Island Joshua O, Gaudenzi Rocco, de Bruijckere Joeri, Burzurí Enrique, Franco Carlos, Mas-Torrent Marta, Rovira Concepció, Veciana Jaume, Klapwijk Teun M, Aguado Ramón, van der Zant Herre S J
Kavli Institute of Nanoscience, Delft University of Technology, Lorentzweg 1, 2628 CJ Delft, Netherlands.
Institut de Ciéncia de Materials de Barcelona (ICMAB-CSIC) and CIBER-BBN, Campus de la UAB, 08193 Bellaterra, Spain.
Phys Rev Lett. 2017 Mar 17;118(11):117001. doi: 10.1103/PhysRevLett.118.117001.
Superconductors containing magnetic impurities exhibit intriguing phenomena derived from the competition between Cooper pairing and Kondo screening. At the heart of this competition are the Yu-Shiba-Rusinov (Shiba) states which arise from the pair breaking effects a magnetic impurity has on a superconducting host. Hybrid superconductor-molecular junctions offer unique access to these states but the added complexity in fabricating such devices has kept their exploration to a minimum. Here, we report on the successful integration of a model spin 1/2 impurity, in the form of a neutral and stable all organic radical molecule, in proximity-induced superconducting break junctions. Our measurements reveal excitations which are characteristic of a spin-induced Shiba state due to the radical's unpaired spin strongly coupled to a superconductor. By virtue of a variable molecule-electrode coupling, we access both the singlet and doublet ground states of the hybrid system which give rise to the doublet and singlet Shiba excited states, respectively. Our results show that Shiba states are a robust feature of the interaction between a paramagnetic impurity and a proximity-induced superconductor where the excited state is mediated by correlated electron-hole (Andreev) pairs instead of Cooper pairs.
含有磁性杂质的超导体表现出源自库珀对和近藤屏蔽之间竞争的有趣现象。这种竞争的核心是由磁性杂质对超导主体产生的对破坏效应所导致的汤浅-芝-鲁西诺夫(芝)态。混合超导体-分子结为研究这些态提供了独特途径,但制造此类器件的额外复杂性使得对它们的探索程度降至最低。在此,我们报告了成功将一个模型自旋1/2杂质(呈中性且稳定的全有机自由基分子形式)集成到近邻诱导超导断结中。我们的测量揭示了由于自由基未配对自旋与超导体强耦合而产生的自旋诱导芝态所特有的激发。借助可变的分子-电极耦合,我们获得了混合体系的单重态和双重态基态,它们分别产生双重态和单重态芝激发态。我们的结果表明,芝态是顺磁杂质与近邻诱导超导体之间相互作用的一个稳健特征,其中激发态由关联的电子-空穴(安德列夫)对而非库珀对介导。