Abstract

We propose here a theory of pure type-II superconductors in high magnetic fields. Making use of the guess that the effect of the magnetic field on a pure type-II superconductor in a high field is similar to that of a transport current, we circumvent the difficulty associated with the expansion in powers of the order parameter $\ensuremath{\Delta}$. As an application of this conjecture, we calculate here the ultrasonic attenuation coefficients in the gapless region of a pure type-II superconductor. The attenuation coefficients decrease sharply in the superconducting region as ${({H}_{c2}\ensuremath{-}H)}^{\frac{1}{2}}$, where $H$ is the external field, and are strongly anisotropic---a simple manifestation of the anisotropy in the excitation spectrum of quasiparticles.

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