Abstract
Combined measurements of the production and decay rates of the Higgs boson, as well as its couplings to vector bosons and fermions, are presented. The analysis uses the LHC proton–proton collision data set recorded with the CMS detector in 2016 at s=13Te, corresponding to an integrated luminosity of 35.9fb-1. The combination is based on analyses targeting the five main Higgs boson production mechanisms (gluon fusion, vector boson fusion, and associated production with a W or Z boson, or a top quark-antiquark pair) and the following decay modes: H → γγ, Z Z , W W , ττ, b b , and μμ. Searches for invisible Higgs boson decays are also considered. The best-fit ratio of the signal yield to the standard model expectation is measured to be μ= 1.17 ± 0.10 , assuming a Higgs boson mass of 125.09Ge. Additional results are given for various assumptions on the scaling behavior of the production and decay modes, including generic parametrizations based on ratios of cross sections and branching fractions or couplings. The results are compatible with the standard model predictions in all parametrizations considered. In addition, constraints are placed on various two Higgs doublet models.
Original language | English |
---|---|
Article number | 421 |
Number of pages | 44 |
Journal | European Physical Journal C |
Volume | 79 |
Issue number | 5 |
DOIs | |
Publication status | Published - 1 May 2019 |
Externally published | Yes |
Keywords
- Collisions
- Proton–proton collisions
- Jets
Cite this
- APA
- Author
- BIBTEX
- Harvard
- Standard
- RIS
- Vancouver
}
In: European Physical Journal C, Vol. 79, No. 5, 421, 01.05.2019.
Research output: Contribution to journal › Article › Research › peer-review
TY - JOUR
T1 - Combined measurements of Higgs boson couplings in proton–proton collisions at √s=13TeV
AU - Sirunyan, A. M.
AU - Tumasyan, A.
AU - Adam, W.
AU - Ambrogi, F.
AU - Asilar, E.
AU - Bergauer, T.
AU - Brandstetter, J.
AU - Dragicevic, M.
AU - Erö, J.
AU - Del Valle, A. Escalante
AU - Flechl, M.
AU - Frühwirth, R.
AU - Ghete, V. M.
AU - Hrubec, J.
AU - Jeitler, M.
AU - Krammer, N.
AU - Krätschmer, I.
AU - Liko, D.
AU - Madlener, T.
AU - Mikulec, I.
AU - Rad, N.
AU - Rohringer, H.
AU - Schieck, J.
AU - Schöfbeck, R.
AU - Spanring, M.
AU - Spitzbart, D.
AU - Taurok, A.
AU - Waltenberger, W.
AU - Wittmann, J.
AU - Wulz, C. E.
AU - Zarucki, M.
AU - Chekhovsky, V.
AU - Mossolov, V.
AU - Gonzalez, J. Suarez
AU - De Wolf, E. A.
AU - Di Croce, D.
AU - Janssen, X.
AU - Lauwers, J.
AU - Pieters, M.
AU - Van Haevermaet, H.
AU - Van Mechelen, P.
AU - Van Remortel, N.
AU - Zeid, S. Abu
AU - Blekman, F.
AU - D’Hondt, J.
AU - De Bruyn, I.
AU - De Clercq, J.
AU - Deroover, K.
AU - Flouris, G.
AU - Lontkovskyi, D.
AU - Lowette, S.
AU - Marchesini, I.
AU - Moortgat, S.
AU - Moreels, L.
AU - Python, Q.
AU - Skovpen, K.
AU - Tavernier, S.
AU - Van Doninck, W.
AU - Van Mulders, P.
AU - Van Parijs, I.
AU - Beghin, D.
AU - Bilin, B.
AU - Brun, H.
AU - Clerbaux, B.
AU - De Lentdecker, G.
AU - Delannoy, H.
AU - Dorney, B.
AU - Fasanella, G.
AU - Favart, L.
AU - Goldouzian, R.
AU - Grebenyuk, A.
AU - Kalsi, A. K.
AU - Lenzi, T.
AU - Luetic, J.
AU - Postiau, N.
AU - Starling, E.
AU - Thomas, L.
AU - Velde, C. Vander
AU - Vanlaer, P.
AU - Vannerom, D.
AU - Wang, Q.
AU - Cornelis, T.
AU - Dobur, D.
AU - Fagot, A.
AU - Gul, M.
AU - Khvastunov, I.
AU - Poyraz, D.
AU - Roskas, C.
AU - Trocino, D.
AU - Tytgat, M.
AU - Verbeke, W.
AU - Vermassen, B.
AU - Vit, M.
AU - Zaganidis, N.
AU - Bakhshiansohi, H.
AU - Bondu, O.
AU - Brochet, S.
AU - Bruno, G.
AU - Caputo, C.
AU - David, P.
AU - Delaere, C.
AU - Delcourt, M.
AU - Francois, B.
AU - Giammanco, A.
AU - Krintiras, G.
AU - Lemaitre, V.
AU - Magitteri, A.
AU - Mertens, A.
AU - Musich, M.
AU - Piotrzkowski, K.
AU - Saggio, A.
AU - Marono, M. Vidal
AU - Wertz, S.
AU - Zobec, J.
AU - Alves, F. L.
AU - Alves, G. A.
AU - Martins Junior, M. Correa
AU - Silva, G. Correia
AU - Hensel, C.
AU - Moraes, A.
AU - Pol, M. E.
AU - Teles, P. Rebello
AU - Das Chagas, E. Belchior Batista
AU - Carvalho, W.
AU - Chinellato, J.
AU - Coelho, E.
AU - Da Costa, E. M.
AU - Da Silveira, G. G.
AU - De Jesus Damiao, D.
AU - De Oliveira Martins, C.
AU - De Souza, S. Fonseca
AU - Malbouisson, H.
AU - Figueiredo, D. Matos
AU - De Almeida, M. Melo
AU - Herrera, C. Mora
AU - Mundim, L.
AU - Nogima, H.
AU - Da Silva, W. L.Prado
AU - Rosas, L. J.Sanchez
AU - Santoro, A.
AU - Sznajder, A.
AU - Thiel, M.
AU - Manganote, E. J.Tonelli
AU - De Araujo, F. Torres Da Silva
AU - Pereira, A. Vilela
AU - Ahuja, S.
AU - Bernardes, C. A.
AU - Calligaris, L.
AU - Tomei, T. R.Fernandez Perez
AU - Gregores, E. M.
AU - Mercadante, P. G.
AU - Novaes, S. F.
AU - Padula, Sandra S.
AU - Aleksandrov, A.
AU - Hadjiiska, R.
AU - Iaydjiev, P.
AU - Marinov, A.
AU - Misheva, M.
AU - Rodozov, M.
AU - Shopova, M.
AU - Sultanov, G.
AU - Dimitrov, A.
AU - Litov, L.
AU - Pavlov, B.
AU - Petkov, P.
AU - Fang, W.
AU - Gao, X.
AU - Yuan, L.
AU - Ahmad, M.
AU - Bian, J. G.
AU - Chen, G. M.
AU - Chen, H. S.
AU - Chen, M.
AU - Chen, Y.
AU - Jiang, C. H.
AU - Leggat, D.
AU - Liao, H.
AU - Liu, Z.
AU - Romeo, F.
AU - Shaheen, S. M.
AU - Spiezia, A.
AU - Tao, J.
AU - Wang, C.
AU - Wang, Z.
AU - Yazgan, E.
AU - Zhang, H.
AU - Zhang, S.
AU - Zhao, J.
AU - Ban, Y.
AU - Chen, G.
AU - Levin, A.
AU - Li, J.
AU - Li, L.
AU - Li, Q.
AU - Mao, Y.
AU - Qian, S. J.
AU - Wang, D.
AU - Xu, Z.
AU - Wang, Y.
AU - Avila, C.
AU - Cabrera, A.
AU - Montoya, C. A.Carrillo
AU - Sierra, L. F.Chaparro
AU - Florez, C.
AU - Hernández, C. F.González
AU - Delgado, M. A.Segura
AU - Courbon, B.
AU - Godinovic, N.
AU - Lelas, D.
AU - Puljak, I.
AU - Sculac, T.
AU - Antunovic, Z.
AU - Kovac, M.
AU - Brigljevic, V.
AU - Ferencek, D.
AU - Kadija, K.
AU - Mesic, B.
AU - Starodumov, A.
AU - Susa, T.
AU - Ather, M. W.
AU - Attikis, A.
AU - Kolosova, M.
AU - Mavromanolakis, G.
AU - Mousa, J.
AU - Nicolaou, C.
AU - Ptochos, F.
AU - Razis, P. A.
AU - Rykaczewski, H.
AU - Finger, M.
AU - Finger, M.
AU - Ayala, E.
AU - Jarrin, E. Carrera
AU - Abdalla, H.
AU - Abdelalim, A. A.
AU - Salama, E.
AU - Bhowmik, S.
AU - De Oliveira, A. Carvalho Antunes
AU - Dewanjee, R. K.
AU - Ehataht, K.
AU - Kadastik, M.
AU - Raidal, M.
AU - Veelken, C.
AU - Eerola, P.
AU - Kirschenmann, H.
AU - Pekkanen, J.
AU - Voutilainen, M.
AU - Havukainen, J.
AU - Heikkilä, J. K.
AU - Nash, J.
AU - Laird, E.
AU - CMS Collaboration
PY - 2019/5/1
Y1 - 2019/5/1
N2 - Combined measurements of the production and decay rates of the Higgs boson, as well as its couplings to vector bosons and fermions, are presented. The analysis uses the LHC proton–proton collision data set recorded with the CMS detector in 2016 at s=13Te, corresponding to an integrated luminosity of 35.9fb-1. The combination is based on analyses targeting the five main Higgs boson production mechanisms (gluon fusion, vector boson fusion, and associated production with a W or Z boson, or a top quark-antiquark pair) and the following decay modes: H → γγ, Z Z , W W , ττ, b b , and μμ. Searches for invisible Higgs boson decays are also considered. The best-fit ratio of the signal yield to the standard model expectation is measured to be μ= 1.17 ± 0.10 , assuming a Higgs boson mass of 125.09Ge. Additional results are given for various assumptions on the scaling behavior of the production and decay modes, including generic parametrizations based on ratios of cross sections and branching fractions or couplings. The results are compatible with the standard model predictions in all parametrizations considered. In addition, constraints are placed on various two Higgs doublet models.
AB - Combined measurements of the production and decay rates of the Higgs boson, as well as its couplings to vector bosons and fermions, are presented. The analysis uses the LHC proton–proton collision data set recorded with the CMS detector in 2016 at s=13Te, corresponding to an integrated luminosity of 35.9fb-1. The combination is based on analyses targeting the five main Higgs boson production mechanisms (gluon fusion, vector boson fusion, and associated production with a W or Z boson, or a top quark-antiquark pair) and the following decay modes: H → γγ, Z Z , W W , ττ, b b , and μμ. Searches for invisible Higgs boson decays are also considered. The best-fit ratio of the signal yield to the standard model expectation is measured to be μ= 1.17 ± 0.10 , assuming a Higgs boson mass of 125.09Ge. Additional results are given for various assumptions on the scaling behavior of the production and decay modes, including generic parametrizations based on ratios of cross sections and branching fractions or couplings. The results are compatible with the standard model predictions in all parametrizations considered. In addition, constraints are placed on various two Higgs doublet models.
KW - Collisions
KW - Proton–proton collisions
KW - Jets
UR - http://www.scopus.com/inward/record.url?scp=85066045697&partnerID=8YFLogxK
U2 - 10.1140/epjc/s10052-019-6909-y
DO - 10.1140/epjc/s10052-019-6909-y
M3 - Article
AN - SCOPUS:85066045697
SN - 1434-6044
VL - 79
JO - European Physical Journal C
JF - European Physical Journal C
IS - 5
M1 - 421
ER -