A supersymmetric color superconductor from holography
A bstract We use holography to study d = 4, N = 4 , SU( N c ) super Yang-Mills coupled to N f ≪ N c quark flavors. We place the theory at finite isospin density n I by turning on an isospin chemical potential μ I = M q , with M q the quark mass. We also turn on two R-symmetry charge densities n 1 =...
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Veröffentlicht in: | The journal of high energy physics 2019-05, Vol.2019 (5), p.1-13, Article 106 |
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Format: | Artikel |
Sprache: | eng |
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Zusammenfassung: | A
bstract
We use holography to study
d
= 4,
N
=
4
, SU(
N
c
) super Yang-Mills coupled to
N
f
≪
N
c
quark flavors. We place the theory at finite isospin density
n
I
by turning on an isospin chemical potential
μ
I
=
M
q
, with
M
q
the quark mass. We also turn on two R-symmetry charge densities
n
1
=
n
2
. We show that the ground state is a supersymmetric, superfluid, color superconductor, namely a finite-density state that preserves a fraction of supersymmetry in which part of the global symmetries and part of the gauge symmetries are spontaneously broken. The holographic description consists of
N
f
D7-brane probes in AdS
5
× S
5
. The symmetry breaking is due to the dissolution of some D3-branes inside the D7-branes triggered by the electric field associated to the isospin charge. The massless spectrum contains Goldstone bosons and their fermionic superpartners. The massive spectrum contains long-lived, mesonic quasi-particles if
n
I
≪
μ
I
3
, and no quasi-particles otherwise. We discuss the possibility that, despite the presence of mass scales and charge densities in the theory, conformal and relativistic invariance arise as emergent symmetries in the infrared. |
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ISSN: | 1029-8479 1029-8479 |
DOI: | 10.1007/JHEP05(2019)106 |