  A slow $J/\psi$ bump exists in the inclusive $B\to J/\psi + X$ spectrum,
while the softness of $J/\psi$ spectrum in $\Upsilon(1S) \to J/\psi + X$ decay
is in strong contrast with expectations from color octet mechanism. We propose
{\it intrinsic} charm as the explanation:the former is due to $\bar B\to J/\psi
D \pi$,with three charm quarks in the final state; the latter is just a small
fraction of $\Upsilon(1S) \to (c\bar c)_{\rm slow} + 2$"jet" events, where the
slow moving $c\bar c$ system evolves into $D^{(*)}$ pairs. Experimental search
for these phenomena at B Factories and the Tevatron is strongly urged, as the
implications go beyond QCD.

High Energy Physics - Phenomenology