XMM-Newton observations of the first unidentified TeV gamma-ray source TeV J2032+4130

• Published in: Astronomy and astrophysics (Berlin) Vol. 469; no. 1; pp. L17 - L21
• Main Authors: Horns, D., Hoffmann, A. I. D., Santangelo, A., Aharonian, F. A., Rowell, G. P.
• Format: Journal Article
• Language: English
• Published: Les Ulis EDP Sciences 01.07.2007
• Subjects: Astronomy; Earth, ocean, space; Exact sciences and technology; X ray observation; Angular dimension; Thermal electron; X-rays: general; Energy spectra; acceleration of particles; X ray counterpart; Particle acceleration; Radio observation; gamma rays: observations; TeV range; Point sources; gamma rays: theory; Gamma radiation; Gamma ray source; Emission spectra; Positions; Models; Power law; Plasma temperature; Energy transfer; Very high energy; X ray emission
• ISSN: 0004-6361; 1432-0746
• DOI: 10.1051/0004-6361:20066836

Context. The first unidentified very high energy gamma ray source (TeV J2032+4130) in the Cygnus region has been the subject of intensive search for a counterpart source at other wavelengths. In particular, observations in radio and X-rays are important to trace a population of non- thermal electrons. Aims. A deep (\approx50 ks) exposure of TeV J2032+4130 with XMM-Newton has been obtained. The large collection area and the field of view of the X-ray telescopes on-board of XMM-Newton allow to search for faint extended X-ray emission possibly linked to TeV J2032+4130. Methods. The contribution of point sources to the observed X-ray emission from TeV J2032+4130 is subtracted from the data. The point-source subtracted X-ray data are analyzed using blank sky exposures and regions adjacent to the position of TeV J2032+4130 in the field of view covered by the XMM-Newton telescopes to search for diffuse X-ray emission. Results. An extended X- ray emission region with a full width half maximum ( FWHM) size of \approx12 arcmin is found. The centroid of the emission is co-located with the position of TeV J2032+4130. The angular extension of the X-ray emission region is slightly smaller than the angular size of TeV J2032+4130 ( FWHM =14 \pm 3 arcmin). The energy spectrum of the emission coinciding with the position and extension of TeV J2032+4130 can be modeled by a power-law model with a photon index \Gamma=1.5 \pm 0.2 _{\rm stat} \pm 0.3 _{\rm sys} and an energy flux integrated between 2 and 10 keV of f_{2-10 similar to {\rm keV}} \approx 7\times10 super(-13) erg/(cm super(2) s) which is lower than the very high energy gamma-ray flux observed from TeV J2032+4130. The energy flux detected from the extended emission region is about a factor of two smaller than the summed contribution of the point sources present. The energy spectrum can also be fit with a thermal emission model from an ionized plasma with a temperature k_{\rm B}T\approx 10 keV. Conclusions. We conclude that the faint extended X-ray emission discovered in this observation is the X-ray counterpart of TeV J2032+4130. Formally, it can not be excluded that the extended emission is due to an unrelated population of faint, hot (k_{\rm B}T\approx 10 keV) unresolved point-sources which by chance coincides with the position and extension of TeV J2032+4130. We discuss our findings in the frame of both hadronic and leptonic gamma-ray production scenarios.