What Chern–Simons theory assigns to a point
We answer the questions, “What does Chern–Simons theory assign to a point?” and “What kind of mathematical object does Chern–Simons theory assign to a point?” Our answer to the first question is representations of the based loop group. More precisely, we identify a certain class of projective unitar...
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Veröffentlicht in: | Proceedings of the National Academy of Sciences - PNAS 2017-12, Vol.114 (51), p.13418-13423 |
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Sprache: | eng |
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Zusammenfassung: | We answer the questions, “What does Chern–Simons theory assign to a point?” and “What kind of mathematical object does Chern–Simons theory assign to a point?” Our answer to the first question is representations of the based loop group. More precisely, we identify a certain class of projective unitary representations of the based loop group ΩG. We define the fusion product of such representations, and we prove that, modulo certain conjectures, the Drinfel’d center of that representation category of ΩG is equivalent to the category of positive energy representations of the free loop group LG. The abovementioned conjectures are known to hold when the gauge group is abelian or of type A₁. Our answer to the second question is bicommutant categories. The latter are higher categorical analogs of von Neumann algebras: They are tensor categories that are equivalent to their bicommutant inside Bim(R), the category of bimodules over a hyperfinite III₁ factor. We prove that, modulo certain conjectures, the category of representations of the based loop group is a bicommutant category. The relevant conjectures are known to hold when the gauge group is abelian or of type A
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ISSN: | 0027-8424 1091-6490 |
DOI: | 10.1073/pnas.1711591114 |