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Table 2.

Relative intensity of the stationary components.

θ = 5°
θ = 10°
θ = 20°
Model Mp MB Mp MB Mp MB
𝒩ϕ453.5β1 2.8 ± 3.0 7.8 ± 3.6 68.4 ± 3.6 66.9 ± 5.7 75.7 ± 6.0 74.4 ± 8.2
𝒩ϕ453.5β17.5 43.9 ± 3.6 9.7 ± 4.2 75.1 ± 2.7 64.4 ± 5.7 76.3 ± 3.6 69.6 ± 8.0
𝒩ϕ4510β1 61.5 ± 1.9 68.9 ± 2.0 73.4 ± 1.2 79.4 ± 1.9 75.3 ± 0.6 82.5 ± 1.0
𝒩ϕ4510β17.5 71.7 ± 5.1 61.6 ± 3.5 75.4 ± 4.4 74.2 ± 2.9 69.7 ± 6.0 75.9 ± 1.7

𝒩ϕ77.53.5β1 17.2 ± 1.8 3.4 ± 3.8 51.0 ± 4.6 45.9 ± 4.4 53.7 ± 9.4 47.4 ± 9.2
𝒩ϕ77.53.5β2.34 11.2 ± 1.3 1.8 ± 3.4 26.4 ± 4.4 17.7 ± 4.0 33.1 ± 7.3 23.6 ± 5.4
𝒩ϕ77.510β1 47.7 ± 5.7 43.1 ± 5.7 52.7 ± 5.1 43.1 ± 3.4 53.0 ± 4.7 44.1 ± 4.1
𝒩ϕ77.510β2.34 14.9 ± 6.3 13.3 ± 5.1 18.0 ± 7.1 14.3 ± 2.2 21.5 ± 7.6 18.1 ± 3.9

ϕ77.53.5β100 5.1 ± 2.6 14.8 ± 2.8 24.2 ± 4.0
ϕ77.510β100 21.1 ± 2.9 22.3 ± 4.7 21.6 ± 4.6

Notes. The tabulated data denote the jet model and the average relative intensity, in percentage, of the stationary components with respect to the underlying jet emission for the viewing angles θ = 5°, 10°, and 20° and the two particle injection models (Mp and MB).

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