
Release 2026.10.29 introduces multiple fixes and new capabilities. We highlight (1) a new workflow for Schottky barrier heights at metal/semiconductor contacts; (2) new examples calculating valence band offsets at the Si/Ge and GaAs/AlAs semiconductor interfaces; (3) new examples of graphene on substrates, including the p-doping of graphene on alpha-quartz; and (4) new examples for point defects in graphene and GaN.

Release 2026.10.29 introduces multiple fixes and new capabilities. We highlight (1) a new workflow for Schottky barrier heights at metal/semiconductor contacts; (2) new examples calculating valence band offsets at the Si/Ge and GaAs/AlAs semiconductor interfaces; (3) new examples of graphene on substrates, including the p-doping of graphene on alpha-quartz; and (4) new examples for point defects in graphene and GaN, with formation energies and band structures.
A new Quantum ESPRESSO workflow calculates the Schottky barrier height at a metal/semiconductor contact. It shares the electrostatic potential steps with the band offset workflow and lines up the metal Fermi level with the semiconductor band edges through the averaged potential across the interface. The job page reports the p-type and n-type barrier heights as separate results:

Two new examples calculate the valence band offset at a semiconductor heterojunction with the platform's valence band offset workflow. Each builds a strained superlattice and the matching bulk references, then lines up the bulk valence band maxima through the average electrostatic potential across the interface. For the Si/Ge (001) superlattice, following Van de Walle and Martin (Phys. Rev. B, 1986), the offset comes out at 0.765 eV, against 0.74 eV in the publication, with the germanium valence band above silicon's:

The same approach applied to the GaAs/AlAs (110) interface, following Hinuma et al. (Phys. Rev. B, 2014), gives 0.471 eV against the published 0.45 eV at the same level of theory:

New examples compute how a substrate changes the electronic structure of graphene. A new tutorial builds graphene on O-terminated alpha-quartz(0001) in the metastable geometry of Kang et al. (Phys. Rev. B, 2008) and calculates its band structure (published structure on the left, ours on the right):

As in the publication, the graphene comes out p-doped, with the Dirac point 1.171 eV above the Fermi level against the published 1.28 eV (published band structure on the left, platform result on the right):

A companion example places graphene on hexagonal boron nitride and calculates the stacking energy and the small band gap that the substrate opens at the Dirac point (Giovannetti et al., Phys. Rev. B, 2007).
We continue adding defect calculations that reproduce published results. A new example computes the formation energy and band structure of the pyridinic N₃-vacancy defect in graphene, following Fujimoto and Saito (Phys. Rev. B, 2011), with the acceptor-like defect states near the Fermi level (published band structure on the left, platform result on the right). Another computes the neutral formation energy of the Mg_Ga–V_N defect pair in GaN, following Miceli and Pasquarello (Phys. Rev. B, 2016):

Try the new functionality online at https://platform.mat3ra.com/