105 research outputs found
Preventing violence by intimate partners in adolescence: an integrative review
- Author
- Akers AY
- Avery-Leaf S
- Ball B
- Bianca de Cássia Alvarez Brancaglioni
- Boinvin S
- Egry EY
- Emiko Yoshikawa Egry
- Fernández-Fuertes AA
- Fonseca RMGS
- Foshee VA
- Foshee VA
- Foshee VA
- Foshee VA
- Foshee VA
- Foshee VA
- Foshee VA
- Foshee VA
- Fredland NM
- Howard D
- Knafl K
- Lundgren R
- Martsolf DS
- Mendes KDS
- Miller E
- Minayo MCS
- Munoz Sanchez AI Bertolozzi MR
- Murphy KA
- Murta SG
- Pick S
- Pradubmook-Sherer P
- Póo AM
- Rafaela Gessner
- Rebeca Nunes Guedes De Oliveira
- Rey-Anacona CA
- Richmond LS
- Rosa Maria Godoy Serpa da Fonseca
- Saavedra R
- Swart LA
- Taylor BG
- Teitelman AM
- Thongpriwan V
- Wiklund M
- Wolfe DA
- Publication venue
- 'FapUNIFESP (SciELO)'
- Publication date
- 01/02/2016
- Field of study
Abstract OBJECTIVE To analyze the scientific literature on preventing intimate partner violence among adolescents in the field of health based on gender and generational categories. METHOD This was an integrative review. We searched for articles using LILACS, PubMed/MEDLINE, and SciELO databases. RESULTS Thirty articles were selected. The results indicate that most studies assessed interventions conducted by programs for intimate partner violence prevention. These studies adopted quantitative methods, and most were in the area of nursing, psychology, and medicine. Furthermore, most research contexts involved schools, followed by households, a hospital, a health center, and an indigenous tribe. CONCLUSION The analyses were not conducted from a gender- and generation-based perspective. Instead, the scientific literature was based on positivist research models, intimately connected to the classic public healthcare model and centered on a singular dimension
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
- Adam L
- Adamczyk L
- Adamek L
- Adelman J
- Adersberger M
- Adiguzel A
- Adorni S
- Adye T
- Affolder AA
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- Agapopoulou C
- Agaras MN
- Aggarwal A
- Agheorghiesei C
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- Aielli G
- Akatsuka S
- Akesson TPA
- Akilli E
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- Al Khoury K
- Alberghi GL
- Albert J
- Alderweireldt S
- Aleksa M
- Aleksandrov IN
- Alexa C
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- Allbrooke BMM
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- Allport PP
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- Alviggi MG
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- Sinervo P
- Sinetckii V
- Sinev NB
- Singh S
- Sioli M
- Siral I
- Sivoklokov SY
- Sjolin J
- Skorda E
- Skubic P
- Slawinska M
- Sliwa K
- Slovak R
- Smakhtin V
- Smart BH
- Smiesko J
- Smirnov N
- Smirnov SY
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- Smirnova LN
- Smirnova O
- Smith JW
- Smizanska M
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- Snesarev AA
- Snoek HL
- Snyder IM
- Snyder S
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- Sola JDB
- Soldatov EY
- Soldevila U
- Solis AL
- Solodkov AA
- Soloshenko A
- Solovyanov O
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- Sommer P
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- Stark GH
- Stark J
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- Steinhebel AL
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- Stenzel H
- Stevenson TJ
- Stewart GA
- Stockton MC
- Stoicea G
- Stolarski M
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- Straessner A
- Strandberg J
- Strandberg S
- Strauss M
- Strizenec P
- Stroehmer R
- Strom DM
- Stroynowski R
- Strubig A
- Stucci SA
- Stugu B
- Stupak J
- Styles NA
- Su D
- Su W
- Suchek S
- Sulin VV
- Sullivan MJ
- Sultan DMS
- Sultansoy S
- Sumida T
- Sun S
- Sun X
- Suruliz K
- Suster CJE
- Sutton MR
- Suzuki S
- Svatos M
- Swiatlowski M
- Swift SP
- Swirski T
- Sydorenko A
- Sykora I
- Sykora M
- Sykora T
- Ta D
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- Taenzer J
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- Tas P
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- Tayalati Y
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- Tehrani FS
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- Teoh JJ
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- Terashi K
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- Testa M
- Teuscher RJ
- Thais SJ
- Theveneaux-Pelzer T
- Thiele F
- Thomas DW
- Thomas JO
- Thomas JP
- Thompson PD
- Thomsen LA
- Thomson E
- Thorpe EJ
- Tikhomirov VO
- Tikhonov YA
- Timoshenko S
- Tipton P
- Tisserant S
- Tobon CAM
- Todome K
- Todorova-Nova S
- Todt S
- Tojo J
- Tokar S
- Tokushuku K
- Tolley E
- Tomiwa KG
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- Torres RET
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- Toth J
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- Tsai F
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- Tsiareshka P
- Tsirigotis A
- Tsiskaridze V
- Tskhadadze EG
- Tsopoulou M
- Tsukerman II
- Tsulaia V
- Tsuno S
- Tsybychev D
- Tu Y
- Tudorache A
- Tudorache V
- Tulbure TT
- Tuna AN
- Turchikhin S
- Turgeman D
- Turner RJ
- Turra RT
- Tuts PM
- Tzamarias S
- Tzovara E
- Ucchielli G
- Uchida K
- Ukegawa F
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- Ungaro FC
- Unno Y
- Uno K
- Urban J
- Urquijo P
- Usai G
- Uysal Z
- Vacek V
- Vachon B
- Vadla KOH
- Vaidya A
- Valderanis C
- Vale MAB
- Valente M
- Valentinetti S
- Valero A
- Valery L
- Vallance RA
- Vallier A
- Van Daalen TR
- Van Gemmeren P
- Van Vulpen I
- Vanadia M
- Vandelli W
- Vandenbroucke M
- Vandewall ER
- Vaniachine A
- Vannicola D
- Vari R
- Varnes EW
- Varni C
- Varol T
- Varouchas D
- Varvell KE
- Vasile ME
- Vasquez GA
- Vazeille F
- Vazquez Furelos D
- Vazquez CJB
- Vazquez JGP
- Veatch J
- Vecchio V
- Veen MJ
- Veloce LM
- Veloso F
- Veneziano S
- Ventura A
- Venturi N
- Vera AMR
- Verbytskyi A
- Vercesi V
- Verducci M
- Vergara JCR
- Vergis C
- Verkerke W
- Vermeulen AT
- Vermeulen JC
- Verzini MJA
- Vetterli MC
- Viaux Maira N
- Vickey T
- Viehhauser GHA
- Vigani L
- Villa M
- Vilucchi E
- Vincter MG
- Virdee GS
- Vishwakarma A
- Vittori C
- Vivarelli I
- Vogel M
- Vokac P
- von Buddenbrock SE
- Von Toerne E
- Vorobel V
- Vorobev K
- Vos M
- Vossebeld JH
- Vozak M
- Vranjes N
- Vrba V
- Vreeswijk M
- Vuillermet R
- Vukotic I
- Wagner P
- Wagner W
- Wagner-Kuhr J
- Wahdan S
- Wahlberg H
- Walbrecht VM
- Walder J
- Walker R
- Walker SD
- Walkowiak W
- Wallangen V
- Wang AM
- Wang AZ
- Wang C
- Wang F
- Wang H
- Wang J
- Wang P
- Wang Q
- Wang R
- Wang R-J
- Wang SM
- Wang W
- Wang WT
- Wang WX
- Wang Y
- Wang Z
- Wanotayaroj C
- Warburton A
- Ward CP
- Wardrope DR
- Warrack N
- Washbrook A
- Watson AT
- Watson MF
- Watts G
- Waugh BM
- Webb AF
- Webb S
- Weber C
- Weber MS
- Weber SA
- Weber SM
- Weidberg AR
- Weingarten J
- Weirich M
- Weiser C
- Wells PS
- Wenaus T
- Wengler T
- Wenig S
- Wermes N
- Werner MD
- Wessels M
- Weston TD
- Whalen K
- Whallon NL
- Wharton AM
- White A
- White AS
- White MJ
- Whiteson D
- Whitmore BW
- Wiedenmann W
- Wiel C
- Wielers M
- Wieseotte N
- Wiglesworth C
- Wiik-Fuchs LAM
- Wilkens HG
- Wilkins LJ
- Williams HH
- Williams S
- Willis C
- Willocq S
- Wingerter-Seez I
- Winkels E
- Winklmeier F
- Winston OJ
- Winter BT
- Wittgen M
- Wobisch M
- Wolf A
- Wolf TMH
- Wolff R
- Wolker R
- Wollrath J
- Wolter MW
- Wolters H
- Wong VWS
- Woods NL
- Worm SD
- Wosiek BK
- Wozniak KW
- Wraight K
- Wu SL
- Wu X
- Wu Y
- Wyatt TR
- Wynne BM
- Xella S
- Xi Z
- Xia L
- Xiao X
- Xiotidis I
- Xu D
- Xu H
- Xu L
- Xu T
- Xu W
- Xu Z
- Yabsley B
- Yacoob S
- Yajima K
- Yallup DP
- Yamaguchi N
- Yamaguchi Y
- Yamamoto A
- Yamatani M
- Yamazaki T
- Yamazaki Y
- Yan Z
- Yang HJ
- Yang HT
- Yang S
- Yang T
- Yang X
- Yang Y
- Yao W-M
- Yap YC
- Yasu Y
- Yatsenko E
- Ye H
- Ye J
- Ye S
- Yeletskikh I
- Yexley MR
- Yigitbasi E
- Yildiz HD
- Yorita K
- Yoshihara K
- Young C
- Young CJS
- Yu J
- Yuan R
- Yue X
- Zaazoua M
- Zabinski B
- Zacharis G
- Zaffaroni E
- Zahreddine J
- Zaitsev AM
- Zakareishvili T
- Zakharchuk N
- Zambito S
- Zanzi D
- Zaripovas DR
- Zeissner S
- Zeitnitz C
- Zemaityte G
- Zeng JC
- Zenin O
- Zenis T
- Zerwas D
- Zgubic M
- Zhang B
- Zhang DF
- Zhang G
- Zhang H
- Zhang J
- Zhang L
- Zhang M
- Zhang R
- Zhang S
- Zhang X
- Zhang Y
- Zhang Z
- Zhao P
- Zhao Z
- Zhemchugov A
- Zheng Z
- Zhong D
- Zhou B
- Zhou C
- Zhou M
- Zhou MS
- Zhou N
- Zhou Y
- Zhu C
- Zhu CG
- Zhu H
- Zhu HL
- Zhu J
- Zhu Y
- Zhuang X
- Zhukov K
- Zhulanov V
- Zieminska D
- Zimine N
- Zimmermann S
- Zinonos Z
- Ziolkowski M
- Zivkovic L
- Zobernig G
- Zoccoli A
- Zoch K
- Zorbas TG
- Zou R
- Zu Theenhausen HM
- Zwalinski L
- Publication venue
- '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
Simulation and experimental study of proton bunch self-modulation in plasma with linear density gradients
- Author
- Agnello R
- Ahdida CC
- Aladi M
- Amoedo Goncalves MC
- Andrebe Y
- Apsimon O
- Apsimon R
- Bachmann AM
- Baistrukov MA
- Batsch F
- Bergamaschi M
- Blanchard P
- Braunmüller F
- Burrows PN
- Buttenschön B
- Caldwell A
- Chappell J
- Chevallay E
- Chung M
- Cooke DA
- Damerau H
- Davut C
- Demeter G
- Dexter A
- Doebert S
- Farmer J
- Fasoli A
- Fedosseev VN
- Fiorito R
- Fonseca RA
- Furno I
- Gessner S
- Gorn AA
- Granados E
- Granetzny M
- Graubner T
- Grulke O
- Gschwendtner E
- Guran ED
- Hafych V
- Henderson JR
- Hüther M
- Kedves M
- Khudyakov V
- Kim SY
- Kraus F
- Krupa M
- Lefevre T
- Liang L
- Lopes N
- Lotov KV
- Martyanov M
- Mazzoni S
- Medina Godoy D
- Moody JT
- Moon K
- Morales Guzmán PI
- Moreira M
- Muggli P
- Nechaeva T
- Nowak E
- Pakuza C
- Panuganti H
- Pardons A
- Perera A
- Pucek J
- Pukhov A
- Ramjiawan RL
- Rey S
- Ráczkevi B
- Schmitz O
- Senes E
- Silva LO
- Stollberg C
- Sublet A
- Topaloudis A
- Torrado N
- Tuev PV
- Turner M
- Velotti F
- Verra L
- Vieira J
- Vincke H
- Welsch CP
- Wendt M
- Wing M
- Wolfenden J
- Woolley B
- Xia G
- Zepp M
- Zevi Della Porta G
- Publication venue
- Publication date
- 01/10/2021
- Field of study
We present numerical simulations and experimental results of the self-modulation of a long proton bunch in a plasma with linear density gradients along the beam path. Simulation results agree with the experimental results reported [F. Braunmller, T. Nechaeva et al. (AWAKE Collaboration), Phys. Rev. Lett. 125, 264801 (2020)PRLTAO0031-900710.1103/PhysRevLett.125.264801]: with negative gradients, the charge of the modulated bunch is lower than with positive gradients. In addition, the bunch modulation frequency varies with gradient. Simulation results show that dephasing of the wakefields with respect to the relativistic protons along the plasma is the main cause for the loss of charge. The study of the modulation frequency reveals details about the evolution of the self-modulation process along the plasma. In particular for negative gradients, the modulation frequency across time-resolved images of the bunch indicates the position along the plasma where protons leave the wakefields. Simulations and experimental results are in excellent agreement
Experimental study of extended timescale dynamics of a plasma wakefield driven by a self-modulated proton bunch
- Author
- Adli E
- Agnello R
- Aladi M
- Andrebe Y
- Apsimon O
- Apsimon R
- Bachmann AM
- Baistrukov MA
- Batsch F
- Bergamaschi M
- Blanchard P
- Burrows PN
- Buttenschön B
- Caldwell A
- Chappell J
- Chevallay E
- Chung M
- Cooke DA
- Damerau H
- Davut C
- Demeter G
- Deubner LH
- Dexter A
- Djotyan GP
- Doebert S
- Farmer J
- Fasoli A
- Fedosseev VN
- Fiorito R
- Fonseca RA
- Friebel F
- Furno I
- Garolfi L
- Gessner S
- Goddard B
- Gorgisyan I
- Gorn AA
- Granados E
- Granetzny M
- Grulke O
- Gschwendtner E
- Hafych V
- Hartin A
- Helm A
- Henderson JR
- Howling A
- Hüther M
- Jacquier R
- Jolly S
- Kargapolov IY
- Kedves MA
- Keeble F
- Kelisani MD
- Kim SY
- Kraus F
- Krupa M
- Lefevre T
- Li Y
- Liang L
- Liu S
- Lopes N
- Lotov KV
- Martyanov M
- Mazzoni S
- Medina Godoy D
- Minakov VA
- Moody JT
- Morales Guzmán PI
- Moreira M
- Panuganti H
- Pardons A
- Perera A
- Petrenko A
- Peña Asmus F
- Pucek J
- Pukhov A
- Ramjiawan RL
- Rey S
- Ruhl H
- Ráczkevi B
- Saberi H
- Schmitz O
- Senes E
- Sherwood P
- Silva LO
- Spitsyn RI
- Tuev PV
- Velotti F
- Verra L
- Verzilov VA
- Vieira J
- Welsch CP
- Williamson B
- Wing M
- Wolfenden J
- Woolley B
- Xia G
- Zepp M
- Zevi Della Porta G
- Publication venue
- Publication date
- 01/01/2021
- Field of study
Plasma wakefield dynamics over timescales up to 800 ps, approximately 100 plasma periods, are studied
experimentally at the Advanced Wakefield Experiment (AWAKE). The development of the longitudinal
wakefield amplitude driven by a self-modulated proton bunch is measured using the external injection of
witness electrons that sample the fields. In simulation, resonant excitation of the wakefield causes plasma
electron trajectory crossing, resulting in the development of a potential outside the plasma boundary as
electrons are transversely ejected. Trends consistent with the presence of this potential are experimentally
measured and their dependence on wakefield amplitude are studied via seed laser timing scans and electron
injection delay scan
Experimental Observation of Proton Bunch Modulation in a Plasma at Varying Plasma Densities
- Author
- Adli E
- Ahuja A
- Apsimon O
- Apsimon R
- Asmus F Pena
- Bachmann A-M
- Barrientos D
- Barros MM
- Batkiewicz J
- Batsch F
- Bauche J
- Bernardini M
- Biskup B
- Boccardi A
- Bogey T
- Bohl T
- Bracco C
- Braunmueller F
- Brun L Maricalva
- Burger S
- Burt G
- Bustamante S
- Buttenschoen B
- Caldwell A
- Cascella M
- Chappell J
- Chevallay E
- Chung M
- Collaboration AWAKE
- Cooke D
- Damerau H
- Deacon L
- Deubner LH
- Dexter A
- Doebert S
- Farmer J
- Fedosseev VN
- Fior G
- Fiorito R
- Fonseca RA
- Friebel F
- Garolfi L
- Gessner S
- Godoy D Medina
- Gorgisyan I
- Gorn AA
- Granados E
- Grulke O
- Gschwendtner E
- Guerrero A
- Hansen J
- Helm A
- Henderson JR
- Hessler C
- Hofle W
- Huether M
- Ibison M
- Jensen L
- Jolly S
- Keeble F
- Kim S-Y
- Kraus F
- Lefevre T
- LeGodec G
- Li Y
- Liu S
- Lopes N
- Lotov KV
- Martyanov M
- Mazzoni S
- Minakov VA
- Mitchell J
- Molendijk JC
- Mompo R
- Moody JT
- Moreira M
- Muggli P
- Mutin C
- Oez E
- Olsen VK Berglyd
- Ozturk E
- Pardons A
- Pasquino C
- Pepitone K
- Perera A
- Petrenko A
- Pitman S
- Plyushchev G
- Pukhov A
- Rey S
- Rieger K
- Ruhl H
- Schmidt JS
- Shalimova IA
- Shaposhnikova E
- Sherwood P
- Silva LO
- Soby L
- Sosedkin AP
- Speroni R
- Spitsyn RI
- Tuev PV
- Turner M
- Velotti F
- Verra L
- Verzilov VA
- Vieira J
- Vincke H
- Welsch CP
- Williamson B
- Wing M
- Woolley B
- Xia G
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 12/09/2018
- Field of study
We give direct experimental evidence for the observation of the full transverse self-modulation of a long, relativistic proton bunch propagating through a dense plasma. The bunch exits the plasma with a periodic density modulation resulting from radial wakefield effects. We show that the modulation is seeded by a relativistic ionization front created using an intense laser pulse copropagating with the proton bunch. The modulation extends over the length of the proton bunch following the seed point. By varying the plasma density over one order of magnitude, we show that the modulation frequency scales with the expected dependence on the plasma density, i.e., it is equal to the plasma frequency, as expected from theory
Macroinvertebrates in low-order streams in two fragments of Atlantic Forest in different states of conservation, in the State of São Paulo (Brazil)
- Author
- AA Fonseca-Gessner
- ALLAN JD
- ANGERMEIER PL.
- ANGRISANO EB.
- BAPTISTA DF.
- BERTRAND HPI.
- BISPO PC.
- BISPO PC.
- BISPO PC.
- BRINKHURST RO.
- BUNN SE.
- Cetra M.
- CLARKE A.
- CLENAGHAN C.
- CORBI JJ.
- COSTA C.
- COSTA JM.
- DOMÍNGUEZ E.
- DOMÍNGUEZ E.
- DUDGEON D.
- EPLER JH.
- FERNÁNDEZ HR.
- FROEHLICH CG.
- GILLER PS
- GREGORY SV.
- GUERESCHI RM.
- HARDING JS.
- HAWKINS CP.
- HYNES HBN.
- INT PANIS L.
- KIKUCHI RM.
- KLEINE P.
- LEECH HB
- LIND OT.
- MANZO V.
- MARQUES MMGSM.
- MC. Paula
- OLIFIERS MH.
- PES AMO.
- RODRIGUES RR
- ROQUE FO.
- ROSENBERG DM.
- SALLES FF.
- SURIANO MT.
- TRIVINHO-STRIXINO S
- VANNOTE RL.
- WALLACE JB.
- WARD JV.
- WETZEL RG.
- WHITE DS.
- WHITTON BA.
- WIGGINS GB
- Publication venue
- 'FapUNIFESP (SciELO)'
- Publication date
- Field of study
Measurement of single top-quark production in association with a W boson in the single-lepton channel at \sqrt{s} = 8\,\text {TeV} with the ATLAS detector
- Author
- Aad G
- Abbott B
- Abbott DC
- Abeling K
- Abhayasinghe DK
- Abidi SH
- AbouZeid OS
- Abraham NL
- Abramowicz H
- Abreu H
- Abud AA
- Abulaiti Y
- Acharya BS
- Achkar B
- Adachi S
- Adam L
- Adamczyk L
- Adamek L
- Adelman J
- Adersberger M
- Adiguzel A
- Adorni S
- Adye T
- Affolder AA
- Afik Y
- Agapopoulou C
- Agaras MN
- Aggarwal A
- Agheorghiesei C
- Aguilar-Saavedra JA
- Ahmadov F
- Ahmed WS
- Ai X
- Aielli G
- Akatsuka S
- Akesson TPA
- Akilli E
- Akimov A
- Al Khoury K
- Alberghi GL
- Albert J
- Alderweireldt S
- Aleksa M
- Aleksandrov IN
- Alexa C
- Alexandre D
- Alexopoulos T
- Alfonsi A
- Alfonsi F
- Alhroob M
- Ali B
- Aliev M
- Alimonti G
- Alison J
- Alkire SP
- Allaire C
- Allbrooke BMM
- Allen BW
- Allport PP
- Aloisio A
- Alonso A
- Alonso F
- Alpigiani C
- Alshehri AA
- Alvarez Estevez M
- Alvarez Piqueras D
- Alviggi MG
- Ambler A
- Ambroz L
- Amelung C
- Amidei D
- Amoroso S
- Amrouche CS
- An F
- Anastopoulos C
- Andari N
- Andeen T
- Anders CF
- Anders JK
- Andreazza A
- Andrei V
- Anelli CR
- Angelidakis S
- Angerami A
- Anisenkov A
- Annovi A
- Antel C
- Anthony MT
- Antipov E
- Antonelli M
- Antrim DJA
- Anulli F
- Aoki M
- Aparisi Pozo JA
- Arabidze G
- Araque JP
- Araya ST
- Arcangeletti C
- Arce ATH
- Arduh FA
- Arguin J-F
- Argyropoulos S
- Arling J-H
- Armadans RC
- Armbruster AJ
- Armstrong A
- Arnaez O
- Arnold H
- Artoni G
- Artz S
- Asai S
- Asbah N
- Asimakopoulou EM
- Asquith L
- Assahsah J
- Assamagan K
- Astalos R
- Astigarraga MEP
- Atkin RJ
- Atkinson M
- Atlay NB
- Atmani H
- Augsten K
- Avolio G
- Avramidou R
- Ayoub MK
- Azoulay AM
- Azuelos G
- Bachacou H
- Bachas K
- Backes M
- Backman F
- Bagnaia P
- Bahmani M
- Bahrasemani H
- Bailey AJ
- Bailey VR
- Baines JT
- Bajic M
- Bakalis C
- Baker OK
- Bakker PJ
- Balaji S
- Baldin EM
- Balek P
- Balli F
- Balunas WK
- Balz J
- Banas E
- Bandyopadhyay A
- Banerjee S
- Bannoura AAE
- Barak L
- Barbe WM
- Barberio EL
- Barberis D
- Barbero M
- Barbour G
- Barillari T
- Barisits M-S
- Barkeloo J
- Barklow T
- Barnea R
- Barnes SL
- Barnett BM
- Barnett RM
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- Zhemchugov A
- Zheng Z
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- Zou R
- Zu Theenhausen HM
- Zwalinski L
- Publication venue
- 'Springer Fachmedien Wiesbaden GmbH'
- Publication date
- 01/01/2021
- Field of study
The production cross-section of a top quark in association with a W boson is measured using proton–proton collisions at \sqrt{s} = 8\,\text {TeV}. The dataset corresponds to an integrated luminosity of 20.2\,\text {fb}^{-1}, and was collected in 2012 by the ATLAS detector at the Large Hadron Collider at CERN. The analysis is performed in the single-lepton channel. Events are selected by requiring one isolated lepton (electron or muon) and at least three jets. A neural network is trained to separate the tW signal from the dominant t{\bar{t}} background. The cross-section is extracted from a binned profile maximum-likelihood fit to a two-dimensional discriminant built from the neural-network output and the invariant mass of the hadronically decaying W boson. The measured cross-section is \sigma _{tW} = 26 \pm 7\,\text {pb}, in good agreement with the Standard Model expectation
Measurements of Higgs bosons decaying to bottom quarks from vector boson fusion production with the ATLAS experiment at √=13TeV
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- Zhemchugov A
- Zheng Z
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- Zhulanov V
- Zieminska D
- Zimine NI
- Zimmermann S
- Zinonos Z
- Ziolkowski M
- Zoccoli A
- Zoch K
- Zorbas TG
- Zou R
- Zwalinski L
- Åkesson TPA
- Öncel ÖO
- Ženiš T
- Živković L
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 23/06/2021
- Field of study
The paper presents a measurement of the Standard Model Higgs Boson decaying to b-quark pairs in the vector boson fusion (VBF) production mode. A sample corresponding to 126 fb−1 of s√=13TeV proton–proton collision data, collected with the ATLAS experiment at the Large Hadron Collider, is analyzed utilizing an adversarial neural network for event classification. The signal strength, defined as the ratio of the measured signal yield to that predicted by the Standard Model for VBF Higgs production, is measured to be 0.95+0.38−0.36 , corresponding to an observed (expected) significance of 2.6 (2.8) standard deviations from the background only hypothesis. The results are additionally combined with an analysis of Higgs bosons decaying to b-quarks, produced via VBF in association with a photon
Muon reconstruction and identification efficiency in ATLAS using the full Run 2 pp collision data set at \sqrt{s}=13 TeV
- 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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- Acharya BS
- Achkar B
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- Adamek L
- Adelman J
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- Zhao P
- Zhao Y
- Zhao Z
- Zhemchugov A
- Zheng Z
- Zhong D
- Zhou B
- Zhou C
- Zhou H
- Zhou M
- Zhou N
- Zhou Y
- Zhu C
- Zhu CG
- Zhu H
- Zhu HL
- Zhu J
- Zhu Y
- Zhuang X
- Zhukov K
- Zhulanov V
- Zieminska D
- Zimine NI
- Zimmermann S
- Zinonos Z
- Ziolkowski M
- Zivkovic L
- Zobernig G
- Zoccoli A
- Zoch K
- Zorbas TG
- Zou R
- Zwalinski L
- Publication venue
- 'Springer Fachmedien Wiesbaden GmbH'
- Publication date
- 01/01/2021
- Field of study
This article documents the muon reconstruction and identification efficiency obtained by the ATLAS experiment for 139 \hbox {fb}^{-1} of pp collision data at \sqrt{s}=13 TeV collected between 2015 and 2018 during Run 2 of the LHC. The increased instantaneous luminosity delivered by the LHC over this period required a reoptimisation of the criteria for the identification of prompt muons. Improved and newly developed algorithms were deployed to preserve high muon identification efficiency with a low misidentification rate and good momentum resolution. The availability of large samples of Z\rightarrow \mu \mu and J/\psi \rightarrow \mu \mu decays, and the minimisation of systematic uncertainties, allows the efficiencies of criteria for muon identification, primary vertex association, and isolation to be measured with an accuracy at the per-mille level in the bulk of the phase space, and up to the percent level in complex kinematic configurations. Excellent performance is achieved over a range of transverse momenta from 3 GeV to several hundred GeV, and across the full muon detector acceptance of |\eta |<2.7
Performance of the upgraded PreProcessor of the ATLAS Level-1 Calorimeter Trigger
- Author
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- Abbott B
- Abbott DC
- Abeling K
- Abhayasinghe DK
- Abidi SH
- AbouZeid OS
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- Castillo Gimenez V
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- Zhemchugov A
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- Zu Theenhausen H Meyer
- Zwalinski L
- Publication venue
- 'IOP Publishing'
- Publication date
- 01/01/2020
- Field of study
The PreProcessor of the ATLAS Level-1 Calorimeter Trigger prepares the analogue trigger signals sent from the ATLAS calorimeters by digitising, synchronising, and calibrating them to reconstruct transverse energy deposits, which are then used in further processing to identify event features. During the first long shutdown of the LHC from 2013 to 2014, the central components of the PreProcessor, the Multichip Modules, were replaced by upgraded versions that feature modern ADC and FPGA technology to ensure optimal performance in the high pile-up environment of LHC Run 2. This paper describes the features of the newMultichip Modules along with the improvements to the signal processing achieved.ANPCyTYerPhI, ArmeniaAustralian Research CouncilBMWFW, AustriaAustrian Science Fund (FWF)Azerbaijan National Academy of Sciences (ANAS)SSTC, BelarusNational Council for Scientific and Technological Development (CNPq)Fundacao de Amparo a Pesquisa do Estado de Sao Paulo (FAPESP)Natural Sciences and Engineering Research Council of CanadaCanada Foundation for InnovationNational Natural Science Foundation of China (NSFC)Departamento Administrativo de Ciencia, Tecnología e Innovación ColcienciasMinistry of Education, Youth & Sports - Czech Republic
Czech Republic GovernmentCzech Republic GovernmentDNRF, DenmarkDanish Natural Science Research CouncilCentre National de la Recherche Scientifique (CNRS)CEA-DRF/IRFU, FranceFederal Ministry of Education & Research (BMBF)Max Planck SocietyGreek Ministry of Development-GSRTRGC and Hong Kong SAR, ChinaIsrael Science FoundationBenoziyo Center, IsraelIstituto Nazionale di Fisica Nucleare (INFN)Ministry of Education, Culture, Sports, Science and Technology, Japan (MEXT)Ministry of Education, Culture, Sports, Science and Technology, Japan (MEXT)
Japan Society for the Promotion of ScienceCNRST, MoroccoRCN, NorwayPortuguese Foundation for Science and TechnologyMNE/IFA, RomaniaMES of RussiaMESTD, SerbiaMSSR, SlovakiaSlovenian Research Agency - SloveniaMIZS, SloveniaSpanish GovernmentSRC, SwedenWallenberg Foundation, SwedenSNSF Geneva, SwitzerlandMinistry of Science and Technology, TaiwanMinistry of Energy & Natural Resources - TurkeyScience & Technology Facilities Council (STFC)United States Department of Energy (DOE)National Science Foundation (NSF)BCKDF, CanadaCANARIE, CanadaCRC, CanadaEuropean Research Council (ERC)European Union (EU)French National Research Agency (ANR)German Research Foundation (DFG)Alexander von Humboldt FoundationGreek NSRF, GreeceBSF-NSF, IsraelGerman-Israeli Foundation for Scientific Research and DevelopmentLa Caixa Banking Foundation, SpainCERCA Programme Generalitat de Catalunya, SpainPROMETEO, SpainGenT Programmes Generalitat Valenciana, SpainGoran Gustafssons Stiftelse, SwedenRoyal Society of LondonLeverhulme TrustNRC, CanadaCERNANID, ChileChinese Academy of SciencesMinistry of Science and Technology, ChinaSRNSFG, GeorgiaHGF, GermanyNetherlands Organization for Scientific Research (NWO)
Netherlands GovernmentMinistry of Science and Higher Education, PolandNCN, PolandNRCKI, Russia FederationJINRDST/NRF, South AfricaSERI, Geneva, SwitzerlandCantons of Bern and Geneva, SwitzerlandCompute Canada, CanadaHorizon 2020Marie Sklodowska-Curie ActionsEuropean Cooperation in Science and Technology (COST)EU-ESF, Greec
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