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  Mapping the Mottness under Magnetic Field

Wei, L., Gu, Z.-L., Fischer, A., He, Y., Xu, Q., Ghiotto, A., et al. (2023). Mapping the Mottness under Magnetic Field. doi:10.21203/rs.3.rs-3385782/v1.

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 Creators:
Wei, L.1, Author
Gu, Z.-L.1, Author
Fischer, A.2, Author
He, Y.3, Author
Xu, Q.4, Author
Ghiotto, A.5, Author
Weber, C. S.2, Author
Watanabe, K.6, Author
Taniguchi, T.7, Author
Claassen, M.8, Author
Rubio, A.9, Author           
Millis, A. J.5, Author
Pasupathy, A. N.5, Author
Xian, L. D.9, Author           
Rhodes, D. A.10, Author
Kennes, D. M.2, Author
Li, J.-X.1, Author
Wang, L.1, Author
Affiliations:
1Nanjing University, ou_persistent22              
2RWTH Aachen University, ou_persistent22              
3University of Wisconsin, ou_persistent22              
4Songshan Lake Materials Laboratory, ou_persistent22              
5Columbia University, ou_persistent22              
6National Institute for Materials Science, ou_persistent22              
7National Institute for Materials Science, Tsukuba, Ibaraki, ou_persistent22              
8University of Pennsylvania, ou_persistent22              
9Theory Group, Theory Department, Max Planck Institute for the Structure and Dynamics of Matter, Max Planck Society, ou_2266715              
10University of Wisconsin - Madison, ou_persistent22              

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 Abstract: Charge and spin are two intrinsic degrees of freedom of an electron. In a Mott insulator (MI), they are separated in that the charge degree is frozen due to strong Coulomb interaction U while the spin degree can still fluctuate and is governed by the energy scale of spin exchange J ≈ 4t2/U (t, hopping integral). Usually, a magnetic field can only manipulate the spin degree as the attainable Zeeman energy Ez can only compete with J at the scale of tens of milli-electron volts, while it does not affect the charge degree with U being at least two orders of magnitude larger [1–3]. Therefore, the complete evolution of a Mott insulator under magnetic field with both charge and spin impacted has yet to be explored. With recent progress in two-dimensional (2D) moiré systems, Mott insulators have been realized with significantly reduced U [4–9], providing an opportunity to investigate this problem. Here, we map out the full picture of Mottness under magnetic field by transport measurements on twisted bilayer (TB) WSe2 with twist angle θ ranging from 2.4° to 3.2°. We achieve the tuning of the charge dynamics of the Mott insulator using magnetic fields and observe unexpected Mott insulator-metal-Mott insulator (IMI) transitions. We theoretically establish that these IMI transitions are driven by an exotic form of spectral weight transfer (SWT) between the spin-split Hubbard bands due to carrier occupancy variations of different spins. We further identify the reentrant insulating phase at higher magnetic fields as a Mott-Zeeman insulator (MZI) with its gap determined collectively by U and Ez. Remarkably, with SWT, the observed critical magnetic field for this reentrance is as low as 5 T, which corresponds to a Zeeman energy approximately an order of magnitude smaller than U. The unveiled IMI transitions experimentally and theoretically evidence SWT as a crucial driving mechanism for the evolution of a Mott insulator in response to control parameters, which offers an unprecedented perspective into the nature of Mott physics.

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Language(s): eng - English
 Dates: 2023-10-08
 Publication Status: Published online
 Pages: 12
 Publishing info: -
 Table of Contents: -
 Rev. Type: No review
 Identifiers: DOI: 10.21203/rs.3.rs-3385782/v1
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