"Dimer model"의 두 판 사이의 차이

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*  energy and weight function<br><math>w(e)=\exp (-\frac{\epsilon(e)}{T})</math><br>
 
*  energy and weight function<br><math>w(e)=\exp (-\frac{\epsilon(e)}{T})</math><br>
 
*  partition function<br><math>Z_{\Gamma}=\sum_{D\subset \Gamma} \prod_{e\in D} w(e)</math><br>
 
*  partition function<br><math>Z_{\Gamma}=\sum_{D\subset \Gamma} \prod_{e\in D} w(e)</math><br>
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<h5>fH</h5>
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P(z_1,z_2,w) if weights are positive real., then P=0 is a Harnack curve of genus
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g=|int(N)|
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P(z_0,z_2)=0 is harnack if the amoeba map is at most 2-to-1.
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166번째 줄: 186번째 줄:
 
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* Cimasoni, David, 와/과Nicolai Reshetikhin. 2007. “Dimers on surface graphs and spin structures. II”. <em>0704.0273</em> (4월 2). doi:doi:10.1007/s00220-008-0488-3. http://arxiv.org/abs/0704.0273.<br>  <br>
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* Cimasoni, David, 와/과Nicolai Reshetikhin. 2007. “Dimers on surface graphs and spin structures. II”. <em>0704.0273</em> (4월 2). doi:doi:10.1007/s00220-008-0488-3. http://arxiv.org/abs/0704.0273.
 
* [http://dx.doi.org/10.1103/PhysRevE.75.040105 Exact solution of close-packed dimers on the kagome lattice]<br>
 
* [http://dx.doi.org/10.1103/PhysRevE.75.040105 Exact solution of close-packed dimers on the kagome lattice]<br>
 
** Fa Wang, F. Y. Wu, 2006
 
** Fa Wang, F. Y. Wu, 2006

2011년 11월 5일 (토) 14:52 판

introduction

 

 

basic notions
  • dimer configurations
  • set of dimer configurations
  • partition function
  • Kasteleyn matrix
  • height function
  • spectral curve
  • surface tension

 

 

physics motivation
  • dimer configuration can be considered as the covering of the graph by pairs of fermions connected by an edge

 

 

Termperley equivalence
  • spanning trees on \gamma rooted at x
  • dimers on D(\gamma)

 

 

Domino tiling and height function
  • bipartite graph

 

 

energy and weight systems
  • define a weight function on the edges of the graph \gamma
    \(w:E(\Gamma)\to \mathbb{R}_{\geq 0}\)
  • For a dimer configuration D,
    \(w(D)=\prod_{e\in D} w(e)\)
  • energy function
    \(\epsilon:E(\Gamma)\to \mathbb{R}\)
  • For a dimer configuration D,
    \(\epsilon(D)=\sum_{e\in D} \epsilon(e)\)
  • energy and weight function
    \(w(e)=\exp (-\frac{\epsilon(e)}{T})\)
  • partition function
    \(Z_{\Gamma}=\sum_{D\subset \Gamma} \prod_{e\in D} w(e)\)

 

 

fH

 

P(z_1,z_2,w) if weights are positive real., then P=0 is a Harnack curve of genus

g=|int(N)|

P(z_0,z_2)=0 is harnack if the amoeba map is at most 2-to-1.

 

 

 

 

 

하위페이지

 

 

 

 

memo

 

 

 

history

 

 

related items[[Schramm–Loewner evolution (SLE)|]]

 

 

encyclopedia

 

 

books

 

 

links

 

 

expositions

 

 

articles

 

 

question and answers(Math Overflow)

 

 

blogs