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000277057 0248_ $$aoai:cds.cern.ch:277057$$pcerncds:CERN$$pcerncds:CERN:FULLTEXT$$pcerncds:FULLTEXT
000277057 0247_ $$2DOI$$a10.1016/0370-2693(95)00431-J
000277057 035__ $$9SLAC$$a3096718
000277057 035__ $$9SPIRES$$a3096718
000277057 035__ $$9arXiv$$aoai:arXiv.org:hep-ph/9502309
000277057 035__ $$9Inspire$$a392838
000277057 037__ $$9arXiv$$ahep-ph/9502309$$chep-ph
000277057 037__ $$aFTUAM-94-30
000277057 037__ $$aFTUCM-94-20
000277057 037__ $$aCMS-TN-94-276
000277057 041__ $$aeng
000277057 088__ $$aCMS-TN-94-276
000277057 088__ $$aFTUAM-94-20
000277057 088__ $$aFTUAM-94-30
000277057 100__ $$aDobado, A.$$uMadrid U.
000277057 245__ $$aLearning about the strongly interacting symmetry breaking sector at LHC
000277057 246__ $$aLARGE HADRON COLLIDER
000277057 260__ $$c1995
000277057 269__ $$aGeneva$$bCERN$$c15 Feb 1995
000277057 300__ $$a13 p
000277057 340__ $$apaper
000277057 500__ $$9arXiv$$a18 pages, Latex, 4 figures available on request
000277057 520__ $$aIn the present work we study the predictions for WZ and ZZ production at LHC with the Electroweak Chiral Lagrangian (EChL) approach. Our analysis will be focused on the less favored case from the experimental point of view, in which the predictions for the gauge bosons scattering amplitudes are considered in the low energy range where, by construction of the low energy approach, they reveal no resonant behavior. The study includes the complete set of amplitudes for all the polarization states of the initial and/or final gauge bosons and makes no use of the Equivalence Theorem. We express the results in terms of the range of values of the chiral parameters that will be accessible at LHC.
000277057 520__ $$aIn the present work we study the predictions for $WZ$ and $ZZ$ production at LHC with the Electroweak Chiral Lagrangian (EChL) approach. Our analysis will be focused on the less favored case from the experimental point of view, in which the predictions for the gauge bosons scattering amplitudes are considered in the low energy range where, by construction of the low energy approach, they reveal no resonant behavior. The study includes the complete set of amplitudes for all the polarization states of the initial and/or final gauge bosons and makes no use of the Equivalence Theorem. We express the results in terms of the range of values of the chiral parameters that will be accessible at LHC.
000277057 520__ $$aIn the present work we study the predictions for $WZ$ and $ZZ$ production at LHC with the Electroweak Chiral Lagrangian (EChL) approach. Our analysis will be focused on the less favored case from the experimental point of view, in which the predictions for the gauge bosons scattering amplitudes are considered in the low energy range where, by construction of the low energy approach, they reveal no resonant behavior. The study includes the complete set of amplitudes for all the polarization states of the initial and/or final gauge bosons and makes no use of the Equivalence Theorem. We express the results in terms of the range of values of the chiral parameters that will be accessible at LHC.
000277057 520__ $$9Elsevier$$aIn the present work we study the predictions for WZ and ZZ production at the LHC with the Electroweak Chiral Lagrangian (EChL) approach. Our analysis will be focused on the less favored case from the experimental point of view, in which the predictions for the gauge bosons scattering amplitudes are considered in the low energy range where, by construction of the low energy approach, they reveal no resonant behavior. The study includes the complete set of amplitudes for all the polarization states of the initial and/or final gauge bosons and makes no use of the Equivalence Theorem. We express the results in terms of the range of values of the chiral parameters that will be accessible at the LHC.
000277057 542__ $$fCopyright @ unknown. Published by Elsevier B.V.
000277057 595__ $$aLANL EDS
000277057 65017 $$2SzGeCERN$$aParticle Physics - Phenomenology
000277057 693__ $$aCERN LHC$$eCMS
000277057 690C_ $$aARTICLE
000277057 690C_ $$aCERN
000277057 695__ $$9LANL EDS$$ahep-ph
000277057 700__ $$aHerrero, M.J.$$uMadrid, Autonoma U.
000277057 700__ $$aPelaez, J.R.$$uMadrid U.
000277057 700__ $$aRuiz Morales, E.$$uMadrid, Autonoma U.
000277057 700__ $$aUrdiales, M.T.$$uMadrid, Autonoma U.
000277057 710__ $$5CERN?
000277057 720__ $$aDobado, A
000277057 720__ $$aHerrero, M J
000277057 720__ $$aPelaez, J R
000277057 720__ $$aRuiz, E
000277057 720__ $$aUrdiales, M T
000277057 773__ $$c400-410$$oPhys.Lett.B352:400-410,1995$$pPhys. Lett. B$$v352$$y1995
000277057 852__ $$cCERN Central Library$$hhep-ph/9502309
000277057 859__ [email protected]
000277057 8564_ $$uhttp://preprints.cern.ch/cgi-bin/setlink?base=preprint&categ=hep-ph&id=9502309$$yAccess to fulltext document
000277057 8564_ $$823534$$s169355$$uhttps://cds.cern.ch/record/277057/files/9502309.fig1.pdf$$yAccess to fulltext document
000277057 8564_ $$823532$$s54819$$uhttps://cds.cern.ch/record/277057/files/9502309.fig2.pdf$$yAccess to fulltext document
000277057 8564_ $$823533$$s206838$$uhttps://cds.cern.ch/record/277057/files/9502309.pdf$$yAccess to fulltext document
000277057 8564_ $$82434417$$s144105$$uhttps://cds.cern.ch/record/277057/files/arXiv:hep-ph_9502309.pdf
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