| Full text | |
| Author(s): |
Total Authors: 4
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| Affiliation: | [1] Univ Fed ABC, Ctr Matemat Computacao & Cognicao, Santo Andre, SP - Brazil
[2] UERJ Univ Estado Rio de Janeiro, Inst Fis, Dept Fis Teor, Rua Sao Francisco Xavier 524, BR-20550013 Maracana, RJ - Brazil
[3] INFN, Sez Napoli, Via Cintia, I-80126 Naples - Italy
[4] Univ Napoli Federico II, Dipartimento Matemat & Applicaz R Caccioppoli, Via Cintia, I-80126 Naples - Italy
[5] Univ Napoli Federico II, Dipartimento Fis E Pancini, Via Cintia, I-80126 Naples - Italy
Total Affiliations: 5
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| Document type: | Journal article |
| Source: | Nuclear Physics B; v. 974, JAN 2022. |
| Web of Science Citations: | 1 |
| Abstract | |
It is known that Noncommutative QED (NCQED) exhibits Gribov ambiguities in the Landau gauge. These ambiguities are related to zero modes of the Faddeev-Popov operator and arise in the ghost propagator when it has a pole. In this work, we establish a positive Faddeev-Popov operator for NCQED and the condition for the ghost propagator not to have poles, the so-called Gribov no-pole condition. This condition is implemented in the path integral and allows for the calculation of the photon propagator in momentum space, which is dependent on the squared non-commutativity parameter. In the commutative limit, the standard QED is recovered. (C) 2021 The Authors. Published by Elsevier B.V. (AU) | |
| FAPESP's process: | 19/26291-8 - Aspects of non-commutative gauge theories |
| Grantee: | Ozorio Bezerra Holanda Neto |
| Support Opportunities: | Scholarships in Brazil - Post-Doctoral |