273 research outputs found
Search for new phenomena in final states with an energetic jet and large missing transverse momentum in pp collisions at √ s = 8 TeV with the ATLAS detector
- Author
- Aad G
- Abbott B
- Abbott DC
- Abeling K
- Abhayasinghe DK
- Abidi SH
- AbouZeid OS
- Abraham NL
- Abramowicz H
- Abreu H
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- 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
Recommended from our members
Expert consensus document: The International Scientific Association for Probiotics and Prebiotics (ISAPP) consensus statement on the definition and scope of prebiotics
- Author
- A Campananti
- A Costabile
- A Drakoularakou
- A Everard
- A Firmansyah
- A Koh
- A Kulinich
- A McMillan
- A Verbrugghe
- AL Morrow
- AM Armanian
- AY Albert
- BJ Marriage
- BTS Beserra
- C Hill
- CA Cuello-Garcia
- CA Lozupone
- Catherine Stanton
- CE Stevens
- CJ Apanavicius
- D Baines
- D Dang
- D Garrido
- DA Osborn
- DB Silk
- DC Savage
- E Barengolts
- E Boets
- E Elison
- E Pruszynska-Oszmalek
- E Sherwin
- EE Canfora
- EL Propst
- EM Dewulf
- EMMF Gouveia
- F Depeint
- F Respondek
- F Respondek
- F Respondek
- F Shannahan
- G Moro
- G Reid
- G Rogler
- Glenn R. Gibson
- GR Gibson
- GR Gibson
- GR Gibson
- Gregor Reid
- HA Paul
- HL Simpson
- HM Savignac
- I Coste
- J Schrezenmeir
- J Verspreet
- J Vulevic
- J Vulevic
- J Vulevic
- JA Delcour
- JA Parnell
- JA Parnell
- JD Quigley III
- JH Cho
- JL Pluznick
- K Kanakupt
- K Miyazaki
- K Schmidt
- Karen Scott
- KB Hong
- KC Goehring
- Kelly S. Swanson
- Kristin Verbeke
- L Bomar
- L Holloway
- L McCabe
- LA David
- LB Bindels
- LC Paulino
- LF Rettger
- LM Morgan
- LT Ortiz
- M Bednarczyk
- M Depner
- M Duenas
- M Giovannini
- M Kano
- M Malaguarnera
- M Pineiro
- M Radke
- M Roberfroid
- MA Antonio
- MA Underwood
- MA van de Pol
- Mary Ellen Sanders
- MJ Blaser
- MLA De Leoz
- MN Clifford
- MR Charbonneau
- MR Charbonneau
- MU Sohail
- NJ Correa-Matos
- NJ Kellow
- NM Delzenne
- NW Griffin
- P Chatchatee
- P Li
- P Liu
- P Louis
- Patrice D. Cani
- PD Cani
- PD Cani
- PD Cani
- PM Roodposhti
- R Closa-Monasterolo
- R Dubos
- R Luoto
- R Oozeer
- R Shanmugasundaram
- RA Rastall
- RA Rastall
- Raylene A. Reimer
- RB Canani
- RCR Martinez
- RJ Boyle
- Robert Hutkins
- RW Hutkins
- S Christodoulides
- S Collins
- S Ghosh
- S Lohner
- S Rockova
- S Sarbini
- SA Abrams
- SA Joyce
- Seppo J. Salminen
- SH Hoseinifar
- SH Hoseinifar
- SH Park
- SJ O'Keefe
- SL Prescott
- SM Kuo
- SM Roto
- SP Verhoef
- Susan L. Prescott
- T Matsuki
- TM Che
- TM Marques
- V de Preter
- V Halas
- V Madhok
- VM Korshonov
- Y Ben David
- Y He
- Y Valdez
- YA Ghouri
- YJ Goh
- YY Kim
- Z Gao
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2017
- Field of study
In December 2016, a panel of experts in microbiology, nutrition and clinical research was convened by the International Scientific Association for Probiotics and Prebiotics to review the definition and scope of prebiotics. Consistent with the original embodiment of prebiotics, but aware of the latest scientific and clinical developments, the panel updated the definition
of a prebiotic: a substrate that is selectively utilized by host microorganisms conferring a health benefit. This definition expands the concept of prebiotics to possibly include non-carbohydrate substances, applications to body sites other than the gastrointestinal tract, and diverse categories other than food. The requirement for selective microbiota-mediated mechanisms was retained. Beneficial health effects must be documented for a substance to be considered a prebiotic. The consensus definition applies also to prebiotics for use by animals, in which microbiota-focused strategies to maintain health and prevent disease is as relevant as for humans. Ultimately, the goal of this Consensus Statement is to engender appropriate use of the term ‘prebiotic’ by relevant stakeholders so that consistency and clarity can be achieved in research reports, product marketing and regulatory oversight of the category. To this end, we have reviewed several aspects of prebiotic science including its development, health benefits and legislation
Combined measurement of differential and total cross sections in the H → γγ and the H → ZZ* → 4ℓ decay channels at s=13 TeV with the ATLAS detector
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- Perepelitsa DV
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- Ristić B
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- Rusakovich NA
- Russell HL
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- Ruthmann N
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- Rybar M
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- Ryu S
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- Rzehorz GF
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- Schäfer U
- Sciandra A
- Sciolla G
- Scornajenghi M
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- Sebastiani CD
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- Sekhon K
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- Shabalina E
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- Shaikh NW
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- Sharma A
- Sharma AS
- Shatalov PB
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- Shaw SM
- Shcherbakova A
- Shen Y
- Sherafati N
- Sherman AD
- Sherwood P
- Shi L
- Shimizu S
- Shimmin CO
- Shimojima M
- Shipsey IPJ
- Shirabe S
- Shiyakova M
- Shlomi J
- Shmeleva A
- Shoaleh Saadi D
- Shochet MJ
- Shojaii S
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- Siragusa G
- Siral I
- Sivoklokov SY
- Sjölin J
- Skinner MB
- Skubic P
- Slater M
- Slavicek T
- Slawinska M
- Sliwa K
- Slovak R
- Smakhtin V
- Smart BH
- Smiesko J
- Smirnov N
- Smirnov SY
- Smirnov Y
- Smirnova LN
- Smirnova O
- Smith JW
- Smith MNK
- Smith RW
- Smizanska M
- Smolek K
- Snesarev AA
- Snyder IM
- Snyder S
- Sobie R
- Soffa AM
- Soffer A
- Soh DA
- Sokhrannyi G
- Solans Sanchez CA
- Solar M
- Soldatov EY
- Soldevila U
- Solodkov AA
- Soloshenko A
- Solovyanov OV
- Solovyev V
- Sommer P
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- Song W
- Sopczak A
- Sopkova F
- Sosa D
- Sotiropoulou CL
- Sottocornola S
- Soualah R
- Soukharev AM
- South D
- Sowden BC
- Spagnolo S
- Spalla M
- Spangenberg M
- Spanò F
- Sperlich D
- Spettel F
- Spieker TM
- Spighi R
- Spigo G
- Spiller LA
- Spiteri DP
- Spousta M
- Stabile A
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- Starovoitov P
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- Svatos M
- Swiatlowski M
- Swift SP
- Sydorenko A
- Sykora I
- Sykora T
- Sánchez J
- Søgaard A
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- Taenzer J
- Taffard A
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- Tahirovic E
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- Takeshita T
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- Talby M
- Talyshev AA
- Tanaka J
- Tanaka M
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- Tapia Araya S
- Tapprogge S
- Tarek Abouelfadl Mohamed A
- Tarem S
- Tarna G
- Tartarelli GF
- Tas P
- Tasevsky M
- Tashiro T
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- Tayalati Y
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- Thomsen LA
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- Tian Y
- Ticse Torres RE
- Tikhomirov VO
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- Timoshenko S
- Tipton P
- Tisserant S
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- Todt S
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- Tokushuku K
- Tokár S
- Tolley E
- Tomiwa KG
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- Torrence E
- Torres H
- Torró Pastor E
- Tosciri C
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- Tovey DR
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- Tskhadadze EG
- Tsukerman II
- Tsulaia V
- Tsuno S
- Tsybychev D
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- Tulbure TT
- Tuna AN
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- Turgeman D
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- Ucchielli G
- Ueda I
- Ughetto M
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- Unal G
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- 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
- Valdes Santurio E
- Valente M
- Valentinetti S
- Valero A
- Vallance RA
- Vallier A
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- Valéry L
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- Van Gemmeren P
- Van Nieuwkoop J
- Van Vulpen I
- Van Woerden MC
- Vanadia M
- Vandelli W
- Vaniachine A
- Vankov P
- Vari R
- Varnes EW
- Varni C
- Varol T
- Varouchas D
- Vartapetian A
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- Vazeille F
- Vazquez Furelos D
- Vazquez Schroeder T
- Veatch J
- Vecchio V
- Veloce LM
- Veloso F
- Veneziano S
- Ventura A
- Venturi M
- Venturi N
- Vercesi V
- Verducci M
- Vergel Infante CM
- Verkerke W
- Vermeulen AT
- Vermeulen JC
- Vetterli MC
- Viaux Maira N
- Viazlo O
- Vichou I
- Vickey Boeriu OE
- Vickey T
- Viehhauser GHA
- Viel S
- Vigani L
- Villa M
- Villaplana Perez M
- Vilucchi E
- Vincter MG
- Vinogradov VB
- Vishwakarma A
- Vittori C
- Vivarelli I
- Vlachos S
- Vogel M
- Vokac P
- Volpi G
- Von Buddenbrock SE
- Von Toerne E
- Vorobel V
- Vorobev K
- Vos M
- Vossebeld JH
- Vranjes Milosavljevic M
- Vranjes N
- Vrba V
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- Vuillermet R
- Vukotic I
- Wagner P
- Wagner W
- Wagner-Kuhr J
- Wahlberg H
- Wahrmund S
- Wakamiya K
- Walbrecht VM
- Walder J
- Walker R
- Walkowiak W
- Wallangen V
- Wang AM
- Wang C
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- Wanotayaroj C
- Warburton A
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- Weidberg AR
- Weinert B
- Weingarten J
- Weirich M
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- Wengler T
- Wenig S
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- Werner MD
- Werner P
- Wessels M
- Weston TD
- 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
- Wilkens HG
- Wilkins LJ
- Williams HH
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- Willis C
- 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
- Woźniak KW
- Wraight K
- Wu M
- Wu SL
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- Wu Y
- Wyatt TR
- Wynne BM
- Xella S
- Xi Z
- Xia L
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- Xu H
- Xu L
- Xu T
- 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
- Yorita K
- Yoshihara K
- Young C
- Young CJS
- Yu J
- Yu J
- Yue X
- Yuen SPY
- Yusuff I
- Zabinski B
- Zacharis G
- Zaffaroni E
- Zaidan R
- Zaitsev AM
- Zakharchuk N
- Zalieckas J
- Zambito S
- Zanzi D
- Zaripovas DR
- Zeitnitz C
- Zeißner SV
- Zemaityte G
- Zeng JC
- Zeng Q
- Zenin O
- Zerwas D
- Zgubič M
- Zhang D
- Zhang DF
- Zhang F
- Zhang G
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- Zhang J
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- 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
- 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
- Elsevier
- Publication date
- 01/01/2018
- Field of study
A combined measurement of differential and inclusive total cross sections of Higgs boson production is performed using 36.1 fb−1 of 13 TeV proton–proton collision data produced by the LHC and recorded by the ATLAS detector in 2015 and 2016. Cross sections are obtained from measured H→γγ and H→ZZ*(→4ℓ event yields, which are combined taking into account detector efficiencies, resolution, acceptances and branching fractions. The total Higgs boson production cross section is measured to be 57.0−5.9 +6.0 (stat.) −3.3 +4.0 (syst.) pb, in agreement with the Standard Model prediction. Differential cross-section measurements are presented for the Higgs boson transverse momentum distribution, Higgs boson rapidity, number of jets produced together with the Higgs boson, and the transverse momentum of the leading jet. The results from the two decay channels are found to be compatible, and their combination agrees with the Standard Model predictions
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
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- 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
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- Alhroob M
- Ali B
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- Allen BW
- Allport PP
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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
Performance of missing transverse momentum reconstruction with the ATLAS detector using proton–proton collisions at √s = 13 TeV
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- Zhemchugov A
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- Zorbas TG
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- Zur Nedden M
- Zwalinski L
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2018
- Field of study
The performance of the missing transverse momentum (EmissT) reconstruction with the ATLAS detector is evaluated using data collected in proton–proton collisions at the LHC at a centre-of-mass energy of 13 TeV in 2015. To reconstruct EmissT, fully calibrated electrons, muons, photons, hadronically decaying τ -leptons, and jets reconstructed from calorimeter energy deposits and charged-particle tracks are used. These are combined with the soft hadronic activity measured by reconstructed charged-particle tracks not associated with the hard objects. Possible double counting of contributions from reconstructed charged-particle tracks from the inner detector, energy deposits in the calorimeter, and reconstructed muons from the muon spectrometer is avoided by applying a signal ambiguity resolution procedure which rejects already used signals when combining the various EmissT contributions. The individual terms as well as the overall reconstructed EmissT are evaluated with various performance metrics for scale (linearity), resolution, and sensitivity to the data-taking conditions. The method developed to determine the systematic uncertainties of the EmissT scale and resolution is discussed. Results are shown based on the full 2015 data sample corresponding to an integrated luminosity of 3.2 fb−1
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
- Akesson TPA
- Akilli E
- Akimov AV
- Al Khoury K
- Alberghi GL
- Alberich LC
- Albert J
- Alconada Verzini MJ
- Alderweireldt S
- Aleksa M
- Aleksandrov IN
- Alexa C
- Alexandre D
- Alexopoulos T
- Alfonsi A
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- Zhemchugov A
- Zheng Z
- Zhong D
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- Zieminska D
- Zimine NI
- 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
- 01/01/2019
- 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
Search for High-Mass Resonances Decaying to τν in pp Collisions at √s=13 TeV with the ATLAS Detector
- Author
- Aaboud M
- Aad G
- Abbott B
- Abdinov O
- Abeloos B
- Abidi SH
- AbouZeid OS
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- Alconada Verzini MJ
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- Aleksandrov IN
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- Casadei D
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- Castelijn R
- Castillo Gimenez V
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- Cavasinni V
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- Charlton DG
- Chau CC
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- Damazio D Oliveira
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- Yildiz H Duran
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- Yusuff I
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- Zalieckas J
- Zambito S
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- Zemaityte G
- Zeng JC
- Zeng Q
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- Zhemchugov A
- Zhou B
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- Zhou M
- Zhou M
- Zhou N
- Zhou Y
- Zhu CG
- Zhu H
- Zhu H
- 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
- Zu Theenhausen H Meyer
- zur Nedden M
- Zwalinski L
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2018
- Field of study
A search for high-mass resonances decaying to τν using proton-proton collisions at √s=13 TeV produced by the Large Hadron Collider is presented. Only τ-lepton decays with hadrons in the final state are considered. The data were recorded with the ATLAS detector and correspond to an integrated luminosity of 36.1 fb−1. No statistically significant excess above the standard model expectation is observed; model-independent upper limits are set on the visible τν production cross section. Heavy W′ bosons with masses less than 3.7 TeV in the sequential standard model and masses less than 2.2–3.8 TeV depending on the coupling in the nonuniversal G(221) model are excluded at the 95% credibility level
Search for the direct production of charginos and neutralinos in final states with tau leptons in √s=13 TeV collisions with the ATLAS detector
- Author
- Aaboud M
- Aad G
- Abbott B
- Abdinov O
- Abeloos B
- Abidi SH
- AbouZeid OS
- Abraham NL
- Abramowicz H
- Abreu H
- Abreu R
- Abulaiti Y
- Acharya BS
- Adachi S
- Adamczyk L
- Adelman J
- Adersberger M
- Adye T
- Affolder AA
- Afik Y
- Agatonovic-Jovin T
- Agheorghiesei C
- Aguilar-Saavedra JA
- Ahlen SP
- Ahmadov F
- Aielli G
- Akatsuka S
- Akerstedt H
- Akesson TPA
- Akilli E
- Akimov AV
- Albergh GL
- Albert J
- Albicocco P
- Alconada Verzini MJ
- Alderweireldt SC
- Aleksa M
- Aleksandrov IN
- Alexa C
- Alexander G
- Alexopoulos T
- Alhroob M
- Ali B
- Aliev M
- Alimonti G
- Alison J
- Alkire SP
- 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
- Amelung C
- Amidei D
- Amoroso S
- Amundsen G
- Anastopoulos C
- Ancu LS
- Andari N
- Andeen T
- Anders CF
- Anders JK
- Anderson KJ
- Andreazza A
- Andrei V
- Angelidakis S
- Angelozzi I
- Angerami A
- Anisenkov AV
- Anjos N
- Annovi A
- Antel C
- Antonelli M
- Antonov A
- Antrim DJ
- Anulli F
- Aoki M
- Arabidze G
- Arai Y
- Araque JP
- Arce ATH
- Ardell RE
- Arduh FA
- Arguin J-F
- Argyropoulos S
- Arik M
- Armadans R Caminal
- Armbruster AJ
- Armitage LJ
- Arnaez O
- Arnold H
- Arratia M
- Arslan O
- Artamonov A
- Artoni G
- Artz S
- Asai S
- Asbah N
- Ashkenazi A
- Asquith L
- Assamagan K
- Astalos R
- Astigarraga ME Pozo
- Atkinson M
- Atlay NB
- Augsten K
- Avolio G
- Axen B
- Ayoub MK
- Azuelos G
- Baas AE
- Baca MJ
- Bachacou H
- Bachas K
- Backes M
- Bagnaia P
- Bahmani M
- Bahrasemani H
- Baines JT
- Bajic M
- Baker OK
- Baldin EM
- Balek P
- Balli F
- Balunas WK
- Banas E
- Bandyopadhyay A
- Banerjee Sw
- Bannoura AAE
- Barajas CA Chavez
- Barak L
- Barberio EL
- Barberis D
- Barbero M
- Barillari T
- Barisits M-S
- Barkeloo JT
- Barklow T
- Barlow N
- Barnes SL
- Barnett BM
- Barnett RM
- Barnovska-Blenessy Z
- Baroncelli A
- Barone G
- Barr AJ
- Barranco Navarro L
- Barreiro F
- Bartoldus R
- Barton AE
- Bartos P
- Basalaev A
- Bassalat A
- Bates RL
- Batista SJ
- Batley JR
- Battaglia M
- Bauce M
- Bauer F
- 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
- Behr JK
- Bell AS
- Bella G
- Bella L Aperio
- Bellagamba L
- Bellerive A
- Bellomo M
- Belotskiy K
- Beltramello O
- Belyaev NL
- Benary O
- Benchekroun D
- Bender M
- Bendtz K
- Benekos N
- Benhammou Y
- Benitez J
- Benjamin DP
- Benoit M
- Bensinger JR
- Bentvelsen S
- Beresford L
- Beretta M
- Berge D
- Berger N
- Beringer J
- Berlendis S
- Berlingen J Montejo
- Bernard NR
- Bernardi G
- Bernius C
- Bernlochner FU
- Berry T
- Berta P
- Bertella C
- Bertoli G
- Bertolucci F
- Bertram IA
- Bertsche C
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- Besjes GJ
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- Bevan AJ
- Beyer J
- Bianchi RM
- Biebel O
- Biedermann D
- Bielski R
- Bierwagen K
- Biesuz NV
- Biglietti M
- Billoud TRV
- Bilokon H
- Bindi M
- Bingul A
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- Yildirim E
- Yildiz H Duran
- Yorita K
- Yoshihara K
- Young C
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- Yusuff I
- Zabinski B
- Zacharis G
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- Zalieckas J
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- Zemaityte G
- Zemla A
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- Zhang X
- Zhang Y
- Zhang Z
- Zhao X
- Zhao Y
- Zhao Z
- Zhemchugov A
- Zhou B
- Zhou C
- Zhou L
- Zhou M
- Zhou M
- Zhou N
- Zhu CG
- Zhu H
- Zhu J
- Zhu Y
- Zhuang X
- Zhukov K
- Zibell A
- Zieminska D
- Zimine NI
- Zimmermann C
- Zimmermann S
- Zinonos Z
- Zinser M
- Ziolkowski M
- Zivkovic L
- Zobernig G
- Zoccoli A
- Zou R
- zur Nedden M
- Zwalinski L
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2017
- Field of study
A search for the direct production of charginos and neutralinos in final states with at least two hadronically decaying tau leptons is presented. The analysis uses a dataset of pp collisions corresponding to an integrated luminosity of 36.1 fb−1, recorded with the ATLAS detector at the Large Hadron Collider at a centre-of-mass energy of 13TeV.Nosignificant deviation from the expected Standard Model background is observed. Limits are derived in scenarios of ˜χ+1 ˜χ−1 pair production and of ˜χ±1 ˜χ02 and ˜χ+1 ˜χ−1 production in simplified models where the neutralinos and charginos decay solely via intermediate left-handed staus and tau sneutrinos, and the mass of the ˜ τL state is set to be halfway between the masses of the ˜χ±1 and the ˜χ01. Chargino masses up to 630 GeV are excluded at 95% confidence level in the scenario of direct production of ˜χ+1 ˜χ−1 for a massless ˜χ01. Common ˜χ±1 and ˜χ02 masses up to 760 GeV are excluded in the case of production of ˜χ±1 ˜χ02 and ˜χ+1 ˜χ−1 assuming a massless ˜χ01. Exclusion limits for additional benchmark scenarios with large and small mass-splitting between the ˜χ±1 and the ˜χ01 are also studied by varying the ˜ τL mass between the masses of the ˜χ±1 and the ˜χ01
Measurement of the t¯tZ and t¯tW cross sections in proton-proton collisions at √s=13 TeV with the ATLAS detector
- Author
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- Aad G
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- Abdinov O
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- Zhemchugov A
- Zheng Z
- Zhong D
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- Zhulanov V
- Zibell A
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- Zimine NI
- Zimmermann S
- Zinonos Z
- Ziolkowski M
- Zobernig G
- Zoccoli A
- Zoch K
- Zorbas TG
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- 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
Measurement of differential cross sections and W + /W − cross-section ratios for W boson production in association with jets at √s =8 TeV with the ATLAS detector
- Author
- Aaboud M
- Aad G
- Abbott B
- Abdinov O
- Abeloos B
- Abidi SH
- AbouZeid OS
- Abraham NL
- Abramowicz H
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- Acharya BS
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- Adelman J
- Adersberger M
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- Aguilar-Saavedra JA
- Ahlen SP
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- Aielli G
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- Akerstedt H
- Akesson TPA
- Akilli E
- Akimov AV
- Alberghi GL
- Alberich L Cerda
- Albert J
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- Alderweireldt SC
- Aleksa M
- Aleksandrov IN
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- Allbrooke BMM
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- Amadio BT
- Amelung C
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- Armitage LJ
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- Wu SL
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- Wu Y
- Wyatt TR
- Wynne BM
- Xella S
- Xi Z
- Xia L
- Xu D
- Xu L
- Xu T
- Xu W
- Yabsley B
- Yacoob S
- Yamaguchi D
- Yamaguchi Y
- Yamamoto A
- Yamamoto S
- Yamanaka T
- Yamane F
- Yamatani M
- Yamazaki T
- Yamazaki Y
- Yan Z
- Yang H
- Yang H
- Yang Y
- Yang Z
- Yao W-M
- Yap YC
- Yasu Y
- Yatsenko E
- Ye J
- Ye S
- Yeletskikh I
- Yigitbasi E
- Yildirim E
- Yildiz H Duran
- Yorita K
- Yoshihara K
- Young C
- Young CJS
- Yu J
- Yu J
- Yuen SPY
- Yusuff I
- Zabinski B
- Zacharis G
- Zaidan R
- Zaitsev AM
- Zakharchuk N
- Zalieckas J
- Zaman A
- Zambito S
- Zanzi D
- Zeitnitz C
- Zemaityte G
- Zemla A
- Zeng JC
- Zeng Q
- Zenin O
- Zenis T
- Zerwas D
- Zhang D
- Zhang D
- 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 X
- Zhao Y
- Zhao Z
- Zhemchugov A
- Zhou B
- Zhou C
- Zhou L
- Zhou M
- Zhou M
- Zhou N
- Zhou Y
- Zhu CG
- Zhu H
- Zhu J
- Zhu Y
- Zhuang X
- Zhukov K
- Zibell A
- Zieminska D
- Zimine NI
- Zimmermann C
- Zimmermann S
- Zinonos Z
- Zinser M
- Ziolkowski M
- Zivkovic L
- Zobernig G
- Zoccoli A
- Zou R
- zur Nedden M
- Zwalinski L
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2018
- Field of study
This paper presents a measurement of the W boson production cross section and the W + /W − cross-section ratio, both in association with jets, in proton--proton collisions at s √ =8 TeV with the ATLAS experiment at the Large Hadron Collider. The measurement is performed in final states containing one electron and missing transverse momentum using data corresponding to an integrated luminosity of 20.2 fb −1 . Differential cross sections for events with one or two jets are presented for a range of observables, including jet transverse momenta and rapidities, the scalar sum of transverse momenta of the visible particles and the missing transverse momentum in the event, and the transverse momentum of the W boson. For a subset of the observables, the differential cross sections of positively and negatively charged W bosons are measured separately. In the cross-section ratio of W + /W − the dominant systematic uncertainties cancel out, improving the measurement precision by up to a factor of nine. The observables and ratios selected for this paper provide valuable input for the up quark, down quark, and gluon parton distribution functions of the proto
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