"R-matrix"의 두 판 사이의 차이

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* from this intertwining property we need to consider  <math>\bar R=p\circ R</math> instead of the <math>R</math> matrix where <math>p</math> is the permutation map
 
* from this intertwining property we need to consider  <math>\bar R=p\circ R</math> instead of the <math>R</math> matrix where <math>p</math> is the permutation map
 
* this is what makes the module category into braided monoidal category
 
* this is what makes the module category into braided monoidal category
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<h5 style="line-height: 3.428em; margin-top: 0px; margin-right: 0px; margin-bottom: 0px; margin-left: 0px; color: rgb(34, 61, 103); font-family: 'malgun gothic', dotum, gulim, sans-serif; font-size: 1.166em; background-image: ; background-color: initial; background-position: 0px 100%;">YBE</h5>
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* [[Yang-Baxter equation (YBE)|Yang-Baxter equation]]<br><math>R_{12}R_{13}R_{23}=R_{23}R_{13}R_{12}</math><br>
  
 
 
 
 
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<h5>YBE</h5>
 
 
 
* [[Yang-Baxter equation (YBE)|Yang-Baxter equation]]<br><math>R_{12}R_{13}R_{23}=R_{23}R_{13}R_{12}</math><br>
 
 
 
 
 
  
 
 
 
 

2010년 1월 22일 (금) 14:08 판

introduction
  • R-matrix has entries from Boltzman weights.
  • From quantum group point of view, R-matrix naturally appears as intertwiners of tensor product of two evaluation modules
  • from this intertwining property we need to consider  \(\bar R=p\circ R\) instead of the \(R\) matrix where \(p\) is the permutation map
  • this is what makes the module category into braided monoidal category

 

 

 

YBE

 

 

 

R-matrix and Braid groups

For \(R\) matrix on \(V \otimes V\), define \(\bar R=p\circ R\) where \(p\) is the permutation map.

\(\bar R_i=1\otimes \cdots \otimes\bar R \cdots \otimes 1\), \(\bar R_i\) sitting in i and i+1 th slot.

Then YB reduces to

\(\bar R_i\bar R_j =\bar R_j\bar R_i\) whenever \(|i-j| \geq 2 \)

\(\bar R_i\bar R_{i+1}\bar R_i= \bar R_{i+1}\bar R_i \bar R_{i+1}\)

which are the Braid group relations.

 


 

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