<p>We offer a streamlined and computationally powerful characterization of higher representations (higher charges) for defect operators under generalized symmetries, employing the powerful framework of Symmetry TFT <InlineEquation ID="IEq1"> <EquationSource Format="MATHML"><math display="inline"> <mi mathvariant="script">Z</mi> <mfenced close=")" open="("> <mi mathvariant="script">C</mi> </mfenced> </math></EquationSource> <EquationSource Format="TEX">\( \mathcal{Z}\left(\mathcal{C}\right) \)</EquationSource> </InlineEquation>. For a defect <InlineEquation ID="IEq2"> <EquationSource Format="MATHML"><math display="inline"> <mi mathvariant="script">D</mi> </math></EquationSource> <EquationSource Format="TEX">\( \mathcal{D} \)</EquationSource> </InlineEquation> of codimension <i>p</i>, these representations (charges) are in one-to-one correspondence with gapped boundary conditions for the SymTFT <InlineEquation ID="IEq3"> <EquationSource Format="MATHML"><math display="inline"> <mi mathvariant="script">Z</mi> <mfenced close=")" open="("> <mi mathvariant="script">C</mi> </mfenced> </math></EquationSource> <EquationSource Format="TEX">\( \mathcal{Z}\left(\mathcal{C}\right) \)</EquationSource> </InlineEquation> on a manifold <i>Y</i> = Σ<sub><i>d</i>−<i>p</i>+1</sub> × <i>S</i><sup><i>p</i>−1</sup>, and can be efficiently described through dimensional reduction. We explore numerous applications of our construction, including scenarios where an anomalous bulk theory can host a symmetric defect. This generalizes the connection between ’t Hooft anomalies and the absence of symmetric boundary conditions to defects of any codimension. Finally we describe some properties of surface charges for 3 + 1d duality symmetries, which should be relevant to the study of Gukov-Witten operators in gauge theories.</p>

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Defect charges, gapped boundary conditions, and the symmetry TFT

  • Christian Copetti

摘要

We offer a streamlined and computationally powerful characterization of higher representations (higher charges) for defect operators under generalized symmetries, employing the powerful framework of Symmetry TFT Z C \( \mathcal{Z}\left(\mathcal{C}\right) \) . For a defect D \( \mathcal{D} \) of codimension p, these representations (charges) are in one-to-one correspondence with gapped boundary conditions for the SymTFT Z C \( \mathcal{Z}\left(\mathcal{C}\right) \) on a manifold Y = Σdp+1 × Sp−1, and can be efficiently described through dimensional reduction. We explore numerous applications of our construction, including scenarios where an anomalous bulk theory can host a symmetric defect. This generalizes the connection between ’t Hooft anomalies and the absence of symmetric boundary conditions to defects of any codimension. Finally we describe some properties of surface charges for 3 + 1d duality symmetries, which should be relevant to the study of Gukov-Witten operators in gauge theories.