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Table 1

Physical parameters resulting from modelling the observed spectra.

Pos V s 1 n 0 2 F 3 D 4 Hβ abs5 Pos V s 1 n 0 2 F 3 D 4 Hβ abs5
35 300. 90. 20 7.8 0.096 123 750. 90 16 0.74 0.04
36 300. 100. 70 9.5 0.25 124 60. 60. 1 860 0.0047
37 160. 100. 4 0.76 0.0073 124 600. 80. 30 54 0.3
38 110. 110. 9 5.6 0.02 125 600. 90. 30 63 0.39
39 120. 110. 8 2.9 0.0165 132 550. 60. 95 50 0.5
40 120. 110. 8 3.5 0.018 133 110. 110. 10 6 0.022
51 120. 100. 12 230 0.04 134 110. 110. 10 6 0.022
52 90. 130. 12 17 0.038 135 110. 110. 10 6 0.022
53 80. 120. 12 15 0.029 136 110. 110. 10 13 0.025
54 110. 130. 10 5. 0.032 137 100. 110. 10 30 0.026
55 140. 130. 9 2.3 0.026 138 100. 120. 12 280 0.04
56 110. 110. 10 5.6 0.022 139 100. 120. 10 280 0.042
57 110. 100. 10 6.8 0.02 139 750. 90. 13 0.5 0.057
58 180. 100. 18 3.6 0.025 140 90. 90. 11 73 0.046
60 750. 110. 80 0.1 0.13 140 750. 80. 13 0.92 0.037
66 160. 100. 15 4. 0.026 141 90. 90. 11 1000 0.06
67 130. 100. 5 4.7 0.015 141 600. 90. 20 27.2 0.156
68 110. 100. 4.5 5. 0.01 142 80. 90. 1 2.4 0.0023
69 110. 100. 4.5 4.4 0.01 148 380. 120. 33 3.5 0.1
70 110. 110. 10 6. 0.027 149 110. 110. 9 7.6 0.021
71 550. 80. 50 9.5 0.3 150 220. 100. 10 1.6 0.02
72 220. 190. 32 1. 0.09 151 160. 100. 5 1.7 0.011
73 220. 100. 8 1.23 0.02 152 160. 100. 4 1.3 0.009
74 220. 110. 10 1.33 0.025 153 160. 100. 4 1.75 0.01
83 60. 100. 11 50 0.019 154 70. 90. 0.7 2 0.0016
84 100. 90. 5 170 0.013 155 70. 90. 0.7 1.6 0.0015
85 110. 100. 11 12 0.03 155 750. 90. 1 0.2 0.0013
85 110. 100. 7 5.5 0.02 156 50. 100. 0.07 0.15 0.00009
86 320. 100. 60 7 0.23 156 600. 60. 0.04 0.5 0.0003
87 320. 100. 15 7 0.28 157 650. 60. 0.05 0.5 0.0003
88 280. 120. 15 7 0.28 165 110. 110. 13 13 0.039
89 120. 150. 13 7 0.04 166 220. 100. 8 1.2 0.019
90 80. 90. 0.3 2.7 0.0001 167 160. 100. 5 1.4 0.011
91 120. 100. 5 5 0.013 168 160. 100. 4 1.2 0.0087
91 800. 100. 13 0.24 0.028 169 160. 100. 3.5 1.1 0.0085
92 120. 100. 4 4.7 0.013 170 70. 90. 0.7 1.7 0.0016
92 700. 100. 13 0.33 0.039 171 70. 100. 0.25 0.09 0.000135
93 650. 90. 13 0.49 0.036 172 50. 100. 0.07 0.12 0.000067
99 120. 110. 8 3.8 0.018 173 80. 70. 0.05 0.15 0.0001
100 550. 80. 45 10 0.28 181 300. 120. 26 1.7 0.07
101 550. 80. 70 22 0.45 182 160. 100. 5 1.4 0.011
102 550. 70. 50 8.3 0.2 183 120. 100. 3 1.5 0.006
103 550. 70. 50 12.4 0.22 184 160. 100. 4 1.2 0.001
104 380. 120. 33 1.5 0.11 185 80. 90. 1 1.6 0.0022
105 180. 180. 20 1. 0.05 186 70. 90. 0.7 1.5 0.0015
106 110. 110. 10 13 0.04 187 180. 70. 0.03 0.2 0.00019
107 50. 100. 0.5 2.2 0.001 188 180. 70. 0.06 0.14 0.00011
107 800. 100. 3 0.156 0.002 197 110. 110. 9 6.1 0.021
108 100. 110. 9 280 0.033 198 180. 160. 20 1.6 0.051
108 750. 90. 16 0.58 0.07 199 90. 100. 1.6 1.2 0.003
109 750. 90. 16 0.58 0.07 200 70. 90. 0.9 2.7 0.0018
110 750. 90. 13 0.65 0.06 201 70. 90. 0.7 1.3 0.0015
111 750. 90. 10 0.4 0.04 202 100. 100. 0.8 0.4 0.0017
115 600. 80. 65 12 0.36 203 160. 60. 0.9 1 0.002
116 550. 80. 60 7 0.28 213 300. 120. 30 1.8 0.05
117 550. 80. 50 9.5 0.3 214 500. 80. 40 7 0.225
118 550. 80. 60 11.3 0.3 215 120. 150. 13 2.7 0.037
119 550. 80. 70 9.2 0.32 216 160. 100. 3.5 1 0.0085
120 380. 120. 33 1.5 0.11 217 90. 90. 11 45 0.0045
121 120. 150. 13 4 0.04 218 100. 80. 7 20 0.023
122 130. 80. 6 37 0.028 219 90. 120. 0.75 0.73 0.002
123 110. 110. 10 15 0.04

Notes. 

(1)

In km s-1;

(2)

in cm-3;

(3)

in 109 photons cm-2 s-1 eV-1 at the Lyman limit;

(4)

in 1017 cm;

(5)

in erg cm-2 s-1.

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