73 research outputs found
Measurement of VH, H → b b ¯ production as a function of the vector-boson transverse momentum in 13 TeV pp collisions with the ATLAS detector
- Author
- Aaboud M
- Aad G
- Abbott B
- Abbott DC
- Abdinov O
- Abhayasinghe DK
- Abidi SH
- AbouZeid OS
- Abraham NL
- Abramowicz H
- Abreu H
- Abud AA
- Abulaiti Y
- Acharya BS
- 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
- Aielli G
- Akatsuka S
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- Alberghi GL
- Alberich LC
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- Alconada Verzini MJ
- Alderweireldt S
- Aleksa M
- Aleksandrov IN
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- Zaripovas DR
- Zeissner SV
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- Zemaityte G
- Zeng JC
- Zenin O
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- Zerwas D
- Zgubic M
- Zhang DF
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- Zhang G
- Zhang G
- Zhang H
- Zhang J
- Zhang L
- Zhang L
- Zhang M
- Zhang R
- Zhang R
- Zhang X
- Zhang Y
- Zhang Z
- Zhang Z
- Zhao P
- Zhao Y
- Zhao Z
- Zhemchugov A
- Zheng Z
- Zhong D
- Zhou B
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- Zhou MS
- Zhou N
- Zhou Y
- 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
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- Zorbas TG
- Zou R
- Zu Theenhausen HM
- Zwalinski L
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2019
- Field of study
Cross-sections of associated production of a Higgs boson decaying into bottom-quark pairs and an electroweak gauge boson, W or Z, decaying into leptons are measured as a function of the gauge boson transverse momentum. The measurements are performed in kinematic fiducial volumes defined in the `simplified template cross-section' framework. The results are obtained using 79.8 fb-1 of proton-proton collisions recorded by the ATLAS detector at the Large Hadron Collider at a centre-of-mass energy of 13 TeV. All measurements are found to be in agreement with the Standard Model predictions, and limits are set on the parameters of an effective Lagrangian sensitive to modifications of the Higgs boson couplings to the electroweak gauge bosons
Study of the spin and parity of the Higgs boson in diboson decays with the ATLAS detector
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- A. A. Affolder
- A. A. E. Bannoura
- A. A. Elliot
- A. A. Grillo
- A. A. Komar
- A. A. Korol
- A. A. Maier
- A. A. Minaenko
- A. A. Nepomuceno
- A. A. Snesarev
- A. A. Solodkov
- A. A. Talyshev
- A. Aloisio
- A. Alonso
- A. Altheimer
- A. Amorim
- A. Andreazza
- A. Angerami
- A. Annovi
- A. Antonov
- A. Artamonov
- A. Ashkenazi
- A. B. Fenyuk
- A. Baroncelli
- A. Basalaev
- A. Bassalat
- A. Basye
- A. Beddall
- A. Bellerive
- A. Bingul
- A. Bocci
- A. Borisov
- A. Boveia
- A. Brandt
- A. Bruni
- A. Buzatu
- A. C. Daniells
- A. C. König
- A. C. Martyniuk
- A. C. Schaffer
- A. Calandri
- A. Campoverde
- A. Canepa
- A. Castelli
- A. Catinaccio
- A. Cattai
- A. Cerri
- A. Cervelli
- A. Chafaq
- A. Chegwidden
- A. Cheplakov
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- A. Coccaro
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- A. Cortes-Gonzalez
- A. D. Hawkins
- A. D. Pilkington
- A. Dafinca
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- A. Dell’Acqua
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- W. Wiedenmann
- X. Chen
- X. Hu
- X. Ju
- X. Lei
- X. Lou
- X. Ruan
- X. Sun
- X. Wang
- X. Wu
- X. Zhang
- X. Zhao
- X. Zhuang
- Y Gao
- Y. A. Kurochkin
- Y. Abulaiti
- Y. Amaral Coutinho
- Y. Arai
- Y. B. Pan
- Y. Bai
- Y. Benhammou
- Y. Chen
- Y. Cheng
- Y. Coadou
- Y. Davygora
- Y. Enari
- Y. F. Ryabov
- Y. Fang
- Y. Gao
- Y. Guo
- Y. Hasegawa
- Y. Heng
- Y. Hernández Jiménez
- Y. Horii
- Y. Huang
- Y. Ikegami
- Y. Ilchenko
- Y. J. Schnellbach
- Y. Jiang
- Y. Kataoka
- Y. Kim
- Y. Komori
- Y. Kulchitsky
- Y. Li
- Y. Liu
- Y. Makida
- Y. Minami
- Y. Ming
- Y. Nagai
- Y. Nagasaka
- Y. Nakahama
- Y. Ninomiya
- Y. Okumura
- Y. Oren
- Y. Qin
- Y. Rozen
- Y. S. Gao
- Y. Sakurai
- Y. Sasaki
- Y. Silver
- Y. Smirnov
- Y. Sugaya
- Y. Takubo
- Y. Tayalati
- Y. Unno
- Y. Wu
- Y. Yamaguchi
- Y. Yamazaki
- Y. Yang
- Y. Yasu
- Y. Zhao
- Y. Zhu
- Yu. A. Tikhonov
- Z. Barnovska
- Z. D. Greenwood
- Z. Dolezal
- Z. Gecse
- Z. H. Citron
- Z. Hajduk
- Z. Hubacek
- Z. Idrissi
- Z. J. Grout
- Z. Kohout
- Z. Liang
- Z. M. Karpova
- Z. Marshall
- Z. Rurikova
- Z. V. Krumshteyn
- Z. Vykydal
- Z. Yan
- Z. Zhang
- Z. Zhao
- Z. Zinonos
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2015
- Field of study
Studies of the spin, parity and tensor couplings of the Higgs boson in the H→ZZ∗→4ℓ, H→WW∗→eνμν and H→γγ decay processes at the LHC are presented. The investigations are based on 25fb−1 of pp collision data collected by the ATLAS experiment at √s=7 TeV and √s=8 TeV. The Standard Model (SM) Higgs boson hypothesis, corresponding to the quantum numbers JP=0+, is tested against several alternative spin scenarios, including non-SM spin-0 and spin-2 models with universal and non-universal couplings to fermions and vector bosons. All tested alternative models are excluded in favour of the SM Higgs boson hypothesis at more than 99.9 % confidence level. Using the H → ZZ∗ → 4ℓ and H → WW∗ → eνμν decays, the tensor structure of the interaction between the spin-0 boson and the SM vector bosons is also investigated. The observed distributions of variables sensitive to the non-SM tensor couplings are compatible with the SM predictions and constraints on the non-SM couplings are derived
Measurement of the t¯tZ and t¯tW cross sections in proton-proton collisions at √s=13 TeV with the ATLAS detector
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- Zhemchugov A
- Zheng Z
- Zhong D
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- Zhuang X
- Zhukov K
- Zhulanov V
- Zibell A
- Zieminska D
- Zimine NI
- Zimmermann S
- Zinonos Z
- Ziolkowski M
- Zobernig G
- Zoccoli A
- Zoch K
- Zorbas TG
- Zou R
- Zur Nedden M
- Zwalinski L
- Álvarez Piqueras D
- Åkesson TPA
- Šfiligoj T
- Ženiš T
- Živković L
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2019
- Field of study
A measurement of the associated production of a top-quark pair (t¯t) with a vector boson (W, Z) in proton-proton collisions at a center-of-mass energy of 13 TeV is presented, using 36.1 fb−1 of integrated luminosity collected by the ATLAS detector at the Large Hadron Collider. Events are selected in channels with two same- or opposite-sign leptons (electrons or muons), three leptons or four leptons, and each channel is further divided into multiple regions to maximize the sensitivity of the measurement. The t¯tZ and t¯tW production cross sections are simultaneously measured using a combined fit to all regions. The best-fit values of the production cross sections are σt¯tZ=0.95±0.08stat±0.10syst pb and σt¯tW=0.87±0.13stat±0.14syst pb in agreement with the Standard Model predictions. The measurement of the t¯tZ cross section is used to set constraints on effective field theory operators which modify the t¯tZ vertex
Search for excited electrons singly produced in proton–proton collisions at \sqrt{s} = 13 TeV with the ALAS experiment at the LHC
- Author
- Aaboud M
- Aad G
- Abbott B
- Abbott DC
- Abdinov O
- Abeloos B
- Abhayasinghe DK
- Abidi SH
- AbouZeid OS
- Abraham NL
- Abramowicz H
- Abreu H
- Abulaiti Y
- Acharya BS
- Adachi S
- Adam L
- Adamczyk L
- Adamek L
- Adelman J
- Adersberger M
- Adiguzel A
- Adye T
- Affolder AA
- Afik Y
- Agapopoulou C
- Agheorghiesei C
- Aguilar-Saavedra JA
- Ahmadov F
- Aielli G
- Akatsuka S
- Akilli E
- Akimov AV
- Alberghi GL
- Alberich LC
- Albert J
- Alderweireldt S
- Aleksa M
- Aleksandrov IN
- Alexa C
- Alexandre D
- Alexopoulos T
- Alhroob M
- Ali B
- Alimonti G
- Alison J
- Alkire SP
- Allaire C
- Allbrooke BMM
- Allen BW
- Allport PP
- Aloisio A
- Alonso A
- Alonso F
- Alpigiani C
- Alshehri AA
- Alstaty MI
- 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
- Angelozzi I
- Angerami A
- Anisenkov AV
- Annovi A
- Antel C
- Anthony MT
- Antonelli M
- Antrim DJA
- Anulli F
- Aoki M
- Arabidze G
- Aranda CP
- Araque JP
- Araya ST
- Arce ATH
- Arduh FA
- Arguin J-F
- Argyropoulos S
- Arling J-H
- Armadans RC
- Armbruster AJ
- Armitage LJ
- Armstrong A
- Arnaez O
- Arnold H
- Artamonov A
- Artoni G
- Artz S
- Asai S
- Asbah N
- Asimakopoulou EM
- Asquith L
- Assamagan K
- Astalos R
- Astigarraga MEP
- Atkin RJ
- Atkinson M
- Atlay NB
- Augsten K
- Avolio G
- Avramidou R
- Ayoub MK
- Azoulay AM
- Azuelos G
- Baas AE
- Baca MJ
- Bachacou H
- Bachas K
- Backes M
- Backman F
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- Bahilo JJL
- 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
- Barajas CAC
- Barak L
- Barbe WM
- Barberio EL
- Barberis D
- Barbero M
- Barillari T
- Barisits M-S
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- Barklow T
- Barnea R
- Barnes SL
- Barnett BM
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- Barnovska-Blenessy Z
- Baroncelli A
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- Barr AJ
- Barreiro F
- Bartoldus R
- Barton AE
- Bartos P
- Basalaev A
- Bassalat A
- Bates RL
- Batista SJ
- Batlamous S
- Batley JR
- Battaglia M
- Bauce M
- Bauer F
- Bauer KT
- Bawa HS
- Beacham JB
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- Beauchemin PH
- Bechtle P
- Beck HC
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- Becot C
- Beddall A
- Beddall AJ
- Bednyakov VA
- Bedognetti M
- Bee CP
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- Begalli M
- Begel M
- Behera A
- Behr JK
- Beisiegel F
- Bell AS
- Bella G
- Bella LA
- Bellagamba L
- Bellerive A
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- Bellomo M
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- Beloborodov K
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- Belyaev NL
- Benary O
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- Benhammou Y
- Benjamin DP
- Benoit M
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- Beresford L
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- Biesuz NV
- Biglietti M
- Billoud TRV
- Bindi M
- Bingul A
- Bini C
- Biondi S
- Birman M
- Bisanz T
- Biswal JP
- Bitadze A
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- Zhemchugov A
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- Zhulanov V
- Zibell A
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- Zimine NI
- Zimmermann S
- Zinonos Z
- Ziolkowski M
- Zobernig G
- Zoccoli A
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- Zorbas TG
- Zou R
- Zwalinski L
- Åkesson TPA
- Šfiligoj T
- Ženiš T
- Živković L
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/09/2019
- Field of study
A search for excited electrons produced in pp collisions at s√ = 13 TeV via a contact interaction qq¯→ee∗ is presented. The search uses 36.1 fb −1 of data collected in 2015 and 2016 by the ATLAS experiment at the Large Hadron Collider. Decays of the excited electron into an electron and a pair of quarks ( eqq¯ ) are targeted in final states with two electrons and two hadronic jets, and decays via a gauge interaction into a neutrino and a W boson ( νW ) are probed in final states with an electron, missing transverse momentum, and a large-radius jet consistent with a hadronically decaying W boson. No significant excess is observed over the expected backgrounds. Upper limits are calculated for the pp→ee∗→eeqq¯ and pp→ee∗→eνW production cross sections as a function of the excited electron mass me∗ at 95% confidence level. The limits are translated into lower bounds on the compositeness scale parameter Λ of the model as a function of me∗ . For me∗<0.5 TeV , the lower bound for Λ is 11 TeV . In the special case of me∗=Λ , the values of me∗<4.8 TeV are excluded. The presented limits on Λ are more stringent than those obtained in previous searches
Observation of Electroweak Production of a Same-Sign W Boson Pair in Association with Two Jets in pp Collisions root s=13 TeV with the ATLAS Detector
- Author
- Aaboud M
- Aad G
- Abbott B
- Abdinov O
- Abeloos B
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- Zhemchugov A
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- Zinonos Z
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- Zivkovic L
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- Zou R
- Zu Theenhausen HM
- Zur Nedden M
- Zwalinski L
- Publication venue
- AMER PHYSICAL SOC
- Publication date
- 18/10/2019
- Field of study
This Letter presents the observation and measurement of electroweak production of a same-sign
W
boson pair in association with two jets using
36.1
fb
−
1
of proton-proton collision data recorded at a center-of-mass energy of
√
s
=
13
TeV
by the ATLAS detector at the Large Hadron Collider. The analysis is performed in the detector fiducial phase-space region, defined by the presence of two same-sign leptons, electron or muon, and at least two jets with a large invariant mass and rapidity difference. A total of 122 candidate events are observed for a background expectation of
69
±
7
events, corresponding to an observed signal significance of 6.5 standard deviations. The measured fiducial signal cross section is
σ
fid
=
2.89
+
0.51
−
0.48
(
stat
)
+
0.29
−
0.28
(
syst
)
fb
Search for squarks and gluinos in final states with jets and missing transverse momentum using 139 fb−1 of s√ = 13 TeV pp collision data with the ATLAS detector
- Author
- Aaboud M
- Aad G
- Abbott B
- Abdinov O
- Abeloos B
- Abhayasinghe DK
- Abidi SH
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- Abulaiti Y
- Acharya BS
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- Zhulanov V
- Zibell A
- Zieminska D
- Zimine NI
- Zimmermann S
- Zinonos Z
- Zinser M
- Ziolkowski M
- Zivkovic L
- Zobernig G
- Zoccoli A
- Zoch K
- Zorbas TG
- Zou R
- Zwalinski L
- Publication venue
- 'Springer Fachmedien Wiesbaden GmbH'
- Publication date
- 17/02/2021
- Field of study
A search for the supersymmetric partners of quarks and gluons (squarks and gluinos) in final states containing jets and missing transverse momentum, but no electrons or muons, is presented. The data used in this search were recorded by the ATLAS experiment in proton-proton collisions at a centre-of-mass energy of s√ = 13 TeV during Run 2 of the Large Hadron Collider, corresponding to an integrated luminosity of 139 fb−1. The results are interpreted in the context of various R-parity-conserving models where squarks and gluinos are produced in pairs or in association and a neutralino is the lightest supersymmetric particle. An exclusion limit at the 95% confidence level on the mass of the gluino is set at 2.30 TeV for a simplified model containing only a gluino and the lightest neutralino, assuming the latter is massless. For a simplified model involving the strong production of mass-degenerate first- and second-generation squarks, squark masses below 1.85 TeV are excluded if the lightest neutralino is massless. These limits extend substantially beyond the region of supersymmetric parameter space excluded previously by similar searches with the ATLAS detector
Measurement of Azimuthal Anisotropy of Muons from Charm and Bottom Hadrons in pp Collisions at √s = 13 TeV with the ATLAS Detector
- Author
- Aaboud M
- Aad G
- Abbott B
- Abdinov O
- Abeloos B
- Abhayasinghe DK
- Abidi SH
- AbouZeid OS
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- Abramowicz H
- Abreu H
- Abulaiti Y
- Acharya BS
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- Cardillo FC
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- Carlson BT
- Carminati L
- Carney RMD
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- Publication venue
- AMER PHYSICAL SOC
- Publication date
- 28/02/2020
- Field of study
The elliptic flow of muons from the decay of charm and bottom hadrons is measured in
p
p
collisions at
√
s
=
13
TeV
using a data sample with an integrated luminosity of
150
pb
−
1
recorded by the ATLAS detector at the LHC. The muons from heavy-flavor decay are separated from light-hadron decay muons using momentum imbalance between the tracking and muon spectrometers. The heavy-flavor decay muons are further separated into those from charm decay and those from bottom decay using the distance-of-closest-approach to the collision vertex. The measurement is performed for muons in the transverse momentum range 4–7 GeV and pseudorapidity range
|
η
|
<
2.4
. A significant nonzero elliptic anisotropy coefficient
v
2
is observed for muons from charm decays, while the
v
2
value for muons from bottom decays is consistent with zero within uncertainties
Properties of jet fragmentation using charged particles measured with the ATLAS detector in pp collisions at root s=13 TeV
- Author
- Aaboud M
- Aad G
- Abbott B
- Abdinov O
- Abeloos B
- Abhayasinghe DK
- Abidi SH
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- Zaripovas DR
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- Zhemchugov A
- Zhou B
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- Zhu CG
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- Zhukov K
- Zhulanov V
- Zibell A
- Zieminska D
- Zimine NI
- Zimmermann S
- Zinonos Z
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- Ziolkowski M
- Zivkovic L
- Zobernig G
- Zoccoli A
- Zoch K
- Zorbas TG
- Zou R
- Zwalinski L
- Publication venue
- AMER PHYSICAL SOC
- Publication date
- 01/09/2019
- Field of study
This paper presents a measurement of quantities related to the formation of jets from high-energy quarks and gluons (fragmentation). Jets with transverse momentum 100 GeV 500 MeV and |η| < 2.5 are used to probe the detailed structure of the jet. The fragmentation properties of the more forward and the more central of the two leading jets from each event are studied. The data are unfolded to correct for detector resolution and acceptance effects. Comparisons with parton shower Monte Carlo generators indicate that existing models provide a reasonable description of the data across a wide range of phase space, but there are also significant differences. Furthermore, the data are interpreted in the context of quark- and gluon-initiated jets by exploiting the rapidity dependence of the jet flavor fraction. A first measurement of the charged-particle multiplicity using model-independent jet labels (topic modeling) provides a promising alternative to traditional quark and gluon extractions using input from simulation. The simulations provide a reasonable description of the quark-like data across the jet
Pt range presented in -this measurement, but the gluon-like data have systematically fewer charged particles than the simulation
Reconstruction and identification of boosted di-τ systems in a search for Higgs boson pairs using 13 TeV proton-proton collision data in ATLAS
- Author
- Aaboud M
- Aad G
- Abbott B
- Abdinov O
- Abeloos B
- Abhayasinghe DK
- Abidi SH
- AbouZeid OS
- Abraham NL
- Abramowicz H
- Abreu H
- Abulaiti Y
- Acharya BS
- Adachi S
- Adamczyk L
- Adelman J
- Adersberger M
- Adiguzel A
- Adye T
- Affolder AA
- Afik Y
- Agheorghiesei C
- Aguilar-Saavedra JA
- Ahmadov F
- Aielli G
- Akatsuka S
- Akesson TPA
- Akilli E
- Akimov AV
- Alberghi GL
- Albert J
- Albicocco P
- Alderweireldt S
- Aleksa M
- Aleksandrov IN
- Alexa C
- Alexopoulos T
- Alhroob M
- Ali B
- Alimonti G
- Alison J
- Alkire SP
- Allaire C
- Allbrooke BMM
- Allen BW
- Allport PP
- Aloisio A
- Alonso A
- Alonso F
- Alpigiani C
- Alshehri AA
- Alstaty MI
- Alvarez Piqueras D
- Alviggi MG
- Amadio BT
- Ambroz L
- Amelung C
- Amidei D
- Amor Dos Santos SP
- Amoroso S
- Amrouche CS
- Anastopoulos C
- Ancu LS
- Andari N
- Andeen T
- Anders CF
- Anders JK
- Anderson KJ
- Andreazza A
- Andrei V
- Anelli CR
- Angelidakis S
- Angelozzi I
- Angerami A
- Anisenkov AV
- Annovi A
- Antel C
- Anthony MT
- Antonelli M
- Antrim DJA
- Anulli F
- Aoki M
- Aparisi Pozo JA
- Aperio Bella L
- Arabidze G
- Aranda CP
- Araque JP
- Araujo Ferraz V
- Araujo Pereira R
- Araya ST
- Arce ATH
- Ardell RE
- Arduh FA
- Arguin J-F
- Argyropoulos S
- Armadans RC
- Armbruster AJ
- Armitage LJ
- Armstrong A
- Arnaez O
- Arnold H
- Arratia M
- Arslan O
- Artamonov A
- Artoni G
- Artz S
- Asai S
- Asbah N
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- Zhemchugov A
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- Zorbas TG
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- Publication venue
- 'Springer Fachmedien Wiesbaden GmbH'
- Publication date
- 30/11/2020
- Field of study
In this paper, a new technique for reconstructing and identifying hadronically decaying τ+τ− pairs with a large Lorentz boost, referred to as the di-τ tagger, is developed and used for the first time in the ATLAS experiment at the Large Hadron Collider. A benchmark di-τ tagging selection is employed in the search for resonant Higgs boson pair production, where one Higgs boson decays into a boosted bb¯¯ pair and the other into a boosted τ+τ− pair, with two hadronically decaying τ-leptons in the final state. Using 139 fb−1 of proton-proton collision data recorded at a centre-of-mass energy of 13 TeV, the efficiency of the di-τ tagger is determined and the background with quark- or gluon-initiated jets misidentified as di-τ objects is estimated. The search for a heavy, narrow, scalar resonance produced via gluon-gluon fusion and decaying into two Higgs bosons is carried out in the mass range 1–3 TeV using the same dataset. No deviations from the Standard Model predictions are observed, and 95% confidence-level exclusion limits are set on this model
A search for the dimuon decay of the Standard Model Higgs boson with the ATLAS detector
- Author
- Aaboud M
- Aad G
- Abbott B
- Abdinov O
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- Abhayasinghe DK
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- Publication venue
- 'Elsevier BV'
- Publication date
- 10/01/2021
- Field of study
A search for the dimuon decay of the Standard Model (SM) Higgs boson is performed using data corresponding to an integrated luminosity of collected with the ATLAS detector in Run 2 pp collisions at TeV at the Large Hadron Collider. The observed (expected) significance over the background-only hypothesis for a Higgs boson with a mass of 125.09 GeV is 2.0σ (1.7σ). The observed upper limit on the cross section times branching ratio for is 2.2 times the SM prediction at 95% confidence level, while the expected limit on a signal assuming the absence (presence) of a SM signal is 1.1 (2.0). The best-fit value of the signal strength parameter, defined as the ratio of the observed signal yield to the one expected in the SM, is
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