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Outline
Motivation: [OI] 1s^2 2s^2 2p^4 S=1
Discovery stories of FSL (Martin Harwit)
spectro. notation (term symbols) : S, L, J
Spin-orbit-coupling (Russell-Saunders 1925)
- Pauli’s exclusion principle
- Hund’s rules (ground states)
CASE by CASE:
- particularly why for [OI] spin S = 1 (triplet)
- [OIII] and [CI] similar e-config, [CII] S=1/2
- energy levels, critical densities, ionis. pot.
Pauli’s exclusion principle
–Pauli (1925), based on empirical spectral data:
“No two electrons in an atom can exist in the same
quantum state; each electron must have a different
set of quantum numbers n, l, m_l, m_s. “
Pauli noticed that certain missing transitions would
correspond to two or more electrons in identical
quantum states (e.g. no He triplet lines observed).
Hund’s rules
• Hund 1927, based on empirical atomic spectra
Rule 1: unpaired, parallel spins preferred
Rule 2: maximizing orbital A.M. L is preferred
Rule 3: ground state: higher J, when shell > half full
E_J = A/2 [J(J+1) – L(L+1) – S(S+1)], A < 0
Reason: electrons with same spin need to have a wider
spatial distribution (which according to Pauli’s principle
correspond to different values m_l). The larger electron
separations (less overlap, less repulsion) indeed lead to
energetically more stable electronic configurations! (BE)
Oxygen [OI] spin-orbit states
3P states (S=1, L=1) fine structure lines
1D states (S=0, L=2) no spin, no FSL
1S states (S=0, L=0) no spin, no FSL
oxygen p sub-shell is more than half full
Hund’s rule then says 3P2 is ground state
nd
and 3P1 first excited state, 3P0 2 excited
(the other way round for [OIII] and [CI])
Oxygen [OI] multi-electron system:
outer sub-shell (4 electrons): 2p^4
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