If you have stopped laughing at my last email, I
can suggest a simple test, which, if successful, would also give some
information about the number of interactions, but which, if unsuccessful, would
probably invalidate the idea.
The red shift is defined as (fe - fo)/fe, where fe
is the emitted line frequency, and fo is the observed frequency. My claim is
that:
(fe - fo)/fo ~ N, the
mean number of interactions (scatters).
But there will be an uncertainty in the number of
scatters ~ SQRT(N).
So the apparent increase in the width of the line
will also be ~ SQRT(N).
hence if one plots dfo (the observed width of a
particular line) vs distance, one should see
(dfo - dfe)/fo ~
SQRT(N)/N
For large red shifts, dfe is probably negligible,
so one has
dfo/fo ~ 1/SQRT(N)
Now, I have noticed that illustrations of
spectra of objects with large red shifts normally exhibit very large line widths
also. How is this explained in conventional
cosmology?
Geoff
Indeed (assuming the original width is
negligible)