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Table A.6.

Parameters derived from the fits of the lines of J1713+57.

Line FWHM vs Flux x 10−15 Flux fraction
[km s−1] [km s−1] [erg cm−2s−1)] [%]
Paα (n1) 128±28 118±15 0.43±0.19 7
Paα (n2) 284±47 -112±24 0.85±0.37 14
Paα (i) 1225±85 14±50 3.01±1.26 51
Paα (b) 2546±803 -619±370 1.6±0.97 27
He II (n1) 128 21±50 0.03±0.02 26
He II (n2) 284 -209±50* 0.1±0.05 73
He I (n) 128 -5±48 0.03±0.02 100
Brδ (n) 278±115 28±56 0.09±0.05 100
[Si VI] (n) 384±87 31±21 0.31±0.15 21
[Si VI] (i) 1119±122 14 0.55±0.29 39
[Si VI] (b) 1966±104 -618 0.55±0.25 38
H2 1-0S(1) (n) 392±35 36±23 0.41±0.17 100
H2 1-0S(2) (n) 462±46 5±30 0.19±0.08 100
H2 1-0S(3) (n) 341±23 -21±17 0.33±0.14 100
H2 1-0S(4) (n) 284±71 -11±34 0.08±0.04 100
H2 1-0S(5) (n) 424±61 -9±23 0.29±0.13 100

Notes. Same as in Table A.1, but for J1713+57.* The shift between the n and i components was tied following the fit of Paα.

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