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Nov 02 (Mon)

Responsible party: Captain America, David Hilbert's hat

To go back to the lecture note list, click Lecture Notes
previous lecture note: Oct 30 (Fri) Uncertainty Principle
next lecture note: Nov 04 (Wed) Laplacian in Spherical Coordinate, Legendre Polynomals

Main class wiki page: Physics 4101.001 QM wiki page

Please try to include the following

  • main points understood, and expand them - what is your understanding of what the points were.
    • expand these points by including many of the details the class discussed.
  • main points which are not clear. - describe what you have understood and what the remain questions surrounding the point(s).
    • Other classmates can step in and clarify the points, and expand them.
  • How the main points fit with the big picture of QM. Or what is not clear about how today's points fit in in a big picture.
  • wonderful tricks which were used in the lecture.


Class input on main points of the beginning of Chapter 4:

  • \nabla^2 spherical coordinates
  • L^2, L_z, and why they have discrete values
  • The Hydrogen atom model
  • How spin affects this
  • Degenerate energies and states
  • Quantum numbers
    • Where are they from?
    • What do they do?

Using 3-D Coordinates: From the one-dimensional Schrodinger Equation: [-\frac{\hbar^2}{2m}\frac{ \partial^2}{ \partial x^2} + V(x)]\psi=E \psi

The kinetic energy term, -\frac{\hbar^2}{2m}\frac{\partial^2}{ \partial x^2}, must model the 3-Dimensional kinetic energy of the system, and therefore turns into:

[-\frac{\hbar^2}{2m}\nabla^2+ V(x)]\psi=E \psi

Where \nabla^2 is equal to \frac{ \partial^2}{ \partial x^2} + \frac{  \partial^2}{ \partial y^2} + \frac{ \partial^2}{ \partial z^2}

To Be Finished:

  • Discussion on The Angular Equation
  • Legendre Polynomials

To go back to the lecture note list, click Lecture Notes
previous lecture note: Oct 30 (Fri) Uncertainty Principle
next lecture note: Nov 04 (Wed) Laplacian in Spherical Coordinate, Legendre Polynomals

 
 
 
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