| Thread Closed |
Quantum Operators (or just operators in general) |
Share Thread | Thread Tools |
| Feb15-10, 05:36 PM | #18 |
|
|
Quantum Operators (or just operators in general)
The normalization condition always turns out to be real because the squared terms always involve the multiplication of a complex number by its conjugate and the cross terms are complex conjugates of each other so when they combine, the imaginary part cancels out.
In this problem, because c is assumed to be real, a and b can be real simultaneously. You could always multiply the state by an arbitrary phase and get complex coefficients if you want, but the relative phase of a and b will remain unchanged. |
| Feb15-10, 05:38 PM | #19 |
|
|
Thanks guys! have been very helpful!
|
| Feb15-10, 05:40 PM | #20 |
|
|
[tex]ae^{i\phi_a}; \:be^{i\phi_b}[/tex] where a and b are real. Then the normalization condition will be in terms of a, b and the (arbitrary) phase difference φa-φb. Still two equations and two unknowns. |
| Feb15-10, 05:41 PM | #21 |
|
|
Finally, vela and I converged.
|
| Feb15-10, 06:10 PM | #22 |
|
|
ok guys, so:
a + bc = 0 aa* + ab*c + ba*c + bb* = 1 2aa* + bb* - ccbb* = 1 are my equations, where do I go from here? If a and b are in general complex, how do I solve for them? does the phase not matter like whatsoever? so I can just write aa* as a^2 |
| Feb15-10, 06:38 PM | #23 |
|
|
Use the first equation to eliminate a from the second equation. You should write bb* = |b|2. The best you can do is get the relative phase between a and b, so you can assume one is real.
|
| Thread Closed |
| Thread Tools | |
Similar Threads for: Quantum Operators (or just operators in general)
|
||||
| Thread | Forum | Replies | ||
| proof help - quantum operators | Advanced Physics Homework | 5 | ||
| Operators in quantum mechanics | Linear & Abstract Algebra | 4 | ||
| quantum mechanical operators. | Quantum Physics | 7 | ||
| Quantum mechanics and operators? | General Physics | 15 | ||
| Quantum Mechanics => Operators | Introductory Physics Homework | 1 | ||