In a molecule, hydrogen sometimes resembles not a ball but a wave that can leak through an energy barrier, like a ghost through a wall. Chemists call this tunneling, and it underlies many processes, from enzyme function to charge transfer in materials. But how exactly does a molecule find its path for such a transition? For a long time, we could only see the starting and ending points, while the route itself remained shrouded in mist.
The new work offers a map of this invisible route. The researchers created a method called V-SHAKE, which, like a leash, holds a molecule on the "seam": the boundary where the initial and final states have equal energy. Previously, we could only guess what happens at this boundary, but now we can stroll along it and examine every stone.
The method was applied to two molecules: 4-cyanobutanolate (CBO) and (Z)-4-hydroxybut-3-en-2-one (HEO). In each, a hydrogen atom can jump from one oxygen atom to another. It turns out that the interaction strength between states, the so-called vibronic coupling, is not constant but varies widely. It is like the tension of a rubber band, which depends on how stretched the band itself is.
Previously, theories of tunneling reaction rates assumed that the coupling could be considered constant near the transition point. The new data show that for one molecule this approximation works, but for the other it does not. In CBO, configurations were found with energy close to the minimum but with significantly stronger coupling. This means the molecule has more freedom than we thought.
And here we are again, standing on the seam, but now with a map in hand. Hydrogen glides along it like a dancer on a tightrope, and at last we see which movements help it keep its balance. This method can already be applied to test models of tunneling reactions in chemistry and biology, especially in calculating kinetic isotope effects, a sensitive indicator of hydrogen's quantum behavior.
The vibronic coupling between reactant and product states can change by an order of magnitude when the donor-acceptor distance changes by only 0.1 Å, which is comparable to the thickness of a single atomic layer.