File indexing completed on 2022-03-17 03:23:37
0001 import os
0002 import collections
0003
0004 _sampleName = {
0005 "RelValCloseByParticleGun_CE_H_Fine_300um" : "CloseByParticleGun in CE-H Fine section with 300 um",
0006 "RelValCloseByParticleGun_CE_H_Fine_200um" : "CloseByParticleGun in CE-H Fine section with 200 um",
0007 "RelValCloseByParticleGun_CE_H_Fine_120um" : "CloseByParticleGun in CE-H Fine section with 120 um",
0008 "RelValCloseByParticleGun_CE_H_Coarse_Scint" : "CloseByParticleGun in CE-H Coarse section with scintillator",
0009 "RelValCloseByParticleGun_CE_H_Coarse_300um" : "CloseByParticleGun in CE-H Coarse section with 300 um",
0010 "RelValCloseByParticleGun_CE_E_Front_300um" : "CloseByParticleGun in CE-E Front section with 300 um",
0011 "RelValCloseByParticleGun_CE_E_Front_200um" : "CloseByParticleGun in CE-E Front section with 200 um",
0012 "RelValCloseByPGun_CE_E_Front_120um" : "CloseByParticleGun in CE-E Front section with 120 um",
0013 "RelValCloseByPGun_CE_H_Fine_300um" : "CloseByParticleGun in CE-H Fine section with 300 um",
0014 "RelValCloseByPGun_CE_H_Fine_200um" : "CloseByParticleGun in CE-H Fine section with 200 um",
0015 "RelValCloseByPGun_CE_H_Fine_120um" : "CloseByParticleGun in CE-H Fine section with 120 um",
0016 "RelValCloseByPGun_CE_H_Coarse_Scint" : "CloseByParticleGun in CE-H Coarse section with scintillator",
0017 "RelValCloseByPGun_CE_H_Coarse_300um" : "CloseByParticleGun in CE-H Coarse section with 300 um",
0018 "RelValCloseByPGun_CE_E_Front_300um" : "CloseByParticleGun in CE-E Front section with 300 um",
0019 "RelValCloseByPGun_CE_E_Front_200um" : "CloseByParticleGun in CE-E Front section with 200 um",
0020 "RelValCloseByPGun_CE_E_Front_120um" : "CloseByParticleGun in CE-E Front section with 120 um",
0021 "RelValTTbar" : "TTbar",
0022 "RelValSingleGammaFlatPt8To150" : "Single Gamma Pt 8 GeV to 150 GeV ",
0023 "RelValSingleMuPt10" : "Single Muon Pt 10 GeV",
0024 "RelValSingleMuPt100" : "Single Muon Pt 100 GeV",
0025 "RelValSingleMuPt1000" : "Single Muon Pt 1000 GeV",
0026 "RelValSingleMuFlatPt2To100" : "Single Muon Pt 2 GeV to 100 GeV",
0027 "RelValSingleMuFlatPt0p7To10" : "Single Muon Pt 0.7 GeV to 10 GeV",
0028 "RelValSingleEFlatPt2To100" : "Single Electron Pt 2 GeV to 100 GeV",
0029 "RelValSingleTauFlatPt2To150" : "Single Tau Pt 2 GeV to 150 GeV",
0030 "RelValSinglePiFlatPt0p7To10" : "Single Pion Pt 0.7 GeV to 10 GeV",
0031 "RelValQCD_Pt20toInfMuEnrichPt15" : "QCD Pt 20 GeV to Inf with Muon Pt 15 GeV",
0032 "RelValQCD_Pt15To7000_Flat" : "QCD Pt 15 GeV to 7 TeV",
0033 "RelValZTT" : "ZTauTau",
0034 "RelValZMM" : "ZMuMu",
0035 "RelValZEE" : "ZEleEle",
0036 "RelValB0ToKstarMuMu" : "B0 To Kstar Muon Muon",
0037 "RelValBsToEleEle" : "Bs To Electron Electron",
0038 "RelValBsToMuMu" : "Bs To Muon Muon",
0039 "RelValBsToJpsiGamma" : "Bs To Jpsi Gamma",
0040 "RelValBsToJpsiPhi_mumuKK" : "Bs To JpsiPhi_mumuKK",
0041 "RelValBsToPhiPhi_KKKK" : "Bs To PhiPhi_KKKK",
0042 "RelValDisplacedMuPt30To100" : "Displaced Muon Pt 30 GeV to 100 GeV",
0043 "RelValDisplacedMuPt2To10" : "Displaced Muon Pt 2 GeV to 10 GeV",
0044 "RelValDisplacedMuPt10To30" : "Displaced Muon Pt 10 GeV to 30 GeV",
0045 "RelValTauToMuMuMu" : "Tau To Muon Muon Muon",
0046 "RelValMinBias" : "Min Bias",
0047 "RelValH125GGgluonfusion" : "Higgs to gamma gamma",
0048 "RelValNuGun" : "Neutrino gun",
0049 "RelValZpTT_1500" : "Z prime with 1500 GeV nominal mass",
0050 "RelValTenTau_15_500_Eta3p1" : "Ten Taus with energy from 15 GeV to 500 GeV"
0051 }
0052
0053 _sampleFileName = {
0054 "RelValCloseByParticleGun_CE_H_Fine_300um" : "closebycehf300",
0055 "RelValCloseByParticleGun_CE_H_Fine_200um" : "closebycehf200",
0056 "RelValCloseByParticleGun_CE_H_Fine_120um" : "closebycehf120",
0057 "RelValCloseByParticleGun_CE_H_Coarse_Scint" : "closebycehcscint",
0058 "RelValCloseByParticleGun_CE_H_Coarse_300um" : "closebycehc300",
0059 "RelValCloseByParticleGun_CE_E_Front_300um" : "closebyceef300",
0060 "RelValCloseByParticleGun_CE_E_Front_200um" : "closebyceef200",
0061 "RelValCloseByParticleGun_CE_E_Front_120um" : "closebyceef120",
0062 "RelValTTbar" : "ttbar",
0063 "RelValSingleGammaFlatPt8To150" : "gam8",
0064 "RelValSingleMuPt10" : "m10",
0065 "RelValSingleMuPt100" : "m100",
0066 "RelValSingleMuPt1000" : "m1000",
0067 "RelValSingleMuFlatPt2To100" : "mflat2t100",
0068 "RelValSingleMuFlatPt0p7To10" : "mflat0p7t10",
0069 "RelValSingleEFlatPt2To100" : "eflat2t100",
0070 "RelValSingleTauFlatPt2To150" : "tauflat2t150",
0071 "RelValSinglePiFlatPt0p7To10" : "piflat0p7t10",
0072 "RelValQCD_Pt20toInfMuEnrichPt15" : "qcd20enmu15",
0073 "RelValQCD_Pt15To7000_Flat" : "qcdflat15",
0074 "RelValZTT" : "ztautau",
0075 "RelValZMM" : "zmm",
0076 "RelValZEE" : "zee",
0077 "RelValB0ToKstarMuMu" : "b0kstmm",
0078 "RelValBsToEleEle" : "bsee",
0079 "RelValBsToMuMu" : "bsmm",
0080 "RelValBsToJpsiGamma" : "bsjpsg",
0081 "RelValBsToJpsiPhi_mumuKK" : "bsjpspmmkk",
0082 "RelValBsToPhiPhi_KKKK" : "bsjpsppkkkk",
0083 "RelValDisplacedMuPt30To100" : "dm30",
0084 "RelValDisplacedMuPt2To10" : "dm2",
0085 "RelValDisplacedMuPt10To30" : "dm10",
0086 "RelValTauToMuMuMu" : "taummm",
0087 "RelValMinBias" : "minbias",
0088 "RelValH125GGgluonfusion" : "hgg",
0089 "RelValNuGun" : "nug",
0090 "RelValZpTT_1500" : "zp1500tautau",
0091 "RelValTenTau_15_500" : "tentaus15to1500"
0092
0093 }
0094
0095
0096 _pageNameMap = {
0097 "summary": "Summary",
0098 "hitCalibration": "Reconstructed hits calibration",
0099 "hitValidation" : "Simulated hits, digis, reconstructed hits validation" ,
0100 "layerClusters": "Layer clusters",
0101 "tracksters":"Tracksters",
0102 "Tracksters":"Tracksters",
0103 "Test-TICL":"Tracksters Linking",
0104 "TICL-patternRecognition":"Tracksters Pattern Recognition",
0105 "ticlMultiClustersFromTrackstersEM": "Electromagnetic multiclusters",
0106 "ticlMultiClustersFromTrackstersHAD": "Hadronic multiclusters",
0107 "hgcalMultiClusters" : "Old multiclusters",
0108 "standalone" : "Standalone study on simulated hits, digis, reconstructed hits"
0109 }
0110
0111 _sectionNameMapOrder = collections.OrderedDict([
0112
0113
0114
0115 ("layerClusters", "Layer clusters"),
0116
0117 ("ticlMultiClustersFromTrackstersEM","Electromagnetic multiclusters"),
0118
0119 ("ticlMultiClustersFromTrackstersHAD","Hadronic multiclusters"),
0120 ("tracksters","Tracksters"),
0121 ("Tracksters","Tracksters"),
0122 ("Test-TICL","Tracksters Linking"),
0123 ("TICL-patternRecognition","Tracksters Pattern Recognition"),
0124
0125 ("hgcalMultiClusters","Old multiclusters"),
0126 ])
0127
0128
0129 _summary = {}
0130
0131
0132
0133 _summobj = ['hitCalibration','hitValidation', 'layerClusters','Tracksters','Test-TICL','TICL-patternRecognition']
0134
0135
0136
0137 summhitcalib=[
0138 'Layer_Occupancy/LayerOccupancy/LayerOccupancy.png',
0139 'ReconstructableEnergyOverCPenergy/ReconstructableEnergyOverCPenergy/h_EoP_CPene_300_calib_fraction.png',
0140 'ReconstructableEnergyOverCPenergy/ReconstructableEnergyOverCPenergy/h_EoP_CPene_200_calib_fraction.png',
0141 'ReconstructableEnergyOverCPenergy/ReconstructableEnergyOverCPenergy/h_EoP_CPene_100_calib_fraction.png',
0142 'ReconstructableEnergyOverCPenergy/ReconstructableEnergyOverCPenergy/h_EoP_CPene_scint_calib_fraction.png'
0143 ]
0144
0145
0146 summhitvalid = [
0147 'SimHits_Validation/HitValidation/heeEnSim.png',
0148 'SimHits_Validation/HitValidation/hebEnSim.png',
0149 'SimHits_Validation/HitValidation/hefEnSim.png']
0150
0151
0152 summlc = [
0153 'hgcalLayerClusters_Z-minus: LC_CP association/Efficiencies_vs_layer/globalEfficiencies.png' ,
0154 'hgcalLayerClusters_Z-plus: LC_CP association/Efficiencies_vs_layer/globalEfficiencies.png' ,
0155 'hgcalLayerClusters_Z-minus: LC_CP association/Duplicates_vs_layer/globalEfficiencies.png' ,
0156 'hgcalLayerClusters_Z-plus: LC_CP association/Duplicates_vs_layer/globalEfficiencies.png' ,
0157 'hgcalLayerClusters_Z-minus: LC_CP association/FakeRate_vs_layer/globalEfficiencies.png' ,
0158 'hgcalLayerClusters_Z-plus: LC_CP association/FakeRate_vs_layer/globalEfficiencies.png' ,
0159 'hgcalLayerClusters_Z-minus: LC_CP association/MergeRate_vs_layer/globalEfficiencies.png' ,
0160 'hgcalLayerClusters_Z-plus: LC_CP association/MergeRate_vs_layer/globalEfficiencies.png'
0161
0162
0163
0164
0165
0166 ]
0167
0168
0169 summmcEM = [
0170 'ticlTrackstersEM/EtaPhiPtEnergy/trackster_eta.png' ,
0171 'ticlTrackstersEM/EtaPhiPtEnergy/trackster_pt.png' ,
0172 'ticlTrackstersEM/TotalNumberofTracksters/tottracksternum.png',
0173 'ticlTrackstersEM/NumberofLayerClustersinTrackster/clusternum_in_trackster.png'
0174 ]
0175
0176
0177 summmcEM_Link = [
0178 'ticlTrackstersEM/Purities_Link/globalEfficiencies.png' ,
0179 'ticlTrackstersEM/Duplicates_Link/globalEfficiencies.png' ,
0180 'ticlTrackstersEM/FakeRate_Link/globalEfficiencies.png' ,
0181 'ticlTrackstersEM/MergeRate_Link/globalEfficiencies.png'
0182 ]
0183
0184 summmcEM_PR = [
0185 'ticlTrackstersEM/Purities_PR/globalEfficiencies.png' ,
0186 'ticlTrackstersEM/Duplicates_PR/globalEfficiencies.png' ,
0187 'ticlTrackstersEM/FakeRate_PR/globalEfficiencies.png' ,
0188 'ticlTrackstersEM/MergeRate_PR/globalEfficiencies.png'
0189 ]
0190
0191
0192 summmcHAD = [
0193 'ticlTrackstersHAD/EtaPhiPtEnergy/trackster_eta.png' ,
0194 'ticlTrackstersHAD/EtaPhiPtEnergy/trackster_pt.png' ,
0195 'ticlTrackstersHAD/TotalNumberofTracksters/tottracksternum.png',
0196 'ticlTrackstersHAD/NumberofLayerClustersinTrackster/clusternum_in_trackster.png'
0197 ]
0198
0199 summmcHAD_Link = [
0200 'ticlTrackstersHAD/Purities_Link/globalEfficiencies.png' ,
0201 'ticlTrackstersHAD/Duplicates_Link/globalEfficiencies.png' ,
0202 'ticlTrackstersHAD/FakeRate_Link/globalEfficiencies.png' ,
0203 'ticlTrackstersHAD/MergeRate_Link/globalEfficiencies.png'
0204 ]
0205
0206 summmcHAD_PR = [
0207 'ticlTrackstersHAD/Purities_PR/globalEfficiencies.png' ,
0208 'ticlTrackstersHAD/Duplicates_PR/globalEfficiencies.png' ,
0209 'ticlTrackstersHAD/FakeRate_PR/globalEfficiencies.png' ,
0210 'ticlTrackstersHAD/MergeRate_PR/globalEfficiencies.png'
0211 ]
0212
0213 summmcTICL = summmcEM + summmcHAD
0214 summmcTICL_Link = summmcEM_Link + summmcHAD_Link
0215 summmcTICL_PR = summmcEM_PR + summmcHAD_PR
0216
0217
0218 summstandalone = [
0219 'hgcalSimHitStudy/RZ_AllDetectors.png'
0220 ]
0221
0222
0223 for obj in _summobj:
0224 _summary[obj] = {}
0225 _summary['hitCalibration'] = summhitcalib
0226 _summary['hitValidation'] = summhitvalid
0227 _summary['layerClusters'] = summlc
0228 _summary['Tracksters'] = summmcTICL
0229 _summary['Test-TICL'] = summmcTICL_Link
0230 _summary['TICL-patternRecognition'] = summmcTICL_PR
0231
0232
0233
0234
0235
0236
0237
0238 _MatBudSections = ["allhgcal","indimat","fromvertex"]
0239
0240 _geoPageNameMap = {
0241 "allhgcal": "All materials",
0242
0243
0244 "indimat" : "Individual materials",
0245 "fromvertex": "From vertex up to in front of muon stations"
0246 }
0247
0248 _individualmaterials =['Air','Aluminium','Cables','Copper','Epoxy','HGC_G10-FR4','Kapton','Lead','Other','Scintillator','Silicon','Stainless_Steel','WCu','Polystyrene','HGC_EEConnector','HGC_HEConnector']
0249
0250 _matPageNameMap = {
0251 'Air': 'Air',
0252 'Aluminium': 'Aluminium',
0253 'Cables': 'Cables',
0254 'Copper': 'Copper',
0255 'Epoxy': 'Epoxy',
0256 'HGC_G10-FR4': 'HGC_G10-FR4',
0257 'Kapton': 'Kapton',
0258 'Lead': 'Lead',
0259 'Other': 'Other',
0260 'Scintillator': 'Scintillator',
0261 'Silicon': 'Silicon',
0262 'Stainless_Steel': 'Stainless Steel',
0263 'WCu': 'WCu',
0264 'Polystyrene' : 'Polystyrene',
0265 'HGC_EEConnector': 'CE-E Connector',
0266 'HGC_HEConnector': 'CE-H Connector'
0267 }
0268
0269 _individualmatplots = {"HGCal_x_vs_z_vs_Rsum","HGCal_l_vs_z_vs_Rsum","HGCal_x_vs_z_vs_Rsumcos","HGCal_l_vs_z_vs_Rsumcos","HGCal_x_vs_z_vs_Rloc","HGCal_l_vs_z_vs_Rloc"}
0270
0271 _allmaterialsplots = {"HGCal_x_vs_eta","HGCal_l_vs_eta","HGCal_x_vs_phi","HGCal_l_vs_phi","HGCal_x_vs_R","HGCal_l_vs_R","HGCal_x_vs_eta_vs_phi","HGCal_l_vs_eta_vs_phi","HGCal_x_vs_z_vs_Rsum","HGCal_l_vs_z_vs_Rsum","HGCal_x_vs_z_vs_Rsumcos","HGCal_l_vs_z_vs_Rsumcos","HGCal_x_vs_z_vs_Rloc","HGCal_l_vs_z_vs_Rloc"}
0272
0273 _fromvertexplots = {"HGCal_l_vs_eta","HGCal_l_vs_z_vs_Rsum","HGCal_l_vs_z_vs_Rsum_Zpluszoom"}
0274
0275 _individualMatPlotsDesc = {
0276 "HGCal_x_vs_z_vs_Rsum" : "The plots below shows the 2D profile histogram for THEMAT in all HGCAL that displays the mean value of the material budget in units of radiation length in each R-z cell. R-z cell is 1 cm x 1 mm. The plots depict the accumulated material budget as seen by the track, as the track travels throughout the detector.",
0277 "HGCal_l_vs_z_vs_Rsum" : "The plots below shows the 2D profile histogram for THEMAT in all HGCAL that displays the mean value of the material budget in units of interaction length in each R-z cell. R-z cell is 1 cm x 1 mm. The plots depict the accumulated material budget as seen by the track, as the track travels throughout the detector.",
0278 "HGCal_x_vs_z_vs_Rsumcos" : "The plots below shows the 2D profile histogram for THEMAT in all HGCAL that displays the mean value of the material budget in units of radiation length in each R-z cell. R-z cell is 1 cm x 1 mm. The plots depict the orthogonal accumulated material budget, that is cos(theta) what the track sees. ",
0279 "HGCal_l_vs_z_vs_Rsumcos" : "The plots below shows the 2D profile histogram for THEMAT in all HGCAL that displays the mean value of the material budget in units of interaction length in each R-z cell. R-z cell is 1 cm x 1 mm. The plots depict the orthogonal accumulated material budget, that is cos(theta) what the track sees. ",
0280 "HGCal_x_vs_z_vs_Rloc" : "The plots below shows the 2D profile histogram for THEMAT in all HGCAL that displays the local mean value of the material budget in units of radiation length in each R-z cell. R-z cell is 1 cm x 1 mm. The plots depict the local material budget as seen by the track, as the track travels throughout the detector. ",
0281 "HGCal_l_vs_z_vs_Rloc" : "The plots below shows the 2D profile histogram for THEMAT in all HGCAL that displays the local mean value of the material budget in units of interaction length in each R-z cell. R-z cell is 1 cm x 1 mm. The plots depict the local material budget as seen by the track, as the track travels throughout the detector. "
0282 }
0283
0284 _allmaterialsPlotsDesc= {
0285 "HGCal_x_vs_eta" : "The plot on the left shows the stacked profile histograms of all materials in HGCal geometry. These profile histograms display the mean value of the material budget in units of radiation length in each eta bin. 250 bins in eta (-5,5), so eta is divided in 0.04 width bins. ",
0286
0287 "HGCal_l_vs_eta" : "The plot on the left shows the stacked profile histograms of all materials in HGCal geometry. These profile histograms display the mean value of the material budget in units of interaction length in each eta bin. 250 bins in eta (-5,5), so eta is divided in 0.04 width bins. ",
0288
0289 "HGCal_x_vs_phi" : "The plot on the left shows the stacked profile histograms of all materials in HGCal geometry. These profile histograms display the mean value of the material budget in units of radiation length in each phi bin. 180 bins in phi (-3.2,3.2), so phi is divided in 0.036 rad width bins or 2.038 degrees width bins. ",
0290
0291 "HGCal_l_vs_phi" : "The plot on the left shows the stacked profile histograms of all materials in HGCal geometry. These profile histograms display the mean value of the material budget in units of interaction length in each phi bin. 180 bins in phi -3.2,3.2), so phi is divided in 0.036 rad width bins or 2.038 degrees width bins. ",
0292
0293 "HGCal_x_vs_R" : "The plot on the left shows the stacked profile histograms of all materials in HGCal geometry. These profile histograms display the mean value of the material budget in units of radiation length in each radius bin. 300 bins in radius (0,3000 mm), so radius is defined in 1 cm width bins. Both endcaps are in this histogram. Entries are huge since the radius is filled for each step of the track. Statistics in the HEB part above 1565 mm is smaller (although non visible, error is small), since in most part nothing is infront to keep account of the step. ",
0294
0295 "HGCal_l_vs_R" : "The plot on the left shows the stacked profile histograms of all materials in HGCal geometry. These profile histograms display the mean value of the material budget in units of interaction length in each radius bin. 300 bins in radius (0,3000 mm), so radius is defined in 1 cm width bins. Both endcaps are in this histogram. Entries are huge since the radius is filled for each step of the track. Statistics in the HEB part above 1565 mm is smaller (although non visible, error is small), since in most part nothing is in front to keep account of the step. ",
0296
0297 "HGCal_x_vs_eta_vs_phi" : "The plot on the left shows the 2D profile histogram that displays the mean value of the material budget in units of radiation length in each eta-phi cell. 180 bins in phi (-3.2,3.2), so phi is divided in 0.036 rad width bins or 2.038 degrees width bins. 250 bins in eta -5., 5., so eta is divided in 0.04 width bins. Therefore, eta-phi cell is 2.038 degrees x 0.04 . ",
0298
0299 "HGCal_l_vs_eta_vs_phi" : "The plot on the left shows the 2D profile histogram that displays the mean value of the material budget in units of interaction length in each eta-phi cell. 180 bins in phi (-3.2,3.2), so phi is divided in 0.036 rad width bins or 2.038 degrees width bins. 250 bins in eta -5., 5., so eta is divided in 0.04 width bins. Therefore, eta-phi cell is 2.038 degrees x 0.04 . ",
0300
0301 "HGCal_x_vs_z_vs_Rsum" : "The plots below shows the 2D profile histogram that displays the mean value of the material budget in units of radiation length in each R-z cell. R-z cell is 1 cm x 1 mm. The plots depict the accumulated material budget as seen by the track, as the track travels throughout the detector.",
0302
0303 "HGCal_l_vs_z_vs_Rsum" : "The plots below shows the 2D profile histogram that displays the mean value of the material budget in units of interaction length in each R-z cell. R-z cell is 1 cm x 1 mm. The plots depict the accumulated material budget as seen by the track, as the track travels throughout the detector.",
0304
0305 "HGCal_x_vs_z_vs_Rsumcos" : "The plots below shows the 2D profile histogram that displays the mean value of the material budget in units of radiation length in each R-z cell. R-z cell is 1 cm x 1 mm. The plots depict the orthogonal accumulated material budget, that is cos(theta) what the track sees. ",
0306
0307 "HGCal_l_vs_z_vs_Rsumcos" : "The plots below shows the 2D profile histogram that displays the mean value of the material budget in units of interaction length in each R-z cell. R-z cell is 1 cm x 1 mm. The plots depict the orthogonal accumulated material budget, that is cos(theta) what the track sees. " ,
0308
0309 "HGCal_x_vs_z_vs_Rloc" : "The plots below shows the 2D profile histogram that displays the local mean value of the material budget in units of radiation length in each R-z cell. R-z cell is 1 cm x 1 mm. The plots depict the local material budget as seen by the track, as the track travels throughout the detector. ",
0310
0311 "HGCal_l_vs_z_vs_Rloc" : "The plots below shows the 2D profile histogram that displays the local mean value of the material budget in units of interaction length in each R-z cell. R-z cell is 1 cm x 1 mm. The plots depict the local material budget as seen by the track, as the track travels throughout the detector. "
0312
0313
0314 }
0315
0316 _fromVertexPlotsDesc = {
0317 "HGCal_x_vs_eta" : "The plot below shows the stacked profile histogram of all sub detectors in front of muon stations. This profile histogram displays the mean value of the material budget in units of radiation length in each eta bin. 250 bins in eta (-5,5), so eta is divided in 0.04 width bins. ",
0318
0319 "HGCal_l_vs_eta" : "The plots below shows the stacked profile histogram of all sub detectors in front of muon stations. This profile histogram displays the mean value of the material budget in units of interaction length in each eta bin. 250 bins in eta (-5,5), so eta is divided in 0.04 width bins. ",
0320
0321 "HGCal_l_vs_z_vs_Rsum" : "The plots below shows the detectors that are taken into account in the calculation of the material budget. Keep in mind that coloured regions that depicts each sub-detector area may contain Air as material.",
0322
0323 "HGCal_l_vs_z_vs_Rsum_Zpluszoom" : "The zoomed plots below shows the detectors that are taken into account in the calculation of the material budget. Keep in mind that coloured regions that depicts each sub-detector area may contain Air as material."
0324
0325
0326
0327 }
0328
0329 _hideShowFun = {
0330 "thestyle" : "<meta name=\"viewport\" content=\"width=device-width, initial-scale=1\"> \n <style> \n body {font-family: Arial;} \n.tab { \n overflow: hidden; \n border: 1px solid #ccc; \n background-color: #f1f1f1;} \n .tab button { background-color: inherit; \n float: left; \n border: none; \n outline: none; \n cursor: pointer; \n padding: 14px 16px; \n transition: 0.3s; \n font-size: 17px; } \n .tab button:hover { background-color: #ddd; } \n .tab button.active { background-color: #ccc; } \n .tabcontent { display: none; \n padding: 6px 12px; \n border: 1px solid #ccc; \n border-top: none; \n} \n </style>",
0331 "buttonandFunction" : "<script> \n function openRegion(evt, regionName) { \n var i, tabcontent, tablinks;\n tabcontent = document.getElementsByClassName(\"tabcontent\"); \n for (i = 0; i < tabcontent.length; i++) {\n tabcontent[i].style.display = \"none\";\n }\n tablinks = document.getElementsByClassName(\"tablinks\"); \n for (i = 0; i < tablinks.length; i++) {\n tablinks[i].className = tablinks[i].className.replace(\" active\", \"\"); \n }\n document.getElementById(regionName).style.display = \"block\";\n evt.currentTarget.className += \" active\"; \n}\n</script>\n",
0332 "divTabs" : "<div class=\"tab\">\n <button class=\"tablinks\" onclick=\"openRegion(event, \'_AllHGCAL\')\">All HGCAL</button>\n <button class=\"tablinks\" onclick=\"openRegion(event, \'_ZminusZoom\')\">Zminus</button>\n <button class=\"tablinks\" onclick=\"openRegion(event, \'_ZplusZoom\')\">Zplus</button>\n </div>\n "
0333 }
0334
0335
0336
0337
0338
0339
0340