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Mapping the Mottness under Magnetic Field

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Rubio,  A.
Theory Group, Theory Department, Max Planck Institute for the Structure and Dynamics of Matter, Max Planck Society;

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Xian,  L. D.
Theory Group, Theory Department, Max Planck Institute for the Structure and Dynamics of Matter, Max Planck Society;

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Citation

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.


Cite as: https://hdl.handle.net/21.11116/0000-000D-CA3E-B
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.