"Finite size effect"의 두 판 사이의 차이

수학노트
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* Casimir effect is one example of finite size effect
 
* Casimir effect is one example of finite size effect
 
* any kind of constraint or boudary conditions on the the zero-point modes of the quantum fields in question, including backgrounds such as gravity
 
* any kind of constraint or boudary conditions on the the zero-point modes of the quantum fields in question, including backgrounds such as gravity
* Hamiltonian value associated wih the vacuum or ground state, called zero-point energy
+
* In a model without boundary conditions, the Hamiltonian value associated wih the vacuum or ground state, called zero-point energy, is usually discarded because, despite being infinite, may be reabsorbed in a suitable redefinition of the energy origin
 +
* there are several ways to put such an adjustment into practice, normal ordering being oneof the most popular
 +
*  
  
 
 
 
 
33번째 줄: 35번째 줄:
  
 
* [[2009년 books and articles|찾아볼 수학책]]
 
* [[2009년 books and articles|찾아볼 수학책]]
 +
*  
 
* [http://www.springerlink.com/content/f374835722j24555/ Conformal invariance and finite size effects in critical two dimensional statistical models]<br>
 
* [http://www.springerlink.com/content/f374835722j24555/ Conformal invariance and finite size effects in critical two dimensional statistical models]<br>
 
** Claude Itzykson
 
** Claude Itzykson

2009년 8월 9일 (일) 17:56 판

introduction
  • Casimir effect is one example of finite size effect
  • any kind of constraint or boudary conditions on the the zero-point modes of the quantum fields in question, including backgrounds such as gravity
  • In a model without boundary conditions, the Hamiltonian value associated wih the vacuum or ground state, called zero-point energy, is usually discarded because, despite being infinite, may be reabsorbed in a suitable redefinition of the energy origin
  • there are several ways to put such an adjustment into practice, normal ordering being oneof the most popular
  •  

 

QFT interpretation of the Casimirt effect
  •  

 

 

conformal transform from the plane to cylinder
  • \(z \to w=\frac{L}{2\pi}\ln z\)
  • energy momentum tensor changes
    \(T_{cyl}(w)=(\frac{2\pi}{L})^2\{T_{pl}(z)z^2-\frac{c}{24}\}\)
    \(L_0 \to L_0-c/24\)
  • the central charge emerges
  • central charge is proportional to the Casimir energy, the change in the vacuum energy density brought about by the periodicity condition on the cylinder

 

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