"Six-vertex model and Quantum XXZ Hamiltonian"의 두 판 사이의 차이

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3번째 줄: 3번째 줄:
 
* Boltzmann weights
 
* Boltzmann weights
 
* monodromy matrix
 
* monodromy matrix
* trace of monodromy matrix is the transfer
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* trace of monodromy matrix is the transfer matrix
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* power of transfer matrix becomes the partition function
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<h5>tr</h5>
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<h5>partition function</h5>
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<h5>free energy</h5>
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* <math>F=-kT \ln Z</math>
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<h5>correlation functions</h5>
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54번째 줄: 83번째 줄:
 
* [http://www.springerlink.com/content/f9961j132852j27q/ Integrability of the Quantum XXZ Hamiltonian]<br>
 
* [http://www.springerlink.com/content/f9961j132852j27q/ Integrability of the Quantum XXZ Hamiltonian]<br>
 
** T Miwa, 2009
 
** T Miwa, 2009
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* [http://arxiv.org/abs/cond-mat/0304309 Introduction to solvable lattice models in statistical and mathematical physics]<br>
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** Tetsuo Deguchi, 2003
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* [http://arxiv.org/abs/hep-th/9204064 Diagonalization of the XXZ Hamiltonian by Vertex Operators]<br>
 
* [http://arxiv.org/abs/hep-th/9204064 Diagonalization of the XXZ Hamiltonian by Vertex Operators]<br>
 
** Authors: Brian Davies, Omar Foda, Michio Jimbo, Tetsuji Miwa, Atsushi Nakayashiki, 1993
 
** Authors: Brian Davies, Omar Foda, Michio Jimbo, Tetsuji Miwa, Atsushi Nakayashiki, 1993

2010년 2월 24일 (수) 06:02 판

introduction
  • Boltzmann weights
  • monodromy matrix
  • trace of monodromy matrix is the transfer matrix
  • power of transfer matrix becomes the partition function

 

 

tr

 

partition function

 

 

free energy
  • \(F=-kT \ln Z\)

 

 

correlation functions

 

 

 

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books

 

 

encyclopedia

 

 

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