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String Quantization in Curved Spacetimes: Null String Approach
High Energy Physics - Theory · Submitted 9 Dec 1994
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim No critical dimension appears.
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The abstract, sentence by sentence
We study quantum strings in strong gravitational fields. The relevant small parameter is $g=R_c{\sqrt T_0}$, where $R_c$ is the curvature of the spacetime and $T_0$ is the string tension. Within our systematic expansion we obtain to zeroth order the null string (string with zero tension), while the first order correction incorporates the string dynamics. We apply our formalism to quantum null strings in de Sitter spacetime. After a reparametrization of the world-sheet coordinates, the equations of motion are simplified. The quantum algebra generated by the constraints is considered, ordering the momentum operators to the right of the coordinate operators. No critical dimension appears. It is anticipated however that the conformal anomaly will appear when the first order corrections proportional to $T_0$, are introduced.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | We study quantum strings in strong gravitational fields. | contribution 0.78 | 0.88 | 0.04 | asserted 0.94 |
| s1 | The relevant small parameter is $g=R_c{\sqrt T_0}$, where $R_c$ is the curvature of the spacetime and $T_0$ is the string tension. | method 0.91 | 0.55 | 0.05 | asserted 1.00 |
| s2 | Within our systematic expansion we obtain to zeroth order the null string (string with zero tension), while the first order correction incorporates the string dynamics. | result 0.78 | 0.95 | 0.22 | asserted 1.00 |
| s3 | We apply our formalism to quantum null strings in de Sitter spacetime. | contribution 0.86 | 0.91 | 0.06 | asserted 0.98 |
| s4 | After a reparametrization of the world-sheet coordinates, the equations of motion are simplified. | method 0.99 | 0.82 | 0.03 | asserted 1.00 |
| s5 | The quantum algebra generated by the constraints is considered, ordering the momentum operators to the right of the coordinate operators. | method 0.94 | 0.88 | 0.04 | asserted 0.97 |
| s6 | No critical dimension appears. | result 1.00 | 0.82 | 0.17 | asserted 1.00 |
| s7 | It is anticipated however that the conformal anomaly will appear when the first order corrections proportional to $T_0$, are introduced. | interpretation 0.64 | 0.19 | 0.20 | hedged possibility 0.61 |
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Original abstract
We study quantum strings in strong gravitational fields. The relevant small parameter is $g=R_c{\sqrt T_0}$, where $R_c$ is the curvature of the spacetime and $T_0$ is the string tension. Within our systematic expansion we obtain to zeroth order the null string (string with zero tension), while the first order correction incorporates the string dynamics. We apply our formalism to quantum null strings in de Sitter spacetime. After a reparametrization of the world-sheet coordinates, the equations of motion are simplified. The quantum algebra generated by the constraints is considered, ordering the momentum operators to the right of the coordinate operators. No critical dimension appears. It is anticipated however that the conformal anomaly will appear when the first order corrections proportional to $T_0$, are introduced.
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2 arXiv papers cite this in 2 sentences
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Cites it as background 1 paper
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The “tensionless” limit ($l_s →∞$ or $T →0$) [ref] is of physical significance for ultra-high energy regimes near the Hagedorn transition [ref] and for strings probing black hole or cosmological horizons where redshift factors diverge [ref] .
An Inconsistency in the Null Strings Literature: The Tale of an Overlooked Symmetry · Introduction · 0.85
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