J
Jeroen Belleman
Guest
pcdhobbs@gmail.com wrote:
A physically possible wave-like influence doesn't start and stop
instantly either, so that makes good sense.
Jeroen Belleman
There are a couple of interesting quirks for the wavefunction
though. The probability envelope for a photon (or particle)
in transit must be exactly zero for all regions ahead of its
starting point+ct which means that a symmetric Gaussian
distribution just will not do.
That is causality. An effect cannot occur where the wave that
carries it hasn't reached yet.
Interestingly that isn't quite true. I recall from my long-ago
relativistic quantum class that solutions to the Dirac equation
don't go identically to zero outside the light cone, but do decay
exponentially there.
Otherwise you can't satisfy the patching condition at the light
cone boundary.
Cheers
Phil Hobbs
A physically possible wave-like influence doesn't start and stop
instantly either, so that makes good sense.
Jeroen Belleman