32 research outputs found
Measurements of differential cross-sections in top-quark pair events with a high transverse momentum top quark and limits on beyond the Standard Model contributions to top-quark pair production with the ATLAS detector at √s = 13 TeV
- Author
- Aad G
- Abbott B
- Abbott DC
- Abeling K
- Abhayasinghe DK
- Abidi SH
- Aboulhorma A
- Abramowicz H
- Abreu H
- Abud AA
- Abulaiti Y
- Acharya BS
- Achkar B
- Adam L
- Adamczyk L
- Adamek L
- Addepalli SV
- Adelman J
- Adiguzel A
- Adorni S
- Adye T
- Affolder AA
- Afik Y
- Agaras MN
- Agarwala J
- Aggarwal A
- Agheorghiesei C
- Aguilar-Saavedra JA
- Agullo PM
- Ahmad A
- Ahmadov F
- Ahmed WS
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- Aielli G
- Aizenberg I
- Akbiyik M
- Akesson TPA
- Akimov AV
- Al Khoury K
- Alberghi GL
- Albert J
- Albicocco P
- Alderweireldt S
- Aleksa M
- Aleksandrov IN
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- Alfonsi A
- Alfonsi F
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- Ali B
- Ali S
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- Allport PP
- Aloisio A
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- Alviggi MG
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- Amelung C
- Amidei D
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- Amos KR
- Amrouche CS
- Ananiev V
- Anastopoulos C
- Andana RYG
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- Anders JK
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- Angelidakis S
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- Anisenkov AV
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- Aparo MA
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- Arguin JF
- Argyropoulos S
- Arling JH
- Armbruster AJ
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- Asada H
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- Asimakopoulou EM
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- Zhemchugov A
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- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2022
- Field of study
Cross-section measurements of top-quark pair production where the hadronically decaying top quark has transverse momentum greater than 355 GeV and the other top quark decays into ℓνb are presented using 139 fb−1 of data collected by the ATLAS experiment during proton-proton collisions at the LHC. The fiducial cross-section at s = 13 TeV is measured to be σ = 1.267 ± 0.005 ± 0.053 pb, where the uncertainties reflect the limited number of data events and the systematic uncertainties, giving a total uncertainty of 4.2%. The cross-section is measured differentially as a function of variables characterising the tt¯ system and additional radiation in the events. The results are compared with various Monte Carlo generators, including comparisons where the generators are reweighted to match a parton-level calculation at next-to-next-to-leading order. The reweighting improves the agreement between data and theory. The measured distribution of the top-quark transverse momentum is used to search for new physics in the context of the effective field theory framework. No significant deviation from the Standard Model is observed and limits are set on the Wilson coefficients of the dimension-six operators OtG and Otq(8), where the limits on the latter are the most stringent to date. [Figure not available: see fulltext.]
Accuracy versus precision in boosted top tagging with the ATLAS detector
- Author
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- Aakvaag E
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- Abdelhameed S
- Abeling K
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- Fenton MJ
- Ferencz L
- Ferguson RAM
- Fernandez AA
- Fernoux MJV
- Ferrando J
- Ferrari A
- Ferrari P
- Ferrari R
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- Ferrer JAV
- Ferrere D
- Ferretti C
- Fiacco D
- Fiedler F
- Fiedler P
- Filho LEB
- Filipčič A
- Filmer EK
- Filthaut F
- Fiolhais MCN
- Fiorini L
- Fisher WC
- Fitschen T
- Fitzhugh PM
- Fleck I
- Fleischmann P
- Flick T
- Flores CAA
- Flores M
- Follega FM
- Fomin N
- Foo JH
- Formica A
- Forti AC
- Fortin E
- Fortman AW
- Foti MG
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- Fox H
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- Gabrielli A
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- Gaid S
- Galantzan S
- Gallas EJ
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- García C
- Gardner GL
- Gardner RW
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- Garg D
- Garg RB
- Gargan JM
- Garner CA
- Garrido SF
- Garvey CM
- Garzon GOY
- Gassmann VK
- Gaudio G
- Gautam V
- Gauzzi P
- Gavranovic J
- Gavrilenko IL
- Gavrilyuk A
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- Gekow A
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- Genest MH
- Gentry AD
- George S
- George WF
- Geralis T
- Gessinger-Befurt P
- Geyik ME
- Ghani M
- Ghazali YE
- Ghorbanian K
- Ghosal A
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- Ghosh A
- Giacobbe B
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- Giannini A
- Gibson SM
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- Gilbert AK
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- Gillberg D
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- Ginabat L
- Gingrich DM
- Giordani MP
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- Giugni D
- Giuli F
- Gkialas I
- Gladilin LK
- Glasman C
- Gledhill GR
- Glemža G
- Glisic M
- Gnesi I
- Go Y
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- Gocke B
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- Gokturk B
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- Gololo MGD
- Golubkov D
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- Gonzalez SV
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- Gonçalo R
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- Gorini B
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- Goshaw AT
- Gostkin MI
- Goswami S
- Gottardo CA
- Gotz SA
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- Goussiou AG
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- Gramstad E
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- Grant CM
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- Gravili FG
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- Gregor IM
- Greif KT
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- Gross E
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- Grundy JC
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- Guardia AB
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- Guida A
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- Guindon S
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- Gurdasani SS
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- Hangal DA
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- Harris YT
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- Hasegawa Y
- Haslbeck F
- Hassan S
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- Hawkings RJ
- Hayashi Y
- Hayden D
- Hayes C
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- Hays CP
- Hays JM
- Hayward HS
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- Heatley NB
- Hedberg V
- Heggelund AL
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- Hertenberger R
- Hervas L
- Hesping ME
- Hessey NP
- Hidaoui M
- Hidic N
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- Horii Y
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- Hrynevich A
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- Hsu S-C
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- Huang X
- Huang Y
- Huang Y
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- Iakovidis G
- Ibanez AP
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- Iglesias JAS
- Iguchi R
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- Iizawa T
- Ikegami Y
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- Irwin RK
- Ishino M
- Islam W
- Issever C
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- Izzo V
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- Jiménez YH
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- Ju X
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- Kalaitzidou I
- Kalderon CW
- Kang NJ
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- Kareem MJ
- Karentzos E
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- Karpova ZM
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- Karyukhin AN
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- Keeler R
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- Klimentov A
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- Koch SF
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- Kolay O
- Koletsou I
- Komarek T
- Kong AXY
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- Kontaxakis P
- Konya B
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- Kostyukhin VV
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- Kotwal A
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- Kourlitis E
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- Kurdysh O
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- Kyriacou NG
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- Lahbabi FZ
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- Latonova V
- Latour BMD
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- Le Pottier LT
- Le B
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- Liberti B
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- Luengo SIF
- Luise I
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- Ogrodnik A
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- Okumura Y
- Oleksiyuk I
- Oliveira MVS
- Oliver JL
- Onofre A
- Onyisi PUE
- Oreglia MJ
- Orellana GE
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- Ospanov R
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- Ovsiannikova T
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- Pizzi DA
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- Poblete PAU
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- Pollock ZB
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- Popa S
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- Poreba A
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- Zou W
- Zwalinski L
- Åkesson TPA
- Öncel ÖO
- Ženiš T
- Živković L
- Publication venue
- IOP Publishing
- Publication date
- 01/08/2024
- Field of study
Abstract
The identification of top quark decays where the top quark has a large momentum transverse to the beam axis, known as top tagging, is a crucial component in many measurements of Standard Model processes and searches for beyond the Standard Model physics at the Large Hadron Collider.
Machine learning techniques have improved the performance of top tagging algorithms, but the size of the systematic uncertainties for all proposed algorithms has not been systematically studied.
This paper presents the performance of several machine learning based top tagging algorithms on a dataset constructed from simulated proton-proton collision events measured with the ATLAS detector at √
s
= 13 TeV.
The systematic uncertainties associated with these algorithms are estimated through an approximate procedure that is not meant to be used in a physics analysis, but is appropriate for the level of precision required for this study.
The most performant algorithms are found to have the largest uncertainties, motivating the development of methods to reduce these uncertainties without compromising performance.
To enable such efforts in the wider scientific community, the datasets used in this paper are made publicly available.</jats:p
Modeling rare pediatric neurogenetic disorders with IPSCs
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- Publication venue
- 'American Institute of Mathematical Sciences (AIMS)'
- Publication date
- 01/01/2019
- Field of study
Recommended from our members
Search for Eccentric Black Hole Coalescences during the Third Observing Run of LIGO and Virgo
- Author
- Abac AG
- Abbott R
- Abe H
- Acernese F
- Ackley K
- Adamcewicz C
- Adhicary S
- Adhikari N
- Adhikari RX
- Adkins VK
- Adya VB
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- Aguiar OD
- Aguilar I
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- Yang Y-C
- Yang Yang
- Yang Yi
- Yap MJ
- Yarbrough Z
- Yeh S-W
- Yelikar AB
- Yeung SMC
- Yeung TY
- Yokoyama J
- Yokozawa T
- Yoo J
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- Yuzurihara H
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- Zanolin M
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- Zhao C
- Zhao Yue
- Zhao Yuhang
- Zheng Y
- Zhong H
- Zhou R
- Zhu Z-H
- Zimmerman AB
- Zucker ME
- Zweizig J
- Álvarez-López S
- Publication venue
- The Astrophysical Journal
- Publication date
- 04/10/2024
- Field of study
Abstract
Despite the growing number of binary black hole coalescences confidently observed through gravitational waves so far, the astrophysical origin of these binaries remains uncertain. Orbital eccentricity is one of the clearest tracers of binary formation channels. Identifying binary eccentricity, however, remains challenging due to the limited availability of gravitational waveforms that include the effects of eccentricity. Here, we present observational results for a waveform-independent search sensitive to eccentric black hole coalescences, covering the third observing run (O3) of the LIGO and Virgo detectors. We identified no new high-significance candidates beyond those that have already been identified with searches focusing on quasi-circular binaries. We determine the sensitivity of our search to high-mass (total source-frame mass M > 70 M
⊙) binaries covering eccentricities up to 0.3 at 15 Hz emitted gravitational-wave frequency, and use this to compare model predictions to search results. Assuming all detections are indeed quasi-circular, for our fiducial population model, we place a conservative upper limit for the merger rate density of high-mass binaries with eccentricities 0 < e ≤ 0.3 at 16.9 Gpc−3 yr−1 at the 90% confidence level.</jats:p
Recommended from our members
Search for Eccentric Black Hole Coalescences during the Third Observing Run of LIGO and Virgo
- Author
- Abac AG
- Abbott R
- Abe H
- Acernese F
- Ackley K
- Adamcewicz C
- Adhicary S
- Adhikari N
- Adhikari RX
- Adkins VK
- Adya VB
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- Aguilar I
- Aiello L
- Ain A
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- Albanesi S
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- Wysocki DM
- Xiao L
- Xu VA
- Yaala M Ben
- Yadav N
- Yamamoto H
- Yamamoto K
- Yamamoto M
- Yamamoto T
- Yamamoto TS
- Yamamura S
- Yamazaki R
- Yan S
- Yang FW
- Yang KZ
- Yang L-C
- Yang Y-C
- Yang Yang
- Yang Yi
- Yap MJ
- Yarbrough Z
- Yeh S-W
- Yelikar AB
- Yeung SMC
- Yeung TY
- Yokoyama J
- Yokozawa T
- Yoo J
- Yu H
- Yuzurihara H
- Zadrożny A
- Zannelli AJ
- Zanolin M
- Zeeshan M
- Zelenova T
- Zendri J-P
- Zevin M
- Zhang J
- Zhang L
- Zhang R
- Zhang T
- Zhang Ya
- Zhang Yanqi
- Zhao C
- Zhao Yue
- Zhao Yuhang
- Zheng Y
- Zhong H
- Zhou R
- Zhu Z-H
- Zimmerman AB
- Zucker ME
- Zweizig J
- Álvarez-López S
- Publication venue
- The Astrophysical Journal
- Publication date
- 27/09/2024
- Field of study
Abstract
Despite the growing number of binary black hole coalescences confidently observed through gravitational waves so far, the astrophysical origin of these binaries remains uncertain. Orbital eccentricity is one of the clearest tracers of binary formation channels. Identifying binary eccentricity, however, remains challenging due to the limited availability of gravitational waveforms that include the effects of eccentricity. Here, we present observational results for a waveform-independent search sensitive to eccentric black hole coalescences, covering the third observing run (O3) of the LIGO and Virgo detectors. We identified no new high-significance candidates beyond those that have already been identified with searches focusing on quasi-circular binaries. We determine the sensitivity of our search to high-mass (total source-frame mass M > 70 M
⊙) binaries covering eccentricities up to 0.3 at 15 Hz emitted gravitational-wave frequency, and use this to compare model predictions to search results. Assuming all detections are indeed quasi-circular, for our fiducial population model, we place a conservative upper limit for the merger rate density of high-mass binaries with eccentricities 0 < e ≤ 0.3 at 16.9 Gpc−3 yr−1 at the 90% confidence level.</jats:p
Search for the charged-lepton-flavor-violating decay Z→eμ in pp collisions at s=13 TeV with the ATLAS detector
- Author
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- Yildiz HD
- Yin P
- Yorita K
- Yoshihara K
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- Yuan M
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- Yue X
- Zaazoua M
- Zabinski B
- Zacharis G
- Zagazeta LFG
- Zaid E
- Zakareishvili T
- Zakharchuk N
- Zambito S
- Zanzi D
- Zeitnitz C
- Zeißner SV
- Zeng JC
- Zenger DT
- Zenin O
- Zenz S
- Zerradi S
- Zerwas D
- Zhang B
- Zhang DF
- Zhang G
- Zhang J
- Zhang K
- Zhang L
- Zhang M
- Zhang R
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- Zhang X
- Zhang X
- Zhang Z
- Zhao P
- Zhao T
- Zhao Y
- Zhao Z
- Zhemchugov A
- Zheng Z
- Zhong D
- Zhou B
- Zhou C
- Zhou H
- Zhou N
- Zhou Y
- Zhu C
- Zhu CG
- Zhu H
- Zhu HL
- Zhu J
- Zhu Y
- Zhuang X
- Zhukov K
- Zhulanov V
- Zieminska D
- Zimine NI
- Zimmermann S
- 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
- American Physical Society (APS)
- Publication date
- 01/01/2023
- Field of study
Search for associated production of a Z boson with an invisibly decaying Higgs boson or dark matter candidates at s=13 TeV with the ATLAS detector
- Author
- Aad G
- Abbott B
- Abbott DC
- Abeling K
- Abhayasinghe DK
- Abidi SH
- Aboulhorma A
- Abramowicz H
- Abreu H
- Abud AA
- Abulaiti Y
- Acharya BS
- Achkar B
- Adam L
- Adamczyk L
- Adamek L
- Addepalli SV
- Adelman J
- Adiguzel A
- Adorni S
- Adye T
- Affolder AA
- Afik Y
- Agapopoulou C
- Agaras MN
- Agarwala J
- Aggarwal A
- Agheorghiesei C
- Aguilar-Saavedra JA
- Agullo PM
- Ahmad A
- Ahmadov F
- Ahmed WS
- Ai X
- Aielli G
- Aizenberg I
- Akatsuka S
- Akbiyik M
- Akesson TPA
- Akimov AV
- Al Khoury K
- Alberghi GL
- Albert J
- Albicocco P
- Alderweireldt S
- Aleksa M
- Aleksandrov IN
- Alexa C
- Alexopoulos T
- Alfonsi A
- Alfonsi F
- Alhroob M
- Ali B
- Ali S
- Aliev M
- Alimonti G
- Allaire C
- Allbrooke BMM
- Allport PP
- Aloisio A
- Alonso F
- Alpigiani C
- Alves FLL
- Alviggi MG
- Ambler A
- Ambroz L
- Amelung C
- Amidei D
- Amoroso S
- Amos KR
- Amrouche CS
- Ananiev V
- Anastopoulos C
- Andana RYG
- Andari N
- Andeen T
- Anders JK
- Andrean SY
- Andreazza A
- Anelli CR
- Angelidakis S
- Angerami A
- Anisenkov AV
- Annovi A
- Antel C
- Anthony MT
- Antipov E
- Antonelli M
- Antrim DJA
- Anulli F
- Aoki M
- Aparo MA
- Aranda CP
- Aranzabal N
- Araya ST
- Arcangeletti C
- Arce ATH
- Arena E
- Arguin JF
- Argyropoulos S
- Arling JH
- Armbruster AJ
- Armstrong A
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- Artoni G
- Asada H
- Asai K
- Asai S
- Asbah NA
- Asimakopoulou EM
- Asquith L
- Assahsah J
- Assamagan K
- Astalos R
- Astigarraga MEP
- Atkin RJ
- Atkinson M
- Atlay NB
- Atmani H
- Atmasiddha PA
- Augsten K
- Auricchio S
- Austrup VA
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- Ayoub MK
- Azuelos G
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- Bahilo JJL
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- Baroncelli A
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- Bartolini G
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- Burton CD
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- Casadei D
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- Casha AF
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- Castillo FL
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- Castro NF
- Catinaccio A
- Catmore JR
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- Cavaliere V
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- Celebi E
- Celli F
- Centonze MS
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- Cerqueira AS
- Cerri A
- Cerrito L
- Cerutti F
- Cervelli A
- Cetin SA
- Chadi Z
- Chakraborty D
- Chala M
- Chan J
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- Chan WY
- Chapman JD
- Chargeishvili B
- Charlton DG
- Charman TP
- Chatterjee M
- Chekanov S
- Chekulaev SV
- Chelkov GA
- Chen A
- Chen B
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- Chen H
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- Chen X
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- Cheplakov A
- Cheremushkina E
- Cherepanova E
- Cheu E
- Cheung K
- Chevalier L
- Chiarella V
- Chiarelli G
- Chiodini G
- Chisholm AS
- Chitan A
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- Christopher LD
- Chu MC
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- Ciesla KM
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- Ciocio A
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- Ciubotaru DA
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- Conventi F
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- Cooper-Sarkar AM
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- Corradi M
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- Corrigan EE
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- Crepe-Renaudin S
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- D'amen G
- D'Amico V
- D'Auria S
- D'Eramo L
- D'onofrio A
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- da Costa JBG
- Da Via C
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- Dai T
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- Dam M
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- Dao V
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- Dawson I
- de Andrade LM
- De Araujo MV
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- De Beurs M
- De Carvalho ALM
- De Castro S
- De Groot N
- de Jong P
- De K
- de la Hoz SG
- De la Torre H
- De Lima RT
- De Maria A
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- De Regie JBD
- de Renstrom PAB
- De Sa RCL
- De Salvo A
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- De Santo A
- De Sousa MJDS
- De Souza EEP
- Dedovich DV
- Degens J
- Deiana AM
- Del Peso J
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- Delitzsch CM
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- Della Pietra M
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- Delmastro M
- Delsart PA
- Demers S
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- Denisov SP
- Derendarz D
- Derkaoui JE
- Derue F
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- Dette K
- Deutsch C
- Deviveiros PO
- Di Bello FA
- Di Ciaccio A
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- Di Domenico A
- Di Donato C
- Di Girolamo A
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- Di Nardo R
- Diaconu C
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- Diaz MA
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- Dominguez LP
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- Zakharchuk N
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- Zanzi D
- Zeissner SV
- Zeitnitz C
- Zeng JC
- Zenger DT
- Zenin O
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- Zerradi S
- Zerwas D
- Zhang B
- Zhang DF
- Zhang G
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- Zhang X
- Zhang Z
- Zhao P
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- Zhao Z
- Zhemchugov A
- Zheng Z
- Zhong D
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- Zhu H
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- Zhu Y
- Zhuang X
- Zhukov K
- Zhulanov V
- Zieminska D
- Zimine NI
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- Ziolkowski M
- Zivkovic L
- Zoccoli A
- Zoch K
- Zorbas TG
- Zormpa O
- Zou W
- Zwalinski L
- Publication venue
- 'Elsevier BV'
- Publication date
- 01/01/2022
- Field of study
A search for invisible decays of the Higgs boson as well as searches for dark matter candidates, produced together with a leptonically decaying Z boson, are presented. The analysis is performed using proton−proton collisions at a centre-of-mass energy of 13 TeV, delivered by the LHC, corresponding to an integrated luminosity of 139 fb−1 and recorded by the ATLAS experiment. Assuming Standard Model cross-sections for ZH production, the observed (expected) upper limit on the branching ratio of the Higgs boson to invisible particles is found to be 19% (19%) at the 95% confidence level. Exclusion limits are also set for simplified dark matter models and two-Higgs-doublet models with an additional pseudoscalar mediator
A search for an unexpected asymmetry in the production of e + μ − and e − μ + pairs in proton–proton collisions recorded by the ATLAS detector at s = 13 TeV
- Author
- Aad G
- Abbott B
- Abbott DC
- Abeling K
- Abhayasinghe DK
- Abidi SH
- Aboulhorma A
- Abramowicz H
- Abreu H
- Abud AA
- Abulaiti Y
- Acharya BS
- Achkar B
- Adam L
- Adamczyk L
- Adamek L
- Addepalli SV
- Adelman J
- Adiguzel A
- Adorni S
- Adye T
- Affolder AA
- Afik Y
- Agapopoulou C
- Agaras MN
- Agarwala J
- Aggarwal A
- Agheorghiesei C
- Aguilar-Saavedra JA
- Agullo PM
- Ahmad A
- Ahmadov F
- Ahmed WS
- Ai X
- Aielli G
- Aizenberg I
- Akatsuka S
- Akbiyik M
- Akimov AV
- Alberghi GL
- Albert J
- Albicocco P
- Alderweireldt S
- Aleksa M
- Aleksandrov IN
- Alexa C
- Alexopoulos T
- Alfonsi A
- Alfonsi F
- Alhroob M
- Ali B
- Ali S
- Aliev M
- Alimonti G
- Allaire C
- Allbrooke BMM
- Allport PP
- Aloisio A
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- Alpigiani C
- Alves FLL
- Alviggi MG
- Ambler A
- Ambroz L
- Amelung C
- Amidei D
- Amoroso S
- Amos KR
- Amrouche CS
- Ananiev V
- Anastopoulos C
- Andana RYG
- Andari N
- Andeen T
- Anders JK
- Andrean SY
- Andreazza A
- Angelidakis S
- Angerami A
- Anisenkov AV
- Annovi A
- Antel C
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- Antrim DJA
- Anulli F
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- Aranda CP
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- Armbruster AJ
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- Asai K
- Asai S
- Asbah NA
- Asimakopoulou EM
- Asquith L
- Assahsah J
- Assamagan K
- Astalos R
- Astigarraga MEP
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- Atlay NB
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- Austrup VA
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- Ayoub MK
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- Bachiu A
- Backman F
- Badea A
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- Bahilo JJL
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- Baldin EM
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- Baltes LM
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- Bandyopadhyay A
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- Barberis D
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- Bates RL
- Batlamous S
- Batley JR
- Batool B
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- Birman M
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- Blumenthal J
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- Bobrovnikov VS
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- Borecka-Bielska HM
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- Burgard CD
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- Burghgrave B
- Burr JTP
- Burton CD
- Burzynski JC
- Busch EL
- Bussey PJ
- Butler JM
- Buttar CM
- Butterworth JM
- Buttinger W
- Buzykaev AR
- Bylund OB
- Büscher V
- Cabras G
- Caforio D
- Cai H
- Cairo VMM
- Cakir IT
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- Calace N
- Calafiura P
- Calderini G
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- Caloba LP
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- Camerlingo MT
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- Canale V
- Canesse A
- Cantero J
- Cao Y
- Capocasa F
- Capriles FGD
- Capua M
- Carbone A
- Cardarelli R
- Cardenas JCJ
- Cardillo F
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- Carlson BT
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- Casha AF
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- Castillo FL
- Castillo LRF
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- Catmore JR
- Cattai A
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- Celebi E
- Celli F
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- Chen A
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- Cheplakov A
- Cheremushkina E
- Cherepanova E
- Cheu E
- Cheung K
- Chevalier L
- Chiarella V
- Chiarelli G
- Chiodini G
- Chisholm AS
- Chitan A
- Chiu YH
- Chizhov MV
- Choi K
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- Chou Y
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- Chowdhury T
- Christopher LD
- Chu MC
- Chu X
- Chudoba J
- Chwastowski JJ
- Cieri D
- Ciesla KM
- Cindro V
- Cioară IA
- Ciocio A
- Cirotto F
- Citron ZH
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- Ciubotaru DA
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- Conventi F
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- Corpe LD
- Corradi M
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- Corriveau F
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- Czurylo MM
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- D'Amico V
- D'Auria S
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- D'onofrio A
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- D'uffizi M
- Da Costa AMMJ
- da Costa JBG
- Da Cruz E Silva CB
- Da Fonseca Pinto JV
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- Dam M
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- de Jong P
- de la Hoz SG
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- De Maria A
- De Pedis D
- de Renstrom PAB
- De Sa RCL
- De Salvo A
- De Sanctis U
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- De Sousa MJDCS
- De Souza EEP
- De K
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- Degens J
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- Dell'Acqua A
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- Deutsch C
- Deviveiros PO
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- Di Ciaccio A
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- Di Domenico A
- Di Donato C
- Di Girolamo A
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- Dodsworth D
- Doglioni C
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- Filthaut F
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- Fischer F
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- Fleck I
- Fleischmann P
- Flick T
- Flierl BM
- Flores L
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- Follega FM
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- Forland BC
- Formica A
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- Liberti B
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- Wilbern DJ
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- Winklmeier F
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- Yacoob S
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- Yamauchi H
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- Yan J
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- Yao W-M
- Yap YC
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- Yexley MR
- Yildiz HD
- Yin P
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- Yoshihara K
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- Yuan M
- Yuan R
- Yue X
- Zaazoua M
- Zabinski B
- Zacharis G
- Zagazeta LFG
- Zaid E
- Zaitsev AM
- Zakareishvili T
- Zakharchuk N
- Zambito S
- Zanzi D
- Zeitnitz C
- Zeißner SV
- Zeng JC
- Zenger DT
- Zenin O
- Zenz S
- Zerradi S
- Zerwas D
- Zhang B
- Zhang DF
- Zhang G
- Zhang J
- Zhang K
- Zhang L
- Zhang M
- Zhang R
- Zhang S
- Zhang X
- Zhang X
- Zhang Z
- Zhao P
- Zhao T
- Zhao Y
- Zhao Z
- Zhemchugov A
- Zheng Z
- Zhong D
- Zhou B
- Zhou C
- Zhou H
- Zhou N
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- Zhu C
- Zhu CG
- Zhu H
- Zhu HL
- Zhu J
- Zhu Y
- Zhuang X
- Zhukov K
- Zhulanov V
- Zieminska D
- Zimine NI
- Zimmermann S
- 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
- 'Elsevier BV'
- Publication date
- 01/07/2022
- Field of study
Measurements of Higgs boson production by gluon-gluon fusion and vector-boson fusion using H→WW*→eνμν decays in pp collisions at s=13 TeV with the ATLAS detector
- Author
- Aad G
- Abbott B
- Abbott DC
- Abeling K
- Abidi SH
- Aboulhorma A
- Abramowicz H
- Abreu H
- Abud AA
- Abulaiti Y
- Acharya BS
- Achkar B
- Adam L
- Adamczyk L
- Adamek L
- Addepalli SV
- Adelman J
- Adiguzel A
- Adorni S
- Adye T
- Affolder AA
- Afik Y
- Agaras MN
- Agarwala J
- Aggarwal A
- Agheorghiesei C
- Aguilar-Saavedra JA
- Agullo PM
- Ahmad A
- Ahmadov F
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- Aielli G
- Aizenberg I
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- Akimov AV
- Alberghi GL
- Albert J
- Albicocco P
- Alderweireldt S
- Aleksa M
- Aleksandrov IN
- Alexa C
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- Alfonsi A
- Alfonsi F
- Alhroob M
- Ali B
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- Aliev M
- Alimonti G
- Allaire C
- Allbrooke BMM
- Allport PP
- Aloisio A
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- Ames CG
- Amidei D
- Amoroso S
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- Anastopoulos C
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- Andeen T
- Anders JK
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- Angerami A
- Anisenkov AV
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- Antel C
- Anthony MT
- Antipov E
- Antonelli M
- Antrim DJA
- Anulli F
- Aoki M
- Aparo MA
- Appelt C
- Aranda CP
- Aranzabal N
- Araya ST
- Arcangeletti C
- Arce ATH
- Arena E
- Arguin J-F
- Argyropoulos S
- Arling J-H
- Armbruster AJ
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- de Andrade Filho LM
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- Zhemchugov A
- Zheng Z
- Zhong D
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- Zwalinski L
- Åkesson TPA
- Öncel ÖO
- Ženiš T
- Živković L
- Publication venue
- American Physical Society (APS)
- Publication date
- 01/01/2023
- Field of study
Higgs boson production via gluon-gluon fusion and vector-boson fusion in proton-proton collisions is measured in the
H
→
W
W
∗
→
e
ν
μ
ν
decay channel. The Large Hadron Collider delivered proton-proton collisions at a center-of-mass energy of 13 TeV between 2015 and 2018, which were recorded by the ATLAS detector, corresponding to an integrated luminosity of
139
fb
−
1
. The total cross sections for Higgs boson production by gluon-gluon fusion and vector-boson fusion times the
H
→
W
W
∗
branching ratio are measured to be
12.0
±
1.4
and
0.75
+
0.19
−
0.16
pb
, respectively, in agreement with the Standard Model predictions of
10.4
±
0.6
and
0.81
±
0.02
pb
. Higgs boson production is further characterized through measurements of Simplified Template Cross Sections in a total of 11 kinematic fiducial regions
Recommended from our members
Observation of Gravitational Waves from the Coalescence of a 2.5–4.5 M <sub>⊙</sub> Compact Object and a Neutron Star
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- Villarreal F Llamas
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- Vinet J-Y
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- von Wrangel JSA
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- Wajid A
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- Wofford JK
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- Wu H
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- Wysocki DM
- Xu VA
- Xu Y
- Yaala M Ben
- Yadav N
- Yamamoto H
- Yamamoto K
- Yamamoto T
- Yamamoto TS
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- Yamazaki R
- Yan S
- Yan T
- Yang F
- Yang FW
- Yang KZ
- Yang Y
- Yarbrough Z
- Yasui H
- Yeh S-W
- Yelikar AB
- Yin X
- Yokoyama J
- Yokozawa T
- Yoo J
- Yu H
- Yuan S
- Yuzurihara H
- Zadrożny A
- Zanolin M
- Zeeshan M
- Zelenova T
- Zendri J-P
- Zeoli M
- Zerrad M
- Zevin M
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- Zhang R
- Zhang T
- Zhang Y
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- Zheng Y
- Zhong H
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- Zhu X-J
- Zhu Z-H
- Zimmerman AB
- Zucker ME
- Zweizig J
- Publication venue
- The Astrophysical Journal Letters
- Publication date
- 26/07/2024
- Field of study
Abstract
We report the observation of a coalescing compact binary with component masses 2.5–4.5 M
⊙ and 1.2–2.0 M
⊙ (all measurements quoted at the 90% credible level). The gravitational-wave signal GW230529_181500 was observed during the fourth observing run of the LIGO–Virgo–KAGRA detector network on 2023 May 29 by the LIGO Livingston observatory. The primary component of the source has a mass less than 5 M
⊙ at 99% credibility. We cannot definitively determine from gravitational-wave data alone whether either component of the source is a neutron star or a black hole. However, given existing estimates of the maximum neutron star mass, we find the most probable interpretation of the source to be the coalescence of a neutron star with a black hole that has a mass between the most massive neutron stars and the least massive black holes observed in the Galaxy. We provisionally estimate a merger rate density of
55
−
47
+
127
Gpc
−
3
yr
−
1
for compact binary coalescences with properties similar to the source of GW230529_181500; assuming that the source is a neutron star–black hole merger, GW230529_181500-like sources may make up the majority of neutron star–black hole coalescences. The discovery of this system implies an increase in the expected rate of neutron star–black hole mergers with electromagnetic counterparts and provides further evidence for compact objects existing within the purported lower mass gap.</jats:p