Artículo

Evidence for the spin-0 nature of the Higgs boson using ATLAS data

Aad, G. ; Abajyan, T. ; Abbott, B. ; Abdallah, J. ; Abdel Khalek, S. ; Alonso, Francisco Icon; Anduaga, Xabier Sebastian Icon; Dova, Maria Teresa Icon; González Silva, María Laura Icon; Monticelli, Fernando Gabriel Icon; Otero y Garzon, Gustavo Javier Icon; Piegaia, Ricardo Nestor Icon; Romeo, Gaston Leonardo Icon; Tripiana, Martin Fernando Icon; Zhuang, X. ; Zhuravlov, V. ; Zieminska, D. ; Zimin, N. I. ; Zimmermann, R. ; Zimmermann, S. ; Zimmermann, S. ; Ziolkowski, M. ; Zitoun, R. ; Živković, L. ; Zmouchko, V. V. ; Zobernig, G. ; Zoccoli, A. ; zur Nedden, M. ; Zutshi, V. ; Zwalinski, L

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Fecha

07/2013

Editorial

Elsevier Science

Revista

Physics Letters B

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Institución organizadora

ISSN

0370-2693

eISSN

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Inglés

Tipo del evento

Clasificación temática

Resumen

Studies of the spin and parity quantum numbers of the Higgs boson are presented, based on proton– proton collision data collected by the ATLAS experiment at the LHC. The Standard Model spin–parity J P = 0+ hypothesis is compared with alternative hypotheses using the Higgs boson decays H → γγ , H → Z Z∗ → 4 and H → W W ∗ → ν ν, as well as the combination of these channels. The analysed dataset corresponds to an integrated luminosity of 20.7 fb−1 collected at a centre-of-mass energy of √s = 8 TeV. For the H → Z Z∗ → 4 decay mode the dataset corresponding to an integrated luminosity of 4.6 fb−1 collected at √s = 7 TeV is included. The data are compatible with the Standard Model J P = 0+ quantum numbers for the Higgs boson, whereas all alternative hypotheses studied in this Letter, namely some specific J P = 0−, 1+, 1−, 2+ models, are excluded at confidence levels above 97.8%. This exclusion holds independently of the assumptions on the coupling strengths to the Standard Model particles and in the case of the J P = 2+ model, of the relative fractions of gluon-fusion and quark–antiquark production of the spin-2 particle. The data thus provide evidence for the spin-0 nature of the Higgs boson, with positive parity being strongly preferred.

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