Fig. 4
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Position–velocity cuts taken along the outflow axis (PA = 0°) of the CO(2–1) 230.54 GHz (top) and the CO υ = 1–0 P(5) 4.709 µm (bottom) transitions. For the CO(2–1), we used the spatially unsmoothed cube with a beam FWHM of 0″.23 × 0″.20. The nuclear P(5) absorption around the offset of ~0″ is masked in the bottom panel. Positive offsets are north of the nucleus.
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