129x Filetype PPTX File size 0.24 MB Source: www.mpia.de
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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