arXiv subjects

Zhuo Bin Siu

Publications and source records attributed to Zhuo Bin Siu.

40 records · Page 3Linked to original sources

arXiv2016

Influence of Fermi arc states and double Weyl node on tunneling in a Dirac semimetal

Most theoretical studies of tunneling in Dirac and the closely related Weyl semimetals have modeled these materials as single Weyl nodes described by the three-dimensional Dirac equation $H = v_f \vec{p}\cdot\vecσ$. The influence of scattering between the different valleys centered around different Weyl nodes, and the Fermi arc states which connect these nodes are hence not evident from these studies. In this work we study the tunneling in a thin film system of the Dirac semimetal $\text{Na}_3\text{Bi}$ consisting of a central segment with a gate potential, sandwiched between identical semi-infinite source and drain segments. The model Hamiltonian we use for $\text{Na}_3\text{Bi}$ gives, for each spin, two Weyl nodes separated in $k$-space symmetrically about $k_z=0$. The presence of a top and bottom surface in the thin film geometry results in the appearance of Fermi arc states and energy subbands. We show that (for each spin) the presence of two Weyl nodes and the Fermi arc states result in enhanced transmission oscillations, and finite transmission even when the energy falls within the \textit{bulk} band gap in the central segment respectively. These features are not evident in single Weyl node models.

cond-mat.mes-hall↗

arXiv2016

Dirac semimetal thin films in in-plane magnetic fields

In this work we study the effects of in-plane magnetic fields on thin films of the Dirac Semimetal (DSM) \ce{Na2Bi} where one of the in-plane directions is perpendicular to the $k$-separation between the two Weyl points for each spin orientation. We show numerically that the states localized near the surface of these thin films are related to the Fermi arc states in semi-infinite slabs. Due to the anisotropy between the two in-plane directions, the application of a magnetic field along these directions have differing effects. A field parallel to the $k$ space separation between the Weyl points leads to a broadening of the surface state band and a formation of an energy plateau, while a perpendicular field shifts the energy where the hole and particle bands meet upwards and sharpens the tips of the bands. We illustrate the effects of these changes to the bandstructure by studying the transmission from a source segment without a magnetic field to a drain segment with a field with the field and interface at various in-plane directions.

cond-mat.mes-hall↗

arXiv2016

Curvature induced out of plane spin accumulation

In this work we show that (real space) curvature in the geometry of curved waveguides with Rashba spin orbit interaction (RSOI) can lead to out of plane spin accumulations. We first derive the RSOI Hamiltonian on arbitrarily curved surfaces. We then analyze the effects of curvature with two distinct methods. We first apply an adiabatic approximation on gently curved, planar waveguides lying flat on the $xy$ plane to show that analogous to the acceleration of the charge carriers by an electric field, the change in momentum direction of the charge carriers as they move along the waveguide leads to an out of plane spin accumulation. We then use the Heisenberg equations of motion to establish the relationships between spin currents and accumulations on non-planar waveguides. These relations predict the existence of out of plane spin accumulation on asymmetrically curved, non-planar waveguides. We finally solve for the eigenstates on such waveguides numerically, and present numerical results to verify our earlier analytic predictions.

cond-mat.mes-hall↗

arXiv2016

Effective Hamiltonian for surface states of \ce{Bi2Te3} nanocylinders with hexagonal warping

The three-dimensional topological insulator \ce{Bi2Te3} differs from other topological insulators in the \ce{Bi2Se3} family in that the effective Hamiltonian of its surface states on a flat semi-infinite slab requires the addition of a cubic momentum hexagonal warping term in order to reproduce the experimentally measured constant energy contours. In this work, we derive the appropriate effective Hamiltonian for the surface states of a \ce{Bi2Te3} \textit{cylinder} incorporating the corresponding hexagonal warping terms in a cylindrical geometry. We show that at the energy range where the surface states dominate, the effective Hamiltonian adequately reproduces the dispersion relation obtained from a full four-band Hamiltonian, which describe both the bulk and surface states. As an example application of our effective Hamiltonian, we study the transmission between two collinear \ce{Bi2Te3} cylinders magnetized in different directions perpendicular to their axes. We show that the hexagonal warping term results in a transmission profile between the cylinders which may be of utility in a multiple state magnetic memory bit.

cond-mat.mes-hall↗