Four-Dimensional Spin Foam Perturbation Theory
We define a four-dimensional spin-foam perturbation theory for the BF-theory with a B∧B potential term defined for a compact semi-simple Lie group G on a compact orientable 4-manifold M. This is done by using the formal spin foam perturbative series coming from the spin-foam generating functional. W...
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National Academy of Science of Ukraine
2011-10-01
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Series: | Symmetry, Integrability and Geometry: Methods and Applications |
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Online Access: | http://dx.doi.org/10.3842/SIGMA.2011.094 |
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doaj-fec07eb4ea544a7f821499aa7df5cba22020-11-24T22:57:43ZengNational Academy of Science of UkraineSymmetry, Integrability and Geometry: Methods and Applications1815-06592011-10-017094Four-Dimensional Spin Foam Perturbation TheoryJoão Faria MartinsAleksandar MikovicWe define a four-dimensional spin-foam perturbation theory for the BF-theory with a B∧B potential term defined for a compact semi-simple Lie group G on a compact orientable 4-manifold M. This is done by using the formal spin foam perturbative series coming from the spin-foam generating functional. We then regularize the terms in the perturbative series by passing to the category of representations of the quantum group U_q(g) where g is the Lie algebra of G and q is a root of unity. The Chain-Mail formalism can be used to calculate the perturbative terms when the vector space of intertwiners Λ⊗Λ→A, where A is the adjoint representation of g, is 1-dimensional for each irrep Λ. We calculate the partition function Z in the dilute-gas limit for a special class of triangulations of restricted local complexity, which we conjecture to exist on any 4-manifold M. We prove that the first-order perturbative contribution vanishes for finite triangulations, so that we define a dilute-gas limit by using the second-order contribution. We show that Z is an analytic continuation of the Crane-Yetter partition function. Furthermore, we relate Z to the partition function for the F∧F theory.http://dx.doi.org/10.3842/SIGMA.2011.094spin foam modelsBF-theoryspin networksdilute-gas limitCrane-Yetter invariantspin-foam perturbation theory |
collection |
DOAJ |
language |
English |
format |
Article |
sources |
DOAJ |
author |
João Faria Martins Aleksandar Mikovic |
spellingShingle |
João Faria Martins Aleksandar Mikovic Four-Dimensional Spin Foam Perturbation Theory Symmetry, Integrability and Geometry: Methods and Applications spin foam models BF-theory spin networks dilute-gas limit Crane-Yetter invariant spin-foam perturbation theory |
author_facet |
João Faria Martins Aleksandar Mikovic |
author_sort |
João Faria Martins |
title |
Four-Dimensional Spin Foam Perturbation Theory |
title_short |
Four-Dimensional Spin Foam Perturbation Theory |
title_full |
Four-Dimensional Spin Foam Perturbation Theory |
title_fullStr |
Four-Dimensional Spin Foam Perturbation Theory |
title_full_unstemmed |
Four-Dimensional Spin Foam Perturbation Theory |
title_sort |
four-dimensional spin foam perturbation theory |
publisher |
National Academy of Science of Ukraine |
series |
Symmetry, Integrability and Geometry: Methods and Applications |
issn |
1815-0659 |
publishDate |
2011-10-01 |
description |
We define a four-dimensional spin-foam perturbation theory for the BF-theory with a B∧B potential term defined for a compact semi-simple Lie group G on a compact orientable 4-manifold M. This is done by using the formal spin foam perturbative series coming from the spin-foam generating functional. We then regularize the terms in the perturbative series by passing to the category of representations of the quantum group U_q(g) where g is the Lie algebra of G and q is a root of unity. The Chain-Mail formalism can be used to calculate the perturbative terms when the vector space of intertwiners Λ⊗Λ→A, where A is the adjoint representation of g, is 1-dimensional for each irrep Λ. We calculate the partition function Z in the dilute-gas limit for a special class of triangulations of restricted local complexity, which we conjecture to exist on any 4-manifold M. We prove that the first-order perturbative contribution vanishes for finite triangulations, so that we define a dilute-gas limit by using the second-order contribution. We show that Z is an analytic continuation of the Crane-Yetter partition function. Furthermore, we relate Z to the partition function for the F∧F theory. |
topic |
spin foam models BF-theory spin networks dilute-gas limit Crane-Yetter invariant spin-foam perturbation theory |
url |
http://dx.doi.org/10.3842/SIGMA.2011.094 |
work_keys_str_mv |
AT joaofariamartins fourdimensionalspinfoamperturbationtheory AT aleksandarmikovic fourdimensionalspinfoamperturbationtheory |
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