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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Main Authors: João Faria Martins, Aleksandar Mikovic
Format: Article
Language:English
Published: National Academy of Science of Ukraine 2011-10-01
Series:Symmetry, Integrability and Geometry: Methods and Applications
Subjects:
Online Access:http://dx.doi.org/10.3842/SIGMA.2011.094
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spelling 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
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AT aleksandarmikovic fourdimensionalspinfoamperturbationtheory
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