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Manipulating superconducting phases via current-driven magnetic states in rare-earth-doped CaFe2As2


Inhomogeneous superconductivity in rare-earth (RE)-doped CaFe2As2 (Ca122) compounds leads to a novel state of matter in which the superconducting and magnetic states can be simultaneously controlled by using an electric current (I). Both La- and Ce-doped Ca122 single crystals show a very broad superconducting transition width (ΔTc) due to their non-bulk nature. Surprisingly, ΔTc becomes sharper or broader after an electric current larger than a threshold value (It) is applied, with a concomitant change in the normal-state magnetism. The sharpened (broadened) ΔTc is accompanied by a decrease (an increase) in the amplitude of the ferromagnetic signals. The sensitive changes in the superconductivity and magnetism that occur when an external current is applied are related to the inhomogeneous electronic states that originate from the Fe magnetic state and/or self-organized superconducting/magnetic composites in Ca122 compounds. These discoveries shed new light on the role of Fe in Fe-based superconductors and will provide new ideas for the design of novel superconducting devices.


The magnetic state of Fe coupled with interlayer As–As bonding has been intensively investigated as a crucial source to mediate Cooper pairs in Fe-based superconductors (FeSCs)1,2,3,4,5. The CaFe2As2 (Ca122) compound is an ideal candidate for studying the influence of the Fe magnetic state on FeSCs due to its extremely sensitive lattice parameters, which affect the Fe magnetic state1,2,4,5,6,7. Therefore, recent results for the Ca122 system have mostly focused on the relation between the Fe magnetic state and superconductivity because the interplay between magnetism and superconductivity is a key to understanding the mechanisms at play in FeSCs, as well as other unconventional superconductors, such as high-Tc cuprates and heavy fermion superconductors8,9.

Recently, a superconducting transition temperature (Tc) as high as 49 K was reported in rare-earth (RE: La, Ce, Pr, Nd)-doped Ca122 compounds10,11,12. However, the nature of the high-Tc is unclear due to the small volume fractions of the high-Tc phases and their inhomogeneities. High-Tc regions have been reported to be nucleated around doped RE clusters11,13. The results of scanning tunneling microscopy (STM) measurements for Pr-doped Ca122 indicate that the high-Tc regions around the Pr clusters are surrounded by weak- or non-SC regions11. Therefore, the supercurrent will mainly percolate along weak-SC or non-SC regions, leading to another SC transition at temperatures of approximately 10–20 K in RE-doped Ca122 compounds11,12,14.

The inhomogeneities or phase separations in a material often complicate the investigation of its intrinsic physical properties due to secondary effects. On the other hand, such complexity may bring about unexpected results, including disorder-induced superconductivity15,16. Complex phases in RE-doped Ca122 produce unpredicted results, such as a magnetic state that can be manipulated by using an electric current, which consequently affects the SC state. A superconducting current can be a good source for controlling the magnetic moment of nanoscale magnetic clusters as it is large enough to switch the magnetization. The effective magnetic field generated by the superconducting current affects the magnetic impurities/clusters; thus, the magnetic state of magnetic clusters with a large anisotropy can be manipulated17,18.

In this study, we report on manipulating the superconductivity of La- and Ce-doped Ca122 crystals by using the current-driven magnetic state. The SC percolation path, which is mainly composed of the low-Tc phase, is greatly modified, as is the magnetic state, when a current larger than a threshold value (It) is applied, but the high-Tc phase is not significantly changed. In addition, both the transport and magnetization measurements show aging effects. These novel behaviors can be attributed to the sensitive Fe magnetic state or to self-assembled superconducting/magnetic composites inside the crystals.

Materials and methods

Synthesis and characterization of rare-earth-doped CaFe2As2 single crystals

Undoped and rare-earth (RE)-doped CaFe2As2 single crystals were grown by using the FeAs self-flux method6,19; these crystals were easily cleaved into plate-like shapes with typical sizes of 4 × 2 × 0.25 mm3. Binary FeAs was synthesized by reacting Fe powder (99.998%, Alfa Aesar, Ward Hill, MA, USA) with an As lump (99.999%, Alfa Aesar) in a quartz tube that was heated at 500 °C for 10 h and then at 700 °C for 10 h in a box-type furnace. The elements Ca (granules 99.5%, Alfa Aesar), Ce, and La (both rods 99.9%, Alfa Aesar) as well as the FeAs precursor were placed into an alumina crucible at a ratio of (Ca, La, or Ce):FeAs = 1:4 and then sealed in an evacuated quartz tube. The ampoules were heated at 1180 °C for 24 h before being slowly cooled to 960 °C at a rate of 4 °C/h. The heater was then turned off at that temperature. The composition ratio of the synthesized CaFe2As2 compounds was investigated by using energy dispersive spectroscopy (EDS).

Measurements of electronic transport and magnetization

The electrical resistivity of the superconducting transition was measured by using the standard four-probe method with an applied current of 1 mA for all samples, with the measurements carried out in a physical property measurement system (PPMS 9T, Quantum Design). Small, pure, and RE-doped CaFe2As2 pieces that cleaved from the large samples, with a typical size of 1.2–2.7 × 0.3 × 0.1 mm3, were used to investigate the effects of the electric current on the materials. Pt wires and Epotek H20E silver epoxy were used to make good electrical contacts. Large electrical currents, up to 110 mA, were generated by using an Advantest R6142 unit under cryogenic conditions (5 and 10 K). The magnetization hysteresis (M − H) loops and temperature dependence of the magnetization (M) were measured by using a magnetic property measurement system (MPMS 5T, Quantum Design). To observe the effects of aging, we placed the samples inside desiccators at room temperature.


Figure 1 shows representative results for the superconducting (SC) and magnetic states in La- and Ce-doped Ca122 crystals that were tuned by application of an electric current. The SC transition widths (ΔTc) for both La- and Ce-doped Ca122 become sharper after a current larger than a threshold value (I > It) is applied to the samples, while the temperature for the onset of superconductivity (Tc,onset) does not change significantly, as shown in Fig. 1a, b. Simultaneously, the SC magnetization hysteresis (M − H) loop is prominently modified, which is accompanied by a large suppression in the ferromagnetic (FM) signal for La-doped Ca122, as shown in Fig. 1c. On the other hand, the slightly improved SC M − H loop observed for Ce-doped Ca122 can be ascribed to the relatively large magnetic moment of Ce at low temperatures, as shown in Fig. 1d (see also Figure S1 in SI)13. The exact origin of the FM phase in RE-doped Ca122 compounds is still unclear, but the defects at the Fe/As sites, such as As deficiency or Fe excess, have been suggested to be a source of the FM phase in FeSCs13,20,21,22.

Fig. 1: Effects of an electric current on rare-earth-doped CaFe2As2 compounds.

Temperature dependence of the in-plane resistivity (ρab) for a La-doped CaFe2As2 (LaCa122) and b Ce-doped CaFe2As2 (CeCa122), where ρab is normalized to the value at 46 K. For LaCa122, the zero-resistivity temperature is much improved after application of a large current of 100 mA, and aging effects clearly seen in the SC transition curves. CeCa122 also shows a behavior similar to that of LaCa122 following application of an electric current. Magnetization hysteresis (M − H) loops at 2 K for c LaCa122 and d CeCa122. Interestingly, for both samples, the M − H curves are also changed when a current is applied, indicating that the current-driven magnetic state affects the SC state for La- and Ce-doped Ca122. The weak-SC signals in the M − H loops for CeCa122 are most likely due to the strong Ce 4f magnetic moment

Aging effects are also observed in the temperature dependence of the in-plane electrical resistivity (ρab), as presented in Fig. 1a. In La-doped Ca122, ΔTc is sharpened by applying a current of 100 mA, but it becomes broader after 40 h. A similar behavior can also be observed in Ce-doped Ca122, as shown in Fig. 1b. These unexpected features in RE-doped Ca122 are more prominent in La-doped Ca122 than Ce-doped Ca122. Hence, we focus on La-doped Ca122 to investigate the origin of the changes in superconductivity and magnetism induced by applying a current in RE-doped Ca122 compounds.

Synthesized La-doped CaFe2As2 single crystals were easily cleaved into plate-like shapes with a typical size of 4 × 2 × 0.25 mm3. Homogeneous distributions for all of the elements in the crystals were confirmed by using energy dispersive spectroscopy (EDS) elemental mapping, as shown by the results presented in Fig. 2a. Nanoscale inhomogeneities have been suggested to be important for understanding the origin of the high-Tc phase in RE-doped Ca122 superconductors11,13. Figure 2b shows a magneto-optical (MO) image in the remanent state measured at 3.3, 10, and 20 K. The bright regions indicate strong-SC phases, and the dark regions show weak- or non-SC regions, indicating that the high-Tc phase is localized and rapidly suppressed with increasing temperature (see also Figure S2 in SI). Inhomogeneously distributed SC areas cannot be clearly distinguished by using EDS elemental mapping, which is particularly true for the La concentrations. The La concentrations of the rectangular region that has a magenta color and for regions 1 and 2 in Fig. 2b are 18.6% and 20.4%, respectively.

Fig. 2: EDS elemental mapping and superconducting magnetization properties for La-doped CaFe2As2.

a The EDS elemental mapping for LaCa122 shows that all of the elements in the crystal are homogeneously distributed. b However, the magneto-optical (MO) images show localized strong-SC regions. The MO images at 3.3, 10, and 20 K are measured in the remanent states, and the bright regions indicate strong-SC regions, where the high-Tc phase is dominant. The EDS results in regions 1 and 2 are not different despite the presence of very different SC states, implying that nanoscale inhomogeneity is important. c Zero-field-cooled (ZFC) and field-cooled (FC) dc magnetization (M) data for applied magnetic fields of 2, 5, 10, 20, 50, 100, and 200 Oe. Here, M(T) is normalized to the ZFC M value at 2 K. As shown in the inset, a clear separation between the ZFC and FC data at 2 Oe is observed at temperatures below 40 K, but the SC volume fraction at high temperatures is easily suppressed by small magnetic fields. d The magnetic field dependence of M at temperatures of 2, 5, 10, 15, and 20 K. The rapid suppression of M(H) at high temperatures implies a small volume fraction for the high-Tc phase in LaCa122

The strong temperature dependence and small volume fraction of the high-Tc phase are also observed in the magnetization (M) characteristics for the large size La-doped Ca122 crystal (4.19 × 2.09 × 0.25 mm3). The zero-field-cooled (ZFC) and field-cooled (FC) dc M for La-doped Ca122 in magnetic fields of 2, 5, 10, 20, 50, 100, and 200 Oe are shown in Fig. 2c. Here, M(T) is normalized to the ZFC M value at 2 K for comparison. The ZFC M(T) shows a rapid suppression even at small magnetic fields, although an irreversible line between the ZFC and FC data measured at 2 Oe is clearly observed at 40 K, as shown in the inset of Fig. 2c. Figure 2d shows the M − H curves at low fields for several representative temperatures: 2, 5, 10, 15, and 20 K. The large reduction in the Meissner signal caused by small magnetic fields also indicates a small volume fraction for the high-Tc phase. The diamagnetic signals in the Meissner state are significantly suppressed at temperatures higher than 10 K, which corresponds to the MO images shown in Fig. 2b. The large suppression of the SC diamagnetic signal by small perturbations, such as temperature and magnetic field perturbations, is consistent with a small SC volume fraction and/or with isolated SC domains with small sizes comparable to the penetration depth (λ)10,23.

We selected two types of small La-doped Ca122 pieces, LaCa122-A and LaCa122-B, which have SC states that can be tuned by using the current-driven magnetic state (see Figure S3 in SI). The La concentration estimated by EDS is 17.9% and 18.1% for LaCa122-A and LaCa122-B, respectively. Figure 3a, b plots the values for ρab(T) normalized to the value at 46 K, ρab(T)/ρab(46 K), for LaCa122-A and -B, respectively, on a semi-logarithmic scale. When a large electric current (110 mA) is applied, the SC transition for LaCa122-A becomes sharper, while it is broadened for LaCa122-B. Multiple SC phases with a low and high-Tc were clearly observed in LaCa122-B, which has been widely reported in RE-doped CaFe2As2 (see also Figure S4 in SI)10,11,12,13,14,24.

Fig. 3: Manipulation of the superconducting states for two pieces of La-doped CaFe2As2 by using an electric current.

Temperature dependence of the normalized in-plane resistivity (ρab) for a LaCa122-A and b LaCa122-B, where the resistivity is normalized to its value at 46 K. The SC transition width for LaCa122-A becomes narrower after application of a current, whereas LaCa122-B shows a broader SC transition compared to the pristine state. M − H loops at 2 and 50 K for c LaCa122-A and d LaCa122-B, indicating that the normal-state magnetism (50 K), which is changed by the electric current, strongly affects the shape of the SC M − H loops. In addition, the changes in the SC transition in the ρab(T) curves correspond to the modified M − H loops. For instance, suppression of the FM signal when a current is applied in LaCa122-A may indicate improved SC percolation paths because ferromagnetism is detrimental to superconductivity. The pictures in the insets of (c, d) simply describe the high-Tc regions and magnetic domains in each case based on the MO images and the M − H curves at 50 K. The red and blue arrows represent the “up” and “down” direction of the magnetization, respectively, while the length of the arrow corresponds to the magnitude of the magnetic domain

Figure 3c, d shows the M − H loops for LaCa122-A and -B at 2 K (T < Tc) and 50 K (T > Tc), where the top, middle, and bottom panels show the results for pristine crystals, crystals treated with a current of 110 mA, and aged single crystals. The pristine states for LaCa122-A and -B are different. LaCa122-A has a stronger FM signal compared to LaCa122-B, and the shape of the MH curves at 2 K is reversed after application of a large current of 110 mA. Interestingly, the M − H loops also show aging effects, but they do not return to their initial states even after a relatively long time (see Figure S5 in SI). Similarly, M − H curves have been reported in ferromagnet/superconductor systems, such as Co/Nb, with the shape of the MH curve controlled by the thickness of the SC or FM layer25,26. When the shapes of the MH curves at 2 K for LaCa122-A are considered, the states of pristine crystals, crystals treated with a current of 110 mA, and crystals aged for 20 days are found to contain a mixed phase of SC and FM, dominant SC state, and dominant FM phase, respectively25.


Current annealing has been used to rearrange the magnetic domains in Co-based amorphous ribbons through short-time heat treatment via Joule heating27,28. In the present study, the simultaneous changes in the SC and magnetic states due to the applied electric current are not a result of thermal annealing because aging effects are observed and the current was applied under cryogenic conditions.

Magnetic states tuned by using the electric current and time are clearly seen for both LaCa122-A and -B, as shown in Fig. 3c, d, respectively. Pristine LaCa122-A is in a mixed phase of superconductivity and ferromagnetism. When a larger current of 110 mA is applied, however, the FM signal is considerably suppressed; consequently, a typical SC M − H curve appears. In striking contrast, current-treated LaCa122-A recovers the large FM signal after storage for 20 days. On the other hand, LaCa122-B with a small FM signal in the pristine state shows the opposite behavior. When a current of 110 mA is applied, the FM signal increases significantly, followed by a rapid decrease over a period of 3 days, after which it hardly changes over the next 47 days (50-day observation period) (see Figures S5 and S6 in SI).

The M − H loops for all cases measured at 2 and 50 K are superimposed on top of a linear background, and Ms − H loops for the pure SC phase can be obtained, as shown in Fig. 4a, b, where Ms(2 K, H) = M(2 K, H) – M(50 K, H). The Ms − H loops for both LaCa122-A and -B present no significant changes in the high-Tc phase with changing current and/or time, implying that the current-driven magnetic state and simultaneous change in the SC state mostly emerge in weak- or non-SC regions. The temperature dependence of the magnetization (MT) also presents a rare change in the SC volume fraction following application of a current, as shown in Fig. 4c, d. Measurements for zero-field cooling (ZFC) were started from “0” gauss at 2 K; the negligible M values at “0” gauss (remanent fields) for all cases indicate that the MT results are reliable. The lack of change in the ZFC and MsH data suggests that the percolation paths surrounding the high-Tc phases are mainly affected by the applied electric current.

Fig. 4: Magnetization curves for the superconducting phase of La-doped CaFe2As2.

Ms − H loops when pure SC phases are considered for a LaCa122-A and b LaCa122-B, respectively, where Ms is the magnetization of the pure SC phase. Because the M − H loops at 2 and 50 K are superimposed as the FM background, as shown in Fig. 3c, d, the Ms – H loops can simply be calculated by using the relation Ms(2 K, H) = M(2 K, H) – M(50 K, H). The temperature dependence of the magnetization (MT) for c LaCa122-A and d LaCa122-B shows that the SC volume fraction barely changes with current and time. Zero-field cooling starts from zero gauss at 2 K for both samples, with the negligible M values at zero gauss (remanent fields) for all cases, indicating that the MT results are acceptable

In order to understand the different M – H behaviors for LaCa122-A and -B, we considered the simple pictorials, taking into account the current and relaxation time, as described in the insets of Fig. 3c, d. First, the size of the magnetic signals for La-doped Ca122 compounds is changed by applying an electric current, but the magnetic states return to their original states because the current-driven magnetic states are unstable. However, the observation that the M – H curves for the final states are not exactly the same as those for the initial states is probably strongly related to the relaxation time. For example, the observation that the FM signal is enhanced after 20 days for LaCa122-A in comparison with the initial FM signal is closely related to the relatively long relaxation time because the surroundings can be greatly influenced by the FM state during such a long relaxation time.

Current-driven magnetization switching is a central issue in the field of spintronics. We considered the threshold current density (Jt ~ 107–108 A/cm2) for magnetization switching in FM/SC or FM/AFM metallic composites29,30. In this study, large changes in the ΔTc and M – H curves were mostly observed at applied currents between 50 and 80 mA, as shown in Fig. 1b (see also Figure S7 in SI). If the percolation path has the shape of a long wire and Jt = 107–108 A/cm2, the estimated average radius ravg is a few hundred nanometers (see also Figure S8 in SI), which is close to the typical penetration depth (λab) for FeSCs31. Recently, the possibility of manipulating magnetic moments by using superconducting currents was suggested theoretically, considering the interplay between the spin–orbit interaction and a large transport current17,18. Persistent currents can be induced to circulate in FM impurities/islands with radii R < ξ (SC coherence length) on an s-wave 2D SC layer with large spin–orbit coupling (SOC), thereby generating large magnetic anisotropy. In addition, during electrical current flow in a superconductor, an effective magnetic field is generated, which acts on the FM impurities/islands; consequently, the orientations of the magnetic moments of the FM impurities/islands can be manipulated17,18.

The mechanism of the superconductivity in the Ca122 compounds is still unclear, but numerous results have suggested that an adequate Fe magnetic moment is crucial to mediating Cooper pairs in the compounds1,2,4. The interface superconductivity that emerges in undoped Ca122 has been reported to originate from the interface between the collapsed tetragonal (cT) and orthorhombic (O) phases or between the AFM antiphase domain boundaries32,33. For undoped and Co-doped Ca122, nuclear magnetic resonance (NMR) results suggest that FM fluctuations compete with superconductivity but can coexist with a stripe-type AFM phase34. The high-Tc phase in the RE-doped Ca122 is considered to be due to the interface associated with RE dopants13,22,35,36. Zhou et al. recently reported evidence for the interfacial nature of high-Tc superconductivity, where the interface is located between the pristine and reconstructed FeAs layers near RE dopants36. These complexities lead to unexpected results and allow manipulation of the SC and magnetic states by using an electric current, providing new insight into the role of Fe in Fe-based superconductors. We note that the switching of magnetism and superconductivity has also been reported by controlling the magnetic state of the Fe layer via the spin-polarized current in a FeSC Sr2VO3FeAs single crystal21.


We discovered that the current-driven magnetic state in rare-earth-doped CaFe2As2 can be used to tune the superconducting state. Simultaneous changes in the superconductivity and magnetism in response to an applied electric current can be ascribed to the unstable Fe magnetic state or self-assembled superconductor/magnet composites in the CaFe2As2 compounds. These results provide a new route for investigating the role of Fe in Fe-based superconductors. In addition, current-driven magnetization switching is expected to guide the design of new functional superconducting devices, such as superconductor-based on/off switch systems and superconducting spintronics37.


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We thank S. Park, J. H. Yun, and T. H. Park for helpful discussions. This work was supported by the National Research Foundation (NRF) of Korea grant funded by the Korean Ministry of Science, ICT and Planning (No. 2012R1A3A2048816). S.-G.J. was also supported by Basic Science Research Program through the National Research Foundation of Korea (NRF) funded by the Ministry of Education (NRF-2015R1D1A1A01060382). This work is partly supported by a Grant-in-Aid for Scientific Research from the Ministry of Education, Culture, Sports, Science and Technology, Japan.

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Jung, SG., Shin, S., Jang, H. et al. Manipulating superconducting phases via current-driven magnetic states in rare-earth-doped CaFe2As2. NPG Asia Mater 10, 156–162 (2018).

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