"BRST quantization and cohomology"의 두 판 사이의 차이

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<h5 style="margin: 0px; line-height: 2em;">ghost variables</h5>
 
<h5 style="margin: 0px; line-height: 2em;">ghost variables</h5>
  
* [[#]]<br>
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* [[Faddeev–Popov ghost fields|ghost fields]]<br>
  
 
 
 
 
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* [http://bolvan.ph.utexas.edu/%7Evadim/Classes/2008f.homeworks/brst.pdf http://bolvan.ph.utexas.edu/~vadim/Classes/2008f.homeworks/brst.pdf]<br>
 
* [http://bolvan.ph.utexas.edu/%7Evadim/Classes/2008f.homeworks/brst.pdf http://bolvan.ph.utexas.edu/~vadim/Classes/2008f.homeworks/brst.pdf]<br>
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* [http://www.nuclecu.unam.mx/%7Echryss/papers/brst_final.pdf http://www.nuclecu.unam.mx/~chryss/papers/brst_final.pdf]<br>
  
 
 
 
 
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*  Quantum Group as Semi-infinite Cohomology<br>
 
*  Quantum Group as Semi-infinite Cohomology<br>
 
** Igor B. Frenkel, Anton M. Zeitlin
 
** Igor B. Frenkel, Anton M. Zeitlin
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*  The BRST complex and the cohomology of compact lie algebras<br>
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** van Holten, J. W.
 
* [http://dx.doi.org/10.1007/BF01466770 BRST cohomology in classical mechanics]
 
* [http://dx.doi.org/10.1007/BF01466770 BRST cohomology in classical mechanics]
 
*  Symplectic Reduction, BRS Cohomology, and Infinite-Dimensional Clifford algebras<br>
 
*  Symplectic Reduction, BRS Cohomology, and Infinite-Dimensional Clifford algebras<br>

2010년 11월 14일 (일) 08:10 판

introduction
  • Gauge theory = principal G-bundle
  • We require a quantization of gauge theory.
  • BRST quantization is one way to quantize the theory and is a part of path integral.
  • Gauge theory allows 'local symmetry' which should be ignored to be physical. 
  • This ignoring process leads to the cohomoloy theory.
  • BRST = quantization procedure of a classical system with constraints by introducing odd variables (“ghosts”)
  • the conditions D = 26 and α0 = 1 for the space-time dimension D and the zero-intercept α0 of leading trajectory are required by the nilpotency QB2 = 0 of the BRS charge

 

 

\Lambda_{\infty} semi-infinite form

\mathfrak{g} : \mathbb{Z}-graded Lie algebra

\sigma : anti-linear automorphism sending \mathfrak{g}_{n} to \mathfrak{g}_{-n}

H^2(\mathfrak{g})=0 (i.e. no non-trivial central extension)

 

 

ghost variables

 

 

 

nilpotency of BRST operator

 

 

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