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Table A.2.

Parameters derived from the fits of the lines of J0945+17.

Line FWHM vs Flux x10−15 Flux fraction
[km s−1] [km s−1] [erg cm−2 s−1)] [%]
Paα (n) 273±11 0±4 1.94±0.72 33
Paα (i) 837±41 -132±14 3.32±1.26 57
Paα (b) 1663 -374±129 0.51±0.33 8
He II (n) 272 -53±32 0.12±0.05 41
He II (i) 837 -184±34* 0.18±0.07 58
He I (n) 272 62±29 0.2±0.08 45
He I (i) 837 -69±39* 0.24±0.14 54
Brδ (n) 540±198 -79±44 0.26±0.14 100
[Si VI] (n) 290 -48±7 0.59±0.22 31
[Si VI] (i) 762 -248±41 0.62±0.29 33
[Si VI] (b) 1601±340 -449±288 0.65±0.36 34
H2 1-0S(1) (n) 361±104 -9±45 0.42±0.23 100
H2 1-0S(2) (n) 202±198 -129±78 0.11±0.12 100
H2 1-0S(3) (n) 317±61 -71±20 0.3±0.13 100
H2 1-0S(4) (n) 280±188 -23±38 0.1±0.08 100

Notes. Same as in Table A.1, but for J0945+17. * The shift between the n and i components was tied following the fit of Paα.

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