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Table 4

Best fits for specific DM annihilation channels assuming the best propagation parameter set.

Channel m χ σv K 0 L δ χ 2 p
[TeV] [ cm3 s-1 ] [ kpc2 Myr-1 ] [ kpc ]

e 0.350 ± 0.001 (1.88 ± 0.03) × 10-24 0.00405 1.5 0.70 682 16.6 0
μ 0.422 ± 0.018 (3.99 ± 0.30) × 10-24 0.00540 2.0 0.70 99.2 2.42 9.8 × 10-7
τ 1.26 ± 0.07 (3.47 ± 0.31) × 10-23 0.00670 2.0 0.65 24.1 0.59 0.98
u 33.7 ± 3.3 (1.61 ± 0.24) × 10-21 0.00930 2.0 0.60 18.1 0.44 0.99
b 30.3 ± 2.7 (1.19 ± 0.16) × 10-21 0.00910 2.0 0.60 17.7 0.43 0.99
t 50.8 ± 4.1 (2.39 ± 0.30) × 10-21 0.00775 2.5 0.70 17.7 0.43 0.99
Z 20.0 ± 1.3 (9.65 ± 1.01) × 10-22 0.00675 3.0 0.75 17.7 0.43 0.99
W 17.5 ± 0.1 (8.40 ± 0.90) × 10-22 0.00675 3.0 0.75 17.6 0.43 0.99
H 31.7 ± 2.2 (1.26 ± 0.14) × 10-21 0.00690 3.0 0.75 17.6 0.43 0.99
φe 0.350 ± 0.005 (1.31 ± 0.02) × 10-24 0.00440 2.0 0.65 143 3.48 0
φμ 0.763 ± 0.034 (7.77 ± 0.56) × 10-24 0.00660 2.0 0.65 44.7 1.09 0.32
φτ 2.43 ± 0.13 (6.80 ± 0.61) × 10-23 0.00680 2.0 0.65 22.9 0.56 0.99

Notes. The recently published positron fraction (Accardo et al. 2014) and the AMS-02 lepton spectrum (Weng et al. 2014) are used to derive the χ2, as in formula (20). The p-value, indicated in the last column, is defined in formula (22).

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