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Noncommuting mixed states cannot be broadcast

H. Barnum, C. M. Caves, C. A. Fuchs, R. Jozsa, B. Schumacher

arXiv:quant-ph/9511010v1quant-ph

TL;DR

The paper asks whether unknown mixed quantum states can be broadcast onto two systems, extending the pure-state no-cloning question. It proves that broadcasting is possible only for commuting states, while noncommuting states cannot be broadcast.

  • Problem

    The paper asks whether physical processes can broadcast an unknown quantum state onto separate systems, since the no-cloning theorem alone does not address mixed states.

    Source: p. 2
  • Method

    The authors model the most general quantum process using an auxiliary system, a standard auxiliary state, and unitary evolution, then analyze fidelity and commutation.

    Source: p. 3
  • Results

    Broadcasting is possible if and only if the states commute; noncommuting mixed states therefore cannot be broadcast.

    Source: pp. 3, 10
  • Takeaways & Limitations

    The theorem generalizes and extends the pure-state no-cloning theorem to mixed quantum states.

    Source: p. 2

    The analysis constrains broadcasting to physical processes modeled within quantum theory, and sufficient conditions for process realizability are not known.

    Source: pp. 3, 10

Abstract

from arXiv · show

We show that, given a general mixed state for a quantum system, there are no physical means for {\it broadcasting\/} that state onto two separate quantum systems, even when the state need only be reproduced marginally on the separate systems. This result generalizes and extends the standard no-cloning theorem for pure states.

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