Generation of the Jovian hectometric radiation: First lessons from Juno

Using Juno plasma and wave and magnetic observations (JADE and Waves and MAG instruments), the generation mechanism of the Jovian hectometric radio emission is analyzed. It is shown that suitable conditions for the cyclotron maser instability (CMI) are observed in the regions of the radio sources. Pronounced loss cone in the electron distributions are likely the source of free energy for the instability. The theory reveals that sufficient growth rates are obtained from the distribution functions that are measured by the JADE-Electron instrument. The CMI would be driven by upgoing electron populations at 5–10 keV and 10–30° pitch angle, the amplified waves propagating at 82°–87° from the B field, a fraction of a percent above the gyrofrequency. Typical e-folding times of 10−4 s are obtained, leading to an amplification path of ~1000 km. Overall, this scenario for generation of the Jovian hectometric waves differs significantly from the case of the auroral kilometric radiation at Earth.

[1]  P. Louarn,et al.  Trapped electrons as a free energy source for the auroral kilometric radiation , 1990 .

[2]  P. Louarn,et al.  Auroral kilometric radiation sources: In situ and remote observations from Viking , 1993 .

[3]  Donald B. Melrose,et al.  Electron-cyclotron masers as the source of certain solar and stellar radio bursts , 1982 .

[4]  N. Omidi,et al.  Generation of Auroral Kilometric and Z Mode Radiation , 1984 .

[5]  A. Roux,et al.  Direct generation of the auroral kilometric radiation by the Maser synchrotron Instability: Physical mechanism and parametric study , 1984 .

[6]  R. Wilson,et al.  Electron beams and loss cones in the auroral regions of Jupiter , 2017 .

[7]  P. Pritchett Cyclotron maser radiation from a source structure localized perpendicular to the ambient magnetic field , 1986 .

[8]  P. Schippers,et al.  Properties of Saturn kilometric radiation measured within its source region , 2010, 1101.3842.

[9]  P. Zarka Auroral radio emissions at the outer planets: Observations and theories , 1998 .

[10]  P. Louarn,et al.  Plasma measurements in the Jovian polar region with Juno/JADE , 2017 .

[11]  R. Elphic,et al.  FAST satellite wave observations in the AKR source region , 1998 .

[12]  B. Burke,et al.  Observations of a variable radio source associated with the planet Jupiter , 1955 .

[13]  A. Roux,et al.  Direct generation of the auroral kilometric radiation by the maser synchrotron instability: An analytical approach , 1984 .

[14]  J. H. Waite,et al.  Magnetospheric Science Objectives of the Juno Mission , 2017 .

[15]  P. Louarn,et al.  Analytical study of the relativistic dispersion: application to the generation of the auroral kilometric radiation , 1989 .

[16]  R. Ergun,et al.  FAST observations of electron distributions within AKR source regions , 1998 .

[17]  P. Louarn,et al.  A new view of Jupiter's auroral radio spectrum , 2017 .

[18]  R. Schnurr,et al.  The Juno Magnetic Field Investigation , 2017 .

[19]  C. S. Wu,et al.  Kinetic cyclotron and synchrotron maser instabilities: Radio emission processes by direct amplification of radiation , 1985 .

[20]  B. Mauk,et al.  Plasma waves in Jupiter's high‐latitude regions: Observations from the Juno spacecraft , 2017 .

[21]  Lou‐Chuang Lee,et al.  A theory of the terrestrial kilometric radiation , 1979 .

[22]  J. Rouzaud,et al.  The Jovian Auroral Distributions Experiment (JADE) on the Juno Mission to Jupiter , 2017 .