"R-matrix"의 두 판 사이의 차이

수학노트
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imported>Pythagoras0
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<h5>introduction</h5>
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==introduction==
  
 
* R-matrix has entries from Boltzman weights.
 
* 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 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  <math>\bar R=p\circ R</math> instead of the <math>R</math> matrix where <math>p</math> is the permutation map
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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
* this is what makes the module category into braided monoidal category
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* this is what makes the module category into braided monoidal category
  
 
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<h5 style="line-height: 3.428em; margin: 0px; color: rgb(34, 61, 103); font-family: 'malgun gothic',dotum,gulim,sans-serif; font-size: 1.166em; background-position: 0px 100%;">YBE</h5>
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==YBE==
  
 
* [[Yang-Baxter equation (YBE)|Yang-Baxter equation]]<br><math>R_{12}R_{13}R_{23}=R_{23}R_{13}R_{12}</math><br>
 
* [[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 style="margin: 0px; line-height: 2em;">R-matrix and Braid groups</h5>
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==R-matrix and Braid groups==
  
For <math>R</math> matrix on <math>V \otimes V</math>, define <math>\bar R=p\circ R</math> where <math>p</math> is the permutation map.<br><math>\bar R_i=1\otimes \cdots \otimes\bar R \cdots \otimes 1</math>, <math>\bar R_i</math> sitting in i and i+1 th slot.<br>
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For <math>R</math> matrix on <math>V \otimes V</math>, define <math>\bar R=p\circ R</math> where <math>p</math> is the permutation map.<br><math>\bar R_i=1\otimes \cdots \otimes\bar R \cdots \otimes 1</math>, <math>\bar R_i</math> sitting in i and i+1 th slot.<br>
*  Then YB reduces to<br><math>\bar R_i\bar R_j =\bar R_j\bar R_i</math> whenever <math>|i-j| \geq 2 </math><br><math>\bar R_i\bar R_{i+1}\bar R_i= \bar R_{i+1}\bar R_i \bar R_{i+1}</math><br> which are the [[Braid group]] relations.<br>
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*  Then YB reduces to<br><math>\bar R_i\bar R_j =\bar R_j\bar R_i</math> whenever <math>|i-j| \geq 2 </math><br><math>\bar R_i\bar R_{i+1}\bar R_i= \bar R_{i+1}\bar R_i \bar R_{i+1}</math><br> which are the [[Braid group]] relations.<br>
 
*  with an R-matrix satisfying the YBE, we obtain a representation of the [[Braid group]], which then gives a link invariant in [[Knot theory]]<br>
 
*  with an R-matrix satisfying the YBE, we obtain a representation of the [[Braid group]], which then gives a link invariant in [[Knot theory]]<br>
  
 
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<h5>related items</h5>
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==related items==
  
 
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<h5>books</h5>
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==books==
  
 
* [[2009년 books and articles|찾아볼 수학책]]
 
* [[2009년 books and articles|찾아볼 수학책]]
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* http://www.amazon.com/s/ref=nb_ss_gw?url=search-alias%3Dstripbooks&field-keywords=
 
* http://www.amazon.com/s/ref=nb_ss_gw?url=search-alias%3Dstripbooks&field-keywords=
  
 
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<h5>encyclopedia</h5>
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==encyclopedia==
  
 
* http://ko.wikipedia.org/wiki/
 
* http://ko.wikipedia.org/wiki/
60번째 줄: 60번째 줄:
 
* Princeton companion to mathematics([[2910610/attachments/2250873|Companion_to_Mathematics.pdf]])
 
* Princeton companion to mathematics([[2910610/attachments/2250873|Companion_to_Mathematics.pdf]])
  
 
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<h5>blogs</h5>
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==blogs==
  
 
*  구글 블로그 검색<br>
 
*  구글 블로그 검색<br>
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** http://blogsearch.google.com/blogsearch?q=
 
** http://blogsearch.google.com/blogsearch?q=
  
 
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<h5>articles</h5>
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==articles==
  
 
*  R-matrix arising from affine Hecke algebras and its application to Macdonald's difference operators<br>
 
*  R-matrix arising from affine Hecke algebras and its application to Macdonald's difference operators<br>
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* http://dx.doi.org/
 
* http://dx.doi.org/
  
 
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<h5>TeX </h5>
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==TeX ==

2012년 10월 26일 (금) 11:20 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.
  • with an R-matrix satisfying the YBE, we obtain a representation of the Braid group, which then gives a link invariant in Knot theory



related items

books



encyclopedia



blogs


articles


TeX