480 research outputs found
Jet energy measurement with the ATLAS detector in proton-proton collisions at root s=7 TeV
- Author
- Aad G
- Abbott B
- Abdallah J
- Abdelalim AA
- Abdesselam A
- Abdinov O
- Abi B
- Abolins M
- Abramowicz H
- Abreu H
- Acerbi E
- Acharya BS
- Adams DL
- Addy TN
- Adelman J
- Aderholz M
- Adomeit S
- Adragna P
- Adye T
- Aefsky S
- Aguilar-Saavedra JA
- Aharrouche M
- Ahlen SP
- Ahles F
- Ahmad A
- Ahsan M
- Aielli G
- Akdogana T
- Akesson TPA
- Akimoto G
- Akimov AV
- Akiyama A
- Aktas A
- Alam MA
- Alam MS
- Albert J
- Albrand S
- Aleksa M
- Aleksandrov IN
- Alessandria F
- Alexa C
- Alexander G
- Alexandre G
- Alexopoulos T
- Alhroob M
- Aliev M
- Alimonti G
- Alison J
- Aliyev M
- Allport PP
- Allwood-Spiers SE
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- Almond J
- Aloisio A
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- Alonso A
- Alviggi MG
- Amako K
- Amaral P
- Amelung C
- Ammosov VV
- Amorim A
- Amoros G
- Amram N
- Anastopoulos C
- Ancu LS
- Andari N
- Andeen T
- Anders CF
- Anders G
- Anderson KJ
- Andreazza A
- Andrei V
- Andrieux M-L
- Anduaga XS
- Angerami A
- Anghinolfi F
- Anh TV
- Anjos N
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- Antonaki A
- Antonelli M
- Antonov A
- Antos J
- Anulli F
- Aoun S
- Apolle R
- Arabidze G
- Aracena I
- Arai Y
- Aranda CP
- Arce ATH
- Archambault JP
- Arfaoui S
- Arguin J-F
- Arik E
- Arik M
- Armbruster AJ
- Arnaez O
- Arnault C
- Artamonov A
- Artoni G
- Arutinov D
- Asai S
- Asfandiyarov R
- Ask S
- Asman B
- Asner D
- Asquith L
- Assamagan K
- Astbury A
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- Atoian G
- Aubert B
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- Augsten K
- Aurousseau M
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- Avramidou R
- Axen D
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- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/03/2013
- Field of study
The jet energy scale and its systematic uncertainty are determined for jets measured with the ATLAS detector at the LHC in proton-proton collision data at a centre-of-mass energy of √s = 7TeV corresponding to an integrated luminosity of 38 pb-1. Jets are reconstructed with the anti-kt algorithm with distance parameters R=0. 4 or R=0. 6. Jet energy and angle corrections are determined from Monte Carlo simulations to calibrate jets with transverse momenta pT≥20 GeV and pseudorapidities {pipe}η{pipe}<4. 5. The jet energy systematic uncertainty is estimated using the single isolated hadron response measured in situ and in test-beams, exploiting the transverse momentum balance between central and forward jets in events with dijet topologies and studying systematic variations in Monte Carlo simulations. The jet energy uncertainty is less than 2. 5 % in the central calorimeter region ({pipe}η{pipe}<0. 8) for jets with 60≤pT<800 GeV, and is maximally 14 % for pT<30 GeV in the most forward region 3. 2≤{pipe}η{pipe}<4. 5. The jet energy is validated for jet transverse momenta up to 1 TeV to the level of a few percent using several in situ techniques by comparing a well-known reference such as the recoiling photon pT, the sum of the transverse momenta of tracks associated to the jet, or a system of low-pT jets recoiling against a high-pT jet. More sophisticated jet calibration schemes are presented based on calorimeter cell energy density weighting or hadronic properties of jets, aiming for an improved jet energy resolution and a reduced flavour dependence of the jet response. The systematic uncertainty of the jet energy determined from a combination of in situ techniques is consistent with the one derived from single hadron response measurements over a wide kinematic range. The nominal corrections and uncertainties are derived for isolated jets in an inclusive sample of high-pT jets. Special cases such as event topologies with close-by jets, or selections of samples with an enhanced content of jets originating from light quarks, heavy quarks or gluons are also discussed and the corresponding uncertainties are determined. © 2013 CERN for the benefit of the ATLAS collaboration
Search for the neutral Higgs bosons of the minimal supersymmetric standard model in pp collisions at root s=7 TeV with the ATLAS detector
- Author
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- Publication venue
- Publication date
- 01/02/2013
- Field of study
A search for neutral Higgs bosons of the Minimal Supersymmetric Standard Model (MSSM) is reported. The analysis is based on a sample of proton-proton collisions at a centre-of-mass energy of 7TeV recorded with the ATLAS detector at the Large Hadron Collider. The data were recorded in 2011 and correspond to an integrated luminosity of 4.7 fb-1 to 4.8 fb-1. Higgs boson decays into oppositely-charged muon or τ lepton pairs are considered for final states requiring either the presence or absence of b-jets. No statistically significant excess over the expected background is observed and exclusion limits at the 95% confidence level are derived. The exclusion limits are for the production cross-section of a generic neutral Higgs boson, φ, as a function of the Higgs boson mass and for h/A/H production in the MSSM as a function of the parameters mA and tan β in the mhmax scenario for mA in the range of 90GeV to 500 GeV. Copyright CERN
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
- Afik Y
- Agapopoulou C
- Agaras MN
- Aggarwal A
- Agheorghiesei C
- Aguilar-Saavedra JA
- Ahmadov F
- Ahmed WS
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- Suzuki S
- Svatos M
- Swiatlowski M
- Swift SP
- Swirski T
- Sydorenko A
- Sykora I
- Sykora M
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- Ta D
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- Tavares Delgado A
- Tayalati Y
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- Ten Kate H
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- Tsukerman II
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- Tsuno S
- Tsybychev D
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- Tudorache A
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- Tulbure TT
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- Vaidya A
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- Valero A
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- 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
Expression and function of G-protein-coupled receptorsin the male reproductive tract
- Author
- ABOUD R
- ALONSO-LLAMAZARES A
- ANAND-IVELL RJ
- ANDERSON MB
- BAN Y
- BATHGATE RA
- BATHGATE RA
- BERNARD V
- BERNARD V
- BHATHAL PS
- BIRDSALL NJ
- BISHOP MJ
- BLANCO M
- BOGIC L
- BORGES MOR
- BRADDON SA
- BRODDE OE
- BURAZIN TC
- BURT RP
- BURT RP
- CAMPOS M
- Catarina S. Porto
- CAULFIELD MP
- CHALOTHORN D
- CHAN HC
- CHANG DJ
- CHATURAPANICH G
- CHEAH SH
- CHEN S
- CHEN S
- COGÉ F ET AL
- DA SILVA MC
- DALY CJ
- DANIELS DV
- DAVENPORT CW
- DEBRUYNE FM
- DENG XF
- DIVIANI D
- DOCHERTY JR
- DOCHERTY JR
- DOGGRELL SA
- DU JY
- EGLEN RM
- EGLEN RM
- EHRÉN I
- EISENHOFER G
- ERRASTI AE
- ESBENSHADE TA
- ESSIG M
- FENG S
- FEVOLD HL
- FILONZI M
- FORD APDW
- FORD APDW
- FORRAY C
- FUKASAWA R
- GAO B
- GAO B
- GOBEIL F JR
- GONZÁLEZ-ESPINOSA C
- GRAHAM RM
- GRIMM U
- GUNNERSEN JM
- GUNNERSEN JM
- HAAG C
- HAGUE C
- HAGUE C
- HALLS ML
- HALLS ML
- HALLS ML
- HAMAMURA M
- HANFT G
- HANSELL DJ
- HAUSER F
- HAWRYLYSHYN KA
- HEIN P
- HIB J
- HIB J
- HIEBLE JP
- HIEBLE JP
- HIRASAWA A
- HIRASAWA A
- HIRASAWA A
- HISAW FL
- HOMMA Y
- HORIE K
- HROMETZ SL
- HSU SY
- HSU SY
- HU K
- HULEIHEL M
- HULME EC
- HWA J
- HWA J
- HWA J
- II M
- IRAM S
- IVELL R
- IVELL R
- JACKSON VM
- JEYABALAN A
- JEYABALAN A
- JIANG X
- JOCKENHOVEL F
- JUDSON DG
- JURKIEWICZ NH
- KAMAT AA
- KARKANIAS GB
- KERN A
- KIM JK
- KINGHORN EM
- KOHSAKA T
- KONDO S
- KRAJNC-FRANKEN MA
- KUBO T
- KUDO M
- LACEY JP
- LANGER S
- LANZAFAME AA
- LAU WA
- LAZ TM
- LEEB-LUNDBERG LM
- LEFKOWITZ RJ
- LEFKOWITZ RJ
- LEFKOWITZ RJ
- LENHART JA
- LEPOR H
- LEUNG AYH
- LIU C
- LOCKWOOD DH
- LONGHURST PA
- LOPEZ-GIMENEZ JF
- LUCAS TFG
- LUCAS TFG
- LUTHIN GR
- MACDONALD A
- MACKENZIE JF
- MACKINNON AC
- MALLARD NJ
- MANNI L
- MANNI L
- Maria Christina W. Avellar
- Maria Fatima M. Lázari
- MARKUS RP
- MARÓSTICA E
- MARÓSTICA E
- MCCUNE DF
- MCCUNE SK
- MENDES FR
- MICHELOTTI GA
- MICHELOTTI GA
- MIRANDA HF
- MIRANDA HF
- MIRANDA HF
- MOOKERJEE I
- MORIYAMA N
- MORROW AL
- MURAMATSU I
- MURRAY KT
- NADELHAFT I
- NAKAOKA H
- NASU K
- NASU K
- NEWINGER J
- NISHIS
- NOTHACKER HP
- OBARA K
- PAPATSORIS AG
- PATRÃO MT
- PEDRETTI A
- PEREZ DM
- PETITTI N
- PIASCIK MT
- PIASCIK MT
- PIASCIK MT
- PONTARI MA
- PORTER JE
- PRENZEL N
- PRICE DT
- PRICE DT
- PRICE RR
- PUPO AS
- PUPO AS
- QUEIRÓZ DB
- QUEIRÓZ DBC
- QUESADA A
- RAMARAO CS
- RAMSAY D
- RATNASOORIYA WD
- RATNASOORIYA WD
- RAYFORD W
- RICKER DD
- ROEHRBORN CG
- ROKOSH DG
- ROKOSH DG
- RUDNER XL
- RUFFOLO RR JR
- RUGGIERI MR
- SALAMANCA AE
- SALLÉS J
- SAMUEL CS
- SAMUEL CS
- SAMUEL CS
- SANBE A
- SANBORN BM
- SAROSI P
- SATO T
- SAUSSY DL JR
- SAWUTZ DG
- SCARPARO AC
- SCHWINN DA
- SCHWINN DA
- SCOFIELD MA
- SCOTT DJ
- SCOTT DJ
- SHANNON HE
- SHAPIRO E
- SHEN H
- SHERWOOD OD
- SHIMA S
- SHINOURA H
- SILVA MA
- SIU ER
- SKINNER MK
- SOKOL RZ
- STEINETZ BG
- SUDO S
- SUGAWARA T
- SUZUKI F
- TAYEBATI SK
- TENG CM
- TENSEN CP
- TESTA R
- THEBAULT S
- THEROUX TL
- TOEWS ML
- UBERTI MA
- UBERTI MA
- VAN DIJK MM
- VAN KOPPEN CJ
- VARMA DR
- VENTURA S
- VICENTIC A
- VIVAS NM
- VÁZQUEZ-PRADO J
- WALDEN PD
- WALKER WH
- WANG JM
- WANG X ET AL
- WAUGH DJ
- WESS J
- WIER WG
- XIAO L
- XU Z
- YAN HH
- YANG M
- YANG-FENG TL
- YANG-FENG TL
- YASUOKA A
- YAZAWA H
- YAZAWA H
- YKI-JARVINEN H
- YOSHINAGA T
- ZHAO L
- ZHONG H
- ZHONG H
- ZIMMERMANN S
- ZUSCIK MJ
- Publication venue
- 'FapUNIFESP (SciELO)'
- Publication date
- 01/09/2009
- Field of study
This review focuses on the expression and function of muscarinic acetylcholine receptors (mAChRs), α1-adrenoceptors and relaxin receptors in the male reproductive tract. The localization and differential expression of mAChR and α1-adrenoceptor subtypes in specific compartments of the efferent ductules, epididymis, vas deferens, seminal vesicle and prostate of various species indicate a role for these receptors in the modulation of luminal fluid composition and smooth muscle contraction, including effects on male fertility. Furthermore, the activation of mAChRs induces transactivation of the epidermal growth factor receptor (EGFR) and the Sertoli cell proliferation. The relaxin receptors are present in the testis, RXFP1 in elongated spermatids and Sertoli cells from rat, and RXFP2 in Leydig and germ cells from rat and human, suggesting a role for these receptors in the spermatogenic process. The localization of both receptors in the apical portion of epithelial cells and smooth muscle layers of the vas deferens suggests an involvement of these receptors in the contraction and regulation of secretion.Esta revisão enfatiza a expressão e a função dos receptores muscarínicos, adrenoceptores α1 e receptores para relaxina no sistema reprodutor masculino. A expressão dos receptores muscarínicos e adrenoceptores α1 em compartimentos específicos de dúctulos eferentes, epidídimo, ductos deferentes, vesícula seminal e próstata de várias espécies indica o envolvimento destes receptores na modulação da composição do fluido luminal e na contração do músculo liso, incluindo efeitos na fertilidade masculina. Além disso, a ativação dos receptores muscarínicos leva à transativação do receptor para o fator crescimento epidermal e proliferação das células de Sertoli. Os receptores para relaxina estão presentes no testículo, RXFP1 nas espermátides alongadas e células de Sertoli de rato e RXFP2 nas células de Leydig e germinativas de ratos e humano, sugerindo o envolvimento destes receptores no processo espermatogênico. A localização de ambos os receptores na porção apical das células epiteliais e no músculo liso dos ductos deferentes de rato sugere um papel na contração e na regulação da secreção.Fundação de Amparo à Pesquisa do Estado de São Paulo (FAPESP)Conselho Nacional de Desenvolvimento Científico e Tecnológico (CNPq)Universidade Federal de São Paulo (UNIFESP) Escola Paulista de Medicina Departamento de FarmacologiaUNIFESP, EPM, Depto. de FarmacologiaSciEL
Expression and function of G-protein-coupled receptorsin the male reproductive tract
- Author
- ABOUD R
- ALONSO-LLAMAZARES A
- ANAND-IVELL RJ
- ANDERSON MB
- BAN Y
- BATHGATE RA
- BATHGATE RA
- BERNARD V
- BERNARD V
- BHATHAL PS
- BIRDSALL NJ
- BISHOP MJ
- BLANCO M
- BOGIC L
- BORGES MOR
- BRADDON SA
- BRODDE OE
- BURAZIN TC
- BURT RP
- BURT RP
- CAMPOS M
- Catarina S. Porto
- CAULFIELD MP
- CHALOTHORN D
- CHAN HC
- CHANG DJ
- CHATURAPANICH G
- CHEAH SH
- CHEN S
- CHEN S
- COGÉ F ET AL
- DA SILVA MC
- DALY CJ
- DANIELS DV
- DAVENPORT CW
- DEBRUYNE FM
- DENG XF
- DIVIANI D
- DOCHERTY JR
- DOCHERTY JR
- DOGGRELL SA
- DU JY
- EGLEN RM
- EGLEN RM
- EHRÉN I
- EISENHOFER G
- ERRASTI AE
- ESBENSHADE TA
- ESSIG M
- FENG S
- FEVOLD HL
- FILONZI M
- FORD APDW
- FORD APDW
- FORRAY C
- FUKASAWA R
- GAO B
- GAO B
- GOBEIL F JR
- GONZÁLEZ-ESPINOSA C
- GRAHAM RM
- GRIMM U
- GUNNERSEN JM
- GUNNERSEN JM
- HAAG C
- HAGUE C
- HAGUE C
- HALLS ML
- HALLS ML
- HALLS ML
- HAMAMURA M
- HANFT G
- HANSELL DJ
- HAUSER F
- HAWRYLYSHYN KA
- HEIN P
- HIB J
- HIB J
- HIEBLE JP
- HIEBLE JP
- HIRASAWA A
- HIRASAWA A
- HIRASAWA A
- HISAW FL
- HOMMA Y
- HORIE K
- HROMETZ SL
- HSU SY
- HSU SY
- HU K
- HULEIHEL M
- HULME EC
- HWA J
- HWA J
- HWA J
- II M
- IRAM S
- IVELL R
- IVELL R
- JACKSON VM
- JEYABALAN A
- JEYABALAN A
- JIANG X
- JOCKENHOVEL F
- JUDSON DG
- JURKIEWICZ NH
- KAMAT AA
- KARKANIAS GB
- KERN A
- KIM JK
- KINGHORN EM
- KOHSAKA T
- KONDO S
- KRAJNC-FRANKEN MA
- KUBO T
- KUDO M
- LACEY JP
- LANGER S
- LANZAFAME AA
- LAU WA
- LAZ TM
- LEEB-LUNDBERG LM
- LEFKOWITZ RJ
- LEFKOWITZ RJ
- LEFKOWITZ RJ
- LENHART JA
- LEPOR H
- LEUNG AYH
- LIU C
- LOCKWOOD DH
- LONGHURST PA
- LOPEZ-GIMENEZ JF
- LUCAS TFG
- LUCAS TFG
- LUTHIN GR
- MACDONALD A
- MACKENZIE JF
- MACKINNON AC
- MALLARD NJ
- MANNI L
- MANNI L
- Maria Christina W. Avellar
- Maria Fatima M. Lázari
- MARKUS RP
- MARÓSTICA E
- MARÓSTICA E
- MCCUNE DF
- MCCUNE SK
- MENDES FR
- MICHELOTTI GA
- MICHELOTTI GA
- MIRANDA HF
- MIRANDA HF
- MIRANDA HF
- MOOKERJEE I
- MORIYAMA N
- MORROW AL
- MURAMATSU I
- MURRAY KT
- NADELHAFT I
- NAKAOKA H
- NASU K
- NASU K
- NEWINGER J
- NISHIS
- NOTHACKER HP
- OBARA K
- PAPATSORIS AG
- PATRÃO MT
- PEDRETTI A
- PEREZ DM
- PETITTI N
- PIASCIK MT
- PIASCIK MT
- PIASCIK MT
- PONTARI MA
- PORTER JE
- PRENZEL N
- PRICE DT
- PRICE DT
- PRICE RR
- PUPO AS
- PUPO AS
- QUEIRÓZ DB
- QUEIRÓZ DBC
- QUESADA A
- RAMARAO CS
- RAMSAY D
- RATNASOORIYA WD
- RATNASOORIYA WD
- RAYFORD W
- RICKER DD
- ROEHRBORN CG
- ROKOSH DG
- ROKOSH DG
- RUDNER XL
- RUFFOLO RR JR
- RUGGIERI MR
- SALAMANCA AE
- SALLÉS J
- SAMUEL CS
- SAMUEL CS
- SAMUEL CS
- SANBE A
- SANBORN BM
- SAROSI P
- SATO T
- SAUSSY DL JR
- SAWUTZ DG
- SCARPARO AC
- SCHWINN DA
- SCHWINN DA
- SCOFIELD MA
- SCOTT DJ
- SCOTT DJ
- SHANNON HE
- SHAPIRO E
- SHEN H
- SHERWOOD OD
- SHIMA S
- SHINOURA H
- SILVA MA
- SIU ER
- SKINNER MK
- SOKOL RZ
- STEINETZ BG
- SUDO S
- SUGAWARA T
- SUZUKI F
- TAYEBATI SK
- TENG CM
- TENSEN CP
- TESTA R
- THEBAULT S
- THEROUX TL
- TOEWS ML
- UBERTI MA
- UBERTI MA
- VAN DIJK MM
- VAN KOPPEN CJ
- VARMA DR
- VENTURA S
- VICENTIC A
- VIVAS NM
- VÁZQUEZ-PRADO J
- WALDEN PD
- WALKER WH
- WANG JM
- WANG X ET AL
- WAUGH DJ
- WESS J
- WIER WG
- XIAO L
- XU Z
- YAN HH
- YANG M
- YANG-FENG TL
- YANG-FENG TL
- YASUOKA A
- YAZAWA H
- YAZAWA H
- YKI-JARVINEN H
- YOSHINAGA T
- ZHAO L
- ZHONG H
- ZHONG H
- ZIMMERMANN S
- ZUSCIK MJ
- Publication venue
- 'FapUNIFESP (SciELO)'
- Publication date
- Field of study
Measurement of Higgs boson production in the diphoton decay channel in pp collisions at center-of-mass energies of 7 and 8 TeV with the ATLAS detector
- Author
- Aad G
- Abbott B
- Abdallah J
- Abdinov O
- Aben R
- Abi B
- Abolins M
- AbouZeid OS
- Abramowicz H
- Abreu H
- Abreu R
- Abulaiti Y
- Acharya BS
- Adam ER
- Adamczyk L
- Adams DL
- Adelman J
- Adomeit S
- Adye T
- Agatonovic-Jovina T
- Aguilar-Saavedra JA
- Agustoni M
- Ahlen SP
- Ahmadov F
- Aielli G
- Akerstedt H
- Akesson TP
- Akimoto G
- Akimov AV
- Alberghi GL
- Albert J
- Albrand S
- Alconada Verzini MJ
- Aleksa M
- Aleksandrov IN
- Alexa C
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- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2014
- Field of study
A measurement of the production processes of the recently discovered Higgs boson is performed in the two-photon final state using 4.5 fb[superscript −1] of proton-proton collisions data at √s=7 TeV and 20.3 fb[superscript −1] at √s=8 TeV collected by the ATLAS detector at the Large Hadron Collider. The number of observed Higgs boson decays to diphotons divided by the corresponding Standard Model prediction, called the signal strength, is found to be μ=1.17±0.27 at the value of the Higgs boson mass measured by ATLAS, m[subscript H]=125.4 GeV. The analysis is optimized to measure the signal strengths for individual Higgs boson production processes at this value of m[subscript H]. They are found to be μ[subscript ggF]=1.32±0.38, μ[subscript VBF]=0.8±0.7, μ[subscript WH]=1.0±1.6, μ[subscript ZH]=0.1[superscript +3.7 subscript −0.1], and μ[subscript t [bar over t] H] =1.6[superscript +2.7 subscript −1.8], for Higgs boson production through gluon fusion, vector-boson fusion, and in association with a W or Z boson or a top-quark pair, respectively. Compared with the previously published ATLAS analysis, the results reported here also benefit from a new energy calibration procedure for photons and the subsequent reduction of the systematic uncertainty on the diphoton mass resolution. No significant deviations from the predictions of the Standard Model are found.European Organization for Nuclear ResearchUnited States. Dept. of EnergyNational Science Foundation (U.S.)Brookhaven National Laborator
Measurement of the transverse polarization of Λ and Λ¯ hyperons produced in proton-proton collisions at √s=7 TeV using the ATLAS detector
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- Zhemchugov A
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- Zibell A
- Zieminska D
- Zimine NI
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- Zobernig G
- Zoccoli A
- Zurzolo G
- Zwalinski L
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/12/2014
- Field of study
The transverse polarization of Λ and Λ¯ hyperons produced in proton-proton collisions at a center-of-mass energy of 7 TeV is measured. The analysis uses 760 μb−1 of minimum bias data collected by the ATLAS detector at the LHC in the year 2010. The measured transverse polarization averaged over Feynman xF from 5×10−5 to 0.01 and transverse momentum pT from 0.8 to 15 GeV is −0.010±0.005(stat)±0.004(syst) for Λ and 0.002±0.006(stat)±0.004(syst) for Λ¯. It is also measured as a function of xF and pT, but no significant dependence on these variables is observed. Prior to this measurement, the polarization was measured at fixed-target experiments with center-of-mass energies up to about 40 GeV. The ATLAS results are compatible with the extrapolation of a fit from previous measurements to the xF range covered by this measurement
Measurements of differential cross-sections in four-lepton events in 13 TeV proton-proton collisions with the ATLAS detector
- Author
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- Abhayasinghe DK
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- Bloch I
- Blocker C
- Blue A
- Blumenschein U
- Bobbink GJ
- Bobrovnikov VS
- Bocchetta SS
- Boeriu OEV
- Bogavac D
- Bogdanchikov AG
- Bohm C
- Boisvert V
- Bokan P
- Bolanos GR
- Bold T
- Bolz AE
- Bomben M
- Bona M
- Bonilla JS
- Boonekamp M
- Booth CD
- Borbely AG
- Borecka-Bielska HM
- Borgna LS
- Borisov A
- Borissov G
- Bortoletto D
- Boscherini D
- Bosman M
- Bostanabad MG
- Bouaouda K
- Boudreau J
- Bouhova-Thacker E
- Boumediene D
- Bourdarios CA
- Boveia A
- Boyd J
- Boye D
- Boyko IR
- Bozson AJ
- Bracinik J
- Brahimi N
- Brandt G
- Brandt O
- Braren F
- Brau B
- Brau JE
- Brendlinger K
- Brener R
- Brenner L
- Brenner R
- Bressler S
- Bret MC
- Brickwedde B
- Briglin DL
- Britton D
- Britzger D
- Brock I
- Brock R
- Brooks WK
- Brost E
- Bruers B
- Bruncko D
- Bruni A
- Bruni G
- Bruschi M
- Bruscino N
- Bryngemark L
- Buanes T
- Buat Q
- Buchholz P
- Buckley AG
- Budagov IA
- Buescher V
- Bugge MK
- Bulekov O
- Bullard BA
- Burch TJ
- Burdin S
- Burgard CD
- Burger AM
- Burghgrave B
- Burr JTP
- Burton CD
- Burzynski JC
- Buschmann E
- Bussey PJ
- Butler JM
- Buttar CM
- Butterworth JM
- Butti P
- Buttinger W
- Buzatu A
- Buzykaev AR
- Bylund OB
- Cabras G
- Cabrera Urban S
- Caforio D
- Cai H
- Cairo VMM
- Cakir IT
- Cakir O
- Calace N
- Calafiura P
- Calderini G
- Calfayan P
- Callea G
- Caloba LP
- Caltabiano A
- Calvet D
- Calvet S
- Calvet TP
- Calvetti M
- Camarda S
- Camarero Munoz D
- Camarri P
- Camelia EA
- Camerlingo MT
- Cameron D
- Camincher C
- Campana S
- Campanelli M
- Camplani A
- Canale V
- Canesse A
- Cantero J
- Cao T
- Cao Y
- Capriles FGD
- Capua M
- Cardarelli R
- Cardillo F
- Carducci G
- Carli I
- Carli T
- Carlino G
- Carlson BT
- Carlson EM
- Carminati L
- Carney RMD
- Caron S
- Carquin E
- Carra S
- Carratta G
- Carter JWS
- Carter TM
- Casado MP
- Casha AF
- Castiglia EG
- Castillo Garcia L
- Castillo Gimenez V
- Castillo FL
- Castillo LRF
- Castro NF
- Catinaccio A
- Catmore JR
- Cattai A
- Cavaliere V
- Cavasinni V
- Celebi E
- Celli F
- Cerny K
- Cerqueira AS
- Cerri A
- Cerrito L
- Cerutti F
- Cervelli A
- Cetin SA
- Chadi Z
- Chakraborty D
- Chan J
- Chan WS
- Chan WY
- Chapman JD
- Chargeishvili B
- Charlton DG
- Charman TP
- Chatterjee M
- Chau CC
- Che S
- Chekanov S
- Chekulaev S
- Chelkov GA
- Chen B
- Chen C
- Chen CH
- Chen H
- Chen H
- Chen J
- Chen J
- Chen J
- Chen S
- Chen SJ
- Chen X
- Chen Y
- Chen Y-H
- Cheng HC
- Cheng HJ
- Cheplakov A
- Cheremushkina E
- Cheu E
- Cheung K
- Chevalerias TJA
- Chevalier L
- Chiarella V
- Chiarelli G
- Chiodini G
- Chisholm AS
- Chitan A
- Chiu I
- Chiu YH
- Chizhov M
- Choi K
- Chomont AR
- Chou Y
- Chow YS
- Christopher LD
- Chu MC
- Chu X
- Chudoba J
- Chwastowski JJ
- Chytka L
- Cieri D
- Ciesla KM
- Cindro V
- Ciocio A
- Cirotto F
- Citron ZH
- Citterio M
- Ciubotaru DA
- Ciungu BM
- Clark A
- Clark PJ
- Clawson SE
- Clement C
- Clissa L
- Coadou Y
- Cobal M
- Coccaro A
- Cochran J
- Codina EP
- Cohen H
- Coimbra AEC
- Cole B
- Collot J
- Connell SH
- Connelly IA
- Constantinescu S
- Conventi F
- Cooper-Sarkar AM
- Cormier F
- Cormier KJR
- Cornell SD
- Corpe LD
- Corradi M
- Correia AMH
- Corrigan EE
- Corriveau F
- Costa MJ
- Costanza F
- Costanzo D
- Coutinho YA
- Cowan G
- Cowley JW
- Crane J
- Cranmer K
- Creager RA
- Crepe-Renaudin S
- Crescioli F
- Cristinziani M
- Croft V
- Crosetti G
- Cueto A
- Cui H
- Cukierman AR
- Cunningham WR
- Czekierda S
- Czodrowski P
- Czurylo MM
- D'amen G
- D'Amico V
- D'Auria S
- D'Eramo L
- D'onofrio A
- D'Onofrio M
- D'uffizi M
- da Costa JBG
- Da Via C
- Dabrowski W
- Dachs F
- Dado T
- Dahbi S
- Dai T
- Dallapiccola C
- Dam M
- Damazio DO
- Damp J
- Dandoy JR
- Daneri MF
- Danninger M
- Dao V
- Darbo G
- Dartsi O
- Dattagupta A
- Daubney T
- David C
- Davidek T
- Davis DR
- Dawson I
- de Andrade Filho LM
- De Asmundis R
- De Beurs M
- De Castro S
- De Groot N
- de Jong P
- De la Torre H
- de Lima DEF
- De Lima RT
- De Maria A
- De Pedis D
- De Regie JBDV
- de Renstrom PAB
- De Sa RCL
- De Salvo A
- De Sanctis U
- De Santis M
- De Santo A
- De Sousa MJDCS
- De K
- Dedovich D
- Deiana AM
- Del Peso J
- Delgado AT
- Delgove D
- Deliot F
- Delitzsch CM
- Dell'Acqua A
- Dell'Asta L
- Della Pietra M
- Della Volpe D
- Delmastro M
- Delporte C
- Delsart PA
- Demers S
- Demichev M
- Demontigny G
- Denisov SP
- Derendarz D
- Derkaoui JE
- Derue F
- Dervan P
- Desch K
- Dette K
- Deutsch C
- Devesa MR
- Deviveiros PO
- Di Bello FA
- Di Ciaccio A
- Di Ciaccio L
- Di Donato C
- Di Girolamo A
- Di Gregorio G
- Di Luca A
- Di Micco B
- Di Nardo R
- Di Petrillo KF
- Di Sipio R
- Diaconu C
- Dias FA
- Diaz LP
- Diaz MA
- Diaz YD
- Dickinson J
- Didenko M
- Diehl EB
- Dietrich J
- Dimitrievska A
- Ding W
- Dingfelder J
- Dittmeier SJ
- Dittus F
- Djama F
- Djobava T
- Djuvsland J
- Do Vale MAB
- Do Vale TD
- Dobre M
- Dodsworth D
- Doglioni C
- Dolejsi J
- Dolezal Z
- Dominguez LP
- Don MMR
- Donadelli M
- Donaldson CP
- Dong B
- Donini J
- Donszelmann TC
- Dopke J
- Doria A
- Dova MT
- Doyle AT
- Drechsler E
- Dreyer E
- Dreyer T
- Drobac AS
- du Pree TA
- Du D
- Duan Y
- Dubinin F
- Dubovsky M
- Dubreuil A
- Duchovni E
- Duckeck G
- Ducu OA
- Duda D
- Dudarev A
- Dudder AC
- Duffield EM
- Duflot L
- Duhrssen M
- Dulsen C
- Dumancic M
- Dumitriu AE
- Dunford M
- Dungs S
- Duperrin A
- Duren M
- Durglishvili A
- Duschinger D
- Dutta B
- Duvnjak D
- Dyckes G
- Dyndal M
- Dysch S
- Dziedzic BS
- Eggleston MG
- Eifert T
- Eigen G
- Einsweiler K
- Ekelof T
- El Jarrari H
- El Moursli RC
- Ellajosyula V
- Ellert M
- Ellinghaus F
- Elliot AA
- Ellis N
- Elmsheuser J
- Elsing M
- Emeliyanov D
- Emerman A
- Enari Y
- Epland MB
- Erdmann J
- Ereditato A
- Erland PA
- Errenst M
- Escalier M
- Escobar C
- Estrada Pastor O
- Etzion E
- Evans G
- Evans H
- Evans MO
- Ezhilov A
- Fabbri F
- Fabbri L
- Fabiani V
- Facini G
- Fakhrutdinov RM
- Falciano S
- Falke PJ
- Falke S
- Faltova J
- Fang Y
- Fang Y
- Fanourakis G
- Fanti M
- Faraj M
- Farbin A
- Farilla A
- Farina EM
- Farooque T
- Farrington SM
- Farthouat P
- Fassi F
- Fassnacht P
- Fassouliotis D
- Fawcett WJ
- Fayard L
- Fedin OL
- Fedorko W
- Fehr A
- Feickert M
- Feligioni L
- Fell A
- Feng C
- Feng M
- Fenton MJ
- Fenyuk AB
- Ferguson SW
- Ferrando J
- Ferrari A
- Ferrari P
- Ferrari R
- Ferraz VA
- Ferrer A
- Ferrere D
- Ferretti C
- Fiedler F
- Filthaut F
- Finelli KD
- Fiolhais MCN
- Fiorini L
- Fischer F
- Fischer J
- Fisher WC
- Fitschen T
- Fleck I
- Fleischmann P
- Flick T
- Flierl BM
- Flores L
- Follega FM
- Fomin N
- Foo JH
- Forcolin GT
- Forland BC
- Formica A
- Forster FA
- Forti AC
- Fortin E
- Foti MG
- Fournier D
- Fox H
- Francavilla P
- Francescato S
- Franchini M
- Franchino S
- Francis D
- Franco L
- Franconi L
- Franklin M
- Frattari G
- Fray AN
- Freeman PM
- Freund B
- Freund WS
- Freundlich EM
- Frizzell DC
- Froidevaux D
- Frost JA
- Fujimoto M
- Fukunaga C
- Fullana Torregrosa E
- Fusayasu T
- Fuster J
- Gabrielli A
- Gabrielli A
- Gadatsch S
- Gadow P
- Gagliardi G
- Gagnon LG
- Gajardo CMR
- Gallardo GE
- Gallas EJ
- Gallop BJ
- Gama RG
- Gan KK
- Ganguly S
- Gao J
- Gao Y
- Gao YS
- Garay Walls FM
- Garcia Navarro JE
- Garcia BRM
- Garcia C
- Garcia RFN
- Garcia-Argos C
- Garcia-Sciveres M
- Gardner RW
- Garelli N
- Gargiulo S
- Garner CA
- Garonne V
- Gasiorowski SJ
- Gaspar P
- Gaudiello A
- Gaudio G
- Gauzzi P
- Gavrilenko IL
- Gavrilyuk A
- Gay C
- Gaycken G
- Gazis EN
- Geanta AA
- Gee CM
- Gee CNP
- Geisen J
- Geisen M
- Gemme C
- Genest MH
- Geng C
- Gentile S
- George S
- Geralis T
- Gerlach LO
- Gessinger-Befurt P
- Gessner G
- Ghneimat M
- Ghosh A
- Ghosh A
- Giacobbe B
- Giagu S
- Giangiacomi N
- Giannelli MF
- Giannetti P
- Giannini A
- Giannini G
- Gibson SM
- Gignac M
- Gil DT
- Gilbert BJ
- Gillberg D
- Gilles G
- Gillwald NEK
- Gingrich DM
- Giordani MP
- Giraud PF
- Giugliarelli G
- Giugni D
- Giuli F
- Gkaitatzis S
- Gkialas I
- Gkougkousis EL
- Gkountoumis P
- Gladilin LK
- Glasman C
- Glatzer J
- Glaysher PCF
- Glazov A
- Gledhill GR
- Gnesi I
- Goblirsch-Kolb M
- Godin D
- Goldfarb S
- Golling T
- Golubkov D
- Gomes A
- Goncalo R
- Gonella G
- Gonella L
- Gongadze A
- Goni RG
- Gonnella F
- Gonski JL
- Gonzalez de la Hoz S
- Gonzalez Fernandez S
- Gonzalez-Sevilla S
- Gonzalvo Rodriguez GR
- Goossens L
- Gorasia NA
- Gorbounov PA
- Gordon HA
- Gorini B
- Gorini E
- Gorisek A
- Goshaw AT
- Gostkin M
- Gottardo CA
- Gouighri M
- Goussiou AG
- Govender N
- Goy C
- Grabowska-Bold I
- Graham EC
- Gramling J
- Gramstad E
- Grancagnolo S
- Grandi M
- Gratchev V
- Gravila PM
- Gravili FG
- Gray C
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- Grefe C
- Gregersen K
- Gregor IM
- Grenier P
- Grevtsov K
- Grieco C
- Grieser NA
- Grillo AA
- Grimm K
- Grinstein S
- Griso SP
- Grivaz J-F
- Groh S
- Gross E
- Grosse-Knetter J
- Grout ZJ
- Grud C
- Grummer A
- Grundy JC
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- Guan W
- Gubbels C
- Guenther J
- Guerguichon A
- Guerrero Rojas JGR
- Guescini F
- Guest D
- Gugel R
- Guida A
- Guillemin T
- Guindon S
- Guo J
- Guo W
- Guo Y
- Guo Z
- Gupta DB
- Gupta R
- Gurbuz S
- Gustavino G
- Guth M
- Gutierrez P
- Gutschow C
- Guyot C
- Gwenlan C
- Gwilliam CB
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- Harrison PF
- Hartman NM
- Hartmann NM
- Hasegawa Y
- Hasib A
- Hassani S
- Haug S
- Hauser R
- Havranek M
- Hawkes CM
- Hawkings RJ
- Hayashida S
- Hayden D
- Hayes C
- Hayes RL
- Hays CP
- Hays JM
- Hayward HS
- Haywood SJ
- He F
- He Y
- Heath MP
- Hedberg V
- Heggelund AL
- Hehir ND
- Heidegger C
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- Heinlein JG
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- Helary L
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- Hellesund S
- Helling CM
- Hellman S
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- Henderson RCW
- Henkelmann L
- Herde H
- Hernandez DP
- Herr H
- Herrmann MG
- Herrmann T
- Herten G
- Hertenberger R
- Hervas L
- Hesketh GG
- Hessey NP
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- Higashino S
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- Hildebrand K
- Hill JC
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- Hiller KH
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- Hinchliffe I
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- Hiti B
- Hladik O
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- Iakovidis G
- Ibragimov I
- Iconomidou-Fayard L
- Iengo P
- Ignazzi R
- Iguchi R
- Iizawa T
- Ikegami Y
- Ikeno M
- Ilic N
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- Infante CMV
- Introzzi G
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- Ippolito V
- Isacson MF
- Ishino M
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- Izzo V
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- Karkanias I
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- Karyukhin AN
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- Knue A
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- Kodama T
- Kodys P
- Koeck DM
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- Koffas T
- Kohler NM
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- Koletsou I
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- Kondo T
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- Kong AXY
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- Konya B
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- Kotwal A
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- Kourlitis E
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- LeBlanc M
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- Leite MAL
- Leitgeb CE
- Leitner R
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- Leopold A
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- Yildiz HD
- Yin P
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- Yoshihara K
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- Zahreddine J
- Zaitsev AM
- Zakareishvili T
- Zakharchuk N
- Zambito S
- Zanzi D
- Zeissner S
- Zeitnitz C
- Zemaityte G
- Zeng JC
- Zenin O
- Zenis T
- Zerwas D
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- Zhang DF
- Zhang G
- Zhang J
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- Zhang L
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- Zhang X
- Zhang X
- Zhang Y
- Zhang Z
- Zhang Z
- Zhao P
- Zhao Y
- Zhao Z
- Zhemchugov A
- Zheng Z
- Zhong D
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- Zhu H
- Zhu HL
- Zhu J
- Zhu Y
- Zhuang X
- Zhukov K
- Zhulanov V
- Zieminska D
- Zimine N
- Zimmermann S
- Zinonos Z
- Ziolkowski M
- Zobernig G
- Zoccoli A
- Zoch K
- Zorbas TG
- Zou R
- Zwalinski L
- Publication venue
- 'Springer Fachmedien Wiesbaden GmbH'
- Publication date
- 02/07/2021
- Field of study
Measurements of four-lepton differential and integrated fiducial cross-sections in events with two same-flavour, opposite-charge electron or muon pairs are presented. The data correspond to 139 fb−1 of s√ = 13 TeV proton-proton collisions, collected by the ATLAS detector during Run 2 of the Large Hadron Collider (2015–2018). The final state has contributions from a number of interesting Standard Model processes that dominate in different four-lepton invariant mass regions, including single Z boson production, Higgs boson production and on-shell ZZ production, with a complex mix of interference terms, and possible contributions from physics beyond the Standard Model. The differential cross-sections include the four-lepton invariant mass inclusively, in slices of other kinematic variables, and in different lepton flavour categories. Also measured are dilepton invariant masses, transverse momenta, and angular correlation variables, in four regions of four-lepton invariant mass, each dominated by different processes. The measurements are corrected for detector effects and are compared with state-of-the-art Standard Model calculations, which are found to be consistent with the data. The Z → 4ℓ branching fraction is extracted, giving a value of (4.41 ± 0.30) × 10−6. Constraints on effective field theory parameters and a model based on a spontaneously broken B − L gauge symmetry are also evaluated. Further reinterpretations can be performed with the provided information
Search for scalar diphoton resonances in the mass range 65-600 GeV with the ATLAS detector in pp collision data at √s = 8 TeV
- Author
- Aad G
- Abbott B
- Abdallah J
- Abdinov O
- Aben R
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- Zhemchugov A
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- Zobernig G
- Zoccoli A
- zur Nedden M
- Zurzolo G
- Zutshi V
- Zwalinski L
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2014
- Field of study
A search for scalar particles decaying via narrow resonances into two photons in the mass range 65–600 GeV is performed using 20.3 fb−¹ of √s=8 TeV pp collision data collected with the ATLAS detector at the Large Hadron Collider. The recently discovered Higgs boson is treated as a background. No significant evidence for an additional signal is observed. The results are presented as limits at the 95% confidence level on the production cross section of a scalar boson times branching ratio into two photons, in a fiducial volume where the reconstruction efficiency is approximately independent of the event topology. The upper limits set extend over a considerably wider mass range than previous searches
Search for anomalous couplings in the W tb vertex from the measurement of double differential angular decay rates of single top quarks produced in the t-channel with the ATLAS detector
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- Chelkov GA
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- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 13/10/2015
- Field of study
The electroweak production and subsequent decay of single top quarks is determined by the properties of the Wtb vertex. This vertex can be described by the complex parameters of an effective Lagrangian. An analysis of angular distributions of the decay products of single top quarks produced in the t -channel constrains these parameters simultaneously. The analysis described in this paper uses 4.6 fb−1 of proton-proton collision data at √s =7 TeV collected with the ATLAS detector at the LHC. Two parameters are measured simultaneously in this analysis. The fraction f 1 of decays containing transversely polarised W bosons is measured to be 0.37 ± 0.07 (stat.⊕syst.). The phase δ − between amplitudes for transversely and longitudinally polarised W bosons recoiling against left-handed b-quarks is measured to be −0.014π ± 0.036π (stat.⊕syst.). The correlation in the measurement of these parameters is 0.15. These values result in two-dimensional limits at the 95% confidence level on the ratio of the complex coupling parameters g R and V L, yielding Re[g R /V L] ∈ [−0.36, 0.10] and Im[g R /V L] ∈ [−0.17, 0.23] with a correlation of 0.11. The results are in good agreement with the predictions of the Standard Model
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