Recent content by matonski

  1. M

    Can the Big Rip affect virtual particles' annihilation process?

    Virtual Particles: What are they? by Matt Strassler.
  2. M

    How Does U(x) Relate to Pion Dynamics in Chiral Symmetry Breaking?

    I'm studying this right now as well and had the same question. I think the answer has to do with the concept of "universality class" from statistical mechanics. Basically, I think the idea is that two Lagrangians that are invariant under the same symmetries will flow to the same fixed point in...
  3. M

    Fourier Transforms: Exp(-iwt) or Exp(iwt)?

    Ditto about the 2\pi 's.
  4. M

    Favorite physics videos on internet

    Here are a great set of supersymmetry lectures.
  5. M

    Favorite physics videos on internet

    Someone sent me a private message asking about a better version of these videos. It won't let me respond so I'll just respond here for everyone. Anyway, I don't know of better videos, but after awhile, you can start to see what he writes on the board. Especially in some of the later videos...
  6. M

    Favorite physics videos on internet

    Sidney Coleman's http://www.physics.harvard.edu/about/Phys253.html. I went through these over and over during my QFT class last year. I really feel like he has been my teacher.
  7. M

    Understanding Scattering Theory: Seeking Easy-to-Read References

    I love this book. I used it as a supplement during a second semester QM course that used Sakurai. I still read it now for fun.
  8. M

    Solutions to the Harmonic Oscillator Equation and Hermite Polynomials

    Being a solution to the Schrodinger equation and being normalizable are two different things.
  9. M

    Solving J.E = W/V with Dimensional Analysis

    Yeah J dot E is power per unit volume. That's usually the starting point for deriving expressions for the poynting vector and the energy density in the field.
  10. M

    Why in two dimension space many QTFtheory become renormalizable?

    Because loops now go as \int d^2 p while propagators still go as p^2
  11. M

    Induced emf when accelerates in uniform magnetic field

    After the initial motion, there will be no emf. Charge will build up on both ends, causing an electric field inside the conductor such that E + v x B = 0. Thus, the net force on each charge will be zero. Therefore, the emf will be zero as well since it's the integral of the force per unit charge.
  12. M

    Don't understand dispersive medium

    In Fourier space, you are referring to the equation \left[ \nabla^2 +\mu(\omega)\epsilon(\omega) \omega^2 \right] \mathbf E(\mathbf r, \omega)=0 To find out what that equation is in terms of time, you would have to take its inverse Fourier transform. Then, the functions of \omega will become...
  13. M

    Energy of a system: multiply by velocity?

    The justification is the result. Multiplying both sides of an equation by the same thing doesn't need any justification since it is a valid algebraic manipulation. Perhaps you mean more motivation or intuition? Well, Force x Velocity = Power = rate of change of energy, and the first equation...
  14. M

    Conservation of Momentum = Conservation of Energy?

    At the atomic/particle physics level, there is still potential energy.
  15. M

    No more than two electrons in the entire universe can have the same momentum

    Our classical ideas align more closely with expectation values anyway. It's definitely possible for any number of electrons in the universe to have the same expectation value of momentum.
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