The Higgs-branch conjecture for Sicilian theories

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Let GG be a simple group, let gg be the genus of a Riemann surface, and let e(1),…,e(p)e^{(1)},\dots,e^{(p)} be nilpotent labels for its punctures. Write M(G∨,V)\mathcal{M}(G^{\vee},V) for the Coulomb branch associated with the dual group G∨G^{\vee} and representation VV, let WW be the Weyl group, and let Me\mathcal{M}_e denote the Higgs branch associated with a puncture labeled by ee. For an unpunctured surface, set

Mg−loop⁡(G)=M(G∨,(g∨)⊕g)≅M(T∨,(g∨)⊕g−1)/W.\mathcal{M}_{g-\operatorname{loop}}^{(G)}=\mathcal{M}(G^{\vee},(\mathfrak{g}^{\vee})^{\oplus g})\cong \mathcal{M}(T^{\vee},(\mathfrak{g}^{\vee})^{\oplus g-1})/W.

For a puncture labeled by ee, let Se\mathcal{S}_e be the Slodowy slice for the corresponding nilpotent element, and let Sreg\mathcal{S}_{\mathsf{reg}} be the regular Kostant slice. The Higgs-branch conjecture for Sicilian theories. The Higgs branches of Sicilian theories are given by the following constructions: for an unpunctured surface, the Higgs branch is Mg−loop⁡(G)\mathcal{M}_{g-\operatorname{loop}}^{(G)}; for a genus-zero surface with one puncture labeled by ee, it is

Me=μ−1(Sreg×Se)⊆T∗G,\mathcal{M}_e=\mu^{-1}(\mathcal{S}_{\mathsf{reg}}\times\mathcal{S}_e)\subseteq T^*G,

where μ ⁣:T∗G→g∗×g∗\mu\colon T^*G\to\mathfrak{g}^*\times\mathfrak{g}^* is the moment map for the left and right actions of GG; and for a genus-gg surface with punctures labeled by e(1),…,e(p)e^{(1)},\dots,e^{(p)}, it is isomorphic to

Mg−loop⁡(G)×cG∨Me(1)×cG∨⋯×cG∨Me(p)/M(G∨)0r+1,\mathcal{M}_{g-\operatorname{loop}}^{(G)}\times_{\mathfrak{c}_{G^{\vee}}}\mathcal{M}_{e^{(1)}}\times_{\mathfrak{c}_{G^{\vee}}}\cdots\times_{\mathfrak{c}_{G^{\vee}}}\mathcal{M}_{e^{(p)}}/\mathcal{M}(G^{\vee})^{r+1}_0,

where

M(G∨)0r+1={(a1,…,ar+1)∈M(G∨)×cG∨⋯×cG∨M(G∨)∣a1⋯ar+1=1}.\mathcal{M}(G^{\vee})^{r+1}_0=\{(a_1,\dots,a_{r+1})\in\mathcal{M}(G^{\vee})\times_{\mathfrak{c}_{G^{\vee}}}\cdots\times_{\mathfrak{c}_{G^{\vee}}}\mathcal{M}(G^{\vee})\mid a_1\cdots a_{r+1}=1\}.

The action on Mg−loop⁡(G)\mathcal{M}_{g-\operatorname{loop}}^{(G)} is induced from M(G∨)t∨→M(T∨)≅t∨×T\mathcal{M}(G^{\vee})_{\mathfrak{t}^{\vee}}\to\mathcal{M}(T^{\vee})\cong\mathfrak{t}^{\vee}\times T, while the action on Me\mathcal{M}_e is by left multiplication under the identification of M(G∨)\mathcal{M}(G^{\vee}) with the regular centralizers of GG. These proposals describe how the Higgs branches assigned to the basic pieces of a Sicilian theory are assembled by connected sum; the individual constructions have appeared in earlier work, while the asserted general assembly is the conjectural part.

References

Primary source

Tom Gannon and Ben Webster, “Functoriality of Coulomb branches”, arXiv:2501.09962 (2025).

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