Open Access

Table A.1.

Limited ranges for the Model parameters

Line λ0 σ flux
dim state
HαB 6565.0±1.1 19.1±1.2 100±8
HβN 4860.7±1.2 4.6±1.2 10±2
HαN 6564.1±0.2 2.5±0.3 22±3
[N II]λ6583Å 6583.9±0.2 3.5±0.2 39±3
[O III]λ5007Å 5000.5±0.4 7.9±0.4 81±4
[S II]λ6716Å 6715.8±0.7 5.1±0.6 19±2
[S II]λ6732Å 6731.5±1.4 5.1±0.6 14±2

bright state

HαB1 6562.1±1.2 22.9±0.7 2194±254
HαB2 6572.3±2.4 72.9±4.3 1061±51
HαB3 6572.8±1.1 15.3±0.9 1081±251
HβB1 4862.3±0.8 29.1±1.7 580±50
HβB2 4864.7±0.3 13.1±0.6 488±54
HαN* 6564.1 2.5 25±8
HβN 4860.7 4.6 0
[O III]λ5007Åc 5007.2±0.2 1.7±0.3 22±4
[O III]λ5007Åe 4999.2±0.9 8.8±0.7 73±7
[N II]λ6583Å* 6583.9 3.5 88±9
[S II]λ6716Å 6718.2±0.7 2.7±0.8 11±3
[S II]λ6732Å 6732.6±0.8 2.8±0.8 9±3

Notice: The first column shows which emission component is described. The second, the third and the fourth columns show the determined central wavelength in units of Å, the line width (second moment) in units of Å and the emission flux in units of 10−17erg/s/cm2 of the corresponding emission component. For the component with suffix N (B) means narrow (broad) component in Balmer emission line. The narrow emission lines of HαN and [N II]λ6583Å in the bright state are measured by their central wavelengths and line widths to be fixed to the values measured in the dim state, therefore, corresponding uncertainties (same as the ones in the dim state) are not given.

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