Abstract
The theory of electron tunneling is extended to treat the generation and detection of an imbalance Q between electronlike and holelike quasiparticle populations in superconductors. The equilibration of injected high-energy quasiparticles owing to inelastic phonon processes is discussed, and it is shown that in tin, Q relaxes in τQ[Δ(0)Δ(T)](2×1010) sec. It is also shown that even a small (∼1%) anisotropy of the gap can lead to significant Q relaxation by elastic scattering processes. This discussion extends our previous brief interpretation of the pairquasiparticle potential difference measured by Clarke.

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