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Table 1:

Constraints on PBHs of mass $M_{\star }$ for different dark matter distributionsa.
DM distribution $f(M_{\star})$ $\Omega_{\rm PBH}(M_{\star})$ $\beta(M_\star)$
Moore $ 6.04 \pm 0.05\times 10^{-9}$ $1.38\times 10^{-9}$ $0.98\times 10^{-27}$
Moore$_{\rm c}$ $ 1.07 \pm 0.07\times 10^{-9}$ $0.24\times 10^{-9}$ $0.17\times 10^{-27}$
NFW $ 6.70 \pm 0.05\times 10^{-9}$ $1.53\times 10^{-9}$ $1.08\times 10^{-27}$
NFW$_{\rm c}$ $ 1.93 \pm 0.08\times 10^{-9}$ $0.44\times 10^{-9}$ 0.31 10-27
isothermal $11.62 \pm 0.04\times 10^{-9}$ $2.65\times 10^{-9}$ $1.87\times 10^{-27}$
a f is the maximum fraction of dark matter in the form of PBHs, $\Omega_{\rm PBH}(M_{\star})$ is the corresponding cosmological density, and $\beta$ is the fraction of regions undergoing collapse when the mass enclosed within the cosmological horizon was $M_{\star }$.


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