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.)")>> {{{#!wiki comment * <<color("Corrections:")>> Quite a few small corrections after proof-reading.—~-''<<DateTime(2013-10-22T12:37:15-0700)>>''-~ }}} |
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{{{#!wiki comment * <<color("Addition:")>> Page 8, a new paragraph at the end of Section 7.4.—~-''<<DateTime(2013-10-28T14:50:34-0700)>>''-~ * <<color("Corrections:")>> Page 8, before Eq. 7.13: $m_e^4c^4 \rightarrow m_e^2c^4$, and $m_ec^4 \rightarrow m_ec^2$.—~-''<<DateTime(2013-10-24T13:10:54-0700)>>''-~ * <<color("Additions:")>> Footnotes 7 and 8.—~-''<<DateTime(2013-10-22T12:07:21-0700)>>''-~ }}} |
Lecture Notes
Lecture 9, Oct 24: Variational principle
Lecture 8, Oct 22: Hydrogen-like atom (cont.)
Corrections: Quite a few small corrections after proof-reading.—12:37PM, Oct 22, 2013
Lecture 7, Oct 17: Hydrogen-like atom
Addition: Page 8, a new paragraph at the end of Section 7.4.—2:50PM, Oct 28, 2013
Corrections: Page 8, before Eq. 7.13: $m_e^4c^4 \rightarrow m_e^2c^4$, and $m_ec^4 \rightarrow m_ec^2$.—1:10PM, Oct 24, 2013
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