Abstract
We investigate the charge density wave (CDW) instability in single and double layers, as well as in the bulk 2H-NbSe. We demonstrate that the density functional theory correctly describes the metallic CDW state in the bulk 2H-NbSe. We predict that both mono- and bilayer NbSe undergo a CDW instability. However, while in the bulk the instability occurs at a momentum , in free-standing layers it occurs at . Furthermore, while in the bulk the CDW leads to a metallic state, in a monolayer the ground state becomes semimetallic, in agreement with recent experimental data. We elucidate the key role that an enhancement of the electron-phonon matrix element at plays in forming the CDW ground state.
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