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This research demonstrates a novel mechanism where a uniform magnetic field can reverse charge polarization in asymmetric double quantum dots without altering electrostatic detuning. By leveraging Zeeman splitting and Coulomb blockade, the study establishes a pathway for magnetic control of single-electron states, which is critical for developing scalable spin-based qubits and quantum logic gates. The findings advance our understanding of mesoscopic transport phenomena essential for next-generation quantum computing architectures.
Turning Zeeman splitting into switchable charge polarization in a double quantum dot
arXiv:2608.27625v1 Announce Type: cross Abstract: A magnetic field that acts identically on two quantum dots is not expected to move charge between them. Nevertheless, we show that a uniform Zeeman field can strongly reconfigure and even reverse the single-electron charge polarization of an asymmetric open double quantum dot. Using a symmetry-preserving Green's-function equation-of-motion approach, we identify regimes where the preferred dot occupation reverses while the system remains in the single-electron charge sector. Two distinct mechanisms produce this behavior. Unequal gate levels produce different occupation responses because the Zeeman-shifted resonances lie at different positions relative to the reservoir chemical potential, whereas unequal onsite interactions distinguish the dots through their many-body addition spectra. Coulomb blockade stabilizes the single-electron sector, causing the reservoir-mediated response to appear as spatial charge redistribution rather than a change in total occupation. Our results establish a mechanism for magnetic control of charge polarization at fixed electrostatic detuning.
Abstract:A magnetic field that acts identically on two quantum dots is not expected to move charge between them. Nevertheless, we show that a uniform Zeeman field can strongly reconfigure and even reverse the single-electron charge polarization of an asymmetric open double quantum dot. Using a symmetry-preserving Green's-function equation-of-motion approach, we identify regimes where the preferred dot occupation reverses while the system remains in the single-electron charge sector. Two distinct mechanisms produce this behavior. Unequal gate levels produce different occupation responses because the Zeeman-shifted resonances lie at different positions relative to the reservoir chemical potential, whereas unequal onsite interactions distinguish the dots through their many-body addition spectra. Coulomb blockade stabilizes the single-electron sector, causing the reservoir-mediated response to appear as spatial charge redistribution rather than a change in total occupation. Our results establish a mechanism for magnetic control of charge polarization at fixed electrostatic detuning.
Mesoscale and Nanoscale Physics (cond-mat.mes-hall); Quantum Physics (quant-ph)
arXiv:2608.27625 [cond-mat.mes-hall]
(or arXiv:2608.27625v1 [cond-mat.mes-hall] for this version)
https://doi.org/10.48550/arXiv.2608.27625 Focus to learn more arXiv-issued DOI via DataCite (pending registration)
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