Browsing by Department "O.A. Arcetri"
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Publication Open Access A 10-M☉ YSO with a Keplerian disk and a nonthermal radio jet(2019); ; ; ; ;Goddi, C.Context. To constrain present star formation models, we need to simultaneously establish the dynamical and physical properties of disks and jets around young stars. Aims: We previously observed the star-forming region G16.59-0.05 through interferometric observations of both thermal and maser lines, and identified a high-mass young stellar object (YSO) which is surrounded by an accretion disk and drives a nonthermal radio jet. Our goals are to establish the physical conditions of the environment hosting the high-mass YSO and to study the kinematics of the surrounding gas in detail. Methods: We performed high-angular-resolution (beam FWHM ≈ 0''.15) 1.2-mm continuum and line observations towards G16.59-0.05 with the Atacama Large Millimeter Array (ALMA). Results: The main dust clump, with size ≈104 au, is resolved into four distinct, relatively compact (diameter 2000 au) millimeter (mm) sources. The source harboring the high-mass YSO is the most prominent in molecular emission. By fitting the emission profiles of several unblended and optically thin transitions of CH3OCH3 and CH3OH, we derived gas temperatures inside the mm sources in the range 42-131 K, and calculated masses of 1-5 M☉. A well-defined Local Standard of Rest (LSR) velocity (VLSR) gradient is detected in most of the high-density molecular tracers at the position of the high-mass YSO, pinpointed by compact 22-GHz free-free emission. This gradient is oriented along a direction forming a large (≈70°) angle with the radio jet, traced by elongated 13-GHz continuum emission. The butterfly-like shapes of the P-V plots and the linear pattern of the emission peaks of the molecular lines at high velocity confirm that this VLSR gradient is due to rotation of the gas in the disk surrounding the high-mass YSO. The disk radius is ≈500 au, and the VLSR distribution along the major axis of the disk is well reproduced by a Keplerian profile around a central mass of 10 ± 2 M☉. The position of the YSO is offset by ≳0''.1 from the axis of the radio jet and the dust emission peak. To explain this displacement we argue that the high-mass YSO could have moved from the center of the parental mm source owing to dynamical interaction with one or more companions.106 21 - Some of the metrics are blocked by yourconsent settings
Publication Open Access A 100 au Wide Bipolar Rotating Shell Emanating from the HH 212 Protostellar Disk: A Disk Wind?(2018) ;Lee, Chin-Fei ;Li, Zhi-Yun; ;Ho, Paul T. P.; ;Hirano, Naomi ;Shang, Hsien ;Turner, Neal J.Zhang, QizhouHH 212 is a Class 0 protostellar system found to host a “hamburger”-shaped dusty disk with a rotating disk atmosphere and a collimated SiO jet at a distance of ∼400 pc. Recently, a compact rotating outflow has been detected in SO and SO2 toward the center along the jet axis at ∼52 au (0.″13) resolution. Here we resolve the compact outflow into a small-scale wide-opening rotating outflow shell and a collimated jet, with the observations in the same S-bearing molecules at ∼16 au (0.″04) resolution. The collimated jet is aligned with the SiO jet, tracing the shock interactions in the jet. The wide-opening outflow shell is seen extending out from the inner disk around the SiO jet and has a width of ∼100 au. It is not only expanding away from the center, but also rotating around the jet axis. The specific angular momentum of the outflow shell is ∼40 au km s-1. Simple modeling of the observed kinematics suggests that the rotating outflow shell can trace either a disk wind or disk material pushed away by an unseen wind from the inner disk or protostar. We also resolve the disk atmosphere in the same S-bearing molecules, confirming the Keplerian rotation there.98 27 - 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.
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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.105 42 - Some of the metrics are blocked by yourconsent settings
Publication Open Access 108 34 - Some of the metrics are blocked by yourconsent settings
Publication Open Access 1D Kinematics from Stars and Ionized Gas at z ∼ 0.8 from the LEGA-C Spectroscopic Survey of Massive Galaxies(2018) ;Bezanson, Rachel; ;Straatman, Caroline ;Pacifici, Camilla ;Wu, Po-Feng ;Barišić, Ivana ;Bell, Eric F. ;Conroy, Charlie ;D'Eugenio, Francesco ;Franx, Marijn; ;van Houdt, Josha ;Maseda, Michael V. ;Muzzin, Adam ;van de Sande, Jesse ;Sobral, DavidSpilker, JustinWe present a comparison of the observed, spatially integrated stellar and ionized gas velocity dispersions of ∼1000 massive ({log} {M}\star /{M}☉ ≳ 10.3) galaxies in the Large Early Galaxy Astrophysics Census survey at 0.6 ≲ z ≲ 1.0. The high S/N ∼ 20 Å-1 afforded by 20 hr Very Large Telescope/Visible Multi-Object Spectrograph spectra allows for joint modeling of the stellar continuum and emission lines in all galaxies, spanning the full range of galaxy colors and morphologies. These observed integrated velocity dispersions (denoted as {σ }g,{int}{\prime } and {σ }\star ,{int}{\prime }) are related to the intrinsic velocity dispersions of ionized gas or stars, but also include rotational motions through beam smearing and spectral extraction. We find good average agreement between observed velocity dispersions, with < {log}({σ }g,{int}{\prime }/{σ }\star ,{int}{\prime })> =-0.003. This result does not depend strongly on stellar population, structural properties, or alignment with respect to the slit. However, in all regimes we find significant scatter between {σ }g,{int}{\prime } and {σ }\star ,{int}{\prime }, with an overall scatter of 0.13 dex of which 0.05 dex is due to observational uncertainties. For an individual galaxy, the scatter between {σ }g,{int}{\prime } and {σ }\star ,{int}{\prime } translates to an additional uncertainty of ∼0.24 dex on dynamical mass derived from {σ }g,{int}{\prime }, on top of measurement errors and uncertainties from Virial constant or size estimates. We measure the z ∼ 0.8 stellar mass Faber-Jackson relation and demonstrate that emission line widths can be used to measure scaling relations. However, these relations will exhibit increased scatter and slopes that are artificially steepened by selecting on subsets of galaxies with progressively brighter emission lines.75 16 - 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.
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Publication Open Access The 2008 outburst in the young stellar system Z CMa. III. Multi-epoch high-angular resolution images and spectra of the components in near-infrared(2017) ;Bonnefoy, M. ;Chauvin, G. ;Dougados, C. ;Kóspál, Á. ;Benisty, M. ;Duchêne, G. ;Bouvier, J. ;Garcia, P. J. V. ;Whelan, E.; Context. Z CMa is a complex pre-main sequence binary with a current separation of 110 mas, known to consist of an FU Orionis star (SE component) and an embedded Herbig Be star (NW component). Although it represents a well-studied and characterized system, the origin of photometric variabilities, the component properties, and the physical configuration of the system remain mostly unknown.
Aims: Immediately when the late-2008 outburst of Z CMa was announced to the community, we initiated a high angular resolution imaging campaign aimed at characterizing the outburst state of both components of the system in the near-infrared.
Methods: We used the VLT/NACO and the Keck/NIRC2 near-infrared adaptive optics instrument to monitor the astrometric position and the near-infrared photometry of the Z CMa components during the outburst phase and one year after. The VLT/SINFONI and Keck/OSIRIS integral field spectroscrographs were in addition used to characterize for the first time the resolved spectral properties of the FU Orionis and the Herbig Be component during and after the outburst.
Results: We confirm that the NW star dominates the system flux in the 1.1-3.8 μm range and is responsible for the photometric outburst. We extract the first medium-resolution (R 2000-4000) near-infrared (1.1-2.4 μm) spectra of the individual components. The SE component has a spectrum typical of FU Orionis objects. The NW component spectrum is characteristic of embedded outbursting protostars and EX Or objects. It displays numerous emission lines whose intensity correlates with the system activity. In particular, we find a correlation between the Brγ equivalent width and the system brightness. The bluing of the continuum of the NW component along with the absolute flux and color-variation of the system during the outburst suggests that the outburst was caused by a complex interplay between a variation of the extinction in the line of sight of the NW component on one hand, and the emission of shocked regions close to the NW component on the other. We confirm the recently reported wiggling of the SE component jet from [Fe II] line emission. We find a point-like structure associated with a peak emission at 2.098 μm coincidental with the clump or arm seen in broadband polarization differential imaging as well as additional diffuse emission along a PA = 214°. The origin of these two structures is unclear and deserves further investigation.75 50 - Some of the metrics are blocked by yourconsent settings
Publication Open Access The 2014 ALMA Long Baseline Campaign: First Results from High Angular Resolution Observations toward the HL Tau Region(2015) ;ALMA Partnership ;Brogan, C. L. ;Pérez, L. M. ;Hunter, T. R. ;Dent, W. R. F. ;Hales, A. S. ;Hills, R. E. ;Corder, S. ;Fomalont, E. B. ;Vlahakis, C. ;Asaki, Y. ;Barkats, D. ;Hirota, A. ;Hodge, J. A. ;Impellizzeri, C. M. V. ;Kneissl, R.; ;Lucas, R. ;Marcelino, N. ;Matsushita, S. ;Nakanishi, K. ;Phillips, N. ;Richards, A. M. S. ;Toledo, I. ;Aladro, R. ;Broguiere, D. ;Cortes, J. R. ;Cortes, P. C. ;Espada, D. ;Galarza, F. ;Garcia-Appadoo, D. ;Guzman-Ramirez, L. ;Humphreys, E. M. ;Jung, T. ;Kameno, S. ;Laing, R. A. ;Leon, S. ;Marconi, G. ;Mignano, A. ;Nikolic, B. ;Nyman, L. -A. ;Radiszcz, M. ;Remijan, A. ;Rodón, J. A. ;Sawada, T. ;Takahashi, S. ;Tilanus, R. P. J. ;Vila Vilaro, B. ;Watson, L. C. ;Wiklind, T. ;Akiyama, E. ;Chapillon, E. ;de Gregorio-Monsalvo, I. ;Di Francesco, J. ;Gueth, F. ;Kawamura, A. ;Lee, C. -F. ;Nguyen Luong, Q. ;Mangum, J. ;Pietu, V. ;Sanhueza, P. ;Saigo, K. ;Takakuwa, S. ;Ubach, C. ;van Kempen, T. ;Wootten, A. ;Castro-Carrizo, A. ;Francke, H. ;Gallardo, J. ;Garcia, J. ;Gonzalez, S. ;Hill, T. ;Kaminski, T. ;Kurono, Y. ;Liu, H. -Y. ;Lopez, C. ;Morales, F. ;Plarre, K. ;Schieven, G.; ;Videla, L. ;Villard, E. ;Andreani, P. ;Hibbard, J. E.Tatematsu, K.We present Atacama Large Millimeter/submillimeter Array (ALMA) observations from the 2014 Long Baseline Campaign in dust continuum and spectral line emission from the HL Tau region. The continuum images at wavelengths of 2.9, 1.3, and 0.87 mm have unprecedented angular resolutions of 0.″ 075 (10 AU) to 0.″ 025 (3.5 AU), revealing an astonishing level of detail in the circumstellar disk surrounding the young solar analog HL Tau, with a pattern of bright and dark rings observed at all wavelengths. By fitting ellipses to the most distinct rings, we measure precise values for the disk inclination (46\buildrel{\circ}\over{.} 72+/- 0\buildrel{\circ}\over{.} 05) and position angle (+138\buildrel{\circ}\over{.} 02+/- 0\buildrel{\circ}\over{.} 07). We obtain a high-fidelity image of the 1.0 mm spectral index (α), which ranges from α ̃ 2.0 in the optically thick central peak and two brightest rings, increasing to 2.3-3.0 in the dark rings. The dark rings are not devoid of emission, and we estimate a grain emissivity index of 0.8 for the innermost dark ring and lower for subsequent dark rings, consistent with some degree of grain growth and evolution. Additional clues that the rings arise from planet formation include an increase in their central offsets with radius and the presence of numerous orbital resonances. At a resolution of 35 AU, we resolve the molecular component of the disk in HCO+ (1-0) which exhibits a pattern over LSR velocities from 2-12 km s-1 consistent with Keplerian motion around a ̃1.3 {M}☉ star, although complicated by absorption at low blueshifted velocities. We also serendipitously detect and resolve the nearby protostars XZ Tau (A/B) and LkHα358 at 2.9 mm.86 66 - Some of the metrics are blocked by yourconsent settings
Publication Open Access The 2014 KIDA Network for Interstellar Chemistry(2015) ;Wakelam, V. ;Loison, J. -C. ;Herbst, E. ;Pavone, B. ;Bergeat, A. ;Béroff, K. ;Chabot, M. ;Faure, A.; ;Geppert, W. D. ;Gerlich, D. ;Gratier, P. ;Harada, N. ;Hickson, K. M. ;Honvault, P. ;Klippenstein, S. J. ;Le Picard, S. D. ;Nyman, G. ;Ruaud, M. ;Schlemmer, S. ;Sims, I. R. ;Talbi, D. ;Tennyson, J.Wester, R.Chemical models used to study the chemical composition of the gas and the ices in the interstellar medium are based on a network of chemical reactions and associated rate coefficients. These reactions and rate coefficients are partially compiled from data in the literature, when available. We present in this paper kida.uva.2014, a new updated version of the kida.uva public gas-phase network first released in 2012. In addition to a description of the many specific updates, we illustrate changes in the predicted abundances of molecules for cold dense cloud conditions as compared with the results of the previous version of our network, kida.uva.2011.83 43 - Some of the metrics are blocked by yourconsent settings
Publication Open Access The 2014 TeV γ-Ray Flare of Mrk 501 Seen with H.E.S.S.: Temporal and Spectral Constraints on Lorentz Invariance Violation(2019) ;Abdalla, H. ;Aharonian, F. ;Ait Benkhali, F. ;Angüner, E. O. ;Arakawa, M. ;Arcaro, C. ;Armand, C. ;Arrieta, M. ;Backes, M. ;Barnard, M. ;Becherini, Y. ;Becker Tjus, J. ;Berge, D. ;Bernhard, S. ;Bernlöhr, K. ;Blackwell, R. ;Böttcher, M. ;Boisson, C. ;Bolmont, J. ;Bonnefoy, S. ;Bordas, P. ;Bregeon, J. ;Brun, F. ;Brun, P. ;Bryan, M. ;Büchele, M. ;Bulik, T. ;Bylund, T. ;Capasso, M. ;Caroff, S. ;Carosi, A. ;Cerruti, M. ;Chakraborty, N. ;Chandra, S. ;Chaves, R. C. G. ;Chen, A. ;Colafrancesco, S. ;Condon, B. ;Davids, I. D. ;Deil, C. ;Devin, J. ;deWilt, P. ;Dirson, L. ;Djannati-Ataï, A. ;Dmytriiev, A. ;Donath, A. ;Doroshenko, V. ;O'C. Drury, L. ;Dyks, J. ;Egberts, K. ;Emery, G. ;Ernenwein, J. -P. ;Eschbach, S. ;Fegan, S. ;Fiasson, A. ;Fontaine, G. ;Funk, S. ;Füßling, M. ;Gabici, S. ;Gallant, Y. A. ;Gaté, F. ;Giavitto, G. ;Glawion, D. ;Glicenstein, J. F. ;Gottschall, D. ;Grondin, M. -H. ;Hahn, J. ;Haupt, M. ;Heinzelmann, G. ;Henri, G. ;Hermann, G. ;Hinton, J. A. ;Hofmann, W. ;Hoischen, C. ;Holch, T. L. ;Holler, M. ;Horns, D. ;Huber, D. ;Iwasaki, H. ;Jacholkowska, A. ;Jamrozy, M. ;Jankowsky, D. ;Jankowsky, F. ;Jouvin, L. ;Jung-Richardt, I. ;Kastendieck, M. A. ;Katarzyński, K. ;Katsuragawa, M. ;Katz, U. ;Kerszberg, D. ;Khangulyan, D. ;Khélifi, B. ;King, J. ;Klepser, S. ;Kluźniak, W. ;Komin, Nu. ;Kosack, K. ;Krakau, S. ;Kraus, M. ;Krüger, P. P. ;Lamanna, G. ;Lau, J. ;Lefaucheur, J. ;Lemière, A. ;Lemoine-Goumard, M. ;Lenain, J. -P. ;Leser, E. ;Lohse, T. ;Lorentz, M. ;López-Coto, R. ;Lypova, I. ;Malyshev, D. ;Marandon, V. ;Marcowith, A. ;Mariaud, C. ;Martí-Devesa, G. ;Marx, R. ;Maurin, G. ;Meintjes, P. J. ;Mitchell, A. M. W. ;Moderski, R. ;Mohamed, M. ;Mohrmann, L. ;Moulin, E. ;Murach, T. ;Nakashima, S. ;de Naurois, M. ;Ndiyavala, H. ;Niederwanger, F. ;Niemiec, J. ;Oakes, L. ;O'Brien, P. ;Odaka, H. ;Ohm, S. ;Ostrowski, M. ;Oya, I.; ;Panter, M. ;Parsons, R. D. ;Perennes, C. ;Petrucci, P. -O. ;Peyaud, B. ;Piel, Q. ;Pita, S. ;Poireau, V. ;Priyana Noel, A. ;Prokhorov, D. ;Prokoph, H. ;Pühlhofer, G. ;Punch, M. ;Quirrenbach, A. ;Raab, S. ;Rauth, R. ;Reimer, A. ;Reimer, O. ;Renaud, M. ;Rieger, F. ;Rinchiuso, L. ;Romoli, C. ;Rowell, G. ;Rudak, B. ;Ruiz-Velasco, E. ;Sahakian, V. ;Saito, S. ;Sanchez, D. A. ;Santangelo, A. ;Sasaki, M. ;Schlickeiser, R. ;Schüssler, F. ;Schulz, A. ;Schwanke, U. ;Schwemmer, S. ;Seglar-Arroyo, M. ;Senniappan, M. ;Seyffert, A. S. ;Shafi, N. ;Shilon, I. ;Shiningayamwe, K. ;Simoni, R. ;Sinha, A. ;Sol, H. ;Spanier, F. ;Specovius, A. ;Spir-Jacob, M. ;Stawarz, Ł. ;Steenkamp, R. ;Stegmann, C. ;Steppa, C. ;Takahashi, T. ;Tavernet, J. -P. ;Tavernier, T. ;Taylor, A. M. ;Terrier, R. ;Tibaldo, L. ;Tiziani, D. ;Tluczykont, M. ;Trichard, C. ;Tsirou, M. ;Tsuji, N. ;Tuffs, R. ;Uchiyama, Y. ;van der Walt, D. J. ;van Eldik, C. ;van Rensburg, C. ;van Soelen, B. ;Vasileiadis, G. ;Veh, J. ;Venter, C. ;Vincent, P. ;Vink, J. ;Voisin, F. ;Völk, H. J. ;Vuillaume, T. ;Wadiasingh, Z. ;Wagner, S. J. ;Wagner, R. M. ;White, R. ;Wierzcholska, A. ;Yang, R. ;Zaborov, D. ;Zacharias, M. ;Zanin, R. ;Zdziarski, A. A. ;Zech, A. ;Zefi, F. ;Ziegler, A. ;Zorn, J. ;Żywucka, N.H. E. S. S. CollaborationThe blazar Mrk 501 (z = 0.034) was observed at very-high-energy (VHE, E ≳ 100 GeV) gamma-ray wavelengths during a bright flare on the night of 2014 June 23-24 (MJD 56832) with the H.E.S.S. phase-II array of Cherenkov telescopes. Data taken that night by H.E.S.S. at large zenith angle reveal an exceptional number of gamma-ray photons at multi-TeV energies, with rapid flux variability and an energy coverage extending significantly up to 20 TeV. This data set is used to constrain Lorentz invariance violation (LIV) using two independent channels: a temporal approach considers the possibility of an energy dependence in the arrival time of gamma-rays, whereas a spectral approach considers the possibility of modifications to the interaction of VHE gamma-rays with extragalactic background light (EBL) photons. The non-detection of energy-dependent time delays and the non-observation of deviations between the measured spectrum and that of a supposed power-law intrinsic spectrum with standard EBL attenuation are used independently to derive strong constraints on the energy scale of LIV (E QG) in the subluminal scenario for linear and quadratic perturbations in the dispersion relation of photons. For the case of linear perturbations, the 95% confidence level limits obtained are E QG,1 > 3.6 × 1017 GeV using the temporal approach and E QG,1 > 2.6 × 1019 GeV using the spectral approach. For the case of quadratic perturbations, the limits obtained are E QG,2 > 8.5 × 1010 GeV using the temporal approach and E QG,2 > 7.8 × 1011 GeV using the spectral approach.70 35 - Some of the metrics are blocked by yourconsent settings
Publication Open Access The 2D metallicity distribution and mixing scales of nearby galaxies(2021) ;Thomas G Williams ;Kathryn Kreckel; ;Brent Groves ;Karin Sandstrom ;Francesco Santoro ;Guillermo A Blanc ;Frank Bigiel ;Médéric Boquien ;Mélanie Chevance ;Enrico Congiu ;Eric Emsellem ;Simon C O Glover ;Kathryn Grasha ;Ralf S Klessen ;Eric Koch ;J M Diederik Kruijssen ;Adam K Leroy ;Daizhong Liu ;Sharon Meidt ;Hsi-An Pan ;Miguel Querejeta ;Erik Rosolowsky ;Toshiki Saito ;Patricia Sánchez-Blázquez ;Eva Schinnerer ;Andreas SchrubaElizabeth J WatkinsUnderstanding the spatial distribution of metals within galaxies allows us to study the processes of chemical enrichment and mixing in the interstellar medium (ISM). In this work, we map the two-dimensional distribution of metals using a Gaussian Process Regression (GPR) for 19 star-forming galaxies observed with the Very Large Telescope/Multi Unit Spectroscopic Explorer (VLT-MUSE) as part of the PHANGS-MUSE survey. We find that 12 of our 19 galaxies show significant two-dimensional metallicity variation. Those without significant variations typically have fewer metallicity measurements, indicating this is due to the dearth of HII regions in these galaxies, rather than a lack of higher-order variation. After subtracting a linear radial gradient, we see no enrichment in the spiral arms versus the disc. We measure the 50 per cent correlation scale from the two-point correlation function of these radially-subtracted maps, finding it to typically be an order of magnitude smaller than the fitted GPR kernel scale length. We study the dependence of the two-point correlation scale length with a number of global galaxy properties. We find no relationship between the 50 per cent correlation scale and the overall gas turbulence, in tension with existing theoretical models. We also find more actively star forming galaxies, and earlier type galaxies have a larger 50 per cent correlation scale. The size and stellar mass surface density do not appear to correlate with the 50 per cent correlation scale, indicating that perhaps the evolutionary state of the galaxy and its current star formation activity is the strongest indicator of the homogeneity of the metal distribution.8 4 - Some of the metrics are blocked by yourconsent settings
Publication Metadata only 89 - 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 3C 294 revisited: Deep Large Binocular Telescope AO NIR images and optical spectroscopy(2019) ;Heidt, J. ;Quirrenbach, A. ;Hoyer, N. ;Thompson, D. ;Pramskiy, A.; ; ;Gredel, R. ;Miller, D.; ; ; ;Seifert, W.Taylor, G.Context. High redshift radio galaxies are among the most massive galaxies at their redshift, are often found at the center of protoclusters of galaxies, and are expected to evolve into the present day massive central cluster galaxies. Thus they are a useful tool to explore structure formation in the young Universe. Aims: 3C 294 is a powerful FR II type radio galaxy at z = 1.786. Past studies have identified a clumpy structure, possibly indicative of a merging system, as well as tentative evidence that 3C 294 hosts a dual active galactic nucleus (AGN). Due to its proximity to a bright star, it has been subject to various adaptive optics imaging studies.
Methods: In order to distinguish between the various scenarios for 3C 294, we performed deep, high-resolution adaptive optics near-infrared imaging and optical spectroscopy of 3C 294 with the Large Binocular Telescope. Results: We resolve the 3C 294 system into three distinct components separated by a few tenths of an arcsecond on our images. One is compact, the other two are extended, and all appear to be non-stellar. The nature of each component is unclear. The two extended components could be a galaxy with an internal absorption feature, a galaxy merger, or two galaxies at different redshifts. We can now uniquely associate the radio source of 3C 294 with one of the extended components. Based on our spectroscopy, we determined a redshift of z = 1.784 ± 0.001, which is similar to the one previously cited. In addition we found a previously unreported emission line at λ6749.4 Å in our spectra. It is not clear that it originates from 3C 294. It could be the Ne [IV] doublet λ2424/2426 Å at z = 1.783, or belong to the compact component at a redshift of z ∼ 4.56. We thus cannot unambiguously determine whether 3C 294 hosts a dual AGN or a projected pair of AGNs. The reduced AO J,H, and Ks-images and optical spectra shown in Fig. 3 and 4 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/qcat?J/A+A/628/A28The LBT is an international collaboration among institutions in the United States, Italy, and Germany. LBT Corporation partners are: The University of Arizona on behalf of the Arizona Board of Regents; Istituto Nazionale di Astrofisica, Italy; LBT Beteiligungsgesellschaft, Germany, representing the Max-Planck Society, The Leibniz Institute for Astrophysics Potsdam, and Heidelberg University; The Ohio State University, and The Research Corporation, on behalf of The University of Notre Dame, University of Minnesota, and University of Virginia.112 29 - Some of the metrics are blocked by yourconsent settings
Publication Open Access 43 10 - Some of the metrics are blocked by yourconsent settings
Publication Open Access 3D velocity fields from methanol and water masers in an intermediate-mass protostarWe report multi-epoch VLBI observations of molecular masers towards the high-mass star forming region AFGL 5142, leading to the determination of the 3D velocity field of circumstellar molecular gas at radii <0.''23 (or 400 AU) from the protostar MM-1. Our observations of CH3OH maser emission enabled, for the first time, a direct measurement of infall of a molecular envelope on to an intermediate-mass protostar (radius of 300 AU, velocity of 5 km s-1, and infall rate of 6 × 10-4 n 8 M ⊙ yr-1, where n 8 is the ambient volume density in units of 108 cm-3). In addition, our measurements of H2O maser (and radio continuum) emission revealed a collimated bipolar molecular outflow (and ionized jet) from MM-1. The evidence of simultaneous accretion and outflow at small spatial scales, makes AFGL 5142 an extremely compelling target for high-angular resolution studies of high-mass star formation.49 12 - Some of the metrics are blocked by yourconsent settings
Publication Open Access A 3D view of the Taurus star-forming region by Gaia and Herschel: multiple populations related to the filamentary molecular cloud(2020) ;Roccatagliata, V.; ; ; Sicilia-Aguilar, A.Context. Taurus represents an ideal region to study the three-dimensional distribution of the young stellar population and relate it to the associated molecular cloud. Aims. The second Gaia data release (DR2) enables us to investigate the Taurus complex in three dimensions, starting from a previously defined robust membership. The molecular cloud structured in filaments can be traced in emission using the public far-infrared maps from Herschel. Methods. From a compiled catalog of spectroscopically confirmed members, we analyze the 283 sources with reliable parallax and proper motions in the Gaia DR2 archive. We fit the distribution of parallaxes and proper motions with multiple populations described by multivariate Gaussians. We compute the cartesian Galactic coordinates (X,Y,Z) and, for the populations associated with the main cloud, also the galactic space velocity (U,V,W). We discuss the spatial distribution of the populations in relation to the structure of the filamentary molecular cloud traced by Herschel. Results. We discover the presence of six populations which are all well defined in parallax and proper motions, with the only exception being Taurus D. The derived distances range between 130 and 160 pc. We do not find a unique relation between stellar population and the associated molecular cloud: while the stellar population seems to be on the cloud surface, both lying at similar distances, this is not the case when the molecular cloud is structured in filaments. Taurus B is probably moving in the direction of Taurus A, while Taurus E appears to be moving towards them. Conclusions. The Taurus region is the result of a complex star formation history which most probably occurred in clumpy and filamentary structures that are evolving independently.66 32 - 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 6% measurement of the Hubble parameter at z~0.45: direct evidence of the epoch of cosmic re-acceleration(2016) ;Moresco, Michele; ;CIMATTI, ANDREA ;Jimenez, Raul ;Maraston, Claudia ;Verde, Licia ;Thomas, Daniel ;Citro, Annalisa ;Tojeiro, RitaWilkinson, DavidDeriving the expansion history of the Universe is a major goal of modern cosmology. To date, the most accurate measurements have been obtained with Type Ia Supernovae (SNe) and Baryon Acoustic Oscillations (BAO), providing evidence for the existence of a transition epoch at which the expansion rate changes from decelerated to accelerated. However, these results have been obtained within the framework of specific cosmological models that must be implicitly or explicitly assumed in the measurement. It is therefore crucial to obtain measurements of the accelerated expansion of the Universe independently of assumptions on cosmological models. Here we exploit the unprecedented statistics provided by the Baryon Oscillation Spectroscopic Survey (BOSS, [1-3]) Data Release 9 to provide new constraints on the Hubble parameter H(z) using the cosmic chronometers approach. We extract a sample of more than 130000 of the most massive and passively evolving galaxies, obtaining five new cosmology-independent H(z) measurements in the redshift range 0.3 < z < 0.5, with an accuracy of ~11-16% incorporating both statistical and systematic errors. Once combined, these measurements yield a 6% accuracy constraint of H(z = 0.4293) = 91.8 ± 5.3 km/s/Mpc. The new data are crucial to provide the first cosmology-independent determination of the transition redshift at high statistical significance, measuring zt = 0.4 ± 0.1, and to significantly disfavor the null hypothesis of no transition between decelerated and accelerated expansion at 99.9% confidence level. This analysis highlights the wide potential of the cosmic chronometers approach: it permits to derive constraints on the expansion history of the Universe with results competitive with standard probes, and most importantly, being the estimates independent of the cosmological model, it can constrain cosmologies beyond—and including—the ΛCDM model.78 29