Order parameter symmetry and mode coupling effects at dirty superconducting quantum phase transitions
arXiv:cond-mat/0211519 · doi:10.1103/PhysRevB.70.104514
Abstract
We derive an order-parameter field theory for a quantum phase transition between a disordered metal and an exotic (non-s-wave) superconductor. Mode coupling effects between the order parameter and other fermionic soft modes lead to an effective long-range interaction between the anomalous density fluctuations which is reflected in singularities in the free energy functional. However, this long-range interaction is not strong enough to suppress disorder fluctuations. The asymptotic critical region is characterized by run-away flow to large disorder. For weak coupling, this asymptotic region is very narrow. It is preempted by a wide crossover regime with mean-field critical behavior and, in the p-wave case, logarithmic corrections to scaling in all dimensions.
final version as published
References in corpus (6)
- Strong Enhancement of Superconducting T_c in Ferromagnetic Phases
- First order superconducting transition near a ferromagnetic quantum critical point
- Fluctuation-Driven Quantum Phase Transitions in Clean Itinerant Ferromagnets
- Nature of the Quantum Phase Transition in Clean, Itinerant Heisenberg Ferromagnets
- Local versus Nonlocal Order Parameter Field Theories for Quantum Phase Transitions
- Fluctuation Conductivity in Unconventional Superconductors near Critical Disorder
Cited by in corpus (5)
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- Infinite-randomness quantum critical points induced by dissipation
- Resilience of Majorana Fermions in the face of Disorder
- Effect of weak disorder on the phase competition in iron pnictides
- Superconducting transition in disordered granular superconductors in magnetic fields