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A number of further electron experiments at high energies also favour the hadronic electron model. The slope of
is the detected pion energy in the final state) near
is similar in the cases of
and
high energy collision, and a cross
section roughly constant with
occurs in both (Cronin et al. 1973; Richter 1974). Furthermore, in the naive
eikonal model, we have a
which yields
nb for
, in rough agreement with
experiment. Assuming that hadron yield is proportional to hadronic core area (the colliding particles will be
Lorentz-contracted to discs in their centre-of-mass system), our choice of radius yields
in good agreement with the experimental data.
Yet more evidence for hadronic electrons comes from the observation of the process
at
with a cross section
times that predicted by standard models (Altarelli et al. 1974; Jain et al. 1974) but consistent with
DEHC. We note that the model proposed here does not contribute to hyperfine splitting in atomic spectra (Bég and
Feinberg 1974) at present energies.