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Evidence of spontaneous vortex ground state in an iron-based ferromagnetic superconductor

npj Quantum Materialsvolume 2, Article number: 50 (2017) | Download Citation


Spontaneous vortex phase (SVP) is an exotic quantum matter in which quantized superconducting vortices form in the absence of external magnetic field. Although being predicted theoretically nearly 40 years ago, its rigorous experimental verification still appears to be lacking. Here we present low-field magnetic measurements on single crystals of the iron-based ferromagnetic superconductor Eu(Fe0.91Rh0.09)2As2 which undergoes a superconducting transition at T sc = 19.6 K followed by a magnetic transition at T m = 16.8 K. We observe a characteristic first-order transition from a Meissner state within T m < T < T sc to an SVP below T m, under a magnetic field approaching zero. Additional isothermal magnetization and ac magnetic susceptibility measurements at \(T \ll {T_{{\rm{sc}}}}\) confirm that the system is intrinsically in a spontaneous-vortex ground state. The unambiguous demonstration of SVP in the title material lays a solid foundation for future imaging and spectroscopic studies on this intriguing quantum matter.


Spontaneous vortex (SV) phase, originally predicted by theoretical investigations,1,2,3,4 is an exotic quantum matter in which superconducting vortices form in the absence of external magnetic field, which can be qualitatively different from those induced by an external field.5 While SV state was also predicted to be present in the pseudogap phase of cuprates due to local spins of the paramagnetic phase,6 self-induced vortices are mostly generated by an internal magnetic field, H int = 4πM, due to the spontaneous magnetization M. This means that the prerequisite of realization of an SV state is that superconductivity (SC) coexists with magnetic order, the latter of which at least gives rise to a ferromagnetic component. Such a coexistence is rare because of the antagonism between SC and ferromagnetism (FM). Additional requirements for observation of the SV phenomenon include yet, are not limited to, (1) the SC alone (a hypothetical nonmagnetic analog without any internal field) belongs to the second type with intrinsic lower and upper critical fields (\(H_{{\rm{c1}}}^{\rm{*}}\) and \(H_{{\rm{c2}}}^*\)); and (2) the internal magnetic field strength lies in the range of \(H_{{\rm{c1}}}^{\rm{*}} < {H_{{\rm{int}}}} < H_{{\rm{c2}}}^{\rm{*}}\).

Materials that bear both SC and FM generally have distinct superconducting critical temperature T sc and magnetic transition temperature T m. If T sc > T m, they are traditionally called “ferromagnetic superconductors” (FSCs).7 Otherwise, the terminology “superconducting ferromagnets” (SFMs) are often employed.8 According to this classification and, with the consideration of the relative strength between \(H_{{\rm{c1}}}^*\) and H int, possible existence of an SV phase is schematically depicted in Fig. 1 for an extremely type-II superconductor in which \(H_{{\rm{c2}}}^*(0) \gg H_{{\rm{c1}}}^*(0)\) holds. In the cases of \(H_{\rm{int}}(0) >H_{{\rm{c1}}}^*(0)\), as shown in the panels (a) and (b), the SV phase can be realized as a ground state. If \({H_{{\rm{int}}}}(0) < H_{{\rm{c1}}}^*(0)\), however, possible SV phase appears only at finite temperatures above zero, as is seen in the panels (c) and (d).

Fig. 1
Fig. 1

Classification of magnetic superconductors that may host the spontaneous vortex (SV) phase. The left panels show superconducting ferromagnets (SFMs), while the right panels describe ferromagnetic superconductors (FSCs). a, b, \({H_{{\rm{int}}}}(0) >H_{{\rm{c1}}}^*(0)\); c, d, \(H_{{\rm{c1}}}^*(0) > {H_{{\rm{int}}}}(0)\). See the text for the definitions of H int and \(H_{{\rm{c1}}}^*\). M and M’ denote Meissner states, and NF stands for a non-superconducting ferromagnetic state. Here the upper critical fields, \(H_{{\rm{c2}}}^*(0)\), are assumed to be much larger than \(H_{{\rm{c1}}}^*(0)\) and H int(0)

There have been a few systems that may host an SV state. In the SFMs, Ru-containing cuprates8, 9 and U-based UCoGe,10, 11 which can be categorized into scenarios (c) and (a) in Fig. 1, respectively, were argued to have an SV state on the basis of magnetic measurements. For FSCs, however, evidence of SV phase from bulk magnetic measurements is still lacking, although theoretical12 and experimental13 investigations suggested an SV state in the weakly ferromagnetic superconductor ErNi2B2C. In fact, rigorous demonstration of a bulk SV phase by magnetic measurements is challenging primarily because an external field, which by itself induces vortices and, possibly changes the magnetic state, has to be applied. In general, one needs to demonstrate the existence of SV state as the external field approaches zero, which requires a sufficiently high measurement precision. This issue becomes more stringent in the cases above where the internal field generated by the small ferromagnetic component is very weak (e.g., the spontaneous magnetization of UCoGe is ~0.04 μ B/U, corresponding to ~30 Oe field). Furthermore, the magnetic measurements always encounter the interferences of ferromagnetic domains.11

As was first pointed out by Ng and Varma,12 nevertheless, the SV phase can be manifested by the unique first-order phase transition from a Meissner state to an SV phase, which can be possibly seen in cases of Fig. 1b–d. The first-order transition is expected to accompany with a thermal hysteresis that may be easily captured experimentally. Indeed, a thermal hysteresis in magnetic susceptibility was observed in the SFM RuSr2GdCu2O8, which is interpreted as a characteristic of SV state.9 However, the observed phenomenon was sample dependent and, the polycrystalline samples employed expose the flaw: the magnetic-flux pinning by grain boundaries might also account for the phenomenon.14 Therefore, detection of a Meissner-to-SV transition should be done at least using single crystalline samples.

In this context, the recently discovered FSCs in doped EuFe2As2 systems,15 which show a remarkable coexistence of SC and strong FM in a broad temperature range (note that the temperature window for probing an SV phase is mostly below 2.5 K in previous systems10, 11, 13), provide a desirable platform to look into the SV state. Through either P doping at As site16 or transition-metal (such as Ru, Co, Rh, and Ir) doping at Fe site,17,18,19,20,21 SC can be induced with a T sc between 20 and 30 K, and the Eu2+ spins (with S = 7/2) become ferromagnetically ordered at T m a few kelvins lower. Although there were debates on details of the magnetic order,15, 22,23,24,25,26 recent x-ray resonant magnetic scattering and neutron diffraction studies27,28,29,30 show that the Eu2+ spins always align ferromagnetically along the c axis with an ordered moment of about 7 μ B. The ferromagnetic ordering gives rise to a large spontaneous magnetization that generates an internal field of H int ≈ 9000 Oe along the c axis, well above the expected \(H_{{\rm{c1}}}^*(0)\) of ~150 Oe.31 Additional important advantage of the iron-based FSC is that the high-quality single crystals are easily accessible.17,18,19,20 Note that the internal-field direction induces superconducting vortices within the FeAs layers. As such, the magnetic measurements can be limited to those under external fields parallel to the c axis, which greatly simplifies the interpretation of the measurement result.


We employed an optimally Rh-doped single crystal of Eu(Fe0.91Rh0.09)2As2 with T sc = 19.6 K, T m = 16.8 K, and a saturation magnetization M sat = 6.5 μ B/Eu.19 The saturation magnetization is close to gS = 7.0, which tells that the Eu2+ spins align ferromagnetically, similar to other Eu-containing FSC,27,28,29,30 as shown in Fig. 2a. The superconducting transition of in-plane resistivity is plotted in Fig. 2b. The relatively broadened resistive transition seems to be related to the Eu-spin exchange field which suppresses the T sc value (note that T sc is 21.9 K for the optimally Rh-doped SrFe2As2 32). Below T m, the ferromagnetic ordering leads to a re-appearance of resistivity [Fig. 2b]. The maximum of the reentrant resistivity is only 1/40 the normal-state value, indicating that it is by no means a recovery of the normal state, instead, it is associated with the SV formation. Specifically speaking, the revival of resistivity comes from the vortex flow in an SV liquid state. With decreasing temperature, \(H_{{\rm{irr}}}^*\) surpasses H int, as shown in Fig. 2c, making the vortices frozen, hence zero-resistance state is achieved below ~8 K. Note that the SV scenario naturally explains various resistivity states below T m,15,16,17,18,19,20,21 some of which show absence of the resistivity reentrance,20, 23,24,25 depending on the doping levels and physical pressures. As is seen, the absence of reentrant behaviour is more easily to be observed in P-doped EuFe2As2 23,24,25 where T sc is significantly higher than T m such that \(H_{{\rm{irr}}}^* > {H_{{\rm{int}}}}\) is satisfied.

Fig. 2
Fig. 2

Characteristic of the ferromagnetic superconductor Eu(Fe0.91Rh0.09)2As2 in relation with a spontaneous vortex phase. a The crystal and magnetic structure. b The superconducting resistive transition at T sc, followed by a resistivity revival below T m (note the logarithmic scale for resistivity). c Schematic H − T diagram showing the internal field H int (solid blue line), in comparison with the hypothetical irreversible field \(H_{{\rm{irr}}}^*\) (assuming H int = 0) as well as the hypothetical lower and upper critical fields, \(H_{{\rm{c1}}}^*\) and \(H_{{\rm{c2}}}^*\). SV and M denote the spontaneous-vortex phase and the Meissner state, respectively. d Temperature dependence of the dc magnetic susceptibility measured while heating up, with both field-cooled (FC) and zero-field-cooled (ZFC) histories. The demagnetization effect has been taken into account

The dc magnetic susceptibility shows a kink for the field-cooling (FC) protocol and a peak for the zero-field-cooling (ZFC) protocol at T m, as shown in Fig. 2d. This can be interpreted as the formation of antiparallel ferromagnetic domains.20 Because of the proximity between SC and FM, the superconducting transition is not distinctly seen in the dc magnetic measurements (although it was directly observable at very low fields20). Nevertheless, \(\chi _c^{{\rm{FC}}}\) and \(\chi _c^{{\rm{ZFC}}}\) bifurcate just at T sc, owing to the magnetic-flux pinning effect. The superconducting magnetic shielding effect below T sc is confirmed by the following ac susceptibility measurement.

Since the internal field generated by the Eu2+-spin FM is much stronger than the expected \(H_{{\rm{c1}}}^*(0)\), as described above, the SV state is stabilized once the FM develops. On the other hand, the internal field vanishes for T > T m, hence it is in a Meissner state at zero external field in the temperature range T m < T < T sc, as shown in Fig. 2c. Therefore, a transition from the Meissner state to the SV phase definitely occurs as temperature decreases. During the transition, the spontaneous vortices (SVs) suddenly penetrate the crystal’s interior, which gives rise to a unique first-order transition with a magnetization discontinuity at around T m for the ideal case with single magnetic domain. In the case of a large sample with multi-domains, nevertheless, a “continuous” change with an obvious thermal hysteresis is expected because of the latent heat in the first-order transition. The possible thermal hysteresis from the domain-wall depinning can be avoided by employing magnetic fields that are much lower than the coercive field (~200 Oe20).

As shown in Fig. 3a, the FC magnetization data indeed show a thermal hysteresis in the vicinity of T m, demonstrating the nature of first-order transition. In the cooling process, Meissner state is first stabilized, which expectedly gives a lower value of magnetization because of Meissner effect (For the SFM RuSr2GdCu2O8 where the SV state is stabilized at the high-temperature side, in contrast, the FCC curve has a larger magnetic susceptibility.9). On the other hand, In the FCH process from T m to T sc, some “superheated” spontaneous vortices survive accompanying with the “polarization” of Eu spins until T sc, which gives rise to a higher magnetization value. The hysteresis regime extends up to T sc, suggesting that the SV state could be stabilized by the Eu-spin ferromagnetic fluctuations. The magnetization differences of the cooling and warming data, ΔM c  = M FCC − M FCH, are plotted in Fig. 3b. One sees that ΔM c drops at T sc, and it increases rapidly till T m. The maximum of \(\left| {\Delta {M_c}} \right|\) increases with the applied field. Figure 3c plots the ΔM c value at T m \(\left( {\Delta M_c^{{T_{\rm{m}}}}} \right)\) as a function of external field. Remarkably, \(\Delta M_c^{{T_{\rm{m}}}}\) is exactly proportional to the field (note that the field accuracy is self-checked by the field-dependent magnetization at 30 K shown on the right axis). In fact, ΔM c can be fully scaled with the applied field, as shown in Fig. 3d. Here we emphasize that the thermal hysteresis is always observable, even at very low magnetic fields, for different pieces of the sample. By contrast, no thermal hysteresis is seen in overdoped samples where only a ferromagnetic transition takes place. This further rules out the possibility that the domain-wall depinning could be responsible for the large thermal hysteresis.

Fig. 3
Fig. 3

Evidence of the first-order transition from a Meissner state to a spontaneous vortex phase with decreasing temperature in Eu(Fe0.91Rh0.09)2As2 crystals. a Field-cooling magnetization (M c ) on both heating (FCH) and cooling (FCC) processes under magnetic fields along the c axis. The rectangles with arrows schematically represent different statuses of sample in the presence of external field (multi-domains and pinned fluxes are not shown). See the text for the inserted cartoon pictures b The magnetization difference ΔM c between the FCH and FCC data. c ΔM c at T m (left axis) and M c at 30 K (right axis) as functions of the applied field. d ΔM c /H vs. T in an expanded temperature range

The magnetization difference at T m, \(\Delta M_c^{{T_{\rm{m}}}}\), can be understood as follows. For \(T \to T_{\rm{m}}^ -\) (FCH data), the SV state dominates. The magnetic contribution of SVs is always accompanied with the ferromagnetic domains. Owing to the existence of multi-domain, the magnetic fluxes from SVs cancels out at zero field,11 and with applying fields, the moment appears to be proportional to the external field. When temperature exceeds T m, SVs still survive (superheating effect) although the FM vanishes. Namely, the external magnetic field penetrates the sample where superconducting layers contain SVs and, the Eu2+ spins are basically in the Curie-Weiss paramagnetic state [see the two right-side cartoons in Fig. 3a]. Thus, the FCH magnetic susceptibility at T m is approximately equal to the Curie-Weiss paramagnetic susceptibility, i.e., \(\chi _{{\rm{FCH}}}^{{T_{\rm{m}}}} \approx \chi _{{\rm{CW}}}^{{T_{\rm{m}}}}\). For \(T \to T_{\rm{m}}^ +\) (FCC data), on the other hand, the Meissner state dominates, which gives an additional diamagnetic susceptibility of \(\chi _{{\rm{sc}}}^{{T_{\rm{m}}}}\), yielding \(\chi _{{\rm{FCC}}}^{{T_{\rm{m}}}} \approx \chi _{{\rm{CW}}}^{{T_{\rm{m}}}} + \chi _{{\rm{sc}}}^{{T_{\rm{m}}}}\). Thus we have, \(\Delta \chi _c^{{T_{\rm{m}}}} = \chi _{{\rm{FCC}}}^{{T_{\rm{m}}}} - \chi _{{\rm{FCH}}}^{{T_{\rm{m}}}} \approx \chi _{{\rm{sc}}}^{{T_{\rm{m}}}}\), which simply reflects the superconducting magnetic expulsion (see the cartoon pictures). The Meissner volume fraction can be estimated to be, \(4\pi \Delta M_c^{{T_{\rm{m}}}}{\rm{/}}H \approx 15\%\), which is not surprising because of the unavoidable flux pinning effect.

Above we demonstrate the first-order transition from a Meissner state to an SV phase with decreasing temperature. This suggests that the SV phase represents the ground state in Eu(Fe0.91Rh0.09)2As2. If this is the case, one expects that the lower critical field at zero temperature, H c1(0), would be zero.10,11,12 Figure 4 shows the low-temperature isothermal magnetization, M c (H), for Eu(Fe0.91Rh0.09)2As2, in comparison with that of the nonmagnetic superconducting analog, Ba(Fe0.9Co0.1)2As2. The latter shows an essentially linear M c (H) since the applied fields are much lower than the H c1(0). In contrast, Eu(Fe0.91Rh0.09)2As2 displays a non-linear virgin M c (H) curve and an obvious magnetic hysteresis loop. This means that, in addition to the superconducting magnetic shielding effect, the external field always penetrates the sample, even if the field is around zero. In other words, Eu(Fe0.91Rh0.09)2As2 is intrinsically in a mixed state below T m.

Fig. 4
Fig. 4

Isothermal magnetization curves at 1.90 K under magnetic fields parallel to the c axis for Eu(Fe0.91Rh0.09)2As2 and Ba(Fe0.9Co0.1)2As2

Another piece of evidence for the mixed state at zero field comes from the ac magnetic susceptibility measurements. As shown in the main panel of Fig. 5, one can clearly distinguish T sc and T m from the real part of the ac susceptibility, χ′. The magnetic shielding effect below T sc is much more obvious than that of the dc magnetic measurement above. The imaginary part of the susceptibility, χ″, which is sensitive to dissipations, shows two sharp peaks below T sc and T m, respectively. An additional large broad peak appears below the re-entrant spin-glass temperature T sg ≈ 13.5 K.19 Note that this χ″ peak may also be contributed from the SV liquid-to-solid transition.

Fig. 5
Fig. 5

Temperature dependence of real and imaginary parts (χ′ and χ″) of ac susceptibility at zero dc magnetic field. The amplitude of the driving ac magnetic field (along the c axis) is, H ac = 2.5 Oe. The demagnetization effect has been taken into consideration. T sc, T m, and T sg are the superconducting, ferromagnetic, and spin-glass transition temperatures, respectively. The inset plots the imaginary part of the ac magnetization at 1.9 K as a function of H ac. The solid line is the linear fit

Remarkably, the χ″ value at the lowest temperature of 1.90 K in our measurements remains considerably high at the driving field H ac = 2.5 Oe, verifying that it is in a mixed state. To examine if there is a lower limit of the ac field, we performed a field-dependent ac magnetization measurement, the imaginary part \(\left( {m_c^{\prime\prime}} \right)\) of which is shown in the inset of Fig. 5. One sees that \({m_c^{\prime\prime}}\) is exactly proportional to H ac. According to the critical-state model,33 \({m_c^{\prime\prime}}\) will be zero for H ac < H c1; while \({m_c^{\prime\prime}}\) = β(H ac − H c1)2/H ac (β is the sample’s geometrical factor) for H ac > H c1. Both the non-zero \({m_c^{\prime\prime}}\) and the linearity of \({m_c^{\prime\prime}}\)(H ac) through the origin indicate that H c1 must be zero. Similar observation is seen in the SFM UCoGe.11


The above results allow us to arrive at the following picture for the Eu(Fe0.91Rh0.09)2As2 FSC in the absence of external magnetic field. At T > T sc, the [(Fe,Rh)2As2]2− and Eu2+ layers are Pauli paramagnetic and Curie-Weiss paramagnetic, respectively. When cooled below T sc, the [(Fe,Rh)2As2]2− layers become superconducting, showing a Meissner state coexisting with the Curie-Weiss paramagnetism of Eu2+ spins. With further decreasing temperature to below T m, the Eu2+ spins are ferromagnetic ordered along the c axis, which generates an internal field far above the expected \(H_{{\rm{c1}}}^*(0)\). Superconducting vortices then form spontaneously in the [(Fe,Rh)2As2]2− layers. In the temperature range of 8 K < T < T m, the SVs are mobile, which leads to the revival of resistance. The subsequent solidification of the SVs below 8 K gives rise to the zero-resistance state. Therefore, the ground state is an SV solid, which reconciles SC and FM in Eu(Fe0.91Rh0.09)2As2.

Finally we note that, apart from the formation of the SV phase, an alternative that allows to reconcile the SC and FM is the so-called Fulde-Ferrell-Larkin-Ovchinnikov (FFLO) state characterized by a spatial modulation of the superconducting order parameter.34, 35 Nevertheless, in general, realization of an FFLO state at zero external field needs more rigorous conditions. Among them are Pauli-limited \(H_{{\rm{c2}}}^ \bot\) (for H ab) with a large Maki parameter and clean limit for the SC, which cannot be satisfied in the present system. The \(H_{{\rm{c2}}}^ \bot (T)\) curve in Eu(Fe0.91Rh0.09)2As2 keeps linear down to 0.2T sc,19 indicating that the orbital-limiting effect dominates. Besides, the large residual resistivity (~60 μΩ cm) as well as the small residual resistivity ratio (RRR = 2.6)19 suggests a dirty limit. Both properties actually favor the SV scenario. Nevertheless, here we note that the recently discovered 1144-type FSC36, 37 could be the candidate for an FFLO state, because their nonmagnetic analog, CaKFe4As4, indeed shows a large Maki parameter together with a clean limit for the SC.38

In summary, we have studied the low-field magnetic properties for the iron-based ferromagnetic superconductor Eu(Fe0.91Rh0.09)2As2. We observed a remarkable thermal hysteresis around the ferromagnetic transition in the superconducting state, even under a vanishingly small field, demonstrating the unique first-order transition from a Meissner state to an SV phase. The SV ground state is further corroborated by the non-linear virgin dc magnetization as well as the non-zero imaginary part of ac magnetic susceptibility under extremely low external fields at \(T \ll {T_{{\rm{sc}}}}\). The unambiguous demonstration of the SV ground state in the iron-based FSC lays a solid foundation for future studies. For example, it is of great interest to see whether the SV solid behaves like a glassy or a lattice state. The imaging observations such as magnetic-force microscopy as well as the small-angle neutron scattering technique may help to clarify this interesting issue.


Crystal growth

High-quality crystals of Eu(Fe0.91Rh0.09)2As2 were grown by a self-flux method.19, 20 First, mixtures of Eu (99.9%), Fe (99.998%), Rh (99.9%), and As (99.999%) powders in a molar ratio of Eu:Fe:Rh:As = 1:4.4:0.6:5 reacted at 973 K for 24 h in a sealed evacuated quartz ampoule. The precursor was ground, and then was loaded into an alumina crucible. The crucible was sealed in a stainless steel tube by arc welding under an atmosphere of argon. The assembly was subsequently heated up to 1573 K and, holding for 5 h, in a muffle furnace with the flow of argon gas. The crystal growth took place during the slow cooling down to 1223 K at the rate of 4 K/h. Large crystals with typical size of 3 × 3 × 0.5 mm3 were harvested.

Structural and compositional characterizations

We checked the as-grown crystal flakes by x-ray diffraction using a PANAlytical x-ray diffractometer (using Cu K α1 monochromatic radiation) at room temperature. All the crystals show only (00l) reflections with even l values, similar to the previous report.19 The c axis is then determined to be 12.016(1) Å. The crystal structure is analogous to EuFe2As2 (c = 12.136 Å),39 yet it consists of superconducting [(Fe,Rh)2As2]2− layers separated by magnetic Eu2+ ions. The full width at half maximum (FWHM) of the reflection peaks is typically 2θ = 0.06°, verifying the high quality of the crystals. The real composition of the crystal was determined by energy dispersive x-ray spectroscopy, which gives the chemical formula of Eu(Fe0.91Rh0.09)2As2.

Physical properties

The electrical and magnetic properties of the Eu(Fe0.91Rh0.09)2As2 crystals were reported previously19 which demonstrate a superconducting transition at T sc = 19.6 K, followed by a ferromagnetic transition at T m = 16.8 K. The isothermal magnetization loops below T m show characteristic features for both FM and SC. The saturation magnetization achieves M sat = 6.5 μ B/Eu, confirming that the Eu spins align ferromagnetically.

Low-field magnetic measurements

We selected a free-standing crystal for all the measurements in this paper. Magnetic measurements were carried out on a Quantum Design Magnetic Property Measurement System. The residual field in the superconducting magnet, after being removed by a degaussing procedure prior to the measurements, is less than ±0.05 Oe. The crystal was carefully mounted into the sample holder with the applied field perpendicular to the crystal plate, such that the external field is either parallel or antiparallel to the internal field. The FC data were collected in both heating and cooling procedures. In the ac susceptibility measurement, the frequency was set to 1.0 Hz. The demagnetization effect is taken into account on the basis of the sample’s geometry in respect to the field direction.

Data availability

The data that support the findings of this study are available from the corresponding author (G.H.C.) upon reasonable request.

Additional information

Publisher's note: Springer Nature remains neutral with regard to jurisdictional claims in published maps and institutional affiliations.


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This work is supported by the National Science Foundation of China (Nos.11474252 and 11504329), the National Key Research and Development Program of China (No.2016YFA0300202), and the Fundamental Research Funds for the Central Universities of China.

Author information


  1. Department of Physics, Zhejiang University, Hangzhou, 310027, P. R. China

    • Wen-He Jiao
    • , Qian Tao
    • , Yi Liu
    •  & Guang-Han Cao
  2. Department of Physics, Zhejiang University of Science and Technology, Hangzhou, 310023, P. R. China

    • Wen-He Jiao
  3. Institute for Natural Sciences, Westlake Institute for Advanced Study, Hangzhou, 310013, P. R. China

    • Zhi Ren
  4. State Key Lab of Silicon Materials, Zhejiang University, Hangzhou, 310027, P. R. China

    • Guang-Han Cao
  5. Collaborative Innovation Centre of Advanced Microstructures, Nanjing, 210093, P. R. China

    • Guang-Han Cao


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W.H.J. and Y.L. grew and characterized the crystals. W.H.J. and Q.T. performed the magnetic measurements. W.H.J., Z.R. and G.H.C. analyzed and interpreted the data, and wrote the paper. This work was coordinated and designed by G.H.C.

Competing interests

The authors declare no competing financial interests.

Corresponding author

Correspondence to Guang-Han Cao.

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