Muon spin rotation and neutron scattering investigations of the B-site ordered double perovskite Sr2DyRuO6

TL;DR

This study investigates the magnetic ground state of Sr2DyRuO6 using muSR, neutron scattering, and other techniques, revealing long-range antiferromagnetic order below 39.5 K and insights into the magnetic structure and crystal field effects.

Contribution

It provides the first detailed magnetic structure and ordering behavior of Sr2DyRuO6, highlighting the role of Ru 4d electrons in magnetic ordering and identifying crystal field excitations.

Findings

Long-range antiferromagnetic order below 39.5 K

Magnetic moments aligned along the b-axis: Dy 4.92 muB, Ru 1.94 muB

Crystal field splitting of 73.8 meV in the paramagnetic state

Abstract

The magnetic ground state of double perovskite Sr2DyRuO6 has been investigated using muon spin rotation and relaxation (muSR), neutron powder diffraction (NPD) and inelastic neutron scattering (INS), in addition to heat capacity and magnetic susceptibility (ac and dc) measurements. A clear signature of a long-range ordered magnetic ground state has been observed in the heat capacity data, which exhibit two sharp anomalies at 39.5 and 36 K found as well in the magnetic data. Further confirmation of long-range magnetic ordering comes from a sharp drop in the muon initial asymmetry and a peak in the relaxation rate at 40 K, along with a weak anomaly near 36 K. Based on temperature dependent NPD, the low temperature magnetic structure contains two interpenetrating lattices of Dy and Ru5, forming an antiferromagnetic ground state below 39.5 K with magnetic propagation vector k = (0,0,0). The magnetic moments of Dy and Ru at 3.5 K are pointing along the crystallographic b-axis with values of muDy = 4.92(10) muB and muRu = 1.94(7) muB, respectively. The temperature dependence of the Ru moments follows a mean field type behaviour, while that of the Dy moments exhibits a deviation indicating that the primary magnetic ordering is induced by the order of the 4d electrons of Ru rather than that of its proper 4f Dy electrons. The origin of the second anomaly observed in the heat capacity data at 36.5 K must be connected to a very small spin reorientation as the NPD studies do not reveal any clear change in the observed magnetic Bragg peaks positions or intensities between these two transitions. INS measurements reveal the presence of crystal field excitations (CEF) in the paramagnetic state with overall CEF splitting of 73.8 meV, in agreement with the point change model calculations.