{ "id": "2107.06361", "version": "v1", "published": "2021-07-13T19:57:40.000Z", "updated": "2021-07-13T19:57:40.000Z", "title": "Quantum spins and hybridization in artificially-constructed chains of magnetic adatoms on a superconductor", "authors": [ "Eva Liebhaber", "Lisa M. Rütten", "Gaël Reecht", "Jacob F. Steiner", "Sebastian Rohlf", "Kai Rossnagel", "Felix von Oppen", "Katharina J. Franke" ], "categories": [ "cond-mat.mes-hall", "cond-mat.str-el", "cond-mat.supr-con" ], "abstract": "Magnetic adatom chains on surfaces constitute fascinating quantum spin systems. Superconducting substrates suppress interactions with bulk electronic excitations but couple the adatom spins to a chain of subgap Yu-Shiba-Rusinov (YSR) quasiparticles. Using a scanning tunneling microscope, we investigate such correlated spin-fermion systems by constructing Fe chains adatom by adatom on superconducting NbSe$_2$. The adatoms couple entirely via the substrate, retaining their quantum spin nature. In dimers, we observe that the deepest YSR state undergoes a quantum phase transition due to Ruderman-Kittel-Kasuya-Yosida interactions, a distinct signature of quantum spins. Chains exhibit coherent hybridization and band formation of the YSR excitations, indicating ferromagnetic coupling. Longer chains develop separate domains due to coexisting charge-density-wave order of NbSe$_2$. Despite the spin-orbit-coupled substrate, we find no signatures of Majoranas, possibly because quantum spins reduce the parameter range for topological superconductivity. We suggest that adatom chains are versatile systems for investigating correlated-electron physics and its interplay with topological superconductivity.", "revisions": [ { "version": "v1", "updated": "2021-07-13T19:57:40.000Z" } ], "analyses": { "keywords": [ "magnetic adatom", "artificially-constructed chains", "hybridization", "superconductor", "surfaces constitute fascinating quantum spin" ], "note": { "typesetting": "TeX", "pages": 0, "language": "en", "license": "arXiv", "status": "editable" } } }