Impact of Stoichiometry of Yb$_{\mathrm{2+}}_{x}$Ti$_{\mathrm{2-}}_{x}$O$_{\mathrm{7-}}_{x}_{\mathrm{/2}}$ on its Structure and Physical Properties
ORAL
Abstract
The rare-earth pyrochlores ($R_{\mathrm{2}}M_{\mathrm{2}}$O$_{\mathrm{7}})$ are topic of intense study in the field of magnetism as an ideal host for geometric frustration including spin-liquid and spin-ice behaviour. Specifically, $R_{\mathrm{2}}$Ti$_{\mathrm{2}}$O$_{\mathrm{7\thinspace }}$has proved a rich playground: compounds $R \quad =$ Ho and Dy are classical spin ices, $R \quad =$ Tb has been shown to be a spin liquid at low temperatures, and $R \quad =$ Yb is a candidate quantum spin ice. This system is attractive for the large anisotropic magnetic properties of rare earth ions, Ti$^{\mathrm{4+}}$'s lack of magnetic moment which isolates the magnetic ordering of $R^{\mathrm{3+}}$, and the comparative ease of making single crystals via the floating zone technique. This talk will present the structure and physical properties of a Yb$_{\mathrm{2+}}_{x}$Ti$_{\mathrm{2-}}_{x}$O$_{\mathrm{7-}}_{x}_{\mathrm{/2}}$ series including both the pure and stuffed samples. The series shows a dramatic change in the low-temperature (50-200 mK) specific heat signature upon doping away from the pure compound. Understanding the magnetic and physical properties of the off-stoichiometric series sheds light both on the magnetic ordering of the ideal spin ice candidate compound as well as aids in evaluating the quality and stoichiometry of a measured sample. In this vein, proper single-crystal growth conditions in order to ensure single crystals of appropriate stoichiometry will also be discussed.
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Authors
K. A. Arpino
Johns Hopkins Univ, Institute for Quantum Matter, Johns Hopkins University
Benjamin Trump
Institute for Quantum Matter and Jonhs Hopkins University, Johns Hopkins University, Johns Hopkins Univ
Tyrel M. McQueen
Johns Hopkins Univ, Institute for Quantum Matter and Jonhs Hopkins University, Institute for Quantum Matter and Johns Hopkins University, Johns Hopkins University, Institute for Quantum Matter, Johns Hopkins University
Collin Broholm
Institute for Quantum Matter, Jonhs Hopkins University, and Quantum Condensed Matter Division, Oak Ridge National Laboratories, Johns Hopkins University, Institute for Quantum Matter and Johns Hopkins University, Johns Hopkins University, Institute for Quantum Matter, Johns Hopkins Univ
S. M. Koopayeh
Institute for Quantum Matter and Johns Hopkins University, Johns Hopkins University, Johns Hopkins Univ, Institute for Quantum Matter, Johns Hopkins University