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On 't Hooft Defects, Monopole Bubbling and Supersymmetric Quantum Mechanics

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arxiv 1801.01986 v1 pith:QXCU4LSY submitted 2018-01-06 hep-th

On 't Hooft Defects, Monopole Bubbling and Supersymmetric Quantum Mechanics

classification hep-th
keywords mechanicsquantumbubblingmathbbmathcalmonopolequivervalues
verification ladder T0 review T1 audit T2 compute T3 formal T4 reserved
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We revisit the localization computation of the expectation values of 't Hooft operators in $\mathcal{N}=2^*$ SU(N) theory on $\mathbb{R}^3 \times S^1$. We show that the part of the answer arising from "monopole bubbling" on $\mathbb{R}^3$ can be understood as an equivariant integral over a Kronheimer-Nakajima moduli space of instantons on an orbifold of $\mathbb{C}^2$. It can also be described as a Witten index of a certain supersymmetric quiver quantum mechanics with $\mathcal{N}=(4,4)$ supersymmetry. The map between the defect data and the quiver quantum mechanics is worked out for all values of N. For the SU(2) theory, we compute several examples of these line defect expectation values using the Witten index formula and confirm that the expressions agree with the formula derived by Okuda, Ito and Taki. In addition, we present a Type IIB construction -- involving D1-D3-NS5-branes -- for monopole bubbling in $\mathcal{N}=2^*$ SU(N) SYM and demonstrate how the quiver quantum mechanics arises in this brane picture.

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Cited by 2 Pith papers

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    Quantized Coulomb branch of 4d N=2 Sp(N) theory with given matter content matches spherical DAHA of (C_N^vee, C_N) type, proven for N=1 and conjectured for higher N with 't Hooft loop evidence.

  2. Refined Vafa-Witten invariants for toric surfaces from supersymmetric localization in 5D gauge theory

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    5D N=1* supersymmetric localization on toric surfaces equals refined Vafa–Witten invariants for odd first Chern class; the even-c1 case fails without a hand-added constant.