophysical Research, 1985
Journal of Geophysical Research, 1986
By means of a numerical simulation, nonlinear evolution of large amplitude dispersive Alfven wave... more By means of a numerical simulation, nonlinear evolution of large amplitude dispersive Alfven waves is studied. An energy transfer from the parent wave to two daughter Alfven‐like waves and a soundlike wave is observed (a stimulated Brillouin scattering process). The observed growth rates and propagation characteristics of these daughter waves agree with the analytical results, which we obtain by extending the previous treatments by Goldstein, Derby, Sakai, and Sonnerup. Ions are first trapped by the electrostatic potential of the daughter soundlike waves. Along with the eventual decay (ion Landau damping) of the soundlike waves, ions are phase‐mixed and left heated in the parallel direction. The increased parallel energy of ions is transferred to the perpendicular thermal energy through the nonresonant scattering process in the colliding Alfven waves (parent and daughter waves). We further observe that the daughter Alfven waves, which still have a large amplitude, are also unstable for further decay, and that the wave energy is continuously transferred to the longer wavelength regime (inverse cascading process).
Japan Geoscience Union, Mar 14, 2019
Advances in Space Research, 2001
Physics of fluids. B, Plasma physics, Nov 1, 1990
The chaos in a one-dimensional system, which would be nonlinear stationary Alfvén waves in the ab... more The chaos in a one-dimensional system, which would be nonlinear stationary Alfvén waves in the absence of an external driver, is characterized. The evolution equations are numerically integrated for the transverse wave magnetic field amplitude and phase using the derivative nonlinear Schrödinger equation (DNLS), including resistive wave damping and a long-wavelength monochromatic, circularly polarized driver. A Poincaré map analysis shows that, for the nondissipative (Hamiltonian) case, the solutions near the phase space (soliton) separatrices of this system become chaotic as the driver amplitude increases, and ‘‘strong’’ chaos appears when the driver amplitude is large. The dissipative system exhibits a wealth of dynamical behavior, including quasiperiodic orbits, period-doubling bifurcations leading to chaos, sudden transitions to chaos, and several types of strange attractors.
Bulletin of the American Physical Society, Nov 16, 2015
Physics of Plasmas, May 1, 2019
Japanese Journal of Applied Physics, Sep 1, 2012
Physics of Plasmas, Feb 1, 2019
Physics of Plasmas, Jun 1, 2016
Japan Geoscience Union, May 1, 2015
Japan Geoscience Union, Mar 10, 2017
Japan Geoscience Union, Mar 10, 2017
Earth, Planets and Space, Jul 13, 2020
Journal of Geophysical Research, Jul 1, 2009
The proton velocity distribution functions (VDFs) observed in the solar wind often show beam comp... more The proton velocity distribution functions (VDFs) observed in the solar wind often show beam components. In this study, by means of one-dimensional hybrid simulation, parametric instabilities of circularly polarized Alfvén waves in core proton-electron-beam proton plasmas are discussed. Numerical results show that nonlinear evolution of parametric instabilities in core proton-electron-beam proton plasmas are different from those in core proton-electron plasmas. Furthermore, numerical solutions of the linear dispersion relations suggest the importance of the proton kinetic effects, which agrees with the past studies. In the case that the beams are stable, according to the excitation of the broadband Alfvén waves by the parametric instabilities, protons are diffused in the velocity space, resulting in the scattering and broadening of the beam components. Such time evolution of the proton VDFs changes the wave dispersion relation and affects the properties of the parametric instabilities, in agreement with the past theoretical studies. As a result, even if a decay instability is dominant at the linear stage, the parent wave can mainly be dissipated by the modulational instability at the nonlinear stage. Phase coherent turbulence is generated corresponding to the occurrence of the modulational instability. Parametric instabilities are also observed in plasmas with unstable beams. When left-hand polarized (LH-) Alfvén wave is initially given, both backward propagating right-hand polarized (RH-) and LH- Alfvén waves are excited by the decay instabilities in our runs. As time elapses, phase coherent turbulence is generated by the modulational instabilities, as in the case of stable beams. Some of the beam protons are perpendicularly accelerated by cyclotron resonance with the primary wave.
Nonlinear Processes in Geophysics, Feb 14, 2014
Journal of Geophysical Research, 1985
Journal of Geophysical Research, 1986
By means of a numerical simulation, nonlinear evolution of large amplitude dispersive Alfven wave... more By means of a numerical simulation, nonlinear evolution of large amplitude dispersive Alfven waves is studied. An energy transfer from the parent wave to two daughter Alfven‐like waves and a soundlike wave is observed (a stimulated Brillouin scattering process). The observed growth rates and propagation characteristics of these daughter waves agree with the analytical results, which we obtain by extending the previous treatments by Goldstein, Derby, Sakai, and Sonnerup. Ions are first trapped by the electrostatic potential of the daughter soundlike waves. Along with the eventual decay (ion Landau damping) of the soundlike waves, ions are phase‐mixed and left heated in the parallel direction. The increased parallel energy of ions is transferred to the perpendicular thermal energy through the nonresonant scattering process in the colliding Alfven waves (parent and daughter waves). We further observe that the daughter Alfven waves, which still have a large amplitude, are also unstable for further decay, and that the wave energy is continuously transferred to the longer wavelength regime (inverse cascading process).
Japan Geoscience Union, Mar 14, 2019
Advances in Space Research, 2001
Physics of fluids. B, Plasma physics, Nov 1, 1990
The chaos in a one-dimensional system, which would be nonlinear stationary Alfvén waves in the ab... more The chaos in a one-dimensional system, which would be nonlinear stationary Alfvén waves in the absence of an external driver, is characterized. The evolution equations are numerically integrated for the transverse wave magnetic field amplitude and phase using the derivative nonlinear Schrödinger equation (DNLS), including resistive wave damping and a long-wavelength monochromatic, circularly polarized driver. A Poincaré map analysis shows that, for the nondissipative (Hamiltonian) case, the solutions near the phase space (soliton) separatrices of this system become chaotic as the driver amplitude increases, and ‘‘strong’’ chaos appears when the driver amplitude is large. The dissipative system exhibits a wealth of dynamical behavior, including quasiperiodic orbits, period-doubling bifurcations leading to chaos, sudden transitions to chaos, and several types of strange attractors.