EBS Radionuclide Transport Abstraction

Schreiber, J.D.

doi:10.2172/893809

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Introduction and Results1

Fake Curvature Gauge Transformations and Differential 2-cro1

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Cited by 3 publications

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“…This is clearly too strong a condition in the ABJM model. Here, we use the observation that a higher gauge theory on a principal 2-bundle with non-vanishing F can be reformulated as a higher gauge theory on a principal 3-bundle for which the fake curvature does vanish [7,2].…”

Section: Introduction and Resultsmentioning

confidence: 99%

The ABJM model is a higher gauge theory

Palmer

Saemann

2014

Int. J. Geom. Methods Mod. Phys.

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Section: Introduction and Resultsmentioning

confidence: 99%

The ABJM model is a higher gauge theory

Palmer

Saemann

2014

Int. J. Geom. Methods Mod. Phys.

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“…It is clear that to impose (5.2), we have to generalize our differential crossed module A 4 t → g A 4 , as the triviality of t would imply F = 0. Note that a higher gauge theory on principal 2-bundles with non-vanishing fake curvature can be reformulated as a higher gauge theory on principal 3-bundles with vanishing fake curvature [38,39]. We used this idea previously to demonstrate that the ABJM model is a higher gauge theory [7].…”

Section: Fake Curvature Gauge Transformations and Differential 2-cromentioning

confidence: 99%