Unraveling the origin of Kondo-like behavior in the 3d-electron heavy-fermion compound YFe2Ge2

Edited by J.C. Davis, University of Oxford, Oxford, United Kingdom; received January 22, 2024; accepted August 21, 2024
September 19, 2024
121 (39) e2401430121

Significance

We present a combined experimental and theoretical study of the optical conductivity of 3d-electron compound YFe2Ge2. Our work reveals the presence of a flat band at the Fermi level and related optical features that are typical for heavy fermion (HF) systems. However, unlike the Kondo scenario and its analog driven by strong Hund’s coupling, we obtain evidence for an alternative mechanism which accounts for the HF-like response of YFe2Ge2 in terms of the combined effects of kinetic frustration, band hybridization, and electron correlations. Our results help to unravel the origin of the HF properties of YFe2Ge2 and also provide a broad perspective on the exotic phenomena of other d-electron materials with HF-like properties, like some of the iron arsenide superconductors.

Abstract

The heavy fermion (HF) state of d-electron systems is of great current interest since it exhibits various exotic phases and phenomena that are reminiscent of the Kondo effect in f-electron HF systems. Here, we present a combined infrared spectroscopy and first-principles band structure calculation study of the 3d-electron HF compound YFe2Ge2. The infrared response exhibits several charge-dynamical hallmarks of HF and a corresponding scaling behavior that resemble those of the f-electron HF systems. In particular, the low-temperature spectra reveal a dramatic narrowing of the Drude response along with the appearance of a hybridization gap (Δ 50 meV) and a strongly enhanced quasiparticle effective mass. Moreover, the temperature dependence of the infrared response indicates a crossover around T 100 K from a coherent state at low temperature to a quasi-incoherent one at high temperature. Despite of these striking similarities, our band structure calculations suggest that the mechanism underlying the HF behavior in YFe2Ge2 is distinct from the Kondo scenario of the f-electron HF compounds and even from that of the d-electron iron-arsenide superconductor KFe2As2. For the latter, the HF state is driven by orbital-selective correlations due to a strong Hund’s coupling. Instead, for YFe2Ge2 the HF behavior originates from the band flatness near the Fermi level induced by the combined effects of kinetic frustration from a destructive interference between the direct Fe-Fe and indirect Fe-Ge-Fe hoppings, band hybridization involving Fe 3d and Y 4d electrons, and electron correlations. This highlights that rather different mechanisms can be at the heart of the HF state in d-electron systems.

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Data, Materials, and Software Availability

All study data are included in the article and/or SI Appendix.

Acknowledgments

This work was supported by the National Natural Science Foundation of China (Grant No. 12274442) and the National Key Research and Development Program of China (Grant No. 2022YFA1403901), as well as by the Swiss National Science Foundation through Grants No. 200020-172611 and 200021-214905. Z.Y. and R.L. were supported by the Fundamental Research Funds for the Central Universities (Grant No. 2243300003), the Innovation Program for Quantum Science and Technology (Grant No. 2021ZD0302800), and the National Natural Science Foundation of China (Grant No. 12074041). The DFT+DMFT calculations were carried out with high-performance computing cluster of Beijing Normal University in Zhuhai. J.Z. was supported by the Key Program of National Natural Science Foundation of China (Grant No. 12234006), National Key Research and Development Program of China (Grant No. 2022YFA14032), and the Innovation Program for Quantum Science and Technology (Grant No. 2024ZD0300103). H.W. was supported by the Youth Foundation of the National Natural Science Foundation of China (Grant No. 12204108).

Author contributions

B.X. and C.B. designed research; B.X., R.L., H.W., Z.L., S.Y., C.L., J.Z., X.Q., and Z.Y. performed research; B.X., Z.Y., and C.B. analyzed data; and B.X. and C.B. wrote the paper.

Competing interests

The authors declare no competing interest.

Supporting Information

Appendix 01 (PDF)

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Information & Authors

Information

Published in

Go to Proceedings of the National Academy of Sciences
Proceedings of the National Academy of Sciences
Vol. 121 | No. 39
September 24, 2024
PubMed: 39298483

Classifications

Data, Materials, and Software Availability

All study data are included in the article and/or SI Appendix.

Submission history

Received: January 22, 2024
Accepted: August 21, 2024
Published online: September 19, 2024
Published in issue: September 24, 2024

Keywords

  1. flat band
  2. heavy fermion
  3. optical conductivity

Acknowledgments

This work was supported by the National Natural Science Foundation of China (Grant No. 12274442) and the National Key Research and Development Program of China (Grant No. 2022YFA1403901), as well as by the Swiss National Science Foundation through Grants No. 200020-172611 and 200021-214905. Z.Y. and R.L. were supported by the Fundamental Research Funds for the Central Universities (Grant No. 2243300003), the Innovation Program for Quantum Science and Technology (Grant No. 2021ZD0302800), and the National Natural Science Foundation of China (Grant No. 12074041). The DFT+DMFT calculations were carried out with high-performance computing cluster of Beijing Normal University in Zhuhai. J.Z. was supported by the Key Program of National Natural Science Foundation of China (Grant No. 12234006), National Key Research and Development Program of China (Grant No. 2022YFA14032), and the Innovation Program for Quantum Science and Technology (Grant No. 2024ZD0300103). H.W. was supported by the Youth Foundation of the National Natural Science Foundation of China (Grant No. 12204108).
Author Contributions
B.X. and C.B. designed research; B.X., R.L., H.W., Z.L., S.Y., C.L., J.Z., X.Q., and Z.Y. performed research; B.X., Z.Y., and C.B. analyzed data; and B.X. and C.B. wrote the paper.
Competing Interests
The authors declare no competing interest.

Notes

This article is a PNAS Direct Submission.

Authors

Affiliations

Beijing National Laboratory for Condensed Matter Physics, Institute of Physics, Chinese Academy of Sciences, Beijing 100190, China
School of Physical Sciences, University of Chinese Academy of Sciences, Beijing 100049, China
Department of Physics and Fribourg Center for Nanomaterials, University of Fribourg, Fribourg CH-1700, Switzerland
School of Physics and Astronomy and Center for Advanced Quantum Studies, Beijing Normal University, Beijing 100875, China
State Key Laboratory of Surface Physics and Department of Physics, Fudan University, Shanghai 200433, China
Zhiyu Liao
Beijing National Laboratory for Condensed Matter Physics, Institute of Physics, Chinese Academy of Sciences, Beijing 100190, China
School of Physical Sciences, University of Chinese Academy of Sciences, Beijing 100049, China
Shaohui Yi
Beijing National Laboratory for Condensed Matter Physics, Institute of Physics, Chinese Academy of Sciences, Beijing 100190, China
School of Physical Sciences, University of Chinese Academy of Sciences, Beijing 100049, China
Chunhong Li
Beijing National Laboratory for Condensed Matter Physics, Institute of Physics, Chinese Academy of Sciences, Beijing 100190, China
Jun Zhao
State Key Laboratory of Surface Physics and Department of Physics, Fudan University, Shanghai 200433, China
Xianggang Qiu
Beijing National Laboratory for Condensed Matter Physics, Institute of Physics, Chinese Academy of Sciences, Beijing 100190, China
School of Physical Sciences, University of Chinese Academy of Sciences, Beijing 100049, China
School of Physics and Astronomy and Center for Advanced Quantum Studies, Beijing Normal University, Beijing 100875, China
Key Laboratory of Multiscale Spin Physics (Ministry of Education), Beijing Normal University, Beijing 100875, China
Department of Physics and Fribourg Center for Nanomaterials, University of Fribourg, Fribourg CH-1700, Switzerland

Notes

2
To whom correspondence may be addressed. Email: [email protected], [email protected], or [email protected].
1
B.X. and R.L contributed equally to this work.

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Unraveling the origin of Kondo-like behavior in the 3d-electron heavy-fermion compound YFe2Ge2
Proceedings of the National Academy of Sciences
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