The attractive/repulsive relationship between superconductivity and magnetic ordering has fascinated the condensed matter physics community for a century. In the early days, magnetic impurities doped into a superconductor were found to quickly suppress superconductivity. Later, a variety of systems, such as cuprates, heavy fermions, and Fe pnictides, showed superconductivity in a narrow region near the border to antiferromagnetism (AFM) as a function of pressure or doping. However, the coexistence of superconductivity and ferromagnetic (FM) or AFM ordering is found in a few compounds [RRh 4 B 4 (R = Nd, Sm, Tm, Er), R′Mo 6 X 8 (R′ = Tb, Dy, Er, Ho, and X = S, Se), UMGe (M = Ge, Rh, Co), CeCoIn 5 , EuFe 2 (As 1−x P x ) 2 , etc.], providing evidence for their compatibility. Here, we present a third situation, where superconductivity coexists with FM and near the border of AFM in Fe 1−x Pd x Te. The doping of Pd for Fe gradually suppresses the first-order AFM ordering at temperature T N/S , and turns into short-range AFM correlation with a characteristic peak in magnetic susceptibility at T ′ N . Superconductivity sets in when T ′ N reaches zero. However, there is a gigantic ferromagnetic dome imposed in the superconducting-AFM (short-range) cross-over regime. Such a system is ideal for studying the interplay between superconductivity and two types of magnetic (FM and AFM) interactions.
Since the first discovery of superconductivity (SC) a century ago, the effects of magnetic impurities and the possibility of magnetic ordering in superconductors has been a central topic of condensed matter physics. Due to strong spin scattering (1, 2), it has generally been believed that the conduction electrons cannot be both magnetically ordered and superconducting. Even though it is thought that Cooper pairs in cuprates, heavy fermions, and Fe-based compounds are mediated by spin fluctuations (3-5), SC generally occurs after suppressing the magnetic ordering either through chemical doping or the application of hydrostatic pressure (6-10). However, there is growing evidence for the coexistence of superconductivity with either ferromagnetic (FM) (11)(12)(13)(14)(15)(16)(17)(18)(19)(20) or antiferromagnetic (AFM) ordering (21-24). With the decrease of temperature (T), some of these systems show magnetic ordering before the superconducting transition (T c ) (14-17, 20), some are ordered in a reversed sequence (11-13, 18, 19, 22), some have the two orderings occur concomitantly (22,25), and some show reentrant superconductivity (partially) overlapping with a magnetically ordered phase (11)(12)(13)26). Despite extensive investigations of interaction between SC and magnetic moments, there is so far no unified theory for the coexistence of SC and magnetism. With the lack of theoretic guidance, the existing experimental findings lead to two schools of thought: one is that both orders result from the same conduction electrons as evidenced by their synchronized magnetic and superconducting orders (22), and the other is that there are two s...