In ggland the Si-detector has been simulated as a mimic-cylinder (test-01) and a ”black hole''-screen (test-13) that excludes hits at the front and inside of the mimic-cylinder with the following bash-script:
--test-01=dz=37.465cm,z0=-20.8cm,ir=0.8cm,r=1.2cm,type=Si,enter,tree=1 \
Figure 1: The distribution of θ in the lab frame of protonhits for different excitation energies Ex ∈ [6, 10].
In an initial attempt to convert θ from the lab frame to the center of mass frame, Catkin2.03 was used. The conversion between integer degrees 0-180 in the lab frame to the CM frame was calculated with the excel sheet for different excitation energies and the results are shown in Figure 3 below. The float values in the θ_lab distributions from Figure 1 was converted using Cubic Spline interpolation of the integer conversion from Catkin, resulting in the distribution of θ in the CM frame of protonhits for different excitation energies Ex ∈ [6, 10] in Figure 3.
Figure 2: Conversion between the cosine value of integer degrees θ ∈ [0,180] in the lab frame to the CM frame calculated by Catkin2.03 for different excitation energies Ex ∈ [6, 10].
Figure 3: The distribution of θ in the CM frame of protonhits for different excitation energies Ex ∈ [6, 10].
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