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On the generalized Komar charge of Kaluza-Klein theories and higher-form symmetries
by G. Barbagallo, J. L. V. Cerdeira, C. Gómez-Fayrén, P. Meessen, T. Ortín
This is not the latest submitted version.
Submission summary
| Authors (as registered SciPost users): | Tomás Ortín |
| Submission information | |
|---|---|
| Preprint Link: | https://arxiv.org/abs/2506.15615v1 (pdf) |
| Date submitted: | June 30, 2025, 10:28 a.m. |
| Submitted by: | Tomás Ortín |
| Submitted to: | SciPost Physics Core |
| Ontological classification | |
|---|---|
| Academic field: | Physics |
| Specialties: |
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| Approach: | Theoretical |
Abstract
The generalized Komar $(d-2)$-form charge can be modified by the addition of any other on-shell closed (conserved) $(d-2)$-form charge. We show that, with Kaluza--Klein boundary conditions, one has to add a charge related to the higher-form symmetry identified in Ref.~\cite{Gomez-Fayren:2024cpl} to the naive Komar charge of pure 5-dimensional gravity to obtain a conserved charge charge whose integral at spatial infinity gives the mass. The new term also contains the contribution of the Kaluza--Klein monopole charge leading to electric-magnetic duality invariance.
Current status:
Reports on this Submission
Report #2 by Anonymous (Referee 2) on 2025-8-27 (Invited Report)
- Cite as: Anonymous, Report on arXiv:2506.15615v1, delivered 2025-08-27, doi: 10.21468/SciPost.Report.11815
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Report
The presentation is clear, and it provides an appropriate amount of details and references. In my opinion, the paper is suitable for publication in SciPost in its current form.
Requested changes
The main result eq. (3.15) gives the five-dimensional counterpart of the Komar current associated with the Killing vector (called $l$) generating a black hole event horizon. This gives rise to a conserved charge which is the combination of the four-dimensional mass and angular momentum. On the other hand, at different points in the paper (including the abstract) it is stated that the five-dimensional counterpart of the integral giving the mass is obtained. I suggest the author clarify how one can obtain the mass and the angular momentum separately from (3.15).
A minor point: the indices should be fixed in eq. (2.26a).
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Author: Tomás Ortín on 2025-09-22 [id 5846]
(in reply to Report 2 on 2025-08-27)Dear editor,
in order to answer the referee's point we have added the following paragraph below (3.15):
The first term in the right-hand side of the above equation is the standard
Komar charge whose integral gives the gravitational conserved charge
associated to the Killing vector $l$. In this case, $l$ is given by the linear
combination in Eq.~(\ref{eq:lhatdef}) (just the first two terms) when $m$
generates time translations and $n$ rotations around one axis. Since the Komar
charge is linear, its integral will give a linear combination of the mass and
and angular momentum with the angular velocity $\Omega_{\mathcal{H}}$ as
coefficient.
We have also corrected the typo in (2.26a)
We attach the PDF file of the corrected manuscript.
Yours,
Attachment:
KOMARKK.pdf