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The Intergalactic Medium: The Cosmic Web of Matter Connecting Galaxies Kenneth Sembach Space Telescope Science Institute Slide 2 27-Mar-2007K. Sembach - NSN Telecon 2 Outline I.Brief Introduction II.What is the Intergalactic Medium and Why is it Important? III.Spectroscopy of the Intergalactic Medium IV.Hubble - Current Status and Future Prospects V.Questions from you (and hopefully some satisfying answers!) Slide 3 27-Mar-2007K. Sembach - NSN Telecon 3 Where is the Material that Forms Stars and Galaxies? Interstellar medium Gas and dust between stars inside galaxies Circumgalactic medium Gas and dust outside but near galaxies Intergalactic medium Gas and dust between galaxies ? Slide 4 27-Mar-2007K. Sembach - NSN Telecon 4 The Mass/Energy Budget of the Universe Even though ordinary matter accounts for only a small fraction of the mass of the Universe, it is the only form of matter that is directly observable. About 50% of ordinary matter has yet to be accounted for in the present-day Universe. It is hidden (or missing) in the form of tenuous intergalactic material. The rest of this presentation concentrates on ordinary matter, where it is located, and how it is studied. Slide 5 27-Mar-2007K. Sembach - NSN Telecon 5 Where is the Ordinary Matter? Most of the ordinary matter in the Universe is in the intergalactic medium. Galaxies contain less than 10% of the ordinary matter. Gas near galaxies (in clusters and groups) accounts for about 30%. Another 10-20% has been identified in the intergalactic medium. The remaining 50% is believed to be in the form of hot, ionized intergalactic gas. The intergalactic medium provides the raw materials needed to build galaxies, stars, planets, and life. The intergalactic gas is hard to detect because it is so tenuous. It has such a low density that it is not yet possible to image it. Slide 6 27-Mar-2007K. Sembach - NSN Telecon 6 What is the Density of the Intergalactic Medium? Air has a density of ~ 3x10 19 molecules per cubic centimeter. This is about 30 billion billion molecules. 1 cubic centimeter is about the size of a sugar cube. The Suns photosphere has a density of about 10 9 atoms per cc. This is a much better vacuum than can be produced in any laboratory. The interstellar medium has a density of about 1 atom per cc. Take the air particles in a box the size of a sugar cube and stretch the cube in one dimension 33 light years to get the same density! The intergalactic medium has a density of about 1/100,000 atom per cc. Take the box and stretch it 3 million light years, or about 4 times further than the Andromeda galaxy! 3 million light years Milky WayAndromedaKeep going! 1 cc Slide 7 27-Mar-2007K. Sembach - NSN Telecon 7 Evolution of the Cosmic Web of Matter The intergalactic gas evolves with time under the influence of gravity. The intergalactic gas evolves with time under the influence of gravity. Large-scale gaseous structures collapse into sheets and filaments. Large-scale gaseous structures collapse into sheets and filaments. Shocks in the collapsing structures heat the intergalactic gas to high temperatures. Shocks in the collapsing structures heat the intergalactic gas to high temperatures. Simulation by Volker Springel (MPIA) If this does not play automatically from your computer, go to the still pictures on the next slide (slide 8). Slide 8 27-Mar-2007K. Sembach - NSN Telecon 8 Evolution of the Cosmic Web of Matter Slide 9 27-Mar-2007K. Sembach - NSN Telecon 9 A Representation of What the Cosmic Web Might Look Like Now 10 4 K 10 5 - 10 6 K 10 8 K Redshift = 0 (1024 h -1 Mpc) 3 Temperature Figure from Kang et al. 2004 Clusters of galaxies form at the intersections of the filaments where the gas is hottest (bluish colors in figure). Much of the gas is at temperatures of 100,000 to 1,000,000 degrees (greenish colors in figure). Slide 10 27-Mar-2007K. Sembach - NSN Telecon 10 How Does Matter Get Out of Galaxies? Red: Galaxies Green: Metals Blue: 10 5 -10 7 K gas Cen & Ostriker (1999) Galaxies power strong winds that blow dust, gas, and heavy elements into the intergalactic medium. Credit: X-ray: NASA / CXC / JHU / D.Strickland; Optical: NASA / ESA / STScI / AURA / The Hubble Heritage Team; IR: NASA / JPL-Caltech / Univ. of AZ /C. Engelbracht M82 Slide 11 27-Mar-2007K. Sembach - NSN Telecon 11 Sometimes to study the Universe on large scales, it is necessary to consider what is happening on very small scales. So, lets take a look at atoms for a moment. Slide 12 27-Mar-2007K. Sembach - NSN Telecon 12 Bohr Model of the Hydrogen Atom A negatively charged electron orbits the positively charged proton in one of several possible energy levels n. When the electron moves to a lower energy level (preferred), the atom emits a photon of light with energy E and wavelength. If the atom absorbs a photon of energy E, the electron can move to a higher energy level if the energy separation of the levels equals E. Each element, whether simple like Hydrogen or complex like Iron, has a unique set of energy levels. Slide 13 27-Mar-2007K. Sembach - NSN Telecon 13 Spectroscopy Spectroscopy is the technique that allows us to disperse light into its constituent colors and determine the energy levels of atoms and molecules. Figure reproduced from Universe by Freedman and Kaufmann Types of Spectra Slide 14 27-Mar-2007K. Sembach - NSN Telecon 14 Cosmic Barcodes Each element has its own unique set of spectral lines. The sequence of lines is determined by the energy levels populated within the atom or molecule. These series of lines can be used to identify the chemical composition of the gas causing the absorption. Pop quiz! What elements are present in this spectrum? Answer: Slide 15 27-Mar-2007K. Sembach - NSN Telecon 15 Answer Slide 16 27-Mar-2007K. Sembach - NSN Telecon 16 Decoding the Information in a Spectrum Astronomers convert two-dimensional spectra (below) into one- dimensional plots of intensity versus wavelength. This allows precise line wavelengths, shapes, and strengths to be measured easily. The line parameters contain information about the physical properties of the absorbing material. Intensity Wavelength Collapse and sum spectrum in this direction Plot intensity versus wavelength Slide 17 27-Mar-2007K. Sembach - NSN Telecon 17 A Portion of an Astronomical Spectrum Slide 18 27-Mar-2007K. Sembach - NSN Telecon 18 Spectroscopy with Hubble Hubble has obtained spectra of many astronomical objects Complementary to imaging information A spectrum = information What is it? Chemical composition What state? Molecular/atomic/ionic Hot hot?Temperature How much? Quantity How fast? Velocity Where is it? Location (redshift) The ultraviolet spectral region is loaded with information about atoms and molecules in their ground (lowest) and excited (higher) states. NGC2440 - HST/WFPC2 Slide 19 27-Mar-2007K. Sembach - NSN Telecon 19 Extracting Information How do we extract information about the gas from the spectral lines? QuestionInformationObservable quantity What is it? Chemical compositionPattern of lines What state? Molecular/atomic/ionicPattern of lines How hot?TemperatureWidths of lines How much? Quantity Strengths of lines How fast? Velocity Wavelengths of lines Where is it? Location (redshift)Wavelengths of lines Slide 20 27-Mar-2007K. Sembach - NSN Telecon 20 Redshift of Spectral Lines Wavelength obs abs The light at the wavelength of this line is the color it is when it is absorbed (in this case, yellow). This same line is shifted to redder wavelengths when observed by someone moving away from the absorber. The faster the recession, the greater the redshift. Light Slide 21 27-Mar-2007K. Sembach - NSN Telecon 21 Redshift and Cosmic Expansion Hubbles Law v r = H 0 d v r = velocity of recession d = distance H 0 = Hubbles constant Distance Recession velocity of galaxies vrvr d H0H0 H 0 20 kilometers per second per million light years The Universe is expanding in all directions. Distant objects move away from us faster than nearby objects. As a result, distant objects appear redder than they would if they were nearby - they are redshifted. Slide 22 27-Mar-2007K. Sembach - NSN Telecon 22 Measuring the Redshifts of Intergalactic Gas Clouds with Hubble STIS = Space Telescope Imaging Spectrograph Slide 23 27-Mar-2007K. Sembach - NSN Telecon 23 A Hubble Spectrum is a Beautiful Thing! Hubble spectrum of quasar H1821+643 Slide 24 27-Mar-2007K. Sembach - NSN Telecon 24 Current Hubble Status Wide Field Planetary Camera 2 (WFPC2) Installed in December 1993 Operating well Near Infrared Camera and Multi-Object Spectrometer (NICMOS) Installed in February 1997 Operating well Space Telescope Imaging Spectrograph (STIS) Installed in February 1997 Currently disabled Advanced Camera for Surveys (ACS) Installed in March 2002 Serious electrical failure on January 27, 2007 Optical channels are disabled Only ultraviolet (solar-blind) channel is operational Slide 25 27-Mar-2007K. Sembach - NSN Telecon 25 Hubble Servicing Mission 4 Two new science instruments Wide Field Camera 3 (WFC3) and the Cosmic Origins Spectrograph (COS) Replacement of one of the three Fine Guidance Sensors Repair of the Space Telescope Imaging Spectrograph Replacement of batteries (needed for power during orbital night) Replacement of gyros (used to determine HST pointing) Replacement of thermal blankets (used to maintain temperature) Repair of the Advanced Camera for Surveys? Scheduled for Fall 2008 on Shuttle Atlantis Slide 26 27-Mar-2007K. Sembach - NSN Telecon 26 New Hubble Science Instruments Wide Field Camera 3 (Panchromatic Imaging) Two channels cover near-ultraviolet to near-infrared wavelengths Wide field imaging from 200 to 1000 nm Greater sensitivity, wider field of view Replaces WFPC2 Cosmic Origins Spectrograph (Ultraviolet Spectroscopy) Far-ultraviolet channel (110 nm - 180 nm) Improves HST sensitivity by at least 10x Near-ultraviolet channel (180 nm - 320 nm) Replaces COSTAR Slide 27 27-Mar-2007K. Sembach - NSN Telecon 27 WFC3 Panchromatic Imaging of Star-Forming Regions Ultraviolet observations reveal young stars that are flooding their surroundings with intense ultraviolet light. Infrared observations penetrate deeper into regions heavily obscured by dust. Slide 28 27-Mar-2007K. Sembach - NSN Telecon 28 WFC3 Will Peer into the Hearts of Galaxies High angular resolution, great sensitivity and multi-wavelength coverage will give WFC3 unprecedented views into the cores of galaxies. WFC3 will observe ultraluminous infrared galaxies created by firestorms of star formation after galaxy-galaxy collisions. Slide 29 COS is Designed to Study the Cosmic Web COS will greatly increase the number of quasar sight lines explored by Hubble. Cosmic web absorption features In just a few days, COS can sample as much of the Universe as all existing STIS observations of quasars have probed! Slide 30 27-Mar-2007K. Sembach - NSN Telecon 30 COS Science Themes What is the large-scale structure of matter in the Universe? How did galaxies form out of the intergalactic medium? What types of galactic halos and outflowing winds do star-forming galaxies produce? How were the chemical elements for life created in massive stars and supernovae? How do stars and planetary systems form from dust grains in molecular clouds? What is the composition of planetary atmospheres and comets in our Solar System (and beyond)? Slide 31 27-Mar-2007K. Sembach - NSN Telecon 31 COS and Planets COS can record the ultraviolet spectra of transiting hot Jupiters fainter than those observable with STIS (many more faint stars) Ground-based surveys will find ~10 transiting planets around bright stars (10 m ) over next 3 years HST should be able to detect atmospheric absorption from atoms/molecules in the extended atmospheres of these planets Scintillation noise in the Earths atmosphere makes this problem impossible for terrestrial telescopes