TY - JOUR
T1 - Resistivity and magnetoresistivity measurements near the metal-insulator and superconductor-insulator transition in granular Al-Ge
AU - Eytan, G.
AU - Rosenbaum, R.
AU - McLachlan, D. S.
AU - Albers, A.
PY - 1993
Y1 - 1993
N2 - Granular Al-Ge films just on the metallic side of the critical volume fraction φc (50.7% Al) are found to have critical fields in excess of 1.5 T at 0.47 K due to the fine granular nature of the Al. In barely insulating films where (φc-φ)<2.2% (where φ is the volume percent of aluminum), superconducting fluctuations and Josephson-junction coupling dominate the behavior below Tc (Tc1.6 K). For the more insulating films where 3.4%≤(φc-φ)≤6.2%, the resistivity diverges strongly below Tc and a large negative magnetoresistivity is observed. This behavior is explained in terms of quasiparticle tunneling or alternatively by the Adkins charging model; the magnetoresistivity is explained in terms of a magnetic-field-dependent superconducting energy gap. The upper critical fields of all the samples are found to be almost independent of the bulk resistivities, supporting a picture of weakly coupled grains. The normal resistivity in the insulating films (φ<φc) obeys the hopping relation ρ=ρ0exp(T0/T)x above Tc and also below Tc in a field of 3.48 T, which quenches all superconductivity in the films.
AB - Granular Al-Ge films just on the metallic side of the critical volume fraction φc (50.7% Al) are found to have critical fields in excess of 1.5 T at 0.47 K due to the fine granular nature of the Al. In barely insulating films where (φc-φ)<2.2% (where φ is the volume percent of aluminum), superconducting fluctuations and Josephson-junction coupling dominate the behavior below Tc (Tc1.6 K). For the more insulating films where 3.4%≤(φc-φ)≤6.2%, the resistivity diverges strongly below Tc and a large negative magnetoresistivity is observed. This behavior is explained in terms of quasiparticle tunneling or alternatively by the Adkins charging model; the magnetoresistivity is explained in terms of a magnetic-field-dependent superconducting energy gap. The upper critical fields of all the samples are found to be almost independent of the bulk resistivities, supporting a picture of weakly coupled grains. The normal resistivity in the insulating films (φ<φc) obeys the hopping relation ρ=ρ0exp(T0/T)x above Tc and also below Tc in a field of 3.48 T, which quenches all superconductivity in the films.
UR - http://www.scopus.com/inward/record.url?scp=0010540131&partnerID=8YFLogxK
U2 - 10.1103/PhysRevB.48.6342
DO - 10.1103/PhysRevB.48.6342
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AN - SCOPUS:0010540131
VL - 48
SP - 6342
EP - 6352
JO - Physical Review B-Condensed Matter
JF - Physical Review B-Condensed Matter
SN - 1098-0121
IS - 9
ER -