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Although there is strong theoretical and experimental evidence for electron-hole superfluidity in separated sheets of electrons and holes at low , extending superfluidity to high is limited by strong 2D fluctuations and Kosterlitz-Thouless effects. We show this limitation can be overcome using a superlattice of alternating electron- and hole-doped semiconductor monolayers. The superfluid transition in a 3D superlattice is not topological, and for strong electron-hole pair coupling, the transition temperature can be at room temperature. As a quantitative illustration, we show can reach K for a superfluid in a realistic superlattice of transition metal dichalcogenide monolayers.

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