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

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*  commutation relation<br><math>x</math>, <math>p=\frac{d}{dx}</math><br><math>[x,p]=1</math><br>
  
 
 
 
 
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<h5 style="margin: 0px; line-height: 2em;">Representation theory</h5>
 
 
 
 
 
  
 
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2010년 3월 26일 (금) 09:40 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

 

 

differential operators
  • commutation relation
    \(x\), \(p=\frac{d}{dx}\)
    \([x,p]=1\)

 

 

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
    \([d,x]=d(x)\)
  • In affine Kac-Moody algebra theory, this appears as the loop algebra of Cartan subalgebra

 

 

 

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).

 

 

Heisenberg VOA

 

 


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