Improved constraints on the mixing and mass of Z′ bosons from resonant diboson searches at the LHC at s=13 TeV and predictions for Run II
暂无分享,去创建一个
[1] V. M. Ghete,et al. Search for massive resonances decaying into WW, WZ, ZZ, qW, and qZ with dijet final states at √s =13 TeV , 2018 .
[2] V. M. Ghete,et al. Combination of searches for heavy resonances decaying to WW, WZ, ZZ, WH, and ZH boson pairs in proton–proton collisions at √s = 8 and 13 TeV , 2017 .
[3] A. Pankov,et al. Probing $Z$-$Z'$ mixing with ATLAS and CMS resonant diboson production data at the LHC at $\sqrt{s}=13$ TeV , 2017, 1707.02717.
[4] Atlas Collaboration. Search for new high-mass phenomena in the dilepton final state using 36 fb$^{-1}$ of proton-proton collision data at $\sqrt{s}$ = 13 TeV with the ATLAS detector , 2017, 1707.02424.
[5] C. Collaboration,et al. Combination of searches for heavy resonances decaying to WW, WZ, ZZ, WH, and ZH boson pairs in proton-proton collisions at sqrt(s) = 8 and 13 TeV , 2017, 1705.09171.
[6] M. P. Casado,et al. Searches for heavy diboson resonances in pp collisions at √s=13 TeV with the ATLAS detector , 2016 .
[7] V. Bednyakov,et al. Effects of Z−Z′ mixing in double W-bosons production at the large hadron collider , 2015 .
[8] D. Rathlev,et al. W+ W- production at hadron colliders in next to next to leading order QCD. , 2014, Physical review letters.
[9] Andrea Benaglia,et al. Search for new resonances decaying via WZ to leptons in proton-proton collisions at √s=8TeV , 2014 .
[10] Peter Skands,et al. An introduction to PYTHIA 8.2 , 2014, Comput. Phys. Commun..
[11] J. T. Childers,et al. Search for WZ resonances in the fully leptonic channel using pp collisions at √s = 8 TeV with the ATLAS detector , 2014 .
[12] A. Pankov,et al. Precise determination of Z-Z' mixing at the CERN LHC , 2014, 1406.6776.
[13] Atlas Collaboration. Search for WZ resonances in the fully leptonic channel using pp collisions at sqrt(s) = 8 TeV with the ATLAS detector , 2014, 1406.4456.
[14] Werner Porod,et al. Implications of gauge kinetic mixing on Z ' and slepton production at the LHC , 2012, 1206.3513.
[15] G. Moortgat-pick,et al. Discriminating Z′ from anomalous trilinear gauge coupling signatures in e+e−→W+W− at ILC with polarized beams , 2012, The European Physical Journal C.
[16] Frank Taylor. Search for new particles decaying to ZZ using final states with leptons and jets with the ATLAS detector in √s = 7 TeV proton–proton collisions , 2012 .
[17] A. Pankov,et al. Constraints on the Z-Z′ mixing angle from data measured for the process e+e− → W+W− at the LEP2 collider , 2012 .
[18] T. Hansl-Kozanecka,et al. Commissioning of the ATLAS Muon Spectrometer with Cosmic Rays , 2010, 1006.4384.
[19] J. Blas,et al. Electroweak limits on general new vector bosons , 2010, 1005.3998.
[20] V. Tiwari,et al. Next-to-leading order QCD corrections to $W^+W^-$ production at the LHC in Randall Sundrum model , 2010, 1003.5445.
[21] P. Langacker,et al. Six-lepton Z' resonance at the Large Hadron Collider. , 2009, Physical Review Letters.
[22] Giovanni Villadoro,et al. Minimal Z' models: present bounds and early LHC reach , 2009, 0909.1320.
[23] A. Alves,et al. Signals for new spin-1 resonances in electroweak gauge boson pair production at the LHC , 2009, 0907.2915.
[24] P. Langacker,et al. Improved constraints on Z′ bosons from electroweak precision data , 2009, 0906.2435.
[25] The Aleph Collaboration,et al. Precision electroweak measurements on the Z resonance , 2005, hep-ex/0509008.
[26] P. Langacker,et al. Z′ discovery limits for supersymmetric E6 models , 2004, hep-ph/0412190.
[27] J. Huston,et al. New generation of parton distributions with uncertainties from global QCD analysis , 2002, hep-ph/0201195.
[28] D. Benchekroun,et al. Search for Z’ → WW at LHC with the ATLAS detector , 2001 .
[29] A. Pankov,et al. Z′ interference effects from TRISTAN to LEP2 , 1996, hep-ph/9612314.
[30] Alan D. Martin,et al. Review of Particle Physics , 2000, Physical Review D.
[31] S. Frixione. A next-to-leading order calculation of the cross section for the production of W+W− pairs in hadronic collisions , 1993 .
[32] A. Pankov,et al. Theoretical speculations on the TRISTAN results at s⩽60GeV , 1989 .
[33] B. Mele,et al. Searching for new heavy vector bosons in $$p\bar p$$ colliders , 1989 .
[34] Dib,et al. Extra neutral gauge bosons in electron-positron collisions at resonance. , 1987, Physical review. D, Particles and fields.
[35] Barger,et al. Heavy-Z-boson decays to two bosons in E6 superstring models. , 1987, Physical review. D, Particles and fields.
[36] B. Holdom. Two U(1)'s and Epsilon Charge Shifts , 1986 .
[37] V. M. Ghete,et al. CMS Collaboration , 2019, Nuclear Physics A.
[38] W. Porod,et al. Phenomenology of a supersymmetric U(1)_{B-L} × U(1)_{R} extension of the standard model with inverse seesaw mechanism , 2014 .
[39] Alam,et al. Search for new phenomena in the final state in pp collisions at with the ATLAS detector , 2013 .
[40] P. Langacker,et al. Constraints on additional Z bosons. , 1992, Physical review. D, Particles and fields.
[41] M. Chanowitz,et al. The TeV physics of strongly interacting W's and Z's , 1985 .