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DETECTION OF HF TOWARD PKS 1830–211, SEARCH FOR INTERSTELLAR H{sub 2}F{sup +}, AND LABORATORY STUDY OF H{sub 2}F{sup +} AND H{sub 2}Cl{sup +} DISSOCIATIVE RECOMBINATION

We report extragalactic observations of two fluorine-bearing species, hydrogen fluoride (HF) and fluoronium (H{sub 2}F{sup +}), in the z = 0.89 absorber in front of the lensed blazar PKS 1830−211 with the Atacama Large Millimeter/submillimeter Array. HF was detected toward both southwest and northea...

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Published in:The Astrophysical journal 2016-05, Vol.822 (2)
Main Authors: Kawaguchi, K., Okabayahsi, Y., Nagahiro, H., Miyamoto, Y., Tang, J., Muller, S., Black, J. H., Amano, T., Matsushima, F., Fujimori, R.
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creator Kawaguchi, K.
Okabayahsi, Y.
Nagahiro, H.
Miyamoto, Y.
Tang, J.
Muller, S.
Black, J. H.
Amano, T.
Matsushima, F.
Fujimori, R.
description We report extragalactic observations of two fluorine-bearing species, hydrogen fluoride (HF) and fluoronium (H{sub 2}F{sup +}), in the z = 0.89 absorber in front of the lensed blazar PKS 1830−211 with the Atacama Large Millimeter/submillimeter Array. HF was detected toward both southwest and northeast images of the blazar, with column densities >3.4 × 10{sup 14} cm{sup −2} and 0.18 × 10{sup 14} cm{sup −2}, respectively. H{sub 2}F{sup +} was not detected, down to an upper limit (3σ) of 8.8 × 10{sup 11} cm{sup −2} and an abundance ratio of [H{sub 2}F{sup +}]/[HF] ⩽ 1/386. We also searched for H{sub 2}F{sup +} toward the Galactic sources NGC 6334 I and W51C, and toward Galactic center clouds with the Herschel HIFI spectrometer.{sup 6} The upper limit on the column density was derived to be 2.5 × 10{sup 11} cm{sup −2} in NGC 6334 I, which is 1/68 of that for H{sub 2}Cl{sup +}. In constrast, the ortho transition of H{sub 2}Cl{sup +} is detected toward PKS 1830–211. To understand the small abundance of interstellar H{sub 2}F{sup +}, we carried out laboratory experiments to determine the rate constants for the ion–electron recombination reaction by infrared time-resolved spectroscopy. The constants determined are k {sub e}(209 K) = (1.1±0.3)×10{sup −7} cm{sup 3} s{sup −1} and (0.46±0.05)×10{sup −7} cm{sup 3} s{sup −1} for H{sub 2}F{sup +} and H{sub 2}Cl{sup +}, respectively. The difference in the dissociative recombination rates between H{sub 2}F{sup +} and H{sub 2}Cl{sup +} by a factor ∼2 and the cosmic abundance ratio [F]/[Cl] ≈ 1/6 are not enough to explain the much smaller abundance of H{sub 2}F{sup +}. The difference in the formation mechanism of H{sub 2}F{sup +} and H{sub 2}Cl{sup +} in interstellar space would be a major factor in the small abundance of H{sub 2}F{sup +}.
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We also searched for H{sub 2}F{sup +} toward the Galactic sources NGC 6334 I and W51C, and toward Galactic center clouds with the Herschel HIFI spectrometer.{sup 6} The upper limit on the column density was derived to be 2.5 × 10{sup 11} cm{sup −2} in NGC 6334 I, which is 1/68 of that for H{sub 2}Cl{sup +}. In constrast, the ortho transition of H{sub 2}Cl{sup +} is detected toward PKS 1830–211. To understand the small abundance of interstellar H{sub 2}F{sup +}, we carried out laboratory experiments to determine the rate constants for the ion–electron recombination reaction by infrared time-resolved spectroscopy. The constants determined are k {sub e}(209 K) = (1.1±0.3)×10{sup −7} cm{sup 3} s{sup −1} and (0.46±0.05)×10{sup −7} cm{sup 3} s{sup −1} for H{sub 2}F{sup +} and H{sub 2}Cl{sup +}, respectively. 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The difference in the dissociative recombination rates between H{sub 2}F{sup +} and H{sub 2}Cl{sup +} by a factor ∼2 and the cosmic abundance ratio [F]/[Cl] ≈ 1/6 are not enough to explain the much smaller abundance of H{sub 2}F{sup +}. 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H{sub 2}F{sup +} was not detected, down to an upper limit (3σ) of 8.8 × 10{sup 11} cm{sup −2} and an abundance ratio of [H{sub 2}F{sup +}]/[HF] ⩽ 1/386. We also searched for H{sub 2}F{sup +} toward the Galactic sources NGC 6334 I and W51C, and toward Galactic center clouds with the Herschel HIFI spectrometer.{sup 6} The upper limit on the column density was derived to be 2.5 × 10{sup 11} cm{sup −2} in NGC 6334 I, which is 1/68 of that for H{sub 2}Cl{sup +}. In constrast, the ortho transition of H{sub 2}Cl{sup +} is detected toward PKS 1830–211. To understand the small abundance of interstellar H{sub 2}F{sup +}, we carried out laboratory experiments to determine the rate constants for the ion–electron recombination reaction by infrared time-resolved spectroscopy. The constants determined are k {sub e}(209 K) = (1.1±0.3)×10{sup −7} cm{sup 3} s{sup −1} and (0.46±0.05)×10{sup −7} cm{sup 3} s{sup −1} for H{sub 2}F{sup +} and H{sub 2}Cl{sup +}, respectively. The difference in the dissociative recombination rates between H{sub 2}F{sup +} and H{sub 2}Cl{sup +} by a factor ∼2 and the cosmic abundance ratio [F]/[Cl] ≈ 1/6 are not enough to explain the much smaller abundance of H{sub 2}F{sup +}. The difference in the formation mechanism of H{sub 2}F{sup +} and H{sub 2}Cl{sup +} in interstellar space would be a major factor in the small abundance of H{sub 2}F{sup +}.</abstract><cop>United States</cop></addata></record>
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subjects ABUNDANCE
ASTROPHYSICS, COSMOLOGY AND ASTRONOMY
BEARINGS
DENSITY
DETECTION
GALAXIES
HYDROFLUORIC ACID
HYDROGEN FLUORIDES
INTERSTELLAR SPACE
MOLECULAR IONS
RECOMBINATION
SPECTROMETERS
SPECTROSCOPY
TIME RESOLUTION
title DETECTION OF HF TOWARD PKS 1830–211, SEARCH FOR INTERSTELLAR H{sub 2}F{sup +}, AND LABORATORY STUDY OF H{sub 2}F{sup +} AND H{sub 2}Cl{sup +} DISSOCIATIVE RECOMBINATION
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