The
Current Image of the Fundamental Asymmetry of Time and Space in Molecular
Dynamics
Martin Quack
ETH Zurich, Switzerland
The
traditional image of time and space in molecular dynamics pictured them in two equivalent
mirror image forms each, with a space inverted and a time reversed system being
equivalent to the original systems before taking the mirror image. In technical
terms this corresponds to the symmetry under space inversion and time reversal
in the dynamical system. Symmetries can furthermore be related to conservation
laws and ‘nonobservables’ .
The inversion symmetry of space, for instance, corresponds to parity
conservation. Since the discovery of parity violation 50 years ago in nuclear
and high energy physics, we know that the mirror image of a molecule does not
exactly correspond to the physically realized enantiomer,
or ‘mirror image isomer’, thus the real
image shows a slight asymmetry, which also is observable as a slight energy
difference between enantiomers of chiral
molecules.
The
spectroscopic observation of the small parity violating energy difference DpvE between
the two enantiomers of a chiral molecule predicted within the framework of
the standard model of high energy physics remains one of the greatest
challenges of current molecular physics with possible consequences also for biomolecular evolution [1-3].
A possible,
very difficult spectroscopic experiment has been proposed by us about two
decades ago [4,5].The first requirement for such an
experiment is the analysis of rovibrationally
resolved optical(infrared or visible or ultraviolet) spectra of chiral molecules and
the experimental breakthrough achieving
this goal arose from work in our group around 1995(see refs 1-3 for reviews). A
major theoretical breakthrough occurred about at the same time , when we
discovered that earlier estimates for DpvE were
too low by one to two orders of magnitude for the prototype molecules H2O2
and H2S2 and also other chiral
molecules [6-8]. This striking result has in the
meantime been reconfirmed by a variety of other quantum chemical techniques and
from other theoretical groups and can be considered reliable (for a recent
review see [1-3]). Still the predicted energy
differences remain very small; in the Attohartree
range 10–18 Eh
to 10–15 Eh or
2.6 pJ mol–1 to 2.6 nJ mol–1 is fairly typical, depending on
the molecule. The corresponding spectroscopic challenge is substantial. In the
lecture we shall report about current experimental and theoretical work of the
Zurich group (see also [9,10]) also in relation to work of other
groups. If time permits we will also discuss possible CPT tests according to
our scheme [1,11]. This, indeed, would lead to a
completely revised image of time and space asymmetries in physics and
chemistry.
References:
1. M.
Quack, in Modelling Molecular Structure
and Reactivity in Biological Systems, Proc. 7th WATOC Congress , Capetown 2005, edited by K. Naidoo,
J. Brady, M. Field, J. Gao, and M. Hann (Royal Society of Chemistry, Cambridge, 2006), pp. 3 -
38.
2. M. Quack and J. Stohner, Chimia 59, 530-538 (2005).
3. M. Quack, Angew. Chem. Int. Ed. (Engl.) 114,
4618-4630 (2002).
4. M. Quack, Chem. Phys. Lett.
132, 147-153
(1986).
5. M. Quack, Angew. Chem. Int. Ed. (Engl.) 28,
571-586 (1989).
6. A. Bakasov, T. K.
Ha, and M. Quack, in Chemical Evolution,
Physics of the Origin and Evolution of Life, Proc. of the 4th Trieste
Conference (1995), edited by J. Chela-Flores and
F. Raulin (Kluwer Academic
Publishers, Dordrecht, 1996), pp. 287-296.
7. A. Bakasov,
T. K. Ha, and M. Quack, J. Chem. Phys. 109,
7263-7285 (1998).
8. R. Berger and M.
Quack, J. Chem. Phys. 112 (7), 3148-3158 (2000).
9. R.
Berger, G. Laubender, M. Quack, A. Sieben, J. Stohner, and M. Willeke, Angew. Chem.
Int. Ed. (Engl.) 44, 3623-3626
(2005).
10. M. Quack and M. Willeke, J. Phys. Chem. A 110, 3338-3348 (2006).
11. M. Quack,chapter 27 in Femtosecond
Chemistry, Proc. Berlin Conf. Femtosecond Chemistry, Berlin (March 1993),
edited by J. Manz and L. Woeste
(Verlag Chemie, Weinheim, 1995), pp. 781-818.