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91探花
CMP
Credit: Jack Hobhouse

Paul Goddard

Visiting Lecturer

Sub department

  • Condensed Matter Physics
Paul.Goddard@physics.ox.ac.uk
Telephone: 01865 (2)72318
Clarendon Laboratory, room 252.1
  • About
  • Publications

Test for interlayer coherence in a quasi-two-dimensional superconductor.

Phys Rev Lett 88:3 (2002) 037001

Authors:

John Singleton, PA Goddard, A Ardavan, N Harrison, SJ Blundell, JA Schlueter, AM Kini

Abstract:

Peaks in the magnetoresistivity of the layered superconductor kappa - (BEDT-TTF)2Cu(NCS)(2), measured in fields < or =45 T applied within the layers, show that the Fermi surface is extended in the interlayer direction and enable the interlayer transfer integral (t( perpendicular) approximately 0.04 meV) to be deduced. However, the quasiparticle scattering rate tau(-1) is such that Planck's over 2pi/tau approximately 6t( perpendicular), implying that kappa - (BEDT-TTF)2Cu(NCS)(2) meets the criterion used to identify interlayer incoherence. The applicability of this criterion to anisotropic materials is thus shown to be questionable.

Fermi surface studies of quasi-two-dimensional 畏-Mo4O11

SYNTHETIC METALS 120:1-3 (2001) 783-784

Authors:

PA Goddard, AK Kleh茅, J Singleton, M Sasaki, N Miyajima, M Inoue

X-ray diffraction study of Co-Cu superlattices

Journal of Physics Condensed Matter 12:30 (2000) 6755-6771

Authors:

AY Babkevich, RA Cowley, P Goddard, R Schlinkert, BM Murphy, SP Collins, BJ Hickey

Abstract:

Epitaxial Co/Cu superlattices were grown by molecular beam epitaxy on sapphire substrates and investigated by high-resolution x-ray diffraction at room temperature. Detailed analysis of x-ray scattering along the [10.L] reciprocal-lattice rows revealed that about 80% of Co was hexagonal close packed (h.c.p.) and only 20% was face-centred cubic (f.c.c.). A combination of modelling of x-ray scattering from superlattices with measurements of coherence lengths of individual components of the scattering suggests that the f.c.c. Co grows as a single block at the beginning of Co layers and the growth presumably starts from islands rather than from continuous Co layers. The h.c.p, structure is one-dimensionally disordered by stacking faults which appear after approximately every 12 layers of Co on average. Upon heating in ultrahigh vacuum to 700 掳C the coherent superlattice structure was completely destroyed and the resulting structure consisted of relaxed layers of Co and Cu.

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