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setname: 'ATLAS_TTBAR_13TEV_LJ_DIF' | ||
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nnpdf_metadata: | ||
nnpdf31_process: "TOP" | ||
experiment: "ATLAS" | ||
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arXiv: | ||
url: "https://arxiv.org/abs/1908.07305" | ||
iNSPIRE: | ||
url: "https://inspirehep.net/literature/1750330" | ||
hepdata: | ||
url: "https://www.hepdata.net/record/ins1750330" | ||
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. ttBar invariant mass", label: '$\frac{d\sigma}{dm_{t\bar{t}}}$', units: "$\frac{pb}{GeV}$"} | ||
observable_name: MTTBAR | ||
process_type: HQP_MQQ | ||
ndata: 9 | ||
tables: [618] | ||
kinematics: | ||
variables: | ||
m_ttBar: {description: "invariant mass of ttBar", 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: 'ATLAS 13 TeV top quark pair l+j 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: | ||
- - ATLAS_TTBAR_13TEV_LJ_DIF_MTTBAR | ||
operation: 'null' | ||
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||
- observable: {description: "normalized differential cross section w.r.t. ttBar invariant mass", label: '$\frac{1}{\sigma}\frac{d\sigma}{dm_{t\bar{t}}}$', units: "$\frac{1}{GeV}$"} | ||
observable_name: MTTBAR-NORM | ||
process_type: HQP_MQQ | ||
ndata: 9 | ||
tables: [616] | ||
kinematics: | ||
variables: | ||
m_ttBar: {description: "invariant mass of ttBar", 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: 'ATLAS 13 TeV top quark pair l+j 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: | ||
- - ATLAS_TTBAR_13TEV_LJ_DIF_MTTBAR | ||
- - ATLAS_TTBAR_13TEV_TOT_X-SEC | ||
operation: 'ratio' | ||
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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: 8 | ||
tables: [610] | ||
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: 'ATLAS 13 TeV top quark pair l+j channel: $\frac{d\sigma}{dpT_t}$' | ||
kinematics_override: identity | ||
x_scale: log | ||
plot_x: pT_t | ||
figure_by: | ||
- sqrt_s | ||
theory: | ||
FK_tables: | ||
- - ATLAS_TTBAR_13TEV_LJ_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: 8 | ||
tables: [608] | ||
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: 'ATLAS 13 TeV top quark pair l+j 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: | ||
- - ATLAS_TTBAR_13TEV_LJ_DIF_PTT | ||
- - ATLAS_TTBAR_13TEV_TOT_X-SEC | ||
operation: 'ratio' | ||
|
||
- observable: {description: "differential cross section w.r.t. absolute rapidity of t", label: '$\frac{d\sigma}{d|y_{t}|}$', units: "$pb$"} | ||
observable_name: YT | ||
process_type: HQP_YQ | ||
ndata: 5 | ||
tables: [614] | ||
kinematics: | ||
variables: | ||
y_t: {description: "absolute 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: 'ATLAS 13 TeV top quark pair l+j channel: $\frac{d\sigma}{d|y_{t}|}$' | ||
kinematics_override: identity | ||
x_scale: log | ||
plot_x: y_t | ||
figure_by: | ||
- sqrt_s | ||
theory: | ||
FK_tables: | ||
- - ATLAS_TTBAR_13TEV_LJ_DIF_YT | ||
operation: 'null' | ||
|
||
- observable: {description: "normalized differential cross section w.r.t. absolute rapidity of t", label: '$\frac{1}{\sigma}\frac{d\sigma}{d|y_{t}|}$', units: ""} | ||
observable_name: YT-NORM | ||
process_type: HQP_YQ | ||
ndata: 5 | ||
tables: [612] | ||
kinematics: | ||
variables: | ||
y_t: {description: "absolute 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: 'ATLAS 13 TeV top quark pair l+j channel: $\frac{1}{\sigma}\frac{d\sigma}{d|y_{t}|}$' | ||
kinematics_override: identity | ||
x_scale: log | ||
plot_x: y_t | ||
figure_by: | ||
- sqrt_s | ||
theory: | ||
FK_tables: | ||
- - ATLAS_TTBAR_13TEV_LJ_DIF_YT | ||
- - ATLAS_TTBAR_13TEV_TOT_X-SEC | ||
operation: 'ratio' | ||
|
||
- observable: {description: "differential cross section w.r.t. absolute rapidity of ttBar", label: '$\frac{d\sigma}{d|y_{t\bar{t}}|}$', units: "$pb$"} | ||
observable_name: YTTBAR | ||
process_type: HQP_YQQ | ||
ndata: 7 | ||
tables: [626] | ||
kinematics: | ||
variables: | ||
y_ttBar: {description: "absolute rapidity of ttBar", 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: 'ATLAS 13 TeV top quark pair l+j channel: $\frac{d\sigma}{d|y_{t\bar{t}}|}$' | ||
kinematics_override: identity | ||
x_scale: log | ||
plot_x: y_ttBar | ||
figure_by: | ||
- sqrt_s | ||
theory: | ||
FK_tables: | ||
- - ATLAS_TTBAR_13TEV_LJ_DIF_YTTBAR | ||
operation: 'null' | ||
|
||
- observable: {description: "normalized differential cross section w.r.t. absolute rapidity of ttBar", label: '$\frac{1}{\sigma}\frac{d\sigma}{d|y_{t\bar{t}}|}$', units: ""} | ||
observable_name: YTTBAR-NORM | ||
process_type: HQP_YQQ | ||
ndata: 7 | ||
tables: [624] | ||
kinematics: | ||
variables: | ||
y_ttBar: {description: "absolute rapidity of ttBar", 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: 'ATLAS 13 TeV top quark pair l+j channel: $\frac{1}{\sigma}\frac{d\sigma}{d|y_{t\bar{t}}|}$' | ||
kinematics_override: identity | ||
x_scale: log | ||
plot_x: y_ttBar | ||
figure_by: | ||
- sqrt_s | ||
theory: | ||
FK_tables: | ||
- - ATLAS_TTBAR_13TEV_LJ_DIF_YTTBAR | ||
- - ATLAS_TTBAR_13TEV_TOT_X-SEC | ||
operation: 'ratio' |
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