Coulomb Effects and theO14β-Decay Matrix Element,

1962 ◽  
Vol 127 (6) ◽  
pp. 2287-2287
Author(s):  
Hans A. Weidenmüller
1962 ◽  
Vol 127 (2) ◽  
pp. 537-544 ◽  
Author(s):  
Hans A. Weidenmüller

1962 ◽  
Vol 128 (2) ◽  
pp. 841-848 ◽  
Author(s):  
Hans A. Weidenmüller

2012 ◽  
Vol 86 (1) ◽  
Author(s):  
J. H. Thies ◽  
D. Frekers ◽  
T. Adachi ◽  
M. Dozono ◽  
H. Ejiri ◽  
...  

2004 ◽  
Vol 70 (11) ◽  
Author(s):  
N. Tsutsui ◽  
S. Aoki ◽  
M. Fukugita ◽  
S. Hashimoto ◽  
K-I. Ishikawa ◽  
...  

2017 ◽  
Vol 45 ◽  
pp. 1760072
Author(s):  
Eduardo S. da Veiga ◽  
Daniel T. da Silva ◽  
Mario L. L. da Silva ◽  
Dimiter Hadjimichef

A form to describe hadron strong decays is in terms of quark and gluon degrees of freedom in microscopic decay models. Initially we assume that strong decays are driven by the same inter-quark Hamiltonian which determines the spectrum, and that it incorporates gaussian confinement. An [Formula: see text] decay matrix element of the JKJ Hamiltonian involves a pair-production current matrix elements times a scattering matrix element. Diagrammatically this corresponds to an interaction between an initial line and produced pair. In this work we apply the model to the light meson sector and calculate the decay rate, comparing with the experimental values.


1972 ◽  
Vol 38 (5) ◽  
pp. 335-338 ◽  
Author(s):  
W.T. Ford ◽  
P.A. Piroué ◽  
R.S. Remmel ◽  
A.J.S. Smith ◽  
P.A. Souder

2020 ◽  
Vol 809 ◽  
pp. 135702
Author(s):  
B.M. Rebeiro ◽  
S. Triambak ◽  
P.E. Garrett ◽  
B.A. Brown ◽  
G.C. Ball ◽  
...  

1954 ◽  
Vol 95 (1) ◽  
pp. 122-126 ◽  
Author(s):  
Martin G. Redlich ◽  
Eugene P. Wigner

Sign in / Sign up

Export Citation Format

Share Document