[show abstract][hide abstract] ABSTRACT: We report muon spin rotation (muSR) measurements on the moving vortex lattice (VL) in the type-II superconductor Pb-In, backed up by small-angle neutron scattering (SANS) observations on the same sample. We observe a motional narrowing of the muSR lineshape p(B) and by SANS, alignment of the VL to the direction of vortex motion. We have calculated the muSR lineshape expected with a range of orientations of the moving VL. We demonstrate how the new muSR results give information on the moving VL which is complementary and consistent with the SANS data.
[show abstract][hide abstract] ABSTRACT: A new type of muonium defect center has been observed in undoped CdS below 20 K. The hyperfine interaction amounts only to approximately 10-4 of the vacuum value, and is shown to have axial symmetry along the Cd-S bond direction. Results suggest that the muon is close to the sulfur antibonding site and the paramagnetic electron density is distributed over a large volume. In contrast to the behavior in other semiconductors, muonium forms a shallow center in CdS. By implication, analog isolated hydrogen impurity atoms act as electrically active shallow-level defect centers in CdS.
[show abstract][hide abstract] ABSTRACT: We have measured the zero-field muon spin relaxation (ZF mu +SR) spectra of the quasi-one-dimensional fulleride conductor CsC60. Static magnetic order of a random nature develops gradually below about 30 K. The local field distribution at the muon site has a Gaussian shape with a width of 48.3(7) G at 2.8 K. Muon spin rotation (TF mu +SR) measurements at an applied transverse field of 6 kG also show the onset of magnetic order in the same temperature range.
Journal of Physics Condensed Matter 01/1995; · 2.36 Impact Factor
[show abstract][hide abstract] ABSTRACT: An unusual longitudinal-magnetic-field dependence of the muon polarization for anomalous muonium (Mu[sup *]) in polycrystalline semiconductor targets is predicted, and has been observed for Si. As a function of field, the experimentally measured muon polarization at 53 K exhibits a cusp, i.e., a discontinuous jump in the slope from negative to positive, at 340(5) mT, in good agreement with theory. This occurs because the effective field on the [mu][sup +] vanishes at this external field as the angle between it and the Mu[sup *] symmetry axis approaches 90[degree]. At 200 K no cusp is seen because Mu[sup *] has been thermally annihilated. Fractional populations of the different muonium species are derived from the 53-K data. All Mu[sup *] and other anisotropic centers, including molecular radicals, should exhibit such a cusp, allowing the possibility of observing such species even in disordered or amorphous solids where spectroscopic detection might be impossible. Integral counting (and therefore very high data rates) can be used for these observations.