"3-states Potts model"의 두 판 사이의 차이

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* [[discrete series unitary representations|discrete series unitary representations and GKO coset construction]]<br><math>m= 5</math><br><math>c = \frac{4}{5}</math><br><math>h_{r,s}(c) = {((m+1)r-ms)^2-1 \over 4m(m+1)}</math><br><math>r = 1, 2, 3,4</math> and <math>s= 1, 2, 3,\cdots, r</math> i.e. <math>1\leq s\leq r< 5</math><br> ( or <math>1\leq r< s\leq m</math> condition is also used)<br>
 
* [[discrete series unitary representations|discrete series unitary representations and GKO coset construction]]<br><math>m= 5</math><br><math>c = \frac{4}{5}</math><br><math>h_{r,s}(c) = {((m+1)r-ms)^2-1 \over 4m(m+1)}</math><br><math>r = 1, 2, 3,4</math> and <math>s= 1, 2, 3,\cdots, r</math> i.e. <math>1\leq s\leq r< 5</math><br> ( or <math>1\leq r< s\leq m</math> condition is also used)<br>
*  conformal dimensions<br>
 
 
*  10 irreducible representations<br>
 
*  10 irreducible representations<br>
 +
*  conformal dimensions<br><math>\Delta_{r,s}^{(p,p')}=h_{r,s}^{(p,p')}=\frac{(p'r-ps)^2-(p'-p)^2}{4pp'}</math><br><math>1\leq r \leq p-1</math> and <math>1\leq s \leq p'-1</math><br> note that <math>\Delta_{r,s}^{(p,p')}=\Delta_{p-r,p'-s}^{(p,p')}</math><br> r=1,2,3,4 s=1,2,3,4,5<br>
  
 
 
 
 
109번째 줄: 109번째 줄:
 
* [http://dx.doi.org/10.1016/0550-3213%2887%2990166-0 Conformal quantum field theory models in two dimensions having Z3 symmetry]<br>
 
* [http://dx.doi.org/10.1016/0550-3213%2887%2990166-0 Conformal quantum field theory models in two dimensions having Z3 symmetry]<br>
 
**  V. A. Fateev and A. B. Zamolodchikov, Nuclear Phys. B 280 (1987), no. 4, 644–660<br>
 
**  V. A. Fateev and A. B. Zamolodchikov, Nuclear Phys. B 280 (1987), no. 4, 644–660<br>
*  <br>[http://dx.doi.org/10.1143/JPSJ.55.3285 Virasoro Algebra, von Neumann Algebra and Critical Eight-Vertex SOS Models]<br>
+
* [http://dx.doi.org/10.1143/JPSJ.55.3285 Virasoro Algebra, von Neumann Algebra and Critical Eight-Vertex SOS Models]<br>
 
** Atsuo Kuniba, Yasuhiro Akutsu1 and Miki Wadati, 1986
 
** Atsuo Kuniba, Yasuhiro Akutsu1 and Miki Wadati, 1986
 
* [http://dx.doi.org/10.1103/PhysRevB.28.3897 Critical behavior of the three-state Potts model: Monte Carlo renormalization group]<br>
 
* [http://dx.doi.org/10.1103/PhysRevB.28.3897 Critical behavior of the three-state Potts model: Monte Carlo renormalization group]<br>

2010년 12월 4일 (토) 12:46 판

introduction

 

 

ferromagnetic three-state Potts spin chain

  • [DKMM93]

 

 

 

 

conformal field theory
  • discrete series unitary representations and GKO coset construction
    \(m= 5\)
    \(c = \frac{4}{5}\)
    \(h_{r,s}(c) = {((m+1)r-ms)^2-1 \over 4m(m+1)}\)
    \(r = 1, 2, 3,4\) and \(s= 1, 2, 3,\cdots, r\) i.e. \(1\leq s\leq r< 5\)
    ( or \(1\leq r< s\leq m\) condition is also used)
  • 10 irreducible representations
  • conformal dimensions
    \(\Delta_{r,s}^{(p,p')}=h_{r,s}^{(p,p')}=\frac{(p'r-ps)^2-(p'-p)^2}{4pp'}\)
    \(1\leq r \leq p-1\) and \(1\leq s \leq p'-1\)
    note that \(\Delta_{r,s}^{(p,p')}=\Delta_{p-r,p'-s}^{(p,p')}\)
    r=1,2,3,4 s=1,2,3,4,5

 

 

eight vertex model

 

 

 

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