Mochamad Januar, Cheng‐Hong Liu, Abhijit Aich, J. H. Lee, Siddheswar Maikap, Min-Hung Lee
High Resolution Image Download MS PowerPoint Slide Rhombohedral hafnia-based ferroelectrics promise low-coercive, scalable nonvolatile memories, yet their realization has traditionally relied on complex cation intercalation or external stress. Here, we demonstrate a possible intrinsic route to the rhombohedral ( R3 ) phase in Hf 1– x Zr x O 2 through symmetry breaking of the parent fluorite lattice. First-principles calculations under R3 symmetry-constrained equation-of-state conditions show that the 12-atom fluorite-derived configuration, at equiatomic composition ( x = 0.5), stabilizes an intrinsically polar R3 ground state with spontaneous polarization P s = 44.9 μC cm –2, dielectric permittivity ε r = 51.3, an ultralow switching barrier of 27.8 meV f.u .–1, and a coercive field of 0.46 MV cm –1 . Distinct from orthorhombic Pca2 1, the R3 structure shows nonmonotonic dielectric behavior, revealing a symmetry-renormalized polarization mechanism beyond conventional Vegard-type ferroelectricity. Moreover, the R3 phase stabilizes at reduced thickness, with low built-in potential at proper electrodes preserving its low coercive field. Experiments using fast Fourier transform and geometric-phase analysis validate these predictions, and R3 -phase-dominant Hf 1– x Zr x O 2 capacitors exhibit comparably low coercive fields (0.65 MV cm –1 ) and enhanced dielectric permittivity ε r = 39.1.