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Table 1.

Rankings of different fitted models with their parameters.

Model Normalized Ranking
parameters (normalized) flux density AIC BIC lnL
Broken power-lawa
α1 = 0.53 ± 0.04 ( = 0.42 ± 0.06) Eq. (3) 2 2 1
α2 = 0.94 ± 0.06

Model (1) – mixed modelb
α = 0.74 ± 0.06 6 5 6
τ1 = 0.2 ± 0.2

Model (2) – foreground screen modelb
α = 0.73 ± 0.06 6 7 7
τ1 = 0.11 ± 0.08

Model (3) – synchrotron aging modelb
α = 0.24 ± 0.06 4 4 5
Δα = 0.55 ± 0.04

Model (4) – synchrotron self-absorption modelc
α = 0.70 ± 0.05 8 8 8
νb = 0.76 ± 0.07 GHz

Model (5) – (Lisenfeld et al. 2004)b 1 1 3
α = 0.47 ± 0.03

Model (6a) – synchrotron aging+FFEb
α = 0.24 ± 0.07
Δα = 0.55 ± 0.04 7 5 4
fth(1 GHz)=0.00 ± 0.02

Model (6b) – Lisenfeld et al. (2004)+FFEb
α = 0.50 ± 0.06 3 3 2
fth(1 GHz)=0.01 ± 0.027

Notes.

For simplicity, we show models without their normalization parameter and indicate the additional contribution of free–free emission with a thermal fraction at 1GHz by “FFE”. We show the rankings based on the Akaike and Bayesian information criteria and the log-likelihood test (lnL).

(a)

The broken power-law model was included in the table for comparison.

(b)

See Pacholczyk (1980) for details.

(c)

See Condon & Ransom (2016) for details.

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