Heavy fermions
Description
Heavy fermion systems are a class of strongly correlated electron systems in which charge carrier can have masses as large 1000 times the free electron mass. This large effective mass often derives from f orbitals of rare earth or actinide atoms. The ground state of heavy fermions is easily tuned and controlled with an external thermodynamic parameter. For instance, magnetic phases can be suppressed at a quantum phase transition with pressure or magnetic field.
Research staff
Topics
Unconventional superconductivity
Quantum Critical Points
Magnetic Phase Diagrams
Quantum oscillations and Fermi surfaces
Techniques
Magnetization
Specific Heat
Publications
Selected publications
Toni Helm, Motoi Kimata, Kenta Sudo, Atsuhiko Miyata, Julia Stirnat, Tobias Förster, Jacob Hornung, Markus König, Ilya Sheikin, Alexandre Pourret, Gerard Lapertot, Dai Aoki, Georg Knebel, Joachim Wosnitza & Jean-Pascal Brison, “Field-induced compensation of magnetic exchange as the possible origin of reentrant superconductivity in UTe2”, Nature Communications Vol. 15, Article number 37 (2024).
Dai Aoki, Ilya Sheikin, Nils Marquardt, Gerard Lapertot, Jacques Flouquet, and Georg Knebel, “High Field Superconducting Phases of Ultra Clean Single Crystal UTe2”, Journal of the Physical Society of Japan, vol. 93, No. 12, pp. 123702 (2024).
Klein, C. Marcenat, A. Demuer, J. Sarrade, D. Aoki, and I. Sheikin “Exotic magnetic phase diagram and extremely robust antiferromagnetism in Ce2RhIn8”, Physical Review B 111, L201110 (2025).
LNCMI thematic publications on HAL





Above we show an example of magnetization measurement in high magnetic field and low temperature in a Weyl semimetal. de Haas van Alphen quantum oscillations are measured up to the highest field when applied along the a-axis of the hexagonal structure.
