Another X-ray UFO without a momentum-boosted molecular outflow: ALMA CO(1–0) observations of the galaxy pair IRAS 05054+1718
We present Atacama Large Millimetre/submillimetre Array (ALMA) CO(1–0) observations of the nearby infrared luminous (LIRG) galaxy pair IRAS 05054+1718 (also known as CGCG 468-002), as well as a new analysis of X-ray data of this source collected between 2012 and 2021 using the Nuclear Spectroscopic...
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Veröffentlicht in: | Astronomy and astrophysics (Berlin) 2023-05, Vol.673, p.A46 |
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Hauptverfasser: | , , , , , , , , , , |
Format: | Artikel |
Sprache: | eng |
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Zusammenfassung: | We present Atacama Large Millimetre/submillimetre Array (ALMA) CO(1–0) observations of the nearby infrared luminous (LIRG) galaxy pair IRAS 05054+1718 (also known as CGCG 468-002), as well as a new analysis of X-ray data of this source collected between 2012 and 2021 using the Nuclear Spectroscopic Telescope Array (
NuSTAR
),
Swift
, and the
XMM-Newton
satellites. The western component of the pair, NED01, hosts a Seyfert 1.9 nucleus that is responsible for launching a powerful X-ray ultra-fast outflow (UFO). Our X-ray spectral analysis suggests that the UFO could be variable or multi-component in velocity, ranging from
v
/
c
∼ −0.12 (as seen in
Swift
) to
v
/
c
∼ −0.23 (as seen in
NuSTAR
), and constrains its momentum flux to be
ṗ
out
X−ray
∼ (4 ± 2) × 10
34
g cm s
−2
. The ALMA CO(1–0) observations, obtained with an angular resolution of 2.2″, although targeting mainly NED01, also include the eastern component of the pair, NED02, a less-studied LIRG with no clear evidence of an active galactic nucleus (AGN). We study the CO(1–0) kinematics in the two galaxies using the 3D-BAROLO code. In both sources we can model the bulk of the CO(1–0) emission with rotating disks and, after subtracting the best-fit models, we detect compact residual emission at
S
/
N
= 15 within ∼3 kpc of the centre. A molecular outflow in NED01, if present, cannot be brighter than such residuals, implying an upper limit on its outflow rate of
Ṁ
out
mol
≲ 19 ± 14
M
⊙
yr
−1
and on its momentum rate of
ṗ
out
mol
≲ (2.7 ± 2.4) × 10
34
g cm s
−1
. Combined with the revised energetics of the X-ray wind, we derive an upper limit on the momentum rate ratio of
ṗ
out
mol
/
ṗ
out
X−ray
|
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ISSN: | 0004-6361 1432-0746 1432-0746 |
DOI: | 10.1051/0004-6361/202245630 |