"Path integral and moduli space of Riemann surfaces"의 두 판 사이의 차이

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잔글 (찾아 바꾸기 – “<h5>” 문자열을 “==” 문자열로)
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<h5>introduction</h5>
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==introduction</h5>
  
 
<math>Z=\sum_{g=0}^{\infty} g_{s}^{-\chi(\Sigma_{g})}Z_{g}=\sum_{g=0}^{\infty} g_{s}^{2g-2}Z_{g}=\frac{1}{g_{s}^2}Z_{0}+g_{s}^{0}Z_{1}+g_{s}^2Z_{2}+\cdtos</math>
 
<math>Z=\sum_{g=0}^{\infty} g_{s}^{-\chi(\Sigma_{g})}Z_{g}=\sum_{g=0}^{\infty} g_{s}^{2g-2}Z_{g}=\frac{1}{g_{s}^2}Z_{0}+g_{s}^{0}Z_{1}+g_{s}^2Z_{2}+\cdtos</math>
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<h5>Scattering amplitude</h5>
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==Scattering amplitude</h5>
  
 
<math>Z(V_1,\cdots, V_{s},V_{s+1},\cdots, V_{s+p})=\sum_{g=0}^{\infty} g_{s}^{-\chi(\Sigma_{g})}Z_{g}(V_1,\cdots, V_{s},V_{s+1},\cdots, V_{s+p})</math>
 
<math>Z(V_1,\cdots, V_{s},V_{s+1},\cdots, V_{s+p})=\sum_{g=0}^{\infty} g_{s}^{-\chi(\Sigma_{g})}Z_{g}(V_1,\cdots, V_{s},V_{s+1},\cdots, V_{s+p})</math>
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<h5>history</h5>
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==history</h5>
  
 
* http://www.google.com/search?hl=en&tbs=tl:1&q=
 
* http://www.google.com/search?hl=en&tbs=tl:1&q=
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<h5>related items</h5>
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==related items</h5>
  
 
* [[0 modular invariance in math and physics]]
 
* [[0 modular invariance in math and physics]]
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<h5>books</h5>
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==books</h5>
  
 
 
 
 
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<h5>expositions</h5>
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==expositions</h5>
  
 
 
 
 
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<h5>question and answers(Math Overflow)</h5>
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==question and answers(Math Overflow)</h5>
  
 
* http://mathoverflow.net/search?q=
 
* http://mathoverflow.net/search?q=
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<h5>blogs</h5>
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==blogs</h5>
  
 
*  구글 블로그 검색<br>
 
*  구글 블로그 검색<br>
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<h5>experts on the field</h5>
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==experts on the field</h5>
  
 
* http://arxiv.org/
 
* http://arxiv.org/
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<h5>links</h5>
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==links</h5>
  
 
* [http://detexify.kirelabs.org/classify.html Detexify2 - LaTeX symbol classifier]
 
* [http://detexify.kirelabs.org/classify.html Detexify2 - LaTeX symbol classifier]
 
* [http://pythagoras0.springnote.com/pages/1947378 수식표현 안내]
 
* [http://pythagoras0.springnote.com/pages/1947378 수식표현 안내]

2012년 10월 28일 (일) 14:55 판

==introduction

\(Z=\sum_{g=0}^{\infty} g_{s}^{-\chi(\Sigma_{g})}Z_{g}=\sum_{g=0}^{\infty} g_{s}^{2g-2}Z_{g}=\frac{1}{g_{s}^2}Z_{0}+g_{s}^{0}Z_{1}+g_{s}^2Z_{2}+\cdtos\)

classical

\(\frac{1}{g_{s}^2}Z_{0}\)

other terms : loop (=quantum ) corrections

 

 

 

==Scattering amplitude

\(Z(V_1,\cdots, V_{s},V_{s+1},\cdots, V_{s+p})=\sum_{g=0}^{\infty} g_{s}^{-\chi(\Sigma_{g})}Z_{g}(V_1,\cdots, V_{s},V_{s+1},\cdots, V_{s+p})\)

 

Polchinski I,5

 

 

 

==history

 

 

==related items

 

 

encyclopedia

 

 

==books

 

 

 

==expositions

 

 

articles

 

 

 

==question and answers(Math Overflow)

 

 

 

==blogs

 

 

==experts on the field

 

 

==links