Phenomenological consequences of a bound state of weak vector bosons

1986 ◽  
Vol 95 (2) ◽  
pp. 121-136
Author(s):  
M. Hayashi ◽  
K. Yamagishi
1986 ◽  
Vol 180 (1-2) ◽  
pp. 163-170 ◽  
Author(s):  
U. Baur ◽  
K.H. Schwarzer
Keyword(s):  

1967 ◽  
Vol 205 (5) ◽  
pp. 465-471
Author(s):  
R. Gruber ◽  
A. D. Karpf
Keyword(s):  

2007 ◽  
Vol 22 (39) ◽  
pp. 2971-2977
Author(s):  
VICTOR FLAMBAUM ◽  
MICHAEL KUCHIEV

The Coulomb problem for vector bosons W± incorporates a known difficulty; the boson falls on the center. In QED the fermion vacuum polarization produces a barrier at small distances which solves the problem. In a renormalizable SU(2) theory containing vector triplet (W+, W-, γ) and a heavy fermion doublet F with mass M the W- falls on F+ to distances r ~ 1/M, where M can be made arbitrary large. The collapse may be prevented if the theory contains additional light fermions or scalars, which switch the ultraviolet behavior of the theory from anti-screening to screening. Similar situation can take place in the Standard Model. Thus, the renormalizability of a theory may be not sufficient to guarantee a reasonable behavior at small distances for nonperturbative problems, such as a bound state problem.


1996 ◽  
Vol 96 (3) ◽  
pp. 623-637
Author(s):  
M. Sekiguchi ◽  
S. Ishida ◽  
H. Wada
Keyword(s):  

2019 ◽  
Vol 99 (7) ◽  
Author(s):  
Axel Maas ◽  
Sebastian Raubitzek ◽  
Pascal Törek

1987 ◽  
Vol 193 (1) ◽  
pp. 110-116 ◽  
Author(s):  
U. Baur ◽  
M. Lindner ◽  
K.H. Schwarzer

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