"Universal chiral partition function"의 두 판 사이의 차이

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잔글 (찾아 바꾸기 – “<h5 (.*)">” 문자열을 “==” 문자열로)
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==introduction==
  
 
*  grand partition function for n species of right moving (chiral) particles with fugacities z<br>
 
*  grand partition function for n species of right moving (chiral) particles with fugacities z<br>
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<h5 style="line-height: 2em; margin: 0px;">physical meaning==
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==physical meaning==
  
 
<math>f_{A,B,C}(\tau)=\sum_{n\in \mathbb{Z}_{\geq 0}^r}\frac {q^{\frac{1}{2}n^{t}An+B^{t}\cdot n+C}} {(q)_{n_1}\cdots(q)_{n_r}}</math>
 
<math>f_{A,B,C}(\tau)=\sum_{n\in \mathbb{Z}_{\geq 0}^r}\frac {q^{\frac{1}{2}n^{t}An+B^{t}\cdot n+C}} {(q)_{n_1}\cdots(q)_{n_r}}</math>
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<h5 style="line-height: 2em; margin: 0px;">special cases==
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==special cases==
  
 
*  rank 1 case examples<br>
 
*  rank 1 case examples<br>
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==history==
  
 
* 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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==related items==
  
 
* [[fractional and exclusion statistics]]<br>
 
* [[fractional and exclusion statistics]]<br>
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==encyclopedia==
  
 
* http://en.wikipedia.org/wiki/
 
* http://en.wikipedia.org/wiki/
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==books==
  
 
 
 
 
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==articles==
  
 
* [http://arxiv.org/abs/hep-th/9903176 Exclusion statistics in conformal field theory and the UCPF for WZW models]<br>
 
* [http://arxiv.org/abs/hep-th/9903176 Exclusion statistics in conformal field theory and the UCPF for WZW models]<br>
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==question and answers(Math Overflow)==
  
 
* http://mathoverflow.net/search?q=
 
* http://mathoverflow.net/search?q=
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==blogs==
  
 
*  구글 블로그 검색<br>
 
*  구글 블로그 검색<br>
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==experts on the field==
  
 
* http://arxiv.org/
 
* http://arxiv.org/
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==links==
  
 
* [http://detexify.kirelabs.org/classify.html Detexify2 - LaTeX symbol classifier]
 
* [http://detexify.kirelabs.org/classify.html Detexify2 - LaTeX symbol classifier]

2012년 10월 28일 (일) 18:12 판

introduction

  • grand partition function for n species of right moving (chiral) particles with fugacities z
  • N개의 보존 입자가 있고, 에너지의 단위를 \(\hbar\omega=1\)으로 하여, 에너지레벨이  \(E_0,E_1,E_2,\cdots\) 인 시스템을 생각하자.

N개의 입자가 있는 보존 시스템의 분배함수를  \(Z_B(N)\) 이라 두자.

큰 분배함수(grand partition function)는 \(Z_G=\sum_{n=0}^{\infty}Z_B(N)z^N\) 으로 쓸수 있다.

\(n_0,n_1,n_2,\cdots\) 은 각각 에너지가 \(E_0,E_1,E_2,\cdots\)인 입자의 수라고 하자.

 \(Z_B(N)=\sum_{\sum n_r=N}\exp(-\beta\sum_{r}n_r E_r)\) 이므로, 

\(Z_G=\sum_{N=0}^{\infty}Z_B(N)z^N=\sum_{N=0}^{\infty} \sum_{\sum n_r=N}\exp(-\beta\sum_{r}n_r E_r)z^N\)

\(=\prod_{r=0}^{\infty}\sum_{n_r=0}^{\infty} (ze^{-\beta E_r})^{n_r}=\prod_{r=0}\frac{1}{1-ze^{-\beta E_r}}\)

 

 

physical meaning

\(f_{A,B,C}(\tau)=\sum_{n\in \mathbb{Z}_{\geq 0}^r}\frac {q^{\frac{1}{2}n^{t}An+B^{t}\cdot n+C}} {(q)_{n_1}\cdots(q)_{n_r}}\)

A: energy shift due to interaction

B : energy shift due to (global) statistics

C : ground state Casimir energy

 

 

 

special cases

  • rank 1 case examples
  • Berkovich1998 and Wu's paper

 

 

history

 

 

related items

 

 

encyclopedia

 

 

books

 

4909919

 

 

articles

 

 

question and answers(Math Overflow)

 

 

blogs

 

 

experts on the field

 

 

links