Last hour Selection rules for el dipole transitions

  • Slides: 3
Download presentation
Last hour: • Selection rules for el. dipole transitions in the H-atom: • ℓ

Last hour: • Selection rules for el. dipole transitions in the H-atom: • ℓ = ± 1; m = 0 (z- direction) or m = ± 1 (xy plane) • Addition of angular momenta: L = |ℓ 1 - ℓ 2|. . . |ℓ 1 + ℓ 2| in steps of 1 • Recap on electron spin: two EF’s: (up) and (down); s = ½ ; ms = ±½ • Pauli Principle: The total WF must be antisymmetric w. r. to exchange of two electrons a singlet state has symmetric spatial, antisymmetric spin function, triplet vice versa. • Pauli Exclusion Principle: No two e- can have the same set of quantum numbers. Example: 1 st excited state of He • Singlet: symmetric spatial WF, antisymm. spin function • Triplet: antisymmetric spatial WF, symm. spin function

L-S coupling in multielectron atoms: • Every electron has angular momentum • Define and

L-S coupling in multielectron atoms: • Every electron has angular momentum • Define and spin . ”total orbital angular momentum” • The individual but in the absence of spin-orbit interaction for each electron, the total angular momentum is conserved! That means we can label the states by the quantum number L • Define: ”total spin” → label with quantum number S • Define ”total angular momentum” → label with quantum number J = |L+S|. . . |L-S| in steps of 1 • Levels of the same L are called terms and are described by a capital letter: S, P, D, F, . . . • MJ (z-projection of J) can have values between –J and +J in steps of 1 • Unsöld’s Theorem: Full shells and subshells have L = 0, S = 0 e. g. L(1 s 2) = 0; L(2 p 6) = 0 • Atomic term symbols: 2 S+1 L J

John Robinson Pierce, American engineer and author. Coined the term "transistor”, wrote science fiction

John Robinson Pierce, American engineer and author. Coined the term "transistor”, wrote science fiction under the pseudonym “J. J. Coupling” http: //en. wikipedia. org/wiki/File: John_Robinson_Pierce. jpg