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The journal of high energy physics, 2018-01, Vol.2018 (1), p.1-24, Article 109
Ort / Verlag
Berlin/Heidelberg: Springer Berlin Heidelberg
Erscheinungsjahr
2018
Link zum Volltext
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Beschreibungen/Notizen
A
bstract
We consider the dynamics of 2+1 dimensional SU(
N
) gauge theory with Chern-Simons level
k
and
N
f
fundamental fermions. By requiring consistency with previously suggested dualities for
N
f
≤ 2
k
as well as the dynamics at
k
= 0 we propose that the theory with
N
f
>
2
k
breaks the U(
N
f
) global symmetry spontaneously to U(
N
f
/
2 +
k
) × U(
N
f
/
2 −
k
). In contrast to the 3+1 dimensional case, the symmetry breaking takes place in a range of quark masses and not just at one point. The target space never becomes parametrically large and the Nambu-Goldstone bosons are therefore not visible semi-classically. Such symmetry breaking is argued to take place in some intermediate range of the number of flavors, 2
k < N
f
< N
∗
(
N, k
), with the upper limit
N
∗
obeying various constraints. The Lagrangian for the Nambu-Goldstone bosons has to be supplemented by nontrivial Wess-Zumino terms that are necessary for the consistency of the picture, even at
k
= 0. Furthermore, we suggest two scalar dual theories in this range of
N
f
. A similar picture is developed for SO(
N
) and Sp(
N
) gauge theories. It sheds new light on monopole condensation and confinement in the SO(
N
) & Spin(
N
) theories.