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Fig. 2.

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Line-to-continuum ratio plots of H2, [Fe II], and Br-γ emission. Intrinsic emission appears bright in these images, whereas scattered light is represented by a constant ratio close to unity. The source position is represented with a red plus symbol. A signal-to-noise threshold, set at three times the background noise, is implemented in these images to reject background emission, meaning the morphologies one sees in these figures is due to a combination of the continuum and the intrinsic line emission. Top left: Integrated H2 emission between −140 km s−1 and +60 km s−1 divided by nearby continuum. The intrinsic line emission here comes from the cavity walls and a H2 knot at the base of the left cavity wall (A1). Top right: Integrated [Fe II] emission between −310 km s−1 and −100 km s−1 divided by nearby continuum. The intrinsic line emission here traces the high-velocity atomic jet. Bottom left: Integrated high-velocity Br-γ emission between −230 km s−1 and −130 km s−1 divided by nearby continuum. The intrinsic line emission here again traces the high-velocity atomic jet. Bottom right: Integrated low-velocity Br-γ emission between −100 km s−1 and +100 km s−1 divided by nearby continuum. There is no spatially extended intrinsic emission detected here.

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