Among the recently discovered iron-based superconductors1,2,3, ultrathin films of FeSe grown on SrTiO3 substrates have uniquely evolved into a high-transition-temperature (Tc) superconducting material4,5,6,7,8,9,10,11,12,13,14,15. The mechanisms for the high-Tc superconductivity are under debate, with the superconducting gap mainly characterized with in situ analysis for FeSe films grown by molecular beam epitaxy. Here, we investigate the high-Tc superconductivity in ultrathin FeSe using an alternative top-down electrochemical etching technique in a three-terminal transistor configuration. In addition to the high-temperature superconductivity in FeSe on SrTiO3, the electrochemically etched ultrathin FeSe transistor on MgO also exhibits superconductivity around 40 K, implying that the application of an electric field effectively contributes to the high-Tc superconductivity in ultrathin FeSe regardless of substrate material. Moreover, the observable critical thickness for the high-Tc superconductivity is expanded up to 10 unit cells under an applied electric field and the insulator–superconductor transition is electrostatically controlled. The present demonstration implies that the modification of charge imbalance of holes and electrons by the electric-field effect plays a crucial role in inducing high-Tc superconductivity in FeSe-based electric double-layer transistors.
Iron selenide (FeSe) is one of a family of iron-based superconductors (Tc ∼ 8 K; refs 1,2,3), having a tetragonal PbO structure consisting of the layered atomic stacking of iron and selenium along the c-axis. In single or two unit-cell-thick FeSe films grown by state-of-the-art bottom-up molecular beam epitaxy (MBE; refs 4,5,6,7,8,9,10,11,12,13,14,15) on insulating SrTiO3 (refs 12,13,14) or Nb-doped SrTiO3 (refs 4,5,6,7,8,9,10,11,12,15), a large superconducting gap of about 20 meV has been detected by angle-resolved photoemission spectroscopy (ARPES; refs 4,5,6,7,8,9,10) and scanning tunnelling microscopy (STM; ref. 11). Compared to expected Tc values as high as 65 K (ref. 6) or 80 K (ref. 11) from the large gap energy evaluated by ARPES or STM, the temperature dependence of resistivity yields a consensus of the onset Tc value about 40 K (refs 11,12,13,14). However, a very recent report of superconductivity above 100 K detected by in situ electrical resistance measurements for FeSe films grown on Nb-doped SrTiO3 would apparently increase the spread in Tc (refs 15,16). The mechanisms for the enhancement of the superconducting gap energy in ultrathin FeSe are now considered to be strong electron–phonon coupling10, variation of the electronic band structure at the M point and the Γ point4, and a charge transfer effect from the substrates5,13,17. Ex situ characterizations based on the temperature dependence of resistivity regarding the effect of an electric field, magnetic field, thickness dependence of Tc and substrate material dependence are matters of interest for a deeper understanding of high-Tc superconductivity in ultrathin FeSe studies.
In contrast to the in situ bottom-up MBE technique, classical electrochemical etching is one of the best means of carrying out a top-down approach to ultrathin FeSe films, owing to a high uniformity and fine tunability in thickness being possible through continuous monitoring of the electrical current originating from the electrochemical reaction. In our experiments, we employed this electrochemical etching approach in a three-terminal transistor configuration, the so-called electric double-layer (EDL) transistor (Fig. 1a)18. The EDL transistors were fabricated from 13- and 18-nm-thick FeSe films grown on insulating SrTiO3 and MgO substrates, respectively, by pulsed-laser deposition, as described in Methods. The films and Pt gate electrode are covered with the ionic liquid (IL) N, N-dethyl-N-methyl-N-(2-methoxyethyl)ammonium bis(trifluoromethanesulphonyl)imide (DEME-TFSI), as schematically shown in Fig. 1a. The original concept of the EDL transistor involves an electrostatic charge carrier doping based on the giant capacitance originating from a very narrow (<1 nm) EDL width. Following this concept, various kinds of physical phenomena, such as superconductivity18,19,20,21,22,23, ferromagnetism24 and an insulator–metal transition in correlated electron systems25, have been induced or controlled electrostatically. Another feature of EDL transistors is the electrochemical reaction26,27,28. These two features appear separately, with some boundary that depends on the temperature of the IL and the applied gate voltage26,27, as schematically shown by the dashed black line in Fig. 1b. In this study, we have applied an electrostatic doping effect with varying VG below the characteristic temperature (blue arrow in Fig. 1b) and electrochemical etching to peel FeSe layers while tuning the sample temperature under a constant applied VG (red arrow in Fig. 1b). For each etching sequence, the systematic dependence on thickness and the effect of the field on superconductivity in FeSe films can be investigated, all within a single EDL transistor.
The temperature dependence of the channel sheet resistance (Rs–T curve) and its superconducting properties were measured using a standard d.c. four-terminal method. In the initial thick films on SrTiO3 and on MgO, onset superconducting transition temperatures Tcon = 8.2 K and 4.8 K are clearly observed on lowering the temperature T, as shown in Fig. 1c (solid lines), which is consistent with the bulk properties of FeSe (ref. 3). No significant change in the Rs–T curves (broken lines) is observed with electrostatic doping using VG = 5 V at 220 K for the initial thick condition, implying that high-Tc superconductivity is not induced at the IL/FeSe interface (see Supplementary Information) at this temperature.
The high-Tc superconductivity appears in FeSe films grown on both SrTiO3 (sample A) and MgO (sample N) after a series of etching, as shown in Fig. 2a, b. During the etching sequence, with a constant VG = 5 V at about 245 K, Rs–T measurements were performed regularly (black arrow in Fig. 1b) showing that the onset Tc in the normalized sheet resistance Rs/Rs100 K is greatly increased from the bulk value up to Tcon = 43.3 and 39.0 K for samples A and N, respectively (the corresponding raw data are presented in Supplementary Information). The estimated Tcon values from Rs–T curves shown in Fig. 2a, b are summarized in Fig. 2c, d as a function of the average thickness, which is carefully estimated from the initial thickness and the etching rate in the electrochemical reaction from the gate leakage current (see Supplementary Information). There are four implications derived from these figures. The first implication is that two-step transitions are observed in the intermediate etching region. Accompanying the enhancement of metallic behaviour, Rs drops first at around T = 30 K, with second steps at 8 K and 4 K in the case of FeSe on SrTiO3 and MgO, respectively, giving a first signature of the appearance of high-Tc superconducting region in the device. The systematic disappearance of the bulky low-Tc region with decreasing thickness is evidence of our fine tuning of the thicknesses. Indeed, the zero-resistance temperature of about 30 K implies that the FeSe layers are uniformly etched down to approximately one/two unit cells in thickness in our primitive devices. The second implication is that the high-Tc superconductivity emerges in the ultrathin FeSe film on MgO as a result of the electric-field effect in the EDL transistor. Such high-Tc superconductivity in FeSe on MgO has not been reported in in situ MBE studies—probably owing to there being no charge transfer from MgO to FeSe. In reality, in Hall effect measurements on high-Tc one/two-unit-cell-thick FeSe on MgO, a negative Hall coefficient is observed, indicating electron accumulation is realized. The third implication is that the values of Tcon for both samples on SrTiO3 and MgO are close to the highest values that have been reported in capped single-unit-cell-thick FeSe films grown by MBE (refs 12,13,14). If the disorder at the IL/FeSe interface limits Tcon to about 40 K, as low as the capped FeSe, further improvements of the interface quality are required to enhance Tcon towards 100 K (refs 15,16). The final implication is that the high-Tc superconductivity emerges under a relatively thicker condition of about ten unit cells, followed by a weak thickness dependence. At present, it is not clear whether the whole thick-film region contributes high-Tc superconductivity or not. We will return to this later.
To further investigate the superconducting properties, we performed Rs–T measurements under perpendicular magnetic fields B for sample N on MgO. As shown in Fig. 2e, the tail of the resistive transition is broadened by applying B, indicating the two-dimensional nature of the FeSe film. Figure 2f shows the temperature dependence of the perpendicular upper critical field Bc2(T) derived from the midpoint temperature of the resistance drop Tc(B) in the Rs–T curves in Fig. 2e. From the linear relation, which is consistent with the Ginzburg–Landau (GL) theory given as Bc2(T) = (φ0/(2πξ2(0)))(1 − (T/Tc(0))), with φ0 and ξ(0) being the flux quantum and the GL coherence length at zero temperature, respectively, we obtained ξ(0) = 2.0 nm, which is around half of the bulk value3. We further compare the GL coherence length ξ(0) to the expression of 0.74ξ0 in the clean limit based on the Bardeen, Cooper, and Schrieffer (BCS) theory with ξ0 = ℏvF/πΔ(0) = ℏvF/π(1.76kBTc). Here, ℏ, vF, Δ(0) and kB are the reduced Planck constant, Fermi velocity, BCS superconducting gap and Boltzmann constant, respectively. Using a value of vF ∼ 9.56 × 104 m s−1 (ref. 5), we determined 0.74ξ0 to be ∼2.1 nm. This value is comparable to ξ(0) = 2.0 nm obtained from the experiments, indicating the system is almost in the clean limit.
Returning to the thickness dependence of Tcon in Fig. 2c, d, we note that the first single-step superconducting transition occurs at thicknesses of 9.6 nm and 5.9 nm for samples A and N, respectively. The appearance of high-Tc superconductivity in the rather thicker conditions prompted us to consider how the electric-field effect contributes. Here, we examined the effect of electrostatic doping on the superconductivity in both ultrathin and thicker conditions using different experimental schemes in the same device set-up as for sample A. First, samples B and C on SrTiO3 and samples M and L on MgO were etched at T = 245 K to induce the superconductivity, as shown in Fig. 3a, the top panel of Fig. 3c, and in Fig. 3d (red line data) and the inset of Fig. 3d (red line data). The thicknesses of sample B on SrTiO3 and sample L on MgO are tuned to approximately one/two unit cells in thickness (the red square in Fig. 2c and the purple triangle in Fig. 2d), whereas sample C on SrTiO3 and sample M on MgO are etched to intermediate thicknesses of 9.4 nm (the blue triangle in Fig. 2c) and 3.7 nm (the green circle in Fig. 2d), by monitoring the leakage current under the assumption that the same etching rate holds as for sample A. After detection of the high-Tc superconducting behaviour, we examined the electrostatic effect by removing and then reapplying VG at T = 220 K (along the blue arrow in Fig. 1b; note that no electrochemical etching occurs at this temperature, as mentioned above).
For sample B, expectedly at a thickness of one/two unit cells, the initial insulating behaviour was not recovered on reducing VG from 5 to 3 and then to 0 V, as shown in Fig. 3b. This result is good evidence for the thickness having reached close to one/two unit cells, because the high-Tc superconductivity under VG = 0 V is consistent with the result of a previous report on FeSe/SrTiO3 with charge transfer solely from the SrTiO3 substrate13. Interestingly, the increase of Tcon from 43.5 to 46.3 K as a result of reduced VG implicates an over-doping effect from electrostatic doping. In contrast, in sample C, under the thicker 9.4 nm condition, the superconductivity vanishes and the Rs–T curve returns to insulating behaviour when VG is removed (blue line in middle panel of Fig. 3c). The reappearance of insulating behaviour indicates uniform etching without a local ultrathin region providing a high-Tc superconducting current path. Then, application of VG = 5 V recovers the superconductivity (blue line in bottom panel of Fig. 3c), demonstrating reversible control of the insulator–superconductor transition by electrostatic means. We note that the possibility of intercalation can be excluded for two reasons: no significant variation of the c-axis length was observed after etching (see Supplementary Information) and reversible control of the insulator–superconductor transition was possible by gating. This series of results in sample C suggests that the observable thickness condition for high-Tcon superconductivity is greatly expanded from one/two unit cells to more than ten unit cells by the application of an electric field. Furthermore, Tcon values in samples M and L decrease on reducing the accumulated charge, as shown in Fig. 3d. Therefore, we suppose that the high-Tc superconductivity in ultrathin FeSe on MgO is fully controllable by the application of an electric field and confirm that a thickness of one/two unit cells of FeSe itself is not superconducting on MgO, as distinct from on SrTiO3 substrates.
Finally, we discuss possible mechanisms for the high-Tc superconductivity in FeSe EDL transistors from the view point of the thickness dependence. The comparable values of Tcon shown in Fig. 2c, d for SrTiO3 and MgO suggest that the electric-field effect induces superconductivity at 40 K despite one possibly expecting different electron–phonon coupling between the FeSe film and the substrate10. Concomitantly, the small thickness dependence of Tcon below a thickness of ten unit cells indicates that an ultrathin condition, particularly for a single unit cell itself, probably does not play a crucial role in the increase of Tc for the superconductivity of ultrathin FeSe. Nevertheless, the origin of the difference in the critical thickness for SrTiO3 (9.6 nm) and MgO (5.9 nm) is still not clear at present, although it may be linked to the degree of charge transfer from the substrates to the FeSe. Naively, it is likely that the positive VG depletes holes in the valence band at the Γ point and accumulates electrons in the conduction band at the M point through the IL/FeSe interface, while the interface between the IL and the thick FeSe does not work as the high-Tc superconducting channel (see Fig. 1c). As a consequence, a similar modification of the electronic band structure at the Γ and M points, as proved by ARPES for the single-unit-cell and three-unit-cell FeSe on SrTiO3 exhibiting large superconducting gap energy5,29, may be realized by applying an electric field below the critical thicknesses on SrTiO3 and MgO. In other words, the electric-field effect in FeSe-EDLT expands the modified layer width yielding the high-Tc superconductivity, which was one/two-unit-cell FeSe in the case of charge doping only from the SrTiO3 substrate. Furthermore, we suppose that the whole sample contributes high-Tc superconductivity when the modified layer width at IL/FeSe interface touches the interface of the FeSe/substrates. This is what we observed in Rs–T curve as the single-step transition. However, further investigation into the modification of electronic band structures in etched FeSe under the application of VG is required to verify our speculation.
By employing the EDL transistor configuration, high-Tc superconductivity in ultrathin FeSe films has been investigated from several perspectives, such as thickness and substrate material dependence. The application of the electric-field effect to induce modification of the electronic band structure would be a major contribution towards Tcon values of 40 K below a thickness of ten unit cells regardless of substrate material. Our demonstration of etching that is controlled well by the temperature of the IL under an applied VG sheds light on new aspects of the EDL transistor as a useful approach in carrying out ultrathin-film studies and expands the opportunities for demonstrating ex situ the superconductivity of ultrathin FeSe grown on various insulating substrates12,13,15,30.
The FeSe films were grown at 300 °C on insulating SrTiO3(001) and MgO(001) substrates by pulsed-laser deposition with an as-delivered FeSe target (Kojundo Chemical Laboratory), followed by in situ post annealing at 450 °C for 30 min. The growth rate with a laser repetition rate of 5 Hz is approximately 17 nm h−1, the value of which is estimated by X-ray Laue fringes (see Supplementary Information). After cutting the film into a 2 × 5 mm2 rectangular pieces, the channel and the four-terminal electrode (indium pads) were prepared to confine the current flow within the channel by scratching the film. Then, the electrodes were covered with a silicone sealant to prevent them from reacting chemically with the ionic liquid. A platinum plate for the side gate electrode was placed next to the FeSe channel on the same chip and indium pads were attached to the gate electrode in the same way (see Supplementary Information). Then, the FeSe channel and the gate electrode were covered by the ionic liquid, N, N-dethyl-N-methyl-N-(2-methoxyethyl)ammonium bis(trifluoromethanesulphonyl)imide (DEME-TFSI) to form an EDL transistor configuration, as shown in Fig. 1a. To suppress degradation of the sample in air, we carried out the EDL fabrication process as soon as possible. However, it usually took 6 h before starting the measurement and the sample surface was inevitably exposed to air for about 2–3 h. The thickness after etching is estimated from the initial thickness and the etching rate by summing the leakage current (see Supplementary Information). Surface roughness contributes a ±0.6 nm error to the thickness.
The sheet resistance Rs is measured by the standard four-terminal method, where a constant current of typically 0.5 μA is applied and the longitudinal voltage drop is measured by a nanovoltmeter. The temperature is controlled by dipping the sample into the liquid helium vessel in electrical measurements for samples A–C. The sample temperature is monitored by means of a calibrated resistance thermometer (Cernox1050 resistor) inserted in the copper block where the sample is mounted. The Rs–T curve and magnetotransport properties for samples M and N are measured using a Quantum Design physical property measurement system (PPMS). To control the doping level electrostatically through EDL tuning, we fix the temperature at T = 220 K while varying VG. In contrast, the occurrence of the electrochemical reaction is controlled by tuning T in the range from 240 to 250 K while keeping a constant VG = 5.0 V.
The authors thank S. Tanaka and T. Ouchi for experimental help and M. Kawasaki, Y. Iwasa and K. Fujiwara for stimulating discussions. This work is partly supported by Grant-in-Aid for Scientific Research on Innovative Areas (No. KAKENHI 22103004) from MEXT of Japan and Grant-in-Aid for Specially Promoted Research (No. KAKENHI 25000003) from the Japan Society for the Promotion of Science (JSPS).