TY - JOUR
T1 - Chain-based order and quantum spin liquids in dipolar spin ice
AU - McClarty, P. A.
AU - Sikora, O.
AU - Moessner, R.
AU - Penc, K.
AU - Pollmann, F.
AU - Shannon, N.
N1 - Publisher Copyright:
© 2015 American Physical Society.
PY - 2015/9/11
Y1 - 2015/9/11
N2 - Recent experiments on the spin-ice material Dy2Ti2O7 suggest that the Pauling "ice entropy," characteristic of its classical Coulombic spin-liquid state, may be lost at low temperatures [Pomaranski, Nat. Phys. 9, 353 (2013)1745-247310.1038/nphys2591]. However, despite nearly two decades of intensive study, the nature of the equilibrium ground state of spin ice remains uncertain. Here we explore how long-range dipolar interactions D, short-range exchange interactions, and quantum fluctuations combine to determine the ground state of dipolar spin ice. We identify the organizational principle that ordered ground states are selected from a set of "chain states" in which dipolar interactions are exponentially screened. Using both quantum and classical Monte Carlo simulation, we establish phase diagrams as a function of quantum tunneling g and temperature T, and find that only a very small gcaD is needed to stabilize a quantum spin liquid ground state. We discuss the implications of these results for Dy2Ti2O7.
AB - Recent experiments on the spin-ice material Dy2Ti2O7 suggest that the Pauling "ice entropy," characteristic of its classical Coulombic spin-liquid state, may be lost at low temperatures [Pomaranski, Nat. Phys. 9, 353 (2013)1745-247310.1038/nphys2591]. However, despite nearly two decades of intensive study, the nature of the equilibrium ground state of spin ice remains uncertain. Here we explore how long-range dipolar interactions D, short-range exchange interactions, and quantum fluctuations combine to determine the ground state of dipolar spin ice. We identify the organizational principle that ordered ground states are selected from a set of "chain states" in which dipolar interactions are exponentially screened. Using both quantum and classical Monte Carlo simulation, we establish phase diagrams as a function of quantum tunneling g and temperature T, and find that only a very small gcaD is needed to stabilize a quantum spin liquid ground state. We discuss the implications of these results for Dy2Ti2O7.
UR - https://www.scopus.com/pages/publications/84942540603
U2 - 10.1103/PhysRevB.92.094418
DO - 10.1103/PhysRevB.92.094418
M3 - Article
AN - SCOPUS:84942540603
SN - 1098-0121
VL - 92
JO - Physical Review B - Condensed Matter and Materials Physics
JF - Physical Review B - Condensed Matter and Materials Physics
IS - 9
M1 - 094418
ER -