Abstract:Recent radio astronomical observations have revealed that HC 5 N, the second shortest cyanopolyyne (HC 2n+1 N), is abundant around some massive young stellar objects (MYSOs), which is not predicted by classical carbon-chain chemistry. For example, the observed HC 5 N abundance toward the G28.28−0.36 MYSO is higher than that in L1527, which is one of the warm carbon chain chemistry (WCCC) sources, by more than one order of magnitude . In this paper, we present chemical simulations of hot-core models with a warm… Show more
“…Grain-surface reactions are also proposed in order to explain the observed abundances of CH 3 CCH (Hickson et al 2016;Guzmán et al 2018). Regarding massive environments, Taniguchi et al (2019) have constructed hot-core models to investigate the formation pathways of cyanopolyynes and other carbonchain species, including CH 3 CCH and c-C 3 H 2 , around MYSOs. They found chemical similarities between methyl acetylene, methane and cyanopolyynes, being all triggered by CH 4 sublimation from dust grains.…”
A spectral survey of methyl acetylene (CH 3 CCH) was conducted toward the hot molecular core/outflow G331.512-0.103. Our APEX observations allowed the detection of 41 uncontaminated rotational lines of CH 3 CCH in the frequency range between 172-356 GHz. Through an analysis under the local thermodynamic equilibrium assumption, by means of rotational diagrams, we determined.05 for an extended emitting region (∼10 ). The relative intensities of the K=2 and K=3 lines within a given K-ladder are strongly negatively correlated to the transitions' upper J quantum-number (r=-0.84). Pure rotational spectra of CH 3 CCH were simulated at different temperatures, in order to interpret this observation. The results indicate that the emission is characterized by a non-negligible temperature gradient with upper and lower limits of ∼45 and ∼60 K, respectively. Moreover, the line widths and peak velocities show an overall strong correlation with their rest frequencies, suggesting that the warmer gas is also associated with stronger turbulence effects. The K=0 transitions present a slightly different kinematic signature than the remaining lines, indicating that they might be tracing a different gas component. We speculate that this component is characterized by lower temperatures, and therefore larger sizes. Moreover, we predict and discuss the temporal evolution of the CH 3 CCH abundance using a two-stage zero-dimensional model of the source constructed with the three-phase Nautilus gas-grain code.
“…Grain-surface reactions are also proposed in order to explain the observed abundances of CH 3 CCH (Hickson et al 2016;Guzmán et al 2018). Regarding massive environments, Taniguchi et al (2019) have constructed hot-core models to investigate the formation pathways of cyanopolyynes and other carbonchain species, including CH 3 CCH and c-C 3 H 2 , around MYSOs. They found chemical similarities between methyl acetylene, methane and cyanopolyynes, being all triggered by CH 4 sublimation from dust grains.…”
A spectral survey of methyl acetylene (CH 3 CCH) was conducted toward the hot molecular core/outflow G331.512-0.103. Our APEX observations allowed the detection of 41 uncontaminated rotational lines of CH 3 CCH in the frequency range between 172-356 GHz. Through an analysis under the local thermodynamic equilibrium assumption, by means of rotational diagrams, we determined.05 for an extended emitting region (∼10 ). The relative intensities of the K=2 and K=3 lines within a given K-ladder are strongly negatively correlated to the transitions' upper J quantum-number (r=-0.84). Pure rotational spectra of CH 3 CCH were simulated at different temperatures, in order to interpret this observation. The results indicate that the emission is characterized by a non-negligible temperature gradient with upper and lower limits of ∼45 and ∼60 K, respectively. Moreover, the line widths and peak velocities show an overall strong correlation with their rest frequencies, suggesting that the warmer gas is also associated with stronger turbulence effects. The K=0 transitions present a slightly different kinematic signature than the remaining lines, indicating that they might be tracing a different gas component. We speculate that this component is characterized by lower temperatures, and therefore larger sizes. Moreover, we predict and discuss the temporal evolution of the CH 3 CCH abundance using a two-stage zero-dimensional model of the source constructed with the three-phase Nautilus gas-grain code.
“…The HC 3 N/CH 3 OH ratios in the n3 field have larger values than those in the n5 field systematically. The HC 3 N abundance is likely less sensitive to protostellar evolution compared to CH 3 OH, because HC 3 N is continually formed from CH 4 and/or C 2 H 2 , which are sublimated from dust grains, in warm or hot regions (25 K < T < 100 K) (e.g., Taniguchi et al 2019a). Thus, these results imply that CH 3 OH is efficiently sublimated from dust grains in the n5 field.…”
Section: Comparison Of Chemical Composition Between Ngc 2264-d and Ng...mentioning
confidence: 99%
“…1). The n3 position is located at the northern edge of NGC 2264-D and the integrated intensity ratio of HC 3 N and CH 3 OH, I(HC 3 N)/I(CH 3 OH), at this position shows the highest value among the other positions in NGC 2264-C and NGC 2264-D. A variety in the I(HC 3 N)/I(CH 3 OH) ratio implies a chemical differentiation in the clusterforming region, suggestive of different evolutionary histories and/or different environments (Spezzano et al 2016;Taniguchi et al 2019a;Spezzano et al 2020). The n3 position is located to the west of the IRS2 source (IRAS 06382+0939).…”
We have conducted mapping observations toward the n3 and n5 positions in the NGC 2264-D cluster-forming region with the Atacama Compact Array (ACA) of the Atacama Large Millimeter/submillimeter Array (ALMA) in Band 3. Observations with 10000 au scale beam reveal the chemical composition at the clump scale. The spatial distributions of the observed low upper-state-energy lines of CH 3 OH are similar to those of CS and SO, and the HC 3 N emission seems to be predominantly associated with clumps containing young stellar objects. The turbulent gas induced by the star formation activities produces large-scale shock regions in NGC 2264-D, which are traced by the CH 3 OH, CS and SO emissions. We derive the HC 3 N, CH 3 CN, and CH 3 CHO abundances with respect to CH 3 OH. Compared to the n5 field, the n3 field is farther (in projected apparent distance) from the neighboring NGC 2264-C, yet the chemical composition in the n3 field tends to be similar to that of the protostellar candidate CMM3 in NGC 2264-C. The HC 3 N/CH 3 OH ratios in the n3 field are higher than those in the n5 field. We find an anti-correlation between the HC 3 N/CH 3 OH ratio and their excitation temperatures. The low HC 3 N/CH 3 OH abundance ratio at the n5 field implies that the n5 field is an environment with more active star formation compared with the n3 field.
“…Recent observations have shown chemical differentiation not only around low-mass YSOs, but around high-mass YSOs as well (Taniguchi et al 2018(Taniguchi et al , 2019b(Taniguchi et al , 2021a. Although the origin of the chemical differentiation around YSOs is still controversial, three possible factors have been proposed: the different timescale of the prestellar collapse (Sakai et al 2008), the different ultraviolet (UV) radiation field (Spezzano et al 2016), and the different timescale of the warm-up stage (Taniguchi et al 2019a). In order to reveal the effects of the above factors, we need to investigate molecular spatial distributions on large scales (e.g., the clump scale).…”
We have analyzed Atacama Large Millimeter/submillimeter Array (ALMA) Cycle 4 Band 6 data toward two young stellar objects (YSOs), Oph-emb5 and Oph-emb9, in the Ophiuchus star-forming region. The YSO Oph-emb5 is located in a relatively quiescent region, whereas Oph-emb9 is irradiated by a nearby bright Herbig Be star. Molecular lines from cyclic-C 3 H 2 (c-C 3 H 2 ), H 2 CO, CH 3 OH, 13 CO, C 18 O, and DCO + have been detected from both sources, while DCN is detected only in Oph-emb9. Around Oph-emb5, c-C 3 H 2 is enhanced at the west side, relative to the IR source, whereas H 2 CO and CH 3 OH are abundant at the east side. In the field of Oph-emb9, moment 0 maps of the c-C 3 H 2 lines show a peak at the eastern edge of the field of view, which is irradiated by the Herbig Be star. Moment 0 maps of CH 3 OH and H 2 CO show peaks farther from the bright star. We derive the N (c-C 3 H 2 )/N (CH 3 OH) column density ratios at the peak positions of c-C 3 H 2 and CH 3 OH near each YSO, which are identified based on their moment 0 maps. The N (c-C 3 H 2 )/N (CH 3 OH) ratio at the c-C 3 H 2 peak is significantly higher than at the CH 3 OH peak by a factor of ∼ 19 in Oph-emb9, while the difference in this column density ratio between these two positions is a factor of ∼ 2.6 in Oph-emb5. These differences are attributed to the efficiency of the photon-dominated region (PDR) chemistry in Oph-emb9. The higher DCO + column density and the detection of DCN in Oph-emb9 are also discussed in the context of UV irradiation flux.
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