Novel Strongly Spin-Orbit Coupled Quantum Dimer Magnet: Yb$_2$Si$_2$O$_7$
Autor: | Hester, Gavin, Nair, H. S., Reeder, T., Yahne, D. R., DeLazzer, T. N., Berges, L., Ziat, D., Neilson, J. R., Aczel, A. A., Sala, G., Quilliam, J. A., Ross, K. A. |
---|---|
Rok vydání: | 2018 |
Předmět: | |
Zdroj: | Phys. Rev. Lett. 123, 027201 (2019) |
Druh dokumentu: | Working Paper |
DOI: | 10.1103/PhysRevLett.123.027201 |
Popis: | The quantum dimer magnet (QDM) is the canonical example of quantum magnetism. The QDM state consists of entangled nearest-neighbor spin dimers and often exhibits a field-induced triplon Bose-Einstein condensate (BEC) phase. We report on a new QDM in the strongly spin-orbit coupled, distorted honeycomb-lattice material Yb$_2$Si$_2$O$_7$. Our single crystal neutron scattering, specific heat, and ultrasound velocity measurements reveal a gapped singlet ground state at zero field with sharp, dispersive excitations. We find a field-induced magnetically ordered phase reminiscent of a BEC phase, with exceptionally low critical fields of $H_{c1} \sim 0.4$ T and $H_{c2} \sim 1.4$ T. Using inelastic neutron scattering in an applied magnetic field we observe a Goldstone mode (gapless to within $\delta E$ = 0.037 meV) that persists throughout the entire field-induced magnetically ordered phase, suggestive of the spontaneous breaking of U(1) symmetry expected for a triplon BEC. However, in contrast to other well-known cases of this phase, the high-field ($\mu$$_0$$H\geq1.2$T) part of the phase diagram in Yb$_2$Si$_2$O$_7$ is interrupted by an unusual regime signaled by a change in the field dependence of the ultrasound velocity and magnetization, as well as the disappearance of a sharp anomaly in the specific heat. These measurements raise the question of how anisotropy in strongly spin-orbit coupled materials modifies the field induced phases of QDMs. Comment: 6 pages, 4 figures, 12 pages of Supplemental Information, 15 Supplemental figures. Updated to published version |
Databáze: | arXiv |
Externí odkaz: |