\[g_{\mu \nu }=\tilde{g}_{\mu \nu }+h_{\mu \nu }\]
and fall-off conditions w.r.t $r$, where $\tilde{g}_{\mu \nu }$ is the AdS soliton metric. Horowitz and Myers go on to propose two conjectures, which are as follows:
- SUGRA solutions: $g_{\mu \nu }=\tilde{g}_{\mu \nu }$ is the only solution to $D=10$ type IIB SUGRA, taking $\tilde{g}_{\mu \nu }\times S^{5}_{l}$ for which $\mathcal{E}= 0$, and $\mathcal{E}\geq 0$ in general.
- Geometric solutions: $g_{\mu \nu }=\tilde{g}_{\mu \nu }$ is the only solution to $D=5$ field equations with $\Lambda = -6/l^{2}$ so that $\mathcal{E}=0$, and $\mathcal{E}\geq 0$ in general.
Seemingly, these are still open problems. However, I believe that resolving at least some aspects of these conjectures will go a long way in making sense of the geometric description of AdS/CFT.
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