Dynamical Effects in Heavy-Fermion Systems
Creators: name: Lenk, Marvin
Publisher: name: Universitäts- und Landesbibliothek Bonn
Year: 2025
Subjects: subject: Theorie der kondensierten Materie
subject: kondensierte Materie
subject: Kondo-Effekt
subject: Kondo-Gitter
subject: Hilfsteilchen
subject: Schwerfermionen
subject: Schwerfermionsysteme
subject: Kristallfelder
subject: Kristallfeldzustände
subject: Kristallfeldaufspaltung
subject: Gitterkohärenz
subject: Nicht-Fermiflüssigkeit
subject: Periodisches Andersonmodell
subject: Zweikanal-Kondo-Effekt
subject: condensed matter theory
subject: condensed matter
subject: Kondo effect
subject: Kondo lattice
subject: auxiliary particles
subject: non-crossing approximation
subject: heavy fermions
subject: heavy-fermion systems
subject: crystal fields
subject: crystal field states
subject: crystal field splitting
subject: lattice coherence
subject: non-Fermi liquid
subject: periodic Anderson model
subject: two-channel Kondo effect
subject: ddc:530

description: When atoms in solids have unfilled <em>d</em>- or <em>f</em>-orbitals, local Coulomb interaction often becomes non-negligible due to the strongly localized nature of those orbitals. A hallmark effect of such systems is the formation of a set of localized states at the Fermi energy due to the local nature of the Kondo effect. If the so-formed Kondo singlets become lattice coherent, a heavy Fermi liquid is formed. A long-standing open question is the fate of individual crystal (electric) field (CEF) states involved in this process. Lattice coherence of different CEF states could, in principle, occur at different temperatures and extents.<br> This is the case in YbRh<sub>2</sub>Si<sub>2</sub>, for which scanning tunneling microscopy (STM) revealed a puzzling picture. The Kondo effect leads to a dip in the STM spectrum. Below temperatures where the dip was already clearly pronounced, a peak close to the minimum of the dip arose, which was attributed to the formation of lattice coherence. Simultaneously, additional peaks at the CEF energies arose, hinting towards lattice coherence in all states.<br> In this thesis, I present a comprehensive overview of lattice coherence in heavy fermion systems, from the basics of quantum particles in periodic potentials to methods for interacting systems and how to modify them to include CEF states and methods for solving such systems with quantum field theory and numerically. I construct a minimalistic model for YbRh<sub>2</sub>Si<sub>2</sub>, including all four CEF states of the Yb<sup>3+</sup> 4<em>f</em><sup>13</sup> configuration. With this, I present results confirming the observed behavior qualitatively. The Kondo dip and the coherence peak are reproduced faithfully. The first excited CEF level shows clear signs of lattice coherence, and higher excited CEF states show weaker signs of coherence.<br> The non-Fermi liquid behavior in two-channel Kondo heavy-fermion systems is explored as a second topic. Intriguingly, such behavior was experimentally observed in PrV<sub>2</sub>Al<sub>20</sub>, whereas PrTi<sub>2</sub>Al<sub>20</sub> showed regular heavy Fermi liquid behavior. It was proposed that the former sits closer to a putative quantum-critical point. While this could explain the observed behavior, another possible explanation can be formulated. The two-channel Kondo effect gives rise to a local non-Fermi liquid behavior. If this picture translates to the lattice case, it could fully explain the experimentally observed scaling.<br> This option is explored as the second main subject of this thesis. I present a model incorporating the relevant CEF states of the Pr<sup>3+</sup> 4<em>f</em><sup>2</sup> configuration and using ab initio band structure data. While including only the CEF ground state already leads to non-Fermi liquid behavior in the lattice model, the stark deviation from the experimentally observed magnetic susceptibility necessitates the inclusion of the first excited CEF state as well. This is shown to improve the scale of the onset of non-Fermi liquid behavior and reproduce the qualitatively correct scaling of the magnetic susceptibility, confirming the alternative explanation for the experimentally observed behavior.