CCL: ZPE in non-stationary points
- From: Jussi Lehtola <jussi.lehtola|helsinki.fi>
- Subject: CCL: ZPE in non-stationary points
- Date: Sun, 4 Nov 2012 02:10:11 +0200
Sent to CCL by: Jussi Lehtola [jussi.lehtola]^[helsinki.fi]
On Sat, 3 Nov 2012 16:05:34 -0700 (PDT)
"Sebastian Kozuch kozuchs]~[yahoo.com"
<owner-chemistry[A]ccl.net> wrote:
> Dear all,
> Does anyone know of a (simple) method to calculate ZPE and maybe
> Gibbs energies for geometries that are not stationary points (i.e.
> not a stable intermediate or a TS)? How valid is a typical frequency
> calculation for these geometries?
Please elaborate on what you mean.
Zero point vibrations only make sense in cases where the potential can
be expanded locally as a Taylor series as
V(r) ~ V(r0) + (r-r0)*d2V/dr2*(r-r0)
where d2V/dr2 is the Hessian computed at r0. This means that you must
be in a stationary point, since the first derivative (gradient) needs to
vanish.
Secondly, any stationary point will not do, since otherwise you will
have a saddle point, meaning that vibrations do not exist in some
directions, instead the system is just unstable: when the system is
pushed in this direction, it will not start to oscillate around the
configuration in the stationary point, instead the perturbation will
just start growing.
To calculate ZPE you need a bound system. This is not the case even for
all stationary points -- and even less for non-stationary points.
--
--------------------------------------------------------
Mr. Jussi Lehtola, M. Sc. Doctoral Student
jussi.lehtola[A]helsinki.fi Department of Physics
http://www.helsinki.fi/~jzlehtol University of Helsinki
Office phone: +358 9 191 50 632 Finland
--------------------------------------------------------
Jussi Lehtola, FM Tohtorikoulutettava
jussi.lehtola[A]helsinki.fi Fysiikan laitos
http://www.helsinki.fi/~jzlehtol Helsingin Yliopisto
TyÃpuhelin: (0)9 191 50 632
--------------------------------------------------------