2018
DOI: 10.1007/jhep06(2018)058
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D-type conformal matter and SU/USp quivers

Abstract: Abstract:We discuss the four dimensional models obtained by compactifying a single M5 brane probing D N singularity (minimal D-type (1, 0) conformal matter in six dimensions) on a torus with flux for abelian subgroups of the SO(4N ) flavor symmetry. We derive the resulting quiver field theories in four dimensions by first compactifying on a circle and relating the flux to duality domain walls in five dimensions. This leads to novel N = 1 dualities in 4 dimensions which arise from distinct five dimensional real… Show more

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Cited by 76 publications
(282 citation statements)
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“…Where C 1 (U (1) is the first Chern class of the chosen U (1). All our normalizations follow the conventions of [11]. Carrying on with the compactification process, we now wish to compactify the above anomaly polynomial on a Riemann surface Σ of genus g with flux under the chosen U (1).…”
Section: Expectations From Six Dimensionsmentioning
confidence: 99%
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“…Where C 1 (U (1) is the first Chern class of the chosen U (1). All our normalizations follow the conventions of [11]. Carrying on with the compactification process, we now wish to compactify the above anomaly polynomial on a Riemann surface Σ of genus g with flux under the chosen U (1).…”
Section: Expectations From Six Dimensionsmentioning
confidence: 99%
“…These operators have natural 4d operators with same values of charges under the internal symmetries. These operators in known minimal class S D N +3 theories [11,12], as in the A-type case, are the Φ fields added in the process of Φ-gluing (see Figure 16 for a quiver illustration of the added fields).…”
Section: Flows That Generate Extra Punctures In D N +3 Compactificationsmentioning
confidence: 99%
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“…The explanation will be in terms of the compactification of 6d SCFTs on a torus with fluxes. In order to understand the logic of the approach we first review the methods introduced in [15][16][17] to conjecture 4d field theories generated by such compactifications. We start with a 6d N = (1, 0) SCFT that we wish to compactify on a torus to four dimensions with fluxes in its global symmetry supported on the torus.…”
Section: Compactification From Six Dimensionsmentioning
confidence: 99%
“…However, we need to consider the effect of the flux. This was analyzed in [15][16][17], and the conclusion reached there is that the flux leads to domain walls between different 5d gauge theories. The resulting picture is that when we reduce on the first circle to 5d we end up with multiple copies of the 5d gauge theory description of the 6d SCFT interacting through the fields living on the domain walls.…”
Section: Compactification From Six Dimensionsmentioning
confidence: 99%