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Beecroft building, Department of Physics, University of Oxford
Credit: Jack Hobhouse

Prof. J. C. Seamus Davis

Professor of Physics

Research theme

  • Fields, strings, and quantum dynamics
  • Quantum materials

Sub department

  • Condensed Matter Physics

Research groups

  • Macroscopic Quantum Matter
seamus.davis@physics.ox.ac.uk
Telephone: +353830392937
Clarendon Laboratory, room 512.40.28
davis-group-quantum-matter-research.ie
  • About
  • Publications

Microscopic electronic inhomogeneity in the high-Tc superconductor Bi2Sr2CaCu2O8+x.

Nature 413:6853 (2001) 282-285

Authors:

SH Pan, JP O'Neal, RL Badzey, C Chamon, H Ding, JR Engelbrecht, Z Wang, H Eisaki, S Uchida, AK Gupta, KW Ng, EW Hudson, KM Lang, JC Davis

Abstract:

The parent compounds of the copper oxide high-transition-temperature (high-Tc) superconductors are unusual insulators (so-called Mott insulators). Superconductivity arises when they are 'doped' away from stoichiometry. For the compound Bi2Sr2CaCu2O8+x, doping is achieved by adding extra oxygen atoms, which introduce positive charge carriers ('holes') into the CuO2 planes where the superconductivity is believed to originate. Aside from providing the charge carriers, the role of the oxygen dopants is not well understood, nor is it clear how the charge carriers are distributed on the planes. Many models of high-Tc superconductivity accordingly assume that the introduced carriers are distributed uniformly, leading to an electronically homogeneous system as in ordinary metals. Here we report the presence of an electronic inhomogeneity in Bi2Sr2CaCu2O8+x, on the basis of observations using scanning tunnelling microscopy and spectroscopy. The inhomogeneity is manifested as spatial variations in both the local density of states spectrum and the superconducting energy gap. These variations are correlated spatially and vary on the surprisingly short length scale of approximately 14 A. Our analysis suggests that this inhomogeneity is a consequence of proximity to a Mott insulator resulting in poor screening of the charge potentials associated with the oxygen ions left in the BiO plane after doping, and is indicative of the local nature of the superconducting state.
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Observation of the superfluid Shapiro effect in a 3He weak link

Physical Review Letters 87:3 (2001) 353011-353014

Authors:

RW Simmonds, A Marchenkov, JC Davis, RE Packard

Abstract:

Superfluid Josephson weak links were established by studying the mass currents through the links in the presence of an externally applied ac pressure modulation. A superfluid analog of the superconducting Shapiro effect in Josephson weak links was obtained. Chararacteristic changes in dc mass currents were observed when the superfluid Josephson frequency happened to be an integral multiple of the ac modulation frequency ω. The dependence of current changes on ac pressure amplitude were in agreement with the theory describing quantum phase dynamics of superfluid weak links.

Observation of the superfluid shapiro effect in a 3He weak link.

Physical review letters 87:3 (2001) 035301

Authors:

RW Simmonds, A Marchenkov, JC Davis, RE Packard

Abstract:

We have studied the mass currents through a superfluid 3He Josephson weak link in the presence of an externally applied ac pressure modulation. Characteristic changes in the dc mass currents are observed whenever the superfluid Josephson frequency omega(J) is an integer multiple of the ac modulation frequency omega. The measured dependencies of these current changes on ac pressure amplitude are in excellent agreement with theory describing quantum phase dynamics of superfluid 3He weak links. These results establish the superfluid analog of the superconducting Shapiro effect.
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Quantum interference of superfluid 3He.

Nature 412:6842 (2001) 55-58

Authors:

RW Simmonds, A Marchenkov, E Hoskinson, JC Davis, RE Packard

Abstract:

Celebrated interference experiments have demonstrated the wave nature of light and electrons, quantum interference being the manifestation of wave-particle duality. More recently, double-path interference experiments have also demonstrated the quantum-wave nature of beams of neutrons, atoms and Bose-Einstein condensates. In condensed matter systems, double-path quantum interference is observed in the d.c. superconducting quantum interference device (d.c. SQUID). Here we report a double-path quantum interference experiment involving a liquid: superfluid 3He. Using a geometry analogous to the superconducting d.c. SQUID, we control a quantum phase shift by using the rotation of the Earth, and find the classic interference pattern with periodicity determined by the 3He quantum of circulation.
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Interplay of magnetism and high-Tc superconductivity at individual Ni impurity atoms in Bi2Sr2CaCu2O8+delta.

Nature 411:6840 (2001) 920-924

Authors:

EW Hudson, KM Lang, V Madhavan, SH Pan, H Eisaki, S Uchida, JC Davis

Abstract:

Magnetic interactions and magnetic impurities are destructive to superconductivity in conventional superconductors. By contrast, in some unconventional macroscopic quantum systems (such as superfluid 3He and superconducting UGe2), the superconductivity (or superfluidity) is actually mediated by magnetic interactions. A magnetic mechanism has also been proposed for high-temperature superconductivity. Within this context, the fact that magnetic Ni impurity atoms have a weaker effect on superconductivity than non-magnetic Zn atoms in the high-Tc superconductors has been put forward as evidence supporting a magnetic mechanism. Here we use scanning tunnelling microscopy to determine directly the influence of individual Ni atoms on the local electronic structure of Bi2Sr2CaCu2O8+delta. At each Ni site we observe two d-wave impurity states of apparently opposite spin polarization, whose existence indicates that Ni retains a magnetic moment in the superconducting state. However, analysis of the impurity-state energies shows that quasiparticle scattering at Ni is predominantly non-magnetic. Furthermore, we show that the superconducting energy gap and correlations are unimpaired at Ni. This is in strong contrast to the effects of non-magnetic Zn impurities, which locally destroy superconductivity. These results are consistent with predictions for impurity atom phenomena derived from a magnetic mechanism.
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