A DFT + DMFT study of the two-channel quadrupolar Kondo effect in PrV<sub>2</sub>Al<sub>20</sub>
ORAL
Abstract
Praseodymium-based cubic 1-2-20 materials like PrV2Al20 exhibit a strong coupling between Pr 4f states and conduction electrons. They experimentally show traces of a two-channel quadrupolar Kondo effect in competition with quadrupolar ordering and superconductivity [1]. Valence fluctuations on the Pr atom occur between the magnetic quadrupole 4f2 Γ3 doublet and the excited 4f1 configuration with a dipole Kramers-doublet Γ7. This specific setup leads to an exotic two-channel quadrupolar Kondo effect, where the channel degree of freedom carries a dipole moment and the Kondo degree of freedom a quadrupolar moment. A quadrupolar analog to the famous Ruderman-Kittel-Kasuya-Yosida (RKKY) interaction principally allows for quadrupolar ordering in competition with the Kondo singlet formation.
We develop a dynamical mean-field theory (DMFT) with a non-crossing approximation (NCA) local impurity solver, that is able to faithfully capture the exotic two-channel Kondo physics in this class of materials, including a momentum-dependent hybridization. This method is then combined with a density functional theory (DFT) calculation, allowing us to quantitatively compare the results to experimental data down to the Kondo regime. Within this approximation, we calculate several temperature dependent quantities: density of states, band structure and magnetic susceptibility.
[1] For review, see: T. Onimaru and H. Kusunose, J. Phys. Soc. Jpn. 85, 082002 (2016)
We develop a dynamical mean-field theory (DMFT) with a non-crossing approximation (NCA) local impurity solver, that is able to faithfully capture the exotic two-channel Kondo physics in this class of materials, including a momentum-dependent hybridization. This method is then combined with a density functional theory (DFT) calculation, allowing us to quantitatively compare the results to experimental data down to the Kondo regime. Within this approximation, we calculate several temperature dependent quantities: density of states, band structure and magnetic susceptibility.
[1] For review, see: T. Onimaru and H. Kusunose, J. Phys. Soc. Jpn. 85, 082002 (2016)
*M. L. and J. K. acknowledge financial support by the Deutsche Forschungsgemeinschaft (DFG) within the Cooperative Research Center SFB/TR 185 (277625399) and the Cluster of Excellence ML4Q (390534769).F. G. and A. H. N. were supported by the National Science Foundation Division of Materials Research Award DMR-1917511 and by Robert A. Welch Foundation grant C-1818.
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Presenters
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Marvin Lenk
- Physikalisches Institut & Bethe Center for Theoretical Physics, Universität Bonn, Germany