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Ge+ and H2+: ESR g-tensor (epr program)
Sample directories: adf/Epr_Ge2+ and adf/Epr_H2+
The NMR/EPR program gives functionality that partially overlaps and partially
differs from the ESR keyword inside ADF. Please check the ADF and Property
Programs User's Guides for details.
In this example a scalar relativistic Pauli calculation is performed (ZORA is not
implemented in this program).
The preparatory ADF calculation can run parallel, the EPR module should run serial.
The ADF calculation should not use symmetry. It uses a high numerical integration accuracy. The revised PBE
functional is invoked. The implementation allows spin-unrestricted high-spin
inputs and as does the ESR implementation within ADF itself.
The H2+ example is very similar and in fact a but simpler, so it will not be
discussed separately here.
$ADFBIN/adf << eor
TITLE Ge2+, scf
SYMMETRY NOSYM
UNRESTRICTED
CHARGE +1 3
ATOMS Cart
1 Ge 0.0000 0.0000 -1.2344
2 Ge 0.0000 0.0000 1.2344
END
INTEGRATION 6.0
FRAGMENTS
Ge t21.Ge
END
COREPOTENTIALS t12.rel &
Ge 1
END
XC
GGA revPBE
END
RELATIVISTIC Scalar Pauli
END INPUT
eor
The
EPR calculation itself then has a fairly simple input. It uses the TAPE21 file
generated by ADF. The full EPR G-tensor is printed, including an extensive
analysis for the contribution of different terms.
The
input line
NUCLEI NONE
implies
that no NMR calculation is requested.
$ADFBIN/epr -n1 << eor
CLGEPR
EPRGT
SUBEND
NUCLEI NONE
OUTPUT
EPRSIZE LARGE
SUBEND
END
END INPUT
eor
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