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Several interstellar environments produce 'anomalous microwave emission', withbrightness-peaks at tens-of-gigahertz frequencies 1 . The emission's origins are uncertainrapidly-spinning nano-particles could emit electric-dipole radiation 2 , but polycyclic aromatic hydrocarbons proposed as the carrier are now found not to correlate with Galactic signals 3,4 . The difficulty is to identify co-spatial sources over long lines of sight. Here we identify anomalous microwave emission in three proto-planetary discs. These are the only known systems that host hydrogenated nano-diamonds 5 , in contrast to very common detection of polycyclic aromatic hydrocarbons 6 . Spectroscopy locates the nanodiamonds close to the host-stars, at physically-constrained temperatures 7 . Developing disc models 8 , we reproduce the emission with diamonds 0.75-1.1 nanometres in radius, holding ≤1-2% of the carbon budget. The microwave-emission:stellar-luminosity ratios are approximately constant, allowing nano-diamonds to be ubiquitous but emitting below detection thresholds in many star-systems. This can unify the findings with similar-sized diamonds found within solar system meteorites 9 . As nano-diamond spectral absorption is seen in interstellar sightlines 10 , these particles are also a candidate for generating galaxyscale 3 anomalous microwave emission.Here we analyse discs around luminous stars, mainly Herbig A-type emission-line (HAe) objects, rather than 'classical T Tauri' stars (CTTS) like the young Sun (where the discs evolve somewhat differently 11,12 ). Disc masses are characterised using thermal radiation from dust grains, and superposed spectral features indicate types of small particles, down to molecular sizes, e.g. polycyclic aromatic hydrocarbons (PAHs). One prominent PAH feature is at 3.3 μm, and this infrared band has also revealed 13 a few sources with 3.43, 3.53 μm peaks. These features are identified 5 with hydrogenated nano-diamonds 14 , of special interest as connecting to solar system nano-diamonds in meteorites 9 . The diamonds may form under conditions of high pressure, shocks or vapour deposition 15 , either internal or external to the proto-solar and extrasolar discs. We discuss the only three extrasolar discs found to host nano-diamonds, after systematic searches 5,16 of over 80 HAe stars. Many HAes 6 and some CTTS 17 exhibit PAHs, while diamonds could be rather ubiquitous but only rarely sufficiently excited to produce infrared features 5 .
Several interstellar environments produce 'anomalous microwave emission', withbrightness-peaks at tens-of-gigahertz frequencies 1 . The emission's origins are uncertainrapidly-spinning nano-particles could emit electric-dipole radiation 2 , but polycyclic aromatic hydrocarbons proposed as the carrier are now found not to correlate with Galactic signals 3,4 . The difficulty is to identify co-spatial sources over long lines of sight. Here we identify anomalous microwave emission in three proto-planetary discs. These are the only known systems that host hydrogenated nano-diamonds 5 , in contrast to very common detection of polycyclic aromatic hydrocarbons 6 . Spectroscopy locates the nanodiamonds close to the host-stars, at physically-constrained temperatures 7 . Developing disc models 8 , we reproduce the emission with diamonds 0.75-1.1 nanometres in radius, holding ≤1-2% of the carbon budget. The microwave-emission:stellar-luminosity ratios are approximately constant, allowing nano-diamonds to be ubiquitous but emitting below detection thresholds in many star-systems. This can unify the findings with similar-sized diamonds found within solar system meteorites 9 . As nano-diamond spectral absorption is seen in interstellar sightlines 10 , these particles are also a candidate for generating galaxyscale 3 anomalous microwave emission.Here we analyse discs around luminous stars, mainly Herbig A-type emission-line (HAe) objects, rather than 'classical T Tauri' stars (CTTS) like the young Sun (where the discs evolve somewhat differently 11,12 ). Disc masses are characterised using thermal radiation from dust grains, and superposed spectral features indicate types of small particles, down to molecular sizes, e.g. polycyclic aromatic hydrocarbons (PAHs). One prominent PAH feature is at 3.3 μm, and this infrared band has also revealed 13 a few sources with 3.43, 3.53 μm peaks. These features are identified 5 with hydrogenated nano-diamonds 14 , of special interest as connecting to solar system nano-diamonds in meteorites 9 . The diamonds may form under conditions of high pressure, shocks or vapour deposition 15 , either internal or external to the proto-solar and extrasolar discs. We discuss the only three extrasolar discs found to host nano-diamonds, after systematic searches 5,16 of over 80 HAe stars. Many HAes 6 and some CTTS 17 exhibit PAHs, while diamonds could be rather ubiquitous but only rarely sufficiently excited to produce infrared features 5 .
Planck has mapped the microwave sky in temperature over nine frequency bands between 30 and 857 GHz and in polarization over seven frequency bands between 30 and 353 GHz in polarization. In this paper we consider the problem of diffuse astrophysical component separation, and process these maps within a Bayesian framework to derive an internally consistent set of full-sky astrophysical component maps. Component separation dedicated to cosmic microwave background (CMB) reconstruction is described in a companion paper. For the temperature analysis, we combine the Planck observations with the 9-yr Wilkinson Microwave Anisotropy Probe (WMAP) sky maps and the Haslam et al. 408 MHz map, to derive a joint model of CMB, synchrotron, free-free, spinning dust, CO, line emission in the 94 and 100 GHz channels, and thermal dust emission. Full-sky maps are provided for each component, with an angular resolution varying between 7. 5 and 1 • . Global parameters (monopoles, dipoles, relative calibration, and bandpass errors) are fitted jointly with the sky model, and best-fit values are tabulated. For polarization, the model includes CMB, synchrotron, and thermal dust emission. These models provide excellent fits to the observed data, with rms temperature residuals smaller than 4 µK over 93% of the sky for all Planck frequencies up to 353 GHz, and fractional errors smaller than 1% in the remaining 7% of the sky. The main limitations of the temperature model at the lower frequencies are internal degeneracies among the spinning dust, free-free, and synchrotron components; additional observations from external low-frequency experiments will be essential to break these degeneracies. The main limitations of the temperature model at the higher frequencies are uncertainties in the 545 and 857 GHz calibration and zero-points. For polarization, the main outstanding issues are instrumental systematics in the 100-353 GHz bands on large angular scales in the form of temperature-to-polarization leakage, uncertainties in the analogue-to-digital conversion, and corrections for the very long time constant of the bolometer detectors, all of which are expected to improve in the near future.
Context. Sensitive ground-based submillimeter surveys, such as ATLASGAL, provide a global view on the distribution of cold dense gas in the Galactic plane at up to two-times better angular-resolution compared to recent space-based surveys with Herschel. However, a drawback of ground-based continuum observations is that they intrinsically filter emission, at angular scales larger than a fraction of the field-of-view of the array, when subtracting the sky noise in the data processing. The lost information on the distribution of diffuse emission can be, however, recovered from space-based, all-sky surveys with Planck. Aims.Here we aim to demonstrate how this information can be used to complement ground-based bolometer data and present reprocessed maps of the APEX Telescope Large Area Survey of the Galaxy (ATLASGAL) survey. Methods. We use the maps at 353 GHz from the Planck/HFI instrument, which performed a high sensitivity all-sky survey at a frequency close to that of the APEX/LABOCA array, which is centred on 345 GHz. Complementing the ground-based observations with information on larger angular scales, the resulting maps reveal the distribution of cold dust in the inner Galaxy with a larger spatial dynamic range. We visually describe the observed features and assess the global properties of dust distribution. Results. Adding information from large angular scales helps to better identify the global properties of the cold Galactic interstellar medium. To illustrate this, we provide mass estimates from the dust towards the W43 star-forming region and estimate a column density contrast of at least a factor of five between a low intensity halo and the star-forming ridge. We also show examples of elongated structures extending over angular scales of 0.5 • , which we refer to as thin giant filaments. Corresponding to >30 pc structures in projection at a distance of 3 kpc, these dust lanes are very extended and show large aspect ratios. We assess the fraction of dense gas by determining the contribution of the APEX/LABOCA maps to the combined maps, and estimate 2−5% for the dense gas fraction (corresponding to A v > 7 mag) on average in the Galactic plane. We also show probability distribution functions of the column density (N-PDF), which reveal the typically observed log-normal distribution for low column density and exhibit an excess at high column densities. As a reference for extragalactic studies, we show the line-of-sight integrated N-PDF of the inner Galaxy, and derive a contribution of this excess to the total column density of ∼2.2%, corresponding to N H 2 = 2.92 × 10 22 cm −2 . Taking the total flux density observed in the maps, we provide an independent estimate of the mass of molecular gas in the inner Galaxy of ∼1 × 10 9 M , which is consistent with previous estimates using CO emission. From the mass and dense gas fraction ( f DG ), we estimate a Galactic SFR ofṀ = 1.3 M yr −1 . Conclusions. Retrieving the extended emission helps to better identify massive giant filaments which are elongated and c...
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