I found your formula h/(2(pi) p) derived in the following on page 5 formula 1
Fractional Statistics and Anyon Superconductivity http://books.google.com/books/about/Fractional_Statistics_and_Anyon_Supercon.html ? At first blush it looks like we are dealing with Anyon formation in a superconductive condensate; where an electron orbits around a current flow. The Orbiton can join a condensate and may be subject to Anyon quantum mechanical statistical description, but it may reflect from the reference, the author is talking about spin as in the spintons. This stuff is all new to me but it looks like you are on to something. We may need to do some digging to see what the physical reality behind this subject is all about. Superconductive quasi particles and their condensates are deep stuff. On Sun, May 13, 2012 at 6:07 PM, <[email protected]> wrote: > In reply to Axil Axil's message of Wed, 9 May 2012 19:00:06 -0400: > Hi, > [snip] > >Since the original electrons in the system are fermions, one of the spinon > >and chargon has to be a fermion, and the other one has to be a boson. One > >is theoretically free to make the assignment in either way, and no > >observable quantity can depend on this choice. The formalism with bosonic > >chargon and fermionic spinion is usually referred to as the > "slave–fermion" > >formalism. > > > >If “chargon” is a boson, it could support a condensate within the two > >dimensional crystal that enables a charge accumulation mechanism whereby > >the large electric charge which has been decupled from the electron; > either > >positive or negative localized in a very small volume can remove the > >coulomb barrier to allow fusion to occur. > [snip] > I'm not quite sure how this ties in, or even if it does, but if you take a > look > at my model (http://rvanspaa.freehostia.com/Non-relativisitic.pdf) you > will see > that electrons in sub-orbitals have fractional angular momentum that > depends on > the quantum number. > > Regards, > > Robin van Spaandonk > > http://rvanspaa.freehostia.com/project.html > >
