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On intrinsic and extrinsic effects in the surface impedance of cuprate superconductors

Journal Article · · Journal of Superconductivity; (United States)
DOI:https://doi.org/10.1007/BF00618132· OSTI ID:7046388
 [1]
  1. Kernforschungszentrum, Karlsruhe (Germany)
Surface impedance measurements in the normal and superconducting state are an excellent method to study conduction electron dynamics and extended defects. Electron dynamics show up most clearly in the relaxation range, i.e., for distances traveled in one rf period s = v[sub F]/[omega] (v[sub F] Fermi velocity) being smaller or of the order of the penetration depth [lambda] and mean free path l. For materials with v[sub F][le]10[sup 7] cm/sec the relaxation range is easily accessible for f[ge]0.1 THz. Then, in the normal state, relaxation defines the surface impedance with an intrinsic penetration depth [lambda][sub I] approaching the London penetration depth [lambda][sub L] and R[sub I][approx][mu][sub 0][lambda][sub L]/2[tau] as surface resistance, allowing measurement of [lambda][sub L] and relaxation time [tau](T, [omega]). In the superconducting state the photon interaction scales with [xi][sub F]/[lambda][sub L] = 1/[gamma] ([xi][sub F] dimension of Cooper pairs for l[yields][infinity]) and causes at low frequencies an absorption rate growing with [gamma], which is decreasing with [xi][sub F]/l. The rate increase proportional to [gamma] turns to a decrease above 0.1 THz, which is accompanied by a decrease of [lambda] with frequency which is stronger for large [gamma] and small [xi][sub F]/l. These characteristic dependences allow measurement of material parameters, anisotropy, and dynamics of electrons, especially the relaxation rate [tau]. 19 refs., 6 figs., 1 tab.
OSTI ID:
7046388
Journal Information:
Journal of Superconductivity; (United States), Journal Name: Journal of Superconductivity; (United States) Vol. 5:4; ISSN JOUSEH; ISSN 0896-1107
Country of Publication:
United States
Language:
English