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 | | time | views | |
 | L14.2 Quantization of the magnetic field on a torus | 25:15 | 1,487 | |
 | L4.1 Scales and zeroth-order spectrum | 25:51 | 1,430 | |
 | L9.1 The interaction picture and time evolution | 26:34 | 1,501 | |
 | L23.4 Symmetric and Antisymmetric states of N particles | 11:35 | 775 | |
 | L21.2 Phase shifts and impact parameter | 27:39 | 801 | |
 | L17.3 Properties of Berry's phase | 11:13 | 1,239 | |
 | L21.1 General computation of the phase shifts | 18:15 | 849 | |
 | L18.2 Effective nuclear Hamiltonian. Electronic Berry connection | 20:30 | 713 | |
 | L2.4 Degenerate Perturbation Theory: Leading energy corrections | 6:52 | 1,916 | |
 | L6.1 Zeeman effect and fine structure | 13:70 | 6,533 | |
 | L5.2 Interpretation of the Darwin correction from nonlocality | 21:47 | 1,155 | |
 | L6.3 Weak-field Zeeman effect; the projection lemma | 19:10 | 1,326 | |
 | L8.4 Deriving the connection formulae (continued) logical arrows | 14:45 | 660 | |
 | L14.4 Landau levels (continued). Finite sample | 9:80 | 966 | |
 | L3.1 Remarks on a 'good basis' | 17:39 | 1,776 | |
 | L10.3 Integrating over the continuum to find Fermi's Golden Rule | 19:38 | 1,393 | |
 | L1.2 Setting up the perturbative equations | 16:90 | 7,578 | |
 | L20.2 The one-dimensional analogy for phase shifts | 16:58 | 899 | |
 | L5.5 Assembling the fine-structure corrections | 15:23 | 892 | |
 | L19.3 Differential and total cross section | 20:21 | 3,096 | |
 | L18.3 Example: The hydrogen molecule ion | 27:20 | 746 | |
 | L10.4 Autoionization transitions | 11:31 | 626 | |
 | L7.1 The WKB approximation scheme | 22:51 | 3,010 | |
 | L11.1 Harmonic transitions between discrete states | 15:13 | 709 | |
 | L4.4 Dirac equation for the electron and hydrogen Hamiltonian | 15:10 | 6,752 | |
 | L5.4 Spin-orbit correction | 8:32 | 1,409 | |
 | L15.4 Instantaneous energy eigenstates and Schrodinger equation | 26:47 | 730 | |
 | L24.4 The symmetrization postulate (continued) | 20:51 | 1,159 | |
 | L6.4 Strong-field Zeeman | 9:50 | 1,058 | |
 | L22.3 Diagrammatic representation of the Born series. Scattering amplitude for spherically symm... | 21:42 | 728 | |
 | L20.1 Review of scattering concepts developed so far | 9:30 | 972 | |
 | L23.1 Permutation operators and projectors for two particles | 22:23 | 640 | |
 | L10.1 Box regularization: density of states for the continuum | 20:32 | 1,139 | |
 | L21.3 Integral equation for scattering and Green's function | 30:27 | 1,953 | |
 | L13.5 Charged particles in EM fields: Schrodinger equation | 8:39 | 883 | |
 | L3.4 Degeneracy resolved to second order (continued) | 11:36 | 863 | |
 | L5.1 Evaluating the Darwin correction | 12:51 | 1,430 | |
 | L7.2 Approximate WKB solutions | 19:20 | 1,187 | |
 | L1.3 Calculating the energy corrections | 6:27 | 4,510 | |
 | L14.3 Particle in a constant magnetic field: Landau levels | 18:20 | 1,953 | |
 | L16.2 Analysis with an orthonormal basis of instantaneous energy eigenstates | 14:32 | 665 | |
 | L12.3 Einstein's argument: the need for spontaneous emission | 19:32 | 706 | |
 | L15.3 Phase space and intuition for quantum adiabatic invariants | 16:24 | 721 | |
 | L24.1 Symmetrizer and antisymmetrizer for N particles | 16:50 | 619 | |
 | L15.1 Classical analog: oscillator with slowly varying frequency | 16:35 | 724 | |
 | L3.2 Degeneracy resolved to first order; state and energy corrections | 29:12 | 1,681 | |
 | L16.1 Quantum adiabatic theorem stated | 13:30 | 1,662 | |
 | L23.2 Permutation operators acting on operators | 11:45 | 497 | |
 | L4.3 The Pauli equation for the electron in an electromagnetic field | 18:12 | 2,067 | |
 | L20.3 Scattering amplitude in terms of phase shifts | 15:00 | 1,084 | |
 | L22.4 Identical particles and exchange degeneracy | 19:42 | 1,402 | |
 | L11.2 Transition rates for stimulated emission and absorption processes | 17:13 | 756 | |
 | L11.3 Ionization of hydrogen: conditions of validity, initial and final states | 20:55 | 653 | |
 | L12.4 Einstein's argument: B and A coefficients | 9:43 | 543 | |
 | L20.5 Identification of phase shifts. Example: hard sphere | 18:20 | 888 | |
 | L12.1 Ionization rate for hydrogen: final result | 16:24 | 508 | |
 | L20.4 Cross section in terms of partial cross sections. Optical theorem | 13:14 | 994 | |
 | L16.4 Landau-Zener transitions | 19:31 | 1,044 | |
 | L18.1 Born-Oppenheimer approximation: Hamiltonian and electronic states | 24:49 | 2,307 | |
 | L9.4 Setting up perturbation theory | 6:36 | 787 | |
 | L8.2 Asymptotic expansions of Airy functions | 19:38 | 915 | |
 | L2.2 Anharmonic Oscillator via a quartic perturbation | 20:56 | 3,168 | |
 | L24.2 Symmetrizer and antisymmetrizer for N particles (continued) | 24:55 | 615 | |
 | L7.3 Validity of the WKB approximation | 17:10 | 1,162 | |
 | L17.2 Berry's phase and Berry's connection | 25:50 | 2,744 | |
 | L9.3 Example: Instantaneous transitions in a two-level system | 29:25 | 888 | |
 | L22.1 Setting up the Born Series | 21:80 | 846 | |
 | L17.1 Configuration space for Hamiltonians | 15:28 | 1,454 | |
 | L12.2 Light and atoms with two levels, qualitative analysis | 14:32 | 536 | |
 | L8.3 Deriving the connection formulae | 22:32 | 659 | |
 | L5.3 The relativistic correction | 19:16 | 1,529 | |
 | L6.2 Weak-field Zeeman effect; general structure | 10:90 | 1,647 | |
 | L15.2 Classical adiabatic invariant | 15:80 | 798 | |
 | L13.4 Charged particles in EM fields: potentials and gauge invariance | 21:51 | 1,300 | |
 | L13.2 Transition rates induced by thermal radiation (continued) | 16:36 | 444 | |
 | L13.3 Einstein's B and A coefficients determined. Lifetimes and selection rules | 13:55 | 726 | |
 | L23.3 Permutation operators on N particles and transpositions | 29:40 | 627 | |
 | 28. Modern Electronic Structure Theory: Basis Sets | 50:60 | 6,297 | |
 | 36. Time Dependence of Two-Level Systems: Density Matrix, Rotating Wave Approximation | 48:41 | 3,438 | |
 | 9. The Harmonic Oscillator: Creation and Annihilation Operators | 48:14 | 2,434 | |
 | 8. Quantum Mechanical Harmonic Oscillator | 52:28 | 2,678 | |
 | 20. Hydrogen Atom I | 48:57 | 3,614 | |
 | 34. Chirped Pulse Microwave: Free Induction Decay, Bloch Visualization | 50:27 | 236 | |
 | 26. Qualitative MO Theory: Hückel | 52:48 | 803 | |
 | 17. Rigid Rotor I; Orbital Angular Momentum | 51:29 | 1,593 | |
 | 29. Modern Electronic Structure Theory: Electronic Correlation | 52:13 | 1,522 | |
 | 32. Intermolecular Interactions by Non-Degenerate Perturbation Theory | 54:30 | 802 | |
 | 31. Time-Dependent Perturbation Theory II: H is Time-Dependent: Two-Level Problem | 52:45 | 918 | |
 | 25. Molecular Orbital Theory II; H2+, A2, AB Diatomics | 53:60 | 831 | |
 | 3. Two-Slit Experiment; Quantum Weirdness | 50:58 | 4,321 | |
 | 5. Quantum Mechanics: Free Particle and Particle in 1D Box | 54:39 | 3,348 | |
 | 7. Classical Mechanical Harmonic Oscillator | 51:11 | 1,609 | |
 | 13. From Hij Integrals to H Matrices I | 54:36 | 972 | |
 | 19. Spectroscopy: Probing Molecules with Light | 50:37 | 1,190 | |
 | 10. The Time-Dependent Schrödinger Equation | 52:23 | 1,747 | |
 | 21. Hydrogen Atom II; Rydberg States | 52:42 | 835 | |
 | 22. Helium Atom | 52:41 | 1,420 | |
 | 23. Many-Electron Atoms | 51:60 | 861 | |
 | 2. Wave Nature of the Electron and the Internal Structure of an Atom | 45:16 | 6,767 | |
 | 11. Wavepacket Dynamics for Harmonic Oscillator and PIB | 54:59 | 152 | |
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