J. W. Schneider
University of Zurich
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Featured researches published by J. W. Schneider.
Physica C-superconductivity and Its Applications | 1989
B. Pümpin; H. Keller; W. Kündig; W. Odermatt; I.M. Savić; J. W. Schneider; H. Simmler; P. Zimmermann; J. G. Bednorz; Y. Maeno; K. A. Müller; C. Rossel; E. Kaldis; S. Rusiecki; W. Assmus; J. Kowalewski
Abstract To get accurate values of the London penetration depths in YBa2Cu3O x , μSR measurements were performed on a high quality, sintered sample and a c-axis-oriented polycrystal. For the sintered sample the temperature dependence of the effective penetration depth λeff is well described by the two-fluid model, with λeff(0) = 155(10) nm. This behavior of λeff(T) is consistent with conventional s-wave pairing. The anisotropy ratio λ c λ ab ⋍ 5(1) was determined from measurements on the polycrystal. These results were used to calculate λab(0) = 130(10) nm and λ c (0) ⋍ 500 – 800 nm .
European Physical Journal B | 1988
B. Pümpin; H. Keller; W. Kündig; W. Odermatt; B. D. Patterson; J. W. Schneider; H. Simmler; S. Connell; K. A. Müller; J. G. Bednorz; K. W. Blazey; Ingo Morgenstern; C. Rossel; I. M. Savic
Muon spin rotation (μSR) measurements of the internal magnetic fields in sintered YBa2Cu3O7−δ samples are reported. Pronounced differences between field-cooled (FC) and zero-field-cooled (ZFC) μSR signals, hysteresis effects and flux trapping are observed. The μSR results are compared with the results of macroscopic experiments (susceptibility, magnetization, resistivity) and with predictions obtained from models of weakly-coupled superconducting regions.
Journal of The Less Common Metals | 1990
B. Pümpin; H. Keller; W. Kündig; I. M. Savić; J. W. Schneider; H. Simmler; P. Zimmermann; E. Kaldis; S. Rusiecki; C. Rossel; E.M. Forgan
Abstract A systematic study of the local magnetic field distribution p(B) in the perovskite-type superconductor YBa2Cu3Ox is presented. Special attention is given to the second moment 〈 ΔB2 〉 of p(B) which is closely related to the superconducting carrier density ns and the effective mass m ∗ of the superconducting carriers. The influence of temperature, anisotropy and hole doping are investigated in detail. It is found that the temperature dependence of the magnetic penetration depth in YBa2Cu3Ox is in agreement with conventional s-wave pairing and suggests strong coupling. The anisotropic behavior of p(B) is well described by a theory for uniaxial type II superconductors, with an anisotropy ratio γ ∼- 5(1). Moreover, the zero-temperature values λab(0) = 130(10) nm and λc(0) ∼- 500–800 nm (penetration depth for screening currents flowing in the ab-planes and along the c-axis, respectively) were extracted from our data. μSR experiments performed on oxygen deficient samples indicate that the structural and electronic properties of YBa2Cu3Ox are strongly correlated via the oxygen content x.
Hyperfine Interactions | 1986
Hp. Baumeler; Robert F. Kiefl; H. Keller; W. Kündig; W. Odermatt; B. D. Patterson; J. W. Schneider; T. L. Estle; S. P. Rudaz; D. P. Spencer; K. W. Blazey; I. M. Savic
Muonium centers (Mu) in single crystals and powdered alkali halides have been studied using the high-timing-resolution transverse field μSR technique. Mu has been observed and its hyperfine parameter (HF) determined inevery alkali halide. For the rocksalt alkali halides, the HF parameter Aμ shows a systematic dependence on the host lattice constant. A comparison of the Mu HF parameter with hydrogen ESR data suggests that the Mu center is the muonic analogue of the interstitial hydrogenHi0-center. The rate of Mu diffusion can be deduced from the motional narrowing of the nuclear hyperfine interaction. KBr shows two different Mu states, a low-temperatureMuI-state and a high-temperatureMuII-state.
Hyperfine Interactions | 1991
B. Pümpin; H. Keller; W. Kündig; I. M. Savić; J. W. Schneider; H. Simmler; P. Zimmermann; E. Kaldis; S. Rusiecki; C. Rossel
A systematic μSR study of the local magnetic field distribution in a series of oxygen deficient YBa2Cu3Ox samples with 6.5⩽x⩽7.0 is reported. Special attention was given to perform the experiments under the same conditions, so that the oxygen content of the measured samples was the only parameter varied. The behavior of the depolarization rate σ as a function of the oxygen contentx was found to have strong similarities with the behavior of the critical temperatureTc as a function ofx. In particular, two step-like increases of σ were observed abovex=6.7 and 6.9. The temperature dependence of the normalized depolarization rate σ(T)/σ(0) is well described by the two-fluid model forx⩾6.781(1) and clearly deviates from this behavior forx⩽6.704(1). Our results are compared to those obtained by other groups.
Physics Letters A | 1987
J. W. Schneider; Hp. Baumeler; H. Keller; W. Odermatt; B. D. Patterson; K. A. Müller; J. G. Bednorz; K. W. Blazey; Ingo Morgenstern; I. M. Savic
Abstract Measurements of the internal magnetic field in the high- T c superconductors La 1.8 Sr 0.2 CuO 4 and YBa 2 Cu 3 O 7−δ have been performed after zero-field cooling using the muon spin rotation (μSR) technique. Temperature-dependent changes are observed below T c in both the magnitude of the internal field and the fraction of muons which experience this field.
Hyperfine Interactions | 1986
J. W. Schneider; Hp. Baumeler; H. Keller; R. F. Kiefl; W. Kündig; W. Odermatt; B. D. Patterson; T. L. Estle; S. P. Rudaz; K. W. Blazey; C. Schwab
The authors present a list of results of μSR experiments in materials with the diamond and zincblende structure. Besides the muonium hyperfine parameters, additional information is tabulated: the formation probability for the different muon states, the highest temperatures at which muonium states have been observed and the types of transitions found to occur between these states. The muonium hyperfine parameters show a linear rise as a function of host ionicity from Ge to GaAs to ZnSe followed by a sharp drop to CuBr.
Hyperfine Interactions | 1986
B. D. Patterson; Hp. Baumeler; H. Keller; R. F. Kiefl; W. Kündig; W. Odermatt; J. W. Schneider; W. J. Choyke; T. L. Estle; D. P. Spencer; K. W. Blazey; I. M. Savic
Implanted muons in samples of silicon carbide have been observed to form paramagnetic muonium centers (μ+ e−). Muonium precession signals in low applied magnetic fields have been observed at 22 K in a granular sample of cubic β-SiC, however it was not possible to determine the hyperfine frequency. In a single crystal sample of hexagonal 6H-SiC, three apparently isotropic muonium states were observed at 20 K and two at 300 K, all with hyperfine frequencies intermediate between those of the isotropic muonium centers in diamond and silicon. No evidence was seen of an anisotropic muonium state analogous to the Mu* state in diamond and silicon.
Hyperfine Interactions | 1991
H. Simmler; P. Eschle; H. Keller; W. Kündig; W. Odermatt; B. D. Patterson; B. Pümpin; I. M. Savić; J. W. Schneider; U. Straumann; P. Truöl
Planar channeling data ofμ+-decay positrons in various semiconductors are reported. Together with the extensive spectroscopic data supplied by transverse μSR, the location of the different states of the hydrogen pseudo-isotopeμ+ e− (muonium) can be identified by means of planar simulations. In high purity silicon as well as in gallium arsenide a thermally activated site transition is observed which can be assigned to a transition between different muonium states.
Physica C-superconductivity and Its Applications | 1988
H. Keller; B. Pümpin; W. Kündig; W. Odermatt; B. D. Patterson; J. W. Schneider; H. Simmler; S. Connell; K. A. Müller; J. G. Bednorz; K. W. Blazey; Ingo Morgenstern; C. Rossel; I. M. Savic
Muon spin rotation (μSR) measurements of the internal magnetic fields in YBa2Cu3O7−δ are reported. Pronounced differences between field-cooled (FC) and zero-field-cooled (ZFC) μSR signals, hysteresis effects and flux trapping are observed. The μSR depolarization rate provides information regarding the local magnetic field distribution in the superconducting state. The present results show similarities to calculations that model a glasslike superconducting state.