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07_HEA09_Observatories_&_Instrumentation

Course: PHYS 20692, Fall 2009
School: East Los Angeles College
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Energy High Astrophysics Observatories & Instrumentation Giampaolo Pisano Jodrell Bank Centre for Astrophysics - University of Manchester giampaolo.pisano@manchester.ac.uk March 2009 The great observatories - Brief summary of some of the current observatories and related techniques in the wavebands: - Radio - Millimetre and Sub-millimetre - Infrared - Optical - X-ray - Gamma-ray Future observatories at...

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Energy High Astrophysics Observatories & Instrumentation Giampaolo Pisano Jodrell Bank Centre for Astrophysics - University of Manchester giampaolo.pisano@manchester.ac.uk March 2009 The great observatories - Brief summary of some of the current observatories and related techniques in the wavebands: - Radio - Millimetre and Sub-millimetre - Infrared - Optical - X-ray - Gamma-ray Future observatories at the end of the course Observatories across the e.m. spectrum Radio mm/sub-mm FIR MIR NIR V NUV UV Soft X-ray Hard X-ray -ray 10 3 10 2 101 10 10 1 10 2 10 3 10 4 10 5 10 6 10 7 10 8 10 9 10 10 10 11 10 12 [m ] The atmospheric windows Atmosphere Trasparency Radio mm/sub-mm FIR MIR NIR V NUV UV Soft X-ray Hard X-ray -ray 10 3 10 5 10 2 10 6 101 10 7 10 10 8 10 1 10 2 10 3 10 4 10 5 10 6 10 7 10 8 10 9 10 10 10 11 10 12 10 9 10 10 10 11 10 12 10 13 10 14 10 15 10 16 10 17 10 18 10 19 10 20 [m ] [ Hz ] Altitude [km] Minimum altitude for transparent atmosphere Sea Level Angular resolution of a telescope - In general, the angular resolution of an optical system is: : Wavelength D : Telescope diameter 1.22 D - Optical system angular resolution Example - Jodrell Bank dish operating at: = 408MHz D = 76m 3 108 0.735m = = 8 4.08 10 c 0.735 1.22 = 0.0116 76 0.66 deg 40 arcmin A bit bigger than the Moon angular size Radio wavelengths Radio mm/sub-mm FIR MIR NIR V NUV UV Soft X-ray Hard X-ray -ray 10 3 10 5 10 2 10 6 101 10 7 10 10 8 10 1 10 2 10 3 10 4 10 5 10 6 10 7 10 8 10 9 10 10 10 11 10 12 10 9 10 10 10 11 10 12 10 13 10 14 10 15 10 16 10 17 10 18 10 19 10 20 [m ] [ Hz ] Radio waveband - Technology: 3MHz 30GHz 100m 1cm 0.01eV E 100eV T ~ (10 4 1) K - Single radio antennas: need to be extremely large - Radio interferometry: antenna arrays (aperture synthesis) - Observations: - 30 GHz -10 MHz : Atmosphere Radio window 1 - 10 MHz : very difficult reflection from ionosphere reflection interplanetary/interstellar plasmas < 1 MHz : even more difficult Radio Astronomy 1/5 Jodrell Bank: 76 m Effelsberg: 100 m Green Bank: 100 m - Frequencies: ~ 300 MHz - 86 GHz - Resolution: 10 arcsec - 30 arcmins - Observation: galactic plane, SNR, neutral H, molecular lines, radio galaxies, quasars, pulsars, etc. Radio Astronomy 2/5 - Arecibo (Arecibo, Puerto Rico) - Frequencies: ~ 300 MHz - 30 GHz - Diameter: 305 m World largest filled-aperture telescope - Technique: Steerable beam by means of moving receiver Radio Astronomy 3/5 Radio Interferometry - Technique: Observation of the same object made simultaneously by many telescopes connected together (need phase information) - Resolution: Vast increase on angular resolution emulation of a telescope of the size of the array - Telescopes: Need many telescopes and baselines to have good quality images Radio Astronomy 4/5 Very Large Array (VLA) (NRAO New Mexico) - Frequencies: 73 MHz - 50 GHz - Telescopes: 27 independent antennas, each with 25 m diameter (sensitivity equivalent to a 130 m diameter dish) - Resolution: 0.05 - 700 arcsec (equivalent to a 36 km antenna) - Technique: Aperture synthesis interferometry - Observations: AGN, jets, pulsars and GRBs Radio Astronomy 5/5 - VLBI Arrays in the world Galaxy M87 - Technique: - Resolution: Very Long Baseline Interferometry Extremely high micro-arcsec Higher than any other astronomical instrument - Data from each antenna recorded using atomic clocks and analysed later Millimetre and Sub-millimetre wavelengths Radio mm/sub-mm FIR MIR NIR V NUV UV Soft X-ray Hard X-ray -ray 10 3 10 5 10 2 10 6 101 10 7 10 10 8 10 1 10 2 10 3 10 4 10 5 10 6 10 7 10 8 10 9 10 10 10 11 10 12 10 9 10 10 10 11 10 12 10 13 10 14 10 15 10 16 10 17 10 18 10 19 10 20 [m ] [ Hz ] Millimetre and sub-mm - Technology: 30GHz 3THz 10mm 0.1mm 0.1meV E 10meV T ~ (1 100) K - Solid state mixers for heterodyne receivers - Bolometers for continuum receivers - Observations: - <1mm : strong absorption bands atmosphere (water vapour, CO2, ...) - Windows available at 0.8, 0.65, 0.45 and 0.35 mm - High dry sites, aircrafts, balloons or satellites Millimetre and sub-mm Astronomy 1/3 - Cosmic Background Explorer (COBE) - Observation: Black-body spectrum & 7 degrees scale full sky anisotropies Nobel Price in 2006 Millimetre and sub-mm Astronomy 2/3 - Wilkinson Microwave Anisotropy Probe (WMAP) - Frequencies: 23 - 94 GHz - Observation: Full sky CMB anisotropies at small angular scales and Temperature anisotropy - Polarisation correlation Millimetre and sub-mm Astronomy 3/3 - Planck Mission (2009) - Frequencies: LFI: 30 70 GHz ; HFI: 100 - 857 GHz - Observation: Full sky CMB anisotropies and E-Modes polarisation Infrared Wavelengths Radio mm/sub-mm FIR MIR NIR V NUV UV Soft X-ray Hard X-ray -ray 10 3 10 5 10 2 10 6 101 10 7 10 10 8 10 1 10 2 10 3 10 4 10 5 10 6 10 7 10 8 10 9 10 10 10 11 10 12 10 9 10 10 10 11 10 12 10 13 10 14 10 15 10 16 10 17 10 18 10 19 10 20 [m ] [ Hz ] Infrared waveband - Technology: - Silicon detectors - Observations: 3THz 300THz 100m 1m 0.01eV E 1eV T ~ (102 10 4 ) K - Atmosphere windows at 1.2, 1.65, 2.2, 3.5, 5, 10, 20 and 30 m. - Atmosphere as strong thermal emitter (a 300K Black-Body peaks at 10m) - High dry sites, balloons, aircrafts or satellites Infrared Astronomy 1/3 - Spitzer Space Telescope (2003) - Wavelength: 3-180 micron - Observation: interstellar dust, star formation, extra-solar planets, young stellar objects, etc. - Characteristics: - Largest IR telescope ever in space - Unprecedented resolution & sensitivity Infrared Astronomy 2/3 - Spitzer Space Telescope - Revealed inner dust ring in galaxy M31 evidence of a violent head-on collision with companion dwarf galaxy M32 happened 210 My ago. Infrared Astronomy 3/3 - Spitzer Space Telescope - Object: Supernova Remnants images superposition at different wavelengths - Infrared emission: warm dust emission from dust heated by the primary blast wave Optical wavelengths Radio mm/sub-mm FIR MIR NIR V NUV UV Soft X-ray Hard X-ray -ray 10 3 10 5 10 2 10 6 101 10 7 10 10 8 10 1 10 2 10 3 10 4 10 5 10 6 10 7 10 8 10 9 10 10 10 11 10 12 10 9 10 10 10 11 10 12 10 13 10 14 10 15 10 16 10 17 10 18 10 19 10 20 [m ] [ Hz ] Optical waveband - Technology: 3 1014 Hz 1015 Hz 1m 300nm 1eV E 4eV T ~ 3 10 4 K - Photographic emulsions (few % efficiency) - Charge Coupled Devices (CCDs) (70% efficiency) (small field of view) - Observations: - Optical window wider than our eyes sensitivity (from ~ 400nm to 700 nm ) - < 320 nm : absorption ozone begins Optical Astronomy 1/3 - Hubble Space Telescope (HST) - Largest telescope in orbit - It revolutionised Optical Astronomy but greatly contributed to HEA discoveries Optical Astronomy 2/3 Mauna Kea - Keck telescope (4145 m) - Telescope: Two twin telescopes 10 m each in diameter World largest optical and infrared telescopes - Resolution: 0.04 - 0.4 arcsec Interferometer mode: 5 - 24 milliarcsec (infrared) - Techniques: - Adaptive optics mirrors composed of 36 hexagonal segments - Interferometer the two telescope can operate together Optical Astronomy 3/3 - Very Large Telescope (VLT) - Chile (2635 m) - Telescope: Four 8.2 m diameter telescope array, plus additional telescopes - Wavelengths: From Infrared to UV - Resolution: will be 0.002 arcsec at 2um - Techniques: Adaptive optics & different interferometric modes (VLTI) Ultraviolet wavelengths Radio mm/sub-mm FIR MIR NIR V NUV UV Soft X-ray Hard X-ray -ray 10 3 10 5 10 2 10 6 101 10 7 10 10 8 10 1 10 2 10 3 10 4 10 5 10 6 10 7 10 8 10 9 10 10 10 11 10 12 10 9 10 10 10 11 10 12 10 13 10 14 10 15 10 16 10 17 10 18 10 19 10 20 [m ] [ Hz ] Ultraviolet waveband - Technology: 1015 Hz 3 1016 Hz 300nm 10nm 4eV E 100eV T ~ (105 106 ) K - NUV: 300nm > >100nm : similar to optical waveband - UV: 100nm > >10nm : reflection at grazing incidence necessary - Observations: - Atmosphere opaque because of ozone absorption - Rockets and satellites - < 91.2 nm : Hydrogen Lyman limit interstellar gas opaque (neutral H clumps) The great observatories - Brief summary of some of the current observatories and related techniques in the wavebands: - Radio - Millimetre and Sub-mm - Infrared - Optical X-ray - - Gamma-ray X-ray wavelengths Radio mm/sub-mm FIR MIR NIR V NUV UV Soft X-ray Hard X-ray -ray 10 3 10 5 10 2 10 6 101 10 7 10 10 8 10 1 10 2 10 3 10 4 10 5 10 6 10 7 10 8 10 9 10 10 10 11 10 12 10 9 10 10 10 11 10 12 10 13 10 14 10 15 10 16 10 17 10 18 10 19 10 20 [m ] [ Hz ] X-ray waveband - Technology: 3 1016 Hz 3 1019 Hz 10nm 0.01nm 0.1KeV E 100KeV T ~ (106 109 ) K - Detectors similar to particle physics detectors - Proportional counters, scintillation detectors, CCDs - Telescopes as collimators - Observations: - Wholly above atmosphere because of photoelectric absorption of X-rays by atoms and molecules of Earth atmosphere. X-ray Astronomy 1/21 Wilhelm Conrad Roentgen discovered Roentgen or X-ray emission in November 1895 X-ray Astronomy 2/21 1948: First evidence of solar corona X-ray emission X-ray Astronomy 3/21: Detectors Proportional Counter ( & Mechanical Collimator ) X-Ray Photon Energy < 20keV - X-ray photons ionise atoms gas - Electrons drift to the central wire-anode (2000 V) - Further ionisation - Pulse of electrons avalanche of electrons close to the anode electronics count Spectrum Number electrons proportional to X-ray photon energy X-ray Astronomy 4/21: Detectors Scintillation Counter Hard X-Ray Scintillators Balloon-based mission 50 Km altitude Photon Energies: 20 - 200 keV - Gas proportional counter not massive enough to stop high energy photons - Solid state detector Crystal of sodium iodide or caesium iodide scintillation detected by a photomultiplier - Photon absorbed by an atom of the crystal and part of this energy immediately reappears as a pulse of light Amount of scintillation light proportional to X-ray photon energy X-ray Astronomy 5/21 - Discovery and identification of Tau X-1 (Boyer 1964) - 1963: Discovery of Tau X-1 - 1964: Identification with Crab Nebula using Moon coverage Source emission is diffused Pulsar account only for 5% X-ray emission X-ray Astronomy 6/21: Detectors Rotation Modulator Collimator Incident X-rays Wires of first grid Strips of Sky seen by collimator Direction of Maximum transmisison Wires second grid Wire Thin window Proportional Counter - Wire-grids defining a set of bands in the sky - Rotating the spacecraft - Accuracy at arcmin level modulated count rate for a point source X-ray Astronomy 7/21 - Sco X-1 localisation Rotation Modulation Collimator data - It was very difficult to identify the object associated with Sco X-1 - The Modulation Collimator technique allowed to find the counterpart X-ray Astronomy 8/21 es transients) mission X-ray Astronomy 9/21 - Most important satellite missions X-ray Astronomy 10/21 - ROSAT - Optics: Wolter type mirrors for grazing incidence reflection - Detector using photoelectrical absorption in gas - Anti-coincidence circuits to check for charged particles - Detector window produced artefacts X-ray Astronomy 11/21 - ROSAT results - Resolution: 1 arcmin - First deep all sky survey in soft X-ray followed by point source phase X-ray Astronomy 12/21 Chandra (NASA) Dedicated to the Astrophysicist S. Chandrasekhar - Optics: Wolter type mirrors and CCDs detectors - Best angular (0.5arcsec) and spectral resolution ever; Energies: 0.1-10 KeV - Capable to measure emission variations as short as 16 s (bursts) - Discoveries: stellar black-holes, shock accelerations in SNRs, X-rays from AGN jets X-ray Astronomy 13/21 - Chandras elliptical orbit - Cosmic rays extremely energetic particles can pass through the detectors - High energy protons and electrons are trapped in the van Allen radiation belts It is better to operate outside the radiation belt X-ray Astronomy 14/21 - Wolter type X-ray Mirrors - A mirror used at normal incidence would scatter the x-ray photons - Wolter type I X-ray mirrors are used in Chandra and XMM-Newton X-ray Astronomy 15/21 Chandra: X-ray Mirrors - Four nested Zerodur glass mirrors, polished, coated with iridium on a binding layer of chromium X-ray Astronomy 16/21 XMM-Newton (ESA) X-Ray Multi-Mirror Mission - CCDs as detectors - Optics: three independent X-ray telescopes pointing same direction - Largest collecting area ever Highest sensitivity (5 x Chandra) - Additional Optical-UV telescope - Angular resolution: 6 arcsec - Results: detection heavy elements in GBRs, mapping elements SNRs X-ray Astronomy 17/21 XMM-Newton: Optics - Grazing incidence reflection gratings spectrometers X-ray Astronomy 18/21 X-MM Newton: X-ray Mirrors - Each mirror system has 58 Wolter gold plated mirrors less than 2 mm thick ! - Separation between mirrors 1-2mm - Surface accuracy better than 0.1 nm ! X-ray Astronomy 19/21 X-ray Mirrors - Grazing geometry implies large focal length Big satellites X-ray Astronomy 20/21 XMM-Newton: CCD detectors - CCD (Charge Coupled Device) developed in UK and Germany - Semiconductor device giving both spectral and imaging information - Simpler versions used in digital cameras X-ray Astronomy 21/21 - Instrum...

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Wireless Wide Area Networks3G3G (or 3-G) is short for third-generation technology. It is used in the context of mobile phone standards. The services associated with 3G provide the ability to transfer simultaneously both voice data (a telephone cal
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Chapter 2 MatLab Interactive EnvironmentInstructor: Fang Chu fc48@njit.edu1 Homework Format Name Major Email Address Date Chapter # Problem #2 Homework Policy No Late Homework!-Unless get Prof. Hung's permission. Completed in class. Sub
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iperations Desert Shield and Desert Storm saw the massive ux' of foreign commercial contracts to support the soldiers. Not since thr Vlrtnam War has the military relted so heavily on commercial contracts. Operations Urgent Fury and just Cause were
University of Alabama in Huntsville - CS - 570
A SURVEY ON SENSOR NETWORKSPrathima Anantha &amp; Phani K KattamudiOverview1.Introduction2. Sensor network communication Architecture 3. Design Factors4.Protocal stack5.Conclusion 6.ReferencesIntroductionRecent advances in wireless communica
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Introduction to The Normal DistributionINTRODUCTIONL L L The most important probability distribution The very foundation for more advanced statistical analyses A continuous distributionTHE GENERAL NATURE OF THE NORMAL DISTRIBUTIONL The probabili
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Java CodingCMP 328 Object Oriented Programming in JavaLecture 03 &amp; 04: Java Application and AppletProfessor Peichung Shih Identify how the code can be accessed with an access modifier public indicates that the code can be accessed by all obj