Controlling unconventional superconductivity in artificially engineered f-electron Kondo superlattices

Unconventional superconductivity and magnetism are intertwined on a microscopic level in a wide class of materials, including high-T (c) cuprates, iron pnictides, and heavy-fermion compounds. Interactions between superconducting electrons and bosonic fluctuations at the interface between adjacent layers in heterostructures provide a new approach to this most fundamental and hotly debated subject. We have been able to use a recent state-of-the-art molecular-beam-epitaxy technique to fabricate superlattices consisting of different heavy-fermion compounds with atomic thickness. These Kondo superlattices provide a unique opportunity to study the mutual interaction between unconventional superconductivity and magnetic order through the atomic interface. Here, we design and fabricate hybrid Kondo superlattices consisting of alternating layers of superconducting CeCoIn5 with d-wave pairing symmetry and nonmagnetic metal YbCoIn5 or antiferromagnetic heavy fermion metals such as CeRhIn5 and CeIn3. In these Kondo superlattices, superconducting heavy electrons are confined within the two-dimensional CeCoIn5 block layers and interact with neighboring nonmagnetic or magnetic layers through the interface. Superconductivity is strongly influenced by local inversion symmetry breaking at the interface in CeCoIn5/YbCoIn5 superlattices. The superconducting and antiferromagnetic states coexist in spatially separated layers in CeCoIn5/CeRhIn5 and CeCoIn5/CeIn3 superlattices, but their mutual coupling via the interface significantly modifies the superconducting and magnetic properties. The fabrication of a wide variety of hybrid superlattices paves a new way to study the relationship between unconventional superconductivity and magnetism in strongly correlated materials.

Automated summary

Unconventional superconductivity and magnetism are studied through atomic interface in hybrid superlattices. Different Kondo superlattices with heavy-fermion compounds are fabricated to investigate the mutual interaction between superconductivity and magnetic order. The coexistence and coupling of superconducting and antiferromagnetic states in spatially separated layers are observed, providing new insights into the relationship between unconventional superconductivity and magnetism.