Spectroscopic evidence of disorder-induced quantum phase transitions in monolayer Fe(Te,Se) superconductor
arXiv:2603.04717 · doi:10.1103/gkvs-4vsb
Abstract
The superconductor-insulator transition as a paradigm of quantum phase transitions has attracted tremendous interest over the past three decades. While the magnetic field and carrier density can be tuned to drive the transition, the role of disorder in the transition is not well understood due to the complicated interplay between superconductivity and electron localization. In this work, we controllably introduce disorder in a two-dimensional high-temperature superconductor by depositing iron clusters onto the superconducting monolayer Fe(Te,Se) crystalline film. The spectral evolution from superconducting gaps to insulating gaps with increasing disorder is detected by scanning tunneling spectroscopy measurements. When the disorder is strong, large U-shaped gaps are observed and attributed to the localization-enhanced Cooper pair correlation. Our observations provide the insight into the emergent phases of low-dimensional and high-temperature superconductors with disorder.
References in corpus (13)
- Anderson Transitions
- Localization of preformed Cooper-pairs in disordered superconductors
- Nature of the superconductor-insulator transition in disordered superconductors
- Eigenfunction fractality and pseudogap state near superconductor-insulator transition
- Phase fluctuations in a strongly disordered s-wave superconductor close to the metal-insulator transition
- Quantum breakdown of superconductivity in low-dimensional materials
- Universal Substrate Effect on the Superconductivity of FeSe Monolayer Films
- Spin-polarized Yu-Shiba-Rusinov states in an iron based superconductor
- High-temperature superconductivity in one-unit-cell FeSe films
- When Superconductivity Crosses Over: From BCS to BEC
- Quantum phase transitions in two-dimensional superconductors: a review on recent experimental progress
- Real-space BCS-BEC crossover in FeSe monolayer
- Lateral quantum confinement effect on monolayer high-Tc superconductors