341 research outputs found
Search for new phenomena in final states with an energetic jet and large missing transverse momentum in pp collisions at √ s = 8 TeV with the ATLAS detector
- Author
- Aad G
- Abbott B
- Abbott DC
- Abeling K
- Abhayasinghe DK
- Abidi SH
- AbouZeid OS
- Abraham NL
- Abramowicz H
- Abreu H
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- Abulaiti Y
- Acharya BS
- Achkar B
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- Zhemchugov A
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- Zwalinski L
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2015
- Field of study
Results of a search for new phenomena in final states with an energetic jet and large missing transverse momentum are reported. The search uses 20.3 fb−1 of √ s = 8 TeV data collected in 2012 with the ATLAS detector at the LHC. Events are required to have at least one jet with pT > 120 GeV and no leptons. Nine signal regions are considered with increasing missing transverse momentum requirements between Emiss T > 150 GeV and Emiss T > 700 GeV. Good agreement is observed between the number of events in data and Standard Model expectations. The results are translated into exclusion limits on models with either large extra spatial dimensions, pair production of weakly interacting dark matter candidates, or production of very light gravitinos in a gauge-mediated supersymmetric model. In addition, limits on the production of an invisibly decaying Higgs-like boson leading to similar topologies in the final state are presente
Muon reconstruction and identification efficiency in ATLAS using the full Run 2 pp collision data set at \sqrt{s}=13 TeV
- Author
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- Zhemchugov A
- Zheng Z
- Zhong D
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- Zieminska D
- Zimine NI
- Zimmermann S
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- Ziolkowski M
- Zivkovic L
- Zobernig G
- Zoccoli A
- Zoch K
- Zorbas TG
- Zou R
- Zwalinski L
- Publication venue
- 'Springer Fachmedien Wiesbaden GmbH'
- Publication date
- 01/01/2021
- Field of study
This article documents the muon reconstruction and identification efficiency obtained by the ATLAS experiment for 139 \hbox {fb}^{-1} of pp collision data at \sqrt{s}=13 TeV collected between 2015 and 2018 during Run 2 of the LHC. The increased instantaneous luminosity delivered by the LHC over this period required a reoptimisation of the criteria for the identification of prompt muons. Improved and newly developed algorithms were deployed to preserve high muon identification efficiency with a low misidentification rate and good momentum resolution. The availability of large samples of Z\rightarrow \mu \mu and J/\psi \rightarrow \mu \mu decays, and the minimisation of systematic uncertainties, allows the efficiencies of criteria for muon identification, primary vertex association, and isolation to be measured with an accuracy at the per-mille level in the bulk of the phase space, and up to the percent level in complex kinematic configurations. Excellent performance is achieved over a range of transverse momenta from 3 GeV to several hundred GeV, and across the full muon detector acceptance of |\eta |<2.7
Dijet Resonance Search with Weak Supervision Using root S=13 TeV pp Collisions in the ATLAS Detector
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- Abbott B
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- Abhayasinghe DK
- Abidi SH
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- Zhemchugov A
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- Zinonos Z
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- Zu Theenhausen HM
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- Publication venue
- AMER PHYSICAL SOC
- Publication date
- 25/09/2020
- Field of study
This Letter describes a search for narrowly resonant new physics using a machine-learning anomaly
detection procedure that does not rely on signal simulations for developing the analysis selection. Weakly
supervised learning is used to train classifiers directly on data to enhance potential signals. The targeted
topology is dijet events and the features used for machine learning are the masses of the two jets. The
resulting analysis is essentially a three-dimensional search A → BC, for mA ∼ OðTeVÞ, mB; mC ∼
Oð100 GeVÞ and B, C are reconstructed as large-radius jets, without paying a penalty associated with
a large trials factor in the scan of the masses of the two jets. The full run 2 ffiffi
s p ¼ 13 TeV pp collision
dataset of 139 fb−1 recorded by the ATLAS detector at the Large Hadron Collider is used for the search.
There is no significant evidence of a localized excess in the dijet invariant mass spectrum between 1.8 and
8.2 TeV. Cross-section limits for narrow-width A, B, and C particles vary with mA, mB, and mC. For
example, when mA ¼ 3 TeV and mB ≳ 200 GeV, a production cross section between 1 and 5 fb is
excluded at 95% confidence level, depending on mC. For certain masses, these limits are up to 10 times
more sensitive than those obtained by the inclusive dijet search. These results are complementary to the
dedicated searches for the case that B and C are standard model boson
Erratum: Measurement of angular and momentum distributions of charged particles within and around jets in Pb + Pb and pp collisions at √sNN = 5.02 TeV with the ATLAS detector [Phys. Rev. C 100 , 064901 (2019)]
- Author
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- Campoverde A
- Canale V
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- Pogrebnyak I
- Pohl D
- Pokharel I
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- Sano Y
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- Sawyer C
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- Scanlon T
- Schaarschmidt J
- Schacht P
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- Schegelsky Va
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- Schoening A
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- Schramm S
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- Schumacher M
- Schumm Ba
- Schune P
- Schwartzman A
- Schwarz Ta
- Schwemling P
- Schwienhorst R
- Sciandra A
- Sciolla G
- Scodeggio M
- Scornajenghi M
- Scuri F
- Scutti F
- Scyboz Lm
- Sebastiani Cd
- Seema P
- Seidel Sc
- Seiden A
- Seidlitz Bd
- Seiss T
- Seixas Jm
- Sekhniaidze G
- Sekhon K
- Sekula Sj
- Semprini-Cesari N
- Sen S
- Senkin S
- Serfon C
- Serin L
- Serkin L
- Sessa M
- Severini H
- Sfiligoj T
- Sforza F
- Sfyrla A
- Shabalina E
- Shahinian Jd
- Shaikh Nw
- Shaked Renous D
- Shan Ly
- Shang R
- Shank Jt
- Shapiro M
- Sharma A
- Sharma As
- Shatalov Pb
- Shaw K
- Shaw Sm
- Shcherbakova A
- Shehade M
- Shen Y
- Sherafati N
- Sherman Ad
- Sherwood P
- Shi L
- Shimizu S
- Shimmin Co
- Shimogama Y
- Shimojima M
- Shipsey Ipj
- Shirabe S
- Shiyakova M
- Shlomi J
- Shmeleva A
- Shochet Mj
- Shojaii J
- Shope Dr
- Shrestha S
- Shrif Em
- Shulga E
- Sicho P
- Sickles Am
- Sidebo Pe
- Sideras Haddad E
- Sidiropoulou O
- Sidoti A
- Siegert F
- Sijacki D
- Silva Oliveira Mv
- Silva Mj
- Silverstein Sb
- Simion S
- Simioni E
- Simoniello R
- Simsek S
- Sinervo P
- Sinetckii V
- Sinev Nb
- Sioli M
- Siral I
- Sivoklokov Sy
- Sjolin J
- Skorda E
- Skubic P
- Slawinska M
- Sliwa K
- Slovak R
- Smakhtin V
- Smart Bh
- Smiesko J
- Smirnov N
- Smirnov Sy
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- Smirnova Ln
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- Smith Jw
- Smizanska M
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- Smykiewicz A
- Snesarev Aa
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- Sobie R
- Soffer A
- Sogaard A
- Sohns F
- Solans Sanchez Ca
- Soldatov Ey
- Soldevila U
- Solodkov Aa
- Soloshenko A
- Solovyanov Ov
- Solovyev V
- Sommer P
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- Song W
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- Sopczak A
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- Sotiropoulou Cl
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- Soualah R
- Soukharev Am
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- Spangenberg M
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- Spighi R
- Spigo G
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- Spousta M
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- Stanecka E
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- Stockton Mc
- Stoicea G
- Stolarski M
- Stonjek S
- Straessner A
- Strandberg J
- Strandberg S
- Strauss M
- Strizenec P
- Strohmer R
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- Stroynowski R
- Strubig A
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- Tapprogge S
- Tarek Abouelfadl Mohamed A
- Tarem S
- Tariq K
- Tarna G
- Tartarelli Gf
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- Tashiro T
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- Tayalati Y
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- Teixeira-Dias P
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- Teoh Jj
- Terada S
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- Terron J
- Terzo S
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- Teuscher Rj
- Thais Sj
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- Thiele F
- Thomas Dw
- Thomas Jo
- Thomas Jp
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- Thompson Pd
- Thomsen La
- Thomson E
- Thorpe Ej
- Ticse Torres Re
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- Tokar S
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- Tolley E
- Tomiwa Kg
- Tomoto M
- Tompkins L
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- Trischuk W
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- Tsukerman Ii
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- Tudorache A
- Tudorache V
- Tulbure Tt
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- Turchikhin S
- Turgeman D
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- Vivarelli I
- Vogel M
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- Wanotayaroj C
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- Wengler T
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- Whallon Nl
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- Whitmore Bw
- Wiedenmann W
- Wielers M
- Wieseotte N
- Wiglesworth C
- Wiik-Fuchs Lam
- Wilk F
- Wilkens Hg
- Wilkins Lj
- Williams Hh
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- Willis C
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- Wilson Ja
- Wingerter-Seez I
- Winkels E
- Winklmeier F
- Winston Oj
- Winter Bt
- Wittgen M
- Wobisch M
- Wolf A
- Wolf Tmh
- Wolff R
- Wolker Rw
- Wollrath J
- Wolter Mw
- Wolters H
- Wong Vws
- Woods Nl
- Worm Sd
- Wosiek Bk
- Wozniak Kw
- Wraight K
- Wu Sl
- Wu X
- Wu Y
- Wyatt Tr
- Wynne Bm
- Xella S
- Xi Z
- Xia L
- Xiao X
- Xiotidis I
- Xu D
- Xu H
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- Xu T
- Xu W
- Xu Z
- Xu Z
- Yabsley B
- Yacoob S
- Yajima K
- Yallup Dp
- Yamaguchi D
- Yamaguchi Y
- Yamamoto A
- Yamatani M
- Yamazaki T
- Yamazaki Y
- Yan Z
- Yang Hj
- Yang Ht
- Yang S
- Yang X
- Yang Y
- Yao W-
- Yap Yc
- Yasu Y
- Yatsenko E
- Ye J
- Ye S
- Yeletskikh I
- Yexley Mr
- Yigitbasi E
- Yorita K
- Yoshihara K
- Young C
- Young Cjs
- Yu J
- Yuan R
- Yue X
- Yuen Spy
- Zaazoua M
- Zabinski B
- Zacharis G
- Zaffaroni E
- Zahreddine J
- Zaitsev Am
- Zakareishvili T
- Zakharchuk N
- Zambito S
- Zanzi D
- Zaripovas Dr
- Zeissner Sv
- Zeitnitz C
- Zemaityte G
- Zeng Jc
- Zenin O
- Zenis T
- Zerwas D
- Zgubic M
- Zhang B
- Zhang Df
- Zhang G
- Zhang H
- Zhang J
- Zhang L
- Zhang L
- Zhang M
- Zhang R
- Zhang X
- Zhang Y
- Zhang Z
- Zhang Z
- Zhao P
- Zhao Y
- Zhao Z
- Zhemchugov A
- Zheng Z
- Zhong D
- Zhou B
- Zhou C
- Zhou M
- Zhou Ms
- 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
- Zinonos Z
- Ziolkowski M
- Zivkovic L
- Zobernig G
- Zoccoli A
- Zoch K
- Zorbas Tg
- Zou R
- Zwalinski L
- Publication venue
- American Physical Society
- Publication date
- 01/01/2020
- Field of study
Measurement of single top-quark production in association with a W boson in the single-lepton channel at \sqrt{s} = 8\,\text {TeV} with the ATLAS detector
- Author
- Aad G
- Abbott B
- Abbott DC
- Abeling K
- Abhayasinghe DK
- Abidi SH
- AbouZeid OS
- Abraham NL
- Abramowicz H
- Abreu H
- Abud AA
- Abulaiti Y
- Acharya BS
- Achkar B
- Adachi S
- Adam L
- Adamczyk L
- Adamek L
- Adelman J
- Adersberger M
- Adiguzel A
- Adorni S
- Adye T
- Affolder AA
- Afik Y
- Agapopoulou C
- Agaras MN
- Aggarwal A
- Agheorghiesei C
- Aguilar-Saavedra JA
- Ahmadov F
- Ahmed WS
- Ai X
- Aielli G
- Akatsuka S
- Akesson TPA
- Akilli E
- Akimov A
- Al Khoury K
- Alberghi GL
- Albert J
- Alderweireldt S
- Aleksa M
- Aleksandrov IN
- Alexa C
- Alexandre D
- Alexopoulos T
- Alfonsi A
- Alfonsi F
- Alhroob M
- Ali B
- Aliev M
- Alimonti G
- Alison J
- Alkire SP
- Allaire C
- Allbrooke BMM
- Allen BW
- Allport PP
- Aloisio A
- Alonso A
- Alonso F
- Alpigiani C
- Alshehri AA
- Alvarez Estevez M
- Alvarez Piqueras D
- Alviggi MG
- Ambler A
- Ambroz L
- Amelung C
- Amidei D
- Amoroso S
- Amrouche CS
- An F
- Anastopoulos C
- Andari N
- Andeen T
- Anders CF
- Anders JK
- Andreazza A
- Andrei V
- Anelli CR
- Angelidakis S
- Angerami A
- Anisenkov A
- Annovi A
- Antel C
- Anthony MT
- Antipov E
- Antonelli M
- Antrim DJA
- Anulli F
- Aoki M
- Aparisi Pozo JA
- Arabidze G
- Araque JP
- Araya ST
- Arcangeletti C
- Arce ATH
- Arduh FA
- Arguin J-F
- Argyropoulos S
- Arling J-H
- Armadans RC
- Armbruster AJ
- Armstrong A
- Arnaez O
- Arnold H
- Artoni G
- Artz S
- Asai S
- Asbah N
- Asimakopoulou EM
- Asquith L
- Assahsah J
- Assamagan K
- Astalos R
- Astigarraga MEP
- Atkin RJ
- Atkinson M
- Atlay NB
- Atmani H
- Augsten K
- Avolio G
- Avramidou R
- Ayoub MK
- Azoulay AM
- Azuelos G
- Bachacou H
- Bachas K
- Backes M
- Backman F
- Bagnaia P
- Bahmani M
- Bahrasemani H
- Bailey AJ
- Bailey VR
- Baines JT
- Bajic M
- Bakalis C
- Baker OK
- Bakker PJ
- Balaji S
- Baldin EM
- Balek P
- Balli F
- Balunas WK
- Balz J
- Banas E
- Bandyopadhyay A
- Banerjee S
- Bannoura AAE
- Barak L
- Barbe WM
- Barberio EL
- Barberis D
- Barbero M
- Barbour G
- Barillari T
- Barisits M-S
- Barkeloo J
- Barklow T
- Barnea R
- Barnes SL
- Barnett BM
- Barnett RM
- Barnovska-Blenessy Z
- Baroncelli A
- Barone G
- Barr AJ
- Barreiro F
- Barsov S
- Bartoldus R
- Bartolini G
- Barton AE
- Bartos P
- Basalaev A
- Bassalat A
- Basso MJ
- Bates RL
- Batlamous S
- Batley JR
- Batool B
- Battaglia M
- Bauce M
- Bauer F
- Bauer KT
- Bawa HS
- Beacham JB
- Beau T
- Beauchemin PH
- Becherer F
- Bechtle P
- Beck HC
- Beck HP
- Becker K
- Becker M
- Becot C
- Beddall A
- Beddall AJ
- Bednyakov VA
- Bedognetti M
- Bee CP
- Beermann TA
- Begalli M
- Begel M
- Behera A
- Behr JK
- Beisiegel F
- Bell AS
- Bella G
- Bella LA
- Bellagamba L
- Bellerive A
- Bellos P
- Beloborodov K
- Belotskiy K
- Belyaev NL
- Benchekroun D
- Benekos N
- Benhammou Y
- Benjamin DP
- Benoit M
- Bensinger JR
- Bentvelsen S
- Beresford L
- Beretta M
- Berge D
- Berger N
- Bergmann B
- Bergsten LJ
- Beringer J
- Berlendis S
- Berlingen JM
- Bernardi G
- Bernius C
- Bernlochner FU
- Berry T
- Bertella C
- Bertram IA
- Besson N
- Bethani A
- Bethke S
- Betti A
- Bevan AJ
- Beyer J
- Bhattacharya DS
- Bhattarai P
- Bi R
- Bianchi RM
- Biebel O
- Biedermann D
- Bielski R
- Bierwagen K
- Biesuz N
- Biglietti M
- Billoud TR
- Bindi M
- Bingul A
- Bini C
- Biondi S
- Birman M
- Bisanz T
- Biswal JP
- Biswas D
- Bitadze A
- Bittrich C
- Bjorke K
- Black KM
- Blazek T
- Bloch I
- Blocker C
- Blue A
- Blumenschein U
- Bobbink GJ
- Bobrovnikov VS
- Bocchetta SS
- Bocci A
- Boeriu OEV
- Bogavac D
- Bogdanchikov AG
- Bohm C
- Boisvert V
- Bokan P
- Bold T
- Boldyrev AS
- Bolz AE
- Bomben M
- Bona M
- Bonilla JS
- Boonekamp M
- Booth CD
- Borecka-Bielska HM
- Borisov A
- Borissov G
- Bortfeldt J
- Bortoletto D
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- Yildiz HD
- Yorita K
- Yoshihara K
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- Yuen SPY
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- Zacharis G
- Zaffaroni E
- Zahreddine J
- Zaitsev AM
- Zakareishvili T
- Zakharchuk N
- Zambito S
- Zanzi D
- Zaripovas DR
- Zeissner S
- Zeitnitz C
- Zemaityte G
- Zeng JC
- Zenin O
- Zenis T
- Zerwas D
- Zhang B
- Zhang DF
- Zhang G
- Zhang H
- Zhang J
- Zhang L
- Zhang L
- Zhang M
- Zhang R
- Zhang X
- Zhang Y
- Zhang Z
- Zhang Z
- Zhao P
- Zhao Y
- Zhao Z
- Zhemchugov A
- Zheng Z
- Zhong D
- Zhou B
- Zhou C
- Zhou M
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- 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 N
- Zimmermann S
- Zinonos Z
- Ziolkowski M
- Zobernig G
- Zoccoli A
- Zoch K
- Zorbas TG
- Zou R
- Zu Theenhausen HM
- Zwalinski L
- Publication venue
- 'Springer Fachmedien Wiesbaden GmbH'
- Publication date
- 01/01/2021
- Field of study
The production cross-section of a top quark in association with a W boson is measured using proton–proton collisions at \sqrt{s} = 8\,\text {TeV}. The dataset corresponds to an integrated luminosity of 20.2\,\text {fb}^{-1}, and was collected in 2012 by the ATLAS detector at the Large Hadron Collider at CERN. The analysis is performed in the single-lepton channel. Events are selected by requiring one isolated lepton (electron or muon) and at least three jets. A neural network is trained to separate the tW signal from the dominant t{\bar{t}} background. The cross-section is extracted from a binned profile maximum-likelihood fit to a two-dimensional discriminant built from the neural-network output and the invariant mass of the hadronically decaying W boson. The measured cross-section is \sigma _{tW} = 26 \pm 7\,\text {pb}, in good agreement with the Standard Model expectation
Performance of the upgraded PreProcessor of the ATLAS Level-1 Calorimeter Trigger
- Author
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- Castillo Gimenez V
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- Zhemchugov A
- Zheng Z
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- Zhukov K
- Zhulanov V
- Zieminska D
- Zimine NI
- Zimmermann S
- Zinonos Z
- Ziolkowski M
- Zivkovic L
- Zobernig G
- Zoccoli A
- Zoch K
- Zorbas TG
- Zou R
- Zu Theenhausen H Meyer
- Zwalinski L
- Publication venue
- 'IOP Publishing'
- Publication date
- 01/01/2020
- Field of study
The PreProcessor of the ATLAS Level-1 Calorimeter Trigger prepares the analogue trigger signals sent from the ATLAS calorimeters by digitising, synchronising, and calibrating them to reconstruct transverse energy deposits, which are then used in further processing to identify event features. During the first long shutdown of the LHC from 2013 to 2014, the central components of the PreProcessor, the Multichip Modules, were replaced by upgraded versions that feature modern ADC and FPGA technology to ensure optimal performance in the high pile-up environment of LHC Run 2. This paper describes the features of the newMultichip Modules along with the improvements to the signal processing achieved.ANPCyTYerPhI, ArmeniaAustralian Research CouncilBMWFW, AustriaAustrian Science Fund (FWF)Azerbaijan National Academy of Sciences (ANAS)SSTC, BelarusNational Council for Scientific and Technological Development (CNPq)Fundacao de Amparo a Pesquisa do Estado de Sao Paulo (FAPESP)Natural Sciences and Engineering Research Council of CanadaCanada Foundation for InnovationNational Natural Science Foundation of China (NSFC)Departamento Administrativo de Ciencia, Tecnología e Innovación ColcienciasMinistry of Education, Youth & Sports - Czech Republic
Czech Republic GovernmentCzech Republic GovernmentDNRF, DenmarkDanish Natural Science Research CouncilCentre National de la Recherche Scientifique (CNRS)CEA-DRF/IRFU, FranceFederal Ministry of Education & Research (BMBF)Max Planck SocietyGreek Ministry of Development-GSRTRGC and Hong Kong SAR, ChinaIsrael Science FoundationBenoziyo Center, IsraelIstituto Nazionale di Fisica Nucleare (INFN)Ministry of Education, Culture, Sports, Science and Technology, Japan (MEXT)Ministry of Education, Culture, Sports, Science and Technology, Japan (MEXT)
Japan Society for the Promotion of ScienceCNRST, MoroccoRCN, NorwayPortuguese Foundation for Science and TechnologyMNE/IFA, RomaniaMES of RussiaMESTD, SerbiaMSSR, SlovakiaSlovenian Research Agency - SloveniaMIZS, SloveniaSpanish GovernmentSRC, SwedenWallenberg Foundation, SwedenSNSF Geneva, SwitzerlandMinistry of Science and Technology, TaiwanMinistry of Energy & Natural Resources - TurkeyScience & Technology Facilities Council (STFC)United States Department of Energy (DOE)National Science Foundation (NSF)BCKDF, CanadaCANARIE, CanadaCRC, CanadaEuropean Research Council (ERC)European Union (EU)French National Research Agency (ANR)German Research Foundation (DFG)Alexander von Humboldt FoundationGreek NSRF, GreeceBSF-NSF, IsraelGerman-Israeli Foundation for Scientific Research and DevelopmentLa Caixa Banking Foundation, SpainCERCA Programme Generalitat de Catalunya, SpainPROMETEO, SpainGenT Programmes Generalitat Valenciana, SpainGoran Gustafssons Stiftelse, SwedenRoyal Society of LondonLeverhulme TrustNRC, CanadaCERNANID, ChileChinese Academy of SciencesMinistry of Science and Technology, ChinaSRNSFG, GeorgiaHGF, GermanyNetherlands Organization for Scientific Research (NWO)
Netherlands GovernmentMinistry of Science and Higher Education, PolandNCN, PolandNRCKI, Russia FederationJINRDST/NRF, South AfricaSERI, Geneva, SwitzerlandCantons of Bern and Geneva, SwitzerlandCompute Canada, CanadaHorizon 2020Marie Sklodowska-Curie ActionsEuropean Cooperation in Science and Technology (COST)EU-ESF, Greec
Search for long-lived neutral particles produced in pp collisions at √s = 13 TeV decaying into displaced hadronic jets in the ATLAS inner detector and muon spectrometer
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- Aad G
- Abbott B
- Abbott DC
- Abeling K
- Abhayasinghe DK
- Abidi SH
- AbouZeid OS
- Abraham NL
- Abramowicz H
- Abreu H
- Abud AA
- Abulaiti Y
- Acharya BS
- Achkar B
- Adachi S
- Adam L
- Adamczyk L
- Adamek L
- Adelman J
- Adersberger M
- Adiguzel A
- Adorni S
- Adye T
- Affolder AA
- Afik Y
- Agapopoulou C
- Agaras MN
- Aggarwal A
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- Aguilar-Saavedra JA
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- Ahmed WS
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- Akatsuka S
- Akesson TPA
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- Alberghi GL
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- Aleksandrov IN
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- Xella S
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- Xiao X
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- Xu D
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- Yabsley B
- Yacoob S
- Yajima K
- Yallup DP
- Yamaguchi N
- Yamaguchi Y
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- Yildiz HD
- Yorita K
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- Yuen SPY
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- Zahreddine J
- Zaitsev AM
- Zakareishvili T
- Zakharchuk N
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- Zemaityte G
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- Zhao Y
- Zhao Z
- Zhemchugov A
- Zheng Z
- Zhong D
- Zhou B
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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 N
- Zimmermann S
- Zinonos Z
- Ziolkowski M
- Zivkovic L
- Zobernig G
- Zoccoli A
- Zoch K
- Zorbas TG
- Zou R
- Zu Theenhausen HM
- Zwalinski L
- Publication venue
- AMER PHYSICAL SOC
- Publication date
- 01/03/2020
- Field of study
A search is presented for pair production of long-lived neutral particles using
33
fb
−
1
of
√
s
=
13
TeV
proton–proton collision data, collected during 2016 by the ATLAS detector at the LHC. This search focuses on a topology in which one long-lived particle decays in the ATLAS inner detector and the other decays in the muon spectrometer. Special techniques are employed to reconstruct the displaced tracks and vertices in the inner detector and in the muon spectrometer. One event is observed that passes the full event selection, which is consistent with the estimated background. Limits are placed on scalar boson propagators with masses from 125 GeV to 1000 GeV decaying into pairs of long-lived hidden-sector scalars with masses from 8 GeV to 400 GeV. The limits placed on several low-mass scalars extend previous exclusion limits in the range of proper lifetimes
c
τ
from 5 cm to 1 m
Measurements of Higgs bosons decaying to bottom quarks from vector boson fusion production with the ATLAS experiment at √=13TeV
- Author
- Aad G
- Abbott B
- Abbott DC
- Abeling K
- Abhayasinghe DK
- Abidi SH
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- Zwalinski L
- Åkesson TPA
- Öncel ÖO
- Ženiš T
- Živković L
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 23/06/2021
- Field of study
The paper presents a measurement of the Standard Model Higgs Boson decaying to b-quark pairs in the vector boson fusion (VBF) production mode. A sample corresponding to 126 fb−1 of s√=13TeV proton–proton collision data, collected with the ATLAS experiment at the Large Hadron Collider, is analyzed utilizing an adversarial neural network for event classification. The signal strength, defined as the ratio of the measured signal yield to that predicted by the Standard Model for VBF Higgs production, is measured to be 0.95+0.38−0.36 , corresponding to an observed (expected) significance of 2.6 (2.8) standard deviations from the background only hypothesis. The results are additionally combined with an analysis of Higgs bosons decaying to b-quarks, produced via VBF in association with a photon
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
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- Zenger DT
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- Zhemchugov A
- Zheng Z
- Zhong D
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- Zhukov K
- Zhulanov V
- Zieminska D
- Zimine NI
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- Zorbas TG
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- Zou W
- Zwalinski L
- 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.]
Search for long-lived, massive particles in events with a displaced vertex and a muon with large impact parameter in pp collisions at root s=13 TeV with the ATLAS detector
- Author
- Aad G
- Abbott B
- Abbott DC
- Abeling K
- Abhayasinghe DK
- Abidi SH
- AbouZeid OS
- Abraham NL
- Abramowicz H
- Abreu H
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- Abulaiti Y
- Acharya BS
- Achkar B
- Adachi S
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- Adelman J
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- Adiguzel A
- Adorni S
- Adye T
- Affolder AA
- Afik Y
- Agapopoulou C
- Agaras MN
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- Ahmed WS
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- Akesson TPA
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- Alberghi GL
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- Aleksandrov IN
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- Urban J
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- Usai G
- Uysal Z
- Vacek V
- Vachon B
- Vadla KOH
- Vaidya A
- Valderanis C
- Vale MAB
- Vale TD
- Valente M
- Valentinetti S
- Valero A
- Valery L
- Vallance RA
- Vallier A
- Van Daalen TR
- Van Gemmeren P
- Van Vulpen I
- Vanadia M
- Vandelli W
- Vandewall ER
- Vaniachine A
- Vannicola D
- Vari R
- Varnes EW
- Varni C
- Varol T
- Varouchas D
- Varvell KE
- Vasile ME
- Vasquez GA
- Vasquez JG
- Vazeille F
- Vazquez Furelos D
- Vazquez CJB
- Vazquez JGP
- Veatch J
- Vecchio V
- Veen MJ
- Veloce LM
- Veloso F
- Veneziano S
- Ventura A
- Venturi N
- Verbytskyi A
- Vercesi V
- Verducci M
- Vergara JCR
- Vergis C
- Verkerke W
- Vermeulen AT
- Vermeulen JC
- Verzini MJA
- Vetterli MC
- Via C
- Vickey T
- Viehhauser GHA
- Vigani L
- Villa M
- Vilucchi E
- Vincter MG
- Virdee GS
- Vishwakarma A
- Vittori C
- Vivarelli I
- Vogel M
- Vokac P
- von Buddenbrock SE
- Von Toerne E
- Vorobel V
- Vorobev K
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- Vossebeld JH
- Vozak M
- Vranjes N
- Vrba V
- Vreeswijk M
- Vuillermet R
- Vukotic I
- Wagner P
- Wagner W
- Wagner-Kuhr J
- Wahdan S
- Wahlberg H
- Walbrecht VM
- Walder J
- Walker R
- Walker SD
- Walkowiak W
- Wallangen V
- Wang AM
- Wang C
- Wang C
- Wang F
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- Wang J
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- Warburton A
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- Wardrope DR
- Warrack N
- Washbrook A
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- Webb AF
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- Weidberg AR
- Weingarten J
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- Weston TD
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- Whitmore BW
- Wiedenmann W
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- Yamamoto A
- Yamatani M
- Yamazaki T
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- Yao W-M
- Yap YC
- Yasu Y
- Yatsenko E
- Ye J
- Ye S
- Yeletskikh I
- Yexley MR
- Yigitbasi E
- Yildiz HD
- Yorita K
- Yoshihara K
- Young C
- Young CJS
- Yu J
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- Yue X
- Yuen SPY
- Zaazoua M
- Zabinski B
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- Zaffaroni E
- Zahreddine J
- Zaitsev AM
- Zakareishvili T
- Zakharchuk N
- Zambito S
- Zanzi D
- Zaripovas DR
- Zeissner S
- Zeitnitz C
- Zemaityte G
- Zeng JC
- Zenin O
- Zenis T
- Zerwas D
- Zgubic M
- Zhang B
- Zhang DF
- Zhang G
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- Zhang J
- Zhang L
- Zhang L
- Zhang M
- Zhang R
- Zhang X
- Zhang Y
- Zhang Z
- Zhang Z
- Zhao P
- Zhao Y
- Zhao Z
- Zhemchugov A
- Zheng Z
- Zhong D
- Zhou B
- Zhou C
- Zhou M
- Zhou MS
- 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 N
- Zimmermann S
- Zinonos Z
- Ziolkowski M
- Zivkovic L
- Zobernig G
- Zoccoli A
- Zoch K
- Zorbas TG
- Zou R
- Zu Theenhausen HM
- Zwalinski L
- Publication venue
- AMER PHYSICAL SOC
- Publication date
- 01/08/2020
- Field of study
A search for long-lived particles decaying into hadrons and at least one muon is presented. The analysis selects events that pass a muon or missing-transverse-momentum trigger and contain a displaced muon track and a displaced vertex. The analyzed dataset of proton-proton collisions at
√
s
=
13 TeV
was collected with the ATLAS detector and corresponds to
136
fb
−
1. The search employs dedicated reconstruction techniques that significantly increase the sensitivity to long-lived particle decays that occur in the ATLAS inner detector. Background estimates for Standard Model processes and instrumental effects are extracted from data. The observed event yields are compatible with those expected from background processes. The results are presented as limits at 95% confidence level on model-independent cross sections for processes beyond the Standard Model, and interpreted as exclusion limits in scenarios with pair production of long-lived top squarks that decay via a small
R
-parity-violating coupling into a quark and a muon. Top squarks with masses up to 1.7 TeV are excluded for a lifetime of 0.1 ns, and masses below 1.3 TeV are excluded for lifetimes between 0.01 ns and 30 ns
- …