Quantum / CONCEPT
M-resistant qudit states exist in every admissible range
For every N at least three and every m at most N minus two, a normalized pure state is entangled after every m-particle loss and fully separable after every (m+1)-particle loss.
Closed
DIRECT PREREQUISITES3
DIRECT CONSEQUENCES0
PROOF DEPTH7
DOCUMENT LINKS0
Existence by shared labels and localized bits
RELATIONSHIP ATLAS
Every connection, in context.
Direct recorded relationships
Proof dependencyStructural affinityDocument link
Certified topology / UPSTREAM
Prerequisites
Certified topology / DOWNSTREAM
Consequences
None recorded in this release.
RELATED KNOWLEDGE
Structural connections
- A counterexample to the negative-q commutator boundstructural-affinity · Closed
- A traceless counterexample to the q-deformed commutator boundstructural-affinity · Closed
- Classical-quantum Gram realizationstructural-affinity · Closed
- Exact ranks and entropy for direct concatenationstructural-affinity · Closed
- Full separability and exchanged diagonalsstructural-affinity · Closed
- Guessing probabilitystructural-affinity · Closed
- Optimal quantum states depend on the Renyi ordersstructural-affinity · Closed
- Orthogonal Records and Pointer Informationstructural-affinity · Closed
- Selective LOCC can increase the Moreau-Yosida entanglement of formationstructural-affinity · Closed
- The complementary W-state effect is not fully separablestructural-affinity · Closed
- The Pure-State Handshakestructural-affinity · Closed
Documents & exposition
None recorded in this release.
Other authored & advisory relationships
None recorded in this release.
LIBRARY / RELEASE VERSIONS
Content history
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