Noise threshold for positive quantum capacity of the depolarizing channel · revision history
Revision 2
Accepted · core change · record
Changes against revision 1:
- Title
- Noise threshold for positive quantum capacity of the depolarizing channel
- Plain
- The simplest noisy quantum channel replaces a qubit by a random error with probability p. The noise level above which it can no longer carry any quantum information at all is not known.
- Precise · changed · core
- Revision 1: For the qubit depolarizing channel $D_p(\rho) = (1 - p) \rho + (p/3)(X \rho X + Y \rho Y + Z \rho Z)$, find p* with quantum capacity $Q(D_p) > 0$ if and only if p < p*. Known: $Q = 0$ for $p \ge 1/4$; the hashing bound is positive up to $p \sim 0.1893$, and degenerate codes push positivity above 0.19 (DiVincenzo, Shor and Smolin 1998; Smith and Smolin 2007), with further small improvements since. More generally, compute $Q(D_p)$ for any $0 < p < 1/4$.
- Revision 2: For the qubit depolarizing channel $D_p(\rho) = (1 - p) \rho + (p/3)(X \rho X + Y \rho Y + Z \rho Z)$, find $p*$ with quantum capacity $Q(D_p) > 0$ if and only if $p < p*$. Known: $Q = 0$ for $p \ge 1/4$; the hashing bound is positive up to $p \sim 0.1893$, and degenerate codes push positivity above 0.19 (DiVincenzo, Shor and Smolin 1998; Smith and Smolin 2007), with further small improvements since. More generally, compute $Q(D_p)$ for any $0 < p < 1/4$.
- Settled by
- A matching upper bound below $1/4$ and code construction, or an exact capacity formula.
- Kind
- well-posed
- Answer type
- value
- References
- (empty)
- Literature status
- open
- Status note
- 2026 preprints refine lower bounds on the threshold (e.g. arXiv:2608.15870, arXiv:2609.39747); $p*$ is unknown.
- Posed since
- 1996
Decisions
- Accept · 2026-10-15 · record