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100
101
102
103
Eγ [GeV]
10−7
E2
dN/dE[GeVcm−2
s−1
]
2 × 10−8
MDM = 130 GeV, hh, χ2
= 35.5, σv = 0.43 × 10−26
100
101
102
103
Eγ [GeV]
10−7
E2
dN/dE[GeVcm−2
s−1
]
2 × 10−8
MDM = 135 GeV, hh, χ2
= 38.6, σv = 0.41 × 10−26
100
101
102
103
Eγ [GeV]
10−7
E2
dN/dE[GeVcm−2
s−1
]
2 × 10−8
MDM = 140 GeV, hh, χ2
= 41.6, σv = 0.39 × 10−26
100
101
102
103
Eγ [GeV]
10−7
E2
dN/dE[GeVcm−2
s−1
]
2 × 10−8
MDM = 145 GeV, hh, χ2
= 44.4, σv = 0.38 × 10−26
100
101
102
103
Eγ [GeV]
10−7
E2
dN/dE[GeVcm−2
s−1
]
2 × 10−8
MDM = 150 GeV, hh, χ2
= 47.0, σv = 0.36 × 10−26
100
101
102
103
Eγ [GeV]
10−7
E2
dN/dE[GeVcm−2
s−1
]
2 × 10−8
MDM = 155 GeV, hh, χ2
= 49.6, σv = 0.35 × 10−26
100
101
102
103
Eγ [GeV]
10−7
E2
dN/dE[GeVcm−2
s−1
]
2 × 10−8
MDM = 160 GeV, hh, χ2
= 52.1, σv = 0.33 × 10−26
100
101
102
103
Eγ [GeV]
10−7
E2
dN/dE[GeVcm−2
s−1
]
2 × 10−8
MDM = 165 GeV, hh, χ2
= 54.4, σv = 0.32 × 10−26
100
101
102
103
Eγ [GeV]
10−7
E2
dN/dE[GeVcm−2
s−1
]
2 × 10−8
MDM = 170 GeV, hh, χ2
= 56.6, σv = 0.31 × 10−26
100
101
102
Eγ [GeV]
0
10
20
30
40
50E2
dN/dE[arbitraryunits]
χχ → hh
130 GeV
200 GeV
300 GeV

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hh fit to the GC GeV gamma-ray excess