Table 1. Inseparability of entangled modes.
N | I | II | III | IV | V | VI | VII | Average |
---|---|---|---|---|---|---|---|---|
2 | 0.39 | 0.39 | ||||||
3 | 0.56 | 0.56 | 0.56 | |||||
4 | 0.64 | 0.63 | 0.64 | 0.64 | ||||
5 | 0.69 | 0.69 | 0.70 | 0.70 | 0.69 | |||
6 | 0.73 | 0.73 | 0.75 | 0.74 | 0.74 | 0.74 | ||
7 | 0.77 | 0.78 | 0.77 | 0.76 | 0.77 | 0.77 | 0.77 | |
8 |
0.79 |
0.79 |
0.78 |
0.81 |
0.79 |
0.80 |
0.79 |
0.79 |
Data are based on the van Loock–Furusawa criteria, given in equation (4). Each row shows that for a basis of N quantum modes, the N−1 values obtained from quadrature variances are well below 1. This verifies entanglement of the N modes.
Uncertainty is ±0.01 in all cases.