287 research outputs found
Jet energy measurement with the ATLAS detector in proton-proton collisions at root s=7 TeV
- Author
- Aad G
- Abbott B
- Abdallah J
- Abdelalim AA
- Abdesselam A
- Abdinov O
- Abi B
- Abolins M
- Abramowicz H
- Abreu H
- Acerbi E
- Acharya BS
- Adams DL
- Addy TN
- Adelman J
- Aderholz M
- Adomeit S
- Adragna P
- Adye T
- Aefsky S
- Aguilar-Saavedra JA
- Aharrouche M
- Ahlen SP
- Ahles F
- Ahmad A
- Ahsan M
- Aielli G
- Akdogana T
- Akesson TPA
- Akimoto G
- Akimov AV
- Akiyama A
- Aktas A
- Alam MA
- Alam MS
- Albert J
- Albrand S
- Aleksa M
- Aleksandrov IN
- Alessandria F
- Alexa C
- Alexander G
- Alexandre G
- Alexopoulos T
- Alhroob M
- Aliev M
- Alimonti G
- Alison J
- Aliyev M
- Allport PP
- Allwood-Spiers SE
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- Almond J
- Aloisio A
- Alon R
- Alonso A
- Alviggi MG
- Amako K
- Amaral P
- Amelung C
- Ammosov VV
- Amorim A
- Amoros G
- Amram N
- Anastopoulos C
- Ancu LS
- Andari N
- Andeen T
- Anders CF
- Anders G
- Anderson KJ
- Andreazza A
- Andrei V
- Andrieux M-L
- Anduaga XS
- Angerami A
- Anghinolfi F
- Anh TV
- Anjos N
- Annovi A
- Antonaki A
- Antonelli M
- Antonov A
- Antos J
- Anulli F
- Aoun S
- Apolle R
- Arabidze G
- Aracena I
- Arai Y
- Aranda CP
- Arce ATH
- Archambault JP
- Arfaoui S
- Arguin J-F
- Arik E
- Arik M
- Armbruster AJ
- Arnaez O
- Arnault C
- Artamonov A
- Artoni G
- Arutinov D
- Asai S
- Asfandiyarov R
- Ask S
- Asman B
- Asner D
- Asquith L
- Assamagan K
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- Atoian G
- Aubert B
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- Augsten K
- Aurousseau M
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- Avramidou R
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- Chernyatin V
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- Wickens FJ
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- Wiglesworth C
- Wiik-Fuchs LAM
- Wijeratne PA
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- Wilkens HG
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- Willocq S
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- Wilson JA
- Wilson MG
- Wingerter-Seez I
- Winkelmann S
- Winklmeier F
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- Wolter MW
- Wolters H
- Wong WC
- Wooden G
- Wosiek BK
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- Wraight K
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- Wu X
- Wu Y
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- Wunstorf R
- Wynne BM
- Xaplanteris L
- Xella S
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- Xie Y
- Xu C
- Xu D
- Xu G
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- Yagci KD
- Yamada M
- Yamaguchi H
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- Yamamoto K
- Yamamoto S
- Yamamura T
- Yamanaka T
- Yamaoka J
- Yamazaki T
- Yamazaki Y
- Yan Z
- Yang H
- Yang UK
- Yang Y
- Yang Y
- Yang Z
- Yanush S
- Yao Y
- Yasu Y
- Ye J
- Ye S
- Yildizb HD
- Yilmaz M
- Yoosootiniya R
- Yorita K
- Yoshida R
- Young C
- Youssef S
- Yu D
- Yu J
- Yu J
- Yuan L
- Yurkewicz A
- Zaets VG
- Zaidan R
- Zaitsev AM
- Zajacova Z
- Zalite YK
- Zanello L
- Zarzhitsky P
- Zaytsev A
- Zeitnitz C
- Zeller M
- Zeman M
- Zemla A
- Zendler C
- Zenin O
- Zenonos Z
- Zenz S
- Zerwas D
- Zhan Z
- Zhang D
- Zhang H
- Zhang J
- Zhang Q
- Zhang X
- Zhang Z
- Zhao L
- Zhao T
- Zhao Z
- Zhemchugov A
- Zheng S
- Zhong J
- Zhou B
- Zhou N
- Zhou Y
- Zhu CG
- Zhu H
- Zhu J
- Zhu Y
- Zhuang X
- Zhuravlov V
- Zieminska D
- Zimmermann R
- Zimmermann S
- Zimmermann S
- Zinonos Z
- Ziolkowski M
- Zitoun R
- Zivkovic L
- Zmouchko VV
- Zobernig G
- Zoccoli A
- Zolnierowski Y
- Zsenei A
- Zutshi V
- Zwalinski L
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/03/2013
- Field of study
The jet energy scale and its systematic uncertainty are determined for jets measured with the ATLAS detector at the LHC in proton-proton collision data at a centre-of-mass energy of √s = 7TeV corresponding to an integrated luminosity of 38 pb-1. Jets are reconstructed with the anti-kt algorithm with distance parameters R=0. 4 or R=0. 6. Jet energy and angle corrections are determined from Monte Carlo simulations to calibrate jets with transverse momenta pT≥20 GeV and pseudorapidities {pipe}η{pipe}<4. 5. The jet energy systematic uncertainty is estimated using the single isolated hadron response measured in situ and in test-beams, exploiting the transverse momentum balance between central and forward jets in events with dijet topologies and studying systematic variations in Monte Carlo simulations. The jet energy uncertainty is less than 2. 5 % in the central calorimeter region ({pipe}η{pipe}<0. 8) for jets with 60≤pT<800 GeV, and is maximally 14 % for pT<30 GeV in the most forward region 3. 2≤{pipe}η{pipe}<4. 5. The jet energy is validated for jet transverse momenta up to 1 TeV to the level of a few percent using several in situ techniques by comparing a well-known reference such as the recoiling photon pT, the sum of the transverse momenta of tracks associated to the jet, or a system of low-pT jets recoiling against a high-pT jet. More sophisticated jet calibration schemes are presented based on calorimeter cell energy density weighting or hadronic properties of jets, aiming for an improved jet energy resolution and a reduced flavour dependence of the jet response. The systematic uncertainty of the jet energy determined from a combination of in situ techniques is consistent with the one derived from single hadron response measurements over a wide kinematic range. The nominal corrections and uncertainties are derived for isolated jets in an inclusive sample of high-pT jets. Special cases such as event topologies with close-by jets, or selections of samples with an enhanced content of jets originating from light quarks, heavy quarks or gluons are also discussed and the corresponding uncertainties are determined. © 2013 CERN for the benefit of the ATLAS collaboration
Performance of novel VUV-sensitive Silicon Photo-Multipliers for nEXO
- Author
- Adhikari G.
- Angelico E.
- Arnquist I.J.
- Arsenault P.
- Badhrees I.
- Bane J.
- Belov V.
- Bernard E.P.
- Bhat A.
- Bhatta T.
- Bolotnikov A.
- Bolster J.
- Breur P.A.
- Brodsky J.P.
- Brown E.
- Brunner T.
- Caden E.
- Cao G.
- Cao L.
- Chambers C.
- Chana B.
- Charlebois S.A.
- Chernyak D.
- Chiu M.
- Cleveland B.
- Cohen J.R.
- Collister R.
- Cvitan M.
- Dalmasson J.
- Daniels T.
- Darroch L.
- Deslandes K.
- DeVoe R.
- Ding Y.
- diVacri M.L.
- Dolinski M.J.
- Dragone A.
- Echevers J.
- Eckert B.
- Elbeltagi M.
- Fabris L.
- Fairbank W.
- Farine J.
- Franco T. Pinto
- Fu Y.S.
- Gallacher D.
- Gallina G.
- Gautam P.
- Giacomini G.
- Gillis W.C.
- Gingras C.
- Goeldi D.
- Gornea R.
- Gratta G.
- Guan Y.
- Hardy C.A.
- Hedges S.
- Heffner M.
- Hein E.
- Holt J.
- Hoppe E.W.
- Hossl J.
- House A.
- Hunt W.
- Iverson A.
- Jamil A.
- Jiang X.S.
- Karelin A.
- Kaufman L.J.
- Kharusi S. Al
- Kotov I.
- Krucken R.
- Kuchenkov A.
- Kumar K.S.
- Larson A.
- Leach K.G.
- Lenardo B.G.
- Leonard Douglas
- Lessard G.
- Li G.
- Li S.
- Li Z.
- Licciardi C.
- Lindsay R.
- MacLellan R.
- Mahtab M.
- Majidi S.
- Malbrunot C.
- Margetak P.
- Martel-Dion P.
- Martin L.
- Masbou J.
- Massacret N.
- McMichael K.
- Mong B.
- Moore D.C.
- Murray K.
- Nattress J.
- Natzke C.R.
- Ngwadla X.E.
- Odian A.
- Ondze J. C. Nzobadila
- Orrell J.L.
- Ortega G.S.
- Overman C.T.
- Parent S.
- Perna A.
- Piepke A.
- Pletskova N.
- Pocar A.
- Pratte J.F.
- Radeka V.
- Raguzin E.
- Ramonnye G.J.
- Rao T.
- Rasiwala H.
- Raymond K.
- Rebeiro B.M.
- Rescia S.
- Retiere F.
- Richardson G.
- Ringuette J.
- Riot V.
- Rossignol T.
- Rowson P.C.
- Rudolph L.
- Saldanha R.
- Sangiorgio S.
- Shang X.
- Smalley H. Peltz
- Soma A.K.
- Spadoni F.
- Stekhanov V.
- Sun X.L.
- Thibado S.
- Tidball A.
- Totev T.
- Triambak S.
- Tsang R.H.M.
- Tsang T.
- Tyuka O.A.
- Vachon F.
- Vidal M.
- Viel S.
- Visser G.
- Wagenpfeil M.
- Walent M.
- Wamba K.
- Wang Q.
- Wang W.
- Wang Y.
- Watts M.
- Wei W.
- Wen L.J.
- Wichoski U.
- Wilde S.
- Worcester M.
- Wu W.H.
- Wu X.
- Xie L.
- Yan W.
- Yang H.
- Yang L.
- Zeldovich O.
- Zhao J.
- Ziegler T.
- Publication venue
- Publication date
- 16/09/2022
- Field of study
Liquid xenon time projection chambers are promising detectors to search for
neutrinoless double beta decay (0νββ), due to their response
uniformity, monolithic sensitive volume, scalability to large target masses,
and suitability for extremely low background operations. The nEXO collaboration
has designed a tonne-scale time projection chamber that aims to search for
0νββ of \ce{^{136}Xe} with projected half-life sensitivity of
1.35×1028~yr. To reach this sensitivity, the design goal for nEXO is
≤1\% energy resolution at the decay Q-value (2458.07±0.31~keV).
Reaching this resolution requires the efficient collection of both the
ionization and scintillation produced in the detector. The nEXO design employs
Silicon Photo-Multipliers (SiPMs) to detect the vacuum ultra-violet, 175 nm
scintillation light of liquid xenon. This paper reports on the characterization
of the newest vacuum ultra-violet sensitive Fondazione Bruno Kessler VUVHD3
SiPMs specifically designed for nEXO, as well as new measurements on new test
samples of previously characterised Hamamatsu VUV4 Multi Pixel Photon Counters
(MPPCs). Various SiPM and MPPC parameters, such as dark noise, gain, direct
crosstalk, correlated avalanches and photon detection efficiency were measured
as a function of the applied over voltage and wavelength at liquid xenon
temperature (163~K). The results from this study are used to provide updated
estimates of the achievable energy resolution at the decay Q-value for the
nEXO design
An integrated online radioassay data storage and analytics tool for nEXO
- Author
- Angelico E.
- Arnquist I. J.
- Atencio A.
- Badhrees I.
- Bane J.
- Barakoohi E. Teimoori
- Belov V.
- Bernard E. P.
- Bhat A.
- Bhatta T.
- Bolotnikov A.
- Breur P. A.
- Brodsky J. P.
- Brown E.
- Brunner T.
- Caden E.
- Cao G. F.
- Cao L. Q.
- Cesmecioglu D.
- Chambers C.
- Chambers E.
- Chana B.
- Charlebois S. A.
- Chernyak D.
- Chiu M.
- Cleveland B.
- Cohen J. R.
- Collister R.
- Cvitan M.
- Dalmasson J.
- Darroch L.
- Deslandes K.
- DeVoe R.
- di Vacri M. L.
- Ding Y. Y.
- Dolinski M. J.
- Echevers J.
- Eckert B.
- Elbeltagi M.
- Elmansali R.
- Fabris L.
- Fairbank W.
- Farine J.
- Franco T. Pinto
- Fu Y. S.
- Gallacher D.
- Gallina G.
- Gautam P.
- Giacomini G.
- Gillis W.
- Gingras C.
- Goeldi D.
- Gornea R.
- Gratta G.
- Guan Y. D.
- Hardy C. A.
- Hedges S.
- Heffner M.
- Hein E.
- Holt J.
- Hoppe E. W.
- House A.
- Hunt W.
- Iverson A.
- Jamil A.
- Jiang X. S.
- Karelin A.
- Kaufman L. J.
- Kharusi S. Al
- Kotov I.
- Krücken R.
- Kuchenkov A.
- Kumar K. S.
- Larson A.
- Leach K. G.
- Lenardo B. G.
- Leonard D. S.
- Li G.
- Li S.
- Li Z.
- Licciardi C.
- Lindsay R.
- MacLellan R.
- Mahtab M.
- Majidi S.
- Malbrunot C.
- Martel-Dion P.
- Masbou J.
- Massacret N.
- McMichael K.
- Mong B.
- Moore D. C.
- Murray K.
- Nattress J.
- Natzke C. R.
- Ngwadla X. E.
- Ni K.
- Nolan A.
- Nowicki S. C.
- Ondze J. C. Nzobadila
- Orrell J. L.
- Ortega G. S.
- Overman C. T.
- Peltz-Smalley H.
- Perna A.
- Piepke A.
- Pocar A.
- Pratte J. -F.
- Radeka V.
- Raguzin E.
- Rasiwala H.
- Ray D.
- Rebeiro B.
- Rescia S.
- Retière F.
- Richardson G.
- Ringuette J.
- Riot V.
- Rowson P. C.
- Roy N.
- Rudolph L.
- Saldanha R.
- Sangiorgio S.
- Schwartz S.
- Soderstrom J.
- Soma A. K.
- Spadoni F.
- Stekhanov V.
- Sun X. L.
- Thibado S.
- Tidball A.
- Totev T.
- Triambak S.
- Tsang R. H. M.
- Tsang T.
- Tyuka O. A.
- Underwood R.
- van Bruggen E.
- Veeraraghavan V.
- Vidal M.
- Viel S.
- Walent M.
- Wamba K.
- Wang Q. D.
- Wang W.
- Wang Y. G.
- Watts M.
- Wei W.
- Wen L. J.
- Wichoski U.
- Wilde S.
- Worcester M.
- Wu S.
- Wu X. M.
- Yang H.
- Yang L.
- Yvaine M.
- Zeldovich O.
- Zhao J.
- Ziegler T.
- Publication venue
- Publication date
- 12/04/2023
- Field of study
Large-scale low-background detectors are increasingly used in rare-event
searches as experimental collaborations push for enhanced sensitivity. However,
building such detectors, in practice, creates an abundance of radioassay data
especially during the conceptual phase of an experiment when hundreds of
materials are screened for radiopurity. A tool is needed to manage and make use
of the radioassay screening data to quantitatively assess detector design
options. We have developed a Materials Database Application for the nEXO
experiment to serve this purpose. This paper describes this database, explains
how it functions, and discusses how it streamlines the design of the
experiment
Measurement and interpretation of same-sign W boson pair production in association with two jets in pp collisions at s = 13 TeV with the ATLAS detector
- Author
- Aad G
- Abbott B
- Abeling K
- Abicht NJ
- Abidi SH
- Aboulhorma A
- Abramowicz H
- Abreu H
- Abulaiti Y
- Abusleme Hoffman AC
- Acharya BS
- Adam Bourdarios C
- Adamczyk L
- Adamek L
- Addepalli SV
- Addison MJ
- Adelman J
- Adiguzel A
- Adye T
- Affolder AA
- Afik Y
- Agaras MN
- Agarwala J
- Aggarwal A
- Agheorghiesei C
- Ahmad A
- Ahmadov F
- Ahmed WS
- Ahuja S
- Ai X
- Aielli G
- Aikot A
- Ait Tamlihat M
- Aitbenchikh B
- Aizenberg I
- Akbiyik M
- Akimov AV
- Akiyama D
- Akolkar NN
- Al Khoury K
- Alberghi GL
- Albert J
- Albicocco P
- Albouy GL
- Alderweireldt S
- Aleksa M
- Aleksandrov IN
- Alexa C
- Alexopoulos T
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- Åkesson TPA
- Öncel ÖO
- Ženiš T
- Živković L
- Publication venue
- Springer Nature
- Publication date
- 01/04/2024
- Field of study
This paper presents the measurement of fducial and diferential cross sections for both the inclusive and electroweak production of a same-sign W-boson pair in association with two jets (W±W±jj) using 139 fb−1 of proton-proton collision data recorded at a centre-of-mass energy of √s = 13 TeV by the ATLAS detector at the Large Hadron Collider. The analysis is performed by selecting two same-charge leptons, electron or muon, and at least two jets with large invariant mass and a large rapidity diference. The measured fducial cross sections for electroweak and inclusive W±W±jj production are 2.92 ± 0.22 (stat.) ± 0.19 (syst.)fb and 3.38±0.22 (stat.)±0.19 (syst.)fb, respectively, in agreement with Standard Model predictions. The measurements are used to constrain anomalous quartic gauge couplings by extracting 95% confdence level intervals on dimension-8 operators. A search for doubly charged Higgs bosons H±± that are produced in vector-boson fusion processes and decay into a same-sign W boson pair is performed. The largest deviation from the Standard Model occurs for an H±± mass near 450 GeV, with a global signifcance of 2.5 standard deviations
Combination of searches for heavy spin-1 resonances using 139 fb−1 of proton-proton collision data at s = 13 TeV with the ATLAS detector
- Author
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- Yamaguchi Y
- Yamashita E
- Yamauchi H
- Yamazaki T
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- Yao W-M
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- Yeletskikh I
- Yeo BK
- Yexley MR
- Yin P
- Yorita K
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- Young CJS
- Yu C
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- Yuan R
- Yue L
- Zaazoua M
- Zabinski B
- Zaid E
- Zak ZK
- Zakareishvili T
- Zakharchuk N
- Zambito S
- Zamora Saa JA
- Zang J
- Zanzi D
- Zaplatilek O
- Zeitnitz C
- Zeng H
- Zeng JC
- Zenger DT
- Zenin O
- Zenz S
- Zerradi S
- Zerwas D
- Zhai M
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- Zhang L
- Zhang P
- Zhang R
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- Zhang S
- Zhang T
- Zhang X
- Zhang X
- Zhang Y
- Zhang Y
- Zhang Y
- Zhang Z
- Zhang Z
- Zhao H
- Zhao T
- Zhao Y
- Zhao Z
- Zhao Z
- Zhemchugov A
- Zheng J
- Zheng K
- Zheng X
- Zheng Z
- Zhong D
- Zhou B
- Zhou H
- Zhou N
- Zhou Y
- Zhou Y
- Zhu CG
- Zhu J
- Zhu Y
- Zhu Y
- Zhuang X
- Zhukov K
- Zimine NI
- Zinsser J
- Ziolkowski M
- Zoccoli A
- Zoch K
- Zorbas TG
- Zormpa O
- Zou W
- Zwalinski L
- Åkesson TPA
- Öncel ÖO
- Ženiš T
- Živković L
- Publication venue
- Springer Nature
- Publication date
- 19/04/2024
- Field of study
A combination of searches for new heavy spin-1 resonances decaying into different pairings of W, Z, or Higgs bosons, as well as directly into leptons or quarks, is presented. The data sample used corresponds to 139 fb−1 of proton-proton collisions at
= 13 TeV collected during 2015–2018 with the ATLAS detector at the CERN Large Hadron Collider. Analyses selecting quark pairs (qq, bb,
, and tb) or third-generation leptons (τν and ττ) are included in this kind of combination for the first time. A simplified model predicting a spin-1 heavy vector-boson triplet is used. Cross-section limits are set at the 95% confidence level and are compared with predictions for the benchmark model. These limits are also expressed in terms of constraints on couplings of the heavy vector-boson triplet to quarks, leptons, and the Higgs boson. The complementarity of the various analyses increases the sensitivity to new physics, and the resulting constraints are stronger than those from any individual analysis considered. The data exclude a heavy vector-boson triplet with mass below 5.8 TeV in a weakly coupled scenario, below 4.4 TeV in a strongly coupled scenario, and up to 1.5 TeV in the case of production via vector-boson fusion
Studies of new Higgs boson interactions through nonresonant HH production in the b¯bγγ fnal state in pp collisions at √s = 13 TeV with the ATLAS detector
- Author
- A. A. Affolder
- A. A. Geanta
- A. A. Grillo
- A. A. Minaenko
- A. A. Snesarev
- A. A. Solodkov
- A. A. Talyshev
- A. Aboulhorma
- A. Adiguzel
- A. Aggarwal
- A. Ahmad
- A. Aikot
- A. Aloisio
- A. Alvarez Fernandez
- A. Ambler
- A. Andreazza
- A. Angerami
- A. Annovi
- A. Apyan
- A. B. Fenyuk
- A. B. Lux
- A. Bachiu
- A. Badea
- A. Bandyopadhyay
- A. Baroncelli
- A. Basan
- A. Bassalat
- A. Behera
- A. Bellerive
- A. Berrocal Guardia
- A. Berthold
- A. Betti
- A. Bingul
- A. Biondini
- A. Bitadze
- A. Blue
- A. Boveia
- A. Bruni
- A. C. A. Lee
- A. C. Forti
- A. C. Freegard
- A. C. Martyniuk
- A. C. Romero Hernandez
- A. C. Schaffer
- A. C. Sidley
- A. C. Smith
- A. C. Tate
- A. Camplani
- A. Canesse
- A. Carbone
- A. Carnelli
- A. Catinaccio
- A. Cerri
- A. Cervelli
- A. Chen
- A. Cheplakov
- A. Chitan
- A. Ciocio
- A. Clark
- A. Coccaro
- A. Cordeiro Oudot Choi
- A. Cortes-Gonzalez
- A. Cueto
- A. D. Auriol
- A. D. Gentry
- A. D. Pilkington
- A. De Maria
- A. De Salvo
- A. De Santo
- A. Dell’Acqua
- A. Di Ciaccio
- A. Di Domenico
- A. Di Girolamo
- A. Di Luca
- A. Dimitrievska
- A. Dohnalova
- A. Doria
- A. Dudarev
- A. Duperrin
- A. Durglishvili
- A. D’Onofrio
- A. E. Barton
- A. E. C. Coimbra
- A. E. Dumitriu
- A. E. Kiryunin
- A. E. McDougall
- A. E. Pinto Pinoargote
- A. El Moussaouy
- A. Ezhilov
- A. F. Mohammed
- A. F. Wongel
- A. Farbin
- A. Farilla
- A. Ferrari
- A. Filipčič
- A. Formica
- A. Froch
- A. G. Bogdanchikov
- A. G. Borbély
- A. G. Buckley
- A. G. Garcia Caffaro
- A. G. Goussiou
- A. G. Kharlamov
- A. G. Myagkov
- A. G. Rennie
- A. Gabrielli
- A. Gabrielli
- A. Garcia Alonso
- A. Gavrilyuk
- A. Gekow
- A. Ghosal
- A. Ghosh
- A. Ghosh
- A. Giannini
- A. Gomes
- A. Gongadze
- A. Gorišek
- A. Guida
- A. H. Melo
- A. Haas
- A. Hadef
- A. Held
- A. Hoecker
- A. Hrynevich
- A. I. Hagan
- A. I. Mincer
- A. Ivina
- A. J. Bailey
- A. J. Barr
- A. J. Beddall
- A. J. Bevan
- A. J. Gomez Delegido
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- S. Zambito
- S. Zenz
- S. Zerradi
- S. Zhang
- S. Zhang
- S.-C. Hsu
- T. A. Beermann
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- T. A. Martin
- T. A. Ruggeri
- T. A. Schwarz
- T. Adye
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- T. Aoki
- T. B. Huffman
- T. Barillari
- T. Barklow
- T. Beau
- T. Berry
- T. Bisanz
- T. Bold
- T. Buanes
- T. C. Gosart
- T. C. Mclachlan
- T. C. Petersen
- T. Carli
- T. Chowdhury
- T. Cuhadar Donszelmann
- T. Dado
- T. Dai
- T. Davidek
- T. Dias Do Vale
- T. Djobava
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- T. G. Hitchings
- T. G. Zorbas
- T. Geralis
- T. Giani
- T. Golling
- T. H. Park
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- T. Heim
- T. Herrmann
- T. Holm
- T. Hryn’ova
- T. Iizawa
- T. Ingebretsen Carlson
- T. J. Jones
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- T. J. Neep
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- T. Junkermann
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- T. Koffas
- T. Komarek
- T. Kono
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- T. Kuhl
- T. Kupfer
- T. Kwan
- T. L. Bruckler
- T. Lagouri
- T. Lari
- T. Lenz
- T. Li
- T. Lohse
- T. Lyubushkina
- T. M. Baer
- T. M. Carter
- T. M. Hong
- T. M. Knight
- T. M. Pham
- T. Madula
- T. Maeno
- T. Mashimo
- T. Masubuchi
- T. Mathisen
- T. Min
- T. Mkrtchyan
- T. Mlinarevic
- T. Moskalets
- T. Nobe
- T. Nommensen
- T. Novak
- T. P. A. Åkesson
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- T. Pan
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- T. Poulsen
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- T. Wengler
- T. Xu
- T. Yamazaki
- T. Yang
- T. Zakareishvili
- T. Zhang
- T. Zhao
- T. Ženiš
- The ATLAS collaboration
- U. Barron
- U. Blumenschein
- U. De Sanctis
- U. Klein
- U. Kruchonak
- U. Landgraf
- U. M. Patel
- U. Mallik
- U. Parzefall
- U. Schäfer
- U. Soldevila
- V. A. Austrup
- V. A. Bednyakov
- V. A. Kramarenko
- V. A. Mitsou
- V. A. Parrish
- V. A. Schegelsky
- V. Ananiev
- V. Balakrishnan
- V. Boisvert
- V. Büscher
- V. Canale
- V. Castillo Gimenez
- V. Cavaliere
- V. Cavasinni
- V. Cepaitis
- V. Chiarella
- V. Cindro
- V. Croft
- V. Dao
- V. D’Amico
- V. E. Ozcan
- V. Ellajosyula
- V. F. Kazanin
- V. Fadeyev
- V. Franco Lima
- V. Gautam
- V. Goumarre
- V. H. Ruelas Rivera
- V. Hedberg
- V. I. Martinez Outschoorn
- V. Ippolito
- V. Izzo
- V. J. Martin
- V. K. Gassmann
- V. Kartvelishvili
- V. Kukhtin
- V. Latonova
- V. Lyubushkin
- V. M. M. Cairo
- V. Maiboroda
- V. Maksimovic
- V. Nikolaenko
- V. O’Shea
- V. P. Maleev
- V. Petousis
- V. Plesanovs
- V. Pleskot
- V. Polychronakos
- V. R. Bailey
- V. Raskina
- V. S. Bhopatkar
- V. S. Bobrovnikov
- V. S. Lang
- V. S. Martoiu
- V. Sanchez Sebastian
- V. Senthilkumar
- V. Smakhtin
- V. Solovyev
- V. Sothilingam
- V. Tikhomirov
- V. Tsiskaridze
- V. Tsulaia
- V. Tudorache
- V. V. Kostyukhin
- V. V. Sulin
- V. Vacek
- V. Vecchio
- V. Vorobel
- V. Zhulanov
- W-M. Yao
- W. A. Leight
- W. Alkakhi
- W. Buttinger
- W. C. Fisher
- W. D. Heidorn
- W. Dabrowski
- W. F. George
- W. F. Mader
- W. Guan
- W. H. Hopkins
- W. H. Kostecka
- W. Islam
- W. J. Fawcett
- W. J. Murray
- W. K. Balunas
- W. K. Brooks
- W. Kozanecki
- W. Lampl
- W. Leinonen
- W. Ma
- W. R. Cunningham
- W. S. Ahmed
- W. S. Freund
- W. Su
- W. T. Wang
- W. Taylor
- W. Vandelli
- W. Verkerke
- W. W. Przygoda
- W. Wagner
- W. Walkowiak
- W. Wang
- W. Wiedenmann
- W. Y. Chan
- W. Y. Song
- W. Zou
- X. Ai
- X. Chen
- X. Chen
- X. Chu
- X. Huang
- X. Huang
- X. Jia
- X. Jia
- X. Ju
- X. Li
- X. Liu
- X. Liu
- X. Lou
- X. Lou
- X. Mapekula
- X. Ruan
- X. Shi
- X. Su
- X. Wang
- X. Wang
- X. Wang
- X. Wu
- X. Xie
- X. Yang
- X. Yang
- X. Ye
- X. Zhang
- X. Zhang
- X. Zheng
- X. Zhuang
- Y. A. Kurochkin
- Y. A. R. Khwaira
- Y. Abulaiti
- Y. Afik
- Y. Amaral Coutinho
- Y. Benhammou
- Y. C. Cekmecelioglu
- Y. C. Yap
- Y. Cai
- Y. Cai
- Y. Cao
- Y. Chen
- Y. Chou
- Y. Coadou
- Y. El Ghazali
- Y. Enari
- Y. F. Han
- Y. F. Hu
- Y. Fan
- Y. Fang
- Y. Fu
- Y. Gao
- Y. Go
- Y. Guo
- Y. Hasegawa
- Y. Hayashi
- Y. He
- Y. He
- Y. Hernández Jiménez
- Y. Horii
- Y. Huang
- Y. Huang
- Y. Ikegami
- Y. J. Lu
- Y. K. Kim
- Y. Ke
- Y. Kulchitsky
- Y. L. Liu
- Y. Liu
- Y. Ma
- Y. Mino
- Y. Mitsumori
- Y. Nakahama
- Y. Okumura
- Y. Qin
- Y. Rodriguez Garcia
- Y. Rozen
- Y. Smirnov
- Y. T. Harris
- Y. Takubo
- Y. Tayalati
- Y. Tian
- Y. Tsujikawa
- Y. Tu
- Y. W. Liu
- Y. W. Y. Ng
- Y. Wang
- Y. Wang
- Y. Wei
- Y. Wu
- Y. Xu
- Y. Y. Frid
- Y. Yamaguchi
- Y. Yamazaki
- Y. Yang
- Y. Yang
- Y. Yeh
- Y. Yu
- Y. Zhang
- Y. Zhang
- Y. Zhang
- Y. Zhao
- Y. Zhou
- Y. Zhu
- Y. Zhu
- Yu. A. Tikhonov
- Yu. Volkotrub
- Z. B. Pollock
- Z. Cui
- Z. Dolezal
- Z. Farazpay
- Z. Feng
- Z. H. Citron
- Z. Huang
- Z. Hubacek
- Z. Jia
- Z. K. Zak
- Z. L. Alegria
- Z. Lawrence
- Z. Li
- Z. Li
- Z. Li
- Z. Liang
- Z. M. A. Rozario
- Z. M. Karpova
- Z. Marshall
- Z. O. Earnshaw
- Z. Rurikova
- Z. Soumaimi
- Z. Tao
- Z. Uysal
- Z. Wang
- Z. Wang
- Z. Wang
- Z. Wolffs
- Z. Wu
- Z. Xu
- Z. Xu
- Z. Yan
- Z. Yang
- Z. Zhang
- Z. Zhang
- Z. Zhao
- Z. Zheng
- Ö. O. Öncel
- Publication venue
- Springer
- Publication date
- 01/01/2024
- Field of study
A search for nonresonant Higgs boson pair production in the b
¯bγγ fnal state
is performed using 140 fb−1 of proton-proton collisions at a centre-of-mass energy of 13 TeV
recorded by the ATLAS detector at the CERN Large Hadron Collider. This analysis supersedes
and expands upon the previous nonresonant ATLAS results in this fnal state based on the
same data sample. The analysis strategy is optimised to probe anomalous values not only of
the Higgs (H) boson self-coupling modifer κλ but also of the quartic HHV V (V = W, Z)
coupling modifer κ2V . No signifcant excess above the expected background from Standard
Model processes is observed. An observed upper limit µHH < 4.0 is set at 95% confdence
level on the Higgs boson pair production cross-section normalised to its Standard Model
prediction. The 95% confdence intervals for the coupling modifers are −1.4 < κλ < 6.9 and
−0.5 < κ2V < 2.7, assuming all other Higgs boson couplings except the one under study are
fxed to the Standard Model predictions. The results are interpreted in the Standard Model
efective feld theory and Higgs efective feld theory frameworks in terms of constraints on
the couplings of anomalous Higgs boson (self-)interactions
- …