<p>We analyze the non-semisimple category of line operators in Chern–Simons gauge theories based off the Lie superalgebra <InlineEquation ID="IEq1"> <EquationSource Format="TEX">\(\mathfrak {gl}(1|1)\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi mathvariant="fraktur">gl</mi> <mo stretchy="false">(</mo> <mn>1</mn> <mo stretchy="false">|</mo> <mn>1</mn> <mo stretchy="false">)</mo> </mrow> </math></EquationSource> </InlineEquation>. Our proposal is that the category of line operators <InlineEquation ID="IEq2"> <EquationSource Format="TEX">\(\mathcal {C}\)</EquationSource> <EquationSource Format="MATHML"><math> <mi mathvariant="script">C</mi> </math></EquationSource> </InlineEquation> can be identified with the derived category of modules for a boundary vertex operator algebra <InlineEquation ID="IEq3"> <EquationSource Format="TEX">\(\mathcal {V}\)</EquationSource> <EquationSource Format="MATHML"><math> <mi mathvariant="script">V</mi> </math></EquationSource> </InlineEquation> realized as a certain infinite-order simple current extension of the affine current algebra <InlineEquation ID="IEq4"> <EquationSource Format="TEX">\(V(\mathfrak {gl}(1|1))\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>V</mi> <mo stretchy="false">(</mo> <mi mathvariant="fraktur">gl</mi> <mo stretchy="false">(</mo> <mn>1</mn> <mo stretchy="false">|</mo> <mn>1</mn> <mo stretchy="false">)</mo> <mo stretchy="false">)</mo> </mrow> </math></EquationSource> </InlineEquation> by boundary monopole operators. By translating this simple current extension of <InlineEquation ID="IEq5"> <EquationSource Format="TEX">\(V(\mathfrak {gl}(1|1))\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>V</mi> <mo stretchy="false">(</mo> <mi mathvariant="fraktur">gl</mi> <mo stretchy="false">(</mo> <mn>1</mn> <mo stretchy="false">|</mo> <mn>1</mn> <mo stretchy="false">)</mo> <mo stretchy="false">)</mo> </mrow> </math></EquationSource> </InlineEquation> to the unrolled, restricted quantum group <InlineEquation ID="IEq6"> <EquationSource Format="TEX">\(\overline{U}^E(\mathfrak {gl}(1|1))\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msup> <mover> <mi>U</mi> <mo>¯</mo> </mover> <mi>E</mi> </msup> <mrow> <mo stretchy="false">(</mo> <mi mathvariant="fraktur">gl</mi> <mrow> <mo stretchy="false">(</mo> <mn>1</mn> <mo stretchy="false">|</mo> <mn>1</mn> <mo stretchy="false">)</mo> </mrow> <mo stretchy="false">)</mo> </mrow> </mrow> </math></EquationSource> </InlineEquation>, we show that our category of line operators admits a second description in terms of a quasi-quantum group <InlineEquation ID="IEq7"> <EquationSource Format="TEX">\(\mathcal {A}\)</EquationSource> <EquationSource Format="MATHML"><math> <mi mathvariant="script">A</mi> </math></EquationSource> </InlineEquation> realized by uprolling. We also compare our results across an expected physical duality with the cyclic orbifold of a free, <i>B</i>-twisted hypermultiplet and find a slight discrepancy at the level of braiding and associator. We end with a detailed analysis of coupling to background flat <InlineEquation ID="IEq8"> <EquationSource Format="TEX">\(GL(1, {\mathbb {C}})\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>G</mi> <mi>L</mi> <mo stretchy="false">(</mo> <mn>1</mn> <mo>,</mo> <mi mathvariant="double-struck">C</mi> <mo stretchy="false">)</mo> </mrow> </math></EquationSource> </InlineEquation> connections and the resulting category of non-genuine line operators.</p>

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Line Operators in U(1|1) Chern–Simons Theory

  • Niklas Garner,
  • Wenjun Niu

摘要

We analyze the non-semisimple category of line operators in Chern–Simons gauge theories based off the Lie superalgebra \(\mathfrak {gl}(1|1)\) gl ( 1 | 1 ) . Our proposal is that the category of line operators \(\mathcal {C}\) C can be identified with the derived category of modules for a boundary vertex operator algebra \(\mathcal {V}\) V realized as a certain infinite-order simple current extension of the affine current algebra \(V(\mathfrak {gl}(1|1))\) V ( gl ( 1 | 1 ) ) by boundary monopole operators. By translating this simple current extension of \(V(\mathfrak {gl}(1|1))\) V ( gl ( 1 | 1 ) ) to the unrolled, restricted quantum group \(\overline{U}^E(\mathfrak {gl}(1|1))\) U ¯ E ( gl ( 1 | 1 ) ) , we show that our category of line operators admits a second description in terms of a quasi-quantum group \(\mathcal {A}\) A realized by uprolling. We also compare our results across an expected physical duality with the cyclic orbifold of a free, B-twisted hypermultiplet and find a slight discrepancy at the level of braiding and associator. We end with a detailed analysis of coupling to background flat \(GL(1, {\mathbb {C}})\) G L ( 1 , C ) connections and the resulting category of non-genuine line operators.