Chandra observations of the HII complex G5.89-0.39 and TeV gamma-ray source HESSJ1800-240B
- 1. School of Chemistry & Physics, University of Adelaide, Adelaide 5005 (Australia)
- 2. Max Planck Institüt für Kernhysik, P.O. Box 103980, D 69029 Heidelberg (Germany)
- 3. Institut fuer Experimental Physik, Universitaet Hamburg, Luruper Chausse 149, D22761 Hamburg (Germany)
- 4. Department of Physics, Rikkyo University, 3-34-1 Nishi-Ikebukuro, Toshima-ku, Tokyo, 171-8501 (Japan)
- 5. Landessternwarte, Universitaet Heidelberg, Koenigtuhl, D69117 Heidelberg (Germany)
Description
We present the results of our investigation, using a Chandra X-ray observation, into the stellar population of the massive star formation region G5.89-0.39, and its potential connection to the coincident TeV gamma-ray source HESSJ1800-240B. G5.89-0.39 comprises two separate HII regions G5.89-0.39A and G5.89-0.39B (an ultra-compact HII region). We identified 159 individual X-ray point sources in our observation using the source detection algorithm wavdetect. 35 X-ray sources are associated with the HII complex G5.89-0.39. The 35 X-ray sources represent an average unabsorbed luminosity (0.3–10 keV) of , typical of B7–B5 type stars. The potential ionising source of G5.89-0.39B known as Feldt's star is possibly identified in our observation with an unabsorbed X-ray luminosity suggestive of a B7–B5 star. The stacked energy spectra of these sources is well-fitted with a single thermal plasma APEC model with kT ∼ 5 keV, and column density (). The residual (source-subtracted) X-ray emission towards G5.89-0.39A and B is about 30% and 25% larger than their respective stacked source luminosities. Assuming this residual emission is from unresolved stellar sources, the total B-type-equivalent stellar content in G5.89-0.39A and B would be 75 stars, consistent with an earlier estimate of the total stellar mass of hot stars in G5.89-0.39. We have also looked at the variability of the 35 X-ray sources in G5.89-0.39. Ten of these sources are flagged as being variable. Further studies are needed to determine the exact causes of the variability, however the variability could point towards pre-main sequence stars. Such a stellar population could provide sufficient kinetic energy to account for a part of the GeV to TeV gamma-ray emission in the source HESSJ1800-240B. However, future arc-minute angular resolution gamma-ray imaging will be needed to disentangle the potential gamma-ray components powered by G5.89-0.39 from those powered by the W28 SNR.
Availability note (English)
Available from http://dx.doi.org/10.1016/j.jheap.2016.05.001Additional details
Identifiers
- DOI
- 10.1016/j.jheap.2016.05.001;
- arXiv
- arXiv:1606.08138v1;
- PII
- S221440481630009X;
Publishing Information
- Journal Title
- Journal of High Energy Astrophysics (Print)
- Journal Volume
- 11
- Journal Page Range
- p. 1-19
- ISSN
- 2214-4048
INIS
- Country of Publication
- Netherlands
- Country of Input or Organization
- International Atomic Energy Agency (IAEA)
- INIS RN
- 51081272
- Subject category
- S79: ASTROPHYSICS, COSMOLOGY AND ASTRONOMY;
- Descriptors DEI
- DETECTION; ENERGY SPECTRA; GAMMA RADIATION; GEV RANGE; H2 REGIONS; LUMINOSITY; MAIN SEQUENCE STARS; POINT SOURCES; POTENTIALS; TEV RANGE; X RADIATION; X-RAY SOURCES
- Descriptors DEC
- COSMIC RADIO SOURCES; ELECTROMAGNETIC RADIATION; ENERGY RANGE; IONIZING RADIATIONS; OPTICAL PROPERTIES; PHYSICAL PROPERTIES; RADIATION SOURCES; RADIATIONS; SPECTRA; STARS
Optional Information
- Copyright
- Copyright (c) 2016 Elsevier B.V.