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Title: Measurement of the Multi-T{bold e}V Gamma-Ray Flare Spectra of Markarian 421 and Markarian 501

Journal Article · · Astrophysical Journal
DOI:https://doi.org/10.1086/306677· OSTI ID:347038
 [1];  [2];  [3];  [4];  [3];  [4];  [5];  [3];  [4]; ;  [1];  [6];  [4]; ; ;  [7];  [3];  [8];  [7];  [4] more »;  [9];  [1]; « less
  1. Department of Physics and Astronomy, Iowa State University, Ames, IA 50011-3160 (United States)
  2. Department of Physics, Oxford University, Oxford, England (United Kingdom)
  3. Department of Physics, University of Leeds, Leeds, LS2 9JT, England (United Kingdom)
  4. Experimental Physics Department, University College, Belfield, Dublin 4 (Ireland)
  5. Department of Physics, Washington University, St. Louis, MO 63130 (United States)
  6. Physics Department, National University of Ireland, Maynooth (Ireland)
  7. Department of Physics, Purdue University, West Lafayette, IN 47907 (United States)
  8. Space Radiation Laboratory, California Institute of Technology, Pasadena, CA 91125 (United States)
  9. Department of Physics, University of Utah, Salt Lake City, UT 84112 (United States)

The energy spectrum of Markarian 421 in flaring states has been measured from 0.3 to 10 TeV using both small and large zenith angle observations with the Whipple Observatory 10 m imaging telescope. The large zenith angle technique is useful for extending spectra to high energies, and the extraction of spectra with this technique is discussed. The resulting spectrum of Markarian 421 is fitted reasonably well by a simple power law: J(E)=E{sup {minus}2.54{plus_minus}0.03{plus_minus}0.10} photons m{sup {minus}1} s{sup {minus}1} TeV{sup {minus}1}, where the first set of errors is statistical and the second set is systematic. This is in contrast to our recently reported spectrum of Markarian 501, which over a similar energy range has substantial curvature. The differences in TeV energy spectra of gamma-ray blazars reflect both the physics of the gamma-ray production mechanism and possibly differential absorption effects at the source or in the intergalactic medium. Since Markarian 421 and Markarian 501 have almost the same redshift (0.031 and 0.033, respectively), the difference in their energy spectra must be intrinsic to the sources and not due to intergalactic absorption, assuming the intergalactic infrared background is uniform. {copyright} {ital {copyright} 1999.} {ital The American Astronomical Society}

OSTI ID:
347038
Journal Information:
Astrophysical Journal, Vol. 511, Issue 1; Other Information: PBD: Jan 1999
Country of Publication:
United States
Language:
English

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