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The Status and Future of EUV Astronomy
The status and future of EUV astronomy M. A. Barstow∗, S. L. Casewell Department of Physics and Astronomy, University of Leicester, University Road, Leicester, LE1 7RH, UK J. B. Holberg Lunar and Planetary Laboratory, 1541 East University Boulevard, Sonett Space Sciences Building, University of Arizona, Tucson, AZ 85721, USA M.P. Kowalski Naval Research Laboratory,4555 Overlook Ave SW Washington, DC 20375, USA Abstract The Extreme Ultraviolet wavelength range was one of the final windows to be opened up to astronomy. Nevertheless, it provides very important diagnostic tools for a range of astronomical objects, although the opacity of the interstellar medium restricts the majority of observations to sources in our own galaxy. This review gives a historical overview of EUV astronomy, describes current instrumental capabilities and examines the prospects for future facilities on small and medium-class satellite platforms. Keywords: Extreme Ultraviolet, Spectroscopy, White Dwarfs, Stellar Coronae, Interstellar Medium 1. Introduction arXiv:1309.2181v1 [astro-ph.SR] 9 Sep 2013 The Extreme Ultraviolet (EUV) nominally spans the wavelength range from 100 to 912 A,˚ although for practical purposes the edges are often some- what indistinct as instrument band-passes may extend short-ward into the soft X-ray or long-ward into the far ultraviolet (far-UV). The production of EUV photons is primarily associated with the existence of hot, 105-107 K gas ∗Corresponding Author: [email protected] Preprint submitted to Advances in Space Research October 29, 2018 in the Universe. Sources of EUV radiation can be divided into two main cat- egories, those where the emission arises from recombination of ions and elec- trons in a hot, optically thin plasma, giving rise to emission line spectra, and objects which are seen by thermal emission from an optically thick medium, resulting in a strong continuum spectrum which may contain features arising from transitions between different energy levels or ionisation stages of sev- eral elements. -
The Spitzer Space Telescope First-Look Survey. II. KPNO
The Spitzer Space Telescope First-Look Survey: KPNO MOSAIC-1 R-band Images and Source Catalogs Dario Fadda1, Buell T. Jannuzi2, Alyson Ford2, Lisa J. Storrie-Lombardi1 [January, 2004 { Submitted to AJ] ABSTRACT We present R-band images covering more than 11 square degrees of sky that were obtained in preparation for the Spitzer Space Telescope First Look Survey (FLS). The FLS was designed to characterize the mid-infrared sky at depths 2 orders of magnitude deeper than previous surveys. The extragalactic component is the ¯rst cosmological survey done with Spitzer. Source catalogs extracted from the R-band images are also presented. The R-band images were obtained using the MOSAIC-1 camera on the Mayall 4m telescope of the Kitt Peak National Observatory. Two relatively large regions of the sky were observed to modest depth: the main FLS extra galac- tic ¯eld (17h18m00s +59o3000000:0 J2000; l= 88:3, b= +34:9) and ELAIS-N1 ¯eld (16h10m01s +54o3003600:0 J2000; l= 84:2, b= +44:9). While both of these ¯elds were in early plans for the FLS, only a single deep pointing test observation were made at the ELAIS-N1 location. The larger Legacy program SWIRE (Lonsdale et al., 2003) will include this region among its sur- veyed areas. The data products of our KPNO imaging (images and object catalogs) are made available to the community through the World Wide Web (via the Spitzer Science Center and NOAO Science Archives). The overall quality of the images is high. The measured positions of sources detected in the images have RMS uncertainties in their absolute positions of order 0.35 arc-seconds with possible systematic o®sets of order 0.1 arc-seconds, depending on the reference frame of comparison. -
Publications of the Astronomical Society of the Pacific 97:165-174, Febmary 1985
Publications of the Astronomical Society of the Pacific 97:165-174, Febmary 1985 PHOTOMETRY OF STARS IN THE uvgr SYSTEM* STEPHEN M. KENT Harvard-Smithsonian Center for Astrophysics, 60 Garden Street Cambridge, Massachusetts 02138 Received 1984 July 23, revised 1984 November 17 Photoelectric photometry is presented for over 400 stars using the uvgr system of Thuan and Gunn. Stars were selected to cover a wide range of spectral type, luminosity class, and metallicity. A mean main sequence is derived along with red- dening curves and approximate transformations to the UBVR system. The calibration of the standard-star sequence is sig- nificantly improved. Key words: photometry—stellar classification I. Introduction II. Observations The uvgr system (Thuan and Gunn 1976, hereafter The observations were made during several runs from TG) was developed as a four-color intermediate-to-wide- 1976 through 1978 on the Palomar 60-inch (1.5-m) tele- band photometric system which was designed to avoid a scope. The instrumentation and equipment were identi- number of pitfalls of the standard UBV system. The four cal with that used by TG. A two-channel pulse-counting bands are nonoverlapping and exclude the strongest S20 photometer allowed for the simultaneous measure- night-sky lines. The u and ν filters lie in a region of ment of object and sky. Each star was observed in both strong line blanketing in late-type stars and measure the apertures except for the globular-cluster stars, where it Balmer jump in early-type stars; the g and r filters lie in was necessary to go off the cluster to measure sky. -
Calibration Against Spectral Types and VK Color Subm
Draft version July 19, 2021 Typeset using LATEX default style in AASTeX63 Direct Measurements of Giant Star Effective Temperatures and Linear Radii: Calibration Against Spectral Types and V-K Color Gerard T. van Belle,1 Kaspar von Braun,1 David R. Ciardi,2 Genady Pilyavsky,3 Ryan S. Buckingham,1 Andrew F. Boden,4 Catherine A. Clark,1, 5 Zachary Hartman,1, 6 Gerald van Belle,7 William Bucknew,1 and Gary Cole8, ∗ 1Lowell Observatory 1400 West Mars Hill Road Flagstaff, AZ 86001, USA 2California Institute of Technology, NASA Exoplanet Science Institute Mail Code 100-22 1200 East California Blvd. Pasadena, CA 91125, USA 3Systems & Technology Research 600 West Cummings Park Woburn, MA 01801, USA 4California Institute of Technology Mail Code 11-17 1200 East California Blvd. Pasadena, CA 91125, USA 5Northern Arizona University Department of Astronomy and Planetary Science NAU Box 6010 Flagstaff, Arizona 86011, USA 6Georgia State University Department of Physics and Astronomy P.O. Box 5060 Atlanta, GA 30302, USA 7University of Washington Department of Biostatistics Box 357232 Seattle, WA 98195-7232, USA 8Starphysics Observatory 14280 W. Windriver Lane Reno, NV 89511, USA (Received April 18, 2021; Revised June 23, 2021; Accepted July 15, 2021) Submitted to ApJ ABSTRACT We calculate directly determined values for effective temperature (TEFF) and radius (R) for 191 giant stars based upon high resolution angular size measurements from optical interferometry at the Palomar Testbed Interferometer. Narrow- to wide-band photometry data for the giants are used to establish bolometric fluxes and luminosities through spectral energy distribution fitting, which allow for homogeneously establishing an assessment of spectral type and dereddened V0 − K0 color; these two parameters are used as calibration indices for establishing trends in TEFF and R. -
UV and Infrared Astronomy
Why Put a Telescope In Space? • Access to light that does not penetrate the atmosphere • No seeing. A telescope can reach the diffraction limit: 1.22 l/D radians Astronomy in Space. I. UV Astronomy Ultraviolet Astronomy 912-3650 Å (Lyman Limit to Balmer jump) • Continuua of hot stars (spectral types O,B,A) • H I Lyman lines (1-n transitions) • Resonance lines of Li-like ions C IV, N V, O VI • H2 Lyman and Werner bands Normal incidence optics • Special UV-reflective coatings The Far Ultraviolet 912 to 1150 Å • Defined by Lyman limit, MgF cutoff at 1150 Å • LiF + Al reflects longward of 1050 Å • SiC reflects at shorter wavelengths The Astronomy Quarterly, Vol. 7, pp. 131-142, 1990 0364-9229f90 $3.00+.00 Printed in the USA. All rights reserved. Copyright (c) 1990 Pergamon Press plc ASTRONOMICAL ADVANTAGES History OFAN • 9/1/1946: Lyman Spitzer EXTRA-TERRESTRIAL OBSERVATORY proposed a Space Telescope in LYMAN SPITZER, Jr. ’ a Report to project Rand This study points out, in a very preliminary way, the results that might be expected from astronomical measurements made with a satellite • 1966: Spitzer (Princeton) vehicle. The discussion is divided into three parts, corresponding to three different assumptions concerning the amount of instrumentation provided. chairs NASA Ad Hoc In the first section it is assumed that no telescope is provided; in the second a 10-&h reflector is assumed; in the third section some of the results Committee on the "Scientific obtainable with a large reflecting telescope, many feet in diameter, and revolving about the earth above the terrestrial atmosphere, are briefly Uses of the Large Space sketched. -
GRAVITY ASTROPHYSICS a Plan for the 1990S
ULTRAVIOLET, VISIBLE, and GRAVITY ASTROPHYSICS A Plan for the 1990s (NASA-NP-I52) ULTRAVIOLET, N94-24973 VISI3LE, ANO GRAVITY ASTROPHYSICS: A PLAN FOR THE 1990'S (NASA) 76 p Unclas HI190 0207794 ORIGINAL PAGE COLOR PHOTOGRAPH National Aeronautics and Space Administration I-oreword N ASA'sprioritiesOfficefrom oftheSpaceU.S. NationalScience Academyand Applicationsof Sciences.(OSSA)Guidancereceivesto theadviceOSSAon Astrophysicsscientific strategyDivision,and in particular, is provided by dedicated Academy committees, ad hoc study groups and, at 10-year intervals, by broadly mandated astronomy and astrophysics survey committees charged with making recommen- dations for the coming decade. Many of the Academy's recommendations have important implications for the conduct of ultraviolet and visible-light astronomy from space. Moreover, these areas are now poised for an era of rapid growth. Through technological progress, ultraviolet astronomy has already risen from a novel observational technique four decades ago to the mainstream of astronomical research today. Recent developments in space technology and instrumen- tation have the potential to generate comparably dramatic strides in observational astronomy within the next 10 years. In 1989, the Ultraviolet and Visible Astrophysics Branch of the OSSA Astrophysics Division recognized the need for a new, long-range plan that would implement the Academy's recommendations in a way that yielded the most advantageous use of new technology. NASA's Ultraviolet, Visible, and Gravity Astrophysics Management Operations Working Group was asked to develop such a plan for the 1990s. Since the Branch holds programmatic responsibility for space research in gravitational physics and relativity, as well as for ultraviolet and visible-light astrophysics, missions in those areas were also included. -
Observing Photons in Space
—1— Observing photons in space For the truth of the conclusions of physical science, observation is the supreme court of appeals Sir Arthur Eddington Martin C.E. HuberI, Anuschka PauluhnI and J. Gethyn TimothyII Abstract This first chapter of the book ‘Observing Photons in Space’ serves to illustrate the rewards of observing photons in space, to state our aims, and to introduce the structure and the conventions used. The title of the book reflects the history of space astronomy: it started at the high-energy end of the electromagnetic spectrum, where the photon aspect of the radiation dominates. Nevertheless, both the wave and the photon aspects of this radiation will be considered extensively. In this first chapter we describe the arduous efforts that were needed before observations from pointed, stable platforms, lifted by rocket above the Earth’s atmosphere, became the matter of course they seem to be today. This exemplifies the direct link between technical effort — including proper design, construction, testing and calibration — and some of the early fundamental insights gained from space observations. We further report in some detail the pioneering work of the early space astronomers, who started with the study of γ- and X-rays as well as ultraviolet photons. We also show how efforts to observe from space platforms in the visible, infrared, sub-millimetre and microwave domains developed and led to today’s emphasis on observations at long wavelengths. The aims of this book This book conveys methods and techniques for observing photons1 in space. ‘Observing’ photons implies not only detecting them, but also determining their direction at arrival, their energy, their rate of arrival, and their polarisation. -
A Spitzer Irac Search for Substellar Companions of the Debris Disk Star Eridani M
The Astrophysical Journal, 647:1437Y1451, 2006 August 20 A # 2006. The American Astronomical Society. All rights reserved. Printed in U.S.A. A SPITZER IRAC SEARCH FOR SUBSTELLAR COMPANIONS OF THE DEBRIS DISK STAR ERIDANI M. Marengo, S. T. Megeath,1 and G. G. Fazio Harvard-Smithsonian Center for Astrophysics, 60 Garden Street, Cambridge, MA 02138; [email protected] K. R. Stapelfeldt and M. W. Werner Jet Propulsion Laboratory, California Institute of Technology, 4800 Oak Grove Drive, Pasadena, CA 91109 and D. E. Backman NASAYAmes Research Center, Moffett Field, CA 94035 Received 2006 April 10; accepted 2006 April 27 ABSTRACT We have used the Infrared Array Camera (IRAC) on board the Spitzer Space Telescope to search for low-mass companions of the nearby debris disk star Eri. The star was observed in two epochs 39 days apart, with different focal plane rotation to allow the subtraction of the instrumental point-spread function, achieving a maximum 1 1 sensitivity of 0.01 MJy srÀ at 3.6 and 4.5 "m, and 0.05 MJy srÀ at 5.8 and 8.0 "m. This sensitivity is not sufficient to directly detect scattered or thermal radiation from the Eri debris disk. It is, however, sufficient to allow the detection of Jovian planets with mass as low as 1MJ in the IRAC 4.5 "m band. In this band, we detected over 460 sources within the 5A70 field of view of our images. To test if any of these sources could be a low-mass companion to Eri, we have compared their colors and magnitudes with models and photometry of low-mass objects. -
The UKIRT Infrared Deep Sky Survey ZY JHK Photometric System: Passbands and Synthetic Colours
Mon. Not. R. Astron. Soc. 367, 454–468 (2006) doi:10.1111/j.1365-2966.2005.09969.x The UKIRT Infrared Deep Sky Survey ZY JHK photometric system: passbands and synthetic colours P. C. Hewett,1⋆ S. J. Warren,2 S. K. Leggett3 and S. T. Hodgkin1 1Institute of Astronomy, Madingley Road, Cambridge CB3 0HA 2Blackett Laboratory, Imperial College of Science, Technology and Medicine, Prince Consort Road, London SW7 2AZ 3United Kingdom Infrared Telescope, Joint Astronomy Centre, 660 North A‘ohoku Place, Hilo, HI 96720, USA Accepted 2005 December 7. Received 2005 November 28; in original form 2005 September 16 ABSTRACT The United Kingdom Infrared Telescope (UKIRT) Infrared Deep Sky Survey is a set of five surveys of complementary combinations of area, depth and Galactic latitude, which began in 2005 May. The surveys use the UKIRT Wide Field Camera (WFCAM), which has a solid angle of 0.21 deg2. Here, we introduce and characterize the ZY JHK photometric system of the camera, which covers the wavelength range 0.83–2.37 µm. We synthesize response functions for the five passbands, and compute colours in the WFCAM, Sloan Digital Sky Survey (SDSS) and two-Micron All Sky Survey (2MASS) bands, for brown dwarfs, stars, galaxies and quasars of different types. We provide a recipe for others to compute colours from their own spectra. Calculations are presented in the Vega system, and the computed offsets to the AB system are provided, as well as colour equations between WFCAM filters and the SDSS and 2MASS passbands. We highlight the opportunities presented by the new Y filter at 0.97–1.07 µm for surveys for hypothetical Y dwarfs (brown dwarfs cooler than T), and for quasars of very high redshift, z > 6.4. -
Appendix: Spectroscopy of Variable Stars
Appendix: Spectroscopy of Variable Stars As amateur astronomers gain ever-increasing access to professional tools, the science of spectroscopy of variable stars is now within reach of the experienced variable star observer. In this section we shall examine the basic tools used to perform spectroscopy and how to use the data collected in ways that augment our understanding of variable stars. Naturally, this section cannot cover every aspect of this vast subject, and we will concentrate just on the basics of this field so that the observer can come to grips with it. It will be noticed by experienced observers that variable stars often alter their spectral characteristics as they vary in light output. Cepheid variable stars can change from G types to F types during their periods of oscillation, and young variables can change from A to B types or vice versa. Spec troscopy enables observers to monitor these changes if their instrumentation is sensitive enough. However, this is not an easy field of study. It requires patience and dedication and access to resources that most amateurs do not possess. Nevertheless, it is an emerging field, and should the reader wish to get involved with this type of observation know that there are some excellent guides to variable star spectroscopy via the BAA and the AAVSO. Some of the workshops run by Robin Leadbeater of the BAA Variable Star section and others such as Christian Buil are a very good introduction to the field. © Springer Nature Switzerland AG 2018 M. Griffiths, Observer’s Guide to Variable Stars, The Patrick Moore 291 Practical Astronomy Series, https://doi.org/10.1007/978-3-030-00904-5 292 Appendix: Spectroscopy of Variable Stars Spectra, Spectroscopes and Image Acquisition What are spectra, and how are they observed? The spectra we see from stars is the result of the complete output in visible light of the star (in simple terms). -
An Introduction to Photometry and Photometric Measurements Henry
An introduction to photometry and photometric measurements Henry Joy McCracken Institut d’Astrophysique de Paris What is photometry? • Photometry is concerned with obtaining quantitative physical measurements of astrophysical objects using electromagnetic radiation. • The challenge is to relate instrumental measurements (like electrons counted in an electronic detector) to physically meaningful quantities like flux and flux density • The ability to make quantitative measurements transformed astronomy from a purely descriptive science to one with great explanative power. To print higher-resolution math symbols, click the Hi-Res Fonts for Printing button on the jsMath control panel. Brightness and Flux Density Astronomers learn about an astronomical source by measuring the strength of its radiation as a function of direction on the sky (by mapping or imaging) and frequency (spectroscopy), plus other quantities (time, polarization) that we ignore for now. We need precise and quantitative definitions to describe the strength of radiation and how it varies with distance between the source and the observer. The concepts of brightness and flux density are deceptively simple, but they regularly trip up experienced astronomers. It is very important to understand them clearly because they are so fundamental. We start with the simplest possible case of radiation traveling from a source through empty space (so there is no absorption, scattering, or emission along the way) to an observer. In the ray-optics approximation, radiated energy flows in straight lines. This approximation is valid only for systems much larger than the wavelength of the radiation, a criterion easily met by astronomical sources. You may find it helpful to visualize electromagnetic radiation as a stream of light particles (photons), essentially bullets that travel in straight lines at the speed of light. -
Photometry Rule of Thumb
AST 443/ PHY 517 Photometry Rule of Thumb For a uniform flux distribution, V=0 corresponds to • 3.6 x 10-9 erg cm-2 s-1 A-1 (at 5500 A = 550 nm) • 996 photons cm-2 s-1 A-1 remember: E = hn = hc/l Basic Photometry The science of measuring the brightness of an astronomical object. In principle, it is straightforward; in practice (as in much of astronomy), there are many subtleties that can cause you great pains. For this course, you do not need to deal with most of these effects, but you should know about them (especially extinction). Among the details you should be acquainted with are: • Bandpasses • Magnitudes • Absolute Magnitudes • Bolometric Fluxes and Magnitudes • Colors • Atmospheric Extinction • Atmospheric Refraction • Sky Brightness • Absolute Photometry Your detector measures the flux S in a bandpass dw. 2 2 The units of the detected flux S are erg/cm /s/A (fλ) or erg/cm /s/Hz (fν). Bandpasses Set by: • detector response, • the filter response • telescope reflectivity • atmospheric transmission Basic types of filters: • long pass: transmit light longward of some fiducial wavelength. The name of the filter often gives the 50% transmission wavelength in nm. E.g, the GG495 filter transmits 50% of the incident light at 495 nm, and has higher transmission at longer wavelengths. • short pass: transmit light shortward of some fiducial wavelength. Examples are CuSO4 and BG38. • isolating: used to select particular bandpasses. May be made of a combination of long- and short-pass filters. Narrow band filters are generally interference filters. Broadband Filters • The Johnson U,B,V bands are standard.