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

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The automorphisms of the Heisenberg group (fixing its center) form the symplectic group
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<h5 style="line-height: 2em; 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%;">relation to quantum mechanics</h5>
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*   the position operators and momentum operators satisfy the relation<br><math>[X,P] = X P - P X = i \hbar</math><br>
  
 
 
 
 
  
<h5>Stone-Von Neumann theorem</h5>
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* The [[Heisenberg group and Heisenberg algebra|Heisenberg group]] has an essentially unique irreducible unitary representation on a Hilbert space H with the center acting as a given nonzero constant (the content of the Stone-von Neumann theorem).
 
  
 
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<h5 style="margin: 0px; line-height: 3.428em; color: rgb(34, 61, 103); font-family: 'malgun gothic',dotum,gulim,sans-serif; font-size: 1.166em; background-position: 0px 100%;">finite dimensional Heisenberg algebra</h5>
  
<h5 style="margin: 0px; line-height: 3.428em; color: rgb(34, 61, 103); font-family: 'malgun gothic',dotum,gulim,sans-serif; font-size: 1.166em; background-position: 0px 100%;">introduction</h5>
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*  one dimensional [[central extension of groups and Lie algebras|central extension]] of abelian Lie algebra<br>
  
 
* <math>[p_i, q_j] = \delta_{ij}z</math><br>
 
* <math>[p_i, q_j] = \delta_{ij}z</math><br>
 
* <math>[p_i, z] = 0</math><br>
 
* <math>[p_i, z] = 0</math><br>
 
* <math>[q_j, z] = 0</math><br>
 
* <math>[q_j, z] = 0</math><br>
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*  Gannon 180p<br>
 
*  Gannon 180p<br>
  
 
 
 
 
 
 
 
 
<h5 style="margin: 0px; line-height: 2em; color: rgb(34, 61, 103); font-family: 'malgun gothic',dotum,gulim,sans-serif; font-size: 1.166em; background-position: 0px 100%;">relation to quantum mechanics</h5>
 
 
*   the position operators and momentum operators satisfy the above relation<br>
 
  
 
 
 
 
37번째 줄: 30번째 줄:
 
*  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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The automorphisms of the Heisenberg group (fixing its center) form the symplectic group
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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%;">Stone-Von Neumann theorem</h5>
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* The [[Heisenberg group and Heisenberg algebra|Heisenberg group]] has an essentially unique irreducible unitary representation on a Hilbert space H with the center acting as a given nonzero constant (the content of the Stone-von Neumann theorem).
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2010년 3월 26일 (금) 08:56 판

relation to quantum mechanics
  •  the position operators and momentum operators satisfy the relation
    \([X,P] = X P - P X = i \hbar\)

 

 

finite dimensional Heisenberg algebra
  • \([p_i, q_j] = \delta_{ij}z\)
  • \([p_i, z] = 0\)
  • \([q_j, z] = 0\)
  • Gannon 180p

 

 

 

infinite dimensional Heisenberg algebra
  • 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
    \([d,x]=d(x)\)

 

 

 

The automorphisms of the Heisenberg group (fixing its center) form the symplectic group

 

Stone-Von Neumann theorem
  • The Heisenberg group has an essentially unique irreducible unitary representation on a Hilbert space H with the center acting as a given nonzero constant (the content of the Stone-von Neumann theorem).

 

 

 

 

fock space representation

 

 

Representation theory

 

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