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Overview and Status of the Giant Magellan Telescope Project
Invited Paper Overview and Status of the Giant Magellan Telescope Project Patrick J. McCarthy*,a,b, James Fansona, Rebecca Bernsteina,b, David Ashbyc, Bruce Bigelowa, Nune Boyadjiana, Antonin Boucheza, Eric Chauvina, Eduardo Donosoa, Jose Filgueiraa, Robert Goodricha, Frank Groarka, George Jacobya, Eric Pearcea aGMTO Corporation, 451 N. Halstead St., Suite 250, Pasadena, CA 91107, USA bCarnegie Observatories, 813 Santa Barbara St., Pasadena, CA 91101, USA cLarge Binocular Telescope Observatory, Tucson AZ ABSTRACT The Giant Magellan Telescope Project is in the construction phase. Production of the primary mirror segments is underway with four of the seven required 8.4m mirrors at various stages of completion and materials purchased for segments five and six. Development of the infrastructure at the GMT site at Las Campanas is nearing completion. Power, water and data connections sufficient to support the construction of the telescope and enclosure are in place and roads to the summit have been widened and graded to support transportation of large and heavy loads. Construction pads for the support buildings have been graded and the construction residence is being installed. A small number of issues need to be resolved before the final design of the telescope structure and enclosure can proceed and the GMT team is collecting the required inputs to the decision making process. Prototyping activities targeted at the active and adaptive optics systems are allowing us to finalize designs before large scale production of components begins. Our technically driven schedule calls for the telescope to be assembled on site in 2022 and to be ready to receive a subset of the primary and secondary mirror optics late in the year. -
REVIEW ARTICLE the NASA Spitzer Space Telescope
REVIEW OF SCIENTIFIC INSTRUMENTS 78, 011302 ͑2007͒ REVIEW ARTICLE The NASA Spitzer Space Telescope ͒ R. D. Gehrza Department of Astronomy, School of Physics and Astronomy, 116 Church Street, S.E., University of Minnesota, Minneapolis, Minnesota 55455 ͒ T. L. Roelligb NASA Ames Research Center, MS 245-6, Moffett Field, California 94035-1000 ͒ M. W. Wernerc Jet Propulsion Laboratory, California Institute of Technology, MS 264-767, 4800 Oak Grove Drive, Pasadena, California 91109 ͒ G. G. Faziod Harvard-Smithsonian Center for Astrophysics, 60 Garden Street, Cambridge, Massachusetts 02138 ͒ J. R. Houcke Astronomy Department, Cornell University, Ithaca, New York 14853-6801 ͒ F. J. Lowf Steward Observatory, University of Arizona, 933 North Cherry Avenue, Tucson, Arizona 85721 ͒ G. H. Riekeg Steward Observatory, University of Arizona, 933 North Cherry Avenue, Tucson, Arizona 85721 ͒ ͒ B. T. Soiferh and D. A. Levinei Spitzer Science Center, MC 220-6, California Institute of Technology, 1200 East California Boulevard, Pasadena, California 91125 ͒ E. A. Romanaj Jet Propulsion Laboratory, California Institute of Technology, MS 264-767, 4800 Oak Grove Drive, Pasadena, California 91109 ͑Received 2 June 2006; accepted 17 September 2006; published online 30 January 2007͒ The National Aeronautics and Space Administration’s Spitzer Space Telescope ͑formerly the Space Infrared Telescope Facility͒ is the fourth and final facility in the Great Observatories Program, joining Hubble Space Telescope ͑1990͒, the Compton Gamma-Ray Observatory ͑1991–2000͒, and the Chandra X-Ray Observatory ͑1999͒. Spitzer, with a sensitivity that is almost three orders of magnitude greater than that of any previous ground-based and space-based infrared observatory, is expected to revolutionize our understanding of the creation of the universe, the formation and evolution of primitive galaxies, the origin of stars and planets, and the chemical evolution of the universe. -
Detection of Large-Scale X-Ray Bubbles in the Milky Way Halo
Detection of large-scale X-ray bubbles in the Milky Way halo P. Predehl1†, R. A. Sunyaev2,3†, W. Becker1,4, H. Brunner1, R. Burenin2, A. Bykov5, A. Cherepashchuk6, N. Chugai7, E. Churazov2,3†, V. Doroshenko8, N. Eismont2, M. Freyberg1, M. Gilfanov2,3†, F. Haberl1, I. Khabibullin2,3, R. Krivonos2, C. Maitra1, P. Medvedev2, A. Merloni1†, K. Nandra1†, V. Nazarov2, M. Pavlinsky2, G. Ponti1,9, J. S. Sanders1, M. Sasaki10, S. Sazonov2, A. W. Strong1 & J. Wilms10 1Max-Planck-Institut für Extraterrestrische Physik, Garching, Germany. 2Space Research Institute of the Russian Academy of Sciences, Moscow, Russia. 3Max-Planck-Institut für Astrophysik, Garching, Germany. 4Max-Planck-Institut für Radioastronomie, Bonn, Germany. 5Ioffe Institute, St Petersburg, Russia. 6M. V. Lomonosov Moscow State University, P. K. Sternberg Astronomical Institute, Moscow, Russia. 7Institute of Astronomy, Russian Academy of Sciences, Moscow, Russia. 8Institut für Astronomie und Astrophysik, Tübingen, Germany. 9INAF-Osservatorio Astronomico di Brera, Merate, Italy. 10Dr. Karl-Remeis-Sternwarte Bamberg and ECAP, Universität Erlangen-Nürnberg, Bamberg, Germany. †e-mail: [email protected]; [email protected]; [email protected]; [email protected]; [email protected]; [email protected] The halo of the Milky Way provides a laboratory to study the properties of the shocked hot gas that is predicted by models of galaxy formation. There is observational evidence of energy injection into the halo from past activity in the nucleus of the Milky Way1–4; however, the origin of this energy (star formation or supermassive-black-hole activity) is uncertain, and the causal connection between nuclear structures and large-scale features has not been established unequivocally. -
Semiconductor Detectors and Focal Plane Arrays for Far-Infrared Imaging
OPTO−ELECTRONICS REVIEW 21(4), 406–426 DOI: 10.2478/s11772−013−0110−x Semiconductor detectors and focal plane arrays for far-infrared imaging A. ROGALSKI* Institute of Applied Physics, Military University of Technology, 2 Kaliskiego Str., 00–908 Warsaw, Poland The detection of far−infrared (far−IR) and sub−mm−wave radiation is resistant to the commonly employed techniques in the neighbouring microwave and IR frequency bands. In this wavelength detection range the use of solid state detectors has been hampered for the reasons of transit time of charge carriers being larger than the time of one oscillation period of radiation. Also the energy of radiation quanta is substantially smaller than the thermal energy at room temperature and even liquid ni− trogen temperature. The realization of terahertz (THz) emitters and receivers is a challenge because the frequencies are too high for conventional electronics and the photon energies are too small for classical optics. Development of semiconductor focal plane arrays started in seventies last century and has revolutionized imaging sys− tems in the next decades. This paper presents progress in far−IR and sub−mm−wave semiconductor detector technology of fo− cal plane arrays during the past twenty years. Special attention is given on recent progress in the detector technologies for real−time uncooled THz focal plane arrays such as Schottky barrier arrays, field−effect transistor detectors, and micro− bolometers. Also cryogenically cooled silicon and germanium extrinsic photoconductor arrays, and semiconductor bolome− ter arrays are considered. Keywords: THz detectors, focal plane arrays, Schottky barrier diodes, semiconductor hot electron bolometers, extrinsic photodetectors, performance limits. -
The Space Infrared Telescope Facility (SIRTF)
header for SPIE use The Space Infrared Telescope Facility (SIRTF) James Fansona, Giovanni Faziob, James Houckc, Tim Kellyd, George Riekee, Domenick Tenerellif, and Milt Whittenf aJet Propulsion Laboratory, California Institute of Technology, Pasadena CA 91109 bSmithsonian Astrophysical Observatory, Cambridge, MA 02138 cCornell University, Ithaca, NY, 14853 dBall Aerospace and Technologies Corp., Boulder, CO 80301 eUniversity of Arizona, Tucson, AZ, 85721 fLockheed Martin Missiles and Space Co., Sunnyvale, CA 94089 ABSTRACT This paper describes the design of the Space Infrared Telescope Facility (SIRTF) as the project enters the detailed design phase. SIRTF is the fourth of NASA’s Great Observatories, and is scheduled for launch in December 2001. SIRTF provides background limited imaging and spectroscopy covering the spectral range from 3 to 180 mm, complementing the capabilities of the other Great Observatories – the Hubble Space Telescope (HST), the Advanced X-ray Astrophysics Facility (AXAF), and the Compton Gamma Ray Observatory (CGRO). SIRTF will be the first mission to combine the high sensitivity achievable from a cryogenic space telescope with the imaging and spectroscopic power of the new generation of infrared detector arrays. The scientific capabilities of this combination are so great that SIRTF was designated the highest priority major mission for all of US astronomy in the 1990s. Keywords: telescope, cryogenic, infrared, astronomy, astrophysics, Great Observatory 1. INTRODUCTION The SIRTF mission has experienced dramatic evolution in both architecture and mission design. Originally conceived as a low Earth orbiting observatory serviced by astronauts from the Space Shuttle, SIRTF passed through a phase in high Earth orbit using first the Titan and later the smaller Atlas launch vehicle, to the current concept of a deep-space mission orbiting the sun, and using the still smaller Delta launch vehicle. -
On the Possibility of Registering X-Ray Flares Related to Fast Radio
On the possibility of registering X-ray flares related to fast radio bursts with the SRG/eROSITA telescope A.D. Khokhryakova1, D.A. Lyapina1, S.B. Popov1;2;3 1 Department of Physics, Lomonosov Moscow State University 2 Sternberg Astronomical Institute, Lomonosov Moscow State University 3 Higher School of Economics, Moscow March 27, 2019 Abstract In this note we discuss the possibility of detecting the accompanying X-ray emission from sources of fast radio bursts with the eROSITA telescope on- board the Spektr-RG observatory. It is shown that during four years of the survey program about 300 bursts are expected to appear in the field of view of eROSITA. About 1% of them will be detected by ground-based radio tele- scopes. For a total energy release ∼ 1046 ergs depending on the spectral parameters and absorption in the interstellar and intergalactic media, an X- ray flare can be detected from distances from ∼ 1 Mpc (thermal spectrum with kT = 200 keV and strong absorption) up to ∼ 1 Gpc (power-law spec- trum with photon index Γ = 2 and realistic absorption). Thus, eROSITA observations might help to provide important constraints on parameters of arXiv:1903.10991v1 [astro-ph.HE] 26 Mar 2019 sources of fast radio bursts, or may even allow to identify the X-ray tran- sient counterparts, which will help to constrain models of fast radio bursts generation. 1 1 Introduction Fast radio bursts (FRBs) are short (∼ms) bright (peak fluxes up to ∼100 Jy) radio flashes (for a review, see [1]).1 The first event from this class of tran- sients was introduced in 2007 in [2]. -
Experimental Facilities in Latin America
CLASHEP 2019, Villa General Belgrano, Córdoba, Argentina Experimental Facilities in Latin America Claudio O. Dib Universidad Técnica Federico Santa María, Valparaíso, Chile 7 to 5 Content: • Brief introduction to Particle Physics experiments. • Accelerator Facilities in L.A. • Astronomical Observatories in L.A. (current and future) - VLT, ALMA, DSA3, DES, LSST, GMT, ELT, LLAMA. • Current Astroparticle Facilities in L.A. - Auger - Parenthesis on Cosmic Rays and Extensive Air Showers. - LAGO, HAWC • Future Astroparticle Facilities in L.A. - CTA, ALPACA, LATTES, SGSO, ANDES • Summary 6 to 5 Particle Physics experiments: - Table top experiments E. Rutherford’s lab., Cambridge U. - Cosmic ray detection (Astroparticle Physics) - Accelerators and colliders: (cyclotrons, synchrotrons, linacs; fixed target collisions, colliding beams) 5 to 5 Past table-top experiments 1895: J.J Thomson -> electron J.J. Thomson. Credit: Cambridge U., Cavendish Lab. 1911: E. Rutherford -> nucleus & proton 1932: J. Chadwick -> neutron 4 to 5 J.A. Ratcliffe & E. Rutherford, Cavendish Lab. Cosmic ray experiments • Cosmic rays: radiation that comes from outer space. • Discovered in 1912 by Victor Hess: – Went up a Balloon up to 5300 m: Radiation is higher further above. • Named cosmic rays by R. A. Millikan. Victor F. Hess preparing the baloon flight Cosmic rays are actually… particles! (mainly protons & heavier nuclei) 3 to 5 Robert A. Millikan. Caltech archives. Cosmic ray experiments 1932: C. Anderson discovers the positron. 1947: C. Powell, G. Occhialini, C. Lattes -
Report of Contributions
Mapping the X-ray Sky with SRG: First Results from eROSITA and ART-XC Report of Contributions https://events.mpe.mpg.de/e/SRG2020 Mapping the X- … / Report of Contributions eROSITA discovery of a new AGN … Contribution ID : 4 Type : Oral Presentation eROSITA discovery of a new AGN state in 1H0707-495 Tuesday, 17 March 2020 17:45 (15) One of the most prominent AGNs, the ultrasoft Narrow-Line Seyfert 1 Galaxy 1H0707-495, has been observed with eROSITA as one of the first CAL/PV observations on October 13, 2019 for about 60.000 seconds. 1H 0707-495 is a highly variable AGN, with a complex, steep X-ray spectrum, which has been the subject of intense study with XMM-Newton in the past. 1H0707-495 entered an historical low hard flux state, first detected with eROSITA, never seen before in the 20 years of XMM-Newton observations. In addition ultra-soft emission with a variability factor of about 100 has been detected for the first time in the eROSITA light curves. We discuss fast spectral transitions between the cool and a hot phase of the accretion flow in the very strong GR regime as a physical model for 1H0707-495, and provide tests on previously discussed models. Presenter status Senior eROSITA consortium member Primary author(s) : Prof. BOLLER, Thomas (MPE); Prof. NANDRA, Kirpal (MPE Garching); Dr LIU, Teng (MPE Garching); MERLONI, Andrea; Dr DAUSER, Thomas (FAU Nürnberg); Dr RAU, Arne (MPE Garching); Dr BUCHNER, Johannes (MPE); Dr FREYBERG, Michael (MPE) Presenter(s) : Prof. BOLLER, Thomas (MPE) Session Classification : AGN physics, variability, clustering October 3, 2021 Page 1 Mapping the X- … / Report of Contributions X-ray emission from warm-hot int … Contribution ID : 9 Type : Poster X-ray emission from warm-hot intergalactic medium: the role of resonantly scattered cosmic X-ray background We revisit calculations of the X-ray emission from warm-hot intergalactic medium (WHIM) with particular focus on contribution from the resonantly scattered cosmic X-ray background (CXB). -
Erosita – Mapping the X-Ray Universe by P. Predehl
Astron. Nachr. /AN 335, No. 5, 517 – 522 (2014) / DOI 10.1002/asna.201412059 eROSITA – Mapping the X-ray universe P. Predehl Max-Planck-Institut f¨ur extraterrestrische Physik, Giessenbachstraße, D-85748 Garching, Germany Received 2014 Apr 7, accepted 2014 Apr 10 Published online 2014 Jun 2 Key words space vehicles – surveys – telescopes – X-rays: general eROSITA (extended ROentgen Survey with an Imaging Telescope Array) is the core instrument on the Russian/German Spektrum-Roentgen-Gamma (SRG) mission which is currently scheduled for launch late 2015/early 2016. eROSITA will perform a deep survey of the entire X-ray sky. In the soft band (0.5–2 keV), it will be about 30 times more sensitive than ROSAT, while in the hard band (2–8 keV) it will provide the first ever true imaging survey of the sky. The design driving science is the detection of large samples of galaxy clusters to redshifts z>1 in order to study the large scale structure in the universe and test cosmological models including dark energy. In addition, eROSITA is expected to yield a sample of a few million active galactic nuclei, including obscured objects, revolutionizing our view of the evolution of supermassive black holes. The survey will also provide new insights into a wide range of astrophysical phenomena, including X-ray binaries, active stars, and diffuse emission within the Galaxy. eROSITA is currently (Jan 2014) in its flight model and calibration phase. All seven flight mirror modules (plus one spare) have been delivered and measured in X-rays. The first camera including the complete electronics has been extensively tested. -
The Giant Magellan Telescope. Status
The Giant Magellan Telescope. Status By Dr. Mauricio Pilleux Head of Administration (Chile) GMTO Corporation [email protected] April 17, 2019 Observatories in Chile: The beginnings … a successful experiment Cerro Tololo Interamerican Observatory AURA, 1962 Magellan telescopes, 2000 Las Campanas Carnegie Institution of Washington, 1968 La Silla ESO, 1969 2 Observatories in Chile: “Second stage” Very Large Telescope (VLT) Cerro Paranal, ESO, 1999 Gemini South Cerro Pachón, 2002 (AURA) ALMA NRAO-ESO-NAOJ, 2013 3 Observatories in Chile: “Stage 3.0” – big, big, big Giant Magellan Telescope (GMT) Cerro Las Campanas, 2023 (GMTO Corporation) European- Extremely Large Telescope (EELT) Cerro Armazones, 2026 (ESO) Large Synoptic Survey Telescope (LSST) Cerro Pachón, 2022 (NSF/AURA-DOE/SLAC) 4 What next? Size (physical) GMT TMT EELT LSST Main Author – Presentation Title Observatories in Chile: Where? ALMA CCAT* Nanten 2 ASTE Paranal Vista ACT 2 3 E-ELT* TAO* Apex CTA* Las Campanas GMT* Polar Bear Simons Obs. La Silla 1 Tololo SOAR Gemini LSST* 6 Giant Magellan Telescope (GMT): Will be the largest in the world in 2022 25 meters in diameter “Price”: US$1340 million First light: 2023 Enclosure is 62 m high Groundbreaking research in: . Exoplanets and their atmospheres . Dark matter . Distant objects . Unknown unknowns 7 Just how tall is the GMT? 46 meters 8 Giant Magellan Telescope (GMT): The world’s largest optical telescope Korea Sao Paulo, Brazil Texas A&M Arizona New partners are welcome! Main Author – Presentation Title 9 Central mirror casting -
SRGA J124404. 1-632232/SRGU J124403. 8-632231: a New X-Ray
Astronomy & Astrophysics manuscript no. main ©ESO 2021 June 29, 2021 SRGA J124404.1−632232/SRGU J124403.8−632231: a new X-ray pulsar discovered in the all-sky survey by SRG V.Doroshenko1, R. Staubert1, C. Maitra2, A. Rau2, F. Haberl2, A. Santangelo1, A. Schwope3, J. Wilms4, D.A.H. Buckley5; 6, A. Semena7, I. Mereminskiy7, A. Lutovinov7, M. Gromadzki8, L.J. Townsend5; 9, I.M. Monageng5; 6 1 Institut für Astronomie und Astrophysik, Sand 1, 72076 Tübingen, Germany 2 Max-Planck-Institut für extraterrestrische Physik, Gießenbachstraße 1, 85748 Garching, Germany 3 Leibniz-Institut für Astrophysik Potsdam (AIP), An der Sternwarte 16, 14482 Potsdam, Germany 4 Dr. Karl Remeis-Sternwarte and Erlangen Centre for Astroparticle Physics, Friedrich-Alexander-Universität Erlangen-Nürnberg, Sternwartstr. 7, 96049 Bamberg, Germany 5 South African Astronomical Observatory, PO Box 9, Observatory Rd, Observatory 7935, South Africa 6 Department of Astronomy, University of Cape Town, Private Bag X3, Rondebosch 7701, South Africa 7 Space Research Institute (IKI) of Russian Academy of Sciences, Prosoyuznaya ul 84/32, 117997 Moscow, Russian Federation 8 Astronomical Observatory, University of Warsaw, Al. Ujazdowskie 4, 00-478 Warsaw, Poland 9 Southern African Large Telescope, PO Box 9, Observatory Rd, Observatory 7935, South Africa June 29, 2021 ABSTRACT Ongoing all-sky surveys by the the eROSITA and the Mikhail Pavlinsky ART-XC telescopes on-board the Spec- trum Roentgen Gamma (SRG) mission have already revealed over a million of X-ray sources. One of them, SRGA J124404.1−632232/SRGU J124403.8−632231, was detected as a new source in the third (of the planned eight) consecu- tive X-ray surveys by ART-XC. -
Precision Optics Manufacturing and Control for Next-Generation Large
Nanomanufacturing and Metrology https://doi.org/10.1007/s41871-019-00038-2 REVIEW PAPERS Precision Optics Manufacturing and Control for Next‑Generation Large Telescopes Logan R. Graves1 · Greg A. Smith1 · Dániel Apai2,3 · Dae Wook Kim1,2 Received: 2 December 2018 / Revised: 4 February 2019 / Accepted: 7 February 2019 © International Society for Nanomanufacturing and Tianjin University and Springer Nature Singapore Pte Ltd. 2019 Abstract Next-generation astronomical telescopes will ofer unprecedented observational and scientifc capabilities to look deeper into the heavens, observe closer in time to the epoch of the Big Bang, and resolve fner details of phenomena throughout the universe. The science case for this next generation of observatories is clear, with science goals such as the discovery and exploration of extrasolar planets, exploration of dark matter and dark energy, the formation and evolution of planets, stars, galaxies, and detailed studies of the Sun. Enabling breakthrough astronomical goals requires novel and cutting-edge design choices at all stages of telescope manufacturing. In this paper, we discuss the integrated design and manufacturing of the next-generation large telescopes, from the optical design to enclosures required for optimal performance. Keywords Metrology · Fabrication · Design · Telescope · Optics · Precision 1 Introduction Expanding View of the Universe—Science with the Euro- pean Extremely Large Telescope [2]. To provide these scien- Astronomers studying new phenomena and testing increas- tifc capacities and to advance instrumentation capabilities, ingly detailed models of the universe require ever more pow- the next generation of telescopes (NGT) must provide higher erful instruments to complete their goals and collect photons spatial resolutions, larger light-collecting areas, and more which have traversed immense distances and time, some- sensitive instrumentation.