An internal conversion study of the decay of193Au

1968 ◽  
Vol 210 (5) ◽  
pp. 466-489 ◽  
Author(s):  
B. Svahn ◽  
A. Johansson ◽  
B. Nyman ◽  
G. Malmsten ◽  
H. Pettersson
1984 ◽  
Vol 10 (8) ◽  
pp. 1091-1097 ◽  
Author(s):  
M M Michailova ◽  
T Vylov ◽  
Z Zhelev ◽  
N Kyrova ◽  
A Novgorodov

1966 ◽  
Vol 80 (1) ◽  
pp. 154-176 ◽  
Author(s):  
A. Bäcklin ◽  
N.E. Holmberg ◽  
G. Bäckström

1964 ◽  
Vol 2 (4) ◽  
pp. 241-262 ◽  
Author(s):  
S. Forberg ◽  
E. Odeblad ◽  
R. Söremark ◽  
S. Ullberg

In a previous paper the absorption of γ-rays in the K-X-ray levels of the atom in which they are emitted was calculated according to the Quantum Mechanics, supposing the γ-rays to be emitted from a doublet of moment f ( t ) at the centre of the atom. The non-relativity wave equation derived from the relativity wave equation for an electron of charge — ε moving in an electro-magnetic field of vector potential K and scalar potential V is h 2 ∇ 2 ϕ + 2μ ( ih ∂/∂ t + εV + ih ε/μ c (K. grad)) ϕ = 0. (1) Suppose, however, that K involves the space co-ordinates. Then, (K. grad) ϕ ≠ (grad . K) ϕ , and the expression (K . grad) ϕ is not Hermitic. Equation (1) cannot therefore be the correct non-relativity wave equation for a single electron in an electron agnetic field, and we must substitute h 2 ∇ 2 ϕ + 2μ ( ih ∂/∂ t + εV) ϕ + ih ε/ c ((K. grad) ϕ + (grad. K) ϕ ) = 0. (2)


2009 ◽  
Vol 79 (3) ◽  
Author(s):  
Péter Kálmán ◽  
Tamás Keszthelyi

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