Imperial College London

Dr Clements

Faculty of Natural SciencesDepartment of Physics

Reader in Astrophysics
 
 
 
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Contact

 

+44 (0)20 7594 7693d.clements

 
 
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Location

 

1011Blackett LaboratorySouth Kensington Campus

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Summary

 

Publications

Publication Type
Year
to

672 results found

Negrello M, Gonzalez-Nuevo J, De Zotti G, Bonato M, Cai ZY, Clements D, Danese L, Dole H, Greenslade J, Lapi A, Montier Let al., 2017, On the statistics of proto-cluster candidates detected in the Planck all-sky survey, Monthly Notices of the Royal Astronomical Society, Vol: 470, Pages: 2253-2261, ISSN: 0035-8711

Observational investigations of the abundance of massive precursors of local galaxy clusters ('proto-clusters') allow us to test the growth of density perturbations, to constrain cosmological parameters that control it, to test the theory of non-linear collapse and how the galaxy formation takes place in dense environments. The Planck collaboration has recently published a catalogue of ≳2000 cold extragalactic sub-millimeter sources, i.e. with colours indicative of z ≳ 2, almost all of which appear to be overdensities of star-forming galaxies. They are thus considered as proto-cluster candidates. Their number densities (or their flux densities) are far in excess of expectations from the standard scenario for the evolution of large-scale structure. Simulations based on a physically motivated galaxy evolution model show that essentially all cold peaks brighter than S545GHz= 500 mJy found in Planck maps after having removed the Galactic dust emission can be interpreted as positive Poisson fluctuations of the number of high-z dusty proto-clusters within the same Planck beam, rather then being individual clumps of physically bound galaxies. This conclusion does not change if an empirical fit to the luminosity function of dusty galaxies is used instead of the physical model. The simulations accurately reproduce the statistic of the Planck detections and yield distributions of sizes and ellipticities in qualitative agreement with observations. The redshift distribution of the brightest proto-clusters contributing to the cold peaks has a broad maximum at 1.5 ≤ z ≤ 3. Therefore follow-up of Planck proto-cluster candidates will provide key information on the high-z evolution of large scale structure.

Journal article

MacKenzie TP, Scott D, Bianconi M, Clements DL, Dole HA, Flores-Cacho I, Guery D, Kneissl R, Lagache G, Marleau FR, Montier L, Nesvadba NPH, Pointecouteau E, Soucail Get al., 2017, SCUBA-2 follow-up of Herschel-SPIRE observed Planck overdensities, Monthly Notices of the Royal Astronomical Society, Vol: 468, Pages: 4006-4017, ISSN: 0035-8711

We present SCUBA-2 follow-up of 61 candidate high-redshift Planck sources. Of these, 10 are confirmed strong gravitational lenses and comprise some of the brightest such submm sources on the observed sky, while 51 are candidate proto-cluster fields undergoing massive starburst events. With the accompanying Herschel-Spectral and Photometric Imaging Receiver observations and assuming an empirical dust temperature prior of 34+13−934−9+13 K, we provide photometric redshift and far-IR luminosity estimates for 172 SCUBA-2-selected sources within these Planck overdensity fields. The redshift distribution of the sources peak between a redshift of 2 and 4, with one-third of the sources having S500/S350 > 1. For the majority of the sources, we find far-IR luminosities of approximately 1013 L⊙, corresponding to star formation rates of around 1000 M⊙ yr−1. For S850 > 8 mJy sources, we show that there is up to an order of magnitude increase in star formation rate density and an increase in uncorrected number counts of 6 for S850 > 8 mJy when compared to typical cosmological survey fields. The sources detected with SCUBA-2 account for only approximately 5 per cent of the Planck flux at 353 GHz, and thus many more fainter sources are expected in these fields.

Journal article

Negrello M, Amber S, Amvrosiadis A, Cai Z-Y, Lapi A, Gonzalez-Nuevo J, De Zotti G, Furlanetto C, Maddox SJ, Allen M, Bakx T, Bussmann RS, Cooray A, Covone G, Danese L, Dannerbauer H, Fu H, Greenslade J, Gurwell M, Hopwood R, Koopmans LVE, Napolitano N, Nayyeri H, Omont A, Petrillo CE, Riechers DA, Serjeant S, Tortora C, Valiante E, Kleijn GV, Vernardos G, Wardlow JL, Baes M, Baker AJ, Bourne N, Clements D, Crawford SM, Dye S, Dunne L, Eales S, Ivison RJ, Marchetti L, Michalowski MJ, Smith MWL, Vaccari M, van der Werf Pet al., 2017, The Herschel-ATLAS: a sample of 500 mu m- selected lensed galaxies over 600 deg(2), Monthly Notices of the Royal Astronomical Society, Vol: 465, Pages: 3558-3580, ISSN: 0035-8711

We present a sample of 80 candidate strongly lensed galaxies with flux density above 100 mJy at 500 μm extracted from the Herschel Astrophysical Terahertz Large Area Survey, over an area of 600 deg2. Available imaging and spectroscopic data allow us to confirm the strong lensing in 20 cases and to reject it in one case. For other eight objects, the lensing scenario is strongly supported by the presence of two sources along the same line of sight with distinct photometric redshifts. The remaining objects await more follow-up observations to confirm their nature. The lenses and the background sources have median redshifts zL = 0.6 and zS = 2.5, respectively, and are observed out to zL = 1.2 and zS = 4.2. We measure the number counts of candidate lensed galaxies at 500 μm and compare them with theoretical predictions, finding a good agreement for a maximum magnification of the background sources in the range 10–20. These values are consistent with the magnification factors derived from the lens modelling of individual systems. The catalogue presented here provides sub-mm bright targets for follow-up observations aimed at exploiting gravitational lensing, to study with unprecedented details the morphological and dynamical properties of dusty star-forming regions in z ≳ 1.5 galaxies.

Journal article

Wardlow JL, Cooray A, Osage W, Bourne N, Clements D, Dannerbauer H, Dunne L, Dye S, Eales S, Farrah D, Furlanetto C, Ibar E, Ivison R, Maddox S, Michalowski MM, Riechers D, Rigopoulou D, Scott D, Smith MWL, Wang L, van der Werf P, Valiante E, Valtchanov I, Verma Aet al., 2017, The interstellar medium in high-redshift submillimeter galaxies as probed by infrared spectroscopy, Astrophysical Journal, Vol: 837, ISSN: 0004-637X

Submillimeter galaxies (SMGs) at $z\gtrsim 1$ are luminous in the far-infrared, and have star formation rates, SFR, of hundreds to thousands of solar masses per year. However, it is unclear whether they are true analogs of local ULIRGs or whether the mode of their star formation is more similar to that in local disk galaxies. We target these questions by using Herschel-PACS to examine the conditions in the interstellar medium (ISM) in far-infrared luminous SMGs at $z\sim 1$–4. We present 70–160 μm photometry and spectroscopy of the [O iv]26 μm, [Fe ii]26 μm, [S iii]33 μm, [Si ii]34 μm, [O iii]52 μm, [N iii]57 μm, and [O i]63 μm fine-structure lines and the S(0) and S(1) hydrogen rotational lines in 13 lensed SMGs identified by their brightness in early Herschel data. Most of the 13 targets are not individually spectroscopically detected; we instead focus on stacking these spectra with observations of an additional 32 SMGs from the Herschel archive—representing a complete compilation of PACS spectroscopy of SMGs. We detect [O i]63 μm, [Si ii]34 μm, and [N iii]57 μm at $\geqslant 3\sigma $ in the stacked spectra, determining that the average strengths of these lines relative to the far-IR continuum are $(0.36\pm 0.12)\times {10}^{-3}$, $(0.84\pm 0.17)\times {10}^{-3}$, and $(0.27\pm 0.10)\times {10}^{-3}$, respectively. Using the [O iii]52 μm/[N iii]57 μm emission line ratio, we show that SMGs have average gas-phase metallicities $\gtrsim {Z}_{\odot }$. By using PDR modeling and combining the new spectral measurements with integrated far-infrared fluxes and existing [C ii]158 μm data, we show that SMGs have average gas densities, n, of $\sim {10}^{1-3}\,{\mathrm{cm}}^{-3}$ and FUV field strengths, ${G}_{0}\sim {10}^{2.2-4.5}$ (in Habing units: $1.6\times {10}^{-3}\,\mathrm{erg}\,{\mathrm{cm}}^{-2}\,{{\rm{s}}}^{-1}$), consistent with both local ULIRGs and lower luminosity star-forming galaxies.

Journal article

Geach JE, Dunlop JS, Halpern M, Smail I, van der Werf P, Alexander DM, Almaini O, Aretxaga I, Arumugam V, Asboth V, Banerji M, Beanlands J, Best PN, Blain AW, Birkinshaw M, Chapin EL, Chapman SC, Chen C-C, Chrysostomou A, Clarke C, Clements DL, Conselice C, Coppin KEK, Cowley WI, Danielson ALR, Eales S, Edge AC, Farrah D, Gibb A, Harrison CM, Hine NK, Hughes D, Ivison RJ, Jarvis M, Jenness T, Jones SF, Karim A, Koprowski M, Knudsen KK, Lacey CG, Mackenzie T, Marsden G, McAlpine K, McMahon R, Meijerink R, Michalowski MJ, Oliver SJ, Page MJ, Peacock JA, Rigopoulou D, Robson EI, Roseboom I, Rotermund K, Scott D, Serjeant S, Simpson C, Simpson JM, Smith DJB, Spaans M, Stanley F, Stevens JA, Swinbank AM, Targett T, Thomson AP, Valiante E, Wake DA, Webb TMA, Willott C, Zavala JA, Zemcov Met al., 2017, The SCUBA-2 Cosmology Legacy Survey: 850 mu m maps, catalogues and number counts, Monthly Notices of the Royal Astronomical Society, Vol: 465, Pages: 1789-1806, ISSN: 0035-8711

We present a catalogue of ∼3000 submillimetre sources detected (≥3.5σ) at 850 μm over ∼5 deg2 surveyed as part of the James Clerk Maxwell Telescope (JCMT) SCUBA-2 Cosmology Legacy Survey (S2CLS). This is the largest survey of its kind at 850 μm, increasing the sample size of 850 μm selected submillimetre galaxies by an order of magnitude. The wide 850 μm survey component of S2CLS covers the extragalactic fields: UKIDSS-UDS, COSMOS, Akari-NEP, Extended Groth Strip, Lockman Hole North, SSA22 and GOODS-North. The average 1σ depth of S2CLS is 1.2 mJy beam−1, approaching the SCUBA-2 850 μm confusion limit, which we determine to be σc ≈ 0.8 mJy beam−1. We measure the 850 μm number counts, reducing the Poisson errors on the differential counts to approximately 4 per cent at S850 ≈ 3 mJy. With several independent fields, we investigate field-to-field variance, finding that the number counts on 0.5°–1° scales are generally within 50 per cent of the S2CLS mean for S850 > 3 mJy, with scatter consistent with the Poisson and estimated cosmic variance uncertainties, although there is a marginal (2σ) density enhancement in GOODS-North. The observed counts are in reasonable agreement with recent phenomenological and semi-analytic models, although determining the shape of the faint-end slope (S850 < 3 mJy) remains a key test. The large solid angle of S2CLS allows us to measure the bright-end counts: at S850 > 10 mJy there are approximately 10 sources per square degree, and we detect the distinctive up-turn in the number counts indicative of the detection of local sources of 850 μm emission, and strongly lensed high-redshift galaxies. All calibrated maps and the catalogue are made publicly available.

Journal article

Zavala JA, Aretxaga I, Geach JE, Hughes DH, Birkinshaw M, Chapin E, Chapman S, Chen C-C, Clements DL, Dunlop JS, Farrah D, Ivison RJ, Jenness T, Michalowski MJ, Robson EI, Scott D, Simpson J, Spaans M, van der Werf Pet al., 2017, The SCUBA-2 Cosmology Legacy Survey: the EGS deep field - I. Deep number counts and the redshift distribution of the recovered cosmic infrared background at 450 and 850 mu m, Monthly Notices of the Royal Astronomical Society, Vol: 464, Pages: 3369-3384, ISSN: 0035-8711

We present deep observations at 450 and 850 μm in the Extended Groth Strip field taken with the SCUBA-2 camera mounted on the James Clerk Maxwell Telescope as part of the deep SCUBA-2 Cosmology Legacy Survey (S2CLS), achieving a central instrumental depth of σ450 = 1.2 mJy beam−1 and σ850 = 0.2 mJy beam−1. We detect 57 sources at 450 μm and 90 at 850 μm with signal-to-noise ratio >3.5 over ∼70 arcmin2. From these detections, we derive the number counts at flux densities S450 > 4.0 mJy and S850 > 0.9 mJy, which represent the deepest number counts at these wavelengths derived using directly extracted sources from only blank-field observations with a single-dish telescope. Our measurements smoothly connect the gap between previous shallower blank-field single-dish observations and deep interferometric ALMA results. We estimate the contribution of our SCUBA-2 detected galaxies to the cosmic infrared background (CIB), as well as the contribution of 24 μm-selected galaxies through a stacking technique, which add a total of 0.26 ± 0.03 and 0.07 ± 0.01 MJy sr−1, at 450 and 850 μm, respectively. These surface brightnesses correspond to 60 ± 20 and 50 ± 20 per cent of the total CIB measurements, where the errors are dominated by those of the total CIB. Using the photometric redshifts of the 24 μm-selected sample and the redshift distributions of the submillimetre galaxies, we find that the redshift distribution of the recovered CIB is different at each wavelength, with a peak at z ∼ 1 for 450 μm and at z ∼ 2 for 850 μm, consistent with previous observations and theoretical models.

Journal article

Clements D, Mancarella P, 2017, Risk of Cable Overheating And Premature Ageing due to Load Control Measures, IEEE Manchester PowerTech, Publisher: IEEE

Conference paper

Salzman M, Padron A, Clements D, Mazzarelli A, Robbins M, Braz V, Haroz Ret al., 2017, A survey of buprenorphine use and misuse among opioid users in the emergency department, Publisher: TAYLOR & FRANCIS LTD, Pages: 795-795, ISSN: 1556-3650

Conference paper

Ade PAR, Aghanim N, Arnaud M, Ashdown M, Aumont J, Baccigalupi C, Banday AJ, Barreiro RB, Bartolo N, Battaner E, Benabed K, Benoit-Levy A, Bernard J-P, Bersanelli M, Bielewicz P, Bonaldi A, Bonavera L, Bond JR, Borrill J, Bouchet FR, Burigana C, Butler RC, Calabrese E, Cardoso J-F, Catalano A, Chamballu A, Chiang HC, Christensen PR, Churazov E, Clements DL, Colombo LPL, Combet C, Comis B, Couchot F, Coulais A, Crill BP, Curto A, Cuttaia F, Danese L, Davies RD, Davis RJ, de Bernardis P, de Rosa A, de Zotti G, Delabrouille J, Dickinson C, Diego JM, Dolag K, Dole H, Donzelli S, Dore O, Douspis M, Ducout A, Dupac X, Efstathiou G, Elsner F, Ensslin TA, Eriksen HK, Finelli F, Forni O, Frailis M, Fraisse AA, Franceschi E, Galeotta S, Galli S, Gangal K, Giard M, Giraud-Heraud Y, Gjerlow E, Gonzalez-Nuevo J, Gorski KM, Gregorio A, Gruppuso A, Gudmundsson JE, Hansen FK, Harrison DL, Helou G, Hernandez-Monteagudo C, Herranz D, Hildebrandt SR, Hivon E, Hobson M, Hornstrup A, Hovest W, Huffenberger KM, Hurier G, Jaffe AH, Jaffe TR, Jones WC, Keihanen E, Keskitalo R, Kisner TS, Kneissl R, Knoche J, Kunz M, Kurki-Suonio H, Lagache G, Lamarre J-M, Lasenby A, Lattanzi M, Lawrence CR, Leonardi R, Levrier F, Liguori M, Lilje PB, Linden-Vornle M, Lopez-Caniego M, Lubin PM, Macias-Perez JF, Maffei B, Maggio G, Maino D, Mandolesi N, Mangilli A, Marcos-Caballero A, Maris M, Martin PG, Martinez-Gonzalez E, Masi S, Matarrese S, Mazzotta P, Meinhold PR, Melchiorri A, Mennella A, Migliaccio M, Mitra S, Miville-Deschenes M-A, Moneti A, Montier L, Morgante G, Mortlock D, Munshi D, Murphy JA, Naselsky P, Nati F, Natoli P, Noviello F, Novikov D, Novikov I, Oppermann N, Oxborrow CA, Pagano L, Pajot F, Paoletti D, Pasian F, Pearson TJ, Perdereau O, Perotto L, Pettorino V, Piacentini F, Piat M, Pierpaoli E, Plaszczynski S, Pointecouteau E, Polenta G, Ponthieu N, Pratt GW, Prunet S, Puget J-L, Rachen JP, Reinecke M, Remazeilles M, Renault C, Renzi A, Ristorcelli I, Rocha G, Rosset C, Rossetti M, Roudet al., 2016, Planck intermediate results XL. The Sunyaev-Zeldovich signal from the Virgo cluster, Astronomy and Astrophysics, Vol: 596, ISSN: 0004-6361

The Virgo cluster is the largest Sunyaev-Zeldovich (SZ) source in the sky, both in terms of angular size and total integrated flux. Planck’s wide angular scale and frequency coverage, together with its high sensitivity, enable a detailed study of this big object through the SZ effect. Virgo is well resolved by Planck, showing an elongated structure that correlates well with the morphology observed from X-rays, but extends beyond the observed X-ray signal. We find good agreement between the SZ signal (or Compton parameter, yc) observed by Planck and the expected signal inferred from X-ray observations and simple analytical models. Owing to its proximity to us, the gas beyond the virial radius in Virgo can be studied with unprecedented sensitivity by integrating the SZ signal over tens of square degrees. We study the signal in the outskirts of Virgo and compare it with analytical models and a constrained simulation of the environment of Virgo. Planck data suggest that significant amounts of low-density plasma surround Virgo, out to twice the virial radius. We find the SZ signal in the outskirts of Virgo to be consistent with a simple model that extrapolates the inferred pressure at lower radii, while assuming that the temperature stays in the keV range beyond the virial radius. The observed signal is also consistent with simulations and points to a shallow pressure profile in the outskirts of the cluster. This reservoir of gas at large radii can be linked with the hottest phase of the elusivewarm/hot intergalactic medium. Taking the lack of symmetry of Virgo into account, we find that a prolate model is favoured by the combination of SZ and X-ray data, in agreement with predictions. Finally, based on the combination of the same SZ and X-ray data, we constrain the total amount of gas in Virgo. Under the hypothesis that the abundance of baryons in Virgo is representative of the cosmic average, we also infer a distance for Virgo of approximately 18 Mpc, in g

Journal article

Ade PAR, Aghanim N, Aller HD, Aller MF, Arnaud M, Aumont J, Baccigalupi C, Banday AJ, Barreiro RB, Bartolo N, Battaner E, Benabed K, Benoit-Levy A, Bernard J-P, Bersanelli M, Bielewicz P, Bonaldi A, Bonavera L, Bond JR, Borrill J, Bouchet FR, Burigana C, Calabrese E, Catalano A, Chiang HC, Christensen PR, Clements DL, Colomb LPL, Couchot F, Crill BP, Curto A, Cuttaia F, Danese L, Davies RD, Davis RJ, de Bernardis P, de Rosa A, de Zotti G, Delabrouille J, Dickinson C, Diego JM, Dole H, Donzelli S, Dore O, Ducout A, Dupac X, Efstathiou G, Elsner F, Eriksen HK, Finelli F, Forni O, Frailis M, Fraisse AA, Franceschi E, Galeotta S, Galli S, Ganga K, Giard M, Giraud-Heraud Y, Gjerlow E, Gonzalez-Nuevo J, Gorski KM, Gruppuso A, Gurwel MA, Hansen FK, Harrison DL, Henrot-Versille S, Hernandez-Monteagudo C, Hildebrandt SR, Hobson M, Hornstrup A, Hovatta T, Hovest W, Huffenberger KM, Hurier G, Jaffe AH, Jaffe TR, Jarvela E, Keihanen E, Keskitalo R, Kisner TS, Kneiss R, Knoche J, Kunz M, Kurki-Suonio H, Lahteenmaki A, Lamarre J-M, Lasenby A, Lattanzi M, Lawrence CR, Leonardi R, Levrier F, Liguori M, Lilje PB, Linden-Vornle M, Lopez-Caniego M, Lubin PM, Macias-Perez JF, Maffei B, Maino D, Mandolesi N, Maris M, Martini PG, Martinez-Gonzalez E, Masi S, Matarrese S, Max-Moerbeck W, Meinhold PR, Melchiorri A, Mennella A, Migliaccio M, Millgaliev M, Miville-Deschenes M-A, Moneti A, Montier L, Morgante G, Mortlock D, Munshi D, Murphy JA, Nati F, Natoli P, Nieppola E, Noviello F, Novikov D, Novikov I, Pagano L, Pajot F, Paoletti D, Partridge B, Pasian F, Pearson TJ, Perdereau O, Perotto L, Pettorino V, Piacentini F, Piat M, Pierpaoli E, Plaszczynski S, Pointecouteau E, Polenta G, Pratt GW, Ramakrishnan V, Rastorgueva-Foi EA, Readhead ACS, Reinecke M, Remazeilles M, Renault C, Renzi A, Richards JL, Ristorcelli I, Rocha G, Rossetti M, Roudier G, Rubino-Martin JA, Rusholme B, Sandri M, Savelainen M, Savini G, Scott D, Sotnikova Y, Stolyarov V, Sunyaev R, Sutton D, Suur-Uski A-S, Sygnet J-Fet al., 2016, Planck intermediate results XLV. Radio spectra of northern extragalactic radio sources, Astronomy and Astrophysics, Vol: 596, ISSN: 0004-6361

Continuum spectra covering centimetre to submillimetre wavelengths are presented for a northern sample of 104 extragalactic radio sources, mainly active galactic nuclei, based on four-epoch Planck data. The nine Planck frequencies, from 30 to 857 GHz, are complemented by a set of simultaneous ground-based radio observations between 1.1 and 37 GHz. The single-survey Planck data confirm that the flattest high-frequency radio spectral indices are close to zero, indicating that the original accelerated electron energy spectrum is much harder than commonly thought, with power-law index around 1.5 instead of the canonical 2.5. The radio spectra peak at high frequencies and exhibit a variety of shapes. For a small set of low-z sources, we find a spectral upturn at high frequencies, indicating the presence of intrinsic cold dust. Variability can generally be approximated by achromatic variations, while sources with clear signatures of evolving shocks appear to be limited to the strongest outbursts.

Journal article

Ade PAR, Aghanim N, Ashdown M, Aumont J, Baccigalupi C, Banday AJ, Barreiro RB, Bartolo N, Basak S, Battaner E, Benabed K, Benoit-Levy A, Bernard J-P, Bersanelli M, Bielewicz P, Bock JJ, Bonaldi A, Bonavera L, Bond JR, Borrill J, Bouchet FR, Boulanger F, Burigana C, Butler RC, Calabrese E, Cardoso J-F, Catalano A, Chiang HC, Christensen PR, Clements DL, Colombi S, Colombo LPL, Combet C, Crill BP, Curto A, Cuttaia F, Danese L, Davis RJ, de Bernardis P, de Zotti G, Delabrouille J, Dickinson C, Diego JM, Dore O, Ducout A, Dupac X, Elsner F, Ensslin TA, Eriksen HK, Finelli F, Forni O, Frailis M, Fraisse AA, Franceschi E, Galeotta S, Galli S, Ganga K, Ghosh T, Giard M, Giraud-Heraud Y, Gjerlow E, Gonzalez-Nuevo J, Gorski KM, Gruppuso A, Gudmundsson JE, Harrison DL, Hernandez-Monteagudo C, Herranz D, Hildebrandt SR, Hornstrup A, Hovest W, Hurier G, Jaffe AH, Jones WC, Keihanen E, Keskitalo R, Kisner TS, Knoche J, Knox L, Kunz M, Kurki-Suonio H, Lagache G, Lahteenmaki A, Lamarre J-M, Lasenby A, Lattanzi M, Leonardi R, Levrier F, Lilje PB, Linden-Vornle M, Lopez-Caniego M, Lubin PM, Macias-Perez JF, Maffei B, Maggie G, Maino D, Mandolesi N, Mangilli A, Maris M, Martin PG, Martinez-Gonzalez E, Masi S, Matarrese S, Meinhold PR, Melchiorri A, Mennella A, Migliaccio M, Mitra S, Miville-Deschenes M-A, Moneti A, Montier L, Morgante G, Mortlock D, Moss A, Munshi D, Murphy JA, Naselsky P, Nati F, Natoli P, Netterfield CB, Norgaard-Nielsen HU, Novikov D, Novikov I, Pagano L, Pajot F, Paoletti D, Pasian F, Patanchon G, Perdereau O, Perotto L, Pettorino V, Piacentini F, Piat M, Pierpaoli E, Pointecouteau E, Polenta G, Pratt GW, Rachen JP, Reinecke M, Remazeilles M, Renault C, Renzi A, Ristorcelli I, Rocha G, Rosset C, Rossetti M, Roudier G, Rubino-Martin JA, Rusholme B, Sandri M, Santos D, Savelainen M, Savini G, Scott D, Spencer LD, Stolyarov V, Stompor R, Sudiwala R, Sunyaev R, Sutton D, Suur-Uski A-S, Sygnet J-F, Tauber JA, Terenzi L, Toffolatti L, Tomasi M, Tristram M, Tucci M, Tuet al., 2016, Planck intermediate results XLI. A map of lensing-induced B-modes., Astronomy and Astrophysics, Vol: 596, ISSN: 0004-6361

The secondary cosmic microwave background (CMB) B-modes stem from the post-decoupling distortion of the polarization E-modes due tothe gravitational lensing effect of large-scale structures. These lensing-induced B-modes constitute both a valuable probe of the dark matterdistribution and an important contaminant for the extraction of the primary CMB B-modes from inflation. Planck provides accurate nearly all-sky measurements of both the polarization E-modes and the integrated mass distribution via the reconstruction of the CMB lensing potential. Bycombining these two data products, we have produced an all-sky template map of the lensing-induced B-modes using a real-space algorithm that minimizes the impact of sky masks. The cross-correlation of this template with an observed (primordial and secondary) B-mode map can be used to measure the lensing B-mode power spectrum at multipoles up to 2000. In particular, when cross-correlating with the B-mode contribution directly derived from the Planck polarization maps, we obtain lensing-induced B-mode power spectrum measurement at a significance level of 12σ, which agrees with the theoretical expectation derived from the Planck best-fit Λ cold dark matter model. This unique nearly all-sky secondary B-mode template, which includes the lensing-induced information from intermediate to small (10 <∼ ` <∼ 1000) angular scales, is delivered as part of the Planck 2015 public data release. It will be particularly useful for experiments searching for primordial B-modes, such as BICEP2/Keck Array or LiteBIRD, since it will enable an estimate to be made of the lensing-induced contribution to the measured total CMB B-modes.

Journal article

Ade PAR, Aghanim N, Arnaud M, Aumont J, Baccigalupi C, Banday AJ, Barreiro RB, Bartolo N, Battaner E, Benabed K, Benoit-Levy A, Bernard J-P, Bersanelli M, Bielewicz P, Bonaldi A, Bonavera L, Bond JR, Borrill J, Bouchet FR, Boulanger F, Burigana C, Butler RC, Calabrese E, Catalano A, Chiang HC, Christensen PR, Clements DL, Colombo LPL, Couchot F, Coulais A, Crill BP, Curto A, Cuttaia F, Danese L, Davies RD, Davis RJ, de Bernardis P, de Rosa A, de Zotti G, Delabrouille J, Dickinson C, Diego JM, Dole H, Dore O, Douspis M, Ducout A, Dupac X, Elsner F, Ensslin TA, Eriksen HK, Falgarone E, Finelli F, Flores-Cacho I, Frailis M, Fraisse AA, Franceschi E, Galeotta S, Galli S, Ganga K, Giard M, Giraud-Heraud Y, Gjerlow E, Gonzalez-Nuevo J, Gorski KM, Gregorio A, Gruppuso A, Gudmundsson JE, Hansen FK, Harrison DL, Helou G, Hernandez-Monteagudo C, Herranz D, Hildebrandt SR, Hivon E, Hobson M, Hornstrup A, Hovest W, Huffenberger KM, Hurier G, Jaffe AH, Jaffe TR, Keihanen E, Keskitalo R, Kisner TS, Kneissl R, Knoche J, Kunz M, Kurki-Suonio H, Lagache G, Lamarre J-M, Lasenby A, Lattanzi M, Lawrence CR, Leonardi R, Levrier F, Liguori M, Lilje PB, Linden-Vornle M, Lopez-Caniego M, Lubin PM, Macias-Perez JF, Maffei B, Maggio G, Maino D, Mandolesi N, Mangilli A, Maris M, Martin PG, Martinez-Gonzalez E, Masi S, Matarrese S, Melchiorri A, Mennella A, Migliaccio M, Mitra S, Miville-Deschenes M-A, Moneti A, Montier L, Morgante G, Mortlock D, Munshi D, Murphy JA, Nati F, Natoli P, Nesvadba NPH, Noviello F, Novikov D, Novikov I, Oxborrow CA, Pagano L, Pajot F, Paoletti D, Partridge B, Pasian F, Pearson TJ, Perdereau O, Perotto L, Pettorino V, Piacentini F, Piat M, Plaszczynski S, Pointecouteau E, Polenta G, Pratt GW, Prunet S, Puget J-L, Rachen JP, Reinecke M, Remazeilles M, Renault C, Renzi A, Ristorcelli I, Rocha G, Rosset C, Rossetti M, Roudier G, Rubino-Martin JA, Rusholme B, Sandri M, Santos D, Savelainen M, Savini G, Scott D, Spencer LD, Stolyarov V, Stompor R, Sudiwala R, Sunyaev Ret al., 2016, <i>Planck</i> intermediate results XXXIX. The <i>Planck</i> list of high-redshift source candidates, Publisher: EDP SCIENCES S A

Working paper

Clements D, Lopez JC, Rachakonda S, Sedky K, Pumariega Aet al., 2016, Physical Pain, Opiate Prescription Medications, and Heroin Addiction: A Case Series, ADDICTIVE DISORDERS & THEIR TREATMENT, Vol: 15, Pages: 175-182, ISSN: 1531-5754

Journal article

Fu H, Hennawi JF, Prochaska JX, Mutel R, Casey C, Cooray A, Keres D, Zhang Z-Y, Clements D, Isbell J, Lang C, McGinnis D, Michalowski MJ, Mooley K, Perley D, Stockton A, Thompson Det al., 2016, The circumgalactic medium of submillimeter galaxies. I. First results from a radio-identified sample, Astrophysical Journal, Vol: 832, ISSN: 0004-637X

We present the first results from an ongoing survey to characterize the circumgalactic medium (CGM) of massive high-redshift galaxies detected as submillimeter galaxies (SMGs). We constructed a parent sample of 163 SMG–QSO pairs with separations less than ~36'' by cross-matching far-infrared-selected galaxies from Herschel with spectroscopically confirmed QSOs. The Herschel sources were selected to match the properties of the SMGs. We determined the sub-arcsecond positions of six Herschel sources with the Very Large Array and obtained secure redshift identification for three of those with near-infrared spectroscopy. The QSO sightlines probe transverse proper distances of 112, 157, and 198 kpc at foreground redshifts of 2.043, 2.515, and 2.184, respectively, which are comparable to the virial radius of the ~1013 M ⊙ halos expected to host SMGs. High-quality absorption-line spectroscopy of the QSOs reveals systematically strong H i Lyα absorption around all three SMGs, with rest-frame equivalent widths of ~2–3 Å. However, none of the three absorbers exhibit compelling evidence for optically thick H i gas or metal absorption, in contrast to the dominance of strong neutral absorbers in the CGM of luminous z ~ 2 QSOs. The low covering factor of optically thick H i gas around SMGs tentatively indicates that SMGs may not have as prominent cool gas reservoirs in their halos as the coeval QSOs and that they may inhabit less massive halos than previously thought.

Journal article

Ivison RJ, Lewis AJR, Weiss A, Arumugam V, Simpson JM, Holland WS, Maddox S, Dunne L, Valiante E, van der Werf P, Omont A, Dannerbauer H, Smail I, Bertoldi F, Bremer M, Bussmann RS, Cai Z-Y, Clements DL, Cooray A, De Zotti G, Eales SA, Fuller C, Gonzalez-Nuevo J, Ibar E, Negrello M, Oteo I, Perez-Fournon I, Riechers D, Stevens JA, Swinbank AM, Wardlow Jet al., 2016, The space density of luminous dusty star-forming galaxies at z>4: scuba-2 and laboca imaging of ultrared galaxies from herschel-atlas., Astrophysical Journal, Vol: 832, ISSN: 0004-637X

Until recently, only a handful of dusty, star-forming galaxies (DSFGs) were known at z > 4, most of them significantly amplified by gravitational lensing. Here, we have increased the number of such DSFGs substantially, selecting galaxies from the uniquely wide 250, 350, and 500 μm Herschel-ATLAS imaging survey on the basis of their extremely red far-infrared colors and faint 350 and 500 μm flux densities, based on which, they are expected to be largely unlensed, luminous, rare, and very distant. The addition of ground-based continuum photometry at longer wavelengths from the James Clerk Maxwell Telescope and the Atacama Pathfinder Experiment allows us to identify the dust peak in their spectral energy distributions (SEDs), with which we can better constrain their redshifts. We select the SED templates that are best able to determine photometric redshifts using a sample of 69 high-redshift, lensed DSFGs, then perform checks to assess the impact of the CMB on our technique, and to quantify the systematic uncertainty associated with our photometric redshifts, σ = 0.14 (1 + z), using a sample of 25 galaxies with spectroscopic redshifts, each consistent with our color selection. For Herschel-selected ultrared galaxies with typical colors of S 500/S 250 ~ 2.2 and S 500/S 350 ~ 1.3 and flux densities, S 500 ~ 50 mJy, we determine a median redshift, ${\hat{z}}_{\mathrm{phot}}=3.66$, an interquartile redshift range, 3.30–4.27, with a median rest-frame 8–1000 μm luminosity, ${\hat{L}}_{\mathrm{IR}}$, of 1.3 × 1013 L ⊙. A third of the galaxies lie at z > 4, suggesting a space density, ρ z > 4, of ≈6 × 10−7 Mpc−3. Our sample contains the most luminous known star-forming galaxies, and the most overdense cluster of starbursting proto-ellipticals found to date.

Journal article

Pearson C, Rigopoulou D, Hurley P, Farrah D, Afonso J, Bernard-Salas J, Borys C, Clements DL, Cormier D, Efstathiou A, Gonzalez-Alfonso E, Lebouteiller V, Spoon Het al., 2016, Herus: A CO atlas from spire spectroscopy of local ULIRGs, Astrophysical Journal Supplement Series, Vol: 227, ISSN: 0067-0049

We present the Herschel SPIRE Fourier Transform Spectroscopy (FTS) atlas for a complete flux-limited sample of local ultraluminous infrared galaxies (ULIRGs) as part of the HERschel Ultra Luminous InfraRed Galaxy Survey (HERUS). The data reduction is described in detail and was optimized for faint FTS sources ,with particular care being taken for the subtraction of the background, which dominates the continuum shape of the spectra. To improve the final spectra, special treatment in the data reduction has been given to any observation suffering from artifacts in the data caused by anomalous instrumental effects. Complete spectra are shown covering 200–671 μm, with photometry in the SPIRE bands at 250, 350, and 500 μm. The spectra include near complete CO ladders for over half of our sample, as well as fine structure lines from [C i] 370 μm, [C i] 609 μm, and [N ii] 205 μm. We also detect H2O lines in several objects. We construct CO spectral line energy distributions (SLEDs) for the sample, and compare their slopes with the far-infrared (FIR) colors and luminosities. We show that the CO SLEDs of ULIRGs can be broadly grouped into three classes based on their excitation. We find that the mid-J (5 < J < 8) lines are better correlated with the total FIR luminosity, suggesting that the warm gas component is closely linked to recent star formation. The higher J transitions do not linearly correlate with the FIR luminosity, consistent with them originating in hotter, denser gas that is unconnected to the current star formation. We conclude that in most cases more than one temperature component is required to model the CO SLEDs.

Journal article

Geach JE, Narayanan D, Matsuda Y, Hayes M, Mas-Ribas L, Dijkstra M, Steidel CC, Chapman SC, Feldmann R, Avison A, Agertz O, Ao Y, Birkinshaw M, Bremer MN, Clements DL, Dannerbauer H, Farrah D, Harrison CM, Kubo M, Michalowski MJ, Scott D, Smith DJB, Spaans M, Simpson JM, Swinbank AM, Taniguchi Y, van der Werf P, Verma A, Yamada Tet al., 2016, Alma observations of ly alpha blob 1: halo superstructure illuminated from within., Astrophysical Journal, Vol: 832, ISSN: 0004-637X

We present new Atacama Large Millimeter/Submillimeter Array (ALMA) 850 μm continuum observations of the original Lyα Blob (LAB) in the SSA22 field at z = 3.1 (SSA22-LAB01). The ALMA map resolves the previously identified submillimeter source into three components with a total flux density of S 850 = 1.68 ± 0.06 mJy, corresponding to a star-formation rate of ~150 M ⊙ yr−1. The submillimeter sources are associated with several faint (m ≈ 27 mag) rest-frame ultraviolet sources identified in Hubble Space Telescope Imaging Spectrograph (STIS) clear filter imaging (λ ≈ 5850 Å). One of these companions is spectroscopically confirmed with the Keck Multi-Object Spectrometer For Infra-Red Exploration to lie within 20 projected kpc and 250 km s−1 of one of the ALMA components. We postulate that some of these STIS sources represent a population of low-mass star-forming satellites surrounding the central submillimeter sources, potentially contributing to their growth and activity through accretion. Using a high-resolution cosmological zoom simulation of a 1013 M ⊙ halo at z = 3, including stellar, dust, and Lyα radiative transfer, we can model the ALMA+STIS observations and demonstrate that Lyα photons escaping from the central submillimeter sources are expected to resonantly scatter in neutral hydrogen, the majority of which is predicted to be associated with halo substructure. We show how this process gives rise to extended Lyα emission with similar surface brightness and morphology to observed giant LABs.

Journal article

Clements DL, Sato S, Fonseca AP, 2016, Cosmic sculpture: a new way to visualise the cosmic microwave background, EUROPEAN JOURNAL OF PHYSICS, Vol: 38, ISSN: 0143-0807

Journal article

Farrah D, Balokovic M, Stern D, Harris K, Kunimoto M, Walton DJ, Alexander DM, Arevalo P, Ballantyne DR, Bauer FE, Boggs S, Brandt WN, Brightman M, Christensen F, Clements DL, Craig W, Fabian A, Hailey C, Harrison F, Koss M, Lansbury GB, Luo B, Paine J, Petty S, Pitchford K, Ricci C, Zhang Wet al., 2016, The geometry of the infrared and x-ray obscurer in a dusty hyperluminous quasar, Astrophysical Journal, Vol: 831, ISSN: 0004-637X

We study the geometry of the active galactic nucleus (AGN) obscurer in IRAS 09104+4109, an IR-luminous, radio-intermediate FR-I source at z = 0.442, using infrared data from Spitzer and Herschel, X-ray data from NuSTAR, Swift, Suzaku, and Chandra, and an optical spectrum from Palomar. The infrared data imply a total rest-frame 1–1000 μm luminosity of 5.5 × 1046 erg s−1 and require both an AGN torus and a starburst model. The AGN torus has an anisotropy-corrected IR luminosity of 4.9 × 1046 erg s−1 and a viewing angle and half-opening angle both of approximately 36° from pole-on. The starburst has a star formation rate of (110 ± 34) M ⊙ yr−1 and an age of <50 Myr. These results are consistent with two epochs of luminous activity in IRAS 09104+4109: one approximately 150 Myr ago, and one ongoing. The X-ray data suggest a photon index of Γ sime 1.8 and a line-of-sight column density of N H sime 5 × 1023 cm−2. This argues against a reflection-dominated hard X-ray spectrum, which would have implied a much higher N H and luminosity. The X-ray and infrared data are consistent with a bolometric AGN luminosity of L bol ~ (0.5–2.5) × 1047 erg s−1. The X-ray and infrared data are further consistent with coaligned AGN obscurers in which the line of sight "skims" the torus. This is also consistent with the optical spectra, which show both coronal iron lines and broad lines in polarized but not direct light. Combining constraints from the X-ray, optical, and infrared data suggest that the AGN obscurer is within a vertical height of 20 pc, and a radius of 125 pc, of the nucleus.

Journal article

Smith MWL, Eales SA, De Looze I, Baes M, Bendo GJ, Bianchi S, Boquien M, Boselli A, Buat V, Ciesla L, Clemens M, Clements DL, Cooray AR, Cortese L, Davies JI, Fritz J, Gomez HL, Hughes TM, Karczewski OL, Lu N, Oliver SJ, Remy-Ruyer A, Spinoglio L, Viaene Set al., 2016, Far-reaching dust distribution in galaxy discs, Monthly Notices of the Royal Astronomical Society, Vol: 462, Pages: 331-344, ISSN: 0035-8711

In most studies of dust in galaxies, dust is only detected from its emission to approximately the optical radius of the galaxy. By combining the signal of 110 spiral galaxies observed as part of the Herschel Reference Survey, we are able to improve our sensitivity by an order of magnitude over that for a single object. Here we report the direct detection of dust from its emission that extends out to at least twice the optical radius. We find that the distribution of dust is consistent with an exponential at all radii with a gradient of ∼−1.7 dex R−125 . Our dust temperature declines linearly from ∼25 K in the centre to 15 K at R25 from where it remains constant out to ∼2.0 R25. The surface density of dust declines with radius at a similar rate to the surface density of stars but more slowly than the surface density of the star-formation rate. Studies based on dust extinction and reddening of high-redshift quasars have concluded that there are substantial amounts of dust in intergalactic space. By combining our results with the number counts and angular correlation function from the SDSS, we show that with Milky Way-type dust we can explain the reddening of the quasars by the dust within galactic discs alone. Given the uncertainties in the properties of any intergalactic dust, we cannot rule out its existence, but our results show that statistical investigations of the dust in galactic haloes that use the reddening of high-redshift objects must take account of the dust in galactic discs.

Journal article

Ade PAR, Aghanim N, Arnaud M, Arrojam F, Ashdown M, Aumont J, Baccigalupi C, Ballardini M, Banday AJ, Barreiro RB, Bartolo N, Basak S, Battaner E, Benabed K, Benoit A, Benoit-Levy A, Bernard J-P, Bersanelli M, Bielewicz P, Bock JJ, Bonaldi A, Bonavera L, Bond JR, Borrill J, Bouchet FR, Boulanger F, Bucher M, Burigana C, Butler RC, Calabrese E, Cardoso J-F, Catalano A, Challinor A, Chamballu A, Chiang HC, Christensen PR, Church S, Clements DL, Colombi S, Colombo LPL, Combet C, Couchot F, Coulais A, Crill BP, Curto A, Cuttaia F, Danese L, Davies RD, Davis RJ, de Bernardis P, de Rosa A, de Zotti G, Delabrouille J, Desert F-X, Diego JM, Dole H, Donzelli S, Dore O, Douspis M, Ducout A, Dupac X, Efstathiou G, Elsner F, Ensslin TA, Eriksen HK, Fergusson J, Finelli F, Forni O, Frailis M, Fraisse AA, Franceschi E, Frejsel A, Galeotta S, Galli S, Ganga K, Gauthier C, Ghosh T, Giard M, Giraud-Heraud Y, Gjerlow E, Gonzalez-Nuevo J, Gorski KM, Gratton S, Gregorio A, Gruppuso A, Gudmundsson JE, Hamann J, Hansen FK, Hanson D, Harrison DL, Heavens A, Helou G, Henrot-Versille S, Hernandez-Monteagudo C, Herranz D, Hildebrandt SR, Hivon E, Hobson M, Holmes WA, Hornstrup A, Hovest W, Huang Z, Huffenberger KM, Hurier G, Jaffe AH, Jaffe TR, Jones WC, Juvela M, Keihanen E, Keskitalo R, Kim J, Kisner TS, Knoche J, Kunz M, Kurki-Suonio H, Lacasa F, Lagache G, Lahteenmaki A, Lamarre J-M, Lasenby A, Lattanzi M, Lawrence CR, Leonardi R, Lesgourgues J, Levrier F, Lewis A, Liguori M, Lilje PB, Linden-Vornle M, Lopez-Caniego M, Lubin PM, Macias-Perez JF, Maggio G, Maino D, Mandolesi N, Mangilli A, Marinucci D, Maris M, Martin PG, Martinez-Gonzalez E, Masi S, Matarrese S, McGehee P, Meinhold PR, Melchiorri A, Mendes L, Mennella A, Migliaccio M, Mitra S, Miville-Deschenes M-A, Moneti A, Montier L, Morgante G, Mortlock D, Moss A, Munchmeyer M, Munshi D, Murphy JA, Naselsky P, Nati F, Natoli P, Netterfield CB, Norgaard-Nielsen HU, Noviello F, Novikov D, Novikov I, Oxborrow CA, Paci F, Pagano L, Pajotet al., 2016, Planck 2015 results XVII. Constraints on primordial non-Gaussianity, Astronomy and Astrophysics: a European journal, Vol: 594, ISSN: 0004-6361

The Planck full mission cosmic microwave background (CMB) temperature and E-mode polarization maps are analysed to obtain constraints on primordial non-Gaussianity (NG). Using three classes of optimal bispectrum estimators – separable template-fitting (KSW), binned, and modal – we obtain consistent values for the primordial local, equilateral, and orthogonal bispectrum amplitudes, quoting as our final result from temperature alone ƒlocalNL = 2.5 ± 5.7, ƒequilNL= -16 ± 70, , and ƒorthoNL = -34 ± 32 (68% CL, statistical). Combining temperature and polarization data we obtain ƒlocalNL = 0.8 ± 5.0, ƒequilNL= -4 ± 43, and ƒorthoNL = -26 ± 21 (68% CL, statistical). The results are based on comprehensive cross-validation of these estimators on Gaussian and non-Gaussian simulations, are stable across component separation techniques, pass an extensive suite of tests, and are consistent with estimators based on measuring the Minkowski functionals of the CMB. The effect of time-domain de-glitching systematics on the bispectrum is negligible. In spite of these test outcomes we conservatively label the results including polarization data as preliminary, owing to a known mismatch of the noise model in simulations and the data. Beyond estimates of individual shape amplitudes, we present model-independent, three-dimensional reconstructions of the Planck CMB bispectrum and derive constraints on early universe scenarios that generate primordial NG, including general single-field models of inflation, axion inflation, initial state modifications, models producing parity-violating tensor bispectra, and directionally dependent vector models. We present a wide survey of scale-dependent feature and resonance models, accounting for the “look elsewhere” effect in estimating the statistical significance of features. We also look for isocurvature NG, and find no signal, but we obtain constraints tha

Journal article

Aghanim N, Arnaud M, Ashdown M, Aumont J, Baccigalupi C, Banday AJ, Barreiro RB, Bartlett JG, Bartolo N, Battaner E, Benabed K, Benoît A, Benoit-Lévy A, Bernard J-P, Bersanelli M, Bielewicz P, Bock JJ, Bonaldi A, Bonavera L, Bond JR, Borrill J, Bouchet FR, Boulanger F, Bucher M, Burigana C, Butler RC, Calabrese E, Cardoso J-F, Catalano A, Challinor A, Chiang HC, Christensen PR, Clements DL, Colombo LPL, Combet C, Coulais A, Crill BP, Curto A, Cuttaia F, Danese L, Davies RD, Davis RJ, de Bernardis P, de Rosa A, de Zotti G, Delabrouille J, Désert F-X, Di Valentino E, Dickinson C, Diego JM, Dolag K, Dole H, Donzelli S, Doré O, Douspis M, Ducout A, Dunkley J, Dupac X, Efstathiou G, Elsner F, Enßlin TA, Eriksen HK, Fergusson J, Finelli F, Forni O, Frailis M, Fraisse AA, Franceschi E, Frejsel A, Galeotta S, Galli S, Ganga K, Gauthier C, Gerbino M, Giard M, Gjerløw E, González-Nuevo J, Górski KM, Gratton S, Gregorio A, Gruppuso A, Gudmundsson JE, Hamann J, Hansen FK, Harrison DL, Helou G, Henrot-Versillé S, Hernández-Monteagudo C, Herranz D, Hildebrandt SR, Hivon E, Holmes WA, Hornstrup A, Huffenberger KM, Hurier G, Jaffe AH, Jones WC, Juvela M, Keihänen E, Keskitalo R, Kiiveri K, Knoche J, Knox L, Kunz M, Kurki-Suonio H, Lagache G, Lähteenmäki A, Lamarre J-M, Lasenby A, Lattanzi M, Lawrence CR, Le Jeune M, Leonardi R, Lesgourgues J, Levrier F, Lewis A, Liguori M, Lilje PB, Lilley M, Linden-Vørnle M, Lindholm V, López-Caniego M, Macías-Pérez JF, Maffei B, Maggio G, Maino D, Mandolesi N, Mangilli A, Maris M, Martin PG, Martínez-González E, Masi S, Matarrese S, Meinhold PR, Melchiorri A, Migliaccio M, Millea M, Mitra S, Miville-Deschênes M-A, Moneti A, Montier L, Morgante G, Mortlock D, Mottet S, Munshi D, Murphy JA, Narimani A, Naselsky P, Nati F, Natoli P, Noviello F, Novikov D, Novikov I, Oxborrow CA, Paci F, Pagano L, Pajot F, Paoletti D, Partridge B, Pasian F, Patanchon G, Pearson TJ, Perdereau O, Perotto L, Pettorino V, Piacentini F, Piat M, Pierpaoli E, Pietrobon D Pet al., 2016, Planck 2015 results. XI. CMB power spectra, likelihoods, and robustness of parameters, Astronomy & Astrophysics, Vol: 594, ISSN: 0004-6361

This paper presents the Planck 2015 likelihoods, statistical descriptions of the 2-point correlationfunctions of the cosmic microwave background (CMB) temperature and polarization fluctuations that account for relevant uncertainties, both instrumental and astrophysical in nature. They are based on the same hybrid approach used for the previous release, i.e., a pixel-based likelihood at low multipoles (ℓ< 30) and a Gaussian approximation to the distribution of cross-power spectra at higher multipoles. The main improvements are the use of more and better processed data and of Planck polarization information, along with more detailed models of foregrounds and instrumental uncertainties. The increased redundancy brought by more than doubling the amount of data analysed enables further consistency checks and enhanced immunity to systematic effects. It also improves the constraining power of Planck, in particular with regard to small-scale foreground properties. Progress in the modelling of foreground emission enables the retention of a larger fraction of the sky to determine the properties of the CMB, which also contributes to the enhanced precision of the spectra. Improvements in data processing and instrumental modelling further reduce uncertainties. Extensive tests establish the robustness and accuracy of the likelihood results, from temperature alone, from polarization alone, and from their combination. For temperature, we also perform a full likelihood analysis of realistic end-to-end simulations of the instrumental response to the sky, which were fed into the actual data processing pipeline; this does not reveal biases from residual low-level instrumental systematics. Even with the increase in precision and robustness, the ΛCDM cosmological model continues to offer a very good fit to the Planck data. The slope of the primordial scalar fluctuations, ns, is confirmed smaller than unity at more than 5σ from Planck alone. We further validate the robustn

Journal article

Ade PAR, Aghanim N, Arnaud M, Ashdown M, Aumont J, Baccigalupi C, Banday AJ, Barreiro RB, Bartlett JG, Bartolo N, Battaner E, Battye R, Benabed K, Benoît A, Benoit-Lévy A, Bernard J-P, Bersanelli M, Bielewicz P, Bock JJ, Bonaldi A, Bonavera L, Bond JR, Borrill J, Bouchet FR, Boulanger F, Bucher M, Burigana C, Butler RC, Calabrese E, Cardoso J-F, Catalano A, Challinor A, Chamballu A, Chary R-R, Chiang HC, Chluba J, Christensen PR, Church S, Clements DL, Colombi S, Colombo LPL, Combet C, Coulais A, Crill BP, Curto A, Cuttaia F, Danese L, Davies RD, Davis RJ, de Bernardis P, de Rosa A, de Zotti G, Delabrouille J, Désert F-X, Di Valentino E, Dickinson C, Diego JM, Dolag K, Dole H, Donzelli S, Doré O, Douspis M, Ducout A, Dunkley J, Dupac X, Efstathiou G, Elsner F, Enßlin TA, Eriksen HK, Farhang M, Fergusson J, Finelli F, Forni O, Frailis M, Fraisse AA, Franceschi E, Frejsel A, Galeotta S, Galli S, Ganga K, Gauthier C, Gerbino M, Ghosh T, Giard M, Giraud-Héraud Y, Giusarma E, Gjerløw E, González-Nuevo J, Górski KM, Gratton S, Gregorio A, Gruppuso A, Gudmundsson JE, Hamann J, Hansen FK, Hanson D, Harrison DL, Helou G, Henrot-Versillé S, Hernández-Monteagudo C, Herranz D, Hildebrandt SR, Hivon E, Hobson M, Holmes WA, Hornstrup A, Hovest W, Huang Z, Huffenberger KM, Hurier G, Jaffe AH, Jaffe TR, Jones WC, Juvela M, Keihänen E, Keskitalo R, Kisner TS, Kneissl R, Knoche J, Knox L, Kunz M, Kurki-Suonio H, Lagache G, Lähteenmäki A, Lamarre J-M, Lasenby A, Lattanzi M, Lawrence CR, Leahy JP, Leonardi R, Lesgourgues J, Levrier F, Lewis A, Liguori M, Lilje PB, Linden-Vørnle M, López-Caniego M, Lubin PM, Macías-Pérez JF, Maggio G, Maino D, Mandolesi N, Mangilli A, Marchini A, Maris M, Martin PG, Martinelli M, Martínez-González E, Masi S, Matarrese S, McGehee P, Meinhold PR, Melchiorri A, Melin J-B, Mendes L, Mennella A, Migliaccio M, Millea M, Mitra S, Miville-Deschênes M-A, Moneti A, Montier L, Morgante G, Mortlock D, Moss A, Munshi D, Murphy JA, Naselsky P, Nati F, Natoli P, Netteet al., 2016, Planck 2015 results. XIII. Cosmological parameters, Astronomy & Astrophysics, Vol: 594, ISSN: 1432-0746

This paper presents cosmological results based on full-mission Planck observations of temperature and polarization anisotropies of the cosmic microwave background (CMB) radiation. Our results are in very good agreement with the 2013 analysis of the Planck nominal-mission temperature data, but with increased precision. The temperature and polarization power spectra are consistent with the standard spatially-flat 6-parameter ΛCDM cosmology with a power-law spectrum of adiabatic scalar perturbations (denoted “base ΛCDM” in this paper). From the Planck temperature data combined with Planck lensing, for this cosmology we find a Hubble constant, H0 = (67.8 ± 0.9) km s-1Mpc-1, a matter density parameter Ωm = 0.308 ± 0.012, and a tilted scalar spectral index with ns = 0.968 ± 0.006, consistent with the 2013 analysis. Note that in this abstract we quote 68% confidence limits on measured parameters and 95% upper limits on other parameters. We present the first results of polarization measurements with the Low Frequency Instrument at large angular scales. Combined with the Planck temperature and lensing data, these measurements give a reionization optical depth of τ = 0.066 ± 0.016, corresponding to a reionization redshift of . These results are consistent with those from WMAP polarization measurements cleaned for dust emission using 353-GHz polarization maps from the High Frequency Instrument. We find no evidence for any departure from base ΛCDM in the neutrino sector of the theory; for example, combining Planck observations with other astrophysical data we find Neff = 3.15 ± 0.23 for the effective number of relativistic degrees of freedom, consistent with the value Neff = 3.046 of the Standard Model of particle physics. The sum of neutrino masses is constrained to ∑ mν < 0.23 eV. The spatial curvature of our Universe is found to be very close to zero, with | ΩK | < 0.005. Adding

Journal article

Ade PAR, Aghanim N, Akrami Y, Aluri PK, Arnaud M, Ashdown M, Aumont J, Baccigalupi C, Banday AJ, Barreiro RB, Bartolo N, Basak S, Battaner E, Benabed K, Benoit A, Benoit-Levy A, Bernard J-P, Bersanelli M, Bielewicz P, Bock JJ, Bonaldi A, Bonavera L, Bond JR, Borrill J, Bouchet FR, Boulanger F, Bucher M, Burigana C, Butler RC, Calabrese E, Cardoso J-F, Casaponsa B, Catalano A, Challinor A, Chamballu A, Chiang HC, Christensen PR, Church S, Clements DL, Colombi S, Colombo LPL, Combet C, Contreras D, Couchot F, Coulais A, Crill BP, Cruz M, Curto A, Cuttaia F, Danese L, Davies RD, Davis RJ, de Bernardis P, de Rosa A, de Zotti G, Delabrouille J, Desert F-X, Diego JM, Dole H, Donzelli S, Dore O, Douspis M, Ducout A, Dupac X, Efstathiou G, Elsner F, Ensslin TA, Eriksen HK, Fantaye Y, Ferguson J, Fernandez-Cobos R, Finelli F, Forni O, Frailis M, Fraisse AA, Franceschi E, Frejsel A, Frolov A, Galeotta S, Galli S, Ganga K, Gauthier C, Ghosh T, Giard M, Giraud-Heraud Y, Gjerlow E, Gonzalez-Nuevo J, Gorski KM, Gratton S, Gregorio A, Gruppuso A, Gudmundsson JE, Hansen FK, Hanson D, Harrison DL, Henrot-Versille S, Hernandez-Monteagudo C, Herranz D, Hildebrandt SR, Hivon E, Hobson M, Holmes WA, Hornstrup A, Hovest W, Huang Z, Huffenberger KM, Hurier G, Jaffe AH, Jaffe TR, Jones WC, Juvela M, Keihanen E, Keskitalo R, Kim J, Kisner TS, Knoche J, Kunz M, Kurki-Suonio H, Lagache G, Lahteenmaki A, Lamarre J-M, Lasenby A, Lattanzi M, Lawrence CR, Leonardi R, Lesgourgues J, Levrier F, Liguori M, Lilje PB, Linden-Vornle M, Liu H, Lopez-Caniego M, Lubin PM, Macias-Perez JF, Maggio G, Maino D, Mandolesi N, Mangilli A, Marinucci D, Maris M, Martin PG, Martinez-Gonzalez E, Masi S, Matarrese S, McGehee P, Meinhold PR, Melchiorri A, Mendes L, Mennella A, Migliaccio M, Mikkelsen K, Mitra S, Miville-Deschenes M-A, Molinari D, Moneti A, Montier L, Morgante G, Mortlock D, Moss A, Munshi D, Murphy JA, Naselsky P, Nati F, Natoli P, Netterfield CB, Norgaard-Nielsen HU, Noviello F, Novikov D, Novikov Iet al., 2016, Planck 2015 results XVI. Isotropy and statistics of the CMB, ASTRONOMY & ASTROPHYSICS, Vol: 594, ISSN: 1432-0746

Journal article

Ade PAR, Aghanim N, Arnaud M, Ashdown M, Aumont J, Baccigalupi C, Banday AJ, Barreiro RB, Bartlett JG, Bartolo N, Battaner E, Benabed K, Benoit A, Benoit-Levy A, Bernard J-P, Bersanelli M, Bielewicz P, Bock JJ, Bonaldi A, Bonavera L, Bond JR, Borrill J, Bouchet FR, Boulanger F, Bucher M, Burigana C, Butler RC, Calabrese E, Cardoso J-F, Castex G, Catalano A, Challinor A, Chamballu A, Chiang HC, Christensen PR, Clements DL, Colombi S, Colombo LPL, Combet C, Couchot F, Coulais A, Crill BP, Curto A, Cuttaia F, Danese L, Davies RD, Davis RJ, de Bernardis P, de Rosa A, de Zotti G, Delabrouille J, Delouis J-M, Desert F-X, Dickinson C, Diego JM, Dolag K, Dole H, Donzelli S, Dore O, Douspis M, Ducout A, Dupac X, Efstathiou G, Elsner F, Ensslin TA, Eriksen HK, Fergusson J, Finelli F, Forni O, Frailis M, Fraisse AA, Franceschi E, Frejsel A, Galeotta S, Galli S, Ganga K, Ghosh T, Giard M, Giraud-Heraud Y, Gjerlow E, Gonzalez-Nuevo J, Gorski KM, Gratton S, Gregorio A, Gruppuso A, Gudmundsson JE, Hansen FK, Hanson D, Harrison DL, Henrot-Versille S, Hernandez-Monteagudo C, Herranz D, Hildebrandt SR, Hivon E, Hobson M, Holmes WA, Hornstrup A, Hovest W, Huffenberger KM, Hurier G, Jaffe AH, Jaffe TR, Jones WC, Juvela M, Karakei A, Keihanen E, Keskitalo R, Kiiveri K, Kisner TS, Kneissl R, Knoche J, Kunz M, Kurki-Suonio H, Lagache G, Lamarre J-M, Lasenby A, Lattanzi M, Lawrence CR, Leonardi R, Lesgourgues J, Levrier F, Liguori M, Lilje PB, Linden-Vornle M, Lindholm V, Lopez-Caniego M, Lubin PM, Macias-Perez JF, Maggio G, Maino D, Mandolesi N, Mangilli A, Maris M, Martin PG, Martinez-Gonzalez E, Masi S, Matarrese S, McGehee P, Meinhold PR, Melchiorri A, Melin J-B, Mendes L, Mennella A, Migliaccio M, Mitra S, Miville-Deschenes M-A, Moneti A, Montier L, Morgante G, Mortlock D, Moss A, Munshi D, Murphy JA, Naselsky P, Nati F, Natoli P, Netterfield CB, Norgaard-Nielsen HU, Noviello F, Novikov D, Novikov I, Oxborrow CA, Paci F, Pagano L, Pajot F, Paoletti D, Pasian F, Patanchon G, Pearson TJet al., 2016, Planck 2015 results XII. Full focal plane simulations, Astronomy and Astrophysics, Vol: 594, ISSN: 0004-6361

We present the 8th full focal plane simulation set (FFP8), deployed in support of the Planck 2015 results. FFP8 consists of 10 fiducial mission realizations reduced to 18 144 maps, together with the most massive suite of Monte Carlo realizations of instrument noise and CMB ever generated, comprising 104 mission realizations reduced to about 106 maps. The resulting maps incorporate the dominant instrumental, scanning, and data analysis effects, and the remaining subdominant effects will be included in future updates. Generated at a cost of some 25 million CPU-hours spread across multiple high-performance-computing (HPC) platforms, FFP8 is used to validate and verify analysis algorithms and their implementations, and to remove biases from and quantify uncertainties in the results of analyses of the real data.

Journal article

Ade PAR, Aghanim N, Arnaud M, Aumont J, Baccigalupi C, Banday AJ, Barreiro RB, Bartlett JG, Bartolo N, Battaner E, Benabed K, Benoit-Levy A, Bernard J-P, Bersanelli M, Bielewicz P, Bock JJ, Bonaldi A, Bonavera L, Bond JR, Borrill J, Bouchet FR, Burigana C, Butler RC, Calabrese E, Catalano A, Chamballu A, Chiang HC, Christensen PR, Churazov E, Clements DL, Colombo LPL, Combet C, Comis B, Couchot F, Coulais A, Crill BP, Curto A, Cuttaia F, Danese L, Davies RD, Davis RJ, de Bernardis P, de Rosa A, de Zotti G, Delabrouille J, Dickinson C, Diego JM, Dole H, Donzelli S, Dore O, Douspis M, Ducout A, Dupac X, Efstathiou G, Elsner F, Ensslin TA, Eriksen HK, Finelli F, Flores-Cacho I, Forni O, Frailis M, Fraisse AA, Franceschi E, Galeotta S, Galli S, Ganga K, Genova-Santos RT, Giard M, Giraud-Heraud Y, Gjerlow E, Gonzalez-Nuevo J, Gorski KM, Gregorio A, Gruppuso A, Gudmundsson JE, Hansen FK, Harrison DL, Helou G, Hernandez-Monteagudo C, Herranz D, Hildebrandt SR, Hivon E, Hobson M, Hornstrup A, Hovest W, Huffenberger KM, Hurier G, Jaffe AH, Jaffe TR, Jones WC, Keihanen E, Keskitalo R, Kisner TS, Kneissl R, Knoche J, Kunz M, Kurki-Suonio H, Lagache G, Lamarre J-M, Langer M, Lasenby A, Lattanzi M, Lawrence CR, Leonardi R, Levrier F, Lilje PB, Linden-Vornle M, Lopez-Caniego M, Lubin PM, Macias-Perez JF, Maffei B, Maggio G, Maino D, Mak DSY, Mandolesi N, Mangilli A, Maris M, Martin PG, Martinez-Gonzalez E, Masi S, Matarrese S, Melchiorri A, Mennella A, Migliaccio M, Mitra S, Miville-Deschenes M-A, Moneti A, Montier L, Morgante G, Mortlock D, Munshi D, Murphy JA, Nati F, Natoli P, Noviello F, Novikov D, Novikov I, Oxborrow CA, Paci F, Pagano L, Pajot F, Paoletti D, Partridge B, Pasian F, Pearson TJ, Perdereau O, Perotto L, Pettorino V, Piacentini F, Piat M, Pierpaoli E, Plaszczynski S, Pointecouteau E, Polenta G, Ponthieu N, Pratt GW, Prunet S, Puget J-L, Rachen JP, Reinecke M, Remazeilles M, Renault C, Renzi A, Ristorcelli I, Rocha G, Rosset C, Rossetti M, Roudier G, Rubino-Martiet al., 2016, Planck 2015 results XXIII. The thermal Sunyaev-Zeldovich effect-cosmic infrared background correlation, ASTRONOMY & ASTROPHYSICS, Vol: 594, ISSN: 0004-6361

We use Planck data to detect the cross-correlation between the thermal Sunyaev-Zeldovich (tSZ) effect and the infrared emission from the galaxies that make up the the cosmic infrared background (CIB). We first perform a stacking analysis towards Planck-confirmed galaxy clusters. We detect infrared emission produced by dusty galaxies inside these clusters and demonstrate that the infrared emission is about 50% more extended than the tSZ effect. Modelling the emission with a Navarro-Frenk-White profile, we find that the radial profile concentration parameter is c500 = 1.00+0.18-0.15 . This indicates that infrared galaxies in the outskirts of clusters have higher infrared flux than cluster-core galaxies. We also study the cross-correlation between tSZ and CIB anisotropies, following three alternative approaches based on power spectrum analyses: (i) using a catalogue of confirmed clusters detected in Planck data; (ii) using an all-sky tSZ map built from Planck frequency maps; and (iii) using cross-spectra between Planck frequency maps. With the three different methods, we detect the tSZ-CIB cross-power spectrum at significance levels of (i) 6σ; (ii) 3σ; and (iii) 4σ. We model the tSZ-CIB cross-correlation signature and compare predictions with the measurements. The amplitude of the cross-correlation relative to the fiducial model is AtSZ−CIB = 1.2 ± 0.3. This result is consistent with predictions for the tSZ-CIB cross-correlation assuming the best-fit cosmological model from Planck 2015 results along with the tSZ and CIB scaling relations.

Journal article

Adam R, Ade PAR, Aghanim N, Arnaud M, Ashdown M, Aumont J, Baccigalupi C, Banday AJ, Barreiro RB, Bartlett JG, Bartolo N, Basak S, Battaner E, Benabed K, Benoit A, Benoit-Levy A, Bernard J-P, Bersanelli M, Bielewicz P, Bock JJ, Bonaldi A, Bonavera L, Bond JR, Borrill J, Bouchet FR, Boulanger F, Bucher M, Burigana C, Butler RC, Calabrese E, Cardoso J-F, Casaponsa B, Castex G, Catalano A, Challinor A, Chamballu A, Chary R-R, Chiang HC, Christensen PR, Clements DL, Colombi S, Colombo LPL, Combet C, Couchot F, Coulais A, Crill BP, Curto A, Cuttaia F, Danese L, Davies RD, Davis RJ, de Bernardis P, de Rosa A, de Zotti G, Delabrouille J, Desert F-X, Dickinson C, Diego JM, Dole H, Donzelli S, Dore O, Douspis M, Ducout A, Dupac X, Efstathiou G, Elsner F, Ensslin TA, Eriksen HK, Falgarone E, Fantaye Y, Fergusson J, Finelli F, Forni O, Frailis M, Fraisse AA, Francescht E, Frejsel A, Galeotta S, Galli S, Ganga K, Ghosh T, Giard M, Giraud-Heraud Y, Gjerlow E, Gonzalez-Nuevo J, Gorski KM, Gratton S, Gregorio A, Gruppuso A, Gudmundsson JE, Hansen FK, Hanson D, Harrison DL, Helou G, Henrot-Versille S, Hernandez-Monteagudo C, Herranz D, Hildebrandt SR, Hivon E, Hobson M, Holmes WA, Hornstrup A, Hovest W, Huffenberger KM, Hurier G, Jaffe AH, Jaffe TR, Jones WC, Juvela M, Keihanen E, Keskitalo R, Kisner TS, Kneissl R, Knoche J, Krachmalnicoff N, Kunz M, Kurki-Suonio H, Lagache G, Lamarre J-M, Lasenby A, Lattanzi M, Lawrence CR, Le Jenne M, Leonardi R, Lesgourgues J, Levrier F, Liguori M, Lilje PB, Linden-Vornle M, Lopez-Caniego M, Lubin PM, Macias-Perez JF, Maggio G, Maino D, Mandolesi N, Mangilli A, Maris M, Marshall DJ, Martin PG, Martinez-Gonzalez E, Masi S, Matarrese S, McGehee P, Meinhold PR, Melchiorri A, Mendes L, Mennella A, Migliaccio M, Mitra S, Miville-Deschenes M-A, Molinari D, Moneti A, Montier L, Morgante G, Mortlock D, Moss A, Munshi D, Murphy JA, Naselsky P, Nati F, Natoli P, Netterfield CB, Norgaard-Nielsen HU, Noviello F, Novikov D, Novikov I, Oxborrow CA, Paci F, Paet al., 2016, Planck 2015 results IX. Diffuse component separation: CMB maps, Astronomy and Astrophysics, Vol: 594, ISSN: 0004-6361

We present foreground-reduced cosmic microwave background (CMB) maps derived from the full Planck data set in both temperature and polarization. Compared to the corresponding Planck 2013 temperature sky maps, the total data volume is larger by a factor of 3.2 for frequencies between 30 and 70 GHz, and by 1.9 for frequencies between 100 and 857 GHz. In addition, systematic errors in the forms of temperature-to-polarization leakage, analogue-to-digital conversion uncertainties, and very long time constant errors have been dramatically reduced, to the extent that the cosmological polarization signal may now be robustly recovered on angular scales ℓ ≳ 40. On the very largest scales, instrumental systematic residuals are still non-negligible compared to the expected cosmological signal, and modes with ℓ< 20 are accordingly suppressed in the current polarization maps by high-pass filtering. As in 2013, four different CMB component separation algorithms are applied to these observations, providing a measure of stability with respect to algorithmic and modelling choices. The resulting polarization maps have rms instrumental noise ranging between 0.21 and 0.27μK averaged over 55′ pixels, and between 4.5 and 6.1μK averaged over pixels. The cosmological parameters derived from the analysis of temperature power spectra are in agreement at the 1σ level with the Planck 2015 likelihood. Unresolved mismatches between the noise properties of the data and simulations prevent a satisfactory description of the higher-order statistical properties of the polarization maps. Thus, the primary applications of these polarization maps are those that do not require massive simulations for accurate estimation of uncertainties, for instance estimation of cross-spectra and cross-correlations, or stacking analyses. However, the amplitude of primordial non-Gaussianity is consistent with zero within 2σ for all local, equilateral, and orthogonal configuration

Journal article

Adam R, Ade PAR, Aghanim N, Akrami Y, Alves MIR, Argüeso F, Arnaud M, Arroja F, Ashdown M, Aumont J, Baccigalupi C, Ballardini M, Banday AJ, Barreiro RB, Bartlett JG, Bartolo N, Basak S, Battaglia P, Battaner E, Battye R, Benabed K, Benoît A, Benoit-Lévy A, Bernard J-P, Bersanelli M, Bertincourt B, Bielewicz P, Bikmaev I, Bock JJ, Böhringer H, Bonaldi A, Bonavera L, Bond JR, Borrill J, Bouchet FR, Boulanger F, Bucher M, Burenin R, Burigana C, Butler RC, Calabrese E, Cardoso J-F, Carvalho P, Casaponsa B, Castex G, Catalano A, Challinor A, Chamballu A, Chary R-R, Chiang HC, Chluba J, Chon G, Christensen PR, Church S, Clemens M, Clements DL, Colombi S, Colombo LPL, Combet C, Comis B, Contreras D, Couchot F, Coulais A, Crill BP, Cruz M, Curto A, Cuttaia F, Danese L, Davies RD, Davis RJ, de Bernardis P, de Rosa A, de Zotti G, Delabrouille J, Delouis J-M, Désert F-X, Di Valentino E, Dickinson C, Diego JM, Dolag K, Dole H, Donzelli S, Doré O, Douspis M, Ducout A, Dunkley J, Dupac X, Efstathiou G, Eisenhardt PRM, Elsner F, Enßlin TA, Eriksen HK, Falgarone E, Fantaye Y, Farhang M, Feeney S, Fergusson J, Fernandez-Cobos R, Feroz F, Finelli F, Florido E, Forni O, Frailis M, Fraisse AA, Franceschet C, Franceschi E, Frejsel A, Frolov A, Galeotta S, Galli S, Ganga K, Gauthier C, Génova-Santos RT, Gerbino M, Ghosh T, Giard M, Giraud-Héraud Y, Giusarma E, Gjerløw E, González-Nuevo J, Górski KM, Grainge KJB, Gratton S, Gregorio A, Gruppuso A, Gudmundsson JE, Hamann J, Handley W, Hansen FK, Hanson D, Harrison DL, Heavens A, Helou G, Henrot-Versillé S, Hernández-Monteagudo C, Herranz D, Hildebrandt SR, Hivon E, Hobson M, Holmes WA, Hornstrup A, Hovest W, Huang Z, Huffenberger KM, Hurier G, Ilić S, Jaffe AH, Jaffe TR, Jin T, Jones WC, Juvela M, Karakci A, Keihänen E, Keskitalo R, Khamitov I, Kiiveri K, Kim J, Kisner TS, Kneissl R, Knoche J, Knox L, Krachmalnicoff N, Kunz M, Kurki-Suonio H, Lacasa F, Lagache G, Lähteenmäki A, Lamarre J-M, Langer M, Lasenby A, Lattanzi M, Lawrence CR, Leet al., 2016, Planck 2015 results. I. Overview of products and scientific results, Astronomy & Astrophysics, Vol: 594, ISSN: 1432-0746

The European Space Agency’s Planck satellite, which is dedicated to studying the early Universe and its subsequent evolution, was launched on 14 May 2009. It scanned the microwave and submillimetre sky continuously between 12 August 2009 and 23 October 2013. In February 2015, ESA and the Planck Collaboration released the second set of cosmology products based ondata from the entire Planck mission, including both temperature and polarization, along with a set of scientific and technical papers and a web-based explanatory supplement. This paper gives an overview of the main characteristics of the data and the data products in the release, as well as the associated cosmological and astrophysical science results and papers. The data products include maps of the cosmic microwave background (CMB), the thermal Sunyaev-Zeldovich effect, diffuse foregrounds in temperature and polarization, catalogues of compact Galactic and extragalactic sources (including separate catalogues of Sunyaev-Zeldovich clusters and Galactic cold clumps), and extensive simulations of signals and noise used in assessing uncertainties and the performance of the analysis methods. The likelihood code used to assess cosmological models against the Planck data is described, along with a CMB lensing likelihood. Scientific results include cosmological parameters derived from CMB power spectra, gravitational lensing, and cluster counts, as well as constraints on inflation, non-Gaussianity, primordial magnetic fields, dark energy, and modified gravity, and new results on low-frequency Galactic foregrounds.

Journal article

Ade PAR, Aghanim N, Arnaud M, Arroja F, Ashdown M, Aumont J, Baccigalupi C, Ballardini M, Banday AJ, Barreiro RB, Bartolo N, Battaner E, Benabed K, Benoit A, Benoit-Levy A, Bernard J-P, Bersanelli M, Bielewicz P, Bock JJ, Bonaldi A, Bonavera L, Bondi JR, Borrillu J, Bouchet FR, Boulanger F, Bucher M, Burigana C, Butler RC, Calabrese E, Cardoso J-F, Catalano A, Challinor A, Chamballu A, Chary R-R, Chiang HC, Christensen PR, Churchl S, Clements DL, Colombi S, Colombo LPL, Combet C, Contreras D, Couchot F, Coulais A, Crill BP, Curto A, Cuttaia F, Danese L, Davies RD, Davis RJ, de Bernardis P, de Rosa A, de Zotti G, Delabrouillei J, Desert F-X, Diego JM, Dole H, Donzelli S, Dore O, Douspis M, Ducout A, Dupac X, Efstathiou G, Elsner F, Ensslin TA, Eriksen HK, Fergusson J, Finelli F, Forni O, Frailis M, Fraisse AA, Franceschi E, Frejsel A, Frolov A, Galeotta S, Galli S, Ganga K, Gauthier C, Giard M, Giraud-Heraud Y, Gjerlow E, Gonzalez-Nuevo J, Gorski KM, Gratton S, Gregorio A, Gruppuso A, Gudmundsson JE, Hamann J, Handley W, Hansen FK, Hanson D, Harrison DL, Henrot-Versille S, Hernandez-Monteagudo C, Herranz D, Hildebrandt SR, Hivon E, Hobson M, Holmes WA, Hornstrup A, Hovest W, Huang Z, Huffenberger KM, Hurier G, Jaffe AH, Jaffe TR, Jones WC, Juvela M, Keihanen E, Keskitalo R, Kim J, Kisner TS, Kneissl R, Knoche J, Kunz M, Kurki-Suonio H, Lagache G, Lahteenmaki A, Lamarre J-M, Lasenby A, Lattanzi M, Lawrence CR, Leonardi R, Lesgourgues J, Levrier F, Lewis A, Liguori M, Lilje PB, Linden-Vornle M, Lopez-Caniego M, Lubin PM, Ma Y-Z, Macias-Perez JF, Maggio G, Maino D, Mandolesi N, Mangilli A, Maris M, Martini PG, Martinez-Gonzalez E, Masi S, Matarrese S, McGehee P, Meinhold PR, Melchiorri A, Mendes L, Mennella A, Migliaccio M, Mitra S, Miville-Deschenes M-A, Molinari D, Moneti A, Montier L, Morgante G, Mortlock D, Moss A, Munchmeyer M, Munshi D, Murphy JA, Naselsky P, Nati F, Natoli P, Netterfield CB, Norgaard-Nielsen HU, Noviello F, Novikov D, Novikov I, Oxborrow CA, Paciet al., 2016, Planck 2015 results XX. Constraints on inflation, Astronomy and Astrophysics, Vol: 594, ISSN: 0004-6361

We present the implications for cosmic inflation of the Planck measurements of the cosmic microwave background (CMB) anisotropies in both temperature and polarization based on the full Planck survey, which includes more than twice the integration time of the nominal survey used for the 2013 release papers. The Planck full mission temperature data and a first release of polarization data on large angular scales measure the spectral index of curvature perturbations to be ns = 0.968 ± 0.006 and tightly constrain its scale dependence to dns/ dlnk = −0.003 ± 0.007 when combined with the Planck lensing likelihood. When the Planck high-ℓ polarization data are included, the results are consistent and uncertainties are further reduced. The upper bound on the tensor-to-scalar ratio is r0.002< 0.11 (95% CL). This upper limit is consistent with the B-mode polarization constraint r< 0.12 (95% CL) obtained from a joint analysis of the BICEP2/Keck Array and Planck data. These results imply that V(φ) ∝ φ2 and natural inflation are now disfavoured compared to models predicting a smaller tensor-to-scalar ratio, such as R2 inflation. We search for several physically motivated deviations from a simple power-law spectrum of curvature perturbations, including those motivated by a reconstruction of the inflaton potential not relying on the slow-roll approximation. We find that such models are not preferred, either according to a Bayesian model comparison or according to a frequentist simulation-based analysis. Three independent methods reconstructing the primordial power spectrum consistently recover a featureless and smooth over the range of scales 0.008 Mpc-1 ≲ k ≲ 0.1 Mpc-1. At large scales, each method finds deviations from a power law, connected to a deficit at multipoles ℓ ≈ 20−40 in the temperature power spectrum, but at an uncompelling statistical significance owing to the large cosmic variance present at these multipoles. By comb

Journal article

Collaboration P, Ade PAR, Aghanim N, Arnaud M, Ashdown M, Aumont J, Baccigalupi C, Banday AJ, Barreiro RB, Bartolo N, Battaner E, Benabed K, Benoît A, Benoit-Lévy A, Bernard J-P, Bersanelli M, Bielewicz P, Bonaldi A, Bonavera L, Bond JR, Borrill J, Bouchet FR, Boulanger F, Bucher M, Burigana C, Butler RC, Calabrese E, Catalano A, Chamballu A, Chiang HC, Christensen PR, Clements DL, Colombi S, Colombo LPL, Combet C, Couchot F, Coulais A, Crill BP, Curto A, Cuttaia F, Danese L, Davies RD, Davis RJ, Bernardis PD, Rosa AD, Zotti GD, Delabrouille J, Désert F-X, Dickinson C, Diego JM, Dole H, Donzelli S, Doré O, Douspis M, Ducout A, Dupac X, Efstathiou G, Elsner F, Enßlin TA, Eriksen HK, Falgarone E, Fergusson J, Finelli F, Forni O, Frailis M, Fraisse AA, Franceschi E, Frejsel A, Galeotta S, Galli S, Ganga K, Giard M, Giraud-Héraud Y, Gjerløw E, González-Nuevo J, Górski KM, Gratton S, Gregorio A, Gruppuso A, Gudmundsson JE, Hansen FK, Hanson D, Harrison DL, Helou G, Henrot-Versillé S, Hernández-Monteagudo C, Herranz D, Hildebrandt SR, Hivon E, Hobson M, Holmes WA, Hornstrup A, Hovest W, Huffenberger KM, Hurier G, Jaffe AH, Jaffe TR, Jones WC, Juvela M, Keihänen E, Keskitalo R, Kisner TS, Knoche J, Kunz M, Kurki-Suonio H, Lagache G, Lamarre J-M, Lasenby A, Lattanzi M, Lawrence CR, Leonardi R, Lesgourgues J, Levrier F, Liguori M, Lilje PB, Linden-Vørnle M, López-Caniego M, Lubin PM, Macías-Pérez JF, Maggio G, Maino D, Mandolesi N, Mangilli A, Marshall DJ, Martin PG, Martínez-González E, Masi S, Matarrese S, Mazzotta P, McGehee P, Melchiorri A, Mendes L, Mennella A, Migliaccio M, Mitra S, Miville-Deschênes M-A, Moneti A, Montier L, Morgante G, Mortlock D, Moss A, Munshi D, Murphy JA, Naselsky P, Nati F, Natoli P, Netterfield CB, Nørgaard-Nielsen HU, Noviello F, Novikov D, Novikov I, Oxborrow CA, Paci F, Pagano L, Pajot F, Paladini R, Paoletti D, Pasian F, Patanchon G, Pearson TJ, Pelkonen V-M, Perdereau O, Perotto L, Perrotta F, Pettorino V, Piacentini F, Piat M, Pierpaoli Eet al., 2016, Planck 2015 results. XXVIII. The Planck Catalogue of Galactic Cold Clumps, Astronomy & Astrophysics, Vol: 594, ISSN: 1432-0746

We present the Planck Catalogue of Galactic Cold Clumps (PGCC), an all-skycatalogue of Galactic cold clump candidates detected by Planck. This catalogueis the full version of the Early Cold Core (ECC) catalogue, which was madeavailable in 2011 with the Early Release Compact Source Catalogue (ERCSC) andcontained 915 high S/N sources. It is based on the Planck 48 months missiondata that are currently being released to the astronomical community. The PGCCcatalogue is an observational catalogue consisting exclusively of Galactic coldsources. The three highest Planck bands (857, 545, 353 GHz) have been combinedwith IRAS data at 3 THz to perform a multi-frequency detection of sourcescolder than their local environment. After rejection of possible extragalacticcontaminants, the PGCC catalogue contains 13188 Galactic sources spread acrossthe whole sky, i.e., from the Galactic plane to high latitudes, following thespatial distribution of the main molecular cloud complexes. The mediantemperature of PGCC sources lies between 13 and 14.5 K, depending on thequality of the flux density measurements, with a temperature ranging from 5.8to 20 K after removing sources with the 1% largest temperature estimates. Usingseven independent methods, reliable distance estimates have been obtained for5574 sources, which allows us to derive their physical properties such as theirmass, physical size, mean density and luminosity. The PGCC sources are locatedmainly in the solar neighbourhood, up to a distance of 10.5 kpc towards theGalactic centre, and range from low-mass cores to large molecular clouds.Because of this diversity and because the PGCC catalogue contains sources invery different environments, the catalogue is useful to investigate theevolution from molecular clouds to cores. Finally, the catalogue also includes54 additional sources located in the SMC and LMC.

Journal article

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