I Effects of photons having a finite mass

Saptarshi Sarkar
Messages
98
Reaction score
13
TL;DR Summary
Effect on Coulomb potential due to finite mass of photons
Few days back, our college professor told us that if a photon were to have a finite mass, then the Coulomb potential between two stationary charges separated by a distance r would be strictly zero beyond some distance.

He told us that it was due to the reason that photon is the elementary particle which is the reason behind Coulomb force. I didn't understand what he really meant as we haven't yet had the course on particle physics. Can anyone please explain it or refer to something that I can read?
 
Physics news on Phys.org
Saptarshi Sarkar said:
then the Coulomb potential between two stationary charges separated by a distance r would be strictly zero beyond some distance.
That is not true. With a massive exchange particle you get a Yukawa potential. For large distances it is decreasing (approximately) exponentially, it quickly gets irrelevant, but never zero. The strong interaction has such a potential, and it can also arise in some cases from the electromagnetic interaction if additional particles shield a point charge.
 
  • Like
Likes Saptarshi Sarkar, ohwilleke and dlgoff
Toponium is a hadron which is the bound state of a valance top quark and a valance antitop quark. Oversimplified presentations often state that top quarks don't form hadrons, because they decay to bottom quarks extremely rapidly after they are created, leaving no time to form a hadron. And, the vast majority of the time, this is true. But, the lifetime of a top quark is only an average lifetime. Sometimes it decays faster and sometimes it decays slower. In the highly improbable case that...
I'm following this paper by Kitaev on SL(2,R) representations and I'm having a problem in the normalization of the continuous eigenfunctions (eqs. (67)-(70)), which satisfy \langle f_s | f_{s'} \rangle = \int_{0}^{1} \frac{2}{(1-u)^2} f_s(u)^* f_{s'}(u) \, du. \tag{67} The singular contribution of the integral arises at the endpoint u=1 of the integral, and in the limit u \to 1, the function f_s(u) takes on the form f_s(u) \approx a_s (1-u)^{1/2 + i s} + a_s^* (1-u)^{1/2 - i s}. \tag{70}...
Back
Top