Tensorial generalization of characters
Autor: | Hiroshi Itoyama, A. Morozov, A. Mironov |
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Rok vydání: | 2019 |
Předmět: |
High Energy Physics - Theory
Physics Nuclear and High Energy Physics Matrix Models 010308 nuclear & particles physics Linear space Random Systems FOS: Physical sciences Mathematical Physics (math-ph) 01 natural sciences Tensor field Combinatorics Lift (mathematics) Matrix (mathematics) High Energy Physics - Theory (hep-th) Symmetric group 0103 physical sciences lcsh:QC770-798 lcsh:Nuclear and particle physics. Atomic energy. Radioactivity Tensor Invariant (mathematics) 010306 general physics Mathematical Physics Gauge symmetry |
Zdroj: | Journal of High Energy Physics Journal of High Energy Physics, Vol 2019, Iss 12, Pp 1-33 (2019) |
ISSN: | 1029-8479 |
DOI: | 10.1007/jhep12(2019)127 |
Popis: | In rainbow tensor models, which generalize rectangular complex matrix model (RCM) and possess a huge gauge symmetry $U(N_1)\times\ldots\times U(N_r)$, we introduce a new sub-basis in the linear space of gauge invariant operators, which is a redundant basis in the space of operators with non-zero Gaussian averages. Its elements are labeled by $r$-tuples of Young diagrams of a given size equal to the power of tensor field. Their tensor model averages are just products of dimensions: $\Big \sim C_{R_1,\ldots, R_r}D_{R_1}(N_1)\ldots D_{R_r}(N_r)$ of representations $R_i$ of the linear group $SL(N_i)$, with $C_{R_1,\ldots, R_r}$ made of the Clebsch-Gordan coefficients of representations $R_i$ of the symmetric group. Moreover, not only the averages but the operators $\chi_{\vec R}$ themselves exist only when these $C_{\vec R}$ are non-vanishing. This sub-basis is much similar to the basis of characters (Schur functions) in matrix models, which is distinguished by the property $\Big \sim { character}$, which opens a way to lift the notion and the theory of characters (Schur functions) from matrices to tensors. In particular, operators $\chi_{\vec R}$ are eigenfunctions of operators which generalize the usual cut-and-join operators $\hat W$; they satisfy orthogonality conditions similar to the standard characters, but they do not form a {\it full} linear basis for all gauge-invariant operators, only for those which have non-vanishing Gaussian averages. Comment: 22 pages |
Databáze: | OpenAIRE |
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