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CMP
Credit: Jack Hobhouse

Robin Nicholas

Emeriti

Sub department

  • Condensed Matter Physics
Robin.Nicholas@physics.ox.ac.uk
Telephone: 01865 (2)72250
Clarendon Laboratory, room 148
  • About
  • Publications

Observation of the zero Hall resistance state in a semimetallic superlattice

SURF SCI 362:1-3 (1996) 481-484

Authors:

MS Daly, KSH Dalton, M Lakrimi, NJ Mason, DK Maude, RJ Nicholas, JC Portal, DM Symons, M vanderBurgt, PJ Walker

Abstract:

The quantum Hall effect has been measured in an intrinsic semimetallic superlattice with almost equal electron and hole densities. Giant oscillations are seen in the Hall resistivity, and at high fields and pressures a zero-resistance state is observed where the Hall resistivity goes to zero due to compensation of the Hall fields of the two carrier types. This behaviour is interpreted in terms of the limiting properties of rho(xx) and rho(xy)
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Photoconductivity studies of InAsP/InP heterostructures in applied magnetic and electric fields

SEMICONDUCTOR SCIENCE AND TECHNOLOGY 11:1 (1996) 34-38

Authors:

D Kinder, RJ Nicholas, PN Stavrinou, SK Haywood, L Hart, M Hopkinson, JPR David, G Hill
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Pulsed-magnetic-field measurements of the composite-fermion effective mass

PHYSICAL REVIEW B 53:4 (1996) 2057-2063

Authors:

DR Leadley, M vanderBurgt, RJ Nicholas, CT Foxon, JJ Harris
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Selective area epitaxy of InGaAs/InGaAsP quantum wells studied by magnetotransport

SEMICONDUCTOR SCIENCE AND TECHNOLOGY 11:5 (1996) 735-740

Authors:

RW Martin, SL Wong, DM Symons, RJ Nicholas, MA Gibbon, EJ Thrush, JP Stagg
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The unifying role of effective field in the composite fermion model of the fractional quantum Hall effect

SURF SCI 362:1-3 (1996) 22-25

Authors:

DR Leadley, M vanderBurgt, RJ Nicholas, PJ Gee, J Singleton, JJ Harris, CT Foxon

Abstract:

Fractional Quantum Hall Effect measurements in 50 T pulsed magnetic fields, are analysed in the Composite Fermion (CF) model. Energy gaps of all fractions in the principal series around nu=1/2 show a simple, sample independent, increase with the CF effective field following root B*. The spin polarised state at nu=5/3 follows exactly the same behaviour, but for mixed spin states like 4/3 the energy gap collapses when B*>1 T.
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