D.R. Noakes

Coexistence of ferromagnetism and superconductivity in the hybrid ruthenate-cuprate compound RuSr 2 GdCu 2 O 8 studied by muon spin rotation and dc magnetization

We have investigated the magnetic and the superconducting properties of the hybrid ruthenate-cuprate compound

Spin dynamics and freezing in magnetic rare-earth quasicrystals

{\mathrm{RuSr}}_{2}{\mathrm{GdCu}}_{2}{\mathrm{O}}_{8}

Expansion of the vortex cores in YBa 2 Cu 3 O 6.95 at low magnetic fields

by means of zero-field muon-spin rotation (ZF-\ensuremath{\mu}SR) and dc magnetization measurements. The dc-magnetization data established that this material exhibits ferromagnetic order of the Ru moments [\ensuremath{\mu}(Ru)\ensuremath{\approx}1

Magnetic properties of the Kondo metals CePtSn and CePdSn from μSR

{\ensuremath{\mu}}_{B}]

Superconductivity and magnetism in Sr2Y(Ru1-uCuu)O6 and in Ba2Gd(Ru1-uCuu)O6

below

Dynamics of the internal field in RB12 (R = Er, Yb, Lu)

{T}_{C}=133

Spin-slip structure induced by the crystalline electric field in the incommensurate magnetic ordering of CePtSn

K and becomes superconducting at a much lower temperature

Properties of incommensurate spin density waves in iron aluminides (invited)

{T}_{c}=16

μSR magnetic response of CeCuSn

K. The ZF-\ensuremath{\mu}SR experiments indicate that the ferromagnetic phase is homogeneous on a microscopic scale and accounts for most of the sample volume. They also suggest that the magnetic order is not significantly modified at the onset of superconductivity.

studies on the development of magnetism in the Kondo semimetal CeNiSn caused by doping with La, Cu and Pt

Abstract Muon spin relaxation measurements of RE 8 Mg 42 Zn 50 (RE = Gd, Tb) quasicrystals have revealed slower spin dynamics and more prompt spin freezing for Tb than Gd, due to “crystalline electric field” splitting in low rare-earth site symmetry. Inhomogeneous spin freezing leads to a low-temperature state with local field distribution characteristic of a concentrated disordered magnet.