Pre-Existing Dwarfs, Tidal Knots and a Tidal Dwarf Galaxy: an Unbiased HI
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Near-Infrared Luminosity Relations and Dust Colors L
A&A 578, A47 (2015) Astronomy DOI: 10.1051/0004-6361/201525817 & c ESO 2015 Astrophysics Obscuration in active galactic nuclei: near-infrared luminosity relations and dust colors L. Burtscher1, G. Orban de Xivry1, R. I. Davies1, A. Janssen1, D. Lutz1, D. Rosario1, A. Contursi1, R. Genzel1, J. Graciá-Carpio1, M.-Y. Lin1, A. Schnorr-Müller1, A. Sternberg2, E. Sturm1, and L. Tacconi1 1 Max-Planck-Institut für extraterrestrische Physik, Postfach 1312, Gießenbachstr., 85741 Garching, Germany e-mail: [email protected] 2 Raymond and Beverly Sackler School of Physics & Astronomy, Tel Aviv University, 69978 Ramat Aviv, Israel Received 5 February 2015 / Accepted 5 April 2015 ABSTRACT We combine two approaches to isolate the AGN luminosity at near-IR wavelengths and relate the near-IR pure AGN luminosity to other tracers of the AGN. Using integral-field spectroscopic data of an archival sample of 51 local AGNs, we estimate the fraction of non-stellar light by comparing the nuclear equivalent width of the stellar 2.3 µm CO absorption feature with the intrinsic value for each galaxy. We compare this fraction to that derived from a spectral decomposition of the integrated light in the central arcsecond and find them to be consistent with each other. Using our estimates of the near-IR AGN light, we find a strong correlation with presumably isotropic AGN tracers. We show that a significant offset exists between type 1 and type 2 sources in the sense that type 1 MIR X sources are 7 (10) times brighter in the near-IR at log LAGN = 42.5 (log LAGN = 42.5). -
On the Origin and Propagation of Ultra-High Energy Cosmic Rays (Measurements & Prediction Techniques)
Dissertation On the Origin and Propagation of Ultra-High Energy Cosmic Rays (Measurements & Prediction Techniques) Nils Nierstenhoefer Wuppertal, 2011 University of Wuppertal Supervisor/First reviewer: Prof. Dr. K.-H. Kampert Second reviewer: Prof. Dr. M. Risse Motivation & Preface It is a long known fact that cosmic rays reach Earth with tremendous energies of even above 1020 eV. Despite of decades of intensive research, it was not possible to finally reveal the origin of these par- ticles. The main obstacle in this field is their rare occurrence. This is due to a very steep energy spectrum. To make this point more clear, one roughly expects to observe less than one particle per km2 in one century exceeding energies larger than 1020 eV. To overcome the limitation of low statis- tics, larger and larger cosmic ray detectors have been deployed. Today’s largest cosmic ray detector is the Pierre Auger observatory (PAO) which was constructed in the Pampa Amarilla in Argentina. It covers an area of 3000 km2 and provides the largest set of observations of ultra-high energy cosmic rays (UHECR) in history. A second difficulty in understanding the origin of UHECR should be pointed out: Galactic and extra- galactic magnetic fields might alter the direction of even the highest energy events in a way that they do not point back to their source. In 2007 and 2008, already before the completion of the full detector, the Auger collaboration pub- lished a set of three important papers [1, 2, 3]. The first paper dealt with the correlation of the arrival directions of the highest energetic events with the distribution of active galactic nuclei (AGN) closer than 75Mpc from a catalog compiled by Veron-Cetty and Veron (VC-V) [4]. -
Nicholas Stone Einstein Fellow, Columbia University MODEST-18 6/29/18
Elevated Tidal Disruption Rates in Post-Starburst Galaxies Nicholas Stone Einstein Fellow, Columbia University MODEST-18 6/29/18 With: Aleksey Generozov, Eugene Vasiliev, Brian Metzger, Sjoert van Velzen A View to a Kill MBH=106M⦿, aBH=0.9, i=90˚ Face-On Edge-On Rt Rt PN-SPH (Hayasaki, NCS & Loeb 16) He IIλ4686 line is still evident as an excess above the model in the later epoch, however it has faded by a factor of ∼ 10 since the pre-preak spectrum, the same factor by which the ultraviolet continuum has faded during this time. Note that the absolute flux scaling in the later epoch is uncertain due to clouds on the date of the observation. Tidal Disruption Events • Empirically: ✦ Rare multiwavelength (radio -> hard X-ray) transients ✦ Dozens of strong candidate flares (most optical/X-ray) • Applications: Figure 2 ✦ Ultraviolet and optical light curve. The GALEX NUV and PS1 gP1-, rP1-, iP1-, and zP1- Tools to measure SMBH demographyband light curve of PS1-10jh (with the host galaxy flux removed) with 1σ error bars and in logarithmic days since the time of disruption determined from the best fit of the rP1-band (mass, maybe spin) light curve to the numerical model20 for the mass accretion rate of a tidally disrupted star with a polytropic exponent of 5/3 (shown with solid lines scaled to the flux in the GALEX and PS1 bands). The GALEX and PS1 photometry at t>240 rest-frame days since ✦ Super-Eddington accretion the peak is shown binned in time in order to increase the signal-to-noise. -
A Disturbed Galactic Duo 20 April 2011
A disturbed galactic duo 20 April 2011 neighbours. This galactic grouping, found about 70 million light- years away in the constellation Sextans (The Sextant), was discovered by the English astronomer William Herschel in 1783. Modern astronomers have gauged the distance between NGC 3169 (left) and NGC 3166 (right) as a mere 50 000 light-years, a separation that is only about half the diameter of the Milky Way galaxy. In such tight quarters, gravity can start to play havoc with galactic structure. Spiral galaxies like NGC 3169 and NGC 3166 tend to have orderly swirls of stars and dust pinwheeling about their glowing centres. Close encounters with other massive objects can jumble this classic configuration, often serving as a disfiguring prelude to the merging of galaxies into one larger galaxy. So far, the interactions of NGC 3169 and NGC 3166 have just lent a bit of character. NGC 3169's This image from the Wide Field Imager on the arms, shining bright with big, young, blue stars, MPG/ESO 2.2-meter telescope at the La Silla have been teased apart, and lots of luminous gas Observatory in Chile captures the pair of galaxies NGC has been drawn out from its disc. In NGC 3166's 3169 (left) and NGC 3166 (right). These adjacent case, the dust lanes that also usually outline spiral galaxies display some curious features, demonstrating arms are in disarray. Unlike its bluer counterpart, that each member of the duo is close enough to feel the NGC 3166 is not forming many new stars. distorting gravitational influence of the other. -
TSP 2004 Telescope Observing Program
THE TEXAS STAR PARTY 2004 TELESCOPE OBSERVING CLUB BY JOHN WAGONER TEXAS ASTRONOMICAL SOCIETY OF DALLAS RULES AND REGULATIONS Welcome to the Texas Star Party's Telescope Observing Club. The purpose of this club is not to test your observing skills by throwing the toughest objects at you that are hard to see under any conditions, but to give you an opportunity to observe 25 showcase objects under the ideal conditions of these pristine West Texas skies, thus displaying them to their best advantage. This year we have planned a program called “Starlight, Starbright”. The rules are simple. Just observe the 25 objects listed. That's it. Any size telescope can be used. All observations must be made at the Texas Star Party to qualify. All objects are within range of small (6”) to medium sized (10”) telescopes, and are available for observation between 10:00PM and 3:00AM any time during the TSP. Each person completing this list will receive an official Texas Star Party Telescope Observing Club lapel pin. These pins are not sold at the TSP and can only be acquired by completing the program, so wear them proudly. To receive your pin, turn in your observations to John Wagoner - TSP Observing Chairman any time during the Texas Star Party. I will be at the outside door leading into the TSP Meeting Hall each day between 1:00 PM and 2:30 PM. If you finish the list the last night of TSP, or I am not available to give you your pin, just mail your observations to me at 1409 Sequoia Dr., Plano, Tx. -
April 14 2018 7:00Pm at the April 2018 Herrett Center for Arts & Science College of Southern Idaho
Snake River Skies The Newsletter of the Magic Valley Astronomical Society www.mvastro.org Membership Meeting President’s Message Tim Frazier Saturday, April 14th 2018 April 2018 7:00pm at the Herrett Center for Arts & Science College of Southern Idaho. It really is beginning to feel like spring. The weather is more moderate and there will be, hopefully, clearer skies. (I write this with some trepidation as I don’t want to jinx Public Star Party Follows at the it in a manner similar to buying new equipment will ensure at least two weeks of Centennial Observatory cloudy weather.) Along with the season comes some great spring viewing. Leo is high overhead in the early evening with its compliment of galaxies as is Coma Club Officers Berenices and Virgo with that dense cluster of extragalactic objects. Tim Frazier, President One of my first forays into the Coma-Virgo cluster was in the early 1960’s with my [email protected] new 4 ¼ inch f/10 reflector and my first star chart, the epoch 1960 version of Norton’s Star Atlas. I figured from the maps I couldn’t miss seeing something since Robert Mayer, Vice President there were so many so closely packed. That became the real problem as they all [email protected] appeared as fuzzy spots and the maps were not detailed enough to distinguish one galaxy from another. I still have that atlas as it was a precious Christmas gift from Gary Leavitt, Secretary my grandparents but now I use better maps, larger scopes and GOTO to make sure [email protected] it is M84 or M86. -
Arxiv:2105.08061V1 [Astro-Ph.GA] 17 May 2021
Draft version May 19, 2021 Typeset using LATEX twocolumn style in AASTeX63 A recently quenched isolated dwarf galaxy outside of the Local Group environment Ava Polzin,1 Pieter van Dokkum,1 Shany Danieli,1, 2, 3, 4, ∗ Johnny P. Greco,5, y and Aaron J. Romanowsky6, 7 1Department of Astronomy, Yale University, New Haven, CT 06511, USA 2Department of Physics, Yale University, New Haven, CT 06520, USA 3Yale Center for Astronomy and Astrophysics, Yale University, New Haven, CT 06511, USA 4Institute for Advanced Study, 1 Einstein Drive, Princeton, NJ 08540, USA 5Center for Cosmology and AstroParticle Physics (CCAPP), The Ohio State University, Columbus, OH 43210, USA 6Department of Physics & Astronomy, One Washington Square, San Jos´eState University, San Jose, CA 95192, USA 7University of California Observatories, 1156 High Street, Santa Cruz, CA 95064, USA (Received March 22, 2021; Revised May 14, 2021; Accepted May 17, 2021) Submitted to ApJL ABSTRACT 6 We report the serendipitous identification of a low mass (M∗ ∼ 2×10 M ), isolated, likely quenched dwarf galaxy in the \foreground" of the COSMOS-CANDELS field. From deep Hubble Space Telescope (HST) imaging we infer a surface brightness fluctuation distance for COSMOS-dw1 of DSBF = 22 ± 3 Mpc, which is consistent with its radial velocity of cz = 1222 ± 64 km s−1 via Keck/LRIS. At this distance, the galaxy is 1.4 Mpc in projection from its nearest massive neighbor. We do not detect significant Hα emission (EW(Hα)= −0:4 ± 0:5 A),˚ suggesting that COSMOS-dw1 is likely quenched. Very little is currently known about isolated quenched galaxies in this mass regime. -
Discovery of Millimeter-Wave Excess Emission in Radio-Quiet Active
Mon. Not. R. Astron. Soc. 000, 1–10 (2014) Printed 18 July 2018 (MN LATEX style file v2.2) Discovery of Millimeter-Wave Excess Emission in Radio-Quiet Active Galactic Nuclei Ehud Behar1⋆, Ranieri D. Baldi1, Ari Laor1, Assaf Horesh2, Jamie Stevens3, and Tasso Tzioumis3 1Department of Physics, Technion 32000, Haifa 32000, Israel 2Weizmann Institute of Science, Rehovot, Israel 3CSIRO Astronomy and Space Science, Australia 18 July 2018 ABSTRACT The physical origin of radio emission in Radio Quiet Active Galactic Nuclei (RQ AGN) remains unclear, whether it is a downscaled version of the relativistic jets typical of Radio Loud (RL) AGN, or whether it originates from the accretion disk. The correlation between 5 GHz and X-ray luminosities of RQ AGN, which follows LR = −5 10 LX observed also in stellar coronae, suggests an association of both X-ray and radio sources with the accretion disk corona. Observing RQ AGN at higher (mm-wave) frequencies, where synchrotron self absorption is diminished, and smaller regions can be probed, is key to exploring this association. Eight RQ AGN, selected based on their high X-ray brightness and variability, were observed at 95 GHz with the CARMA and ATCA telescopes. All targets were detected at the 1 − 10 mJy level. Emission excess at 95 GHz of up to ×7 is found with respect to archival low-frequency steep spectra, suggesting a compact, optically-thick core superimposed on the more extended structures that dominate at low frequencies. Though unresolved, the 95 GHz fluxes imply optically thick source sizes of 10−4 − 10−3 pc, or ∼ 10 − 1000 gravitational −4 radii. -
Making a Sky Atlas
Appendix A Making a Sky Atlas Although a number of very advanced sky atlases are now available in print, none is likely to be ideal for any given task. Published atlases will probably have too few or too many guide stars, too few or too many deep-sky objects plotted in them, wrong- size charts, etc. I found that with MegaStar I could design and make, specifically for my survey, a “just right” personalized atlas. My atlas consists of 108 charts, each about twenty square degrees in size, with guide stars down to magnitude 8.9. I used only the northernmost 78 charts, since I observed the sky only down to –35°. On the charts I plotted only the objects I wanted to observe. In addition I made enlargements of small, overcrowded areas (“quad charts”) as well as separate large-scale charts for the Virgo Galaxy Cluster, the latter with guide stars down to magnitude 11.4. I put the charts in plastic sheet protectors in a three-ring binder, taking them out and plac- ing them on my telescope mount’s clipboard as needed. To find an object I would use the 35 mm finder (except in the Virgo Cluster, where I used the 60 mm as the finder) to point the ensemble of telescopes at the indicated spot among the guide stars. If the object was not seen in the 35 mm, as it usually was not, I would then look in the larger telescopes. If the object was not immediately visible even in the primary telescope – a not uncommon occur- rence due to inexact initial pointing – I would then scan around for it. -
Ngc Catalogue Ngc Catalogue
NGC CATALOGUE NGC CATALOGUE 1 NGC CATALOGUE Object # Common Name Type Constellation Magnitude RA Dec NGC 1 - Galaxy Pegasus 12.9 00:07:16 27:42:32 NGC 2 - Galaxy Pegasus 14.2 00:07:17 27:40:43 NGC 3 - Galaxy Pisces 13.3 00:07:17 08:18:05 NGC 4 - Galaxy Pisces 15.8 00:07:24 08:22:26 NGC 5 - Galaxy Andromeda 13.3 00:07:49 35:21:46 NGC 6 NGC 20 Galaxy Andromeda 13.1 00:09:33 33:18:32 NGC 7 - Galaxy Sculptor 13.9 00:08:21 -29:54:59 NGC 8 - Double Star Pegasus - 00:08:45 23:50:19 NGC 9 - Galaxy Pegasus 13.5 00:08:54 23:49:04 NGC 10 - Galaxy Sculptor 12.5 00:08:34 -33:51:28 NGC 11 - Galaxy Andromeda 13.7 00:08:42 37:26:53 NGC 12 - Galaxy Pisces 13.1 00:08:45 04:36:44 NGC 13 - Galaxy Andromeda 13.2 00:08:48 33:25:59 NGC 14 - Galaxy Pegasus 12.1 00:08:46 15:48:57 NGC 15 - Galaxy Pegasus 13.8 00:09:02 21:37:30 NGC 16 - Galaxy Pegasus 12.0 00:09:04 27:43:48 NGC 17 NGC 34 Galaxy Cetus 14.4 00:11:07 -12:06:28 NGC 18 - Double Star Pegasus - 00:09:23 27:43:56 NGC 19 - Galaxy Andromeda 13.3 00:10:41 32:58:58 NGC 20 See NGC 6 Galaxy Andromeda 13.1 00:09:33 33:18:32 NGC 21 NGC 29 Galaxy Andromeda 12.7 00:10:47 33:21:07 NGC 22 - Galaxy Pegasus 13.6 00:09:48 27:49:58 NGC 23 - Galaxy Pegasus 12.0 00:09:53 25:55:26 NGC 24 - Galaxy Sculptor 11.6 00:09:56 -24:57:52 NGC 25 - Galaxy Phoenix 13.0 00:09:59 -57:01:13 NGC 26 - Galaxy Pegasus 12.9 00:10:26 25:49:56 NGC 27 - Galaxy Andromeda 13.5 00:10:33 28:59:49 NGC 28 - Galaxy Phoenix 13.8 00:10:25 -56:59:20 NGC 29 See NGC 21 Galaxy Andromeda 12.7 00:10:47 33:21:07 NGC 30 - Double Star Pegasus - 00:10:51 21:58:39 -
Using the Local Gas-Phase Oxygen Abundances to Explore a Metallicity Dependence in Sne Ia Luminosities
MNRAS 462, 1281–1306 (2016) doi:10.1093/mnras/stw1706 Advance Access publication 2016 July 18 Using the local gas-phase oxygen abundances to explore a metallicity dependence in SNe Ia luminosities M. E. Moreno-Raya,1‹ A.´ R. Lopez-S´ anchez,´ 2,3‹ M. Molla,´ 1 L. Galbany,4,5 J. M. V´ılchez6 and A. Carnero7,8 1Departamento de Investigacion´ Basica,´ CIEMAT, Avda. Complutense 40, E-28040 Madrid, Spain 2Australian Astronomical Observatory, PO Box 915, North Ryde, NSW 1670, Australia 3Department of Physics and Astronomy, Macquarie University, NSW 2109, Australia 4Millennium Institute of Astrophysics, Chile 5Departamento de Astronom´ıa, Universidad de Chile, Casilla 36-D, Santiago, Chile 6Instituto de Astrof´ısica de Andaluc´ıa-CSIC, Apdo. 3004, E-18008 Granada, Spain 7Laboratorio´ Interinstitucional de e-Astronomia – LIneA, Rua Gal. Jose´ Cristino 77, Rio de Janeiro, RJ 20921-400, Brazil 8Observatorio´ Nacional, Rua Gal. Jose´ Cristino 77, Rio de Janeiro, RJ 20921-400, Brazil Downloaded from Accepted 2016 July 13. Received 2016 July 13; in original form 2016 March 9 ABSTRACT http://mnras.oxfordjournals.org/ We present an analysis of the gas-phase oxygen abundances of a sample of 28 galaxies in the local Universe (z<0.02) hosting Type Ia supernovae (SNe Ia). The data were obtained with the 4.2 m William Herschel Telescope. We derive local oxygen abundances for the regions where the SNe Ia exploded by calculating oxygen gradients through each galaxy (when possible) or assuming the oxygen abundance of the closest H II region. The sample selection only considered galaxies for which distances not based on the SN Ia method are available. -
Finding Local Low-Mass Supermassive Bhs
Finding Local Low-Mass Supermassive BHs Smita Mathur Himel Ghosh The Ohio State University Motivation Low-mass (below 106 M) end of local SMBH mass function can constrain theories of SMBH growth. Do scaling relationships (e.g. MBH-Mbulge) break down at low masses? Graham et al. 2007 Beginning to find some 5 NGC 4395 : 310 M (Peterson et al. 2005) 5 POX 52 : 310 M (Barth et al. 2005) 5 7 SDSS: few 10 -10 M (Green & Ho 2004) 3 NGC 3621 : > 410 M (Satyapal et al. 2007) 4 M31 - G1 : ~210 M (Ulvestad et al. 2007) Push to lower masses 4 6 We aim to obtain a sample of 10 - 10 M SMBH Using dynamical signature presently 5 impossible. Sphere of influence of a 10 M SMBH at 15 Mpc is ~ 3 mas Using AGN signature may be only viable way of detecting these SMBH Exploit “downsizing” of AGN activity The lower the luminosity, the lower the redshift at which space density peaks Lowest luminosity AGN should be active at current epoch From lower mass SMBHs Hasinger et al. 2005 Method Focus on late-type spirals and dE Use X-rays. Use highest angular resolution possible Use multi-wavelength data Identify false positives Building the sample 44 galaxies in RC3 that are: face-on spirals (S0-Sdm), or dE within 20 Mpc NOT known to have AGN not starbursts. LINERS are included. 6 of these already in Chandra archive Proof of principle: Chandra archival study 1 Sa, 1 Sb, 1 Sc, 2 Scd, 1 Sd All six have a nuclear x-ray source NGC 3169 (Sa), 4102 (Sb) : AGN NGC 5457 (Scd), 3184 (Scd) : Can make a strong case for being AGN NGC 4713 (Sd), 4647 (Sc) : Inconclusive but can’t rule out AGN All are candidate SMBH NGC 3169 Sa, 20 Mpc, LINER NGC 3169 (Sa) X-ray Hard x-ray source (Terashima & Wilson 2003) 23 -2 Absorbed power law spectrum with ~2, NH~10 cm F(0.3-8 keV) ~ 10-11 cgs L ~ 51041 erg/s Radio 7 mJy mas-scale radio source (VLBA, 5 GHz, Nagar et al.