We glue together two copies of pure anti–de Sitter (AdS) spacetime along their conformal boundaries creating a manifold without boundaries. The resulting space, which in dimension $d+2$ we denote by $\mathrm{A}\mathrm{d}{\mathrm{S}}_{\pm }^{d+2}$, has the topology of $S^2\times {\mathrm{\Sigma }}^d$, where ${\mathrm{\Sigma }}^d$ is a $d$ manifold without boundary. Acting with ${\mathbb{Z}}_n$ on the $S^2$ factor amounts to coupling a pair of membranes at the north and south poles of the two-sphere. Moreover, extending the domain of the two-sphere polar coordinate from $[0,\pi ]$ to the interval $[0,(2N-1)\pi ]$, where $N>1$, enables the coupling of one stack of $N$ coincident membranes at each pole of the two-sphere ($2N$ membranes in total). Assuming the existence of a quantum gravity theory on the glued spacetime, we compute the classical approximation of the entanglement entropy across an entangling surface consisting of the two antipodal stacks of membranes. We find that the resulting entropy exhibits a boundary cutoff divergence that can be canceled by taking the limit of an infinite number of membranes. This large-$N$ cancelation—possible only in the doubled, extended geometry without boundaries—yields a finite, universal quarter-area law. The calculation does not require details of the quantum theory other than its infrared limit, which we assume to be Einstein gravity.

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• Entanglement in field theory
• Field & string theory models & techniques
• General relativity
• Geometry
• Gravity in dimensions other than four
• Quantum gravity
• Strings & branes