Higher-order induced axial-vector isoscalar neutral current in gauge theories

1979 ◽  
Vol 19 (7) ◽  
pp. 2165-2178 ◽  
Author(s):  
R. N. Mohapatra ◽  
G. Senjanović
2020 ◽  
Vol 15 ◽  
pp. 249
Author(s):  
V. Ch. Chasioti ◽  
T. S. Kosmas ◽  
P. Divari

Inelastic neutrino-nucleus reaction cross sections are studied focusing on the neutral current processes. Particularly, we investigate the angular and initial neutrino-energy dependence of the differential and integrated cross sections for low and intermediate energies of the incoming neutrino (or antineutrino). Contributions coming from both, the vector and axial-vector components of the corresponding hadronic currents have been included. The initial and final state nuclear wave-functions have been calculated in the context of the Quasi-particle Random Phase Approximation (QRPA) tested on the reproducibility of the low-lying energy spectrum (up to about 5 MeV) of the studied nuclei. The results presented here refer to the nuclear isotopes 16O and 98Mo. As it is well known, O plays a significant role in supernova evolution phenomena and Mo is used as a target in the MOON neutrino experiment at Japan.


1978 ◽  
Vol 18 (5) ◽  
pp. 1647-1660 ◽  
Author(s):  
T. Rizzo ◽  
V. S. Mathur

2021 ◽  
pp. 2150039
Author(s):  
Yang Yu ◽  
Jian-Feng Li

In this paper, we find apart from the Ward–Takahashi (WT) identity, the identity between gamma matrices can also constrain the vertex functions in low-dimensional gauge theories. In (1 + 1) dimensions, the identity between gamma matrices gives the identity between vector and axial-vector vertex functions while in (2 + 1) dimensions it leads to the identity between vector and tensor vertex functions. Then, we derive the expressions of the full scalar, vector and tensor vertex functions in (2 + 1) dimensions Quantum Electrodynamics (QED3) by using the longitudinal and transverse WT identities for vector and tensor currents. Furthermore, we find that in the chiral limit with zero fermion masses, the contribution of Wilson line in full vector vertex function is eliminated and the full vector vertex function is strictly expressed in terms of the fermion propagators when using the identity between vector and tensor vertex functions to further constraint the vertex functions.


2003 ◽  
Vol 569 (3-4) ◽  
pp. 211-218 ◽  
Author(s):  
Wei-Min Sun ◽  
Hong-Shi Zong ◽  
Xiang-Song Chen ◽  
Fan Wang

2012 ◽  
Vol 27 (10) ◽  
pp. 1250056
Author(s):  
HITOSHI NISHINO ◽  
SUBHASH RAJPOOT

We consider a total action composed of two Dirac–Born–Infeld (DBI) actions: one for a vector field Aμ and another for an axial vector field Bμ. We impose a duality condition [Formula: see text], where [Formula: see text] is the Hodge dual of Gμν, and g is a DBI interaction constant. Interestingly, there are two different global duality rotation symmetries in the presence of DBI interactions: (i) [Formula: see text], [Formula: see text], and (ii) δζAμ = - ζBμ, δζBμ = + ζAμ. Both of these symmetry are on-shell symmetries, including nonlinear higher-order terms. The remarkable aspect is that these symmetries are valid even in the presence of DBI interactions. The coupling of this system to N = 1 supergravity is also discussed.


1979 ◽  
Vol 19 (1) ◽  
pp. 335-346 ◽  
Author(s):  
James D. Bjorken

2020 ◽  
Vol 2020 (3) ◽  
Author(s):  
Georgios Billis ◽  
Frank J. Tackmann ◽  
Jim Talbert
Keyword(s):  

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