A model of the Earth's gamma-ray emission for GLAST derived from EGRET data. Dirk Petry (UMBC, NASA/GSFC) DC2 Meeting GSFC June 27-29, 2005

Size: px
Start display at page:

Download "A model of the Earth's gamma-ray emission for GLAST derived from EGRET data. Dirk Petry (UMBC, NASA/GSFC) DC2 Meeting GSFC June 27-29, 2005"

Transcription

1 A model of the Earth's gamma-ray emission for GLAST derived from EGRET data (UMBC, NASA/GSFC) DC2 Meeting GSFC June 27-29,

2 Gamma-ray emission from the Earth's atmosphere Incoming cosmic rays Cosmic rays above cut off rigidity ( 15 GV) penetrate atmosphere and cause airshowers. Grazing incidence showers produce forward colimated gamma radiation which can escape atmosphere. Gamma rays from secondaries with large transverse momentum or from low energy pions can escape "upwards". Observer 2

3 First measurement of HE gamma emission of the Earth from space made by SAS-2 Nov June 1973: photons above 35 MeV (Thompson et al., 1981) The next mission taking Earth data flew almost 20 years later: Operational for 9.1 years ( ) circular orbit at approx. 420 km altitude, inclination 28.5º energy range 35 MeV 30 GeV mostly pointed observations => Earth in field of view > 50 % of elapsed time! In spite of special Earth avoidance trigger modes, ca. 60 % of the gold plated EGRET photon events come from zenith angles > 105º (3 million events) 3

4 Data Analysis Results (excerpt) Example of a flux map at MeV Spectral index as a function of zenith angle 5E 5 2E 4 1.5E 3 3E 3 6E 3 2E 2 cm 2 s 1 sr 1 See also astro ph/

5 Flux maps in three energy bands + composite: 2d maps, rgb plots 5

6 Summary of the model properties in Earth (flux v8r20): Bright rim with Gaussian profile and exponential tail towards Nadir Spectrum hardest (1.7) at rim peak, softer both towards Nadir and Zenith, softest at Nadir (2.4) Exponential cutoff at ca. 3 GeV (AZ independent rim and central component), 30 GeV (AZ dependent rim component), consistent with the available data above 10 GeV from EGRET Entire EGRET dataset contains 675 events with E > 10 GeV and zenith angle > 105 deg, only 4 events of these have a zenith angle > 120 deg. The most energetic event has 120 GeV. The energy resolution of EGRET at 10 GeV is 25% FWHM. A detailed calculation predicts that one would expect a spill over of about 20 % with a spectrum like the nominal one measured below 10 GeV. I.e. the model should predict roughly 540 events above 10 GeV. The model parameters were adjusted to fulfill this condition. 6

7 Summary of the model properties in Earth (flux v8r20) contnd.: Rim peak position is energy independent at the geometrical horizon Detailed study showed that the previously assumed energy dependent position of the rim peak can be entirely explained by the PSF. Rim width (std. dev.) = 25 % of angular width of atmosphere Azimuthal variation to a very good approximation symmetric around West (no North South effect) East West ratio first increasing with energy, peaking at around 600 MeV, then decreasing again (implicit property of the model) Altitude dependence consistent with expectations from geometry 7

8 Altitude dependence: Dedicated study of EGRET data confirms: Altitude dependence as one would expect from purely geometrical considerations, i.e. surface brightness constant, intensity decreases as the solid angle. In addition all zenith angle related parameters scale with the Horizon ZA = 90º+acos(R E /R O ) GLAST Earth Change in altitude changes horizon ZA 8

9 Differential flux maps generated from the model (old version before flux v8r20) 9

10 Differential flux maps generated from the model (new, improved version, analytical) 12 Jan 05 10

11 Event maps generated from the model (new version, actual Monte Carlo Photons, ideal detector) 11

12 Spectrum generated by Earth in flux v8r20 (all directions) Number of generated photons log(e/mev) 12

13 Summary New model version has improved correction for EGRET PSF and an improved spectrum above 10 GeV based on all available EGRET data. Total flux has essentially not changed, only the spatial distribution and the spectrum at the highest energies Above 10 GeV, the model is really an intelligient guess ; the EGRET data essentially only gives an integral flux above 10 GeV For the energy range up to 350 GeV and for the present pursposes of GLAST, this model should be sufficient (as already mentioned above: in its entire lifetime, EGRET only detected a single photon above 100 GeV from the Earth). But I will keep working to improve the knowledge of the Earth's spectrum beyond 350 GeV. 13

A New Look at the Galactic Diffuse GeV Excess

A New Look at the Galactic Diffuse GeV Excess A New Look at the Galactic Diffuse GeV Excess Brian Baughman Santa Cruz Institute for Particle Physics 1 Overview Diffuse gamma-ray emission The Galactic diffuse gamma-ray GeV excess Discussion of the

More information

Justin Vandenbroucke (KIPAC, Stanford / SLAC) for the Fermi LAT collaboration

Justin Vandenbroucke (KIPAC, Stanford / SLAC) for the Fermi LAT collaboration Measurement of the cosmic ray positron spectrum with the Fermi LAT using the Earth s magnetic field Justin Vandenbroucke (KIPAC, Stanford / SLAC) for the Fermi LAT collaboration International Cosmic Ray

More information

A Search for Point Sources of High Energy Neutrinos with AMANDA-B10

A Search for Point Sources of High Energy Neutrinos with AMANDA-B10 A Search for Point Sources of High Energy Neutrinos with AMANDA-B10 Scott Young, for the AMANDA collaboration UC-Irvine PhD Thesis: http://area51.berkeley.edu/manuscripts Goals! Perform an all-sky search

More information

Experimental studies of East-West effect of the charge ratio of atmospheric muons with energies relevant to the atmospheric neutrino anomaly

Experimental studies of East-West effect of the charge ratio of atmospheric muons with energies relevant to the atmospheric neutrino anomaly Experimental studies of East-West effect of the charge ratio of atmospheric muons with energies relevant to the atmospheric neutrino anomaly I.M.Brancus, J.Wentz,, B.Mitrica, H.Rebel,, M.Petcu, A.Bercuci,,

More information

The Gamma-ray Albedo of the Moon

The Gamma-ray Albedo of the Moon [albedo] the proportion of the incident light that is reflected by a surface The Gamma-ray Albedo of the Moon Igor V. Moskalenko & Troy A. Porter Astrophys. J. 670, 1467-1472 (2007) Masaki Mori ICRR CANGAROO

More information

IAC-08-A MONTE CARLO SIMULATIONS OF ENERGY LOSSES BY SPACE PROTONS IN THE CRATER DETECTOR

IAC-08-A MONTE CARLO SIMULATIONS OF ENERGY LOSSES BY SPACE PROTONS IN THE CRATER DETECTOR IAC-08-A1.4.06 MONTE CARLO SIMULATIONS OF ENERGY LOSSES BY SPACE PROTONS IN THE CRATER DETECTOR Lawrence W. Townsend The University of Tennessee, Knoxville, Tennessee, United States of America ltownsen@tennessee.edu

More information

The H.E.S.S. Standard Analysis Technique

The H.E.S.S. Standard Analysis Technique The H.E.S.S. Standard Analysis Technique Wystan Benbow for the H.E.S.S. Collaboration Max Planck Institut für Kernphysik Postfach 103980 D-69029 Heidelberg, Germany The High Energy Stereoscopic System

More information

Particle Acceleration in the Universe

Particle Acceleration in the Universe Particle Acceleration in the Universe Hiroyasu Tajima Stanford Linear Accelerator Center Kavli Institute for Particle Astrophysics and Cosmology on behalf of SLAC GLAST team June 7, 2006 SLAC DOE HEP Program

More information

Monte Carlo Studies for a Future Instrument. Stephen Fegan Vladimir Vassiliev UCLA

Monte Carlo Studies for a Future Instrument. Stephen Fegan Vladimir Vassiliev UCLA Monte Carlo Studies for a Future Instrument Stephen Fegan Vladimir Vassiliev UCLA Approach to simulations CORSIKA 6200, 6500, 6502 w/bernlöhr Simulation of response of a single cell of an infinite array

More information

Non-thermal emission from pulsars experimental status and prospects

Non-thermal emission from pulsars experimental status and prospects Non-thermal emission from pulsars experimental status and prospects # γ!"# $%&'() TeV γ-ray astrophysics with VERITAS ( $γ" *$%&'() The charged cosmic radiation - how it all began... Discovery: Victor

More information

IceCube: Ultra-high Energy Neutrinos

IceCube: Ultra-high Energy Neutrinos IceCube: Ultra-high Energy Neutrinos Aya Ishihara JSPS Research Fellow at Chiba University for the IceCube collaboration Neutrino2012 at Kyoto June 8 th 2012 1 Ultra-high Energy Neutrinos: PeV and above

More information

The Sun and the Solar System in Gamma Rays

The Sun and the Solar System in Gamma Rays The Sun and the Solar System in Gamma Rays R. Desiante1 on behalf of the Fermi-LAT collaboration SciNeGHE 2016 1 INFN Torino Outline Introduction The Fermi Gamma-Ray Space Telescope The active Sun as seen

More information

Extreme high-energy variability of Markarian 421

Extreme high-energy variability of Markarian 421 Extreme high-energy variability of Markarian 421 Mrk 421 an extreme blazar Previous observations outstanding science issues 2001 Observations by VERITAS/Whipple 10 m 2001 Light Curve Energy spectrum is

More information

Gamma-ray Astrophysics with VERITAS: Exploring the violent Universe

Gamma-ray Astrophysics with VERITAS: Exploring the violent Universe Gamma-ray Astrophysics with VERITAS: Exploring the violent Universe K. Ragan McGill University Soup & Science 11-Jan-2008 Soup & Science Jan. '08 1 How do we know about the Universe? Historically, all

More information

Atmospheric Neutrinos and Neutrino Oscillations

Atmospheric Neutrinos and Neutrino Oscillations FEATURE Principal Investigator Takaaki Kajita Research Area Experimental Physics Atmospheric Neutrinos and Neutrino Oscillations Introduction About a hundred years ago Victor Hess aboard a balloon measured

More information

Distinct Features of Pulsar Polar-Gap Emission at the High-Energy Spectral Cutoff

Distinct Features of Pulsar Polar-Gap Emission at the High-Energy Spectral Cutoff The Universe Viewed in Gamma-Rays 1 Distinct Features of Pulsar Polar-Gap Emission at the High-Energy Spectral Cutoff Jaros law DYKS and Bronis law RUDAK Nicolaus Copernicus Astronomical Center, Rabiańska

More information

Milagro A TeV Observatory for Gamma Ray Bursts

Milagro A TeV Observatory for Gamma Ray Bursts Milagro A TeV Observatory for Gamma Ray Bursts B.L. Dingus and the Milagro Collaboration Los Alamos National Laboratory University of Maryland, University of California Santa Cruz, University of California

More information

GLAST Large Area Telescope:

GLAST Large Area Telescope: Gamma-ray Large Area Space Telescope GLAST Large Area Telescope: Project Overview Robert P. Johnson Santa Cruz Institute for Particle Physics Physics Department University of California at Santa Cruz LAT

More information

MoonCal An electromagnetic calorimeter on the lunar surface. R.Battiston, M.T.Brunetti, F. Cervelli, C.Fidani, F.Pilo

MoonCal An electromagnetic calorimeter on the lunar surface. R.Battiston, M.T.Brunetti, F. Cervelli, C.Fidani, F.Pilo MoonCal An electromagnetic calorimeter on the lunar surface R.Battiston, M.T.Brunetti, F. Cervelli, C.Fidani, F.Pilo Why the Moon for astroparticle physics? The Moon does not have atmosphere nor water.

More information

Cosmic Neutrinos in IceCube. Naoko Kurahashi Neilson University of Wisconsin, Madison IceCube Collaboration

Cosmic Neutrinos in IceCube. Naoko Kurahashi Neilson University of Wisconsin, Madison IceCube Collaboration Cosmic Neutrinos in IceCube Naoko Kurahashi Neilson University of Wisconsin, Madison IceCube Collaboration HEM KICP UChicago 6/9/2014 1 Outline IceCube capabilities The discovery analysis with updated

More information

Current and Future balloon and space experiments L. Derome (LPSC Grenoble) Tango, May 4-6th, 2009

Current and Future balloon and space experiments L. Derome (LPSC Grenoble) Tango, May 4-6th, 2009 Current and Future balloon and space experiments L. Derome (LPSC Grenoble) Tango, May 4-6th, 2009 L. Derome, Tango, May 4-6th 2009 1 Plan I will focus on: Future experiments which are going to measure

More information

GAMMA-RAY ASTRONOMY: IMAGING ATMOSPHERIC CHERENKOV TECHNIQUE FABIO ZANDANEL - SESIONES CCD

GAMMA-RAY ASTRONOMY: IMAGING ATMOSPHERIC CHERENKOV TECHNIQUE FABIO ZANDANEL - SESIONES CCD GAMMA-RAY ASTRONOMY: IMAGING ATMOSPHERIC CHERENKOV TECHNIQUE COSMIC RAYS Discovered in 1912 by Victor Hess (Nobel Prize) Messengers from the non-thermal part of the Universe E < 15 ev: galactic E > 17

More information

CRaTER Science Requirements

CRaTER Science Requirements CRaTER Science Requirements Lunar Reconnaissance Orbiter CRaTER Preliminary Design Review Justin Kasper (CRaTER Proj. Sci.) Outline Energy deposition Classical ionizing radiation Nuclear fragmentation

More information

Payload for Antimatter Matter Exploration and Light-nuclei Astrophysics. PAMELA MissioN 17 December 2010 Prepared by FatiH KAYA

Payload for Antimatter Matter Exploration and Light-nuclei Astrophysics. PAMELA MissioN 17 December 2010 Prepared by FatiH KAYA Payload for Antimatter Matter Exploration and Light-nuclei Astrophysics PAMELA MissioN 17 December 2010 Prepared by FatiH KAYA Astropartical Physics İssue To inform. What Powered the Big Bang? Inflation

More information

Bethe-Block. Stopping power of positive muons in copper vs βγ = p/mc. The slight dependence on M at highest energies through T max

Bethe-Block. Stopping power of positive muons in copper vs βγ = p/mc. The slight dependence on M at highest energies through T max Bethe-Block Stopping power of positive muons in copper vs βγ = p/mc. The slight dependence on M at highest energies through T max can be used for PID but typically de/dx depend only on β (given a particle

More information

A. Takada (Kyoto Univ.)

A. Takada (Kyoto Univ.) A. Takada (Kyoto Univ.) Nucleosynthesis SNR : Radio-isotopes Galactic plane : 26 Al Annihilation Particle acceleration Jet (AGN) : Synchrotron + Inverse Compton Strong gravitational potential Black hole

More information

Future Gamma-Ray Observations of Pulsars and their Environments

Future Gamma-Ray Observations of Pulsars and their Environments Future Gamma-Ray Observations of Pulsars and their Environments David J. Thompson NASA Goddard Space Flight Center GLAST Large Area Telescope Collaboration djt@egret.gsfc.nasa.gov D. Thompson 363 rd Heraeus

More information

Calibrating Atmospheric Cherenkov Telescopes with the LAT

Calibrating Atmospheric Cherenkov Telescopes with the LAT Gamma-ray Large Area Space Telescope Calibrating Atmospheric Cherenkov Telescopes with the LAT S. W. Digel SLAC GLAST-for-Lunch, 21 April 2005 1 Outline IACTs vs. LAT Cross calibration Issues Advantages

More information

USAAAO Round 2 Qualification Exam 2016

USAAAO Round 2 Qualification Exam 2016 USAAAO Round 2 Qualification Exam 2016 Instructions (Read completely before you begin) This is the second round qualification test for the USAAAO team. The test is short answer, consisting of 12 short

More information

Application of an analysis method based on a semi-analytical shower model to the first H.E.S.S. telescope

Application of an analysis method based on a semi-analytical shower model to the first H.E.S.S. telescope Application of an analysis method based on a semi-analytical shower model to the first H.E.S.S. telescope The 28th International Cosmic Ray Conference Mathieu de Naurois, LPNHE Paris University VI/VII

More information

Prospects for Observations of Very Extended and Diffuse Sources with VERITAS. Josh Cardenzana

Prospects for Observations of Very Extended and Diffuse Sources with VERITAS. Josh Cardenzana Prospects for Observations of Very Extended and Diffuse Sources with VERITAS Josh Cardenzana New era of synergy ~0.5 at 1GeV to 10 GeV) Fermi ~0.15 at 150GeV to 1 TeV) VERITAS ~0.5 at 1TeV

More information

Characterizations and Diagnostics of Compton Light Source

Characterizations and Diagnostics of Compton Light Source Characterizations and Diagnostics of Compton Light Source Advance Light Source (ALS) (LBNL) Ying K. Wu Duke Free Electron Laser Laboratory (DFELL) Acknowledgments: DFELL: B. Jia, G. Swift, H. Hao, J. Li,

More information

Status and Future of the HESS experiment

Status and Future of the HESS experiment Status and Future of the HESS experiment Martin Tluczykont for the HESS Collaboration LLR Ecole Polytechnique Joint Symposium on GeV-TeV Astrophysics in the GLAST Era Stanford, September 2004 HESS Phase

More information

FERMI. YOUNG PULSAR SPECTRA WITH THE LAT FERMI TELESCOPE Ateliers pulsars. 25 novembre 2008 Damien Parent. Gamma-ray Large Area Space Telescope

FERMI. YOUNG PULSAR SPECTRA WITH THE LAT FERMI TELESCOPE Ateliers pulsars. 25 novembre 2008 Damien Parent. Gamma-ray Large Area Space Telescope FERMI Gamma-ray Large Area Space Telescope YOUNG PULSAR SPECTRA WITH THE LAT FERMI TELESCOPE Ateliers pulsars 25 novembre 2008 1 Topics 1. Young pulsars, our best candidates 2 examples : J0205+6449 and

More information

arxiv: v1 [astro-ph.he] 2 Jul 2009

arxiv: v1 [astro-ph.he] 2 Jul 2009 PROCEEDINGS OF THE 31 st ICRC, ŁÓDŹ 2009 1 First results on Cosmic Ray electron spectrum below 20 GeV from the Fermi LAT. M.Pesce-Rollins on behalf of the Fermi LAT Collaboration Istituto Nazionale di

More information

The VelaX pulsar wind nebula in the TeV regime. Bernhard Glück for the H.E.S.S. Collaboration July 8th, 2009, Boston

The VelaX pulsar wind nebula in the TeV regime. Bernhard Glück for the H.E.S.S. Collaboration July 8th, 2009, Boston The VelaX pulsar wind nebula in the TeV regime Bernhard Glück for the H.E.S.S. Collaboration July 8th, 2009, Boston Outline The H.E.S.S. Experiment Results for PWN VelaX from observation 2004 to 2006 Follow

More information

Calibration of the AGILE Gamma Ray Imaging Detector

Calibration of the AGILE Gamma Ray Imaging Detector Calibration of the AGILE Gamma Ray Imaging Detector Andrew Chen on behalf of the AGILE Team April 11, 2011 AGILE Astrorivelatore Gamma ad Immagini LEggero Italian Space Agency (ASI) small mission Participation

More information

arxiv: v2 [hep-ph] 23 Jun 2016

arxiv: v2 [hep-ph] 23 Jun 2016 Energy and angular distributions of atmospheric muons at the Earth arxiv:1606.06907v [hep-ph] Jun 016 Prashant Shukla Nuclear Physics Division, Bhabha Atomic Research Centre, Mumbai 400085, India. Homi

More information

Study of Solar Gamma Rays basing on Geant4 code

Study of Solar Gamma Rays basing on Geant4 code University of Liaoning, Shenyang 1036, China University of Nankai, Tianjin 300071, China Institute of High Energy Physics, Chinese Academy of Sciences, Beijing, 0049, China E-mail: gaobs@ihep.ac.cn Songzhan

More information

A SEARCH FOR ASTROPHYSICAL POINT SOURCES OF 100 TEV GAMMA RAYS BY THE UMC COLLABORATION

A SEARCH FOR ASTROPHYSICAL POINT SOURCES OF 100 TEV GAMMA RAYS BY THE UMC COLLABORATION A SEARCH FOR ASTROPHYSICAL POINT SOURCES OF 100 TEV GAMMA RAYS BY THE UMC COLLABORATION T.A.McKay, b A.Borione, b M.Catanese, a C.E.Covault, b J.W.Cronin, b B.E.Fick, b K.G.Gibbs, b K.D.Green, a S.Hauptfeld,

More information

The Large Area Telescope on-board of the Fermi Gamma-Ray Space Telescope Mission

The Large Area Telescope on-board of the Fermi Gamma-Ray Space Telescope Mission The Large Area Telescope on-board of the Fermi Gamma-Ray Space Telescope Mission 1 Outline Mainly from 2009 ApJ 697 1071 The Pair Conversion Telescope The Large Area Telescope Charged Background and Events

More information

Expected and unexpected gamma-ray emission from GRBs in light of AGILE and Fermi. Marco Tavani (INAF & University of Rome Tor Vergata)

Expected and unexpected gamma-ray emission from GRBs in light of AGILE and Fermi. Marco Tavani (INAF & University of Rome Tor Vergata) Expected and unexpected gamma-ray emission from GRBs in light of AGILE and Fermi Marco Tavani (INAF & University of Rome Tor Vergata) The EGRET heritage; Outline Description of the AGILE detectors for

More information

LAT Automated Science Processing for Gamma-Ray Bursts

LAT Automated Science Processing for Gamma-Ray Bursts SLAC-PUB-12715 LAT Automated Science Processing for Gamma-Ray Bursts James Chiang GLAST Science Support Center SLAC, 2575 Sand Hill Rd, Menlo Park CA 9425 Abstract. The LAT Instrument Science Operations

More information

1. Motivation & Detector concept 2. Performance 3. Confirmation experiments 4. Summary

1. Motivation & Detector concept 2. Performance 3. Confirmation experiments 4. Summary A. Takada, T. Tanimori, H. Kubo, J. D. Parker, T. Mizumoto, Y. Mizumura, T. Sawano, K. Nakamura, Y. Matsuoka, S. Komura, S. Nakamura, T. Kishimoto, M. Oda, T. Takemura, S. Miyamoto, K. Miuchi, S. Kurosawa

More information

Preliminary results from gamma-ray observations with the CALorimeteric Electron Telescope (CALET)

Preliminary results from gamma-ray observations with the CALorimeteric Electron Telescope (CALET) Preliminary results from gamma-ray observations with the CALorimeteric Electron Telescope (CALET) Y.Asaoka for the CALET Collaboration RISE, Waseda University 2016/12/15 CTA-Japan Workshop The extreme

More information

Fluxes of Galactic Cosmic Rays

Fluxes of Galactic Cosmic Rays Fluxes of Galactic Cosmic Rays sr s m - GeV Flux solar Modulation: Φ = 550 MV proton helium positron electron antiproton photon galdef 50080/60080 (γ) Status of Cosmic Ray Measurements: good agreement

More information

Neutral particles energy spectra for 900 GeV and 7 TeV p-p collisions, measured by the LHCf experiment

Neutral particles energy spectra for 900 GeV and 7 TeV p-p collisions, measured by the LHCf experiment Neutral particles energy spectra for 900 GeV and 7 TeV p-p collisions, measured by the LHCf experiment Raffaello D Alessandro 1 Department of Physics Università di Firenze and INFN-Firenze I-50019 Sesto

More information

Atmospheric gamma rays from solar energetic particles and cosmic rays penetrating the magnetosphere

Atmospheric gamma rays from solar energetic particles and cosmic rays penetrating the magnetosphere JOURNAL OF GEOPHYSICAL RESEARCH, VOL. 106, NO. A1, PAGES 77-92, JANUARY 1, 2001 Atmospheric gamma rays from solar energetic particles and cosmic rays penetrating the magnetosphere Gerald H. Share and Ronald

More information

Position Sensitive Germanium Detectors for the Advanced Compton Telescope

Position Sensitive Germanium Detectors for the Advanced Compton Telescope Position Sensitive Germanium Detectors for the Advanced Compton Telescope R.A. Kroeger 1, W.N. Johnson 1, J.D. Kurfess 1, B.F. Phlips, P.N. Luke 3, M. Momayezi 4, W.K. Warburton 4 1 Naval Research Laboratory,

More information

The Physics of Ultrahigh Energy Cosmic Rays. Example Poster Presentation Physics 5110 Spring 2009 Reminder: Posters are due Wed April 29 in class.

The Physics of Ultrahigh Energy Cosmic Rays. Example Poster Presentation Physics 5110 Spring 2009 Reminder: Posters are due Wed April 29 in class. The Physics of Ultrahigh Energy Cosmic Rays Example Poster Presentation Physics 5110 Spring 2009 Reminder: Posters are due Wed April 29 in class. 1 Introduction to Cosmic Rays References: http://www.phy.bris.ac.uk/groups/particle/pus/affo

More information

arxiv:astro-ph/ v2 20 Jul 2001

arxiv:astro-ph/ v2 20 Jul 2001 ISN Grenoble report 0-3 arxiv:astro-ph/003474v2 20 Jul 200 Secondary electrons and positrons in near earth orbit L. Derome, M. Buénerd, and Yong Liu Institut des Sciences Nucléaires, IN2P3/CNRS, 53 av.

More information

VERITAS Design. Vladimir Vassiliev Whipple Observatory Harvard-Smithsonian CfA

VERITAS Design. Vladimir Vassiliev Whipple Observatory Harvard-Smithsonian CfA VERITAS Design Vladimir Vassiliev Whipple Observatory Harvard-Smithsonian CfA VERITAS design goals VERITAS is a ground-based observatory for gamma-ray astronomy VERITAS design is derived from scientific

More information

PAMELA: a Satellite Experiment for Antiparticles Measurement in Cosmic Rays

PAMELA: a Satellite Experiment for Antiparticles Measurement in Cosmic Rays PAMELA: a Satellite Experiment for Antiparticles Measurement in Cosmic Rays PAMELA scientific objectives Detector s overview Subsystems description PAMELA status Massimo Bongi Universita degli Studi di

More information

PoS(ICRC2017)765. Towards a 3D analysis in Cherenkov γ-ray astronomy

PoS(ICRC2017)765. Towards a 3D analysis in Cherenkov γ-ray astronomy Towards a 3D analysis in Cherenkov γ-ray astronomy Jouvin L. 1, Deil C. 2, Donath A. 2, Kerszberg D. 3, Khelifi B. 1, Lemière A. 1, Terrier R. 1,. E-mail: lea.jouvin@apc.in2p3.fr 1 APC (UMR 7164, CNRS,

More information

Detection of TeV Gamma-Rays from Extended Sources with Milagro

Detection of TeV Gamma-Rays from Extended Sources with Milagro Detection of TeV Gamma-Rays from Extended Sources with Milagro P. M. Saz Parkinson for the Milagro Collaboration Santa Cruz Institute for Particle Physics, University of California, 1156 High Street, Santa

More information

High-energy Gamma Rays detection with the AMS-02 electromagnetic calorimeter. F. Pilo for the AMS-02 ECAL Group INFN Sezione di Pisa, Italy

High-energy Gamma Rays detection with the AMS-02 electromagnetic calorimeter. F. Pilo for the AMS-02 ECAL Group INFN Sezione di Pisa, Italy Frascati Physics Series Vol. 58 (2014) Frontier Objects in Astrophysics and Particle Physics May 18-24, 2014 High-energy Gamma Rays detection with the AMS-02 electromagnetic calorimeter F. Pilo for the

More information

Cosmic rays. 1.1 Origin and nature of cosmic rays

Cosmic rays. 1.1 Origin and nature of cosmic rays 1 Cosmic rays Victor Hess s experiments in manned balloons in 1912 demonstrated the existence of penetrating radiation entering the Earth s atmosphere from space. Hess s original observation was that gold-foil

More information

Gamma-ray Astrophysics

Gamma-ray Astrophysics Gamma-ray Astrophysics AGN Pulsar SNR GRB Radio Galaxy The very high energy -ray sky NEPPSR 25 Aug. 2004 Many thanks to Rene Ong at UCLA Guy Blaylock U. of Massachusetts Why gamma rays? Extragalactic Background

More information

Gamma-Ray Polarimetry in the Pair Production Regime

Gamma-Ray Polarimetry in the Pair Production Regime Gamma-Ray Polarimetry in the Pair Production Regime Peter F. Bloser (NASA/GSFC) S. D. Hunter (NASA/GSFC) G. O. Depaola (National University of Córdoba) F. Longo (INFN) Gamma-Ray Polarimetry Polarimetry

More information

Observing TeV Gamma Rays from the Jet Interaction Regions of SS 433 with HAWC

Observing TeV Gamma Rays from the Jet Interaction Regions of SS 433 with HAWC Observing TeV Gamma Rays from the Jet Interaction Regions of SS 433 with HAWC Chang Dong Rho University of Rochester TeVPA 2018 Berlin, Germany 08/28/2018 Overview 2 Microquasars as sources of TeV gamma

More information

Search for GeV neutrinos associated with solar flares with IceCube

Search for GeV neutrinos associated with solar flares with IceCube Search for GeV neutrinos associated with solar flares with IceCube The IceCube Collaboration http://icecube.wisc.edu/collaboration/authors/icrc17_icecube E-mail: gdewasse@icecube.wisc.edu Since the end

More information

ATMOSPHERIC MUONS IN HANOI

ATMOSPHERIC MUONS IN HANOI ATMOSPHERIC MUONS IN HANOI Pham Ngoc Diep, Pham Ngoc Dinh, Pham Thi Tuyet Nhung, Pierre Darriulat, Nguyen Thi Thao, Dang Quang Thieu and Vo Van Thuan Vietnam Auger Training Laboratory Institute for Nuclear

More information

arxiv:hep-ph/ v1 5 Apr 1993

arxiv:hep-ph/ v1 5 Apr 1993 BA-93-07 Calculated Electron Fluxes at Airplane Altitudes R. K. Schaefer, T. K. Gaisser, and T. S. Stanev arxiv:hep-ph/9304215v1 5 Apr 1993 Bartol Research Institute University of Delaware, Newark, DE

More information

Presentation by Indian Delegation. to 49 th STSC UNCOPUOS. February 2012 Vienna

Presentation by Indian Delegation. to 49 th STSC UNCOPUOS. February 2012 Vienna Presentation by Indian Delegation to 49 th STSC UNCOPUOS February 2012 Vienna ASTROSAT Astrosat is India s first dedicated multiwavelength astronomy satellite with a capability to observe target sources

More information

Blazars as the Astrophysical Counterparts of the IceCube Neutrinos

Blazars as the Astrophysical Counterparts of the IceCube Neutrinos Blazars as the Astrophysical Counterparts of the IceCube Neutrinos Maria Petropoulou Department of Physics & Astronomy, Purdue University, West Lafayette, USA Einstein Fellows Symposium Harvard-Smithsonian

More information

GOSAT mission schedule

GOSAT mission schedule GOSAT mission schedule 29 21 12 1 2 3 4 6 7 8 9 1 11 12 1 2 214 1 2 3 ~ Jan. 23 Launch Initial Checkout Initial function check Initial Cal. and Val. Mission life Normal observation operation Extra Operati

More information

Measurement of CR anisotropies with the AMS detector on the ISS

Measurement of CR anisotropies with the AMS detector on the ISS Measurement of CR anisotropies with the AMS detector on the ISS J. Casaus ( CIEMAT Spain ) on behalf of the AMS Collaboration Origin of excess of positrons Positron fraction shows an excess above 10 GeV

More information

Recent Observations of Supernova Remnants

Recent Observations of Supernova Remnants 1 Recent Observations of Supernova Remnants with VERITAS Tülün Ergin (U. of Massachusetts Amherst, MA) on behalf of the VERITAS Collaboration (http://veritas.sao.arizona.edu) 2 Contents Supernova Remnants

More information

arxiv:astro-ph/ v2 10 Mar 2003

arxiv:astro-ph/ v2 10 Mar 2003 Atmospheric Muon and Neutrino Flux From 3-Dimensional Simulation Yong Liu, L. Derome, and M. Buénerd Institut des Sciences Nucléaires, 53 av. des Martyrs, 38026 Grenoble cedex, France The atmospheric muon

More information

EBL Studies with the Fermi Gamma-ray Space Telescope

EBL Studies with the Fermi Gamma-ray Space Telescope EBL Studies with the Fermi Gamma-ray Space Telescope Luis C. Reyes KICP The Extragalactic Background Light (EBL) What is it? Accumulation of all energy releases in the form of electromagnetic radiation.

More information

Cosmic Rays. Discovered in 1912 by Viktor Hess using electroscopes to measure ionization at altitudes via balloon

Cosmic Rays. Discovered in 1912 by Viktor Hess using electroscopes to measure ionization at altitudes via balloon Cosmic Rays Discovered in 1912 by Viktor Hess using electroscopes to measure ionization at altitudes via balloon Nobel Prize in 1936 Origin of high energy cosmic rays is still not completely understood

More information

GLAST Mission: Status and Science Opportunities

GLAST Mission: Status and Science Opportunities Gamma-ray Large Area Space Telescope GLAST Mission: Status and Science Opportunities Bill Atwood SCIPP / UCSC atwood@scipp.ucsc.edu Outline GLAST: An International Science Mission Large Area Telescope

More information

Supernova Remnants and GLAST

Supernova Remnants and GLAST SLAC-PUB-14797 Supernova Remnants and GLAST Patrick Slane Harvard-Smithsonian Center for Astrophysics Abstract. It has long been speculated that supernova remnants represent a major source of cosmic rays

More information

Two recent developments with Gamma Ray Burst Classification. And their implications for GLAST. Eric Charles. Glast Science Lunch Nov.

Two recent developments with Gamma Ray Burst Classification. And their implications for GLAST. Eric Charles. Glast Science Lunch Nov. Two recent developments with Gamma Ray Burst Classification And their implications for GLAST Eric Charles Glast Science Lunch Nov. 2, 2006 Outline Numerology, taxonomy and phrenology of GRBs Salient facts

More information

IPBI-TN June 30, 2004

IPBI-TN June 30, 2004 Spray Electron Beam for Tests of Linear Collider Forward Calorimeter Detectors in SLAC End Station A R. Arnold UMass Amherst, Amherst MA 01003 T. Fieguth Stanford Linear Accelerator Center Menlo Park,

More information

GRAINE project: Cosmic Gamma-ray Observation by Balloon-Borne Telescope with Nuclear Emulsion

GRAINE project: Cosmic Gamma-ray Observation by Balloon-Borne Telescope with Nuclear Emulsion Cosmic Gamma-ray Observation by Balloon-Borne Telescope with Nuclear Emulsion Shigeki Aoki 1 Kobe University Kobe 657-8501 Japan E-mail: aoki@kobe-u.ac.jp for GRAINE collaboration Kobe University, Kobe

More information

Propagation in the Galaxy 2: electrons, positrons, antiprotons

Propagation in the Galaxy 2: electrons, positrons, antiprotons Propagation in the Galaxy 2: electrons, positrons, antiprotons As we mentioned in the previous lecture the results of the propagation in the Galaxy depend on the particle interaction cross section. If

More information

GRB Spectra and their Evolution: - prompt GRB spectra in the γ-regime

GRB Spectra and their Evolution: - prompt GRB spectra in the γ-regime GRB Spectra and their Evolution: - prompt GRB spectra in the γ-regime Andreas von Kienlin MPE -Gamma 14. November 2003 1 Outline Time averaged GRB spectra Example spectra Instrumental response Band function

More information

Search for a diffuse cosmic neutrino flux with ANTARES using track and cascade events

Search for a diffuse cosmic neutrino flux with ANTARES using track and cascade events Search for a diffuse cosmic neutrino flux with ANTARES using track and cascade events Jutta Schnabel on behalf of the ANTARES collaboration Erlangen Centre for Astroparticle Physics, Erwin-Rommel Str.

More information

Gamma rays, electrons and positrons up to 3 TeV with the Fermi Gamma-ray Space Telescope

Gamma rays, electrons and positrons up to 3 TeV with the Fermi Gamma-ray Space Telescope Journal of Physics: Conference Series Gamma rays, electrons and positrons up to 3 TeV with the Fermi Gamma-ray Space Telescope To cite this article: Philippe Bruel and on behalf of the Fermi-LAT collaboration)

More information

9/27 JUNE 2003 SUMMER STAGE PARTICLES REVELATION THROUGH CERENKOV AND SCINTILLATION COUNTER AND THE CEBAF EXPERIMENT

9/27 JUNE 2003 SUMMER STAGE PARTICLES REVELATION THROUGH CERENKOV AND SCINTILLATION COUNTER AND THE CEBAF EXPERIMENT 9/27 JUNE 2003 SUMMER STAGE PARTICLES REVELATION THROUGH CERENKOV AND SCINTILLATION COUNTER AND THE CEBAF EXPERIMENT Students: Riccardo Falcione, Elisa Paris Liceo Scientifico Statale Farnesina Tutor:

More information

Gamma Ray Physics in the Fermi era. F.Longo University of Trieste and INFN

Gamma Ray Physics in the Fermi era. F.Longo University of Trieste and INFN Gamma Ray Physics in the Fermi era F.Longo University of Trieste and INFN Vulcano, May 22, 2018 F.Longo et al. -- 1 Gamma-ray astrophysics above 100 MeV AGILE Fermi 2 Picture of the day, Feb. 28, 2011,

More information

Particle Interactions in Detectors

Particle Interactions in Detectors Particle Interactions in Detectors Dr Peter R Hobson C.Phys M.Inst.P. Department of Electronic and Computer Engineering Brunel University, Uxbridge Peter.Hobson@brunel.ac.uk http://www.brunel.ac.uk/~eestprh/

More information

SUPPLEMENTARY INFORMATION

SUPPLEMENTARY INFORMATION 1. Selecting electrons in ATIC ATIC is a calorimetric instrument and, as such, relies upon the difference in the development of the cascades (showers) initiated by protons and electrons. Moreover, the

More information

Supernova Remnants as Cosmic Ray Accelerants. By Jamie Overbeek Advised by Prof. J. Finley

Supernova Remnants as Cosmic Ray Accelerants. By Jamie Overbeek Advised by Prof. J. Finley Supernova Remnants as Cosmic Ray Accelerants By Jamie Overbeek Advised by Prof. J. Finley Cosmic Rays Discovered by Victor Hess in 1911 during a balloon flight through Austria He used an electroscope to

More information

Foundations of Astronomy 13e Seeds. Chapter 6. Light and Telescopes

Foundations of Astronomy 13e Seeds. Chapter 6. Light and Telescopes Foundations of Astronomy 13e Seeds Chapter 6 Light and Telescopes Guidepost In this chapter, you will consider the techniques astronomers use to study the Universe What is light? How do telescopes work?

More information

Using BATSE to Measure. Gamma-Ray Burst Polarization. M. McConnell, D. Forrest, W.T. Vestrand and M. Finger y

Using BATSE to Measure. Gamma-Ray Burst Polarization. M. McConnell, D. Forrest, W.T. Vestrand and M. Finger y Using BATSE to Measure Gamma-Ray Burst Polarization M. McConnell, D. Forrest, W.T. Vestrand and M. Finger y University of New Hampshire, Durham, New Hampshire 03824 y Marshall Space Flight Center, Huntsville,

More information

The cosmic-ray energy spectrum above ev measured with the LOFAR Radboud Air Shower Array

The cosmic-ray energy spectrum above ev measured with the LOFAR Radboud Air Shower Array The cosmic-ray energy spectrum above 16 ev measured with the LOFAR Radboud Air Shower Array,1, S. Buitink, A. Corstanje 1, J.E. Enriquez 1, H. Falcke 1,,4, J.R. Hörandel 1,, A. Nelles 1,5, J.P. Rachen

More information

Ultra-High-Energy Cosmic Rays: A Tale of Two Observatories

Ultra-High-Energy Cosmic Rays: A Tale of Two Observatories Ultra-High-Energy Cosmic Rays: A Tale of Two Observatories RuoYu Shang Nicholas Sherer Fei Sun Bryce Thurston Measurement of the Depth of Maximumof Extensive Air Showers above 10 18 ev,"phys. Rev. Letters104(2010)

More information

Angular Distribution of Solar Gamma Rays and Solar Neutrons Simulated by GEANT4 Program

Angular Distribution of Solar Gamma Rays and Solar Neutrons Simulated by GEANT4 Program Angular Distribution of Solar Gamma Rays and Solar Neutrons Simulated by GEANT4 Program 1), K. Koga 1), S. Masuda 2), H. Matsumoto 1), Y. Muraki 2), S. Shibata 3), and Y. Tanaka 4) 1) Tsukuba Space Centre,

More information

Neutrino Oscillations and Astroparticle Physics (5) John Carr Centre de Physique des Particules de Marseille (IN2P3/CNRS) Pisa, 10 May 2002

Neutrino Oscillations and Astroparticle Physics (5) John Carr Centre de Physique des Particules de Marseille (IN2P3/CNRS) Pisa, 10 May 2002 Neutrino Oscillations and Astroparticle Physics (5) John Carr Centre de Physique des Particules de Marseille (IN2P3/CNRS) Pisa, 10 May 2002 n High Energy Astronomy Multi-Messanger Astronomy Cosmic Rays

More information

Galactic diffuse gamma-rays

Galactic diffuse gamma-rays Galactic diffuse gamma-rays Masaki Mori Department of Physics, College of Science & Engineering, Ritsumeikan University 1 July 31, 2009, Dept. Astronomy, Kyoto University GeV gamma-ray sky by EGRET Compton

More information

Gamma-ray emission at the base of the Fermi bubbles. Dmitry Malyshev, Laura Herold Erlangen Center for Astroparticle Physics

Gamma-ray emission at the base of the Fermi bubbles. Dmitry Malyshev, Laura Herold Erlangen Center for Astroparticle Physics Gamma-ray emission at the base of the Fermi bubbles Dmitry Malyshev, Laura Herold Erlangen Center for Astroparticle Physics On behalf of the Fermi-LAT collaboration TeVPA 2018, Berlin Fermi bubbles surprise

More information

Gamma-Ray Burst Studies With the. Energetic X-ray Imaging Survey. Telescope (EXIST)

Gamma-Ray Burst Studies With the. Energetic X-ray Imaging Survey. Telescope (EXIST) Gamma-Ray Burst Studies With the Energetic X-ray Imaging Survey Telescope (EXIST) F.A. Harrison 1, N. Gehrels 2, J. E. Grindlay 3,C.J. Hailey 4, W.A. Mahoney 5, T.A. Prince 1, B.D. Ramsey 6, G.K. Skinner

More information

Neutrino induced muons

Neutrino induced muons Neutrino induced muons The straight part of the depth intensity curve at about 10-13 is that of atmospheric neutrino induced muons in vertical and horizontal direction. Types of detected neutrino events:

More information

GRB detection at ground level using Water Cerenkov Tanks

GRB detection at ground level using Water Cerenkov Tanks GRB detection at ground level using Water Cerenkov Tanks Hugo Rivera May 21, 2009 Outline 1 Gamma Ray Bursts Discovery BATSE Beppo-SAX SWIFT 2 Water Cherenkov Tanks Single Particle Technique WCD calibration

More information

Balloon-borne experiment for observation of sub-mev/mev gamma-rays from Crab Nebula using an Electron Tracking Compton Camera

Balloon-borne experiment for observation of sub-mev/mev gamma-rays from Crab Nebula using an Electron Tracking Compton Camera Balloon-borne experiment for observation of sub-mev/mev gamma-rays from Crab Nebula using an Electron Tracking Compton Camera S. Komura, T. Tanimori, H. Kubo, A.Takada, S. Iwaki, S. Kurosawa, Y. Matsuoka,

More information

AGILE Highlights. The AGILE Mission. Stefano Vercellone and the AGILE Team at IASF Milano

AGILE Highlights. The AGILE Mission. Stefano Vercellone and the AGILE Team at IASF Milano The AGILE Mission AGILE Highlights Stefano Vercellone and the AGILE Team at IASF Milano AGILE Highlights Visiting Committee Review - Milano, January 8 th, 2008 1 AGILE in a nutshell Super-AGILE AGILE-GRID

More information

Shell supernova remnants as cosmic accelerators: II

Shell supernova remnants as cosmic accelerators: II Shell supernova remnants as cosmic accelerators: II Stephen Reynolds, North Carolina State University I. Observational tools II. Radio inferences III. X ray synchrotron emission IV. MeV GeV observations

More information

PoS(NOW2016)041. IceCube and High Energy Neutrinos. J. Kiryluk (for the IceCube Collaboration)

PoS(NOW2016)041. IceCube and High Energy Neutrinos. J. Kiryluk (for the IceCube Collaboration) IceCube and High Energy Neutrinos Stony Brook University, Stony Brook, NY 11794-3800, USA E-mail: Joanna.Kiryluk@stonybrook.edu IceCube is a 1km 3 neutrino telescope that was designed to discover astrophysical

More information