<p>We explain the physical origin of a curious property of algebras <InlineEquation ID="IEq4"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="220_2025_5330_Article_IEq4.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="21" /> </InlineMediaObject> <EquationSource Format="TEX">\({{\mathcal {A}}}_{{\mathfrak {q}}}\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi mathvariant="script">A</mi> <mi mathvariant="fraktur">q</mi> </msub> </math></EquationSource> </InlineEquation> which encode the rotation-equivariant fusion ring of half-BPS line defects in four-dimensional <InlineEquation ID="IEq5"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="220_2025_5330_Article_IEq5.gif" Format="GIF" Height="14" Rendition="HTML" Resolution="72" Type="Linedraw" Width="48" /> </InlineMediaObject> <EquationSource Format="TEX">\(\mathcal{N}=2\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi mathvariant="script">N</mi> <mo>=</mo> <mn>2</mn> </mrow> </math></EquationSource> </InlineEquation> supersymmetric quantum field theories. These algebras are a quantization of the algebras of holomorphic functions on the three-dimensional Coulomb branch of the SQFTs, with deformation parameter <InlineEquation ID="IEq6"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="220_2025_5330_Article_IEq6.gif" Format="GIF" Height="17" Rendition="HTML" Resolution="72" Type="Linedraw" Width="33" /> </InlineMediaObject> <EquationSource Format="TEX">\(\log {{\mathfrak {q}}}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mo>log</mo> <mi mathvariant="fraktur">q</mi> </mrow> </math></EquationSource> </InlineEquation>. They are known to acquire a large center, canonically isomorphic to the undeformed algebra, whenever <InlineEquation ID="IEq7"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="220_2025_5330_Article_IEq7.gif" Format="GIF" Height="13" Rendition="HTML" Resolution="72" Type="Linedraw" Width="10" /> </InlineMediaObject> <EquationSource Format="TEX">\({{\mathfrak {q}}}\)</EquationSource> <EquationSource Format="MATHML"><math> <mi mathvariant="fraktur">q</mi> </math></EquationSource> </InlineEquation> is a root of unity. We give a physical explanation of this fact. We also generalize the construction to characterize the action of this center in the <InlineEquation ID="IEq8"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="220_2025_5330_Article_IEq4.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="21" /> </InlineMediaObject> <EquationSource Format="TEX">\({{\mathcal {A}}}_{{\mathfrak {q}}}\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi mathvariant="script">A</mi> <mi mathvariant="fraktur">q</mi> </msub> </math></EquationSource> </InlineEquation>-modules associated to three-dimensional <InlineEquation ID="IEq9"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="220_2025_5330_Article_IEq5.gif" Format="GIF" Height="14" Rendition="HTML" Resolution="72" Type="Linedraw" Width="48" /> </InlineMediaObject> <EquationSource Format="TEX">\(\mathcal{N}=2\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi mathvariant="script">N</mi> <mo>=</mo> <mn>2</mn> </mrow> </math></EquationSource> </InlineEquation> boundary conditions. Finally, we use dualities to relate this construction to a construction in the Kapustin–Witten twist of four-dimensional <InlineEquation ID="IEq10"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="220_2025_5330_Article_IEq10.gif" Format="GIF" Height="14" Rendition="HTML" Resolution="72" Type="Linedraw" Width="48" /> </InlineMediaObject> <EquationSource Format="TEX">\(\mathcal{N}=4\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi mathvariant="script">N</mi> <mo>=</mo> <mn>4</mn> </mrow> </math></EquationSource> </InlineEquation> gauge theory. These considerations give simple physical explanations of certain properties of quantized skein algebras and cluster varieties, and quantum groups, when the deformation parameter is a root of unity.</p>

错误:搜索内容不能为空,请输入英文关键词
错误:关键词超出字数限制,请精简
高级检索

Commuting Line Defects At \(q^N\) = 1

  • Davide Gaiotto,
  • Gregory W. Moore,
  • Andrew Neitzke,
  • Fei Yan

摘要

We explain the physical origin of a curious property of algebras \({{\mathcal {A}}}_{{\mathfrak {q}}}\) A q which encode the rotation-equivariant fusion ring of half-BPS line defects in four-dimensional \(\mathcal{N}=2\) N = 2 supersymmetric quantum field theories. These algebras are a quantization of the algebras of holomorphic functions on the three-dimensional Coulomb branch of the SQFTs, with deformation parameter \(\log {{\mathfrak {q}}}\) log q . They are known to acquire a large center, canonically isomorphic to the undeformed algebra, whenever \({{\mathfrak {q}}}\) q is a root of unity. We give a physical explanation of this fact. We also generalize the construction to characterize the action of this center in the \({{\mathcal {A}}}_{{\mathfrak {q}}}\) A q -modules associated to three-dimensional \(\mathcal{N}=2\) N = 2 boundary conditions. Finally, we use dualities to relate this construction to a construction in the Kapustin–Witten twist of four-dimensional \(\mathcal{N}=4\) N = 4 gauge theory. These considerations give simple physical explanations of certain properties of quantized skein algebras and cluster varieties, and quantum groups, when the deformation parameter is a root of unity.