Magnetism in twisted triangular bilayer graphene quantum dots
M. Mirzakhani, Zebih Çetin, M. Yagmurcukardes, Hee Chul Park, F. M. Peeters, D. R. da Costa
Abstract
Using a tight-binding model along with the mean-field Hubbard method, we investigate the effect of twisting angle on the magnetic properties of twisted bilayer graphene (tBLG) quantum dots (QDs) with triangular shape and zigzag edges. We consider such QDs in two configurations: when their initial untwisted structure is a perfect AA- or AB-stacked BLG, referred to as AA- or AB-like dots. We find that AA-like dots exhibit an antiferromagnetic spin polarization for small twist angles, which transits to a ferromagnetic spin polarization beyond a critical twisting angle ${\ensuremath{\theta}}_{c}$. Our analysis shows that ${\ensuremath{\theta}}_{c}$ decreases as the dot size increases, obeying a criterion, according to which once the maximum energy difference between electron and hole edge states (in the single-particle picture) is less than $(U/{\ensuremath{\gamma}}_{0})\phantom{\rule{0.16em}{0ex}}{t}_{0}$, the spin-polarized energy levels are aligned ferromagnetically $[U$ is the Hubbard parameter and ${\ensuremath{\gamma}}_{0}$ $({t}_{0})$ the graphene intralayer (interlayer) hopping]. Unlike AA-like dots, AB-like dots exhibit finite magnetization for any twist angle. Furthermore, in the ferromagnetic polarization state, the ground net spin for both dot configurations agrees with the prediction from Lieb's theorem.