{"associated_files":[{"alt_location":"/opt/hepdata/var/data/5c/167852/1771605887/submission.tar/datacard_shapelimit13TeV_combined_theory10_scales_pdfs_run2.root","description":"ROOT file","id":4174043,"type":"ROOT"},{"alt_location":"/opt/hepdata/var/data/5c/167852/1771605887/submission.tar/datacard_shapelimit13TeV_combined_theory10_scales_pdfs_run2.png","description":"Image file","id":4174044,"preview_location":"/record/resource/4174045?view=true","type":"png"}],"description":"Normalized CHI = exp(|Y1-Y2|) distributions (1/SIG)*D(SIG)/DCHI in M(JJ) &gt; 7.0 TeV with |Y1+Y2|/2&lt; 1.1 for 138 fb$^{-1}$ of integrated luminosity at $\\sqrt{s} = 13$ TeV. The data distributions corrected for detector effects are compared to NNLO predictions with central scale choices $\\mu_{F}$ = $\\mu_{R}$ = $m_{jj}$ and $\\mu_{F}$ = $\\mu_{R}$ = $&lt;p_{T}&gt;$. Prediction with the alternative CT14 PDF set, and a comparison with the NLO prediction used in the previous publication are also given. Theoretical uncertainties with the central scale $\\mu_{F}$ = $\\mu_{R}$ = $m_{jj}$ and using NNPDF3.1 are provided. We also provide prediction without EW corrections applied.","doi":"10.17182/hepdata.167852.v1/t18","headers":[{"colspan":1,"name":"CHI = exp(|Y1-Y2|)"},{"colspan":1,"name":"Measured"},{"colspan":1,"name":"QCD NNLO + EW NLO ($\\mu=m_{jj}$)"},{"colspan":1,"name":"QCD NNLO + EW NLO ($\\mu=<p_{T}>$)"},{"colspan":1,"name":"QCD NLO + EW NLO ($\\mu=<p_{T}>$)"},{"colspan":1,"name":"QCD NNLO ($\\mu=m_{jj}$)"}],"keywords":{"cmenergies":["13000"],"observables":["DSIG/DCHI"],"reactions":["P P --> JET JET X"]},"location":"Data from Figure 5 lower right","name":"Fig. 5: Particle level CHI distribution (M(JJ) > 7.0 TeV)","qualifier_order":["LUMINOSITY"],"qualifiers":{"LUMINOSITY":[{"colspan":1,"group":0,"type":"LUMINOSITY","value":"138.0 fb$^{-1}$"}]},"related_tables":[],"related_to_this":[],"resources":[{"description":"ROOT file","type":"ROOT","url":"https://www.hepdata.net/record/resource/4174043?landing_page=true"},{"description":"Image file","type":"png","url":"https://www.hepdata.net/record/resource/4174044?landing_page=true"},{"description":"Thumbnail image file","type":"png","url":"https://www.hepdata.net/record/resource/4174045?landing_page=true"}],"review":{"messages":false,"review_flag":"passed"},"size":1994,"size_check":true,"table_license":{"description":"CC0 enables reusers to distribute, remix, adapt, and build upon the material in any medium or format, with no conditions.","name":"CC0","url":"https://creativecommons.org/publicdomain/zero/1.0/"},"values":[{"x":[{"high":"3","low":"1"}],"y":[{"errors":[{"label":"sys","symerror":"0.01275"},{"label":"total","symerror":"0.04935"}],"group":0,"value":"0.16567"},{"errors":[{"asymerror":{"minus":"-0.00428","plus":"0.00302"},"label":"theory"}],"group":1,"value":"0.07482"},{"errors":[{"hide":true,"symerror":0}],"group":2,"value":"0.08145"},{"errors":[{"hide":true,"symerror":0}],"group":3,"value":"0.07587"},{"errors":[{"hide":true,"symerror":0}],"group":4,"value":"0.06723"}]},{"x":[{"high":"6","low":"3"}],"y":[{"errors":[{"label":"sys","symerror":"0.00406"},{"label":"total","symerror":"0.03024"}],"group":0,"value":"0.07871"},{"errors":[{"asymerror":{"minus":"-0.00085","plus":"0.00075"},"label":"theory"}],"group":1,"value":"0.06372"},{"errors":[{"hide":true,"symerror":0}],"group":2,"value":"0.0671"},{"errors":[{"hide":true,"symerror":0}],"group":3,"value":"0.06476"},{"errors":[{"hide":true,"symerror":0}],"group":4,"value":"0.063286"}]},{"x":[{"high":"9","low":"6"}],"y":[{"errors":[{"label":"sys","symerror":"0.0"},{"label":"total","symerror":"0.02116"}],"group":0,"value":"0.02303"},{"errors":[{"asymerror":{"minus":"-0.0002","plus":"0.00052"},"label":"theory"}],"group":1,"value":"0.06506"},{"errors":[{"hide":true,"symerror":0}],"group":2,"value":"0.06551"},{"errors":[{"hide":true,"symerror":0}],"group":3,"value":"0.06483"},{"errors":[{"hide":true,"symerror":0}],"group":4,"value":"0.066406"}]},{"x":[{"high":"12","low":"9"}],"y":[{"errors":[{"label":"sys","symerror":"0.00152"},{"label":"total","symerror":"0.0308"}],"group":0,"value":"0.06797"},{"errors":[{"asymerror":{"minus":"-0.00116","plus":"0.00145"},"label":"theory"}],"group":1,"value":"0.06635"},{"errors":[{"hide":true,"symerror":0}],"group":2,"value":"0.06426"},{"errors":[{"hide":true,"symerror":0}],"group":3,"value":"0.06547"},{"errors":[{"hide":true,"symerror":0}],"group":4,"value":"0.068094"}]},{"x":[{"high":"16","low":"12"}],"y":[{"errors":[{"label":"sys","symerror":"0.00484"},{"label":"total","symerror":"0.02426"}],"group":0,"value":"0.03988"},{"errors":[{"asymerror":{"minus":"-0.00123","plus":"0.00148"},"label":"theory"}],"group":1,"value":"0.06623"},{"errors":[{"hide":true,"symerror":0}],"group":2,"value":"0.06162"},{"errors":[{"hide":true,"symerror":0}],"group":3,"value":"0.06576"},{"errors":[{"hide":true,"symerror":0}],"group":4,"value":"0.068045"}]}],"x_count":1}

