Journal Article10.1103/physrevd.108.046015
Top down approach to topological duality defects
Jonathan J. Heckman,Max Hübner,Ethan Torres,Xingyang Yu,Hao Y. Zhang +4 more
TL;DR: Top-down construction of topological duality defects in quantum field theories with duality symmetry leads to noninvertible symmetries and 5D topological field theories.
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Abstract: Topological duality defects arise as codimension one generalized symmetry operators in quantum field theories (QFTs) with a duality symmetry. Recent investigations have shown that in the case of 4D $\mathcal{N}=4$ Super Yang-Mills (SYM) theory, an appropriate choice of (complexified) gauge coupling and global form of the gauge group can lead to a rather rich fusion algebra for the associated defects, leading to examples of noninvertible symmetries. In this work we present a top down construction of these duality defects which generalizes to QFTs with lower supersymmetry, where other 0-form symmetries are often present. We realize the QFTs of interest via D3-branes probing $X$ a Calabi-Yau threefold cone with an isolated singularity at the tip of the cone. The IIB duality group descends to dualities of the 4D worldvolume theory. Nontrivial codimension one topological interfaces arise from configurations of 7-branes ``at infinity'' which implement a suitable $SL(2,\mathbb{Z})$ transformation when they are crossed. Reduction on the boundary topology $\ensuremath{\partial}X$ results in a 5D symmetry topological field theory. Different realizations of duality defects, such as the gauging of 1-form symmetries with certain mixed anomalies and half-space gauging constructions, simply amount to distinct choices of where to place the branch cuts in the 5D bulk.
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![TABLE I. Elliptic data of 7-brane profiles with constant axiodilaton τ. Their group of lines is isomorphic to cokerðρ − 1Þ which is isomorphic to Zk except for fiber type I 0; II; II . The label m of these lines is determined from the refined self-linking numbers m=2k which gives the spin of nontrivial lines. The refined self-linking numbers compute via the Gordon-Litherland approach laid out in [70] employing the divisors (Kodaira thimbles) computed in [151] or alternatively via the quadratic refinement laid out in [34] and the linking number computations in [48]. Note in particular that in all cases gcdðk;mÞ ¼ 1 and mk ∈ 2Z.](/figures/tablei-1-kq3jetaep1dz.png)
TABLE I. Elliptic data of 7-brane profiles with constant axiodilaton τ. Their group of lines is isomorphic to cokerðρ − 1Þ which is isomorphic to Zk except for fiber type I 0; II; II . The label m of these lines is determined from the refined self-linking numbers m=2k which gives the spin of nontrivial lines. The refined self-linking numbers compute via the Gordon-Litherland approach laid out in [70] employing the divisors (Kodaira thimbles) computed in [151] or alternatively via the quadratic refinement laid out in [34] and the linking number computations in [48]. Note in particular that in all cases gcdðk;mÞ ¼ 1 and mk ∈ 2Z. 
FIG. 3. Case (1). With 7-branes wrapped on M3 × ∂X, we sketch the plane R≥0 × R⊥. The topological boundary conditions jP1; D1i are the monodromy transform of the boundary conditions jP2; D2i and result from stacking the branch cut with the asymptotic boundary. The branch cut is supported on H← × ∂X and runs parallel to the D3-branes. Conventions are such that the monodromy matrix ρ acts by crossing the branch cut top to bottom. 
FIG. 12. The operator O½q;p is defined on M04 in the 5D bulk which is homotopic to either boundary. The operator acts on the topological boundary condition jP;Di by colliding M04 with the corresponding boundary component. 
FIG. 17. Operators O½q;p for 4D N ¼ 4 suð2Þ gauge theory. 
TABLE III. Fields in the 5D TFT and their corresponding global symmetries in 4D SCFTs. The charged operators composed of various types of branes are also presented. σ and γ denote nontorsional and torsional cycles, respectively. We use an upper index for the one cycles and a lower index for the three cycles. 
FIG. 4. Case (2). With 7-branes wrapped on M3 × ∂X, we sketch the plane R≥0 × R⊥. There is a single set of boundary conditions jP1; D1i. The branch cut is supported on H↓ × ∂X and runs perpendicular to the D3-branes. Conventions are such that the monodromy matrix ρ acts by crossing the branch cut left to right.
Citations
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