2006
DOI: 10.1103/physrevb.74.100507
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Evidence of spatial inhomogeneity near the onset of magnetically induced insulating state in superconducting thin films

Abstract: Non-monotonic differential resistance (dV/dI) is observed in magnetically induced insulating films which exhibit apparent superconductor-metal-insulator transitions in the low temperature limit; at low bias currents the nonlinear transport is insulator-like while at high bias currents it is characteristic of metallic phase. The non-monotonic dV/dI may be evidence that the insulating state consists of metallic domains connected by point contacts (insulating gaps), implying that spatial inhomogeneities play a do… Show more

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Cited by 10 publications
(11 citation statements)
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“…With strengthening field, the width of the interval of the superconducting currents decreases (curves at B=1.5 and 2.5 T) and in the vicinity of the critical field B c the minimum of dV /dJ(J ) near J = 0 transforms into a maximum. The same transformation of the dV /dJ curves in the vicinity of the zero current in fields of order B c was also observed in other materials in the neighborhood of superconductor-insulator transitions, e.g., in InO [153] and Ta [154] (Fig. 42b).…”
Section: Current-voltage Characteristics and Nonlinear Phenomenasupporting
confidence: 78%
See 1 more Smart Citation
“…With strengthening field, the width of the interval of the superconducting currents decreases (curves at B=1.5 and 2.5 T) and in the vicinity of the critical field B c the minimum of dV /dJ(J ) near J = 0 transforms into a maximum. The same transformation of the dV /dJ curves in the vicinity of the zero current in fields of order B c was also observed in other materials in the neighborhood of superconductor-insulator transitions, e.g., in InO [153] and Ta [154] (Fig. 42b).…”
Section: Current-voltage Characteristics and Nonlinear Phenomenasupporting
confidence: 78%
“…FIG.42: Differential resistance ∂V /∂J of films near the superconductor-insulator transition in various magnetic fields as a function of a dc current through the film. The measurement temperature was less than 0.1 K. (a) TiN film 5 nm thick with a superconducting transition temperature Tc ≈ 1 K[152]; signs of hysteresis phenomena are seen in the curves at B = 1 and 1.5 T. (b) Ta films 5 nm thick with Tc ≈ 0.67 K[154].…”
mentioning
confidence: 99%
“…There was no sign of transition from the metallic phase to the superconducting vortex solid (vortex glass or Bragg glass with Rsheet 0) as seen in Bi2Sr2CaCu2O8 single crystals150 and YBa2Cu3Oy ultra-thin films15 . A similar phenomenon has been observed in weak pinning systems such as amorphous MoGe 50,151,152 , MoSi 153 , Ta13,[154][155][156]…”
supporting
confidence: 77%
“…5c). In the past, such concurrent variations of linear and non-linear resistance have been taken as evidence for superconductor-insulator transitions in resistively-shunted single Josephson junction, 39 onedimensional (1d) Josephson junction arrays, 40 superconducting nanowires 41,42 and films, 43,44 and for the metal-insulator transition in multilayer MoS 2 . 45 This variation is indeed expected from the general scaling equation, Eq.1, which states that at the critical field and fixed temperature the resistance of a system should not depend on electrical field, regardless of the system dimension.…”
Section: 4 B ≈ −mentioning
confidence: 99%