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The Peres–Horodecki criterion is a necessary condition, for the joint density matrix ρ {\displaystyle \rho } of two quantum mechanical systems A {\displaystyle A} and B {\displaystyle B} , to be separable. It is also called the PPT criterion, for positive partial transpose. In the 2×2 and 2×3 dimensional cases the condition is also sufficient. It is used…
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displaystyle states rho entangled transpose positive criterion partial ppt sufficient also systems separable state condition map entanglement otimes density matrix
| Subject | Predicate | Object | Confidence | Src |
|---|---|---|---|---|
| Peres–Horodecki criterion | is a | necessary condition | 0.90 | text |
| Peres–Horodecki criterion | related to Continuous variable systems | The Peres | 0.60 | section |
| Peres–Horodecki criterion | related to Continuous variable systems | Horodecki | 0.60 | section |
| Peres–Horodecki criterion | related to Continuous variable systems | Rajiah Simon | 0.60 | section |
| Peres–Horodecki criterion | related to Continuous variable systems | PPT | 0.60 | section |
| Peres–Horodecki criterion | related to Continuous variable systems | Gaussian | 0.60 | section |
| Peres–Horodecki criterion | related to Continuous variable systems | Ref | 0.60 | section |
| Peres–Horodecki criterion | related to Continuous variable systems | It | 0.60 | section |
| Peres–Horodecki criterion | related to Continuous variable systems | Simon's | 0.60 | section |
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