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Titlebook: Chern-Simons Theory and Equivariant Factorization Algebras; Corina Keller Book 2019 The Editor(s) (if applicable) and The Author(s), under

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21#
發(fā)表于 2025-3-25 06:31:01 | 只看該作者
Observables in ,(1) Chern-Simons Theory,lence classes of flat .(1)-bundles, which turn out to be the critical points of the action functional. However, for our purposes this ’classical’ moduli space of solutions is not suitable, but instead we have to take the . moduli space.
22#
發(fā)表于 2025-3-25 11:34:45 | 只看該作者
23#
發(fā)表于 2025-3-25 12:38:52 | 只看該作者
24#
發(fā)表于 2025-3-25 18:51:59 | 只看該作者
25#
發(fā)表于 2025-3-25 22:20:56 | 只看該作者
Quantum Dot-Fluorescence-Based Biosensing,al finite-dimensional vector space, then . : M → . is a vector field. More generally, we can consider a family of spaces {.}.?. varying over the points on M, that is .(.) ? . for each . ? .. A field . is then understood as a . from the spacetime manifold into the bundle of spaces over .. This is exa
26#
發(fā)表于 2025-3-26 01:15:49 | 只看該作者
Description of the General Physical Problem, space, comprising the study of ., which are spaces parameterizing equivalence classes of structures. With a . we thus mean the infinitesimal description of a moduli space, capturing the local structure around a given point. In this chapter we first address the classical theory of algebraic deformat
27#
發(fā)表于 2025-3-26 06:16:54 | 只看該作者
28#
發(fā)表于 2025-3-26 08:57:16 | 只看該作者
C. A. Tobias,E. Goodwin,E. A. Blakelylence classes of flat .(1)-bundles, which turn out to be the critical points of the action functional. However, for our purposes this ’classical’ moduli space of solutions is not suitable, but instead we have to take the . moduli space.
29#
發(fā)表于 2025-3-26 14:51:35 | 只看該作者
30#
發(fā)表于 2025-3-26 16:55:36 | 只看該作者
978-3-658-25337-0The Editor(s) (if applicable) and The Author(s), under exclusive license to Springer Fachmedien Wies
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