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picture1_Quantum Theory Ppt 78981 | Zinnecker


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File: Quantum Theory Ppt 78981 | Zinnecker
outline motivation 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 ...

icon picture PPTX Filetype Power Point PPTX | Posted on 06 Sep 2022 | 3 years ago
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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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...Outline motivation s p discovery stories of fsl martin harwit spectro notation term symbols l j spin orbit coupling russell saunders pauli exclusion principle hund rules ground states case by particularly why for triplet and similar e config energy levels critical densities ionis pot based on empirical spectral data no two electrons in an atom can exist the same quantum state each electron must have a different set numbers n m noticed that certain missing transitions would correspond to or more identical g he lines observed atomic spectra rule unpaired parallel spins preferred maximizing orbital is higher when shell half full reason with need wider spatial distribution which according values larger separations less overlap repulsion indeed lead energetically stable electronic configurations be oxygen fine structure d sub than then says nd first excited other way round multi system outer...

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