Chemist@
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If an electron gets excited from K to L shell, it will actually finish in the 2p subshell and then deexcite to 2s and 1s at the end, right?
The discussion revolves around the excitation and de-excitation processes of electrons in atomic shells, specifically focusing on transitions between the K and L shells and the implications of selection rules on these transitions. The scope includes theoretical aspects of quantum mechanics and atomic structure.
Participants express differing views on the allowed transitions between energy levels, with some asserting that direct transitions are possible while others argue that selection rules prohibit certain transitions. The discussion remains unresolved regarding the implications of these rules on the de-excitation processes.
There are limitations regarding the assumptions made about the selection rules and the specific conditions under which transitions occur. The discussion does not resolve the mathematical details or the implications of the cited sources.
One notable feature of the above is that the 2s level of hydrogen cannot decay: the only lower energy level is 1s, and the parity selection rule forbids this. The 2s level instead decays by two-photon decay: H(2s) → H(1s) + γ + γ. The sum of the energies of the two emitted photons is E2s−E1s = 10.2 eV. The photons have a continuous spectrum since there is no other constraint on their energies. This is a major contributor to the UV/optical continuum from many nebulae.