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Randomizing quantum states: Constructions and applications

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arxiv quant-ph/0307104 v3 pith:ANHFYVHK submitted 2003-07-15 quant-ph

classification quant-ph
keywords quantumbitsconstructionperfectlyqubitsstateschannelclassical
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The construction of a perfectly secure private quantum channel in dimension d is known to require 2 log d shared random key bits between the sender and receiver. We show that if only near-perfect security is required, the size of the key can be reduced by a factor of two. More specifically, we show that there exists a set of roughly d log d unitary operators whose average effect on every input pure state is almost perfectly randomizing, as compared to the d^2 operators required to randomize perfectly. Aside from the private quantum channel, variations of this construction can be applied to many other tasks in quantum information processing. We show, for instance, that it can be used to construct LOCC data hiding schemes for bits and qubits that are much more efficient than any others known, allowing roughly log d qubits to be hidden in 2 log d qubits. The method can also be used to exhibit the existence of quantum states with locked classical correlations, an arbitrarily large amplification of the correlation being accomplished by sending a negligibly small classical key. Our construction also provides the basic building block for a method of remotely preparing arbitrary d-dimensional pure quantum states using approximately log d bits of communication and log d ebits of entanglement.

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Cited by 2 Pith papers

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  1. Relative entropy of entanglement of Haar random states

    quant-ph 2026-08 accept novelty 7.0 of 10

    For a bipartite mixed state obtained by tracing out one subsystem of a tripartite Haar-random pure state, the relative entropy of entanglement equals log(d_A d_B / max(d_A,d_B,d_C)) plus an absolute constant, with hig...

  2. Growth and collapse of subsystem complexity under random unitary circuits

    quant-ph 2025-10 unverdicted novelty 7.0 of 10

    Under random brickwork circuits, regions larger than half the system have complexity growing linearly in time, while a smaller region thermalizes to essentially zero complexity by T=ℓ/2 — with holographic and replica ...

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