Muon charge exchange and muonium spin exchange in gases

1991 ◽  
Vol 65 (1-4) ◽  
pp. 779-791 ◽  
Author(s):  
Masayoshi Senba
Keyword(s):  
Charge Exchange ◽  
Spin Exchange ◽  
Muonium Spin

Temperature dependence of muonium spin exchange with O2 in the range 88 K to 478 K

1984 ◽  
Vol 18 (1-4) ◽  
pp. 703-708 ◽  
Author(s):  
M. Senba ◽  
D. M. Garner ◽  
D. J. Arseneau ◽  
D. G. Fleming
Keyword(s):  
Temperature Dependence ◽  
Spin Exchange ◽  
Muonium Spin

Muonium spin‐exchange in low pressure gases: Mu+O2 and Mu+NO

1980 ◽  
Vol 73 (6) ◽  
pp. 2751-2759 ◽  
Author(s):  
Donald G. Fleming ◽  
Randall J. Mikula ◽  
David M. Garner
Keyword(s):  
Spin Exchange ◽  
Low Pressure ◽  
Muonium Spin

?+?e? Hyperfine interactions and muonium spin exchange in low pressure gases

1981 ◽  
Vol 9 (1-4) ◽  
pp. 207-212 ◽  
Author(s):  
Donald G. Fleming ◽  
Randall J. Mikula ◽  
David M. Garner
Keyword(s):  
Spin Exchange ◽  
Hyperfine Interactions ◽  
Low Pressure ◽  
Muonium Spin

First H+ Charge-Exchange Images in the Stim.

1976 ◽  
Vol 34 ◽  
pp. 504-505
Author(s):  
Wm. H. Escovitz ◽  
T. R. Fox ◽  
R. Levi-Setti
Keyword(s):  
Charge Exchange ◽  
Neutral Component ◽  
Channel Electron Multiplier ◽  
Electron Multiplier ◽  
Neutral Particles ◽  
Charged Beam ◽  
Scanning Transmission ◽  
Contrast Mechanism ◽  
Ion Microscopy ◽  
Beam Component

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.

Spin exchange, past, present and future

1985 ◽  
Vol 10 (6) ◽  
pp. 645-657 ◽  
Author(s):  
W. Happer
Keyword(s):  
Spin Exchange

SPECTRUM OF CHARGE EXCHANGE NEUTRALS FROM ROTATING PLASMA

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