Open Access

Table 5

Goodness-of-fit metrics for the GCM models.

TiO/VO Magnetic drag τfric [s] All data No Sp.Ch2
χ2 χ r 2 $\chi_r^2$ χ2 χ r 2 $\chi_r^2$
X X + ∞ 2261.4 44.3 1889.4 37.8
X 104 638.6 12.5 423.4 8.5
X + ∞ 1448.1 28.4 1156.9 23.1
106 498.7 9.8 322.9 6.5
105 362.5 7.1 206.5 4.1
104 265.2 5.2 130.4 2.6

Notes. The inclusion or exclusion of TiO/VO and magnetic drag in the GCM models is indicated by the symbols ✓ and X, respectively. The χ2 metric is computed as χ 2 = ( y i m i ) 2 / σ i 2 $\chi^2=\sum{\left(y_i-m_i\right)^2/\sigma_i^2}$, where y i is the passband-integrated GCM value, and m i and σ i are the occultation depth measurement and uncertainty, respectively. The reduced χ2 metric, χ r 2 $\chi_r^2$, is computed as χ r 2 = χ 2 / N $\chi_r^2=\chi^2/N$, where N is the number of data points. The GCM models with TiO/VO (no drag and τfric = 104 s) are shown in Fig. 9. The measured occultation depths used to compute the χ2 and χ r 2 $\chi_r^2$ values are reported in Table 3. The rightmost 2 columns entitled ‘No Sp.Ch2’ report the metrics computed on all but the Spitzer/IRAC/Ch. 2 data point to account of the GCMs not modelling the high CO/CO2 emission peak.

Current usage metrics show cumulative count of Article Views (full-text article views including HTML views, PDF and ePub downloads, according to the available data) and Abstracts Views on Vision4Press platform.

Data correspond to usage on the plateform after 2015. The current usage metrics is available 48-96 hours after online publication and is updated daily on week days.

Initial download of the metrics may take a while.