Non-Noetherian conformal Cheshire effect
Abstract The gravitational Cheshire effect refers to the possibility of turning off the gravitational field while still leaving an imprint of the nonminimal coupling of matter to gravity. This allows nontrivial solutions in flat spacetime for which no backreaction is possible. The effect was origina...
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| Language: | English |
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SpringerOpen
2025-03-01
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| Series: | European Physical Journal C: Particles and Fields |
| Online Access: | https://doi.org/10.1140/epjc/s10052-025-14011-5 |
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| author | Eloy Ayón-Beato Mokhtar Hassaine Pedro A. Sánchez |
| author_facet | Eloy Ayón-Beato Mokhtar Hassaine Pedro A. Sánchez |
| author_sort | Eloy Ayón-Beato |
| collection | DOAJ |
| description | Abstract The gravitational Cheshire effect refers to the possibility of turning off the gravitational field while still leaving an imprint of the nonminimal coupling of matter to gravity. This allows nontrivial solutions in flat spacetime for which no backreaction is possible. The effect was originally shown to manifest itself for standard nonminimal couplings, such as those allowing conventional conformally invariant scalar fields. Recently, the most general scalar field action yielding a conformally invariant second-order equation was constructed, and entails a more involved nonminimal coupling explicitly breaking the conformal invariance of the action without spoiling it in the equation. We have succeeded in fully describing the spherically symmetric stealth solutions on flat spacetime supporting the Cheshire effect within this general non-Noetherian conformal theory. The allowed configurations are divided into two branches: The first one essentially corresponds to an extension of the solutions already known for the standard Noetherian conformal theory. The second branch is only possible due to the non-Noetherian conformal contribution of the action. The complete characterization of this branch is expressed by a nonlinear first-order partial differential equation. We have found the general solution of this equation using both seemingly new and well-established mathematical tools. |
| format | Article |
| id | doaj-art-02bf4674c8784d6a9050efb11c3e2d99 |
| institution | OA Journals |
| issn | 1434-6052 |
| language | English |
| publishDate | 2025-03-01 |
| publisher | SpringerOpen |
| record_format | Article |
| series | European Physical Journal C: Particles and Fields |
| spelling | doaj-art-02bf4674c8784d6a9050efb11c3e2d992025-08-20T02:12:07ZengSpringerOpenEuropean Physical Journal C: Particles and Fields1434-60522025-03-0185311210.1140/epjc/s10052-025-14011-5Non-Noetherian conformal Cheshire effectEloy Ayón-Beato0Mokhtar Hassaine1Pedro A. Sánchez2Departamento de Física, CINVESTAV-IPNInstituto de Matemática, Universidad de TalcaDepartamento de Física, CINVESTAV-IPNAbstract The gravitational Cheshire effect refers to the possibility of turning off the gravitational field while still leaving an imprint of the nonminimal coupling of matter to gravity. This allows nontrivial solutions in flat spacetime for which no backreaction is possible. The effect was originally shown to manifest itself for standard nonminimal couplings, such as those allowing conventional conformally invariant scalar fields. Recently, the most general scalar field action yielding a conformally invariant second-order equation was constructed, and entails a more involved nonminimal coupling explicitly breaking the conformal invariance of the action without spoiling it in the equation. We have succeeded in fully describing the spherically symmetric stealth solutions on flat spacetime supporting the Cheshire effect within this general non-Noetherian conformal theory. The allowed configurations are divided into two branches: The first one essentially corresponds to an extension of the solutions already known for the standard Noetherian conformal theory. The second branch is only possible due to the non-Noetherian conformal contribution of the action. The complete characterization of this branch is expressed by a nonlinear first-order partial differential equation. We have found the general solution of this equation using both seemingly new and well-established mathematical tools.https://doi.org/10.1140/epjc/s10052-025-14011-5 |
| spellingShingle | Eloy Ayón-Beato Mokhtar Hassaine Pedro A. Sánchez Non-Noetherian conformal Cheshire effect European Physical Journal C: Particles and Fields |
| title | Non-Noetherian conformal Cheshire effect |
| title_full | Non-Noetherian conformal Cheshire effect |
| title_fullStr | Non-Noetherian conformal Cheshire effect |
| title_full_unstemmed | Non-Noetherian conformal Cheshire effect |
| title_short | Non-Noetherian conformal Cheshire effect |
| title_sort | non noetherian conformal cheshire effect |
| url | https://doi.org/10.1140/epjc/s10052-025-14011-5 |
| work_keys_str_mv | AT eloyayonbeato nonnoetherianconformalcheshireeffect AT mokhtarhassaine nonnoetherianconformalcheshireeffect AT pedroasanchez nonnoetherianconformalcheshireeffect |