abinit/tests/v6/Input/t05.abi

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t04o_DEN
0
2
t04o_VHA
0
2
t04o_VHXC
0
2
t04o_POT
0
0
#%%<BEGIN TEST_INFO>
#%% [setup]
#%% executable = cut3d
#%% test_chain = t04.abi, t05.abi
#%% [files]
#%% files_to_test =
#%% t05.stdout, tolnlines = 0, tolabs = 0.0, tolrel = 0.0
#%% [paral_info]
#%% max_nprocs = 1
#%% [extra_info]
#%% authors = Unknown
#%% keywords = MINIMAL
#%% description =
#%% Hydrogen dimer in a big cell.
#%% Read the previously generated files, and analyze them separately, as well as jointly.
#%% Remarkable values of the separate analysis :
#%% - the integral of the charge density over the volume of the unit cell is 2.0
#%% - the mean of the Hartree potential vanishes (G=0) component
#%% - the mean of the Kohn-Sham and XC potentials are the same (as their difference would come from non-zero G=0
#%% contributions from the local potential and Hartree potential), that is
#%% Sum of values, mean, mean times cell volume= -6.859211E+03 -5.292601E-02 -7.938901E+01
#%% - the mean of the XC potential -5.292601E-02 is in perfect agreement with the one from the previous run.
#%% Remarkable values of the joint analysis :
#%% - the integral of the product of charge density and Hartree potential over the volume of the unit cell is
#%% 1.610148E+00, correctly twice the Hartree energy.
#%% - the integral of the product of charge density and Kohn-Sham potential over the volume of the unit cell is
#%% -1.757312E+00, correctly, the difference between the band energy and kinetic energy.
#%%<END TEST_INFO>