Synthesis and transport properties of superconducting thin films of K0.33WO3: Tc reduction due to disorder
Phillip M. Wu, Chris Hart, Katherine Luna, Ko Munakata, Akio Tsukada, Subhash H. Risbud, T. H. Geballe, M. R. Beasley
DOI 10.1103/PhysRevB.89.184501 · 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
Via a two-step deposition and post-annealing procedure, K-doped WO3 thin films with reproducible transport properties are obtained. We observe a larger critical field Hc2 along the c axis, consistent with the picture of the Fermi surface containing one-dimensional bands along this direction. Reducing the film thickness results in a superconductor to insulator transition. Scanning electron microscopy (SEM) images show that KWO3 crystallites become less connected as the deposition time is reduced, providing a microscopic explanation for the transport behavior. In the superconducting films, a resistive anomaly is observed similar to bulk crystals, with a characteristic temperature that shifts lower with decreasing film thickness. The competing electronic effects manifest as a suppression of the density of states at the Fermi level, observed using point contact tunneling spectroscopy, demonstrating that disorder-induced increased Coulomb interactions are present. Using the theory of Belitz for the reduction of Tc due to disorder, we can infer that the film with the highest observed Tc has a relatively large disorder dependent electron-phonon interaction parameter ∼1.2. Understanding microscopically why certain films display higher Tc will aid in the search for the trace high-Tc superconducting anomalies observed in lightly surface doped bronzes.
Source-reported materials — not catalogue approval
| Formula | Reported Tc (K) | Pressure (GPa) | Type |
|---|---|---|---|
| K0.33WO3 Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 2 | Pressure not reported | unknown |
| K0.33WO3-y Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 3 | Pressure not reported | onset |
| K0.33WO3 Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 3 | Pressure not reported | zero_resistance |
Similar papers
Superconducting properties of the KxWO3 tetragonal tungsten bronze and the superconducting phase diagram of the tungsten bronze family
similarity 0.90Neel Haldolaarachchige et al.
Source status unknown — claims are unverified
Emergence of intrinsic superconductivity in monolayer W2N3
similarity 0.89Jianyong Chen & Yanfeng Ge
Source status unknown — claims are unverified
Thin superconducting oxide films
similarity 0.88R. B. Laibowitz et al.
Source status unknown — claims are unverified
Gate tunability of the superconducting state at the EuO/KTaO3 (111) interface
similarity 0.88Weiliang Qiao et al.
Source status unknown — claims are unverified
130-K superconductivity and microwave absorption in Tl-Ba-Ca-Cu-O
similarity 0.88Zhao Min-Guang & Yan Qi-Li
Source status unknown — claims are unverified
Superconductivity in the tungsten bronze RbxWO3 (0.20⩽x⩽0.33) in connection with its structure, electronic density of states, and phonon density of states
similarity 0.88R. Brusetti et al.
Source status unknown — claims are unverified