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setname: "CMS_TTBAR_13TEV_2L_DIF" | ||
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nnpdf_metadata: | ||
nnpdf31_process: "TOP" | ||
experiment: "CMS" | ||
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arXiv: | ||
url: "https://arxiv.org/abs/1811.06625" | ||
iNSPIRE: | ||
url: "https://inspirehep.net/literature/1703993" | ||
hepdata: | ||
url: "https://www.hepdata.net/record/ins1703993" | ||
version: 1 | ||
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version: 1 | ||
version_comment: "NA" | ||
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implemented_observables: | ||
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- observable: {description: "differential cross section w.r.t. transverse momentum of t", label: '$\frac{d\sigma}{dpT_{t}}$', units: "$\frac{pb}{GeV}$"} | ||
observable_name: PTT | ||
process_type: HQP_PTQ | ||
ndata: 6 | ||
tables: [1] | ||
kinematics: | ||
variables: | ||
pT_t: {description: "transverse momentum of t", label: '$pT_{t}$', units: "$GeV$"} | ||
mt_sqr: {description: "mass of top quark squared", label: '$m_{t}^2$', units: '$GeV^2$'} | ||
sqrt_s: {description: "center of mass energy", label: '$\sqrt{s}$', units: "$GeV$"} | ||
file: kinematics_dSig_dpTt.yaml | ||
data_central: data_dSig_dpTt.yaml | ||
data_uncertainties: | ||
- uncertainties_dSig_dpTt.yaml | ||
kinematic_coverage: [pT_t, mt_sqr, sqrt_s] | ||
plotting: | ||
dataset_label: 'CMS 13 TeV TTB dilepton channel: $\frac{d\sigma}{dpT_{t}}$' | ||
kinematics_override: identity | ||
x_scale: log | ||
plot_x: pT_t | ||
figure_by: | ||
- sqrt_s | ||
theory: | ||
FK_tables: | ||
- - CMS_TTBAR_13TEV_2L_DIF_PTT | ||
operation: 'null' | ||
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- observable: {description: "normalized differential cross section w.r.t. transverse momentum of t", label: '$\frac{1}{\sigma}\frac{d\sigma}{dpT_{t}}$', units: "$\frac{1}{GeV}$"} | ||
observable_name: PTT-NORM | ||
process_type: HQP_PTQ | ||
ndata: 5 | ||
tables: [2] | ||
kinematics: | ||
variables: | ||
pT_t: {description: "transverse momentum of t", label: '$pT_{t}$', units: "$GeV$"} | ||
mt_sqr: {description: "mass of top quark squared", label: '$m_{t}^2$', units: '$GeV^2$'} | ||
sqrt_s: {description: "center of mass energy", label: '$\sqrt{s}$', units: "$GeV$"} | ||
file: kinematics_dSig_dpTt_norm.yaml | ||
data_central: data_dSig_dpTt_norm.yaml | ||
data_uncertainties: | ||
- uncertainties_dSig_dpTt_norm.yaml | ||
kinematic_coverage: [pT_t, mt_sqr, sqrt_s] | ||
plotting: | ||
dataset_label: 'CMS 13 TeV TTB dilepton channel: $\frac{1}{\sigma}\frac{d\sigma}{dpT_{t}}$' | ||
kinematics_override: identity | ||
x_scale: log | ||
plot_x: pT_t | ||
figure_by: | ||
- sqrt_s | ||
theory: | ||
FK_tables: | ||
- - CMS_TTBAR_13TEV_2L_DIF_PTT | ||
- - CMS_TTBAR_13TEV_TOT_X-SEC | ||
operation: 'ratio' | ||
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- observable: {description: "differential cross section w.r.t. invariant mass of ttBar pair", label: '$\frac{d\sigma}{dm_{t\bar{t}}}$', units: "$\frac{pb}{GeV}$"} | ||
observable_name: MTTBAR | ||
process_type: HQP_MQQ | ||
ndata: 7 | ||
tables: [45] | ||
kinematics: | ||
variables: | ||
m_ttBar: {description: "invariant mass of ttBar pair", label: '$m_{t\bar{t}}$', units: "$GeV$"} | ||
mt_sqr: {description: "mass of top quark squared", label: '$m_{t}^2$', units: '$GeV^2$'} | ||
sqrt_s: {description: "center of mass energy", label: '$\sqrt{s}$', units: "$GeV$"} | ||
file: kinematics_dSig_dmttBar.yaml | ||
data_central: data_dSig_dmttBar.yaml | ||
data_uncertainties: | ||
- uncertainties_dSig_dmttBar.yaml | ||
kinematic_coverage: [m_ttBar, mt_sqr, sqrt_s] | ||
plotting: | ||
dataset_label: 'CMS 13 TeV TTB dilepton channel: $\frac{d\sigma}{dm_{t\bar{t}}}$' | ||
kinematics_override: identity | ||
x_scale: log | ||
plot_x: m_ttBar | ||
figure_by: | ||
- sqrt_s | ||
theory: | ||
FK_tables: | ||
- - CMS_TTBAR_13TEV_2L_DIF_MTTBAR | ||
operation: 'null' | ||
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||
- observable: {description: "normalized differential cross section w.r.t. invariant mass of ttBar pair", label: '$\frac{1}{\sigma}\frac{d\sigma}{dm_{t\bar{t}}}$', units: "$\frac{1}{GeV}$"} | ||
observable_name: MTTBAR-NORM | ||
process_type: HQP_MQQ | ||
ndata: 6 | ||
tables: [46] | ||
kinematics: | ||
variables: | ||
m_ttBar: {description: "invariant mass of ttBar pair", label: '$m_{t\bar{t}}$', units: "$GeV$"} | ||
mt_sqr: {description: "mass of top quark squared", label: '$m_{t}^2$', units: '$GeV^2$'} | ||
sqrt_s: {description: "center of mass energy", label: '$\sqrt{s}$', units: "$GeV$"} | ||
file: kinematics_dSig_dmttBar_norm.yaml | ||
data_central: data_dSig_dmttBar_norm.yaml | ||
data_uncertainties: | ||
- uncertainties_dSig_dmttBar_norm.yaml | ||
kinematic_coverage: [m_ttBar, mt_sqr, sqrt_s] | ||
plotting: | ||
dataset_label: 'CMS 13 TeV TTB dilepton channel: $\frac{1}{\sigma}\frac{d\sigma}{dm_{t\bar{t}}}$' | ||
kinematics_override: identity | ||
x_scale: log | ||
plot_x: m_ttBar | ||
figure_by: | ||
- sqrt_s | ||
theory: | ||
FK_tables: | ||
- - CMS_TTBAR_13TEV_2L_DIF_MTTBAR | ||
- - CMS_TTBAR_13TEV_TOT_X-SEC | ||
operation: 'ratio' | ||
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||
- observable: {description: "differential cross section w.r.t. rapidity of t", label: '$\frac{d\sigma}{dy_{t}}$', units: "$pb$"} | ||
observable_name: YT | ||
process_type: HQP_YQ | ||
ndata: 10 | ||
tables: [21] | ||
kinematics: | ||
variables: | ||
y_t: {description: "rapidity of t", label: '$y_{t}$', units: ""} | ||
mt_sqr: {description: "mass of top quark squared", label: '$m_{t}^2$', units: '$GeV^2$'} | ||
sqrt_s: {description: "center of mass energy", label: '$\sqrt{s}$', units: "$GeV$"} | ||
file: kinematics_dSig_dyt.yaml | ||
data_central: data_dSig_dyt.yaml | ||
data_uncertainties: | ||
- uncertainties_dSig_dyt.yaml | ||
kinematic_coverage: [y_t, mt_sqr, sqrt_s] | ||
plotting: | ||
dataset_label: 'CMS 13 TeV TTB dilepton channel: $\frac{d\sigma}{dy_{t}}$' | ||
kinematics_override: identity | ||
x_scale: log | ||
plot_x: y_t | ||
figure_by: | ||
- sqrt_s | ||
theory: | ||
FK_tables: | ||
- - CMS_TTBAR_13TEV_2L_DIF_YT | ||
operation: 'null' | ||
|
||
- observable: {description: "normalized differential cross section w.r.t. rapidity of t", label: '$\frac{1}{\sigma}\frac{d\sigma}{dy_{t}}$', units: ""} | ||
observable_name: YT-NORM | ||
process_type: HQP_YQ | ||
ndata: 9 | ||
tables: [22] | ||
kinematics: | ||
variables: | ||
y_t: {description: "rapidity of t", label: '$y_{t}$', units: ""} | ||
mt_sqr: {description: "mass of top quark squared", label: '$m_{t}^2$', units: '$GeV^2$'} | ||
sqrt_s: {description: "center of mass energy", label: '$\sqrt{s}$', units: "$GeV$"} | ||
file: kinematics_dSig_dyt_norm.yaml | ||
data_central: data_dSig_dyt_norm.yaml | ||
data_uncertainties: | ||
- uncertainties_dSig_dyt_norm.yaml | ||
kinematic_coverage: [y_t, mt_sqr, sqrt_s] | ||
plotting: | ||
dataset_label: 'CMS 13 TeV TTB dilepton channel: $\frac{1}{\sigma}\frac{d\sigma}{dy_{t}}$' | ||
kinematics_override: identity | ||
x_scale: log | ||
plot_x: y_t | ||
figure_by: | ||
- sqrt_s | ||
theory: | ||
FK_tables: | ||
- - CMS_TTBAR_13TEV_2L_DIF_YT | ||
- - CMS_TTBAR_13TEV_TOT_X-SEC | ||
operation: 'ratio' | ||
|
||
- observable: {description: "differential cross section w.r.t. rapidity of ttBar pair", label: '$\frac{d\sigma}{dy_{t\bar{t}}}$', units: "$pb$"} | ||
observable_name: YTTBAR | ||
process_type: HQP_YQQ | ||
ndata: 10 | ||
tables: [41] | ||
kinematics: | ||
variables: | ||
y_ttBar: {description: "rapidity of ttBar pair", label: '$y_{t\bar{t}}$', units: ""} | ||
mt_sqr: {description: "mass of top quark squared", label: '$m_{t}^2$', units: '$GeV^2$'} | ||
sqrt_s: {description: "center of mass energy", label: '$\sqrt{s}$', units: "$GeV$"} | ||
file: kinematics_dSig_dyttBar.yaml | ||
data_central: data_dSig_dyttBar.yaml | ||
data_uncertainties: | ||
- uncertainties_dSig_dyttBar.yaml | ||
kinematic_coverage: [y_ttBar, mt_sqr, sqrt_s] | ||
plotting: | ||
dataset_label: 'CMS 13 TeV TTB dilepton channel: $\frac{d\sigma}{dy_{t\bar{t}}}$' | ||
kinematics_override: identity | ||
x_scale: log | ||
plot_x: y_ttBar | ||
figure_by: | ||
- sqrt_s | ||
theory: | ||
FK_tables: | ||
- - CMS_TTBAR_13TEV_2L_DIF_YTTBAR | ||
operation: 'null' | ||
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||
- observable: {description: "normalized differential cross section w.r.t. rapidity of ttBar pair", label: '$\frac{1}{\sigma}\frac{d\sigma}{dy_{t\bar{t}}}$', units: ""} | ||
observable_name: YTTBAR-NORM | ||
process_type: HQP_YQQ | ||
ndata: 9 | ||
tables: [42] | ||
kinematics: | ||
variables: | ||
y_ttBar: {description: "rapidity of ttBar pair", label: '$y_{t\bar{t}}$', units: ""} | ||
mt_sqr: {description: "mass of top quark squared", label: '$m_{t}^2$', units: '$GeV^2$'} | ||
sqrt_s: {description: "center of mass energy", label: '$\sqrt{s}$', units: "$GeV$"} | ||
file: kinematics_dSig_dyttBar_norm.yaml | ||
data_central: data_dSig_dyttBar_norm.yaml | ||
data_uncertainties: | ||
- uncertainties_dSig_dyttBar_norm.yaml | ||
kinematic_coverage: [y_ttBar, mt_sqr, sqrt_s] | ||
plotting: | ||
dataset_label: 'CMS 13 TeV TTB dilepton channel: $\frac{1}{\sigma}\frac{d\sigma}{dy_{t\bar{t}}}$' | ||
kinematics_override: identity | ||
x_scale: log | ||
plot_x: y_ttBar | ||
figure_by: | ||
- sqrt_s | ||
theory: | ||
FK_tables: | ||
- - CMS_TTBAR_13TEV_2L_DIF_YTTBAR | ||
- - CMS_TTBAR_13TEV_TOT_X-SEC | ||
operation: 'ratio' |
39 changes: 39 additions & 0 deletions
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buildmaster/CMS_TTBAR_13TEV_2L_DIF/rawdata/d01-x01-y01.yaml
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dependent_variables: | ||
- header: {name: '$\frac{d\sigma}{dX}$', units: PB/GEV} | ||
qualifiers: | ||
- {name: RE, value: P P --> TOP TOPBAR X} | ||
- {name: SQRT(S), units: GEV, value: '13000.0'} | ||
values: | ||
- errors: | ||
- {label: stat, symerror: 0.0389853} | ||
- {label: sys, symerror: 0.277739} | ||
value: 3.48728 | ||
- errors: | ||
- {label: stat, symerror: 0.0504538} | ||
- {label: sys, symerror: 0.467258} | ||
value: 5.09407 | ||
- errors: | ||
- {label: stat, symerror: 0.0257184} | ||
- {label: sys, symerror: 0.21118} | ||
value: 2.83826 | ||
- errors: | ||
- {label: stat, symerror: 0.0105405} | ||
- {label: sys, symerror: 0.0514395} | ||
value: 0.842426 | ||
- errors: | ||
- {label: stat, symerror: 0.00293571} | ||
- {label: sys, symerror: 0.0130281} | ||
value: 0.187431 | ||
- errors: | ||
- {label: stat, symerror: 0.00130963} | ||
- {label: sys, symerror: 0.00302404} | ||
value: 0.0345005 | ||
independent_variables: | ||
- header: {name: '$p_{T}^{t}$ [GEV]'} | ||
values: | ||
- {high: 65, low: 0} | ||
- {high: 125, low: 65} | ||
- {high: 200, low: 125} | ||
- {high: 290, low: 200} | ||
- {high: 400, low: 290} | ||
- {high: 550, low: 400} |
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