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	<title>리우빌 장론 - 편집 역사</title>
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	<updated>2026-05-08T04:47:41Z</updated>
	<subtitle>이 문서의 편집 역사</subtitle>
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		<id>https://wiki.mathnt.net/index.php?title=%EB%A6%AC%EC%9A%B0%EB%B9%8C_%EC%9E%A5%EB%A1%A0&amp;diff=53058&amp;oldid=prev</id>
		<title>Pythagoras0: /* 메타데이터 */ 새 문단</title>
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		<updated>2022-07-11T10:41:03Z</updated>

		<summary type="html">&lt;p&gt;&lt;span dir=&quot;auto&quot;&gt;&lt;span class=&quot;autocomment&quot;&gt;메타데이터: &lt;/span&gt; 새 문단&lt;/span&gt;&lt;/p&gt;
&lt;table class=&quot;diff diff-contentalign-left diff-editfont-monospace&quot; data-mw=&quot;interface&quot;&gt;
				&lt;col class=&quot;diff-marker&quot; /&gt;
				&lt;col class=&quot;diff-content&quot; /&gt;
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				&lt;tr class=&quot;diff-title&quot; lang=&quot;ko&quot;&gt;
				&lt;td colspan=&quot;2&quot; style=&quot;background-color: #fff; color: #202122; text-align: center;&quot;&gt;← 이전 판&lt;/td&gt;
				&lt;td colspan=&quot;2&quot; style=&quot;background-color: #fff; color: #202122; text-align: center;&quot;&gt;2022년 7월 11일 (월) 10:41 판&lt;/td&gt;
				&lt;/tr&gt;&lt;tr&gt;&lt;td colspan=&quot;2&quot; class=&quot;diff-lineno&quot; id=&quot;mw-diff-left-l29&quot; &gt;29번째 줄:&lt;/td&gt;
&lt;td colspan=&quot;2&quot; class=&quot;diff-lineno&quot;&gt;29번째 줄:&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class=&#039;diff-marker&#039;&gt; &lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;===소스===&lt;/div&gt;&lt;/td&gt;&lt;td class=&#039;diff-marker&#039;&gt; &lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;===소스===&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class=&#039;diff-marker&#039;&gt; &lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;  &amp;lt;references /&amp;gt;&lt;/div&gt;&lt;/td&gt;&lt;td class=&#039;diff-marker&#039;&gt; &lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;  &amp;lt;references /&amp;gt;&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td colspan=&quot;2&quot;&gt; &lt;/td&gt;&lt;td class=&#039;diff-marker&#039;&gt;+&lt;/td&gt;&lt;td style=&quot;color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #a3d3ff; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;&lt;ins style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;&lt;/ins&gt;&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td colspan=&quot;2&quot;&gt; &lt;/td&gt;&lt;td class=&#039;diff-marker&#039;&gt;+&lt;/td&gt;&lt;td style=&quot;color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #a3d3ff; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;&lt;ins style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;== 메타데이터 ==&lt;/ins&gt;&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td colspan=&quot;2&quot;&gt; &lt;/td&gt;&lt;td class=&#039;diff-marker&#039;&gt;+&lt;/td&gt;&lt;td style=&quot;color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #a3d3ff; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;&lt;ins style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;&lt;/ins&gt;&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td colspan=&quot;2&quot;&gt; &lt;/td&gt;&lt;td class=&#039;diff-marker&#039;&gt;+&lt;/td&gt;&lt;td style=&quot;color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #a3d3ff; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;&lt;ins style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;===위키데이터===&lt;/ins&gt;&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td colspan=&quot;2&quot;&gt; &lt;/td&gt;&lt;td class=&#039;diff-marker&#039;&gt;+&lt;/td&gt;&lt;td style=&quot;color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #a3d3ff; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;&lt;ins style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;* ID :  [https://www.wikidata.org/wiki/Q6556124 Q6556124]&lt;/ins&gt;&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td colspan=&quot;2&quot;&gt; &lt;/td&gt;&lt;td class=&#039;diff-marker&#039;&gt;+&lt;/td&gt;&lt;td style=&quot;color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #a3d3ff; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;&lt;ins style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;===Spacy 패턴 목록===&lt;/ins&gt;&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td colspan=&quot;2&quot;&gt; &lt;/td&gt;&lt;td class=&#039;diff-marker&#039;&gt;+&lt;/td&gt;&lt;td style=&quot;color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #a3d3ff; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;&lt;ins style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;* [{&amp;#039;LOWER&amp;#039;: &amp;#039;liouville&amp;#039;}, {&amp;#039;LOWER&amp;#039;: &amp;#039;field&amp;#039;}, {&amp;#039;LEMMA&amp;#039;: &amp;#039;theory&amp;#039;}]&lt;/ins&gt;&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td colspan=&quot;2&quot;&gt; &lt;/td&gt;&lt;td class=&#039;diff-marker&#039;&gt;+&lt;/td&gt;&lt;td style=&quot;color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #a3d3ff; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;&lt;ins style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;* [{&amp;#039;LOWER&amp;#039;: &amp;#039;liouville&amp;#039;}, {&amp;#039;LEMMA&amp;#039;: &amp;#039;theory&amp;#039;}]&lt;/ins&gt;&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td colspan=&quot;2&quot;&gt; &lt;/td&gt;&lt;td class=&#039;diff-marker&#039;&gt;+&lt;/td&gt;&lt;td style=&quot;color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #a3d3ff; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;&lt;ins style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;* [{&amp;#039;LOWER&amp;#039;: &amp;#039;liouville&amp;#039;}, {&amp;#039;LOWER&amp;#039;: &amp;#039;conformal&amp;#039;}, {&amp;#039;LOWER&amp;#039;: &amp;#039;field&amp;#039;}, {&amp;#039;LEMMA&amp;#039;: &amp;#039;theory&amp;#039;}]&lt;/ins&gt;&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;/table&gt;</summary>
		<author><name>Pythagoras0</name></author>
	</entry>
	<entry>
		<id>https://wiki.mathnt.net/index.php?title=%EB%A6%AC%EC%9A%B0%EB%B9%8C_%EC%9E%A5%EB%A1%A0&amp;diff=53057&amp;oldid=prev</id>
		<title>Pythagoras0: /* 노트 */ 새 문단</title>
		<link rel="alternate" type="text/html" href="https://wiki.mathnt.net/index.php?title=%EB%A6%AC%EC%9A%B0%EB%B9%8C_%EC%9E%A5%EB%A1%A0&amp;diff=53057&amp;oldid=prev"/>
		<updated>2022-07-11T10:41:01Z</updated>

		<summary type="html">&lt;p&gt;&lt;span dir=&quot;auto&quot;&gt;&lt;span class=&quot;autocomment&quot;&gt;노트: &lt;/span&gt; 새 문단&lt;/span&gt;&lt;/p&gt;
&lt;p&gt;&lt;b&gt;새 문서&lt;/b&gt;&lt;/p&gt;&lt;div&gt;== 노트 ==&lt;br /&gt;
&lt;br /&gt;
===말뭉치===&lt;br /&gt;
# We define a three-dimensional quantum theory of gravity as the holographic dual of the Liouville conformal field theory.&amp;lt;ref name=&amp;quot;ref_3bc8d30c&amp;quot;&amp;gt;[https://www.sciencedirect.com/science/article/pii/S0550321319303992 Liouville quantum gravity]&amp;lt;/ref&amp;gt;&lt;br /&gt;
# In Liouville theory, momentum is not conserved.&amp;lt;ref name=&amp;quot;ref_e399fb40&amp;quot;&amp;gt;[https://en.wikipedia.org/wiki/Liouville_field_theory Liouville field theory]&amp;lt;/ref&amp;gt;&lt;br /&gt;
# 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.&amp;lt;ref name=&amp;quot;ref_e399fb40&amp;quot; /&amp;gt;&lt;br /&gt;
# The spectrum of Liouville theory does not include a vacuum state.&amp;lt;ref name=&amp;quot;ref_e399fb40&amp;quot; /&amp;gt;&lt;br /&gt;
# Liouville theory can be used to identify patterns in the endless landscape of all possible random, jagged surfaces.&amp;lt;ref name=&amp;quot;ref_0a3d180d&amp;quot;&amp;gt;[https://www.quantamagazine.org/mathematicians-prove-2d-version-of-quantum-gravity-really-works-20210617/ Quanta Magazine]&amp;lt;/ref&amp;gt;&lt;br /&gt;
# Liouville theory packages all those surfaces together into one object.&amp;lt;ref name=&amp;quot;ref_0a3d180d&amp;quot; /&amp;gt;&lt;br /&gt;
# In part I, we review the bosonic Liouville theory.&amp;lt;ref name=&amp;quot;ref_25df893a&amp;quot;&amp;gt;[https://www.worldscientific.com/doi/10.1142/S0217751X04019500 LIOUVILLE FIELD THEORY: A DECADE AFTER THE REVOLUTION]&amp;lt;/ref&amp;gt;&lt;br /&gt;
# In part II, we review the supersymmetric extension of the Liouville theory.&amp;lt;ref name=&amp;quot;ref_25df893a&amp;quot; /&amp;gt;&lt;br /&gt;
# 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.&amp;lt;ref name=&amp;quot;ref_25df893a&amp;quot; /&amp;gt;&lt;br /&gt;
# This review also includes some original material such as the derivation of the conjectured dual action for the Liouville theory from other known dualities.&amp;lt;ref name=&amp;quot;ref_25df893a&amp;quot; /&amp;gt;&lt;br /&gt;
# It is verified that in the classical limit this expression reduces to what the classical Liouville theory predicts.&amp;lt;ref name=&amp;quot;ref_9bcbd65c&amp;quot;&amp;gt;[https://ui.adsabs.harvard.edu/abs/1996NuPhB.477..577Z/abstract Conformal bootstrap in Liouville field theory]&amp;lt;/ref&amp;gt;&lt;br /&gt;
# Abstract: An analytic expression is proposed for the three-point function of the exponential fields in the Liouville field theory on a sphere.&amp;lt;ref name=&amp;quot;ref_0c5f27a7&amp;quot;&amp;gt;[https://typeset.io/topics/liouville-field-theory-vnw073z5 Liouville field theory]&amp;lt;/ref&amp;gt;&lt;br /&gt;
# In the classical limit it coincides with what the classical Liouville theory predicts.&amp;lt;ref name=&amp;quot;ref_0c5f27a7&amp;quot; /&amp;gt;&lt;br /&gt;
# Using quantized self dual fields, the authors present an explicit operator solution to the Liouville theory, and discuss the results.&amp;lt;ref name=&amp;quot;ref_8a22eab2&amp;quot;&amp;gt;[https://www.osti.gov/biblio/5720251-exact-operator-solution-quantum-liouville-field-theory Exact operator solution of the quantum Liouville field theory (Journal Article)]&amp;lt;/ref&amp;gt;&lt;br /&gt;
# The Liouville theory presents many problems; it is known to be integrable, and the authors aim at an explicit solution.&amp;lt;ref name=&amp;quot;ref_8a22eab2&amp;quot; /&amp;gt;&lt;br /&gt;
# Teschner J., Liouville theory revisited, Classical Quantum Gravity 18 (2001), 153-222, hep-th/0104158.&amp;lt;ref name=&amp;quot;ref_f09cc89b&amp;quot;&amp;gt;[http://www.emis.de/journals/SIGMA/2007/012/ Boundary Liouville Theory: Hamiltonian Description and Quantization]&amp;lt;/ref&amp;gt;&lt;br /&gt;
# Liouville conformal field theory (LCFT) was introduced by Polyakov in 1981 as an essential ingredient in his path integral construction of string theory.&amp;lt;ref name=&amp;quot;ref_dda5a4e3&amp;quot;&amp;gt;[https://www.icts.res.in/seminar/2022-05-19/vincent-vargas Liouville conformal field theory: from probability theory to the conformal bootstrap]&amp;lt;/ref&amp;gt;&lt;br /&gt;
# Since then Liouville theory has appeared in a wide variety of contexts ranging from random conformal geometry to 4d Yang-Mills theory with supersymmetry.&amp;lt;ref name=&amp;quot;ref_dda5a4e3&amp;quot; /&amp;gt;&lt;br /&gt;
# 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.&amp;lt;ref name=&amp;quot;ref_c0c47b19&amp;quot;&amp;gt;[https://paperswithcode.com/paper/the-semiclassical-limit-of-liouville The semiclassical limit of Liouville conformal field theory]&amp;lt;/ref&amp;gt;&lt;br /&gt;
# In this paper, we focus on the connection between LCFT and the classical Liouville field theory via the semiclassical approach.&amp;lt;ref name=&amp;quot;ref_c0c47b19&amp;quot; /&amp;gt;&lt;br /&gt;
# The integrable structure of Liouville theory Jorg Teschner DESY Hamburg Joint with A. Bytsko Typeset by FoilTEX What is Liouville theory?&amp;lt;ref name=&amp;quot;ref_38f7825d&amp;quot;&amp;gt;[https://www3.math.tu-berlin.de/geometrie/GI08/slides/Teschner.pdf The integrable structure of liouville theory]&amp;lt;/ref&amp;gt;&lt;br /&gt;
# Typeset by FoilTEX 1 What is Liouville theory?&amp;lt;ref name=&amp;quot;ref_38f7825d&amp;quot; /&amp;gt;&lt;br /&gt;
# Typeset by FoilTEX 2 What is quantum Liouville theory?&amp;lt;ref name=&amp;quot;ref_38f7825d&amp;quot; /&amp;gt;&lt;br /&gt;
# Typeset by FoilTEX 5 The integrable structure of Liouville theory 0 Why are we interested in the integrable structure of Liouville theory ?&amp;lt;ref name=&amp;quot;ref_38f7825d&amp;quot; /&amp;gt;&lt;br /&gt;
# 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.&amp;lt;ref name=&amp;quot;ref_6c896a36&amp;quot;&amp;gt;[https://core.ac.uk/download/pdf/25305103.pdf Core]&amp;lt;/ref&amp;gt;&lt;br /&gt;
===소스===&lt;br /&gt;
 &amp;lt;references /&amp;gt;&lt;/div&gt;</summary>
		<author><name>Pythagoras0</name></author>
	</entry>
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