Recent content by KDPhysics

  1. K

    A Microscopic derivation of Josephson effect

    In section 18.7 of Bruus & Flensberg the authors provide a microscopic derivation of the Josephson effect. The hamiltonian on both sides of the tunnelling junction is just the typical BCS hamiltonian, on one side (with fermion operators ##c##) $$ H_c = \sum_{k,\sigma} \epsilon_k...
  2. K

    I Exact dynamics of spin in varying magnetic field

    It seems like I overlooked the simple fact that the state cannot change during a sudden, ##\textit{finite}## perturbation, so I was right in assuming that the spin would be ##|+\rangle## at ##t=0^+##. To understand why the system's state must be continuous over the sudden perturbation in the...
  3. K

    I Exact dynamics of spin in varying magnetic field

    Consider an uncharged particle with spin one-half moving with speed ##v## in a region with magnetic field ##\textbf{B}=B\textbf{e}_z##. In a certain length ##L## of the particle's path, there is an additional, weak magnetic field ##\textbf{B}_\perp=B_\perp \textbf{e}_x##. Assuming the electron...
  4. K

    A Unruh & Minkowski Modes: Analytic Extension Explained

    One last question, the Unruh modes as defined in Sean Carroll's "Spacetime and Geometry" are: $$h_k^{(1)} = \frac{1}{\sqrt{2\sinh(\pi \omega/a)}}\big(e^{\pi \omega/2a} g_k^{(1)} + e^{-\pi \omega/2a} g_{-k}^{(2)}{}^*\big)$$ On the other hand this paper gives a different definition: $$h_k^{(1)} =...
  5. K

    A Unruh & Minkowski Modes: Analytic Extension Explained

    But couldn't the left moving negative frequency modes be analytic in that half of the complex plane?
  6. K

    A Unruh & Minkowski Modes: Analytic Extension Explained

    In Carroll "Spacetime and Geometry" I found the following explanation for why the analytically extended rindler modes share the same vacuum state as the Minkowski vacuum state: I can't quite understand why the fact that the extended modes [\tex]h_k^{(1),(2)}[\tex] are analytic and bounded on...
  7. K

    I Gauge in the Aharonov Bohm effect

    Thanks for the answers, very enlightening!
  8. K

    I Gauge in the Aharonov Bohm effect

    In p.385 of Griffiths QM the vector potential ##\textbf{A} = \frac{\Phi}{2\pi r}\hat{\phi}## is chosen for the region outside a long solenoid. However, couldn't we also have chosen a vector potential that is a multiple of this, namely ##\textbf{A} = \alpha \frac{\Phi}{2\pi r} \hat{\phi}## where...
  9. K

    I Is this system a superposition?

    Thanks, very clear explanation!
  10. K

    I Is this system a superposition?

    So the so-called act of measurement in the OP is the painting process, not the blind man somehow "measuring" the colour of the apple? This seems to make a lot more sense now.
  11. K

    I Is this system a superposition?

    Thank you. Suppose then that instead of colouring apples i consider randomly assigning a spin to an electron (here surely quantum effects are coherent). If I don't observe the spin of the electron, then does this mean that the electron is in a definite spin state, but I just haven't performed a...
  12. K

    I Is this system a superposition?

    Thank you. So this case would fall under "incomplete information situations" rather than superpositions as you have described?
  13. K

    I Is this system a superposition?

    I guess my question is what makes something capable of being in a superposition, and other things not?
  14. K

    I Is this system a superposition?

    just because an apple isn't an elementary particle doesn't mean that it can't be in a superposition right?
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