Figure 4
From: Electron tunneling through double magnetic barriers in Weyl semimetals
Transmission probability through a parallel square-shaped magnetic double barrier as a function of the incident angle φ and γ, for incident energy V 3 = 40 meV, incident energy E F = 24 meV. (b) The same as panel (a) but for the antiparallel configuration. (c) Transmission probability as a function of the incident energy E F for different incident angle with a potential barrier V 3 = 40 meV. (d) The same as panel (a) but for the antiparallel configuration. The distance is L = 9d = 234 nm.
