Table 2.

RMSE and Log evidence |$\log \mathcal {Z}$|⁠: the foreground signal is modelled using one single beam (⁠|$B_{t_0}$|⁠). Case (Ci) gives the explored cases. [t] lists all the time-steps analysed in each case. RMSE is the root-mean-square error of the detected signal with respect to the injected signal. |$\log \mathcal {Z}_{\mathrm{s}}$| is the evidence yielded by the foreground model including a Gaussian signal model, and |$\Delta \log \mathcal {Z}$| is the difference between the evidence yielded by the foreground model including a Gaussian signal model and the one without.

Case[t]RMSE (K)|$\log \mathcal {Z}_{\mathrm{s}}$||$\Delta \log \mathcal {Z}$|
C1t0, t10.066231.5 ± 0.362.8
C2t0, t20.035520.2 ± 0.3180.4
C3t0, t30.05693.3 ± 0.4161.8
C4t0, t40.024519.0 ± 0.3253.5
Case[t]RMSE (K)|$\log \mathcal {Z}_{\mathrm{s}}$||$\Delta \log \mathcal {Z}$|
C1t0, t10.066231.5 ± 0.362.8
C2t0, t20.035520.2 ± 0.3180.4
C3t0, t30.05693.3 ± 0.4161.8
C4t0, t40.024519.0 ± 0.3253.5

Note. [t0, t1, t2, t3, t4] = [2100′, 2115′, 4515′, 4615′, 4745′]

Table 2.

RMSE and Log evidence |$\log \mathcal {Z}$|⁠: the foreground signal is modelled using one single beam (⁠|$B_{t_0}$|⁠). Case (Ci) gives the explored cases. [t] lists all the time-steps analysed in each case. RMSE is the root-mean-square error of the detected signal with respect to the injected signal. |$\log \mathcal {Z}_{\mathrm{s}}$| is the evidence yielded by the foreground model including a Gaussian signal model, and |$\Delta \log \mathcal {Z}$| is the difference between the evidence yielded by the foreground model including a Gaussian signal model and the one without.

Case[t]RMSE (K)|$\log \mathcal {Z}_{\mathrm{s}}$||$\Delta \log \mathcal {Z}$|
C1t0, t10.066231.5 ± 0.362.8
C2t0, t20.035520.2 ± 0.3180.4
C3t0, t30.05693.3 ± 0.4161.8
C4t0, t40.024519.0 ± 0.3253.5
Case[t]RMSE (K)|$\log \mathcal {Z}_{\mathrm{s}}$||$\Delta \log \mathcal {Z}$|
C1t0, t10.066231.5 ± 0.362.8
C2t0, t20.035520.2 ± 0.3180.4
C3t0, t30.05693.3 ± 0.4161.8
C4t0, t40.024519.0 ± 0.3253.5

Note. [t0, t1, t2, t3, t4] = [2100′, 2115′, 4515′, 4615′, 4745′]

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