Astrophysics with GLAST: dark matter, black holes and other astronomical exotica

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Astrophysics with GLAST: dark matter, black holes and other astronomical exotica Greg Madejski Stanford Linear Accelerator Center and Kavli Institute for Particle Astrophysics and Cosmology (KIPAC) Outline: Multi-band perspective on astronomy - and gamma-rays Stanford s involvement in the future observatories: Gamma-ray Large Space Telescope (GLAST ) What will GLAST study? - supernova remnants, clusters of galaxies, active galaxies

X-rays and gamma-rays in perspective Optical band is only a small part of the electromagnetic spectrum Radio band, opened in the 1930s, revealed the world of exotic processes Studying astronomical sources in other spectral ranges besides the optical band can reveal very rich physical phenomena

X-ray and g-ray observations require detectors above the atmosphere Opacity of the atmosphere as a function of photon energy First observations were conducted using rocket-based instruments

Chandra Observatory: sensitive to X-rays in the 0.3 10 kev band

Compton Gamma-ray Observatory Featured instruments sensitive from ~ 40 kev (OSSE) up to nearly 100 GeV (EGRET)

Future of g-ray observations is here: GLAST Features of the MeV/GeV g-ray sky: * Diffuse extra-galactic background (flux ~ 1.5x10-5 cm -2 s -1 sr -1 ) * Galactic diffuse and galactic sources (pulsars etc.) EGRET all-sky survey (galactic coordinates) E>100 MeV * High latitude (extragalactic) point sources blazars and new sources? - typical flux from EGRET sources 10-7 - 10-6 cm -2 s -1 * Need an instrument with a good sensitivity and a wide field of view * Gamma-ray Large Area Space Telescope (GLAST) with a detector built at Stanford / SLAC - has just been launched!

Schematic principle of operation of the GLAST Large Area Telescope γ-rays interact with the hi-z material in the foils, pairproduce, and are tracked with silicon strip detectors * The instrument looks simultaneously into ~ 2 steradians of the sky * Energy range is ~ 30 MeV 300 GeV, with the peak effective area of ~ 12,000 cm 2 * This allows an overlap with TeV observatories

GLAST LAT instrument overview Si Tracker pitch = 228 µm 8.8 10 5 channels 12 layers 3% X 0 + 4 layers 18% X 0 + 2 layers g ACD Segmented scintillator tiles 0.9997 efficiency minimize self-veto CsI Calorimeter Hodoscopic array 8.4 X 0 8 12 bars 2.0 2.7 33.6 cm cosmic-ray rejection shower leakage correction e + e Data acquisition 3000 kg, 650 W (allocation) 1.8 m 1.8 m 1.0 m 20 MeV >300 GeV Grid (& Thermal Radiators) LAT managed at SLAC Flight Hardware & Spares 16 Tracker Flight Modules + 2 spares 16 Calorimeter Modules + 2 spares 1 Flight Anticoincidence Detector Data Acquisition Electronics + Flight Software

GLAST LAT has much higher sensitivity to weak sources, with much better angular resolution GLAST EGRET

LAT Integration at SLAC Calorimeter module Tracker module LAT Integration & Test Team Anti Coincidence Detector being integrated with 16 towers

Supernovae and their remnants Early Universe contained only the lightest elements: hydrogen, helium Heavy elements were all cooked in stars and ejected into the interstellar space via supernova explosions We are made of those elements! The process of pollution of the interstellar space with the heavy elements is best studied with X-rays: This is because the expected velocity of the ejecta, ~ 10,000 km/s, corresponds to temperatures in the kev (10 7 K) range This temperature range is rich in atomic transitions studied via X-ray spectroscopy Kepler s supernova remnant

Pulsars: rotating neutron stars Neutron stars left behind the explosion are fascinating objects when they rotate and are not perfectly symmetric, they will send out radiation in precisely timed pulses, seen also in γ-rays

Supernova remnants as sources of cosmic rays * Cosmic rays are very energetic particles that come from interplanetary or interstellar space but what is their origin? * Since they are protons and electrons => charged particles - we cannot trace them back to their origin as the trajectories are affected by Galactic magnetic field * Have to use photons to infer their origin Tycho s supernova remnant (Chandra Observatory X-ray image)

Spectrum and origin of cosmic rays Is strong TeV γ-ray emission from supernova remnants also implicating them as sources of cosmic rays? Spectrum of cosmic rays (from Gaisser 2001) (HESS data, Aharonian et al. 2004)

Clusters of galaxies Normal galaxy Messier 100 Cluster of galaxies in constellation Coma Galaxies don t live alone but often are associated with each other in clusters bound by gravity

Clusters of galaxies and their X-ray emission Cluster of galaxies Abell 2029 Clusters of galaxies are largest gravitationally bound and relaxed structures in the Universe they condensed from original perturbations in the Universe Their mass and number density as a function of time are probes of cosmological parameters Clusters of galaxies are bright, extended X-ray emitters since we understand physics, we can weigh them: - and we can t account for all the gravitational pull - member galaxies + hot gas are not enough! Conclusion of those studies is that dark matter is required

Clusters are gravitational lenses Gravitational lensing of background galaxies provides an independent estimate of the mass of the cluster Masses inferred from lensing data generally (but not always!) agree with the X-ray data Hubble space telescope image of cluster Abell 2218

Can t explain all this just via tweaks to gravitational laws

Cosmology with clusters Map of the Universe collected with the WMAP satellite: Ripples have amplitude of less than 0.1% * very smooth The earliest Universe we can observe was very smooth, but today it is very clumpy -> gravity at work What was the history of the formation of structure in the Universe? How did gravity form the current Universe?

Comparison of independent cosmological constraints (? CDM) Color coding: Cluster f gas analysis including standard? b h 2, h and b priors (Allen et al. 2004) CMB data (WMAP +CBI + ACBAR) weak prior 0.3<h<1.0 Supernovae data from Tonry et al. (2003). Figure and analysis from Allen et al. 2004

Cosmology with gamma-rays: Observable signatures of dark matter Extensions to Standard Model of particle physics provide postulated dark matter candidates X X q q or γγ or Zγ If true, there may be observable dark matter particle annihilations producing gamma-ray emission This is just an example of what may await us!

Active galaxies and strong gravity Many galaxies contain exceptionally bright nuclei that are also point-like sources of radio and X-ray emission In some cases, the nuclei are so bright that the galaxy can be barely detected Normal galaxy M74 We now believe that the origin of this emission is the release of gravitational energy by matter flowing onto a supermassive black hole, with a mass of 10 6 or more times the Sun

Weighing the central black hole Radio galaxy M87 (Virgo-A) studied with the Hubble Space Telescope Seyfert galaxy NGC 4258 studied using H 2 O megamaser data Black holes are a common ingredient of nearly all (!) galaxies When fed by galaxian matter, they shine or produce jets or both The BH mass is very important to understand physical processes involved

Unified picture of active galaxies Best scenario has all AGN powered by the same basic engine : a black hole accreting via disk-like structure Some active galaxies possess strong jets Such a jet is most likely relativistically boosted and thus much brighter than the rest Diagram from Padovani and Urry

Radio, optical and X-ray images of the jet in M87 galaxy * Jets are common in AGN and are clearly seen in radio, optical and X-ray images * When the jet points close to the our line of sight, its emission can dominates the observed spectrum, often extending to the highest observable energy (TeV!) gamma-rays and this requires very energetic particles to produce the radiation * Another remarkable example of cosmic accelerators

Most prevalent point-like g-ray sources on the sky: active galaxies dominated by emission from relativistic outflows (=jets) Two examples of broad-band spectra : g-ray emission dominates the E x F(E) spectrum energetically important Bright EGRET-detected GeV emitting blazar: 3C279 (data from Wehrle et al. 1998) First TeV-emitting blazar: Mkn 421 (data from Macomb et al. 1995)

Summary: * Energetic γ-ray astrophysics is uncovering a plethora of new phenomena in the Universe * Following the spectacular discoveries of EGRET, the recently-launched GLAST soon will bring much improved sensitivity and angular resolution, expanded bandpass, and all-sky monitoring capability * GLAST will allow us to better understand the structure and physical processes responsible for radiation in the known γ-ray sources such as pulsars, jets in active galaxies, γ-ray bursts, and supernova remnants contributing to the Galactic diffuse γ ray emission * Much of the improved understanding of those sources will be via multi-band studies, involving radio, optical, and X-ray bands * The most exciting discoveries will be via the new classes of astrophysical γ-ray emitters one example may be γ-rays resulting from annihilation of postulated dark matter particles