A study of the resistively detected nuclear magnetic resonance (RDNMR) lineshape in the vicinity of nu = 1 was performed on a high-mobility 2D electron gas formed in GaAs/AlGaAs.
There exists in the literature a number of transport measurements performed on metallic superlattices.
Resistivities rho(T) of ceramic samples of La sub 1.825 Sr sub 0.175 CuO sub 4 (LSCO) and both ceramic and single-crystalline (a-b plane, containing micro- twins) samples of YBa sub 2 Cu sub 3 O su
Resistivities p(T) of ceramic samples of La sub (1.825) Sr sub (0.175) CuO sub 4 (LSCO) and both ceramic and single-crystalline (a-b plane, containing micro-twins) samples of YBa sub 2 Cu sub 3 O s
We have measured the resistivity anisotropy in single crystals of nominal comosition Ba sub (2.2) Sr sub (1.8) CuO sub 6, the single-copper-layer analog of the 85K superconductor Ba sub 2 Sr sub 2
A diffused layer in silicon is generally characterized by four parameters: the concentration, C,, , of diffused donors or acceptors at the surface, the concentration, C u , of acceptors or donors o
We report resistivity measurements from 0.03 to 10 K in a dilute high mobility 2D electron system.
Resistivity was measured from T sub c to 1100K for La sub (1.825) Sr sub (0.175) CuO sub 4, where it is linear to 1100K, and for YBa sub 2 Cu sub 3 O sub 7, where it is linear to 600K, increases fa
In metallic magnets with a low carrier density, scattering from magnetic fluctuations above and near the transition temperature T sub c provides a large contribution to the electrical resistance.
A strongly anisotropic resistivity tensor was measured from the superconducting T sub c = 81K to 600K in crystals of the new high-T sub c superconductor having nominal composition Bi sub 2 Sr sub (
