post 35 is a gem
Wow!
another great post
a method of identifying that your intuition has merit is to move the slit, closer and further from its optimum wave revealing point. Notice the densities change. (not just coherance) Then bring in a second source of wave/particles and watch the effects, once again these will show your intuition is pretty good.
It is upon the exchange with mass, the appearance of particle phenomenon shows itself, but to use different mediums of mass (elemental structure), then find the particles (released) changes with the mass; see photoelectric effect or even notice the color changes.
great thread
and ben you are better than you realize (thanks)
I could be wrong, so let's sort this out. This is how I understand it, so please tell me if I'm wrong!
When we talk about interactions, we should understand "states" as excitations of quantum fields. Scattering amplitudes are normally described in terms of well-defined set of "out" and "in" states (the S matrix tells you how they interact). These out and in states are written in terms of plane waves, "at infinity". These plane waves appear in the Fourier expansion of the field, with the ladder operators acting as Fourier coefficients. So asymptotically the field is only described in terms of its Fourier expansion, so I don't understand why I shouldn't think of this as just a plane wave.
Interactions (i.e. the whole edifice of perturbation theory/effective field theory) is built on the fact that states can be "localized" (in some sense) near a specific point in space and time. (Local means that the center of mass energy is much less than the largest scale in the problem.) This suggests that, near an interaction zone, the particle description is more fitting. While the decomposition of a field into it's Fourier modes is still legitimate, it is not clear to me how to understand the interaction between particles as an interaction between individual modes of the field. I think that it may be that the equations of motion become non-linear, and it is just not possible to solve for a scattering amplitude. I know this is the case for a general phi-4 theory.
So this is the dichotomy, and we can look at various physical phenomena to see how well we understand them. For example, consider electrons going through a multiple slit experiment. Let the slit separation be d, and the distance to the screen be L. As long as the slit separation is not too big, and not too small, you see a diffraction pattern. "Too big" means that the slit separation has to be much smaller than the distance from the screen. "Too small" is set by the dimensions in the problem. So, for example, the only dimensionful quantity in QED is the electron mass, which corresponds to a length scale of about 1/10000 the Bohr radius (I think). This means that as long as the slit separation is much bigger than the Bohr radius (which is about 5 nm?), the electrons will act as a wave. As soon as the slit separation gets close to the "classical electron radius" (which isn't really possible), I think the electron should behave as a particle, again.
On the one hand, you'd expect the system to be "more quantum" as you probe shorter distance scales. But what I have just proved is that the system becomes "more classical" as we probe smaller scales. The result of the double slit experiment is that
$$n\lambda = \frac{xd}{L}$$
so as d gets smaller and smaller, while holding $$\lambda$$ fixed, the separation of the fringes (x) goes to infinity, and you only see the central peak. Likewise, as d gets bigger and bigger, the fringes start to overlap, and again you only see the central peak!
I am comforted by the fact that there are some equations which support my intuition, but still this is a bit of an awkward result. Hopefully someone can show me where I'm wrong.
Wow!
another great post
a method of identifying that your intuition has merit is to move the slit, closer and further from its optimum wave revealing point. Notice the densities change. (not just coherance) Then bring in a second source of wave/particles and watch the effects, once again these will show your intuition is pretty good.
It is upon the exchange with mass, the appearance of particle phenomenon shows itself, but to use different mediums of mass (elemental structure), then find the particles (released) changes with the mass; see photoelectric effect or even notice the color changes.
great thread
and ben you are better than you realize (thanks)