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Table 6b
Paα and H2 1−0S(1) velocity dispersion values of the ULIRGs subsample
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| IRAS 06206-6315 | IRAS 12112+0305 | ||||||||
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| Region | Paασ | H2 1−0S(1) σ | Region | Paασ | H2 1−0S(1) σ | ||||
| (km s-1) | (km s-1) | (km s-1) | (km s-1) | ||||||
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| Nuclear | 177 ± 4 | 139 ± 2 | Nuclear | 134 ± 1 | 118 ± 3 | ||||
| Integrated | 148 ± 93 | 117 ± 7 | Integrated | 153 ± 5 | 160 ± 8 | ||||
| Paα max† | 177 ± 4 | 139 ± 3 | Paα max† | 134 ± 1 | 119 ± 3 | ||||
| H2 1−0S(1)† | 177 ± 4 | 139 ± 2 | H2 1−0S(1) | 121 ± 1 | 150 ± 2 | ||||
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| IRAS 14348-1447 | IRAS 17208-0014 | ||||||||
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| Region | Paασ | H2 1−0S(1) σ | Region | Paασ | H2 1−0S(1) σ | ||||
| (km s-1) | (km s-1) | (km s-1) | (km s-1) | ||||||
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| Nuclear | 109 ± 1 | 111 ± 2 | Nuclear | 219 ± 6 | 187 ± 3 | ||||
| Integrated | 124 ± 3 | 127 ± 3 | Integrated | 201 ± 5 | 200 ± 18 | ||||
| Paα max† | 109 ± 1 | 111 ± 2 | Paα max† | 219 ± 6 | 187 ± 3 | ||||
| H2 1−0S(1)† | 108 ± 1 | 111 ± 2 | H2 1−0S(1)† | 222 ± 6 | 189 ± 3 | ||||
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| IRAS 21130-4446 | IRAS 22491-1808 | ||||||||
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| Region | Paασ | H2 1−0S(1) σ | Region | Paασ | H2 1−0S(1) σ | ||||
| (km s-1) | (km s-1) | (km s-1) | (km s-1) | ||||||
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| Nuclear | 132 ± 6 | 131 ± 4 | Nuclear | 66 ± 1 | 83 ± 6 | ||||
| Integrated | 119 ± 3 | 113 ± 5 | Integrated | 76 ± 2 | 102 ± 8 | ||||
| Paα max | 75 ± 0 | 74 ± 6 | Paα max | 105 ± 2 | 125 ± 2 | ||||
| H2 1−0S(1)† | 137 ± 6 | 127 ± 4 | H2 1−0S(1) | 105 ± 1 | 125 ± 2 | ||||
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| IRAS 23128-5919 | |||||||||
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| Region | Paασ | H2 1−0S(1) σ | |||||||
| (km s-1) | (km s-1) | ||||||||
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| Nuclear | 116 ± 2 | 81 ± 3 | |||||||
| Integrated | 104 ± 2 | 87 ± 6 | |||||||
| Paα max† | 116 ± 2 | 82 ± 3 | |||||||
| H2 1−0S(1)† | 116 ± 2 | 82 ± 3 | |||||||
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Notes. The method for extracting the spectra and the selection criteria for the regions are the same as for Table 5b.
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