Table 1
Parameters for the different SFH shown in Fig. 6.
| Gaussian | Other | ||||
|
|
|||||
| Name | μ | σ | Gap width | Gap position | c |
|
|
|||||
| basic | 0.5 | 1.0 | 0. | N/A | 0.30 |
| low C | 0.5 | 1.0 | 0. | N/A | 0.01 |
| peak shift | 3.0 | 1.0 | 0. | N/A | 0.01 |
| thin peak (a) | 0.5 | 0.2 | 0. | N/A | 0.01 |
| +gap | 0.5 | 1.0 | 1. | 9 | 0.01 |
| thin peak (b) | 0.5 | 0.2 | 0. | N/A | 0.01 |
Notes. The SFH consists of a Gaussian peak, with μ and σ corresponding to the mean and width of the peak (see Eq. (14)). Low C indicates that the constant part of the SFH has a low value. The thin-peak SFRs (a and b) change the width of the peak. Thin peak (a) shows an SFH where the peak is narrow and the height of the constant part is the same as for the basic case. Thin peak (b) is where the constant is adjusted so that the mass fraction formed in the peak is the same as for the basic case.
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