Abstract
Abstract
Discovery of superconductivity in electride materials has been a topic of interest as their intrinsic electron-rich properties might suggest a considerable electron–phonon interaction. Layered
Y
2
C
is a ferromagnetic quasi-two-dimensional electride with polarized anionic electrons confined in the interlayer space. In this theoretical study, we report
Y
2
C
undergoes a series of structural phase transitions into two superconducting phases with estimated
T
c
of 9.2 and 21.0 K at 19 and 80 GPa, respectively, via the suppression of magnetism. Our extensive first-principles swarm structure searches identify that these two high-pressure superconducting phases possess an orthorhombic Pnma and a tetragonal I4/m structures, respectively, where the Pnma phase is found to be a one-dimensional electride characterized by electron confinements in channel spaces of the crystal lattice, while the electride property in I4/m phase has been completely destroyed. We attribute the development of an unprecedentedly high
T
c
superconductivity in Y-C system to the destructions of magnetism and the delocalization of interlayered anionic electrons under pressures. This work provides a unique example of pressure-induced collapse of magnetism at the onset of superconductivity in electride materials, along with the dramatic changes of electron-confinement topology in crystal lattices.
Funder
the Research Grants Council of Hong Kong
Basic and Applied Basic Research Foundation of Guangdong Province
Guangzhou Basic and Applied Basic Research Foundation
the Open Project of Guangdong Provincial Key Laboratory of Magnetoelectric Physics and Devices
National Natural Science Foundation of China