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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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arXiv IDhep-th/0209134 (version 4)
Pith ID57BR7A3K, Pith's permanent record of this paper and its review
CitationDavid Louapre (ENS-Lyon), Laurent Freidel (PI). "Asymptotics of 6j and 10j symbols." arXiv:hep-th/0209134 (2002). https://pith.science/paper/57BR7A3K
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The paper's own sentences, arranged. Each label is drawn from a closed vocabulary; the number beside it is the probability the classifier gave that label. Numbers in the tables are the authors', checked by code. No sentence in this record was written by a model.

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Compiled by classifier-1.13-20260917 via OpenRouter, question bank abstract-p1-20260923, 2026-09-23: 1 request, 4,313 input tokens, $0.0002 reported.

What the abstract itself states, as probabilities: claims first 0.04 · states limitation 0.12 · human participants 0.01 · controlled comparison 0.02 · randomized assignment 0.01 · states quantitative result 0.09 · compares with prior results 0.87 · mentions code or data availability 0.02.

The abstract, sentence by sentence

arXiv listing abstract v4. Results and the main claim are underlined; .

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

What the classifier reports for each sentence. The number is the probability it gave the label.
#sentencerolethe authors' own workstates the main conclusionstrength
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

What kind of paper the classifier reports this is: theoretical result 0.94 · evidence from proof or derivation 1.00.

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Every quoted sentence on this record is the authors'. Every label is from Pith's closed vocabulary, with the probability shown beside it. Every number in the measurements table is the authors', checked by code. Record as JSON

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

Each citing sentence is taken from the citing paper's LaTeX source and typed by Pith's classifier. A label appears at probability 0.8 or more (0.95 for support), a contest at 0.7 or more; the quoted words are the citing authors'. How each label was checked · JSON

Papers citing it · 55 sentences without a confident label

Uses its method or tool 2 papers
  • 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

  • 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
  • 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

  • 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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