Measurement of the e+e−→ZZ production cross section at centre-of-mass energies of 183 and 189 GeV

Barate, R.; Décamp, D.; Ghez, Philippe; Goy, C.; Jézéquel, S.; Lees, J. P.; Martin, F. F.; Merle, E.; Minard, M.-N.; Pietrzyk, B.; Alemany, R.; Bravo, S.; Casado, M. P.; Chmeissani, M.; Crespo, J.M.; Fernández, E.; Fernández-Bosman, M.; Garrido, Ll.; Graugés, E.; Rozas, A. Juste; Martı́nez, M.; Merino, G.; Miquel, R.; Mir, L. M.; Morawitz, P.; Pacheco, A.; Riu, I.; Ruiz, H.; Colaleo, A.; Creanza, D.; Palma, M. De; Iaselli, G.; Mäggi, G.; Maggi, M.; Nuzzo, S.; Ranieri, A.; Raso, G.; Ruggieri, F.; Selvaggi, G.; Silvestris, L.; Tempesta, P.; Tricomi, A.; Zito, G.; Huang, X. T.; Lin, J.; Ouyang, Q.; Wang, T.; Xie, Y.; Xu, R.; Xue, S.; Zhang, J.; Zhang, L.; Zhao, W.; Abbaneo, D.; Boix, G.; Buchmüller, O.; Cattaneo, M.; Cerutti, F.; Ciulli, V.; Davies, G.; Dissertori, G.; Drevermann, H.; Forty, R.; Frank, M.; Gianotti, F.; Greening, T.C.; Halley, A.W.; Hansen, J. B.; Harvey, J.; Janot, P.; Jost, B.; Lehraus, I.; Leroy, O.; Maley, P.; Mató, P.; Minten, A.; Moutoussi, A.; Ranjard, F.; Rolandi, G.; Schlatter, D.; Schmitt, M.; Schneider, O.; Spagnolo, P.; Tejessy, W.; Teubert, F.; Tournefier, E.; Wright, A.E.; Ajaltouni, Z.; Badaud, F.; Chazelle, G.; Deschamps, O.; Dessagne, S.; Falvard, A.; Ferdi, C.; Guicheney, C.; Henrard, P.; Jousset, J.; Michel, B.; Monteil, S.; Montret, J. C.; Pallin, D.; Perret, P.; Podlyski, F.; Hansen, J. D.; Hansen, J. R.; Hansen, P. H.; Nilsson, B.S.; Rensch, B.; Wäänänen, A.; Daskalakis, G.; Kyriakis, A.; Markou, C.; Simopoulou, E.; Vayaki, A.; Blondel, A.; Brient, J. C.; Machefert, F.; Rougé, A.; Swynghedauw, M.; Tanaka, R.; Valassi, A.; Videau, H.; Focardi, E.; Parrini, G.; Zachariadou, K.; Corden, M.; Georgiopoulos, C.; Antonelli, A.; Bencivenni, G.; Bologna, G.; Bossi, F.; Campana, P.; Capon, G.; Chiarella, V.; Laurelli, P.; Mannocchi, G.; Murtas, F.; Murtas, F.; Passalacqua, L.; Pepe-Altarelli, M.; Chalmers, Matthew; Curtis, L.; Lynch, J.G.; Negus, P.; O’Shea, V.; Raeven, B.; Raine, C.; Smith, D.; Teixeira-Dias, P.; Thompson, A. S.; Ward, J. J.; Cavanaugh, R.; Dhamotharan, S.; Geweniger, C.; Hanke, P.; Hepp, V.; Kluge, E. E.; Putzer, A.; Tittel, K.; Werner, S.; Wunsch, M.; Beuselinck, R.; Binnie, D. M.; Cameron, W.; Dornan, P. J.; Girone, M.; Goodsir, S.; Marinelli, N.; Martin, E. B.; Nash, J.; Nowell, J.; Przysiezniak, H.; Sciabà, A.; Sedgbeer, J. K.; Thomson, E.; Williams, M.; Ghete, V. M.; Girtler, P.; Kneringer, E.; Kühn, D.; Rudolph, G.; Bowdery, C. K.; Buck, P.G.; Ellis, G.; Finch, A. J.; Foster, F.; Hughes, G.; Jones, R. W. L.; Robertson, N. A.; Smižanská, M.; Williams, M.I.; Giehl, I.; Hölldorfer, F.; Jakobs, K.; Kleinknecht, K.; Kröcker, M.; Müller, A.‐S.; Nürnberger, H.-A.; Quast, G.; Renk, B.; Rohne, E.; Sander, H. G.; Schmeling, S.; Wachsmuth, H.; Zeitnitz, C.; Ziegler, T.; Aubert, J.J.; Bonissent, A.; Carr, J.; Coyle, P.; Ealet, A.; Fouchez, D.; Tilquin, A.; Aleppo, M.; Antonelli, M.; Gilardoni, S.; Ragusa, F.; Büscher, V.; Dietl, H.; Ganis, G.; Hüttmann, K.; Lütjens, G.; Mannert, C.; Männer, W.; Moser, H. G.; Schael, S.; Settles, R.; Seywerd, H.; Stenzel, H.; Wiedenmann, W.; Wolf, G.; Azzurri, P.; Boucrot, J.; Callot, O.; Chen, S.; Davier, M.; Duflot, L.; Grivaz, J.-F.; Heusse, P.; Jachołkowska, A.; Kado, M.; Lefrançois, J.; Serin, L.; Veillet, J. J.; Videau, I.; Regie, J.B. De Vivie De; Zerwas, D.; Bagliesi, G.; Boccali, T.; Bozzi, C.; Calderini, G.; Dell’Orso, R.; Ferrante, I.; Giassi, A.; Gregorio, A.; Ligabue, F.; Marrocchesi, P. S.; Messineo, A.; Palla, F.; Rizzo, G.; Sanguinetti, G.; Sguazzoni, G.; Тенчини, Р.; Venturi, A.; Verdini, P. G.; Blair, G.A.; Coles, Jane; Cowan, G.; Green, M.G.; Hutchcroft, D. E.; Jones, L.T.; Medcalf, T.; Strong, J. A.; Botterill, D.; Clifft, R. W.; Edgecock, T.R.; Norton, P. R.; Thompson, J.C.; Tomalin, I. R.; Bloch-Devaux, B.; Colas, P.; Fabbro, B.; Faı̈f, G.; Lançon, E.; Lemaire, M. C.; Locci, E.; Pérez, P.; Rander, J.; Renardy, J. F.; Rosowsky, A.; Seager, P.; Trabelsi, A.; Tuchming, B.; Vallage, B.; Black, S.N.; Dann, J.H.; Loomis, C.; Kim, H.Y.; Konstantinidis, N.; Litke, A. M.; McNeil, M.A.; Taylor, G. N.; Booth, C.N.; Cartwright, S. L.; Combley, F.; Hodgson, P.; Lehto, M.; Thompson, L.F.; Affholderbach, K.; Böhrer, A.; Brandt, Siegmund; Grupen, C.; Heß, J.; Misiejuk, A.; Prange, G.; Sieler, U.; Giannini, G.; Gobbo, B.; Pütz, J.; Rothberg, J.; Wasserbaech, S.; Williams, R.W.; Armstrong, S.R.; Elmer, P.; Ferguson, D.P.S.; Gao, Y. S.; González, S.; Hayes, O.J.; Hu, H.; Jin, S.; Kile, J.; McNamara, P.A.; Nielsen, J.; Orejudos, W.; Pan, Y.; Saadi, Y.; Scott, I.; Walsh, J.; Wimmersperg-Toeller, J. H. von; Wu, S. L.; Wu, X.; Zobernig, G.

doi:10.1016/s0370-2693(99)01288-5

Cited by 31 publications

(10 citation statements)

References 24 publications

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“…The ZZ production process was first studied at the LEP e þ e − collider at CERN [4][5][6][7] and more recently at the Tevatron pp collider. A previous ZZ production cross section measurement from leptonic final states has been published by the CDF Collaboration using 6 fb −1 of integrated luminosity [8], the result of which is extended here.…”

Section: Introductionmentioning

confidence: 99%

Measurement of theZZproduction cross section using the full CDF II data set

Aaltonen¹,

Amerio²,

Amidei³

et al. 2014

Phys. Rev. D

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We present a measurement of the ZZ-boson pair-production cross section in 1.96 TeV center-of-mass energy pp collisions. We reconstruct final states incorporating four charged leptons or two charged leptons and two neutrinos from the full data set collected by the Collider Detector experiment at the Fermilab Tevatron, corresponding to 9.7 fb −1 of integrated luminosity. Combining the results obtained from each final state, we measure a cross section of 1.04 þ0.32 −0.25 pb, in good agreement with the standard model prediction at next-to-leading order in the strong-interaction coupling.

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Section: Introductionmentioning

confidence: 99%

Measurement of theZZproduction cross section using the full CDF II data set

Aaltonen¹,

Amerio²,

Amidei³

et al. 2014

Phys. Rev. D

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“…A good understanding of ZZ production, along with that of the other massive diboson processes (W W , W Z), is an essential component of new physics searches including searches for the Higgs boson, since these processes share similar experimental signatures. ZZ production was first studied at the LEP e + e − collider at CERN [4][5][6][7] and later investigated at the Tevatron pp collider [8,9]. W W [10] and W Z [11] production has already been observed and precisely measured.…”

mentioning

confidence: 99%

Measurement ofZZProduction in Leptonic Final States atsof 1.96 TeV at CDF

Aaltonen¹,

Gonzlez²,

Amerio³

et al. 2012

Phys. Rev. Lett.

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In this Letter, we present a precise measurement of the total ZZ production cross section in pp collisions at sqrt[s]=1.96 TeV, using data collected with the CDF II detector corresponding to an integrated luminosity of approximately 6 fb(-1). The result is obtained by combining separate measurements in the four-charged (ℓℓℓ' ℓ') and two-charged-lepton and two-neutral-lepton (ℓℓνν) decay modes of the Z boson pair. The combined measured cross section for pp → ZZ is 1.64(-0.38)(+0.44) pb. This is the most precise measurement of the ZZ production cross section in 1.96 TeV pp collisions to date.

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“…The production of ZZ dibosons in the 4 final state * aliyilmaz@giresun.edu.tr † senol a@ibu.edu.tr ‡ denizli h@ibu.edu.tr § ilkay.turk.cakir@cern.ch ¶ ocakir@science.ankara.edu.tr have been studied by various collaborations such as the Large Electron-Positron (LEP) [3][4][5][6][7][8] where the first bounds on anomalous neutral triple gauge couplings (aNTGCs) using e + e − collider was obtained, the Collider Detector at Fermilab (CDF) [9,10] and DØ [11,12] also searched the limits of aNTGC at Tevatron pp collider. Recently, ATLAS [13,14] and CMS [15,16] collaborations published the improved limits of aNTGCs thanks to the center of mass energy of LHC in the range of 13 TeV at the LHC.…”

Section: Introductionmentioning

confidence: 99%

Sensitivity on anomalous neutral triple gauge couplings via ZZ production at FCC-hh

et al. 2020

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We study the sensitivity of anomalous neutral triple gauge couplings (aN T GC) via pp → ZZ production in the 4 channel at 100 TeV centre of mass energy of future circular hadron collider, FCC-hh. The analysis including the realistic detector effects is performed in the mode where both Z bosons decay into same flavor, oppositely charged lepton pairs. The sensitivities to the charge-parity (CP)conserving CB W /Λ 4 and CP-violating CW W /Λ 4 , CBW /Λ 4 and CBB/Λ 4 couplings obtained at 95% Confidence Level (C.L.) using the invariant mass distribution of 4 system reconstructing the leading and sub-leading Z boson candidates are [−0.117, +0.117], [−0.293, +0.292], [−0.380, +0.379], and [−0.138, +0.138] in the unit of TeV −4 , respectively.

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Measurement of the e+e−→ZZ production cross section at centre-of-mass energies of 183 and 189 GeV

Cited by 31 publications

References 24 publications

Measurement of theZZproduction cross section using the full CDF II data set

Measurement of theZZproduction cross section using the full CDF II data set

Measurement ofZZProduction in Leptonic Final States atsof 1.96 TeV at CDF

Sensitivity on anomalous neutral triple gauge couplings via ZZ production at FCC-hh

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