JWST/NIRSpec and MIRI observations of an expanding, jet-driven bubble of warm H2 in the radio galaxy 3C 326 N

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Volume 689 (September 2024)

A&A, 689 (2024) A314

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Table 5.

Properties of a one-Gaussian fit to the integrated spectrum for all detected emission lines.

Line	λ	F_Int	FWHM	z	V_off

	[μm]	[10⁻²⁰ W m²]	[km s⁻¹]		[km s⁻¹]
[FeII]	1.644	$60 . 7_{0.68}^{0.64}$ $60.7^{0.64}_{0.68}$	$573 . 0_{5.6}^{5.8}$ $573.0^{5.8}_{5.6}$	$0 . 09006_{1 e - 05}^{1 e - 05}$ $0.09006^{1e-05}_{1e-05}$	$75 . 2_{2.8}^{2.8}$ $75.2^{2.8}_{2.8}$
H₂ 1–0 S(8)	1.7146	$21 . 5_{0.59}^{0.5}$ $21.5^{0.5}_{0.59}$	$523 . 0_{13.0}^{15.0}$ $523.0^{15.0}_{13.0}$	$0 . 09022_{2 e - 05}^{1.9 e - 05}$ $0.09022^{1.9e-05}_{2e-05}$	$119 . 0_{5.4}^{5.2}$ $119.0^{5.2}_{5.4}$
H₂ 1–0 S(7)	1.748	$50 . 4_{0.75}^{0.73}$ $50.4^{0.73}_{0.75}$	$822 . 0_{17.0}^{16.0}$ $822.0^{16.0}_{17.0}$	$0 . 08994_{1.7 e - 05}^{1.7 e - 05}$ $0.08994^{1.7e-05}_{1.7e-05}$	$41 . 5_{4.6}^{4.7}$ $41.5^{4.7}_{4.6}$
H₂ 1–0 S(6)	1.7879	$29 . 0_{0.52}^{0.55}$ $29.0^{0.55}_{0.52}$	$630 . 0_{11.0}^{11.0}$ $630.0^{11.0}_{11.0}$	$0 . 09054_{1.5 e - 05}^{1.6 e - 05}$ $0.09054^{1.6e-05}_{1.5e-05}$	$206 . 0_{4.1}^{4.3}$ $206.0^{4.3}_{4.1}$
H₂ 1–0 S(5)	1.8357	$104 . 0_{0.55}^{0.51}$ $104.0^{0.51}_{0.55}$	$712 . 0_{3.9}^{3.9}$ $712.0^{3.9}_{3.9}$	$0 . 08998_{5.4 e - 06}^{4.9 e - 06}$ $0.08998^{4.9e-06}_{5.4e-06}$	$52 . 5_{1.5}^{1.4}$ $52.5^{1.4}_{1.5}$
Paα	1.8751	$71 . 3_{0.49}^{0.52}$ $71.3^{0.52}_{0.49}$	$571 . 0_{4.7}^{4.6}$ $571.0^{4.6}_{4.7}$	$0 . 09026_{5.4 e - 06}^{5.8 e - 06}$ $0.09026^{5.8e-06}_{5.4e-06}$	$130 . 0_{1.5}^{1.6}$ $130.0^{1.6}_{1.5}$
H₂ 1–0 S(4)	1.8919	$24 . 3_{0.37}^{0.38}$ $24.3^{0.38}_{0.37}$	$516 . 0_{8.0}^{8.1}$ $516.0^{8.1}_{8.0}$	$0 . 09022_{1.2 e - 05}^{1.2 e - 05}$ $0.09022^{1.2e-05}_{1.2e-05}$	$118 . 0_{3.3}^{3.3}$ $118.0^{3.3}_{3.3}$
H₂ 1–0 S(3)	1.9575	$154 . 0_{0.42}^{0.44}$ $154.0^{0.44}_{0.42}$	$625 . 0_{1.9}^{1.8}$ $625.0^{1.8}_{1.9}$	$0 . 09005_{2.4 e - 06}^{2.4 e - 06}$ $0.09005^{2.4e-06}_{2.4e-06}$	$70 . 3_{0.67}^{0.67}$ $70.3^{0.67}_{0.67}$
H₂ 1–0 S(2)	2.0337	$53 . 2_{0.45}^{0.46}$ $53.2^{0.46}_{0.45}$	$635 . 0_{6.0}^{6.7}$ $635.0^{6.7}_{6.0}$	$0 . 09009_{7.2 e - 06}^{7.6 e - 06}$ $0.09009^{7.6e-06}_{7.2e-06}$	$82 . 5_{2.0}^{2.1}$ $82.5^{2.1}_{2.0}$
H₂ 2–1 S(3)	2.0734	$15 . 7_{0.45}^{0.42}$ $15.7^{0.42}_{0.45}$	$669 . 0_{19.0}^{19.0}$ $669.0^{19.0}_{19.0}$	$0 . 09048_{2.5 e - 05}^{2.6 e - 05}$ $0.09048^{2.6e-05}_{2.5e-05}$	$189 . 0_{6.9}^{7.1}$ $189.0^{7.1}_{6.9}$
H₂ 1–0 S(1)	2.1217	$129 . 0_{0.4}^{0.37}$ $129.0^{0.37}_{0.4}$	$623 . 0_{1.9}^{1.8}$ $623.0^{1.8}_{1.9}$	$0 . 0902_{2.7 e - 06}^{2.6 e - 06}$ $0.0902^{2.6e-06}_{2.7e-06}$	$113 . 0_{0.76}^{0.71}$ $113.0^{0.71}_{0.76}$
H₂ 1–0 Q(1)	2.4065	$71 . 5_{0.62}^{0.64}$ $71.5^{0.64}_{0.62}$	$507 . 0_{4.4}^{4.3}$ $507.0^{4.3}_{4.4}$	$0 . 09013_{6.4 e - 06}^{6.9 e - 06}$ $0.09013^{6.9e-06}_{6.4e-06}$	$92 . 3_{1.8}^{1.9}$ $92.3^{1.9}_{1.8}$
H₂ 1–0 Q(3)	2.4235	$111 . 0_{0.73}^{0.71}$ $111.0^{0.71}_{0.73}$	$623 . 0_{2.9}^{2.9}$ $623.0^{2.9}_{2.9}$	$0 . 09022_{3.2 e - 06}^{3 e - 06}$ $0.09022^{3e-06}_{3.2e-06}$	$118 . 0_{0.87}^{0.81}$ $118.0^{0.81}_{0.87}$
H₂ 1–0 Q(4)	2.4374	$29 . 9_{0.52}^{0.54}$ $29.9^{0.54}_{0.52}$	$729 . 0_{11.0}^{11.0}$ $729.0^{11.0}_{11.0}$	$0 . 09067_{1.6 e - 05}^{1.7 e - 05}$ $0.09067^{1.7e-05}_{1.6e-05}$	$241 . 0_{4.4}^{4.6}$ $241.0^{4.6}_{4.4}$
H₂ 1–0 Q(5)	2.4547	$71 . 3_{0.38}^{0.38}$ $71.3^{0.38}_{0.38}$	$620 . 0_{3.3}^{3.3}$ $620.0^{3.3}_{3.3}$	$0 . 09025_{4.4 e - 06}^{4.5 e - 06}$ $0.09025^{4.5e-06}_{4.4e-06}$	$128 . 0_{1.2}^{1.2}$ $128.0^{1.2}_{1.2}$
H₂ 1–0 Q(6)	2.4754	$16 . 1_{0.3}^{0.3}$ $16.1^{0.3}_{0.3}$	$488 . 0_{9.0}^{9.0}$ $488.0^{9.0}_{9.0}$	$0 . 08996_{1.5 e - 05}^{1.4 e - 05}$ $0.08996^{1.4e-05}_{1.5e-05}$	$47 . 0_{4.1}^{3.9}$ $47.0^{3.9}_{4.1}$
H₂ 1–0 Q(7)	2.5	$50 . 3_{0.61}^{0.7}$ $50.3^{0.7}_{0.61}$	$758 . 0_{12.0}^{12.0}$ $758.0^{12.0}_{12.0}$	$0 . 09018_{1.1 e - 05}^{1.1 e - 05}$ $0.09018^{1.1e-05}_{1.1e-05}$	$107 . 0_{3.0}^{3.1}$ $107.0^{3.1}_{3.0}$
H₂ 1–0 O(2)	2.6268	$28 . 0_{0.36}^{0.37}$ $28.0^{0.37}_{0.36}$	$544 . 0_{7.4}^{7.7}$ $544.0^{7.7}_{7.4}$	$0 . 09001_{1 e - 05}^{1.1 e - 05}$ $0.09001^{1.1e-05}_{1e-05}$	$60 . 9_{2.9}^{3.0}$ $60.9^{3.0}_{2.9}$
H₂ 1–0 O(3)	2.8024	$93 . 5_{0.42}^{0.4}$ $93.5^{0.4}_{0.42}$	$655 . 0_{2.9}^{3.2}$ $655.0^{3.2}_{2.9}$	$0 . 0902_{3.9 e - 06}^{3.7 e - 06}$ $0.0902^{3.7e-06}_{3.9e-06}$	$113 . 0_{1.1}^{1.0}$ $113.0^{1.0}_{1.1}$
H₂ 0–0 S(6)	6.1086	$86 . 4_{1.1}^{1.2}$ $86.4^{1.2}_{1.1}$	$485 . 0_{6.7}^{6.9}$ $485.0^{6.9}_{6.7}$	$0 . 09003_{1.1 e - 05}^{1 e - 05}$ $0.09003^{1e-05}_{1.1e-05}$	$65 . 6_{2.9}^{2.8}$ $65.6^{2.8}_{2.9}$
H₂ 0–0 S(5)	6.9089	$453 . 0_{1.5}^{1.4}$ $453.0^{1.4}_{1.5}$	$560 . 0_{1.9}^{2.0}$ $560.0^{2.0}_{1.9}$	$0 . 09_{2.4 e - 06}^{2.5 e - 06}$ $0.09^{2.5e-06}_{2.4e-06}$	$58 . 4_{0.65}^{0.69}$ $58.4^{0.69}_{0.65}$
[ArII]	6.98337	$97 . 4_{1.6}^{1.6}$ $97.4^{1.6}_{1.6}$	$616 . 0_{9.5}^{9.6}$ $616.0^{9.6}_{9.5}$	$0 . 08995_{1.1 e - 05}^{1.2 e - 05}$ $0.08995^{1.2e-05}_{1.1e-05}$	$44 . 3_{3.1}^{3.4}$ $44.3^{3.4}_{3.1}$
H₂ 0–0 S(3)	9.6645	$867 . 0_{0.76}^{0.78}$ $867.0^{0.78}_{0.76}$	$589 . 0_{0.53}^{0.57}$ $589.0^{0.57}_{0.53}$	$0 . 09021_{7.6 e - 07}^{7.7 e - 07}$ $0.09021^{7.7e-07}_{7.6e-07}$	$114 . 0_{0.21}^{0.21}$ $114.0^{0.21}_{0.21}$
[NeIII]	15.5509	$80 . 7_{0.47}^{0.44}$ $80.7^{0.44}_{0.47}$	$608 . 0_{3.7}^{3.8}$ $608.0^{3.8}_{3.7}$	$0 . 09012_{5.1 e - 06}^{5.1 e - 06}$ $0.09012^{5.1e-06}_{5.1e-06}$	$92 . 1_{1.4}^{1.4}$ $92.1^{1.4}_{1.4}$

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