scholarly journals Tau Lorentz Structure with Polarization at SLD

2004 ◽  
Author(s):  
K Abe
Keyword(s):  
2017 ◽  
Vol 10 (4) ◽  
pp. 939
Author(s):  
S. Leitão ◽  
A. Stadler ◽  
M.T. Peña ◽  
E.P. Biernat

1975 ◽  
Vol 18 (5) ◽  
pp. 695-697 ◽  
Author(s):  
K. K. Lee

AbstractIt is shown that the Lorentz structure of a compact prespace- time M can be so chosen such that M can not satisfy the strong energy condition. Thus, combining both the causal and the strong energy conditions, a stronger case against the compact space-times as proper arenas of physics can be made.


1988 ◽  
Vol 03 (03) ◽  
pp. 721-729 ◽  
Author(s):  
P. RAM BABU

We have considered the ‘neutrino counting’ reaction [Formula: see text]. We restrict to V, A Lorentz structure of weak neutral interaction (WNI), allow many Z bosons to mediate WNI and νi to be different from νj. We derive the expression for differential cross section by allowing the polarizations of e+ and e− but summing over the polarizations of final photons. From the study of differential cross section with polarized and unpolarized beams three different coupling constant combinations can be determined. A definite relation between these observables and the observables in [Formula: see text] scatterings is suggested as a test of single-Z-boson hypothesis. Similarly another test relates observables in [Formula: see text] to those of [Formula: see text] scatterings. By assuming universality a test for presence of nondiagonal neutrino neutral currents (NDνNC’s) is also pointed out. The effects of presence of wrong-handed (anti-) neutrinos on our tests are also discussed. As a by-product, we find a way to determine number of neutrino types, in the case i≠j, assuming universality.


1998 ◽  
Vol 81 (3) ◽  
pp. 520-523 ◽  
Author(s):  
B. Armbruster ◽  
I. M. Blair ◽  
B. A. Bodmann ◽  
N. E. Booth ◽  
G. Drexlin ◽  
...  

2000 ◽  
Vol 16 (2) ◽  
pp. 229-252 ◽  
Author(s):  
P. Abreu et al. ◽  
Keyword(s):  

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