Nature Abstract
Abstract
The excess proton in water has many anomalous properties,
most notably its unexpectedly high mobility. Such
unusual characteristics, together with the difficulty
of extracting unambiguous information from experiment, have fueled a
century-long scientific debate that remains unresolved. Starting
with de Grotthuss, who nearly 200 years ago ingeniously introduced the
concept of ``structural diffusion,'' various mechanistic explanations, such
as thermally induced hopping, proton tunneling, or solvation effects
have been put forward. The more recent literature has been mainly
polarized around two seemingly opposing structural models for the hydrated
proton. Eigen proposed the formation of an H9
O4+
complex, wherein an H3
O+ core is strongly
hydrogen bonded to three H2
molecules. Zundel, in contrast, supported the notion of an
H5O2
+ complex, in which
the proton is shared between two H2
molecules. In this study, a powerful computer simulation technique
is applied, which includes time-independent equilibrium thermal
and quantum fluctuations of all nuclei and determines internuclear
interactions from the electronic structure. The key findings are:
(I) The hydrated proton forms a fluxional defect, with
H9O4
+
and H5O2
+II) This defect can become deloclized over several hydrogen
bonds due to quantum fluctuations. (III) Solvent
polarization induces a small transfer barrier, which is
washed out by zero-point motion. This can be classified as a
``low-barrier hydrogen bond,'' where tunneling is negligible
and the simplest of transition state concepts to not apply.
(IV) The rate of structural diffusion is determined by
thermally induced hydrogen-bond breaking in the second solvation shell.