2020
DOI: 10.1007/jhep12(2020)092
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Magnetic lattices for orthosymplectic quivers

Abstract: For any gauge theory, there may be a subgroup of the gauge group which acts trivially on the matter content. While many physical observables are not sensitive to this fact, the choice of the precise gauge group becomes crucial when the magnetic lattice of the theory is considered. This question is addressed in the context of Coulomb branches for 3d $$ \mathcal{N} $$ N = 4 quiver gauge theories, which are moduli spaces of dressed monopole operators. We compute the Coulomb bran… Show more

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Cited by 46 publications
(112 citation statements)
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References 82 publications
(219 reference statements)
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“…In the following, we will denote SU(n)/Z k gauge groups by yellow nodes with the label n/Z k , as in (2.1). See also [50] a for a related recent discussion.…”
Section: Jhep05(2021)274mentioning
confidence: 99%
See 1 more Smart Citation
“…In the following, we will denote SU(n)/Z k gauge groups by yellow nodes with the label n/Z k , as in (2.1). See also [50] a for a related recent discussion.…”
Section: Jhep05(2021)274mentioning
confidence: 99%
“…Moreover, the 3d theories EQ (4) and MQ (5) , in that case, can be described by 3d quiver gauge theories with (special) unitary gauge groups. We can then fruitfully compare our results to complementary approaches that use magnetic quivers derived from brane webs [41,42,[45][46][47][48][49][50][51][52] or from the dual generalized toric polygons [30,35]. Note that our setup implicitly assumes that we obtain a well-defined 4d SCFT in the IR of D S 1 T 5d X , at the origin of the 4d CB; in particular, we assume the 5d Higgs branch consists of a single cone.…”
Section: Hb[t 5dmentioning
confidence: 99%
“…Instead, one must rely on other approaches, using various stringtheory dualities. A particularly fruitful approach, in recent years, has been the study of (p, q)-brane webs engineering T 5d X [29], and the related concept of a "magnetic quiver" whose 3d Coulomb branch is identical to the hyper-Kähler cone of the HB, M H [T 5d X ], that we would like to understand [27,30,31,33,34,38,102]. One interesting outcome of the present work is that it provides a derivation from the geometry of magnetic quivers for the SCFT T 5d X defined as in (1.2), at least in a number of cases [10].…”
Section: Jhep02(2021)003mentioning
confidence: 99%
“…recent development is to use 3d N = 4 theories as a probe to study higher dimensional superconformal field theories (SCFTs) as well as gauge theories [2][3][4][5][6][7][8][9][10][11][12][13][14]. The idea is to relate the Higgs branch of these higher dimensional theories to the Coulomb branch of the 3d theory, the latter of which is dubbed magnetic quiver (MQ).…”
Section: Jhep05(2021)269mentioning
confidence: 99%