002882334 001__ 2882334
002882334 005__ 20241219161726.0
002882334 0248_ $$aoai:cds.cern.ch:2882334$$pcerncds:FULLTEXT$$pcerncds:CERN:FULLTEXT$$pcerncds:CERN
002882334 0247_ $$2DOI$$9arXiv$$a10.1140/epjc/s10052-024-13480-4$$qpublication
002882334 037__ $$9arXiv$$aarXiv:2310.19638$$chep-ph
002882334 037__ $$9arXiv:reportnumber$$aDESY-23-160
002882334 035__ $$9arXiv$$aoai:arXiv.org:2310.19638
002882334 035__ $$9Inspire$$aoai:inspirehep.net:2715747$$d2024-12-13T04:07:20Z$$h2024-12-14T03:00:24Z$$mmarcxml$$ttrue$$uhttps://inspirehep.net/api/oai2d
002882334 035__ $$9Inspire$$a2715747
002882334 041__ $$aeng
002882334 100__ $$aAbdolmaleki, Hamed$$jORCID:[email protected]$$tGRID:grid.418744.a$$tGRID:grid.459711.f$$uIPM, Tehran$$uLorestan U.$$vSchool of Physics, Institute for Research in Fundamental Sciences (IPM), Tehran, Iran$$vDepartment of Physics, Faculty of Science, Malayer University, Malayer, Iran
002882334 245__ $$9Springer$$aExploring SMEFT couplings using the forward–backward asymmetry in neutral current Drell–Yan production at the LHC
002882334 269__ $$c2023-10-30
002882334 260__ $$c2024-12-09
002882334 300__ $$a22 p
002882334 520__ $$9Springer$$aNeutral current Drell–Yan (DY) lepton-pair production is considered to study Z-boson quark couplings. Using the open-source fit platform xFitter, we investigate the impact of high-statistics measurements of the neutral current DY (NCDY) forward–backward asymmetry $A_{\textrm{FB}}$ near the weak boson mass scale in the present and forthcoming stages of the Large Hadron Collider (LHC). Besides recovering earlier results on the $A_{\textrm{FB}}$ sensitivity to parton distribution functions, we analyze the precision determination of Z-boson couplings to left-handed and right-handed u-quarks and d-quarks, and explore Beyond-Standard-Model contributions using the Standard Model Effective Field Theory (SMEFT) framework. We perform a sensitivity study and comment on the role of the $A_{\textrm{FB}}$ asymmetry for the electroweak SMEFT fit and precision Z-boson physics at the LHC and high-luminosity HL-LHC.
002882334 520__ $$9arXiv$$aNeutral current Drell-Yan (DY) lepton-pair production is considered in the framework of the Standard Model Effective Field Theory (SMEFT). Using the open-source fit platform xFitter, we investigate the impact of high-statistics measurements of the neutral current DY (NCDY) forward-backward asymmetry $A_{\rm{FB}}$ near the weak boson mass scale in the present and forthcoming stages of the Large Hadron Collider (LHC). Besides recovering earlier results on the $A_{\rm{FB}}$ sensitivity to parton distribution functions, we analyze the precision determination of $Z$-boson couplings to left-handed and right-handed $u$-quarks and $d$-quarks, and explore Beyond-Standard-Model contributions using the SMEFT framework. We perform a sensitivity study and comment on the role of the $A_{\rm{FB}}$ asymmetry for the electroweak SMEFT fit and precision $Z$-boson physics at the LHC and high-luminosity HL-LHC.
002882334 540__ $$3preprint$$aarXiv nonexclusive-distrib 1.0$$uhttp://arxiv.org/licenses/nonexclusive-distrib/1.0/
002882334 540__ $$3publication$$aCC-BY-4.0$$bSpringer$$fSCOAP3$$uhttp://creativecommons.org/licenses/by/4.0/
002882334 542__ $$3publication$$dThe Author(s)$$g2024
002882334 595_D $$aR$$d2023-11-09$$sabs
002882334 595_D $$aR$$d2023-11-12$$sprinted
002882334 65017 $$2arXiv$$ahep-ph
002882334 65017 $$2SzGeCERN$$aParticle Physics - Phenomenology
002882334 693__ $$aCERN LHC
002882334 690C_ $$aCERN
002882334 690C_ $$aARTICLE
002882334 700__ $$aAmoroso, [email protected]$$tGRID:grid.7683.a$$uDESY$$vDeutsches Elektronen-Synchrotron DESY, Hamburg, Germany
002882334 700__ $$aBritzger, [email protected]$$tGRID:grid.4372.2$$uMunich, Max Planck Inst.$$vMax Planck Institute, Munich, Germany
002882334 700__ $$aDattola, [email protected]$$tGRID:grid.7683.a$$uDESY$$vDeutsches Elektronen-Synchrotron DESY, Hamburg, Germany
002882334 700__ $$aFiaschi, Juri$$jORCID:[email protected]$$tGRID:grid.7563.7$$uINFN, Milan Bicocca$$uMilan Bicocca U.$$vUniversità degli Studi di Milano-Bicocca and INFN, Milan, Italy
002882334 700__ $$aGiuli, Francesco$$jORCID:[email protected]$$tGRID:grid.9132.9$$uCERN$$vCERN, Geneva, Switzerland
002882334 700__ $$aGlazov, [email protected]$$tGRID:grid.7683.a$$uDESY$$vDeutsches Elektronen-Synchrotron DESY, Hamburg, Germany
002882334 700__ $$aHautmann, [email protected]$$tGRID:grid.9132.9$$tGRID:grid.5284.b$$tGRID:grid.4991.5$$uCERN$$uAntwerp U.$$uOxford U.$$vUniversity of Oxford, Oxford, UK$$vUniversity of Antwerp, Antwerpen, Belgium$$vCERN, Geneva, Switzerland
002882334 700__ $$aLuszczak, [email protected]$$tGRID:grid.22555.35$$uCracow Tech. U.$$vCracow University of Technology, Cracow, Poland
002882334 700__ $$aTaheri Monfared, Sara$$jORCID:[email protected]$$tGRID:grid.7683.a$$uDESY$$vDeutsches Elektronen-Synchrotron DESY, Hamburg, Germany
002882334 700__ $$aOlness, [email protected]$$tGRID:grid.263864.d$$uSouthern Methodist U.$$vSMU Physics, Dallas, USA
002882334 700__ $$aVazzoler, [email protected]$$tGRID:grid.7683.a$$uDESY$$vDeutsches Elektronen-Synchrotron DESY, Hamburg, Germany
002882334 700__ $$aZenaiev, Oleksandr$$jORCID:[email protected]$$tGRID:grid.9026.d$$uHamburg U.$$vHamburg University, Hamburg, Germany
002882334 700__ $$aAnataichuk, [email protected]$$tGRID:grid.34555.32$$tGRID:grid.18999.30$$uKharkov Natl. U.$$uTaras Shevchenko U.$$vV. N. Karazin Kharkiv National University, Kharkiv, Ukraine$$vTaras Shevchenko National University of Kyiv, Kyiv, Ukraine
002882334 700__ $$aMoch, [email protected]$$tGRID:grid.9026.d$$uHamburg U.$$vHamburg University, Hamburg, Germany
002882334 773__ $$c1277$$n12$$pEur. Phys. J. C$$v84$$y2024
002882334 8564_ $$82496457$$s101898$$uhttps://cds.cern.ch/record/2882334/files/AFB_RL_Minv.png$$y00001 The partial derivatives of the predicted \afb with respect to $\delta g_R^{Zu}$ (upper left), $\delta g_L^{Zu}$ (upper right), $\delta g_R^{Zd}$ (lower left) and $\delta g_L^{Zd}$ (lower right) couplings as a function of the invariant mass of the dilepton system in different rapidity intervals at LO.
002882334 8564_ $$82496458$$s6935$$uhttps://cds.cern.ch/record/2882334/files/4V_Minv.png$$y00005 The average error in the fitted couplings as a function of the invariant mass (left) and rapidity (right) bin widths.
002882334 8564_ $$82496459$$s30635$$uhttps://cds.cern.ch/record/2882334/files/ell_pdf_unc.png$$y00013 Allowed regions for all pairs of corrections to the $Z$ couplings to $u$- and $d$-type quarks obtained using the ABMP16 and HERAPDF2.0 PDF sets with and without PDF uncertainties.
002882334 8564_ $$82496460$$s32928$$uhttps://cds.cern.ch/record/2882334/files/ell_past_av.png$$y00017 Same as in Fig.~\ref{fig:ell_past} for the axial and vector couplings.
002882334 8564_ $$82496461$$s64345$$uhttps://cds.cern.ch/record/2882334/files/AFB_VA_Y.png$$y00004 Same as in Fig.~\ref{fig:afb-deriv-y} for the axial and vector couplings.
002882334 8564_ $$82496462$$s9327$$uhttps://cds.cern.ch/record/2882334/files/4V_Y.png$$y00006 The average error in the fitted couplings as a function of the invariant mass (left) and rapidity (right) bin widths.
002882334 8564_ $$82496463$$s108724$$uhttps://cds.cern.ch/record/2882334/files/AFB_VA_Minv_with_stat.png$$y00009 Same as in Fig.~\ref{fig:afb-deriv-unc-m} for the axial and vector couplings.
002882334 8564_ $$82496464$$s101480$$uhttps://cds.cern.ch/record/2882334/files/AFB_RL_Minv_with_stat.png$$y00007 The partial derivatives of the predicted \afb with respect to $\delta g_R^{Zu}$ (upper left), $\delta g_L^{Zu}$ (upper right), $\delta g_R^{Zd}$ (lower left) and $\delta g_L^{Zd}$ (lower right) couplings weighted by the inverse of the statistical uncertainty as a function of the invariant mass of the dilepton system in different rapidity intervals at LO.
002882334 8564_ $$82496465$$s64705$$uhttps://cds.cern.ch/record/2882334/files/AFB_RL_Y_with_stat.png$$y00008 The partial derivatives of the predicted \afb with respect to $\delta g_R^{Zu}$ (upper left), $\delta g_L^{Zu}$ (upper right), $\delta g_R^{Zd}$ (lower left) and $\delta g_L^{Zd}$ (lower right) couplings weighted by the inverse of the statistical uncertainty as a function of the rapidity of the dilepton system in different invariant mass intervals at LO.
002882334 8564_ $$82496466$$s68060$$uhttps://cds.cern.ch/record/2882334/files/AFB_VA_Y_with_stat.png$$y00010 Same as in Fig.~\ref{fig:afb-deriv-unc-y} for the axial and vector couplings.
002882334 8564_ $$82496467$$s6345$$uhttps://cds.cern.ch/record/2882334/files/aver.png$$y00020 The average size of the uncertainties on the fitted corrections to the $Z$ couplings to $u$- and $d$-type quarks for different future experiments using the linear (left) or logarithmic (right) scale.
002882334 8564_ $$82496468$$s1103136$$uhttps://cds.cern.ch/record/2882334/files/2310.19638.pdf$$yFulltext
002882334 8564_ $$82496469$$s6030$$uhttps://cds.cern.ch/record/2882334/files/aver_pdf.png$$y00015 The average size of the uncertainties on the fitted corrections to the $Z$ couplings to $u$- and $d$-type quarks obtained using different PDF sets.
002882334 8564_ $$82496470$$s52169$$uhttps://cds.cern.ch/record/2882334/files/AFB.png$$y00000 The predicted \afb as a function of the invariant mass of the dilepton system in different rapidity intervals (left) and rapidity of the dilepton system in different invariant mass intervals (right) at LO in the SM.
002882334 8564_ $$82496471$$s6139$$uhttps://cds.cern.ch/record/2882334/files/aver_log.png$$y00021 The average size of the uncertainties on the fitted corrections to the $Z$ couplings to $u$- and $d$-type quarks for different future experiments using the linear (left) or logarithmic (right) scale.
002882334 8564_ $$82496472$$s45765$$uhttps://cds.cern.ch/record/2882334/files/ell_pdf_av.png$$y00012 Same as in Fig.~\ref{fig:ell_pdf} for the axial and vector couplings.
002882334 8564_ $$82496473$$s32481$$uhttps://cds.cern.ch/record/2882334/files/ell_pdf_unc_av.png$$y00014 Same as in Fig.~\ref{fig:ell_pdf_unc} for the axial and vector couplings.
002882334 8564_ $$82496474$$s29127$$uhttps://cds.cern.ch/record/2882334/files/ell_future_av.png$$y00019 Same as in Fig.~\ref{fig:ell_future} for the axial and vector couplings.
002882334 8564_ $$82496475$$s23974$$uhttps://cds.cern.ch/record/2882334/files/ell_past.png$$y00016 Allowed regions for all pairs of corrections to the $Z$ couplings to $u$- and $d$-type quarks obtained using HL-LHC pseudodata as well as different existing data sets.
002882334 8564_ $$82496476$$s33027$$uhttps://cds.cern.ch/record/2882334/files/ell_pdf.png$$y00011 Allowed regions for all pairs of corrections to the $Z$ couplings to $u$- and $d$-type quarks obtained using different PDF sets.
002882334 8564_ $$82496477$$s24043$$uhttps://cds.cern.ch/record/2882334/files/ell_future.png$$y00018 Allowed regions for all pairs of corrections to the $Z$ couplings to $u$- and $d$-type quarks obtained using HL-LHC pseudodata compared to the ones for different future experiments.
002882334 8564_ $$82496478$$s104307$$uhttps://cds.cern.ch/record/2882334/files/AFB_VA_Minv.png$$y00003 Same as in Fig.~\ref{fig:afb-deriv-m} for the axial and vector couplings.
002882334 8564_ $$82496479$$s71656$$uhttps://cds.cern.ch/record/2882334/files/AFB_RL_Y.png$$y00002 The partial derivatives of the predicted \afb with respect to $\delta g_R^{Zu}$ (upper left), $\delta g_L^{Zu}$ (upper right), $\delta g_R^{Zd}$ (lower left) and $\delta g_L^{Zd}$ (lower right) couplings as a function of the rapidity of the dilepton system in different invariant mass intervals at LO.
002882334 8564_ $$82551979$$s29234$$uhttps://cds.cern.ch/record/2882334/files/ell_pdf_m115.png$$y00023 Allowed regions for all pairs of corrections to the $Z$ couplings to $u$- and $d$-type quarks obtained in the HL-LHC scenario with the ABMP16 PDF set using the $M_{ll}<145$ GeV and $M_{ll}<115$ GeV cuts.
002882334 8564_ $$82551980$$s29563$$uhttps://cds.cern.ch/record/2882334/files/4f.png$$y00022 The linear contributions of four-fermion operators $C_{lq}^{(1)}$ and $C_{eu}$ and the contributions of the vertex corrections to couplings $\delta g_L^{Zu}$, $\delta g_L^{Zd}$, $\delta g_R^{Zu}$ and $\delta g_R^{Zd}$ to \afb as a function of $M_{ll}$. The dotted vertical line shows the value of the cut $M<145$ GeV used in our analysis.
002882334 8564_ $$82700022$$s2208152$$uhttps://cds.cern.ch/record/2882334/files/document.pdf$$yFulltext
002882334 960__ $$a13
002882334 980__ $$aARTICLE