Heavy fermions: Typical phenomena and recent developments |
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Authors: | F. Steglich C. Geibel K. Gloos G. Olesch C. Schank C. Wassilew A. Loidl A. Krimmel G. R. Stewart |
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Affiliation: | (1) Institut für Festkörperphysik, Fachgebiet Technische Physik, SFB 252, Technische Hochschule Darmstadt, D-64289 Darmstadt, Germany;(2) Institut für Festkörperphysik, Fachgebiet Experimentalphysik, SFB 252, Technische Hochschule Darmstadt, D-64289 Darmstadt, Germany;(3) Hahn-Meitner Institut, D-14109 Berlin-Wannsee, Germany;(4) Institut für Physik, Universität Augsburg, D-86159 Augsburg, Germany;(5) Department of Physics, University of Florida, 32611 Gainesville, Fla., USA |
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Abstract: | A survey is given of typical phenomena, new materials and recent developments in heavy-fermion physics. In particular, the following topics are addressed: (i) YbNiAl, a new heavy-fermion local-moment antiferromagnet (LMM) with Néel temperature Tn = 3 K, (ii) non-Fermi-liquid behavior at the magnetic instability in two heavy-fermion systems with intact f-ion sublattice, i.e. orthorhombic CePt(Si1–xGex) and tetragonal U(Cu4+xAl8–x), (iii) the low-temperature properties of the anisotropic Rondo insulator CeNiSn, and (iv) some of the most unusual observations made on low-carrier-density rare-earth systems like Sm3Te4 and Sm3Se4. While the exotic symmetry-broken (superconducting and magnetic) ground states of heavy-fermion metals are discussed in several other contributions to this volume, we focus in the remainder of this paper on the relationship between LMM ordering and heavy-fermion superconductivity: Firstly, the LMM ordered compound CeCu2Ge2 (Tn = 4.1K) is addressed which was recently found to become a non-magnetic heavy-fermion superconductor under high hydrostatic pressure, p 70 kbar (D. Jaccard et al., Phys. Lett. A163,475 (1992)). Point-contact spectroscopy is used to investigate in more detail the high-pressure superconducting phase of CeCu2Ge2. Secondly, we summarize high-pressure results on UPd2Al3, the first compound to show homogeneous coexistence between LMM ordering and heavy-fermion superconductivity. |
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