The double differential cross sections of the Drell–Yan lepton pair (
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- Azimuthal correlations in Z +jets events in proton–proton collisions at $$\sqrt{s} = 13\,\text {Te}\hspace{-.08em}\text {V} $$
This content will become publicly available on August 1, 2024
Title:
Azimuthal correlations in Z +jets events in proton–proton collisions at $$\sqrt{s} = 13\,\text {Te}\hspace{-.08em}\text {V} $$
Abstract The production of Z bosons associated with jets is measured in $$\text {p}\text {p}$$ pp collisions at $$\sqrt{s}=13\,\text {Te}\hspace{-.08em}\text {V} $$ s = 13 Te V with data recorded with the CMS experiment at the LHC corresponding to an integrated luminosity of 36.3 $$\,\text {fb}^{-1}$$ fb - 1 . The multiplicity of jets with transverse momentum $$p_{\textrm{T}} > 30\,\text {Ge}\hspace{-.08em}\text {V} $$ p T > 30 Ge V is measured for different regions of the Z boson’s $$p_{\textrm{T}} (\text {Z })$$ p T ( Z ) , from lower than 10 $$\,\text {Ge}\hspace{-.08em}\text {V}$$ Ge V to higher than 100 $$\,\text {Ge}\hspace{-.08em}\text {V}$$ Ge V . The azimuthal correlation $$\varDelta \phi $$ Δ ϕ between the Z boson and the leading jet, as well as the correlations between the two leading jets are measured in three regions of $$p_{\textrm{T}} (\text {Z })$$ p T ( Z ) . The measurements are compared with several predictions at leading and next-to-leading orders, interfaced with parton showers. Predictions based on transverse-momentum dependent parton distributions and corresponding parton showers give a good description of the measurement in the regions where multiple parton interactions and higher jet multiplicities are not important. The effects of multiple parton interactions are shown to be important to correctly describe the measured spectra in the low $$p_{\textrm{T}} (\text {Z })$$ p T ( Z ) regions.
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- NSF-PAR ID:
- 10463777
- Author(s) / Creator(s):
- Tumasyan, A.; Adam, W.; Andrejkovic, J. W.; Bergauer, T.; Chatterjee, S.; Damanakis, K.; Dragicevic, M.; Valle, A. Escalante; Frühwirth, R.; Jeitler, M.; Krammer, N.; Lechner, L.; Liko, D.; Mikulec, I.; Paulitsch, P.; Pitters, F. M.; Schieck, J.; Schöfbeck, R.; Schwarz, D.; Templ, S.more » ; Waltenberger, W.; Wulz, C.-E.; Darwish, M. R.; De Wolf, E. A.; Janssen, T.; Kello, T.; Lelek, A.; Sfar, H. Rejeb; Mechelen, P. Van; Putte, S. Van; Remortel, N. Van; Bols, E. S.; D’Hondt, J.; De Moor, A.; Delcourt, M.; El Faham, H.; Lowette, S.; Moortgat, S.; Morton, A.; Müller, D.; Sahasransu, A. R.; Tavernier, S.; Van Doninck, W.; Vannerom, D.; Beghin, D.; Bilin, B.; Clerbaux, B.; De Lentdecker, G.; Favart, L.; Kalsi, A. K.; Lee, K.; Mahdavikhorrami, M.; Makarenko, I.; Paredes, S.; Pétré, L.; Popov, A.; Postiau, N.; Starling, E.; Thomas, L.; Bemden, M. Vanden; Velde, C. 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H.; Teague, D.; Trembath-Reichert, S.; Vetens, W.; Afanasiev, S.; Andreev, V.; Andreev, Yu.; Aushev, T.; Azarkin, M.; Babaev, A.; Belyaev, A.; Blinov, V.; Boos, E.; Borshch, V.; Budkouski, D.; Bychkova, O.; Chekhovsky, V.; Chistov, R.; Danilov, M.; Dermenev, A.; Dimova, T.; Dremin, I.; Dubinin, M.; Dudko, L.; Epshteyn, V.; Gavrilov, G.; Gavrilov, V.; Gninenko, S.; Golovtcov, V.; Golubev, N.; Golutvin, I.; Gorbunov, I.; Gribushin, A.; Ivanchenko, V.; Ivanov, Y.; Kachanov, V.; Kardapoltsev, L.; Karjavine, V.; Karneyeu, A.; Kim, V.; Kirakosyan, M.; Kirpichnikov, D.; Kirsanov, M.; Klyukhin, V.; Kodolova, O.; Konstantinov, D.; Korenkov, V.; Kozyrev, A.; Krasnikov, N.; Kuznetsova, E.; Lanev, A.; Litomin, A.; Lukina, O.; Lychkovskaya, N.; Makarenko, V.; Malakhov, A.; Matveev, V.; Murzin, V.; Nikitenko, A.; Obraztsov, S.; Okhotnikov, V.; Oreshkin, V.; Oskin, A.; Ovtin, I.; Palichik, V.; Parygin, P.; Pashenkov, A.; Perelygin, V.; Petrushanko, S.; Pivovarov, G.; Polikarpov, S.; Popov, V.; Radchenko, O.; Savina, M.; Savrin, V.; Shalaev, V.; Shmatov, S.; Shulha, S.; Skovpen, Y.; Slabospitskii, S.; Smirnov, I.; Smirnov, V.; Snigirev, A.; Sosnov, D.; Stepennov, A.; Sulimov, V.; Tcherniaev, E.; Terkulov, A.; Teryaev, O.; Toms, M.; Toropin, A.; Uvarov, L.; Uzunian, A.; Vlasov, E.; Volkov, S.; Vorobyev, A.; Voytishin, N.; Yuldashev, B. S.; Zarubin, A.; Zhizhin, I.; Zhokin, A. « less
- Date Published:
- Journal Name:
- The European Physical Journal C
- Volume:
- 83
- Issue:
- 8
- ISSN:
- 1434-6052
- Format(s):
- Medium: X
- Sponsoring Org:
- National Science Foundation
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Tumasyan, A. ; Adam, W. ; Andrejkovic, J. W. ; Bergauer, T. ; Chatterjee, S. ; Damanakis, K. ; Dragicevic, M. ; Valle, A. Escalante ; Frühwirth, R. ; Jeitler, M. ; et al ( , The European Physical Journal C)Abstract Multijet events at large transverse momentum ( $$p_{\textrm{T}}$$ p T ) are measured at $$\sqrt{s}=13\,\text {TeV} $$ s = 13 TeV using data recorded with the CMS detector at the LHC, corresponding to an integrated luminosity of $$36.3{\,\text {fb}^{-1}} $$ 36.3 fb - 1 . The multiplicity of jets with $$p_{\textrm{T}} >50\,\text {GeV} $$ p T > 50 GeV that are produced in association with a high- $$p_{\textrm{T}}$$ p T dijet system is measured in various ranges of the $$p_{\textrm{T}}$$ p T of the jet with the highest transverse momentum and as a function of the azimuthal angle difference $$\varDelta \phi _{1,2}$$ Δ ϕ 1 , 2 between the two highest $$p_{\textrm{T}}$$ p T jets in the dijet system. The differential production cross sections are measured as a function of the transverse momenta of the four highest $$p_{\textrm{T}}$$ p T jets. The measurements are compared with leading and next-to-leading order matrix element calculations supplemented with simulations of parton shower, hadronization, and multiparton interactions. In addition, the measurements are compared with next-to-leading order matrix element calculations combined with transverse-momentum dependent parton densities and transverse-momentum dependent parton shower.more » « less
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Sirunyan, A. M. ; Tumasyan, A. ; Adam, W. ; Andrejkovic, J. W. ; Bergauer, T. ; Chatterjee, S. ; Dragicevic, M. ; Valle, A. Escalante ; Frühwirth, R. ; Jeitler, M. ; et al ( , The European Physical Journal C)null (Ed.)Abstract Production cross sections of the Higgs boson are measured in the $${\mathrm{H}} \rightarrow {\mathrm{Z}} {\mathrm{Z}} \rightarrow 4\ell $$ H → Z Z → 4 ℓ ( $$\ell ={\mathrm{e}},{{{\upmu }}_{\mathrm{}}^{\mathrm{}}} $$ ℓ = e , μ ) decay channel. A data sample of proton–proton collisions at a center-of-mass energy of 13 $$\,\text {Te}\text {V}$$ Te , collected by the CMS detector at the LHC and corresponding to an integrated luminosity of 137 $$\,\text {fb}^{-1}$$ fb - 1 is used. The signal strength modifier $$\mu $$ μ , defined as the ratio of the Higgs boson production rate in the $$4\ell $$ 4 ℓ channel to the standard model (SM) expectation, is measured to be $$\mu =0.94 \pm 0.07 \,\text {(stat)} ^{+0.09}_{-0.08} \,\text {(syst)} $$ μ = 0.94 ± 0.07 (stat) - 0.08 + 0.09 (syst) at a fixed value of $$m_{{\mathrm{H}}} = 125.38\,\text {Ge}\text {V} $$ m H = 125.38 Ge . The signal strength modifiers for the individual Higgs boson production modes are also reported. The inclusive fiducial cross section for the $${\mathrm{H}} \rightarrow 4\ell $$ H → 4 ℓ process is measured to be $$2.84^{+0.23}_{-0.22} \,\text {(stat)} ^{+0.26}_{-0.21} \,\text {(syst)} \,\text {fb} $$ 2 . 84 - 0.22 + 0.23 (stat) - 0.21 + 0.26 (syst) fb , which is compatible with the SM prediction of $$2.84 \pm 0.15 \,\text {fb} $$ 2.84 ± 0.15 fb for the same fiducial region. Differential cross sections as a function of the transverse momentum and rapidity of the Higgs boson, the number of associated jets, and the transverse momentum of the leading associated jet are measured. A new set of cross section measurements in mutually exclusive categories targeted to identify production mechanisms and kinematical features of the events is presented. The results are in agreement with the SM predictions.more » « less
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Tumasyan, A. ; Adam, W. ; Andrejkovic, J. W. ; Bergauer, T. ; Chatterjee, S. ; Damanakis, K. ; Dragicevic, M. ; Escalante Del Valle, A. ; Hussain, P. S. ; Jeitler, M. ; et al ( , The European Physical Journal C)more » « less
Abstract A search for decays to invisible particles of Higgs bosons produced in association with a top-antitop quark pair or a vector boson, which both decay to a fully hadronic final state, has been performed using proton-proton collision data collected at
$${\sqrt{s}=13\,\text {Te}\hspace{-.08em}\text {V}}$$ $$\,\text {fb}^{-1}$$ $$\,\text {Ge}\hspace{-.08em}\text {V}$$ $${\mathcal {B}({\textrm{H}} \rightarrow \text {inv})}$$ $${\mathcal {B}({\textrm{H}} \rightarrow \text {inv})}$$ $${\sqrt{s}=7}$$ $$\,\text {Te}\hspace{-.08em}\text {V}$$ $${\mathcal {B}({\textrm{H}} \rightarrow \text {inv})}$$ -
Tumasyan, A. ; Adam, W. ; Andrejkovic, J. W. ; Bergauer, T. ; Chatterjee, S. ; Damanakis, K. ; Dragicevic, M. ; Escalante Del Valle, A. ; Hussain, P. S. ; Jeitler, M. ; et al ( , The European Physical Journal C)more » « less
Abstract Production cross sections of the standard model Higgs boson decaying to a pair of W bosons are measured in proton-proton collisions at a center-of-mass energy of 13
$$\,\text {Te\hspace{-.08em}V}$$ $$\,\text {fb}^{-1}$$ $$\mu $$ $$\mu = 0.95^{+0.10}_{-0.09}$$
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- https://doi.org/10.1140/epjc/s10052-023-11833-z
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!- Citation Formats
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Cite: MLA FormatTumasyan, A., Adam, W., Andrejkovic, J. W., Bergauer, T., Chatterjee, S., Damanakis, K., Dragicevic, M., Valle, A. Escalante, Frühwirth, R., Jeitler, M., Krammer, N., Lechner, L., Liko, D., Mikulec, I., Paulitsch, P., Pitters, F. M., Schieck, J., Schöfbeck, R., Schwarz, D., Templ, S., Waltenberger, W., Wulz, C.-E., Darwish, M. R., De Wolf, E. A., Janssen, T., Kello, T., Lelek, A., Sfar, H. Rejeb, Mechelen, P. Van, Putte, S. Van, Remortel, N. Van, Bols, E. S., D’Hondt, J., De Moor, A., Delcourt, M., El Faham, H., Lowette, S., Moortgat, S., Morton, A., Müller, D., Sahasransu, A. R., Tavernier, S., Van Doninck, W., Vannerom, D., Beghin, D., Bilin, B., Clerbaux, B., De Lentdecker, G., Favart, L., Kalsi, A. K., Lee, K., Mahdavikhorrami, M., Makarenko, I., Paredes, S., Pétré, L., Popov, A., Postiau, N., Starling, E., Thomas, L., Bemden, M. Vanden, Velde, C. 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S., Zarubin, A., Zhizhin, I., and Zhokin, A. "Azimuthal correlations in Z +jets events in proton–proton collisions at $$\sqrt{s} = 13\,\text {Te}\hspace{-.08em}\text {V} $$". The European Physical Journal C 83 (8). Country unknown/Code not available. https://doi.org/10.1140/epjc/s10052-023-11833-z. https://par.nsf.gov/biblio/10463777.
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place = {Country unknown/Code not available}, title = {Azimuthal correlations in Z +jets events in proton–proton collisions at $$\sqrt{s} = 13\,\text {Te}\hspace{-.08em}\text {V} $$}, url = {https://par.nsf.gov/biblio/10463777}, DOI = {10.1140/epjc/s10052-023-11833-z}, abstractNote = {Abstract The production of Z bosons associated with jets is measured in $$\text {p}\text {p}$$ pp collisions at $$\sqrt{s}=13\,\text {Te}\hspace{-.08em}\text {V} $$ s = 13 Te V with data recorded with the CMS experiment at the LHC corresponding to an integrated luminosity of 36.3 $$\,\text {fb}^{-1}$$ fb - 1 . The multiplicity of jets with transverse momentum $$p_{\textrm{T}} > 30\,\text {Ge}\hspace{-.08em}\text {V} $$ p T > 30 Ge V is measured for different regions of the Z boson’s $$p_{\textrm{T}} (\text {Z })$$ p T ( Z ) , from lower than 10 $$\,\text {Ge}\hspace{-.08em}\text {V}$$ Ge V to higher than 100 $$\,\text {Ge}\hspace{-.08em}\text {V}$$ Ge V . The azimuthal correlation $$\varDelta \phi $$ Δ ϕ between the Z boson and the leading jet, as well as the correlations between the two leading jets are measured in three regions of $$p_{\textrm{T}} (\text {Z })$$ p T ( Z ) . The measurements are compared with several predictions at leading and next-to-leading orders, interfaced with parton showers. Predictions based on transverse-momentum dependent parton distributions and corresponding parton showers give a good description of the measurement in the regions where multiple parton interactions and higher jet multiplicities are not important. The effects of multiple parton interactions are shown to be important to correctly describe the measured spectra in the low $$p_{\textrm{T}} (\text {Z })$$ p T ( Z ) regions.}, journal = {The European Physical Journal C}, volume = {83}, number = {8}, author = {Tumasyan, A. and Adam, W. and Andrejkovic, J. W. and Bergauer, T. and Chatterjee, S. and Damanakis, K. and Dragicevic, M. and Valle, A. 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