Physics 139B UCSC
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* '''Lecture 9''', ~-Oct 24-~: <<la("L09-Variational-Principle.pdf", "Variational principle")>> * '''Lecture 8''', ~-Oct 22-~: <<la("L08-Hydrogen-like-atom.pdf", "Hydrogen-like atom (cont.)")>> * '''Lecture 7''', ~-Oct 17-~: <<la("L07-Symmetry-Hydrogen-like-atom.pdf", "Hydrogen-like atom")>> {{{#!wiki comment * <<color("Additions:")>> Footnotes 7 and 8.—~-''<<DateTime(2013-10-22T12:07:21-0700)>>''-~ }}} |
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| * <<color("Correction:")>> Section 6.3.3 is revised, to explicitly add vector notations for the angular momentum vectors, and an important correction: “total spin” → &lduo;total angular momentum” in the second paragraph.—~-''<<DateTime(2013-10-10T16:46:44-0700)>>''-~ | * <<color("Addition:")>> A note added in page 9.—~-''<<DateTime(2013-10-14T18:39:27-0700)>>''-~ * <<color("Correction:")>> Section 6.3.3 is revised, to explicitly add vector notations for the angular momentum vectors, and an important correction: “total spin” → “total angular momentum” in the second paragraph.—~-''<<DateTime(2013-10-10T16:46:44-0700)>>''-~ |
Lecture Notes
Lecture 9, Oct 24: Variational principle
Lecture 8, Oct 22: Hydrogen-like atom (cont.)
Lecture 7, Oct 17: Hydrogen-like atom
Additions: Footnotes 7 and 8.—12:07PM, Oct 22, 2013
Lecture 6, Oct 15: Symmetry
Addition: A note added in page 9.—6:39PM, Oct 14, 2013
Correction: Section 6.3.3 is revised, to explicitly add vector notations for the angular momentum vectors, and an important correction: “total spin” → “total angular momentum” in the second paragraph.—4:46PM, Oct 10, 2013
Lecture 5, Oct 10: Time-independent perturbation—examples for the degenerate case—and Symmetry
Lecture 4, Oct 8: Time-independent perturbation: examples for the non-degenerate case and the theory for the degenerate case
Addition: Footnote 4: the word “topology” is added to reflect many recent research results on topological effects.—4:23PM, Oct 10, 2013
Lecture 3, Oct 3: Perturbation theory (time-independent, non-degenerate)
Lecture 2, Oct 1: Representation, Symmetry
Change: Page 14: Notations in the Bart box are consistent with the lecture, now.—1:33PM, Oct 03, 2013
Lecture 1, Sep 26: QM Formalism