"BRST quantization and cohomology"의 두 판 사이의 차이
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* BRST quantization is one way to quantize the theory and is a part of path integral<br> | * BRST quantization is one way to quantize the theory and is a part of path integral<br> | ||
* Gauge theory allows 'local symmetry' which should be ignored to be physical<br> | * Gauge theory allows 'local symmetry' which should be ignored to be physical<br> | ||
− | * | + | * this ignoring process leads to the cohomoloy theory.<br> |
* BRST = quantization procedure of a classical system with constraints by introducing odd variables (“ghosts”)<br> | * BRST = quantization procedure of a classical system with constraints by introducing odd variables (“ghosts”)<br> | ||
* 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<br> | * 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<br> | ||
14번째 줄: | 14번째 줄: | ||
− | \Lambda_{\infty} | + | <math>\Lambda_{\infty}</math> semi-infinite form |
− | \mathfrak{g} : \mathbb{Z}-graded Lie algebra | + | <math>\mathfrak{g}</math> : <math>\mathbb{Z}</math>-graded Lie algebra |
− | \sigma : anti-linear automorphism sending \mathfrak{g}_{n} to \mathfrak{g}_{-n} | + | <math>\sigma</math> : anti-linear automorphism sending \mathfrak{g}_{n} to \mathfrak{g}_{-n} |
H^2(\mathfrak{g})=0 (i.e. no non-trivial central extension) | H^2(\mathfrak{g})=0 (i.e. no non-trivial central extension) |
2011년 9월 27일 (화) 07:52 판
introduction
- PG minicourse: BRST cohomology (http://empg.maths.ed.ac.uk/Activities/BRST/Notes.pdf , very good 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
- http://bolvan.ph.utexas.edu/~vadim/Classes/2008f.homeworks/brst.pdf
- http://www.nuclecu.unam.mx/~chryss/papers/brst_final.pdf
applications
- BRST approach to minimal models
- BRST approach to no-ghost theorem
- BRST approach to coset constructions
books
encyclopedia
- http://en.wikipedia.org/wiki/BRST_quantization
- http://www.scholarpedia.org/article/Becchi-Rouet-Stora-Tyutin_symmetry
- Princeton companion to mathematics(Companion_to_Mathematics.pdf)
expositions
- Introduction to Lie algebra cohomology with a view towards BRST cohomology ,Friedrich Wagemann, 2010-8
- PG minicourse: BRST cohomology (http://empg.maths.ed.ac.uk/Activities/BRST/Notes.pdf , very good introduction)
articles
- Igor B. Frenkel, Anton M. Zeitlin, Quantum Group as Semi-infinite Cohomology
- van Holten, J. W., The BRST complex and the cohomology of compact lie algebras
- D. Bernard and G. Felder, 1990, Fock representations and BRST cohomology inSL(2) current algebra
- BRST cohomology in classical mechanics
- Symplectic Reduction, BRS Cohomology, and Infinite-Dimensional Clifford algebras, B. Kostant, S. Sternberg, Ann. Physics 176 (1987) 49–113
- I. B. Frenkel,. H. Garland, and. G. J. Zuckerman, PNAS November 1, 1986 vol. 83 no. 22 8442-8446, Semi-infinite cohomology and string theory
- http://dx.doi.org/10.1007/BF02096498
blogs
- http://www.math.columbia.edu/~woit/notesonbrst.pdf
- http://www.math.columbia.edu/~woit/wordpress/?cat=12
- Notes on BRST I: Representation Theory and Quantum Mechanics
- Notes on BRST II: Lie Algebra Cohomology, Physicist’s Version
- Notes on BRST III: Lie Algebra Cohomology
- Notes on BRST IV: Lie Algebra Cohomology for Semi-simple Lie Algebras
- Notes on BRST V: Highest Weight Theory
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