Abstract:Field theories on deformed spaces suffer from the IR/UV mixing and renormalization is generically spoiled.In work with R. Wulkenhaar, one of us realized a way to cure this disease by adding one more marginal operator.We review these ideas, show the application to φ 3 models and use the heat kernel expansion methods for a scalar field theory coupled to an external gauge field on a θ-deformed space and derive noncommutative gauge field actions.
“…Historically, (an incomplete list of references is given by [28,29,30,31,32]) the IR divergences have been neglected in the discussion of renormalization. Instead, direct correspondences between known commutative results and the outcome of planar part calculations of the non-commutative counter parts have been sought.…”
When considering quantum field theories on non-commutative spaces one inevitably encounters the infamous UV/IR mixing problem. So far, only very few renormalizable models exist and all of them describe non-commutative scalar field theories on fourdimensional Euclidean Groenewold-Moyal deformed space, also known as 'θ-deformed space' R 4 θ . In this work we discuss some major obstacles of constructing a renormalizable non-commutative gauge field model and sketch some possible ways out.
“…Historically, (an incomplete list of references is given by [28,29,30,31,32]) the IR divergences have been neglected in the discussion of renormalization. Instead, direct correspondences between known commutative results and the outcome of planar part calculations of the non-commutative counter parts have been sought.…”
When considering quantum field theories on non-commutative spaces one inevitably encounters the infamous UV/IR mixing problem. So far, only very few renormalizable models exist and all of them describe non-commutative scalar field theories on fourdimensional Euclidean Groenewold-Moyal deformed space, also known as 'θ-deformed space' R 4 θ . In this work we discuss some major obstacles of constructing a renormalizable non-commutative gauge field model and sketch some possible ways out.
“…In the presence of a potential which grows at infinity the heat kernel expansion is modified essentially even in the commutative case. In the NC case, the heat kernel expansion was constructed in [27,28] and used to study an induced gauge field action (in the spirit of the spectral action principle, see Section 2).…”
Section: Field Theories With An Oscillator Potentialmentioning
confidence: 99%
“…More examples of applications of the heat kernel expansion to renormalization and anomalies in NC theories, as well as comparison to the results obtained by other methods and further references can be found in [18,19,20,23,27,39,40,46,47,48].…”
Section: Application: Renormalization and Anomaliesmentioning
Abstract. This is a mini-review of the heat kernel expansion for generalized Laplacians on various noncommutative spaces. Applications to the spectral action principle, renormalization of noncommutative theories and anomalies are also considered.
“…The uncertainty relation, however, brings us in conflict with Einstein's law of gravity if we assume continuity in the space variable for arbitrary small distances [2]. From the uncertainty relation…”
Section: Introductionmentioning
confidence: 99%
“…This is only one of several arguments that we have to expect some changes in physics for very small distances. Other arguments are based on the singularity problem in Quantum field theory and the fact that Einstein's theory of gravity is nonrenormalizable when quantized [2].…”
Deformed gauge transformations on deformed coordinate spaces are considered for any Lie algebra. The representation theory of this gauge group forces us to work in a deformed Lie algebra as well. This deformation rests on a twisted Hopf algebra, thus we can represent a twisted Hopf algebra on deformed spaces. That leads to the construction of Lagrangian invariant under a twisted Lie algebra.This article is based on common work with
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