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Measurements are made in four fiducial phase space regions, targeting different aspects of the \n \n $$ \\textrm{t}\\overline{\\textrm{t}}\\textrm{b}\\overline{\\textrm{b}} $$<\/jats:tex-math>\n \n t<\/mml:mi>\n \n t<\/mml:mi>\n \u00af<\/mml:mo>\n <\/mml:mover>\n b<\/mml:mi>\n \n b<\/mml:mi>\n \u00af<\/mml:mo>\n <\/mml:mover>\n <\/mml:math>\n <\/jats:alternatives>\n <\/jats:inline-formula> process. Distributions are unfolded to the particle level through maximum likelihood fits, and compared with predictions from several event generators. The inclusive cross section measurements of this process in the fiducial phase space regions are the most precise to date. In most cases, the measured inclusive cross sections exceed the predictions with the chosen generator settings. The only exception is when using a particular choice of dynamic renormalization scale, \n \n $$ {\\mu}_{\\textrm{R}}=\\frac{1}{2}{\\prod}_{i=\\textrm{t},\\overline{\\textrm{t}},\\textrm{b},\\overline{\\textrm{b}}}{m}_{\\textrm{T},i}^{1\/4} $$<\/jats:tex-math>\n \n \n \u03bc<\/mml:mi>\n R<\/mml:mi>\n <\/mml:msub>\n =<\/mml:mo>\n \n 1<\/mml:mn>\n 2<\/mml:mn>\n <\/mml:mfrac>\n \n \u220f<\/mml:mo>\n \n i<\/mml:mi>\n =<\/mml:mo>\n t<\/mml:mi>\n ,<\/mml:mo>\n \n t<\/mml:mi>\n \u00af<\/mml:mo>\n <\/mml:mover>\n ,<\/mml:mo>\n b<\/mml:mi>\n ,<\/mml:mo>\n \n b<\/mml:mi>\n \u00af<\/mml:mo>\n <\/mml:mover>\n <\/mml:mrow>\n <\/mml:msub>\n \n m<\/mml:mi>\n \n T<\/mml:mi>\n ,<\/mml:mo>\n i<\/mml:mi>\n <\/mml:mrow>\n \n 1<\/mml:mn>\n \/<\/mml:mo>\n 4<\/mml:mn>\n <\/mml:mrow>\n <\/mml:msubsup>\n <\/mml:math>\n <\/jats:alternatives>\n <\/jats:inline-formula>, where \n \n $$ {m}_{\\textrm{T},i}^2={m}_i^2+{p}_{\\textrm{T},i}^2 $$<\/jats:tex-math>\n \n \n m<\/mml:mi>\n \n T<\/mml:mi>\n ,<\/mml:mo>\n i<\/mml:mi>\n <\/mml:mrow>\n 2<\/mml:mn>\n <\/mml:msubsup>\n =<\/mml:mo>\n \n m<\/mml:mi>\n i<\/mml:mi>\n 2<\/mml:mn>\n <\/mml:msubsup>\n +<\/mml:mo>\n \n p<\/mml:mi>\n \n T<\/mml:mi>\n ,<\/mml:mo>\n i<\/mml:mi>\n <\/mml:mrow>\n 2<\/mml:mn>\n <\/mml:msubsup>\n <\/mml:math>\n <\/jats:alternatives>\n <\/jats:inline-formula> are the transverse masses of top and bottom quarks. 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