Recoil momentum of an object containing neutrons as a consequence of asymmetric antineutrino emission in the case of neutron beta decay in a magnetic field

Astrophysics ◽  
1988 ◽  
Vol 28 (3) ◽  
pp. 380-386 ◽  
Author(s):  
A. I. Studenikin
1969 ◽  
Vol 187 (5) ◽  
pp. 2141-2146 ◽  
Author(s):  
L. FASSIO-CANUTO

1969 ◽  
Vol 180 (5) ◽  
pp. 1289-1292 ◽  
Author(s):  
J. J. Matese ◽  
R. F. O'Connell

1987 ◽  
Vol 30 (3) ◽  
pp. 209-213
Author(s):  
O. F. Dorofeev ◽  
A. E. Lobanov ◽  
O. S. Pavlova ◽  
V. N. Rodionov

2016 ◽  
Vol 25 (10) ◽  
pp. 1650085 ◽  
Author(s):  
Leif Holmlid

Kaons and pions are observed by their characteristic decay times of 12, 52 and 26 ns after impact of relatively weak ns-long laser pulses on ultra-dense hydrogen H(0), as reported previously. The signal using an ultra-dense protium p(0) generator with natural hydrogen is now studied. Deflection in a weak magnetic field or penetration through metal foils cannot distinguish between the types of decaying mesons. The signals observed are thus not caused by the decaying mesons themselves, but by the fast particles often at [Formula: see text][Formula: see text]MeV u[Formula: see text] formed in their decay. The fast particles are concluded to be mainly muons from their relatively small magnetic deflection and strong penetration. This is further supported by published studies on the direct observation of the beta decay of muons in scintillators and solid converters using the same type of p(0) generator.


2013 ◽  
Vol 110 (17) ◽  
Author(s):  
D. Mund ◽  
B. Märkisch ◽  
M. Deissenroth ◽  
J. Krempel ◽  
M. Schumann ◽  
...  

2019 ◽  
Vol 99 (5) ◽  
Author(s):  
A. N. Ivanov ◽  
R. Höllwieser ◽  
N. I. Troitskaya ◽  
M. Wellenzohn ◽  
Ya. A. Berdnikov

2013 ◽  
Author(s):  
S. Baeßler ◽  
R. Alarcon ◽  
L. P. Alonzi ◽  
S. Balascuta ◽  
L. Barrón-Palos ◽  
...  

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