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Publication Open Access A 1.9 Earth Radius Rocky Planet and the Discovery of a Non-transiting Planet in the Kepler-20 System(2016) ;Buchhave, Lars A. ;Dressing, Courtney D. ;Dumusque, Xavier ;Rice, Ken ;Vanderburg, Andrew ;Mortier, Annelies ;Lopez-Morales, Mercedes ;Lopez, Eric ;Lundkvist, Mia S. ;Kjeldsen, Hans; ; ;Charbonneau, David ;Collier Cameron, Andrew; ;Figueira, Pedro ;Fiorenzano, Aldo F. M.; ;Haywood, Raphaëlle D. ;Johnson, John Asher ;Latham, David W. ;Lovis, Christophe; ;Mayor, Michel; ; ;Motalebi, Fatemeh; ;Pepe, Francesco ;Phillips, David F. ;Piotto, Giampaolo ;Pollacco, Don ;Queloz, Didier ;Sasselov, Dimitar ;Ségransan, Damien; ;Udry, StéphaneWatson, ChrisKepler-20 is a solar-type star (V = 12.5) hosting a compact system of five transiting planets, all packed within the orbital distance of Mercury in our own solar system. A transition from rocky to gaseous planets with a planetary transition radius of ∼1.6 R_E has recently been proposed by several articles in the literature. Kepler-20b (R_p ∼ 1.9 R_E) has a size beyond this transition radius; however, previous mass measurements were not sufficiently precise to allow definite conclusions to be drawn regarding its composition. We present new mass measurements of three of the planets in the Kepler-20 system that are facilitated by 104 radial velocity measurements from the HARPS-N spectrograph and 30 archival Keck/HIRES observations, as well as an updated photometric analysis of the Kepler data and an asteroseismic analysis of the host star (M_star = 0.948+/- 0.051 M☉ and R_star = 0.964+/- 0.018 R☉). Kepler-20b is a 1.868_(-0.034)^(+0.066) R_E planet in a 3.7 day period with a mass of 9.70_(-1.44)^(+1.41) M_E, resulting in a mean density of 8.2_(-1.3)^(+1.5) g/cm^3, indicating a rocky composition with an iron-to-silicate ratio consistent with that of the Earth. This makes Kepler-20b the most massive planet with a rocky composition found to date. Furthermore, we report the discovery of an additional non-transiting planet with a minimum mass of 19.96_(-3.61)^(+3.08) M_E and an orbital period of ∼34 days in the gap between Kepler-20f (P ∼ 11 days) and Kepler-20d (P ∼ 78 days). -- Based on observations made with the Italian Telescopio Nazionale Galileo (TNG) operated on the island of La Palma by the Fundación Galileo Galilei of the INAF (Istituto Nazionale di Astrofísica) at the Spanish Observatorio del Roque de los Muchachos of the Instituto de Astrofísica de Canarias.Scopus© Citations 70 245 113 - Some of the metrics are blocked by yourconsent settings
Publication Metadata only 233 - Some of the metrics are blocked by yourconsent settings
Publication Open Access 10.4 m GTC observations of the nearby VHE-detected GRB 190829A/SN 2019oyw(2021) ;Hu, Y. -D. ;Castro-Tirado, A. J. ;Kumar, A. ;Gupta, R. ;Valeev, A. F. ;Pandey, S. B. ;Kann, D. A. ;Castellón, A. ;Agudo, I. ;Aryan, A. ;Caballero-García, M. D. ;Guziy, S. ;Martin-Carrillo, A. ;Oates, S. R.; ; ;Sokolov, V. V.Zhang, B. -B.Aims: Gamma-ray burst (GRB) 190829A (z = 0.0785) was detected by Fermi and Swift and also at very high energy (VHE) by the High-Energy Stereoscopic System (H.E.S.S.) telescopes. The prompt emission displayed two emission episodes separated by a quiescent gap of ∼40 s. We present the 10.4 m Gran Telescopio Canarias (GTC) observations of the afterglow of GRB 190829A and its underlying supernova. We also compare GRB 190829A to GRB 180728A, a GRB with similar behaviour, and discuss the implications on underlying physical mechanisms producing these two GRBs.
Methods: We present multi-band photometric data along with spectroscopic follow-up observations taken with the 10.4 m GTC telescope. Together with the data from the prompt emission, the 10.4 m GTC data are used to understand the emission mechanisms and possible progenitor.
Results: A detailed analysis of the multi-band observations of the afterglow requires the cooling frequency to pass between the optical and X-ray bands at early epochs. The afterglow then transitions to the underlying supernova (SN) 2019oyw, which dominates later on.
Conclusions: Although the prompt emission temporal properties of GRB 190829A and GRB 180728A are similar, the two pulses are different in the spectral domain. We find that SN 2019oyw associated with GRB 190829A is powered by Ni decay and is a Type Ic-BL SN. The spectroscopic and photometric properties of this SN are consistent with those observed for SN 1998bw, but evolved earlier.The reduced spectra are only available at the CDS via anonymous ftp to http://cdsarc.u-strasbg.fr (ftp://130.79.128.5) or via http://cdsarc.u-strasbg.fr/viz-bin/cat/J/A+A/646/A50
Scopus© Citations 41 158 53 - Some of the metrics are blocked by yourconsent settings
Publication Open Access An 11 Earth-mass, Long-period Sub-Neptune Orbiting a Sun-like Star(2019) ;Mayo, Andrew W. ;Rajpaul, Vinesh M. ;Buchhave, Lars A. ;Dressing, Courtney D. ;Mortier, Annelies ;Zeng, Li ;Fortenbach, Charles D. ;Aigrain, Suzanne; ;Collier Cameron, Andrew ;Charbonneau, David ;Coffinet, Adrien; ; ;Dumusque, Xavier ;Martinez Fiorenzano, A. F. ;Haywood, Raphaëlle D. ;Latham, David W. ;López-Morales, Mercedes; ; ; ;Pearce, Logan ;Pepe, Francesco ;Phillips, David ;Piotto, Giampaolo; ;Rice, Ken; Udry, StephaneAlthough several thousands of exoplanets have now been detected and characterized, observational biases have led to a paucity of long-period, low-mass exoplanets with measured masses and a corresponding lag in our understanding of such planets. In this paper we report the mass estimation and characterization of the long-period exoplanet Kepler-538b. This planet orbits a Sun-like star (V = 11.27) with {M}* ={0.892}-0.035+0.051 M ☉ and {R}* ={0.8717}-0.0061+0.0064 R ☉. Kepler-538b is a {2.215}-0.034+0.040 R ⊕ sub-Neptune with a period of P = 81.73778 ± 0.00013 days. It is the only known planet in the system. We collected radial velocity (RV) observations with the High Resolution Echelle Spectrometer (HIRES) on Keck I and High Accuracy Radial velocity Planet Searcher in North hemisphere (HARPS-N) on the Telescopio Nazionale Galileo (TNG). We characterized stellar activity by a Gaussian process with a quasi-periodic kernel applied to our RV and cross-correlation function FWHM observations. By simultaneously modeling Kepler photometry, RV, and FWHM observations, we found a semi-amplitude of K={1.68}-0.38+0.39 m s-1 and a planet mass of {M}p={10.6}-2.4+2.5 M ⊕. Kepler-538b is the smallest planet beyond P = 50 days with an RV mass measurement. The planet likely consists of a significant fraction of ices (dominated by water ice), in addition to rocks/metals, and a small amount of gas. Sophisticated modeling techniques such as those used in this paper, combined with future spectrographs with ultra high-precision and stability will be vital for yielding more mass measurements in this poorly understood exoplanet regime. This in turn will improve our understanding of the relationship between planet composition and insolation flux and how the rocky to gaseous transition depends on planetary equilibrium temperature.Scopus© Citations 16 185 55 - Some of the metrics are blocked by yourconsent settings
Publication Open Access The 11 yr of low activity of the magnetar XTE J1810-197(2019); ; ; ;Turolla, Roberto; ;Rea, Nanda; In 2003, the magnetar XTE J1810-197 started an outburst that lasted until early 2007. In the following 11 yr, the source stayed in a quiescent/low-activity phase. XTE J1810-197 is one of the closest magnetars, hence its X-ray properties can be studied in detail even in quiescence and an extended monitoring has been carried out to study its long-term timing and spectral evolution. Here, we report the results of new X-ray observations, taken between 2017 September and 2018 April, with XMM-Newton, Chandra, and NICER. We derived a phase-connected timing solution yielding a frequency derivative of -9.26(6) × 10-14 Hz s-1. This value is consistent with that measured between 2009 and 2011, indicating that the pulsar spin-down rate remained quite stable during the long quiescent period. A spectral analysis of all the X-ray observations taken between 2009 and 2018 does not reveal significant spectral and/or flux variability. The spectrum of XTE J1810-197 can be described by the sum of two thermal components with temperatures of 0.15 and 0.3 keV, plus a power-law component with photon index 0.6. We also found evidence for an absorption line at ∼1.2 keV and width of 0.1 keV. Due to the long exposure time of the summed XMM-Newton observations, we could also carry out a phase-resolved spectral analysis for this source in quiescence. This showed that the flux modulation can be mainly ascribed to the warmer of the two thermal components, whose flux varies by ∼45 per cent along the pulse phase.Scopus© Citations 14 170 38 - Some of the metrics are blocked by yourconsent settings
Publication Open Access (121514) 1999 UJ7: A primitive, slow-rotating Martian Trojan(2018) ;Borisov, G. ;Christou, A. A. ;Colas, F. ;Bagnulo, S.;
Aims: The goal of this investigation is to determine the origin and surface composition of the asteroid (121514) 1999 UJ7, the only currently known L4 Martian Trojan asteroid.
Methods: We have obtained visible reflectance spectra and photometry of 1999 UJ7 and compared the spectroscopic results with the spectra of a number of taxonomic classes and subclasses. A light curve was obtained and analysed to determine the asteroid spin state.
Results: The visible spectrum of 1999 UJ7 exhibits a negative slope in the blue region and the presence of a wide and deep absorption feature centred around 0.65 μm. The overall morphology of the spectrum seems to suggest a C-complex taxonomy. The photometric behaviour is fairly complex. The light curve shows a primary period of 1.936 d, but this is derived using only a subset of the photometric data. The asteroid may be in a non-principal axis rotational state, but our observational coverage is insufficient to draw definitive conclusions.
Conclusions: Although the observed spectral absorption is wider and deeper, this finding may be compatible with the 0.7 μm spectral feature exhibited by some Ch-type asteroids and could possibly be interpreted as diagnostic of the presence of hydrated minerals. The inferred composition of 1999 UJ7 as a primitive object can be consistent with a volatile-rich object originally accreted beyond the snow line of the solar system, and subsequently evolved to reach the inner regions of the solar system.Based on service observations made with the 4.2 m William Herschel Telescope operated on the island of La Palma by the Isaac Newton Group of Telescopes in the Spanish Observatorio del Roque de los Muchachos of the Instituto de Astrofísica de Canarias and on data collected with 2 m Ritchey-Chrétien-Coudé (2mRCC) Telescope at Rozhen National Astronomical Observatory.
Scopus© Citations 6 234 89 - Some of the metrics are blocked by yourconsent settings
Publication Open Access The 12C/13C isotopic ratio at the dawn of chemical evolution(2023); ;Aguado, D. S. ;Caffau, E. ;Allende Prieto, C. ;Bonifacio, P. ;González Hernández, J. I. ;Rebolo, R. ;Zapatero Osorio, M. R.; ;Pepe, F. ;Santos, N. C. ;Alibert, Y.; ; ; ;Lovis, C. ;Martins, C. J. A. P. ;Milaković, D. ;Murphy, M. T. ;Nunes, N. J.; ;Sousa, S.; Suárez Mascareño, A.Context. The known mega metal-poor (MMP) and hyper metal-poor (HMP) stars, with [Fe/H] < −6.0 and < −5.0, respectively, likely belong to the CEMP-no class, namely, carbon-enhanced stars with little or no second peak neutron-capture elements. They are likely second-generation stars, and the few elements measurable in their atmospheres are used to infer the properties of a single or very few progenitors.
Aims: The high carbon abundance in the CEMP-no stars offers a unique opportunity to measure the carbon isotopic ratio, which directly indicates the presence of mixing between the He- and H-burning layers either within the star or in the progenitor(s). By means of high-resolution spectra acquired with the ESPRESSO spectrograph at the VLT, we aim to derive values for the 12C/13C ratio at the lowest metallicities.
Methods: We used a spectral synthesis technique based on the SYNTHE code and on ATLAS models within a Markov chain Monte Carlo methodology to derive 12C/13C in the stellar atmospheres of four of the most metal-poor stars known: the MMP giant SMSS J0313-6708 ([Fe/H] < −7.1), the HMP dwarf HE 1327-2326 ([Fe/H] = −5.8), the HMP giant SDSS J1313-0019 ([Fe/H] = −5.0), and the ultra metal-poor subgiant HE0233 -0343 ([Fe/H] = −4.7). We also revised a previous value for the MMP giant SMSS J1605-1443 ([Fe/H] = −6.2).
Results: In four stars we derive an isotopic value while for HE 1327-2326 we provide a lower limit. All measurements are in the range 39 < 12C/13C < 100, showing that the He- and H-burning layers underwent partial mixing either in the stars or, more likely, in their progenitors. This provides evidence of a primary production of 13C at the dawn of chemical evolution. CEMP-no dwarf stars with slightly higher metallicities show lower isotopic values, <30 and even approaching the CNO cycle equilibrium value. Thus, extant data suggest the presence of a discontinuity in the 12C/13C ratio at around [Fe/H] ≈ − 4, which could mark a real difference between the progenitor pollution captured by stars with different metallicities. We also note that some MMP and HMP stars with high 12C/13C show low 7Li values, providing an indication that mixing in the CEMP-no progenitors is not responsible for the observed Li depletion.Scopus© Citations 5 78 24 - Some of the metrics are blocked by yourconsent settings
Publication Open Access The 13th Data Release of the Sloan Digital Sky Survey: First Spectroscopic Data from the SDSS-IV Survey Mapping Nearby Galaxies at Apache Point Observatory(2017) ;Albareti, Franco D. ;Allende Prieto, Carlos ;Almeida, Andres ;Anders, Friedrich ;Anderson, Scott ;Andrews, Brett H. ;Aragón-Salamanca, Alfonso ;Argudo-Fernández, Maria ;Armengaud, Eric ;Aubourg, Eric ;Avila-Reese, Vladimir ;Badenes, Carles ;Bailey, Stephen ;Barbuy, Beatriz ;Barger, Kat ;Barrera-Ballesteros, Jorge ;Bartosz, Curtis ;Basu, Sarbani ;Bates, Dominic ;Battaglia, Giuseppina ;Baumgarten, Falk ;Baur, Julien ;Bautista, Julian ;Beers, Timothy C.; ;Bershady, Matthew ;Bertran de Lis, Sara ;Bird, Jonathan C. ;Bizyaev, Dmitry ;Blanc, Guillermo A. ;Blanton, Michael ;Blomqvist, Michael ;Bolton, Adam S. ;Borissova, J. ;Bovy, Jo ;Brandt, William Nielsen ;Brinkmann, Jonathan ;Brownstein, Joel R. ;Bundy, Kevin ;Burtin, Etienne ;Busca, Nicolás G. ;Orlando Camacho Chavez, Hugo ;Cano Díaz, M. ;Cappellari, Michele; ;Chen, Yanping ;Cherinka, Brian ;Cheung, Edmond ;Chiappini, Cristina ;Chojnowski, Drew ;Chuang, Chia-Hsun ;Chung, Haeun ;Cirolini, Rafael Fernando ;Clerc, Nicolas ;Cohen, Roger E. ;Comerford, Julia M. ;Comparat, Johan ;Correa do Nascimento, Janaina ;Cousinou, Marie-Claude ;Covey, Kevin ;Crane, Jeffrey D. ;Croft, Rupert ;Cunha, Katia ;Darling, Jeremy ;Davidson, James W., Jr. ;Dawson, Kyle ;Da Costa, Luiz ;Da Silva Ilha, Gabriele ;Deconto Machado, Alice ;Delubac, Timothée ;De Lee, Nathan ;De la Macorra, Axel ;De la Torre, Sylvain ;Diamond-Stanic, Aleksandar M. ;Donor, John ;Downes, Juan Jose ;Drory, Niv ;Du, Cheng ;Du Mas des Bourboux, Hélion ;Dwelly, Tom ;Ebelke, Garrett ;Eigenbrot, Arthur ;Eisenstein, Daniel J. ;Elsworth, Yvonne P. ;Emsellem, Eric ;Eracleous, Michael ;Escoffier, Stephanie ;Evans, Michael L. ;Falcón-Barroso, Jesús ;Fan, Xiaohui ;Favole, Ginevra ;Fernandez-Alvar, Emma ;Fernandez-Trincado, J. G. ;Feuillet, Diane ;Fleming, Scott W. ;Font-Ribera, Andreu ;Freischlad, Gordon ;Frinchaboy, Peter ;Fu, Hai ;Gao, Yang ;Garcia, Rafael A. ;Garcia-Dias, R. ;Garcia-Hernández, D. A. ;Garcia Pérez, Ana E. ;Gaulme, Patrick ;Ge, Junqiang ;Geisler, Douglas ;Gillespie, Bruce ;Gil Marin, Hector; ;Goddard, Daniel ;Gomez Maqueo Chew, Yilen ;Gonzalez-Perez, Violeta ;Grabowski, Kathleen ;Green, Paul ;Grier, Catherine J. ;Grier, Thomas ;Guo, Hong ;Guy, Julien ;Hagen, Alex ;Hall, Matt ;Harding, Paul ;Harley, R. E. ;Hasselquist, Sten ;Hawley, Suzanne ;Hayes, Christian R. ;Hearty, Fred ;Hekker, Saskia ;Hernandez Toledo, Hector ;Ho, Shirley ;Hogg, David W. ;Holley-Bockelmann, Kelly ;Holtzman, Jon A. ;Holzer, Parker H. ;Hu, Jian ;Huber, Daniel ;Hutchinson, Timothy Alan ;Hwang, Ho Seong ;Ibarra-Medel, Héctor J. ;Ivans, Inese I. ;Ivory, KeShawn ;Jaehnig, Kurt ;Jensen, Trey W. ;Johnson, Jennifer A. ;Jones, Amy ;Jullo, Eric ;Kallinger, T. ;Kinemuchi, Karen ;Kirkby, David ;Klaene, Mark ;Kneib, Jean-Paul ;Kollmeier, Juna A. ;Lacerna, Ivan ;Lane, Richard R. ;Lang, Dustin ;Laurent, Pierre ;Law, David R. ;Leauthaud, Alexie ;Le Goff, Jean-Marc ;Li, Chen ;Li, Cheng ;Li, Niu ;Li, Ran ;Liang, Fu-Heng ;Liang, Yu ;Lima, Marcos ;Lin, Lihwai ;Lin, Lin ;Lin, Yen-Ting ;Liu, Chao ;Long, Dan; ;MacDonald, Nicholas ;MacLeod, Chelsea L. ;Mackereth, J. Ted ;Mahadevan, Suvrath ;Maia, Marcio Antonio Geimba ;Maiolino, Roberto ;Majewski, Steven R. ;Malanushenko, Olena ;Malanushenko, Viktor ;Mallmann, Nícolas Dullius ;Manchado, Arturo ;Maraston, Claudia ;Marques-Chaves, Rui ;Martinez Valpuesta, Inma ;Masters, Karen L. ;Mathur, Savita ;McGreer, Ian D. ;Merloni, Andrea ;Merrifield, Michael R. ;Mészáros, Szabolcs ;Meza, Andres; ;Minchev, Ivan ;Molaverdikhani, Karan ;Montero-Dorta, Antonio D. ;Mosser, Benoit ;Muna, Demitri ;Myers, Adam ;Nair, Preethi ;Nandra, Kirpal ;Ness, Melissa ;Newman, Jeffrey A. ;Nichol, Robert C. ;Nidever, David L. ;Nitschelm, Christian ;O'Connell, Julia ;Oravetz, Audrey ;Oravetz, Daniel J. ;Pace, Zachary ;Padilla, Nelson ;Palanque-Delabrouille, Nathalie ;Pan, Kaike ;Parejko, John ;Paris, Isabelle ;Park, Changbom ;Peacock, John A. ;Peirani, Sebastien ;Pellejero-Ibanez, Marcos ;Penny, Samantha ;Percival, Will J. ;Percival, Jeffrey W. ;Perez-Fournon, Ismael ;Petitjean, Patrick ;Pieri, Matthew ;Pinsonneault, Marc H. ;Pisani, Alice ;Prada, Francisco ;Prakash, Abhishek ;Price-Jones, Natalie ;Raddick, M. Jordan ;Rahman, Mubdi ;Raichoor, Anand ;Barboza Rembold, Sandro ;Reyna, A. M. ;Rich, James ;Richstein, Hannah ;Ridl, Jethro ;Riffel, Rogemar A. ;Riffel, Rogério ;Rix, Hans-Walter ;Robin, Annie C. ;Rockosi, Constance M. ;Rodríguez-Torres, Sergio ;Rodrigues, Thaíse S. ;Roe, Natalie ;Roman Lopes, A. ;Román-Zúñiga, Carlos ;Ross, Ashley J. ;Rossi, Graziano ;Ruan, John ;Ruggeri, Rossana ;Runnoe, Jessie C. ;Salazar-Albornoz, Salvador ;Salvato, Mara ;Sanchez, Sebastian F. ;Sanchez, Ariel G. ;Sanchez-Gallego, José R. ;Santiago, Basílio Xavier ;Schiavon, Ricardo ;Schimoia, Jaderson S. ;Schlafly, Eddie ;Schlegel, David J. ;Schneider, Donald P. ;Schönrich, Ralph ;Schultheis, Mathias ;Schwope, Axel ;Seo, Hee-Jong ;Serenelli, Aldo ;Sesar, Branimir ;Shao, Zhengyi ;Shetrone, Matthew ;Shull, Michael ;Silva Aguirre, Victor ;Skrutskie, M. F. ;Slosar, Anže ;Smith, Michael ;Smith, Verne V. ;Sobeck, Jennifer ;Somers, Garrett ;Souto, Diogo ;Stark, David V. ;Stassun, Keivan G. ;Steinmetz, Matthias ;Stello, Dennis ;Storchi Bergmann, Thaisa ;Strauss, Michael A. ;Streblyanska, Alina ;Stringfellow, Guy S. ;Suarez, Genaro ;Sun, Jing ;Taghizadeh-Popp, Manuchehr ;Tang, Baitian ;Tao, Charling ;Tayar, Jamie ;Tembe, Mita ;Thomas, Daniel ;Tinker, Jeremy ;Tojeiro, Rita ;Tremonti, Christy ;Troup, Nicholas ;Trump, Jonathan R. ;Unda-Sanzana, Eduardo ;Valenzuela, O. ;Van den Bosch, Remco ;Vargas-Magaña, Mariana ;Vazquez, Jose Alberto ;Villanova, Sandro ;Vivek, M. ;Vogt, Nicole ;Wake, David ;Walterbos, Rene ;Wang, Yuting ;Wang, Enci ;Weaver, Benjamin Alan ;Weijmans, Anne-Marie ;Weinberg, David H. ;Westfall, Kyle B. ;Whelan, David G. ;Wilcots, Eric ;Wild, Vivienne ;Williams, Rob A. ;Wilson, John ;Wood-Vasey, W. M. ;Wylezalek, Dominika ;Xiao, Ting ;Yan, Renbin ;Yang, Meng ;Ybarra, Jason E. ;Yeche, Christophe ;Yuan, Fang-Ting ;Zakamska, Nadia ;Zamora, Olga ;Zasowski, Gail ;Zhang, Kai ;Zhao, Cheng ;Zhao, Gong-Bo ;Zheng, Zheng ;Zhou, Zhi-Min ;Zhu, Guangtun ;Zinn, Joel C.Zou, HuThe fourth generation of the Sloan Digital Sky Survey (SDSS-IV) began observations in 2014 July. It pursues three core programs: the Apache Point Observatory Galactic Evolution Experiment 2 (APOGEE-2), Mapping Nearby Galaxies at APO (MaNGA), and the Extended Baryon Oscillation Spectroscopic Survey (eBOSS). As well as its core program, eBOSS contains two major subprograms: the Time Domain Spectroscopic Survey (TDSS) and the SPectroscopic IDentification of ERosita Sources (SPIDERS). This paper describes the first data release from SDSS-IV, Data Release 13 (DR13). DR13 makes publicly available the first 1390 spatially resolved integral field unit observations of nearby galaxies from MaNGA. It includes new observations from eBOSS, completing the Sloan Extended QUasar, Emission-line galaxy, Luminous red galaxy Survey (SEQUELS), which also targeted variability-selected objects and X-ray-selected objects. DR13 includes new reductions of the SDSS-III BOSS data, improving the spectrophotometric calibration and redshift classification, and new reductions of the SDSS-III APOGEE-1 data, improving stellar parameters for dwarf stars and cooler stars. DR13 provides more robust and precise photometric calibrations. Value-added target catalogs relevant for eBOSS, TDSS, and SPIDERS and an updated red-clump catalog for APOGEE are also available. This paper describes the location and format of the data and provides references to important technical papers. The SDSS web site, http://www.sdss.org, provides links to the data, tutorials, examples of data access, and extensive documentation of the reduction and analysis procedures. DR13 is the first of a scheduled set that will contain new data and analyses from the planned ∼6 yr operations of SDSS-IV.Scopus© Citations 345 197 59 - Some of the metrics are blocked by yourconsent settings
Publication Open Access The 16th Data Release of the Sloan Digital Sky Surveys: First Release from the APOGEE-2 Southern Survey and Full Release of eBOSS Spectra(2020) ;Ahumada, Romina ;Prieto, Carlos Allende ;Almeida, Andrés ;Anders, Friedrich ;Anderson, Scott F. ;Andrews, Brett H. ;Anguiano, Borja ;Arcodia, Riccardo ;Armengaud, Eric ;Aubert, Marie ;Avila, Santiago ;Avila-Reese, Vladimir ;Badenes, Carles ;Balland, Christophe ;Barger, Kat ;Barrera-Ballesteros, Jorge K. ;Basu, Sarbani ;Bautista, Julian ;Beaton, Rachael L. ;Beers, Timothy C. ;Benavides, B. Izamar T. ;Bender, Chad F. ;Bernardi, Mariangela ;Bershady, Matthew ;Beutler, Florian ;Bidin, Christian Moni ;Bird, Jonathan ;Bizyaev, Dmitry ;Blanc, Guillermo A. ;Blanton, Michael R. ;Boquien, Médéric ;Borissova, Jura ;Bovy, Jo ;Brandt, W. N. ;Brinkmann, Jonathan ;Brownstein, Joel R. ;Bundy, Kevin ;Bureau, Martin ;Burgasser, Adam ;Burtin, Etienne ;Cano-Díaz, Mariana; ;Cappellari, Michele; ;Chabanier, Solène ;Chaplin, William ;Chapman, Michael ;Cherinka, Brian ;Chiappini, Cristina ;Doohyun Choi, Peter ;Chojnowski, S. Drew ;Chung, Haeun ;Clerc, Nicolas ;Coffey, Damien ;Comerford, Julia M. ;Comparat, Johan ;da Costa, Luiz ;Cousinou, Marie-Claude ;Covey, Kevin ;Crane, Jeffrey D. ;Cunha, Katia ;Ilha, Gabriele da Silva ;Dai, Yu Sophia ;Damsted, Sanna B. ;Darling, Jeremy ;Davidson, James W., Jr. ;Davies, Roger ;Dawson, Kyle ;De, Nikhil ;de la Macorra, Axel ;De Lee, Nathan ;Queiroz, Anna Bárbara de Andrade ;Deconto Machado, Alice ;de la Torre, Sylvain; ;du Mas des Bourboux, Hélion ;Diamond-Stanic, Aleksandar M. ;Dillon, Sean ;Donor, John ;Drory, Niv ;Duckworth, Chris ;Dwelly, Tom ;Ebelke, Garrett ;Eftekharzadeh, Sarah ;Davis Eigenbrot, Arthur ;Elsworth, Yvonne P. ;Eracleous, Mike ;Erfanianfar, Ghazaleh ;Escoffier, Stephanie ;Fan, Xiaohui ;Farr, Emily ;Fernández-Trincado, José G. ;Feuillet, Diane ;Finoguenov, Alexis ;Fofie, Patricia ;Fraser-McKelvie, Amelia ;Frinchaboy, Peter M. ;Fromenteau, Sebastien ;Fu, Hai ;Galbany, Lluís ;Garcia, Rafael A. ;García-Hernández, D. A. ;Oehmichen, Luis Alberto Garma ;Ge, Junqiang ;Maia, Marcio Antonio Geimba ;Geisler, Doug ;Gelfand, Joseph ;Goddy, Julian ;Gonzalez-Perez, Violeta ;Grabowski, Kathleen ;Green, Paul ;Grier, Catherine J. ;Guo, Hong ;Guy, Julien ;Harding, Paul ;Hasselquist, Sten ;Hawken, Adam James ;Hayes, Christian R. ;Hearty, Fred ;Hekker, S. ;Hogg, David W. ;Holtzman, Jon A. ;Horta, Danny ;Hou, Jiamin ;Hsieh, Bau-Ching ;Huber, Daniel ;Hunt, Jason A. S. ;Chitham, J. Ider ;Imig, Julie ;Jaber, Mariana ;Angel, Camilo Eduardo Jimenez ;Johnson, Jennifer A. ;Jones, Amy M. ;Jönsson, Henrik ;Jullo, Eric ;Kim, Yerim ;Kinemuchi, Karen ;Kirkpatrick, Charles C., IV ;Kite, George W. ;Klaene, Mark ;Kneib, Jean-Paul ;Kollmeier, Juna A. ;Kong, Hui ;Kounkel, Marina ;Krishnarao, Dhanesh ;Lacerna, Ivan ;Lan, Ting-Wen ;Lane, Richard R. ;Law, David R. ;Le Goff, Jean-Marc ;Leung, Henry W. ;Lewis, Hannah ;Li, Cheng ;Lian, Jianhui ;Lin, Lihwai ;Long, Dan ;Longa-Peña, Penélope ;Lundgren, Britt ;Lyke, Brad W. ;Ted Mackereth, J. ;MacLeod, Chelsea L. ;Majewski, Steven R. ;Manchado, Arturo ;Maraston, Claudia ;Martini, Paul ;Masseron, Thomas ;Masters, Karen L. ;Mathur, Savita ;McDermid, Richard M. ;Merloni, Andrea ;Merrifield, Michael ;Mészáros, Szabolcs; ;Minniti, Dante ;Minsley, Rebecca ;Miyaji, Takamitsu; ;Mosser, Benoit ;Mueller, Eva-Maria ;Muna, Demitri ;Muñoz-Gutiérrez, Andrea ;Myers, Adam D. ;Nadathur, Seshadri ;Nair, Preethi ;Nandra, Kirpal ;do Nascimento, Janaina Correa ;Nevin, Rebecca Jean ;Newman, Jeffrey A. ;Nidever, David L. ;Nitschelm, Christian ;Noterdaeme, Pasquier ;O'Connell, Julia E. ;Olmstead, Matthew D. ;Oravetz, Daniel ;Oravetz, Audrey ;Osorio, Yeisson ;Pace, Zachary J. ;Padilla, Nelson ;Palanque-Delabrouille, Nathalie ;Palicio, Pedro A. ;Pan, Hsi-An ;Pan, Kaike ;Parker, James ;Paviot, Romain ;Peirani, Sebastien ;Ramŕez, Karla Peña ;Penny, Samantha ;Percival, Will J. ;Perez-Fournon, Ismael ;Pérez-Ràfols, Ignasi ;Petitjean, Patrick ;Pieri, Matthew M. ;Pinsonneault, Marc ;Poovelil, Vijith Jacob ;Povick, Joshua Tyler ;Prakash, Abhishek ;Price-Whelan, Adrian M. ;Raddick, M. Jordan ;Raichoor, Anand ;Ray, Amy ;Rembold, Sandro Barboza ;Rezaie, Mehdi ;Riffel, Rogemar A. ;Riffel, Rogério ;Rix, Hans-Walter ;Robin, Annie C. ;Roman-Lopes, A. ;Román-Zúñiga, Carlos ;Rose, Benjamin ;Ross, Ashley J. ;Rossi, Graziano ;Rowlands, Kate ;Rubin, Kate H. R. ;Salvato, Mara ;Sánchez, Ariel G. ;Sánchez-Menguiano, Laura ;Sánchez-Gallego, José R. ;Sayres, Conor ;Schaefer, Adam ;Schiavon, Ricardo P. ;Schimoia, Jaderson S. ;Schlafly, Edward ;Schlegel, David ;Schneider, Donald P. ;Schultheis, Mathias ;Schwope, Axel ;Seo, Hee-Jong ;Serenelli, Aldo ;Shafieloo, Arman ;Shamsi, Shoaib Jamal ;Shao, Zhengyi ;Shen, Shiyin ;Shetrone, Matthew ;Shirley, Raphael ;Aguirre, Víctor Silva ;Simon, Joshua D. ;Skrutskie, M. F. ;Slosar, Anže ;Smethurst, Rebecca ;Sobeck, Jennifer ;Sodi, Bernardo Cervantes ;Souto, Diogo ;Stark, David V. ;Stassun, Keivan G. ;Steinmetz, Matthias ;Stello, Dennis ;Stermer, Julianna ;Storchi-Bergmann, Thaisa ;Streblyanska, Alina ;Stringfellow, Guy S. ;Stutz, Amelia ;Suárez, Genaro ;Sun, Jing ;Taghizadeh-Popp, Manuchehr ;Talbot, Michael S. ;Tayar, Jamie ;Thakar, Aniruddha R. ;Theriault, Riley ;Thomas, Daniel ;Thomas, Zak C. ;Tinker, Jeremy ;Tojeiro, Rita ;Toledo, Hector Hernandez ;Tremonti, Christy A. ;Troup, Nicholas W. ;Tuttle, Sarah ;Unda-Sanzana, Eduardo ;Valentini, Marica ;Vargas-González, Jaime ;Vargas-Magaña, Mariana ;Vázquez-Mata, Jose Antonio ;Vivek, M. ;Wake, David ;Wang, Yuting ;Weaver, Benjamin Alan ;Weijmans, Anne-Marie ;Wild, Vivienne ;Wilson, John C. ;Wilson, Robert F. ;Wolthuis, Nathan ;Wood-Vasey, W. M. ;Yan, Renbin ;Yang, Meng ;Yèche, Christophe ;Zamora, Olga ;Zarrouk, Pauline ;Zasowski, Gail ;Zhang, Kai ;Zhao, Cheng ;Zhao, Gongbo ;Zheng, Zheng ;Zhu, GuangtunZou, HuThis paper documents the 16th data release (DR16) from the Sloan Digital Sky Surveys (SDSS), the fourth and penultimate from the fourth phase (SDSS-IV). This is the first release of data from the Southern Hemisphere survey of the Apache Point Observatory Galactic Evolution Experiment 2 (APOGEE-2); new data from APOGEE-2 North are also included. DR16 is also notable as the final data release for the main cosmological program of the Extended Baryon Oscillation Spectroscopic Survey (eBOSS), and all raw and reduced spectra from that project are released here. DR16 also includes all the data from the Time Domain Spectroscopic Survey and new data from the SPectroscopic IDentification of ERosita Survey programs, both of which were co-observed on eBOSS plates. DR16 has no new data from the Mapping Nearby Galaxies at Apache Point Observatory (MaNGA) survey (or the MaNGA Stellar Library "MaStar"). We also preview future SDSS-V operations (due to start in 2020), and summarize plans for the final SDSS-IV data release (DR17).Scopus© Citations 899 34 15 - Some of the metrics are blocked by yourconsent settings
Publication Open Access 2 years with comet 67P/Churyumov-Gerasimenko: H2O, CO2, CO as seen by ROSINA RTOF(2017) ;Hoang, M. ;Garnier, P. ;Lasue, J. ;Reme, H. ;Altwegg, K. ;Balsiger, H. R. ;Bieler, A. M. ;Calmonte, U.; ;Combi, M. R. ;De Keyser, J. M. ;Fiethe, B. ;Fougere, N. ;Fuselier, S. A. ;Galli, A. ;Gasc, S. ;Gombosi, T. I. ;Hansen, K. C. ;Jäckel, A. ;Korth, A. ;Mall, U.; ;Rubin, M. ;Sémon, T. ;Tzou, C. Y. ;Waite, J. H., Jr.Wurz, P.The Rosetta space mission investigated comet 67P/Churyumov-Gerasimenko (67P) over two years from August 2014 to September 2016. Onboard the spacecraft, the ROSINA experiment included two mass spectrometers to derive the composition of neutrals and ions, and a COmet Pressure Sensor (COPS) to monitor the density and velocity of the neutrals in the coma. We will here analyse and discuss data from the Reflectron-type Time-Of-Flight instrument during the comet escort phase. The RTOF mass spectrometer possessed a wide mass range and a high temporal resolution (Balsiger et al., 2007). The analysis of 67P/C-G's coma major molecules over the mission showed strong variability of the comet coma's main volatiles concentrations (H2O, CO2, CO) and their relative abundances. The 2 years long Rosetta mission allowed us to observe the seasonal evolution in the atmosphere of 67P, in particular the change occurring during the equinoxes and at perihelion. In this work, we analyze the asymmetry in the outgassing rate before and after the perihelion (13/08/2015), the evolution of abundance ratios through the whole mission, and in particular the behavior of the very volatile CO molecules. Density maps projected on the surface of 67P demonstrate the evolution of the three main coma species after the outbound equinox. We will present first results of our comet nucleus thermal modelling used to simulate the internal structure and temperature evolution of 67P at characteristic surface areas. These results will be compared with the coma composition measurements obtained by ROSINA....190 28 - Some of the metrics are blocked by yourconsent settings
Publication Open Access The 2-10 keV unabsorbed luminosity function of AGN from the LSS, CDFS, and COSMOS surveys(2016) ;Ranalli, P. ;Koulouridis, E. ;Georgantopoulos, I. ;Fotopoulou, S. ;Hsu, L. -T. ;Salvato, M.; ;Pierre, M. ;Cappelluti, N. ;Carrera, F. J.; ;Clerc, N.; ;Iwasawa, K. ;Pacaud, F. ;Paltani, S. ;Plionis, E.Vignali, C.The XMM-Large scale structure (XMM-LSS), XMM-Cosmological evolution survey (XMM-COSMOS), and XMM-Chandra deep field south (XMM-CDFS) surveys are complementary in terms of sky coverage and depth. Together, they form a clean sample with the least possible variance in instrument effective areas and point spread function. Therefore this is one of the best samples available to determine the 2-10 keV luminosity function of active galactic nuclei (AGN) and their evolution. The samples and the relevant corrections for incompleteness are described. A total of 2887 AGN is used to build the LF in the luminosity interval 1042-1046 erg s-1 and in the redshift interval 0.001-4. A new method to correct for absorption by considering the probability distribution for the column density conditioned on the hardness ratio is presented. The binned luminosity function and its evolution is determined with a variant of the Page-Carrera method, which is improved to include corrections for absorption and to account for the full probability distribution of photometric redshifts. Parametric models, namely a double power law with luminosity and density evolution (LADE) or luminosity-dependent density evolution (LDDE), are explored using Bayesian inference. We introduce the Watanabe-Akaike information criterion (WAIC) to compare the models and estimate their predictive power. Our data are best described by the LADE model, as hinted by the WAIC indicator. We also explore the recently proposed 15-parameter extended LDDE model and find that this extension is not supported by our data. The strength of our method is that it provides unabsorbed, non-parametric estimates, credible intervals for luminosity function parameters, and a model choice based on predictive power for future data.Based on observations obtained with XMM-Newton, an ESA science mission with instruments and contributions directly funded by ESA member states and NASA.Tables with the samples of the posterior probability distributions are only available at the CDS via anonymous ftp to "http://cdsarc.u-strasbg.fr" or via "http://cdsarc.u-strasbg.fr/viz-bin/qcat?J/A+A/590/A80"
Scopus© Citations 25 690 57 - Some of the metrics are blocked by yourconsent settings
Publication Open Access A 2.3-8.2 GHz room temperature multi-channel receiver for phased array feed applicationWe describe the design, fabrication and test results of a multi-channel heterodyne receiver operating at room temperature across the 2.3-8.2 GHz Radio Frequency (RF) band. Such a “Warm Section” (WS) receiver is part of a Phased Array Feed (PAF) demonstrator that is being built for radio astronomy application. The WS receiver is cascaded to the PAF cryogenic section that incorporates an antenna array with low noise pre-amplification stages. The WS receiver consists of four rack-mountable modules, each of which can process eight RF inputs. Four modules are arranged in a standard 19” rack to allow handling a total of 32 RF signals. The modules perform filtering (through four-way switch filter bank) and down-conversion (to the 375-650 MHz IF band). The IF signals are converted to optical through analogue Wavelength Division Multiplexing IFoF (IF over fiber) transmitters incorporated into the WS receiver. The signals are sent through optical fibers to a backend, where they are converted back to IF before digitization by an Analog-to-Digital Unit.Scopus© Citations 5 213 37 - Some of the metrics are blocked by yourconsent settings
Publication Open Access A 20-year H2O maser monitoring program with the Medicina 32-m telescope(Cambridge University Press., 2007); ;Felli, M.; ; ; ;Di Franco, S.; ; ; ; ;Palagi, F. ;Palla, F.; Valdettaro, R.The Arcetri/Bologna H2O maser group has been monitoring the 1.3-cm water maser emission from a sample of 43 star-forming regions (SFRs) and 22 late-type stars for about 20 years at a sampling rate of 4-5 observations each year, using the 32-m Medicina Radio Telescope (HPBW 1.‧9 at 22 GHz). For the late-type stars we observe representative samples of OH/IR-stars, Mira's, semi-regular variables, and supergiants. The SFR-sample spans a large interval in FIR luminosity of the associated Young Stellar Object (YSO), from 20 L to 1.5 × 106 L, and offers a unique data base for the study of the long-term (years) variability of the maser emission in regions of star formation.This presentation concerns only the masers in SFRs. The information obtained from single-dish monitoring is complementary to what is extracted from higher-resolution (VLA and VLBI) observations, and can better explore the velocity domain and the long-term variability therein.
We characterize the variability of the sources in various ways and we study how it depends on the luminosity and other properties of the associated YSO and its environment.
Scopus© Citations 1 139 33 - Some of the metrics are blocked by yourconsent settings
Publication Open Access The 2009 december gamma-ray flare of 3C 454.3: The multifrequency campaign(2010); ; ; ; ; ; ;Sakamoto, T.; ; ; ;Sasada, M. ;Itoh, R. ;Yamanaka, M. ;Uemura, M. ;Striani, E.; ;Tiengo, A. ;Krimm, H.A. ;Stroh, M.C. ;Falcone, A.D. ;Curran, P.A. ;Sadun, A.C. ;Lahteenmaki, A. ;Tornikoski, M. ;Aller, H.D. ;Aller, M.F. ;Lin, C.S. ;Larionov, V.M.; ;Takalo, L.O. ;Berdyugin, A. ;Gurwell, M.A.; ;Chen, A.W. ;Donnarumma, I.; ;Longo, F. ;Pucella, G.; ;Barbiellini, G.; ;Cattaneo, P.W.; ; ;Monte, E.D. ;Cocco, G.D.; ;Ferrari, A.; ; ; ;Galli, M.; ; ;Lapshov, I.; ;Lipari, P.; ; ;Morelli, E. ;Moretti, E. ;Morselli, A.; ;Perotti, F.; ;Picozza, P.; ;Prest, M. ;Rapisarda, M. ;Rappoldi, A. ;Rubini, A. ;Sabatini, S.; ; ; ;Vallazza, E. ;Zanello, D. ;Colafrancesco, S.; ; ;Santolamazza, P.; ;Giommi, P.Salotti, L.During the month of 2009 December, the blazar 3C 454.3 became the brightest gamma-ray source in the sky, reaching a peak flux F 2000 × 10 -8 photons cm-2 s-1 for E > 100 MeV. Starting in 2009 November intensive multifrequency campaigns monitored the 3C 454 gamma-ray outburst. Here, we report on the results of a two-month campaign involving AGILE, INTEGRAL, Swift/XRT, Swift/BAT, and Rossi XTE for the high-energy observations and Swift/UVOT, KANATA, Goddard Robotic Telescope, and REM for the near-IR/optical/UV data. GASP/WEBT provided radio and additional optical data. We detected a long-term active emission phase lasting 1 month at all wavelengths: in the gamma-ray band, peak emission was reached on 2009 December 2-3. Remarkably, this gamma-ray super-flare was not accompanied by correspondingly intense emission in the optical/UV band that reached a level substantially lower than the previous observations in 2007-2008. The lack of strong simultaneous optical brightening during the super-flare and the determination of the broadband spectral evolution severely constrain the theoretical modeling. We find that the pre- and post-flare broadband behavior can be explained by a one-zone model involving synchrotron self-Compton plus external Compton emission from an accretion disk and a broad-line region. However, the spectra of the 2009 December 2-3 super-flare and of the secondary peak emission on 2009 December 9 cannot be satisfactorily modeled by a simple one-zone model. An additional particle component is most likely active during these states. © 2010. The American Astronomical Society. All rights reserved.Scopus© Citations 54 119 56 - Some of the metrics are blocked by yourconsent settings
Publication Open Access The 2016 Feb 19 outburst of comet 67P/CG: an ESA Rosetta multi-instrument study(2016) ;Grün, E. ;Agarwal, J. ;Altobelli, N. ;Altwegg, K. ;Bentley, M. S. ;Biver, N.; ;Edberg, N. ;Feldman, P. D. ;Galand, M. ;Geiger, B. ;Götz, C. ;Grieger, B. ;Güttler, C. ;Henri, P. ;Hofstadter, M. ;Horanyi, M. ;Jehin, E. ;Krüger, H. ;Lee, S. ;Mannel, T. ;Morales, E. ;Mousis, O. ;Müller, M. ;Opitom, C.; ;Schmied, R. ;Schmidt, F. ;Sierks, H. ;Snodgrass, C. ;Soja, R. H. ;Sommer, M. ;Srama, R. ;Tzou, C. -Y. ;Vincent, J. -B. ;Yanamandra-Fisher, P. ;A'Hearn, M. F. ;Erikson, A. I. ;Barbieri, C. ;Barucci, M. A. ;Bertaux, J. -L. ;Bertini, I. ;Burch, J.; ; ;Da Deppo, V. ;Davidsson, B. ;Debei, S. ;De Cecco, M. ;Deller, J. ;Feaga, L. M.; ;Fornasier, S.; ;Gicquel, A. ;Gillon, M. ;Green, S. F. ;Groussin, O. ;Gutiérrez, P. J. ;Hofmann, M. ;Hviid, S. F. ;Ip, W. -H.; ;Jorda, L. ;Keller, H. U. ;Knight, M. M. ;Knollenberg, J. ;Koschny, D. ;Kramm, J. -R. ;Kührt, E. ;Küppers, M. ;Lamy, P. L. ;Lara, L. M. ;Lazzarin, M. ;Lòpez-Moreno, J. J. ;Manfroid, J. ;Epifani, E. Mazzotta ;Marzari, F. ;Naletto, G. ;Oklay, N.; ;Parker, J. Wm. ;Rickman, H. ;Rodrigo, R. ;Rodrìguez, J. ;Schindhelm, E. ;Shi, X.; ;Steffl, A. J. ;Stern, S. A. ;Thomas, N.; ;Weaver, H. A. ;Weissman, P. ;Zakharov, V. V.Taylor, M. G. G. T.On 2016 Feb 19, nine Rosetta instruments serendipitously observed an outburst of gas and dust from the nucleus of comet 67P/Churyumov-Gerasimenko. Among these instruments were cameras and spectrometers ranging from UV over visible to microwave wavelengths, in situ gas, dust and plasma instruments, and one dust collector. At 09:40 a dust cloud developed at the edge of an image in the shadowed region of the nucleus. Over the next two hours the instruments recorded a signature of the outburst that significantly exceeded the background. The enhancement ranged from 50 per cent of the neutral gas density at Rosetta to factors >100 of the brightness of the coma near the nucleus. Dust related phenomena (dust counts or brightness due to illuminated dust) showed the strongest enhancements (factors >10). However, even the electron density at Rosetta increased by a factor 3 and consequently the spacecraft potential changed from ∼-16 V to -20 V during the outburst. A clear sequence of events was observed at the distance of Rosetta (34 km from the nucleus): within 15 min the Star Tracker camera detected fast particles (∼25 m s-1) while 100 μm radius particles were detected by the GIADA dust instrument ∼1 h later at a speed of 6 m s-1. The slowest were individual mm to cm sized grains observed by the OSIRIS cameras. Although the outburst originated just outside the FOV of the instruments, the source region and the magnitude of the outburst could be determined.Scopus© Citations 65 196 149 - Some of the metrics are blocked by yourconsent settings
Publication Open Access A 21-cm power spectrum at 48 MHz, using the Owens Valley Long Wavelength Array(2021) ;Garsden, H. ;Greenhill, L.; ;Fialkov, A. ;Price, D. C. ;Mitchell, D. ;Dowell, J.; Schinzel, F. K.The Large-aperture Experiment to detect the Dark Age (LEDA) was designed to measure the 21-cm signal from neutral hydrogen at Cosmic Dawn, z ≍ 15-30. Using observations made with the ≍ 200 m diameter core of the Owens Valley Radio Observatory Long Wavelength Array (OVRO-LWA), we present a 2D cylindrical spatial power spectrum for data at 43.1-53.5 MHz (zmedian ≍ 28) incoherently integrated for 4 h, and an analysis of the array sensitivity. Power from foregrounds is localized to a 'wedge' within k⊥, $k_\parallel$ space. After calibration of visibilities using five bright compact sources including Vir A, we measure Δ2(k) ≍ 2 × 1012 mK2 outside the foreground wedge, where an uncontaminated cosmological signal would lie, in principle. The measured Δ2(k) is an upper limit that reflects a combination of thermal instrumental and sky noise, and unmodelled systematics that scatter power from the wedge, as will be discussed. By differencing calibrated visibilities for close pairs of frequency channels, we suppress foreground sky structure and systematics, extract thermal noise, and use a mix of coherent and incoherent integration to simulate a noise-dominated power spectrum for a 3000 h observation and z = 16-37. For suitable calibration quality, the resulting noise level, Δ2(k) ≍ 100 mK2 (k = 0.3 Mpc-1), would be sufficient to detect peaks in the 21-cm spatial power spectrum due to early Ly-α and X-ray sources, as predicted for a range of theoretical model parameters.147 73Scopus© Citations 33 - Some of the metrics are blocked by yourconsent settings
Publication Open Access 2PBC J0658.0-1746: a hard X-ray eclipsing polar in the orbital period gap(2019); ; ;Mukai, K. ;Falanga, M.The hard X-ray source 2PBC J0658.0-1746 was proposed as an eclipsing magnetic cataclysmic variable of the polar type, based on optical follow-ups. We present the first spectral and timing analysis at X-ray energies with XMM-Newton, complemented with archival X-ray, optical, infrared (IR) photometry, and spectroscopy. The X-ray emission shows bright and faint phases and total eclipses recurring every 2.38 h, consistent with optical properties. This firmly identifies 2PBC J0658.0-1746 as an eclipsing polar, the second hard X-ray selected in the orbital period gap. The X-ray orbital modulation changes from cycle-to-cycle and the X-ray flux is strongly variable over the years, implying a non-stationary mass accretion rate both on short and long time-scales. The X-ray eclipses allow to refine the orbital ephemeris with period 0.09913398(4) d, and to constrain the binary inclination 79^{circ}≲ i ≲ 90^{circ} and the mass ratio 0.18< M_2/M_{ WD}< 0.40. A companion mass M2=0.2-0.25 M_{\odot } with a radius R2=0.24-0.26 R_{\odot } and spectral type ∼M4, at D=209^{+3}_{-2} pc, is derived. A lower limit to the white dwarf mass of ∼ 0.6 M_{\odot } is obtained from the X-ray spectrum. An upper limit to the magnetic colatitude, β ≲ 50^{circ}, and a shift in azimuth, ψ ∼ 14^{circ}, of the main accreting pole are also estimated. The optical/IR spectral energy distribution shows large excess in the mid-IR due to lower harmonics of cyclotron emission. A high-state mass accretion rate ∼ 0.4-1× 10^{-10} M_{\odot } yr^{-1}, lower than that of cataclysmic variables above the gap and close to that of systems below it, is estimated. With 2PBC J0658.0-1746, the number of hard X-ray-selected polars increases to 13 members, suggesting that they are not as rare as previously believed.Scopus© Citations 11 198 39 - Some of the metrics are blocked by yourconsent settings
Publication Open Access A 3.9 km baseline intensity interferometry photon counting experiment(SPIE, The International Society for Optical Engineering, 2016); ; ;Barbieri, Cesare ;Barbieri, Mauro ;Verroi, Enrico; ;Favazza, Paolo; In the last years we have operated two very similar ultrafast photon counting photometers (Iqueye and Aqueye+) on different telescopes. The absolute time accuracy in time tagging the detected photon with these instruments is of the order of 500 ps for hours of observation, allowing us to obtain, for example, the most accurate ever light curve in visible light of the optical pulsars. Recently we adapted the two photometers for working together on two telescopes at Asiago (Italy), for realizing an Hanbury-Brown and Twiss Intensity Interferometry like experiment with two 3.9 km distant telescopes. In this paper we report about the status of the activity and on the very preliminary results of our first attempt to measure the photon intensity correlation.Scopus© Citations 9 153 24 - Some of the metrics are blocked by yourconsent settings
Publication Open Access 3DPD: A photogrammetric pipeline for a PUSH frame stereo cameras(2021); ; ; ; ;Tulyakov, S.; ;Pommerol, A.Thomas, N.An innovative photogrammetric pipeline has been developed by INAF-Padova for the processing of the stereo images from the CaSSIS (Colour and Stereo Imaging System) (Thomas et al., 2014). CaSSIS is the multispectral stereo push frame camera on board ExoMars TGO (Trace Gas Orbiter) which will image 1.5% of the Mars surface in stereo mode with a spatial resolution of 4.6 m/pixel: the highest resolution single pass stereo capability currently operating at Mars. Data acquisition started in April 2018. The camera is able to provide two images of the same target from two different points of view along the same orbit and within one minute. The telescope is mounted on a rotational stage and its boresight is oriented to 10° with respect to nadir direction. After the acquisition of the first set of images looking forward along track, the rotational stage is rotated by 180° and a second set of images (looking backward) is acquired. The stereo pairs can then be processed to provide the 3D topography of specific targets.The suite of photogrammetry and imaging tools, named 3DPD (3Dimensional reconstruction of Planetary Data) (Simioni et al. 2017), is designed for processing stereo push frame data and producing the three-dimensional data for geomorphological analysis of planetary surfaces.
The workflow involves a MATLAB tool for the preparation of the inputs (the mosaicked images and the projection matrices) to be ingested into the 3DPD matching core software. The pipeline is in continuous development and routinely ingests a large number of images that CaSSIS is presently acquiring and will continue to acquire in the future. CaSSIS 3DPD products are the unique DTMs available nowadays and the stereo products have been considered in some scientific work (as described in Section 6.2). The same pipeline faces the need of a dedicated pipeline for the Mercury Global Mapping with the Spectrometers and Imagers for the Mercury Planetary Orbiter (MPO) BepiColombo Integrated Observatory SYStem (SIMBIO-SYS) (Cremonese et al., 2020).
Scopus© Citations 17 31 13 - Some of the metrics are blocked by yourconsent settings
Publication Open Access The 3rd AGILE Terrestrial Gamma Ray Flash Catalog. Part I: Association to Lightning Sferics(2020) ;Lindanger, A.; ;Maiorana, C. ;Sarria, D. ;Albrechtsen, K. ;Østgaard, N. ;Galli, M.; ; ; ; We present a complete and systematic search for terrestrial gamma-ray flashes (TGFs), detected by AGILE, that are associated with radio sferics detected by the World Wide Lightning Location Network (WWLLN) in the period February 2009 to September 2018. The search algorithms and characteristics of these new TGFs will be presented and discussed. The number of WWLLN identified (WI) TGFs shows that previous TGF selection criteria needs to be reviewed as they do not identify all the WI TGFs in the data set. In this analysis we confirm with an independent data set that WI TGFs tend to have shorter time duration than TGFs without a WWLLN match. TGFs occurs more often on coastal and ocean regions compared to the distribution of lightning activity. Several multipulse TGFs were identified and their WWLLN match are always associated with the last gamma-ray pulse. We also present the first Terrestrial Electron Beam detected by AGILE. This data set together with the TGF sample identified by selection criteria (companion paper Maiorana et al., 2020) constitute the 3rd AGILE TGF catalog.Scopus© Citations 24 98 31