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Abstract
Representation theory provides an efficient framework to count and classify invariants in tensor models of (gauge) symmetry Gd = U(N1) ⊗ · · · ⊗ U(Nd) . We show that there are two natural ways of counting invariants, one for arbitrary Gd and another valid for large rank of Gd. We construct basis of invariant operators based on the counting, and compute correlators of their elements. The basis associated with finite rank of Gd diagonalizes two-point function. It is analogous to the restricted Schur basis used in matrix models. We comment on future directions for investigation.
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1 Department of Physics and Astronomy, University of Lethbridge, Lethbridge, Alberta, Canada
2 Fields, Gravity & Strings, CTPU, Institute for Basic Science, Seoul, Korea; School of Physics and Astronomy & Center for Theoretical Physics, Seoul National University, Seoul, Korea; Department of Basic Sciences, University of Science and Technology, Daejeon, Korea




