論文 Parity-independent Kondo effect of correlated electrons in electrostatically defined ZnO quantum dots

Kosuke Noro ORCID ; Yusuke Kozuka SAMURAI ORCID ; Kazuma Matsumura ; Takeshi Kumasaka ; Yoshihiro Fujiwara ; Atsushi Tsukazaki ORCID ; Masashi Kawasaki ORCID ; Tomohiro Otsuka ORCID

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引用
Kosuke Noro, Yusuke Kozuka, Kazuma Matsumura, Takeshi Kumasaka, Yoshihiro Fujiwara, Atsushi Tsukazaki, Masashi Kawasaki, Tomohiro Otsuka. Parity-independent Kondo effect of correlated electrons in electrostatically defined ZnO quantum dots. Nature Communications. 2024, 15 (), 9556. https://doi.org/10.1038/s41467-024-53890-2
SAMURAI

説明:

(abstract)

Quantum devices such as spin qubits have been extensively investigated in electrostatically confined quantum dots using high-quality semiconductor heterostructures like GaAs and Si. Here, we present a demonstration of electrostatically forming the quantum dots in ZnO heterostructures. Through the transport measurement, we uncover the distinctive signature of the Kondo effect independent of the even-odd electron number parity, which contrasts with the typical behavior of the Kondo effect in GaAs. By analyzing temperature and magnetic field dependences, we find that the absence of the even-odd parity in the Kondo effect is not straightforwardly interpreted by the considerations developed for conventional semiconductors. We propose that, based on the unique parameters of ZnO, electron correlation likely plays a fundamental role in this observation. Our study not only clarifies the physics of correlated electrons in the quantum dot but also holds promise for applications in quantum devices, leveraging the unique features of ZnO.

権利情報:

キーワード: ZnO quantum dot

刊行年月日: 2024-11-07

出版者: Springer Science and Business Media LLC

掲載誌:

  • Nature Communications (ISSN: 20411723) vol. 15 9556

研究助成金:

  • MEXT | Japan Society for the Promotion of Science

原稿種別: 出版者版 (Version of record)

MDR DOI:

公開URL: https://doi.org/10.1038/s41467-024-53890-2

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更新時刻: 2024-11-12 16:30:30 +0900

MDRでの公開時刻: 2024-11-12 16:30:30 +0900

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