26 research outputs found

    Characterizing the transition from diffuse atomic to dense molecular clouds in the Magellanic clouds with [CII], [CI], and CO

    Full text link
    We present and analyze deep Herschel/HIFI observations of the [CII] 158um, [CI] 609um, and [CI] 370um lines towards 54 lines-of-sight (LOS) in the Large and Small Magellanic clouds. These observations are used to determine the physical conditions of the line--emitting gas, which we use to study the transition from atomic to molecular gas and from C^+ to C^0 to CO in their low metallicity environments. We trace gas with molecular fractions in the range 0.1<f(H2)<1, between those in the diffuse H2 gas detected by UV absorption (f(H2)<0.2) and well shielded regions in which hydrogen is essentially completely molecular. The C^0 and CO column densities are only measurable in regions with molecular fractions f(H2)>0.45 in both the LMC and SMC. Ionized carbon is the dominant gas-phase form of this element that is associated with molecular gas, with C^0 and CO representing a small fraction, implying that most (89% in the LMC and 77% in the SMC) of the molecular gas in our sample is CO-dark H2. The mean X_CO conversion factors in our LMC and SMC sample are larger than the value typically found in the Milky Way. When applying a correction based on the filling factor of the CO emission, we find that the values of X_CO in the LMC and SMC are closer to that in the Milky Way. The observed [CII] intensity in our sample represents about 1% of the total far-infrared intensity from the LOSs observed in both Magellanic Clouds.Comment: 32 pages, 21 figures, Accepted to Ap

    The 492 GHz emission of Sgr A* constrained by ALMA

    Full text link
    We report linearly polarized continuum emission properties of Sgr A* at ∌\sim492 GHz, based on the Atacama Large Millimeter Array (ALMA) observations. We used the observations of the likely unpolarized continuum emission of Titan, and the observations of C\textsc{i} line emission, to gauge the degree of spurious polarization. The Stokes I flux of 3.6±\pm0.72 Jy during our run is consistent with extrapolations from the previous, lower frequency observations. We found that the continuum emission of Sgr A* at ∌\sim492 GHz shows large amplitude differences between the XX and the YY correlations. The observed intensity ratio between the XX and YY correlations as a function of parallactic angle may be explained by a constant polarization position angle of ∌\sim158∘^{\circ}±\pm3∘^{\circ}. The fitted polarization percentage of Sgr A* during our observational period is 14\%±\pm1.2\%. The calibrator quasar J1744-3116 we observed at the same night can be fitted to Stokes I = 252 mJy, with 7.9\%±\pm0.9\% polarization in position angle P.A. = 4.1∘^{\circ}±\pm4.2∘^{\circ}. The observed polarization percentage and polarization position angle in the present work appear consistent with those expected from longer wavelength observations in the period of 1999-2005. In particular, the polarization position angle at 492 GHz, expected from the previously fitted 167∘^{\circ}±\pm7∘^{\circ} intrinsic polarization position angle and (-5.6±\pm0.7)×\times105^{5} rotation measure, is 155−8+9^{+9}_{-8}, which is consistent with our new measurement of polarization position angle within 1σ\sigma. The polarization percentage and the polarization position angle may be varying over the period of our ALMA 12m Array observations, which demands further investigation with future polarization observations.Comment: 10 pages, 6 figures, 1st referee report received and revise

    CARMA CO(J = 2 - 1) Observations of the Circumstellar Envelope of Betelgeuse

    Full text link
    We report radio interferometric observations of the 12C16O 1.3 mm J = 2-1 emission line in the circumstellar envelope of the M supergiant Alpha Ori and have detected and separated both the S1 and S2 flow components for the first time. Observations were made with the Combined Array for Research in Millimeter-wave Astronomy (CARMA) interferometer in the C, D, and E antenna configurations. We obtain good u-v coverage (5-280 klambda) by combining data from all three configurations allowing us to trace spatial scales as small as 0.9\arcsec over a 32\arcsec field of view. The high spectral and spatial resolution C configuration line profile shows that the inner S1 flow has slightly asymmetric outflow velocities ranging from -9.0 km s-1 to +10.6 km s-1 with respect to the stellar rest frame. We find little evidence for the outer S2 flow in this configuration because the majority of this emission has been spatially-filtered (resolved out) by the array. We also report a SOFIA-GREAT CO(J= 12-11) emission line profile which we associate with this inner higher excitation S1 flow. The outer S2 flow appears in the D and E configuration maps and its outflow velocity is found to be in good agreement with high resolution optical spectroscopy of K I obtained at the McDonald Observatory. We image both S1 and S2 in the multi-configuration maps and see a gradual change in the angular size of the emission in the high absolute velocity maps. We assign an outer radius of 4\arcsec to S1 and propose that S2 extends beyond CARMA's field of view (32\arcsec at 1.3 mm) out to a radius of 17\arcsec which is larger than recent single-dish observations have indicated. When azimuthally averaged, the intensity fall-off for both flows is found to be proportional to R^{-1}, where R is the projected radius, indicating optically thin winds with \rho \propto R^{-2}.Comment: 11 pages, 8 figures To be published in the Astronomical Journal (Received 2012 February 10; accepted 2012 May 25

    H2CN/H2NC abundance ratio: a new potential temperature tracer for the interstellar medium

    Get PDF
    The H2NC{\rm H_2NC} radical is the high-energy metastable isomer of H2CN{\rm H_2CN} radical, which has been recently detected for the first time in the interstellar medium towards a handful of cold galactic sources, besides a warm galaxy in front of the PKS 1830-211 quasar. These detections have shown that the H2CN{\rm H_2CN}/H2NC{\rm H_2NC} isomeric ratio, likewise the HCN/HNC ratio, might increase with the kinetic temperature (TkinT_{\rm kin}), but the shortage of them in warm sources still prevents us to confirm this hypothesis and shed light about their chemistry. In this work, we present the first detection of H2CN{\rm H_2CN} and H2NC{\rm H_2NC} towards a warm galactic source, the G+0.693-0.027 molecular cloud (with Tkin>70 KT_{\rm kin} > 70 \, {\rm K}), using IRAM 30m observations. We have detected multiple hyperfine components of the NKaKc=101−000N_{K_\text{a}K_\text{c}} = 1_{01} - 0_{00} and 202−1012_{02} - 1_{01} transitions. We derived molecular abundances with respect to H2{\rm H_2} of (6.8±\pm1.3)×10−11\times 10^{-11} for H2CN{\rm H_2CN} and of (3.1±\pm0.7)×10−11\times 10^{-11} for H2NC{\rm H_2NC}, and a H2CN{\rm H_2CN}/H2NC{\rm H_2NC} abundance ratio of 2.2±\pm0.5. These detections confirm that the H2CN{\rm H_2CN}/H2NC{\rm H_2NC} ratio is ≳\gtrsim2 for sources with Tkin>70 KT_{\rm kin} > 70 \, {\rm K}, larger than the ∌\sim1 ratios previously found in colder cores (Tkin∌10 KT_{\rm kin}\sim10 \, {\rm K}). This isomeric ratio dependence with temperature cannot be fully explained with the currently proposed gas-phase formation and destruction pathways. Grain surface reactions, including the H2NC→H2CN{\rm H_2NC} \rightarrow {\rm H_2CN} isomerization, deserve consideration to explain the higher isomeric ratios and H2CN{\rm H_2CN} abundances observed in warm sources, where the molecules can be desorbed into the gas phase through thermal and/or shock-induced mechanisms.Comment: 12 pages, 5 figures, 3 tables, 2 appendix - Accepted for publication in Monthly Notices of the Royal Astronomical Societ

    Interstellar detection of O-protonated carbonyl sulfide, HOCS+

    Full text link
    We present the first detection in space of O-protonated carbonyl sulfide (\ch{HOCS+}), in the midst of an ultradeep molecular line survey toward the G+0.693-0.027 molecular cloud. From the observation of all KKa_a = 0 transitions ranging from JJlo_{lo} = 2 to JJlo_{lo} = 13 of \ch{HOCS+} covered by our survey, we derive a column density of NN = (9 ±\pm 2)×\times1012^{12} cm−2^{-2}, translating into a fractional abundance relative to H2_2 of ∌\sim7×\times10−11^{-11}. Conversely, the S-protonated \ch{HSCO+} isomer remains undetected, and we derive an upper limit to its abundance with respect to H2_2 of ≀\leq3×\times10−11^{-11}, a factor of ≄\geq2.3 less abundant than \ch{HOCS+}. We obtain a \ch{HOCS+}/OCS ratio of ∌\sim2.5×\times10−3^{-3}, in good agreement with the prediction of astrochemical models. These models show that one of the main chemical routes to the interstellar formation of \ch{HOCS+} is likely the protonation of OCS, which appears to be more efficient at the oxygen end. Also, we find that high values of cosmic-ray ionisation rates (10−15^{-15}-10−14^{-14} s−1^{-1}) are needed to reproduce the observed abundance of \ch{HOCS+}. In addition, we compare the O/S ratio across different interstellar environments. G+0.693-0.027 appears as the source with the lowest O/S ratio. We find a \ch{HOCO+}/\ch{HOCS+} ratio of ∌\sim31, in accordance with other O/S molecular pairs detected toward this region and also close to the O/S solar value (∌\sim37). This fact indicates that S is not significantly depleted within this cloud due to the action of large-scale shocks, unlike in other sources where S-bearing species remain trapped on icy dust grains.Comment: Forthcoming paper in The Astrophysical Journal (in press

    Discovery of the elusive carbonic acid (HOCOOH) in space

    Get PDF
    After a quarter century since the detection of the last interstellar carboxylic acid, acetic acid (CH3_3COOH), we report the discovery of a new one, the cis-trans form of carbonic acid (HOCOOH), toward the Galactic Center molecular cloud G+0.693-0.027. HOCOOH stands as the first interstellar molecule containing three oxygen atoms and also the third carboxylic acid detected so far in the interstellar medium. Albeit the limited available laboratory measurements (up to 65 GHz), we have also identified several pairs of unblended lines directly in the astronomical data (between 75-120 GHz), which allowed us to slightly improve the set of spectroscopic constants. We derive a column density for cis-trans HOCOOH of NN = (6.4 ±\pm 0.4) ×\times 1012^{12} cm−2^{-2}, which yields an abundance with respect to molecular H2_2 of 4.7 ×\times 10−11^{-11}. Meanwhile, the extremely low dipole moment (about fifteen times lower) of the lower-energy conformer, cis-cis HOCOOH, precludes its detection. We obtain an upper limit to its abundance with respect to H2_2 of ≀\leq 1.2 ×\times10−9^{-9}, which suggests that cis-cis HOCOOH might be fairly abundant in interstellar space, although it is nearly undetectable by radio astronomical observations. We derive a cis-cis/cis-trans ratio ≀\leq 25, consistent with the smaller energy difference between both conformers compared with the relative stability of trans- and cis-formic acid (HCOOH). Finally, we compare the abundance of these acids in different astronomical environments, further suggesting a relationship between the chemical content found in the interstellar medium and the chemical composition of the minor bodies of the Solar System, which could be inherited during the star formation process.Comment: Accepted for publication in The Astrophysical Journa

    First glycine isomer detected in the interstellar medium: glycolamide (NH2_2C(O)CH2_2OH)

    Full text link
    We report the first detection in the interstellar medium of a C2_2H5_5O2_2N isomer: synsyn-glycolamide (NH2_2C(O)CH2_2OH). The exquisite sensitivity at sub-mK levels of an ultra-deep spectral survey carried out with the Yebes 40m and IRAM 30m telescopes towards the G+0.693-0.027 molecular cloud have allowed us to unambiguously identify multiple transitions of this species. We derived a column density of (7.4 ±\pm 0.7)×\times1012^{12} cm−2^{-2}, which implies a molecular abundance with respect to H2_2 of 5.5×\times10−11^{-11}. The other C2_2H5_5O2_2N isomers, including the higher-energy antianti conformer of glycolamide, and two conformers of glycine, were not detected. The upper limit derived for the abundance of glycine indicates that this amino acid is surely less abundant than its isomer glycolamide in the ISM. The abundances of the C2_2H5_5O2_2N isomers cannot be explained in terms of thermodynamic equilibrium, and thus chemical kinetics need to be invoked. While the low abundance of glycine might not be surprising, based on the relative low abundances of acids in the ISM compared to other compounds (e.g. alcohols, aldehydes or amines), several chemical pathways can favour the formation of its isomer glycolamide. It can be formed through radical-radical reactions on the surface of dust grains. The abundances of these radicals can be significantly boosted in an environment affected by a strong ultraviolet field induced by cosmic rays, such as that expected in G+0.693-0.027. Therefore, as shown by several recent molecular detections towards this molecular cloud, it stands out as the best target to discover new species with carbon, oxygen and nitrogen with increasing chemical complexity.Comment: Accepted in The Astrophysical Journal Letter

    Precursors of fatty alcohols in the ISM: Discovery of n-propanol

    Get PDF
    Theories on the origins of life propose that early cell membranes were synthesized from amphiphilic molecules simpler than phospholipids such as fatty alcohols. The discovery in the interstellar medium (ISM) of ethanolamine, the simplest phospholipid head group, raises the question whether simple amphiphilic molecules are also synthesized in space. We investigate whether precursors of fatty alcohols are present in the ISM. For this, we have carried out a spectral survey at 7, 3, 2 and 1 mm toward the Giant Molecular Cloud G+0.693-0.027 located in the Galactic Center using the IRAM 30m and Yebes 40m telescopes. Here, we report the detection in the ISM of the primary alcohol n-propanol (in both conformers Ga-n-C3H7OH and Aa-n-C3H7OH), a precursor of fatty alcohols. The derived column densities of n-propanol are (5.5+-0.4)x10^13 cm^-2 for the Ga conformer and (3.4+-0.3)x10^13 cm^-2 for the Aa conformer, which imply molecular abundances of (4.1+-0.3)x10^-10 for Ga-n-C3H7OH and of (2.5+-0.2)x10^-10 for Aa-n-C3H7OH. We also searched for the AGa conformer of n-butanol (AGa-n-C4H9OH) without success yielding an upper limit to its abundance of <4.1x10^-11. The inferred CH3OH:C2H5OH:C3H7OH:C4H9OH abundance ratios go as 1:0.04:0.006:<0.0004 toward G+0.693-0.027, i.e. they decrease roughly by one order of magnitude for increasing complexity. We also report the detection of both syn and anti conformers of vinyl alcohol, with column densities of (1.11+-0.08)x10^14 cm^-2 and (1.3+-0.4)x10^13 cm^-2, and abundances of (8.2+-0.6)x10^-10 and (9.6+-3.0)x10^-11, respectively. The detection of n-propanol, together with the recent discovery of ethanolamine in the ISM, opens the possibility that precursors of lipids according to theories of the origin of life, could have been brought to Earth from outer space.Comment: 15 pages, 10 figures, accepted for A&
    corecore