Table II.
τ2/τ1 | Δλ | F | θD | % noise | λ | SD/τi | SD/f2(λ) | Resa |
---|---|---|---|---|---|---|---|---|
2.0b | 20 | 7 | 12 | 2 | 13 | 0.015 | 0.099 | + |
1.8c | 0.016 | 0.13 | M | |||||
1.7 | 0.018 | 0.17 | − | |||||
2.0d | 10 | 0.021 | 0.12 | M | ||||
5 | 0.031 | 0.18 | − | |||||
2.0e | 20 | 5 | 0.016 | 0.10 | M | |||
4 | 0.016 | 0.16 | − | |||||
2.0f | 20 | 7 | 8 | 0.018 | 0.13 | M | ||
6 | 0.021 | 0.13 | − | |||||
2.0 | 20 | 7 | 12 | 3 | 0.022 | 0.14 | M | |
4 | 0.030 | 0.21 | − | |||||
2.0g | 20 | 7 | 12 | 2 | 11 | 0.018 | 0.12 | M/− |
9 | 0.026 | 0.18 | − |
If Res is +, M, or −, the data are resolvable, marginally resolvable, or not resolvable
For all simulated data, τ1 = 5.0 and τ2 = 10 ns and λ1 = 470 and λ2 = 490 nm. Data for seven F between 3.0 and 93.0 MHz, 12 θD total (six θD between 0 and 100° for Ip data), and 13 wavelengths between 450 and 510 nm, were fit except as indicated. See text for further details.
Data as in footnote b but τ2 = 9.0 (τ2/τ1 = 1.8) or 8.5 (τ2/τ1 = 1.7) ns.
As in footnote b but λ2 = 480 (Δλ = 10) or 475 (Δλ = 5) nm.
Data fit as in footnote b but using five (3, 18, 33, 63, 93 MHz) or four (3, 33, 63, 93 MHz) frequencies (F).
Data fit using eight (for L at 0, 20, 60, 100°) or six (for Ip at 20, 60, 100°) detector phase angles (θD).
The number of wavelengths were 11 (from 455 to 505 nm) or 9 (from 460 to 500 nm).