The mass of the top quark is measured in 36.3
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- Search Results
- Measurement of the differential $$\hbox {t}\overline{\hbox {t}}$$ production cross section as a function of the jet mass and extraction of the top quark mass in hadronic decays of boosted top quarks
This content will become publicly available on July 1, 2024
Title:
Measurement of the differential $$\hbox {t}\overline{\hbox {t}}$$ production cross section as a function of the jet mass and extraction of the top quark mass in hadronic decays of boosted top quarks
Abstract A measurement of the jet mass distribution in hadronic decays of Lorentz-boosted top quarks is presented. The measurement is performed in the lepton + jets channel of top quark pair production ( $$\hbox {t}\overline{\hbox {t}}$$ t t ¯ ) events, where the lepton is an electron or muon. The products of the hadronic top quark decay are reconstructed using a single large-radius jet with transverse momentum greater than 400 $$\,\text {Ge}\hspace{-.08em}\text {V}$$ Ge V . The data were collected with the CMS detector at the LHC in proton-proton collisions and correspond to an integrated luminosity of 138 $$\,\text {fb}^{-1}$$ fb - 1 . The differential $$\hbox {t}\overline{\hbox {t}}$$ t t ¯ production cross section as a function of the jet mass is unfolded to the particle level and is used to extract the top quark mass. The jet mass scale is calibrated using the hadronic W boson decay within the large-radius jet. The uncertainties in the modelling of the final state radiation are reduced by studying angular correlations in the jet substructure. These developments lead to a significant increase in precision, and a top quark mass of $$173.06 \pm 0.84\,\text {Ge}\hspace{-.08em}\text {V} $$ 173.06 ± 0.84 Ge V .
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- NSF-PAR ID:
- 10463776
- Author(s) / Creator(s):
- Tumasyan, A.; Adam, W.; Andrejkovic, J. W.; Bergauer, T.; Chatterjee, S.; Damanakis, K.; Dragicevic, M.; Valle, A. Escalante; Hussain, P. S.; 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.; Janssen, T.; Kello, T.; Sfar, H. Rejeb; Mechelen, P. Van; Bols, E. S.; D’Hondt, J.; De Moor, A.; Delcourt, M.; Faham, H. El; Lowette, S.; Moortgat, S.; Morton, A.; Müller, D.; Sahasransu, A. R.; Tavernier, S.; Doninck, W. Van; Vannerom, D.; Clerbaux, B.; De Lentdecker, G.; Favart, L.; Hohov, D.; Jaramillo, J.; Lee, K.; Mahdavikhorrami, M.; Makarenko, I.; Malara, A.; Paredes, S.; Pétré, L.; Postiau, N.; Thomas, L.; Bemden, M. Vanden; Velde, C. Vander; Vanlaer, P.; Dobur, D.; Knolle, J.; Lambrecht, L.; Mestdach, G.; Niedziela, M.; Rendón, C.; Roskas, C.; Samalan, A.; Skovpen, K.; Tytgat, M.; Bossche, N. Van; Vermassen, B.; Wezenbeek, L.; Benecke, A.; Bruno, G.; Bury, F.; Caputo, C.; David, P.; Delaere, C.; Donertas, I. S.; Giammanco, A.; Jaffel, K.; Jain, Sa.; Lemaitre, V.; Mondal, K.; Taliercio, A.; Tran, T. T.; Vischia, P.; Wertz, S.; Alves, G. A.; Coelho, E.; Hensel, C.; Moraes, A.; Teles, P. Rebello; Júnior, W. L.; Pereira, M. Alves; Filho, M. Barroso; Malbouisson, H. Brandao; Carvalho, W.; Chinellato, J.; Da Costa, E. M.; Da Silveira, G. G.; De Jesus Damiao, D.; Sousa, V. Dos; De Souza, S. Fonseca; Martins, J.; Herrera, C. Mora; Amarilo, K. Mota; Mundim, L.; Nogima, H.; Santoro, A.; Amaral, S. M.; Sznajder, A.; Thiel, M.; Da Silva De Araujo, F. Torres; Pereira, A. Vilela; Bernardes, C. A.; Calligaris, L.; Tomei, T. R.; Gregores, E. M.; Mercadante, P. G.; Novaes, S. F.; Padula, Sandra S.; Aleksandrov, A.; Antchev, G.; Hadjiiska, R.; Iaydjiev, P.; Misheva, M.; Rodozov, M.; Shopova, M.; Sultanov, G.; Dimitrov, A.; Ivanov, T.; Litov, L.; Pavlov, B.; Petkov, P.; Petrov, A.; Shumka, E.; Thakur, S.; Cheng, T.; Javaid, T.; Mittal, M.; Yuan, L.; Ahmad, M.; Bauer, G.; Hu, Z.; Lezki, S.; Yi, K.; Chen, G. M.; Chen, H. S.; Chen, M.; Iemmi, F.; Jiang, C. H.; Kapoor, A.; Kou, H.; Liao, H.; Liu, Z.-A.; Milosevic, V.; Monti, F.; Sharma, R.; Tao, J.; Thomas-Wilsker, J.; Wang, J.; Zhang, H.; Zhao, J.; Agapitos, A.; An, Y.; Ban, Y.; Chen, C.; Levin, A.; Li, C.; Li, Q.; Lyu, X.; Mao, Y.; Qian, S. J.; Sun, X.; Wang, D.; Xiao, J.; Yang, H.; Lu, M.; You, Z.; Gao, X.; Leggat, D.; Okawa, H.; Zhang, Y.; Lin, Z.; Lu, C.; Xiao, M.; Avila, C.; Trujillo, D. A.; Cabrera, A.; Florez, C.; Fraga, J.; Guisao, J. Mejia; Ramirez, F.; Rodriguez, M.; Alvarez, J. D.; Giljanovic, D.; Godinovic, N.; Lelas, D.; Puljak, I.; Antunovic, Z.; Kovac, M.; Sculac, T.; Brigljevic, V.; Chitroda, B. 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Zimermmane; Albrecht, A.; Albrecht, S.; Antonello, M.; Bein, S.; Benato, L.; Bonanomi, M.; Connor, P.; De Leo, K.; Eich, M.; Morabit, K. El; Feindt, F.; Fröhlich, A.; Garbers, C.; Garutti, E.; Hajheidari, M.; Haller, J.; Hinzmann, A.; Jabusch, H. R.; Kasieczka, G.; Keicher, P.; Klanner, R.; Korcari, W.; Kramer, T.; Kutzner, V.; Labe, F.; Lange, J.; Lobanov, A.; Matthies, C.; Mehta, A.; Moureaux, L.; Mrowietz, M.; Nigamova, A.; Nissan, Y.; Paasch, A.; Rodriguez, K. J.; Quadfasel, T.; Rieger, M.; Rieger, O.; Savoiu, D.; Schleper, P.; Schröder, M.; Schwandt, J.; Sommerhalder, M.; Stadie, H.; Steinbrück, G.; Tews, A.; Wolf, M.; Brommer, S.; Burkart, M.; Butz, E.; Caspart, R.; Chwalek, T.; Dierlamm, A.; Droll, A.; Faltermann, N.; Giffels, M.; Gosewisch, J. O.; Gottmann, A.; Hartmann, F.; Horzela, M.; Husemann, U.; Klute, M.; Koppenhöfer, R.; Maier, S.; Mitra, S.; Müller, Th.; Neukum, M.; Oh, M.; Quast, G.; Rabbertz, K.; Rauser, J.; Schnepf, M.; Seith, D.; Shvetsov, I.; Simonis, H. J.; Trevisani, N.; Ulrich, R.; Linden, J. van; Cube, R. F.; Wassmer, M.; Wieland, S.; Wolf, R.; Wozniewski, S.; Wunsch, S.; Zuo, X.; Anagnostou, G.; Assiouras, P.; Daskalakis, G.; Kyriakis, A.; Stakia, A.; Diamantopoulou, M.; Karasavvas, D.; Kontaxakis, P.; Manousakis-Katsikakis, A.; Panagiotou, A.; Papavergou, I.; Saoulidou, N.; Theofilatos, K.; Tziaferi, E.; Vellidis, K.; Zisopoulos, I.; Bakas, G.; Chatzistavrou, T.; Kousouris, K.; Papakrivopoulos, I.; Tsipolitis, G.; Zacharopoulou, A.; Adamidis, K.; Bestintzanos, I.; Evangelou, I.; Foudas, C.; Gianneios, P.; Kamtsikis, C.; Katsoulis, P.; Kokkas, P.; Kioseoglou, P. G.; Manthos, N.; Papadopoulos, I.; Strologas, J.; Csanád, M.; Farkas, K.; Gadallah, M. M.; Lökös, S.; Major, P.; Mandal, K.; Pásztor, G.; Rádl, A. J.; Surányi, O.; Veres, G. 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B.; Suryadevara, P.; Banerjee, S.; Chudasama, R.; Guchait, M.; Karmakar, S.; Kumar, S.; Majumder, G.; Mazumdar, K.; Mukherjee, S.; Thachayath, A.; Bahinipati, S.; Kar, C.; Mal, P.; Mishra, T.; Bindhu, V. K.; Nayak, A.; Saha, P.; Swain, S. K.; Vats, D.; Alpana, A.; Dube, S.; Kansal, B.; Laha, A.; Pandey, S.; Rastogi, A.; Sharma, S.; Bakhshiansohi, H.; Khazaie, E.; Zeinali, M.; Chenarani, S.; Etesami, S. M.; Khakzad, M.; Najafabadi, M. Mohammadi; Grunewald, M.; Abbrescia, M.; Aly, R.; Aruta, C.; Colaleo, A.; Creanza, D.; De Filippis, N.; De Palma, M.; Florio, A. Di; Elmetenawee, W.; Errico, F.; Fiore, L.; Iaselli, G.; Ince, M.; Maggi, G.; Maggi, M.; Margjeka, I.; Mastrapasqua, V.; My, S.; Nuzzo, S.; Pellecchia, A.; Pompili, A.; Pugliese, G.; Radogna, R.; Ramos, D.; Ranieri, A.; Selvaggi, G.; Silvestris, L.; Simone, F. 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F.; Vetens, W.; Afanasiev, S.; Andreev, V.; Andreev, Yu.; Aushev, T.; Azarkin, M.; Babaev, A.; Belyaev, A.; Blinov, V.; Boos, E.; Borshch, V.; Budkouski, D.; Bunichev, V.; Chekhovsky, V.; Chistov, R.; 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.; 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.; Levchenko, P.; Litomin, A.; Lychkovskaya, N.; Makarenko, V.; Malakhov, A.; Matveev, V.; Murzin, V.; Nikitenko, A.; Obraztsov, S.; Oskin, A.; Ovtin, I.; Palichik, V.; Parygin, P.; Perelygin, V.; Perfilov, M.; Petrushanko, S.; Polikarpov, S.; Popov, V.; Popova, E.; Radchenko, O.; Savina, M.; Savrin, V.; Selivanova, D.; Shalaev, V.; Shmatov, S.; Shulha, S.; Skovpen, Y.; Slabospitskii, S.; Smirnov, V.; Sosnov, D.; Sulimov, V.; Tcherniaev, E.; Terkulov, A.; Teryaev, O.; Tlisova, I.; Toms, M.; Toropin, A.; Uvarov, L.; Uzunian, A.; Vlasov, E.; Volkov, P.; 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:
- 7
- ISSN:
- 1434-6052
- Format(s):
- Medium: X
- Sponsoring Org:
- National Science Foundation
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Abstract The double differential cross sections of the Drell–Yan lepton pair (
$$\ell ^+\ell ^-$$ $$m_{\ell \ell }$$ $$p_{\textrm{T}} (\ell \ell )$$ $$\varphi ^{*}_{\eta }$$ $$\varphi ^{*}_{\eta }$$ $$p_{\textrm{T}} (\ell \ell )$$ $$p_{\textrm{T}} (\ell \ell )$$ $$\,\text {Te\hspace{-.08em}V}$$ $$m_{\ell \ell }$$ $$\,\text {fb}^{-1}$$ $$\,\text {Te\hspace{-.08em}V}$$ -
Sirunyan, A. M. ; Tumasyan, A. ; Adam, W. ; Ambrogi, F. ; Asilar, E. ; Bergauer, T. ; Brandstetter, J. ; Brondolin, E. ; Dragicevic, M. ; Erö, J. ; et al ( , The European Physical Journal C)Abstract The mass of the top quark is measured using a sample of $${{\text {t}}\overline{{\text {t}}}}$$ t t ¯ events collected by the CMS detector using proton-proton collisions at $$\sqrt{s}=13$$ s = 13 $$\,\text {TeV}$$ TeV at the CERN LHC. Events are selected with one isolated muon or electron and at least four jets from data corresponding to an integrated luminosity of 35.9 $$\,\text {fb}^{-1}$$ fb - 1 . For each event the mass is reconstructed from a kinematic fit of the decay products to a $${{\text {t}}\overline{{\text {t}}}}$$ t t ¯ hypothesis. Using the ideogram method, the top quark mass is determined simultaneously with an overall jet energy scale factor (JSF), constrained by the mass of the W boson in $${\text {q}} \overline{{\text {q}}} ^\prime $$ q q ¯ ′ decays. The measurement is calibrated on samples simulated at next-to-leading order matched to a leading-order parton shower. The top quark mass is found to be $$172.25 \pm 0.08\,\text {(stat+JSF)} \pm 0.62\,\text {(syst)} \,\text {GeV} $$ 172.25 ± 0.08 (stat+JSF) ± 0.62 (syst) GeV . The dependence of this result on the kinematic properties of the event is studied and compared to predictions of different models of $${{\text {t}}\overline{{\text {t}}}}$$ t t ¯ production, and no indications of a bias in the measurements are observed.more » « less
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Sirunyan, A. M. ; Tumasyan, A. ; Adam, W. ; Bergauer, T. ; Dragicevic, M. ; Erö, J. ; Valle, A. Escalante ; Frühwirth, R. ; Jeitler, M. ; Krammer, N. ; et al ( , The European Physical Journal C)null (Ed.)Abstract The rate for Higgs ( $${\mathrm{H}} $$ H ) bosons production in association with either one ( $${\mathrm{t}} {\mathrm{H}} $$ t H ) or two ( $${\mathrm{t}} {{\overline{{{\mathrm{t}}}}}} {\mathrm{H}} $$ t t ¯ H ) top quarks is measured in final states containing multiple electrons, muons, or tau leptons decaying to hadrons and a neutrino, using proton–proton collisions recorded at a center-of-mass energy of $$13\,\text {TeV} $$ 13 TeV by the CMS experiment. The analyzed data correspond to an integrated luminosity of 137 $$\,\text {fb}^{-1}$$ fb - 1 . The analysis is aimed at events that contain $${\mathrm{H}} \rightarrow {\mathrm{W}} {\mathrm{W}} $$ H → W W , $${\mathrm{H}} \rightarrow {\uptau } {\uptau } $$ H → τ τ , or $${\mathrm{H}} \rightarrow {\mathrm{Z}} {\mathrm{Z}} $$ H → Z Z decays and each of the top quark(s) decays either to lepton+jets or all-jet channels. Sensitivity to signal is maximized by including ten signatures in the analysis, depending on the lepton multiplicity. The separation among $${\mathrm{t}} {\mathrm{H}} $$ t H , $${\mathrm{t}} {{\overline{{{\mathrm{t}}}}}} {\mathrm{H}} $$ t t ¯ H , and the backgrounds is enhanced through machine-learning techniques and matrix-element methods. The measured production rates for the $${\mathrm{t}} {{\overline{{{\mathrm{t}}}}}} {\mathrm{H}} $$ t t ¯ H and $${\mathrm{t}} {\mathrm{H}} $$ t H signals correspond to $$0.92 \pm 0.19\,\text {(stat)} ^{+0.17}_{-0.13}\,\text {(syst)} $$ 0.92 ± 0.19 (stat) - 0.13 + 0.17 (syst) and $$5.7 \pm 2.7\,\text {(stat)} \pm 3.0\,\text {(syst)} $$ 5.7 ± 2.7 (stat) ± 3.0 (syst) of their respective standard model (SM) expectations. The corresponding observed (expected) significance amounts to 4.7 (5.2) standard deviations for $${\mathrm{t}} {{\overline{{{\mathrm{t}}}}}} {\mathrm{H}} $$ t t ¯ H , and to 1.4 (0.3) for $${\mathrm{t}} {\mathrm{H}} $$ t H production. Assuming that the Higgs boson coupling to the tau lepton is equal in strength to its expectation in the SM, the coupling $$y_{{\mathrm{t}}}$$ y t of the Higgs boson to the top quark divided by its SM expectation, $$\kappa _{{\mathrm{t}}}=y_{{\mathrm{t}}}/y_{{\mathrm{t}}}^{\mathrm {SM}}$$ κ t = y t / y t SM , is constrained to be within $$-0.9< \kappa _{{\mathrm{t}}}< -0.7$$ - 0.9 < κ t < - 0.7 or $$0.7< \kappa _{{\mathrm{t}}}< 1.1$$ 0.7 < κ t < 1.1 , at 95% confidence level. This result is the most sensitive measurement of the $${\mathrm{t}} {{\overline{{{\mathrm{t}}}}}} {\mathrm{H}} $$ t t ¯ H production rate to date.more » « less
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Cite: MLA FormatTumasyan, A., Adam, W., Andrejkovic, J. W., Bergauer, T., Chatterjee, S., Damanakis, K., Dragicevic, M., Valle, A. Escalante, Hussain, P. S., 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., Janssen, T., Kello, T., Sfar, H. Rejeb, Mechelen, P. Van, Bols, E. S., D’Hondt, J., De Moor, A., Delcourt, M., Faham, H. El, Lowette, S., Moortgat, S., Morton, A., Müller, D., Sahasransu, A. R., Tavernier, S., Doninck, W. Van, Vannerom, D., Clerbaux, B., De Lentdecker, G., Favart, L., Hohov, D., Jaramillo, J., Lee, K., Mahdavikhorrami, M., Makarenko, I., Malara, A., Paredes, S., Pétré, L., Postiau, N., Thomas, L., Bemden, M. Vanden, Velde, C. Vander, Vanlaer, P., Dobur, D., Knolle, J., Lambrecht, L., Mestdach, G., Niedziela, M., Rendón, C., Roskas, C., Samalan, A., Skovpen, K., Tytgat, M., Bossche, N. Van, Vermassen, B., Wezenbeek, L., Benecke, A., Bruno, G., Bury, F., Caputo, C., David, P., Delaere, C., Donertas, I. S., Giammanco, A., Jaffel, K., Jain, Sa., Lemaitre, V., Mondal, K., Taliercio, A., Tran, T. T., Vischia, P., Wertz, S., Alves, G. A., Coelho, E., Hensel, C., Moraes, A., Teles, P. Rebello, Júnior, W. L., Pereira, M. Alves, Filho, M. Barroso, Malbouisson, H. Brandao, Carvalho, W., Chinellato, J., Da Costa, E. M., Da Silveira, G. G., De Jesus Damiao, D., Sousa, V. Dos, De Souza, S. Fonseca, Martins, J., Herrera, C. Mora, Amarilo, K. Mota, Mundim, L., Nogima, H., Santoro, A., Amaral, S. M., Sznajder, A., Thiel, M., Da Silva De Araujo, F. Torres, Pereira, A. Vilela, Bernardes, C. A., Calligaris, L., Tomei, T. R., Gregores, E. M., Mercadante, P. G., Novaes, S. 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S., Zarubin, A., Zhizhin, I., and Zhokin, A. "Measurement of the differential $$\hbox {t}\overline{\hbox {t}}$$ production cross section as a function of the jet mass and extraction of the top quark mass in hadronic decays of boosted top quarks". The European Physical Journal C 83 (7). Country unknown/Code not available. https://doi.org/10.1140/epjc/s10052-023-11587-8. https://par.nsf.gov/biblio/10463776.
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place = {Country unknown/Code not available}, title = {Measurement of the differential $$\hbox {t}\overline{\hbox {t}}$$ production cross section as a function of the jet mass and extraction of the top quark mass in hadronic decays of boosted top quarks}, url = {https://par.nsf.gov/biblio/10463776}, DOI = {10.1140/epjc/s10052-023-11587-8}, abstractNote = {Abstract A measurement of the jet mass distribution in hadronic decays of Lorentz-boosted top quarks is presented. The measurement is performed in the lepton + jets channel of top quark pair production ( $$\hbox {t}\overline{\hbox {t}}$$ t t ¯ ) events, where the lepton is an electron or muon. The products of the hadronic top quark decay are reconstructed using a single large-radius jet with transverse momentum greater than 400 $$\,\text {Ge}\hspace{-.08em}\text {V}$$ Ge V . The data were collected with the CMS detector at the LHC in proton-proton collisions and correspond to an integrated luminosity of 138 $$\,\text {fb}^{-1}$$ fb - 1 . The differential $$\hbox {t}\overline{\hbox {t}}$$ t t ¯ production cross section as a function of the jet mass is unfolded to the particle level and is used to extract the top quark mass. The jet mass scale is calibrated using the hadronic W boson decay within the large-radius jet. The uncertainties in the modelling of the final state radiation are reduced by studying angular correlations in the jet substructure. These developments lead to a significant increase in precision, and a top quark mass of $$173.06 \pm 0.84\,\text {Ge}\hspace{-.08em}\text {V} $$ 173.06 ± 0.84 Ge V .}, journal = {The European Physical Journal C}, volume = {83}, number = {7}, 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. Escalante and Hussain, P. 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