Elias Rudberg 2012 J. Phys.: Condens. Matter 24 072202 doi:10.1088/0953-8984/24/7/072202
Elias Rudberg
Show affiliationsSelf-consistency-based Kohn–Sham density functional theory (KS-DFT) electronic structure calculations with Gaussian basis sets are reported for a set of 17 protein-like molecules with geometries obtained from the Protein Data Bank. It is found that in many cases such calculations do not converge due to vanishing HOMO–LUMO gaps. A sequence of polyproline I helix molecules is also studied and it is found that self-consistency calculations using pure functionals fail to converge for helices longer than six proline units. Since the computed gap is strongly correlated to the fraction of Hartree–Fock exchange, test calculations using both pure and hybrid density functionals are reported. The tested methods include the pure functionals BLYP, PBE and LDA, as well as Hartree–Fock and the hybrid functionals BHandHLYP, B3LYP and PBE0. The effect of including solvent molecules in the calculations is studied, and it is found that the inclusion of explicit solvent molecules around the protein fragment in many cases gives a larger gap, but that convergence problems due to vanishing gaps still occur in calculations with pure functionals. In order to achieve converged results, some modeling of the charge distribution of solvent water molecules outside the electronic structure calculation is needed. Representing solvent water molecules by a simple point charge distribution is found to give non-vanishing HOMO–LUMO gaps for the tested protein-like systems also for pure functionals.
Issue 7 (22 February 2012)
Received 28 October 2011, in final form 9 December 2011
Published 6 January 2012
Elias Rudberg 2012 J. Phys.: Condens. Matter 24 072202
S Fremy et al 2012 Nanotechnology 23 055401
Byeonghee Lee et al 2012 Nanotechnology 23 055709
A Espinosa et al 2012 Meas. Sci. Technol. 23 015602
Johann Mertens et al 2012 Nanotechnology 23 015501
A J Lockwood et al 2010 Meas. Sci. Technol. 21 075901
Sonja Huclova et al 2012 J. Phys. D: Appl. Phys. 45 025301