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Detection and Manipulation of Interaction Between Magnetic DyPc 2 Molecules and Superconducting Pb(111) Surface
Author(s) -
Li Jie,
Xu Zhen,
He Yang,
Yang Qianxi,
Pan Haoyang,
Wang Yudi,
Li Xin,
Chen Huamei,
Wang Yansong,
Dong Wenjie,
Hou Shimin,
Zhou Xiong,
Shen Qian,
Gao Song,
Wu Kai,
Wang Yongfeng,
Zhang Yajie
Publication year - 2025
Publication title -
advanced materials interfaces
Language(s) - English
Resource type - Journals
SCImago Journal Rank - 1.671
H-Index - 65
ISSN - 2196-7350
DOI - 10.1002/admi.202400788
Subject(s) - materials science , superconductivity , molecule , surface (topology) , nanotechnology , condensed matter physics , chemical physics , physics , quantum mechanics , geometry , mathematics
Abstract Lanthanide double‐decker phthalocyanine (LnPc 2 ) complexes are highly coveted for their prospective uses in ultrahigh‐density data storage and quantum computing. Notably, the quantum spin systems comprising these complexes and superconducting substrates exhibit unique quantum magnetic interactions. Through scanning tunneling microscopy (STM) and spectroscopy (STS) experiments, the interaction between the magnetic double‐decker DyPc 2 molecules and the superconducting Pb(111) substrate is investigated. Three distinct adsorption patterns of DyPc 2 on Pb(111) are experimentally observed. Combined with DFT calculations, it is found that the ligand spin of the normal DyPc 2 molecules in the self‐assembled monolayer (SAM) is quenched, which is attributed to strong charge transfer from Pb(111). However, special DyPc 2 molecules embedded in the SAM maintain ligand spin due to weak charge transfer, forming a complex quantum spin system with the superconducting substrate. Similarly, DyPc 2 molecules located on the second layer exhibit the same behavior. Under zero magnetic field, the Yu–Shiba–Rusinov (YSR) resonances are observed within the superconducting energy gap of both spin quantum systems. The Kondo resonance and the superconducting pairing occur at similar energy scales, indicating their coexistence and competition. This ultimately results in a Kondo‐screened state. By controlling the sample bias, the special molecule can be switched to a normal molecule.

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