  We show that a $(\mathbb {RP}^1 \times \mathbb{RP}^1)$-gauged $\mathbb{Z}_2$
quotient of $\mathbb R^{2,2}$ embeds an AdS$_3/\mathbb Z_2/ (\mathbb{RP}^1
\times \mathbb{RP}^1)$ spacetime that is globally hyperbolic, unlike regular
AdS$_3$. This embedded spacetime possesses a single cover of AdS$_3$'s
isometries without producing closed timelike curves and a non-timelike
boundary. After including its gauge symmetries, its AdS$_3$/CFT$_2$
correspondence becomes equivalent to an embedded $\frac{\text{AdS}_3}{\mathbb
Z_2}$ / $\frac{\mathbb R^{2,2}}{\mathbb Z_2}$ embedding correspondence.
