Choice of measurement as signal
  In classical mechanics, performing a measurement without reading the measurement outcome is equivalent to not exploiting the measurement at all. A non-selective measurement in the classical realm carries no information. Here we show that the situation is remarkably different when quantum mechanical systems are concerned. A non-selective measurement on one part of a maximally entangled pair can allow communication between two parties. In the proposed protocol, the signal is encoded in the choice of the measurement basis of one of the communicating parties, while the outcomes of the measurement are irrelevant for the communication and therefore may be discarded. Different choices for the (non-selective) measurement basis correspond to different signals. The scheme is studied in a Hilbert space of odd prime dimension 
A. Kalev, A. Mann, and M. Revzen
quant-ph