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Finally we compute PtCl4H22- from the fragments PtCl42- and H2.
title PtCl4 H2
units
length bohr
end
integration 4.0
xc
LDA vwn
GGA becke perdew
end
relativistic scalar
corepotentials t12rel &
H 0
Cl 1
Pt 2
end
ATOMS
Pt 0 0 0 f=PtCl4
Cl 4.361580 0.000000 0.00000000 f=PtCl4
Cl 0.000000 4.361580 0.00000000 f=PtCl4
Cl -4.361580 0.000000 0.00000000 f=PtCl4
Cl 0.000000 -4.361580 0.00000000 f=PtCl4
H 0.0 0.0 5.58 f=H2
H 0.0 0.0 7.26 f=H2
end
fragments
PtCl4 t21PtCl4
H2 t21H2
end
end input
eor
Note that, although the key CHARGE is not supplied, the molecule is not neutral: the default charge (that is, omitting the keys CHARGE, OCCUPATIONS) is the sum-of-fragments: the fragments here are H2 and PtCl42-, yielding a net charge for the molecule of minus two.
Note the F= fragment specification in the ATOMS block. No fragment-numbering suffix (/n) is required because there is only one fragment of each fragment type.