Superconductivity (SC) and ferromagnetism (FM) are mutually antagonistic collective phenomena in solids. Macroscopically, a superconductor expels magnetic fluxes from its interior (so-called Meissner state) below the superconducting critical temperature TSC. By contrast, a ferromagnet magnetizes itself (for a single magnetic domain) spontaneously below the ferromagnetic transition temperature TFM. Although SC and FM are incompatible in most cases, there is still the possibility of their coexistence which has become a long-standing (since the end of 1950s) interesting issue for scientists who work in the field of superconductivity. Since late of 1970s, a few material systems called "magnetic superconductors" have been considered as the candidates of ferromagnetic superconductors (FMSC), however, bulk SC and full FM were rarely observed simultaneously.
One of the iron-based superconductors, P-doped EuFe2As2, indeed shows evidence of both SC and FM. However, the specific-heat jump at TSC (which demonstrates bulk SC) is not obvious. Furthermore, the details of ferromagnetism are still in debate. Very recently, researchers in Zhejiang University succeeded in replacing every alternate Eu layer by a non-magnetic Rb/Cs layer, yielding twin compounds RbEuFe4As4 and CsEuFe4As4 (see the upper-right panel of Fig. 1). It is in the twin materials that both bulk superconductivity and full ferromagnetism are realized simultaneously.
Fig. 1(a) and 1(b) are the temperature dependence of direct-current magnetic susceptibility and specific heat, respectively, for one of the sister compound CsEuFe4As4. The two transitions at TFM = 15.5 K and TSC =35.2 K can be clearly seen. In general, the dc magnetic susceptibility at a small magnetic field is a measure of superconducting volume fraction. One sees that the superconducting magnetic-shielding fraction, represented by the zero-field cooling data, is almost 100 % at the lowest temperature. This indicates bulk SC, which is further confirmed by the obvious specific-heat jump at TSC. On the other hand, surprisingly, the field-cooling data lose the diamagnetism below TFM, which is due to the Eu-spin ferromagnetic ordering that is demonstrated by the field-dependent magnetization shown in Fig. 1(d). Note that SC persists at the low temperature region, as seen by the initial magnetization (see the inset) as well as the non-convergence of magnetization at high fields at 2 K. The researchers also notice that there is no specific-heat jump (only a kink instead) at TFM. They point out that it is a rare third-order ferromagnetic transition that has not been experimentally found up to date.
Temperature dependence of direct-current magnetic susceptibility, which is a measure of superconducting volume fraction, for CsEuFe4As4. (b) Temperature dependence of the specific-heat capacity, confirming bulk nature of the two transitions at 15.5 and 35.2 K. (c) Crystal structure of (Rb/Cs)EuFe4As4 consisting of alternate Eu, FeAs, Rb/Cs and FeAs layers along the c axis. (b) Field-dependent magnetization curves indicating coexistence of superconductivity and ferromagnetism in CsEuFe4As4. Credit: ©Science China Press
The observation of robust SC and FM in (Rb/Cs)EuFe4As4 strongly suggests that the expected mutual suppression between SC and FM can be minimized via a certain mechanism, which may shed light on the mechanism of iron-based SC, as the team leader Guang-Han Cao said. These authors also address the intriguing issue of how SC can coexist with FM. The details can be found in the reference articles below.
source: Science China Press