The Crab Nebula as a standard candle in very high-energy astrophysics

The continuum high-energy gamma-ray emission between 1 GeV and 100 TeV from the Crab Nebula has been measured for the first time in overlapping energy bands by the Fermi large-area telescope (Fermi/LAT) below ~ 100 GeV and by ground-based imaging air Cherenkov telescopes (IACTs) above ~ 60 GeV. To follow up on the phenomenological approach suggested by Hillas et al. (1998), the broad band spectral and spatial measurement (from radio to low-energy gamma-rays < 1 GeV) is used to extract the shape of the electron spectrum. While this model per construction provides an excellent description of the data at energies < 1 GeV, the predicted inverse Compton component matches the combined Fermi/LAT and IACT measurements remarkably well after including all relevant seed photon fields and fitting the average magnetic field to B = (124 +/- 6 (stat.) +15 / -6 (sys.)) {\mu}G. The close match of the resulting broad band inverse Compton component with the combined Fermi/LAT and IACTs data is used to derive instrument specific energy-calibration factors. These factors can be used to combine data from Fermi/LAT and IACTs without suffering from systematic uncertainties on the common energy scale. As a first application of the cross calibration, we derive an upper limit to the diffuse gamma-ray emission between 250 GeV and 1 TeV based upon the combined measurements of Fermi/LAT and the H.E.S.S. ground-based Cherenkov telescopes. Finally, the predictions of the magneto-hydrodynamic flow model of Kennel & Coroniti (1984) are compared to the measured SED.

[1]  Radio emission and particle acceleration in plerionic supernova remnants , 2004, astro-ph/0405251.

[2]  Simulated synchrotron emission from pulsar wind nebulae , 2006, astro-ph/0603080.

[3]  T. Onaka,et al.  Spitzer Space Telescope Infrared Imaging and Spectroscopy of the Crab Nebula , 2006, astro-ph/0606321.

[4]  J. Chiang,et al.  THE LARGE AREA TELESCOPE ON THE FERMI GAMMA-RAY SPACE TELESCOPE MISSION , 2009, 0902.1089.

[5]  J. W. Watts,et al.  An excess of cosmic ray electrons at energies of 300–800 GeV , 2008, Nature.

[6]  G. Skinner,et al.  INTEGRAL/SPI ground calibration , 2003, astro-ph/0308504.

[7]  F. Coroniti Magnetically Striped Relativistic Magnetohydrodynamic Winds: The Crab Nebula Revisited , 1990 .

[8]  O'Dell,et al.  Discovery of Spatial and Spectral Structure in the X-Ray Emission from the Crab Nebula , 2000, The Astrophysical journal.

[9]  The Crab Nebula's Wisps in Radio and Optical , 2004, astro-ph/0408061.

[10]  et al,et al.  Probing the ATIC peak in the cosmic-ray electron spectrum with H.E.S.S. , 2009, 0905.0105.

[11]  J. Graham,et al.  Infrared and optical imagery of the Crab Nebula , 1989 .

[12]  Felix Aharonian,et al.  The Crab Nebula and Pulsar between 500 GeV and 80 TeV: Observations with the HEGRA Stereoscopic Air Cerenkov Telescopes , 2004 .

[13]  E. Amato,et al.  Axially symmetric relativistic MHD simulations of Pulsar Wind Nebulae in Supernova Remnants. On the origin of torus and jet-like features , 2004, astro-ph/0404355.

[14]  Particle acceleration and relativistic shocks , 1999, astro-ph/9905069.

[15]  D. A. Green,et al.  Far-infrared and submillimetre observations of the Crab nebula , 2004, astro-ph/0409469.

[16]  A. R. Bazer-Bachi,et al.  Energy spectrum of cosmic-ray electrons at TeV energies. , 2008, Physical review letters.

[17]  D. N. Burrows,et al.  Spatial Variation of the X-Ray Spectrum of the Crab Nebula , 2004 .

[19]  J. Aumont,et al.  GLOBAL SPECTRAL ENERGY DISTRIBUTION OF THE CRAB NEBULA IN THE PROSPECT OF THE PLANCK SATELLITE POLARIZATION CALIBRATION , 2008, 0802.0412.

[20]  O. Skjaeraasen,et al.  The Sigma Problem of the Crab Pulsar Wind , 2003, astro-ph/0309573.

[21]  C. Kennel,et al.  Confinement of the Crab pulsar's wind by its supernova remnant , 1984 .

[22]  R. Chevalier,et al.  Shocked relativistic magnetohydrodynamic flows with application to pulsar winds , 1987 .

[23]  F. Aharonian,et al.  On the mechanisms of gamma radiation in the Crab Nebula , 1996 .

[24]  S. Komissarov,et al.  Synchrotron nebulae created by anisotropic magnetized pulsar winds , 2004 .

[25]  J. Arons,et al.  Time Dependence in Relativistic Collisionless Shocks: Theory of the Variable “Wisps” in the Crab Nebula , 2004, astro-ph/0402123.

[26]  Astrophysics,et al.  On the X-ray image of the Crab nebula: comparison with Chandra observations , 2003 .

[27]  L. Zhang,et al.  Nonthermal Radiation from Pulsar Wind Nebulae , 2008 .

[28]  Giuseppe Vacanti,et al.  The Spectrum of TeV Gamma Rays from the Crab Nebula , 1997 .

[29]  G. Blumenthal,et al.  BREMSSTRAHLUNG, SYNCHROTRON RADIATION, AND COMPTON SCATTERING OF HIGH- ENERGY ELECTRONS TRAVERSING DILUTE GASES. , 1970 .

[30]  O. C. de Jager,et al.  The expected high-energy to ultra-high-energy gamma-ray spectrum of the Crab Nebula , 1992 .

[31]  J. Roques,et al.  THE HIGH-ENERGY EMISSION OF THE CRAB NEBULA FROM 20 keV TO 6 MeV WITH INTEGRAL SPI , 2009, 0909.3437.

[32]  J. J. Hester,et al.  The Crab Nebula: An Astrophysical Chimera , 2008 .

[33]  D. A. Green,et al.  Far-infrared and sub-mm observations of the Crab nebula , 2004 .

[34]  Matthew D. Kistler,et al.  Gamma-ray signatures of annihilation to charged leptons in dark matter substructure , 2009, 0909.0519.

[35]  K. Davidson Spectrophotometry of the Crab Nebula as a whole , 1987 .

[36]  R. Fesen,et al.  Recent Developments Concerning the Crab Nebula , 1985 .

[37]  W. BednarekM. Bartosik Gamma-rays from the pulsar wind nebulae , 2003 .

[38]  E. Amato,et al.  Non-thermal emission from relativistic MHD simulations of pulsar wind nebulae , 2008 .

[39]  V. Trimble Motions and Structure of the Filamentary Envelope of the Crab Nebula , 1968 .

[40]  R. Gehrz,et al.  Nucleosynthesis in Classical Novae and Its Contribution to the Interstellar Medium , 1998 .

[41]  J. Gunn,et al.  The Origin of the Magnetic Field and Relativistic Particles in the Crab Nebula , 1974 .

[42]  M. Bietenholz,et al.  The magnetic field of the Crab Nebula and the nature of its jet , 1990 .