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Nonperturbative renormalization of the quark chromoelectric dipole moment with the gradient flow: Power divergences
The CP-violating quark chromoelectric dipole moment (qCEDM) operator, contributing to the electric dipole moment (EDM), mixes under renormalization and-particularly on the lattice-with the pseudoscalar density. The mixing coefficient is power-divergent with the inverse lattice spacing squared, 1/a2,...
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Published in: | Physical review. D 2021-10, Vol.104 (7), p.1, Article 074516 |
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Main Authors: | , , , |
Format: | Article |
Language: | English |
Subjects: | |
Citations: | Items that this one cites Items that cite this one |
Online Access: | Get full text |
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Summary: | The CP-violating quark chromoelectric dipole moment (qCEDM) operator, contributing to the electric dipole moment (EDM), mixes under renormalization and-particularly on the lattice-with the pseudoscalar density. The mixing coefficient is power-divergent with the inverse lattice spacing squared, 1/a2, regardless of the lattice action used. We use the gradient flow to define a multiplicatively renormalized qCEDM operator and study its behavior at small flow time. We determine nonperturbatively the linearly divergent coefficient with the flow time, 1/t, up to subleading logarithmic corrections, and compare it with the 1-loop perturbative expansion in the bare and renormalized strong coupling. We also discuss the O ( a ) improvement of the qCEDM defined at positive flow time. |
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ISSN: | 2470-0010 2470-0029 |
DOI: | 10.1103/PhysRevD.104.074516 |