  An interesting protocol for classical teleportation of an unknown classical
state was recently suggested by Cohen, and by Gour and Meyer. In that protocol,
Bob can sample from a probability distribution P that is given to Alice, even
if Alice has absolutely no knowledge about P. Pursuing a similar line of
thought, we suggest here a limited form of nonlocality - "classical
nonlocality". Our nonlocality is the (somewhat limited) classical analogue of
the Hughston-Jozsa-Wootters (HJW) quantum nonlocality. The HJW nonlocality
tells us how, for a given density matrix rho, Alice can generate any
rho-ensemble on the North Star. This is done using surprisingly few resources -
one shared entangled state (prepared in advance), one generalized quantum
measurement, and no communication. Similarly, our classical nonlocality
presents how, for a given probability distribution P, Alice can generate any
P-ensemble on the North Star, using only one correlated state (prepared in
advance), one (generalized) classical measurement, and no communication.
  It is important to clarify that while the classical teleportation and the
classical non-locality protocols are probably rather insignificant from a
classical information processing point of view, they significantly contribute
to our understanding of what exactly is quantum in their well established and
highly famous quantum analogues.
