abinit/tests/v8/Input/t29.abi

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# Hydrogen diatomic molecule for tests--constrained DFT
ndtset 7
#Constrained DFT
constraint_kind1 11 0
constraint_kind2 11 1
constraint_kind3 11 2
constraint_kind4 11 3
constraint_kind5 11 12
constraint_kind6 11 4
constraint_kind7 11 14
#Constrained DFT data
magcon_lambda 2
spinat 0.0 0.0 0.6 sqrt(0.18) 0.0 -sqrt(0.18)
chrgat 0.0 0.0
#Definition of the atomic spheres
ratsph 2.0 2.0
ratsm 0.05
#System description
acell 15 10 10
ntypat 2
znucl 1.0 1.0
so_psp 0 0
natom 2
typat 1 2
chksymtnons 3 # The default value for chksymtnons (which is 1) is not admitted in case of cDFT calculations.
nspden 4 nspinor 2 # Non-collinear case
nband 2
xcart -1.1 0.0 0.0
1.1 0.0 0.0
#Computational parameters
tolvrs 1.0d-10
nstep 35
ecut 5
pp_dirpath "$ABI_PSPDIR/PseudosTM_pwteter"
pseudos "1h.pspnc, 1h.pspnc"
#%%<BEGIN TEST_INFO>
#%% [setup]
#%% executable = abinit
#%% [files]
#%% files_to_test =
#%% t29.abo, tolnlines = 0, tolabs = 0.000e+00, tolrel = 0.000e+00
#%% [paral_info]
#%% max_nprocs = 1
#%% [extra_info]
#%% authors = X. Gonze
#%% references =
#%% keywords =
#%% description = H2 diatomic molecule, static, to check the constrained DFT implementation in case nspden=4
#%% with mixed constraints (different for different atomic types), and also fixing the amplitude or the direction.
#%% Case where the spheres overlap
#%% Interestingly, in the case where only the magnitude of the magnetization on the second atom is fixed,
#%% without fixing its charge, the optimal configuration gives a 90 degree difference of magnetization direction for both atoms.
#%% It would be interesting to understand the meaning of such results, and see whether one is not in a local minimum.
#%% A full mapping of the energy as a function of both magnitude and direction of the magnetization of the second atom would be interesting ...
#%%<END TEST_INFO>