1 / 15

Who I am: Dan Dessau Dessau@Colorado Prof. Shepard will be back on Wed.

Who I am: Dan Dessau Dessau@Colorado.edu Prof. Shepard will be back on Wed. In 2D:. Chapter 8. The 3D Schrodinger Equation. In 1D:. In 3D:.

addison
Download Presentation

Who I am: Dan Dessau Dessau@Colorado Prof. Shepard will be back on Wed.

An Image/Link below is provided (as is) to download presentation Download Policy: Content on the Website is provided to you AS IS for your information and personal use and may not be sold / licensed / shared on other websites without getting consent from its author. Content is provided to you AS IS for your information and personal use only. Download presentation by click this link. While downloading, if for some reason you are not able to download a presentation, the publisher may have deleted the file from their server. During download, if you can't get a presentation, the file might be deleted by the publisher.

E N D

Presentation Transcript


  1. Who I am: Dan Dessau Dessau@Colorado.edu Prof. Shepard will be back on Wed.

  2. In 2D: Chapter 8. The 3D Schrodinger Equation In 1D: In 3D: Instead of doing a lengthy mathematical proof we will see from various examples that this indeed seems to be the correct generalization of the 1D equation.

  3. Simplest case: 3D box, infinite wall strength V(x,y,z) = 0 inside, = infinite outside. Use separation of variables y(x,y,z) = X(x)Y(y)Z(z)

  4. y(x,y,z) = X(x)Y(y)Z(z) plug in and see what happens! Divide both sides by XYZ

  5. The left side is a constant with respect to x: A) True B) False  The right side is independent from x!  left side must be independent from x as well!!

  6. If we call this const. '-kx2' we can write: X"(x) = - kx2 X(x)  This is the Schrödinger equation for a particle in a one-dimensional rigid box!! We already know the solutions for this equation:

  7. Repeat for Y and Z: And:

  8. or: with: And the total energy is: Now, remember: y(x,y,z) = X(x)Y(y)Z(z) Done! • What is the energy of a particle in the 3D box? • Ex • Ey • Ez • Ex = Ey = Ez • Ex + Ey + Ez

  9. 2D box: Square of the wave function for nx=ny=1 y Probability to find electron at a certain location in the box. Percent relative to maximum |Y(y)|2 |X(x)|2 x y(x,y,z) = X(x)Y(y)Z(z)

  10. 2D box: Square of the wave function of selected excited states 100% 0% ny nx

  11. Degeneracy Sometimes, there are several solutions with the exact same energy. Such solutions are called ‘degenerate’.

  12. The ground state energy of the 2d box of size L x L is 2E0, where E0 = p2ħ2/2mL2 is the ground state energy of a 1d box of size L. y L E=E0(nx2+ny2) x L What is the energy of the 1st excited state of this 2D box? • 3Eo • 4Eo • 5Eo • 8Eo

  13. L x L The ground state energy of the 2d box of size L x L is 2E0, where E0 = p2ħ2/2mL2 is the ground state energy of a 1d box of size L. E=E0(nx2+ny2) What is the energy of the 1st excited state of this 2D box? • 3Eo • 4Eo • 5Eo • 8Eo nx=1, ny=2 or nx=2 ny=1

  14. L L L • Imagine a 3d cubic box of sides L x L x L. What is the degeneracy of the ground state and the first excited state? • Gnd, 1st • 1 , 1 • 3, 1 • 1, 3 • 3, 3

  15. L L L • Imagine a 3d cubic box of sides L x L x L. What is the degeneracy of the ground state and the first excited state? • Gnd, 1st • 1 , 1 • 3, 1 • 1, 3 • 3, 3 Ground state = 1,1,1 1st excited state: 2,1,1 1,2,1 1,1,2

More Related