The hadronic corrections to the muon anomalous magnetic moment a\_mu, due to
the gauge-invariant set of diagrams with dynamical quark loop light-by-light
scattering insertions, are calculated in the framework of the nonlocal chiral
quark model. These results complete calculations of all hadronic light-by-light
scattering contributions to a\_mu in the leading order in the 1/Nc expansion.
The result for the quark loop contribution is
a\_mu^HLbL,Loop=(11.0+-0.9)*10^(-10), and the total result is
a\_mu^HLbL,NxQM=(16.8+-1.2)*10^(-10). This means, that the difference in
values of a\_mu between the standard model and the experiment is 2.4 sigma.
%0 Generic
%1 Dorokhov2015Dynamical
%A Dorokhov, A. E.
%A Radzhabov, A. E.
%A Zhevlakov, A. S.
%D 2015
%K g-2, lbl
%T Dynamical quark loop light-by-light contribution to muon g-2 within the nonlocal chiral quark model
%U http://arxiv.org/abs/1502.04487
%X The hadronic corrections to the muon anomalous magnetic moment a\_mu, due to
the gauge-invariant set of diagrams with dynamical quark loop light-by-light
scattering insertions, are calculated in the framework of the nonlocal chiral
quark model. These results complete calculations of all hadronic light-by-light
scattering contributions to a\_mu in the leading order in the 1/Nc expansion.
The result for the quark loop contribution is
a\_mu^HLbL,Loop=(11.0+-0.9)*10^(-10), and the total result is
a\_mu^HLbL,NxQM=(16.8+-1.2)*10^(-10). This means, that the difference in
values of a\_mu between the standard model and the experiment is 2.4 sigma.
@misc{Dorokhov2015Dynamical,
abstract = {The hadronic corrections to the muon anomalous magnetic moment a\_mu, due to
the gauge-invariant set of diagrams with dynamical quark loop light-by-light
scattering insertions, are calculated in the framework of the nonlocal chiral
quark model. These results complete calculations of all hadronic light-by-light
scattering contributions to a\_mu in the leading order in the 1/Nc expansion.
The result for the quark loop contribution is
a\_mu^{HLbL,Loop}=(11.0+-0.9)*10^(-10), and the total result is
a\_mu^{HLbL,NxQM}=(16.8+-1.2)*10^(-10). This means, that the difference in
values of a\_mu between the standard model and the experiment is 2.4 sigma.},
added-at = {2019-02-23T22:09:48.000+0100},
archiveprefix = {arXiv},
author = {Dorokhov, A. E. and Radzhabov, A. E. and Zhevlakov, A. S.},
biburl = {https://www.bibsonomy.org/bibtex/2dfcb7c7372af49c579f0a8bd5d01e360/cmcneile},
citeulike-article-id = {13519039},
citeulike-linkout-0 = {http://arxiv.org/abs/1502.04487},
citeulike-linkout-1 = {http://arxiv.org/pdf/1502.04487},
day = 16,
eprint = {1502.04487},
interhash = {b5ef63fc008530b46c753555e84812a1},
intrahash = {dfcb7c7372af49c579f0a8bd5d01e360},
keywords = {g-2, lbl},
month = feb,
posted-at = {2015-02-17 08:59:49},
priority = {2},
timestamp = {2019-02-23T22:15:27.000+0100},
title = {{Dynamical quark loop light-by-light contribution to muon g-2 within the nonlocal chiral quark model}},
url = {http://arxiv.org/abs/1502.04487},
year = 2015
}