Abstract:Complex organic molecules (COMs) have been detected in a variety of interstellar sources. The abundances of these COMs in warming sources can be explained by syntheses linked to increasing temperatures and densities, allowing quasi-thermal chemical reactions to occur rapidly enough to produce observable amounts of COMs, both in the gas phase, and upon dust grain ice mantles. The COMs produced on grains then become gaseous as the temperature increases sufficiently to allow their thermal desorption. The recent o… Show more
“…Perhaps even more striking are the observations of COMs in the cold, dark starless core TMC-1 (see, e.g., Agúndez et al 2021), where the kinetic temperatures are well known to be substantially below the thermal desorption threshold. A number of physical and physiochemical processes have been theorized to account for the non-thermal desorption of COMs from grain surfaces (Paulive et al 2021), as well as substantial quantum chemical efforts suggesting potential new pathways for gas-phase formation (Balucani et al 2018). A generalized picture of these processes, and under what conditions they dominate, remains absent.…”
The first set of theoretical cross sections for propylene oxide (CH 3 CHCH 2 O) colliding with cold He atoms has been obtained at the full quantum level using a high-accuracy potential energy surface. By scaling the collision reduced mass, rotational rate coefficients for collisions with para-H 2 are deduced in the temperature range 5−30 K. These collisional coefficients are combined with radiative data in a non-LTE radiative transfer model in order to reproduce observations of propylene oxide made towards the Sagittarius B2(N) molecular cloud with the Green Bank and Parkes radio telescopes. The three detected absorption lines are found to probe the cold (∼ 10 K) and translucent (n H ∼ 2000 cm −3 ) gas in the outer edges of the extended Sgr B2(N) envelope. The derived column density for propylene oxide is N tot ∼ 3 × 10 12 cm −2 , corresponding to a fractional abundance relative to total hydrogen of ∼ 2.5 × 10 −11 . The present results are expected to help our understanding of the chemistry of propylene oxide, including a potential enantiomeric excess, in the cold interstellar medium.
“…Perhaps even more striking are the observations of COMs in the cold, dark starless core TMC-1 (see, e.g., Agúndez et al 2021), where the kinetic temperatures are well known to be substantially below the thermal desorption threshold. A number of physical and physiochemical processes have been theorized to account for the non-thermal desorption of COMs from grain surfaces (Paulive et al 2021), as well as substantial quantum chemical efforts suggesting potential new pathways for gas-phase formation (Balucani et al 2018). A generalized picture of these processes, and under what conditions they dominate, remains absent.…”
The first set of theoretical cross sections for propylene oxide (CH 3 CHCH 2 O) colliding with cold He atoms has been obtained at the full quantum level using a high-accuracy potential energy surface. By scaling the collision reduced mass, rotational rate coefficients for collisions with para-H 2 are deduced in the temperature range 5−30 K. These collisional coefficients are combined with radiative data in a non-LTE radiative transfer model in order to reproduce observations of propylene oxide made towards the Sagittarius B2(N) molecular cloud with the Green Bank and Parkes radio telescopes. The three detected absorption lines are found to probe the cold (∼ 10 K) and translucent (n H ∼ 2000 cm −3 ) gas in the outer edges of the extended Sgr B2(N) envelope. The derived column density for propylene oxide is N tot ∼ 3 × 10 12 cm −2 , corresponding to a fractional abundance relative to total hydrogen of ∼ 2.5 × 10 −11 . The present results are expected to help our understanding of the chemistry of propylene oxide, including a potential enantiomeric excess, in the cold interstellar medium.
“…The chemistry of acetic acid, methyl formate and glycolaldehyde has been extensively discussed in several works (see e.g. Laas et al 2011;Burke et al 2015;Skouteris et al 2018;El-Abd et al 2019;Ahmad et al 2020;Mininni et al 2020;Paulive et al 2021).…”
We present the first detection of (Z)-1,2-ethenediol, (CHOH) 2 , the enol form of glycolaldehyde, in the interstellar medium towards the G+0.693-0.027 molecular cloud located in the Galactic Center. We have derived a column density of (1.8±0.1)×10 13 cm −2 , which translates into a molecular abundance with respect to molecular hydrogen of 1.3×10 −10 . The abundance ratio between glycolaldehyde and (Z)-1,2-ethenediol is ∼5.2. We discuss several viable formation routes through chemical reactions from precursors such as HCO, H 2 CO, HCOH or CH 2 CHOH. We also propose that this species might be an important precursor in the formation of glyceraldehyde (HOCH 2 CHOHCHO) in the interstellar medium through combination with the hydroxymethylene (CHOH) radical.
“…Moreover, observations of COMs in the absence of protostars in cold (T 20 K) regions, for example, the dark cloud TMC-1 (e.g., Agúndez et al 2021, and references therein) or prestellar cores (Bacmann et al 2012;Jiménez-Serra et al 2016, 2021Scibelli & Shirley 2020) but also in protostellar outflows such as L1157 (Codella et al 2015(Codella et al , 2017 and, for example, the shocked region (while quiescent in star formation) G+0.693−0.027 located in the Galactic centre region (e.g., Requena-Torres et al 2006;Zeng et al 2018), point to additional or purely non-thermal desorption processes. These processes may include grain-sputtering and subsequent release of COMs into the gas phase due to shock passing induced by outflows, accretion shocks (e.g., Csengeri et al 2019), or cloud interactions, desorption after interaction of molecules on dust grain surfaces with cosmic rays (Shingledecker et al 2018;Paulive et al 2021), or other diffusive and non-diffusive reactions taking place on the dust surface that lead to the chemical desorption of COMs (e.g, Ruaud et al 2015;Jin & Garrod 2020).…”
Section: Introductionmentioning
confidence: 99%
“…These processes may include grain-sputtering and subsequent release of COMs into the gas phase due to shock passing induced by outflows, accretion shocks (e.g. Csengeri et al 2019), or cloud interactions, desorption after interaction of molecules on dust grain surfaces with cosmic rays (Shingledecker et al 2018;Paulive et al 2021), or other diffusive and non-diffusive reactions taking place on the dust surface that lead to the chemical desorption of COMs (e.g, Ruaud et al 2015;Jin & Garrod 2020).…”