Let three parties share the normalized quantum state
For copies, group each party's qubits together. Across any nontrivial division of these three parties, the Schmidt decomposition has one nonzero coefficient for every binary string of length , so its Schmidt rank is . Similarly, copies of the standard GHZ state have Schmidt rank across the same division.
Every recorded LOCC branch acts by a product of local Kraus operators. Schmidt-rank contraction under product operators therefore rules out an exact successful conversion when , even if success need only have nonzero probability. This is a rank obstruction for the full target, not merely a bound on its entanglement entropy.
Approximation changes the question. In the expansion of , squared coefficients have the binary-product distribution with parameter . A quantum typical subspace retains weight tending to one while using only strings, where is binary entropy. The normalized truncation approaches the full target in quantum fidelity, although its Schmidt rank can be far smaller than . Consequently, the exact finite-copy rank argument does not forbid an asymptotic entanglement dilution protocol with vanishing approximation error.

Articles by others on the same topic (0)

There are currently no matching articles.