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Perturbative Hairy Black Branes in the G2G_{2}-Invariant Sector of Dyonic ISO(7) Gauged Supergravity

Published 19 Aug 2026 in hep-th and gr-qc | (2608.18959v1)

Abstract: We construct perturbative black-brane solutions carrying neutral scalar hair in the G2G_{2}-invariant truncation of four-dimensional dyonic N=8\mathcal{N}=8 ISO(7) gauged supergravity, an exact consistent truncation of massive type~IIA supergravity on S<sup>6S<sup>{6}. Expanding around the G2G_{2}-symmetric AdS<em>4<em>{4}-Schwarzschild black brane in powers of a dimensionless scalar-charge parameter $\eps$, we show that the perturbation hierarchy reduces, order by order, to a nested sequence of inhomogeneous Legendre equations (demonstrated through second order). The first-order scalar satisfies a Pöschl--Teller equation with exact parameter ν(ν+1)=2/3ν(ν+1)=2/3, giving ν=12+336ν=-\frac{1}{2}+\frac{\sqrt{33}}{6}, and the first-order metric is fixed algebraically by the same function, A<sup>(1)=72φ<sup>(1)A<sup>{(1)}=-\tfrac{\sqrt{7}}{2}φ<sup>{(1)}, so the entire $\mathcal{O}(\eps)$ sector is one Legendre function. An identity ν+1=Δ</em>+/3ν+1=Δ</em>{+}/3, with Δ<em>+=(3+33)/24.372Δ<em>{+}=(3+\sqrt{33})/2\approx 4.372 the conformal dimension of the dual scalar operator, relates the Pöschl-Teller parameter to the AdS/CFT dictionary via the nonlinear Fefferman-Graham map zz</em>FG<sup>3z \propto z</em>{\mathrm{FG}}<sup>{3}. The $\mathcal{O}(\eps<sup>{2})$ back-reaction yields explicit corrections to the renormalized free energy and Bekenstein-Hawking entropy density at fixed temperature, consistent with the first law; equivalently, at fixed entropy or energy density it \emph{lowers} the Hawking temperature by $δT/T=\mathcal{O}(\eps<sup>{2})$. For the leading transport coefficients the shear viscosity saturates η/s=1/(4π)η/s=1/(4π), while the Eling-Oz horizon formula gives a nonzero bulk viscosity $ζ/η=\bigl(\tfrac{Δ<em>{+}-3}{2}\bigr)<sup>{2}\eps<sup>{2}=\tfrac{3(7-\sqrt{33})}{8}\eps<sup>{2}\approx0.471\,\eps<sup>{2}$. With $c</em>{s}<sup>{2}=\tfrac12-\mathcal</sup> O(\eps<sup>{2})&lt;\tfrac12$, this indicates a softening of the equation of state.

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