Abstract

Josephson plasma resonance (JPR) experiments under magnetic fields parallel to CUO2 layers have been performed in Bi2Sr2CaCu2O8+δ single crystals with doping range being from optimal to under-doped side. The results are found to be quite unique and cannot be accounted for the conventional notion of JPR for H // c, the systematic measurements as functions of the doping, applied microwave frequency, and magnetic field suggest that the new JPR mode can be excited with strong coupling to the Josephson vortex lattice.

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