Search arXivSearch

arXiv · 1901.08178

Topological valley transport at the curved boundary of a folded bilayer graphene

Abstract

The development of valleytronics demands long-range electronic transport with preserved valley index, a degree of freedom similar to electron spin. A promising structure for this end is a topological one-dimensional (1D) channel formed in bilayer graphene (BLG) under special electrostatic conditions or specific stacking configuration, called domain wall (DW). In these 1D channels, the valley-index defines the propagation direction of the charge carriers and the chiral edge states (kink states) are robust over many kinds of disorder. However, the fabrication of DWs is challenging, requiring the design of complex multi-gate structures or have been producing on rough substrates, showing a limited mean free path. Here, we report on a high-quality DW formed at the curved boundary of folded bilayer graphene (folded-BLG). At such 1D conducting channel we measured a two-terminal resistance close to the quantum resistance $R = e^2/4h$ at zero magnetic field, a signature of kink states. Our experiments reveal a long-range ballistic transport regime that occurs only at the DW of the folded-BLG, while the other regions behave like semiconductors with tunable band gap.

Explore related subjects

Keep this discovery

Explore connections, maps & timelines

BibTeXRIS

E. Mania, A. R. Cadore, T. Taniguchi, K. Watanabe, L. C. Campos. 2019-01-24. Topological valley transport at the curved boundary of a folded bilayer graphene. https://doi.org/10.1038/s42005-018-0106-4

Cite the original work for its findings. Save a collection to share your selection of sources.

KEEP EXPLORING

Related papers

When blinking helps: enhanced single-photon purity in the off states of perovskite quantum dots

Photoluminescence blinking typically degrades the single-photon purity of quantum dot emission. Here, we show that individual CsPbBr$_3$ perovskite quantum dots (PQDs) can exhibit the opposite behavior: low-emitting off states are dimmer and shorter-lived, yet more strongly antibunched than high-intensity on states. Using time-correlated single-photon counting combined with state-resolved second-order correlation analysis, we identify a subset of PQDs in which the zero-delay second-order correlation, $g^{(2)}_0$, decreases upon switching from the on state to the off state, indicating improved single-photon purity. In the most pronounced case, $g^{(2)}_0$ decreases from 0.23 in the on state to 0.08 in the off state. We attribute this counterintuitive behavior to self-trapped-exciton-mediated suppression of the biexciton--exciton cascade, which suppresses multiphoton emission more effectively than single-exciton emission. These findings reveal an unconventional blinking regime in PQDs and show that blinking does not necessarily degrade single-photon purity.

cond-mat.mes-hall

Prediction of two-dimensional $π$-electron half-metallic ferrimagnets

We propose a strategy to obtain conducting organic materials with fully spin-polarized Fermi surface, lying at a singular flat band, with antiferromagnetically coupled magnetic moments that reside in pi-orbitals of nanographenes. We consider a honeycomb crystal whose unit cell combines two different molecules with $S=1/2$: an Aza-3-Triangulene, a molecule with orbital degeneracy, and a 2-Triangulene. The analyzed system is half-metallic with a ferrimagnetic order, presenting a zero net total magnetic moment per unit cell. We combine density functional theory calculations with a Hubbard model Hamiltonian to compute the magnetic interactions, the bands, the intrinsic Anomalous Hall effect, and the collective spin excitations. We obtain very large intermolecular exchange couplings, in the range of 59 meV. Based on the spin excitation dispersion, we estimate thermal stability in the range of 100 Kelvin. When the magnetization is off-plane, intrinsic spin orbit coupling in graphene opens up a topological gap that, despite being very small, leads to a quantized Hall conductance in the tens of mK range, but is thermally smeared above 1 Kelvin.

cond-mat.mes-hall

Analytical and numerical solutions to the non-diffusive Stefan problem

In this work, the Maxwell--Cattaneo--Vernotte (MCV) equation is used to model the one-dimensional hyperbolic Stefan problem in the limit of a small Stefan number (Ste $\ll$ 1). The solutions are approximated with perturbation series expansions using a reformulation in which time is expressed as a function of the solid-liquid interface position. The first proposed solution is derived in a framework that considers diffusive heat transfer at the phase change interface, for analytic tractability. Two rectification strategies are proposed to address the asymptotic divergence present in this formulation: a rescaled inner solution which is then combined with the outer solution to yield a composite solution, and size-dependent thermo-physical system parameters for better capture of hyperbolic effects at the phase change interface. The resulting interface profiles exhibit a characteristic parabolic-like shape, consistent with diffusive Stefan problem findings, with pronounced early-time hyperbolic effects at larger thermal relaxation times. Parametric studies are done over three pertinent variables in the dimensionless system: the Stefan number ($\mathrm{Ste}$), the dimensionless thermal relaxation time ($\widetilde τ$), and the thermal diffusivity ($α$). The studies suggest that model error scales with the Stefan number in accordance with the theoretical truncation error of the perturbation expansion. Additionally, larger values of $\widetilde τ$ amplify early-time hyperbolic effects, thereby increasing model error, while larger $α$ extends the relative temporal domain over which these hyperbolic effects remain significant, also corresponding to an increase in model error.

cond-mat.mes-hall