Table E.1
Best-fit coefficients of the γ-ray models (q for each energy band) and of the dust models (y) for the γ + AVQ (top), γ + τ353 (middle), and γ + R (bottom) analyses.
Energy band | qHI Cha | qHI IVA | qHI Gal | qCOa | qDNMb1 | qIC | qiso |
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102.6–102.8 MeV .............. |
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102.8–103.2 MeV.............. |
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103.2–103.6 MeV.............. |
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103.6–105.0 MeV.............. |
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102.6–105.0 MeV.............. |
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y HI Cha c1 | y HI IVA c1 | y HI Gal c1 | y CO d1 | y DNM c1 | y iso e1 | ||
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Energy band | qHI Cha | qHI IVA | qHI Gal | qCOa | qDNMb2 | qIC | qiso |
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102.6–102.8 MeV.............. |
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102.8–103.2 MeV.............. |
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103.2–103.6 MeV.............. |
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103.6–105.0 MeV.............. |
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102.6–105.0 MeV.............. |
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y HI Cha c2 | y HI IVA c2 | y HI Gal c2 | y CO d2 | y DNM c2 | y iso e2 | ||
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Energy band | q HI Cha | q HI IVA | q HI Gal | q CO a | q DNM b3 | q IC | q iso |
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102.6–102.8 MeV.............. |
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102.8–103.2 MeV.............. |
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103.2–103.6 MeV.............. |
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103.6–105.0 MeV.............. |
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102.6–105.0 MeV.............. |
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y HI Cha c3 | y HI IVA c3 | y HI Gal c3 | y CO d3 | y DNM c3 | y iso e3 | ||
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Notes. The first uncertainties are statistical, the second result from changes in H i spin temperature over the 2σ confidence interval from the optically thin case. The latter do not include the 8% systematic uncertainty in the LAT sensitive area for the q parameters. Model uncertainties have been used to optimize the dust fits.
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