Cyanoacetylene in the outflow/hot molecular core G331.512−0.103

Author:

Duronea N U1,Bronfman L2,Mendoza E3,Merello M3ORCID,Finger R2,Reyes N24,Hervías-Caimapo C5,Faure A6,Cappa C E7,Arnal E M7,Lépine J R D3,Kleiner I8,Nyman L-Å9

Affiliation:

1. Instituto Argentino de Radioastronomía, CONICET, CCT-La Plata, C.C.5., 1894, Villa Elisa, and CIC, Prov. de Bs. As. Argentina

2. Departamento de Astronomía, Universidad de Chile, Casilla 36, Santiago de Chile

3. Instituto de Astronomia, Geofísica e Ciências Atmosféricas, Universidad de São Pãulo, São Pãulo SP-05508-090, Brazil

4. Departamento de Ingeniería Eléctrica, Universidad de Chile, Santiago de Chile

5. Department of Physics, Florida State University, Tallahassee, FL 32306, USA

6. Université Grenoble Alpes, CNRS, IPAG, F-38000 Grenoble, France

7. Facultad de Ciencias Astronómicas y Geofísicas, Universidad Nacional de La Plata, Paseo del Bosque s/n, 1900 La Plata, Argentina

8. Laboratoire Interuniversitaire des Systemes Atmospheriques (LISA), CNRS, UMR 7583, Université de Paris-Est Créteil et Paris Diderot, 61, Av Général de Gaulle, F-94010 Créteil Cedex, France

9. Joint ALMA Observatory, JAO Alonso de Córdova 31070, Vitacura, Santiago de Chile, Chile

Abstract

ABSTRACT Using APEX-1 and APEX-2 observations, we have detected and studied the rotational lines of the HC3N molecule (cyanoacetylene) in the powerful outflow/hot molecular core G331.512−0.103. We identified 31 rotational lines at J levels between 24 and 39; 17 of them in the ground vibrational state v = 0 (9 lines corresponding to the main C isotopologue and 8 lines corresponding to the 13C isotopologues), and 14 in the lowest vibrationally excited state v7 = 1. Using local thermodynamic equilibrium (LTE)-based population diagrams for the beam-diluted v = 0 transitions, we determined Texc = 85 ± 4 K and N(HC3N) = (6.9 ± 0.8) × 1014 cm−2, while for the beam-diluted v7 = 1 transitions we obtained Texc = 89 ± 10 K and N(HC3N) = (2 ± 1) × 1015 cm−2. Non-LTE calculations using H2 collision rates indicate that the HC3N emission is in good agreement with LTE-based results. From the non-LTE method, we estimated Tkin ≃90 K, n(H2) ≃ 2 × 107 cm−3 for a central core of 6 arcsec in size. A vibrational temperature in the range from 130 to 145 K was also determined, values which are very likely lower limits. Our results suggest that rotational transitions are thermalized, while infrared radiative pumping processes are probably more efficient than collisions in exciting the molecule to the vibrationally excited state v7 = 1. Abundance ratios derived under LTE conditions for the 13C isotopologues suggest that the main formation pathway of HC3N is C2H2 + CN → HC3N + H.

Funder

Consejo Nacional de Investigaciones Científicas y Técnicas

Universidad Nacional de La Plata

Comisión Nacional de Investigación Científica y Tecnológica

São Paulo Research Foundation

Publisher

Oxford University Press (OUP)

Subject

Space and Planetary Science,Astronomy and Astrophysics

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