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- We define a three-dimensional quantum theory of gravity as the holographic dual of the Liouville conformal field theory.[1]
- In Liouville theory, momentum is not conserved.[2]
- These quantum symmetries of Liouville theory are however not manifest in the Lagrangian formulation, in particular the exponential potential is not invariant under the duality.[2]
- The spectrum of Liouville theory does not include a vacuum state.[2]
- Liouville theory can be used to identify patterns in the endless landscape of all possible random, jagged surfaces.[3]
- Liouville theory packages all those surfaces together into one object.[3]
- In part I, we review the bosonic Liouville theory.[4]
- In part II, we review the supersymmetric extension of the Liouville theory.[4]
- We first discuss the bulk structure constants and the branes as in the bosonic Liouville theory, and then we present the matrix dual descriptions with some applications.[4]
- This review also includes some original material such as the derivation of the conjectured dual action for the Liouville theory from other known dualities.[4]
- It is verified that in the classical limit this expression reduces to what the classical Liouville theory predicts.[5]
- Abstract: An analytic expression is proposed for the three-point function of the exponential fields in the Liouville field theory on a sphere.[6]
- In the classical limit it coincides with what the classical Liouville theory predicts.[6]
- Using quantized self dual fields, the authors present an explicit operator solution to the Liouville theory, and discuss the results.[7]
- The Liouville theory presents many problems; it is known to be integrable, and the authors aim at an explicit solution.[7]
- Teschner J., Liouville theory revisited, Classical Quantum Gravity 18 (2001), 153-222, hep-th/0104158.[8]
- Liouville conformal field theory (LCFT) was introduced by Polyakov in 1981 as an essential ingredient in his path integral construction of string theory.[9]
- Since then Liouville theory has appeared in a wide variety of contexts ranging from random conformal geometry to 4d Yang-Mills theory with supersymmetry.[9]
- A rigorous probabilistic construction of Liouville conformal field theory (LCFT) on the Riemann sphere was recently given by David-Kupiainen and the last two authors.[10]
- In this paper, we focus on the connection between LCFT and the classical Liouville field theory via the semiclassical approach.[10]
- The integrable structure of Liouville theory Jorg Teschner DESY Hamburg Joint with A. Bytsko Typeset by FoilTEX What is Liouville theory?[11]
- Typeset by FoilTEX 1 What is Liouville theory?[11]
- Typeset by FoilTEX 2 What is quantum Liouville theory?[11]
- Typeset by FoilTEX 5 The integrable structure of Liouville theory 0 Why are we interested in the integrable structure of Liouville theory ?[11]
- CORE Provided by CERN Document Server Metadata, citation and similar papers at core.ac.uk Liouville Field Theory on a Pseudosphere RUNHETC-2001-02 LPM-01-01 January, 2001 A.Zamolodchikov and Al.[12]
소스
- ↑ Liouville quantum gravity
- ↑ 2.0 2.1 2.2 Liouville field theory
- ↑ 3.0 3.1 Quanta Magazine
- ↑ 4.0 4.1 4.2 4.3 LIOUVILLE FIELD THEORY: A DECADE AFTER THE REVOLUTION
- ↑ Conformal bootstrap in Liouville field theory
- ↑ 6.0 6.1 Liouville field theory
- ↑ 7.0 7.1 Exact operator solution of the quantum Liouville field theory (Journal Article)
- ↑ Boundary Liouville Theory: Hamiltonian Description and Quantization
- ↑ 9.0 9.1 Liouville conformal field theory: from probability theory to the conformal bootstrap
- ↑ 10.0 10.1 The semiclassical limit of Liouville conformal field theory
- ↑ 11.0 11.1 11.2 11.3 The integrable structure of liouville theory
- ↑ Core
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- ID : Q6556124
Spacy 패턴 목록
- [{'LOWER': 'liouville'}, {'LOWER': 'field'}, {'LEMMA': 'theory'}]
- [{'LOWER': 'liouville'}, {'LEMMA': 'theory'}]
- [{'LOWER': 'liouville'}, {'LOWER': 'conformal'}, {'LOWER': 'field'}, {'LEMMA': 'theory'}]