Autoionization is a process by which an atom or a molecule in an excited state spontaneously emits one of the electron shell , thus going from a state with charge to a state with charge , for example from an electrically neutral state to a singly ionization state.
Autoionizing states are usually short-half-life, and thus can be described as rather than normal . They can be observed as variations in the ionization cross sections of atoms and molecules, by photoionization, electron ionization and other methods.
Other resonances are attributed to two-electron excitations. The same neon photoionization spectrum considered above contains a fourth strong resonance in the same region at 44.979 eV but with a very different shape, which is interpreted as the 1s2 2s2 2p4 3s 3p (1P) state. For autoionization, the 3s → 2p transition provides the energy to remove the 3p electron.
Electron ionization allows the observation of some states which cannot be excited by photons due to selection rules. In neon for example again, the excitation of triplet states is forbidden by the spin selection rule ΔS = 0, but the 1s2 2s2 2p4 3s 3p (3P) has been observed by electron ionization at 42.04 eV.Bolduc, E., Quéméner, J.J. and Paul Marmet (1972) Autoionizing 2s2 2p4 3s 3l States of Ne and Related Ne− Resonances, J. Chem. Phys. 57
If a core electron is missing, a positive ion can autoionize further and lose a second electron in the Auger effect. In neon, X-ray excitation can remove a 1s electron, producing an excited Ne+ ion with configuration 1s1 2s2 2p6. In the subsequent Auger process a 2s → 1s transition and simultaneous emission of a second electron from 2p leads to the Ne2+ 1s2 2s1 2p5 ionic state.
Molecules, in addition, can have vibrationally autoionizing , in which the small amount of energy necessary to ionize a Rydberg state is provided by vibrational excitation.
/ref> Ion impact by high energy H+, He+ and Ne+ ions has also been used.
Autodetachment
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