Search Results
The influence of the in-plane lattice constant on the superconducting transition temperature of FeSe0.7Te0.3 thin films
2017, Yuan, Feifei, Iida, Kazumasa, Grinenko, Vadim, Chekhonin, Paul, Pukenas, Aurimas, Skrotzki, Werner, Sakoda, Masahito, Naito, Michio, Sala, Alberto, Putti, Marina, Yamashita, Aichi, Takano, Yoshihiko, Shi, Zhixiang, Nielsch, Kornelius, Hühne, Ruben
Epitaxial Fe(Se,Te) thin films were prepared by pulsed laser deposition on (La0.18Sr0.82)(Al0.59Ta0.41)O3 (LSAT), CaF2-buffered LSAT and bare CaF2 substrates, which exhibit an almost identical in-plane lattice parameter. The composition of all Fe(Se,Te) films were determined to be FeSe0.7Te0.3 by energy dispersive X-ray spectroscopy, irrespective of the substrate. Albeit the lattice parameters of all templates have comparable values, the in-plane lattice parameter of the FeSe0.7Te0.3 films varies significantly. We found that the superconducting transition temperature (Tc) of FeSe0.7Te0.3 thin films is strongly correlated with their a-axis lattice parameter. The highest Tc of over 19 K was observed for the film on bare CaF2 substrate, which is related to unexpectedly large in-plane compressive strain originating mostly from the thermal expansion mismatch between the FeSe0.7Te0.3 film and the substrate.
Elastoresistivity of Heavily Hole-Doped 122 Iron Pnictide Superconductors
2022, Hong, Xiaochen, Sykora, Steffen, Caglieris, Federico, Behnami, Mahdi, Morozov, Igor, Aswartham, Saicharan, Grinenko, Vadim, Kihou, Kunihiro, Lee, Chul-Ho, Büchner, Bernd, Hess, Christian
Nematicity in heavily hole-doped iron pnictide superconductors remains controversial. Sizeable nematic fluctuations and even nematic orders far from magnetic instability were declared in RbFe2As2 and its sister compounds. Here, we report a systematic elastoresistance study of a series of isovalent- and electron-doped KFe2As2 crystals. We found divergent elastoresistance on cooling for all the crystals along their [110] direction. The amplitude of elastoresistivity diverges if K is substituted with larger ions or if the system is driven toward a Lifshitz transition. However, we conclude that none of them necessarily indicates an independent nematic critical point. Instead, the increased nematicity can be associated with another electronic criticality. In particular, we propose a mechanism for how elastoresistivity is enhanced at a Lifshitz transition.
Piezoelectric-driven uniaxial pressure cell for muon spin relaxation and neutron scattering experiments
2020, Ghosh, Shreenanda, Brückner, Felix, Nikitin, Artem, Grinenko, Vadim, Elender, Matthias, Mackenzie, Andrew P., Luetkens, Hubertus, Klauss, Hans-Henning, Hicks, Clifford W.
We present a piezoelectric-driven uniaxial pressure cell that is optimized for muon spin relaxation and neutron scattering experiments and that is operable over a wide temperature range including cryogenic temperatures. To accommodate the large samples required for these measurement techniques, the cell is designed to generate forces up to ∼1000 N. To minimize the background signal, the space around the sample is kept as open as possible. We demonstrate here that by mounting plate-like samples with epoxy, a uniaxial stress exceeding 1 GPa can be achieved in an active volume of at least 5 mm3. We show that for practical operation, it is important to monitor both the force and displacement applied to the sample. In addition, because time is critical during facility experiments, samples are mounted in detachable holders that can be rapidly exchanged. The piezoelectric actuators are likewise contained in an exchangeable cartridge. © 2020 Author(s).
Calorimetric evidence for two phase transitions in Ba1−xKxFe2As2 with fermion pairing and quadrupling states
2023, Shipulin, Ilya, Stegani, Nadia, Maccari, Ilaria, Kihou, Kunihiro, Lee, Chul-Ho, Hu, Quanxin, Zheng, Yu, Yang, Fazhi, Li, Yongwei, Yim, Chi-Ming, Hühne, Ruben, Klauss, Hans-Henning, Putti, Marina, Caglieris, Federico, Babaev, Egor, Grinenko, Vadim
Materials that break multiple symmetries allow the formation of four-fermion condensates above the superconducting critical temperature (T c). Such states can be stabilized by phase fluctuations. Recently, a fermionic quadrupling condensate that breaks the Z 2 time-reversal symmetry was reported in Ba1−xKxFe2As2. A phase transition to the new state of matter should be accompanied by a specific heat anomaly at the critical temperature where Z 2 time-reversal symmetry is broken (TcZ2>Tc). Here, we report on detecting two anomalies in the specific heat of Ba1−xKxFe2As2 at zero magnetic field. The anomaly at the higher temperature is accompanied by the appearance of a spontaneous Nernst effect, indicating the breakdown of Z 2 symmetry. The second anomaly at the lower temperature coincides with the transition to a zero-resistance state, indicating the onset of superconductivity. Our data provide the first example of the appearance of a specific heat anomaly above the superconducting phase transition associated with the broken time-reversal symmetry due to the formation of the novel fermion order.
Long-range magnetic order in the ~S=1/2 triangular lattice antiferromagnet KCeS2
2020, Bastien, Gaël, Rubrecht, Bastian, Haeussler, Ellen, Schlender, Philipp, Zangeneh, Ziba, Avdoshenko, Stanislav, Sarkar, Rajib, Alfonsov, Alexey, Luther, Sven, Onykiienko, Yevhen A., Walker, Helen C., Kühne, Hannes, Grinenko, Vadim, Guguchia, Zurab, Kataev, Vladislav, Klauss, Hans-Henning, Hozoi, Liviu, van den Brink, Jeroen, Inosov, Dmytro S., Büchner, Bernd, Wolter, Anja U.B., Doert, Thomas
Recently, several putative quantum spin liquid (QSL) states were discovered in ~S=1/2 rare-earth based triangular-lattice antiferromagnets (TLAF) with the delafossite structure. A way to clarify the origin of the QSL state in these systems is to identify ways to tune them from the putative QSL state towards long-range magnetic order. Here, we introduce the Ce-based TLAF KCeS2 and show via low-temperature specific heat and μSR investigations that it yields magnetic order below TN=0.38 K despite the same delafossite structure. We identify a well separated ~S=1/2 ground state for KCeS2 from inelastic neutron scattering and embedded-cluster quantum chemical calculations. Magnetization and electron spin resonance measurements on single crystals indicate a strong easy-plane g~factor anisotropy, in agreement with the ab initio calculations. Finally, our specific-heat studies reveal an in-plane anisotropy of the magnetic field-temperature phase diagram which may indicate anisotropic magnetic interactions in KCeS2.
Hall-plot of the phase diagram for Ba(Fe1−xCox)2As2
2016, Iida, Kazumasa, Grinenko, Vadim, Kurth, Fritz, Ichinose, Ataru, Tsukada, Ichiro, Ahrens, Eike, Pukenas, Aurimas, Chekhonin, Paul, Skrotzki, Werner, Teresiak, Angelika, Hühne, Ruben, Aswartham, Saicharan, Wurmehl, Sabine, Erbe, Manuela, Hänisch, Jens, Holzapfel, Bernhard, Drechsler, Stefan-Ludwig, Efremov, Dmitri V.
The Hall effect is a powerful tool for investigating carrier type and density. For single-band materials, the Hall coefficient is traditionally expressed simply by , where e is the charge of the carrier, and n is the concentration. However, it is well known that in the critical region near a quantum phase transition, as it was demonstrated for cuprates and heavy fermions, the Hall coefficient exhibits strong temperature and doping dependencies, which can not be described by such a simple expression, and the interpretation of the Hall coefficient for Fe-based superconductors is also problematic. Here, we investigate thin films of Ba(Fe1−xCox)2As2 with compressive and tensile in-plane strain in a wide range of Co doping. Such in-plane strain changes the band structure of the compounds, resulting in various shifts of the whole phase diagram as a function of Co doping. We show that the resultant phase diagrams for different strain states can be mapped onto a single phase diagram with the Hall number. This universal plot is attributed to the critical fluctuations in multiband systems near the antiferromagnetic transition, which may suggest a direct link between magnetic and superconducting properties in the BaFe2As2 system.
Unsplit superconducting and time reversal symmetry breaking transitions in Sr2RuO4 under hydrostatic pressure and disorder
2021, Grinenko, Vadim, Das, Debarchan, Gupta, Ritu, Zinkl, Bastian, Kikugawa, Naoki, Maeno, Yoshiteru, Hicks, Clifford W., Klauss, Hans-Henning, Sigrist, Manfred, Khasanov, Rustem
There is considerable evidence that the superconducting state of Sr2RuO4 breaks time reversal symmetry. In the experiments showing time reversal symmetry breaking, its onset temperature, TTRSB, is generally found to match the critical temperature, Tc, within resolution. In combination with evidence for even parity, this result has led to consideration of a dxz ± idyz order parameter. The degeneracy of the two components of this order parameter is protected by symmetry, yielding TTRSB = Tc, but it has a hard-to-explain horizontal line node at kz = 0. Therefore, s ± id and d ± ig order parameters are also under consideration. These avoid the horizontal line node, but require tuning to obtain TTRSB ≈ Tc. To obtain evidence distinguishing these two possible scenarios (of symmetry-protected versus accidental degeneracy), we employ zero-field muon spin rotation/relaxation to study pure Sr2RuO4 under hydrostatic pressure, and Sr1.98La0.02RuO4 at zero pressure. Both hydrostatic pressure and La substitution alter Tc without lifting the tetragonal lattice symmetry, so if the degeneracy is symmetry-protected, TTRSB should track changes in Tc, while if it is accidental, these transition temperatures should generally separate. We observe TTRSB to track Tc, supporting the hypothesis of dxz ± idyz order.
High field superconducting properties of Ba(Fe1-xCox)2As2 thin films
2015, Hänisch, Jens, Iida, Kazumasa, Kurth, Fritz, Reich, Elke, Tarantini, Chiara, Jaroszynski, Jan, Förster, Tobias, Fuchs, Günther, Hühne, Ruben, Grinenko, Vadim, Schultz, Ludwig, Holzapfel, Bernhard
The film investigated grew phase-pure and highly textured with in-plane and out-of-plane full width at half maximum, FWHM, of = 0.74° and = 0.9°, Suppl. S1. The sample, however, does contain a large density of ab-planar defects, as revealed by transition electron microscope (TEM) images of focused ion beam (FIB) cuts near the microbridges, Fig. 1. These defects are presumably stacking faults (i.e. missing FeAs layers)20. The reason for this defect formation (also observed on technical substrates)21 is not fully understood. Possible reasons are a partial As loss during deposition22, and relaxation processes in combination with the Fe buffer layer23. Estimating the distance between these intergrowths leads to values varying between 5 and 10 nm. Between the planar defects, an orientation contrast is visible in TEM (inset Fig. 1b), i.e. the brighter crystallites are slightly rotated either around (010) (out-of-plane spread, ) or around (001) (in-plane spread, ) and enclosed by dislocation networks or small-angle GBs. Since the crystallites are sandwiched between planar defects, an in-plane misorientation is most likely. The out-of-plane misorientation, on the other hand, is visible as a slight tilt of the ab-planar defects with respect to each other, especially in the upper part of the sample. No globular or columnar precipitates were found.