namespace Gambit::ColliderBit::ATLAS #

ATLAS-specific efficiency and smearing functions for super fast detector simulation.

Functions #

Attributes #

Functions Documentation #

function eff2DEl_Generic #

static const HEPUtils::BinnedFn2D< double > eff2DEl_Generic(
    {0, 1.5, 2.5, DBL_MAX} ,
    {0, 10., DBL_MAX} ,
    { 0., 0.95, 0., 0.85, 0., 0. } 
)

ATLAS Electron, Muon, Tau and Photon efficiencies for the WPs of the identification techniques used in SUSY analyses.

Note: Should be applied after the electron energy smearing

Electron efficiencies Generic electron efficiency Randomly filter the supplied particle list by parameterised electron efficiency

function eff2DEl_ATLAS_CONF_2014_032_Medium #

static const HEPUtils::BinnedFn2D< double > eff2DEl_ATLAS_CONF_2014_032_Medium(
    {-2.5, -2.37, -2.01, -1.81, -1.52, -1.37, -1.15, -0.8, -0.6, -0.1, 0, 0.1, 0.6, 0.8, 1.15, 1.37, 1.52, 1.81, 2.01, 2.37, 2.5} ,
    {0, 7., 10., 15., 20., 25., 30., 35., 40., 45., 50., 60., 80., DBL_MAX} ,
    { 0.000, 0.887, 0.778, 0.827, 0.828, 0.842, 0.848, 0.839, 0.837, 0.807, 0.783, 0.775, 0.949, 0.000, 0.887, 0.778, 0.827, 0.790, 0.826, 0.838, 0.857, 0.870, 0.892, 0.892, 0.894, 0.927, 0.000, 0.736, 0.768, 0.794, 0.795, 0.831, 0.851, 0.868, 0.882, 0.896, 0.900, 0.903, 0.935, 0.000, 0.736, 0.768, 0.794, 0.778, 0.817, 0.840, 0.867, 0.896, 0.912, 0.917, 0.922, 0.946, 0.000, 0.675, 0.569, 0.695, 0.725, 0.756, 0.771, 0.799, 0.840, 0.874, 0.879, 0.893, 0.908, 0.000, 0.775, 0.773, 0.811, 0.802, 0.842, 0.874, 0.897, 0.909, 0.925, 0.927, 0.927, 0.950, 0.000, 0.775, 0.773, 0.811, 0.799, 0.837, 0.867, 0.889, 0.898, 0.911, 0.919, 0.921, 0.953, 0.000, 0.832, 0.782, 0.820, 0.814, 0.847, 0.877, 0.895, 0.908, 0.918, 0.919, 0.921, 0.950, 0.000, 0.832, 0.782, 0.820, 0.812, 0.850, 0.879, 0.897, 0.908, 0.918, 0.923, 0.928, 0.941, 0.000, 0.823, 0.736, 0.786, 0.805, 0.836, 0.870, 0.886, 0.899, 0.907, 0.909, 0.904, 0.936, 0.000, 0.823, 0.736, 0.786, 0.781, 0.826, 0.857, 0.868, 0.888, 0.895, 0.897, 0.893, 0.931, 0.000, 0.832, 0.782, 0.820, 0.821, 0.851, 0.878, 0.896, 0.908, 0.921, 0.923, 0.926, 0.945, 0.000, 0.832, 0.782, 0.820, 0.817, 0.850, 0.882, 0.901, 0.912, 0.925, 0.928, 0.927, 0.954, 0.000, 0.775, 0.773, 0.811, 0.795, 0.838, 0.867, 0.891, 0.902, 0.913, 0.919, 0.921, 0.949, 0.000, 0.775, 0.773, 0.811, 0.790, 0.842, 0.872, 0.895, 0.908, 0.920, 0.923, 0.928, 0.951, 0.000, 0.675, 0.569, 0.695, 0.770, 0.765, 0.776, 0.804, 0.842, 0.872, 0.884, 0.898, 0.914, 0.000, 0.736, 0.768, 0.794, 0.777, 0.815, 0.838, 0.864, 0.892, 0.906, 0.913, 0.920, 0.945, 0.000, 0.736, 0.768, 0.794, 0.796, 0.835, 0.851, 0.869, 0.884, 0.896, 0.902, 0.904, 0.924, 0.000, 0.887, 0.778, 0.827, 0.791, 0.823, 0.839, 0.858, 0.870, 0.888, 0.884, 0.889, 0.924, 0.000, 0.887, 0.778, 0.827, 0.823, 0.836, 0.831, 0.826, 0.817, 0.783, 0.759, 0.741, 0.944, } 
)

Note: Numbers digitised from 8 TeV note (ATLAS-CONF-2014-032) Digitized from Figs 11-12 Combined in 2D efficiency

Efficiency function for Medium ID electrons

function eff2DEl_ATLAS_CONF_2014_032_Tight #

static const HEPUtils::BinnedFn2D< double > eff2DEl_ATLAS_CONF_2014_032_Tight(
    {-2.5, -2.37, -2.01, -1.81, -1.52, -1.37, -1.15, -0.8, -0.6, -0.1, 0, 0.1, 0.6, 0.8, 1.15, 1.37, 1.52, 1.81, 2.01, 2.37, 2.5} ,
    {0, 7., 10., 15., 20., 25., 30., 35., 40., 45., 50., 60., 80., DBL_MAX} ,
    { 0.000, 0.820, 0.687, 0.736, 0.679, 0.684, 0.694, 0.685, 0.694, 0.677, 0.665, 0.658, 0.857, 0.000, 0.820, 0.687, 0.736, 0.710, 0.741, 0.746, 0.759, 0.781, 0.808, 0.813, 0.812, 0.874, 0.000, 0.566, 0.644, 0.670, 0.655, 0.684, 0.715, 0.727, 0.759, 0.781, 0.796, 0.801, 0.858, 0.000, 0.566, 0.644, 0.670, 0.655, 0.696, 0.726, 0.752, 0.785, 0.807, 0.820, 0.834, 0.886, 0.000, 0.535, 0.455, 0.570, 0.603, 0.634, 0.659, 0.685, 0.730, 0.765, 0.784, 0.794, 0.839, 0.000, 0.608, 0.658, 0.702, 0.684, 0.721, 0.748, 0.773, 0.799, 0.817, 0.841, 0.845, 0.899, 0.000, 0.608, 0.658, 0.702, 0.696, 0.735, 0.772, 0.793, 0.803, 0.822, 0.842, 0.853, 0.903, 0.000, 0.712, 0.692, 0.733, 0.730, 0.762, 0.803, 0.822, 0.837, 0.850, 0.860, 0.868, 0.906, 0.000, 0.712, 0.692, 0.733, 0.734, 0.769, 0.803, 0.820, 0.809, 0.827, 0.845, 0.858, 0.887, 0.000, 0.619, 0.581, 0.642, 0.667, 0.698, 0.733, 0.749, 0.746, 0.762, 0.778, 0.779, 0.812, 0.000, 0.619, 0.581, 0.642, 0.641, 0.685, 0.716, 0.727, 0.734, 0.752, 0.766, 0.766, 0.816, 0.000, 0.712, 0.692, 0.733, 0.744, 0.773, 0.803, 0.821, 0.804, 0.823, 0.843, 0.856, 0.894, 0.000, 0.712, 0.692, 0.733, 0.735, 0.772, 0.812, 0.831, 0.844, 0.858, 0.878, 0.877, 0.911, 0.000, 0.608, 0.658, 0.702, 0.697, 0.737, 0.775, 0.798, 0.807, 0.826, 0.851, 0.855, 0.903, 0.000, 0.608, 0.658, 0.702, 0.672, 0.721, 0.749, 0.774, 0.798, 0.818, 0.842, 0.850, 0.892, 0.000, 0.535, 0.455, 0.570, 0.589, 0.639, 0.660, 0.693, 0.730, 0.766, 0.790, 0.801, 0.841, 0.000, 0.566, 0.644, 0.670, 0.661, 0.696, 0.725, 0.751, 0.780, 0.803, 0.817, 0.835, 0.888, 0.000, 0.566, 0.644, 0.670, 0.645, 0.688, 0.715, 0.733, 0.761, 0.782, 0.802, 0.804, 0.860, 0.000, 0.820, 0.687, 0.736, 0.709, 0.733, 0.746, 0.759, 0.781, 0.802, 0.805, 0.803, 0.876, 0.000, 0.820, 0.687, 0.736, 0.670, 0.678, 0.675, 0.669, 0.675, 0.652, 0.649, 0.627, 0.857, } 
)

Note: Numbers digitised from 8 TeV note (ATLAS-CONF-2014-032) Digitized from Figs 11-12 Combined in 2D efficiency

Efficiency function for Tight ID electrons

function eff2DEl_ATLAS_PHYS_PUB_2015_041_Loose #

static const HEPUtils::BinnedFn2D< double > eff2DEl_ATLAS_PHYS_PUB_2015_041_Loose(
    {0.0, 0.1, 0.8, 1.37, 1.52, 2.01, 2.37, 2.47, DBL_MAX} ,
    {0, 10, 20, 25, 30, 35, 40, 45, 50, 60, 80, DBL_MAX} ,
    Utils::outer_product(bineffs_eta_Loose, bineffs_et_Loose) 
)

function eff2DEl_ATLAS_PHYS_PUB_2015_041_Medium #

static const HEPUtils::BinnedFn2D< double > eff2DEl_ATLAS_PHYS_PUB_2015_041_Medium(
    {0.0, 0.1, 0.8, 1.37, 1.52, 2.01, 2.37, 2.47, DBL_MAX} ,
    {0, 10, 20, 25, 30, 35, 40, 45, 50, 60, 80, DBL_MAX} ,
    Utils::outer_product(bineffs_eta_Medium, bineffs_et_Medium) 
)

function eff1DEl_PERF_2017_01_ID_VeryLoose #

static const HEPUtils::BinnedFn1D< double > eff1DEl_PERF_2017_01_ID_VeryLoose(
    {0.0, 6.668795911849248, 9.673354432217419, 14.643593391597225, 19.57318312476409, 24.71356813100665, 29.655352632037403, 34.594233616910074, 39.73636073284749, 44.68221015649952, 49.6292209866148, 59.52440405330856, 79.51859702099242, DBL_MAX} ,
    {0.9054376657824932, 0.9267904509283819, 0.8757294429708221, 0.8450928381962863, 0.8775862068965516, 0.889655172413793, 0.9035809018567638, 0.9193633952254641, 0.929575596816976, 0.9370026525198938, 0.942572944297082, 0.9509283819628646, 0.9592838196286471} 
)

Note: These efficiencies are 1D efficiencies so only pT is used Digitised from Fig 8

Electron 2019 ID efficiency functions from https://arxiv.org/pdf/1902.04655.pdf

function eff1DEl_PERF_2017_01_ID_Loose #

static const HEPUtils::BinnedFn1D< double > eff1DEl_PERF_2017_01_ID_Loose(
    {0.0, 6.668795911849248, 9.673354432217419, 14.643593391597225, 19.57318312476409, 24.71356813100665, 29.655352632037403, 34.594233616910074, 39.73636073284749, 44.68221015649952, 49.6292209866148, 59.52440405330856, 79.51859702099242, DBL_MAX} ,
    {0.9054376657824932, 0.9267904509283819, 0.8757294429708221, 0.8450928381962863, 0.8775862068965516, 0.889655172413793, 0.9035809018567638, 0.9193633952254641, 0.929575596816976, 0.9370026525198938, 0.942572944297082, 0.9509283819628646, 0.9592838196286471} 
)

function eff1DEl_PERF_2017_01_ID_Medium #

static const HEPUtils::BinnedFn1D< double > eff1DEl_PERF_2017_01_ID_Medium(
    {0.0, 6.668795911849248, 9.673354432217419, 14.643593391597225, 19.57318312476409, 24.71356813100665, 29.655352632037403, 34.594233616910074, 39.73636073284749, 44.68221015649952, 49.6292209866148, 59.52440405330856, 79.51859702099242, DBL_MAX} ,
    { 0.7355437665782492, 0.7912466843501325, 0.7986737400530503, 0.7717506631299733, 0.8135278514588858, 0.8348806366047744, 0.8525198938992041, 0.8692307692307691, 0.8822281167108752, 0.889655172413793, 0.902652519893899, 0.9230769230769229, 0.9407161803713526 } 
)

function eff1DEl_PERF_2017_01_ID_Tight #

static const HEPUtils::BinnedFn1D< double > eff1DEl_PERF_2017_01_ID_Tight(
    {0.0, 6.668795911849248, 9.673354432217419, 14.643593391597225, 19.57318312476409, 24.71356813100665, 29.655352632037403, 34.594233616910074, 39.73636073284749, 44.68221015649952, 49.6292209866148, 59.52440405330856, 79.51859702099242, DBL_MAX} ,
    { 0.5572944297082227, 0.6213527851458884, 0.6547745358090185, 0.6714854111405835, 0.699336870026525, 0.7299734748010609, 0.7559681697612731, 0.7754641909814322, 0.7921750663129972, 0.8079575596816975, 0.8311671087533155, 0.8710875331564986, 0.8989389920424402 } 
)

function eff1DEl_PERF_2017_01_Iso_LooseTrackOnly #

static const HEPUtils::BinnedFn1D< double > eff1DEl_PERF_2017_01_Iso_LooseTrackOnly(
    {0.0, 6.548307897301772, 9.706735099256047, 14.643593391597225, 19.611982283197417, 24.561829913760132, 29.71154676569653, 34.461525174885566, 39.61370954807349, 44.56047277707178, 49.5109372879474, 59.60803424919497, 79.4086585320716, DBL_MAX} ,
    {0.9694027334287603, 0.9841898810834618, 0.9915715839022242, 0.9890807366218896, 0.9875756991852016, 0.9875509249064084, 0.9875261506276152, 0.9879947974014535, 0.9884634441752919, 0.9884386698964986, 0.9888959617925568, 0.9907953231667035, 0.9930404921823388} 
)

Note: These efficiencies are 1D efficiencies so only pT is used Digitised from Fig 12

Electron 2019 Isolation efficiency functions from https://arxiv.org/pdf/1902.04655.pdf

function eff1DEl_PERF_2017_01_Iso_Loose #

static const HEPUtils::BinnedFn1D< double > eff1DEl_PERF_2017_01_Iso_Loose(
    {0.0, 6.548307897301772, 9.706735099256047, 14.643593391597225, 19.611982283197417, 24.561829913760132, 29.71154676569653, 34.461525174885566, 39.61370954807349, 44.56047277707178, 49.5109372879474, 59.60803424919497, 79.4086585320716, DBL_MAX} ,
    {0.9595332801145123, 0.9812303870292888, 0.9891055109006828, 0.9875994412023784, 0.9856020149746753, 0.9826167143800926, 0.9820985190486677, 0.9820737447698745, 0.9820489704910813, 0.9825186495265361, 0.9829749091609778, 0.9903008698524555, 0.9930394599207224} 
)

function eff1DEl_PERF_2017_01_Iso_GradientLoose #

static const HEPUtils::BinnedFn1D< double > eff1DEl_PERF_2017_01_Iso_GradientLoose(
    {0.0, 6.548307897301772, 9.706735099256047, 14.643593391597225, 19.611982283197417, 24.561829913760132, 29.71154676569653, 34.461525174885566, 39.61370954807349, 44.56047277707178, 49.5109372879474, 59.60803424919497, 79.4086585320716, DBL_MAX} ,
    {0.8973632597445498, 0.9471843343977098, 0.9693676365338032, 0.9466465260955738, 0.947115172869412, 0.9485706617485136, 0.9539735190486678, 0.9593784408720547, 0.9642868448579609, 0.9706755120017618, 0.9780417308962784, 0.9843808494824929, 0.9851457553402335} 
)

function eff1DEl_PERF_2017_01_Iso_Gradient #

static const HEPUtils::BinnedFn1D< double > eff1DEl_PERF_2017_01_Iso_Gradient(
    {0.0, 6.548307897301772, 9.706735099256047, 14.643593391597225, 19.611982283197417, 24.561829913760132, 29.71154676569653, 34.461525174885566, 39.61370954807349, 44.56047277707178, 49.5109372879474, 59.60803424919497, 79.4086585320716, DBL_MAX} ,
    {0.8425935229024444, 0.9082030389781987, 0.944204195111209, 0.9007573359392205, 0.9081359419731337, 0.9145235768553183, 0.924368255890773, 0.9351987447698745, 0.9460292336489761, 0.9573531435807092, 0.9716251926888351, 0.9838874284298613, 0.9851457553402335} 
)

function eff1DEl_EGAM_2018_01_Recon #

static const HEPUtils::BinnedFn1D< double > eff1DEl_EGAM_2018_01_Recon(
    {0.0, 0.5, 1.0, 1.5, 2.0, 2.5, 3.0, 3.5, 4.0, 4.5, 5.0, 5.5, 6.0, 6.5, 7.0, 7.5, 8.0, 8.5, 9.0, 9.5, 10.0, 10.5, 11.0, 11.5, 12.0, 12.5, 13.0, 13.5, 14.0, 14.5, 15.0, 15.5, 16.0, 16.5, 17.0, 17.5, 18.0, 18.5, 19.0, 19.5, 20.0, 20.5, 21.0, 21.5, 22.0, 22.5, 23.0, 23.5, 24.0, 24.5, DBL_MAX} ,
    {0.0, 0.0, 0.0, 0.0, 0.003218, 0.049709, 0.203532, 0.388353, 0.546803, 0.662459, 0.749662, 0.807719, 0.850278, 0.875487, 0.893757, 0.907169, 0.919424, 0.926128, 0.932831, 0.936759, 0.940224, 0.944846, 0.947386, 0.949695, 0.951078, 0.953849, 0.955695, 0.956847, 0.958924, 0.959845, 0.962154, 0.96238, 0.96492, 0.966766, 0.966762, 0.967914, 0.967678, 0.970912, 0.970676, 0.97229, 0.972286, 0.97205, 0.973664, 0.97366, 0.973655, 0.973419, 0.975496, 0.976417, 0.977106, 0.976639} 
)

Note: These efficiencies are 1D efficiencies so only dependence on p_T is used Digitised from Fig 5

Electron 2020 reconstruction efficiency functions in 1908.00005 using 81 fb^-1 of Run 2 data

function eff1DEl_EGAM_2018_01_ID_Loose #

static const HEPUtils::BinnedFn1D< double > eff1DEl_EGAM_2018_01_ID_Loose(
    {4.5, 7.0, 10.0, 15.0, 20.0, 25.0, 30.0, 35.0, 40.0, 45.0, 50.0, 60.0, 80.0, DBL_MAX} ,
    {0.976333, 0.928653, 0.882698, 0.830078, 0.86466, 0.884306, 0.901769, 0.920381, 0.930032, 0.936581, 0.938994, 0.943589, 0.949449} 
)

Note: These efficiencies are 1D efficiencies so only dependence on p_T is used Digitised from Fig 23a

Electron 2020 ID efficiency functions in 1908.00005 using 81 fb^-1 of Run 2 data

function eff1DEl_EGAM_2018_01_ID_Medium #

static const HEPUtils::BinnedFn1D< double > eff1DEl_EGAM_2018_01_ID_Medium(
    {4.5, 7.0, 10.0, 15.0, 20.0, 25.0, 30.0, 35.0, 40.0, 45.0, 50.0, 60.0, 80.0, DBL_MAX} ,
    {0.790671, 0.797679, 0.816062, 0.752183, 0.794807, 0.82801, 0.847541, 0.868796, 0.882008, 0.887868, 0.897518, 0.916475, 0.93233} 
)

function eff1DEl_EGAM_2018_01_ID_Tight #

static const HEPUtils::BinnedFn1D< double > eff1DEl_EGAM_2018_01_ID_Tight(
    {4.5, 7.0, 10.0, 15.0, 20.0, 25.0, 30.0, 35.0, 40.0, 45.0, 50.0, 60.0, 80.0, DBL_MAX} ,
    {0.582835, 0.608686, 0.670726, 0.651999, 0.684283, 0.716567, 0.747358, 0.768038, 0.782399, 0.795381, 0.815832, 0.853631, 0.884536} 
)

function eff1DEl_EGAM_2018_01_Iso_Gradient #

static const HEPUtils::BinnedFn1D< double > eff1DEl_EGAM_2018_01_Iso_Gradient(
    {4.5, 7.0, 10.0, 15.0, 20.0, 25.0, 30.0, 35.0, 40.0, 45.0, 50.0, 60.0, 80.0, 150.0, 200.0, 250.0, 300.0, 350.0, DBL_MAX} ,
    {0.800008, 0.880847, 0.927209, 0.879823, 0.888724, 0.895806, 0.908012, 0.9198, 0.929307, 0.941235, 0.960432, 0.979162, 0.982515, 0.993515, 0.994261, 0.995376, 0.993139, 0.992581} 
)

Note: These efficiencies are 1D efficiencies so only dependence on p_T is used Digitize from Fig 16

Electron 2020 isolation efficiency functions in 1908.00005 using 81 fb^-1 of Run 2 data, EGAM-2018-01

function eff1DEl_EGAM_2018_01_Iso_Loose #

static const HEPUtils::BinnedFn1D< double > eff1DEl_EGAM_2018_01_Iso_Loose(
    {4.5, 7.0, 10.0, 15.0, 20.0, 25.0, 30.0, 35.0, 40.0, 45.0, 50.0, 60.0, 80.0, 150.0, 200.0, 250.0, 300.0, 350.0, DBL_MAX} ,
    {0.740555, 0.826427, 0.905545, 0.951997, 0.972965, 0.983728, 0.990392, 0.994352, 0.996819, 0.997565, 0.997844, 0.998311, 0.99859, 0.99859, 0.999057, 0.999105, 0.996589, 0.997614} 
)

function eff1DEl_EGAM_2018_01_Iso_Tight #

static const HEPUtils::BinnedFn1D< double > eff1DEl_EGAM_2018_01_Iso_Tight(
    {4.5, 7.0, 10.0, 15.0, 20.0, 25.0, 30.0, 35.0, 40.0, 45.0, 50.0, 60.0, 80.0, 150.0, 200.0, 250.0, 300.0, 350.0, DBL_MAX} ,
    {0.458893, 0.541276, 0.617828, 0.698061, 0.769957, 0.822, 0.862863, 0.895528, 0.924554, 0.940538, 0.95321, 0.970449, 0.985547, 0.992351, 0.993187, 0.993606, 0.991326, 0.991326} 
)

function eff1DEl_EGAM_2018_01_Iso_HighPtCaloOnly #

static const HEPUtils::BinnedFn1D< double > eff1DEl_EGAM_2018_01_Iso_HighPtCaloOnly(
    {4.5, 7.0, 10.0, 15.0, 20.0, 25.0, 30.0, 35.0, 40.0, 45.0, 50.0, 60.0, 80.0, 150.0, 200.0, 250.0, 300.0, 350.0, DBL_MAX} ,
    {0.982097, 0.975105, 0.969703, 0.967933, 0.966908, 0.965137, 0.965416, 0.966859, 0.970449, 0.970358, 0.967138, 0.962014, 0.950973, 0.926185, 0.904053, 0.908291, 0.925906, 0.929168} 
)

function eff1DTau_R2 #

static const HEPUtils::BinnedFn1D< double > eff1DTau_R2(
    binedges_pt ,
    bineffs_pt_avg 
)

function smearElectronEnergy #

inline void smearElectronEnergy(
    std::vector< HEPUtils::Particle * > & electrons
)

Randomly smear the supplied electrons’ momenta by parameterised resolutions.

function smearMuonMomentum #

inline void smearMuonMomentum(
    std::vector< HEPUtils::Particle * > & muons
)

Randomly smear the supplied muons’ momenta by parameterised resolutions.

function smearJets #

inline void smearJets(
    std::vector< HEPUtils::Jet * > & jets
)

Randomly smear the supplied jets’ momenta by parameterised resolutions.

TodoIs this the best way to smear? Should we preserve the mean jet energy, or pT, or direction?

function smearMET #

inline void smearMET(
    HEPUtils::P4 & pmiss,
    double set
)

Randomly smear the MET vector by parameterised resolutions.

function smearTaus #

inline void smearTaus(
    std::vector< HEPUtils::Particle * > & taus
)

Randomly smear the supplied taus’ momenta by parameterised resolutions.

TodoIs this the best way to smear? Should we preserve the mean jet energy, or pT, or direction?

function eff1DMET_CERN_EP_2015_241 #

static const HEPUtils::BinnedFn1D< double > eff1DMET_CERN_EP_2015_241(
    {0, 30, 60, 70, 80, 90, 100, 110, 120, 130, 140, 150, 170, 190, 210, 230, 250, 300, 400, DBL_MAX} ,
    {0.01, 0.01, 0.04, 0.07, 0.17, 0.30, 0.47, 0.63, 0.75, 0.85, 0.90, 0.95, 0.97, 0.98, 0.99, 0.98, 0.99, 1.00, 1.00} 
)

ATLAS trigger efficiencies MET trigger efficiency, from CERN-EP-2016-241 (1611.09661) Binned in MET

function eff2DMu_Generic #

static const HEPUtils::BinnedFn2D< double > eff2DMu_Generic(
    {0, 1.5, 2.7, DBL_MAX} ,
    {0, 10.0, DBL_MAX} ,
    { 0., 0.95, 0., 0.85, 0., 0. } 
)

Muon efficiencies Generic muon efficiency Randomly filter the supplied particle list by parameterised muon efficiency

function eff2DMu_R2 #

static const HEPUtils::BinnedFn2D< double > eff2DMu_R2(
    {0, 2.7, DBL_MAX} ,
    {0., 3.5, 4., 5., 6., 7., 8., 10., DBL_MAX} ,
    { 0.00, 0.76, 0.94, 0.97, 0.98, 0.98, 0.98, 0.99, 0.00, 0.00, 0.00, 0.00, 0.00, 0.00, 0.00, 0.00 } 
)

Generic R2 muon efficiency Randomly filter the supplied particle list by parameterised muon efficiency

function eff1DMu_MUON_2018_03_ID_Loose #

static const HEPUtils::BinnedFn1D< double > eff1DMu_MUON_2018_03_ID_Loose(
    {3.0, 3.5, 4.0, 5.0, 6.0, 7.0, 8.0, 9.0, 10.0, 12.0, 14.0, 16.0, 18.0, 20.0, 100., DBL_MAX} ,
    {0.87075, 0.93129, 0.97241, 0.98851, 0.99157, 0.98851, 0.98799, 0.98799, 0.98799, 0.98748, 0.98672, 0.98748, 0.98927, 0.99, 0.98} 
)

Note: These efficiencies are 1D efficiencies so only dependence on p_T is used Digitised from Fig 11a Additional 20-100; 100-inf bins taken from Table 1

Muon 2020 identification efficiency functions from full Run2 dataset released in 2012.00578, MUON-2018-03

function eff1DMu_MUON_2018_03_ID_Medium #

static const HEPUtils::BinnedFn1D< double > eff1DMu_MUON_2018_03_ID_Medium(
    {3.0, 3.5, 4.0, 5.0, 6.0, 7.0, 8.0, 9.0, 10.0, 12.0, 14.0, 16.0, 18.0, 20.0, 100., DBL_MAX} ,
    {0.45262, 0.61328, 0.80766, 0.9387, 0.96245, 0.97063, 0.97165, 0.97216, 0.97292, 0.97292, 0.97216, 0.97114, 0.97522, 0.97, 0.97} 
)

function eff1DMu_MUON_2018_03_ID_Tight #

static const HEPUtils::BinnedFn1D< double > eff1DMu_MUON_2018_03_ID_Tight(
    {3.0, 3.5, 4.0, 5.0, 6.0, 7.0, 8.0, 9.0, 10.0, 12.0, 14.0, 16.0, 18.0, 20.0, 100., DBL_MAX} ,
    {0.0, 0.0, 0.66948, 0.8143, 0.85466, 0.87816, 0.89246, 0.90421, 0.91418, 0.91877, 0.92031, 0.92669, 0.93972, 0.93, 0.93} 
)

function eff1DMu_MUON_2018_03_Iso_Loose #

static const HEPUtils::BinnedFn1D< double > eff1DMu_MUON_2018_03_Iso_Loose(
    {3.0, 4.0, 5.0, 6.0, 7.0, 8.0, 9.0, 10.0, 15.0, 20.0, 30.0, 40.0, 55.0, 70.0, 90.0, 150.0, DBL_MAX} ,
    {0.655349, 0.725581, 0.765116, 0.788605, 0.82093, 0.851395, 0.877907, 0.92, 0.956279, 0.981163, 0.992558, 0.996744, 0.997442, 0.997442, 0.997674, 0.995116} 
)

Note: These efficiencies are 1D efficiencies so only real dependence on p_T is used Digitised from Fig 19a

Muon 2020 isolation efficiency functions from full Run2 dataset released in 2012.00578, MUON-2018-03

function eff1DMu_MUON_2018_03_Iso_Tight #

static const HEPUtils::BinnedFn1D< double > eff1DMu_MUON_2018_03_Iso_Tight(
    {3.0, 4.0, 5.0, 6.0, 7.0, 8.0, 9.0, 10.0, 15.0, 20.0, 30.0, 40.0, 55.0, 70.0, 90.0, 150.0, DBL_MAX} ,
    {0.56788, 0.63355, 0.66702, 0.68974, 0.70173, 0.71814, 0.7314, 0.75917, 0.79262, 0.84313, 0.9189, 0.96941, 0.9915, 0.99653, 0.99649, 0.99517} 
)

function eff1DMu_ATLAS_PHYS_PUB_2020_002_Medium #

static const HEPUtils::BinnedFn1D< double > eff1DMu_ATLAS_PHYS_PUB_2020_002_Medium(
    {-2.5, -2.4, -2.3, -2.2, -2.1, -2.0, -1.9, -1.8, -1.7, -1.6, -1.5, -1.4, -1.3, -1.2, -1.1, -1.0, -0.9, -0.8, -0.7, -0.6, -0.5, -0.4, -0.3, -0.2, -0.1, 0.0, 0.1, 0.2, 0.3, 0.4, 0.5, 0.6, 0.7, 0.8, 0.9, 1.0, 1.1, 1.2, 1.3, 1.4, 1.5, 1.6, 1.7, 1.8, 1.9, 2.0, 2.1, 2.2, 2.3, 2.4, 2.5} ,
    {90.74, 94.48, 93.50, 95.47, 93.10, 92.91, 94.09, 93.69, 95.07, 91.33, 87.34, 76.55, 54.88, 56.26, 72.61, 71.82, 74.58, 73.99, 65.91, 69.85, 70.84, 73.00, 73.99, 69.06, 69.46, 68.67, 71.43, 74.38, 70.84, 70.44, 65.32, 64.93, 74.58, 75.76, 74.38, 73.20, 60.20, 55.86, 77.54, 87.19, 90.34, 94.48, 94.88, 95.07, 94.88, 95.07, 96.26, 96.26, 96.26, 93.89} 
)

Note: : These are efficiencies binned in eta, so make sure to use the correct function form (applyEfficiency(…,…,false)) Digitised from Fig 2a

Muon 2020 identification efficiencies for very low transverse momentum, from ATL-PHYS-PUB-2020-002

function eff1DMu_ATLAS_PHYS_PUB_2020_002_LowPT #

static const HEPUtils::BinnedFn1D< double > eff1DMu_ATLAS_PHYS_PUB_2020_002_LowPT(
    {-2.5, -2.4, -2.3, -2.2, -2.1, -2.0, -1.9, -1.8, -1.7, -1.6, -1.5, -1.4, -1.3, -1.2, -1.1, -1.0, -0.9, -0.8, -0.7, -0.6, -0.5, -0.4, -0.3, -0.2, -0.1, 0.0, 0.1, 0.2, 0.3, 0.4, 0.5, 0.6, 0.7, 0.8, 0.9, 1.0, 1.1, 1.2, 1.3, 1.4, 1.5, 1.6, 1.7, 1.8, 1.9, 2.0, 2.1, 2.2, 2.3, 2.4, 2.5} ,
    {87.59, 91.72, 90.94, 93.50, 90.34, 90.54, 91.92, 90.34, 91.92, 90.34, 89.75, 87.19, 83.05, 73.60, 86.01, 93.10, 91.92, 92.12, 85.62, 88.37, 90.15, 91.53, 92.12, 88.37, 72.41, 72.22, 88.18, 92.12, 92.12, 90.94, 86.80, 84.24, 91.33, 91.33, 93.89, 87.98, 75.96, 80.69, 86.80, 90.74, 89.56, 90.74, 92.51, 92.51, 91.92, 91.33, 94.68, 93.69, 94.09, 90.74} 
)

function eff1DTrack_ATLAS_SUSY_2018_16_isolated_track #

static const HEPUtils::BinnedFn1D< double > eff1DTrack_ATLAS_SUSY_2018_16_isolated_track(
    {0.0, 1.0, 1.5, 2.0, 2.5, 3.0, 3.5, 4.0, 4.5, 5.0, 6.0, 8.0, DBL_MAX} ,
    {0.0, 0.00554, 0.036175, 0.393355, 0.7706, 0.429725, 0.362845, 0.337615, 0.28892, 0.241395, 0.202085, 0.} 
)

Efficiencies from ATLAS_SUSY_2018_16 Digitised from Figure 3 This is specific to this search, and probably not used on other searches

function eff1DMuon_ATLAS_SUSY_2018_16 #

static const HEPUtils::BinnedFn1D< double > eff1DMuon_ATLAS_SUSY_2018_16(
    {3.0, 3.5, 4.0, 4.5, 5.0, 6.0, 8.0, 10.0, 12.0, 15.0, 20.0, 30.0, 50.0, 80.0, 120.0, DBL_MAX} ,
    {0.51128, 0.64915, 0.68318, 0.712515, 0.72953, 0.7266, 0.77295, 0.773535, 0.77647, 0.813425, 0.85626, 0.90202, 0.927835, 0.93253, 1.} 
)

function eff1DElectron_ATLAS_SUSY_2018_16 #

static const HEPUtils::BinnedFn1D< double > eff1DElectron_ATLAS_SUSY_2018_16(
    {4.5, 5.0, 6.0, 8.0, 10.0, 12.0, 15.0, 20.0, 30.0, 50.0, 80.0, 120.0, DBL_MAX} ,
    {0.230245, 0.385725, 0.50248, 0.59107, 0.646805, 0.660885, 0.636245, 0.701955, 0.77471, 0.86154, 0.89029, 1.} 
)

function eff2DTrack_ATL_PHYS_PUB_2015_051_Tight_Primary #

static const HEPUtils::BinnedFn2D< double > eff2DTrack_ATL_PHYS_PUB_2015_051_Tight_Primary(
    {-2.5, -2.3, -2.1, -1.9, -1.7, -1.5, -1.3, -1.1, -0.9, -0.7, -0.5, -0.3, -0.1, 0.1, 0.3, 0.5, 0.7, 0.9, 1.1, 1.3, 1.5, 1.7, 1.9, 2.1, 2.3, 2.5} ,
    {0, 0.5, 0.6, 0.7, 0.8, 0.9, 1.0, 1.1, 1.2, 1.3, 1.4, 1.5, 2, 2.5, 3.0, 3.5, 4.0, 5, DBL_MAX} ,
    {0.63 *0.73, 0.63 *0.79, 0.63 *0.79, 0.63 *0.80, 0.63 *0.81, 0.63 *0.81, 0.63 *0.81, 0.63 *0.82, 0.63 *0.82, 0.63 *0.82, 0.63 *0.82, 0.63 *0.83, 0.63 *0.84, 0.63 *0.84, 0.63 *0.85, 0.63 *0.85, 0.63 *0.85, 0., 0.71 *0.73, 0.71 *0.79, 0.71 *0.79, 0.71 *0.80, 0.71 *0.81, 0.71 *0.81, 0.71 *0.81, 0.71 *0.82, 0.71 *0.82, 0.71 *0.82, 0.71 *0.82, 0.71 *0.83, 0.71 *0.84, 0.71 *0.84, 0.71 *0.85, 0.71 *0.85, 0.71 *0.85, 0., 0.70 *0.73, 0.70 *0.79, 0.70 *0.79, 0.70 *0.80, 0.70 *0.81, 0.70 *0.81, 0.70 *0.81, 0.70 *0.82, 0.70 *0.82, 0.70 *0.82, 0.70 *0.82, 0.70 *0.83, 0.70 *0.84, 0.70 *0.84, 0.70 *0.85, 0.70 *0.85, 0.70 *0.85, 0., 0.71 *0.73, 0.71 *0.79, 0.71 *0.79, 0.71 *0.80, 0.71 *0.81, 0.71 *0.81, 0.71 *0.81, 0.71 *0.82, 0.71 *0.82, 0.71 *0.82, 0.71 *0.82, 0.71 *0.83, 0.71 *0.84, 0.71 *0.84, 0.71 *0.85, 0.71 *0.85, 0.71 *0.85, 0., 0.75 *0.73, 0.75 *0.79, 0.75 *0.79, 0.75 *0.80, 0.75 *0.81, 0.75 *0.81, 0.75 *0.81, 0.75 *0.82, 0.75 *0.82, 0.75 *0.82, 0.75 *0.82, 0.75 *0.83, 0.75 *0.84, 0.75 *0.84, 0.75 *0.85, 0.75 *0.85, 0.75 *0.85, 0., 0.79 *0.73, 0.79 *0.79, 0.79 *0.79, 0.79 *0.80, 0.79 *0.81, 0.79 *0.81, 0.79 *0.81, 0.79 *0.82, 0.79 *0.82, 0.79 *0.82, 0.79 *0.82, 0.79 *0.83, 0.79 *0.84, 0.79 *0.84, 0.79 *0.85, 0.79 *0.85, 0.79 *0.85, 0., 0.82 *0.73, 0.82 *0.79, 0.82 *0.79, 0.82 *0.80, 0.82 *0.81, 0.82 *0.81, 0.82 *0.81, 0.82 *0.82, 0.82 *0.82, 0.82 *0.82, 0.82 *0.82, 0.82 *0.83, 0.82 *0.84, 0.82 *0.84, 0.82 *0.85, 0.82 *0.85, 0.82 *0.85, 0., 0.84 *0.73, 0.84 *0.79, 0.84 *0.79, 0.84 *0.80, 0.84 *0.81, 0.84 *0.81, 0.84 *0.81, 0.84 *0.82, 0.84 *0.82, 0.84 *0.82, 0.84 *0.82, 0.84 *0.83, 0.84 *0.84, 0.84 *0.84, 0.84 *0.85, 0.84 *0.85, 0.84 *0.85, 0., 0.86 *0.73, 0.86 *0.79, 0.86 *0.79, 0.86 *0.80, 0.86 *0.81, 0.86 *0.81, 0.86 *0.81, 0.86 *0.82, 0.86 *0.82, 0.86 *0.82, 0.86 *0.82, 0.86 *0.83, 0.86 *0.84, 0.86 *0.84, 0.86 *0.85, 0.86 *0.85, 0.86 *0.85, 0., 0.86 *0.73, 0.86 *0.79, 0.86 *0.79, 0.86 *0.80, 0.86 *0.81, 0.86 *0.81, 0.86 *0.81, 0.86 *0.82, 0.86 *0.82, 0.86 *0.82, 0.86 *0.82, 0.86 *0.83, 0.86 *0.84, 0.86 *0.84, 0.86 *0.85, 0.86 *0.85, 0.86 *0.85, 0., 0.87 *0.73, 0.87 *0.79, 0.87 *0.79, 0.87 *0.80, 0.87 *0.81, 0.87 *0.81, 0.87 *0.81, 0.87 *0.82, 0.87 *0.82, 0.87 *0.82, 0.87 *0.82, 0.87 *0.83, 0.87 *0.84, 0.87 *0.84, 0.87 *0.85, 0.87 *0.85, 0.87 *0.85, 0., 0.87 *0.73, 0.87 *0.79, 0.87 *0.79, 0.87 *0.80, 0.87 *0.81, 0.87 *0.81, 0.87 *0.81, 0.87 *0.82, 0.87 *0.82, 0.87 *0.82, 0.87 *0.82, 0.87 *0.83, 0.87 *0.84, 0.87 *0.84, 0.87 *0.85, 0.87 *0.85, 0.87 *0.85, 0., 0.87 *0.73, 0.87 *0.79, 0.87 *0.79, 0.87 *0.80, 0.87 *0.81, 0.87 *0.81, 0.87 *0.81, 0.87 *0.82, 0.87 *0.82, 0.87 *0.82, 0.87 *0.82, 0.87 *0.83, 0.87 *0.84, 0.87 *0.84, 0.87 *0.85, 0.87 *0.85, 0.87 *0.85, 0., 0.87 *0.73, 0.87 *0.79, 0.87 *0.79, 0.87 *0.80, 0.87 *0.81, 0.87 *0.81, 0.87 *0.81, 0.87 *0.82, 0.87 *0.82, 0.87 *0.82, 0.87 *0.82, 0.87 *0.83, 0.87 *0.84, 0.87 *0.84, 0.87 *0.85, 0.87 *0.85, 0.87 *0.85, 0., 0.87 *0.73, 0.87 *0.79, 0.87 *0.79, 0.87 *0.80, 0.87 *0.81, 0.87 *0.81, 0.87 *0.81, 0.87 *0.82, 0.87 *0.82, 0.87 *0.82, 0.87 *0.82, 0.87 *0.83, 0.87 *0.84, 0.87 *0.84, 0.87 *0.85, 0.87 *0.85, 0.87 *0.85, 0., 0.87 *0.73, 0.87 *0.79, 0.87 *0.79, 0.87 *0.80, 0.87 *0.81, 0.87 *0.81, 0.87 *0.81, 0.87 *0.82, 0.87 *0.82, 0.87 *0.82, 0.87 *0.82, 0.87 *0.83, 0.87 *0.84, 0.87 *0.84, 0.87 *0.85, 0.87 *0.85, 0.87 *0.85, 0., 0.86 *0.73, 0.86 *0.79, 0.86 *0.79, 0.86 *0.80, 0.86 *0.81, 0.86 *0.81, 0.86 *0.81, 0.86 *0.82, 0.86 *0.82, 0.86 *0.82, 0.86 *0.82, 0.86 *0.83, 0.86 *0.84, 0.86 *0.84, 0.86 *0.85, 0.86 *0.85, 0.86 *0.85, 0., 0.84 *0.73, 0.84 *0.79, 0.84 *0.79, 0.84 *0.80, 0.84 *0.81, 0.84 *0.81, 0.84 *0.81, 0.84 *0.82, 0.84 *0.82, 0.84 *0.82, 0.84 *0.82, 0.84 *0.83, 0.84 *0.84, 0.84 *0.84, 0.84 *0.85, 0.84 *0.85, 0.84 *0.85, 0., 0.82 *0.73, 0.82 *0.79, 0.82 *0.79, 0.82 *0.80, 0.82 *0.81, 0.82 *0.81, 0.82 *0.81, 0.82 *0.82, 0.82 *0.82, 0.82 *0.82, 0.82 *0.82, 0.82 *0.83, 0.82 *0.84, 0.82 *0.84, 0.82 *0.85, 0.82 *0.85, 0.82 *0.85, 0., 0.79 *0.73, 0.79 *0.79, 0.79 *0.79, 0.79 *0.80, 0.79 *0.81, 0.79 *0.81, 0.79 *0.81, 0.79 *0.82, 0.79 *0.82, 0.79 *0.82, 0.79 *0.82, 0.79 *0.83, 0.79 *0.84, 0.79 *0.84, 0.79 *0.85, 0.79 *0.85, 0.79 *0.85, 0., 0.76 *0.73, 0.76 *0.79, 0.76 *0.79, 0.76 *0.80, 0.76 *0.81, 0.76 *0.81, 0.76 *0.81, 0.76 *0.82, 0.76 *0.82, 0.76 *0.82, 0.76 *0.82, 0.76 *0.83, 0.76 *0.84, 0.76 *0.84, 0.76 *0.85, 0.76 *0.85, 0.76 *0.85, 0., 0.71 *0.73, 0.71 *0.79, 0.71 *0.79, 0.71 *0.80, 0.71 *0.81, 0.71 *0.81, 0.71 *0.81, 0.71 *0.82, 0.71 *0.82, 0.71 *0.82, 0.71 *0.82, 0.71 *0.83, 0.71 *0.84, 0.71 *0.84, 0.71 *0.85, 0.71 *0.85, 0.71 *0.85, 0., 0.71 *0.73, 0.71 *0.79, 0.71 *0.79, 0.71 *0.80, 0.71 *0.81, 0.71 *0.81, 0.71 *0.81, 0.71 *0.82, 0.71 *0.82, 0.71 *0.82, 0.71 *0.82, 0.71 *0.83, 0.71 *0.84, 0.71 *0.84, 0.71 *0.85, 0.71 *0.85, 0.71 *0.85, 0., 0.71 *0.73, 0.71 *0.79, 0.71 *0.79, 0.71 *0.80, 0.71 *0.81, 0.71 *0.81, 0.71 *0.81, 0.71 *0.82, 0.71 *0.82, 0.71 *0.82, 0.71 *0.82, 0.71 *0.83, 0.71 *0.84, 0.71 *0.84, 0.71 *0.85, 0.71 *0.85, 0.71 *0.85, 0., 0.63 *0.73, 0.63 *0.79, 0.63 *0.79, 0.63 *0.80, 0.63 *0.81, 0.63 *0.81, 0.63 *0.81, 0.63 *0.82, 0.63 *0.82, 0.63 *0.82, 0.63 *0.82, 0.63 *0.83, 0.63 *0.84, 0.63 *0.84, 0.63 *0.85, 0.63 *0.85, 0.63 *0.85, 0.} 
)

Track efficiencies from ATL-PHYS-PUB-2015-051 Digitised and made 2d from figs 1a and 1b

function eff2DTrack_ATL_PHYS_PUB_2015_051_Loose #

static const HEPUtils::BinnedFn2D< double > eff2DTrack_ATL_PHYS_PUB_2015_051_Loose(
    {-2.5, -2.3, -2.1, -1.9, -1.7, -1.5, -1.3, -1.1, -0.9, -0.7, -0.5, -0.3, -0.1, 0.1, 0.3, 0.5, 0.7, 0.9, 1.1, 1.3, 1.5, 1.7, 1.9, 2.1, 2.3, 2.5} ,
    {0, 0.5, 0.6, 0.7, 0.8, 0.9, 1.0, 1.1, 1.2, 1.3, 1.4, 1.5, 2, 2.5, 3.0, 3.5, 4.0, 5, DBL_MAX} ,
    {0.73 *0.78, 0.73 *0.84, 0.73 *0.85, 0.73 *0.86, 0.73 *0.86, 0.73 *0.86, 0.73 *0.87, 0.73 *0.87, 0.73 *0.87, 0.73 *0.87, 0.73 *0.88, 0.73 *0.88, 0.73 *0.88, 0.73 *0.89, 0.73 *0.89, 0.73 *0.89, 0.73 *0.90, 0., 0.79 *0.78, 0.79 *0.84, 0.79 *0.85, 0.79 *0.86, 0.79 *0.86, 0.79 *0.86, 0.79 *0.87, 0.79 *0.87, 0.79 *0.87, 0.79 *0.87, 0.79 *0.88, 0.79 *0.88, 0.79 *0.88, 0.79 *0.89, 0.79 *0.89, 0.79 *0.89, 0.79 *0.90, 0., 0.78 *0.78, 0.78 *0.84, 0.78 *0.85, 0.78 *0.86, 0.78 *0.86, 0.78 *0.86, 0.78 *0.87, 0.78 *0.87, 0.78 *0.87, 0.78 *0.87, 0.78 *0.88, 0.78 *0.88, 0.78 *0.88, 0.78 *0.89, 0.78 *0.89, 0.78 *0.89, 0.78 *0.90, 0., 0.78 *0.78, 0.78 *0.84, 0.78 *0.85, 0.78 *0.86, 0.78 *0.86, 0.78 *0.86, 0.78 *0.87, 0.78 *0.87, 0.78 *0.87, 0.78 *0.87, 0.78 *0.88, 0.78 *0.88, 0.78 *0.88, 0.78 *0.89, 0.78 *0.89, 0.78 *0.89, 0.78 *0.90, 0., 0.80 *0.78, 0.80 *0.84, 0.80 *0.85, 0.80 *0.86, 0.80 *0.86, 0.80 *0.86, 0.80 *0.87, 0.80 *0.87, 0.80 *0.87, 0.80 *0.87, 0.80 *0.88, 0.80 *0.88, 0.80 *0.88, 0.80 *0.89, 0.80 *0.89, 0.80 *0.89, 0.80 *0.90, 0., 0.84 *0.78, 0.84 *0.84, 0.84 *0.85, 0.84 *0.86, 0.84 *0.86, 0.84 *0.86, 0.84 *0.87, 0.84 *0.87, 0.84 *0.87, 0.84 *0.87, 0.84 *0.88, 0.84 *0.88, 0.84 *0.88, 0.84 *0.89, 0.84 *0.89, 0.84 *0.89, 0.84 *0.90, 0., 0.87 *0.78, 0.87 *0.84, 0.87 *0.85, 0.87 *0.86, 0.87 *0.86, 0.87 *0.86, 0.87 *0.87, 0.87 *0.87, 0.87 *0.87, 0.87 *0.87, 0.87 *0.88, 0.87 *0.88, 0.87 *0.88, 0.87 *0.89, 0.87 *0.89, 0.87 *0.89, 0.87 *0.90, 0., 0.88 *0.78, 0.88 *0.84, 0.88 *0.85, 0.88 *0.86, 0.88 *0.86, 0.88 *0.86, 0.88 *0.87, 0.88 *0.87, 0.88 *0.87, 0.88 *0.87, 0.88 *0.88, 0.88 *0.88, 0.88 *0.88, 0.88 *0.89, 0.88 *0.89, 0.88 *0.89, 0.88 *0.90, 0., 0.90 *0.78, 0.90 *0.84, 0.90 *0.85, 0.90 *0.86, 0.90 *0.86, 0.90 *0.86, 0.90 *0.87, 0.90 *0.87, 0.90 *0.87, 0.90 *0.87, 0.90 *0.88, 0.90 *0.88, 0.90 *0.88, 0.90 *0.89, 0.90 *0.89, 0.90 *0.89, 0.90 *0.90, 0., 0.90 *0.78, 0.90 *0.84, 0.90 *0.85, 0.90 *0.86, 0.90 *0.86, 0.90 *0.86, 0.90 *0.87, 0.90 *0.87, 0.90 *0.87, 0.90 *0.87, 0.90 *0.88, 0.90 *0.88, 0.90 *0.88, 0.90 *0.89, 0.90 *0.89, 0.90 *0.89, 0.90 *0.90, 0., 0.91 *0.78, 0.91 *0.84, 0.91 *0.85, 0.91 *0.86, 0.91 *0.86, 0.91 *0.86, 0.91 *0.87, 0.91 *0.87, 0.91 *0.87, 0.91 *0.87, 0.91 *0.88, 0.91 *0.88, 0.91 *0.88, 0.91 *0.89, 0.91 *0.89, 0.91 *0.89, 0.91 *0.90, 0., 0.91 *0.78, 0.91 *0.84, 0.91 *0.85, 0.91 *0.86, 0.91 *0.86, 0.91 *0.86, 0.91 *0.87, 0.91 *0.87, 0.91 *0.87, 0.91 *0.87, 0.91 *0.88, 0.91 *0.88, 0.91 *0.88, 0.91 *0.89, 0.91 *0.89, 0.91 *0.89, 0.91 *0.90, 0., 0.91 *0.78, 0.91 *0.84, 0.91 *0.85, 0.91 *0.86, 0.91 *0.86, 0.91 *0.86, 0.91 *0.87, 0.91 *0.87, 0.91 *0.87, 0.91 *0.87, 0.91 *0.88, 0.91 *0.88, 0.91 *0.88, 0.91 *0.89, 0.91 *0.89, 0.91 *0.89, 0.91 *0.90, 0., 0.91 *0.78, 0.91 *0.84, 0.91 *0.85, 0.91 *0.86, 0.91 *0.86, 0.91 *0.86, 0.91 *0.87, 0.91 *0.87, 0.91 *0.87, 0.91 *0.87, 0.91 *0.88, 0.91 *0.88, 0.91 *0.88, 0.91 *0.89, 0.91 *0.89, 0.91 *0.89, 0.91 *0.90, 0., 0.91 *0.78, 0.91 *0.84, 0.91 *0.85, 0.91 *0.86, 0.91 *0.86, 0.91 *0.86, 0.91 *0.87, 0.91 *0.87, 0.91 *0.87, 0.91 *0.87, 0.91 *0.88, 0.91 *0.88, 0.91 *0.88, 0.91 *0.89, 0.91 *0.89, 0.91 *0.89, 0.91 *0.90, 0., 0.90 *0.78, 0.90 *0.84, 0.90 *0.85, 0.90 *0.86, 0.90 *0.86, 0.90 *0.86, 0.90 *0.87, 0.90 *0.87, 0.90 *0.87, 0.90 *0.87, 0.90 *0.88, 0.90 *0.88, 0.90 *0.88, 0.90 *0.89, 0.90 *0.89, 0.90 *0.89, 0.90 *0.90, 0., 0.90 *0.78, 0.90 *0.84, 0.90 *0.85, 0.90 *0.86, 0.90 *0.86, 0.90 *0.86, 0.90 *0.87, 0.90 *0.87, 0.90 *0.87, 0.90 *0.87, 0.90 *0.88, 0.90 *0.88, 0.90 *0.88, 0.90 *0.89, 0.90 *0.89, 0.90 *0.89, 0.90 *0.90, 0., 0.88 *0.78, 0.88 *0.84, 0.88 *0.85, 0.88 *0.86, 0.88 *0.86, 0.88 *0.86, 0.88 *0.87, 0.88 *0.87, 0.88 *0.87, 0.88 *0.87, 0.88 *0.88, 0.88 *0.88, 0.88 *0.88, 0.88 *0.89, 0.88 *0.89, 0.88 *0.89, 0.88 *0.90, 0., 0.87 *0.78, 0.87 *0.84, 0.87 *0.85, 0.87 *0.86, 0.87 *0.86, 0.87 *0.86, 0.87 *0.87, 0.87 *0.87, 0.87 *0.87, 0.87 *0.87, 0.87 *0.88, 0.87 *0.88, 0.87 *0.88, 0.87 *0.89, 0.87 *0.89, 0.87 *0.89, 0.87 *0.90, 0., 0.84 *0.78, 0.84 *0.84, 0.84 *0.85, 0.84 *0.86, 0.84 *0.86, 0.84 *0.86, 0.84 *0.87, 0.84 *0.87, 0.84 *0.87, 0.84 *0.87, 0.84 *0.88, 0.84 *0.88, 0.84 *0.88, 0.84 *0.89, 0.84 *0.89, 0.84 *0.89, 0.84 *0.90, 0., 0.80 *0.78, 0.80 *0.84, 0.80 *0.85, 0.80 *0.86, 0.80 *0.86, 0.80 *0.86, 0.80 *0.87, 0.80 *0.87, 0.80 *0.87, 0.80 *0.87, 0.80 *0.88, 0.80 *0.88, 0.80 *0.88, 0.80 *0.89, 0.80 *0.89, 0.80 *0.89, 0.80 *0.90, 0., 0.78 *0.78, 0.78 *0.84, 0.78 *0.85, 0.78 *0.86, 0.78 *0.86, 0.78 *0.86, 0.78 *0.87, 0.78 *0.87, 0.78 *0.87, 0.78 *0.87, 0.78 *0.88, 0.78 *0.88, 0.78 *0.88, 0.78 *0.89, 0.78 *0.89, 0.78 *0.89, 0.78 *0.90, 0., 0.78 *0.78, 0.78 *0.84, 0.78 *0.85, 0.78 *0.86, 0.78 *0.86, 0.78 *0.86, 0.78 *0.87, 0.78 *0.87, 0.78 *0.87, 0.78 *0.87, 0.78 *0.88, 0.78 *0.88, 0.78 *0.88, 0.78 *0.89, 0.78 *0.89, 0.78 *0.89, 0.78 *0.90, 0., 0.79 *0.78, 0.79 *0.84, 0.79 *0.85, 0.79 *0.86, 0.79 *0.86, 0.79 *0.86, 0.79 *0.87, 0.79 *0.87, 0.79 *0.87, 0.79 *0.87, 0.79 *0.88, 0.79 *0.88, 0.79 *0.88, 0.79 *0.89, 0.79 *0.89, 0.79 *0.89, 0.79 *0.90, 0., 0.72 *0.78, 0.72 *0.84, 0.72 *0.85, 0.72 *0.86, 0.72 *0.86, 0.72 *0.86, 0.72 *0.87, 0.72 *0.87, 0.72 *0.87, 0.72 *0.87, 0.72 *0.88, 0.72 *0.88, 0.72 *0.88, 0.72 *0.89, 0.72 *0.89, 0.72 *0.89, 0.72 *0.90, 0.} 
)

function eff2DPhoton_R2 #

static const HEPUtils::BinnedFn2D< double > eff2DPhoton_R2(
    { 0., 0.6, 1.37, 1.52, 1.81, 2.37, DBL_MAX } ,
    { 0., 10., 15., 20., 25., 30., 35., 40., 45., 50., 60., 80., 100., 125., 150., 175., 250., DBL_MAX } ,
    { 0.00, 0.55, 0.70, 0.85, 0.89, 0.93, 0.95, 0.96, 0.96, 0.97, 0.97, 0.98, 0.97, 0.97, 0.97, 0.97, 0.97, 0.00, 0.47, 0.66, 0.79, 0.86, 0.89, 0.94, 0.96, 0.97, 0.97, 0.98, 0.97, 0.98, 0.98, 0.98, 0.98, 0.98, 0.00, 0.00, 0.00, 0.00, 0.00, 0.00, 0.00, 0.00, 0.00, 0.00, 0.00, 0.00, 0.00, 0.00, 0.00, 0.00, 0.00, 0.00, 0.54, 0.71, 0.84, 0.88, 0.92, 0.93, 0.94, 0.95, 0.96, 0.96, 0.96, 0.96, 0.96, 0.96, 0.96, 0.96, 0.00, 0.61, 0.74, 0.83, 0.88, 0.91, 0.94, 0.95, 0.96, 0.97, 0.98, 0.98, 0.98, 0.98, 0.98, 0.98, 0.98, 0.00, 0.00, 0.00, 0.00, 0.00, 0.00, 0.00, 0.00, 0.00, 0.00, 0.00, 0.00, 0.00, 0.00, 0.00, 0.00, 0.00 } 
)

Photon efficiencies

Attributes Documentation #

variable bineffs_eta_Loose #

static const std::vector< double > bineffs_eta_Loose = { 0.950, 0.965, 0.955, 0.885, 0.950, 0.935, 0.90, 0 };

Note:

• Numbers digitised from Fig 3 of 13 TeV note (ATL-PHYS-PUB-2015-041)
• Manually symmetrised eta eff histogram

Todo: What about faking by jets or non-electrons?

Efficiency function for Loose ID electrons

variable bineffs_et_Loose #

static const std::vector< double > bineffs_et_Loose = {0.0, 0.90/0.95, 0.91/0.95, 0.92/0.95, 0.94/0.95, 0.95/0.95, 0.955/0.95, 0.965/0.95, 0.97/0.95, 0.98/0.95, 0.98/0.95 };

Note: Et eff histogram (10-20 GeV bin added by hand) normalisation factor as approximate double differential

variable bineffs_eta_Medium #

static const std::vector< double > bineffs_eta_Medium = { 0.900, 0.930, 0.905, 0.830, 0.900, 0.880, 0.85, 0 };

Note:

• Numbers digitised from Fig 3 of 13 TeV note (ATL-PHYS-PUB-2015-041)
• Manually symmetrised eta eff histogram

Efficiency function for Medium ID electrons

variable bineffs_et_Medium #

static const std::vector< double > bineffs_et_Medium = {0.0, 0.83/0.95, 0.845/0.95, 0.87/0.95, 0.89/0.95, 0.90/0.95, 0.91/0.95, 0.92/0.95, 0.93/0.95, 0.95/0.95, 0.95/0.95};

Note: Et eff histogram (10-20 GeV bin added by hand) normalisation factor as approximate double differential

variable effTau_R1 #

static const double effTau_R1 = 0.40;

Note: From Delphes 3.1.2

Todo: Use https://cds.cern.ch/record/1233743/files/ATL-PHYS-PUB-2010-001.pdf– it is more accurate and has pT-dependence

Tau efficiencies Generic tau efficiency Randomly filter the supplied particle list by parameterised Run 1 tau efficiency

variable binedges_pt #

static const std::vector< double > binedges_pt = { 0.,  20.,  40.,   60.,   120.,  160.,   220.,   280.,   380.,    500.,  DBL_MAX };

Note:

• From Delphes 3.3.2 & ATL-PHYS-PUB-2015-045, 60% for 1-prong, 70% for multi-prong: this is wrong!!
• No delete, because this should only ever be applied to copies of the Event Particle* vectors in Analysis routines

Randomly filter the supplied particle list by parameterised Run 2 tau efficiency

variable bineffs_pt_avg #

static const std::vector< double > bineffs_pt_avg = { 0.,  .52,  .53,   .54,    .56,   .55,    .54,    .52,     .48,     0. };

variable effTau_R2_RNN_Tight #

static const double effTau_R2_RNN_Tight = 0.58;

Note:

• this is the newer RNN Tau ID Algorithm, use the other function for the older BDT Tau ID Algorithm.
• by design these Tau ID working points have flat signal efficiencies in eta and phi
• using https://cds.cern.ch/record/2688062/files/ATL-PHYS-PUB-2019-033.pdf
• assuming frequency: 85% 1-prong, 15% >=3-prong

Randomly filter the supplied particle list by parameterised Run 2 RNN tau efficiency

variable effTau_R2_RNN_Medium #

static const double effTau_R2_RNN_Medium = 0.73;

variable effTau_R2_RNN_Loose #

static const double effTau_R2_RNN_Loose = 0.84;

variable effTau_R2_RNN_VeryLoose #

static const double effTau_R2_RNN_VeryLoose = 0.95;

variable eff1DMET #

static const efficiency_map< HEPUtils::BinnedFn1D< double > >({ {"CERN_EP_2015_241", eff1DMET_CERN_EP_2015_241}, }) eff1DMET;

variable eff1DEl #

static const efficiency_map< HEPUtils::BinnedFn1D< double > >({ {"PERF_2017_01_ID_VeryLoose", eff1DEl_PERF_2017_01_ID_VeryLoose}, {"PERF_2017_01_ID_Loose", eff1DEl_PERF_2017_01_ID_Loose}, {"PERF_2017_01_ID_Medium", eff1DEl_PERF_2017_01_ID_Medium}, {"PERF_2017_01_ID_Tight", eff1DEl_PERF_2017_01_ID_Tight}, {"PERF_2017_01_Iso_LooseTrackOnly", eff1DEl_PERF_2017_01_Iso_LooseTrackOnly}, {"PERF_2017_01_Iso_Loose", eff1DEl_PERF_2017_01_Iso_Loose}, {"PERF_2017_01_Iso_GradientLoose", eff1DEl_PERF_2017_01_Iso_GradientLoose}, {"PERF_2017_01_Iso_Gradient", eff1DEl_PERF_2017_01_Iso_Gradient}, {"EGAM_2018_01_Recon", eff1DEl_EGAM_2018_01_Recon}, {"EGAM_2018_01_ID_Loose", eff1DEl_EGAM_2018_01_ID_Loose}, {"EGAM_2018_01_ID_Medium", eff1DEl_EGAM_2018_01_ID_Medium}, {"EGAM_2018_01_ID_Tight", eff1DEl_EGAM_2018_01_ID_Tight}, {"EGAM_2018_01_Iso_Gradient", eff1DEl_EGAM_2018_01_Iso_Gradient}, {"EGAM_2018_01_Iso_Loose", eff1DEl_EGAM_2018_01_Iso_Loose}, {"EGAM_2018_01_Iso_Tight", eff1DEl_EGAM_2018_01_Iso_Tight}, {"EGAM_2018_01_Iso_HighPtCaloOnly", eff1DEl_EGAM_2018_01_Iso_HighPtCaloOnly}, {"ATLAS_SUSY_2018_16", eff1DElectron_ATLAS_SUSY_2018_16} }) eff1DEl;

variable eff2DEl #

static const efficiency_map< HEPUtils::BinnedFn2D< double > >({ {"Generic", eff2DEl_Generic}, {"ATLAS_CONF_2014_032_Medium", eff2DEl_ATLAS_CONF_2014_032_Medium}, {"ATLAS_CONF_2014_032_Tight", eff2DEl_ATLAS_CONF_2014_032_Tight}, {"ATLAS_PHYS_PUB_2015_041_Loose", eff2DEl_ATLAS_PHYS_PUB_2015_041_Loose}, {"ATLAS_PHYS_PUB_2015_041_Medium", eff2DEl_ATLAS_PHYS_PUB_2015_041_Medium} }) eff2DEl;

variable eff1DMu #

static const efficiency_map< HEPUtils::BinnedFn1D< double > >({ {"MUON_2018_03_Iso_Loose", eff1DMu_MUON_2018_03_Iso_Loose}, {"MUON_2018_03_Iso_Tight", eff1DMu_MUON_2018_03_Iso_Tight}, {"MUON_2018_03_ID_Loose", eff1DMu_MUON_2018_03_ID_Loose}, {"MUON_2018_03_ID_Medium", eff1DMu_MUON_2018_03_ID_Medium}, {"MUON_2018_03_ID_Tight", eff1DMu_MUON_2018_03_ID_Tight}, {"ATLAS_PHYS_PUB_2020_002_Medium", eff1DMu_ATLAS_PHYS_PUB_2020_002_Medium}, {"ATLAS_PHYS_PUB_2020_002_LowPT", eff1DMu_ATLAS_PHYS_PUB_2020_002_LowPT}, {"ATLAS_SUSY_2018_16", eff1DMuon_ATLAS_SUSY_2018_16} }) eff1DMu;

variable eff2DMu #

static const efficiency_map< HEPUtils::BinnedFn2D< double > >({ {"Generic", eff2DMu_Generic}, {"R2", eff2DMu_R2} }) eff2DMu;

variable effTau #

static const efficiency_map< double >({ {"R1", effTau_R1}, {"R2_RNN_Tight", effTau_R2_RNN_Tight}, {"R2_RNN_Medium", effTau_R2_RNN_Medium}, {"R2_RNN_Loose", effTau_R2_RNN_Loose}, {"R2_RNN_VeryLoose", effTau_R2_RNN_VeryLoose}, }) effTau;

variable eff1DTau #

static const efficiency_map< HEPUtils::BinnedFn1D< double > >({ {"R2", eff1DTau_R2}, }) eff1DTau;

variable eff1DTrack #

static const efficiency_map< HEPUtils::BinnedFn1D< double > >({ {"ATLAS_SUSY_2018_16_isolated_track", eff1DTrack_ATLAS_SUSY_2018_16_isolated_track}, }) eff1DTrack;

variable eff2DTrack #

static const efficiency_map< HEPUtils::BinnedFn2D< double > >({ {"ATL_PHYS_PUB_2015_051_Tight_Primary", eff2DTrack_ATL_PHYS_PUB_2015_051_Tight_Primary}, {"ATL_PHYS_PUB_2015_051_Loose", eff2DTrack_ATL_PHYS_PUB_2015_051_Loose}, }) eff2DTrack;

variable eff2DPhoton #

static const efficiency_map< HEPUtils::BinnedFn2D< double > >({ {"R2", eff2DPhoton_R2}, }) eff2DPhoton;

Updated on 2026-11-03 at 14:50:43 +0000