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Abstract
The interaction among magnetic moments screened by conduction electrons drives quantum phase transitions between magnetically ordered and heavy-fermion ground states. Here, starting from isolated magnetic impurities in the Kondo regime, we investigate the formation of the finite size analogue of a heavy Fermi liquid. We build regularly-spaced chains of Co adatoms on a metallic surface by atomic manipulation. Scanning tunneling spectroscopy is used to obtain maps of the Kondo resonance intensity with sub-atomic resolution. For sufficiently small interatomic separation, the spatial distribution of Kondo screening does not coincide with the position of the adatoms. It also develops enhancements at both edges of the chains. Since we can rule out any other interaction between Kondo impurities, this is explained in terms of the indirect hybridization of the Kondo orbitals mediated by a coherent electron gas, the mechanism that causes the emergence of heavy quasiparticles in the thermodynamic limit.
Unconventional properties in heavy fermion compounds are thought to arise from competing interactions between conduction electrons and localized magnetic moments. Here, the authors build one-dimensional lattices of cobalt atoms on a metallic surface and observe the onset of heavy fermion behaviour.
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1 University of Zaragoza, Laboratorio de Microscopias Avanzadas, Instituto de Nanociencia de Aragón, Zaragoza, Spain (GRID:grid.11205.37) (ISNI:0000 0001 2152 8769); Academy of Sciences, Institute of Physics, Prague, Czech Republic (GRID:grid.418095.1) (ISNI:0000 0001 1015 3316); Palacky University, Regional Centre of Advanced Technologies and Materials, Faculty of Science, Department of Physical Chemistry, Olomouc, Czech Republic (GRID:grid.10979.36) (ISNI:0000 0001 1245 3953)
2 Charles University, Department of Condensed Matter Physics, Faculty of Mathematics and Physics, Prague 2, Czech Republic (GRID:grid.4491.8) (ISNI:0000 0004 1937 116X)
3 University of Zaragoza, Laboratorio de Microscopias Avanzadas, Instituto de Nanociencia de Aragón, Zaragoza, Spain (GRID:grid.11205.37) (ISNI:0000 0001 2152 8769); University of Zaragoza, Dpto.Física Materia Condensada, Zaragoza, Spain (GRID:grid.11205.37) (ISNI:0000 0001 2152 8769)
4 CSIC and BIST, Campus UAB, Bellaterra, Catalan Institute of Nanoscience and Nanotechnology (ICN2), Barcelona, Spain (GRID:grid.7080.f)
5 Centro de Física de Materiales CFM/MPC (CSIC-UPV/EHU), Donostia-San Sebastián, Spain (GRID:grid.7080.f); Donostia International Physics Center (DIPC), Donostia-San Sebastian, Spain (GRID:grid.452382.a) (ISNI:0000 0004 1768 3100)
6 University of Zaragoza, Laboratorio de Microscopias Avanzadas, Instituto de Nanociencia de Aragón, Zaragoza, Spain (GRID:grid.11205.37) (ISNI:0000 0001 2152 8769); CIC NanoGUNE, Donostia-San Sebastián, Spain (GRID:grid.424265.3) (ISNI:0000 0004 1761 1166); Basque Foundation for Science, IKERBASQUE, Bilbao, Spain (GRID:grid.424810.b) (ISNI:0000 0004 0467 2314)
7 University of Zaragoza, Laboratorio de Microscopias Avanzadas, Instituto de Nanociencia de Aragón, Zaragoza, Spain (GRID:grid.11205.37) (ISNI:0000 0001 2152 8769); University of Zaragoza, Dpto.Física Materia Condensada, Zaragoza, Spain (GRID:grid.11205.37) (ISNI:0000 0001 2152 8769); CSIC - Universidad de Zaragoza, Instituto de Ciencia de Materiales de Aragón, Zaragoza, Spain (GRID:grid.11205.37) (ISNI:0000 0001 2152 8769)