Campuses:
This shows you the differences between two versions of the page.
| Both sides previous revisionPrevious revisionNext revision | Previous revision | ||
| classes:2009:fall:phys4101.001:q_a_1030 [2009/10/30 09:50] – x500_chap0326 | classes:2009:fall:phys4101.001:q_a_1030 [2009/11/30 16:32] (current) – youmans | ||
|---|---|---|---|
| Line 2: | Line 2: | ||
| **Return to Q&A main page: [[Q_A]]**\\ | **Return to Q&A main page: [[Q_A]]**\\ | ||
| **Q&A for the previous lecture: [[Q_A_1028]]**\\ | **Q&A for the previous lecture: [[Q_A_1028]]**\\ | ||
| - | **Q&A for the next lecture: [[Q_A_1103]]** | + | **Q&A for the next lecture: [[Q_A_1102]]** |
| **If you want to see lecture notes, click [[lec_notes]]** | **If you want to see lecture notes, click [[lec_notes]]** | ||
| Line 11: | Line 11: | ||
| I'm still a little confused as to how we can show that < | I'm still a little confused as to how we can show that < | ||
| + | ===Hardy 11:20 - 11/ | ||
| + | I also have a hard time to understanding the math inside this equation. It turns out to be equivalent to the proof of equation [3.31] in our textbook. I think the technique used in the proof must be very tricky and just a matter of math. | ||
| + | ===Blackbox 2:10 - 11/ | ||
| + | Yes, it' a kind of Fourier trick. If you look at the equation 2.144, then you would understand how this proof has been made. | ||
| + | === Can 10:48 11/06/09 === | ||
| + | For Chap < | ||
| + | ====ralph - 11:10AM 10/ | ||
| + | In problem 3.13 we had to show three parts. | ||
| + | ====ralph - 11:10AM 10/ | ||
| + | Now that I'm getting a better understanding of the new notation, can someone explain to me if it's possible to have multiple eigenvalues for the same state? | ||
| + | ===Hardy - 11:30 - 11/01/09=== | ||
| + | I think it can't be possible for a same state to have multiple eigenvalues. Because the state is determined by | ||
| + | < | ||
| + | ===Andromeda 10:51 11/01/09=== | ||
| + | the degenerate states of some operator share the same eigenvalues. for example in an atom two or more different configuration of electrons can have the same energy. | ||
| + | ====ralph - 11:10AM 10/ | ||
| + | My understanding is that the space-momentum uncertainty principle is analogous to the time-energy one. What are the implications of this? Should I change my understanding of how momentum and energy are related? | ||
| + | ===Andromeda 10:59 11/ | ||
| + | i think i might be overthinking this too but i am having trouble understanding the whole explanation of how energy time form of the uncertainty principle is a " | ||
| + | == prest121 23:10 11/1/2009 == | ||
| + | I think the point Griffiths is trying to make is that the momentum-position uncertainty principle resembles the energy-time uncertainty principle, primarily because the uncertainty for both is < | ||
| + | ====Dagny==== | ||
| + | What is a good method for finding the determinant of an nxn matrix? Do you think we will need to be able to find such a determinant in this class? Why or why not? | ||
| + | ====Jake22 4:30 11/ | ||
| + | Must all non-degenerate energy eigenfunctions be parity eigenfunctions? | ||
| -------------------------------------- | -------------------------------------- | ||
| **Return to Q&A main page: [[Q_A]]**\\ | **Return to Q&A main page: [[Q_A]]**\\ | ||
| **Q&A for the previous lecture: [[Q_A_1028]]**\\ | **Q&A for the previous lecture: [[Q_A_1028]]**\\ | ||
| - | **Q&A for the next lecture: [[Q_A_1103]]** | + | **Q&A for the next lecture: [[Q_A_1102]]** |