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Quantum Physics III Chapter 2: Hydrogen Fine Structure
2.1. REVIEWOFHYDROGENATOM 29 When we form ℓ⊗swe are tensoring a a full ℓmultiplet to an smultiplet (here, of course, s= 1/2). All states in ℓ⊗sare eigenstates of Lˆ2 and eigenstates of Sˆ2, so ℓand sare good (constant) quantum numbers for all jmultiplets that arise in …
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