A new phenomenological model describing nonequilibrium superconductivity is proposed which is characterized by the introduction of a quasithermal distribution of phonons with energies of 0--{∞}. The model exhibits μ*-model-like and T*-model-like {Δ} vs n and μ* vs n characteristics when the excess quasiparticle density n is low and high, respectively. The estimated critical density nc for the onset of instability is much lower than that of the μ* model. These results are in fairly good agreement with the experimental results reported by Willemsen and Gray, and Akoh and Kajimura.
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Kobayashi et al. (1985) studied this question.
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