CorrectionSet (schema v2)
This json file contains the corrections for deepJet and deepCSV AK4 taggers. Corrections are
supplied for b-tag discriminator shape corrections (shape) and working point corrections
(comb/mujets/incl). For the working point corrections the SFs in 'mujets' and 'comb' are for b/c
jets. The 'mujets' SFs contain only corrections derived in QCD-enriched regions. The 'comb' SFs
contain corrections derived in QCD and ttbar-enriched regions. Hence, 'comb' SFs can be used
everywhere, except for ttbar-dileptonic enriched analysis regions. For the ttbar-dileptonic regions
the 'mujets' SFs should be used. The 'incl' correction is for light-flavoured jets.
📂
├── 📈 deepCSV_wp_values (v1)
│ working points for deepCSV in UL 2016postVFP.
│ Node counts: Category: 1
│ â•─────── â–¶ input ────────╮
│ │ working_point (string) │
│ │ L/M/T │
│ │ Values: L, M, T │
│ ╰────────────────────────╯
│ â•─── â—€ output ───╮
│ │ wp (real) │
│ │ No description │
│ ╰────────────────╯
├── 📈 deepCSV_incl (v1)
│ deepCSV incl working point scale factors for UL 2016postVFP light jets. For the working point
│ correction multiple different uncertainty schemes are provided. If only one year is analyzed,
│ the 'up' and 'down' systematics can be used. If the fullRunII data is analyzed,
│ 'up/down_correlated' and 'up/down_uncorrelated' systematics are provided to be used instead of
│ the 'up/down' ones, which are supposed to be correlated/decorrelated between the different data
│ years.
│ Node counts: Category: 29, Binning: 42, Formula: 21
│ â•────────────────────────────────────────── â–¶ input ───────────────────────────────────────────╮
│ │ systematic (string) │
│ │ No description │
│ │ Values: central, down, down_correlated, down_uncorrelated, up, up_correlated, │
│ │ up_uncorrelated │
│ ╰──────────────────────────────────────────────────────────────────────────────────────────────╯
│ â•────────────────────────────────────────── â–¶ input ───────────────────────────────────────────╮
│ │ working_point (string) │
│ │ L/M/T │
│ │ Values: L, M, T │
│ ╰──────────────────────────────────────────────────────────────────────────────────────────────╯
│ â•────────────────────────────────────────── â–¶ input ───────────────────────────────────────────╮
│ │ flavor (int) │
│ │ hadron flavor definition: 5=b, 4=c, 0=udsg │
│ │ Values: 0 │
│ ╰──────────────────────────────────────────────────────────────────────────────────────────────╯
│ â•────────────────────────────────────────── â–¶ input ───────────────────────────────────────────╮
│ │ abseta (real) │
│ │ No description │
│ │ Range: [0.0, 2.5) │
│ ╰──────────────────────────────────────────────────────────────────────────────────────────────╯
│ â•────────────────────────────────────────── â–¶ input ───────────────────────────────────────────╮
│ │ pt (real) │
│ │ No description │
│ │ Range: [-inf, inf), overflow ok │
│ ╰──────────────────────────────────────────────────────────────────────────────────────────────╯
│ â•─── â—€ output ───╮
│ │ weight (real) │
│ │ No description │
│ ╰────────────────╯
├── 📈 deepCSV_mujets (v1)
│ deepCSV mujets working point scale factors for UL 2016postVFP b/c jets. For the working point
│ correction multiple different uncertainty schemes are provided. If only one year is analyzed,
│ the 'up' and 'down' systematics can be used. If the fullRunII data is analyzed,
│ 'up/down_correlated' and 'up/down_uncorrelated' systematics are provided to be used instead of
│ the 'up/down' ones, which are supposed to be correlated/decorrelated between the different data
│ years. If the impact of b-tagging in the analysis is very dominant a further breakdown of
│ uncertainties is provided. These broken-down sources consist of
│ 'up/down_jes/pileup/statistic/type3'. All of the sources can be correlated between the years,
│ except the 'statistic' source which is to be decorrelated between the years.
│ Node counts: Category: 61, Binning: 180, FormulaRef: 762, Formula: 2
│ â•────────────────────────────────────────── â–¶ input ───────────────────────────────────────────╮
│ │ systematic (string) │
│ │ No description │
│ │ Values: central, down, down_correlated, down_jes, down_pileup, down_statistic, down_type3, │
│ │ down_uncorrelated, up, up_correlated, up_jes, up_pileup, up_statistic, up_type3, │
│ │ up_uncorrelated │
│ ╰──────────────────────────────────────────────────────────────────────────────────────────────╯
│ â•────────────────────────────────────────── â–¶ input ───────────────────────────────────────────╮
│ │ working_point (string) │
│ │ L/M/T │
│ │ Values: L, M, T │
│ ╰──────────────────────────────────────────────────────────────────────────────────────────────╯
│ â•────────────────────────────────────────── â–¶ input ───────────────────────────────────────────╮
│ │ flavor (int) │
│ │ hadron flavor definition: 5=b, 4=c, 0=udsg │
│ │ Values: 4, 5 │
│ ╰──────────────────────────────────────────────────────────────────────────────────────────────╯
│ â•────────────────────────────────────────── â–¶ input ───────────────────────────────────────────╮
│ │ abseta (real) │
│ │ No description │
│ │ Range: [0.0, 2.5) │
│ ╰──────────────────────────────────────────────────────────────────────────────────────────────╯
│ â•────────────────────────────────────────── â–¶ input ───────────────────────────────────────────╮
│ │ pt (real) │
│ │ No description │
│ │ Range: [-inf, inf), overflow ok │
│ ╰──────────────────────────────────────────────────────────────────────────────────────────────╯
│ â•─── â—€ output ───╮
│ │ weight (real) │
│ │ No description │
│ ╰────────────────╯
├── 📈 deepCSV_comb (v1)
│ deepCSV comb working point scale factors for UL 2016postVFP b/c jets. For the working point
│ correction multiple different uncertainty schemes are provided. If only one year is analyzed,
│ the 'up' and 'down' systematics can be used. If the fullRunII data is analyzed,
│ 'up/down_correlated' and 'up/down_uncorrelated' systematics are provided to be used instead of
│ the 'up/down' ones, which are supposed to be correlated/decorrelated between the different data
│ years. If the impact of b-tagging in the analysis is very dominant a further breakdown of
│ uncertainties is provided. These broken-down sources consist of
│ 'up/down_isr/fsr/hdamp/jes/jer/pileup/qcdscale/statistic/topmass/type3'. All of the sources can
│ be correlated between the years, except the 'statistic' source which is to be decorrelated
│ between the years.
│ Node counts: Category: 109, Binning: 324, FormulaRef: 1410, Formula: 2
│ â•────────────────────────────────────────── â–¶ input ───────────────────────────────────────────╮
│ │ systematic (string) │
│ │ No description │
│ │ Values: central, down, down_correlated, down_fsr, down_hdamp, down_isr, down_jer, down_jes, │
│ │ down_pileup, down_qcdscale, down_statistic, down_topmass, down_type3, down_uncorrelated, up, │
│ │ up_correlated, up_fsr, up_hdamp, up_isr, up_jer, up_jes, up_pileup, up_qcdscale, │
│ │ up_statistic, up_topmass, up_type3, up_uncorrelated │
│ ╰──────────────────────────────────────────────────────────────────────────────────────────────╯
│ â•────────────────────────────────────────── â–¶ input ───────────────────────────────────────────╮
│ │ working_point (string) │
│ │ L/M/T │
│ │ Values: L, M, T │
│ ╰──────────────────────────────────────────────────────────────────────────────────────────────╯
│ â•────────────────────────────────────────── â–¶ input ───────────────────────────────────────────╮
│ │ flavor (int) │
│ │ hadron flavor definition: 5=b, 4=c, 0=udsg │
│ │ Values: 4, 5 │
│ ╰──────────────────────────────────────────────────────────────────────────────────────────────╯
│ â•────────────────────────────────────────── â–¶ input ───────────────────────────────────────────╮
│ │ abseta (real) │
│ │ No description │
│ │ Range: [0.0, 2.5) │
│ ╰──────────────────────────────────────────────────────────────────────────────────────────────╯
│ â•────────────────────────────────────────── â–¶ input ───────────────────────────────────────────╮
│ │ pt (real) │
│ │ No description │
│ │ Range: [-inf, inf), overflow ok │
│ ╰──────────────────────────────────────────────────────────────────────────────────────────────╯
│ â•─── â—€ output ───╮
│ │ weight (real) │
│ │ No description │
│ ╰────────────────╯
├── 📈 deepCSV_shape (v3)
│ deepCSV reshaping scale factors for UL 2016postVFP. The scale factors have 8 default uncertainty
│ sources (hf,lf,hfstats1/2,lfstats1/2,cferr1/2). All except the cferr1/2 uncertainties are to be
│ applied to light and b jets. The cferr1/2 uncertainties are to be applied to c jets.
│ hf/lfstats1/2 uncertainties are to be decorrelated between years, the others correlated.
│ Additional jes-varied scale factors are supplied to be applied for the jes variations.
│ Node counts: Category: 92, Binning: 2384, FormulaRef: 11439, Formula: 1
│ â•────────────────────────────────────────── â–¶ input ───────────────────────────────────────────╮
│ │ systematic (string) │
│ │ No description │
│ │ Values: central, down_cferr1, down_cferr2, down_hf, down_hfstats1, down_hfstats2, down_jes, │
│ │ down_jesAbsolute, down_jesAbsoluteMPFBias, down_jesAbsoluteScale, down_jesAbsoluteStat, │
│ │ down_jesAbsolute_2016, down_jesBBEC1, down_jesBBEC1_2016, down_jesEC2, down_jesEC2_2016, │
│ │ down_jesFlavorQCD, down_jesFragmentation, down_jesHF, down_jesHF_2016, down_jesPileUpDataMC, │
│ │ down_jesPileUpPtBB, down_jesPileUpPtEC1, down_jesPileUpPtEC2, down_jesPileUpPtHF, │
│ │ down_jesPileUpPtRef, down_jesRelativeBal, down_jesRelativeFSR, down_jesRelativeJEREC1, │
│ │ down_jesRelativeJEREC2, down_jesRelativeJERHF, down_jesRelativePtBB, down_jesRelativePtEC1, │
│ │ down_jesRelativePtEC2, down_jesRelativePtHF, down_jesRelativeSample, │
│ │ down_jesRelativeSample_2016, down_jesRelativeStatEC, down_jesRelativeStatFSR, │
│ │ down_jesRelativeStatHF, down_jesSinglePionECAL, down_jesSinglePionHCAL, down_jesTimePtEta, │
│ │ down_lf, down_lfstats1, down_lfstats2, up_cferr1, up_cferr2, up_hf, up_hfstats1, │
│ │ up_hfstats2, up_jes, up_jesAbsolute, up_jesAbsoluteMPFBias, up_jesAbsoluteScale, │
│ │ up_jesAbsoluteStat, up_jesAbsolute_2016, up_jesBBEC1, up_jesBBEC1_2016, up_jesEC2, │
│ │ up_jesEC2_2016, up_jesFlavorQCD, up_jesFragmentation, up_jesHF, up_jesHF_2016, │
│ │ up_jesPileUpDataMC, up_jesPileUpPtBB, up_jesPileUpPtEC1, up_jesPileUpPtEC2, │
│ │ up_jesPileUpPtHF, up_jesPileUpPtRef, up_jesRelativeBal, up_jesRelativeFSR, │
│ │ up_jesRelativeJEREC1, up_jesRelativeJEREC2, up_jesRelativeJERHF, up_jesRelativePtBB, │
│ │ up_jesRelativePtEC1, up_jesRelativePtEC2, up_jesRelativePtHF, up_jesRelativeSample, │
│ │ up_jesRelativeSample_2016, up_jesRelativeStatEC, up_jesRelativeStatFSR, │
│ │ up_jesRelativeStatHF, up_jesSinglePionECAL, up_jesSinglePionHCAL, up_jesTimePtEta, up_lf, │
│ │ up_lfstats1, up_lfstats2 │
│ ╰──────────────────────────────────────────────────────────────────────────────────────────────╯
│ â•────────────────────────────────────────── â–¶ input ───────────────────────────────────────────╮
│ │ flavor (int) │
│ │ hadron flavor definition: 5=b, 4=c, 0=udsg │
│ │ Values: 0, 4, 5 │
│ ╰──────────────────────────────────────────────────────────────────────────────────────────────╯
│ â•────────────────────────────────────────── â–¶ input ───────────────────────────────────────────╮
│ │ abseta (real) │
│ │ No description │
│ │ Range: [0.0, 2.5) │
│ ╰──────────────────────────────────────────────────────────────────────────────────────────────╯
│ â•────────────────────────────────────────── â–¶ input ───────────────────────────────────────────╮
│ │ pt (real) │
│ │ No description │
│ │ Range: [20.0, 10000.0), overflow ok │
│ ╰──────────────────────────────────────────────────────────────────────────────────────────────╯
│ â•────────────────────────────────────────── â–¶ input ───────────────────────────────────────────╮
│ │ discriminant (real) │
│ │ deepCSV output value │
│ │ Range: [-inf, inf), overflow ok │
│ ╰──────────────────────────────────────────────────────────────────────────────────────────────╯
│ â•─── â—€ output ───╮
│ │ weight (real) │
│ │ No description │
│ ╰────────────────╯
├── 📈 deepJet_wp_values (v1)
│ working points for deepJet in UL 2016postVFP.
│ Node counts: Category: 1
│ â•─────── â–¶ input ────────╮
│ │ working_point (string) │
│ │ L/M/T │
│ │ Values: L, M, T │
│ ╰────────────────────────╯
│ â•─── â—€ output ───╮
│ │ wp (real) │
│ │ No description │
│ ╰────────────────╯
├── 📈 deepJet_incl (v1)
│ deepJet incl working point scale factors for UL 2016postVFP light jets. For the working point
│ correction multiple different uncertainty schemes are provided. If only one year is analyzed,
│ the 'up' and 'down' systematics can be used. If the fullRunII data is analyzed,
│ 'up/down_correlated' and 'up/down_uncorrelated' systematics are provided to be used instead of
│ the 'up/down' ones, which are supposed to be correlated/decorrelated between the different data
│ years.
│ Node counts: Category: 29, Binning: 42, Formula: 21
│ â•────────────────────────────────────────── â–¶ input ───────────────────────────────────────────╮
│ │ systematic (string) │
│ │ No description │
│ │ Values: central, down, down_correlated, down_uncorrelated, up, up_correlated, │
│ │ up_uncorrelated │
│ ╰──────────────────────────────────────────────────────────────────────────────────────────────╯
│ â•────────────────────────────────────────── â–¶ input ───────────────────────────────────────────╮
│ │ working_point (string) │
│ │ L/M/T │
│ │ Values: L, M, T │
│ ╰──────────────────────────────────────────────────────────────────────────────────────────────╯
│ â•────────────────────────────────────────── â–¶ input ───────────────────────────────────────────╮
│ │ flavor (int) │
│ │ hadron flavor definition: 5=b, 4=c, 0=udsg │
│ │ Values: 0 │
│ ╰──────────────────────────────────────────────────────────────────────────────────────────────╯
│ â•────────────────────────────────────────── â–¶ input ───────────────────────────────────────────╮
│ │ abseta (real) │
│ │ No description │
│ │ Range: [0.0, 2.5) │
│ ╰──────────────────────────────────────────────────────────────────────────────────────────────╯
│ â•────────────────────────────────────────── â–¶ input ───────────────────────────────────────────╮
│ │ pt (real) │
│ │ No description │
│ │ Range: [-inf, inf), overflow ok │
│ ╰──────────────────────────────────────────────────────────────────────────────────────────────╯
│ â•─── â—€ output ───╮
│ │ weight (real) │
│ │ No description │
│ ╰────────────────╯
├── 📈 deepJet_mujets (v1)
│ deepJet mujets working point scale factors for UL 2016postVFP b/c jets. For the working point
│ correction multiple different uncertainty schemes are provided. If only one year is analyzed,
│ the 'up' and 'down' systematics can be used. If the fullRunII data is analyzed,
│ 'up/down_correlated' and 'up/down_uncorrelated' systematics are provided to be used instead of
│ the 'up/down' ones, which are supposed to be correlated/decorrelated between the different data
│ years. If the impact of b-tagging in the analysis is very dominant a further breakdown of
│ uncertainties is provided. These broken-down sources consist of
│ 'up/down_jes/pileup/statistic/type3'. All of the sources can be correlated between the years,
│ except the 'statistic' source which is to be decorrelated between the years.
│ Node counts: Category: 61, Binning: 180, FormulaRef: 762, Formula: 2
│ â•────────────────────────────────────────── â–¶ input ───────────────────────────────────────────╮
│ │ systematic (string) │
│ │ No description │
│ │ Values: central, down, down_correlated, down_jes, down_pileup, down_statistic, down_type3, │
│ │ down_uncorrelated, up, up_correlated, up_jes, up_pileup, up_statistic, up_type3, │
│ │ up_uncorrelated │
│ ╰──────────────────────────────────────────────────────────────────────────────────────────────╯
│ â•────────────────────────────────────────── â–¶ input ───────────────────────────────────────────╮
│ │ working_point (string) │
│ │ L/M/T │
│ │ Values: L, M, T │
│ ╰──────────────────────────────────────────────────────────────────────────────────────────────╯
│ â•────────────────────────────────────────── â–¶ input ───────────────────────────────────────────╮
│ │ flavor (int) │
│ │ hadron flavor definition: 5=b, 4=c, 0=udsg │
│ │ Values: 4, 5 │
│ ╰──────────────────────────────────────────────────────────────────────────────────────────────╯
│ â•────────────────────────────────────────── â–¶ input ───────────────────────────────────────────╮
│ │ abseta (real) │
│ │ No description │
│ │ Range: [0.0, 2.5) │
│ ╰──────────────────────────────────────────────────────────────────────────────────────────────╯
│ â•────────────────────────────────────────── â–¶ input ───────────────────────────────────────────╮
│ │ pt (real) │
│ │ No description │
│ │ Range: [-inf, inf), overflow ok │
│ ╰──────────────────────────────────────────────────────────────────────────────────────────────╯
│ â•─── â—€ output ───╮
│ │ weight (real) │
│ │ No description │
│ ╰────────────────╯
├── 📈 deepJet_comb (v1)
│ deepJet comb working point scale factors for UL 2016postVFP b/c jets. For the working point
│ correction multiple different uncertainty schemes are provided. If only one year is analyzed,
│ the 'up' and 'down' systematics can be used. If the fullRunII data is analyzed,
│ 'up/down_correlated' and 'up/down_uncorrelated' systematics are provided to be used instead of
│ the 'up/down' ones, which are supposed to be correlated/decorrelated between the different data
│ years. If the impact of b-tagging in the analysis is very dominant a further breakdown of
│ uncertainties is provided. These broken-down sources consist of
│ 'up/down_isr/fsr/hdamp/jes/jer/pileup/qcdscale/statistic/topmass/type3'. All of the sources can
│ be correlated between the years, except the 'statistic' source which is to be decorrelated
│ between the years.
│ Node counts: Category: 109, Binning: 324, FormulaRef: 1410, Formula: 2
│ â•────────────────────────────────────────── â–¶ input ───────────────────────────────────────────╮
│ │ systematic (string) │
│ │ No description │
│ │ Values: central, down, down_correlated, down_fsr, down_hdamp, down_isr, down_jer, down_jes, │
│ │ down_pileup, down_qcdscale, down_statistic, down_topmass, down_type3, down_uncorrelated, up, │
│ │ up_correlated, up_fsr, up_hdamp, up_isr, up_jer, up_jes, up_pileup, up_qcdscale, │
│ │ up_statistic, up_topmass, up_type3, up_uncorrelated │
│ ╰──────────────────────────────────────────────────────────────────────────────────────────────╯
│ â•────────────────────────────────────────── â–¶ input ───────────────────────────────────────────╮
│ │ working_point (string) │
│ │ L/M/T │
│ │ Values: L, M, T │
│ ╰──────────────────────────────────────────────────────────────────────────────────────────────╯
│ â•────────────────────────────────────────── â–¶ input ───────────────────────────────────────────╮
│ │ flavor (int) │
│ │ hadron flavor definition: 5=b, 4=c, 0=udsg │
│ │ Values: 4, 5 │
│ ╰──────────────────────────────────────────────────────────────────────────────────────────────╯
│ â•────────────────────────────────────────── â–¶ input ───────────────────────────────────────────╮
│ │ abseta (real) │
│ │ No description │
│ │ Range: [0.0, 2.5) │
│ ╰──────────────────────────────────────────────────────────────────────────────────────────────╯
│ â•────────────────────────────────────────── â–¶ input ───────────────────────────────────────────╮
│ │ pt (real) │
│ │ No description │
│ │ Range: [-inf, inf), overflow ok │
│ ╰──────────────────────────────────────────────────────────────────────────────────────────────╯
│ â•─── â—€ output ───╮
│ │ weight (real) │
│ │ No description │
│ ╰────────────────╯
└── 📈 deepJet_shape (v3)
deepJet reshaping scale factors for UL 2016postVFP. The scale factors have 8 default uncertainty
sources (hf,lf,hfstats1/2,lfstats1/2,cferr1/2). All except the cferr1/2 uncertainties are to be
applied to light and b jets. The cferr1/2 uncertainties are to be applied to c jets.
hf/lfstats1/2 uncertainties are to be decorrelated between years, the others correlated.
Additional jes-varied scale factors are supplied to be applied for the jes variations.
Node counts: Category: 92, Binning: 2384, FormulaRef: 11439, Formula: 1
â•────────────────────────────────────────── â–¶ input ───────────────────────────────────────────╮
│ systematic (string) │
│ No description │
│ Values: central, down_cferr1, down_cferr2, down_hf, down_hfstats1, down_hfstats2, down_jes, │
│ down_jesAbsolute, down_jesAbsoluteMPFBias, down_jesAbsoluteScale, down_jesAbsoluteStat, │
│ down_jesAbsolute_2016, down_jesBBEC1, down_jesBBEC1_2016, down_jesEC2, down_jesEC2_2016, │
│ down_jesFlavorQCD, down_jesFragmentation, down_jesHF, down_jesHF_2016, down_jesPileUpDataMC, │
│ down_jesPileUpPtBB, down_jesPileUpPtEC1, down_jesPileUpPtEC2, down_jesPileUpPtHF, │
│ down_jesPileUpPtRef, down_jesRelativeBal, down_jesRelativeFSR, down_jesRelativeJEREC1, │
│ down_jesRelativeJEREC2, down_jesRelativeJERHF, down_jesRelativePtBB, down_jesRelativePtEC1, │
│ down_jesRelativePtEC2, down_jesRelativePtHF, down_jesRelativeSample, │
│ down_jesRelativeSample_2016, down_jesRelativeStatEC, down_jesRelativeStatFSR, │
│ down_jesRelativeStatHF, down_jesSinglePionECAL, down_jesSinglePionHCAL, down_jesTimePtEta, │
│ down_lf, down_lfstats1, down_lfstats2, up_cferr1, up_cferr2, up_hf, up_hfstats1, │
│ up_hfstats2, up_jes, up_jesAbsolute, up_jesAbsoluteMPFBias, up_jesAbsoluteScale, │
│ up_jesAbsoluteStat, up_jesAbsolute_2016, up_jesBBEC1, up_jesBBEC1_2016, up_jesEC2, │
│ up_jesEC2_2016, up_jesFlavorQCD, up_jesFragmentation, up_jesHF, up_jesHF_2016, │
│ up_jesPileUpDataMC, up_jesPileUpPtBB, up_jesPileUpPtEC1, up_jesPileUpPtEC2, │
│ up_jesPileUpPtHF, up_jesPileUpPtRef, up_jesRelativeBal, up_jesRelativeFSR, │
│ up_jesRelativeJEREC1, up_jesRelativeJEREC2, up_jesRelativeJERHF, up_jesRelativePtBB, │
│ up_jesRelativePtEC1, up_jesRelativePtEC2, up_jesRelativePtHF, up_jesRelativeSample, │
│ up_jesRelativeSample_2016, up_jesRelativeStatEC, up_jesRelativeStatFSR, │
│ up_jesRelativeStatHF, up_jesSinglePionECAL, up_jesSinglePionHCAL, up_jesTimePtEta, up_lf, │
│ up_lfstats1, up_lfstats2 │
╰──────────────────────────────────────────────────────────────────────────────────────────────╯
â•────────────────────────────────────────── â–¶ input ───────────────────────────────────────────╮
│ flavor (int) │
│ hadron flavor definition: 5=b, 4=c, 0=udsg │
│ Values: 0, 4, 5 │
╰──────────────────────────────────────────────────────────────────────────────────────────────╯
â•────────────────────────────────────────── â–¶ input ───────────────────────────────────────────╮
│ abseta (real) │
│ No description │
│ Range: [0.0, 2.5) │
╰──────────────────────────────────────────────────────────────────────────────────────────────╯
â•────────────────────────────────────────── â–¶ input ───────────────────────────────────────────╮
│ pt (real) │
│ No description │
│ Range: [20.0, 10000.0), overflow ok │
╰──────────────────────────────────────────────────────────────────────────────────────────────╯
â•────────────────────────────────────────── â–¶ input ───────────────────────────────────────────╮
│ discriminant (real) │
│ deepJet output value │
│ Range: [-inf, inf), overflow ok │
╰──────────────────────────────────────────────────────────────────────────────────────────────╯
â•─── â—€ output ───╮
│ weight (real) │
│ No description │
╰────────────────╯