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arXiv 1002.0229hep-phastro-ph.GA
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射电和gamma-ray对银河系中心暗物质湮灭的限制

Radio and gamma-ray constraints on dark matter annihilation in the Galactic center

Roland M. Crocker, Nicole F. Bell, Csaba Balázs, David I. Jones

摘要:

对于湮没导致电子-正电子对产生的情况,我们确定了暗物质(DM)自湮没截面的上限。在银河系中心(GC),相对论性电子和正电子通过同步辐射产生射电通量,并通过韧致辐射和逆康普顿散射产生伽马射线通量。根据档案、干涉测量和单碟射电数据,我们确定了银河系中心周围3度半长轴(沿银河系平面)和1度半短轴的椭圆区域的射电频谱,以及第二个矩形区域,也以GC为中心,范围为1.6度x0.6度。这两个地区的无线电频谱在我们有数据的频率范围内是非热的:74 MHz - 10 GHz。我们还考虑伽马射线数据覆盖同一地区的EGRET仪器(约GeV)和HESS(约TeV)。我们展示了如何将这些数据的组合,可以用来放置强大的DM湮灭的情况下,在某种程度上,这是相对不敏感的假设在该地区的磁场振幅的约束。我们的结果是大约一个数量级的限制比现有的银河系中心的无线电和伽马射线的限制。对于质量为m_x =10 GeV的DM和NFW分布,我们发现速度平均截面必须小于10^-25 cm ^3·s^-1的数倍。

英文摘要:

We determine upper limits on the dark matter (DM) self-annihilation cross section for scenarios in which annihilation leads to the production of electron--positron pairs. In the Galactic centre (GC), relativistic electrons and positrons produce a radio flux via synchroton emission, and a gamma ray flux via bremsstrahlung and inverse Compton scattering. On the basis of archival, interferometric and single-dish radio data, we have determined the radio spectrum of an elliptical region around the Galactic centre of extent 3 degrees semi-major axis (along the Galactic plane) and 1 degree semi-minor axis and a second, rectangular region, also centered on the GC, of extent 1.6 degrees x 0.6 degrees. The radio spectra of both regions are non-thermal over the range of frequencies for which we have data: 74 MHz -- 10 GHz. We also consider gamma-ray data covering the same region from the EGRET instrument (about GeV) and from HESS (around TeV). We show how the combination of these data can be used to place robust constraints on DM annihilation scenarios, in a way which is relatively insensitive to assumptions about the magnetic field amplitude in this region. Our results are approximately an order of magnitude more constraining than existing Galactic centre radio and gamma ray limits. For a DM mass of m_χ=10 GeV, and an NFW profile, we find that the velocity-averaged cross-section must be less than a few times 10^-25 cm^3 s^-1.

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