517 research outputs found
Firmware implementation of a recurrent neural network for the computation of the energy deposited in the liquid argon calorimeter of the ATLAS experiment
- Author
- Publication venue
- Publication date
- 01/01/2023
- Field of study
No full textInternational audienceThe ATLAS experiment measures the properties of particles that are products of proton-proton collisions at the LHC. The ATLAS detector will undergo a major upgrade before the high luminosity phase of the LHC. The ATLAS liquid argon calorimeter measures the energy of particles interacting electromagnetically in the detector. The readout electronics of this calorimeter will be replaced during the aforementioned ATLAS upgrade. The new electronic boards will be based on state-of-the-art field-programmable gate arrays (FPGA) from Intel allowing the implementation of neural networks embedded in firmware. Neural networks have been shown to outperform the current optimal filtering algorithms used to compute the energy deposited in the calorimeter. This article presents the implementation of a recurrent neural network (RNN) allowing the reconstruction of the energy deposited in the calorimeter on Stratix 10 FPGAs. The implementation in high level synthesis (HLS) language allowed fast prototyping but fell short of meeting the stringent requirements in terms of resource usage and latency. Further optimisations in Very High-Speed Integrated Circuit Hardware Description Language (VHDL) allowed fulfilment of the requirements of processing 384 channels per FPGA with a latency smaller than 125 ns
Measurements of the suppression and correlations of dijets in Xe+Xe collisions at Formula Presented TeV
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- Liu J. K. K.
- Bruckler TL
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- Arce ATH
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- Publication venue
- Publication date
- 01/01/2023
- Field of study
No full textMeasurements of the suppression and correlations of dijets is performed using 3 μ b − 1 of Xe+Xe data at s N N = 5.44 TeV collected with the ATLAS detector at the CERN Large Hadron Collider. Dijets with jets reconstructed using the R = 0.4 anti- k t algorithm are measured differentially in jet p T over the range of 32 to 398 GeV and the centrality of the collisions. Significant dijet momentum imbalance is found in the most central Xe+Xe collisions, which decreases in more peripheral collisions. Results from the measurement of per-pair normalized and absolutely normalized dijet p T balance are compared with previous Pb + Pb measurements at s N N = 5.02 TeV. The differences between the dijet suppression in Xe+Xe and Pb + Pb are further quantified by the ratio of pair nuclear-modification factors. The results are found to be consistent with those measured in Pb + Pb data when compared in classes of the same event activity and when taking into account the difference between the center-of-mass energies of the initial parton scattering process in Xe+Xe and Pb + Pb collisions. These results should provide input for a better understanding of the role of energy density, system size, path length, and fluctuations in the parton energy loss
Underlying-event studies with strange hadrons in pp collisions at s=13 TeV with the ATLAS detector
- Author
- Birman Mattias
- Arbiol Val S. J.
- Carlino Giampaolo
- Albouy G. L.
- Beddall AJ
- Azuelos Georges
- Carminati L.
- Cantero J.
- Carlotto J. I.
- Aly M
- Zaplatilek O
- Burzynski JC
- Booth C. D.
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- Antipov Egor
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- Beloborodov Konstantin
- Boveia A
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- Arnold Hannah
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- Avolio Giuseppe
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- Astrand K. S. V.
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- Bhopatkar V.S.
- Chitan A.
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- Centonze Martino Salomone
- Chow Edwin
- Alviggi M. G.
- Bachiu Alexander
- Zambito S
- Beemster L. J.
- Blue A
- Barends KN
- Chan WY
- Battulga D.
- Che Y
- Bendebba Fatima
- Buxo Vazquez Carlos Josue
- Barberio E. L.
- Canale V.
- Barberio EL
- Bella Gideon
- Apyan Aram
- Alderweireldt Sara
- Bergmann Benedikt Ludwig
- Ciubotaru D. A.
- Allendes Flores Cristian Andres
- Austrup V. A.
- Alegria Z.L.
- Bee C.P.
- Adelman J.
- Balakrishnan Veena
- Buchin D
- Ames C. G.
- Bulekov Oleg
- Carminati L
- Bussey P. J.
- Saa JAZ
- Ali H. M. J.
- Schimmel Brener Roy
- Allaire C
- Chan J.
- Bhattarai P
- Aggarwal A.
- Barr JD
- Burlayenko O
- Cirotto Francesco
- Chapman J. D.
- Beauchemin PH
- Bruscino Nello
- Beirer JF
- Bielski R
- Adiguzel A.
- Chan W. Y.
- Butterworth J. M.
- Alfonsi Fabrizio
- Canonero E.
- Hurrell L.T.B.
- null null
- Belfkir M.
- Zerradi S
- Alkakhi Wael
- Bhatta Somadutta
- Anders J.K.
- Garcia LC
- Arce A. T. H.
- Borecka-Bielska H.M.
- Balasubramanian R.
- Castillo FL
- Bisanz Tobias
- Cao Y.
- Publication venue
- Publication date
- 01/01/2024
- Field of study
No full textProperties of the underlying-event in pp interactions are investigated primarily via the strange hadrons KS0, Λ and Λ¯, as reconstructed using the ATLAS detector at the LHC in minimum-bias pp collision data at s=13 TeV. The hadrons are reconstructed via the identification of the displaced two-particle vertices corresponding to the decay modes, Λ→π-p and Λ¯→π+p¯. These are used in the construction of underlying-event observables in azimuthal regions computed relative to the leading charged-particle jet in the event. None of the hadronisation and underlying-event physics models considered can describe the data over the full kinematic range considered. Events with a leading charged-particle jet in the range of 10<pT≤40 GeV are studied using the number of prompt charged particles in the transverse region. The ratio N(Λ+Λ¯)/N(KS0) as a function of the number of such charged particles varies only slightly over this range. This disagrees with the expectations of some of the considered Monte Carlo models
Search for heavy Majorana neutrinos in e±e± and e±μ± final states via WW scattering in pp collisions at s=13 TeV with the ATLAS detector
- Author
- Bamwidhi Isaac
- Birman Mattias
- Bellos Panagiotis
- Carlino Giampaolo
- Auriol Adrien
- Camarri Paolo
- Alhroob Muhammad
- Beacham James
- Azuelos Georges
- Abicht Nils Julius
- Bevan Adrian
- Burgard Carsten
- Bahmani Marzieh
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- Albert Justin
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- Basan Alexander
- Agarwala Jinky
- Bokan Petar
- Alpigiani Cristiano
- Beringer Juerg
- Andrean Stefio Yosse
- Aleksa Martin
- Brenner Lydia
- Carroll Anthony Maurel
- Beaucamp Jean Yves
- Burlayenko Oleksandr
- Cavaliere Viviana
- Atkin Ryan Justin
- Barros Maura
- Addison Matt
- Beretta Matteo Mario
- Atashi Rose
- Austrup Volker Andreas
- Begel Michael
- Barak Liron
- Buckley Andy
- Balunas William Keaton
- Bates Richard
- Becker Kathrin
- Catmore James
- Bouchhar Naseem
- Caron Sascha
- Cherkaoui Rajaa
- Betti Alessandra
- Bandieramonte Marilena
- Chen Boping
- Barberis Dario
- Ahmed Waleed Syed
- Addepalli Sagar
- Cai Yizhou
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- Chen Jing
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- Castro Nuno
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- Al Khoury Konie
- Brooijmans Gustaaf
- An Shiwen
- Chu Xiaotong
- Benkendorfer Kees
- Bernon Florent
- Burghgrave Blake Oliver
- Carnesale Maria
- Brandt Oleg
- Camarda Stefano
- Anderson Adam Campbell
- Bianco Gianluca
- Butterworth Jonathan
- Auricchio Silvia
- Berrocal Guardia Adrian
- Buescher Volker
- Chizhov Mihail
- Alegria Zackary Lee
- Axiotis Konstantinos
- Bellerive Alain
- Bruschi Marco
- Bossio Jonathan
- Calvetti Milene
- Angelidakis Stylianos
- Balli Fabrice
- Chatterjee Meghranjana
- Cadamuro Luca
- Cheu Elliott
- Brandt Gerhard Immanuel
- Bhattacharya Deb Sankar
- Aoki Takumi
- Citron Zvi
- Canbay Ali Can
- Batlamous Souad
- Bianchi Riccardo Maria
- Chen Huirun
- Borbely Albert Gyorgy
- Benchekroun Driss
- Bona Marcella
- Bouhova-Thacker Eva
- Brooks Ethan Michael
- Bohm Burkhard
- Buttar Craig Macleod
- Bhide Kartik Deepak
- Bernardi Gregorio
- Astrand Karl Sten Vilhelm
- Carter Thomas Michael
- Banas Elzbieta
- Bullard Brendon
- Asai Kanae
- Chen Ye
- Blue Andrew James
- Cesarini Gianmario
- Beau Tristan
- Bloch Ingo
- Arnold Hannah
- Amerl Maximilian
- Baer Tamas Marton
- Beauchemin Pierre-Hugues
- Benhammou Yan
- Cakir Orhan
- Aitbenchikh Brahim
- Bakos Evelin
- Beresford Lydia Audrey
- Appelt Christian
- Campanelli Mario
- Camplani Alessandra
- Bechtle Philip
- Brenner Richard
- Amor dos Santos Susana Patricia
- Brau Jim
- Abreu Henso
- Chou Yuan-Tang
- Bernius Catrin
- Boveia Antonio
- Barsov Sergey
- Acharya Bobby Samir
- Badea Anthony
- Cerny Karel
- Camincher Clement
- Canonero Enzo
- Barone Gaetano
- Bindi Marcello
- Chevalier Laurent
- Bassalat Ahmed
- Ambler Alessandro
- Ames Christoph
- Agheorghiesei Catalin
- Santiago Cerqueira Augusto
- Caloba Luiz Pereira
- Battulga Daariimaa
- Bouquet Romain
- Ali Shahzad
- Aliev Malik
- Arnaez Olivier
- Avolio Giuseppe
- Cella Sofia
- Calvet Samuel
- Brock Ian
- Aoki Masato
- Alvarez Estevez Manuel
- Bernlochner Florian Urs
- Cervelli Alberto
- Allaire Corentin
- Busch Elena Laura
- Catinaccio Andrea
- Barillari Teresa
- Allbrooke Benedict
- Bressler Shikma
- Bruni Alessia
- Arcangeletti Chiara
- Allen Julia Frances
- Butler John Mark
- Assamagan Ketevi Adikle
- Bruckler Tim Lukas
- Bandyopadhyay Anjishnu
- Chu Michael Kwok Lam
- Ali Babar
- Publication venue
- Publication date
- 01/01/2024
- Field of study
No full textInternational audienceA search for heavy Majorana neutrinos in scattering of same-sign W boson pairs in proton-proton collisions at s=13 TeV at the LHC is reported. The dataset used corresponds to an integrated luminosity of 140 fb−1, collected with the ATLAS detector during 2015-2018. The search is performed in final states including a same-sign ee or eμ pair and at least two jets with large invariant mass and a large rapidity difference. No significant excess of events with respect to the Standard Model background predictions is observed. The results are interpreted in a benchmark scenario of the Phenomenological Type-I Seesaw model. New constraints are set on the values of the ∣VeN∣2 and ∣VeNVμN∗∣ parameters for heavy Majorana neutrino masses between 50 GeV and 20 TeV, where VℓN is the matrix element describing the mixing of the heavy Majorana neutrino mass eigenstate with the Standard Model neutrino of flavour ℓ=e,μ. The sensitivity to the Weinberg operator is investigated and constraints on the effective ee and eμ Majorana neutrino masses are reported. The statistical combination of the ee and eμ channels with the previously published μμ channel is performed
Measurements of longitudinal flow decorrelations in pp and Xe+Xe collisions with the ATLAS detector
- Author
- Birman Mattias
- Bellos Panagiotis
- Auriol Adrien
- Camarri Paolo
- Alhroob Muhammad
- Ana Elena Dumitriu
- Beacham James
- Bernlochner Florian
- Azuelos Georges
- Abicht Nils Julius
- Cardoso Mário
- Cherkaoui El Moursli Rajaa
- Bevan Adrian
- Bahmani Marzieh
- Beck Hans Peter
- Cieri Davide
- Buzykaev Alexey
- Cai Huacheng
- Aly Mohamed
- Belfkir Mohamed
- Beirer Dr. Joshua Falco
- Cerrito Lucio
- Cardillo Fabio
- Chargeishvili Bakar
- Baselga Bacardit Marta
- Chen Xin
- Carnelli Alberto
- Abramowicz Halina
- Biswal Jyoti Prakash
- Boyko Igor
- Aparisi Pozo Javier Alberto
- Cieśla Krzysztof
- Blumenschein Ulla
- Cairo Valentina Maria Martina
- Carrà Sonia
- Barberio Elisabetta
- Alviggi Mariagrazia
- Canale Vincenzo
- Arguin Jean-Francois
- Chen Andy
- Arling Jan-Hendrik
- Boudreau Joseph
- Bohm Christian
- Brooks William
- Brahimi Nihal
- Castillo Florencia Luciana
- Chakraborty Dhiman
- Bogdanchikov Alexander
- Beddall Andrew
- Berry Tracey
- Cervato Beatrice
- Abulaiti Yiming
- Calvet David
- Cantero García Josu
- Bee Christopher
- Britton David
- Bauce Matteo
- Chomont Arthur
- Atmani Hicham
- Casado Lechuga María Pilar
- Cindro Vladimir
- Baroň Petr
- Anthony Matthew
- Buanes Trygve
- Biswas Diptaparna
- Bachacou Henri
- Barbero Marlon Benoit
- Alonso Francisco
- Camerlingo Maria Teresa
- Bracinik Juraj
- Akbiyik Melike
- Carlson Benjamin
- Battaglia Marco
- Abidi Syed Haider
- Çekmeceli̇oğlu Yusuf Can
- Antonelli Mario
- Çeti̇n Serkant Ali̇
- Baltes Lisa Marie
- Chen Shenjian
- Bhamjee Muaaz
- Behera Arabinda
- Cheung Kingman
- Becherer Fabian
- Caspar Maximilian
- Cheremushkina Evgeniya
- Aggarwal Anamika
- Berrocal Guardia Adrián
- Callea Giuseppe
- Biglietti Michela
- Chiarelli Giorgio
- Bagnaia Paolo
- Burdin Sergey
- Chowdhury Tasnuva
- Abeling Kira
- Carlson Evan
- Bellagamba Lorenzo
- Biondini Alessandro
- Choi Kyungeon
- Amos Kieran
- Addison Matthew
- Centonze Martino Salomone
- Aizenberg Iakov
- Castillo Maria Victoria
- Bruckman de Renstrom Pawel
- Akiyama Daiya
- Albouy Guillaume
- Bachiu Alexander
- Boumediene Djamel
- Ai Xiaocong
- Bendebba Fatima
- Buxo Vazquez Carlos Josue
- Carter Joseph
- Chiarella Vitaliano
- Boye Diallo
- Ahmadov Faig
- Assamagan Kétévi Adiklè
- Bella Gideon
- Brown Leesa
- Apyan Aram
- Brost Elizabeth
- Akolkar Nilima
- Cao Yumeng
- Alderweireldt Sara
- Carratta Giuseppe
- Chen Meiqi
- Burger Angela
- Bergmann Benedikt Ludwig
- Černý Karel
- Allendes Flores Cristian Andres
- Balakrishnan Veena
- Bailey Virginia
- Bulekov Oleg
- Carlotto Juan Ignacio
- Blue Andrew
- Ali Hanadi
- Barr Jackson
- Atkinson Markus Julian
- Amelung Christoph
- Chan Jay
- Chiedde Nemer
- Akimov Andrey
- Anders John
- Borissov Guennadi
- Aparo Marco
- Annovi Alberto
- Bird Gareth
- Chapman John
- Chen Hucheng
- Bouhova-Thacker Evelina
- Buttinger William
- Cavasinni Vincenzo
- Atashi Shaghayegh
- Alexa Calin
- Cirotto Francesco
- Bordulev Yuriy
- Aloisio Alberto
- Carter Thomas
- Bruscino Nello
- Chen Jiayi
- Beermann Thomas
- Blumenthal Julian
- Cardarelli Roberto
- Alfonsi Fabrizio
- Cherepanova Elizaveta
- Bielski Rafal
- Bortoletto Daniela
- Akesson Torsten
- Ciocio Alessandra
- Cameron David
- Adamczyk Leszek
- Aielli Giulio
- Alkakhi Wael
- Bhatta Somadutta
- Cepaitis Vilius
- Cheng Hok-Chuen
- Bentvelsen Stan
- Aad Georges
- Bosman Martine
- Ballabene Eric
- Barron Uriel
- Biryukov Stanislav
- Bisanz Tobias
- A Arya
- Balek Petr
- Bartels Falk
- Batool Binish
- Cerutti Fabio
- Arbiol Val Sergio Javier
- Algren Malte
- Boyd James
- Ahuja Sudha
- Calace Noemi
- Alexandrov Igor
- Anastopoulos Christos
- Bjørke Kristian
- Bogavac Danijela
- Adelman Jahred
- Andeen Timothy
- Allport Philip
- Cai Yuchen
- Caforio Davide
- Anulli Fabio
- Burghgrave Blake
- Bini Cesare
- Berthold Anne-Sophie
- Bossio Sola Jonathan David
- Chudoba Jiri
- Adye Tim
- Carquin Edson
- Böhm Burkhard
- Andreazza Attilio
- Alves Fabio Lucio
- Bauer Michael
- Brau James E.
- Brueckler Tim Lukas
- Bruni Graziano
- Bartos Pavol
- Biroš Marek
- Backman Filip
- Bazzano Lisandro Tomás
- Barends Kevin Nicholas
- Bauer Patrick
- Bingul Ahmet
- Ciubotaru Dan Andrei
- Beisiegel Florian
- Asada Haruka
- Chekanov Sergei
- Carducci Giovandomenico
- Ahmad Ammara
- Amidei Dante
- Bold Tomasz
- Cheng Chi Lung
- Chan Wai Yuen
- Cardenas Juan
- Chitishvili Mariam
- Alberghi Gian Luigi
- Camincher Clément
- Adiguzel Aytul
- Bartoldus Rainer
- Chauhan Chainika
- Boisvert Veronique
- Calvet Thomas
- Albicocco Pietro
- Canesse Auriane
- Bergeaas Kuutmann Elin
- Camarero Muñoz Daniel
- Carbone Antonio
- Astalos Robert
- Baines Luke
- Bansal Shubham
- Bisceglie Emanuele
- Bensinger James
- Buttar Craig
- Bhattarai Prajita
- Bhalla Naman Kumar
- Chow Edwin Yun Sang
- Behr J. Katharina
- Bhopatkar Vallary
- Chen Xiang
- Balz Johannes
- Buchin Daniel
- Borbély Albert György
- Capocasa Francesca
- Barone Gaetano Athanassios
- Balasubramanian Rahul
- Busch Elena
- Carminati Leonardo Carlo
- Bednyakov Vadim
- Asbah Nedaa Alexandra
- Arena Eloisa
- Barrué Ricardo
- Atmasiddha Prachi Arvind
- Augsten Kamil
- Acharya Bobby
- Beresford Lydia
- Agaras Merve Nazlim
- Chu Ming-Chung
- Biebel Otmar
- Bomben Marco
- Bouaouda Khalil
- Calfayan Philippe
- Barel Marten
- Borecka-Bielska Hanna
- Chen Charlie
- Camacho Toro Reina Coromoto
- Buat Quentin
- Aperio Bella Ludovica
- Asai Shoji
- Barklow Timothy
- Chitan Adrian
- Chwastowski Janusz
- Amor Santos Susana
- Carli Tancredi
- Berger Nicolas
- Antipov Egor
- Artoni Giacomo
- Barr Alan
- Beloborodov Konstantin
- Alibocus Samuel
- Bobbink Gerard Jan
- Begalli Marcia
- Alexopoulos Theodoros
- Barisits Martin
- Boscherini Davide
- Braren Früd
- Burr Jonathan
- Ait Tamlihat Malak
- Bahner Daniel
- Baldin Evgenii
- Chekulaev Sergey
- Capua Marcella
- Antel Claire
- Babal Dominik
- Berta Peter
- Boonekamp Maarten
- Angerami Aaron
- Cabrera Urbán Susana
- Baron Moreno Diego
- Balunas William
- Burzynski Jackson
- Aboulhorma Asmaa
- Cheplakov Alexander
- Alvarez Fernandez Adrian
- Barakat Marawan
- Calafiura Paolo
- Cheong Sanha
- Baker Oliver
- Birch-Sykes Callum
- Baines John
- Anisenkov Alexey
- Celli Federico
- Chen Shion
- Cavalli Noemi
- Bethke Siegfried
- Ananiev Viktor
- Bachas Konstantinos
- Celebi Emre
- Alimonti Gianluca
- Afik Yoav
- Albert Justin
- Chiodini Gabriele
- Booth Callum
- Bobrovnikov Viktor
- Basan Alexander
- Agarwala Jinky
- Böhler Michael
- Bokan Petar
- Alpigiani Cristiano
- Beringer Juerg
- Banaś Elżbieta
- Andrean Stefio Yosse
- Aleksa Martin
- Brenner Lydia
- Beaucamp Jean Yves
- Burlayenko Oleksandr
- Cavaliere Viviana
- Barros Maura
- Beretta Matteo Mario
- Austrup Volker Andreas
- Begel Michael
- Bertram Iain
- Chapon Émilien
- Barak Liron
- Buckley Andy
- Bates Richard
- Becker Kathrin
- Catmore James
- Bouchhar Naseem
- Caron Sascha
- Betti Alessandra
- Bandieramonte Marilena
- Burgard Carsten Daniel
- Chen Boping
- Barberis Dario
- Ahmed Waleed Syed
- Addepalli Sagar
- Cai Yizhou
- Bussey Peter John
- Calderini Giovanni
- Beemster L.J.
- Chen Jing
- Castro Nuno
- Bi Ran
- Barranco Navarro Laura
- Cerqueira Augusto
- Barton Adam
- Carlino Gianpaolo
- Al Khoury Konie
- Brooijmans Gustaaf
- Atkin Ryan
- Bakshigupta Debottam
- Chu Xiaotong
- Bernon Florent
- Bourdarios Claire
- Carnesale Maria
- Brandt Oleg
- Camarda Stefano
- Bianco Gianluca
- Butterworth Jonathan
- Auricchio Silvia
- Buescher Volker
- Chizhov Mihail
- Axiotis Konstantinos
- Bellerive Alain
- Bruschi Marco
- Calvetti Milene
- Angelidakis Stylianos
- Balli Fabrice
- Chatterjee Meghranjana
- Brüers Ben
- Abbott Braden
- Cadamuro Luca
- Cheu Elliott
- Assahsah Jihad
- Brandt Gerhard Immanuel
- Bhattacharya Deb Sankar
- Aoki Takumi
- Citron Zvi
- Batlamous Souad
- Bianchi Riccardo Maria
- Chen Huirun
- Benchekroun Driss
- Bona Marcella
- Basso Matthew
- Castillo García Lucía
- Butler John
- Batley Richard
- Citterio Mauro
- Brau Benjamin
- Bernardi Gregorio
- Burton Charles
- Charlton David
- Cerri Alessandro
- Bullard Brendon
- Asai Kanae
- Chen Ye
- Cesarini Gianmario
- Beau Tristan
- Bloch Ingo
- Arnold Hannah
- Amerl Maximilian
- Chisholm Andrew
- Beauchemin Pierre-Hugues
- Benhammou Yan
- Cakir Orhan
- Barreiro Fernando
- Aitbenchikh Brahim
- Bakos Evelin
- Bailey Adam
- Appelt Christian
- Caloba L.P.
- Campanelli Mario
- Camplani Alessandra
- Benjamin Trocme
- Bechtle Philip
- Alegria Zackary
- Brenner Richard
- Abreu Henso
- Chou Yuan-Tang
- Bernius Catrin
- Boveia Antonio
- Barsov Sergey
- Badea Anthony
- Carrió Argos Fernando
- Benoit Mathieu
- Argyropoulos Spyridon
- Bindi Marcello
- Bruce Laura
- Chevalier Laurent
- Bassalat Ahmed
- Ambler Alessandro
- Ames Christoph
- Agheorghiesei Catalin
- Battulga Daariimaa
- Bouquet Romain
- Affolder Anthony
- Ali Shahzad
- Aliev Malik
- Baroncelli Antonio
- Arnaez Olivier
- Avolio Giuseppe
- Aranzabal Nordin
- Bitadze Alexander
- Calvet Samuel
- Brock Ian
- Aoki Masato
- Alvarez Estevez Manuel
- Basson Candice
- Cervelli Alberto
- Allaire Corentin
- Catinaccio Andrea
- Allbrooke Benedict
- Bressler Shikma
- Bruni Alessia
- Arcangeletti Chiara
- Allen Julia Frances
- Bandyopadhyay Anjishnu
- Chu Michael Kwok Lam
- Ali Babar
- Cardoso Silva Júlia Manuela
- Publication venue
- Publication date
- 31/08/2023
- Field of study
No full textMeasurements of longitudinal flow decorrelations in 13 TeV pp and 5.44 TeV Xe+Xe collisions with the ATLAS detector are presented. The measurements are performed using the two-particle correlation method, combining charged-particle tracks within |\eta| < 2.5 with either calorimeter energy clusters or towers within 4.0<|\eta|<4.9. A template-based subtraction procedure is used to remove non-flow effects in both the pp and the Xe+Xe analyses. The dependence of the longitudinal flow decorrelations on the pseudorapidity separation between the particles is characterized via the slope parameter Fn for the elliptic (n=2) and triangular (n=3) harmonic moments. The results are reported as a function of charged-particle multiplicity for the pp and Xe+Xe collision systems. Comparing the data to a color string-based model of the initial geometry indicates that in pp and peripheral Xe+Xe collisions, sub-nucleonic structure and fluctuations in longitudinal energy deposition are needed to describe the data
Measurements of longitudinal flow decorrelations in pp and Xe+Xe collisions with the ATLAS detector
- Author
- Birman Mattias
- Bellos Panagiotis
- Carlino Giampaolo
- Auriol Adrien
- Camarri Paolo
- Alhroob Muhammad
- Beacham James
- Azuelos Georges
- Abicht Nils Julius
- Bevan Adrian
- Burgard Carsten
- Bahmani Marzieh
- Beck Hans Peter
- Casado Lechuga Pilar
- Shelkov G
- Cieri Davide
- Bordulev Iurii
- Buzykaev Alexey
- Cai Huacheng
- Aly Mohamed
- Belfkir Mohamed
- Cerrito Lucio
- Cardillo Fabio
- Chargeishvili Bakar
- Barton Adam Edward
- Baselga Bacardit Marta
- Chen Xin
- Carnelli Alberto
- Abramowicz Halina
- Biswal Jyoti Prakash
- Boyko Igor
- Aparisi Pozo Javier Alberto
- Blumenschein Ulla
- Aranzabal Barrio Nordin
- Chapman John Derek
- Barberio Elisabetta
- Alviggi Mariagrazia
- Canale Vincenzo
- Arguin Jean-Francois
- Chen Andy
- Arling Jan-Hendrik
- Boudreau Joseph
- Carrio Argos Fernando
- Bohm Christian
- Brahimi Nihal
- Castillo Florencia Luciana
- Chakraborty Dhiman
- Carquin Lopez Edson
- Bogdanchikov Alexander
- Beddall Andrew
- Berry Tracey
- Abidi Haider
- Cervato Beatrice
- Abulaiti Yiming
- Calvet David
- Britton David
- Bauce Matteo
- Amos Kieran Robert
- Chomont Arthur
- Atmani Hicham
- Cindro Vladimir
- Chu Ming Chung
- Basson Candice Ruth
- Buanes Trygve
- Biswas Diptaparna
- Brau Benjamin Paul
- Bachacou Henri
- Castillo Gimenez Victoria
- Barbero Marlon Benoit
- Bhopatkar Vallary Shashikant
- Alonso Francisco
- Camerlingo Maria Teresa
- Bracinik Juraj
- Akbiyik Melike
- Battaglia Marco
- Antonelli Mario
- Baltes Lisa Marie
- Castillo Garcia Lucia
- Chen Shenjian
- Bhamjee Muaaz
- Bakshi Gupta Debottam
- Behera Arabinda
- Cheung Kingman
- Becherer Fabian
- Caspar Maximilian
- Cheremushkina Evgeniya
- Aggarwal Anamika
- Chapon Emilien
- Callea Giuseppe
- Biglietti Michela
- Chiarelli Giorgio
- Bagnaia Paolo
- Burdin Sergey
- Chowdhury Tasnuva
- Abeling Kira
- Carlson Ben
- Burr Jon
- Bellagamba Lorenzo
- Biondini Alessandro
- Choi Kyungeon
- Abbott Braden Keim
- Cabrera Urban Susana
- Centonze Martino Salomone
- Aizenberg Iakov
- Bruckman de Renstrom Pawel
- Chow Edwin
- Akiyama Daiya
- Bachiu Alexander
- Ai Xiaocong
- Baker Keith
- Bendebba Fatima
- Baroncelli Toni
- Buxo Vazquez Carlos Josue
- Carter Joseph
- Chiarella Vitaliano
- Boye Diallo
- Ahmadov Faig
- Bella Gideon
- Apyan Aram
- Brost Elizabeth
- Cao Yumeng
- Alderweireldt Sara
- Carratta Giuseppe
- Cardenas Juan Carlos
- Boyd Jamie
- Bergmann Benedikt Ludwig
- Allendes Flores Cristian Andres
- Balakrishnan Veena
- Backman Karl Filip
- Bailey Virginia
- Bulekov Oleg
- Carlotto Juan Ignacio
- Ali Hanadi
- Andeen Timothy Robert
- Barr Jackson
- Atkinson Markus Julian
- Amelung Christoph
- Chan Jay
- Chiedde Nemer
- Schimmel Brener Roy
- Borissov Guennadi
- Aparo Marco
- Annovi Alberto
- Chen Hucheng
- Cavasinni Vincenzo
- Alexa Calin
- Akimov Andrei
- Ciesla Krzysztof
- Cirotto Francesco
- Aloisio Alberto
- Bruscino Nello
- Carlson Evan Michael
- Buttinger Will
- Chen Jiayi
- Bee Chris
- Calvet Thomas Philippe
- Cheng Alkaid
- Beermann Thomas
- Blumenthal Julian
- Booth Callum Dale
- Cardarelli Roberto
- Chen Maggie
- Alfonsi Fabrizio
- Cherepanova Elizaveta
- Bielski Rafal
- Affolder Tony
- Bortoletto Daniela
- Akesson Torsten
- Ciocio Alessandra
- Cameron David
- Adamczyk Leszek
- Aielli Giulio
- Albouy Guillaume Lucas
- Alkakhi Wael
- Bhatta Somadutta
- Cepaitis Vilius
- Bensinger Jim
- Bentvelsen Stan
- Aad Georges
- Ballabene Eric
- Barel Marten Zefanja
- Barron Uriel
- Biryukov Stanislav
- Bisanz Tobias
- Balek Petr
- Bartels Falk
- Fernandez-Bosman Martine
- Charlton Dave
- Barreiro Guimaraes da Costa Joao
- Batool Binish
- Cerutti Fabio
- Arbiol Val Sergio Javier
- Algren Malte
- Ahuja Sudha
- Bobbink Gerjan
- Calace Noemi
- Alexandrov Igor
- Bruce Laura Elaine
- Anastopoulos Christos
- Arce Ayana Tamu
- Bogavac Danijela
- Adelman Jahred
- Baron Petr
- Cantero Garcia Josu
- Cai Yuchen
- Caforio Davide
- Anulli Fabio
- Allport Philip Patrick
- Bini Cesare
- Berthold Anne-Sophie
- Chudoba Jiri
- Adye Tim
- Akolkar Nilima Nilesh
- Bazzano Tomas
- Andreazza Attilio
- Caloba Luiz
- Bauer Michael
- Bruni Graziano
- Alibocus Samuel William
- Bartos Pavol
- Boumediene Djamel Eddine
- Barends Kevin Nicholas
- Bauer Patrick
- Bingul Ahmet
- Beisiegel Florian
- Burzynski Jackson Carl
- Asada Haruka
- Brooks William King
- Chekanov Sergei
- Bruers Ben
- Carducci Giovandomenico
- Adam Bourdarios Claire
- Ahmad Ammara
- Amidei Dante
- Bold Tomasz
- Chan Wai Yuen
- Chitishvili Mariam
- Alberghi Gian Luigi
- Adiguzel Aytul
- Bartoldus Rainer
- Chauhan Chainika
- Chisholm Andrew Stephen
- Boisvert Veronique
- Albicocco Pietro
- Canesse Auriane
- Bergeaas Kuutmann Elin
- Carbone Antonio
- Astalos Robert
- Baines Luke
- Bansal Shubham
- Bisceglie Emanuele
- Braren Frued Erik
- Alves Cardoso Mario
- Bhattarai Prajita
- Cerri Alex
- Bhalla Naman Kumar
- Chen Xiang
- Balz Johannes
- Britzger Daniel Andreas
- Buchin Daniel
- Capocasa Francesca
- Balasubramanian Rahul
- Bednyakov Vadim
- Asbah Nedaa Alexandra
- Biros Marek
- Basso Matthew Joseph
- Arena Eloisa
- Augsten Kamil
- Barreiro Alonso Fernando
- Burger Angela Maria
- Agaras Merve Nazlim
- Carra Sonia
- Beemster Lars
- Argyropoulos Spyros
- Biebel Otmar
- Bomben Marco
- Bouaouda Khalil
- Cekmecelioglu Yusuf Can
- Calfayan Philippe
- Chen Charlie
- Camacho Toro Reina Coromoto
- Buat Quentin
- Aikot Arya
- Aperio Bella Ludovica
- Asai Shoji
- Borecka-Bielska Hanna Maria
- Chitan Adrian
- Anders John Kenneth
- Chwastowski Janusz
- Brown Leesa Marea
- Carli Tancredi
- Berger Nicolas
- Antipov Egor
- Artoni Giacomo
- Barr Alan
- Beloborodov Konstantin
- Begalli Marcia
- Alexopoulos Theodoros
- Beirer Joshua Falco
- Cheng Hok Chuen Tom
- Barisits Martin
- Boscherini Davide
- Camarero Munoz Daniel
- Atmasiddha Prachi
- Ait Tamlihat Malak
- Bahner Daniel
- Baldin Evgenii
- Chekulaev Sergey
- Capua Marcella
- Antel Claire
- Babal Dominik
- Berta Peter
- Boonekamp Maarten
- Angerami Aaron
- Bird Gareth Adam
- Aboulhorma Asmaa
- Do Amaral Coutinho Yara
- Cheplakov Alexander
- Behr Janna Katharina
- Alvarez Fernandez Adrian
- Barakat Marawan
- Calafiura Paolo
- Cheong Sanha
- Barklow Tim
- Baines John
- Anisenkov Alexey
- Celli Federico
- Baron Diego
- Chen Shion
- Cavalli Noemi
- Bethke Siegfried
- Ananiev Viktor
- Bachas Konstantinos
- Boehler Michael
- Carminati Leonardo
- Celebi Emre
- Alimonti Gianluca
- Afik Yoav
- Albert Justin
- Chiodini Gabriele
- Bobrovnikov Viktor
- Basan Alexander
- Agarwala Jinky
- Bokan Petar
- Alpigiani Cristiano
- Beringer Juerg
- Andrean Stefio Yosse
- Aleksa Martin
- Brenner Lydia
- Beaucamp Jean Yves
- Burlayenko Oleksandr
- Cavaliere Viviana
- Atkin Ryan Justin
- Barros Maura
- Addison Matt
- Beretta Matteo Mario
- Atashi Rose
- Austrup Volker Andreas
- Begel Michael
- Bertram Iain
- Barak Liron
- Buckley Andy
- Balunas William Keaton
- Bates Richard
- Becker Kathrin
- Catmore James
- Bouchhar Naseem
- Caron Sascha
- Cherkaoui Rajaa
- Betti Alessandra
- Bandieramonte Marilena
- Chen Boping
- Barberis Dario
- Ahmed Waleed Syed
- Addepalli Sagar
- Cai Yizhou
- Bussey Peter John
- Calderini Giovanni
- Chen Jing
- Cairo Valentina
- Castro Nuno
- Bi Ran
- Cetin Serkant
- Barranco Navarro Laura
- Al Khoury Konie
- Brooijmans Gustaaf
- Bjoerke Kristian
- Chu Xiaotong
- Bernon Florent
- Burghgrave Blake Oliver
- Carnesale Maria
- Brandt Oleg
- Camarda Stefano
- Bianco Gianluca
- Birch-Sykes Callum Jacob
- Butterworth Jonathan
- Auricchio Silvia
- Berrocal Guardia Adrian
- Buescher Volker
- Chizhov Mihail
- Alegria Zackary Lee
- Axiotis Konstantinos
- Bellerive Alain
- Bruschi Marco
- Bossio Jonathan
- Calvetti Milene
- Angelidakis Stylianos
- Balli Fabrice
- Chatterjee Meghranjana
- Cadamuro Luca
- Cheu Elliott
- Assahsah Jihad
- Brandt Gerhard Immanuel
- Bhattacharya Deb Sankar
- Aoki Takumi
- Citron Zvi
- Batlamous Souad
- Bianchi Riccardo Maria
- Chen Huirun
- Borbely Albert Gyorgy
- Benchekroun Driss
- Bona Marcella
- Bouhova-Thacker Eva
- Bohm Burkhard
- Buttar Craig Macleod
- Batley Richard
- Bernardi Gregorio
- Carter Thomas Michael
- Burton Charles
- Banas Elzbieta
- Bullard Brendon
- Asai Kanae
- Chen Ye
- Blue Andrew James
- Cesarini Gianmario
- Beau Tristan
- Bloch Ingo
- Arnold Hannah
- Amerl Maximilian
- Beauchemin Pierre-Hugues
- Benhammou Yan
- Cakir Orhan
- Aitbenchikh Brahim
- Bakos Evelin
- Beresford Lydia Audrey
- Bailey Adam
- Appelt Christian
- Campanelli Mario
- Camplani Alessandra
- Anthony Matthew Thomas
- Bechtle Philip
- Brenner Richard
- Amor dos Santos Susana Patricia
- Brau Jim
- Abreu Henso
- Chou Yuan-Tang
- Bernius Catrin
- Boveia Antonio
- Barsov Sergey
- Acharya Bobby Samir
- Badea Anthony
- Cerny Karel
- Camincher Clement
- Benoit Mathieu
- Barone Gaetano
- Bindi Marcello
- Chevalier Laurent
- Bassalat Ahmed
- Ambler Alessandro
- Ames Christoph
- Agheorghiesei Catalin
- Santiago Cerqueira Augusto
- Battulga Daariimaa
- Bouquet Romain
- Ali Shahzad
- Aliev Malik
- Arnaez Olivier
- Avolio Giuseppe
- Bitadze Alexander
- Calvet Samuel
- Brock Ian
- Aoki Masato
- Alvarez Estevez Manuel
- Bernlochner Florian Urs
- Cervelli Alberto
- Allaire Corentin
- Busch Elena Laura
- Catinaccio Andrea
- Barillari Teresa
- Allbrooke Benedict
- Bressler Shikma
- Bruni Alessia
- Arcangeletti Chiara
- Allen Julia Frances
- Butler John Mark
- Assamagan Ketevi Adikle
- Bruckler Tim Lukas
- Bandyopadhyay Anjishnu
- Chu Michael Kwok Lam
- Ali Babar
- Publication venue
- Publication date
- 07/09/2023
- Field of study
No full textInternational audienceMeasurements of longitudinal flow decorrelations in 13 TeV pp and 5.44 TeV Xe+Xe collisions with the ATLAS detector are presented. The measurements are performed using the two-particle correlation method, combining charged-particle tracks within ∣η∣<2.5 with either calorimeter energy clusters or towers within 4.0<∣η∣<4.9. A template-based subtraction procedure is used to remove non-flow effects in both the pp and the Xe+Xe analyses. The dependence of the longitudinal flow decorrelations on the pseudorapidity separation between the particles is characterized via the slope parameter Fn for the elliptic (n=2) and triangular (n=3) harmonic moments. The results are reported as a function of charged-particle multiplicity for the pp and Xe+Xe collision systems. Comparing the data to a color string-based model of the initial geometry indicates that in pp and peripheral Xe+Xe collisions, sub-nucleonic structure and fluctuations in longitudinal energy deposition are needed to describe the data
Test of CP invariance in Higgs boson vector-boson-fusion production using the H → γγ channel with the ATLAS detector
- Author
- Catmore J.R
- G. Khoriauli
- Smizanska M
- Introzzi G.
- A. Lanza
- A. W. Fortman
- Wolter M W
- R. Ushioda
- G. Eigen
- Aguilar-Saavedra J. A.
- Carminati L.
- Cantero J.
- E. Etzion
- Carlotto J. I.
- B. Brickwedde
- Cetin S.A
- Vannicola D
- Borissov G.
- Brüers B.
- E. Jones
- Readioff N P
- Hellman S
- Leopold A
- Pizzini A
- Korn A.
- Y. Smirnov
- Bhopatkar V. S.
- D. Chakraborty
- Catmore J.R.
- Munoz Martinez J L
- J. M. Seixas
- Kupfer T.
- Heidorn W. D.
- Berthold A.
- Kourlitis E
- Hamdaoui H.
- Hawkings R. J.
- Jakoubek T
- Polifka R
- T. Pan
- Cairo V.M.M
- Amaral Coutinho Y
- J. W. S. Carter
- Mochizuki K
- Huang S.
- J. Tojo
- Oyulmaz K Y
- A. J. Gomez Delegido
- P. Gessinger-Befurt
- M. Villa
- Abreu H
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- P. Berta
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- M. Mazza
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- Sultanaliyeva L
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- Kitsaki C
- Chekulaev S.V.
- D. Schaile
- Lee A C A
- C. D. Burgard
- Prades Ibanez A
- A. A. Myers
- Boumediene D.
- D. Varouchas
- Poettgen R
- Iguchi R.
- Akimov A.V
- M. R. Sutton
- H. Kroha
- Nagy E
- D. Pudzha
- B. Dong
- E. Kajomovitz
- M. Belfkir
- L. Tompkins
- K. De
- M. Marinescu
- Vilucchi E
- Hays C P
- Liu M Y
- Kiehn M.
- Sebastiani C D
- Bhopatkar V. S.
- A. Salvador Salas
- Chitan A.
- K. R. Amos
- V. S. Martoiu
- Dias F A
- Nakahama Y
- Nikolaenko V
- Pacheco Pages A
- I. Brock
- Loffredo S
- Owen M
- Burr J.T.P
- E. Higón-Rodriguez
- Publication venue
- Publication date
- 01/01/2023
- Field of study
No full textA test of
C
P
invariance in Higgs boson production via vector-boson fusion has been performed in the
H
→
γ
γ
channel using
139
fb
−
1
of proton-proton collision data at
√
s
=
13
TeV
collected by the ATLAS detector at the LHC. The optimal observable method is used to probe the
C
P
structure of interactions between the Higgs boson and electroweak gauge bosons, as described by an effective field theory. No sign of
C
P
violation is observed in the data. Constraints are set on the parameters describing the strength of the
C
P
-odd component in the coupling between the Higgs boson and the electroweak gauge bosons in two effective field theory bases:
˜
d
in the HISZ basis and
c
H
˜
W
in the Warsaw basis. The results presented are the most stringent constraints on
C
P
violation in the coupling between Higgs and weak bosons. The 95% C.L. constraint on
˜
d
is derived for the first time and the 95% C.L. constraint on
c
H
˜
W
has been improved by a factor of 5 compared to the previous measurement
Search for a resonance decaying into a scalar particle and a Higgs boson in final states with leptons and two photons in proton-proton collisions at s = 13 TeV with the ATLAS detector
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- Barreiro F.
- Ackermann A.
- Brock R.
- Bartos P.
- Ciubotaru D. A.
- Casado M. P.
- Boumediene D.
- Cheng H. C.
- Cerri A.
- Centonze M. S.
- Anisenkov A. V.
- Brahimi N.
- Bhide K. D.
- Citterio M.
- Adelman J.
- Arguin J. -F.
- Bernlochner F. U.
- Calvet S.
- Baer T. M.
- Cavalli N.
- Bracinik J.
- Bachacou H.
- Capua M.
- Aggarwal A.
- Biebel O.
- Alexa C.
- Catinaccio A.
- Bandieramonte M.
- Beemster L. J.
- Chapman J. D.
- Boyko I. R.
- Alviggi M. G.
- Carmignani J.
- Chan J.
- Bokan P.
- Abeling K.
- Axiotis K.
- Alves Cardoso M.
- Balakrishnan V.
- Arnold H.
- Beauchemin P. H.
- Choi K.
- Akbiyik M.
- Beck H. P.
- Begalli M.
- Buscher V.
- Camarda S.
- Cerrito L.
- Bakos E.
- Balli F.
- Chitishvili M.
- Burleson J.
- Cherepanova E.
- Cheu E.
- Assamagan K.
- Buttinger W.
- Cardenas J. C. J.
- Afik Y.
- Cella S.
- Caviedes Betancourt L. J.
- Publication venue
- Publication date
- 01/01/2024
- Field of study
No full textA search for a hypothetical heavy scalar particle, X, decaying into a singlet scalar particle, S, and a Standard Model Higgs boson, H, using 140 fb−1 of proton-proton collision data at the centre-of-mass energy of 13 TeV recorded with the ATLAS detector at the LHC is presented. The explored mass range is 300 ≤ mX ≤ 1000 GeV and 170 ≤ mS ≤ 500 GeV. The signature of this search is one or two leptons (e or μ) from the decay of vector bosons originating from the S particle, S → W±W∓/ZZ, and two photons from the Higgs boson decay, H → γγ. No significant excess is observed above the expected Standard Model background. The observed (expected) upper limits at the 95% confidence level on the cross- section for gg → X → SH, assuming the same S → WW/ZZ branching ratios as for a SM-like heavy Higgs boson, are between 530 (800) fb and 120 (170) fb
Measurement of vector boson production cross sections and their ratios using pp collisions at √s=13.6 TeV with the ATLAS detector
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- Buscher V.
- Bassalat A
- Bakos E.
- Balli F.
- Chitishvili M.
- Cherepanova E.
- Cheu E.
- Blumenthal J
- Boudet L
- Assamagan K.
- Akbiyik M
- Buttinger W.
- Afik Y.
- Publication venue
- Publication date
- 01/01/2024
- Field of study
No full textFiducial and total W± and Z boson cross sections, their ratios and the ratio of top-antitop-quark pair and W-boson fiducial cross sections are measured in proton–proton collisions at a centre-of-mass energy of s=13.6 TeV, corresponding to an integrated luminosity of 29 fb−1 of data collected in 2022 by the ATLAS experiment at the Large Hadron Collider. The measured fiducial cross-section values for W+→l+ν, W−→l−ν ̄, and Z→l+l− (l=e or μ) boson productions are 4250±150 pb, 3310±120 pb, and 744±20 pb, respectively, where the uncertainty is the total uncertainty, including that arising from the luminosity of about 2.2%. The measurements are in agreement with Standard-Model predictions calculated at next-to-next-to-leading-order in αs, next-to-next-to-leading logarithmic accuracy and next-to-leading-order electroweak accuracy
Search for boosted low-mass resonances decaying into hadrons produced in association with a photon in pp collisions at s = 13 TeV with the ATLAS detector
- Author
- Barberio E. L.
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- Balakrishnan V.
- Arnold H.
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- Choi K.
- Akbiyik M.
- Beck H. P.
- Begalli M.
- Buscher V.
- Camarda S.
- Cerrito L.
- Bakos E.
- Balli F.
- Chitishvili M.
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- Cherepanova E.
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- Afik Y.
- Cella S.
- Caviedes Betancourt L. J.
- Publication venue
- Publication date
- 01/01/2025
- Field of study
No full textMany extensions of the Standard Model, including those with dark matter particles, propose new mediator particles that decay into hadrons. This paper presents a search for such low mass narrow resonances decaying into hadrons using 140 fb−1 of proton-proton collision data recorded with the ATLAS detector at a centre-of-mass energy of 13 TeV. The resonances are searched for in the invariant mass spectrum of large-radius jets with two-pronged substructure that are recoiling against an energetic photon from initial state radiation, which is used as a trigger to circumvent limitations on the maximum data recording rate. This technique enables the search for boosted hadronically decaying resonances in the mass range 20–100 GeV hitherto unprobed by the ATLAS Collaboration. The observed data are found to agree with Standard Model predictions and 95% confidence level upper limits are set on the coupling of a hypothetical new spin-1 Z′ resonance with Standard Model quarks as a function of the assumed Z′-boson mass in the range between 20 and 200 GeV
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