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Loop Variables and the Virasoro Group

High Energy Physics - Theory · Submitted 14 Jul 1992

abstract compiled · 2026-09-23 · no language-model review

The authors' main claim We derive an expression in closed form for the action of a finite element of the Virasoro Group on generalized vertex operators.

how it is stated · asserted 1.00 read the record →

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arXiv IDhep-th/9207051 (version 1)
Pith IDRJFCNSNQ, Pith's permanent record of this paper and its review
CitationB. Sathiapalan. "Loop Variables and the Virasoro Group." arXiv:hep-th/9207051 (1992). https://pith.science/paper/RJFCNSNQ
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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, 4,130 input tokens, $0.0002 reported.

What the abstract itself states, as probabilities: claims first 0.09 · states limitation 0.17 · human participants 0.01 · controlled comparison 0.02 · randomized assignment 0.01 · states quantitative result 0.04 · compares with prior results 0.96 · mentions code or data availability 0.02.

The abstract, sentence by sentence

arXiv listing abstract v1. Results and the main claim are underlined; .

We derive an expression in closed form for the action of a finite element of the Virasoro Group on generalized vertex operators. This complements earlier results giving an algorithm to compute the action of a finite string of generators of the Virasoro Algebra on generalized vertex operators. The main new idea is to use a first order formalism to represent the infinitesimal group element as a loop variable. To obtain a finite group element it is necessary to thicken the loop to a band of finite thickness. This technique makes the calculation very simple.

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 We derive an expression in closed form for the action of a finite element of the Virasoro Group on generalized vertex operators. result 0.70 0.96 0.81 asserted 1.00
s1 This complements earlier results giving an algorithm to compute the action of a finite string of generators of the Virasoro Algebra on generalized vertex operators. background 0.90 0.12 0.08 asserted 1.00
s2 The main new idea is to use a first order formalism to represent the infinitesimal group element as a loop variable. contribution 0.60 0.84 0.13 asserted 1.00
s3 To obtain a finite group element it is necessary to thicken the loop to a band of finite thickness. method 0.98 0.71 0.06 asserted 1.00
s4 This technique makes the calculation very simple. interpretation 0.87 0.72 0.08 asserted 1.00

What kind of paper the classifier reports this is: theoretical result 0.93 · evidence from proof or derivation 1.00.

What was examined, and what was not

sources read
  • arXiv listing abstract v1
not examined
  • full text
  • figures and tables
  • references and citing sentences
  • relations to other papers
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  • P abstract
not run
  • S sections
  • T body sentences
  • C citations
  • R cross-paper relations

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

We derive an expression in closed form for the action of a finite element of the Virasoro Group on generalized vertex operators. This complements earlier results giving an algorithm to compute the action of a finite string of generators of the Virasoro Algebra on generalized vertex operators. The main new idea is to use a first order formalism to represent the infinitesimal group element as a loop variable. To obtain a finite group element it is necessary to thicken the loop to a band of finite thickness. This technique makes the calculation very simple.

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