Table 1
Herschel/PACS observations of OH in Mrk 231.
Transition | Rest wavelengthsa | Programb | Obs. IDc | Number of | σ |
(μm) | spatial pixelsd | (Jy) | |||
|
|||||
OH ![]() |
119.233−119.441 | GT | 1342186811 | 1 | 0.29 |
OH ![]() |
79.118−79.181 | GT | 1342186811 | 1 | 0.26 |
GT | 1342186811 | 1 | 0.26 | ||
OT2 | 1342253536 | 1 | 0.23 | ||
OH ![]() |
53.261−53.351 | OT2 | 1342253530 | 1 | 0.24 |
OH ![]() |
84.420−84.597 | OT2 | 1342253537 | 3 | 0.50 |
OH ![]() |
65.132−65.279 | GT | 1342207782 | 1 | 0.19 |
GT | 1342207782 | 3 | 0.24 | ||
OT2 | 1342253532 | 3 | 0.25 | ||
OH ![]() |
71.171−71.216 | OT2 | 1342253534 | 3 | 0.36 |
OH ![]() |
52.934−53.057 | OT2 | 1342253530 | 1 | 0.24 |
OH ![]() |
55.891−55.950 | OT2 | 1342253531 | 3 | 0.19 |
OH ![]() |
163.124−163.397 | OT1 | 1342223369 | 1 | 0.25 |
Notes.
The two values correspond to the two Λ-components of the doublets; each one is the average of the two hyperfine transitions that make up a component.
Number of spatial pixels used to generate the spectrum. In case of 1, the central pixel was used; in case of 3, the spectra from the three brightest spatial pixels were coadded. In all cases, the absolute fluxes were scaled to match the total flux as obtained by coadding the fluxes from the 25 pixels.
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