Hans de Vries
Science Advisor
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tiny-tim said:Hi Hans!
I'm still not quite clear whether your saying that "virtual particles" are real.![]()
Hi, Tiny Tim
The math describes EM fields. These fields follow Maxwell's laws and originate
from the charge current density in the scattering zone just as they would classically.
If I use the term "virtual photon" then it's just a nickname for the EM field.
tiny-tim said:Yes, I'm happy to accept that \psi^\ast\gamma^\mu\psi is a current density and therefore real.
And that the associated field is therefore real.
ok

tiny-tim said:Which part of \psi^\ast\gamma^\mu\psi is the transition current you're talking about?
(I wiki'ed and googled "transition current", but didn't find anything helpful, and it's not in the index of Weinberg's QTF, Vol I, which is the source of most of my knowledge. I vaguely recall seeing \psi_f^\ast (\partial_\mu \psi_i)\ -\ (\partial_\mu \psi_f^\ast)\psi_i somewhere else, but I think it left out an A2 term, and I don't see where it comes in the the simple derivation of the Dyson series, nor why an approximation made of an artificial combination of idealised initial and final fields should be regarded as in any way modelling the real field in the "scattering zone" of an interaction.)
An electron in a scattering zone can change its momentum suddenly from an initial
momentum to a final momentum. Not via a gradually changing path but under a sharp
angle. The reason that it can do so is because an electron can interfere with itself.
For some time the electron will be in a transition state going from initial to final
momentum. Its wavefunction will be a linear combination of the two states and these
states interfere with each other. Now what is this transition interference current?
\psi = \psi_f+\psi_i
Thus the charge current density is given by:
\bar{\psi}\gamma^\mu\psi ~=~ \Big(\bar{\psi_f}\gamma^\mu\psi_f~+~\bar{\psi_i}\gamma^\mu\psi_i \Big) ~~+~~ \Big(\bar{\psi_f}\gamma^\mu\psi_i~+~\bar{\psi_i}\gamma^\mu\psi_f\Big)
The last two terms (the crossterms) represent the interference current. The two
interference terms are each others complex conjugate. Each term contains all
information needed. The Feynman diagram expressions use the first of the two terms.
The basic interference pattern is the same as in the case of a Klein Gordon particle:
\psi_{int} ~~=~~ \exp\left\{ -i(p_f^\mu-p_i^\mu)x_\mu \right\}~+~ \exp\left\{ -i(p_f^\mu-p_i^\mu)x_\mu \right\} ~~=~~ 2\cos\left\{ (p_f^\mu-p_i^\mu)x_\mu \right\}
The cosine functions represents an alternating charge density pattern in case of
a Klein Gordon particle which shifts with a speed of anywhere between 0 and c.
However, we are dealing with a Dirac particle field which also has a spin density.
The alternating spin density is the same as an alternating transverse current density
pattern according to Stokes law. You can see this in figure 1.7 in my book here.
http://physics-quest.org/Book_Chapter_EM_basic.pdf"
The left side of figure 1.7 is effectively the same as the right side according to
Stokes. If you google for "Gordon decomposition" then this is the extra term from
spin in the vector current.
The electromagnetic field from the alternating charge current pattern is derived
in the classical way and this is what is "nicknamed" the "virtual photon"
Regards, Hans
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