Hello,
I have a question related to QuantumATK-2018. Enclosed is an input file (aGNR-2Fe….) for a device calculation involving an armchair graphene nanoribbon (aGNR) with substitutional Fe atoms. This is part of a follow-up project of an earlier study on the spin-filtering efficiency of aGNRs with embedded transition metal impurities (F. Hagelberg, A.Kaiser, I.Sukuba, M. Probst, Mol. Phys. 115, 2231 (2017)). The earlier work was done with ATK-2015. Trying to reproduce some of the previous results with QuantumATK-2018, I fail completely. The atomic populations seem to oscillate between a physically reasonable state and an unphysical state that includes extremely high atomic populations at the ends of the central region. I enclose the output file corresponding (atkjob-aGNR-2Fe…I reduced the size a bit) for illustration (see, for instance, the last population block in that file). I tried to attain convergence by varying the DFT methd (i.e. GGA versus LDA, DFT+U) as well as the exchange-correlation functional, but this didn’t improve the erroneous output. Are there some critical DFT-related features in QuantumATK-2018 that were not present in ATK-2015, and that I possibly mishandle?
Thanks,
Frank Hagelberg