Measurement of the $WZ$ and $ZZ$ production cross sections using eptonic final states in $8.6\ \text{fb}^{ -1}$ of $p\bar p$ collisions

dc.contributor.authorAbazov, V.M.
dc.contributor.authorAbbott, B.
dc.contributor.authorAcharya, B.S.
dc.contributor.authorAdams, M.
dc.contributor.authorAdams, T.
dc.contributor.authorAlexeev, G.D.
dc.contributor.authorAlkhazov, G.
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dc.contributor.authorAtramentov, O.
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dc.contributor.authorWang, M.H.L.S.
dc.contributor.authorWarchol, J.
dc.contributor.authorWatts, G.
dc.contributor.authorWayne, M.
dc.contributor.authorWeber, M.
dc.contributor.authorWeichert, J.
dc.contributor.authorWelty-Rieger, L.
dc.contributor.authorWhite, A.
dc.contributor.authorWicke, D.
dc.contributor.authorWilliams, M.R.J.
dc.contributor.authorWilson, G.W.
dc.contributor.authorWobisch, M.
dc.contributor.authorWood, D.R.
dc.contributor.authorWyatt, T.R.
dc.contributor.authorXie, Y.
dc.contributor.authorYamada, R.
dc.contributor.authorYang, W.-C.
dc.contributor.authorYasuda, T.
dc.contributor.authorYatsunenko, Y.A.
dc.contributor.authorYe, W.
dc.contributor.authorYe, Z.
dc.contributor.authorYin, H.
dc.contributor.authorYip, K.
dc.contributor.authorYoun, S.W.
dc.contributor.authorZhao, T.
dc.contributor.authorZhou, B.
dc.contributor.authorZhu, J.
dc.contributor.authorZielinski, M.
dc.contributor.authorZieminska, D.
dc.contributor.authorZivkovic, L.
dc.date.accessioned2014-08-07T17:00:59Z
dc.date.available2014-08-07T17:00:59Z
dc.date.issued2012
dc.description.abstractWe study the processes $p\bar p \rightarrow WZ \rightarrow ℓ^{±}\nu ℓ^{+}l^{-}$ and $p\bar p \rightarrow ZZ \rightarrow ℓ^{+}ℓ^{−}\nu\bar\nu$, where $ℓ=e$ or $\mu$. Using $8.6 \text{ fb}^{−1}$ of integrated luminosity collected by the D0 experiment at the Fermilab Tevatron collider, we measure the $WZ$ production cross section to be $4.50^{+0.63}_{−0.66}  \text{pb}$ which is consistent with, but slightly larger than, the prediction of the standard model. The $ZZ$ cross section is measured to be $1.64±0.46  \text{pb}$, in agreement with a prediction of the standard model. Combination with an earlier analysis of the $ZZ→ℓ^{+}ℓ^{−}ℓ^{+}ℓ^{−}$ channel yields a $ZZ$ cross section of $1.44^{+0.35}_{−0.34}  \text{pb}$.
dc.identifier.citationAbazov, V. M., Abbott, B., Acharya, B. S., Adams, M., Adams, T., Alexeev, G. D., . . . Zivkovic, L. (2012). Measurement of the $WZ$ and $ZZ$ production cross sections using eptonic final states in $8.6\ \text{fb}^{ -1}$ of $p\bar p$ collisions. Physical Review D - Particles, Fields, Gravitation and Cosmology, 85(11), 112005. http://dx.doi.org/10.1103/PhysRevD.85.112005
dc.identifier.urihttps://hdl.handle.net/2022/18565
dc.language.isoen_US
dc.publisherAmerican Physical Society
dc.relation.isversionofhttps://doi.org/10.1103/PhysRevD.85.112005
dc.rights© 2012 American Physical Society.
dc.titleMeasurement of the $WZ$ and $ZZ$ production cross sections using eptonic final states in $8.6\ \text{fb}^{ -1}$ of $p\bar p$ collisions
dc.typeArticle

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