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Search for the production of four top quarks in the single-lepton and opposite-sign dilepton final states in proton-proton collisions at s = 13 TeV

A bstract A search for the standard model production of four top quarks (pp → t t ¯ t t ¯ ) is reported using single-lepton plus jets and opposite-sign dilepton plus jets signatures. Proton-proton collisions are recorded with the CMS detector at the LHC at a center-of-mass energy of 13 TeV in a samp...

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Published in:The journal of high energy physics 2019-11, Vol.2019 (11), p.1-53
Main Authors: Ambrogi, F., Tavernier, S., Van Parijs, I., Beghin, D., Dorney, B., Roskas, C., Alves, G. A., Shopova, M., Avila, C., Roguljic, M., Starodumov, A., Savoy-Navarro, A., Sordini, V., Sert, H., Asmuss, P., Kasemann, M., Reimers, A., Kudella, S., Katsoulis, P., Keshri, S., Bhardwaj, R., Rout, P. K., Kapoor, A., Fiore, L., Ince, M., Iemmi, F., Viliani, L., Tosi, M., Montagna, P., Vai, I., Vitulo, P., Spiga, D., Del Re, D., Mariotti, C., Pastrone, N., Casarsa, M., Jeon, D., Carrillo Moreno, S., Bunkowski, K., Seixas, J., Toms, M., Vlasov, E., Dremin, I., Boos, E., Blinov, V., Devetak, D., Carrillo Montoya, C. A., Fouz, M. C., Puerta Pelayo, J., Scodellaro, L., Deiters, K., Erdmann, W., Amsler, C., Seitz, C., Guler, EmineGurpinar, Ozturk, S., Heath, H. F., Buchmuller, O., Dauncey, P., Narain, M., Funk, G., Pilot, J., Nash, W. A., Valuev, V., Wimpenny, S., Campagnari, C., Anderson, D., Dutta, I., Andrews, M. B., Mudholkar, T., Sun, M., Banerjee, S., Duarte, J., Gecse, Z., Hasegawa, S., Pena, C., Field, R. D., Tonjes, M. B., Dilsiz, K., Onel, Y., Snyder, C., Feng, L., Mitchell, T., Baty, A., Hsu, D., Fangmeier, C., Gonzalez Suarez, R., Snow, G. R., Nguyen, D., Bucci, R., Flowers, S., Wang, F., Rorie, J., Chiarito, B., De Guio, F., Mengke, T., Undleeb, S., Janjam, R., Johns, W., Dodd, L.
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container_end_page 53
container_issue 11
container_start_page 1
container_title The journal of high energy physics
container_volume 2019
creator Ambrogi, F.
Tavernier, S.
Van Parijs, I.
Beghin, D.
Dorney, B.
Roskas, C.
Alves, G. A.
Shopova, M.
Avila, C.
Roguljic, M.
Starodumov, A.
Savoy-Navarro, A.
Sordini, V.
Sert, H.
Asmuss, P.
Kasemann, M.
Reimers, A.
Kudella, S.
Katsoulis, P.
Keshri, S.
Bhardwaj, R.
Rout, P. K.
Kapoor, A.
Fiore, L.
Ince, M.
Iemmi, F.
Viliani, L.
Tosi, M.
Montagna, P.
Vai, I.
Vitulo, P.
Spiga, D.
Del Re, D.
Mariotti, C.
Pastrone, N.
Casarsa, M.
Jeon, D.
Carrillo Moreno, S.
Bunkowski, K.
Seixas, J.
Toms, M.
Vlasov, E.
Dremin, I.
Boos, E.
Blinov, V.
Devetak, D.
Carrillo Montoya, C. A.
Fouz, M. C.
Puerta Pelayo, J.
Scodellaro, L.
Deiters, K.
Erdmann, W.
Amsler, C.
Seitz, C.
Guler, EmineGurpinar
Ozturk, S.
Heath, H. F.
Buchmuller, O.
Dauncey, P.
Narain, M.
Funk, G.
Pilot, J.
Nash, W. A.
Valuev, V.
Wimpenny, S.
Campagnari, C.
Anderson, D.
Dutta, I.
Andrews, M. B.
Mudholkar, T.
Sun, M.
Banerjee, S.
Duarte, J.
Gecse, Z.
Hasegawa, S.
Pena, C.
Field, R. D.
Tonjes, M. B.
Dilsiz, K.
Onel, Y.
Snyder, C.
Feng, L.
Mitchell, T.
Baty, A.
Hsu, D.
Fangmeier, C.
Gonzalez Suarez, R.
Snow, G. R.
Nguyen, D.
Bucci, R.
Flowers, S.
Wang, F.
Rorie, J.
Chiarito, B.
De Guio, F.
Mengke, T.
Undleeb, S.
Janjam, R.
Johns, W.
Dodd, L.
description A bstract A search for the standard model production of four top quarks (pp → t t ¯ t t ¯ ) is reported using single-lepton plus jets and opposite-sign dilepton plus jets signatures. Proton-proton collisions are recorded with the CMS detector at the LHC at a center-of-mass energy of 13 TeV in a sample corresponding to an integrated luminosity of 35.8 fb − 1 . A multivariate analysis exploiting global event and jet properties is used to discriminate t t ¯ t t ¯ from t t ¯ production. No significant deviation is observed from the predicted background. An upper limit is set on the cross section for t t ¯ t t ¯ production in the standard model of 48 fb at 95% confidence level. When combined with a previous measurement by the CMS experiment from an analysis of other final states, the observed signal significance is 1.4 standard deviations, and the combined cross section measurement is 13 − 9 + 11 fb. The result is also interpreted in the framework of effective field theory.
doi_str_mv 10.1007/JHEP11(2019)082
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Proton-proton collisions are recorded with the CMS detector at the LHC at a center-of-mass energy of 13 TeV in a sample corresponding to an integrated luminosity of 35.8 fb − 1 . A multivariate analysis exploiting global event and jet properties is used to discriminate t t ¯ t t ¯ from t t ¯ production. No significant deviation is observed from the predicted background. An upper limit is set on the cross section for t t ¯ t t ¯ production in the standard model of 48 fb at 95% confidence level. When combined with a previous measurement by the CMS experiment from an analysis of other final states, the observed signal significance is 1.4 standard deviations, and the combined cross section measurement is 13 − 9 + 11 fb. 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All Rights Reserved.</rights><rights>The Author(s) 2019. This work is published under http://creativecommons.org/licenses/by/4.0/ (the “License”). 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R.</creatorcontrib><creatorcontrib>Nguyen, D.</creatorcontrib><creatorcontrib>Bucci, R.</creatorcontrib><creatorcontrib>Flowers, S.</creatorcontrib><creatorcontrib>Wang, F.</creatorcontrib><creatorcontrib>Rorie, J.</creatorcontrib><creatorcontrib>Chiarito, B.</creatorcontrib><creatorcontrib>De Guio, F.</creatorcontrib><creatorcontrib>Mengke, T.</creatorcontrib><creatorcontrib>Undleeb, S.</creatorcontrib><creatorcontrib>Janjam, R.</creatorcontrib><creatorcontrib>Johns, W.</creatorcontrib><creatorcontrib>Dodd, L.</creatorcontrib><title>Search for the production of four top quarks in the single-lepton and opposite-sign dilepton final states in proton-proton collisions at s = 13 TeV</title><title>The journal of high energy physics</title><addtitle>J. High Energ. Phys</addtitle><description>A bstract A search for the standard model production of four top quarks (pp → t t ¯ t t ¯ ) is reported using single-lepton plus jets and opposite-sign dilepton plus jets signatures. Proton-proton collisions are recorded with the CMS detector at the LHC at a center-of-mass energy of 13 TeV in a sample corresponding to an integrated luminosity of 35.8 fb − 1 . A multivariate analysis exploiting global event and jet properties is used to discriminate t t ¯ t t ¯ from t t ¯ production. No significant deviation is observed from the predicted background. An upper limit is set on the cross section for t t ¯ t t ¯ production in the standard model of 48 fb at 95% confidence level. When combined with a previous measurement by the CMS experiment from an analysis of other final states, the observed signal significance is 1.4 standard deviations, and the combined cross section measurement is 13 − 9 + 11 fb. The result is also interpreted in the framework of effective field theory.</description><subject>Classical and Quantum Gravitation</subject><subject>Collaboration</subject><subject>Collisions</subject><subject>Confidence intervals</subject><subject>Cross-sections</subject><subject>Elementary Particles</subject><subject>Field theory</subject><subject>High energy physics</subject><subject>Large Hadron Collider</subject><subject>Leptons</subject><subject>Luminosity</subject><subject>Multivariate analysis</subject><subject>Particle collisions</subject><subject>Physics</subject><subject>Physics and Astronomy</subject><subject>Protons</subject><subject>Quantum Field Theories</subject><subject>Quantum Field Theory</subject><subject>Quantum Physics</subject><subject>Quarks</subject><subject>Regular Article - Experimental Physics</subject><subject>Relativity Theory</subject><subject>Sensors</subject><subject>Simulation</subject><subject>Solenoids</subject><subject>String Theory</subject><issn>1029-8479</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2019</creationdate><recordtype>article</recordtype><sourceid>PIMPY</sourceid><recordid>eNp9kT1PwzAQhi0kJEphZrXEAkPg_JEPDwyoKhRUCSQKa-Q4dusSxWns_BL-MG5TiY3ppPce372-F6ErAncEIL9_XczfCbmhQMQtFPQETQhQkRQ8F2fo3PstAEmJgAn6-dCyVxtsXI_DRuOud_WggnUtdiaqQ5Rdh3eD7L89tu0B8rZdNzppdBciJ9sau65z3gadeLtucW2PLWNb2WAfZNCHx3F6lJOxYOWaxvq4ymMZsMcPmDC80l8X6NTIxuvLY52iz6f5arZIlm_PL7PHZdKRLKcJUSpPmckrroQRRBU1U5QzUUGqQfGsIIKqSlRSpfEGstaMU5YarXgOuQTDpuh6nBv97AbtQ7mN_42OfUkLXvAsE0X6L8UohVQQTiIFI-W7Pl5H938UgXIfSjmGUu5DKaMh9gt1GoIx</recordid><startdate>20191101</startdate><enddate>20191101</enddate><creator>Ambrogi, F.</creator><creator>Tavernier, S.</creator><creator>Van Parijs, I.</creator><creator>Beghin, D.</creator><creator>Dorney, B.</creator><creator>Roskas, C.</creator><creator>Alves, G. 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A. ; Shopova, M. ; Avila, C. ; Roguljic, M. ; Starodumov, A. ; Savoy-Navarro, A. ; Sordini, V. ; Sert, H. ; Asmuss, P. ; Kasemann, M. ; Reimers, A. ; Kudella, S. ; Katsoulis, P. ; Keshri, S. ; Bhardwaj, R. ; Rout, P. K. ; Kapoor, A. ; Fiore, L. ; Ince, M. ; Iemmi, F. ; Viliani, L. ; Tosi, M. ; Montagna, P. ; Vai, I. ; Vitulo, P. ; Spiga, D. ; Del Re, D. ; Mariotti, C. ; Pastrone, N. ; Casarsa, M. ; Jeon, D. ; Carrillo Moreno, S. ; Bunkowski, K. ; Seixas, J. ; Toms, M. ; Vlasov, E. ; Dremin, I. ; Boos, E. ; Blinov, V. ; Devetak, D. ; Carrillo Montoya, C. A. ; Fouz, M. C. ; Puerta Pelayo, J. ; Scodellaro, L. ; Deiters, K. ; Erdmann, W. ; Amsler, C. ; Seitz, C. ; Guler, EmineGurpinar ; Ozturk, S. ; Heath, H. F. ; Buchmuller, O. ; Dauncey, P. ; Narain, M. ; Funk, G. ; Pilot, J. ; Nash, W. A. ; Valuev, V. ; Wimpenny, S. ; Campagnari, C. ; Anderson, D. ; Dutta, I. ; Andrews, M. B. ; Mudholkar, T. ; Sun, M. ; Banerjee, S. ; Duarte, J. ; Gecse, Z. ; Hasegawa, S. ; Pena, C. ; Field, R. D. ; Tonjes, M. B. ; Dilsiz, K. ; Onel, Y. ; Snyder, C. ; Feng, L. ; Mitchell, T. ; Baty, A. ; Hsu, D. ; Fangmeier, C. ; Gonzalez Suarez, R. ; Snow, G. R. ; Nguyen, D. ; Bucci, R. ; Flowers, S. ; Wang, F. ; Rorie, J. ; Chiarito, B. ; De Guio, F. ; Mengke, T. ; Undleeb, S. ; Janjam, R. ; Johns, W. ; Dodd, L.</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-p1672-1cc753f7b4c9f91c8d3c2439b05e0c468192cb9bac5082ade34235fec4707a0f3</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2019</creationdate><topic>Classical and Quantum Gravitation</topic><topic>Collaboration</topic><topic>Collisions</topic><topic>Confidence intervals</topic><topic>Cross-sections</topic><topic>Elementary Particles</topic><topic>Field theory</topic><topic>High energy physics</topic><topic>Large Hadron Collider</topic><topic>Leptons</topic><topic>Luminosity</topic><topic>Multivariate analysis</topic><topic>Particle collisions</topic><topic>Physics</topic><topic>Physics and Astronomy</topic><topic>Protons</topic><topic>Quantum Field Theories</topic><topic>Quantum Field Theory</topic><topic>Quantum Physics</topic><topic>Quarks</topic><topic>Regular Article - Experimental Physics</topic><topic>Relativity Theory</topic><topic>Sensors</topic><topic>Simulation</topic><topic>Solenoids</topic><topic>String Theory</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Ambrogi, F.</creatorcontrib><creatorcontrib>Tavernier, S.</creatorcontrib><creatorcontrib>Van Parijs, I.</creatorcontrib><creatorcontrib>Beghin, D.</creatorcontrib><creatorcontrib>Dorney, B.</creatorcontrib><creatorcontrib>Roskas, C.</creatorcontrib><creatorcontrib>Alves, G. 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A.</au><au>Shopova, M.</au><au>Avila, C.</au><au>Roguljic, M.</au><au>Starodumov, A.</au><au>Savoy-Navarro, A.</au><au>Sordini, V.</au><au>Sert, H.</au><au>Asmuss, P.</au><au>Kasemann, M.</au><au>Reimers, A.</au><au>Kudella, S.</au><au>Katsoulis, P.</au><au>Keshri, S.</au><au>Bhardwaj, R.</au><au>Rout, P. K.</au><au>Kapoor, A.</au><au>Fiore, L.</au><au>Ince, M.</au><au>Iemmi, F.</au><au>Viliani, L.</au><au>Tosi, M.</au><au>Montagna, P.</au><au>Vai, I.</au><au>Vitulo, P.</au><au>Spiga, D.</au><au>Del Re, D.</au><au>Mariotti, C.</au><au>Pastrone, N.</au><au>Casarsa, M.</au><au>Jeon, D.</au><au>Carrillo Moreno, S.</au><au>Bunkowski, K.</au><au>Seixas, J.</au><au>Toms, M.</au><au>Vlasov, E.</au><au>Dremin, I.</au><au>Boos, E.</au><au>Blinov, V.</au><au>Devetak, D.</au><au>Carrillo Montoya, C. A.</au><au>Fouz, M. C.</au><au>Puerta Pelayo, J.</au><au>Scodellaro, L.</au><au>Deiters, K.</au><au>Erdmann, W.</au><au>Amsler, C.</au><au>Seitz, C.</au><au>Guler, EmineGurpinar</au><au>Ozturk, S.</au><au>Heath, H. F.</au><au>Buchmuller, O.</au><au>Dauncey, P.</au><au>Narain, M.</au><au>Funk, G.</au><au>Pilot, J.</au><au>Nash, W. A.</au><au>Valuev, V.</au><au>Wimpenny, S.</au><au>Campagnari, C.</au><au>Anderson, D.</au><au>Dutta, I.</au><au>Andrews, M. B.</au><au>Mudholkar, T.</au><au>Sun, M.</au><au>Banerjee, S.</au><au>Duarte, J.</au><au>Gecse, Z.</au><au>Hasegawa, S.</au><au>Pena, C.</au><au>Field, R. D.</au><au>Tonjes, M. B.</au><au>Dilsiz, K.</au><au>Onel, Y.</au><au>Snyder, C.</au><au>Feng, L.</au><au>Mitchell, T.</au><au>Baty, A.</au><au>Hsu, D.</au><au>Fangmeier, C.</au><au>Gonzalez Suarez, R.</au><au>Snow, G. R.</au><au>Nguyen, D.</au><au>Bucci, R.</au><au>Flowers, S.</au><au>Wang, F.</au><au>Rorie, J.</au><au>Chiarito, B.</au><au>De Guio, F.</au><au>Mengke, T.</au><au>Undleeb, S.</au><au>Janjam, R.</au><au>Johns, W.</au><au>Dodd, L.</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Search for the production of four top quarks in the single-lepton and opposite-sign dilepton final states in proton-proton collisions at s = 13 TeV</atitle><jtitle>The journal of high energy physics</jtitle><stitle>J. High Energ. Phys</stitle><date>2019-11-01</date><risdate>2019</risdate><volume>2019</volume><issue>11</issue><spage>1</spage><epage>53</epage><pages>1-53</pages><eissn>1029-8479</eissn><abstract>A bstract A search for the standard model production of four top quarks (pp → t t ¯ t t ¯ ) is reported using single-lepton plus jets and opposite-sign dilepton plus jets signatures. Proton-proton collisions are recorded with the CMS detector at the LHC at a center-of-mass energy of 13 TeV in a sample corresponding to an integrated luminosity of 35.8 fb − 1 . A multivariate analysis exploiting global event and jet properties is used to discriminate t t ¯ t t ¯ from t t ¯ production. No significant deviation is observed from the predicted background. An upper limit is set on the cross section for t t ¯ t t ¯ production in the standard model of 48 fb at 95% confidence level. When combined with a previous measurement by the CMS experiment from an analysis of other final states, the observed signal significance is 1.4 standard deviations, and the combined cross section measurement is 13 − 9 + 11 fb. The result is also interpreted in the framework of effective field theory.</abstract><cop>Berlin/Heidelberg</cop><pub>Springer Berlin Heidelberg</pub><doi>10.1007/JHEP11(2019)082</doi><tpages>53</tpages><oa>free_for_read</oa></addata></record>
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source Publicly Available Content Database; Springer Nature - SpringerLink Journals - Fully Open Access
subjects Classical and Quantum Gravitation
Collaboration
Collisions
Confidence intervals
Cross-sections
Elementary Particles
Field theory
High energy physics
Large Hadron Collider
Leptons
Luminosity
Multivariate analysis
Particle collisions
Physics
Physics and Astronomy
Protons
Quantum Field Theories
Quantum Field Theory
Quantum Physics
Quarks
Regular Article - Experimental Physics
Relativity Theory
Sensors
Simulation
Solenoids
String Theory
title Search for the production of four top quarks in the single-lepton and opposite-sign dilepton final states in proton-proton collisions at s = 13 TeV
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