scholarly journals Fourth lepton family is natural in technicolor

2010 ◽  
Vol 81 (3) ◽  
Author(s):  
Mads T. Frandsen ◽  
Isabella Masina ◽  
Francesco Sannino
Keyword(s):  
Pramana ◽  
2006 ◽  
Vol 67 (5) ◽  
pp. 803-811 ◽  
Author(s):  
Ernest Ma

1998 ◽  
Vol 432 (1-2) ◽  
pp. 230-234 ◽  
Author(s):  
K. Arisaka ◽  
D. Roberts ◽  
W. Slater ◽  
M. Spencer ◽  
M. Weaver ◽  
...  
Keyword(s):  

1994 ◽  
Vol 320 (3-4) ◽  
pp. 407-410 ◽  
Author(s):  
P. Krolak ◽  
R.A. Briere ◽  
E. Cheu ◽  
D.A. Harris ◽  
K.S. McFarland ◽  
...  
Keyword(s):  

1988 ◽  
Vol 39 (3) ◽  
pp. 371-375 ◽  
Author(s):  
P. Q. Hung ◽  
C. H. Tze
Keyword(s):  

1998 ◽  
Vol 4 (3) ◽  
pp. 525
Author(s):  
V.V. Kabachenko ◽  
Y.F. Pirogov
Keyword(s):  

2002 ◽  
Vol 65 (11) ◽  
Author(s):  
M. Ahmed ◽  
J. F. Amann ◽  
D. Barlow ◽  
K. Black ◽  
R. D. Bolton ◽  
...  
Keyword(s):  

1998 ◽  
Vol 13 (32) ◽  
pp. 5557-5572 ◽  
Author(s):  
UMBERTO COTTI ◽  
RICARDO GAITÁN ◽  
A. HERNÁNDEZ-GALEANA ◽  
WILLIAM A. PONCE ◽  
ARNULFO ZEPEDA

Lepton family number violation processes arise in the SU(6) L⊗ U(1) Y model due to the presence of an extra neutral gauge boson, Z′, with family changing couplings, and due to the fact that this model demands the existence of heavy exotic leptons. The mixing of the standard Z with Z′ and the mixing of ordinary leptons with exotic ones induce together family changing couplings on the Z and therefore nonvanishing rates for lepton family number violation processes, such as [Formula: see text], [Formula: see text] and μ→eγ. Additional contributions to the processes μ→eγ and [Formula: see text] are induced from the mass generation mechanism. This last type of contributions may compete with the above one, depending on the masses of the scalars which participate in the diagrams which generate radiatively the masses of the charged leptons. Using the experimental data we compute some bounds for the mixings parameters and for the masses of the scalars.


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