Hardly a "deep" problem, but yes, sorry about that. I made a mistake saying the disks had the opposite chirality. These things happen from time to time. To clarify, I said you start with two disks both with a clockwise "steering wheel" rotation. You then spin one like a coin with your left hand, and you spin the other like a coin with your right hand. I then said they have the opposite chirality, I was wrong. These are "mirror image" things but you can rotate one to transform it into the other, so they aren't chiral. I know this because I spoke at length with Andrew Worsley about spheres and torii. We drew orthogonal lines around pingpong balls, with arrowheads. We concluded that whilst the electron and the positron are deemed to have a spherically-symmetric electric field, there has to be an underlying toroidal nature because electrons and positrons have opposite chiralities.
Thank you.
I will note that you didn't address the other half of my post (in which I linked back to
these questions). Perhaps next time?
I'd also point out that electrons of
both chiralities exist in nature, as do positrons of both chiralities, but there is an
asymmetry between them.
All of that aside: You don't necessarily need an underlying toroidal nature to your electron to get chirality. If your disks had been oriented in some way (e.g. marked on one side with "heads" and the other with "tails") that would suffice to allow two distinct rotating states. Indeed, you could get away with uniform rotation about a single axis in that case.
If you do want to stick with unmarked disks, something which gets closer to the "torus" depicted in Williamson / van der Mark's paper is the following. Take a disk which rotates "like a steering wheel" as before. Instead of then spinning it like a coin, make it orbit the origin in such a way that centre of the disk traces out a circular path while the disk itself remains coplanar with the origin. The disk boundary traces out a 2-torus. A representative point on the disk boundary might move like so in a typical model (with some uninteresting parameters omitted):
x(t) = (c + cos at) cos bt
y(t) = (c + cos at) sin bt
z(t) = sin at
The parameter
a sets the speed of the "steering wheel" motion,
b sets the rate of the orbital motion, and the positive parameter
c sets the orbital radius. For such a set-up, you can identify five disjoint classes of model, which cannot be transformed into each other by rotations in 3D space:
- Those for which the point never moves (relative to the torus).
- Those for which the point passes through the hole but there is no "orbital" motion.
- Those for which the point never passes through the hole but still orbits.
- Those for which the point passes through the hole in the opposite direction to the vector defined by the "orbital" component of the motion (using the right-hand rule).
- Those for which the point passes through the hole in the same direction as the vector defined by the "orbital" component of the motion.
The first category has
a =
b = 0. The second has non-zero
a but
b = 0. The third has
a = 0 but non-zero
b. The fourth has
a and
b both non-zero with the same sign. The fifth has
a and
b both non-zero with opposite signs. According to you (Farsight) on some occasions at least, electrons and positrons are described by the fourth and fifth classes of model (though maybe not that way around).
There is no reason why we should accept without exceedingly strong evidence that a photon would be moving along such a toroidal surface, as it would require significant alterations to the thoroughly tested laws of electromagnetism. If you
could get it to do so it seems like the resulting states should actually be determined by solving a wave equation on the surface and finding the
eigenvalues, rather than use the Bohr-model-like method of simply looking for closed paths of a certain length. You'd need to adjust the parameters to make the lowest-mass particle appear at 511 keV (the electron mass). At that point, you'd be left with the following problems (all of which have been mentioned before, early on in this thread):
- There should be an infinite discrete series of excited states corresponding to the higher eigenvalues. These have never been observed, despite presumably being well within the range of accelerators.
- Worse still, there should be a continuous infinity of states with higher and lower masses corresponding to similar systems with other values for the torus dimensions. Again, these have never been observed.
- The resulting states are electrically neutral (so they have the wrong charge).
- The resulting states are bosonic (so they have the wrong spin and collective behaviour).
- Photon-photon interactions would need to be much stronger than observed to permit the bound state.
- The resulting states would be unstable, decaying spontaneously into free photons.