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Search for single production of vector-like quarks decaying into Wb in pp collisions at \documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$\sqrt{s} = 8$$\end{document}s=8 TeV with the ATLAS detector

A search for singly produced vector-like Q quarks, where Q can be either a T quark with charge \documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{...

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Published in:The European physical journal. C, Particles and fields Particles and fields, 2016-01, Vol.76 (8)
Main Authors: Aad, G., Abbott, B., Abdallah, J., Abdinov, O., Abeloos, B., Aben, R., Abolins, M., AbouZeid, O. S., Abramowicz, H., Abreu, H., Abreu, R., Abulaiti, Y., Acharya, B. S., Adamczyk, L., Adams, D. L., Adelman, J., Adomeit, S., Adye, T., Affolder, A. A., Agatonovic-Jovin, T., Agricola, J., Aguilar-Saavedra, J. A., Ahlen, S. P., Ahmadov, F., Aielli, G., Akerstedt, H., Åkesson, T. P. A., Akimov, A. V., Alberghi, G. L., Albert, J., Albrand, S., Verzini, M. J. Alconada, Aleksa, M., Aleksandrov, I. N., Alexa, C., Alexander, G., Alexopoulos, T., Alhroob, M., Alimonti, G., Alio, L., Alison, J., Alkire, S. P., Allbrooke, B. M. M., Allen, B. W., Allport, P. P., Aloisio, A., Alonso, A., Alonso, F., Alpigiani, C., Gonzalez, B. Alvarez, Piqueras, D. Álvarez, Alviggi, M. G., Amadio, B. T., Amako, K., Coutinho, Y. Amaral, Amelung, C., Amidei, D., Santos, S. P. Amor Dos, Amorim, A., Amoroso, S., Amram, N., Amundsen, G., Anastopoulos, C., Ancu, L. S., Andari, N., Andeen, T., Anders, C. F., Anders, G., Anders, J. K., Anderson, K. J., Andreazza, A., Andrei, V., Angelidakis, S., Angelozzi, I., Anger, P., Angerami, A., Anghinolfi, F., Anisenkov, A. V., Anjos, N., Annovi, A., Antonelli, M., Antonov, A., Antos, J., Anulli, F., Aoki, M., Bella, L. Aperio, Arabidze, G., Arai, Y., Araque, J. P., Arce, A. T. H., Arduh, F. A., Arguin, J-F., Argyropoulos, S., Arik, M., Armbruster, A. J., Arnaez, O., Arnold, H., Arratia, M., Arslan, O., Artamonov, A.
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container_title The European physical journal. C, Particles and fields
container_volume 76
creator Aad, G.
Abbott, B.
Abdallah, J.
Abdinov, O.
Abeloos, B.
Aben, R.
Abolins, M.
AbouZeid, O. S.
Abramowicz, H.
Abreu, H.
Abreu, R.
Abulaiti, Y.
Acharya, B. S.
Adamczyk, L.
Adams, D. L.
Adelman, J.
Adomeit, S.
Adye, T.
Affolder, A. A.
Agatonovic-Jovin, T.
Agricola, J.
Aguilar-Saavedra, J. A.
Ahlen, S. P.
Ahmadov, F.
Aielli, G.
Akerstedt, H.
Åkesson, T. P. A.
Akimov, A. V.
Alberghi, G. L.
Albert, J.
Albrand, S.
Verzini, M. J. Alconada
Aleksa, M.
Aleksandrov, I. N.
Alexa, C.
Alexander, G.
Alexopoulos, T.
Alhroob, M.
Alimonti, G.
Alio, L.
Alison, J.
Alkire, S. P.
Allbrooke, B. M. M.
Allen, B. W.
Allport, P. P.
Aloisio, A.
Alonso, A.
Alonso, F.
Alpigiani, C.
Gonzalez, B. Alvarez
Piqueras, D. Álvarez
Alviggi, M. G.
Amadio, B. T.
Amako, K.
Coutinho, Y. Amaral
Amelung, C.
Amidei, D.
Santos, S. P. Amor Dos
Amorim, A.
Amoroso, S.
Amram, N.
Amundsen, G.
Anastopoulos, C.
Ancu, L. S.
Andari, N.
Andeen, T.
Anders, C. F.
Anders, G.
Anders, J. K.
Anderson, K. J.
Andreazza, A.
Andrei, V.
Angelidakis, S.
Angelozzi, I.
Anger, P.
Angerami, A.
Anghinolfi, F.
Anisenkov, A. V.
Anjos, N.
Annovi, A.
Antonelli, M.
Antonov, A.
Antos, J.
Anulli, F.
Aoki, M.
Bella, L. Aperio
Arabidze, G.
Arai, Y.
Araque, J. P.
Arce, A. T. H.
Arduh, F. A.
Arguin, J-F.
Argyropoulos, S.
Arik, M.
Armbruster, A. J.
Arnaez, O.
Arnold, H.
Arratia, M.
Arslan, O.
Artamonov, A.
description A search for singly produced vector-like Q quarks, where Q can be either a T quark with charge \documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$+2/3$$\end{document} + 2 / 3 or a Y quark with charge \documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$-4/3$$\end{document} - 4 / 3 , is performed in proton–proton collisions recorded with the ATLAS detector at the LHC. The dataset corresponds to an integrated luminosity of 20.3 fb \documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$^{-1}$$\end{document} - 1 and was produced with a centre-of-mass energy of \documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$\sqrt{s}=8$$\end{document} s = 8  TeV. This analysis targets \documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$Q \rightarrow Wb$$\end{document} Q → W b decays where the W boson decays leptonically. A veto on massive large-radius jets is used to reject the dominant \documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$t\bar{t}$$\end{document} t t ¯ background. The reconstructed Q -candidate mass, ranging from 0.4 to 1.2 TeV, is used in the search to discriminate signal from background processes. No significant deviation from the Standard Model expectation is observed, and limits are set on the \documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{d
doi_str_mv 10.1140/epjc/s10052-016-4281-8
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S. ; Abramowicz, H. ; Abreu, H. ; Abreu, R. ; Abulaiti, Y. ; Acharya, B. S. ; Adamczyk, L. ; Adams, D. L. ; Adelman, J. ; Adomeit, S. ; Adye, T. ; Affolder, A. A. ; Agatonovic-Jovin, T. ; Agricola, J. ; Aguilar-Saavedra, J. A. ; Ahlen, S. P. ; Ahmadov, F. ; Aielli, G. ; Akerstedt, H. ; Åkesson, T. P. A. ; Akimov, A. V. ; Alberghi, G. L. ; Albert, J. ; Albrand, S. ; Verzini, M. J. Alconada ; Aleksa, M. ; Aleksandrov, I. N. ; Alexa, C. ; Alexander, G. ; Alexopoulos, T. ; Alhroob, M. ; Alimonti, G. ; Alio, L. ; Alison, J. ; Alkire, S. P. ; Allbrooke, B. M. M. ; Allen, B. W. ; Allport, P. P. ; Aloisio, A. ; Alonso, A. ; Alonso, F. ; Alpigiani, C. ; Gonzalez, B. Alvarez ; Piqueras, D. Álvarez ; Alviggi, M. G. ; Amadio, B. T. ; Amako, K. ; Coutinho, Y. Amaral ; Amelung, C. ; Amidei, D. ; Santos, S. P. Amor Dos ; Amorim, A. ; Amoroso, S. ; Amram, N. ; Amundsen, G. ; Anastopoulos, C. ; Ancu, L. S. ; Andari, N. ; Andeen, T. ; Anders, C. F. ; Anders, G. ; Anders, J. K. ; Anderson, K. J. ; Andreazza, A. ; Andrei, V. ; Angelidakis, S. ; Angelozzi, I. ; Anger, P. ; Angerami, A. ; Anghinolfi, F. ; Anisenkov, A. V. ; Anjos, N. ; Annovi, A. ; Antonelli, M. ; Antonov, A. ; Antos, J. ; Anulli, F. ; Aoki, M. ; Bella, L. Aperio ; Arabidze, G. ; Arai, Y. ; Araque, J. P. ; Arce, A. T. H. ; Arduh, F. A. ; Arguin, J-F. ; Argyropoulos, S. ; Arik, M. ; Armbruster, A. J. ; Arnaez, O. ; Arnold, H. ; Arratia, M. ; Arslan, O. ; Artamonov, A.</creator><creatorcontrib>Aad, G. ; Abbott, B. ; Abdallah, J. ; Abdinov, O. ; Abeloos, B. ; Aben, R. ; Abolins, M. ; AbouZeid, O. S. ; Abramowicz, H. ; Abreu, H. ; Abreu, R. ; Abulaiti, Y. ; Acharya, B. S. ; Adamczyk, L. ; Adams, D. L. ; Adelman, J. ; Adomeit, S. ; Adye, T. ; Affolder, A. A. ; Agatonovic-Jovin, T. ; Agricola, J. ; Aguilar-Saavedra, J. A. ; Ahlen, S. P. ; Ahmadov, F. ; Aielli, G. ; Akerstedt, H. ; Åkesson, T. P. A. ; Akimov, A. V. ; Alberghi, G. L. ; Albert, J. ; Albrand, S. ; Verzini, M. J. Alconada ; Aleksa, M. ; Aleksandrov, I. N. ; Alexa, C. ; Alexander, G. ; Alexopoulos, T. ; Alhroob, M. ; Alimonti, G. ; Alio, L. ; Alison, J. ; Alkire, S. P. ; Allbrooke, B. M. M. ; Allen, B. W. ; Allport, P. P. ; Aloisio, A. ; Alonso, A. ; Alonso, F. ; Alpigiani, C. ; Gonzalez, B. Alvarez ; Piqueras, D. Álvarez ; Alviggi, M. G. ; Amadio, B. T. ; Amako, K. ; Coutinho, Y. Amaral ; Amelung, C. ; Amidei, D. ; Santos, S. P. Amor Dos ; Amorim, A. ; Amoroso, S. ; Amram, N. ; Amundsen, G. ; Anastopoulos, C. ; Ancu, L. S. ; Andari, N. ; Andeen, T. ; Anders, C. F. ; Anders, G. ; Anders, J. K. ; Anderson, K. J. ; Andreazza, A. ; Andrei, V. ; Angelidakis, S. ; Angelozzi, I. ; Anger, P. ; Angerami, A. ; Anghinolfi, F. ; Anisenkov, A. V. ; Anjos, N. ; Annovi, A. ; Antonelli, M. ; Antonov, A. ; Antos, J. ; Anulli, F. ; Aoki, M. ; Bella, L. Aperio ; Arabidze, G. ; Arai, Y. ; Araque, J. P. ; Arce, A. T. H. ; Arduh, F. A. ; Arguin, J-F. ; Argyropoulos, S. ; Arik, M. ; Armbruster, A. J. ; Arnaez, O. ; Arnold, H. ; Arratia, M. ; Arslan, O. ; Artamonov, A.</creatorcontrib><description>A search for singly produced vector-like Q quarks, where Q can be either a T quark with charge \documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$+2/3$$\end{document} + 2 / 3 or a Y quark with charge \documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$-4/3$$\end{document} - 4 / 3 , is performed in proton–proton collisions recorded with the ATLAS detector at the LHC. The dataset corresponds to an integrated luminosity of 20.3 fb \documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$^{-1}$$\end{document} - 1 and was produced with a centre-of-mass energy of \documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$\sqrt{s}=8$$\end{document} s = 8  TeV. This analysis targets \documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$Q \rightarrow Wb$$\end{document} Q → W b decays where the W boson decays leptonically. A veto on massive large-radius jets is used to reject the dominant \documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$t\bar{t}$$\end{document} t t ¯ background. The reconstructed Q -candidate mass, ranging from 0.4 to 1.2 TeV, is used in the search to discriminate signal from background processes. No significant deviation from the Standard Model expectation is observed, and limits are set on the \documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$Q \rightarrow Wb$$\end{document} Q → W b cross-section times branching ratio. The results are also interpreted as limits on the QWb coupling and the mixing with the Standard Model sector for a singlet T quark or a Y quark from a doublet. T quarks with masses below 0.95 TeV are excluded at 95 % confidence level, assuming a unit coupling and a BR \documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$(T\rightarrow Wb) = 0.5$$\end{document} ( T → W b ) = 0.5 , whereas the expected limit is 1.10 TeV.</description><identifier>ISSN: 1434-6044</identifier><identifier>EISSN: 1434-6052</identifier><identifier>DOI: 10.1140/epjc/s10052-016-4281-8</identifier><identifier>PMID: 28303082</identifier><language>eng</language><publisher>Berlin/Heidelberg: Springer Berlin Heidelberg</publisher><subject>Regular - Experimental Physics</subject><ispartof>The European physical journal. 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A.</creatorcontrib><creatorcontrib>Arguin, J-F.</creatorcontrib><creatorcontrib>Argyropoulos, S.</creatorcontrib><creatorcontrib>Arik, M.</creatorcontrib><creatorcontrib>Armbruster, A. J.</creatorcontrib><creatorcontrib>Arnaez, O.</creatorcontrib><creatorcontrib>Arnold, H.</creatorcontrib><creatorcontrib>Arratia, M.</creatorcontrib><creatorcontrib>Arslan, O.</creatorcontrib><creatorcontrib>Artamonov, A.</creatorcontrib><title>Search for single production of vector-like quarks decaying into Wb in pp collisions at \documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$\sqrt{s} = 8$$\end{document}s=8 TeV with the ATLAS detector</title><title>The European physical journal. C, Particles and fields</title><description>A search for singly produced vector-like Q quarks, where Q can be either a T quark with charge \documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$+2/3$$\end{document} + 2 / 3 or a Y quark with charge \documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$-4/3$$\end{document} - 4 / 3 , is performed in proton–proton collisions recorded with the ATLAS detector at the LHC. The dataset corresponds to an integrated luminosity of 20.3 fb \documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$^{-1}$$\end{document} - 1 and was produced with a centre-of-mass energy of \documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$\sqrt{s}=8$$\end{document} s = 8  TeV. This analysis targets \documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$Q \rightarrow Wb$$\end{document} Q → W b decays where the W boson decays leptonically. A veto on massive large-radius jets is used to reject the dominant \documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$t\bar{t}$$\end{document} t t ¯ background. The reconstructed Q -candidate mass, ranging from 0.4 to 1.2 TeV, is used in the search to discriminate signal from background processes. No significant deviation from the Standard Model expectation is observed, and limits are set on the \documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$Q \rightarrow Wb$$\end{document} Q → W b cross-section times branching ratio. The results are also interpreted as limits on the QWb coupling and the mixing with the Standard Model sector for a singlet T quark or a Y quark from a doublet. T quarks with masses below 0.95 TeV are excluded at 95 % confidence level, assuming a unit coupling and a BR \documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$(T\rightarrow Wb) = 0.5$$\end{document} ( T → W b ) = 0.5 , whereas the expected limit is 1.10 TeV.</description><subject>Regular - Experimental Physics</subject><issn>1434-6044</issn><issn>1434-6052</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2016</creationdate><recordtype>article</recordtype><recordid>eNqlkM9O3DAQxlPUCuifV6jmwDXFTsIqPYCEUKseuLFqD10UOc4kMevYxuOA0mjfhWfpk9WtoNV2j5zG85tvvpG_JHnP2QfOC3aM7kYeE2fsJEsZX6RFVvK03EsOeZEX6SLil3_fRXGQvCa6YYxlBSv3k4OszFnOyuzwxY8rFF720FoPpEynEZy3zSiDsgZsC3cog_WpVmuE21H4NUGDUkxRC8oEC9_qWME5kFZrRXGNQARYNVaOA5ogtSD6zjMXrudBGTUIvYHVSOiEXIsOZzHQIEK_De8FTTQNO8rWmkA7NCrrHVjTtM1-X_HU_rc-us4jriMkDBpNF_p5ZZuGVIOD8J0ymzldfHQhKmqM7fz0s83R0YpufZij4ymUsUPT_JvSafnzYYlf4V6FHkKPcL68PL-K8YU_mb5NXrVCE757rG-Ss8-flhdfUjfWAzYyenihK-djZH6qrFDV9sSovursXXWS57xcFPmzDX4BXWvVdg</recordid><startdate>20160101</startdate><enddate>20160101</enddate><creator>Aad, G.</creator><creator>Abbott, B.</creator><creator>Abdallah, J.</creator><creator>Abdinov, O.</creator><creator>Abeloos, B.</creator><creator>Aben, R.</creator><creator>Abolins, M.</creator><creator>AbouZeid, O. 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V. ; Anjos, N. ; Annovi, A. ; Antonelli, M. ; Antonov, A. ; Antos, J. ; Anulli, F. ; Aoki, M. ; Bella, L. Aperio ; Arabidze, G. ; Arai, Y. ; Araque, J. P. ; Arce, A. T. H. ; Arduh, F. A. ; Arguin, J-F. ; Argyropoulos, S. ; Arik, M. ; Armbruster, A. 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A.</creatorcontrib><creatorcontrib>Arguin, J-F.</creatorcontrib><creatorcontrib>Argyropoulos, S.</creatorcontrib><creatorcontrib>Arik, M.</creatorcontrib><creatorcontrib>Armbruster, A. J.</creatorcontrib><creatorcontrib>Arnaez, O.</creatorcontrib><creatorcontrib>Arnold, H.</creatorcontrib><creatorcontrib>Arratia, M.</creatorcontrib><creatorcontrib>Arslan, O.</creatorcontrib><creatorcontrib>Artamonov, A.</creatorcontrib><collection>PubMed Central (Full Participant titles)</collection><jtitle>The European physical journal. C, Particles and fields</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Aad, G.</au><au>Abbott, B.</au><au>Abdallah, J.</au><au>Abdinov, O.</au><au>Abeloos, B.</au><au>Aben, R.</au><au>Abolins, M.</au><au>AbouZeid, O. S.</au><au>Abramowicz, H.</au><au>Abreu, H.</au><au>Abreu, R.</au><au>Abulaiti, Y.</au><au>Acharya, B. S.</au><au>Adamczyk, L.</au><au>Adams, D. L.</au><au>Adelman, J.</au><au>Adomeit, S.</au><au>Adye, T.</au><au>Affolder, A. A.</au><au>Agatonovic-Jovin, T.</au><au>Agricola, J.</au><au>Aguilar-Saavedra, J. A.</au><au>Ahlen, S. P.</au><au>Ahmadov, F.</au><au>Aielli, G.</au><au>Akerstedt, H.</au><au>Åkesson, T. P. A.</au><au>Akimov, A. V.</au><au>Alberghi, G. L.</au><au>Albert, J.</au><au>Albrand, S.</au><au>Verzini, M. J. Alconada</au><au>Aleksa, M.</au><au>Aleksandrov, I. N.</au><au>Alexa, C.</au><au>Alexander, G.</au><au>Alexopoulos, T.</au><au>Alhroob, M.</au><au>Alimonti, G.</au><au>Alio, L.</au><au>Alison, J.</au><au>Alkire, S. P.</au><au>Allbrooke, B. M. M.</au><au>Allen, B. W.</au><au>Allport, P. P.</au><au>Aloisio, A.</au><au>Alonso, A.</au><au>Alonso, F.</au><au>Alpigiani, C.</au><au>Gonzalez, B. Alvarez</au><au>Piqueras, D. Álvarez</au><au>Alviggi, M. G.</au><au>Amadio, B. T.</au><au>Amako, K.</au><au>Coutinho, Y. Amaral</au><au>Amelung, C.</au><au>Amidei, D.</au><au>Santos, S. P. 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J.</au><au>Arnaez, O.</au><au>Arnold, H.</au><au>Arratia, M.</au><au>Arslan, O.</au><au>Artamonov, A.</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Search for single production of vector-like quarks decaying into Wb in pp collisions at \documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$\sqrt{s} = 8$$\end{document}s=8 TeV with the ATLAS detector</atitle><jtitle>The European physical journal. C, Particles and fields</jtitle><date>2016-01-01</date><risdate>2016</risdate><volume>76</volume><issue>8</issue><issn>1434-6044</issn><eissn>1434-6052</eissn><abstract>A search for singly produced vector-like Q quarks, where Q can be either a T quark with charge \documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$+2/3$$\end{document} + 2 / 3 or a Y quark with charge \documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$-4/3$$\end{document} - 4 / 3 , is performed in proton–proton collisions recorded with the ATLAS detector at the LHC. The dataset corresponds to an integrated luminosity of 20.3 fb \documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$^{-1}$$\end{document} - 1 and was produced with a centre-of-mass energy of \documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$\sqrt{s}=8$$\end{document} s = 8  TeV. This analysis targets \documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$Q \rightarrow Wb$$\end{document} Q → W b decays where the W boson decays leptonically. A veto on massive large-radius jets is used to reject the dominant \documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$t\bar{t}$$\end{document} t t ¯ background. The reconstructed Q -candidate mass, ranging from 0.4 to 1.2 TeV, is used in the search to discriminate signal from background processes. No significant deviation from the Standard Model expectation is observed, and limits are set on the \documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$Q \rightarrow Wb$$\end{document} Q → W b cross-section times branching ratio. The results are also interpreted as limits on the QWb coupling and the mixing with the Standard Model sector for a singlet T quark or a Y quark from a doublet. T quarks with masses below 0.95 TeV are excluded at 95 % confidence level, assuming a unit coupling and a BR \documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$(T\rightarrow Wb) = 0.5$$\end{document} ( T → W b ) = 0.5 , whereas the expected limit is 1.10 TeV.</abstract><cop>Berlin/Heidelberg</cop><pub>Springer Berlin Heidelberg</pub><pmid>28303082</pmid><doi>10.1140/epjc/s10052-016-4281-8</doi><oa>free_for_read</oa></addata></record>
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title Search for single production of vector-like quarks decaying into Wb in pp collisions at \documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$\sqrt{s} = 8$$\end{document}s=8 TeV with the ATLAS detector
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