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The Number of States of Two Dimensional Critical String Theory

High Energy Physics - Theory · Submitted 27 Nov 1995

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

The authors' main claim This leads to the conclusion that it is also improbable to have only two large spacetime dimensions in string theory.

how it is stated · hedged possibility 0.68 read the record →

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arXiv IDhep-th/9511193 (version 1)
Pith ID6EW7FBVU, Pith's permanent record of this paper and its review
CitationL.Susskind, T. Banks. "The Number of States of Two Dimensional Critical String Theory." arXiv:hep-th/9511193 (1995). https://pith.science/paper/6EW7FBVU
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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, 6,732 input tokens, $0.0003 reported.

What the abstract itself states, as probabilities: claims first 0.03 · states limitation 0.98 · human participants 0.01 · controlled comparison 0.03 · randomized assignment 0.01 · states quantitative result 0.10 · compares with prior results 0.27 · mentions code or data availability 0.01.

The abstract, sentence by sentence

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

We discuss string theory vacua which have the wrong number of spacetime dimensions, and give a crude argument that vacua with more than four large dimensions are improbable. We then turn to two dimensional vacua, which naively appear to violate Bekenstein's entropy principle. A classical analysis shows that the naive perturbative counting of states is unjustified. All excited states of the system have strong coupling singularities which prevent us from concluding that they really exist. A speculative interpretation of the classical solutions suggests only a finite number of states will be found in regions bounded by a finite area. We also argue that the vacuum degeneracy of two dimensional classical string theory is removed in quantum mechanics. The system appears to be in a Kosterlitz-Thouless phase. This leads to the conclusion that it is also improbable to have only two large spacetime dimensions in string theory. However, we note that, unlike our argument for high dimensions, our conclusions about the ground state have neglected two dimensional quantum gravitational effects, and are at best incomplete.

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 discuss string theory vacua which have the wrong number of spacetime dimensions, and give a crude argument that vacua with more than four large dimensions are improbable. contribution 0.56 0.87 0.16 hedged possibility 0.85
s1 We then turn to two dimensional vacua, which naively appear to violate Bekenstein's entropy principle. contribution 0.48 0.26 0.04 hedged possibility 0.54
s2 A classical analysis shows that the naive perturbative counting of states is unjustified. result 0.54 0.78 0.05 asserted 1.00
s3 All excited states of the system have strong coupling singularities which prevent us from concluding that they really exist. result 0.95 0.73 0.08 asserted 0.99
s4 A speculative interpretation of the classical solutions suggests only a finite number of states will be found in regions bounded by a finite area. interpretation 0.85 0.60 0.18 speculative 0.60
s5 We also argue that the vacuum degeneracy of two dimensional classical string theory is removed in quantum mechanics. result 0.95 0.70 0.07 asserted 0.93
s6 The system appears to be in a Kosterlitz-Thouless phase. interpretation 0.60 0.58 0.06 asserted 0.88
s7 This leads to the conclusion that it is also improbable to have only two large spacetime dimensions in string theory. result 0.62 0.84 0.35 hedged possibility 0.68
s8 However, we note that, unlike our argument for high dimensions, our conclusions about the ground state have neglected two dimensional quantum gravitational effects, and are at best incomplete. limitation 1.00 0.83 0.09 hedged possibility 0.78

What kind of paper the classifier reports this is: theoretical result 0.70 · evidence from argument 0.94.

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  • references and citing sentences
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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

We discuss string theory vacua which have the wrong number of spacetime dimensions, and give a crude argument that vacua with more than four large dimensions are improbable. We then turn to two dimensional vacua, which naively appear to violate Bekenstein's entropy principle. A classical analysis shows that the naive perturbative counting of states is unjustified. All excited states of the system have strong coupling singularities which prevent us from concluding that they really exist. A speculative interpretation of the classical solutions suggests only a finite number of states will be found in regions bounded by a finite area. We also argue that the vacuum degeneracy of two dimensional classical string theory is removed in quantum mechanics. The system appears to be in a Kosterlitz-Thouless phase. This leads to the conclusion that it is also improbable to have only two large spacetime dimensions in string theory. However, we note that, unlike our argument for high dimensions, our conclusions about the ground state have neglected two dimensional quantum gravitational effects, and are at best incomplete.

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1 arXiv paper cite this in 1 sentence

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

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