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

Similar documents
Pulsar Observations with the Fermi Large Area Telescope

Fermi-Large Area Telescope Observations of Pulsar Wind Nebulae and their associated pulsars

Fermi Large Area Telescope:

Radio counterparts of gamma-ray pulsars

Sources of GeV Photons and the Fermi Results

Gamma-ray observations of millisecond pulsars with the Fermi LAT. Lucas Guillemot, MPIfR Bonn. NS2012 in Bonn 27/02/12.

Pulsar Wind Nebulae as seen by Fermi-Large Area Telescope

Future Gamma-Ray Observations of Pulsars and their Environments

Particle acceleration and pulsars

Remnants and Pulsar Wind

Fermi-LAT and WMAP observations of the SNR Puppis A

A Detailed Study of. the Pulsar Wind Nebula 3C 58

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

Gamma-Ray. Pulsars in the. Les Pulsars gamma avec GLAST. NASA Goddard Space Flight Center. David Smith Centre d Etudes Nucléaires de BordeauxGradignan

H.E.S.S. Unidentified Gamma-ray Sources in a Pulsar Wind Nebula Scenario And HESS J

Cooling Limits for the

A pulsar wind nebula associated with PSR J as the powering source of TeV J

arxiv:astro-ph/ v1 16 Oct 2003

HAWC Observation of Supernova Remnants and Pulsar Wind Nebulae

The Fermi Large Area Telescope View of Gamma-ray Pulsars

Radio Observations of TeV and GeV emitting Supernova Remnants

Search for Pulsed Emission in Archival VERITAS Data

Fermi: Highlights of GeV Gamma-ray Astronomy

Discovery of TeV Gamma-ray Emission Towards Supernova Remnant SNR G Last Updated Tuesday, 30 July :01

Fermi-LAT Searches for gamma-ray pulsars

discovers a radio-quiet gamma-ray millisecond Journal Group

TeV Galactic Source Physics with CTA

New Radio Millisecond Pulsars in Fermi (formerly) Unassociated Sources

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

HESS J : A new gamma-ray binary?

Particle acceleration during the gamma-ray flares of the Crab Nebular

Recent Observations of Supernova Remnants

Detecting New Sources of High-Energy Gamma Rays

Pulsar Wind Nebulae: A Multiwavelength Perspective

Les Pulsars gamma. avec GLAST

PoS(extremesky2009)023

X-ray Observations of Rotation Powered Pulsars

CTB 37A & CTB 37B - The fake twins SNRs

Science of Compact X-Ray and Gamma-ray Objects: MAXI and GLAST

The annular gap model: radio and Gamma-ray emission of pulsars. Qiao,G.J. Dept. of Astronomy, Peking Univ.

Rotating RAdio Transients (RRATs) ApJ, 2006, 646, L139 Nature, 2006, 439, 817 Astro-ph/

Status of the MAGIC telescopes

Pulsars and Pulsar-Wind Nebulae: TeV to X-Ray Connection. Oleg Kargaltsev (University of Florida) George Pavlov (Penn State University)

e - -e + pair production in pulsar magnetospheres

arxiv: v1 [astro-ph] 14 Jul 2008

Observations of. Pulsar Wind Nebulae

On the Spectral Shape of Gamma-ray Pulsars Above the Break Energy

Aldo Morselli INFN Roma Tor Vergata On behalf of Marco Tavani and the AGILE Team

A pulsar wind nebula associated with PSR J as the powering source of TeV J

Pulsar Astronomy with GLAST Steve Thorsett UC Santa Cruz GLAST

Les Pulsars gamma. avec GLAST

A-Exam: e + e Cosmic Rays and the Fermi Large Array Telescope

Progress in Pulsar detection

Supernova Remnants and GLAST

X-ray emission properties vary with spin-down age. Crab-like pulsars (< 10 4 yrs)

Supernova Remnants and Pulsar Wind Nebulae observed in TeV γ rays

Observations of Gamma ray Spiders with the Fermi Large Area Telescope

Non-thermal emission from pulsars experimental status and prospects

Neutron Star Laboratory

VHE γ-ray emitting pulsar wind nebulae discovered by H.E.S.S.

Shell supernova remnants as cosmic accelerators: II

Fermi Gamma Ray Space Telescope: Launch+509. Roger Blandford KIPAC Stanford (With considerable help from Fermi team members working at Stanford)

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

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

astro-ph/ Dec 94

Observing Galactic Sources at GeV & TeV Energies (A Short Summary)

Galactic Variable Sky with EGRET and GLAST. S. W. Digel. Stanford Linear Accelerator Center 2575 Sand Hill Road Menlo Park, CA 94025

Lecture 3 Pulsars and pulsar wind nebulae

High time resolution observations of millisecond pulsars with the Fermi Large Area Telescope

Observations of the Crab Nebula. Elizabeth Hays. Wednesday, October 30, 13

The Fermi Gamma-ray Space Telescope

TeV Gamma Rays from Synchrotron X-ray X

Interstellar gamma rays. New insights from Fermi. Andy Strong. on behalf of Fermi-LAT collaboration. COSPAR Scientific Assembly, Bremen, July 2010

Cosmic Ray Electrons and GC Observations with H.E.S.S.

VERITAS Observations of Supernova Remnants

Gamma-ray Astrophysics and High Density e+ e- Plasma - A new application of Free Electron Laser? -

Search for pulsar wind nebula associations with unidentified TeV gamma-ray sources

Potential Neutrino Signals from Galactic γ-ray Sources

Fermi LAT data analysis

Creative Commons: Attribution 3.0 Hong Kong License

The High-Energy Interstellar Medium

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

PIC modeling of particle acceleration and high-energy radiation in pulsars

Gamma-ray Astrophysics

Recent Results from VERITAS

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

T. J. Brandt. CRISM: 27 Jun On behalf of the Fermi- LAT Collabora:on IRAP/Université Paul Saba:er.

Galactic Accelerators : PWNe, SNRs and SBs

On the scientific motivation for a wide field-of-view TeV gamma-ray observatory in the Southern Hemisphere

X-ray and Gamma-ray. Emission Pulsars and Pulsar Wind Nebulae. K.S. Cheng Department of Physics University of Hong Kong Hong Kong, China

A New Look at the Galactic Diffuse GeV Excess

Galactic sources in GeV/TeV Astronomy and the new HESS Results

HESS discovery of VHE γ-ray emission of a remarkable young composite SNR

PERSPECTIVES of HIGH ENERGY NEUTRINO ASTRONOMY. Paolo Lipari Vulcano 27 may 2006

Calibration of the AGILE Gamma Ray Imaging Detector

arxiv: v1 [astro-ph.he] 5 Sep 2017

A New View of the High-Energy γ-ray Sky with the Fermi Telescope

Pulsars with MAGIC. Jezabel R. Garcia on behalf of the MAGIC collaboration

X-ray Properties of Rotation Powered Pulsars and Thermally Emitting Neutron Stars

Gamma-ray binaries as pulsars spectral & variability behaviour Guillaume Dubus. Laboratoire d Astrophysique de Grenoble UMR 5571 UJF / CNRS

Transcription:

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 J2229+6114 2. What does the flux teach us? 3. Instrument Response Functions 4. How to access the source flux with Fermi? 5. Vela & J2021+3651 spectrum 2

Young pulsars, our best candidates Above some value Edot, gamma-ray emitting electron-positron cascades occur (Arrons 1996). We have listed 224 best gamma-ray pulsar candidates with Edot > 1e34 erg/s (Smith et al. 2008) astro-ph/0810.1637 : Young, energetic and noisy pulsars The most energetic of the known galactic pulsar are : Crab : 4.6e+38 erg/s J1833-1034 : 3.4e+37 erg/s J0205+6449 : 2.7e+37 erg/s J2229+6114 : 2.2e+37 erg/s 3 First Light Image of the LAT Fermi telescope

Young pulsars, J0205+6449 (1) This very young pulsar in the SNR 3C58 was detected in radio after the end of CGRO. F. Camilo et al, Ap J Lett 571, 41-44 (2002). The radio discovery was made possible by the Chandra X-ray discovery of the pulsar shortly before that (Murray et al 2002). With a real weak signal in radio: ~45 ujy at 1400 MHz. Associated to the SNR and the PWN 3C58, the system is the possible remnant of the SN 1181. It has a whopping spin down energy (Crab/15) of 2.7e37 erg/s Optical image of 3C 58 Fesen et al. 2008 VLA images Slane et al. 2008 4

Young pulsars, J0205+6449 (2) An archival observation of RXTE has confirmed the periodic signal of PSR J0205+6449 (image). Estimated characteristic age ~ 5.37e+03 years Estimated distance ~ 3.2 kpc P ~65.7 ms, Pdot ~ 1.93e-13 Estimated surface B ~ 3.61e+12 Image of 3C 58 at 1.4 GHz. The arrow marks the position of the pusar BietenHolz 2006 5

J2229+6114 The high Edot (2.2e37 erg/s) pulsar was discovered at the end of the CGRO mission (2001). Halpern, J. P., Camilo, F., Gotthelf, E. V., Helfand, D. J., Kramer, M., Lyne, A. G., Leighly, K. M. & Eracleous, M., 2001. PSR J2229+6114: Discovery of an Energetic Young Pulsar in the Error Box of the EGRET Source 3EG J2227+6122. Associated to the unidentified 3EG J2227+6122 and to the SNR G106.3+2.7, surrounded by an X-ray PWN. Halpern, J. P.; Gotthelf, E. V.; Camilo, F.; Collins, B.; Helfand, D. J.The New Gamma-ray Pulsar PSR J2229+6114, its Pulsar Wind Nebula, and Comparison with the Vela Pulsar X-ray pulsations Estimated age ~ 1e+04 years Estimated distance ~ 7.25 kpc P ~ 51.6 ms, Pdot ~ 7.83e-14 Estimated surface B ~ 2e+12 G Chandra ACIS-I image showing the pulsar and its associated PWN (greyscale). 6

A search in EGRET data Best EGRET light curve for PSR J2229+6114. After taking N trials into account, the statistical significance of a positive detection is low, and no detection is claimed. Thompson, Reimer, Digel and Nolan, ASP Conference Series, arxiv:astro-ph/0112518 (2002) 7

What does the flux teach us? How and where are particles accelerated in the pulsar magnetosphere? beam geometry phase resolved spectra altitude of acceleration & radiation spectral cut-offs Efficiency : rate for converting its rotational energy loss into gamma-rays Emission comparison : Maximum of emission in the hard Xand γ-ray range Radio beam is a small fraction of emitted energy 8

Instrument response functions - IRF (1) Large Area Telescope Effective area < Geometric surface Gamma = no Gamma = yes Tracker LAT picture Calorimeter Point Spread Funtion theta Mutiple scattering Gamma-ray Burst Monitor (GBM) 9

Instrument response functions - IRF (2) Point spread function ~ 0.5, 68% containment radius at 1 GeV Surface effective ~ 8000 cm² on axis Energy resolution Basically, Nnumber of photons = ʃ Flux(E) x IRF(E) de 10

Instrument performance et al. Point source sensitivity : Integral sensitivity plot (5-sigma sensitivity for E>E0), assuming a 1/E2 spectrum source at high latitude. Comparison between the EGRET and LAT location for CTA1 11

How to compute the point source flux with Fermi? A set of tools were built to analyse the Fermi LAT data : gtselect, gtbin, gtlike, Glast Tools These tools handle FITS files, the standard astronomical data format. Data will be public on the 2009 August 11 Link to the page : http://fermi.gsfc.nasa.gov/ssc/data/analysis/sae_overview.html 12

Vela spectrum Spectrum from the new paper : Fermi Lat Observations of the Vela Pulsar (Abdo et al. 2008) (ApJ submittted) This phase-averaged gammaray energy spectrum can be represented by a power law with a exponential cut-off at 3 GeV According to this result, polar cap model are excluded. Phase-averaged Vela spectral energy distribution 13

J2021+3651 spectrum from AGILE Phase-averaged spectrum for J2021+3651 (Halpern et al. 2008) The energy range 100-1000 is fitted with a power law of photon index g = 1.86+/-0.18, while a turndown is seen above 1.5 GeV. 14

Conclusions Our best gamma-ray pulsar candidates are young, energetic and noisy The instrument performance are still under investigations but are in agreeement with our current simulation of the LAT response. The spectral analysis is a link to understand where and how are particles accelerated in the pulsar magnetosphere : polar cap models are excluded for the Vela pulsar 15

16

What does the flux teach us? How and where are particles accelerated in the pulsar magnetosphere? beam geometry phase resolved spectra altitude of acceleration & radiation spectral cut-offs Efficiency : rate for converting its rotational energy loss into gamma-rays ref 17

Multi-wavelength spectra of EGRET pulsars Emission comparison : Maximum of emission in the hard X- and γ-ray range Radio beam is a small fraction of emitted energy Spectra are very different above 1 GeV High energy spectral cutoffs 18

Models of gamma-ray emission for the pulsars Where do γ-rays come from? Outer gap, polar cap or slot gap? Discrimination between models Different models predict different spectral cutoff. Measuring the spectral tail is possible to distinguish between models. 19