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C2H6 internal rotation: TS search using partial Hessian
Sample directory: adf/TS_C2H6/
Frequently when searching for a transition state, one needs an accurate
second derivatives matrix, a Hessian. An exact Hessian may be obtained analytically
but this may be very expensive for large molecules. In such cases it may be beneficial
to calculate Hessian matrix elements only for atoms directly involved in the
reaction for which a transition state is sought for. The rest of the Hessian
can then be approximated using a cheaper method.
In this example, a saddle point of the ethane internal rotation around C-C
bond is found. In principle, only hydrogen atoms contribute to the normal mode
we are interested in. Therefore we calculate a partial Hessian matrix
including hydrogen atoms only. For this purpose, the AnalyticalFreq block key
is used. In this block, a NUC keyword is added specifying that the second derivatives
are calculated for atom 3 (and its symmetry-equivalents) only. Note that the Hessian matrix
elements between symmetry-equivalent atoms, for example between 3,H and 4.H are also calculated.
The rest of the matrix is estimated using the default method.
$ADFBIN/adf <<eor
TITLE Ethane transition state search using partial Hessian
ATOMS
1 C 0.000000000000 0.000000000000 0.767685465031
2 C 0.000000000000 0.000000000000 -0.767685465031
3 H 0.964354016767 0.347635559279 1.177128271450
4 H -0.181115782790 -1.008972856410 1.177128271450
5 H -0.783238233981 0.661337297125 1.177128271450
6 H -0.500471876676 0.894626767091 -1.177128271450
7 H -0.524533568868 -0.880734742626 -1.177128271450
8 H 1.025005445540 -0.013892024465 -1.177128271450
END
BASIS
type DZ
core Large
END
AnalyticalFreq
NUC 3
End
INTEGRATION 5.0 5.0 5.0
eor
After the Hessian is calculated, the resulting TAPE21 file is used for
a subsequent transition state search:
mv TAPE21 ethane-frq.t21
$ADFBIN/adf <<eor
TITLE Ethane transition state search using partial Hessian
ATOMS
1 C 0.000000000000 0.000000000000 0.767685465031
2 C 0.000000000000 0.000000000000 -0.767685465031
3 H 0.964354016767 0.347635559279 1.177128271450
4 H -0.181115782790 -1.008972856410 1.177128271450
5 H -0.783238233981 0.661337297125 1.177128271450
6 H -0.500471876676 0.894626767091 -1.177128271450
7 H -0.524533568868 -0.880734742626 -1.177128271450
8 H 1.025005445540 -0.013892024465 -1.177128271450
END
Fragments
H t21.H
C t21.C
END
GEOMETRY
smooth conservepoints
TransitionState mode=1
optim All Cartesian
iterations 30
step rad=0.15
hessupd BOFILL
converge e=1.0e-4 grad=1.0e-3 rad=1.0e-3
END
RESTART ethane-frq.t21
INTEGRATION 5.0 5.0 5.0
eor
Important note: care should be taken to specify correct mode in the
TransitionState keyword. Because a significant part of the Hessian will not be
calculated exactly, it is possible that it will have more than one negative eigenvalue,
in which case the one we are interested in may not be the first one. In such a case,
one needs to specify the correct mode number in the TransitionState keyword.
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