2019A&A...632A..60J


Query : 2019A&A...632A..60J

2019A&A...632A..60J - Astronomy and Astrophysics, volume 632A60-60 (2019/12-0)

Fingerprinting the effects of hyperfine structure on CH and OH far infrared spectra using Wiener filter deconvolution.

JACOB A.M., MENTEN K.M., WIESEMEYER H., LEE M.-Y., GUSTEN R. and DURAN C.A.

Abstract (from CDS):


Context. Despite being a commonly observed feature, the modification of the velocity structure in spectral line profiles by hyperfine structure complicates the interpretation of spectroscopic data. This is particularly true for observations of simple molecules such as CH and OH toward the inner Galaxy, which show a great deal of velocity crowding.
Aims. In this paper, we investigate the influence of hyperfine splitting on complex spectral lines, with the aim of evaluating canonical abundances by decomposing their dependence on hyperfine structures. This is achieved from first principles through deconvolution.
Methods. We present high spectral resolution observations of the rotational ground state transitions of CH near 2 THz seen in absorption toward the strong FIR-continuum sources AGAL010.62-00.384, AGAL034.258+00.154, AGAL327.293-00.579, AGAL330.954-00.182, AGAL332.826-00.549, AGAL351.581-00.352 and SgrB2(M). These were observed with the GREAT instrument on board SOFIA. The observed line profiles of CH were deconvolved from the imprint left by the lines' hyperfine structures using the Wiener filter deconvolution, an optimised kernel acting on direct deconvolution.
Results. The quantitative analysis of the deconvolved spectra first entails the computation of CH column densities. Reliable N(CH) values are of importance owing to the status of CH as a powerful tracer for H2 in the diffuse regions of the interstellar medium. The N(OH)/N(CH) column density ratio is found to vary within an order of magnitude with values ranging from one to 10, for the individual sources that are located outside the Galactic centre. Using CH as a surrogate for H2, we determined the abundance of the OH molecule to be X(OH)=1.09x10–7 with respect to H2. The radial distribution of CH column densities along the sightlines probed in this study, excluding SgrB2(M), showcase a dual peaked distribution peaking between 5 and 7kpc. The similarity between the correspondingly derived column density profile of H2 with that of the CO-dark H2 gas traced by the cold neutral medium component of [CII] 158 µm emission across the Galactic plane, further emphasises the use of CH as a tracer for H2.

Abstract Copyright: © A. M. Jacob et al. 2019

Journal keyword(s): ISM: abundances - ISM: clouds - ISM: lines and bands - ISM: molecules - methods: data analysis

VizieR on-line data: <Available at CDS (J/A+A/632/A60): list.dat fits/*>

Simbad objects: 16

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Number of rows : 16
N Identifier Otype ICRS (J2000)
RA
ICRS (J2000)
DEC
Mag U Mag B Mag V Mag R Mag I Sp type #ref
1850 - 2026
#notes
1 NAME Per Arm PoG 03 30 +45.0           ~ 1672 0
2 NAME Crux-Scutum Spiral Arm reg 12 30 -60.0           ~ 323 0
3 OH 327.3-00.6 Mas 15 53 07.65 -54 37 06.1           ~ 35 1
4 AGAL G327.293-00.579 smm 15 53 09 -54 37.1           ~ 33 0
5 NAME Nor Arm PoG 16 00 -50.0           ~ 485 0
6 MMB G330.953-00.182 cor 16 09 52.37 -51 54 57.6           ~ 40 0
7 AGAL G332.826-00.549 cor 16 20 11 -50 53.2           ~ 28 0
8 MMB G351.581-00.353 cor 17 25 25.220 -36 12 45.34           ~ 44 0
9 NAME Galactic Center reg 17 45 39.60213 -29 00 22.0000           ~ 16269 0
10 NAME Sgr B2 MoC 17 47 20.4 -28 23 07           ~ 2443 1
11 NAME Sgr B2 Main Rad 17 47 20.5 -28 23 06           ~ 436 1
12 CORNISH G010.6234-00.3837 HII 18 10 28.70 -19 55 49.1           ~ 10 0
13 [CUS2014] G034.2572+0.1535 cor 18 53 18.6449 +01 15 01.574           ~ 43 0
14 NAME Sgr Arm PoG 19 00 -30.0           ~ 710 1
15 W 49n HII 19 10 13.2 +09 06 12           ~ 497 3
16 NAME Scutum Spiral Arm PoG ~ ~           ~ 393 0

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