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We describe Bose-Einstein condensation of strongly interacting particles intoa quantum state which is an excited single-particle state, but becomes theground state as density increases because it minimizes the interaction energycompared to other states. Mean field calculations for a graphene potential justwide enough for two closely interacting layers of molecular hydrogen showcondensation at temperatures up to 60 K. In the condensed state, molecules hopbetween layers, increasing the first peak in the pair-correlation function justpast the hard core repulsion diameter.

High temperature Bose-Einstein condensation into an excited state at equilibrium