condensed matter physics

Zero-Field Long Range Order at mK in the Proximate Quantum Spin Ice CeSnO and Phase Diagram for Magnetic Fields Along [1,1,0]

arXiv:2607.12274

summary

Heat capacity measurements on a high-quality Ce₂Sn₂O₇ single crystal reveal a first‑order transition to long‑range magnetic order at ~40 mK, disproving a zero‑field quantum spin‑ice ground state, while magnetic fields along [1,1,0] expose a rich phase diagram with spin‑ice‑like features.

Abstract

The Ce pseudospin-1/2 degrees of freedom in the pyrochlore magnets CeXO, with = Zr, Hf, or Sn, possess dipole-octupole character. The XYZ nearest-neighbor model Hamiltonians which have successfully described their properties make them attractive candidates for quantum spin ice ground states. We report new heat capacity measurements to very low temperatures on a high-quality single crystal of CeSnO grown by hydrothermal techniques. Our zero-field measurements uncover a clear first order transition to long-ranged order at K, well below the downturn in the broader Schottky-like anomaly that is a common feature in the zero-field heat capacity for cerium pyrochlores. This observation settles the debate as to whether CeSnO possesses a QSI ground state in zero field - it does not. However, we also find compelling evidence suggesting that spin ice physics is nearby, and remains relevant to CeSnO. Application of a magnetic field along the direction leads to an evolution of this peak to a weak anomaly at higher temperature more characteristic of a continuous, mean field transition. At higher fields along , the Schottky-like anomaly bifurcates similar to expectations for independent polarized and orthogonal chains in classical spin ice. These new experimental results demonstrate richness to the phase diagram for Ce-based pyrochlores.

Main Text (5 pages, 4 figures), Supplemental Material (6 pages, 4 figures)

Topics & keywords

#quantum spin ice#pyrochlore magnets#low-temperature heat capacity#magnetic field phase diagram#dipole-octupole pseudospinsCe2Sn2O7XYZ nearest-neighbor modelfirst-order transitionSchottky anomaly[1,1,0] magnetic field