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      Ionic-liquid-gating induced protonation and superconductivity in FeSe, FeSe0.93S0.07, ZrNCl, 1T-TaS2, and Bi2Se3

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          Abstract

          We report protonation in several compounds by an ionic-liquid-gating method, with optimized gating conditions. This leads to single superconducting phases for several compounds. Non-volatility of protons allow post-gating magnetization and transport measurements. The superconducting transition temperature \(T_C\) is enhanced to 43.5~K for FeSe\(_{0.93}\)S\(_{0.07}\), and 41~K for FeSe after protonation. Superconductivity with \(T_c\)$\approx\(15~K for ZrNCl, \)\approx\(7.2~K for 1\)T\(-TaS\)_2\(, and \)\approx\(3.8~K for Bi\)_2\(Se\)_3\( are induced after protonation. Electric transport in protonated FeSe\)_{0.93}\(S\)_{0.07}\( confirms high-temperature superconductivity. Our \)^{1}\(H NMR measurements on protonated FeSe\)_{1-x}\(S\)_{x}\( reveal enhanced spin-lattice relaxation rate \)1/^{1}T_1\( with increasing \)x\(, which is consistent with LDA calculations that H\)^{+}$ are located in the interstitial sites close to the anions.

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          Most cited references11

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          Topological insulators in Bi2Se3, Bi2Te3 and Sb2Te3 with a single Dirac cone on the surface

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            Liquid-gated interface superconductivity on an atomically flat film.

            Liquid/solid interfaces are attracting growing interest not only for applications in catalytic activities and energy storage, but also for their new electronic functions in electric double-layer transistors (EDLTs) exemplified by high-performance organic electronics, field-induced electronic phase transitions, as well as superconductivity in SrTiO(3) (ref. 12). Broadening EDLTs to induce superconductivity within other materials is highly demanded for enriching the materials science of superconductors. However, it is severely hampered by inadequate choice of materials and processing techniques. Here we introduce an easy method using ionic liquids as gate dielectrics, mechanical micro-cleavage techniques for surface preparation, and report the observation of field-induced superconductivity showing a transition temperature T(c)=15.2 K on an atomically flat film of layered nitride compound, ZrNCl. The present result reveals that the EDLT is an extremely versatile tool to induce electronic phase transitions by electrostatic charge accumulation and provides new routes in the search for superconductors beyond those synthesized by traditional chemical methods.
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              Superconductor-insulator transition in La2 - xSrxCuO4 at the pair quantum resistance.

              High-temperature superconductivity in copper oxides arises when a parent insulator compound is doped beyond some critical concentration; what exactly happens at this superconductor-insulator transition is a key open question. The cleanest approach is to tune the carrier density using the electric field effect; for example, it was learned in this way that weak electron localization transforms superconducting SrTiO(3) into a Fermi-glass insulator. But in the copper oxides this has been a long-standing technical challenge, because perfect ultrathin films and huge local fields (>10(9) V m(-1)) are needed. Recently, such fields have been obtained using electrolytes or ionic liquids in the electric double-layer transistor configuration. Here we report synthesis of epitaxial films of La(2- x)Sr(x)CuO(4) that are one unit cell thick, and fabrication of double-layer transistors. Very large fields and induced changes in surface carrier density enable shifts in the critical temperature by up to 30 K. Hundreds of resistance versus temperature and carrier density curves were recorded and shown to collapse onto a single function, as predicted for a two-dimensional superconductor-insulator transition. The observed critical resistance is precisely the quantum resistance for pairs, R(Q) = h/(2e) = 6.45 kΩ, suggestive of a phase transition driven by quantum phase fluctuations, and Cooper pair (de)localization.

                Author and article information

                Journal
                24 May 2019
                Article
                1905.10080
                0d1ad11f-bd83-46ab-9208-0040e5b81710

                http://arxiv.org/licenses/nonexclusive-distrib/1.0/

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                Custom metadata
                4 pages, 7 figures
                cond-mat.supr-con

                Condensed matter
                Condensed matter

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