Quantum superconductor-insulator transition in titanium monoxide thin films with a wide range of oxygen contents
Y. J. Fan, C. Ma, T. Y. Wang, C. Zhang, Q. L. Chen, X. Liu, Z. Q. Wang, Q. Li, Y. W. Yin, X. G. Li
DOI 10.1103/PhysRevB.98.064501 · Physical Review B
Active bibliographic source — not scientific approval
Bibliographic access preserves source history; it does not approve extracted materials or validate reported claims. Review warnings on each occurrence separately.
Abstract
The superconductor-insulator transition (SIT), one of the most fascinating quantum phase transitions, is closely related to the competition between superconductivity and carrier localization in disordered thin films. Here, superconducting TiOx films with different oxygen contents were grown on Al2O3 substrates by a pulsed laser deposition technique. The increasing oxygen content leads to an increase of disorder, a reduction of carrier density, an enhancement of carrier localization, and therefore a decrease of superconducting transition temperature. A fascinating SIT emerges in cubic TiOx films with increasing oxygen content and its critical sheet resistance is close to the quantum resistance h/(2e)2∼6.45kΩ. The scaling analyses of magnetic field–tuned SITs show that the critical exponent products zν increase from 1.02 to 1.31 with increasing disorder. Based on the results, the SIT can be described by the “dirty boson” model, and a schematic phase diagram for TiOx films was constructed.
Source-reported materials — not catalogue approval
| Formula | Reported Tc (K) | Pressure (GPa) | Type |
|---|---|---|---|
| TiOx Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 6.12 | Pressure not reported | onset |
| TiOx Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 1.08 | Pressure not reported | onset |
| TiOx Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 7.4 | Pressure not reported | unknown |
| TiOx Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 5.5 | Pressure not reported | unknown |
Similar papers
Superconducting phase of TixOy thin films grown by molecular beam epitaxy
similarity 0.92Yasemin Ozbek et al.
Source status unknown — claims are unverified
Pressure-induced resurgence of the superconducting transition in spinel MgTi2O4 thin films
similarity 0.92Lifen Shi et al.
Source status unknown — claims are unverified
Epitaxial stabilization of an orthorhombic Mg-Ti-O superconductor
similarity 0.91Zhuang Ni et al.
Source status unknown — claims are unverified
Thickness-dependent superconductivity and quantum spin Hall effects in Tin+1On (n = 2, 3) MOenes
similarity 0.91Luo Yan et al.
Source status unknown — claims are unverified
Ferroelectricity and superconductivity in strained EuxSr1−xTiO3 films
similarity 0.91Nicholas G. Combs et al.
Source status unknown — claims are unverified
Fluctuation-Limited Noise in a Superconducting Transition-Edge Sensor
similarity 0.91A. Luukanen et al.
Source status unknown — claims are unverified