PDRs4All

IF 5.4 2区 物理与天体物理 Q1 ASTRONOMY & ASTROPHYSICS
M. Zannese, B. Tabone, E. Habart, E. Dartois, J. R. Goicoechea, L. Coudert, B. Gans, M.-A. Martin-Drumel, U. Jacovella, A. Faure, B. Godard, A. G. G. M. Tielens, R. Le Gal, J. H. Black, S. Vicente, O. Berné, E. Peeters, D. Van De Putte, R. Chown, A. Sidhu, I. Schroetter, A. Canin, O. Kannavou
{"title":"PDRs4All","authors":"M. Zannese, B. Tabone, E. Habart, E. Dartois, J. R. Goicoechea, L. Coudert, B. Gans, M.-A. Martin-Drumel, U. Jacovella, A. Faure, B. Godard, A. G. G. M. Tielens, R. Le Gal, J. H. Black, S. Vicente, O. Berné, E. Peeters, D. Van De Putte, R. Chown, A. Sidhu, I. Schroetter, A. Canin, O. Kannavou","doi":"10.1051/0004-6361/202453441","DOIUrl":null,"url":null,"abstract":"<i>Context<i/>. The methylidyne cation (CH<sup>+<sup/>) and the methyl cation (CH<sub>3<sub/><sup>+<sup/>) are building blocks of organic molecules in the ultraviolet (UV) irradiated gas, yet their coupled formation and excitation mechanisms mostly remain unprobed. The James Webb Space Telescope (JWST), with its high spatial resolution and good spectral resolution, provides unique access to the detection of these molecules.<i>Aims<i/>. Our goal is to use the first detection of CH<sup>+<sup/> and CH<sub>3<sub/><sup>+<sup/> infrared rovibrational emission in the Orion Bar and in the protoplanetary disk d203-506 to probe their formation and excitation mechanisms and constrain the physico-chemical conditions of the environment.<i>Methods<i/>. We used spectro-imaging acquired using both the NIRSpec and MIRI-MRS instruments on board JWST to study the infrared CH<sup>+<sup/> and CH<sub>3<sub/><sup>+<sup/> spatial distribution at very small scales (down to 0.1′′) and compared it to excited H<sub>2<sub/> emission. We studied their excitation in detail, and in the case of CH<sup>+<sup/>, we compared the observed line intensities with chemical formation pumping models based on recent quantum dynamical calculations. Throughout this study, we compare the emission of these molecules in two environments: the Bar a photodissociation region – and a protoplanetary disk (d203-506), both of which are irradiated by the Trapezium cluster.<i>Results<i/>. We detected CH<sup>+<sup/> and CH<sub>3<sub/><sup>+<sup/> vibrationally excited emission both in the Bar and d203-506. These emissions originate from the same region as highly excited H<sub>2<sub/> (high rotational and rovibrational levels) and correlate less with the lower rotational levels of H<sub>2<sub/> (<i>J<i/>′ < 5) or the emission of aromatic and aliphatic infrared bands. Our comparison between the Bar and d203-506 revealed that both CH<sup>+<sup/> and CH<sub>3<sub/><sup>+<sup/> excitation and/or formation are highly dependent on gas density. The excitation temperature of the observed CH<sup>+<sup/> and CH<sub>3<sub/><sup>+<sup/> rovibrational lines is around <i>T<i/> ∼ 1500 K in the Bar and <i>T<i/> ∼ 800 K in d203-506. Moreover, the column densities derived from the rovibrational emission are less than 0.1% of the total known (CH<sup>+<sup/>) and expected (CH<sub>3<sub/><sup>+<sup/>) column densities. These different results show that CH<sup>+<sup/> and CH<sub>3<sub/><sup>+<sup/> level populations strongly deviate from local thermodynamical equilibrium. The CH<sup>+<sup/> rovibrational supra-thermal emission (<i>v<i/> = 1 and <i>v<i/> = 2) can be explained by chemical formation pumping with excited H<sub>2<sub/> via C<sup>+<sup/> + H<sub>2<sub/><sup>*<sup/> = CH<sup>+<sup/> + H. The difference in the population distribution of the H<sub>2<sub/><sup>*<sup/> energy levels between the Orion Bar and d203-506 then result in different excitation temperatures. These results support a gas phase formation pathway of CH<sup>+<sup/> and CH<sub>3<sub/><sup>+<sup/> via successive hydrogen abstraction reactions. However, we do not find any evidence of CH<sub>3<sub/><sup>+<sup/> emission in the JWST spectrum, which may be explained by the fact its spectroscopic signatures could be spread in the JWST spectra. Finally, the observed CH<sup>+<sup/> intensities coupled with a chemical formation pumping model provide a diagnostic tool to trace the local density.<i>Conclusions<i/>. Line emission from vibrationally excited CH<sup>+<sup/> and CH<sub>3<sub/><sup>+<sup/> provides new insight into the first steps of hydrocarbon gas-phase chemistry in action. This study highlights the need for extended molecular data of detectable molecules in the interstellar medium in order to analyze the JWST observations.","PeriodicalId":8571,"journal":{"name":"Astronomy & Astrophysics","volume":"42 12 1","pages":""},"PeriodicalIF":5.4000,"publicationDate":"2025-04-08","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"PDRs4All\",\"authors\":\"M. Zannese, B. Tabone, E. Habart, E. Dartois, J. R. Goicoechea, L. Coudert, B. Gans, M.-A. Martin-Drumel, U. Jacovella, A. Faure, B. Godard, A. G. G. M. Tielens, R. Le Gal, J. H. Black, S. Vicente, O. Berné, E. Peeters, D. Van De Putte, R. Chown, A. Sidhu, I. Schroetter, A. Canin, O. Kannavou\",\"doi\":\"10.1051/0004-6361/202453441\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"<i>Context<i/>. The methylidyne cation (CH<sup>+<sup/>) and the methyl cation (CH<sub>3<sub/><sup>+<sup/>) are building blocks of organic molecules in the ultraviolet (UV) irradiated gas, yet their coupled formation and excitation mechanisms mostly remain unprobed. The James Webb Space Telescope (JWST), with its high spatial resolution and good spectral resolution, provides unique access to the detection of these molecules.<i>Aims<i/>. Our goal is to use the first detection of CH<sup>+<sup/> and CH<sub>3<sub/><sup>+<sup/> infrared rovibrational emission in the Orion Bar and in the protoplanetary disk d203-506 to probe their formation and excitation mechanisms and constrain the physico-chemical conditions of the environment.<i>Methods<i/>. We used spectro-imaging acquired using both the NIRSpec and MIRI-MRS instruments on board JWST to study the infrared CH<sup>+<sup/> and CH<sub>3<sub/><sup>+<sup/> spatial distribution at very small scales (down to 0.1′′) and compared it to excited H<sub>2<sub/> emission. We studied their excitation in detail, and in the case of CH<sup>+<sup/>, we compared the observed line intensities with chemical formation pumping models based on recent quantum dynamical calculations. Throughout this study, we compare the emission of these molecules in two environments: the Bar a photodissociation region – and a protoplanetary disk (d203-506), both of which are irradiated by the Trapezium cluster.<i>Results<i/>. We detected CH<sup>+<sup/> and CH<sub>3<sub/><sup>+<sup/> vibrationally excited emission both in the Bar and d203-506. These emissions originate from the same region as highly excited H<sub>2<sub/> (high rotational and rovibrational levels) and correlate less with the lower rotational levels of H<sub>2<sub/> (<i>J<i/>′ < 5) or the emission of aromatic and aliphatic infrared bands. Our comparison between the Bar and d203-506 revealed that both CH<sup>+<sup/> and CH<sub>3<sub/><sup>+<sup/> excitation and/or formation are highly dependent on gas density. The excitation temperature of the observed CH<sup>+<sup/> and CH<sub>3<sub/><sup>+<sup/> rovibrational lines is around <i>T<i/> ∼ 1500 K in the Bar and <i>T<i/> ∼ 800 K in d203-506. Moreover, the column densities derived from the rovibrational emission are less than 0.1% of the total known (CH<sup>+<sup/>) and expected (CH<sub>3<sub/><sup>+<sup/>) column densities. These different results show that CH<sup>+<sup/> and CH<sub>3<sub/><sup>+<sup/> level populations strongly deviate from local thermodynamical equilibrium. The CH<sup>+<sup/> rovibrational supra-thermal emission (<i>v<i/> = 1 and <i>v<i/> = 2) can be explained by chemical formation pumping with excited H<sub>2<sub/> via C<sup>+<sup/> + H<sub>2<sub/><sup>*<sup/> = CH<sup>+<sup/> + H. The difference in the population distribution of the H<sub>2<sub/><sup>*<sup/> energy levels between the Orion Bar and d203-506 then result in different excitation temperatures. These results support a gas phase formation pathway of CH<sup>+<sup/> and CH<sub>3<sub/><sup>+<sup/> via successive hydrogen abstraction reactions. However, we do not find any evidence of CH<sub>3<sub/><sup>+<sup/> emission in the JWST spectrum, which may be explained by the fact its spectroscopic signatures could be spread in the JWST spectra. Finally, the observed CH<sup>+<sup/> intensities coupled with a chemical formation pumping model provide a diagnostic tool to trace the local density.<i>Conclusions<i/>. Line emission from vibrationally excited CH<sup>+<sup/> and CH<sub>3<sub/><sup>+<sup/> provides new insight into the first steps of hydrocarbon gas-phase chemistry in action. 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引用次数: 0

摘要

上下文。甲基阳离子(CH3+)和甲基阳离子(CH3+)是紫外线(UV)照射气体中有机分子的组成部分,但它们的耦合形成和激发机制大多尚未被探索。詹姆斯·韦伯太空望远镜(JWST)以其高空间分辨率和良好的光谱分辨率,为探测这些分子提供了独特的途径。我们的目标是利用首次探测到猎户座酒吧和原行星盘d203-506中CH+和CH3+的红外旋转振动发射,探索它们的形成和激发机制,并约束环境的物理化学条件。我们使用JWST上的NIRSpec和MIRI-MRS仪器获得的光谱成像,研究了非常小尺度(小至0.1”)的红外CH+和CH3+的空间分布,并将其与激发H2发射进行了比较。我们详细研究了它们的激发,并在CH+的情况下,我们将观测到的线强度与基于最近量子动力学计算的化学形成泵浦模型进行了比较。在整个研究中,我们比较了这些分子在两种环境中的发射:Bar光解区和原行星盘(d203-506),两者都受到四边形星团的辐射。我们在Bar和d203-506中都检测到CH+和CH3+的振动激发辐射。这些辐射与高激发的H2(高旋转和旋转振动能级)来自同一区域,与H2的低旋转能级(J′< 5)或芳族和脂肪族红外波段的发射相关性较小。我们对Bar和d203-506的比较表明,CH+和CH3+的激发和/或形成都高度依赖于气体密度。观测到的CH+和CH3+振动谱线的激发温度在Bar中约为T ~ 1500 K,在d203-506中约为T ~ 800 K。此外,由旋转振动发射得到的柱密度小于总已知(CH3+)和预期(CH3+)柱密度的0.1%。这些不同的结果表明,CH+和CH3+水平居群严重偏离了局部热力学平衡。CH+的振动超热发射(v = 1和v = 2)可以用C+ + H2* = CH+ + h激发H2的化学形成泵送来解释。因此,猎户座与d203-506之间H2*能级的居群分布差异导致了激发温度的不同。这些结果支持了连续抽氢反应形成CH+和CH3+气相的途径。然而,我们没有在JWST的光谱中发现任何CH3+发射的证据,这可能是因为它的光谱特征可以在JWST的光谱中扩散。最后,观察到的CH+强度与化学地层泵送模型相结合,为追踪局部密度提供了一种诊断工具。振动激发的CH+和CH3+的谱线发射提供了对作用中的烃类气相化学的第一步的新认识。这项研究强调了对星际介质中可探测分子的扩展分子数据的需要,以便分析JWST的观测结果。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
PDRs4All
Context. The methylidyne cation (CH+) and the methyl cation (CH3+) are building blocks of organic molecules in the ultraviolet (UV) irradiated gas, yet their coupled formation and excitation mechanisms mostly remain unprobed. The James Webb Space Telescope (JWST), with its high spatial resolution and good spectral resolution, provides unique access to the detection of these molecules.Aims. Our goal is to use the first detection of CH+ and CH3+ infrared rovibrational emission in the Orion Bar and in the protoplanetary disk d203-506 to probe their formation and excitation mechanisms and constrain the physico-chemical conditions of the environment.Methods. We used spectro-imaging acquired using both the NIRSpec and MIRI-MRS instruments on board JWST to study the infrared CH+ and CH3+ spatial distribution at very small scales (down to 0.1′′) and compared it to excited H2 emission. We studied their excitation in detail, and in the case of CH+, we compared the observed line intensities with chemical formation pumping models based on recent quantum dynamical calculations. Throughout this study, we compare the emission of these molecules in two environments: the Bar a photodissociation region – and a protoplanetary disk (d203-506), both of which are irradiated by the Trapezium cluster.Results. We detected CH+ and CH3+ vibrationally excited emission both in the Bar and d203-506. These emissions originate from the same region as highly excited H2 (high rotational and rovibrational levels) and correlate less with the lower rotational levels of H2 (J′ < 5) or the emission of aromatic and aliphatic infrared bands. Our comparison between the Bar and d203-506 revealed that both CH+ and CH3+ excitation and/or formation are highly dependent on gas density. The excitation temperature of the observed CH+ and CH3+ rovibrational lines is around T ∼ 1500 K in the Bar and T ∼ 800 K in d203-506. Moreover, the column densities derived from the rovibrational emission are less than 0.1% of the total known (CH+) and expected (CH3+) column densities. These different results show that CH+ and CH3+ level populations strongly deviate from local thermodynamical equilibrium. The CH+ rovibrational supra-thermal emission (v = 1 and v = 2) can be explained by chemical formation pumping with excited H2 via C+ + H2* = CH+ + H. The difference in the population distribution of the H2* energy levels between the Orion Bar and d203-506 then result in different excitation temperatures. These results support a gas phase formation pathway of CH+ and CH3+ via successive hydrogen abstraction reactions. However, we do not find any evidence of CH3+ emission in the JWST spectrum, which may be explained by the fact its spectroscopic signatures could be spread in the JWST spectra. Finally, the observed CH+ intensities coupled with a chemical formation pumping model provide a diagnostic tool to trace the local density.Conclusions. Line emission from vibrationally excited CH+ and CH3+ provides new insight into the first steps of hydrocarbon gas-phase chemistry in action. This study highlights the need for extended molecular data of detectable molecules in the interstellar medium in order to analyze the JWST observations.
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来源期刊
Astronomy & Astrophysics
Astronomy & Astrophysics 地学天文-天文与天体物理
CiteScore
10.20
自引率
27.70%
发文量
2105
审稿时长
1-2 weeks
期刊介绍: Astronomy & Astrophysics is an international Journal that publishes papers on all aspects of astronomy and astrophysics (theoretical, observational, and instrumental) independently of the techniques used to obtain the results.
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