Kalb-Ramond topological term in Majorana superspace and Kaluza-Klein spectrum deformation in five dimensions
- 1Universidade Federal Rural do Semi-Árido (UFERSA)
- 2Universidade Federal do Ceará, Departamento de Física
Abstract
A bstract : We construct an intrinsic N = 1, D = 5 superspace whose Grassmann coordinate is a five-dimensional Dirac spinor decomposed into two four-dimensional Majorana spinors, Θ =θ +ioverset∼ θ Θ = θ + i θ ~ , and use it to analyze the supersymmetric structure of the five-dimensional Kalb-Ramond (KR) topological term. The supersymmetry algebra closes on the fifth momentum through anticommutators of opposite-sector generators, realizing ∂ ₅ as a central charge in the sense of Sohnius; we show that this assignment is the unique covariant one, and we give an explicit dictionary to the N = 1/2 superspace of Linch, Luty and Phillips and to the four-dimensional N = 1 superform hierarchies of Becker, Becker, Linch, Randall and Robbins. Two structural results follow. First, a tensor multiplet subjected to both available same-side chirality conditions cannot propagate in the fifth dimension; the KR multiplet is therefore described by a singly chiral spinor superfield whose composite field strength T 5 α = ∂ ₅ B α + W α ( V T ) realizes the single-chain tensor hierarchy with differential ∂ ₅ , and the supersymmetric completion of the topological term is the corresponding BF -type quadratic invariant, whose component form agrees, up to normalization conventions, with the pseudo-supersymmetric action. Second, we correct the six-dimensional origin of the topological term, S ₆ = ∫ dϕ ∧ B ∧ H , and show that for the KR field alone the five-dimensional term is a total derivative and leaves the Kaluza-Klein tower undeformed. After the superfield-level identification B m 5 → A m , however, the mixed topological term becomes a genuine BF coupling between independent multiplets, and the Kaluza-Klein spectrum splits exactly into mn,±2=(√(n2/R2+M2)± M)2 m n , ± 2 = n 2 / R 2 + M 2 ± M 2 , with M fixed by the topological coupling: the zero mode acquires a topological mass 2 M , and the excited towers are displaced by the constant ±M relative to bulk fields that share the compactification radius but lack the coupling. This relative deformation cannot be absorbed into a redefinition of R and constitutes a sharp, calculable prediction for compactification on S ¹ . On the orbifold S ¹ / ℤ ₂ relevant to brane worlds the situation is qualitatively different, and we show that it is controlled by supersymmetry: the gauge structure of the hierarchy correlates the ℤ ₂ parities of the two multiplets, the topological term is parity-odd, and a constant coupling is projected out, so that the deformation is governed by a coupling of the kink type — precisely the one generated by the six-dimensional parent action — and becomes second order in the coupling, with brane-localized contributions at the fixed points.
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BibTeX
@article{nunes2026kalbramond,
title = {{Kalb-Ramond topological term in Majorana superspace and Kaluza-Klein spectrum deformation in five dimensions}},
author = {L. A. S. Nunes and C. A. S. Almeida},
journal = {Journal of High Energy Physics},
year = {2026},
month = oct,
doi = {10.1007/jhep10(2026)235},
url = {https://link.springer.com/article/10.1007/JHEP10(2026)235},
note = {CC BY 4.0},
}
RIS
TY - JOUR
TI - Kalb-Ramond topological term in Majorana superspace and Kaluza-Klein spectrum deformation in five dimensions
AU - L. A. S. Nunes
AU - C. A. S. Almeida
PY - 2026
DA - 2026/10/22
JO - Journal of High Energy Physics
DO - 10.1007/jhep10(2026)235
UR - https://link.springer.com/article/10.1007/JHEP10(2026)235
AB - A bstract : We construct an intrinsic N = 1, D = 5 superspace whose Grassmann coordinate is a five-dimensional Dirac spinor decomposed into two four-dimensional Majorana spinors, Θ =θ +ioverset∼ θ Θ = θ + i θ ~ , and use it to analyze the supersymmetric structure of the five-dimensional Kalb-Ramond (KR) topological term. The supersymmetry algebra closes on the fifth momentum through anticommutators of opposite-sector generators, realizing ∂ ₅ as a central charge in the sense of Sohnius; we show that this assignment is the unique covariant one, and we give an explicit dictionary to the N = 1/2 superspace of Linch, Luty and Phillips and to the four-dimensional N = 1 superform hierarchies of Becker, Becker, Linch, Randall and Robbins. Two structural results follow. First, a tensor multiplet subjected to both available same-side chirality conditions cannot propagate in the fifth dimension; the KR multiplet is therefore described by a singly chiral spinor superfield whose composite field strength T 5 α = ∂ ₅ B α + W α ( V T ) realizes the single-chain tensor hierarchy with differential ∂ ₅ , and the supersymmetric completion of the topological term is the corresponding BF -type quadratic invariant, whose component form agrees, up to normalization conventions, with the pseudo-supersymmetric action. Second, we correct the six-dimensional origin of the topological term, S ₆ = ∫ dϕ ∧ B ∧ H , and show that for the KR field alone the five-dimensional term is a total derivative and leaves the Kaluza-Klein tower undeformed. After the superfield-level identification B m 5 → A m , however, the mixed topological term becomes a genuine BF coupling between independent multiplets, and the Kaluza-Klein spectrum splits exactly into m_n,±^2=(√(n^2/R^2+M^2)± M)^2 m n , ± 2 = n 2 / R 2 + M 2 ± M 2 , with M fixed by the topological coupling: the zero mode acquires a topological mass 2 M , and the excited towers are displaced by the constant ±M relative to bulk fields that share the compactification radius but lack the coupling. This relative deformation cannot be absorbed into a redefinition of R and constitutes a sharp, calculable prediction for compactification on S ¹ . On the orbifold S ¹ / ℤ ₂ relevant to brane worlds the situation is qualitatively different, and we show that it is controlled by supersymmetry: the gauge structure of the hierarchy correlates the ℤ ₂ parities of the two multiplets, the topological term is parity-odd, and a constant coupling is projected out, so that the deformation is governed by a coupling of the kink type — precisely the one generated by the six-dimensional parent action — and becomes second order in the coupling, with brane-localized contributions at the fixed points.
SN - 1029-8479
ER -