scholarly journals The roles of charge exchange and dissociation in spreading Saturn's neutral clouds

2012 ◽  
Vol 117 (E5) ◽  
pp. n/a-n/a ◽  
Author(s):  
B. L. Fleshman ◽  
P. A. Delamere ◽  
F. Bagenal ◽  
T. Cassidy
2020 ◽  
Author(s):  
Fran Bagenal ◽  
Vincent Dols ◽  
Edward Nerney ◽  
Frank Crary ◽  
Tim Cassidy

<p>The plasma interaction with Io’s atmosphere results in at least a ton per second of escaping neutrals. Most of these neutrals supply extended neutral clouds along Io's orbit  and eventually become ionized and accelerated to corotation with Jupiter, populating the Io plasma torus as well as spreading out to fill Jupiter’s vast magnetosphere. About half to two-thirds of the plasma torus ions charge-exchange with the extended neutral clouds  and leave the torus as energetic neutral atoms, passing Europa’s orbit. Energetic neutrals are also produced directly in the plasma-atmosphere interaction, escaping with sufficient speed to reach Europa’s orbit before being ionized. The iogenic ions that are accelerated to high energies in the middle magnetosphere ultimately move back inward, again crossing Europa’s orbit. We present estimates of the fluxes of these various iogenic populations and how much oxygen, sulfur and sodium might be hitting Europa.</p>


Author(s):  
Wm. H. Escovitz ◽  
T. R. Fox ◽  
R. Levi-Setti

Charge exchange, the neutralization of ions by electron capture as the ions traverse matter, is a well-known phenomenon of atomic physics which is relevant to ion microscopy. In conventional transmission ion microscopes, the neutral component of the beam after it emerges from the specimen cannot be focused. The scanning transmission ion microscope (STIM) enables the detection of this signal to make images. Experiments with a low-resolution 55 kV STIM indicate that the charge-exchange signal provides a new contrast mechanism to detect extremely small amounts of matter. In an early version of charge-exchange detection (fig. 1), a permanent magnet installed between the specimen and the detector (a channel electron multiplier) sweeps the charged beam component away from the detector and allows only the neutrals to reach it. When the magnet is removed, both charged and neutral particles reach the detector.


1979 ◽  
Vol 40 (C7) ◽  
pp. C7-503-C7-504
Author(s):  
M. P. Ryutova
Keyword(s):  

1989 ◽  
Vol 50 (C1) ◽  
pp. C1-349-C1-352
Author(s):  
R. HOEKSTRA ◽  
K. BOORSMA ◽  
F. J . de HEER ◽  
R. MORGENSTERN

1989 ◽  
Vol 50 (C1) ◽  
pp. C1-329-C1-335
Author(s):  
M. MATTIOLI ◽  
N. J. PEACOCK ◽  
H. P. SUMMERS ◽  
B. DENNE ◽  
N. C. HAWKES
Keyword(s):  

1984 ◽  
Vol 18 (1-4) ◽  
pp. 697-701 ◽  
Author(s):  
Ralph Eric Turner ◽  
Masayoshi Senba
Keyword(s):  

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