Abstract:Millimeter molecular line observations have been conducted toward the young (∼900 yr) bipolar planetary nebula (PN) K4-47, using the 12 m antenna and the Submillimeter Telescope of the Arizona Radio Observatory, and the Institut de Radioastronomie Millimétrique 30 m Telescope. Measurements at 1, 2, and 3 mm of multiple transitions were carried out to ensure the accuracy of all molecular identifications. K4-47 was found to be unusually chemically rich, containing three complex species, CH 3 CN, H 2 CNH, and CH … Show more
“…Since its first detection, CH 3 CCH has been extensively studied toward star-forming regions (e.g., Zhang et al 2014;Taniguchi et al 2018;Guzmán et al 2018;Bøgelund et al 2019;Calcutt et al 2019), and has proven to be a reliable tracer of their physical conditions (e.g., Bergin et al 1994). It has also been observed toward extagalactic sources, such as M 82, NGC 253, and NGC 1068 (Mauersberger et al, 1991;Qiu et al, 2020), and even toward a planetary nebula, as recently reported by Schmidt and Ziurys (2019). As a matter of fact, the widespread detection of CH 3 CCH even extends to planetary atmospheres (e.g.,…”
Section: The Spectral Tracer Methyl Acetylenesupporting
Nesta dissertação de mestrado, nós pretendemos explorar as propriedades físicas de regiões de formação estelar massiva através de seus espectros de emissão molecular, os quais têm a capacidade de prover informações importantes a respeito da fonte. Dessa forma, nós conduzimos um survey espectral de metil-acetileno (CH 3 CCH) no Hot Molecular Core/Outflow massivo G331.512-0.103, usando o telescópio de 12 m APEX. As nossas observações resultaram na detecção de 41 linhas nítidas e não-contaminadas de CH 3 CCH no intervalo de frequências entre 172 e 356 GHz. Através de uma análise assumindo o Equilíbrio Termodinâmico Local, na qual utilizamos diagramas rotacionais, determinamos T exc =47.1±1.2 K, N tot (CH 3 CCH)=6.9±0.5×10 15 cm −2 e X[CH 3 CCH/H 2 ]≈(1.5-7.6)×10 −8 para uma região extensa de emissão (∼10). Nós observamos que as intensidades relativas das linhas com K=2 e K=3 em um determinado K-ladder apresentam uma forte correlação negativa com o número quântico J superior da transição (r=-0.84). Essa observação foi analisada em conjunto com simulações dos espectros rotacionais puros de CH 3 CCH em diferentes temperaturas, juntamente com adaptações da técnica do diagrama rotacional. Os resultados indicaram que a emissãoé caracterizada por um gradiente de temperaturas, com limites inferior e superior de ∼40 e ∼60 K, respectivamente. Além disso, as larguras das linhas e as velocidades dos picos apresentam, em geral, uma forte correlação com as frequências das transições, sugerindo que o gás mais quente também está associado a efeitos mais fortes de turbulência. As transições com K=0 apresentam uma assinatura cinemática ligeiramente diferente do resto das linhas, indicando que elas podem estar traçando uma componente distinta do gás. Nós especulamos que essa componenteé caracterizada por temperaturas mais baixas, e portanto tamanhos maiores. No entanto, observações com maiores resoluções angulares são necessárias para verificar estas conclusões.
“…Since its first detection, CH 3 CCH has been extensively studied toward star-forming regions (e.g., Zhang et al 2014;Taniguchi et al 2018;Guzmán et al 2018;Bøgelund et al 2019;Calcutt et al 2019), and has proven to be a reliable tracer of their physical conditions (e.g., Bergin et al 1994). It has also been observed toward extagalactic sources, such as M 82, NGC 253, and NGC 1068 (Mauersberger et al, 1991;Qiu et al, 2020), and even toward a planetary nebula, as recently reported by Schmidt and Ziurys (2019). As a matter of fact, the widespread detection of CH 3 CCH even extends to planetary atmospheres (e.g.,…”
Section: The Spectral Tracer Methyl Acetylenesupporting
Nesta dissertação de mestrado, nós pretendemos explorar as propriedades físicas de regiões de formação estelar massiva através de seus espectros de emissão molecular, os quais têm a capacidade de prover informações importantes a respeito da fonte. Dessa forma, nós conduzimos um survey espectral de metil-acetileno (CH 3 CCH) no Hot Molecular Core/Outflow massivo G331.512-0.103, usando o telescópio de 12 m APEX. As nossas observações resultaram na detecção de 41 linhas nítidas e não-contaminadas de CH 3 CCH no intervalo de frequências entre 172 e 356 GHz. Através de uma análise assumindo o Equilíbrio Termodinâmico Local, na qual utilizamos diagramas rotacionais, determinamos T exc =47.1±1.2 K, N tot (CH 3 CCH)=6.9±0.5×10 15 cm −2 e X[CH 3 CCH/H 2 ]≈(1.5-7.6)×10 −8 para uma região extensa de emissão (∼10). Nós observamos que as intensidades relativas das linhas com K=2 e K=3 em um determinado K-ladder apresentam uma forte correlação negativa com o número quântico J superior da transição (r=-0.84). Essa observação foi analisada em conjunto com simulações dos espectros rotacionais puros de CH 3 CCH em diferentes temperaturas, juntamente com adaptações da técnica do diagrama rotacional. Os resultados indicaram que a emissãoé caracterizada por um gradiente de temperaturas, com limites inferior e superior de ∼40 e ∼60 K, respectivamente. Além disso, as larguras das linhas e as velocidades dos picos apresentam, em geral, uma forte correlação com as frequências das transições, sugerindo que o gás mais quente também está associado a efeitos mais fortes de turbulência. As transições com K=0 apresentam uma assinatura cinemática ligeiramente diferente do resto das linhas, indicando que elas podem estar traçando uma componente distinta do gás. Nós especulamos que essa componenteé caracterizada por temperaturas mais baixas, e portanto tamanhos maiores. No entanto, observações com maiores resoluções angulares são necessárias para verificar estas conclusões.
“…It has been proven to be a reliable tracer of physical conditions, such as temperature and density, and has been extensively studied toward star-forming regions (e.g., Buhl & Snyder 1973;Lovas et al 1976;Hollis et al 1981;Kuiper et al 1984;Taniguchi et al 2018;Guzmán et al 2018;Bøgelund et al 2019;Calcutt et al 2019). It has also been observed toward extragalactic sources, such as M 82, NGC 253, and NGC 1068 (Mauersberger et al 1991;Qiu et al 2020), and toward a planetary nebula (Schmidt & Ziurys 2019).…”
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.
“…It is as low as about 20 to 25 in the Galactic center region [21,26,27,28], increases to about 68 in the Solar neighborhood and even further in the outskirts of the Milky Way [21,29,30]. Much lower 12 C/ 13 C ratios than 20 were found in the envelopes of some late-type stars, for example ∼10 for CRL618 [12,31], ∼4 for CK Vulpécula [32], and ∼2 for K4−47 [14,33].…”
Section: Introductionmentioning
confidence: 95%
“…Temperatures of other starforming regions were determined via early propyne observations, such as Orion and DR 21 [6], and of many other sources, including the cold and dense star-less core TMC-1 [7,8]. The molecule was also detected in near-by galaxies, such as M82 and NGC253 [9], in more distant galaxies, such as the foreground galaxy at z ≈ 0.89 in the direction of the quasar PKS 1810−211 [10], in translucent molecular clouds [11], and in the envelopes of late-type stars, such as the protoplanetary nebular CRL618 [12], the asymptotic giant branch star CW Leonis [13] and the planetary nebula K4−47 [14]. Infrared observations with Voyager led to the detection of CH 3 CCH in the atmosphere of Titan [15]; the ISO satellite was employed later to discover propyne in the atmospheres of Saturn [16], Jupiter [17], and Uranus [18].…”
Section: Introductionmentioning
confidence: 99%
“…Propyne is so abundant in some astronomical sources that minor isotopic species were discovered as well. Even though CH 3 C 13 CH was found serendipitously [20], all isotopomers containing one 13 C were observed later [14,21,22]. The deuterated isotopologs CH 2 DCCH [23] and CH 3 CCD [24] were also detected.…”
Submillimeter spectra of three isotopomers of propyne containing one 13 C atom were recorded in natural isotopic composition in the region of 426 GHz to 785 GHz. Additional measurements were carried out near 110 GHz. Combining these with earlier data resulted in greatly improved spectroscopic parameters which permit reliable extrapolations up to about 1.5 THz. Coupled cluster quantum-chemical calculations were carried out in order to assess the differences between equilibrium and ground state rotational parameters of these and many other isotopic species to evaluate semi-empirical equilibrium structural parameters. In addition, we estimated the main spectroscopic parameters of the isotopomers of propyne with two 13 C atoms, which have not yet been studied in the laboratory, but which may be detectable in astronomical sources with a large amount of 13 C compared to the dominant 12 C.
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