Recent content by Quasi Particle

  1. Q

    Optics: polarisation alignment

    Thank you. I calculated the problem now, but the solution is lengthy and I guess it'll be easier to just try it out with the accordant waveplates :rolleyes: :smile: I figured that I only need two waveplates to produce any desired linear polarisation. A quarter-wave plate will turn elliptical...
  2. Q

    Optics: polarisation alignment

    With a combination of wave plates in the order \lambda/2 - \lambda/4 - \lambda/2 it should be possible to achieve any polarisation. But I don't understand why: the first wave plate switches the polarisation direction, the second changes linear to circular polarisation and vice versa, and the...
  3. Q

    Focusing a Collimated Beam: Calculating f & f' for w"0=25µm

    hello. I've got a gaussean beam, which is collimated with a diameter of 2mm, and a wavelength of 1112nm. I need to focus it to a beam waist of 25µm, but my lens with the smallest focal length I have is still f=300mm, so I need to build a telescope: ---collimated beam (w0)-----|lens f)-----beam...
  4. Q

    Can lasers emit anticoherent photons? 180°

    Well I thought that the text is a bit biased...
  5. Q

    Delocalization of states in valence band du to doping

    The idea behind it is: Before it gets doped, the semiconductor is perfectly happy with its electron distribution. Then it gets, e.g., p-doped. Nothing holds the extra hole anywhere except for the potential of the doping atom, so you can calculate its effective Bohr radius as said above, taking...
  6. Q

    Can Doping Transform Any Isolator into a Semiconductor?

    Semiconductors and isolators are only different in that the energy gap of the former is smaller than 2eV, and of the latter it is larger. I can change the energy gap by doping - but can I make any isolator a semiconducter? What are the limitations?
  7. Q

    Delocalization of states in valence band du to doping

    If you use the envelope wave function, you get an H-atom like energy spectrum (e.g. for n-doping): E_D(n) = E_C+\frac{m*}{c^2 m}E_H = E_C - 13.6 eV \frac{m*}{j^2c^2m} where Ec is the energy of the conduction band, m* the effective mass of an electron, and j an integer. From that, you get an...
  8. Q

    Dispersion Relations: Confusing Me & What Information is Gained?

    Yes I know it sounds a pretty stupid question, but it just seems to be opaque to my understanding. Thanks for your answers so far (*notes* effective mass, velocity of sound) If, say, I had an exam about solid state physics and plasma physics and I were asked to draw and explain dispersion...
  9. Q

    Dispersion Relations: Confusing Me & What Information is Gained?

    Dispersion relations have the tendency to confuse me. In general, I know what dispersion is, but trying to apply it to crystals, I just "can't see the forest among all those trees". :uhh: In phonon dispersion, acoustical and optical phonons have quite a different dispersion behaviour. Why is...
  10. Q

    Valley Degeneracy of Semiconductor Band Systems

    So I seem to have mixed up the 2fold degeneracy of the conduction band with the 3fold (2fold) degeneracy of the valence band. Thank you for your answers, it all makes more sense now.
  11. Q

    Valley Degeneracy of Semiconductor Band Systems

    Hm, I was thinking too one-dimensionally. Cheers. But wait. Why are there only different valleys (or directions) if the band gap is indirect? There is no valley degeneracy in GaAs, and it has the same crystal structure as Si except that it has a basis of two different atoms and Si a basis of...
  12. Q

    Valley Degeneracy of Semiconductor Band Systems

    Hiya, trying to learn something about the band system of semiconductors, I found that the conduction band is degenerated at the minimum by valley degeneracy. Do you know where this comes from? In how far is it dependent of the form of the band gap (i.e. direct, indirect)? I would be...
  13. Q

    Interference (Michelson Interferometer)

    Hello, . I have got a Michelson interferometer and measure a laser beam (HeNe @ 633nm). I move the mirror with a step motor of unknown step length and measure the intensity of the beam. I get a nice beat pattern out of that, with "wavelength" of the carrier wave being 14 steps and of the...
  14. Q

    Why U is a State Function if W(adiabatic) Does Not Depend on State?

    No, work is not a state function, only U is. As said above: U = Q + W You can get the same value for U for many different combinations of Q and W. In this special case, Q = 0 so U = W.
  15. Q

    Explaining Wavelength Change in Shallow Water

    It is not the water that is travelling: the water particles are only moving upwards and downwards. The formula you quoted is for phase speed: v = \nu \lambda = \frac{\lambda}{T} because a wave propagates exactly one wavelength \lambda far in the period T=1/\nu In general, the velocity of...
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