Generation of High-frequency Whistler Waves in the Earth’s Quasi-perpendicular Bow Shock

2021 ◽  
Vol 919 (2) ◽  
pp. L17
Author(s):  
Brent Page ◽  
Ivan Y. Vasko ◽  
Anton V. Artemyev ◽  
Stuart D. Bale
2017 ◽  
Vol 842 (2) ◽  
pp. L11 ◽  
Author(s):  
M. Oka ◽  
L. B. Wilson III ◽  
T. D. Phan ◽  
A. J. Hull ◽  
T. Amano ◽  
...  

1991 ◽  
Vol 96 (A9) ◽  
pp. 15841-15852 ◽  
Author(s):  
Charles W. Smith ◽  
Hung K. Wong ◽  
Melvyn L. Goldstein
Keyword(s):  

1969 ◽  
Vol 74 (19) ◽  
pp. 4601-4617 ◽  
Author(s):  
John V. Olson ◽  
Robert E. Holzer ◽  
Edward J. Smith

2021 ◽  
Author(s):  
Martin Volwerk ◽  

<p>The induced magnetosphere of Venus is created by the interaction of the solar wind and embedded interplanetary magnetic field with the exosphere and ionosphere of Venus. Solar Orbiter entered Venus’s magnetotail far downstream, > 70 Venus radii, of the planet and exited the magnetosphere over the north pole. This offered a unique view of the system over distances that were only flown through once by three other missions before, Mariner 10, Galileo and Bepi-Colombo. The large-scale structure and activity of the induced magnetosphere is studied as well as the high-frequency plasma waves both in the magnetosphere and in a limited region upstream of the planet where interaction with Venus’s exosphere is expected.  It is shown that Venus’s magnetotail is very active during the Solar Orbiter flyby. Structures such as flux ropes, and reconnection sites are encountered as well as a strongly overdraping of the magnetic field downstream of the bow shock and planet. High-frequency plasma waves (up to 6 times the local proton cyclotron frequency) are observed in the magnetotail, which are identified as Doppler-shifted proton cyclotron waves, whereas in the upstream solar wind these waves appear just below the proton cyclotron frequency (as expected) but are very patchy. The bow shock is quasi perpendicular, however, expected mirror mode activity is not found directly behind it; instead there is strong cyclotron wave power. This is most-likely caused by the relatively low plasma-beta  behind the bow shock. Much further downstream in the magnetosheath mirror mode of magnetic hole structures are identified. This presentation will take place after the second Venus flyby by Solar Orbiter and BepiColombo and Solar Orbiter on 9 and 10 August, respectively.</p>


2019 ◽  
Vol 886 (1) ◽  
pp. 53 ◽  
Author(s):  
M. Oka ◽  
F. Otsuka ◽  
S. Matsukiyo ◽  
L. B. Wilson ◽  
M. R. Argall ◽  
...  

1989 ◽  
Vol 94 (A10) ◽  
pp. 13397 ◽  
Author(s):  
T. G. Onsager ◽  
R. H. Holzworth ◽  
H. C. Koons ◽  
O. H. Bauer ◽  
D. A. Gurnett ◽  
...  

2012 ◽  
Vol 117 (A12) ◽  
pp. n/a-n/a ◽  
Author(s):  
A. J. Hull ◽  
L. Muschietti ◽  
M. Oka ◽  
D. E. Larson ◽  
F. S. Mozer ◽  
...  
Keyword(s):  

2021 ◽  
Author(s):  
Niklas J. T. Edberg ◽  
Lina Hadid ◽  
Milan Maksimovic ◽  
Stuart D. Bale ◽  
Thomas Chust ◽  
...  

<p>We present measurements from the Radio and Plasma Wave (RPW) instrument suite onboard the Solar Orbiter mission during the first Venus encounter. RPW consists of several units and is capable of measuring both the electric and magnetic field fluctuations with three electric antennas and a search-coil magnetometer: The Low Frequency Receiver (LFR) cover the range from DC up to 10kHz when measuring the electric and magnetic waveform and spectra; the Thermal Noise and High Frequency Receiver (TNR-HFR) determines the electric power spectra and magnetic power spectra from 4kHz-20MHz, and 4kHz to 500kHz, respectively, to determine properties of the electron population; the Time Domain Sampler (TDS) measures and digitizes onboard the electric and magnetic field waveforms from 100 Hz to 250 kHz. The BIAS subunit measures DC and LF electric fields as well as the spacecraft potential, which gives a high cadence measure of the local plasma density when calibrated to the low-cadence tracking of the plasma peak from the TNR. Solar Orbiter approached Venus from the induced magnetotail and had its closest approach at an altitude of 7500 km over the north pole of Venus on 27 Dec 2020. The RPW instruments observed a tail region that extended several 10’s of Venus radii downstream of the planet. The induced magnetosphere was characterized to be a highly dynamic environment as Solar Orbiter traversed the downstream tail and magnetosheath before it crossed the Bow Shock outbound at ~12:40 UT. Polarized whistler waves, high frequency electrostatic waves, narrow-banded emissions, possible electron double layers were observed. The fine structure of the bow shock could also be investigated in detail. Solar Orbiter could hence enhance the knowledge of the structure of the solar wind-Venus interaction.</p>


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