Recent content by 43arcsec

  1. 4

    I Spin operator and spin quantum number give different values, why?

    Thanks Peter and DrClaude, I think you may have led me to my mistake. When I looked at S=Sx+Sy+Sz and squared both sides, I dropped the cross terms, ie, SxSy, SxSz, SySz thinking they are orthogonal. But these are 2x2 matrices, so they are not 0. In fact, they are all (hbar/2)^2. This...
  2. 4

    I Spin operator and spin quantum number give different values, why?

    ok, so I think I almost have it, thanks for the help. S^2=Sx^2+Sy^2+Sz^2 S^2 |z+>= Sx Sx |z+>+SySy|z+>+SzSz|z+>=(hbar/2)^2 * 3 |z+> S=hbar/2*sqrt(3) If I got this right, then shouldn't S=Sx+Sy+Sz ? And if you go through the same calculation, you get S=3 hbar/ 2 Thanks for hanging in there...
  3. 4

    I Spin operator and spin quantum number give different values, why?

    Thanks again for the response, I appreciate it. I think you hit the essence of my problem, although I can't give you an anwers. A spin operator measures the value of a particles spin. The spin formula by quantum number, S, is: "The expression √(s(s+1))ħ represents the magnitude of the spin...
  4. 4

    I Spin operator and spin quantum number give different values, why?

    Sorry for the lack of clarity. Let's take S_z |z;+> = hbar/2 |z;+> but I think all spin operators in any direction have the same eigenvalue, hbar/2 And yes, mea culpa, I left off the sqrt. As you said, it's S = sqrt(s(s+1))hbar I thought this was a common formuler for spin, it's on the...
  5. 4

    I Spin operator and spin quantum number give different values, why?

    Assume spin 1/2 particle So the spin operator gives +/- hbar/2 eg. S |n+> = +/- hbar/2 |n+> But S= s(s+1) hbar = sqrt(3)/2 hbar So I'm off by a factor of sqrt(3). I suspect I am missing something fundamental about my understanding of spin. My apologies and thanks in advance.
  6. 4

    I Richard Feynman: Deriving Lorentz Mass Transformation

    In section 3.8, Feynman does a derivation of the Lorentz transformation for mass starting from $$\frac{d}{dt}E=F \cdot v \hspace{1cm}(1) $$ But is this a valid starting point if you are going to show mass changes with velocity? He says (1) comes from chapter 13 of his Lectures which he...
  7. 4

    I Measuring Time with Mirrors: Exploring Special Relativity

    So summing up, a photon heads towards a mirror, at the mirror, something complicated yet instantaneous happens, resulting in a photon seemingly being reflected with the same energy in the opposite direction with 0 delay. How's that?
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    I Measuring Time with Mirrors: Exploring Special Relativity

    Thanks Vandium50. I read the link, finding this: "So the lattice does not absorb this photon and it is re-emitted but with a very slight delay. This, naively, is the origin of the apparent slowdown of the light speed in the material. " Which doesn't seem too far off from my misunderstanding...
  9. 4

    I Measuring Time with Mirrors: Exploring Special Relativity

    OK, so photons are not absorbed by electrons and re-emitted, as evidenced by no loss in phase. They do however interact in some complicated way, resulting in a photon being reflected elastically with the same phase so we still see the same image. So let me focus on the interaction. It is my...
  10. 4

    I Measuring Time with Mirrors: Exploring Special Relativity

    Ok, while I'm not sure what plasmon-polariton-like modes" are, but after reading up here I think I might have stumbled on to something: electrons can be absorbed and re-emitted, but they can also be scattered (Compton scattering). Is it correct to say that in a mirror the incident photons...
  11. 4

    I Measuring Time with Mirrors: Exploring Special Relativity

    So are you saying the absorption and re-emission is a real world effect?
  12. 4

    I Measuring Time with Mirrors: Exploring Special Relativity

    Hmmm, I don't believe mirrors reflect all frequencies, here's a Physics Forum link discussing that. Seems like that would be evidence that there is absorption.
  13. 4

    I Measuring Time with Mirrors: Exploring Special Relativity

    Special relativity is replete with examples of turning mirrors into clocks. Place two mirrors across from one another, bounce light between them, and measure the time. But as I thought about this, when a photon hits the mirror, it is absorbed by an electron which moves to a higher energy...
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