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Asymptotics of 6j and 10j symbols
High Energy Physics - Theory · Submitted 17 Sep 2002
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim Finally we compute the asymptotic expansion of the 10j symbol which is shown to be non-oscillating in agreement with a recent result of Baez et al. We discuss the physical origin of this behavior and a way to modify the Barrett-Crane model in order to cure this disease.
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The abstract, sentence by sentence
It is well known that the building blocks for state sum models of quantum gravity are given by 6j and 10j symbols. In this work we study the asymptotics of these symbols by using their expressions as group integrals. We carefully describe the measure involved in terms of invariant variables and develop new technics in order to study their asymptotics. Using these technics we compute the asymptotics of the various Euclidean and Lorentzian 6j-symbols. Finally we compute the asymptotic expansion of the 10j symbol which is shown to be non-oscillating in agreement with a recent result of Baez et al. We discuss the physical origin of this behavior and a way to modify the Barrett-Crane model in order to cure this disease.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | It is well known that the building blocks for state sum models of quantum gravity are given by 6j and 10j symbols. | background 1.00 | 0.03 | 0.02 | asserted 1.00 |
| s1 | In this work we study the asymptotics of these symbols by using their expressions as group integrals. | contribution 0.81 | 0.90 | 0.05 | asserted 0.97 |
| s2 | We carefully describe the measure involved in terms of invariant variables and develop new technics in order to study their asymptotics. | method 0.87 | 0.95 | 0.04 | asserted 1.00 |
| s3 | Using these technics we compute the asymptotics of the various Euclidean and Lorentzian 6j-symbols. | result 0.74 | 0.96 | 0.14 | asserted 1.00 |
| s4 | Finally we compute the asymptotic expansion of the 10j symbol which is shown to be non-oscillating in agreement with a recent result of Baez et al. We discuss the physical origin of this behavior and a way to modify the Barrett-Crane model in order to cure this disease. | result 0.88 | 0.92 | 0.70 | asserted 0.99 |
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The paper
Original abstract
It is well known that the building blocks for state sum models of quantum gravity are given by 6j and 10j symbols. In this work we study the asymptotics of these symbols by using their expressions as group integrals. We carefully describe the measure involved in terms of invariant variables and develop new technics in order to study their asymptotics. Using these technics we compute the asymptotics of the various Euclidean and Lorentzian 6j-symbols. Finally we compute the asymptotic expansion of the 10j symbol which is shown to be non-oscillating in agreement with a recent result of Baez et al. We discuss the physical origin of this behavior and a way to modify the Barrett-Crane model in order to cure this disease.
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References
How the literature uses it
31 arXiv papers cite this in 68 sentences
Papers citing it · 55 sentences without a confident label
Uses its method or tool 2 papers
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Starting from [ref], we use the character formula ($θ$ is the $SU(2)$ angle) [equation] to divide the integral into several parts (the sines from [ref] cancel with the sines from the integral) [equation] to which stationary point method can be applied – boundary terms contribute non geometric asymptotics as shown in [ref] and will be omitted.
The Barrett-Crane model: asymptotic measure factor · Stationary point conditions · 0.96
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The above formula can be used to extract the asymptotic behavior of the 6j-symbol at large spin through a saddle point analysis [ref] .
A New Recursion Relation for the 6j-Symbol · 6j-Symbol as a Group Integral · 0.83
Cites it as support 2 papers
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Accordingly, we investigate the consequences of replacing ([ref]) by a similar expression that is conjectured to result from the large spin limit of the spin foam vertex amplitude corresponding to each simplex: [equation] where the term $D_σ$ is dominant but slowly varying; this ansatz is motivated by the results on the asymptotics of the Barrett-Crane model [ref] .
Semiclassical regime of Regge calculus and spin foams · Introduction · 0.96
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The suggested problems with the models were of two main types: 1) the absence or very limited nature of correlation between amplitudes of neighboring simplices glued together (the so-called ultra-locality problem); 2) analytical and numerical evidence (in the case of a single simplex) that the simplicial geometries dominating the partition function of the model in the limit of large representations are the degenerate ones [ref] , [ref] , [ref] .
A New Spin Foam Model for 4d Gravity · Introduction · 0.97
Cites it as background 7 papers
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The asymptotics of the 6j-symbol has been studied and proved in [ref] , and next-to-leading orders have been obtained in [ref] .
A New Recursion Relation for the 6j-Symbol · Introduction · 0.92
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Its asymptotic limit, relevant to the semi-classical behaviour of the model, has been well-studied analytically [ref] .
Sub-leading asymptotic behaviour of area correlations in the Barrett-Crane model · Introduction · 0.82
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The most studied Wigner symbol is the 6j-symbol, whose asymptotics is known when all spins are large (the Ponzano-Regge formula, [ref] ), or with one being small (the Edmonds' formula [ref] ).
Asymptotics of Wigner 3nj-symbols with Small and Large Angular Momenta: an Elementary Method · Introduction · 0.96
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