93 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
- Abud AA
- Abulaiti Y
- Acharya BS
- Achkar B
- Adachi S
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- Adamek L
- Adelman J
- Adersberger M
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- Trigger IM
- Trincaz-Duvoid S
- Trischuk DA
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- Trocme B
- Trofymov A
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- Zhao Z
- Zhemchugov A
- Zheng Z
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- Zieminska D
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- 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
- '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
Guidance to 2018 good practice : ARIA digitally-enabled, integrated, person-centred care for rhinitis and asthma
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- Aberer W
- Agache I
- Agache I
- Akdis CA
- Akdis M
- Aliberti MR
- Almeida R
- Amat F
- Angles R
- Annesi-Maesano I
- Annesi-Maesano I
- Ansotegui IJ
- Ansotegui IJ
- Anto JM
- Anto JM
- Arnavielhe S
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- Arshad H
- Asarnoj A
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- Bateman ED
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- Bedbrook A
- Bedbrook A
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- Beghe B
- Bel EH
- Bennoor KS
- Benson M
- Bergmann KC
- Bergmann KC
- Bertorello L
- Bewick M
- Bewick M
- Bialek S
- Bialoszewski AZ
- Bieber T
- Bindslev-Jensen C
- Bindslev-Jensen C
- Bjermer L
- Blain H
- Blain H
- Blasi F
- Blua A
- Bogado DM
- Bogus-Buczynska I
- Boner AL
- Bonini M
- Bonini S
- Bonniaud P
- Bosnic-Anticevich CS
- Bosnic-Anticevich S
- Bosse I
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- Bouchard J
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- Boulet LP
- Bourret R
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- Braido F
- Briedis V
- Brightling CE
- Brozek J
- Brusselle G
- Bucca C
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- Buonaiuto R
- Burte E
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- Cecchi L
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- Chavannes NH
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- Chen Y
- Chiron R
- Chivato T
- Chkhartishvili E
- Christoff G
- Chu DK
- Chuchalin AG
- Chung KF
- Ciaravolo MM
- Ciceran A
- Cingi C
- Ciprandi G
- Cisneros MO
- Coehlo ACC
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- Coll J
- Conforti D
- Cortes-Grimaldo RM
- Corti F
- Costa E
- Costa E
- Costa-Dominguez MC
- Courbis AL
- Cox L
- Crescenzo M
- Cruz AA
- Cruz AA
- Custovic A
- Czarlewski W
- Czarlewski W
- D'Amato G
- Da Silva J
- Da Silva J
- Dahlen SE
- Dario C
- Darsow U
- Dauvilliers Y
- Dauvilliers Y
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- Eller E
- Eller E
- Emerson MDF
- Emuzyte R
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- Ferrero J
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- Fontaine JF
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- Fuentes-Perez JM
- Galvez-Romero JL
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- Maurer M
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- Mayora O
- Medina-Avalos MA
- Melen E
- Melen E
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- Meltzer EO
- Menditto E
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- Mercier J
- Miculinic N
- Mihaltan F
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- Mohammad Y
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- Nyembue TD
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- Odzhakova C
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- Okubo K
- Onorato GL
- Onorato GL
- Ouedraogo S
- Pali-Scholl I
- Palkonen S
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- Panaitescu C
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- Papadopoulos NG
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- Papi A
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- Passalacqua G
- Paulino E
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- Persico M
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- Scadding GK
- Schmid-Grendelmeier P
- Schmidt-Grendelmeier P
- Schunemann HJ
- Schunemann HJ
- Scichilone N
- Serpa FS
- Serpa FS
- Shamai S
- Sheikh A
- Sheikh A
- Sierra M
- Simons FER
- Siroux V
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- Walker S
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- Wallace D
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- Wang DY
- Waserman S
- Waserman S
- Werfel T
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- Wickman M
- Williams DM
- Williams S
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- Wilson N
- Wright J
- Wroczynski P
- Yakovliev P
- Yawn BP
- Yiallouros PK
- Yorgancioglu A
- Yorgancioglu A
- Yusuf OM
- Zar HJ
- Zernotti ME
- Zernotti ME
- Zhanat I
- Zhang L
- Zhong N
- Zidarn M
- Zuberbier T
- Zuberbier T
- Zubrinich C
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- Publication venue
- Publication date
- 01/01/2019
- Field of study
AimsMobile Airways Sentinel NetworK (MASK) belongs to the Fondation Partenariale MACVIA-LR of Montpellier, France and aims to provide an active and healthy life to rhinitis sufferers and to those with asthma multimorbidity across the life cycle, whatever their gender or socio-economic status, in order to reduce health and social inequities incurred by the disease and to improve the digital transformation of health and care. The ultimate goal is to change the management strategy in chronic diseases.MethodsMASK implements ICT technologies for individualized and predictive medicine to develop novel care pathways by a multi-disciplinary group centred around the patients.StakeholdersInclude patients, health care professionals (pharmacists and physicians), authorities, patient's associations, private and public sectors.ResultsMASK is deployed in 23 countries and 17 languages. 26,000 users have registered.EU grants (2018)MASK is participating in EU projects (POLLAR: impact of air POLLution in Asthma and Rhinitis, EIT Health, DigitalHealthEurope, Euriphi and Vigour).Lessons learnt(i) Adherence to treatment is the major problem of allergic disease, (ii) Self-management strategies should be considerably expanded (behavioural), (iii) Change management is essential in allergic diseases, (iv) Education strategies should be reconsidered using a patient-centred approach and (v) Lessons learnt for allergic diseases can be expanded to chronic diseases.Peer reviewe
Search for Higgs boson pair production in the two bottom quarks plus two photons final state in pp collisions at root s=13 TeV with the ATLAS detector
- Author
- Aad G
- Abbott B
- Abbott D
- Abed Abud A
- Abeling K
- Abhayasinghe D
- Abidi S
- Abramowicz H
- Abreu H
- Abulaiti Y
- Abusleme Hoffman A
- Acharya B
- Achkar B
- Adam Bourdarios C
- Adam L
- Adamczyk L
- Adamek L
- Adelman J
- Adiguzel A
- Adorni S
- Adye T
- Affolder A
- Afik Y
- Agapopoulou C
- Agaras M
- Agarwala J
- Aggarwal A
- Agheorghiesei C
- Aguilar-Saavedra J
- Ahmad A
- Ahmadov F
- Ahmed W
- Ai X
- Aielli G
- Akatsuka S
- Akbiyik M
- Akimov A
- Al Khoury K
- Alberghi G
- Albert J
- Alconada Verzini M
- Alderweireldt S
- Aleksa M
- Aleksandrov I
- Alexa C
- Alexopoulos T
- Alfonsi A
- Alfonsi F
- Alhroob M
- Ali B
- Ali S
- Aliev M
- Alimonti G
- Allaire C
- Allbrooke B
- Allport P
- Aloisio A
- Alonso F
- Alpigiani C
- Alunno Camelia E
- Alvarez Estevez M
- Alviggi M
- Amaral Coutinho Y
- Ambler A
- Ambroz L
- Amelung C
- Amidei D
- Amor Dos Santos S
- Amoroso S
- Amrouche C
- Anastopoulos C
- Andari N
- Andeen T
- Anders J
- Andrean S
- Andreazza A
- Andrei V
- Angelidakis S
- Angerami A
- Anisenkov A
- Annovi A
- Antel C
- Anthony M
- Antipov E
- Antonelli M
- Antrim D
- Anulli F
- Aoki M
- Aparisi Pozo J
- Aparo M
- Aperio Bella L
- Aranzabal N
- Araujo Ferraz V
- Arcangeletti C
- Arce A
- Arena E
- Arguin J
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- Tzamarias S
- Tzanis P
- Tzovara E
- Uchida K
- Ukegawa F
- Unal G
- Unal M
- Undrus A
- Unel G
- Ungaro F
- Uno K
- Urban J
- Urquijo P
- Usai G
- Ushioda R
- Usman M
- Uysal Z
- Vacek V
- Vachon B
- Vadla K
- Vafeiadis T
- Valderanis C
- Valdes Santurio E
- Valente M
- Valentinetti S
- Valero A
- Vallance R
- Vallier A
- Valls Ferrer J
- Valéry L
- Van Daalen T
- Van Gemmeren P
- Van Stroud S
- Van Vulpen I
- Vanadia M
- Vandelli W
- Vandenbroucke M
- Vandewall E
- Vannicola D
- Vannoli L
- Vari R
- Varnes E
- Varni C
- Varol T
- Varouchas D
- Varvell K
- Vasile M
- Vaslin L
- Vasquez G
- Vazeille F
- Vazquez Furelos D
- Vazquez Schroeder T
- Veatch J
- Vecchio V
- Veen M
- Veliscek I
- Veloce L
- Veloso F
- Veneziano S
- Ventura A
- Verbytskyi A
- Verducci M
- Vergis C
- Verissimo De Araujo M
- Verkerke W
- Vermeulen A
- Vermeulen J
- Vernieri C
- Verschuuren P
- Vesterbacka M
- Vetterli M
- Viaux Maira N
- Vickey Boeriu O
- Vickey T
- Viehhauser G
- Vigani L
- Villa M
- Villaplana Perez M
- Villhauer E
- Vilucchi E
- Vincter M
- Virdee G
- Vishwakarma A
- Vittori C
- Vivarelli I
- Vladimirov V
- Voevodina E
- Vogel M
- Vokac P
- Von Ahnen J
- von Buddenbrock S
- Von Toerne E
- Vorobel V
- Vorobev K
- Vos M
- Vossebeld J
- Vozak M
- Vozdecky L
- Vranjes Milosavljevic M
- Vranjes N
- Vrba V
- Vreeswijk M
- Vu N
- Vuillermet R
- Vukotic I
- Wada S
- Wagner C
- Wagner P
- Wagner W
- Wahdan S
- Wahlberg H
- Wakasa R
- Wakida M
- Walbrecht V
- Walder J
- Walker R
- Walker S
- Walkowiak W
- Wang A
- Wang C
- Wang H
- Wang J
- Wang P
- Wang R
- Wang S
- Wang T
- Wang W
- Wang X
- Wang Y
- Wang Z
- Wanotayaroj C
- Warburton A
- Ward C
- Ward R
- Warrack N
- Watson A
- Watson M
- Watts G
- Waugh B
- Webb A
- Weber C
- Weber M
- Weber S
- Wei C
- Wei Y
- Weidberg A
- Weingarten J
- Weirich M
- Weiser C
- Wenaus T
- Wendland B
- Wengler T
- Wenig S
- Wermes N
- Wessels M
- Whalen K
- Wharton A
- White A
- White M
- Whiteson D
- Wiedenmann W
- Wiel C
- Wielers M
- Wieseotte N
- Wiglesworth C
- Wiik-Fuchs L
- Wilbern D
- Wilkens H
- Wilkins L
- Williams D
- Williams H
- Williams S
- Willocq S
- Windischhofer P
- Wingerter-Seez I
- Winklmeier F
- Winter B
- Wittgen M
- Wobisch M
- Wolf A
- Wollrath J
- Wolter M
- Wolters H
- Wong V
- Wongel A
- Worm S
- Wosiek B
- Woźniak K
- Wraight K
- Wu J
- Wu S
- Wu X
- Wu Y
- Wu Z
- Wuerzinger J
- Wyatt T
- Wynne B
- Wölker R
- Xella S
- Xiang J
- Xiao X
- Xie X
- Xiotidis I
- Xu D
- Xu H
- Xu L
- Xu R
- Xu T
- Xu W
- Xu Y
- Xu Z
- Yabsley B
- Yacoob S
- Yamaguchi N
- Yamaguchi Y
- Yamatani M
- Yamauchi H
- Yamazaki T
- Yamazaki Y
- Yan J
- Yan S
- Yan Z
- Yang H
- Yang S
- Yang T
- Yang X
- Yang Y
- Yang Z
- Yao W
- Yap Y
- Ye H
- Ye J
- Ye S
- Yeletskikh I
- Yexley M
- Yin P
- Yorita K
- Yoshihara K
- Young C
- Yuan R
- Yue X
- Zaazoua M
- Zabinski B
- Zacharis G
- Zaffaroni E
- Zaitsev A
- Zakareishvili T
- Zakharchuk N
- Zambito S
- Zanzi D
- Zeitnitz C
- Zeißner S
- Zemaityte G
- Zeng J
- Zenin O
- Zenz S
- Zerradi S
- Zerwas D
- Zgubič M
- Zhang B
- Zhang D
- Zhang G
- Zhang J
- Zhang K
- Zhang L
- Zhang M
- Zhang R
- Zhang S
- Zhang X
- Zhang Z
- Zhao P
- Zhao Y
- Zhao Z
- Zhemchugov A
- Zheng Z
- Zhong D
- Zhou B
- Zhou C
- Zhou H
- Zhou N
- Zhou Y
- Zhu C
- Zhu H
- Zhu J
- Zhu Y
- Zhuang X
- Zhukov K
- Zhulanov V
- Zieminska D
- Zimine N
- Zimmermann S
- Ziolkowski M
- Zoccoli A
- Zoch K
- Zorbas T
- Zormpa O
- Zou W
- Zwalinski L
- Åkesson T
- Öncel Ö
- Ženiš T
- Živković L
- Publication venue
- Publication date
- 01/01/2022
- Field of study
Operation and performance of the ATLAS Tile Calorimeter in Run 1
- Author
- Aaboud M
- Aad G
- Abbott B
- Abdallah J
- Abdinov O
- Abeloos B
- Abhayasinghe DK
- Abidi SH
- Abouelfadl 
- 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
- Akerstedt H
- Akilli E
- Akimov AV
- Alberghi GL
- Albert J
- Albicocco P
- Alconada Verzini MJ
- Alderweireldt S
- Aleksa M
- Aleksandrov IN
- Alexa C
- Alexander G
- 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 
- Alviggi MG
- Amadio BT
- Amaral Coutinho Y
- Ambroz L
- Amelung C
- Amidei D
- Amor 
- 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
- Aperio Bella L
- Arabidze G
- Arai Y
- Araque JP
- Araujo Ferraz V
- Arce ATH
- Ardell RE
- Arduh FA
- Argos FC
- Arguin J-
- Argyropoulos S
- Armadans R
- Armbruster AJ
- Armitage LJ
- Armstrong A
- Arnaez O
- Arnold H
- Arratia M
- Arslan O
- Artamonov A
- Artoni G
- Artz S
- Asai S
- Asbah N
- Ashkenazi A
- Asimakopoulou EM
- Asquith L
- Assamagan K
- Astalos R
- Astigarraga ME
- Atkin RJ
- Atkinson M
- Atlay NB
- Auerbach B
- Augsten K
- Avolio G
- Avramidou R
- Axen B
- Ayoub MK
- Azuelos G
- Álvarez Piqueras D
- Åkesson TPA
- Baas AE
- Baca MJ
- Bachacou H
- Bachas K
- Backes M
- Bagnaia P
- Bahilo JJL
- Bahmani M
- Bahrasemani H
- Bailey AJ
- Baines JT
- Bajic M
- Bakalis C
- Baker OK
- Bakker PJ
- 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
- Barillari T
- Barisits M
- Barkeloo J
- Barklow T
- Barlow N
- Barnea R
- Barnes SL
- Barnett BM
- Barnett RM
- Barnovska-Blenessy Z
- Baroncelli A
- Barone G
- Barr AJ
- Barranco Navarro L
- Barreiro Guimarães da Costa J
- 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
- Beattie MD
- Beau T
- Beauchemin PH
- 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
- Bell AS
- Bella G
- Bellagamba L
- Bellerive A
- Bello FA
- Bellomo M
- Belotskiy K
- Belyaev NL
- Benary O
- Benchekroun D
- Bender M
- Benekos N
- Benhammou Y
- Benhar Noccioli E
- Benitez J
- Benjamin DP
- Benoit M
- Bensinger JR
- Bentvelsen S
- Beresford L
- Beretta M
- Berge D
- Bergeaas Kuutmann E
- Berger N
- Bergsten LJ
- Beringer J
- Berlendis S
- Bernard NR
- Bernardi G
- Bernius C
- Bernlochner FU
- Berry T
- Berta P
- Bertella C
- Bertoli G
- Bertram IA
- Besjes GJ
- Bessidskaia Bylund O
- Bessner M
- Besson N
- Bethani A
- Bethke S
- Betti A
- Bevan AJ
- Beyer J
- Bianchi RM
- Biebel O
- Biedermann D
- Bielski R
- Bierwagen K
- Biesuz NV
- Biglietti M
- Billoud TRV
- Bindi M
- Bingul A
- Bini C
- Biondi S
- Bisanz T
- Biswal JP
- Bittrich C
- Bjergaard DM
- Black JE
- Black KM
- Blair RE
- Blazek T
- Bloch I
- Blocker C
- Blue A
- Blumenschein U
- Blunier D
- Bobbink GJ
- Bobrovnikov VS
- Bocchetta SS
- Bocci A
- Boerner D
- Bogavac D
- Bogdanchikov AG
- Bohm C
- Boisvert V
- Bokan P
- Bold T
- Boldyrev AS
- Bolz AE
- Bomben M
- Bona M
- Bonilla JS
- Boonekamp M
- Borisov A
- Borissov G
- Bortfeldt J
- Bortoletto D
- Bortolotto V
- Boscherini D
- Bosman M
- Bossio Sola JD
- Bostanabad M
- Bouaouda K
- Boudreau J
- Bouhova-Thacker EV
- Boumediene D
- Bourdarios C
- Boutle SK
- Boveia A
- Boyd J
- Boyko IR
- Bozson AJ
- Bracinik J
- Brahimi N
- Brandt A
- Brandt G
- Brandt O
- Braren F
- Bratzler U
- Brau B
- Brau JE
- Breaden Madden WD
- Brendlinger K
- Brennan AJ
- Brenner L
- Brenner R
- Bressler S
- Brickwedde B
- Briglin DL
- Britton D
- Britzger D
- Brock I
- Brock R
- Brooijmans G
- Brooks T
- Brooks WK
- Brost E
- Broughton JH
- Brown H
- Bruckman de Renstrom PA
- Bruncko D
- Bruni A
- Bruni G
- Bruni LS
- Bruno S
- Brunt BH
- Bruschi M
- Bruscino N
- Bryant P
- Bryngemark L
- Buanes T
- Buat Q
- Buchholz P
- Buckley AG
- Budagov IA
- Bugge MK
- Bulekov O
- Bullock D
- Burch TJ
- Burdin S
- Burgard CD
- Burger AM
- Burghgrave B
- Burka K
- Burke S
- Burmeister I
- Burr JTP
- Busato E
- Buschmann E
- Bussey P
- Butler JM
- Buttar CM
- Butterworth JM
- Butti P
- Buttinger W
- Buzatu A
- Buzykaev AR
- Bührer F
- Büscher D
- Büscher V
- Cabras G
- Cabrera Urbán S
- Caforio D
- Cai H
- Cairo VMM
- Cakir I
- Cakir O
- Calace N
- Calafiura P
- Calandri A
- Calderini G
- Calfayan P
- Callea G
- Caloba LP
- Calvente Lopez S
- Calvet D
- Calvet S
- Calvet TP
- Calvetti M
- Camacho Toro R
- Camarda S
- Camarri P
- Cameron D
- Caminal 
- Camincher C
- Campana S
- Campanelli M
- Camplani A
- Campoverde A
- Canale V
- Cano Bret M
- Cantero J
- Cao T
- Cao Y
- Capeans Garrido MDM
- Caprini I
- Caprini M
- Capua M
- Carbone RM
- Cardarelli R
- Cardillo FC
- Carli I
- Carli T
- Carlino G
- Carlson BT
- Carminati L
- Carney RMD
- Caron S
- Carquin E
- Carrá S
- Carrillo-Montoya GD
- Casadei D
- Casado MP
- Casha AF
- Casolino M
- Casper DW
- Castelijn R
- Castillo Gimenez V
- Castillo FL
- Castro NF
- Catinaccio A
- Catmore JR
- Cattai A
- Caudron J
- Cavaliere V
- Cavallaro E
- Cavalli D
- Cavalli-Sforza M
- Cavasinni V
- Celebi E
- Ceradini F
- Cerda Alberich L
- Cerqueira AS
- Cerri A
- Cerrito L
- Cerutti F
- Cervelli A
- Cetin SA
- Chafaq A
- Chakraborty D
- Chan SK
- Chan WS
- Chan YL
- Chang P
- Chapman JD
- Charlton DG
- Chau CC
- Chavez Barajas CA
- Che S
- Chegwidden A
- Chekanov S
- Chekulaev SV
- Chelkov GA
- Chelstowska MA
- Chen C
- Chen CH
- Chen H
- Chen J
- Chen J
- Chen S
- Chen SJ
- Chen X
- Chen Y
- Chen Y
- Cheng HC
- Cheng HJ
- Cheplakov A
- Cheremushkina E
- Cherkaoui El Moursli R
- Cheu E
- Cheung K
- Chevalier L
- Chiarella V
- Chiarelli G
- Chiodini G
- Chisholm AS
- Chitan A
- Chiu I
- Chiu YH
- Chizhov MV
- Choi K
- Chomont AR
- Chouridou S
- Chow YS
- Christodoulou V
- Chu MC
- Chudoba J
- Chuinard AJ
- Chwastowski JJ
- Chytka L
- Ciaccio A
- Ciaccio L
- Cinca D
- Cindro V
- Cioară IA
- Ciocio A
- Cirotto F
- Citron ZH
- Citterio M
- Clark A
- Clark MR
- Clark PJ
- Clement C
- Clemente WK
- Coadou Y
- Cobal M
- Coccaro A
- Cochran J
- Coimbra AEC
- Colasurdo L
- Cole B
- Colijn AP
- Collot J
- Conde Muiño P
- Coniavitis E
- Connell SH
- Connelly IA
- Constantinescu S
- Conventi F
- Cooper-Sarkar AM
- Cormier F
- Cormier KJR
- Corradi M
- Correia AM
- Corrigan EE
- Corriveau F
- Cortes-Gonzalez A
- Costa MJ
- Costanzo D
- Cottin G
- Cowan G
- Cox BE
- Crane J
- Cranmer K
- Crawley SJ
- Creager RA
- Cree G
- Crescioli F
- Crépé-Renaudin S
- Cristinziani M
- Croft V
- Crosetti G
- Cueto A
- Cuhadar Donszelmann T
- Cukierman AR
- Cunha 
- Curatolo M
- Cúth J
- Czekierda S
- Czodrowski P
- Da Via C
- Da 
- Dabrowski W
- Dado T
- Dahbi S
- Dai T
- Dallaire F
- Dallapiccola C
- Dam M
- Damp J
- Dandoy JR
- Daneri MF
- Dang NP
- Dann ND
- Danninger M
- Dao V
- Darbo G
- Darmora S
- Dartsi O
- Dattagupta A
- Daubney T
- Davey W
- David C
- Davidek T
- Davis DR
- Davydov Y
- Dawe E
- Dawson I
- De Asmundis R
- De Benedetti A
- De Castro S
- De Cecco S
- De Groot N
- de Jong P
- De la Torre H
- De Lorenzi F
- De Maria A
- De Moura 
- De Pedis D
- De Salvo A
- De Sanctis U
- De Santo A
- De Vasconcelos Corga K
- De Vivie 
- De 
- De 
- De K
- Debenedetti C
- Dedovich DV
- Dehghanian N
- Del Gaudio M
- Del Peso J
- Delgado A
- Delgove D
- Deliot F
- Delitzsch CM
- Della Pietra M
- Della Volpe D
- Dell’Acqua A
- Dell’Asta L
- Delmastro M
- Delporte C
- Delsart PA
- DeMarco DA
- Demers S
- Demichev M
- Denisov SP
- Denysiuk D
- Derendarz D
- Derkaoui JE
- Derue F
- Dervan P
- Desch K
- Deterre C
- Dette K
- Devesa MR
- Deviveiros PO
- Dewhurst A
- Dhaliwal S
- Di 
- Di 
- Di 
- Di 
- Di 
- Di 
- Di 
- Di 
- Di 
- Di 
- Di 
- Di 
- Diaconu C
- Diamond M
- Dias 
- Dias FA
- Diaz LP
- Diaz MA
- Dickinson J
- Diehl EB
- Dietrich J
- Dimitrievska A
- Dingfelder J
- Dittus F
- Díez Cornell S
- Djama F
- Djobava T
- Djuvsland JI
- Do 
- Do 
- Dobre M
- Dodsworth D
- Doglioni C
- Dolejsi J
- Dolezal Z
- Donadelli M
- Donato C
- Donini J
- Dopke J
- Doria A
- Dortz O
- Dos 
- Dova MT
- Doyle AT
- Drechsler E
- Dreyer E
- Dreyer T
- Dris M
- Du Y
- Duarte-Campderros J
- Dubinin F
- Dubreuil A
- Duchovni E
- Duckeck G
- Ducourthial A
- Ducu OA
- Duda D
- Dudarev A
- Dudder AC
- Duffield EM
- Duflot L
- Dumancic M
- Dumitriu AE
- Duncan AK
- Dunford M
- Duperrin A
- Duran 
- Durglishvili A
- Duschinger D
- Dutta B
- Duvnjak D
- Dührssen M
- Dülsen C
- Düren M
- Dyndal M
- Dysch S
- Dziedzic BS
- D’amen G
- D’Auria S
- D’Eramo L
- D’onofrio A
- D’Onofrio M
- Eckardt C
- Ecker KM
- Edgar RC
- Eifert T
- Eigen G
- Einsweiler K
- Ekelof T
- El Kacimi M
- El Kosseifi R
- Ellajosyula V
- Ellert M
- Ellinghaus F
- Elliot AA
- Ellis N
- Elmsheuser J
- Elsing M
- Emeliyanov D
- Enari Y
- Ennis JS
- Epland MB
- Erdmann J
- Ereditato A
- Errede S
- Escalier M
- Escobar C
- Esposito B
- Estrada 
- Etienvre AI
- Etzion E
- Evans H
- Ezhilov A
- Ezzi M
- Fabbri F
- Fabbri L
- Fabiani V
- Facini G
- Faisca 
- Fakhrutdinov RM
- Falciano S
- Falke PJ
- Falke S
- Faltova J
- Fang Y
- Fanti M
- Farbin A
- Farilla A
- Farina EM
- Farooque T
- Farrell S
- Farrington SM
- Farthouat P
- Fassi F
- Fassnacht P
- Fassouliotis D
- Faucci Giannelli M
- Favareto A
- Fawcett WJ
- Fayard L
- Fedin OL
- Fedorko W
- Feickert M
- Feigl S
- Feligioni L
- Feng C
- Feng EJ
- Feng M
- Fenton MJ
- Fenyuk AB
- Feremenga L
- Ferrando J
- Ferrari A
- Ferrari P
- Ferrari R
- Ferreira de Lima DE
- Ferrer A
- Ferrere D
- Ferretti C
- Fiedler F
- Filipčič A
- Filthaut F
- Finelli KD
- Fiolhais MCN
- Fiorini L
- Fischer C
- Fisher WC
- Flaschel N
- Fleck I
- Fleischmann P
- Fletcher RRM
- Flick T
- Flierl BM
- Flores Castillo LR
- Flores LM
- Fomin N
- Forcolin GT
- Formica A
- Forti AC
- Foster AG
- Fournier D
- Fox H
- Förster FA
- Fracchia S
- Francavilla P
- Franchini M
- Franchino S
- Francis D
- Franconi L
- Franklin M
- Frate M
- Fraternali M
- Freeborn D
- Fressard-Batraneanu SM
- Freund B
- Freund WS
- Froidevaux D
- Frost JA
- Fukunaga C
- Furelos D
- Fusayasu T
- Fuster J
- Gabizon O
- Gabrielli A
- Gabrielli A
- Gach GP
- Gadatsch S
- Gadow P
- Gagliardi G
- Gagnon LG
- Galea C
- Galhardo B
- Gallas EJ
- Gallop BJ
- Gallus P
- Galster G
- Gamboa 
- Gan KK
- Ganguly S
- Gao Y
- Gao YS
- Garcia RF
- Garcia-Sciveres M
- García Navarro JE
- García Pascual JA
- García C
- Gardner RW
- Garelli N
- Garonne V
- Gasnikova K
- Gaudiello A
- Gaudio G
- Gavrilenko IL
- Gavrilyuk A
- Gay C
- Gaycken G
- Gazis EN
- Gee CNP
- Geisen J
- Geisen M
- Geisler MP
- Gellerstedt K
- Gemme C
- Genest MH
- Geng C
- Gentile S
- Gentsos C
- George S
- Gerbaudo D
- Gessner G
- Ghasemi 
- Ghasemi S
- Ghneimat M
- Giacobbe B
- Giagu S
- Giangiacomi N
- Giannetti P
- Gibson SM
- Gignac M
- Gillberg D
- Gilles G
- Gingrich DM
- Giordani MP
- Giorgi FM
- Giraud PF
- Girolamo A
- Giromini P
- Giugliarelli G
- Giugni D
- Giuli F
- Giulini M
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- Zur 
- Zwalinski L
- Ženiš T
- Živković L
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2018
- Field of study
The Tile Calorimeter is the hadron calorimeter covering the central region of the ATLAS experiment at the Large Hadron Collider. Approximately 10,000 photomultipliers collect light from scintillating tiles acting as the active material sandwiched between slabs of steel absorber. This paper gives an overview of the calorimeter’s performance during the years 2008–2012 using cosmic-ray muon events and proton–proton collision data at centre-of-mass energies of 7 and 8TeV with a total integrated luminosity of nearly 30 fb−1. The signal reconstruction methods, calibration systems as well as the detector operation status are presented. The energy and time calibration methods performed excellently, resulting in good stability of the calorimeter response under varying conditions during the LHC Run 1. Finally, the Tile Calorimeter response to isolated muons and hadrons as well as to jets from proton–proton collisions is presented. The results demonstrate excellent performance in accord with specifications mentioned in the Technical Design Report
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
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- Aad G
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- Abdinov O
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- Yildirim E
- Yildiz HD
- Yorita K
- Yoshihara K
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- Yu J
- Yu J
- Yue X
- Yuen SPY
- Zabinski B
- Zacharis G
- Zaffaroni E
- Zaidan R
- Zaitsev AM
- Zakareishvili T
- Zakharchuk N
- Zalieckas J
- Zambito S
- Zanzi D
- Zaripovas DR
- Zeissner SV
- Zeitnitz C
- Zemaityte G
- Zeng JC
- Zeng Q
- Zenin O
- Zenis T
- Zerwas D
- Zgubic M
- Zhang D
- Zhang DF
- Zhang F
- Zhang G
- Zhang H
- Zhang J
- Zhang L
- Zhang L
- Zhang M
- Zhang P
- Zhang R
- Zhang R
- Zhang X
- Zhang Y
- Zhang Z
- Zhao P
- Zhao X
- Zhao Y
- Zhao Z
- Zhemchugov A
- Zhou B
- Zhou C
- Zhou L
- Zhou M
- Zhou MS
- Zhou N
- Zhou Y
- Zhu CG
- Zhu H
- Zhu HL
- Zhu J
- Zhu Y
- Zhuang X
- Zhukov K
- 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
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
- AbouZeid OS
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- 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
Measurement of Azimuthal Anisotropy of Muons from Charm and Bottom Hadrons in pp Collisions at √s = 13 TeV with the ATLAS Detector
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- Aad G
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- Shaikh NW
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- Smirnov N
- Smirnov SY
- Smirnov Y
- Smirnova LN
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- Smizanska M
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- Soldatov EY
- Soldevila U
- Solis AL
- Solodkov AA
- Soloshenko A
- Solovyanov OV
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- Strubig A
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- Stupak J
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- Su D
- Su J
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- Sugaya Y
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- Sultan DMS
- Sultansoy S
- Sumida T
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- Sun X
- Suruliz K
- Suster CJE
- Sutton MR
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- Svatos M
- Swiatlowski M
- Swift SP
- Sydorenko A
- Sykora I
- Sykora T
- Ta D
- Tackmann K
- Taenzer J
- Taffard A
- Tafirout R
- Tahirovic E
- Taiblum N
- Takai H
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- Takeshita T
- Takubo Y
- Talby M
- Talyshev AA
- Tanaka J
- Tanaka M
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- Tapprogge S
- Tarem S
- Tarna G
- Tartarelli GF
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- Tasevsky M
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- Taylor AJ
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- Taylor PTE
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- Theveneaux-Pelzer T
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- Thomsen LA
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- Tian Y
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- Tikhonov YA
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- Tripiana MF
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- Trofymov A
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- Tsiskaridze V
- Tskhadadze EG
- Tsukerman II
- Tsulaia V
- Tsuno S
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- Tudorache A
- Tudorache V
- Tulbure TT
- Tuna AN
- Turchikhin S
- Turgeman D
- Turra R
- Tuts PM
- Tzovara E
- Ucchielli G
- Ueda I
- Ughetto M
- Ukegawa F
- Unal G
- Undrus A
- Unel G
- Ungaro FC
- Unno Y
- Uno K
- Urban J
- Urquijo P
- Urrejola P
- Usai G
- Usui J
- Vacavant L
- Vacek V
- Vachon B
- Vadla KOH
- Vaidya A
- Valderanis C
- Valente M
- Valentinetti S
- Valero A
- Valery L
- Vallance RA
- Vallier A
- Valls Ferrer JA
- Van Daalen TR
- Van der Graaf H
- Van Gemmeren P
- Van Nieuwkoop J
- Van Vulpen I
- Vanadia M
- Vandelli W
- Vaniachine A
- Vankov P
- Vari R
- Varnes EW
- Varni C
- Varol T
- Varouchas D
- Varvell KE
- Vasquez GA
- Vasquez JG
- Vazeille F
- Vazquez Furelos D
- Vazquez Schroeder T
- Vazquez JGP
- Veatch J
- Vecchio V
- Veloce LM
- Veloso F
- Veneziano S
- Ventura A
- Venturi M
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- Vera AMR
- Vercesi V
- Verducci M
- Vergara JCR
- Vergis C
- Verkerke W
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- Vermeulen JC
- Verzini MJA
- Vetterli MC
- Vichou I
- Vickey T
- Viehhauser GHA
- Viel S
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- Villar DIN
- Vilucchi E
- Vincter MG
- Vinogradov VB
- Vishwakarma A
- Vittori C
- Vivarelli I
- Vlachos S
- Vogel M
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- von Buddenbrock SE
- Von Toerne E
- Vorobel V
- Vorobev K
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- Vuillermet R
- Vukotic I
- Wagner P
- Wagner W
- Wagner-Kuhr J
- Wahlberg H
- Wahrmund S
- Wakamiya K
- Walbrecht VM
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- Walker R
- Walker SD
- Walkowiak W
- Wallangen V
- Wang AM
- Wang C
- Wang F
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- Wanotayaroj C
- Warburton A
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- Washbrook A
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- Webb AF
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- Weber MS
- Weber SA
- Weber SM
- Weidberg AR
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- Weingarten J
- Weirich M
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- Whalen K
- Whallon NL
- Wharton AM
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- White MJ
- White R
- Whiteson D
- Whitmore BW
- Wickens FJ
- Wiedenmann W
- Wielers M
- Wiglesworth C
- Wiik-Fuchs LAM
- Wildauer A
- Wilk F
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- Wilkins LJ
- Williams HH
- Williams S
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- Willocq S
- Wilson JA
- Wingerter-Seez I
- Winkels E
- Winklmeier F
- Winston OJ
- Winter BT
- Wittgen M
- Wobisch M
- Wolf A
- Wolf TMH
- Wolff R
- Wolter MW
- Wolters H
- Wong VWS
- Woods NL
- Worm SD
- Wosiek BK
- Wozniak KW
- Wraight K
- Wu M
- Wu SL
- Wu X
- Wu Y
- Wyatt TR
- Wynne BM
- Xella S
- Xi Z
- Xia L
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- Xu H
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- Xu W
- Yabsley B
- Yacoob S
- Yajima K
- Yallup DP
- Yamaguchi D
- Yamaguchi Y
- Yamamoto A
- Yamanaka T
- Yamane F
- Yamatani M
- Yamazaki T
- Yamazaki Y
- Yan Z
- Yang HJ
- Yang HT
- Yang S
- Yang Y
- Yang Z
- Yao W-M
- Yap YC
- Yasu Y
- Yatsenko E
- Ye J
- Ye S
- Yeletskikh I
- Yigitbasi E
- Yildirim E
- Yildiz HD
- Yorita K
- Yoshihara K
- Young C
- Young CJS
- Yu J
- Yu J
- Yue X
- Yuen SPY
- Zabinski B
- Zacharis G
- Zaffaroni E
- Zaidan R
- Zaitsev AM
- Zakareishvili T
- Zakharchuk N
- Zalieckas J
- Zambito S
- Zanzi D
- Zaripovas DR
- Zeissner SV
- Zeitnitz C
- Zemaityte G
- Zeng JC
- Zeng Q
- Zenin O
- Zenis T
- Zerwas D
- Zgubic M
- Zhang D
- Zhang DF
- Zhang F
- Zhang G
- Zhang H
- Zhang J
- Zhang L
- Zhang L
- Zhang M
- Zhang P
- Zhang R
- Zhang R
- Zhang X
- Zhang Y
- Zhang Z
- Zhao P
- Zhao X
- Zhao Y
- Zhao Z
- Zhemchugov A
- Zhou B
- Zhou C
- Zhou L
- Zhou M
- Zhou MS
- Zhou N
- Zhou Y
- Zhu CG
- Zhu H
- Zhu HL
- Zhu J
- Zhu Y
- Zhuang X
- Zhukov K
- 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
- 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
Search for heavy diboson resonances in semileptonic final states in pp collisions at s√=13 TeV with the ATLAS detector
- Author
- Aaboud M
- Aad G
- Abbott B
- Abdinov O
- Abeloos B
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- Publication venue
- 'Springer Fachmedien Wiesbaden GmbH'
- Publication date
- 17/12/2020
- Field of study
This paper reports on a search for heavy resonances decaying into WW, ZZ or WZ using proton–proton collision data at a centre-of-mass energy of s√=13 TeV. The data, corresponding to an integrated luminosity of 139 fb1, were recorded with the ATLAS detector from 2015 to 2018 at the Large Hadron Collider. The search is performed for final states in which one W or Z boson decays leptonically, and the other W boson or Z boson decays hadronically. The data are found to be described well by expected backgrounds. Upper bounds on the production cross sections of heavy scalar, vector or tensor resonances are derived in the mass range 300–5000 GeV within the context of Standard Model extensions with warped extra dimensions or including a heavy vector triplet. Production through gluon–gluon fusion, Drell–Yan or vector-boson fusion are considered, depending on the assumed model
Search for heavy neutral Higgs bosons produced in association with b-quarks and decaying into b-quarks at root s=13 TeV with the ATLAS detector
- Author
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- Yigitbasi E
- Yildiz HD
- Yorita K
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- Yuen SPY
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- Zahreddine J
- Zaitsev AM
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- Zakharchuk N
- Zambito S
- Zanzi D
- Zaripovas DR
- Zeiner S
- Zeitnitz C
- Zemaityte G
- Zeng JC
- Zenin O
- Zenis T
- Zerwas D
- Zgubic M
- Zhang DF
- Zhang F
- 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
- Zhou C
- Zhou M
- 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 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
- 13/08/2020
- Field of study
A search for heavy neutral Higgs bosons produced in association with one or two
b
-quarks and decaying to
b
-quark pairs is presented using
27.8
fb
−
1
of
√
s
=
13
TeV
proton-proton collision data recorded by the ATLAS detector at the Large Hadron Collider during 2015 and 2016. No evidence of a signal is found. Upper limits on the heavy neutral Higgs boson production cross section times its branching ratio to
b
¯
b
are set, ranging from 4.0 to 0.6 pb at 95% confidence level over a Higgs boson mass range of 450 to 1400 GeV. Results are interpreted within the two-Higgs-doublet model and the minimal supersymmetric Standard Model
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
- Ashkenazi A
- Asimakopoulou EM
- Asquith L
- Assamagan K
- Astalos R
- Astigarraga MEP
- Atkin RJ
- Atkinson M
- Atlay NB
- Augsten K
- Avolio G
- Avramidou R
- Ayoub MK
- Azuelos G
- Baas AE
- Baca MJ
- Bachacou H
- Bachas K
- Backes M
- Bagnaia P
- Bahmani M
- Bahrasemani H
- Bailey AJ
- Baines JT
- Bajic M
- Bakalis C
- Baker OK
- Bakker PJ
- 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
- Barkeloo J
- Barklow T
- Barlow N
- Barnea R
- Barnes SL
- Barnett BM
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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
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