diff --git a/buildmaster/meta/ATLAS_TOPDIFF_DILEPT_8TEV_TTRAPNORM.yaml b/buildmaster/meta/ATLAS_TOPDIFF_DILEPT_8TEV_TTRAPNORM.yaml index 91c386de4..afaed66d0 100644 --- a/buildmaster/meta/ATLAS_TOPDIFF_DILEPT_8TEV_TTRAPNORM.yaml +++ b/buildmaster/meta/ATLAS_TOPDIFF_DILEPT_8TEV_TTRAPNORM.yaml @@ -1,4 +1,4 @@ ndata: 5 nsys: 5 setname: "ATLAS_TOPDIFF_DILEPT_8TEV_TTRAPNORM" -proctype: "HQP_YQ" +proctype: "HQP_YQQ" diff --git a/nnpdfcpp/data/NNLOCFAC/CF_QCD_CMS_TTB_DIFF_13TEV_2016_2L_TTMNORM_DEN.dat b/nnpdfcpp/data/NNLOCFAC/CF_QCD_CMS_TTB_DIFF_13TEV_2016_2L_TTMNORM_DEN.dat index c8a699ea2..181c31090 100644 --- a/nnpdfcpp/data/NNLOCFAC/CF_QCD_CMS_TTB_DIFF_13TEV_2016_2L_TTMNORM_DEN.dat +++ b/nnpdfcpp/data/NNLOCFAC/CF_QCD_CMS_TTB_DIFF_13TEV_2016_2L_TTMNORM_DEN.dat @@ -13,4 +13,3 @@ Warnings: 1.07030 0.00000 1.07030 0.00000 1.07030 0.00000 -1.07030 0.00000 diff --git a/nnpdfcpp/data/NNLOCFAC/CF_QCD_CMS_TTB_DIFF_13TEV_2016_2L_TTMNORM_NUM.dat b/nnpdfcpp/data/NNLOCFAC/CF_QCD_CMS_TTB_DIFF_13TEV_2016_2L_TTMNORM_NUM.dat index 9e2f6fbc7..efb970017 100644 --- a/nnpdfcpp/data/NNLOCFAC/CF_QCD_CMS_TTB_DIFF_13TEV_2016_2L_TTMNORM_NUM.dat +++ b/nnpdfcpp/data/NNLOCFAC/CF_QCD_CMS_TTB_DIFF_13TEV_2016_2L_TTMNORM_NUM.dat @@ -13,4 +13,3 @@ Warnings: 1.08225 0.00000 1.09178 0.00000 1.09284 0.00000 -1.12079 0.00000 diff --git a/nnpdfcpp/data/commondata/DATA_ATLAS_TOPDIFF_DILEPT_8TEV_TTRAPNORM.dat b/nnpdfcpp/data/commondata/DATA_ATLAS_TOPDIFF_DILEPT_8TEV_TTRAPNORM.dat index 78c5b9031..44b2d4bfb 100644 --- a/nnpdfcpp/data/commondata/DATA_ATLAS_TOPDIFF_DILEPT_8TEV_TTRAPNORM.dat +++ b/nnpdfcpp/data/commondata/DATA_ATLAS_TOPDIFF_DILEPT_8TEV_TTRAPNORM.dat @@ -1,6 +1,6 @@ ATLAS_TOPDIFF_DILEPT_8TEV_TTRAPNORM 5 5 - 1 HQP_YQ 2.000000000000e-01 3.003289000000e+04 8.000000000000e+03 8.210000000000e-01 0.000000000000e+00 2.880822776869e-02 3.508919338452e+00 -8.379445396709e-03 -1.020638903375e+00 -8.308848565496e-03 -1.012040020158e+00 -1.007667443919e-03 -1.227365948744e-01 -8.276176108275e-05 -1.008060427317e-02 - 2 HQP_YQ 6.000000000000e-01 3.003289000000e+04 8.000000000000e+03 7.210000000000e-01 0.000000000000e+00 -2.065837286933e-02 -2.865238955524e+00 -1.798747836570e-02 -2.494795889834e+00 -5.635869564862e-03 -7.816740034483e-01 -1.753133177919e-03 -2.431530066462e-01 -1.070081468065e-04 -1.484162923807e-02 - 3 HQP_YQ 1.000000000000e+00 3.003289000000e+04 8.000000000000e+03 4.990000000000e-01 0.000000000000e+00 -9.477603208718e-03 -1.899319280304e+00 1.411259972037e-02 2.828176296668e+00 -1.278787511604e-02 -2.562700424056e+00 -6.230360112141e-05 -1.248569160750e-02 5.901562153626e-06 1.182677786298e-03 - 4 HQP_YQ 1.600000000000e+00 3.003289000000e+04 8.000000000000e+03 2.060000000000e-01 0.000000000000e+00 8.295367941452e-04 4.026877641482e-01 4.398008172997e-03 2.134955423785e+00 2.136815949654e-03 1.037289295948e+00 -9.026705106575e-03 -4.381895682804e+00 -3.641501526012e-04 -1.767719187384e-01 - 5 HQP_YQ 2.400000000000e+00 3.003289000000e+04 8.000000000000e+03 2.260000000000e-02 0.000000000000e+00 2.082642466025e-04 9.215232150554e-01 -4.309558781916e-04 -1.906884416777e+00 -1.712566084069e-04 -7.577726035702e-01 -1.393760275119e-03 -6.167080863358e+00 2.552594073529e-03 1.129466404216e+01 + 1 HQP_YQQ 2.000000000000e-01 3.003289000000e+04 8.000000000000e+03 8.210000000000e-01 0.000000000000e+00 2.880822776869e-02 3.508919338452e+00 -8.379445396709e-03 -1.020638903375e+00 -8.308848565496e-03 -1.012040020158e+00 -1.007667443919e-03 -1.227365948744e-01 -8.276176108275e-05 -1.008060427317e-02 + 2 HQP_YQQ 6.000000000000e-01 3.003289000000e+04 8.000000000000e+03 7.210000000000e-01 0.000000000000e+00 -2.065837286933e-02 -2.865238955524e+00 -1.798747836570e-02 -2.494795889834e+00 -5.635869564862e-03 -7.816740034483e-01 -1.753133177919e-03 -2.431530066462e-01 -1.070081468065e-04 -1.484162923807e-02 + 3 HQP_YQQ 1.000000000000e+00 3.003289000000e+04 8.000000000000e+03 4.990000000000e-01 0.000000000000e+00 -9.477603208718e-03 -1.899319280304e+00 1.411259972037e-02 2.828176296668e+00 -1.278787511604e-02 -2.562700424056e+00 -6.230360112141e-05 -1.248569160750e-02 5.901562153626e-06 1.182677786298e-03 + 4 HQP_YQQ 1.600000000000e+00 3.003289000000e+04 8.000000000000e+03 2.060000000000e-01 0.000000000000e+00 8.295367941452e-04 4.026877641482e-01 4.398008172997e-03 2.134955423785e+00 2.136815949654e-03 1.037289295948e+00 -9.026705106575e-03 -4.381895682804e+00 -3.641501526012e-04 -1.767719187384e-01 + 5 HQP_YQQ 2.400000000000e+00 3.003289000000e+04 8.000000000000e+03 2.260000000000e-02 0.000000000000e+00 2.082642466025e-04 9.215232150554e-01 -4.309558781916e-04 -1.906884416777e+00 -1.712566084069e-04 -7.577726035702e-01 -1.393760275119e-03 -6.167080863358e+00 2.552594073529e-03 1.129466404216e+01 diff --git a/validphys2/src/validphys/cuts/filters.yaml b/validphys2/src/validphys/cuts/filters.yaml index 29dae5db1..eff089ade 100644 --- a/validphys2/src/validphys/cuts/filters.yaml +++ b/validphys2/src/validphys/cuts/filters.yaml @@ -1,3 +1,39 @@ +- dataset: ATLAS_TTBARZ_13TEV_PTZNORM + reason: | + We remove the last bin of the normalised distribution because it is + linearly dependent on the others + rule: "p_T<300.0" + +- dataset: ATLAS_TTBAR_13TEV_HADRONIC_TTMNORM + reason: | + We remove the last bin of the normalised distribution because it is + linearly dependent on the others + rule: "MQQ<1101" + +- dataset: CMS_TTBARZ_13TEV_PTZNORM + reason: | + We remove the last bin of the normalised distribution because it is + linearly dependent on the others + rule: "p_T<250.0" + +- dataset: CMS_TTBAR_13TEV_LJETS_2D_TTM_ABSYTTNORM + reason: | + We remove the last bin of the normalised distribution because it is + linearly dependent on the others + rule: "(yQQ<1.4) or (mu2<820000)" + +- dataset: ATLAS_TTBAR_13TEV_HADRONIC_2D_TTM_ABSYTTNORM + reason: | + We remove the last bin of the normalised distribution because it is + linearly dependent on the others + rule: "(yQQ<1.4) or (mu2<3610000)" + +- dataset: ATLAS_TTBAR_13TEV_TTMNORM + reason: | + We remove the last bin of the normalised distribution because it is + linearly dependent on the others + rule: "MQQ<1600" + - dataset: ATLAS_TTB_DIFF_8TEV_LJ_TPTNORM reason: | We remove the last bin of the normalised distribution because it is @@ -22,6 +58,18 @@ linearly dependent on the others rule: "MQQ<1350" +- dataset: ATLAS_TOPDIFF_DILEPT_8TEV_TTRAPNORM + reason: | + We remove the last bin of the normalised distribution because it is + linearly dependent on the others + rule: "yQQ<2.00" + +- dataset: ATLAS_TOPDIFF_DILEPT_8TEV_TTMNORM + reason: | + We remove the last bin of the normalised distribution because it is + linearly dependent on the others + rule: "MQQ<1000" + - dataset: CMSTOPDIFF8TEVTRAPNORM reason: | We remove the last bin of the normalised distribution because it is @@ -42,18 +90,10 @@ for the NNLO jet project. rule: eta < 0.3 -- dataset: ATLAS1JET11_NEW_SCALE - reason: | - We keep only the first rapidity bin since the chi2 to the whole set of - rapidity bins is too large (known problems with correlation matrix). - This cut will be removed in the new bunch of fits that we are going to do - for the NNLO jet project. - rule: eta < 0.3 - - dataset: CMS_1JET_8TEV reason: | We keep only the bins with pTjet>74 GeV because fixed-order theory does - not provide a good description of the data for smalle values of the jet + not provide a good description of the data for smalle values of the jet transverse momentum. rule: "p_T2 >= 5476" @@ -104,15 +144,15 @@ for which the asymmetry is small is unfeasible. So we can only fit points at NNLO for which the value of the asymmetry is not too small. PTO: NNLO - rule: "central_value >= 0.03" + rule: "fabs(central_value) >= 0.03" -#- dataset: ATLAS_WP_JET_8TEV_PT - #reason: Avoid the region where small-pT resummation effects become important. - #rule: "p_T >= 30" +- dataset: ATLAS_WP_JET_8TEV_PT + reason: Avoid the region where small-pT resummation effects become important. + rule: "p_T >= 30" -#- dataset: ATLAS_WM_JET_8TEV_PT - #reason: Avoid the region where small-pT resummation effects become important. - #rule: "p_T >= 30" +- dataset: ATLAS_WM_JET_8TEV_PT + reason: Avoid the region where small-pT resummation effects become important. + rule: "p_T >= 30" - dataset: ATLASZPT7TEV reason: Avoid the region where resummation effects become important. @@ -159,67 +199,67 @@ max_M: 116.0 rule: M <= max_M -#- dataset: CMSDY2D11 - #reason: | - #Removes data points for which the NNLO K-factors are very large and - #thus the NLO calculation is unreliable. - #PTO: NNLO- - #local_variables: - #M: sqrt(M2) - #max_M: 200.0 - #rule: M <= max_M - -#- dataset: CMSDY2D11 - #reason: Remove data points for which electroweak corrections are large. - #PTO: NNLO- - #local_variables: - #M: sqrt(M2) - #min_M: 30.0 - #max_rapidity: 2.2 - #rule: M >= min_M and etay <= max_rapidity - -#- dataset: CMSDY2D11 - #reason: Remove data points for which electroweak corrections are large. - #PTO: NNLO - #local_variables: - #M: sqrt(M2) - #max_rapidity: 2.2 - #max_M: 200.0 - #rule: M <= max_M and etay <= max_rapidity - -#- dataset: CMSDY2D12 - #reason: | - #Removes data points for which the NNLO K-factors are very large and - #thus the NLO calculation is unreliable. - #PTO: NNLO- - #local_variables: - #M: sqrt(M2) - #max_M: 200.0 - #rule: M <= max_M - -#- dataset: CMSDY2D12 - #reason: Remove data points for which electroweak corrections are large. - #PTO: NNLO- - #local_variables: - #M: sqrt(M2) - #min_M: 30.0 - #max_rapidity: 2.2 - #rule: M >= min_M and etay <= max_rapidity - -#- dataset: CMSDY2D12 - #reason: Remove data points for which electroweak corrections are large. - #PTO: NNLO - #local_variables: - #M: sqrt(M2) - #max_rapidity: 2.2 - #max_M: 200.0 - #rule: M <= max_M and etay <= max_rapidity - -#- dataset: ATLASZHIGHMASS49FB - #reason: Avoid the region where resummation effects become important. - #local_variables: - #max_M: 200.0 - #rule: M_ll <= max_M +- dataset: CMSDY2D11 + reason: | + Removes data points for which the NNLO K-factors are very large and + thus the NLO calculation is unreliable. + PTO: NNLO- + local_variables: + M: sqrt(M2) + max_M: 200.0 + rule: M <= max_M + +- dataset: CMSDY2D11 + reason: Remove data points for which electroweak corrections are large. + PTO: NNLO- + local_variables: + M: sqrt(M2) + min_M: 30.0 + max_rapidity: 2.2 + rule: M >= min_M and etay <= max_rapidity + +- dataset: CMSDY2D11 + reason: Remove data points for which electroweak corrections are large. + PTO: NNLO + local_variables: + M: sqrt(M2) + max_rapidity: 2.2 + max_M: 200.0 + rule: M <= max_M and etay <= max_rapidity + +- dataset: CMSDY2D12 + reason: | + Removes data points for which the NNLO K-factors are very large and + thus the NLO calculation is unreliable. + PTO: NNLO- + local_variables: + M: sqrt(M2) + max_M: 200.0 + rule: M <= max_M + +- dataset: CMSDY2D12 + reason: Remove data points for which electroweak corrections are large. + PTO: NNLO- + local_variables: + M: sqrt(M2) + min_M: 30.0 + max_rapidity: 2.2 + rule: M >= min_M and etay <= max_rapidity + +- dataset: CMSDY2D12 + reason: Remove data points for which electroweak corrections are large. + PTO: NNLO + local_variables: + M: sqrt(M2) + max_rapidity: 2.2 + max_M: 200.0 + rule: M <= max_M and etay <= max_rapidity + +- dataset: ATLASZHIGHMASS49FB + reason: Avoid the region where resummation effects become important. + local_variables: + max_M: 200.0 + rule: M_ll <= max_M # - dataset: LHCBLOWMASS37PB # rule: "pT <= maxCMSDY2Dminv" @@ -258,57 +298,57 @@ maxY: 0.663 rule: "tau <= maxTau and fabs(y/ymax) <= maxY" -#- dataset: DYE605_dw - #reason: | - #Remove data points for which the fixed-order perturbative expansion is not - #reliable since resummation effects are large. A justification of these cuts - #can be found in arXiv:1507.01006. - #process_type: DYP - #local_variables: - #tau: M2 / sqrts**2 - #ymax: -0.5 * log(tau) - #maxTau: 0.080 - #maxY: 0.663 - #rule: "tau <= maxTau and fabs(y/ymax) <= maxY" - -#- dataset: DYE605_sh - #reason: | - #Remove data points for which the fixed-order perturbative expansion is not - #reliable since resummation effects are large. A justification of these cuts - #can be found in arXiv:1507.01006. - #process_type: DYP - #local_variables: - #tau: M2 / sqrts**2 - #ymax: -0.5 * log(tau) - #maxTau: 0.080 - #maxY: 0.663 - #rule: "tau <= maxTau and fabs(y/ymax) <= maxY" - -#- dataset: DYE605_dw_ite - #reason: | - #Remove data points for which the fixed-order perturbative expansion is not - #reliable since resummation effects are large. A justification of these cuts - #can be found in arXiv:1507.01006. - #process_type: DYP - #local_variables: - #tau: M2 / sqrts**2 - #ymax: -0.5 * log(tau) - #maxTau: 0.080 - #maxY: 0.663 - #rule: "tau <= maxTau and fabs(y/ymax) <= maxY" - -#- dataset: DYE605_sh_ite - #reason: | - #Remove data points for which the fixed-order perturbative expansion is not - #reliable since resummation effects are large. A justification of these cuts - #can be found in arXiv:1507.01006. - #process_type: DYP - #local_variables: - #tau: M2 / sqrts**2 - #ymax: -0.5 * log(tau) - #maxTau: 0.080 - #maxY: 0.663 - #rule: "tau <= maxTau and fabs(y/ymax) <= maxY" +- dataset: DYE605_dw + reason: | + Remove data points for which the fixed-order perturbative expansion is not + reliable since resummation effects are large. A justification of these cuts + can be found in arXiv:1507.01006. + process_type: DYP + local_variables: + tau: M2 / sqrts**2 + ymax: -0.5 * log(tau) + maxTau: 0.080 + maxY: 0.663 + rule: "tau <= maxTau and fabs(y/ymax) <= maxY" + +- dataset: DYE605_sh + reason: | + Remove data points for which the fixed-order perturbative expansion is not + reliable since resummation effects are large. A justification of these cuts + can be found in arXiv:1507.01006. + process_type: DYP + local_variables: + tau: M2 / sqrts**2 + ymax: -0.5 * log(tau) + maxTau: 0.080 + maxY: 0.663 + rule: "tau <= maxTau and fabs(y/ymax) <= maxY" + +- dataset: DYE605_dw_ite + reason: | + Remove data points for which the fixed-order perturbative expansion is not + reliable since resummation effects are large. A justification of these cuts + can be found in arXiv:1507.01006. + process_type: DYP + local_variables: + tau: M2 / sqrts**2 + ymax: -0.5 * log(tau) + maxTau: 0.080 + maxY: 0.663 + rule: "tau <= maxTau and fabs(y/ymax) <= maxY" + +- dataset: DYE605_sh_ite + reason: | + Remove data points for which the fixed-order perturbative expansion is not + reliable since resummation effects are large. A justification of these cuts + can be found in arXiv:1507.01006. + process_type: DYP + local_variables: + tau: M2 / sqrts**2 + ymax: -0.5 * log(tau) + maxTau: 0.080 + maxY: 0.663 + rule: "tau <= maxTau and fabs(y/ymax) <= maxY" - process_type: DIS_ALL reason: Generalised cut for all DIS processes @@ -350,26 +390,3 @@ FNS: FONLL-C IC: True rule: "Q2 > 8" - -# Below are cuts that are specific to the PDF4EFT fits - -- dataset: CMSDY2D11 - reason: | - Remove points at large values of the rapidity. The theoretical description - of these points is poor, even at NNLO QCD + NLO EW. Removing these points - results in a significant improvement in this dataset's chi2. Note that this - cut is part of the standard NNPDF cuts for this dataset. - rule: etay <= 2.2 - -- dataset: CMSDY2D11 - reason: | - Specific to PDF4EFT fits. Cut points that go beyond LO kinematic limit in - rapidity for highest invariant mass bin. - rule: etay < 1.5 if M2 == 7.225e+05 else True - -- dataset: ATLASDY2D8TEV - reason: | - Specific to PDF4EFT fits. Cut points that go beyond LO kinematic limit in - rapidity for highest invariant mass bin. - rule: etay < 1.68 if M2 == 1.0e+06 else True -