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Casimir energy and radius stabilization in five and six dimensional orbifolds
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The paper computes one-loop Casimir energies on five- and six-dimensional orbifolds and studies whether they can stabilize the compactification radius. It finds that massless-field Casimir energy alone is typically repulsive in the motivated models, but brane-localized kinetic terms, massive fields, and tuned brane/cosmological counterterms can produce minima.
Key findings
- For \(S^1/Z_2\), neglecting fixed-point terms, the Casimir energy is one half that of \(S^1\). The massless periodic scalar result is \(V_{+,{\rm scalar}}(\phi)=-\frac{3\zeta(5)}{64\pi^2}\frac{1}{\phi^2 L^4}\), with ratios \(V_{+,{\rm graviton}}=5V_{+,{\rm scalar}}\), \(V_{+,{\rm fermion}}=-4V_{+,{\rm scalar}}\), \(V_{+,{\rm vector}}=3V_{+,{\rm scalar}}\), \(V_{+,{\rm gravitino}}=-8V_{+,{\rm scalar}}\); antiperiodic scalar gives \(V_{-,{\rm scalar}}=-\frac{15}{16}V_{+,{\rm scalar}}\) and antiperiodic fermion \(V_{-,{\rm fermion}}=\frac{15}{4}V_{+,{\rm scalar}}\).
- Massive fields can stabilize the radius if their Casimir contribution is repulsive and dominates at small radii, while the massless contribution is attractive and the bulk cosmological constant is fine-tuned positive; the radius is then typically of order the inverse mass.
- Brane-localized kinetic terms can also stabilize the radion. With one boundary term vanishing, a minimum occurs at a radius of order the nonzero \(c_i\); with both present, a local minimum persists for asymmetry \(c_0/c_L\sim 0.3\), but there is no minimum if \(c_0=c_L\). NDA-sized terms can yield a radius several times the cutoff, and larger terms can yield a larger radius while perturbation theory remains consistent.
- In the 6D toroidal case, for repulsive total Casimir energy the fixed-area minimum is at \(\tau=e^{2\pi i/3}\). Applying the results to the 5D supersymmetric model of ref. [22], the massless-field radion potential is repulsive, \(V_{\rm massless}(\phi)=-1364V_{+,{\rm scalar}}(\phi)=+\frac{1023\zeta(5)}{16}\frac{1}{\phi^2 L^4}\); a stable minimum with vanishing cosmological constant requires positive bulk cosmological constant and negative brane tensions, which appears problematic for supersymmetry.
Methods
- One-loop Casimir energies are computed using \(\zeta\)-function regularization on \(S^1/Z_2\) and \(T^2/Z_k\) orbifolds, for gravitational, massless, and massive fields with periodic or antiperiodic boundary conditions.
- The radius potential is analyzed including bulk cosmological constant, brane-tension counterterms, and brane-localized kinetic/mass terms; normalization conditions \(V(\phi)=V'(\phi)=0\) are imposed to seek minima with vanishing four-dimensional cosmological constant.
- An exact tree-level propagator with brane kinetic terms is derived to check perturbativity, and the general results are applied to the 5D supersymmetric electroweak model of ref. [22] and the 6D composite-Higgs model of ref. [23].
Limitations
- The paper states that it neglects warping/backreaction from brane tensions and bulk cosmological constant counterterms, assumes brane tensions are small enough, and treats only static minima; cosmological evolution is left for future work.
- It states that deciding whether the required stabilization is viable in the supersymmetric 5D case requires a full embedding in 5D supergravity, since the needed bulk counterterm is not supersymmetric in the simplest 5D supergravities.
- The text also notes that the field-theory orbifolds considered cannot at present be derived from known string constructions and are treated only as low-energy effective theories up to a cutoff; additionally, the 5D SUSY model has a second degenerate minimum at \(\phi=\infty\), and for negative bulk cosmological constant the true minimum would be AdS, raising tunneling concerns.
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In the paper
“We will show that in some cases it is possible to achieve a (local) minimum of V (φ) with vanishing cosmological constant.”
§ Casimir energy and radius stabilization in five and six dimensional orbifolds > JHEP06(2001)019
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“As noted in the introduction, including the contribution to the Casimir energy of the massless fields alone (without including brane tensions) it is not possible to obtain a minimum for φ with vanishing cosmological constant.”
§ Casimir energy and radius stabilization in five and six dimensional orbifolds > JHEP06(2001)019
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“All of these give a contribution to the Casimir energy which is 9 times that of eq.(4.6).”
§ Casimir energy and radius stabilization in five and six dimensional orbifolds > JHEP06(2001)019
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In the paper
“Since Li 5 (1) = ζ(5) and Li 5 (-1) = -15ζ(5)/16, the above expression reduces to the massless formulae for the periodic (2.11) and antiperiodic (2.13) case in the small mass or small radius (φ → 0) limit.”
§ Casimir energy and radius stabilization in five and six dimensional orbifolds > JHEP06(2001)019
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In the paper
“We calculate, in section 3, the Casimir energy in the theory with the inclusion of such terms and find that it is possible to achieve a minimum for φ with vanishing cosmological constant; we also discuss localized mass terms.”
§ Casimir energy and radius stabilization in five and six dimensional orbifolds > JHEP06(2001)019
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Pinto, P. F. S. (2026) · Physics of the Dark Universe · doi:10.1016/j.dark.2026.102266 · Cited by 1
Conformal matter in warped backgrounds
Hofmann, R., & Pospelov, M. (2003) · Physics Letters B · doi:10.1016/s0370-2693(03)00135-7 · Cited by 1
Self-energies for interacting fields with a compactified spatial dimension
Barone, F. A., & Hott, M. (2008) · Brazilian Journal of Physics · doi:10.1590/s0103-97332008000200002 · Cited by 1
Casimir energy and the possibility of higher dimensional manipulationPreprint
Obousy, R., & SAHARIAN, A. A. (2009) · arXiv (Cornell University) · doi:10.48550/arxiv.0906.4601 · Cited by 1
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On the problem of vacuum energy in brane theories
Gurwich, I., Rubin, S., & Davidson, A. (2009) · Physics Letters B · doi:10.1016/j.physletb.2009.08.009 · Cited by 1
GUT scale extra dimensions and light moduli in supergravity and cosmology
Moller, J. (2010) · DESY (CERN, DESY, Fermilab, IHEP, and SLAC) · doi:10.3204/desy-thesis-2010-017 · Cited by 1
Conformal matter in warped backgroundsPreprint
Hofmann, R., & Pospelov, M. (2003) · Cited by 1
Sequestered Conformal Anomaly Mediation (SCAM)Preprint
Nee, M., & Randall, L. (2025) · arXiv (Cornell University) · doi:10.48550/arxiv.2510.11784 · Cited by 1
A Casimir turning point as the beginning of a small flat universe
Zhang, A. (2026) · arXiv · doi:10.48550/arxiv.2610.24905
“The same mechanism is known on a two-torus [140–142], Casimir back-reaction makes a torus ever thinner in 2 + 1 gravity [143] and more elongated in de Sitter space [144], and a fully compactified Standard Model on T 3 is unstable against decompactification, crunching or anisotropic evolution [39].”
Constraints on Models with Warped Extra DimensionsPreprint
Archer, P. R. (2012) · arXiv (Cornell University) · doi:10.48550/arxiv.1201.1561
The Zeta Function Approach to Casimir Energy Calculations in Higher DimensionsPreprint
Obousy, R. (2011) · arXiv (Cornell University) · doi:10.48550/arxiv.1108.5997
New Form of the T-Duality Due to the Stability of a Compact Dimension
Kamani, D. (2008) · International Journal of Theoretical Physics · doi:10.1007/s10773-008-9834-7
Supersymmetric large extra dimensions
Hoover, D. (2009) · eScholarship@McGill (McGill) · doi:10.82308/52208
Possible contributions to the bulk Casimir energy in heterotic M-theory
Ahmed, N. (2014) · Advanced Studies in Theoretical Physics · doi:10.12988/astp.2014.49129
Teeple, B. (2015) · TSpace (University of Toronto)
Strongly coupled scenarios of electro-weak symmetry breaking
Vecchi, L. (2009) · SDL
Dark energy from antigravitons in in stringy black holes
Douhou, K. (2019) · Advanced Studies in Theoretical Physics · doi:10.12988/astp.2019.929
Dimension spatiale supplémentaire compactifiée et champ de Higgs branaire
Nortier, F. (2021) · HAL · doi:10.5281/zenodo.4892767
Cosmological phase transitions: extra dimensions and black holes
Manuel, J. P. (2020) · Sussex Research Online (University of Sussex)
Dark Energy from Cosmic Antineutrinos in Large Extradimensions
Ennadifi, S. E., & Kowalewska, S. M. (2021) · Arabian Journal for Science and Engineering · doi:10.1007/s13369-021-05823-0
Metadata
- Authors
- Pontón, E., & Poppitz, E.
- Affiliations
- Yale University (US)
- Venue
- Journal of High Energy Physics
- Published
- 2001-06-08
- Volume
- 2001
- Issue
- 06
- Pages
- 019-019
- ISSN
- 1029-8479 (ISSN-L)
- OpenAlex
- W2026481067
- Cited by
- 210
- References
- 44
- Citations by year
- 2026: 7 · 2025: 3 · 2024: 5 · 2023: 5 · 2022: 6 · 2021: 7 · 2020: 8 · 2019: 2 · 2018: 5 · 2017: 3 · 2016: 2 · 2015: 6 · 2014: 10 · 2013: 7 · 2012: 1
- FWCI
- 8.86
- Type
- journal article
- Language
- en
- Open access
- bronze
- doi.org
- Locations
- Journal of High Energy Physics (publishedVersion)
- arXiv (Cornell University) (submittedVersion)
- CERN Document Server (European Organization for Nuclear Research) (submittedVersion)
- arXiv (Cornell University)
- Funders
- U.S. Department of Energy (DE‐FG02‐, DEFG0292ER40704)
- Topics
- Physical Sciences › Physics and Astronomy › Nuclear and High Energy Physics › Black Holes and Theoretical Physics
- Physical Sciences › Physics and Astronomy › Astronomy and Astrophysics › Cosmology and Gravitation Theories
- Physical Sciences › Physics and Astronomy › Atomic and Molecular Physics, and Optics › Quantum Electrodynamics and Casimir Effect
- Keywords
- Casimir energy, radius stabilization, orbifolds, one-loop effective action, boundary conditions, fixed points, cosmological constant, brane tension
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Bibliographic data: Semantic Scholar, OpenAlex, Crossref.
Contains information from the Semantic Scholar Academic Graph Datasets, made available under the ODC Attribution License (ODC-BY 1.0).
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