Abstract

We present and study a 4-d Chern-Simons (CS) model whose gauge symmetry is encoded in a balanced Lie group crossed module. Using the derived formal set-up recently found, the model can be formulated in a way that in many respects closely parallels that of the familiar 3-d CS one. In spite of these formal resemblance, the gauge invariance properties of the 4-d CS model differ considerably. The 4-d CS action is fully gauge invariant if the underlying base 4-fold has no boundary. When it does, the action is gauge variant, the gauge variation being a boundary term. If certain boundary conditions are imposed on the gauge fields and gauge transformations, level quantization can then occur. In the canonical formulation of the theory, it is found that, depending again on boundary conditions, the 4-d CS model is characterized by surface charges obeying a non trivial Poisson bracket algebra. This is a higher counterpart of the familiar WZNW current algebra arising in the 3-d model. 4-d CS theory thus exhibits rich holographic properties. The covariant Schroedinger quantization of the 4-d CS model is performed. A preliminary analysis of 4-d CS edge field theory is also provided. The toric and Abelian projected models are described in some detail.

Highlights

  • There are several reasons why the formulation and study of 4-dimensional higher ChernSimons (CS) theory is an interesting and worthwhile endeavour

  • We present and study a 4-d Chern-Simons (CS) model whose gauge symmetry is encoded in a balanced Lie group crossed module

  • 4-dimensional BF theory is an instance of 4-dimensional CS theory

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Summary

Introduction

There are several reasons why the formulation and study of 4-dimensional higher ChernSimons (CS) theory is an interesting and worthwhile endeavour. Since particle-like excitations do not braid and have only ordinary bosonic/fermionic statistics in this case, fractional statistics can only arise from the braiding of either a point-like and a loop-like or two loop-like excitations This has been adequately described through BF type TQFTs [28,29,30] through the correlation functions of Wilson loops and surfaces, pointing again to 4-dimensional CS theory. The 4-dimensional counterpart of Wilson lines, Wilson surfaces, are expected to be relevant in the analysis of non perturbative features of higher form gauge theory and quantum gravity They should be a basic element of any field theoretic approach to 4-dimensional 2-knot topology [32]. To the best of our knowledge on the holographic features of 4-dimensional CS theory

Outline of the paper
Outlook
Lie crossed modules and invariant pairings
Lie group and algebra crossed modules
Crossed modules with invariant pairing
Crossed submodules and isotropy
Higher gauge theory in the derived formulation
Derived Lie groups and algebras
Derived superfield formulation
The derived functional framework of higher gauge theory
Derived description of non trivial higher principal bundles
Mloc pBM q thus is kż ΥB “ δBΓB “ 4π T r1sBM
Gauge invariance of the 4-d Chern-Simons model
Level quantization
Global issues in 4-d Chern-Simons theory
Canonical formulation
Surface charges and holography
Toward the edge field theory of 4-d Chern-Simons theory
Covariant Schroedinger quantization
F ΘB Ψ pωBq
Sample applications
The toric 4-dimensional CS model
The Abelian projection model
Basic definitions and identities of crossed module theory
Lie differentiation of crossed modules
Proof of the decomposition theorem
Basic results of Cartan-Weyl theory

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