论文标题

从弥漫性超新星通量的轴突样颗粒上的边界

Bounds on axion-like particles from the diffuse supernova flux

论文作者

Calore, Francesca, Carenza, Pierluca, Giannotti, Maurizio, Jaeckel, Joerg, Mirizzi, Alessandro

论文摘要

从过去的所有核心折叠超新星(SNE)中的轴状颗粒(ALP)的累积发射将导致带有能量$ {\ MATHCAL O}(50)$ MEV的扩散通量。我们使用它来限制以耦合为特征的阿尔卑斯山和光子和核子。仅与光子耦合的阿尔卑斯山通过Primakoff工艺在SN核中产生,然后转换为银河磁场中的γ射线。我们设置了$ g_ {aγ} \ Lessim 5 \ times 10^{ - 10}〜{\ rm gev}^{ - 1} $ for $ m_a \ lyseSim 10^{ - 11}}〜{\ rm ev} $,使用diffuse gamma-ray comporter of diffuse compers op comport fiff comport fiffuse comport fiff comma-ray compore flors flers formi flers formi force。但是,如果阿尔卑斯山与核子也与核子夫妇一起,则由于阿尔卑斯核核子核子Bremsstrahlung工艺,它们的SN生产率可以大大提高。假设从现象学上允许最大的ALP核子耦合,则弥漫性伽马射线通量的界限会导致更强的$ g_ {aγ} \ lyseSim 6 \ times 10^{ - 13}〜{\ rm gev}^{\ rm gev}^{ - 1}^{ - 1} $ for同一质量范围。如果阿尔卑斯山比$ \ sim $ keV重,那么对光子的衰减会变得很大,再次导致弥漫性伽马射线通量。在仅光子耦合的情况下,我们发现,例如$ g_ {aγ} \ sillsim 5 \ times 10^{ - 11}〜{\ rm gev}^{ - 1} $ for $ m_a \ sim \ sim 5〜 {\ rm kev} $。允许(最大)与核子耦合,极限提高到$ g_ {aγ} \ lyseSim 10^{ - 19}〜{\ rm gev}^{ - 1} $ for $ m_a \ sim \ sim 20〜 {\ rmmev} $,代表强生于日期。

The cumulative emission of Axion-Like Particles (ALPs) from all past core-collapse supernovae (SNe) would lead to a diffuse flux with energies ${\mathcal O}(50)$ MeV. We use this to constrain ALPs featuring couplings to photons and to nucleons. ALPs coupled only to photons are produced in the SN core via the Primakoff process, and then converted into gamma rays in the Galactic magnetic field. We set a bound on $g_{aγ} \lesssim 5 \times 10^{-10}~{\rm GeV}^{-1}$ for $m_a \lesssim 10^{-11}~{\rm eV}$, using recent measurements of the diffuse gamma-ray flux observed by the Fermi-LAT telescope. However, if ALPs couple also with nucleons, their production rate in SN can be considerably enhanced due to the ALPs nucleon-nucleon bremsstrahlung process. Assuming the largest ALP-nucleon coupling phenomenologically allowed, bounds on the diffuse gamma-ray flux lead to a much stronger $g_{aγ} \lesssim 6 \times 10^{-13}~{\rm GeV}^{-1}$ for the same mass range. If ALPs are heavier than $\sim$ keV, the decay into photons becomes significant, leading again to a diffuse gamma-ray flux. In the case of only photon coupling, we find, e.g. $g_{aγ} \lesssim 5 \times 10^{-11}~{\rm GeV}^{-1}$ for $m_a \sim 5~{\rm keV}$. Allowing for a (maximal) coupling to nucleons, the limit improves to the level of $g_{aγ} \lesssim 10^{-19}~{\rm GeV}^{-1}$ for $m_a \sim 20~{\rm MeV}$, which represents the strongest constraint to date.

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