8
views
0
recommends
+1 Recommend
0 collections
    0
    shares
      • Record: found
      • Abstract: not found
      • Article: not found

      Electric field-induced superconducting transition of insulating FeSe thin film at 35 K

      , , , ,
      Proceedings of the National Academy of Sciences
      Proceedings of the National Academy of Sciences

      Read this article at

      ScienceOpenPublisherPMC
      Bookmark
          There is no author summary for this article yet. Authors can add summaries to their articles on ScienceOpen to make them more accessible to a non-specialist audience.

          Abstract

          <p id="d15025885e197">One of the key strategies for obtaining higher superconducting critical temperature ( <i>T</i> <sub>c</sub>) is to dope carriers into an insulator parent material with strong electron correlation. Here, we examined electrostatic carrier doping to insulator-like thin (∼10-nm-thick) FeSe epitaxial films using an electric double-layer transistor (EDLT) structure. The maximum <i>T</i> <sub>c</sub> obtained is 35 K, which is 4× higher than that of bulk FeSe. This result demonstrates that EDLTs are useful tools to explore the ultimate <i>T</i> <sub>c</sub> for insulating parent materials, and opens a way to explore high- <i>T</i> <sub>c</sub> superconductivity, where carrier doping is difficult by conventional chemical substitution. </p><p class="first" id="d15025885e225">It is thought that strong electron correlation in an insulating parent phase would enhance a critical temperature ( <i>T</i> <sub>c</sub>) of superconductivity in a doped phase via enhancement of the binding energy of a Cooper pair as known in high- <i>T</i> <sub>c</sub> cuprates. To induce a superconductor transition in an insulating phase, injection of a high density of carriers is needed (e.g., by impurity doping). An electric double-layer transistor (EDLT) with an ionic liquid gate insulator enables such a field-induced transition to be investigated and is expected to result in a high <i>T</i> <sub>c</sub> because it is free from deterioration in structure and carrier transport that are in general caused by conventional carrier doping (e.g., chemical substitution). Here, for insulating epitaxial thin films (∼10 nm thick) of FeSe, we report a high <i>T</i> <sub>c</sub> of 35 K, which is 4× higher than that of bulk FeSe, using an EDLT under application of a gate bias of +5.5 V. Hall effect measurements under the gate bias suggest that highly accumulated electron carrier in the channel, whose area density is estimated to be 1.4 × 10 <sup>15</sup> cm <sup>–2</sup> (the average volume density of 1.7 × 10 <sup>21</sup> cm <sup>–3</sup>), is the origin of the high- <i>T</i> <sub>c</sub> superconductivity. This result demonstrates that EDLTs are useful tools to explore the ultimate <i>T</i> <sub>c</sub> for insulating parent materials. </p>

          Related collections

          Most cited references26

          • Record: found
          • Abstract: not found
          • Article: not found

          Iron-based layered superconductor La[O(1-x)F(x)]FeAs (x = 0.05-0.12) with T(c) = 26 K.

            Bookmark
            • Record: found
            • Abstract: not found
            • Article: not found

            Temperature and Purity Dependence of the Superconducting Critical Field,Hc2. III. Electron Spin and Spin-Orbit Effects

              Bookmark
              • Record: found
              • Abstract: not found
              • Article: not found

              Superconductivity at 55 K in Iron-Based F-Doped Layered Quaternary Compound Sm[O1-xFx] FeAs

                Bookmark

                Author and article information

                Journal
                Proceedings of the National Academy of Sciences
                Proc Natl Acad Sci USA
                Proceedings of the National Academy of Sciences
                0027-8424
                1091-6490
                April 12 2016
                April 12 2016
                April 12 2016
                March 28 2016
                : 113
                : 15
                : 3986-3990
                Article
                10.1073/pnas.1520810113
                4839426
                27035956
                703c85c1-ed2a-432e-b450-6e910b7cdda8
                © 2016
                History

                Comments

                Comment on this article