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and Khakzad, M and Mohammadi Najafabadi, M and Naseri, M and Rezaei Hosseinabadi, F and Felcini, M and Grunewald, M and Abbrescia, M and Aly, R and Calabria, C and Colaleo, A and Creanza, D and Cristella, L and De Filippis, N and De Palma, M and Di Florio, A and Elmetenawee, W and Fiore, L and Gelmi, A and Iaselli, G and Ince, M and Lezki, S and Maggi, G and Maggi, M and Merlin, JA and Miniello, G and My, S and Nuzzo, S and Pompili, A and Pugliese, G and Radogna, R and Ranieri, A and Selvaggi, G and Silvestris, L and Simone, FM and Venditti, R and Verwilligen, P and Abbiendi, G and Battilana, C and Bonacorsi, D and Borgonovi, L and Braibant-Giacomelli, S and Campanini, R and Capiluppi, P and Castro, A and Cavallo, FR and Ciocca, C and Codispoti, G and Cuffiani, M and Dallavalle, GM and Fabbri, F and Fanfani, A and Fontanesi, E and Giacomelli, P and Grandi, C and Guiducci, L and Iemmi, F and Lo Meo, S and Marcellini, S and Masetti, G and Navarria, FL and Perrotta, A and Primavera, F and Rossi, AM and Rovelli, T and Siroli, GP and Tosi, N and Albergo, S and Costa, S and Di Mattia, A and Potenza, R and Tricomi, A and Tuve, C and Barbagli, G and Cassese, A and Ceccarelli, R and Ciulli, V and Civinini, C and D'Alessandro, R and Fiori, F and Focardi, E and Latino, G and Lenzi, P and Meschini, M and Paoletti, S and Sguazzoni, G and Viliani, L and Benussi, L and Bianco, S and Piccolo, D and Bozzo, M and Ferro, F and Mulargia, R and Robutti, E and Tosi, S and Benaglia, A and Beschi, A and Brivio, F and Ciriolo, V and Di Guida, S and Dinardo, ME and Dini, P and Gennai, S and Ghezzi, A and Govoni, P and Guzzi, L and Malberti, M and Malvezzi, S and Menasce, D and Monti, F and Moroni, L and Paganoni, M and Pedrini, D and Ragazzi, S and Tabarelli De Fatis, T and Zuolo, D and Buontempo, S and Cavallo, N and De Iorio, A and Di Crescenzo, A and Fabozzi, F and Fienga, F and Galati, G and Iorio, AOM and Lista, L and Meola, S and Paolucci, P and Rossi, B and Sciacca, C and Voevodina, E 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Manca, E and Mandorli, G and Messineo, A and Palla, F and Rizzi, A and Rolandi, G and Roy Chowdhury, S and Scribano, A and Spagnolo, P and Tenchini, R and Tonelli, G and Turini, N and Venturi, A and Verdini, PG and Cavallari, F and Cipriani, M and Del Re, D and Di Marco, E and Diemoz, M and Longo, E and Meridiani, P and Organtini, G and Pandolfi, F and Paramatti, R and Quaranta, C and Rahatlou, S and Rovelli, C and Santanastasio, F and Soffi, L and Amapane, N and Arcidiacono, R and Argiro, S and Arneodo, M and Bartosik, N and Bellan, R and Bellora, A and Biino, C and Cappati, A and Cartiglia, N and Cometti, S and Costa, M and Covarelli, R and Demaria, N and Kiani, B and Legger, F and Mariotti, C and Maselli, S and Migliore, E and Monaco, V and Monteil, E and Monteno, M and Obertino, MM and Ortona, G and Pacher, L and Pastrone, N and Pelliccioni, M and Pinna Angioni, GL and Romero, A and Ruspa, M and Salvatico, R and Sola, V and Solano, A and Soldi, D and Staiano, A and Trocino, D and 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Chadeeva, M and Parygin, P and Philippov, D and Popova, E and Rusinov, V and Andreev, V and Azarkin, M and Dremin, I and Kirakosyan, M and Terkulov, A and Belyaev, A and Boos, E and Bunichev, V and Dubinin, M and Dudko, L and Klyukhin, V and Kodolova, O and Lokhtin, I and Obraztsov, S and Perfilov, M and Petrushanko, S and Savrin, V and Snigirev, A and Barnyakov, A and Blinov, V and Dimova, T and Kardapoltsev, L and Skovpen, Y and Azhgirey, I and Bayshev, I and Bitioukov, S and Kachanov, V and Konstantinov, D and Mandrik, P and Petrov, V and Ryutin, R and Slabospitskii, S and Sobol, A and Troshin, S and Tyurin, N and Uzunian, A and Volkov, A and Babaev, A and Iuzhakov, A and Okhotnikov, V and Borchsh, V and Ivanchenko, V and Tcherniaev, E and Adzic, P and Cirkovic, P and Dordevic, M and Milenovic, P and Milosevic, J and Stojanovic, M and Aguilar-Benitez, M and Alcaraz Maestre, J and Ã�lvarez Fernández, A and Bachiller, I and Barrio Luna, M and Bedoya, CF and Brochero Cifuentes, JA and 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In: Physical Review D, 102 (3).
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Abstract
Ratios of cross sections, Ï�(Z+c jets)/Ï�(Z+jets), Ï�(Z+b jets)/Ï�(Z+jets), and Ï�(Z+c jets)/Ï�(Z+b jets) in the associated production of a Z boson with at least one charm or bRatios of cross sections, σ(Z+c jets)/σ(Z+jets), σ(Z+b jets)/σ(Z+jets), and σ(Z+c jets)/σ(Z+b jets) in the associated production of a Z boson with at least one charm or bottom quark jet are measured in proton-proton collisions at s=13 TeV. The data sample, collected by the CMS experiment at the CERN LHC, corresponds to an integrated luminosity of 35.9 fb-1, with a fiducial volume of pT>30 GeV and |η|<2.4 for the jets, where pT and η represent transverse momentum and pseudorapidity, respectively. The Z boson candidates come from leptonic decays into electrons or muons with pT>25 GeV and |η|<2.4, and the dilepton mass satisfies 71<mZ<111 GeV. The measured values are σ(Z+c jets)/σ(Z+jets)=0.102±0.002±0.009, σ(Z+b jets)/σ(Z+jets)=0.0633±0.0004±0.0015, and σ(Z+c jets)/σ(Z+b jets)=1.62±0.03±0.15. Results on the inclusive and differential cross section ratios as functions of jet and Z boson transverse momentum are compared with predictions from leading and next-to-leading order perturbative quantum chromodynamics calculations. These are the first measurements of the cross section ratios at 13 TeV. © 2020 American Physical Society. All rights reserved.ottom quark jet are measured in proton-proton collisions at s=13 TeV. The data sample, collected by the CMS experiment at the CERN LHC, corresponds to an integrated luminosity of 35.9 fb-1, with a fiducial volume of pT>30 GeV and |η|<2.4 for the jets, where pT and η represent transverse momentum and pseudorapidity, respectively. The Z boson candidates come from leptonic decays into electrons or muons with pT>25 GeV and |η|<2.4, and the dilepton mass satisfies 71<mZ<111 GeV. The measured values are Ï�(Z+c jets)/Ï�(Z+jets)=0.102±0.002±0.009, Ï�(Z+b jets)/Ï�(Z+jets)=0.0633±0.0004±0.0015, and Ï�(Z+c jets)/Ï�(Z+b jets)=1.62±0.03±0.15. Results on the inclusive and differential cross section ratios as functions of jet and Z boson transverse momentum are compared with predictions from leading and next-to-leading order perturbative quantum chromodynamics calculations. These are the first measurements of the cross section ratios at 13 TeV. © 2020 American Physical Society. All rights reserved.
| Item Type: | Journal Article |
|---|---|
| Publication: | Physical Review D |
| Publisher: | American Physical Society |
| Additional Information: | The copyright for this article belongs to the Author(s). |
| Department/Centre: | Division of Physical & Mathematical Sciences > Centre for High Energy Physics |
| Date Deposited: | 13 Jan 2023 06:42 |
| Last Modified: | 13 Jan 2023 06:42 |
| URI: | https://eprints.iisc.ac.in/id/eprint/79107 |
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