The Schmidt coefficients of a normalized bipartite pure state are the nonnegative numbers sj in its Schmidt decomposition; they satisfy ∑jsj2=1 and their squares are the nonzero eigenvalues of either reduced density matrix.
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- Schmidt decomposition
- Entanglement entropy
- Von Neumann entropy
- Density matrix
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- CHSH axes for an entangled pure two-qubit state
- Collective advantage over independent two-qubit filtering
- Deterministic reduction of maximally entangled Schmidt rank
- Entanglement dilution
- Gisin's theorem
- Local-unitary invariance of reduced-state spectra
- Local unitary operation
- Maximally entangled overlap bound from Schmidt rank
- Nielsen's pure-state conversion theorem
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- Pure-state negative conditional entropy criterion
- Schmidt-basis Pauli correlation tensor
- Schmidt projection entanglement concentration
- Schmidt-tail entanglement monotone
- Two-outcome LOCC dilution of a Bell pair
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