The Proper Motion of the Local Group Galaxy IC 10
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The Dunhuang Chinese Sky: a Comprehensive Study of the Oldest Known Star Atlas
25/02/09JAHH/v4 1 THE DUNHUANG CHINESE SKY: A COMPREHENSIVE STUDY OF THE OLDEST KNOWN STAR ATLAS JEAN-MARC BONNET-BIDAUD Commissariat à l’Energie Atomique ,Centre de Saclay, F-91191 Gif-sur-Yvette, France E-mail: [email protected] FRANÇOISE PRADERIE Observatoire de Paris, 61 Avenue de l’Observatoire, F- 75014 Paris, France E-mail: [email protected] and SUSAN WHITFIELD The British Library, 96 Euston Road, London NW1 2DB, UK E-mail: [email protected] Abstract: This paper presents an analysis of the star atlas included in the medieval Chinese manuscript (Or.8210/S.3326), discovered in 1907 by the archaeologist Aurel Stein at the Silk Road town of Dunhuang and now held in the British Library. Although partially studied by a few Chinese scholars, it has never been fully displayed and discussed in the Western world. This set of sky maps (12 hour angle maps in quasi-cylindrical projection and a circumpolar map in azimuthal projection), displaying the full sky visible from the Northern hemisphere, is up to now the oldest complete preserved star atlas from any civilisation. It is also the first known pictorial representation of the quasi-totality of the Chinese constellations. This paper describes the history of the physical object – a roll of thin paper drawn with ink. We analyse the stellar content of each map (1339 stars, 257 asterisms) and the texts associated with the maps. We establish the precision with which the maps are drawn (1.5 to 4° for the brightest stars) and examine the type of projections used. -
CO Multi-Line Imaging of Nearby Galaxies (COMING) IV. Overview Of
Publ. Astron. Soc. Japan (2018) 00(0), 1–33 1 doi: 10.1093/pasj/xxx000 CO Multi-line Imaging of Nearby Galaxies (COMING) IV. Overview of the Project Kazuo SORAI1, 2, 3, 4, 5, Nario KUNO4, 5, Kazuyuki MURAOKA6, Yusuke MIYAMOTO7, 8, Hiroyuki KANEKO7, Hiroyuki NAKANISHI9 , Naomasa NAKAI4, 5, 10, Kazuki YANAGITANI6 , Takahiro TANAKA4, Yuya SATO4, Dragan SALAK10, Michiko UMEI2 , Kana MOROKUMA-MATSUI7, 8, 11, 12, Naoko MATSUMOTO13, 14, Saeko UENO9, Hsi-An PAN15, Yuto NOMA10, Tsutomu, T. TAKEUCHI16 , Moe YODA16, Mayu KURODA6, Atsushi YASUDA4 , Yoshiyuki YAJIMA2 , Nagisa OI17, Shugo SHIBATA2, Masumichi SETA10, Yoshimasa WATANABE4, 5, 18, Shoichiro KITA4, Ryusei KOMATSUZAKI4 , Ayumi KAJIKAWA2, 3, Yu YASHIMA2, 3, Suchetha COORAY16 , Hiroyuki BAJI6 , Yoko SEGAWA2 , Takami TASHIRO2 , Miho TAKEDA6, Nozomi KISHIDA2 , Takuya HATAKEYAMA4 , Yuto TOMIYASU4 and Chey SAITA9 1Department of Physics, Faculty of Science, Hokkaido University, Kita 10 Nishi 8, Kita-ku, Sapporo 060-0810, Japan 2Department of Cosmosciences, Graduate School of Science, Hokkaido University, Kita 10 Nishi 8, Kita-ku, Sapporo 060-0810, Japan 3Department of Physics, School of Science, Hokkaido University, Kita 10 Nishi 8, Kita-ku, Sapporo 060-0810, Japan 4Division of Physics, Faculty of Pure and Applied Sciences, University of Tsukuba, 1-1-1 Tennodai, Tsukuba, Ibaraki 305-8571, Japan 5Tomonaga Center for the History of the Universe (TCHoU), University of Tsukuba, 1-1-1 Tennodai, Tsukuba, Ibaraki 305-8571, Japan 6Department of Physical Science, Osaka Prefecture University, Gakuen 1-1, -
Constraining the Masses of Microlensing Black Holes and the Mass Gap with Gaia DR2 Łukasz Wyrzykowski1 and Ilya Mandel2,3,4
A&A 636, A20 (2020) Astronomy https://doi.org/10.1051/0004-6361/201935842 & c ESO 2020 Astrophysics Constraining the masses of microlensing black holes and the mass gap with Gaia DR2 Łukasz Wyrzykowski1 and Ilya Mandel2,3,4 1 Warsaw University Astronomical Observatory, Al. Ujazdowskie 4, 00-478 Warszawa, Poland e-mail: [email protected] 2 Monash Centre for Astrophysics, School of Physics and Astronomy, Monash University, Clayton, Victoria 3800, Australia 3 OzGrav: The ARC Center of Excellence for Gravitational Wave Discovery, Australia 4 Institute of Gravitational Wave Astronomy and School of Physics and Astronomy, University of Birmingham, Edgbaston, Birmingham B15 2TT, UK Received 6 May 2019 / Accepted 27 January 2020 ABSTRACT Context. Gravitational microlensing is sensitive to compact-object lenses in the Milky Way, including white dwarfs, neutron stars, or black holes, and could potentially probe a wide range of stellar-remnant masses. However, the mass of the lens can be determined only in very limited cases, due to missing information on both source and lens distances and their proper motions. Aims. Our aim is to improve the mass estimates in the annual parallax microlensing events found in the eight years of OGLE-III observations towards the Galactic Bulge with the use of Gaia Data Release 2 (DR2). Methods. We use Gaia DR2 data on distances and proper motions of non-blended sources and recompute the masses of lenses in parallax events. We also identify new events in that sample which are likely to have dark lenses; the total number of such events is now 18. Results. -
The Extragalactic Distance Scale
The Extragalactic Distance Scale Published in "Stellar astrophysics for the local group" : VIII Canary Islands Winter School of Astrophysics. Edited by A. Aparicio, A. Herrero, and F. Sanchez. Cambridge ; New York : Cambridge University Press, 1998 Calibration of the Extragalactic Distance Scale By BARRY F. MADORE1, WENDY L. FREEDMAN2 1NASA/IPAC Extragalactic Database, Infrared Processing & Analysis Center, California Institute of Technology, Jet Propulsion Laboratory, Pasadena, CA 91125, USA 2Observatories, Carnegie Institution of Washington, 813 Santa Barbara St., Pasadena CA 91101, USA The calibration and use of Cepheids as primary distance indicators is reviewed in the context of the extragalactic distance scale. Comparison is made with the independently calibrated Population II distance scale and found to be consistent at the 10% level. The combined use of ground-based facilities and the Hubble Space Telescope now allow for the application of the Cepheid Period-Luminosity relation out to distances in excess of 20 Mpc. Calibration of secondary distance indicators and the direct determination of distances to galaxies in the field as well as in the Virgo and Fornax clusters allows for multiple paths to the determination of the absolute rate of the expansion of the Universe parameterized by the Hubble constant. At this point in the reduction and analysis of Key Project galaxies H0 = 72km/ sec/Mpc ± 2 (random) ± 12 [systematic]. Table of Contents INTRODUCTION TO THE LECTURES CEPHEIDS BRIEF SUMMARY OF THE OBSERVED PROPERTIES OF CEPHEID -
Lecture 10 Milky Way II
Measuring Structure of the Galaxy • To invert the measured distribution of stars One needs to make a lot – A(m,l,b): # of stars at an of 'corrections' the biggest one apparent mag m, at galactic is due to extinction so one coordinates l,b per sq degree does not repeat Herschel's error! per unit mag. – N(m,l,b): cumulative # of stars with mag < m, at galactic coordinates l,b per sq degree per unit mag. N(m,l,b)=∫ A(m',l,b) dm Into a true 3-D structure 36 Need to Measure Extinction Accurately 37 APOGEE Results • Metallicity across the Milky Way • An example of the fine grain knowledge now being obtained. 38 Gaia Capability • Gaia will survey ~1/4 of the MW (Luri and Robin) 39 Early GAIA Results • Proper motions in the M67 star cluster-accuracies of ~5mas/year (5x10-9 radians/year or 4.3x10-5 pc/year (42 km/sec- 2.5x the speed of the earth around the sun) at distance of M67 ) 40 MW II • Use of gas (HI) to trace velocity field and thus mass of the disk (discuss a bit of the geometry details in the next lecture) – dependence on distance to center of MW • properties of MW (e.g. mass of components) • Cosmic Rays – only directly observable in MW • Start of dynamics 41 Timescales 7 • crossing time tc=2R/σ∼5x10 yrs (R10kpc/v200) • dynamical time td=sqrt(3π/16Gρ)- related to the orbital time; assumption homogenous sphere of density ρ • Relaxation time- the time for a system to 'forget' its initial conditions S+G (eq. -
High-Drag Interstellar Objects and Galactic Dynamical Streams
Draft version March 25, 2019 Typeset using LATEX twocolumn style in AASTeX62 High-Drag Interstellar Objects And Galactic Dynamical Streams T.M. Eubanks1 1Space Initiatives Inc, Clifton, Virginia 20124 (Received; Revised March 25, 2019; Accepted) Submitted to ApJL ABSTRACT The nature of 1I/’Oumuamua (henceforth, 1I), the first interstellar object known to pass through the solar system, remains mysterious. Feng & Jones noted that the incoming 1I velocity vector “at infinity” (v∞) is close to the motion of the Pleiades dynamical stream (or Local Association), and suggested that 1I is a young object ejected from a star in that stream. Micheli et al. subsequently detected non-gravitational acceleration in the 1I trajectory; this acceleration would not be unusual in an active comet, but 1I observations failed to reveal any signs of activity. Bialy & Loeb hypothesized that the anomalous 1I acceleration was instead due to radiation pressure, which would require an extremely low mass-to-area ratio (or area density). Here I show that a low area density can also explain the very close kinematic association of 1I and the Pleiades stream, as it renders 1I subject to drag capture by interstellar gas clouds. This supports the radiation pressure hypothesis and suggests that there is a significant population of low area density ISOs in the Galaxy, leading, through gas drag, to enhanced ISO concentrations in the galactic dynamical streams. Any interstellar object entrained in a dynamical stream will have a predictable incoming v∞; targeted deep surveys using this information should be able to find dynamical stream objects months to as much as a year before their perihelion, providing the lead time needed for fast-response missions for the future in situ exploration of such objects. -
The Stellar Populacons of IC 10 and NGC 1569 Observed with Keck
The Stellar Populaons of IC 10 and NGC 1569 observed with Keck LGSAO and HST William D. Vacca (USRA‐SOFIA) Chris Sheehy James Graham (UC Berkeley) Nate McCrady (UCLA) Properes of IC 10 • Small irregular starburst (BCD) galaxy on outskirts of Local Group – R ~ 1 kpc 9 – M ~ 1‐2 x 10 M • Low metallicity (Z ~ 0.2‐0.3 Z~ ZSMC) • Brief, galaxy‐wide burst of SF occurred within last 10 Myr – Numerous HII regions – Large Hα and FIR luminosity ‐1 • Highest SFR of any LG dwarf (> 0.7 M yr ) – Large populaon of W‐R stars (NWR > 24; SMC has ~ 8) • Highest surface density of W‐Rs in LG ( ~ 8 kpc‐2; MW ~ 2.5 kpc‐2) • Anomalously high WC/WN rao ( ~ 1‐2) for its Z (10x too large!) • Have WN stars been missed in surveys? • b = −3.3° – Uncertain reddening: AV = 1.2 – 6.0 mag – Uncertain distance: D = 0.5 – 3.0 Mpc • Ideal extragalacc target for NIR observaons with LGSAO – Nearby, relavely large AV (foreground and internal), high ρ★ – Bright p‐lt guide stars available N IC 10 HST/ACS/WFC F435W, F606W, F814W 1” ≈ 4 pc WR Object: [MAC92] 24 • Brightest W‐R candidate in HST/WFPC2 F555W IC10 • Lies within prominent H II region HL 111c • Lies at center of a young stellar cluster (Hunter 2001) • Uncertain spectral type 5’’ – Weak, broad He II 4686 emission (Massey & Holmes 2002) – WN+OB? • Three components (A, B, C) • Cluster itself? Crowther et al. (2003) Observaons • NIR Data: • Opcal Data: – NIRC2/Keck II/LGSAO H and K’ – HST/ACS/WFC F814W – 0.01”pixel‐1 – 0.05”pixel‐1 – Final FOV = 12.2” x 12.2” – texp = 1080 s – texp = 1200 s (H); 1500 s (K’) – FWHM = 0.08” – FWHM = 0.048” (H); 0.051” (K’) – Strehl ~ 18% (H); 32% (K’) ACS WFC / NIRC2 Comparison HST/ACS/WFC F814W Keck II/NIRC2/LGSAO K’ IC 10 IHK’ N E 12.2” x 12.2” 47 pc x 47 pc Vacca, Sheehy, & Graham (2007) CMD of IC 10 [MAC92] 24 Region Opcal Data: • PSF fing (Anderson & King 2006) • 690 stars found in F814W • [F814W]Lim ~ 25.25 • σ < 0.04 mag for [F814W] < 23.0 NIR Data: • MTF‐fing method (Sheehy et al. -
New Wide Common Proper Motion Binaries
Vol. 6 No. 1 January 1, 2010 Journal of Double Star Observations Page 30 New Wide Common Proper Motion Binaries Rafael Benavides1,2, Francisco Rica2,3, Esteban Reina4, Julio Castellanos5, Ramón Naves6, Luis Lahuerta7, Salvador Lahuerta7 1. Astronomical Society of Córdoba, Observatory of Posadas, MPC-IAU Code J53, C/.Gaitán nº 20, 1º, 14730 Posadas (Spain) 2. Double Star Section of Liga Iberoamericana de Astronomía (LIADA), Avda. Almirante Guillermo Brown No. 4998, 3000 Santa Fe (Argentina) 3. Astronomical Society of Mérida, C/José Ruíz Azorín, 14, 4º D, 06800 Mérida (Spain) 4. Plza. Mare de Dèu de Montserrat, 1 Etlo 2ªB, 08901 L'Hospitalet de Llobregat (Spain) 5. 0bservatory with MPC-IAU Code 939, Av. Primado Reig 183, 46020 Valencia (Spain) 6. Observatory of Montcabrer, MPC-IAU Code 213, C/Jaume Balmes, 24, 08348 Cabrils (Spain) 7. G.E.O.D.A., Observatorio Manises, MPC-IAU Code J98, C/ Mayor, 111-4, 46940 Manises (Spain) Abstract: In this work we report the discovery of 150 new double stars of which 142 are wide common proper motion stellar systems. In addition to this, we report the study of 23 recently catalogued wide common proper motion binaries discovered by other observers. Spectral types, photometric distances, kinematics and ages were determined from data ob- tained consulting the literature. Several criteria were used to determine the nature of each double star. Orbital periods and the semimajor axes were calculated. they are good sensors to detect unknown mass concen- 1. Introduction trations that they may encounter along their galactic For several years double-star amateurs have con- trajectories. -
ISOCAM Observations of Normal Star-Forming Galaxies: the Key Project Sample’
ISOCAM Observations of Normal Star-Forming Galaxies: The Key Project Sample’ D.A. Dale,2 N.A. Silbermann,2 G. Heloq2 E. Valjaveq2 S. Malhotra,2 C.A. Beichman,2 J. Brauher,2 A. Contursi,2H. Diner~tein,~D. H~llenbach,~D. Hunter,s S. Kolhatkar,2 K.Y. LO,^ S. Lord,2 N.Y. Lu,~R. Rubiq4 G. Stacey,? H. Thronson, Jr.,’ M. Werner,g H. Corwin2 ABSTRACT We present mid-infrared maps and preliminary analysis for 61 galaxies observed with the Infrared Space Observatory. Many of the general features of galaxies observed at optical wavelengths-spiral arms, disks, rings, and bright knots of emission-are also seen in the mid-infrared, except the prominent optical bulges are absent at 6.75 and 15 pm. In addition, the maps are quite similar at 6.75 and 15 pm, except for a few cases where a central starburst leads to lower !dS3~4ratios in the inner region. kVe also present infrared flux densities and mid-infrared sizes for these galasies. The mid-infrared color Iu(6.Zpm) Iu(l.5pm) shows a distincttrend with the far-infrared color m.The quiescent galasies in our sample 1, (60~)g 0.6) show unity,near ( I,( 1OOpm) whereas this ratio drops significantly for galaxies with higher global heating intensity levels. Azimuthally-averaged surface brightness profiles indicate the extent to which the mid-infrared flux is centrally concerltratecl, a,rltl provide information on the radial dependence of mid-infrared colors. The galaxies are mostly well resolved in these maps: almost half of them have < 10% of their flux in the central resolution element. -
Water Maser Emission in IC 342
Astronomy & Astrophysics manuscript no. (will be inserted by hand later) Water maser emission in IC 342 A. Tarchi1, C. Henkel1, A. B. Peck1, and K. M. Menten1 Max-Planck-Institut f¨ur Radioastronomie, Auf dem H¨ugel 69, D-53121 Bonn, Germany Received date / Accepted date Abstract. The detection of 22 GHz water vapor emission from IC 342 is reported, raising the detection rate among northern galaxies with IRAS point source fluxes S100µm > 50 Jy to 16%. The maser, associated with a star forming region ∼10–15′′ west of the nucleus, consists of a single 0.5 km s−1 wide feature and reaches an isotropic −2 < 16 < luminosity of 10 L⊙ (D=1.8 Mpc). If the time variability is intrinsic, the maser size is ∼ 1.5×10 cm (∼0.5 mas) which corresponds to a brightness temperature of ∼>109 K. The linewidth, luminosity, and rapid variability are reminiscent of the 8 km s−1 super maser in Orion-KL. A velocity shift of 1 km s−1 within two weeks and subsequent rapid fading is explained in terms of a chance alignment of two dense molecular clouds. Observations at 22 GHz toward Maffei 2 are also reported, yielding a 5σ upper limit of 25 mJy for a channel spacing of 1.05 km s−1. Key words. Galaxies: individual: IC 342, Maffei 2 – Galaxies: starburst – ISM: molecules – masers – Radio lines: ISM 1. Introduction star formation, to measure the velocity vectors of these regions through VLBI proper motion studies, and to de- Isotropic luminosities of extragalactic 22 GHz H2O masers termine true distances through complementary measure- span a huge range (see e.g. -
Lecture 8: Stellar Motions Reading: Box 19-1
Lecture 8: Stellar Motions Reading: Box 19-1 Key Ideas The stars are in constant motion. Observed Motions Proper motions (motion against the background, measured in angular motion/time) Radial velocities (motion towards or away, measured from the Doppler shift) True Space Motion Combination of radial velocity, proper motion, and distance (important for proper motion!) The “Fixed” Stars Although the stars are moving, their motions across the sky are so small that to the naked eye, the stars appear “fixed” to the sky. Great distances make the amount of motion small on human lifetimes. (Of course, stars moving directly away or towards us will not to appear to move across the sky) Proper Motions Apparent angular motion across the sky of nearby stars with respect to distant objects. (Distant stars are used because we assume that even though they are moving through space they are so far away that from our perspective they are fixed). It is the projection of the star’s true motion through space relative to the Sun. Typical proper motion for stars in the solar neighborhood is about 0.1 arcsec/year Largest proper motion measured is 10.25 arcsec/year Barnard’s Star) Proper motions are cumulative. Effects build up over time. The longer you wait, the greater apparent angular motion is. Measuring proper motions: Compare photos of the sky taken 20 to 50 years apart Measure how much stars have moved compared to more distant background objects (galaxies, quasars). Example: if a star has a proper motion of 0.1 arcsec/year: In one year, it moves 0.1 arcsec In 10 years, it moves 10x0.1= 1 arcsec In 100 years, it moves 100x0.1 =10 arcsec It can take a long time for the constellations to noticeably change shape. -