Wind properties of variable B supergiants - Evidence of pulsations connected with mass-loss episodes

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Table 3

Stellar and wind parameters derived from line fitting procedures.

STAR	T_eff	log g	β	Ṁ	V_∞	V_macro	V_micro	V sin i	R_⋆	log (L∕L_⊙)	log D_mom	log (L∕M)	log Q
	K	dex		10⁻⁶ M_⊙ yr⁻¹	km s⁻¹	km s⁻¹	km s⁻¹	km s⁻¹	R_⊙	dex	dex	dex	dex
HD 34085	12 700 ± 500	1.70 ± 0.1	2.6	0.23±0.02	155±46	52±3	10 ± 2	30	72	5.09 ± 0.09	27.22 ± 0.19	4.13	− 12.71 ± 0.32
HD 38771	25 000 ± 1000	2.70 ± 0.1	1.5	0.14±0.04	1500±150	60±10	13 ± 2	80	13	4.78 ± 0.07	27.69 ± 0.19	4.27	− 13.29 ± 0.24
HD 41117	19 000 ± 1000	2.30 ± 0.1	2.0	0.17±0.03	510±51	65±20	10 ± 5	40	23	4.84 ± 0.16	27.38 ± 0.15	4.27	− 12.78 ± 0.23
HD 42087	16 500 ± 1000	2.45 ± 0.1	2.0	0.57±0.05	700±70	80±15	15 ± 5	80	55	5.31 ± 0.43	28.27 ± 0.13	3.83	− 13.12 ± 0.23
HD 47240	19 000 ± 1000	2.40 ± 0.1	1.0	0.24±0.02	450±90	60±10	10 ± 3	95	30	5.03 ± 0.30	27.57 ± 0.15	4.08	− 12.82 ± 0.26
HD 52089	23 000 ± 1000	3.00 ± 0.1	1.0	0.02±0.006	900±270	65±5	8 ± 2	10	11	4.49 ± 0.05	26.58 ± 0.28	3.88	− 13.69 ± 0.38
HD 52382	21 500 ± 1000	2.45 ± 0.1	2.2	0.24±0.04	1000±100	65±5	10 ± 2	55	21	4.94 ± 0.32	27.84 ± 0.14	4.29	− 13.10 ± 0.21
HD 53138	18 000 ± 1000	2.25 ± 0.2	2.0	0.24±0.02	600±120	50±10	10 ± 4	40	46	5.31 ± 0.32	27.79 ± 0.14	4.19	− 13.09 ± 0.22
	18 000 ± 1000	2.25 ± 0.2	2.0	0.20±0.01	450±135	60±5	9 ± 3	40	46	5.31 ± 0.32	27.59 ± 0.14	4.19	− 13.36 ± 0.22
HD 58350	15 000 ± 500	2.00 ± 0.1	3.0	0.15±0.02	233 ±23	70±10	12 ± 2	40	54	5.13 ± 0.23	27.21 ± 0.13	4.12	− 12.97 ± 0.20
	16 000 ± 500	2.00 ± 0.1	3.0	0.12±0.01	175±18	50±10	10 ± 5	40	54	5.24 ± 0.23	26.98 ± 0.13	4.23	− 12.90 ± 0.20
HD 64760	23 000 ± 1000	2.90 ± 0.1	0.5	0.42±0.06	1500 ± 150	100 ± 50	15 ± 5	230	12	4.57 ± 0.08	28.14 ± 0.12	3.73	− 12.76 ± 0.18
HD 74371	13 700 ± 500	1.80 ± 0.1	2.0	0.28±0.03	200±60	60±10	10 ± 3	30	73	5.23 ± 0.19	27.48 ± 0.21	4.17	− 12.80 ± 0.33
HD 75149	16 000 ± 1000	2.10 ± 0.1	2.5	0.09±0.03	400±40	62±12	9 ± 3	40	61	5.35 ± 0.29	27.25 ± 0.11	4.14	− 13.63 ± 0.22
	16 000 ± 1 000	2.10 ± 0.1	2.5	0.20±0.01	350±35	52±12	11 ± 1	40	61	5.35 ± 0.29	27.54 ± 0.11	4.14	− 13.19 ± 0.22
	16 000 ± 1000	2.10 ± 0.1	2.5	0.16±0.05	400±40	57±7	17 ± 1	40	61	5.35 ± 0.29	27.50 ± 0.11	4.14	− 13.37 ± 0.22
	16 000 ± 1000	2.10 ± 0.1	2.5	0.25±0.01	350±35	55±10	15 ± 1	40	61	5.35 ± 0.29	27.64 ± 0.11	4.14	− 13.10 ± 0.22
HD 79186	15 800 ± 500	2.00 ± 0.1	3.3	0.40±0.02	400±40	53±7	11 ± 1	40	61	5.33 ± 0.38	27.90 ± 0.11	4.21	− 12.98 ± 0.20
HD 80077	17 700 ± 1000	2.20 ± 0.1	3.2	5.4±0.50	200±20	⋯	⋯	10	195	6.53 ± 0.17	28.86 ± 0.14	4.23	− 12.15 ± 0.26
	17 700 ± 1000	2.20 ± 0.1	3.0	5.4±0.50	150±15	60±5	10 ± 5	10	195	6.53 ± 0.17	28.98 ± 0.14	4.23	− 11.97 ± 0.26
HD 92964	18 000 ± 1000	2.20 ± 0.1	2.0	0.49±0.03	370±55	40± 5	11 ± 1	45	70	5.67 ± 0.49	27.98 ± 0.13	4.25	− 12.93 ± 0.25
HD 99953	19 000 ± 1000	2.30 ± 0.1	2.0	0.08±0.01	250±50	50± 5	18 ± 2	50	25	4.87 ± 0.37	26.80 ± 0.14	4.22	− 12.79 ± 0.24
	19 000 ± 1000	2.30 ± 0.1	2.0	0.13 ± 0.01	500±100	50 ± 5	18 ± 2	50	25	4.87 ± 0.37	27.33 ± 0.14	4.22	− 13.03 ± 0.24
	19 000 ± 1000	2.30 ± 0.1	2.0	0.22 ± 0.01	700±140	50 ± 5	18 ± 2	50	25	4.87 ± 0.37	27.69 ± 0.14	4.22	− 13.02 ± 0.24
HD 111973	16 500 ± 1000	2.10 ± 0.1	2.0	0.21 ± 0.01	350±70	57±8	12 ± 2	35	46	5.16 ± 0.20	27.51 ± 0.15	4.19	− 13.02 ± 0.27
	16 500 ± 1000	2.10 ± 0.1	2.0	0.14 ± 0.004	350 ± 105	63± 3	12 ± 2	35	46	5.16 ± 0.20	27.33 ± 0.15	4.19	− 13.19 ± 0.27
HD 115842	25 500 ± 1000	2.75 ± 0.1	2.5	1.80±0.30	1700±340	63±3	23 ± 7	50	35	5.67 ± 0.62	29.06 ± 0.18	4.30	− 12.91 ± 0.28
HD 148688	21 000 ± 1000	2.45 ± 0.1	2.5	1.15±0.20	1200±360	65±5	11 ± 1	50	31	5.23 ± 0.28	28.69 ± 0.23	4.26	− 12.80 ± 0.36

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