Measurement of electroweak $ Z\left(\nu \overline{\nu}\right)\gamma jj $ production and limits on anomalous quartic gauge couplings in pp collisions at $ \sqrt{s} $ = 13 TeV with the ATLAS detector
The electroweak production of $ Z\left(\nu \overline{\nu}\right)\gamma $ in association with two jets is studied in a regime with a photon of high transverse momentum above 150 GeV using proton–proton collisions at a centre-of-mass energy of 13 TeV at the Large Hadron Collider. The analysis uses a d...
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creator | Aad, G Abbott, B Abbott, D.C Abeling, K Abidi, S.H Aboulhorma, A Abramowicz, H Abreu, H Abulaiti, Y Abusleme Hoffman, A.C Acharya, B.S Achkar, B Adam Bourdarios, C Adamczyk, L Adamek, L Addepalli, S.V Adelman, J Adiguzel, A Adorni, S Adye, T Affolder, A.A Afik, Y Agaras, M.N Agarwala, J Aggarwal, A Agheorghiesei, C Aguilar-Saavedra, J.A Ahmad, A Ahmadov, F Ahmed, W.S Ahuja, S Ai, X Aielli, G Aizenberg, I Akbiyik, M Åkesson, T.P. A Akimov, A.V Al Khoury, K Alberghi, G.L Albert, J Albicocco, P Alconada Verzini, M.J Alderweireldt, S Aleksa, M Aleksandrov, I.N Alexa, C Alexopoulos, T Alfonsi, A Alfonsi, F Alhroob, M Ali, B Ali, S Aliev, M Alimonti, G Alkakhi, W Allaire, C Allbrooke, B.M. M Allport, P.P Aloisio, A Alonso, F Alpigiani, C Alunno Camelia, E Alvarez Estevez, M Alviggi, M.G Amaral Coutinho, Y Ambler, A Amelung, C Ames, C.G Amidei, D Amor dos Santos, S.P Amoroso, S Amos, K.R Amrouche, C.S Ananiev, V Anastopoulos, C Andeen, T Anders, J.K Andrean, S.Y Andreazza, A Angelidakis, S Angerami, A Anisenkov, A.V Annovi, A Antel, C Anthony, M.T Antipov, E Antonelli, M Antrim, D.J. A Anulli, F Aoki, M Aoki, T Aparisi Pozo, J.A Aparo, M.A Aperio Bella, L Appelt, C Aranzabal, N Araujo Ferraz, V Arcangeletti, C Arce, A.T. H Arena, E |
description | The electroweak production of $ Z\left(\nu \overline{\nu}\right)\gamma $ in association with two jets is studied in a regime with a photon of high transverse momentum above 150 GeV using proton–proton collisions at a centre-of-mass energy of 13 TeV at the Large Hadron Collider. The analysis uses a data sample with an integrated luminosity of 139 fb$^{−1}$ collected by the ATLAS detector during the 2015–2018 LHC data-taking period. This process is an important probe of the electroweak symmetry breaking mechanism in the Standard Model and is sensitive to quartic gauge boson couplings via vector-boson scattering. The fiducial $ Z\left(\nu \overline{\nu}\right)\gamma jj $ cross section for electroweak production is measured to be $ {0.77}_{-0.30}^{+0.34} $ fb and is consistent with the Standard Model prediction. Evidence of electroweak $ Z\left(\nu \overline{\nu}\right)\gamma jj $ production is found with an observed significance of 3.2σ for the background-only hypothesis, compared with an expected significance of 3.7σ. The combination of this result with the previously published ATLAS observation of electroweak $ Z\left(\nu \overline{\nu}\right)\gamma jj $ production yields an observed (expected) signal significance of 6.3σ (6.6σ). Limits on anomalous quartic gauge boson couplings are obtained in the framework of effective field theory with dimension-8 operators.[graphic not available: see fulltext] |
doi_str_mv | 10.1007/JHEP06(2023)082 |
format | Article |
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The analysis uses a data sample with an integrated luminosity of 139 fb$^{−1}$ collected by the ATLAS detector during the 2015–2018 LHC data-taking period. This process is an important probe of the electroweak symmetry breaking mechanism in the Standard Model and is sensitive to quartic gauge boson couplings via vector-boson scattering. The fiducial $ Z\left(\nu \overline{\nu}\right)\gamma jj $ cross section for electroweak production is measured to be $ {0.77}_{-0.30}^{+0.34} $ fb and is consistent with the Standard Model prediction. Evidence of electroweak $ Z\left(\nu \overline{\nu}\right)\gamma jj $ production is found with an observed significance of 3.2σ for the background-only hypothesis, compared with an expected significance of 3.7σ. The combination of this result with the previously published ATLAS observation of electroweak $ Z\left(\nu \overline{\nu}\right)\gamma jj $ production yields an observed (expected) signal significance of 6.3σ (6.6σ). 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H</creatorcontrib><creatorcontrib>Arena, E</creatorcontrib><title>Measurement of electroweak $ Z\left(\nu \overline{\nu}\right)\gamma jj $ production and limits on anomalous quartic gauge couplings in pp collisions at $ \sqrt{s} $ = 13 TeV with the ATLAS detector</title><title>JHEP</title><description>The electroweak production of $ Z\left(\nu \overline{\nu}\right)\gamma $ in association with two jets is studied in a regime with a photon of high transverse momentum above 150 GeV using proton–proton collisions at a centre-of-mass energy of 13 TeV at the Large Hadron Collider. The analysis uses a data sample with an integrated luminosity of 139 fb$^{−1}$ collected by the ATLAS detector during the 2015–2018 LHC data-taking period. This process is an important probe of the electroweak symmetry breaking mechanism in the Standard Model and is sensitive to quartic gauge boson couplings via vector-boson scattering. The fiducial $ Z\left(\nu \overline{\nu}\right)\gamma jj $ cross section for electroweak production is measured to be $ {0.77}_{-0.30}^{+0.34} $ fb and is consistent with the Standard Model prediction. Evidence of electroweak $ Z\left(\nu \overline{\nu}\right)\gamma jj $ production is found with an observed significance of 3.2σ for the background-only hypothesis, compared with an expected significance of 3.7σ. The combination of this result with the previously published ATLAS observation of electroweak $ Z\left(\nu \overline{\nu}\right)\gamma jj $ production yields an observed (expected) signal significance of 6.3σ (6.6σ). 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A ; Akimov, A.V ; Al Khoury, K ; Alberghi, G.L ; Albert, J ; Albicocco, P ; Alconada Verzini, M.J ; Alderweireldt, S ; Aleksa, M ; Aleksandrov, I.N ; Alexa, C ; Alexopoulos, T ; Alfonsi, A ; Alfonsi, F ; Alhroob, M ; Ali, B ; Ali, S ; Aliev, M ; Alimonti, G ; Alkakhi, W ; Allaire, C ; Allbrooke, B.M. M ; Allport, P.P ; Aloisio, A ; Alonso, F ; Alpigiani, C ; Alunno Camelia, E ; Alvarez Estevez, M ; Alviggi, M.G ; Amaral Coutinho, Y ; Ambler, A ; Amelung, C ; Ames, C.G ; Amidei, D ; Amor dos Santos, S.P ; Amoroso, S ; Amos, K.R ; Amrouche, C.S ; Ananiev, V ; Anastopoulos, C ; Andeen, T ; Anders, J.K ; Andrean, S.Y ; Andreazza, A ; Angelidakis, S ; Angerami, A ; Anisenkov, A.V ; Annovi, A ; Antel, C ; Anthony, M.T ; Antipov, E ; Antonelli, M ; Antrim, D.J. A ; Anulli, F ; Aoki, M ; Aoki, T ; Aparisi Pozo, J.A ; Aparo, M.A ; Aperio Bella, L ; Appelt, C ; Aranzabal, N ; Araujo Ferraz, V ; Arcangeletti, C ; Arce, A.T. H ; Arena, E</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-h752-22b59aeb6c9c44341dd81ffd299fc39ccabd7a3518aaef3c1af55f1a75fba81d0</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2023</creationdate><topic>High Energy Physics - Experiment</topic><topic>Physics</topic><toplevel>peer_reviewed</toplevel><creatorcontrib>Aad, G</creatorcontrib><creatorcontrib>Abbott, B</creatorcontrib><creatorcontrib>Abbott, D.C</creatorcontrib><creatorcontrib>Abeling, K</creatorcontrib><creatorcontrib>Abidi, S.H</creatorcontrib><creatorcontrib>Aboulhorma, A</creatorcontrib><creatorcontrib>Abramowicz, H</creatorcontrib><creatorcontrib>Abreu, H</creatorcontrib><creatorcontrib>Abulaiti, Y</creatorcontrib><creatorcontrib>Abusleme Hoffman, A.C</creatorcontrib><creatorcontrib>Acharya, B.S</creatorcontrib><creatorcontrib>Achkar, B</creatorcontrib><creatorcontrib>Adam Bourdarios, C</creatorcontrib><creatorcontrib>Adamczyk, L</creatorcontrib><creatorcontrib>Adamek, L</creatorcontrib><creatorcontrib>Addepalli, S.V</creatorcontrib><creatorcontrib>Adelman, J</creatorcontrib><creatorcontrib>Adiguzel, A</creatorcontrib><creatorcontrib>Adorni, S</creatorcontrib><creatorcontrib>Adye, T</creatorcontrib><creatorcontrib>Affolder, A.A</creatorcontrib><creatorcontrib>Afik, Y</creatorcontrib><creatorcontrib>Agaras, M.N</creatorcontrib><creatorcontrib>Agarwala, J</creatorcontrib><creatorcontrib>Aggarwal, A</creatorcontrib><creatorcontrib>Agheorghiesei, C</creatorcontrib><creatorcontrib>Aguilar-Saavedra, J.A</creatorcontrib><creatorcontrib>Ahmad, A</creatorcontrib><creatorcontrib>Ahmadov, F</creatorcontrib><creatorcontrib>Ahmed, W.S</creatorcontrib><creatorcontrib>Ahuja, S</creatorcontrib><creatorcontrib>Ai, X</creatorcontrib><creatorcontrib>Aielli, G</creatorcontrib><creatorcontrib>Aizenberg, I</creatorcontrib><creatorcontrib>Akbiyik, M</creatorcontrib><creatorcontrib>Åkesson, T.P. 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H</creatorcontrib><creatorcontrib>Arena, E</creatorcontrib><collection>Hyper Article en Ligne (HAL)</collection><jtitle>JHEP</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>no_fulltext</fulltext></delivery><addata><au>Aad, G</au><au>Abbott, B</au><au>Abbott, D.C</au><au>Abeling, K</au><au>Abidi, S.H</au><au>Aboulhorma, A</au><au>Abramowicz, H</au><au>Abreu, H</au><au>Abulaiti, Y</au><au>Abusleme Hoffman, A.C</au><au>Acharya, B.S</au><au>Achkar, B</au><au>Adam Bourdarios, C</au><au>Adamczyk, L</au><au>Adamek, L</au><au>Addepalli, S.V</au><au>Adelman, J</au><au>Adiguzel, A</au><au>Adorni, S</au><au>Adye, T</au><au>Affolder, A.A</au><au>Afik, Y</au><au>Agaras, M.N</au><au>Agarwala, J</au><au>Aggarwal, A</au><au>Agheorghiesei, C</au><au>Aguilar-Saavedra, J.A</au><au>Ahmad, A</au><au>Ahmadov, F</au><au>Ahmed, W.S</au><au>Ahuja, S</au><au>Ai, X</au><au>Aielli, G</au><au>Aizenberg, I</au><au>Akbiyik, M</au><au>Åkesson, T.P. A</au><au>Akimov, A.V</au><au>Al Khoury, K</au><au>Alberghi, G.L</au><au>Albert, J</au><au>Albicocco, P</au><au>Alconada Verzini, M.J</au><au>Alderweireldt, S</au><au>Aleksa, M</au><au>Aleksandrov, I.N</au><au>Alexa, C</au><au>Alexopoulos, T</au><au>Alfonsi, A</au><au>Alfonsi, F</au><au>Alhroob, M</au><au>Ali, B</au><au>Ali, S</au><au>Aliev, M</au><au>Alimonti, G</au><au>Alkakhi, W</au><au>Allaire, C</au><au>Allbrooke, B.M. M</au><au>Allport, P.P</au><au>Aloisio, A</au><au>Alonso, F</au><au>Alpigiani, C</au><au>Alunno Camelia, E</au><au>Alvarez Estevez, M</au><au>Alviggi, M.G</au><au>Amaral Coutinho, Y</au><au>Ambler, A</au><au>Amelung, C</au><au>Ames, C.G</au><au>Amidei, D</au><au>Amor dos Santos, S.P</au><au>Amoroso, S</au><au>Amos, K.R</au><au>Amrouche, C.S</au><au>Ananiev, V</au><au>Anastopoulos, C</au><au>Andeen, T</au><au>Anders, J.K</au><au>Andrean, S.Y</au><au>Andreazza, A</au><au>Angelidakis, S</au><au>Angerami, A</au><au>Anisenkov, A.V</au><au>Annovi, A</au><au>Antel, C</au><au>Anthony, M.T</au><au>Antipov, E</au><au>Antonelli, M</au><au>Antrim, D.J. A</au><au>Anulli, F</au><au>Aoki, M</au><au>Aoki, T</au><au>Aparisi Pozo, J.A</au><au>Aparo, M.A</au><au>Aperio Bella, L</au><au>Appelt, C</au><au>Aranzabal, N</au><au>Araujo Ferraz, V</au><au>Arcangeletti, C</au><au>Arce, A.T. H</au><au>Arena, E</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Measurement of electroweak $ Z\left(\nu \overline{\nu}\right)\gamma jj $ production and limits on anomalous quartic gauge couplings in pp collisions at $ \sqrt{s} $ = 13 TeV with the ATLAS detector</atitle><jtitle>JHEP</jtitle><date>2023</date><risdate>2023</risdate><volume>6</volume><abstract>The electroweak production of $ Z\left(\nu \overline{\nu}\right)\gamma $ in association with two jets is studied in a regime with a photon of high transverse momentum above 150 GeV using proton–proton collisions at a centre-of-mass energy of 13 TeV at the Large Hadron Collider. The analysis uses a data sample with an integrated luminosity of 139 fb$^{−1}$ collected by the ATLAS detector during the 2015–2018 LHC data-taking period. This process is an important probe of the electroweak symmetry breaking mechanism in the Standard Model and is sensitive to quartic gauge boson couplings via vector-boson scattering. The fiducial $ Z\left(\nu \overline{\nu}\right)\gamma jj $ cross section for electroweak production is measured to be $ {0.77}_{-0.30}^{+0.34} $ fb and is consistent with the Standard Model prediction. Evidence of electroweak $ Z\left(\nu \overline{\nu}\right)\gamma jj $ production is found with an observed significance of 3.2σ for the background-only hypothesis, compared with an expected significance of 3.7σ. The combination of this result with the previously published ATLAS observation of electroweak $ Z\left(\nu \overline{\nu}\right)\gamma jj $ production yields an observed (expected) signal significance of 6.3σ (6.6σ). Limits on anomalous quartic gauge boson couplings are obtained in the framework of effective field theory with dimension-8 operators.[graphic not available: see fulltext]</abstract><doi>10.1007/JHEP06(2023)082</doi><orcidid>https://orcid.org/0000-0003-3552-6566</orcidid><orcidid>https://orcid.org/0000-0002-2837-2442</orcidid><orcidid>https://orcid.org/0000-0002-2190-272X</orcidid><orcidid>https://orcid.org/0000-0001-9500-2487</orcidid><orcidid>https://orcid.org/0000-0001-9398-1909</orcidid><orcidid>https://orcid.org/0000-0002-3598-2847</orcidid><orcidid>https://orcid.org/0000-0002-6665-4934</orcidid><orcidid>https://orcid.org/0000-0002-9807-861X</orcidid><orcidid>https://orcid.org/0000-0002-4098-2024</orcidid><orcidid>https://orcid.org/0000-0002-0948-5775</orcidid><orcidid>https://orcid.org/0000-0002-2551-5751</orcidid><oa>free_for_read</oa></addata></record> |
fulltext | no_fulltext |
identifier | DOI: 10.1007/JHEP06(2023)082 |
ispartof | JHEP, 2023, Vol.6 |
issn | |
language | eng |
recordid | cdi_hal_primary_oai_HAL_hal_04132486v1 |
source | |
subjects | High Energy Physics - Experiment Physics |
title | Measurement of electroweak $ Z\left(\nu \overline{\nu}\right)\gamma jj $ production and limits on anomalous quartic gauge couplings in pp collisions at $ \sqrt{s} $ = 13 TeV with the ATLAS detector |
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