Nuclear gamma-ray lines from low-energy cosmic rays
Predicted gamma-ray emission from the inner galaxy (|l| < 60°, (|b| < 10°) compared to data from CGRO/COMPTEL and Fermi/LAT. The hadronic emission is produced by a wealth of nuclear de-excitation lines below 10 MeV and by pion decay at higher energies. Credit: J. Kiener et al. |
Required instrument performances:
The diffuse emission is certainly concentrated in the Galactic plane with a longitudinal profile following roughly the H2 column density with eventual concentrations around acceleration sites. A large field-of-view is necessary for the observation of diffuse emission, ideally covering the inner Galaxy (longitude |l| < 60°). The required energy resolution is of the order of the width of the strongest lines at 4.4 and 6.1 MeV, ΔE ~ 100 keV. The angular resolution should be of the order of the Galactic latitude profile of the emission, i.e. about 1o. The brightness of the 4.4-MeV narrow line from the inner Galaxy is expected to be in the range (0.2 – 2) × 10-5 cm-2 s-1 sr-1 and the broadband emission (in the energy ranges 1 – 3 and 3 – 8 MeV) is about ten times brighter.
Performance parameter | Goal value | Remarks and notes |
Field-of-view (FWHM, deg) |
2 sr | |
Angular resolution (FWHM, deg) |
1 | |
Spectral resolution (ΔE/E @ Energy) |
0.02 @ 5 MeV | |
Line sensitivity (@ Energy) (cm-2 s-1, 3σ, 1 Ms) |
~10-5 @ 5 MeV | Diffuse emission. To detect the line from the inner Galaxy. |
Continuum sensitivity (in which energy band?) (cm-2 s-1 keV-1, ΔE=E, 3σ, 1 Ms) |
2×10-8 @ 1-8 MeV | Diffuse emission. To map the broadband emission from the inner Galaxy. |
Timing performances | - | |
Polarimetric capability (Minimum Polarization Fraction for a Crab source in 1 Ms) |
- |
|
Real-time data? | no |