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Table 1

Characteristic quantities for λ,IMF(t) when modeled as a power law.

Index α tλ % at tλ t λ,99% t λ,95% t λ,90% t λ,80% t λ,50%
106 yr 106 yr 106 yr 106 yr 106 yr 106 yr

generic Q(H) >2.00 <13 >89% <148 <30 <15 <7.5 <3
generic UV 1.50 131 91% 3325 375 112 31 5
generic U 1.10 937 80% 11156 6187 3100 885 43
generic IR/V 0.80 2549 67% 12457 10462 8337 5120 817

α values from comparison with synthesis models in Sect. 3.3

Q(H) 4.00 2 56% 9 5 4 3 2
galex/FUV 1.55 101 91% 2386 254 80 24 5
galex/NUV 1.50 131 91% 3325 375 112 31 5
sdss/u 1.07 1060 79% 11 401 6824 3683 1156 58
sdss/g 0.88 2055 71% 12 284 9753 7243 3861 413
sdss/r 0.75 2865 65% 12 534 10 796 8885 5834 1157
sdss/i 0.72 3055 64% 12 573 10 965 9170 6228 1388
sdss/z 0.66 3430 62% 12 636 11 246 9656 6936 1890

Notes. Values of the slope of the SSP luminosity evolution λ,IMF(t) when modeled as a power law α (see below), the mean age of λ,IMF(t) denoted as tλ, the percentage of the sensitivity of λ,IMF(t) in the 0 to tλ age range, and the ages where the sensitivity to λ,IMF(t) reaches a x% value of the total sensitivity, , for 99, 95, 90, 80, and 50% for the set of bands used in this work. The results assume that λ,IMF(t) is flat up to 3 Myr and follows a decreasing power law with exponent α for older ages up to tage = 13 Gyr. The upper part of the table shows the generic α values used in this section for different bands, guided by the results in Fig. 1. The lower part of the table shows α values chosen a posteriori to roughly fit the results of the detailed computations presented in Sect. 3.3 (Table 2).

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