"Heisenberg group and Heisenberg algebra"의 두 판 사이의 차이

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*  start with a Lattice <math><\cdot,\cdot></math><br>
 
*  start with a Lattice <math><\cdot,\cdot></math><br>
 
*  make a vector space from it<br>
 
*  make a vector space from it<br>
* <math>[\alpha(m),\beta(n)]=m\delta_{m,-n}<\alpha,\beta>c</math><br>
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* Construct a Loop algbera<br><math>A\otimes\mathbb{C}[t,t^{-1}]\oplus\mathbb{C}c</math><br><math>\alpha(m)=\alpha\otimes t^m</math><br>
 +
*  Give a bracket <br><math>[\alpha(m),\beta(n)]=m\delta_{m,-n}<\alpha,\beta>c</math><br>
 
*  add a derivation <math>d</math><br><math>d(\alpha(n))=n\alpha(n)</math><br><math>d(c)=0</math><br>
 
*  add a derivation <math>d</math><br><math>d(\alpha(n))=n\alpha(n)</math><br><math>d(c)=0</math><br>
 
*  define a Lie bracket<br><math>[d,x]=d(x)</math><br>
 
*  define a Lie bracket<br><math>[d,x]=d(x)</math><br>
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 +
 
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<h5 style="line-height: 2em; margin-top: 0px; margin-right: 0px; margin-bottom: 0px; margin-left: 0px;">relation to quantum mechanics</h5>
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*   the position operators and momentum operators<br>
  
 
 
 
 

2009년 8월 13일 (목) 01:43 판

introduction
  • start with a Lattice \(<\cdot,\cdot>\)
  • make a vector space from it
  • Construct a Loop algbera
    \(A\otimes\mathbb{C}[t,t^{-1}]\oplus\mathbb{C}c\)
    \(\alpha(m)=\alpha\otimes t^m\)
  • Give a bracket 
    \([\alpha(m),\beta(n)]=m\delta_{m,-n}<\alpha,\beta>c\)
  • add a derivation \(d\)
    \(d(\alpha(n))=n\alpha(n)\)
    \(d(c)=0\)
  • define a Lie bracket
    \([d,x]=d(x)\)

 

relation to quantum mechanics
  •  the position operators and momentum operators

 

 

fock space representation

 

 

Representation theory

 

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