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Energy Gap Induced by Impurity Scattering: New Phase Transition in Anisotropic Superconductors
Condensed Matter · Submitted 10 Mar 1995
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim It is shown that layered superconductors are subjected to a phase transition at zero temperature provided the order parameter (OP) reverses its sign on the Fermi-surface but its angular average is finite.
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The abstract, sentence by sentence
It is shown that layered superconductors are subjected to a phase transition at zero temperature provided the order parameter (OP) reverses its sign on the Fermi-surface but its angular average is finite. The transition is regulated by an elastic impurity scattering rate $1/\tau$. The excitation energy spectrum, being gapless at the low level of scattering, develops a gap as soon as the scattering rate exceeds some critical value of $1/\tau_\star$.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | It is shown that layered superconductors are subjected to a phase transition at zero temperature provided the order parameter (OP) reverses its sign on the Fermi-surface but its angular average is finite. | result 0.98 | 0.81 | 0.79 | asserted 1.00 |
| s1 | The transition is regulated by an elastic impurity scattering rate $1/\tau$. | result 0.96 | 0.69 | 0.09 | asserted 1.00 |
| s2 | The excitation energy spectrum, being gapless at the low level of scattering, develops a gap as soon as the scattering rate exceeds some critical value of $1/\tau_\star$. | result 1.00 | 0.78 | 0.34 | asserted 1.00 |
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The paper
Original abstract
It is shown that layered superconductors are subjected to a phase transition at zero temperature provided the order parameter (OP) reverses its sign on the Fermi-surface but its angular average is finite. The transition is regulated by an elastic impurity scattering rate $1/\tau$. The excitation energy spectrum, being gapless at the low level of scattering, develops a gap as soon as the scattering rate exceeds some critical value of $1/\tau_\star$.
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