Physics 139B UCSC
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| * '''Lecture 4''', ~-Oct 8-~: <<la("L04-Perturbation-TI-D.pdf", "Perturbation: examples for the non-degenerate case and the theory for the degenerate case")>> | * '''Lecture 6''', ~-Oct 15-~: <<la("L06-Symmetry.pdf", "Symmetry")>> {{{#!wiki comment * <<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 5''', ~-Oct 10-~: <<la("L05-Perturbation-TI-D.pdf", "Time-independent perturbation---examples for the degenerate case---and Symmetry")>> * '''Lecture 4''', ~-Oct 8-~: <<la("L04-Perturbation-TI-D.pdf", "Time-independent perturbation: examples for the non-degenerate case and the theory for the degenerate case")>> {{{#!wiki comment * <<color("Addition:")>> Footnote 4: the word “topology” is added to reflect many recent research results on topological effects.—~-''<<DateTime(2013-10-10T16:23:14-0700)>>''-~ }}} |
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Lecture Notes
Lecture 6, Oct 15: Symmetry
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