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Abstract
Application of the Luttinger theorem to the Kondo lattice YbRh2Si2 suggests that its large 4f-derived Fermi surface (FS) in the paramagnetic (PM) regime should be similar in shape and volume to that of the divalent local-moment antiferromagnet (AFM) EuRh2Si2 in its PM regime. Here we show by angle-resolved photoemission spectroscopy that paramagnetic EuRh2Si2 has a large FS essentially similar to the one seen in YbRh2Si2 down to 1 K. In EuRh2Si2 the onset of AFM order below 24.5 K induces an extensive fragmentation of the FS due to Brillouin zone folding, intersection and resulting hybridization of the Fermi-surface sheets. Our results on EuRh2Si2 indicate that the formation of the AFM state in YbRh2Si2 is very likely also connected with similar changes in the FS, which have to be taken into account in the controversial analysis and discussion of anomalies observed at the quantum critical point in this system.
Heavy-fermion materials have unusual electronic behavior due to a dual localized-itinerant character of 4f electrons. Here, by studying divalent EuRh2Si2, the authors gain insight into the electronic states of the trivalent heavy fermion system YbRh2Si2 and show that it experimentally demonstrates Luttinger’s theorem.
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1 Technische Universität Dresden, Institut für Festkörper- und Materialphysik, Dresden, Germany (GRID:grid.4488.0) (ISNI:0000 0001 2111 7257)
2 Lund University, MAX IV Laboratory, Lund, Sweden (GRID:grid.4514.4) (ISNI:0000 0001 0930 2361)
3 Japan Atomic Energy Agency, Sayo, Materials Sciences Research Center, Hyogo, Japan (GRID:grid.20256.33) (ISNI:0000 0001 0372 1485)
4 71 Avenue des Martyrs, European Synchrotron Radiation Facility, 38043 Grenoble, France (GRID:grid.5398.7) (ISNI:0000 0004 0641 6373)
5 Paul Scherrer Institute, Swiss Light Source and Swiss FEL, Villigen-PSI, Switzerland (GRID:grid.5991.4) (ISNI:0000 0001 1090 7501)
6 IFW Dresden, Dresden, Germany (GRID:grid.14841.38) (ISNI:0000 0000 9972 3583); Max-Planck-Institut für Chemische Physik fester Stoffe, Dresden, Germany (GRID:grid.419507.e) (ISNI:0000 0004 0491 351X)
7 Tomsk State University, Lenina Av., 36, Tomsk, Russia (GRID:grid.77602.34) (ISNI:0000 0001 1088 3909); Institute of Strength Physics and Materials Science, RAS, Tomsk, Russia (GRID:grid.467103.7) (ISNI:0000 0001 0094 8940)
8 Tomsk State University, Lenina Av., 36, Tomsk, Russia (GRID:grid.77602.34) (ISNI:0000 0001 1088 3909); Centro de Física de Materiales CFM-MPC and Centro Mixto CSIC-UPV/EHU, San Sebastián/Donostia, Spain (GRID:grid.482265.f) (ISNI:0000 0004 1762 5146); Donostia International Physics Center (DIPC), San Sebastian, Spain (GRID:grid.452382.a) (ISNI:0000 0004 1768 3100); Saint Petersburg State University, Saint Petersburg, Russia (GRID:grid.15447.33) (ISNI:0000 0001 2289 6897)
9 University of Michigan, Randall Laboratory, Ann Arbor, USA (GRID:grid.214458.e) (ISNI:0000000086837370)
10 Goethe-Universität Frankfurt, Max-von-Laue Strasse 1, Kristall- und Materiallabor, Physikalisches Institut, Frankfurt am Main, Germany (GRID:grid.7839.5) (ISNI:0000 0004 1936 9721)
11 Max-Planck-Institut für Chemische Physik fester Stoffe, Dresden, Germany (GRID:grid.419507.e) (ISNI:0000 0004 0491 351X)
12 Donostia International Physics Center (DIPC), San Sebastian, Spain (GRID:grid.452382.a) (ISNI:0000 0004 1768 3100); IKERBASQUE, Basque Foundation for Science, Bilbao, Spain (GRID:grid.424810.b) (ISNI:0000 0004 0467 2314)