50 research outputs found

    Seeds of Life in Space: methanol towards the pre-stellar core L1544

    Full text link
    В докладе представлены результаты интерферометрических наблюдений метанола на частоте 96.7 ГГц в направлении метанольного пика дозвездного ядра L1544. Профиль содержания метанола в L1544, полученный с помощью не-ЛТР моделирования спектральных линий, сравнивается с результатами химической модели.We present the results of the interferometric observations of methanol at 96.7 GHz towards the methanol peak near the pre-stellar core L1544. The methanol abundance profile derived with the non-LTE modelling of the methanol spectral lines is compared with the results of chemical modelling.Работа выполнена при поддержке грантов ERC-PALs 320620, ERCDOC 741002; STFC ST/L004801, ST/M004139; CITA National Fellowship

    The shocked molecular layer in RCW 120

    Get PDF
    Expansion of wind-blown bubbles or H ii regions lead to formation of shocks in the interstellar medium, which compress surrounding gas into dense layers. We made spatially and velocity-resolved observations of the RCW 120 photo-dissociation region (PDR) and nearby molecular gas with CO(6-5) and (CO)-C-13(6-5) lines and distinguished a bright CO-emitting layer, which we related with the dense shocked molecular gas moving away from the ionizing star due to expansion of H ii region. Simulating gas density and temperature, as well as brightness of several CO and C+ emission lines from the PDR, we found reasonable agreement with the observed values. Analysing gas kinematics, we revealed the large-scale shocked PDR and also several dense environments of embedded protostars and outflows. We observe the shocked layer as the most regular structure in the CO(6-5) map and in the velocity space, when the gas around Young stellar objects (YSOs) is dispersed by the outflows

    Ethynyl Around the HII Regions S255 and S257

    Full text link
    Abstract: We present the results of the ethynyl (C2H) emission line observations towards the S255 and S257 HII regions and the molecular cloud between them. Radial profiles of line brightness, column density, and abundance of C2H are obtained. We show that the radial profile of the ethynyl abundance is almost flat towards the HII regions and drops by a factor of two towards the molecular cloud. At the same time, we find that the ethynyl abundance is at maximum towards the point sources in the molecular cloud—the stars with emission lines or emitting in X-ray. Line profiles are consistent with the assumption that both HII regions have front and back neutral walls those move relative to each other. © 2021, Pleiades Publishing, Ltd.We are grateful to L.E. Pirogov, S.V. Kalenskii for valuable advice during the processing of observational data, to D.A. Semenov for a discussion of the chemistry of ethynyl, and to anonymous referee for valuable comments. This study was supported by Russian Foundation for Basic Research (contract No. 20-02-00643 А). Anna Punanova is a member of the Max-Planck-Gesellschaft partner group in the Ural Federal University. Anna Punanova is supported by the Russian Ministry of Science and Higher Education via state assignment FEUZ-2020-0038

    Deuterium fractionation in low-mass star-forming regions

    Full text link
    В этой работе мы исследуем, как меняется доля дейтерия в зависимости от физических условий в холодных ядрах на примере молекулярных облаков Тельца, Персея и Змееносца. Результаты показывают, что доля дейтерия в холодных ядрах в среднем разная в разных областях звездообразования. В наиболее плотной и турбулентной из рассматриваемых областей L1688 в Змееносце доля дейтерия в соединениях в два раза выше, чем L1495 в Тельце и в В5 в Персее. В L1495 и L1688 доли дейтерия в центральных частях и оболочке ядер отличаются примерно в 10 раз, тогда как в В5 только в 2—3 раза.In this work, we study how deuterium fraction changes depending on the physical conditions in cold cores embedded in the molecular clouds of Taurus, Perseus and Ophiuchus. The results show that the deuterium fraction in cold cores varies in different star-forming regions. In the densest and most turbulent of the studied regions, L1688 in Ophiuchus, the deuterium fraction is two times higher than that of L1495 in Taurus and B5 in Perseus. In L1495 and L1688, the deuterium fraction in the central parts of the cores and in their envelopes differ by a factor of 10, while in B5 only by a factor of 2—3.Работа выполнена при поддержке Российского научного фонда, проект 19-72-00064

    Deuterium fraction in cold dense cores in the star-forming region L1688

    Full text link
    В работе изучена доля дейтерия в холодных плотных ядрах в области маломассивного звездообразования L1688. Для изучения доли дейтерия и ее зависимости от физических параметров холодного плотного ядра построены наблюдательные карты трех пар соединений (N2H+ и N2D+, NH3 и NH2D, H13CO+ и DCO+) в направлении четырех холодных плотных ядер. Наблюдения выполнены на телескопе IRAM 30m (кроме данных NH3, взятых из обзора GAS по наблюдениям на GBT).The work presents a study of deuterium fraction in cold dense cores in the low mass starforming region L1688. To study the deuterium fraction and its correlation with physical conditions in a cold dense core, we produced the observational maps of three pairs of species (N2H+ and N2D+, NH3 and NH2D, H13CO+ and DCO+) towards four cold dense cores. The observations were carried out with the IRAM 30m telescope (except for NH3 data taken from the GAS survey based on observations with GBT).Работа выполнена при поддержке Российского научного фонда, проект 19-72-00064

    Deuterium fractionation in cold dense cores in the low-mass star forming region L1688

    Full text link
    In this work, we study deuterium fractionation in four starless cores in the low-mass star-forming region L1688 in the Ophiuchus molecular cloud. We study how the deuterium fraction (RDR_D) changes with environment, compare deuteration of ions and neutrals, core centre and its envelope, and attempt to reproduce the observed results with a gas-grain chemical model. We chose high and low gas density tracers to study both core centre and the envelope. With the IRAM 30m antenna, we mapped N2_2H+^+(1-0), N2_2D+^+(1-0), H13^{13}CO+^+ (1-0) and (2-1), DCO+^+(2-1), and pp-NH2_2D(111_{11}-101_{01}) towards the chosen cores. The missing pp-NH3_3 and N2_2H+^+(1-0) data were taken from the literature. To measure the molecular hydrogen column density, dust and gas temperature within the cores, we used the Herschel/SPIRE dust continuum emission data, the GAS survey data (ammonia), and the COMPLETE survey data to estimate the upper limit on CO depletion. We present the deuterium fraction maps for three species towards four starless cores. Deuterium fraction of the core envelopes traced by DCO+^+/H13^{13}CO+^+ is one order of magnitude lower (\sim0.08) than that of the core central parts traced by the nitrogen-bearing species (\sim0.5). Deuterium fraction increases with the gas density as indicated by high deuterium fraction of high gas density tracers and low deuterium fraction of lower gas density tracers and by the decrease of RDR_D with core radii, consistent with the predictions of the chemical model. Our model results show a good agreement with observations for RDR_D(N2_2D+^+/N2_2H+^+) and RD_D(DCO+^+/HCO+^+) and underestimate the RDR_D(NH2_2D/NH3_3).Comment: 30 pages with 22 figures, accepted for publication in MNRA

    Deuterium Fractionation in Pre-Stellar Cores in the ρ Ophiuchi Star Forming Region

    Full text link
    In this work we study deuterium fractionation in dense cores in the ρ Oph star-forming region. Deuterium fractionation is a result of the chemical reactions which take place under conditions of cold dense cores. For this study, we use the observations of two lines, N2H+(1–0) and N2D+(1–0), towards 5 dense cores, obtained with the IRAM 30m telescope.В работе рассматривается фракционирование дейтерия в плотных ядрах в области звездообразования ρ Змееносца. Фракционирование дейтерия является результатом химических реакций, протекающих в условиях плотных холодных ядер. Для исследования используются наблюдения двух линий, N2H+(1–0) и N2D+(1–0), в направлении пяти плотных ядер, полученные при помощи телескопа IRAM 30m.Работа выполнена при финансовой поддержке Российского научного фонда (проект 19-72-00064)

    Modeling of the Deuterium Fraction in the Low-Mass Star Formation Region L1688

    Full text link
    В этой работе представлено моделирование доли дейтерия в направлении холодных плотных ядер Oph-E-MM2, Oph-C-N, Oph-H-MM1 и Oph-F в области образования звезд малых масс L1688. Для исследования мы выбрали те соединения (N2H+ и N2D+, H13CO+ и DCO+, NH3 и NH2D), для которых мы ранее исследовали наблюдательные данные, полученные на телескопе IRAM-30m. Для определения доли дейтерия были использованы лучевые концентрации, полученные с помощью химической модели PyRate3. Были построены профили плотности и температуры для работы модели. Мы сравнили смоделированные и наблюдаемые доли дейтерия и лучевые концентрации, все наблюдаемые значения доли дейтерия и лучевые концентрации попали в пределы погрешности модели на моментах времени 2.3×105 лет, 2.8×105 лет, 8.2×104 лет и 2.8×105 лет для Oph-E-MM2, Oph-C-N, Oph-F и Oph-H-MM1 соответственно. Эти моменты времени можно считать химическими возрастами исследуемых холодных плотных ядер.In this work, we present the modelling of the deuterium fraction in the cold dense cores Oph-E-MM2, Oph-C-N, Oph-H-MM1, and Oph-F in the low-mass star formation region L1688. We selected species (N2H+ and N2D+, H13CO+ and DCO+, NH3 and NH2D) that were previously studied by observations, which were obtained with the IRAM-30m telescope. The column densities obtained using with the chemical model PyRate3 were used to estimate the deuterium fractions. Density and temperature profiles were used as a base of the model. We compared the modelled and observed deuterium fractions and column densities, all observed values of deuterium fraction and column densities fell within the uncertainties of the model at time points 2.3×105 years, 2.8×105 years, 8.2×104 years and 2.8×105 years for Oph-E-MM2, Oph-C-N, Oph-F and Oph-H-MM1 respectively. These moments of time can be considered the chemical ages of the cold dense cores.Работа выполнена при поддержке Российского научного фонда, проект 19-72-00064, а также при поддержке Министерства науки и образования России, проект FEUZ-2020-0038. Авторы благодарят анонимного рецензента за полезные замечания
    corecore