Low-temperature transport in highly boron-doped nanocrystalline diamond
Author(s) -
P. Achatz,
Wojciech Gajewski,
E. Bustarret,
C. Marcenat,
R. Piquerel,
C. Chapelier,
Thomas Dubouchet,
Oliver A. Williams,
Ken Haenen,
José A. Garrido,
M. Stutzmann
Publication year - 2009
Publication title -
physical review b
Language(s) - English
Resource type - Journals
eISSN - 1538-4489
pISSN - 1098-0121
DOI - 10.1103/physrevb.79.201203
Subject(s) - condensed matter physics , materials science , magnetoresistance , metal–insulator transition , doping , weak localization , conductance , electrical resistivity and conductivity , thermal conduction , diamond , superconductivity , conductivity , boron , metal , magnetic field , physics , metallurgy , quantum mechanics , composite material , nuclear physics
We studied the transport properties of highly boron-doped nanocrystalline diamond thin films at temperatures down to 50 mK. The system undergoes a doping-induced metal-insulator transition with an interplay between intergranular conductance g and intragranular conductance g0, as expected for a granular system. The conduction mechanism in the case of the low-conductivity films close to the metal-insulator transition has a temperature dependence similar to Efros-Shklovskii type of hopping. On the metallic side of the transition, in the normal state, a logarithmic temperature dependence of the conductivity is observed, as expected for a metallic granular system. Metallic samples far away from the transition show similarities to heavily boron-doped single-crystal diamond. Close to the transition, the behavior is richer. Global phase coherence leads in both cases to superconductivity (also checked by ac susceptibility), but a peak in the low-temperature magnetoresistance measurements occurs for samples close to the transition. Corrections to the conductance according to superconducting fluctuations account for this negative magnetoresistance.
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