Table 3 from Stockman and Sharpe (2000)Table 3 from Stockman and Sharpe (2000)
Table 3 in ascii format. Column key as first four
columns below.
NotesTable 3 legend (HTML table follows)
Stiles & Burch red, 
, green, 
, and
blue,
, 10° CMFs used to calculate the cone fundamentals tabulated in
Table 2. The CMFs are from Table I(5.5.4) of Wyszecki & Stiles , in which they are
tabulated in wavelength steps of 5 nm, and from Tables 7 and 8 of Stiles & Burch
(1959), in which they are tabulated in wavenumber steps of 250 or 500 cm-1. At
shorter wavelengths, the CMFs are from Table I(5.5.4). At longer wavelengths, however,
those CMFs are uncorrected for rod intrusion, and are tabulated only to 4 decimal places,
which is too imprecise to define the cone sensitivities at longer wavelengths. At longer
wavelengths, therefore, we have corrected the original CMFs (Table 7 of Stiles &
Burch, 1959) for rod intrusion (according to the corrections given in Table 8 of Stiles
& Burch, 1959) and re-interpolated them at 5-nm intervals. The Stiles & Burch
(1959) CMFs were based on data from 49 observers below 714.3 nm, but on data from only 9
observers from 714.3 to 824.2 nm.
Table 3
nm |
|
|
|
nm |
|
|
|
390 |
0.001500 |
-0.000400 |
0.006200 |
615 |
2.719400 |
0.093800 |
-0.001030 |
395 |
0.003800 |
-0.001000 |
0.016100 |
620 |
2.452600 |
0.061100 |
-0.000680 |
400 |
0.008900 |
-0.002500 |
0.040000 |
625 |
2.170000 |
0.037100 |
-0.000442 |
405 |
0.018800 |
-0.005900 |
0.090600 |
630 |
1.835800 |
0.021500 |
-0.000272 |
410 |
0.035000 |
-0.011900 |
0.180200 |
635 |
1.517900 |
0.011200 |
-0.000141 |
415 |
0.053100 |
-0.020100 |
0.308800 |
640 |
1.242800 |
0.004400 |
-5.49E-05 |
420 |
0.070200 |
-0.028900 |
0.467000 |
645 |
1.007000 |
0.000078 |
-2.20E-06 |
425 |
0.076300 |
-0.033800 |
0.615200 |
650 |
0.782700 |
-0.001368 |
2.37E-05 |
430 |
0.074500 |
-0.034900 |
0.763800 |
655 |
0.593400 |
-0.001988 |
2.86E-05 |
435 |
0.056100 |
-0.027600 |
0.877800 |
660 |
0.444200 |
-0.002168 |
2.61E-05 |
440 |
0.032300 |
-0.016900 |
0.975500 |
665 |
0.328300 |
-0.002006 |
2.25E-05 |
445 |
-0.004400 |
0.002400 |
1.001900 |
670 |
0.239400 |
-0.001642 |
1.82E-05 |
450 |
-0.047800 |
0.028300 |
0.999600 |
675 |
0.172200 |
-0.001272 |
1.39E-05 |
455 |
-0.097000 |
0.063600 |
0.913900 |
680 |
0.122100 |
-0.000947 |
1.03E-05 |
460 |
-0.158600 |
0.108200 |
0.829700 |
685 |
0.085300 |
-0.000683 |
7.38E-06 |
465 |
-0.223500 |
0.161700 |
0.741700 |
690 |
0.058600 |
-0.000478 |
5.22E-06 |
470 |
-0.284800 |
0.220100 |
0.613400 |
695 |
0.040800 |
-0.000337 |
3.67E-06 |
475 |
-0.334600 |
0.279600 |
0.472000 |
700 |
0.028400 |
-0.000235 |
2.56E-06 |
480 |
-0.377600 |
0.342800 |
0.349500 |
705 |
0.019700 |
-0.000163 |
1.76E-06 |
485 |
-0.413600 |
0.408600 |
0.256400 |
710 |
0.013500 |
-0.000111 |
1.20E-06 |
490 |
-0.431700 |
0.471600 |
0.181900 |
715 |
0.009240 |
-7.48E-05 |
8.17E-07 |
495 |
-0.445200 |
0.549100 |
0.130700 |
720 |
0.006380 |
-5.08E-05 |
5.55E-07 |
500 |
-0.435000 |
0.626000 |
0.091000 |
725 |
0.004410 |
-3.44E-05 |
3.75E-07 |
505 |
-0.414000 |
0.709700 |
0.058000 |
730 |
0.003070 |
-2.34E-05 |
2.54E-07 |
510 |
-0.367300 |
0.793500 |
0.035700 |
735 |
0.002140 |
-1.59E-05 |
1.71E-07 |
515 |
-0.284500 |
0.871500 |
0.020000 |
740 |
0.001490 |
-1.07E-05 |
1.16E-07 |
520 |
-0.185500 |
0.947700 |
0.009500 |
745 |
0.001050 |
-7.23E-06 |
7.85E-08 |
525 |
-0.043500 |
0.994500 |
0.000700 |
750 |
0.000739 |
-4.87E-06 |
5.31E-08 |
530 |
0.127000 |
1.020300 |
-0.004300 |
755 |
0.000523 |
-3.29E-06 |
3.60E-08 |
535 |
0.312900 |
1.037500 |
-0.006400 |
760 |
0.000372 |
-2.22E-06 |
2.44E-08 |
540 |
0.536200 |
1.051700 |
-0.008200 |
765 |
0.000265 |
-1.50E-06 |
1.65E-08 |
545 |
0.772200 |
1.039000 |
-0.009400 |
770 |
0.000190 |
-1.02E-06 |
1.12E-08 |
550 |
1.005900 |
1.002900 |
-0.009700 |
775 |
0.000136 |
-6.88E-07 |
7.53E-09 |
555 |
1.271000 |
0.969800 |
-0.009700 |
780 |
9.84E-05 |
-4.65E-07 |
5.07E-09 |
560 |
1.557400 |
0.916200 |
-0.009300 |
785 |
7.13E-05 |
-3.12E-07 |
3.40E-09 |
565 |
1.846500 |
0.857100 |
-0.008700 |
790 |
5.18E-05 |
-2.08E-07 |
2.27E-09 |
570 |
2.151100 |
0.782300 |
-0.008000 |
795 |
3.77E-05 |
-1.37E-07 |
1.50E-09 |
575 |
2.425000 |
0.695300 |
-0.007300 |
800 |
2.76E-05 |
-8.80E-08 |
9.86E-10 |
580 |
2.657400 |
0.596600 |
-0.006300 |
805 |
2.03E-05 |
-5.53E-08 |
6.39E-10 |
585 |
2.915100 |
0.506300 |
-0.005370 |
810 |
1.49E-05 |
-3.36E-08 |
4.07E-10 |
590 |
3.077900 |
0.420300 |
-0.004450 |
815 |
1.10E-05 |
-1.96E-08 |
2.53E-10 |
595 |
3.161300 |
0.336000 |
-0.003570 |
820 |
8.18E-06 |
-1.09E-08 |
1.52E-10 |
600 |
3.167300 |
0.259100 |
-0.002770 |
825 |
6.09E-06 |
-5.70E-09 |
8.64E-11 |
605 |
3.104800 |
0.191700 |
-0.002080 |
830 |
4.55E-06 |
-2.77E-09 |
4.42E-11 |
610 |
2.946200 |
0.136700 |
-0.001500 |
ReferencesStiles, W. S. & Burch, J. M. (1959). NPL colour-matching investigation: Final report. Optica Acta, 6, 1-26.
Stockman, A., & Sharpe, L. T. (2000). Spectral sensitivities of the middle- and long-wavelength sensitive cones derived from measurements in observers of known genotype. Vision Research, 40, 1711-1737.
