2024-02-04 16:56:05 +01:00
|
|
|
{
|
|
|
|
|
"cells": [
|
|
|
|
|
{
|
|
|
|
|
"cell_type": "code",
|
2024-02-13 09:16:19 +01:00
|
|
|
"execution_count": 1,
|
2024-02-04 16:56:05 +01:00
|
|
|
"metadata": {},
|
|
|
|
|
"outputs": [],
|
|
|
|
|
"source": [
|
|
|
|
|
"import uproot\n",
|
|
|
|
|
"import numpy as np\n",
|
|
|
|
|
"import sys\n",
|
|
|
|
|
"import os\n",
|
|
|
|
|
"import matplotlib\n",
|
|
|
|
|
"import matplotlib.pyplot as plt\n",
|
|
|
|
|
"import mplhep\n",
|
|
|
|
|
"from mpl_toolkits import mplot3d\n",
|
|
|
|
|
"import itertools\n",
|
|
|
|
|
"import awkward as ak\n",
|
|
|
|
|
"from scipy.optimize import curve_fit\n",
|
|
|
|
|
"from utils.components import unique_name_ext_re\n",
|
|
|
|
|
"mplhep.style.use([\"LHCbTex2\"])\n",
|
|
|
|
|
"plt.rcParams[\"savefig.dpi\"] = 600\n",
|
|
|
|
|
"%matplotlib inline"
|
|
|
|
|
]
|
|
|
|
|
},
|
|
|
|
|
{
|
|
|
|
|
"cell_type": "code",
|
2024-02-13 09:16:19 +01:00
|
|
|
"execution_count": 2,
|
2024-02-04 16:56:05 +01:00
|
|
|
"metadata": {},
|
|
|
|
|
"outputs": [
|
|
|
|
|
{
|
|
|
|
|
"data": {
|
|
|
|
|
"text/plain": [
|
|
|
|
|
"50501"
|
|
|
|
|
]
|
|
|
|
|
},
|
2024-02-13 09:16:19 +01:00
|
|
|
"execution_count": 2,
|
2024-02-04 16:56:05 +01:00
|
|
|
"metadata": {},
|
|
|
|
|
"output_type": "execute_result"
|
|
|
|
|
}
|
|
|
|
|
],
|
|
|
|
|
"source": [
|
|
|
|
|
"file = uproot.open(\n",
|
2024-02-13 09:16:19 +01:00
|
|
|
" \"/work/cetin/LHCb/reco_tuner/data/tracking_losses_ntuple_B_thesis.root:PrDebugTrackingLosses.PrDebugTrackingTool/Tuple;1\"\n",
|
2024-02-04 16:56:05 +01:00
|
|
|
")\n",
|
|
|
|
|
"\n",
|
|
|
|
|
"# selektiere nur elektronen von B->K*ee\n",
|
|
|
|
|
"allcolumns = file.arrays()\n",
|
|
|
|
|
"electrons = allcolumns[(allcolumns.isElectron) & (allcolumns.fromB)]\n",
|
|
|
|
|
"\n",
|
|
|
|
|
"ak.num(electrons, axis=0)\n",
|
|
|
|
|
"# ak.count(found, axis=None)"
|
|
|
|
|
]
|
|
|
|
|
},
|
|
|
|
|
{
|
|
|
|
|
"cell_type": "code",
|
2024-02-13 09:16:19 +01:00
|
|
|
"execution_count": 3,
|
2024-02-04 16:56:05 +01:00
|
|
|
"metadata": {},
|
2024-02-08 17:43:22 +01:00
|
|
|
"outputs": [],
|
2024-02-04 16:56:05 +01:00
|
|
|
"source": [
|
2024-02-08 17:43:22 +01:00
|
|
|
"# electrons.type.show()"
|
2024-02-04 16:56:05 +01:00
|
|
|
]
|
|
|
|
|
},
|
|
|
|
|
{
|
|
|
|
|
"cell_type": "code",
|
2024-02-13 13:01:49 +01:00
|
|
|
"execution_count": 4,
|
2024-02-04 16:56:05 +01:00
|
|
|
"metadata": {},
|
|
|
|
|
"outputs": [],
|
|
|
|
|
"source": [
|
2024-02-08 17:43:22 +01:00
|
|
|
"cut_prop: bool = electrons.p_end_velo > 0 # 3e3\n",
|
2024-02-05 15:44:27 +01:00
|
|
|
"found = electrons[~electrons.lost & cut_prop]\n",
|
|
|
|
|
"lost = electrons[electrons.lost & cut_prop]\n",
|
2024-02-04 16:56:05 +01:00
|
|
|
"\n",
|
|
|
|
|
"eloss_found = (found[\"p\"] - found[\"p_end_scifi\"]) / found[\"p\"]\n",
|
|
|
|
|
"eloss_lost = (lost[\"p\"] - lost[\"p_end_scifi\"]) / lost[\"p\"]\n",
|
|
|
|
|
"\n",
|
2024-02-05 15:44:27 +01:00
|
|
|
"eloss = (electrons[\"p\"] - electrons[\"p_end_scifi\"]) / electrons[\"p\"]\n",
|
|
|
|
|
"eloss_magnet_found = ak.to_numpy(\n",
|
2024-02-13 09:16:19 +01:00
|
|
|
" (found[\"p_end_velo\"] - found[\"p_end_scifi\"]) / found[\"p_end_velo\"]\n",
|
|
|
|
|
")\n",
|
2024-02-05 15:44:27 +01:00
|
|
|
"eloss_magnet_lost = ak.to_numpy(\n",
|
2024-02-13 09:16:19 +01:00
|
|
|
" (lost[\"p_end_velo\"] - lost[\"p_end_scifi\"]) / lost[\"p_end_velo\"]\n",
|
|
|
|
|
")"
|
2024-02-04 16:56:05 +01:00
|
|
|
]
|
|
|
|
|
},
|
|
|
|
|
{
|
|
|
|
|
"cell_type": "code",
|
2024-02-13 13:01:49 +01:00
|
|
|
"execution_count": 5,
|
2024-02-04 16:56:05 +01:00
|
|
|
"metadata": {},
|
|
|
|
|
"outputs": [],
|
|
|
|
|
"source": [
|
2024-02-08 17:43:22 +01:00
|
|
|
"eloss_velo_found = (found[\"p\"] - found[\"p_end_velo\"]) / found[\"p\"]\n",
|
|
|
|
|
"eloss_velo_lost = (lost[\"p\"] - lost[\"p_end_velo\"]) / lost[\"p\"]"
|
2024-02-04 16:56:05 +01:00
|
|
|
]
|
|
|
|
|
},
|
|
|
|
|
{
|
|
|
|
|
"cell_type": "code",
|
2024-02-13 13:01:49 +01:00
|
|
|
"execution_count": 6,
|
2024-02-04 16:56:05 +01:00
|
|
|
"metadata": {},
|
|
|
|
|
"outputs": [
|
|
|
|
|
{
|
|
|
|
|
"data": {
|
2024-02-08 17:43:22 +01:00
|
|
|
"image/png": "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
|
|
|
|
|
"text/plain": [
|
|
|
|
|
"<Figure size 1200x900 with 1 Axes>"
|
|
|
|
|
]
|
|
|
|
|
},
|
|
|
|
|
"metadata": {},
|
|
|
|
|
"output_type": "display_data"
|
|
|
|
|
}
|
|
|
|
|
],
|
|
|
|
|
"source": [
|
|
|
|
|
"nbins = 50\n",
|
|
|
|
|
"plt.hist(\n",
|
|
|
|
|
" ak.to_numpy(eloss_lost),\n",
|
|
|
|
|
" bins=nbins,\n",
|
|
|
|
|
" density=True,\n",
|
|
|
|
|
" alpha=0.5,\n",
|
|
|
|
|
" histtype=\"bar\",\n",
|
|
|
|
|
" color=\"#F05342\",\n",
|
|
|
|
|
" label=\"lost\",\n",
|
|
|
|
|
" range=[0.001, 1],\n",
|
|
|
|
|
")\n",
|
|
|
|
|
"# #2A9D8F another teal color\n",
|
|
|
|
|
"plt.hist(\n",
|
|
|
|
|
" ak.to_numpy(eloss_found),\n",
|
|
|
|
|
" bins=nbins,\n",
|
|
|
|
|
" density=True,\n",
|
|
|
|
|
" alpha=0.5,\n",
|
|
|
|
|
" histtype=\"bar\",\n",
|
|
|
|
|
" color=\"#107E7D\",\n",
|
|
|
|
|
" label=\"found\",\n",
|
|
|
|
|
" range=[0.001, 1],\n",
|
|
|
|
|
")\n",
|
|
|
|
|
"\n",
|
|
|
|
|
"plt.xlabel(r\"$E_\\gamma/E_0$\")\n",
|
|
|
|
|
"plt.ylabel(\"a.u.\")\n",
|
|
|
|
|
"# plt.title(r'$B\\rightarrow K^\\ast ee$, $p>5$GeV, photons w/ brem_vtx_z$<9500$mm')\n",
|
|
|
|
|
"plt.legend(title=\"LHCb Simulation\")\n",
|
|
|
|
|
"plt.show()\n",
|
|
|
|
|
"# plt.savefig(\n",
|
|
|
|
|
"# \"/work/cetin/Projektpraktikum/thesis/emitted_energy_beginVelo2endT.pdf\",\n",
|
|
|
|
|
"# format=\"PDF\",\n",
|
|
|
|
|
"# )"
|
|
|
|
|
]
|
|
|
|
|
},
|
|
|
|
|
{
|
|
|
|
|
"cell_type": "code",
|
2024-02-13 09:16:19 +01:00
|
|
|
"execution_count": 7,
|
2024-02-08 17:43:22 +01:00
|
|
|
"metadata": {},
|
|
|
|
|
"outputs": [
|
|
|
|
|
{
|
|
|
|
|
"data": {
|
|
|
|
|
"image/png": "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
|
2024-02-04 16:56:05 +01:00
|
|
|
"text/plain": [
|
|
|
|
|
"<Figure size 1200x900 with 1 Axes>"
|
|
|
|
|
]
|
|
|
|
|
},
|
|
|
|
|
"metadata": {},
|
|
|
|
|
"output_type": "display_data"
|
|
|
|
|
}
|
|
|
|
|
],
|
|
|
|
|
"source": [
|
|
|
|
|
"nbins = 50\n",
|
|
|
|
|
"plt.hist(\n",
|
2024-02-05 15:44:27 +01:00
|
|
|
" ak.to_numpy(eloss_magnet_lost),\n",
|
2024-02-04 16:56:05 +01:00
|
|
|
" bins=nbins,\n",
|
|
|
|
|
" density=True,\n",
|
|
|
|
|
" alpha=0.5,\n",
|
|
|
|
|
" histtype=\"bar\",\n",
|
|
|
|
|
" color=\"#F05342\",\n",
|
|
|
|
|
" label=\"lost\",\n",
|
|
|
|
|
" range=[0.001, 1],\n",
|
|
|
|
|
")\n",
|
|
|
|
|
"# #2A9D8F another teal color\n",
|
|
|
|
|
"plt.hist(\n",
|
2024-02-05 15:44:27 +01:00
|
|
|
" ak.to_numpy(eloss_magnet_found),\n",
|
2024-02-04 16:56:05 +01:00
|
|
|
" bins=nbins,\n",
|
|
|
|
|
" density=True,\n",
|
|
|
|
|
" alpha=0.5,\n",
|
|
|
|
|
" histtype=\"bar\",\n",
|
|
|
|
|
" color=\"#107E7D\",\n",
|
|
|
|
|
" label=\"found\",\n",
|
|
|
|
|
" range=[0.001, 1],\n",
|
|
|
|
|
")\n",
|
|
|
|
|
"\n",
|
2024-02-05 15:44:27 +01:00
|
|
|
"plt.xlabel(r\"$E_\\gamma/E_{VELO}$\")\n",
|
2024-02-04 16:56:05 +01:00
|
|
|
"plt.ylabel(\"a.u.\")\n",
|
|
|
|
|
"# plt.title(r'$B\\rightarrow K^\\ast ee$, $p>5$GeV, photons w/ brem_vtx_z$<9500$mm')\n",
|
|
|
|
|
"plt.legend(title=\"LHCb Simulation\")\n",
|
2024-02-05 15:44:27 +01:00
|
|
|
"plt.show()\n",
|
|
|
|
|
"# plt.savefig(\n",
|
2024-02-08 17:43:22 +01:00
|
|
|
"# \"/work/cetin/Projektpraktikum/thesis/emitted_energy_endVelo2endT.pdf\", format=\"PDF\"\n",
|
|
|
|
|
"# )"
|
|
|
|
|
]
|
|
|
|
|
},
|
|
|
|
|
{
|
|
|
|
|
"cell_type": "code",
|
2024-02-13 09:16:19 +01:00
|
|
|
"execution_count": 8,
|
2024-02-08 17:43:22 +01:00
|
|
|
"metadata": {},
|
|
|
|
|
"outputs": [
|
|
|
|
|
{
|
|
|
|
|
"data": {
|
|
|
|
|
"image/png": "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
|
|
|
|
|
"text/plain": [
|
|
|
|
|
"<Figure size 1200x900 with 1 Axes>"
|
|
|
|
|
]
|
|
|
|
|
},
|
|
|
|
|
"metadata": {},
|
|
|
|
|
"output_type": "display_data"
|
|
|
|
|
}
|
|
|
|
|
],
|
|
|
|
|
"source": [
|
|
|
|
|
"nbins = 50\n",
|
|
|
|
|
"plt.hist(\n",
|
|
|
|
|
" ak.to_numpy(eloss_velo_lost),\n",
|
|
|
|
|
" bins=nbins,\n",
|
|
|
|
|
" density=True,\n",
|
|
|
|
|
" alpha=0.5,\n",
|
|
|
|
|
" histtype=\"bar\",\n",
|
|
|
|
|
" color=\"#F05342\",\n",
|
|
|
|
|
" label=\"lost\",\n",
|
|
|
|
|
" range=[0.001, 1],\n",
|
|
|
|
|
")\n",
|
|
|
|
|
"# #2A9D8F another teal color\n",
|
|
|
|
|
"plt.hist(\n",
|
|
|
|
|
" ak.to_numpy(eloss_velo_found),\n",
|
|
|
|
|
" bins=nbins,\n",
|
|
|
|
|
" density=True,\n",
|
|
|
|
|
" alpha=0.5,\n",
|
|
|
|
|
" histtype=\"bar\",\n",
|
|
|
|
|
" color=\"#107E7D\",\n",
|
|
|
|
|
" label=\"found\",\n",
|
|
|
|
|
" range=[0.001, 1],\n",
|
|
|
|
|
")\n",
|
|
|
|
|
"\n",
|
|
|
|
|
"plt.xlabel(r\"$E_\\gamma/E_0$\")\n",
|
|
|
|
|
"plt.ylabel(\"a.u.\")\n",
|
|
|
|
|
"# plt.title(r'$B\\rightarrow K^\\ast ee$, $p>5$GeV, photons w/ brem_vtx_z$<9500$mm')\n",
|
|
|
|
|
"plt.legend(title=\"LHCb Simulation\")\n",
|
|
|
|
|
"plt.show()\n",
|
|
|
|
|
"# plt.savefig(\n",
|
|
|
|
|
"# \"/work/cetin/Projektpraktikum/thesis/emitted_energy_beginVelo2endVelo.pdf\",\n",
|
|
|
|
|
"# format=\"PDF\",\n",
|
|
|
|
|
"# )"
|
2024-02-04 16:56:05 +01:00
|
|
|
]
|
|
|
|
|
},
|
|
|
|
|
{
|
|
|
|
|
"cell_type": "code",
|
2024-02-13 13:01:49 +01:00
|
|
|
"execution_count": 9,
|
2024-02-08 17:43:22 +01:00
|
|
|
"metadata": {},
|
|
|
|
|
"outputs": [],
|
|
|
|
|
"source": [
|
|
|
|
|
"### --- ### above should be correct"
|
|
|
|
|
]
|
|
|
|
|
},
|
|
|
|
|
{
|
|
|
|
|
"cell_type": "code",
|
|
|
|
|
"execution_count": null,
|
|
|
|
|
"metadata": {},
|
|
|
|
|
"outputs": [],
|
|
|
|
|
"source": []
|
|
|
|
|
},
|
|
|
|
|
{
|
|
|
|
|
"cell_type": "code",
|
2024-02-13 13:01:49 +01:00
|
|
|
"execution_count": 10,
|
2024-02-04 16:56:05 +01:00
|
|
|
"metadata": {},
|
|
|
|
|
"outputs": [],
|
|
|
|
|
"source": [
|
|
|
|
|
"# magnet kick position\n",
|
2024-02-08 17:43:22 +01:00
|
|
|
"input_tree = uproot.open({\n",
|
2024-02-13 13:01:49 +01:00
|
|
|
" \"/work/cetin/Projektpraktikum/tracking_losses_ntuple_test_zmag.root\" : \"PrDebugTrackingLosses.PrDebugTrackingTool/Tuple;1\"\n",
|
2024-02-08 17:43:22 +01:00
|
|
|
"})\n",
|
2024-02-04 16:56:05 +01:00
|
|
|
"array = input_tree.arrays()\n",
|
2024-02-13 13:01:49 +01:00
|
|
|
"array = array[(array.isElectron) & (array.fromB)]\n"
|
2024-02-04 16:56:05 +01:00
|
|
|
]
|
|
|
|
|
},
|
|
|
|
|
{
|
|
|
|
|
"cell_type": "code",
|
2024-02-08 17:43:22 +01:00
|
|
|
"execution_count": 21,
|
2024-02-04 16:56:05 +01:00
|
|
|
"metadata": {},
|
|
|
|
|
"outputs": [
|
|
|
|
|
{
|
|
|
|
|
"data": {
|
2024-02-13 13:01:49 +01:00
|
|
|
"image/png": "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
|
2024-02-04 16:56:05 +01:00
|
|
|
"text/plain": [
|
|
|
|
|
"<Figure size 1200x900 with 1 Axes>"
|
|
|
|
|
]
|
|
|
|
|
},
|
|
|
|
|
"metadata": {},
|
|
|
|
|
"output_type": "display_data"
|
|
|
|
|
}
|
|
|
|
|
],
|
|
|
|
|
"source": [
|
2024-02-13 13:01:49 +01:00
|
|
|
"xmin: float = 5200\n",
|
|
|
|
|
"xmax: float = 5600\n",
|
|
|
|
|
"\n",
|
2024-02-04 16:56:05 +01:00
|
|
|
"fig = plt.figure()\n",
|
2024-02-13 13:01:49 +01:00
|
|
|
"plt.hist(array[array.lost][\"match_zmag\"],\n",
|
|
|
|
|
" bins=80,\n",
|
|
|
|
|
" range=[xmin, xmax],\n",
|
|
|
|
|
" color=\"#F05342\",\n",
|
|
|
|
|
" alpha=0.5,\n",
|
|
|
|
|
" label=\"lost\",\n",
|
|
|
|
|
" density=True)\n",
|
|
|
|
|
"plt.hist(array[~array.lost][\"match_zmag\"],\n",
|
|
|
|
|
" bins=80,\n",
|
|
|
|
|
" range=[xmin, xmax],\n",
|
|
|
|
|
" color=\"#107E7D\",\n",
|
|
|
|
|
" alpha=0.5,\n",
|
|
|
|
|
" label=\"found\",\n",
|
2024-02-05 15:44:27 +01:00
|
|
|
" density=True)\n",
|
2024-02-04 16:56:05 +01:00
|
|
|
"plt.xlabel(r\"z$_{Mag}$ [mm]\")\n",
|
|
|
|
|
"plt.ylabel(\"Number of Tracks (normalised)\")\n",
|
2024-02-13 13:01:49 +01:00
|
|
|
"plt.legend(loc=\"best\")\n",
|
|
|
|
|
"mplhep.lhcb.text(\"Simulation\",loc=0)\n",
|
|
|
|
|
"plt.show()\n",
|
|
|
|
|
"# plt.savefig(\n",
|
|
|
|
|
"# \"/work/cetin/Projektpraktikum/thesis/match_zmag_lost_found.pdf\",\n",
|
|
|
|
|
"# format=\"PDF\")"
|
2024-02-04 16:56:05 +01:00
|
|
|
]
|
|
|
|
|
},
|
|
|
|
|
{
|
|
|
|
|
"cell_type": "code",
|
|
|
|
|
"execution_count": 29,
|
|
|
|
|
"metadata": {},
|
|
|
|
|
"outputs": [
|
|
|
|
|
{
|
|
|
|
|
"data": {
|
|
|
|
|
"text/plain": [
|
|
|
|
|
"50501"
|
|
|
|
|
]
|
|
|
|
|
},
|
|
|
|
|
"execution_count": 29,
|
|
|
|
|
"metadata": {},
|
|
|
|
|
"output_type": "execute_result"
|
|
|
|
|
}
|
|
|
|
|
],
|
|
|
|
|
"source": [
|
|
|
|
|
"ak.num(array, axis=0)"
|
|
|
|
|
]
|
|
|
|
|
},
|
|
|
|
|
{
|
|
|
|
|
"cell_type": "code",
|
|
|
|
|
"execution_count": null,
|
|
|
|
|
"metadata": {},
|
|
|
|
|
"outputs": [],
|
|
|
|
|
"source": []
|
|
|
|
|
}
|
|
|
|
|
],
|
|
|
|
|
"metadata": {
|
|
|
|
|
"kernelspec": {
|
|
|
|
|
"display_name": "tuner",
|
|
|
|
|
"language": "python",
|
|
|
|
|
"name": "python3"
|
|
|
|
|
},
|
|
|
|
|
"language_info": {
|
|
|
|
|
"codemirror_mode": {
|
|
|
|
|
"name": "ipython",
|
|
|
|
|
"version": 3
|
|
|
|
|
},
|
|
|
|
|
"file_extension": ".py",
|
|
|
|
|
"mimetype": "text/x-python",
|
|
|
|
|
"name": "python",
|
|
|
|
|
"nbconvert_exporter": "python",
|
|
|
|
|
"pygments_lexer": "ipython3",
|
|
|
|
|
"version": "3.10.12"
|
|
|
|
|
}
|
|
|
|
|
},
|
|
|
|
|
"nbformat": 4,
|
|
|
|
|
"nbformat_minor": 2
|
|
|
|
|
}
|
