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Non-Commutative Integration, Zeta Functions and the Haar State for SU q (2)
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  • 作者:Marco Matassa (1)

    1. SISSA
    ; Via Bonomea 265 ; I-34136 ; Trieste ; Italy
  • 关键词:Spectral triple ; Non ; commutative integral ; Zeta function ; Spectral dimension ; Primary 58B32 ; Secondary 58B34 ; 33D80
  • 刊名:Mathematical Physics, Analysis and Geometry
  • 出版年:2015
  • 出版时间:December 2015
  • 年:2015
  • 卷:18
  • 期:1
  • 全文大小:960 KB
  • 参考文献:1. Carey, AL, Gayral, V, Rennie, A, Sukochev, FA (2012) Integration on locally compact noncommutative spaces. J. Funct. Anal. 263: pp. 383-414 CrossRef
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    3. Carey, AL, Phillips, J, Rennie, A (2010) Twisted cyclic theory and an index theory for the gauge invariant KMS state on the Cuntz algebra On. Journal of K-theory: K-theory and its Applications to Algebra, Geometry, and Topology 6: pp. 339-380 CrossRef
    4. Carey, AL, Phillips, J, Rennie, A, Sukochev, FA (2006) The local index formula in semifinite von Neumann algebras I: Spectral flow. Adv. Math. 202: pp. 451-516 CrossRef
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    6. Carey, AL, Rennie, A, Tong, K (2009) Spectral flow invariants and twisted cyclic theory for the Haar state on SUq(2). J. Geom. Phys. 59: pp. 1431-1452 CrossRef
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    15. Kaad, J: On modular semifinite index theory, arXiv preprint arXiv:1111.6546 (2011)
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  • 刊物类别:Physics and Astronomy
  • 刊物主题:Physics
    Mathematical and Computational Physics
    Analysis
    Geometry
    Group Theory and Generalizations
    Applications of Mathematics
  • 出版者:Springer Netherlands
  • ISSN:1572-9656
文摘
We study a notion of non-commutative integration, in the spirit of modular spectral triples, for the quantum group SU q (2). In particular we define the non-commutative integral as the residue at the spectral dimension of a zeta function, which is constructed using a Dirac operator and a weight. We consider the Dirac operator introduced by Kaad and Senior and a family of weights depending on two parameters, which are related to the diagonal automorphisms of SU q (2). We show that, after fixing one of the parameters, the non-commutative integral coincides with the Haar state of SU q (2). Moreover we can impose an additional condition on the zeta function, which also fixes the second parameter. For this unique choice the spectral dimension coincides with the classical dimension.

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