Emergent layered Cu-bearing van der
Waals (vdW) compounds have
great potentials for use in electrocatalysis, lithium batteries, and
electronic and optoelectronic devices. However, many of their alluring
properties such as potential superconductivity remain unknown. In
this work, using CuP2Se as a model compound, we explored
its electrical transport and structural evolution at pressures up
to ∼60 GPa using both experimental determinations and ab initio
calculations. We found that CuP2Se undergoes a semiconductor-to-metal
transition at ∼20 GPa at room temperature and a metal-to-superconductor
transition at 3.3–5.7 K in the pressure range from 27.0 to
61.4 GPa. At ∼10 and 20 GPa, there are two isostructural changes
in the compound, corresponding to, respectively, the emergence of
the interlayer coupling and start of interlayer atomic bonding. At
a pressure between 35 and 40 GPa, the vdW layers start to slide and
then merge, forming a new phase with high coordination numbers. We
also found that the Bardeen–Cooper–Schrieffer (BCS)
theory describes quite well the pressure dependence of the critical
temperature despite occurrence of a possible medium-to-strong electron–phonon
coupling, revealing the determinant roles of the enhanced bulk modulus
and electron density of states at high pressure. Moreover, nanosizing
of CuP2Se at high pressure further increased the critical
temperature even at sizes approaching the Anderson limit. These findings
would have important implications for developing novel applications
of layered vdW compounds through simple pressure tuning of the interlayer
coupling.