Valley-selective Landau-Zener oscillations in semi-Dirac p − n junctions

Physical Review B American Physical Society 96:4 (2017) 045424

Authors:

K Saha, R Nandkishore, Siddharth Parameswaran

Abstract:

We study transport across p-n junctions of gapped two-dimensional semi-Dirac materials: nodal semimetals whose energy bands disperse quadratically and linearly along distinct crystal axes. The resulting electronic properties - relevant to materials such as TiO2/VO2 multilayers and α-(BEDT-TTF)2I3 salts - continuously interpolate between those of mono- and bilayer graphene as a function of propagation angle. We demonstrate that tunneling across the junction depends on the orientation of the tunnel barrier relative to the crystalline axes, leading to strongly nonmonotonic current-voltage characteristics, including negative differential conductance in some regimes. In multivalley systems, these features provide a natural route to engineering valley-selective transport.

Behavior of l-bits near the many-body localization transition

(2017)

Authors:

Abishek K Kulshreshtha, Arijeet Pal, Thorsten B Wahl, Steven H Simon

Exothermicity Is Not a Necessary Condition for Enhanced Diffusion of Enzymes

Nano Letters American Chemical Society (ACS) 17:7 (2017) 4415-4420

Authors:

Pierre Illien, Xi Zhao, Krishna K Dey, Peter J Butler, Ayusman Sen, Ramin Golestanian

Electric-field induced shape transition of nematic tactoids

(2017)

Authors:

Luuk Metselaar, Ivan Dozov, Krassimira Antonova, Emmanuel Belamie, Patrick Davidson, Julia M Yeomans, Amin Doostmohammadi

Variation of the contact time of droplets bouncing on cylindrical ridges with ridge size.

Langmuir American Chemical Society 33:30 (2017) 7583-7587

Authors:

M Andrew, Y Liu, Julia Yeomans

Abstract:

Reducing the contact time between bouncing droplets and an underlying solid surface is relevant to a broad range of industrial applications, such as anti-icing and self-cleaning. Previous work has found that placing cylindrical obstacles on the substrate leads to a reduction in contact time. For obstacles large compared to the drop, this is a result of hydrodynamic coupling between the azimuthal and axial spreading directions. For obstacles small compared to the drop, the reduction in contact time is interpreted as being due to fast retraction along the cylindrical ridge, followed by drop breakup. Here we use simulations to discuss in greater detail the effect of varying the obstacle size on the dynamics of the drop bouncing. We investigate the crossover between the two regimes and explain why the contact time is minimized when the radii of the drop and the cylindrical obstacle are comparable.