Recent content by joycey

  1. J

    Understanding Operation of Back-to-Back Schottky Diodes

    I have been searching for a description of how these diodes operate. I am reasonably familiar with solid state physics and the physics of semiconductors and think I have worked out how these should work (being two back-to-back Schottky diodes) based on the Fermi levels and band-bending, but I'm...
  2. J

    Evaluating Commutator for Operators on f(x)

    By that definition (very different than the one I have learned) these operators do commute. Something I am quite certain they should not. Your definition leads to, \begin{array}{rl} [\hat{U_t}(a),\hat{U_p}]f(x)&=\hat{U_t}(a)\hat{U_p}f(x)-\hat{U_p}\hat{U_t}(a)f(x)\\...
  3. J

    Evaluating Commutator for Operators on f(x)

    lalbatros, To manipulate it in such a manner, you assume the particle is at x, not x+a. The parity operator should effectively reflect around the axis, meaning something that is at x+a must be x+a to the left, or, at -x-a.
  4. J

    Evaluating Commutator for Operators on f(x)

    lalbatros, I think you made a mistake in going from g(-x') to f(-x-a). If we define x' \equiv x-a, as you have done to go from f(x-a) \Rightarrow g(x'), then shouldn't we find that -x'=-(x-a)=-x+a?
  5. J

    Evaluating Commutator for Operators on f(x)

    I just want to ensure that I understand you correctly. Especially since I wrote out the statements in two different orders. To recap how I interpret things, f(x)=<x|f> \begin{array}{rl} \hat{A}f(x)&=<x|\hat{A}|f>\\ &=\int dx' <x|\hat{A}|x'><x|f> \end{array} Now, if I let...
  6. J

    Evaluating Commutator for Operators on f(x)

    In fact, \hat{U_t}(a)|x> = |x+a> \hat{U_t}(a) represents the translation operator, translating the current x-coordinate. <x|\hat{U_t}(a) = <x|\hat{U_t}^\dagger(-a) = <x-a| hence, my statement that \hat{U_t}(a)f(x) = <x|\hat{U_t}(a)|f> = <x-a|f> = f(x-a) So, if the current x...
  7. J

    Evaluating Commutator for Operators on f(x)

    Hey Marlon, Thanks for the answer, but that's not what I was trying to get at. I realize that either way I evaluate these the commutation relation will be non-zero, I just get a different relation depending on the method. Which is what I'm wondering here. \begin{array}{rl}...
  8. J

    Evaluating Commutator for Operators on f(x)

    I'm having difficulty trying to figure out which of the following is the correct method to properly evaluate the effect of the operators on f(x). Given that, \hat{A}f(x)=<x|\hat{A}|f> If the polarity operator, \hat{U_p}, and the translation operator, \hat{U_t}(a), act as...
Back
Top