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The universal Racah-Wigner symbol for Uq(osp(1|2))
High Energy Physics - Theory · Submitted 25 Jul 2013
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim We propose a new and elegant formula for the Racah-Wigner symbol of self-dual continuous series of representations of Uq(osp(1|2)).
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The abstract, sentence by sentence
We propose a new and elegant formula for the Racah-Wigner symbol of self-dual continuous series of representations of Uq(osp(1|2)). It describes the entire fusing matrix for both NS and R sector of N=1 supersymmetric Liouville field theory. In the NS sector, our formula is related to an expression derived in [1]. Through analytic continuation in the spin variables, our universal expression reproduces known formulas for the Racah-Wigner coefficients of finite dimensional representations.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | We propose a new and elegant formula for the Racah-Wigner symbol of self-dual continuous series of representations of Uq(osp(1|2)). | contribution 0.98 | 0.95 | 0.81 | asserted 1.00 |
| s1 | It describes the entire fusing matrix for both NS and R sector of N=1 supersymmetric Liouville field theory. | interpretation 0.55 | 0.74 | 0.35 | asserted 1.00 |
| s2 | In the NS sector, our formula is related to an expression derived in [1]. | result 0.43 | 0.27 | 0.05 | asserted 1.00 |
| s3 | Through analytic continuation in the spin variables, our universal expression reproduces known formulas for the Racah-Wigner coefficients of finite dimensional representations. | result 0.84 | 0.85 | 0.15 | asserted 1.00 |
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The paper
Original abstract
We propose a new and elegant formula for the Racah-Wigner symbol of self-dual continuous series of representations of Uq(osp(1|2)). It describes the entire fusing matrix for both NS and R sector of N=1 supersymmetric Liouville field theory. In the NS sector, our formula is related to an expression derived in [1]. Through analytic continuation in the spin variables, our universal expression reproduces known formulas for the Racah-Wigner coefficients of finite dimensional representations.
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References
How the literature uses it
13 arXiv papers cite this in 22 sentences
Papers citing it · 13 sentences without a confident label
Builds on it 1 paper
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And, finally, we give general expression for the supersymmetric Racah-Wigner symbols, considered in [ref] , in all available parametrizations for both the Neveu-Schwarz and Ramond sectors.
A parafermionic hypergeometric function and supersymmetric 6j-symbols · Introduction · 0.81
Compares with it 2 papers
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Then we check that the restriction to the Neveu-Schwarz sector of the general supersymmetric Racah-Wigner symbol, suggested in [ref] , is in agreement with the Neveu-Schwarz sector Racah-Wigner symbols derived in [ref] .
A parafermionic hypergeometric function and supersymmetric 6j-symbols · Introduction · 0.91
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Let us mention that in [ref] a similar restriction has been implemented for Racah-Wigner 6j-symbols.
Matrix factorization for solutions of the Yang-Baxter equation · Trigonometric factorization · 0.93
Cites it as background 5 papers
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In this last appendix we discuss the fusion kernel of (spacelike) $𝒩=1$ Liouville theory in the NS-sector as obtained in [ref] .
On the three-point functions in timelike N=1 Liouville CFT · Relation to the $𝒩=1$ fusion kernel · 0.80
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Some attempts to find the fusion matrix also in the Ramond sector can be found in [ref] .
Comments on fusion matrix in N=1 super Liouville field theory · Introduction · 0.95
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While several results are known on this object, the fusion matrix with this specific configuration is not yet available [ref] .
Solving the Schwarzian via the Conformal Bootstrap · $𝒩=1$ Schwarzian theory · 0.87
What it cites · 8 sentences without a confident label
Compares with 1 paper
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Thus the Racah-Wigner symbol [ref] coincides with the fusion matrix of Liouville theory [ref] .
6j symbols for the modular double, quantum hyperbolic geometry, and supersymmetric gauge theories · The Racah-Wigner symbol of · 0.89
Cites as background 3 papers
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As we recalled in the introduction, the fusing matrix of $N=1$ Liouville field theory should be a central ingredient in the construction of a new 3-dimensional topological quantum field theory, just as Faddeev's quantum dilogarithm [ref] , i.e. the building block of the fusing matrix on Liouville field theory, is used to construct SL(2) Chern-Simons or quantum Teichmueller theory, see e.g. [ref] .
Chern-Simons Theory and S-duality · The Racah-Wigner symbol of · 0.85
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As we recalled in the introduction, the fusing matrix of $N=1$ Liouville field theory should be a central ingredient in the construction of a new 3-dimensional topological quantum field theory, just as Faddeev's quantum dilogarithm [ref] , i.e. the building block of the fusing matrix on Liouville field theory, is used to construct SL(2) Chern-Simons or quantum Teichmueller theory, see e.g. [ref] .
A TQFT from quantum Teichm\"uller theory · The Racah-Wigner symbol of · 0.85
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As we recalled in the introduction, the fusing matrix of $N=1$ Liouville field theory should be a central ingredient in the construction of a new 3-dimensional topological quantum field theory, just as Faddeev's quantum dilogarithm [ref] , i.e. the building block of the fusing matrix on Liouville field theory, is used to construct SL(2) Chern-Simons or quantum Teichmueller theory, see e.g. [ref] .
On the relation between the modular double of U_q(sl(2,R)) and the quantum Teichmueller theory · The Racah-Wigner symbol of · 0.85
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