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Quantization of a gauge theory on a curved noncommutative space
High Energy Physics - Theory · Submitted 14 Mar 2012
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim We obtain that five counterterms are necessary for renormalization and that all divergences are logarithmic.
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The abstract, sentence by sentence
We study quantization of a gauge analogon of the Grosse-Wulkenhaar model: we find divergent one-loop contributions to the 1-point and 2-point Green functions. We obtain that five counterterms are necessary for renormalization and that all divergences are logarithmic.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | We study quantization of a gauge analogon of the Grosse-Wulkenhaar model: we find divergent one-loop contributions to the 1-point and 2-point Green functions. | result 0.72 | 0.96 | 0.32 | asserted 1.00 |
| s1 | We obtain that five counterterms are necessary for renormalization and that all divergences are logarithmic. | result 1.00 | 0.95 | 0.51 | asserted 1.00 |
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The paper
Original abstract
We study quantization of a gauge analogon of the Grosse-Wulkenhaar model: we find divergent one-loop contributions to the 1-point and 2-point Green functions. We obtain that five counterterms are necessary for renormalization and that all divergences are logarithmic.
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How the literature uses it
3 arXiv papers cite this in 10 sentences
Papers citing it · 8 sentences without a confident label
Builds on it 1 paper
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In Section 3 we go through the main steps and some details of the calculation and list additional propagator corrections, completing the earlier result [ref] .
One-loop structure of the U(1) gauge model on the truncated Heisenberg space · Introduction · 0.99
Uses its data or values 1 paper
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The one-loop propagator corrections $P_ϕϕ,7$, $P_ϕϕ,8$, $P_ϕϕ, 9$ and $P_ϕϕ,10$ which were calculated in [ref] are [equation] The ghost contributions are zero.
One-loop structure of the U(1) gauge model on the truncated Heisenberg space · Conclusion and outlook · 0.86
What it cites · 18 sentences without a confident label
Uses the method or tool of 1 paper
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In order to find divergences and the form of counterterms we apply the method developed in [ref] : we amputate the leg of the tadpole, multiply it with the corresponding external field then and integrate.
Loop Calculations for the Non-Commutative U(1) Gauge Field Model with Oscillator Term · Tadpoles: one-loop divergences · 1.00
Cites as background 4 papers
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The classical model was constucted in [ref] and some of its propeties were explored there: the equations of motion, the vacuum solutions, the BRST symmetry.
Gauge fields on noncommutative geometries with curvature · Conclusions and outlook · 0.85
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Two different possibilities are known: one can add either a position-dependent potential term $(x̅⋆ϕ)^2$ [ref] , or a nonlocal kinetic term $ϕ ^-1ϕ$ [ref] to the original action.
A translation-invariant renormalizable non-commutative scalar model · Introduction · 0.80
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Another, simplified version of a gauge model was discussed in [ref] .
Non-Commutative U(1) Gauge Theory on R**4 with Oscillator Term and BRST Symmetry · Introduction · 0.92
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