ABSTRACT
The problem of the stability of the hydrogen atom when it is released from a confining environment is studied. The stability is analysed in terms of excitation and ionisation probabilities of the final state for different initial states. A spherical confining cavity of finite barrier height with inner radius
and thickness Δ with the nuclear position at its centre has been considered. The ionisation probability presents different sharply peaked, non-symmetric local maxima as a function of the confinement size. This behaviour is related to the energy of the initial confined state that presents several maxima and minima in a kink-like structure as a function of the confinement size. The physical origin of these effects has been explained in terms of tunnelling and re-tunnelling of the atomic states. The sudden approximation and the analytic continuation method have been employed.
GRAPHICAL ABSTRACT
![](/cms/asset/219c53c3-ba55-4dc0-b9dd-95c1caa95470/tmph_a_1547429_uf0001_oc.jpg)
Acknowledgements
A.S. would like to thank Dra. M Pilar de Lara Castells for many fruitful discussions and encouraging conversations during the realisation of this and other works.
Disclosure statement
No potential conflict of interest was reported by the authors.
ORCID
Antonio Sarsa http://orcid.org/0000-0002-7123-4598