# single H atom, Fermi-Amaldi xc, so this corresponds to the real H atom ixc 20 ndtset 2 acell1 3*30 ecut1 25 typat1 1 effmass_free2 10 acell2 3*3 ecut2 2500 typat2 2 diemac 1.0d0 diemix 0.5d0 kptopt 0 kpt 3*0.25 nkpt 1 natom 1 nband 2 nline 3 nsppol 2 nstep 2 ntypat 2 tolwfr 1.0d-14 znucl 2*1 xred 3*0 # Avoid printing Wavefunction and Density prtden 0 prtwf 0 pp_dirpath "$ABI_PSPDIR" pseudos "01h.bare, 01h.bare2" #%% #%% [setup] #%% executable = abinit #%% [files] #%% files_to_test = t25.out, tolnlines = 0, tolabs = 0.000e+00, tolrel = 0.000e+00 #%% [paral_info] #%% max_nprocs = 2 #%% [extra_info] #%% keywords = NC #%% authors = Unknown #%% description = #%% Isolated Hydrogen atom. Treated with the Fermi-Amaldi correction (ixc=20), so that this #%% corresponds to exact cancellation of the Hartree and XC contributions, #%% as it should for Hydrogen atom. #%% Examine the 1s-2s splitting, that should be equal to 0.375 Ha, #%% and is obtained at 0.368 Ha (so within 2%), with the chosen ecut and acell. #%% This quantity converges much faster to the correct value than either the total #%% energy or the 1s eigenenergy. #%% Also test effmass_free. A value 10 times bigger than the usual electron mass #%% leads to a 10-fold contraction of the system. The 1s-2s splitting is #%% multiplied by 10 exactly, provided ecut, acell and the smearing of the #%% potential at origin are scaled appropriately. #%% topics = xc, Artificial #%%