Browsing by Department "O.A. Torino"
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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.152 68 - Some of the metrics are blocked by yourconsent settings
Publication Open Access The 10 parsec sample in the Gaia era(2021) ;Céline Reylé ;Kevin Jardine ;Pascal Fouqué ;Jose A. Caballero ;Richard L. SmartThe nearest stars provide a fundamental constraint for our understanding of stellar physics and the Galaxy. The nearby sample serves as an anchor where all objects can be seen and understood with precise data. This work is triggered by the most recent data release of the astrometric space mission Gaia and uses its unprecedented high precision parallax measurements to review the census of objects within 10 pc. The first aim of this work was to compile all stars and brown dwarfs within 10 pc observable by Gaia, and compare it with the Gaia Catalogue of Nearby Stars as a quality assurance test. We complement the list to get a full 10 pc census, including bright stars, brown dwarfs, and exoplanets. We started our compilation from a query on all objects with a parallax larger than 100 mas using SIMBAD. We completed the census by adding companions, brown dwarfs with recent parallax measurements not in SIMBAD yet, and vetted exoplanets. The compilation combines astrometry and photometry from the recent Gaia Early Data Release 3 with literature magnitudes, spectral types and line-of-sight velocities. We give a description of the astrophysical content of the 10 pc sample. We find a multiplicity frequency of around 28%. Among the stars and brown dwarfs, we estimate that around 61% are M stars and more than half of the M stars are within the range M3.0 V to M5.0 V. We give an overview of the brown dwarfs and exoplanets that should be detected in the next Gaia data releases along with future developments. We provide a catalogue of 540 stars, brown dwarfs, and exoplanets in 339 systems, within 10 pc from the Sun. This list is as volume-complete as possible from current knowledge and provides benchmark stars that can be used, for instance, to define calibration samples and to test the quality of the forthcoming Gaia releases. It also has a strong outreach potential.93 56 - 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.112 34 - 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.61 24 - Some of the metrics are blocked by yourconsent settings
Publication Open Access 2nd generation ITM M2Number: 271This report describes the study of an alternative optical design for the ITM (International Telescope Maffei) ex-IRAIT telescope installed at Concordia Base in Antarctica1234 . The goal is to reduce the focal number of the telescope.67 23 - Some of the metrics are blocked by yourconsent settings
Publication Open Access A 3-Year Sample of Almost 1,600 Elves Recorded Above South America by the Pierre Auger Cosmic-Ray Observatory(2020) ;Aab, A. ;Abreu, P.; ;Albuquerque, I. F. M. ;Albury, J. M. ;Allekotte, I. ;Almela, A. ;Alvarez Castillo, J. ;Alvarez-Muñiz, J. ;Anastasi, G. A. ;Anchordoqui, L. ;Andrada, B. ;Andringa, S. ;Aramo, C. ;Asorey, H. ;Assis, P. ;Avila, G. ;Badescu, A. M. ;Bakalova, A. ;Balaceanu, A. ;Barbato, F. ;Barreira Luz, R. J. ;Baur, S. ;Becker, K. H. ;Bellido, J. A. ;Berat, C. ;Bertaina, M. E. ;Bertou, X. ;Biermann, P. L. ;Biteau, J. ;Blaess, S. G. ;Blanco, A. ;Blazek, J. ;Bleve, C. ;Boháčová, M. ;Boncioli, D. ;Bonifazi, C. ;Borodai, N. ;Botti, A. M. ;Brack, J. ;Bretz, T. ;Bridgeman, A. ;Briechle, F. L. ;Buchholz, P. ;Bueno, A. ;Buitink, S. ;Buscemi, M. ;Caballero-Mora, K. S. ;Caccianiga, L. ;Calcagni, L. ;Cancio, A. ;Canfora, F. ;Carceller, J. M. ;Caruso, R.; ;Catalani, F. ;Cataldi, G. ;Cazon, L. ;Cerda, M. ;Chinellato, J. A. ;Chudoba, J. ;Chytka, L. ;Clay, R. W. ;Cobos Cerutti, A. C. ;Colalillo, R. ;Coleman, A. ;Coluccia, M. R. ;Conceição, R. ;Condorelli, A. ;Consolati, G. ;Contreras, F. ;Cooper, M. J. ;Coutu, S. ;Covault, C. E. ;Daniel, B. ;Dasso, S. ;Daumiller, K. ;Dawson, B. R. ;Day, J. A. ;de Almeida, R. M. ;de Jong, S. J. ;Mauro, G. ;de Mello Neto, J. R. T. ;Mitri, I. ;de Oliveira, J. ;de Oliveira Salles, F. O. ;de Souza, V. ;Debatin, J. ;del Río, M. ;Deligny, O. ;Dhital, N. ;Díaz Castro, M. L. ;Diogo, F. ;Dobrigkeit, C. ;D'Olivo, J. C. ;Dorosti, Q. ;dos Anjos, R. C. ;Dova, M. T. ;Dundovic, A. ;Ebr, J. ;Engel, R. ;Erdmann, M. ;Escobar, C. O. ;Etchegoyen, A. ;Falcke, H. ;Farmer, J. ;Farrar, G. ;Fauth, A. C. ;Fazzini, N. ;Feldbusch, F. ;Fenu, F. ;Ferreyro, L. P. ;Figueira, J. M. ;Filipčič, A. ;Freire, M. M. ;Fujii, T. ;Fuster, A. ;García, B. ;Gemmeke, H. ;Gherghel-Lascu, A. ;Ghia, P. L. ;Giaccari, U. ;Giammarchi, M. ;Giller, M. ;Głas, D. ;Glombitza, J. ;Gobbi, F. ;Golup, G. ;Gómez Berisso, M. ;Gómez Vitale, P. F. ;Gongora, J. P. ;González, N. ;Goos, I. ;Góra, D.; ;Gottowik, M. ;Grubb, T. D. ;Guarino, F. ;Guedes, G. P. ;Guido, E. ;Halliday, R. ;Hampel, M. R. ;Hansen, P. ;Harari, D. ;Harrison, T. A. ;Harvey, V. M. ;Haungs, A. ;Hebbeker, T. ;Heck, D. ;Heimann, P. ;Hill, G. C. ;Hojvat, C. ;Holt, E. M. ;Homola, P. ;Hörandel, J. R. ;Horvath, P. ;Hrabovský, M. ;Huege, T. ;Hulsman, J. ;Insolia, A. ;Isar, P. G. ;Jandt, I. ;Johnsen, J. A. ;Josebachuili, M. ;Jurysek, J. ;Kääpä, A. ;Kampert, K. H. ;Keilhauer, B. ;Kemmerich, N. ;Kemp, J. ;Klages, H. O. ;Kleifges, M. ;Kleinfeller, J. ;Krause, R. ;Kuempel, D. ;Kukec Mezek, G. ;Kuotb Awad, A. ;Lago, B. L. ;LaHurd, D. ;Lang, R. G. ;Legumina, R. ;Leigui de Oliveira, M. A. ;Lenok, V. ;Letessier-Selvon, A. ;Lhenry-Yvon, I. ;Lippmann, O. C. ;Lo Presti, D. ;Lopes, L. ;López, R. ;López Casado, A. ;Lorek, R. ;Luce, Q. ;Lucero, A. ;Malacari, M. ;Mancarella, G. ;Mandat, D. ;Manning, B. C. ;Mantsch, P. ;Mariazzi, A. G. ;Mariş, I. C. ;Marsella, G. ;Martello, D. ;Martinez, H. ;Martínez Bravo, O. ;Mastrodicasa, M. ;Mathes, H. J. ;Mathys, S. ;Matthews, J. ;Matthiae, G. ;Mayotte, E. ;Mazur, P. O. ;Medina-Tanco, G. ;Melo, D. ;Menshikov, A. ;Merenda, K. -D. ;Michal, S. ;Micheletti, M. I. ;Middendorf, L. ;Miramonti, L. ;Mitrica, B. ;Mockler, D. ;Mollerach, S. ;Montanet, F. ;Morello, C.; ;Mostafá, M. ;Müller, A. L. ;Muller, M. A. ;Müller, S. ;Mussa, R. ;Nellen, L. ;Nguyen, P. H. ;Niculescu-Oglinzanu, M. ;Niechciol, M. ;Nitz, D. ;Nosek, D. ;Novotny, V. ;Noža, L. ;Nucita, A. ;Núñez, L. A. ;Olinto, A. ;Palatka, M. ;Pallotta, J. ;Panetta, M. P. ;Papenbreer, P. ;Parente, G. ;Parra, A. ;Pech, M. ;Pedreira, F. ;Pekala, J. ;Pelayo, R. ;Peña-Rodriguez, J. ;Pereira, L. A. S. ;Perlin, M. ;Perrone, L. ;Peters, C. ;Petrera, S. ;Phuntsok, J. ;Pierog, T. ;Pimenta, M. ;Pirronello, V. ;Platino, M. ;Poh, J. ;Pont, B. ;Porowski, C. ;Prado, R. R. ;Privitera, P. ;Prouza, M. ;Puyleart, A. ;Querchfeld, S. ;Quinn, S. ;Ramos-Pollan, R. ;Rautenberg, J. ;Ravignani, D. ;Reininghaus, M. ;Ridky, J. ;Riehn, F. ;Risse, M. ;Ristori, P. ;Rizi, V. ;Rodrigues de Carvalho, W. ;Rodriguez Rojo, J. ;Roncoroni, M. J. ;Roth, M. ;Roulet, E. ;Rovero, A. C. ;Ruehl, P. ;Saffi, S. J. ;Saftoiu, A. ;Salamida, F. ;Salazar, H. ;Salina, G. ;Sanabria Gomez, J. D. ;Sánchez, F. ;Santos, E. M. ;Santos, E. ;Sarazin, F. ;Sarmento, R. ;Sarmiento-Cano, C. ;Sato, R. ;Savina, P. ;Schauer, M. ;Scherini, V. ;Schieler, H. ;Schimassek, M. ;Schimp, M. ;Schlüter, F. ;Schmidt, D. ;Scholten, O. ;Schovánek, P. ;Schröder, F. G. ;Schröder, S. ;Schumacher, J. ;Sciutto, S. J. ;Scornavacche, M. ;Shellard, R. C. ;Sigl, G. ;Silli, G. ;Sima, O. ;Å mída, R. ;Snow, G. R. ;Sommers, P. ;Soriano, J. F. ;Souchard, J. ;Squartini, R. ;Stanca, D. ;Stanič, S. ;Stasielak, J. ;Stassi, P. ;Stolpovskiy, M. ;Streich, A. ;Suarez, F. ;Suárez-Durán, M. ;Sudholz, T. ;Suomijärvi, T. ;Supanitsky, A. D. ;Å upík, J. ;Szadkowski, Z. ;Taboada, A. ;Taborda, O. A. ;Tapia, A. ;Timmermans, C. ;Todero Peixoto, C. J. ;Tomé, B. ;Torralba Elipe, G. ;Travaini, A. ;Travnicek, P. ;Trini, M. ;Tueros, M. ;Ulrich, R. ;Unger, M. ;Urban, M. ;Valdés Galicia, J. F. ;Valiño, I. ;Valore, L. ;van Bodegom, P. ;van den Berg, A. M. ;van Vliet, A. ;Varela, E. ;Vargas Cárdenas, B. ;Veberič, D. ;Ventura, C. ;Vergara Quispe, I. D. ;Verzi, V. ;Vicha, J. ;Villaseñor, L. ;Vink, J. ;Vorobiov, S. ;Wahlberg, H. ;Watson, A. A. ;Weber, M. ;Weindl, A. ;Wiedeński, M. ;Wiencke, L. ;Wilczyński, H. ;Winchen, T. ;Wirtz, M. ;Wittkowski, D. ;Wundheiler, B. ;Yang, L. ;Yushkov, A. ;Zas, E. ;Zavrtanik, D. ;Zavrtanik, M. ;Zehrer, L. ;Zepeda, A. ;Zimmermann, B. ;Ziolkowski, M. ;Zong, Z.Elves are a class of transient luminous events, with a radial extent typically greater than 250 km, that occur in the lower ionosphere above strong electrical storms. We report the observation of 1,598 elves, from 2014 to 2016, recorded with unprecedented time resolution (100 ns) using the fluorescence detector (FD) of the Pierre Auger Cosmic-Ray Observatory. The Auger Observatory is located in the Mendoza province of Argentina with a viewing footprint for elve observations of 3·106 km2, reaching areas above the Pacific and Atlantic Oceans, as well as the Córdoba region, which is known for severe convective thunderstorms. Primarily designed for ultrahigh energy cosmic-ray observations, the Auger FD turns out to be very sensitive to the ultraviolet emission in elves. The detector features modified Schmidt optics with large apertures resulting in a field of view that spans the horizon, and year-round operation on dark nights with low moonlight background, when the local weather is favorable. The measured light profiles of 18% of the elve events have more than one peak, compatible with intracloud activity. Within the 3-year sample, 72% of the elves correlate with the far-field radiation measurements of the World Wide Lightning Location Network. The Auger Observatory plans to continue operations until at least 2025, including elve observations and analysis. To the best of our knowledge, this observatory is the only facility on Earth that measures elves with year-round operation and full horizon coverage.95 30 - Some of the metrics are blocked by yourconsent settings
Publication Open Access The 3CR Chandra Snapshot Survey: Extragalactic Radio Sources with 0.5 < z < 1.0(2018); ;Missaglia, V. ;Stuardi, C. ;Harris, D. E. ;Kraft, R. P.; ; ;Tremblay, G. R. ;Baum, S. A. ;O'Dea, C. P. ;Wilkes, B. J. ;Kuraszkiewicz, J.Forman, W. R.This paper presents the analysis of Chandra X-ray snapshot observations of a subsample of the extragalactic sources listed in the revised Third Cambridge radio catalog (3CR), previously lacking X-ray observations and thus observed during Chandra Cycle 15. This data set extends the current Chandra coverage of the 3CR extragalactic catalog up to redshift z = 1.0. Our sample includes 22 sources consisting of 1 compact steep spectrum source, 3 quasars (QSOs), and 18 FR II radio galaxies. As in our previous analyses, here we report the X-ray detections of radio cores and extended structures (i.e., knots, hotspots, and lobes) for all sources in the selected sample. We measured their X-ray intensities in three energy ranges, soft (0.5-1 keV), medium (1-2 keV), and hard (2-7 keV), and we also performed standard X-ray spectral analysis for brighter nuclei. All radio nuclei in our sample have an X-ray counterpart. We also discovered X-ray emission associated with the eastern knot of 3CR 154, with radio hotspots in 3CR 41, 3CR 54, and 3CR 225B, and with the southern lobe of 3CR 107. Extended X-ray radiation around the nuclei 3CR 293.1 and 3CR 323 on a scale of few tens of kiloparsecs was also found. X-ray extended emission, potentially arising from the hot gas in the intergalactic medium and/or due to the high-energy counterpart of lobes, is detected for 3CR 93, 3CR 154, 3CR 292, and 3CR 323 over a scale of a few hundred kiloparsecs. Finally, this work also presents an update on the state-of-the-art of Chandra and XMM-Newton observations for the entire 3CR sample.83 18 - Some of the metrics are blocked by yourconsent settings
Publication Open Access The 3CR Chandra Snapshot Survey: Extragalactic Radio Sources with Redshifts between 1 and 1.5(2018) ;Stuardi, C. ;Missaglia, V.; ;Ricci, F.; ; ;Kraft, R. P. ;Tremblay, G. R. ;Baum, S. A. ;O'Dea, C. P. ;Wilkes, B. J. ;Kuraszkiewicz, J. ;Forman, W. R.Harris, D. E.The aim of this paper is to present an analysis of newly acquired X-ray observations of 16 extragalactic radio sources listed in the Third Cambridge Revised (3CR) catalog and not previously observed by Chandra. Observations were performed during Chandra Cycle 17, extending X-ray coverage for the 3CR extragalactic catalog up to z = 1.5. Among the 16 targets, two lie at z < 0.5 (3CR 27 at z = 0.184 and 3CR 69 at z = 0.458) all of the remaining 14 have redshifts between 1.0 and 1.5. In the current sample, there are three compact steep spectrum (CSS) sources, three quasars, and an FR I radio galaxy, while the other nine are FR II radio galaxies. All radio sources have an X-ray counterpart. We measured nuclear X-ray fluxes as well as X-ray emission associated with radio jet knots, hotspots, or lobes in three energy bands: soft (0.5-1 keV), medium (1-2 keV), and hard (2-7 keV). We also performed standard X-ray spectral analysis for the four brightest nuclei. We discovered X-ray emission associated with the radio lobe of 3CR 124, a hotspot of the quasar 3CR 220.2, another hotspot of the radio galaxy 3CR 238, and the jet knot of 3CR 297. We also detected extended X-ray emission around the nuclear region of 3CR 124 and 3CR 297 on scales of several tens of kiloparsecs. Finally, we present an update on the X-ray observations performed with Chandra and XMM-Newton on the entire 3CR extragalactic catalog.78 21 - Some of the metrics are blocked by yourconsent settings
Publication Open Access 3D Relativistic MHD numerical simulations of X-shaped radio sources(2017); ; ; Massaglia S.A significant fraction of extended radio sources presents a peculiar X-shaped radio morphology: in addition to the classical double lobed structure, radio emission is also observed along a second axis of symmetry in the form of diffuse wings or tails. In a previous investigation we showed the existence of a connection between the radio morphology and the properties of the host galaxies. Motivated by this connection we performed two-dimensional numerical simulations showing that X-shaped radio sources may naturally form as a jet propagates along the major axis a highly elliptical density distribution, because of the fast expansion of the cocoon along the minor axis of the distribution. Aims: We intend to extend our analysis by performing three-dimensional numerical simulations and investigating the role of different parameters in determining the formation of the X-shaped morphology. Methods: The problem is addressed by numerical means, carrying out three-dimensional relativistic magnetohydrodynamic simulations of bidirectional jets propagating in a triaxial density distribution. Results: We show that only jets with power ≲ 1044 erg s-1 can give origin to an X-shaped morphology and that a misalignment of 30° between the jet axis and the major axis of the density distribution is still favourable to the formation of this kind of morphology. In addition we compute synthetic radio emission maps and polarization maps. Conclusions: In our scenario for the formation of X-shaped radio sources only low power FRII can give origin to such kind of morphology. Our synthetic emission maps show that the different observed morphologies of X-shaped sources can be the result of similar structures viewed under different perspectives.104 46 - Some of the metrics are blocked by yourconsent settings
Publication Open Access A 3D view of the Hyades stellar and sub-stellar population(2019) ;Lodieu, N.; ;Perez-Garrido, A.Our scientific goal is to provide a 3D map of the nearest open cluster to the Sun, the Hyades, combining the recent release of Gaia astrometric data, ground-based parallaxes of sub-stellar member candidates and photometric data from surveys which cover large areas of the cluster. We combined the second Gaia release with ground-based H-band parallaxes obtained with the infrared camera on the 2-m robotic Liverpool telescope to astrometrically identify stellar and sub-stellar members of the Hyades, the nearest open cluster to the Sun. We find 1764 objects within 70 degree radius from the cluster center from the Gaia second data release, whose kinematic properties are consistent with the Hyades. We limit our study to 30 pc from the cluster center (47.03+/-0.20 pc) where we identify 710 candidate members, including 85 and 385 in the core and tidal radius, respectively. We determine proper motions and parallaxes of eight candidate brown dwarf members and confirm their membership. Using the 3D positions and a model-based mass-luminosity relation we derive a luminosity and mass function in the 0.04 to 2.5 Msun range. We confirm evidence for mass segregation in the Hyades and find a dearth of brown dwarfs in the core of the cluster. From the white dwarf members we estimate an age of 640$^{+67}_{-49}$ Myr. We identify a list of members in the Hyades cluster from the most massive stars down to the brown dwarfs. We produce for the first time a 3D map of the Hyades cluster in the stellar and sub-stellar regimes and make available the list of candidate members.90 30 - Some of the metrics are blocked by yourconsent settings
Publication Open Access 4.5 Years of Multi-wavelength Observations of MRK 421 During the ARGO-YBJ and FERMI Common Operation Time(2016) ;Bartoli, B. ;Bernardini, P. ;Bi, X. J. ;Cao, Z. ;Catalanotti, S. ;Chen, S. Z. ;Chen, T. L. ;Cui, S. W. ;Dai, B. Z. ;D'Amone, A. ;Danzengluobu ;De Mitri, I. ;D'Ettorre Piazzoli, B. ;Di Girolamo, T. ;Di Sciascio, G. ;Feng, C. F. ;Feng, Zhaoyang ;Feng, Zhenyong ;Gou, Q. B. ;Guo, Y. Q. ;He, H. H. ;Hu, Haibing ;Hu, Hongbo ;Iacovacci, M. ;Iuppa, R. ;Jia, H. Y. ;Labaciren ;Li, H. J. ;Liu, C.; ;Liu, M. Y. ;Lu, H. ;Ma, L. L. ;Ma, X. H. ;Mancarella, G. ;Mari, S. M. ;Marsella, G. ;Mastroianni, S. ;Montini, P. ;Ning, C. C. ;Perrone, L. ;Pistilli, P. ;Salvini, P. ;Santonico, R. ;Shen, P. R. ;Sheng, X. D. ;Shi, F. ;Surdo, A. ;Tan, Y. H.; ; ;Vigorito, C. ;Wang, H. ;Wu, C. Y. ;Wu, H. R. ;Xue, L. ;Yang, Q. Y. ;Yang, X. C. ;Yao, Z. G. ;Yuan, A. F. ;Zha, M. ;Zhang, H. M. ;Zhang, L. ;Zhang, X. Y. ;Zhang, Y. ;Zhao, J. ;Zhaxiciren ;Zhaxisangzhu ;Zhou, X. X. ;Zhu, F. R. ;Zhu, Q. Q.ARGO-YBJ CollaborationWe report on the extensive multi-wavelength observations of the blazar Markarian 421 (Mrk 421) covering radio to γ-rays, during the 4.5 year period of ARGO-YBJ and Fermi common operation time, from 2008 August to 2013 February. These long-term observations, extending over an energy range of 18 orders of magnitude, provide a unique chance to study the variable emission of Mrk 421. In particular, due to the ARGO-YBJ and Fermi data, the entire energy range from 100 MeV to 10 TeV is covered without any gap. In the observation period, Mrk 421 showed both low- and high-activity states at all wavebands. The correlations among flux variations in different wavebands were analyzed. The X-ray flux is clearly correlated with the TeV γ-ray flux, while the GeV γ-rays only show a partial correlation with the TeV γ-rays. Radio and UV fluxes seem to be weakly or not correlated with the X-ray and γ-ray fluxes. Seven large flares, including five X-ray flares and two GeV γ-ray flares with variable durations (3-58 days), and one X-ray outburst phase were identified and used to investigate the variation of the spectral energy distribution with respect to a relative quiescent phase. During the outburst phase and the seven flaring episodes, the peak energy in X-rays is observed to increase from sub-keV to a few keV. The TeV γ-ray flux increases up to 0.9-7.2 times the flux of the Crab Nebula. The behavior of GeV γ-rays is found to vary depending on the flare, a feature that leads us to classify flares into three groups according to the GeV flux variation. Finally, the one-zone synchrotron self-Compton model was adopted to describe the emission spectra. Two out of three groups can be satisfactorily described using injected electrons with a power-law spectral index around 2.2, as expected from relativistic diffuse shock acceleration, whereas the remaining group requires a harder injected spectrum. The underlying physical mechanisms responsible for different groups may be related to the acceleration process or to the environment properties.98 26 - Some of the metrics are blocked by yourconsent settings
Publication Open Access 49 new T dwarfs identified using methane imaging(2015) ;Cardoso, C. V. ;Burningham, B.; ;van Spaandonk, L. ;Baker, D. ;Smith, L. C. ;Zhang, Z. H. ;Andrei, A. H.; ;Dhital, S. ;Jones, H. R. A.; ; ;Pinfield, D. J.Tinney, C. G.We present the discovery of 49 new photometrically classified T dwarfs from the combination of large infrared and optical surveys combined with follow-up Telescopio Nazionale Galileo photometry. We used multiband infrared and optical photometry from the United Kingdom Infrared Telescope and Sloan Digital Sky Surveys to identify possible brown dwarf candidates, which were then confirmed using methane filter photometry. We have defined a new photometric conversion between CH4s - CH4l colour and spectral type for T4-T8 brown dwarfs based on a part of the sample that has been followed up using methane photometry and spectroscopy. Using methane differential photometry as a proxy for spectral type for T dwarfs has proved to be a very efficient technique. Of a subset of 45 methane selected brown dwarfs that were observed spectroscopically, 100 per cent were confirmed as T dwarfs. Future deep imaging surveys will produce large samples of faint brown dwarf candidates, for which spectroscopy will not be feasible. When broad wavelength coverage is unavailable, methane imaging offers a means to efficiently classify candidates from such surveys using just a pair of near-infrared images.113 23 - Some of the metrics are blocked by yourconsent settings
Publication Open Access The 500 ks Chandra observation of the z = 6.31 QSO SDSS J1030 + 0524(2018) ;Nanni, R.; ;Vignali, C.; ; ; ;Zamorani, G.; ; ;Brusa, M.; ;Iwasawa, K.; ;Vito, F.; ;Costa, T. ;Risaliti, G.; ; ; ;Rosati, P. ;Chiaberge, M. ;Caminha, G. B. ;Sani, E. ;Cappelluti, N.Norman, C.We present the results from a 500 ks Chandra observation of the z = 6.31 QSO SDSS J1030 + 0524. This is the deepest X-ray observation to date of a z 6 QSO. The QSO is detected with a total of 125 net counts in the full (0.500A0-7 keV) band and its spectrum can be modeled by a single power-law model with photon index of Γ = 1.81 ± 0.18 and full band flux of f = 3.95 × 10-15 erg s-1 cm-2. When compared with the data obtained by XMM-Newton in 2003, our Chandra observation in 2017 shows a harder (∆Γ ≈ -0.6) spectrum and a 2.5 times fainter flux. Such a variation, in a timespan of 2 yr rest-frame, is unexpected for such a luminous QSO powered by a > 109M☉ black hole. The observed source hardening and weakening could be related to an intrinsic variation in the accretion rate. However, the limited photon statistics does not allow us to discriminate between an intrinsic luminosity and spectral change, and an absorption event produced by an intervening gas cloud along the line of sight. We also report the discovery of diffuse X-ray emission that extends for 30″ × 20″ southward of the QSO with a signal-to-noise ratio (S/N) of approximately six, hardness ratio of HR = 0.03+0.20-0.25, and soft band flux of f0.5- keV = 1.1+0.3-0.3 × 10-15 erg s-1 cm-2 , that is not associated to a group or cluster of galaxies. We discuss two possible explanations for the extended emission, which may be either associated with the radio lobe of a nearby, foreground radio galaxy (at z ≈ 1 - 2), or ascribed to the feedback from the QSO itself acting on its surrounding environment, as proposed by simulations of early black hole formation.92 21 - Some of the metrics are blocked by yourconsent settings
Publication Open Access A 5D view of the Alpha Per, Pleiades, and Praesepe clusters(2019) ;Lodieu, N. ;Perez-Garrido, A.; Aims: Our scientific goal is to provide revised membership lists of the Alpha Per, Pleiades, and Praesepe clusters exploiting the second data release of Gaia and produce five-dimensional maps (ra, dec, parallax, pmRA, pmDEC) of these clusters. Methods: We implemented the kinematic method combined with the statistical treatment of parallaxes and proper motions to identify astrometric member candidates of three of the most nearby and best studied open clusters in the sky. Results: We cross-correlated the Gaia catalogue with large-scale public surveys to complement the astrometry of Gaia with multi-band photometry from the optical to the mid-infrared. We identified 517, 1248, and 721 bona-fide astrometric member candidates inside the tidal radius of the Alpha Per, the Pleiades, and Praesepe, respectively. We cross-matched our final samples with catalogues from previous surveys to address the level of completeness. We update the main physical properties of the clusters, including mean distance and velocity as well as core, half-mass, and tidal radii. We infer updated ages from the white dwarf members of the Pleiades and Praesepe. We derive the luminosity and mass functions of the three clusters and compare them to the field mass function. We compute the positions in space of all member candidates in the three regions to investigate their distribution in space. Conclusions: We provide updated distances and kinematics for the three clusters. We identify a list of members in the Alpha Per, Pleiades, and Praesepe clusters from the most massive stars all the way down into the hydrogen-burning limit with a higher confidence and better astrometry than previous studies. We produce complete 5D maps of stellar and substellar bona-fide members in these three regions. ABRIDGED78 38 - Some of the metrics are blocked by yourconsent settings
Product Metadata only A centred three mirror anastigmat(2024); ; ; ; The CEntral (field) Three-mirror Anastigmat (CETA) telescope is designed on the specifications of the proposed Theia mission, aiming at high precision differential astrometry over a large field, for exo-planetary system characterization and dark matter /dark energy search through the dynamics of star clusters. Usually, Three Mirror Anastigmat designs are either off-axis in terms of field, or decentered in terms of pupil. We propose a family of solutions using fully centred optics and a large on-axis field, at the expense of a non negligible central obscuration. We analyse in particular a 1 m class compact telescope, with 15 m effective focal length, i.e. suited to small pixel (4-6 μm) CMOS detectors operating in the visible and near IR. Due to the underlying symmetry, the resulting optical response is quite good over a 14 arcmin radius field, and it is of special interest to astrometry applications. Also, manufacturing, alignment and calibration can be expected to benefit significantly; some basic aspects are preliminarily considered. - Some of the metrics are blocked by yourconsent settings
Publication Restricted A chemical survey of exoplanets with ARIEL(2018) ;Tinetti, Giovanna ;Drossart, Pierre ;Eccleston, Paul ;Hartogh, Paul ;Heske, Astrid ;Leconte, Jérémy; ;Ollivier, Marc ;Pilbratt, Göran ;Puig, Ludovic; ;Radioti, Aikaterini ;Réess, Jean-Michel ;Rezac, Ladislav ;Rocchetto, Marco ;Rosich, Albert; ; ;Santerne, Alexandre; ; ;Duong, Bastien ;Savini, Giorgio; ;Sicardy, Bruno ;Sierra, Carles; ;Skup, Konrad ;Snellen, Ignas ;Sobiecki, Mateusz; ;Soret, Lauriane ;Eales, Stephen ;Charnay, Bejamin; ;Min, Michiel ;Stiepen, A. ;Strugarek, Antoine ;Taylor, Jake ;Taylor, William; ;Tessenyi, Marcell; ;Edwards, Billy ;Brun, Allan Sacha ;Miguel, Yamila ;Tucker, C. ;Valencia, Diana ;Vasisht, Gautam ;Nørgaard-Nielsen, Hans Ulrik ;Vazan, Allona ;Vilardell, Francesc ;Vinatier, Sabrine; ; ;Waters, Rens ;Wawer, Piotr ;Pinfield, David ;Bryson, Ian ;Wawrzaszek, Anna ;Whitworth, Anthony ;Yung, Yuk L. ;Yurchenko, Sergey N. ;Rataj, Mirek ;Osorio, María Rosa Zapatero; ;Zellem, Robert; ;Zwart, Frans ;Sarkar, Subhajit ;Ray, Tom ;Bujwan, Waldemar ;Ribas, Ignasi ;Swain, Mark ;Szabo, Robert ;Werner, Stephanie ;Fletcher, Leigh ;Barstow, Joanna ;Burleigh, Matt ;Cho, James ;du Foresto, Vincent Coudé ;Selsis, Franck ;Coustenis, Athena ;Decin, Leen ;Casewell, Sarah ;Encrenaz, Therese ;Tennyson, Jonathan ;Beaulieu, Jean-Philippe ;Triaud, Amaury ;Venot, Olivia ;Waldmann, Ingo ;Waltham, David ;Wright, Gillian ;Amiaux, Jerome ;Minier, Vincent; ;Auguères, Jean-Louis ;Berthé, Michel ;Forget, François ;Bezawada, Naidu ;Bishop, Georgia ;Bowles, Neil ;Coffey, Deirdre ;Colomé, Josep ;Crook, Martin ;Crouzet, Pierre-Elie ;Morello, Giuseppe ;Da Peppo, Vania ;Vandenbussche, Bart ;Fossey, Steve ;Sanz, Isabel Escudero; ;Frericks, Martin ;Hunt, Tom ;Kohley, Ralf ;Middleton, Kevin; ;Ottensamer, Roland; ; ; ;Pearson, Chris ;Chen, Guo ;Stamper, Richard ;Symonds, Kate ;Rengel, Miriam ;Renotte, Etienne ;Ade, Peter; ;Alard, Christophe ;Narita, Norio ;Galand, Marina ;Allard, Nicole; ;André, Yves; ; ;Argyriou, Ioannis ;Aylward, Alan; ;Bakos, Gaspar ;Banaszkiewicz, Marek ;Fränz, Markus; ;Barlow, Mike ;Batista, Virginie; ; ; ;Bernardi, Pernelle ;Bézard, Bruno ;Blecka, Maria ;Bolmont, Emeline ;Fujii, Yuka ;Clédassou, Rodolphe ;Nguyen Tong, N.; ; ; ;Deroo, Pieter; ;Dominik, Carsten; ;Doublier, Vanessa ;García-Piquer, Álvaro ;Doyle, Simon ;Doyon, René; ;Drummond, Benjamin ;Gear, Walter ;Geoffray, Hervé ;Gérard, Jean Claude ;Gesa, Lluis ;Gomez, H. ;Buchave, Lars A. ;Graczyk, Rafał ;Gillon, Michael ;Lagage, Pierre-Olivier ;Griffith, Caitlin ;Grodent, Denis; ;Gustin, Jacques ;Hamano, Keiko ;Hargrave, Peter ;Hello, Yann ;Heng, Kevin ;Herrero, Enrique ;Helled, Ravit ;Ferus, Martin ;Bonfond, Bertrand ;Hornstrup, Allan ;Hubert, Benoit ;Ida, Shigeru ;Ikoma, Masahiro ;Iro, Nicolas ;Irwin, Patrick ;Jarchow, Christopher ;Jaubert, Jean ;Morales, Juan Carlos ;Jones, Hugh ;Julien, Queyrel ;Palle, Enric ;Griffin, Matt ;Kameda, Shingo ;Kerschbaum, Franz ;Kervella, Pierre ;Koskinen, Tommi ;Krijger, Matthijs ;Krupp, Norbert ;Muñoz, Antonio García ;Lafarga, Marina; ;Lellouch, Emanuel ;Palmer, Paul; ;Guedel, Manuel ;Luntzer, A. ;Rank-Lüftinger, Theresa; ;Maldonado, Jesus ;Moneti, Andrea ;Maillard, Jean-Pierre ;Mall, Urs ;Marquette, Jean-Baptiste ;Mathis, Stephane; ;Maxted, Pierre ;Matsuo, Taro ;Justtanont, Kay ;Medvedev, Alexander ;Papageorgiou, Andreas; ;Parmentier, Vivien ;Perger, Manuel; ; ;Pierrehumbert, Ray; ; ;Machado, Pedro ;Piotto, Giampaolo ;Pisano, Giampaolo ;Pascale, EnzoThousands of exoplanets have now been discovered with a huge range of masses, sizes and orbits: from rocky Earth-like planets to large gas giants grazing the surface of their host star. However, the essential nature of these exoplanets remains largely mysterious: there is no known, discernible pattern linking the presence, size, or orbital parameters of a planet to the nature of its parent star. We have little idea whether the chemistry of a planet is linked to its formation environment, or whether the type of host star drives the physics and chemistry of the planet's birth, and evolution. ARIEL was conceived to observe a large number ( 1000) of transiting planets for statistical understanding, including gas giants, Neptunes, super-Earths and Earth-size planets around a range of host star types using transit spectroscopy in the 1.25-7.8 μm spectral range and multiple narrow-band photometry in the optical. ARIEL will focus on warm and hot planets to take advantage of their well-mixed atmospheres which should show minimal condensation and sequestration of high-Z materials compared to their colder Solar System siblings. Said warm and hot atmospheres are expected to be more representative of the planetary bulk composition. Observations of these warm/hot exoplanets, and in particular of their elemental composition (especially C, O, N, S, Si), will allow the understanding of the early stages of planetary and atmospheric formation during the nebular phase and the following few million years. ARIEL will thus provide a representative picture of the chemical nature of the exoplanets and relate this directly to the type and chemical environment of the host star. ARIEL is designed as a dedicated survey mission for combined-light spectroscopy, capable of observing a large and well-defined planet sample within its 4-year mission lifetime. Transit, eclipse and phase-curve spectroscopy methods, whereby the signal from the star and planet are differentiated using knowledge of the planetary ephemerides, allow us to measure atmospheric signals from the planet at levels of 10-100 part per million (ppm) relative to the star and, given the bright nature of targets, also allows more sophisticated techniques, such as eclipse mapping, to give a deeper insight into the nature of the atmosphere. These types of observations require a stable payload and satellite platform with broad, instantaneous wavelength coverage to detect many molecular species, probe the thermal structure, identify clouds and monitor the stellar activity. The wavelength range proposed covers all the expected major atmospheric gases from e.g. H2O, CO2, CH4 NH3, HCN, H2S through to the more exotic metallic compounds, such as TiO, VO, and condensed species. Simulations of ARIEL performance in conducting exoplanet surveys have been performed - using conservative estimates of mission performance and a full model of all significant noise sources in the measurement - using a list of potential ARIEL targets that incorporates the latest available exoplanet statistics. The conclusion at the end of the Phase A study, is that ARIEL - in line with the stated mission objectives - will be able to observe about 1000 exoplanets depending on the details of the adopted survey strategy, thus confirming the feasibility of the main science objectives.176 3 - Some of the metrics are blocked by yourconsent settings
Product Metadata only A hot-Jupiter progenitor on a super-eccentric retrograde orbit(2024) ;Gupta, Arvind F. ;Millholland, Sarah C. ;Im, Haedam ;Dong, Jiayin ;Jackson, Jonathan M. ;Carleo, Ilaria ;Libby-Roberts, Jessica ;Delamer, Megan ;Giovinazzi, Mark R. ;Lin, Andrea S. J. ;Kanodia, Shubham ;Wang, Xian-Yu ;Stassun, Keivan ;Masseron, Thomas ;Dragomir, Diana ;Mahadevan, Suvrath ;Wright, Jason ;Alvarado-Montes, Jaime A. ;Bender, Chad ;Blake, Cullen H. ;Caldwell, Douglas ;Cañas, Caleb I. ;Cochran, William D. ;Dalba, Paul ;Everett, Mark E. ;Fernandez, Pipa ;Golub, Eli ;Guillet, Bruno ;Halverson, Samuel ;Hebb, Leslie ;Higuera, Jesus ;Huang, Chelsea X. ;Klusmeyer, Jessica ;Knight, Rachel ;Leroux, Liouba ;Logsdon, Sarah E. ;Loose, Margaret ;McElwain, Michael W. ;Monson, Andrew ;Ninan, Joe P. ;Nowak, Grzegorz ;Palle, Enric ;Patel, Yatrik ;Pepper, Joshua ;Primm, Michael ;Rajagopal, Jayadev ;Robertson, Paul ;Roy, Arpita ;Schneider, Donald P. ;Schwab, Christian ;Schweiker, Heidi ;Sgro, Lauren ;Shimizu, Masao ;Simard, Georges ;Stefánsson, Gudmundur ;Stevens, Daniel J. ;Villanueva, Steven ;Wisniewski, John ;Will, StefanZiegler, CarlGiant exoplanets orbiting close to their host stars are unlikely to have formed in their present configurations1. These `hot Jupiter' planets are instead thought to have migrated inward from beyond the ice line and several viable migration channels have been proposed, including eccentricity excitation through angular-momentum exchange with a third body followed by tidally driven orbital circularization2,3. The discovery of the extremely eccentric (e = 0.93) giant exoplanet HD 80606 b (ref. 4) provided observational evidence that hot Jupiters may have formed through this high-eccentricity tidal-migration pathway5. However, no similar hot-Jupiter progenitors have been found and simulations predict that one factor affecting the efficacy of this mechanism is exoplanet mass, as low-mass planets are more likely to be tidally disrupted during periastron passage6-8. Here we present spectroscopic and photometric observations of TIC 241249530 b, a high-mass, transiting warm Jupiter with an extreme orbital eccentricity of e = 0.94. The orbit of TIC 241249530 b is consistent with a history of eccentricity oscillations and a future tidal circularization trajectory. Our analysis of the mass and eccentricity distributions of the transiting-warm-Jupiter population further reveals a correlation between high mass and high eccentricity. - Some of the metrics are blocked by yourconsent settings
Publication Metadata only A PAthway Towards the Characterization of Habitable Earths (APACHE)(O.A. Torino, 2008); ; ; ; ; ; ; ;Jones, H.R.A. ;Pinfield, D. ;Calcidese, P. ;Bernagozzi, A.98 - Some of the metrics are blocked by yourconsent settings
Publication Metadata only 75 - Some of the metrics are blocked by yourconsent settings
Publication Open Access A very dark stellar system lost in Virgo: kinematics and metallicity of SECCO 1 with MUSE(2017) ;Beccari, G.; ; ;Coccato, L.; ;Fraternali, F. ;de Zeeuw, P. T. ;Husemann, B. ;Ibata, R. ;Battaglia, G. ;Martin, N.; ; Correnti, M.We present the results of VLT-MUSE (Very Large Telescope-Multi Unit Spectroscopic Explorer) integral field spectroscopy of SECCO 1, a faint, star-forming stellar system recently discovered as the stellar counterpart of an ultracompact high-velocity cloud (HVC 274.68+74.0), very likely residing within a substructure of the Virgo cluster of galaxies. We have obtained the radial velocity of a total of 38 individual compact sources identified as H II regions in the main and secondary bodies of the system, and derived the metallicity for 18 of them. We provide the first direct demonstration that the two stellar bodies of SECCO 1 are physically associated and that their velocities match the H I velocities. The metallicity is quite uniform over the whole system, with a dispersion lower than the uncertainty on individual metallicity estimates. The mean abundance, <12 + log(O/H)> = 8.44, is much higher than the typical values for local dwarf galaxies of similar stellar mass. This strongly suggests that the SECCO 1 stars were born from a pre-enriched gas cloud, possibly stripped from a larger galaxy. Using archival Hubble Space Telescope (HST) images, we derive a total stellar mass of ≃1.6 × 105 M☉ for SECCO 1, confirming that it has a very high H I-to-stellar mass ratio for a dwarf galaxy, M_{H I}/M* ∼ 100. The star formation rate, derived from the Hα flux, is a factor of more than 10 higher than in typical dwarf galaxies of similar luminosity.69 13