G4 . | ||||
---|---|---|---|---|
FAST++ | Bagpipes | Bagpipes | CIGALE | |
Redshift | 2.13a | 2.13a | 2.13a | 2.13a |
log M⋆ | 10.99 ± 0.05 | 11.16 | 11.22 | 11.25 ± 0.10 |
[11.10,11.21] | [11.17,11.30] | |||
SFR|$_{\rm SED}^{\dagger }$|d | 0.02 | 0.00b | 0.01b | 1.3e−4 ± 7.04e−5b,c |
[0.00,0.00] | [0.00,0.04] | |||
log(ΔMS)d | −3.79 | −69.68 | −4.40 | −6.20 |
log (age)e | 9.15 | 8.83 | 9.27 | 9.26 ± 0.20 |
[8.79,8.97] | [9.20,9.30] | |||
SFH | Delayed-τ | Double-power law | Non-parametric | Delayed-τ |
AV | 0.10 | 0.75 | 0.51 | 0.57 ± 0.10 |
[0.50,0.93] | [0.33,0.72] | |||
χ2f | 2.1 | 15.8 | 22.4 | 11.3 |
G4 . | ||||
---|---|---|---|---|
FAST++ | Bagpipes | Bagpipes | CIGALE | |
Redshift | 2.13a | 2.13a | 2.13a | 2.13a |
log M⋆ | 10.99 ± 0.05 | 11.16 | 11.22 | 11.25 ± 0.10 |
[11.10,11.21] | [11.17,11.30] | |||
SFR|$_{\rm SED}^{\dagger }$|d | 0.02 | 0.00b | 0.01b | 1.3e−4 ± 7.04e−5b,c |
[0.00,0.00] | [0.00,0.04] | |||
log(ΔMS)d | −3.79 | −69.68 | −4.40 | −6.20 |
log (age)e | 9.15 | 8.83 | 9.27 | 9.26 ± 0.20 |
[8.79,8.97] | [9.20,9.30] | |||
SFH | Delayed-τ | Double-power law | Non-parametric | Delayed-τ |
AV | 0.10 | 0.75 | 0.51 | 0.57 ± 0.10 |
[0.50,0.93] | [0.33,0.72] | |||
χ2f | 2.1 | 15.8 | 22.4 | 11.3 |
aBest-fitting photo-z from eazy-py.bAveraged over 100 Myr. cIncluding the ALMA 2 mm data point. dWe note the limitation of the SFR from the SED which is likely to introduce an unrealistically low value of SFR and hence ΔMS especially for the parametric SFH models. The photometry (|$\mathcal {R}_s$|-band) and the best-fitting dust attenuation (AV) suggest the SFR of |$\sim 8\, {\rm M}_{\odot }$| yr−1 and log (ΔMS) ∼−1.6 (see also the main text in Section 4.1). eMass weighted.
fWe quote the absolute χ2 value, as the templates employed (as is the case for many SED fitting codes) are not independent of each other, and degrees of freedom are ill-defined (e.g. Smith et al. 2012).
G4 . | ||||
---|---|---|---|---|
FAST++ | Bagpipes | Bagpipes | CIGALE | |
Redshift | 2.13a | 2.13a | 2.13a | 2.13a |
log M⋆ | 10.99 ± 0.05 | 11.16 | 11.22 | 11.25 ± 0.10 |
[11.10,11.21] | [11.17,11.30] | |||
SFR|$_{\rm SED}^{\dagger }$|d | 0.02 | 0.00b | 0.01b | 1.3e−4 ± 7.04e−5b,c |
[0.00,0.00] | [0.00,0.04] | |||
log(ΔMS)d | −3.79 | −69.68 | −4.40 | −6.20 |
log (age)e | 9.15 | 8.83 | 9.27 | 9.26 ± 0.20 |
[8.79,8.97] | [9.20,9.30] | |||
SFH | Delayed-τ | Double-power law | Non-parametric | Delayed-τ |
AV | 0.10 | 0.75 | 0.51 | 0.57 ± 0.10 |
[0.50,0.93] | [0.33,0.72] | |||
χ2f | 2.1 | 15.8 | 22.4 | 11.3 |
G4 . | ||||
---|---|---|---|---|
FAST++ | Bagpipes | Bagpipes | CIGALE | |
Redshift | 2.13a | 2.13a | 2.13a | 2.13a |
log M⋆ | 10.99 ± 0.05 | 11.16 | 11.22 | 11.25 ± 0.10 |
[11.10,11.21] | [11.17,11.30] | |||
SFR|$_{\rm SED}^{\dagger }$|d | 0.02 | 0.00b | 0.01b | 1.3e−4 ± 7.04e−5b,c |
[0.00,0.00] | [0.00,0.04] | |||
log(ΔMS)d | −3.79 | −69.68 | −4.40 | −6.20 |
log (age)e | 9.15 | 8.83 | 9.27 | 9.26 ± 0.20 |
[8.79,8.97] | [9.20,9.30] | |||
SFH | Delayed-τ | Double-power law | Non-parametric | Delayed-τ |
AV | 0.10 | 0.75 | 0.51 | 0.57 ± 0.10 |
[0.50,0.93] | [0.33,0.72] | |||
χ2f | 2.1 | 15.8 | 22.4 | 11.3 |
aBest-fitting photo-z from eazy-py.bAveraged over 100 Myr. cIncluding the ALMA 2 mm data point. dWe note the limitation of the SFR from the SED which is likely to introduce an unrealistically low value of SFR and hence ΔMS especially for the parametric SFH models. The photometry (|$\mathcal {R}_s$|-band) and the best-fitting dust attenuation (AV) suggest the SFR of |$\sim 8\, {\rm M}_{\odot }$| yr−1 and log (ΔMS) ∼−1.6 (see also the main text in Section 4.1). eMass weighted.
fWe quote the absolute χ2 value, as the templates employed (as is the case for many SED fitting codes) are not independent of each other, and degrees of freedom are ill-defined (e.g. Smith et al. 2012).
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