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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) |
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Main Authors: | , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , |
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container_title | The European physical journal. C, Particles and fields |
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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 |
format | article |
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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. C, Particles and fields, 2016-01, Vol.76 (8)</ispartof><rights>CERN for the benefit of the ATLAS collaboration 2016</rights><lds50>peer_reviewed</lds50><oa>free_for_read</oa><woscitedreferencessubscribed>false</woscitedreferencessubscribed></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><link.rule.ids>230,314,777,781,882,27905,27906</link.rule.ids></links><search><creatorcontrib>Aad, G.</creatorcontrib><creatorcontrib>Abbott, B.</creatorcontrib><creatorcontrib>Abdallah, J.</creatorcontrib><creatorcontrib>Abdinov, O.</creatorcontrib><creatorcontrib>Abeloos, B.</creatorcontrib><creatorcontrib>Aben, R.</creatorcontrib><creatorcontrib>Abolins, M.</creatorcontrib><creatorcontrib>AbouZeid, O. S.</creatorcontrib><creatorcontrib>Abramowicz, H.</creatorcontrib><creatorcontrib>Abreu, H.</creatorcontrib><creatorcontrib>Abreu, R.</creatorcontrib><creatorcontrib>Abulaiti, Y.</creatorcontrib><creatorcontrib>Acharya, B. S.</creatorcontrib><creatorcontrib>Adamczyk, L.</creatorcontrib><creatorcontrib>Adams, D. L.</creatorcontrib><creatorcontrib>Adelman, J.</creatorcontrib><creatorcontrib>Adomeit, S.</creatorcontrib><creatorcontrib>Adye, T.</creatorcontrib><creatorcontrib>Affolder, A. A.</creatorcontrib><creatorcontrib>Agatonovic-Jovin, T.</creatorcontrib><creatorcontrib>Agricola, J.</creatorcontrib><creatorcontrib>Aguilar-Saavedra, J. A.</creatorcontrib><creatorcontrib>Ahlen, S. P.</creatorcontrib><creatorcontrib>Ahmadov, F.</creatorcontrib><creatorcontrib>Aielli, G.</creatorcontrib><creatorcontrib>Akerstedt, H.</creatorcontrib><creatorcontrib>Åkesson, T. P. A.</creatorcontrib><creatorcontrib>Akimov, A. V.</creatorcontrib><creatorcontrib>Alberghi, G. L.</creatorcontrib><creatorcontrib>Albert, J.</creatorcontrib><creatorcontrib>Albrand, S.</creatorcontrib><creatorcontrib>Verzini, M. J. Alconada</creatorcontrib><creatorcontrib>Aleksa, M.</creatorcontrib><creatorcontrib>Aleksandrov, I. N.</creatorcontrib><creatorcontrib>Alexa, C.</creatorcontrib><creatorcontrib>Alexander, G.</creatorcontrib><creatorcontrib>Alexopoulos, T.</creatorcontrib><creatorcontrib>Alhroob, M.</creatorcontrib><creatorcontrib>Alimonti, G.</creatorcontrib><creatorcontrib>Alio, L.</creatorcontrib><creatorcontrib>Alison, J.</creatorcontrib><creatorcontrib>Alkire, S. P.</creatorcontrib><creatorcontrib>Allbrooke, B. M. M.</creatorcontrib><creatorcontrib>Allen, B. W.</creatorcontrib><creatorcontrib>Allport, P. P.</creatorcontrib><creatorcontrib>Aloisio, A.</creatorcontrib><creatorcontrib>Alonso, A.</creatorcontrib><creatorcontrib>Alonso, F.</creatorcontrib><creatorcontrib>Alpigiani, C.</creatorcontrib><creatorcontrib>Gonzalez, B. Alvarez</creatorcontrib><creatorcontrib>Piqueras, D. Álvarez</creatorcontrib><creatorcontrib>Alviggi, M. G.</creatorcontrib><creatorcontrib>Amadio, B. T.</creatorcontrib><creatorcontrib>Amako, K.</creatorcontrib><creatorcontrib>Coutinho, Y. Amaral</creatorcontrib><creatorcontrib>Amelung, C.</creatorcontrib><creatorcontrib>Amidei, D.</creatorcontrib><creatorcontrib>Santos, S. P. Amor Dos</creatorcontrib><creatorcontrib>Amorim, A.</creatorcontrib><creatorcontrib>Amoroso, S.</creatorcontrib><creatorcontrib>Amram, N.</creatorcontrib><creatorcontrib>Amundsen, G.</creatorcontrib><creatorcontrib>Anastopoulos, C.</creatorcontrib><creatorcontrib>Ancu, L. S.</creatorcontrib><creatorcontrib>Andari, N.</creatorcontrib><creatorcontrib>Andeen, T.</creatorcontrib><creatorcontrib>Anders, C. F.</creatorcontrib><creatorcontrib>Anders, G.</creatorcontrib><creatorcontrib>Anders, J. K.</creatorcontrib><creatorcontrib>Anderson, K. J.</creatorcontrib><creatorcontrib>Andreazza, A.</creatorcontrib><creatorcontrib>Andrei, V.</creatorcontrib><creatorcontrib>Angelidakis, S.</creatorcontrib><creatorcontrib>Angelozzi, I.</creatorcontrib><creatorcontrib>Anger, P.</creatorcontrib><creatorcontrib>Angerami, A.</creatorcontrib><creatorcontrib>Anghinolfi, F.</creatorcontrib><creatorcontrib>Anisenkov, A. V.</creatorcontrib><creatorcontrib>Anjos, N.</creatorcontrib><creatorcontrib>Annovi, A.</creatorcontrib><creatorcontrib>Antonelli, M.</creatorcontrib><creatorcontrib>Antonov, A.</creatorcontrib><creatorcontrib>Antos, J.</creatorcontrib><creatorcontrib>Anulli, F.</creatorcontrib><creatorcontrib>Aoki, M.</creatorcontrib><creatorcontrib>Bella, L. Aperio</creatorcontrib><creatorcontrib>Arabidze, G.</creatorcontrib><creatorcontrib>Arai, Y.</creatorcontrib><creatorcontrib>Araque, J. P.</creatorcontrib><creatorcontrib>Arce, A. T. H.</creatorcontrib><creatorcontrib>Arduh, F. 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. Amor Dos</au><au>Amorim, A.</au><au>Amoroso, S.</au><au>Amram, N.</au><au>Amundsen, G.</au><au>Anastopoulos, C.</au><au>Ancu, L. S.</au><au>Andari, N.</au><au>Andeen, T.</au><au>Anders, C. F.</au><au>Anders, G.</au><au>Anders, J. K.</au><au>Anderson, K. J.</au><au>Andreazza, A.</au><au>Andrei, V.</au><au>Angelidakis, S.</au><au>Angelozzi, I.</au><au>Anger, P.</au><au>Angerami, A.</au><au>Anghinolfi, F.</au><au>Anisenkov, A. V.</au><au>Anjos, N.</au><au>Annovi, A.</au><au>Antonelli, M.</au><au>Antonov, A.</au><au>Antos, J.</au><au>Anulli, F.</au><au>Aoki, M.</au><au>Bella, L. Aperio</au><au>Arabidze, G.</au><au>Arai, Y.</au><au>Araque, J. P.</au><au>Arce, A. T. H.</au><au>Arduh, F. A.</au><au>Arguin, J-F.</au><au>Argyropoulos, S.</au><au>Arik, M.</au><au>Armbruster, A. 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$$\end{document}s=8 TeV with the ATLAS detector</atitle><jtitle>The European physical journal. C, Particles and fields</jtitle><date>2016-01-01</date><risdate>2016</risdate><volume>76</volume><issue>8</issue><issn>1434-6044</issn><eissn>1434-6052</eissn><abstract>A search for singly produced vector-like
Q
quarks, where
Q
can be either a
T
quark with charge
\documentclass[12pt]{minimal}
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\begin{document}$$+2/3$$\end{document}
+
2
/
3
or a
Y
quark with charge
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\begin{document}$$-4/3$$\end{document}
-
4
/
3
, is performed in proton–proton collisions recorded with the ATLAS detector at the LHC. The dataset corresponds to an integrated luminosity of 20.3 fb
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\begin{document}$$^{-1}$$\end{document}
-
1
and was produced with a centre-of-mass energy of
\documentclass[12pt]{minimal}
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\begin{document}$$\sqrt{s}=8$$\end{document}
s
=
8
TeV. This analysis targets
\documentclass[12pt]{minimal}
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\begin{document}$$Q \rightarrow Wb$$\end{document}
Q
→
W
b
decays where the
W
boson decays leptonically. A veto on massive large-radius jets is used to reject the dominant
\documentclass[12pt]{minimal}
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\begin{document}$$t\bar{t}$$\end{document}
t
t
¯
background. The reconstructed
Q
-candidate mass, ranging from 0.4 to 1.2 TeV, is used in the search to discriminate signal from background processes. No significant deviation from the Standard Model expectation is observed, and limits are set on the
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\begin{document}$$Q \rightarrow Wb$$\end{document}
Q
→
W
b
cross-section times branching ratio. The results are also interpreted as limits on the
QWb
coupling and the mixing with the Standard Model sector for a singlet
T
quark or a
Y
quark from a doublet.
T
quarks with masses below 0.95 TeV are excluded at 95 % confidence level, assuming a unit coupling and a BR
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\begin{document}$$(T\rightarrow Wb) = 0.5$$\end{document}
(
T
→
W
b
)
=
0.5
, whereas the expected limit is 1.10 TeV.</abstract><cop>Berlin/Heidelberg</cop><pub>Springer Berlin Heidelberg</pub><pmid>28303082</pmid><doi>10.1140/epjc/s10052-016-4281-8</doi><oa>free_for_read</oa></addata></record> |
fulltext | fulltext |
identifier | ISSN: 1434-6044 |
ispartof | The European physical journal. C, Particles and fields, 2016-01, Vol.76 (8) |
issn | 1434-6044 1434-6052 |
language | eng |
recordid | cdi_pubmedcentral_primary_oai_pubmedcentral_nih_gov_5331864 |
source | Publicly Available Content Database; Springer Nature - SpringerLink Journals - Fully Open Access |
subjects | Regular - Experimental Physics |
title | Search for single production of vector-like quarks decaying into Wb in pp collisions at \documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$\sqrt{s} = 8$$\end{document}s=8 TeV with the ATLAS detector |
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