Abstract:In this paper we explore the effects of 3.5 MeV proton irradiation on Fe(Se,Te) thin films grown on CaF2. In particular, we carry out a systematic experimental investigation with different irradiation fluences up to 7.30·10 16 cm -2 and different proton implantation depths, in order to clarify whether and to what extent the critical current is enhanced or suppressed, what are the effects of irradiation on the critical temperature, the resistivity and the critical magnetic fields, and finally what is the role p… Show more
“…T with respect to the pristine film almost without a decrease in Tc [22]. On the contrary, Jc of 3.5 MeV proton irradiated Fe(Se,Te) films covered with 80 μm thick Al foil decreased by up to 80% after irradiation at 4.2 K. The in-field Jc performance in the irradiated FST films in our study could be attributed to the small number of vortex pinning defects created by the irradiation at low fluence.…”
Section: Magnetic Measurementscontrasting
confidence: 58%
“…A degradation of T c after the ion irradiation is commonly reported in iron-based superconductors [19], although there have been a few reports on an increased T c in iron-based superconductors irradiated with proton and electron [16,20,21]. In previous work, the Fe(Se,Te) films were covered by Al foil with 80 µm thickness and irradiated with 3.5 MeV protons at doses of 2.68 × 10 16 and 5.35 × 10 16 p/cm 2 , corresponding to 2.30 × 10 -3 and 4.59 × 10 -3 dpa, respectively [22][23][24]. The average bombarding energy of the protons on the Fe(Se,Te) film was calculated to be 1.43 ± 0.07 MeV.…”
Section: Magnetic Measurementsmentioning
confidence: 99%
“…In contrast, we observed almost no change in the in-field J c above 1 T. Irradiation with MeV protons could produce mostly random point defects and nanocluster [27] due to ion-nucleus collisions. Sylva et al reported that 3.5 MeV proton irradiation with 6.40 × 10 16 p/cm 2 dose (corresponding to 2.27 × 10 -3 dpa) yields J c improvement of about 40% at 4.2 K and 7 T with respect to the pristine film almost without a decrease in T c [22]. On the contrary, J c of 3.5 MeV proton irradiated Fe(Se,Te) films covered with 80 µm thick Al foil decreased by up to 80% after irradiation at 4.2 K. The in-field J c performance in the irradiated FST films in our study could be attributed to the small number of vortex pinning defects created by the irradiation at low fluence.…”
Raising the critical current density Jc in magnetic fields is crucial to applications such as rotation machines, generators for wind turbines and magnet use in medical imaging machines. The increase in Jc has been achieved by introducing structural defects including precipitates and vacancies. Recently, a low-energy ion irradiation has been revisited as a practically feasible approach to create nanoscale defects, resulting in an increase in Jc in magnetic fields. In this paper, we report the effect of proton irradiation with 1.5 MeV on superconducting properties of iron–chalcogenide FeSe0.5Te0.5 films through the transport and magnetization measurements. The 1.5 MeV proton irradiation with 1 × 1016 p/cm2 yields the highest Jc increase, approximately 30% at 5–10 K and below 1 T without any reduction in Tc. These results indicate that 1.5 MeV proton irradiations could be a practical tool to enhance the performance of iron-based superconducting tapes under magnetic fields.
“…T with respect to the pristine film almost without a decrease in Tc [22]. On the contrary, Jc of 3.5 MeV proton irradiated Fe(Se,Te) films covered with 80 μm thick Al foil decreased by up to 80% after irradiation at 4.2 K. The in-field Jc performance in the irradiated FST films in our study could be attributed to the small number of vortex pinning defects created by the irradiation at low fluence.…”
Section: Magnetic Measurementscontrasting
confidence: 58%
“…A degradation of T c after the ion irradiation is commonly reported in iron-based superconductors [19], although there have been a few reports on an increased T c in iron-based superconductors irradiated with proton and electron [16,20,21]. In previous work, the Fe(Se,Te) films were covered by Al foil with 80 µm thickness and irradiated with 3.5 MeV protons at doses of 2.68 × 10 16 and 5.35 × 10 16 p/cm 2 , corresponding to 2.30 × 10 -3 and 4.59 × 10 -3 dpa, respectively [22][23][24]. The average bombarding energy of the protons on the Fe(Se,Te) film was calculated to be 1.43 ± 0.07 MeV.…”
Section: Magnetic Measurementsmentioning
confidence: 99%
“…In contrast, we observed almost no change in the in-field J c above 1 T. Irradiation with MeV protons could produce mostly random point defects and nanocluster [27] due to ion-nucleus collisions. Sylva et al reported that 3.5 MeV proton irradiation with 6.40 × 10 16 p/cm 2 dose (corresponding to 2.27 × 10 -3 dpa) yields J c improvement of about 40% at 4.2 K and 7 T with respect to the pristine film almost without a decrease in T c [22]. On the contrary, J c of 3.5 MeV proton irradiated Fe(Se,Te) films covered with 80 µm thick Al foil decreased by up to 80% after irradiation at 4.2 K. The in-field J c performance in the irradiated FST films in our study could be attributed to the small number of vortex pinning defects created by the irradiation at low fluence.…”
Raising the critical current density Jc in magnetic fields is crucial to applications such as rotation machines, generators for wind turbines and magnet use in medical imaging machines. The increase in Jc has been achieved by introducing structural defects including precipitates and vacancies. Recently, a low-energy ion irradiation has been revisited as a practically feasible approach to create nanoscale defects, resulting in an increase in Jc in magnetic fields. In this paper, we report the effect of proton irradiation with 1.5 MeV on superconducting properties of iron–chalcogenide FeSe0.5Te0.5 films through the transport and magnetization measurements. The 1.5 MeV proton irradiation with 1 × 1016 p/cm2 yields the highest Jc increase, approximately 30% at 5–10 K and below 1 T without any reduction in Tc. These results indicate that 1.5 MeV proton irradiations could be a practical tool to enhance the performance of iron-based superconducting tapes under magnetic fields.
“…After the milling process, the photoresist was removed by mild sonication in acetone for a few tens of seconds and dried in nitrogen air. Nine Hall bar-shaped micro-bridges 20 μm wide and 50 μm long were realized 29 . The electrical transport properties were investigated by means of a Cryogenic Ltd. full cryogen free cryostat equipped with an integrated cryogen-free variable-temperature insert operating in the range 1.6–300 K up to a maximum magnetic field of 16 T. In this system, the sample was cooled by a continuous helium gas flow and the temperature stability was within 0.01 K. The electrical resistance measurements as a function of the temperature were performed by a four-probe method, and the critical current data were extracted from I-V measurements using the standard voltage criterion set at 10 µV/cm.…”
The process of developing superconducting materials for large scale applications is mainly oriented to optimize flux pinning and the current carrying capability. A powerful approach to investigate pinning properties is to combine high resolution imaging with transport measurements as a function of the magnetic field orientation, supported by a pinning modelling. We carry out Transmission Electron Microscopy, Electron Energy Loss Spectroscopy and critical current measurements in fields up to 16 T varying the angle between the field and c-axis of Fe(Se,Te) epitaxial thin films deposited on CaF2 substrates. We find evidence of nanoscale domains with different Te:Se stoichiometry and/or rotated and tilted axes, as well as of lattice distortions and two-dimensional defects at the grain boundaries. These elongated domains are tens of nm in size along the in-plane axes. We establish a correlation between these observed microstructural features and the pinning properties, specifically strongly enhanced pinning for the magnetic field oriented in-plane and pinning emerging at higher fields for out-of-plane direction. These features can be accounted for within a model where pinning centers are local variations of the critical temperature and local variations of the mean free path, respectively. The identification of all these growth induced defects acting as effective pinning centers may provide useful information for the optimization of Fe(Se,Te) coated conductors.
“…Several microbridges were patterned by standard UV lithography on 100 nm thick films of Fe(Se,Te). These films have been grown on a CaF 2 substrate by pulsed laser deposition using a Nd:YAG laser at 1024 starting from a target whose nominal composition is FeSe 0.5 Te 0.5 , as previously described [15]. The actual film composition is Fe 0.98 Se 0.67 Te 0.33 and it results in a critical temperature T c = 18.5 K as estimated by the 50% of the normal state resistance criterion.…”
The role of a layered structure in superconducting pinning properties is still at a debate. The effects of the vortex shape, which can assume for example a staircase form, could influence the interplay with extrinsic pinning coming from the specific defects of the material, thus inducing an effective magnetic field dependence. To enlighten this role, we analysed the angular dependence of flux pinning energy U(H,θ) as a function of magnetic field in FeSe0.5Te0.5 thin film by considering the field components along the ab-plane of the crystal structure and the c-axis direction. U(H,θ) has been evaluated from magneto-resistivity measurements acquired at different orientations between the applied field up to 16 T and FeSe0.5Te0.5 thin films grown on a CaF2 substrate. We observed that the U(H,θ) shows an anisotropic trend as a function of both the intensity and the direction of the applied field. Such a behaviour can be correlated to the presence of extended defects elongated in the ab-planes, thus mimicking a layered superconductor, as we observed in the microstructure of the compound. The comparison of FeSe0.5Te0.5 with other superconducting materials provides a more general understanding on the flux pinning energy in layered superconductors.
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