Two Wolf-Rayet Stars at the Heart of Colliding-Wind Binary Apep
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Naming the Extrasolar Planets
Naming the extrasolar planets W. Lyra Max Planck Institute for Astronomy, K¨onigstuhl 17, 69177, Heidelberg, Germany [email protected] Abstract and OGLE-TR-182 b, which does not help educators convey the message that these planets are quite similar to Jupiter. Extrasolar planets are not named and are referred to only In stark contrast, the sentence“planet Apollo is a gas giant by their assigned scientific designation. The reason given like Jupiter” is heavily - yet invisibly - coated with Coper- by the IAU to not name the planets is that it is consid- nicanism. ered impractical as planets are expected to be common. I One reason given by the IAU for not considering naming advance some reasons as to why this logic is flawed, and sug- the extrasolar planets is that it is a task deemed impractical. gest names for the 403 extrasolar planet candidates known One source is quoted as having said “if planets are found to as of Oct 2009. The names follow a scheme of association occur very frequently in the Universe, a system of individual with the constellation that the host star pertains to, and names for planets might well rapidly be found equally im- therefore are mostly drawn from Roman-Greek mythology. practicable as it is for stars, as planet discoveries progress.” Other mythologies may also be used given that a suitable 1. This leads to a second argument. It is indeed impractical association is established. to name all stars. But some stars are named nonetheless. In fact, all other classes of astronomical bodies are named. -
Assaj V2 N4 1930-Jan
ijtlJt Journal {If tl]t J\.strauamital ~ add!,! af ~ autb J\.frita. Vol. II. JANUARY, 1930. No.4. Astronomical Society of South Africa~ "' AT HOME" TO VISITING ASTRONOMERS OF THE BRITISH ASSOCIATION. July 26, 1929, will long be remembered in the annals of the Astronomical Society of South Africa, for on the evening of that day it was "At Home" at the Oddfellows' Hall, Plein Street, Cape Town, to the visiting astronomers who were attending the meetings of the British Association. The chair was taken by Mr. A. W. Long, President of the Society, who, in opening the proceedings, said: This gathering of the Astronomical Society of South Africa has been arranged to enable the members to greet the distinguished astronomers and other eminent scien tists interested in astronomy who are visiting South Africa in connection with the meetings of the British Association. We have with us to-night Sir Frank Dyson, the Astronomer Royal; Professor Eddington, Director of the Cambridge University Observatory; Professor Fowl~r, Yarrow Research Professor of the Royal Society; Pro fessor Chapman, of the Imperial College of Science; Professor De Sitter, Director of the Leiden Observatory; Dr. Guthnick, Director of the Berlin-Babelsberg Obser vatory; Dr. K110x-Shaw, Director of the Radcliffe Observatory; Mr. Greaves, of the Greenwich Observa tory; Mr. Wrigley, of the Edinburgh Observatory; Dr. Aston, of Cambridge, and I am pleased to say that at a later stage Lord Rayleigh will also be here. In the name of the Society I extend to these gentlemen a very hearty welcome. We have been familiar with them for a very long time by name, and through their scientific attainments; now we are delighted to have the honour of meeting them in person. -
A Basic Requirement for Studying the Heavens Is Determining Where In
Abasic requirement for studying the heavens is determining where in the sky things are. To specify sky positions, astronomers have developed several coordinate systems. Each uses a coordinate grid projected on to the celestial sphere, in analogy to the geographic coordinate system used on the surface of the Earth. The coordinate systems differ only in their choice of the fundamental plane, which divides the sky into two equal hemispheres along a great circle (the fundamental plane of the geographic system is the Earth's equator) . Each coordinate system is named for its choice of fundamental plane. The equatorial coordinate system is probably the most widely used celestial coordinate system. It is also the one most closely related to the geographic coordinate system, because they use the same fun damental plane and the same poles. The projection of the Earth's equator onto the celestial sphere is called the celestial equator. Similarly, projecting the geographic poles on to the celest ial sphere defines the north and south celestial poles. However, there is an important difference between the equatorial and geographic coordinate systems: the geographic system is fixed to the Earth; it rotates as the Earth does . The equatorial system is fixed to the stars, so it appears to rotate across the sky with the stars, but of course it's really the Earth rotating under the fixed sky. The latitudinal (latitude-like) angle of the equatorial system is called declination (Dec for short) . It measures the angle of an object above or below the celestial equator. The longitud inal angle is called the right ascension (RA for short). -
Dr Joseph Callingham
Dr Joseph Callingham PERSONAL DETAILS Nationality: Australian Address: Leiden Observatory, Leiden University J.H. Oort Building, Niels Bohrweg 2, 2333 CA, Leiden, The Netherlands Phone Number: +31 629 297 915 Email: [email protected] Website: www.astron.nl/~callingham EDUCATION THE UNIVERSITY OF SYDNEY 2013 - 2017 PhD in Astrophysics Title: The Extragalactic Sky at Low Radio Frequencies: A Study of Peaked-Spectrum Sources Supervisors: Prof. Bryan Ganesler and Prof. Ron Ekers 2009 - 2012 Bachelor of Science (Advanced) - First Class Honours (Physics) Majors: Physics, Applied Mathematics. Minors: Ancient Greek History, Political Science. EMPLOYMENT January 2020 - present NWO Veni Fellow, Leiden University January 2017 - December 2019 de Bruyn (ASTRON) Fellow, Netherlands Institute for Radio Astronomy REFEREED PAPERS I am first author of eight papers published in Nature Astronomy, The Astrophysical Journal, and Monthly Notices of the Royal Astronomical Society. I am also co-author of an additional 62 papers published in a range of peer-reviewed journals, 30 of which I have contributed to significantly. My h-index is 17, with a total of 1,018 citations. Two of my papers have over 100 citations each. Bibliographic information for my highest impact work and total publication record can be found at the end of this curriculum vitae. SUCCESSFUL TELESCOPE PROPOSALS I have been the principal investigator and a co-investigator on successful proposals for a range of telescopes spanning the electromagnetic spectrum. For co-investigated proposals, -
Anisotropic Winds in Wolf-Rayet Binary Identify Potential Gamma-Ray Burst Progenitor
DRAFT VERSION SEPTEMBER 24, 2018 Typeset using LATEX preprint style in AASTeX61 ANISOTROPIC WINDS IN WOLF-RAYET BINARY IDENTIFY POTENTIAL GAMMA-RAY BURST PROGENITOR J. R. CALLINGHAM,1 P. G. TUTHILL,2 B. J. S. POPE,2, 3, 4 P. M. WILLIAMS,5 P. A. CROWTHER,6 M. EDWARDS,2 B. NORRIS,2 AND L. KEDZIORA-CHUDCZER7 1ASTRON, Netherlands Institute for Radio Astronomy, PostBus 2, 7990 AA, Dwingeloo, The Netherlands 2Sydney Institute for Astronomy (SIfA), School of Physics, The University of Sydney, NSW 2006, Australia 3Center for Cosmology and Particle Physics, Department of Physics, New York University, 726 Broadway, New York, NY 10003, USA 4NASA Sagan Fellow 5Institute for Astronomy, University of Edinburgh, Royal Observatory, Edinburgh EH9 3HJ, UK 6Department of Physics & Astronomy, University of Sheffield, Sheffield, S3 7RH, UK 7School of Physics, University of New South Wales, NSW 2052, Australia (Accepted to Nature Astronomy, Revision 3) INTRODUCTORY PARAGRAPH The massive evolved Wolf-Rayet stars sometimes occur in colliding-wind binary systems in which dust plumes are formed as a result of the collision of stellar winds1. These structures are known to encode the parameters of the binary orbit and winds2,3,4. Here we report observations of a pre- viously undiscovered Wolf-Rayet system, 2XMM J160050.7–514245, with a spectroscopically deter- mined wind speed of 3400 km s−1. In the thermal infrared, the system is adorned with a prominent 1200 spiral dust plume,≈ revealed by proper motion studies to be expanding at only 570 km s−1. As≈ the dust and gas appear coeval, these observations are inconsistent with existing models≈ of the dynamics of such colliding wind systems5,6,7. -
The Promise and Challenges of Multiplex Spectroscopy for Exoplanet Science
The Promise and Challenges of Multiplex Spectroscopy for Exoplanet Science Wide-Field InfraRed Surveys: Science and Techniques Michael W. McElwain November 18, 2014 Roman Technology Fellow Goddard AFTA Study Scienst Exo-C Science and Technology Definion Team Goddard Space Flight Center Recent Collaborators Goddard: Qian Gong, Marshall Perrin (STScI), Karl Stapelfeldt (Exo-C Chair), Bruce Woodgate, Jorge Llop, Daniel Angerhausen, James Bubeck, Ken Carpenter, Mark Clampin, Rick Demers (JPL), Shawn Domagal-Goldman, Janan Ferdosi (JPL), Carol Grady, Bryan Grammer, Brad Greeley, George Hilton, Sally Heap, Marc Kuchner, Don Lindler, Avi Mandell, Nargess Memarsadeghi, Bre Morris, Tim Norton, Debbie Padge, Bernie Rauscher, Aki Roberge, Chris Stark, Hong Tang (JPL), Harley Thronson, John Trauger (JPL), Ashlee Wilkins, GIFS team, JWST Team, Exo-C Team Princeton: Tim Brandt (IAS), N. Jeremy Kasdin, Cullen Blake (UPenn), Adam Burrows, Eric Cady (JPL), Michael Carr, Courtney Dressing (Harvard), Tyler Groff, Jim Gunn, Jason Kay (Bell Labs), Jill Knapp, Mary Ann Limbach, Nikku Madhusudhan (Cambridge), Amaya Moro-Marn (STScI), Laurent Pueyo (STScI), Dave Spiegel (Project Florida), Dan Sirbu (NASA Ames), David SperGel, Ed Turner, Robert Vanderbei SEEDS: Motohide Tamura (PI), Joe Carson, Thayne Currie, Markus Feldt, Miwa Goto, Carol Grady, Olivier Guyon, Thomas Henning, Klaus Hodapp, Markus Janson, Ryo Kandori, Jungmi Kwon, Masayuki Kuzuhara, Taro Matsuo, Ryuji Suzuki, Chrisan Thalmann, John Wisniewski, + ~60 others Primary AFTA-C Exoplanet Imaging Spectrograph Design Goals Specificaons AFTA-C Spectrograph Field of View < 48 λ/D × 48 λ/D (TBR) 2.5”×2.5” at 600 nm Spaal Sampling 0.3 λ/D at 600nm (TBR) Spectral Range 600-970 nm 18% at λc 720, 840, 970 Spectral Resoluon R=70 Detector Read Noise < 1e-3 e-/frame (TBR) Detector Dark Current < 1e-4 e-/pix/s (TBR) *See Wilkins, McElwain, Norton, Rauscher, et al. -
Ann16 17.Pdf
Front cover page: A system of channels (centered at 20.53◦N, -118.49◦E) emanated from the graben near to Jovis Tholus region, Mars. MRO-CTX stereo pair derived DTM draped over the CTX image. Presence of multiple channels, braided-like channel network at the downstream end, and terraces suggests their plausible fluvial origin. Lava flow into the channels termini hindered the real extent of the channel network, b) an example of a streamlined island form ed within the channel and c) an example of a curvilinear island suggesting the possible flow direction. Inside back cover pages: Events at PRL Back cover page: Top Panel: Alpha Particle X-ray Spectrometer on-board Chandrayaan-2 rover [Mechanical Configuration] Middle Panel: AMS Laboratory Bottom Panels: Pre-monsoon and post-monsoon δ18O & d-excess maps of shallow groundwater in India. Compilation and Layout by: Office of the Dean, PRL. Published by: Physical Research Laboratory, Ahmedabad. Contact: Physical Research Laboratory Navrangpura Ahmedabad - 380 009, India Phone: +91-79-2631 4000 / 4855 Fax: +91-79-2631 4900 Cable: RESEARCH Email: [email protected] Website: https://www.prl.res.in/ PRL Annual Report 2016 { 2017 PRL Council of Management Three nominees from Govt. of India Professor U.R. Rao, Former Chairman, ISRO Chairman Antariksh Bhavan, New BEL Road Bengaluru-560231 Shri A. S. Kiran Kumar, Secretary, Member Department of Space, Govt. of India & Chairman, ISRO Antariksh Bhavan, Bengaluru-560231 Shri A. Vijay Anand, IRS, Additional Secretary & FA Member Department of Space, Govt. of India (Up to 31.08.2016) Antariksh Bhavan, Bengaluru-560231 Shri S. -
The Extreme Colliding-Wind System Apep : Resolved Imagery of the Central Binary and Dust Plume in the Infrared
This is a repository copy of The extreme colliding-wind system Apep : resolved imagery of the central binary and dust plume in the infrared. White Rose Research Online URL for this paper: http://eprints.whiterose.ac.uk/166781/ Version: Published Version Article: Han, Y., Tuthill, P.G., Lau, R.M. et al. (6 more authors) (2020) The extreme colliding-wind system Apep : resolved imagery of the central binary and dust plume in the infrared. Monthly Notices of the Royal Astronomical Society, 498 (4). pp. 5604-5619. ISSN 0035-8711 https://doi.org/10.1093/mnras/staa2349 This is a pre-copyedited, author-produced version of an article accepted for publication in Monthly Notices of the Royal Astronomical Society following peer review. The version of record [Y Han, P G Tuthill, R M Lau, A Soulain, J R Callingham, P M Williams, P A Crowther, B J S Pope, B Marcote, The extreme colliding-wind system Apep: resolved imagery of the central binary and dust plume in the infrared, Monthly Notices of the Royal Astronomical Society, Volume 498, Issue 4, November 2020, Pages 5604–5619, https://doi.org/10.1093/mnras/staa2349] is available online at: https://academic.oup.com/mnras/article/498/4/5604/5917924 Reuse Items deposited in White Rose Research Online are protected by copyright, with all rights reserved unless indicated otherwise. They may be downloaded and/or printed for private study, or other acts as permitted by national copyright laws. The publisher or other rights holders may allow further reproduction and re-use of the full text version. -
Two Wolf-Rayet Stars at the Heart of Colliding-Wind Binary Apep
MNRAS 000, 1–10 (2020) Preprint 4 May 2020 Compiled using MNRAS LATEX style file v3.0 Two Wolf-Rayet stars at the heart of colliding-wind binary Apep J. R. Callingham,1,2⋆ P. A. Crowther,3 P. M. Williams,4 P. G. Tuthill,5 Y. Han,5 B. J. S. Pope,6,7,8 and B. Marcote9 1Leiden Observatory, Leiden University, PO Box 9513, 2300 RA, Leiden, The Netherlands 2ASTRON, Netherlands Institute for Radio Astronomy, Oude Hoogeveensedijk 4, Dwingeloo, 7991 PD, The Netherlands 3Department of Physics & Astronomy, University of Sheffield, Sheffield, S3 7RH, UK 4Institute for Astronomy, University of Edinburgh, Royal Observatory, Edinburgh EH9 3HJ, UK 5Sydney Institute for Astronomy (SIfA), School of Physics, The University of Sydney, NSW 2006, Australia 6Center for Cosmology and Particle Physics, Department of Physics, New York University, 726 Broadway, New York, NY 10003, USA 7Center for Data Science, New York University, 60 5th Ave, New York, NY 10011, USA 8NASA Sagan Fellow 9Joint Institute for VLBI ERIC, Oude Hoogeveensedijk 4, 7991 PD Dwingeloo, The Netherlands Accepted 1 May 2020. Received 1 May 2020; in original form 3 April 2020 ABSTRACT Infrared imaging of the colliding-wind binary Apep has revealed a spectacular dust plume with complicated internal dynamics that challenges standard colliding-wind binary physics. Such challenges can be potentially resolved if a rapidly-rotating Wolf-Rayet star is located at the heart of the system, implicating Apep as a Galactic progenitor system to long-duration gamma-ray bursts. One of the difficulties in interpreting the dynamics of Apep is that the spectral composition of the stars in the system was unclear. -
Multicolour Deep CCD Photometric Study of the Moderately Young Southern Open Star Clusters NGC 3228, NGC 4103, NGC 5662 and NGC 6087? R
ASTRONOMY & ASTROPHYSICS APRIL I 1997,PAGE9 SUPPLEMENT SERIES Astron. Astrophys. Suppl. Ser. 122, 9-29 (1997) Multicolour deep CCD photometric study of the moderately young southern open star clusters NGC 3228, NGC 4103, NGC 5662 and NGC 6087? R. Sagar1,2,?? and R.D. Cannon2 1 Indian Institute of Astrophysics, Bangalore 560034, India e-mail address: [email protected] 2 Anglo-Australian Observatory, P.O. Box 296, Epping NSW 2121, Australia e-mail address: [email protected] Received April 2; accepted June 26, 1996 Abstract. CCD observations in the U, B, V , R 1. Introduction and I passbands have been used to generate colour- colour and deep colour-magnitude diagrams for the The colour magnitude diagrams (CMDs) of moderately young open star clusters NGC 3228, NGC 4103, young (∼ 20−50 Myr) open star clusters show the effect of NGC 5662 and NGC 6087. The sample consists of about stellar evolution at the brighter end and contain pre−main 2000 stars reaching down to V = 20 mag. The interstel- sequence (PMS) stars at the fainter end. Consequently, lar extinction across the face of the imaged cluster regions they provide a rare opportunity for reliable estimation of seems to be uniform with average values of E(B − V )= ages of high and low mass stars formed in a molecular 0.31, 0.34 and 0.22 mag for NGC 4103, NGC 5662 and cloud. So they can be used to determine the length of NGC 6087 respectively. The distances to the clusters time over which star formation was active in a particular NGC 3228, NGC 4103, NGC 5662 and NGC 6087 have region and also to know which stars form first − high mass been estimated as 0.5 ± 0.05, 2.0 ± 0.3, 0.8 ± 0.1and or low mass ones or if they formed together. -
Research Paper
DRAFT VERSION SEPTEMBER 20, 2018 Typeset using LATEX preprint style in AASTeX61 ANISOTROPIC WINDS IN WOLF-RAYET BINARY IDENTIFY POTENTIAL GAMMA-RAY BURST PROGENITOR J. R. CALLINGHAM,1 P. G. TUTHILL,2 B. J. S. POPE,2, 3, 4 P. M. WILLIAMS,5 P. A. CROWTHER,6 M. EDWARDS,2 B. NORRIS,2 AND L. KEDZIORA-CHUDCZER7 1ASTRON, Netherlands Institute for Radio Astronomy, PostBus 2, 7990 AA, Dwingeloo, The Netherlands 2Sydney Institute for Astronomy (SIfA), School of Physics, The University of Sydney, NSW 2006, Australia 3Center for Cosmology and Particle Physics, Department of Physics, New York University, 726 Broadway, New York, NY 10003, USA 4NASA Sagan Fellow 5Institute for Astronomy, University of Edinburgh, Royal Observatory, Edinburgh EH9 3HJ, UK 6Department of Physics & Astronomy, University of Sheffield, Sheffield, S3 7RH, UK 7School of Physics, University of New South Wales, NSW 2052, Australia (Accepted to Nature Astronomy, Revision 3) INTRODUCTORY PARAGRAPH The massive evolved Wolf-Rayet stars sometimes occur in colliding-wind binary systems in which dust plumes are formed as a result of the collision of stellar winds1. These structures are known to encode the parameters of the binary orbit and winds2,3,4. Here we report observations of a pre- viously undiscovered Wolf-Rayet system, 2XMM J160050.7–514245, with a spectroscopically deter- mined wind speed of 3400 km s−1. In the thermal infrared, the system is adorned with a prominent 1200 spiral dust plume,≈ revealed by proper motion studies to be expanding at only 570 km s−1. As≈ the dust and gas appear coeval, these observations are inconsistent with existing models≈ of the dynamics of such colliding wind systems5,6,7. -
Lists and Charts of Autostar Named Stars
APPENDIX A Lists and Charts of Autostar Named Stars Table A.I provides a list of named stars that are stored in the Autostar database. Following the list, there are constellation charts which show where the stars are located. The names are in alphabetical orderalong with their Latin designation (see Appendix B for complete list ofconstellations). Names in brackets 0 in the table denote a different spelling to one that is known in the list. The star's co-ordinates are set to the same as accuracy as the Autostar co-ordinates i.e. the RA or Dec 'sec' values are omitted. Autostar option: Select Item: Object --+ Star --+ Named 215 216 Appendix A Table A.1. Autostar Named Star List RA Dec Named Star Fig. Ref. latin Designation Hr Min Deg Min Mag Acamar A5 Theta Eridanus 2 58 .2 - 40 18 3.2 Achernar A5 Alpha Eridanus 1 37.6 - 57 14 0.4 Acrux A4 Alpha Crucis 12 26.5 - 63 05 1.3 Adara A2 EpsilonCanis Majoris 6 58.6 - 28 58 1.5 Albireo A4 BetaCygni 19 30.6 ++27 57 3.0 Alcor Al0 80 Ursae Majoris 13 25.2 + 54 59 4.0 Alcyone A9 EtaTauri 3 47.4 + 24 06 2.8 Aldebaran A9 Alpha Tauri 4 35.8 + 16 30 0.8 Alderamin A3 Alpha Cephei 21 18.5 + 62 35 2.4 Algenib A7 Gamma Pegasi 0 13.2 + 15 11 2.8 Algieba (Algeiba) A6 Gamma leonis 10 19.9 + 19 50 2.6 Algol A8 Beta Persei 3 8.1 + 40 57 2.1 Alhena A5 Gamma Geminorum 6 37.6 + 16 23 1.9 Alioth Al0 EpsilonUrsae Majoris 12 54.0 + 55 57 1.7 Alkaid Al0 Eta Ursae Majoris 13 47.5 + 49 18 1.8 Almaak (Almach) Al Gamma Andromedae 2 3.8 + 42 19 2.2 Alnair A6 Alpha Gruis 22 8.2 - 46 57 1.7 Alnath (Elnath) A9 BetaTauri 5 26.2