147 research outputs found
Measurement of the cross-section of high transverse momentum vector bosons reconstructed as single jets and studies of jet substructure in pp collisions at âs = 7 TeV with the ATLAS detector
- Author
- Aad G
- Abajyan T
- Abbott B
- Abdallah J
- Abdinov O
- Aben R
- Abi B
- Abolins M
- AbouZeid OS
- Abramowicz H
- Abreu H
- Abulaitia Y
- Acharya BS
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- Adelman J
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- Akimov AV
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- Aleksandrov IN
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- Zurzolo G
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- Publication venue
- 'IOP Publishing'
- Publication date
- 01/01/2014
- Field of study
This paper presents a measurement of the cross-section for high transverse momentum W and Z bosons produced in pp collisions and decaying to all-hadronic final states. The data used in the analysis were recorded by the ATLAS detector at the CERN Large Hadron Collider at a centre-of-mass energy of âs = 7 TeV;{\rm Te}{\rm V}andcorrespondtoanintegratedluminosityof4.6\;{\rm f}{{{\rm b}}^{-1}}.ThemeasurementisperformedbyreconstructingtheboostedWorZbosonsinsinglejets.ThereconstructedjetmassisusedtoidentifytheWandZbosons,andajetsubstructuremethodbasedonenergyclusterinformationinthejetcentreâofâmassframeisusedtosuppressthelargemultiâjetbackground.ThecrossâsectionforeventswithahadronicallydecayingWorZboson,withtransversemomentum{{p}_{{\rm T}}}\gt 320\;{\rm Ge}{\rm V}andpseudorapidity|\eta |\lt 1.9,ismeasuredtobe{{\sigma }_{W+Z}}=8.5\pm 1.7$ pb and is compared to next-to-leading-order calculations. The selected events are further used to study jet grooming techniques
Search for high-mass resonances decaying to dilepton final states in pp collisions at sâ=7 TeV with the ATLAS detector
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- Zinonos Z
- Ziolkowski M
- Zitoun R
- Zivkovic L
- Zmouchko VV
- Zobernig G
- Zoccoli A
- zur Nedden M
- Zutshi V
- Zwalinski L
- Publication venue
- Springer
- Publication date
- 01/01/2012
- Field of study
The ATLAS detector at the Large Hadron Collider is used to search for high-mass resonances decaying to an electron-positron pair or a muon-antimuon pair. The search is sensitive to heavy neutral ZâČ gauge bosons, Randall-Sundrum gravitons, Z * bosons, techni-mesons, Kaluza-Klein Z/Îł bosons, and bosons predicted by Torsion models. Results are presented based on an analysis of pp collisions at a center-of-mass energy of 7 TeV corresponding to an integrated luminosity of 4.9 fbâ1 in the e + e â channel and 5.0 fbâ1 in the ÎŒ + ÎŒ âchannel. A Z âČ boson with Standard Model-like couplings is excluded at 95 % confidence level for masses below 2.22 TeV. A Randall-Sundrum graviton with coupling k/MPl=0.1 is excluded at 95 % confidence level for masses below 2.16 TeV. Limits on the other models are also presented, including Technicolor and Minimal ZâČ Models
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 Ï 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, Ï, 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 ÎČ in the mhmax scenario for mA in the range of 90GeV to 500 GeV. Copyright CERN
Observation of associated near-side and away-side long-range correlations in âsNN=5.02ââTeV proton-lead collisions with the ATLAS detector
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- Yamanaka T
- Yamauchi K
- Yamazaki T
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- Yang UK
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- Yanush S
- Yao L
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- Yen AL
- Yilmaz M
- Yoosoofmiya R
- Yorita K
- Yoshida R
- Yoshihara K
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- Young CJ
- Youssef S
- Yu D
- Yu DR
- Yu J
- Yu J
- Yuan L
- Yurkewicz A
- Zabinski B
- Zaidan R
- Zaitsev AM
- Zambito S
- Zanello L
- Zanzi D
- Zaytsev A
- Zeitnitz C
- Zeman M
- Zemla A
- Zenin O
- ZeniĆĄ T
- Zerwas D
- Zevi Della Porta G
- Zhang D
- Zhang H
- Zhang J
- Zhang L
- Zhang X
- Zhang Z
- Zhao L
- Zhao Z
- Zhemchugov A
- Zhong J
- Zhou B
- Zhou N
- Zhou Y
- Zhu CG
- Zhu H
- Zhu J
- Zhu Y
- Zhuang X
- Zhuravlov V
- Zibell A
- Zieminska D
- Zimin NI
- Zimmermann R
- Zimmermann S
- Zimmermann S
- Zinonos Z
- Ziolkowski M
- Zitoun R
- ZivkoviÄ L
- Zmouchko VV
- Zobernig G
- Zoccoli A
- Zur Nedden M
- Zutshi V
- Zwalinski L
- Publication venue
- American Physical Society
- Publication date
- 01/01/2012
- Field of study
Two-particle correlations in relative azimuthal angle (ÎÏ) and pseudorapidity (Îη) are measured in âsNN=5.02ââTeV p+Pb collisions using the ATLAS detector at the LHC. The measurements are performed using approximately 1ââÎŒb-1 of data as a function of transverse momentum (pT) and the transverse energy (ÎŁETPb) summed over 3.1<η<4.9 in the direction of the Pb beam. The correlation function, constructed from charged particles, exhibits a long-range (2<|Îη|<5) ânear-sideâ (ÎÏâŒ0) correlation that grows rapidly with increasing ÎŁETPb. A long-range âaway-sideâ (ÎÏâŒÏ) correlation, obtained by subtracting the expected contributions from recoiling dijets and other sources estimated using events with small ÎŁETPb, is found to match the near-side correlation in magnitude, shape (in Îη and ÎÏ) and ÎŁETPb dependence. The resultant ÎÏ correlation is approximately symmetric about Ï/2, and is consistent with a dominant cosâĄ2ÎÏ modulation for all ÎŁETPb ranges and particle pT
Search for direct pair production of the top squark in all-hadronic final states in proton-proton collisions at sâ=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
- Adamczyk L
- Adams DL
- Adelman J
- Adomeit S
- Adye T
- Agatonovic-Jovin T
- Aguilar-Saavedra JA
- Agustoni M
- Ahlen SP
- Ahmadov F
- Aielli G
- Akerstedt H
- Akesson TPA
- Akimoto G
- Akimov AV
- Alberghi GL
- Albert J
- Albrand S
- Alconada Verzini MJ
- Aleksa M
- Aleksandrov IN
- Alexa C
- Alexander G
- Alexandre G
- Alexopoulos T
- Alhroob M
- Alimonti G
- Alio L
- Alison J
- Allbrooke BMM
- Allison LJ
- Allport PP
- Almond J
- Aloisio A
- Alonso A
- Alonso F
- Alpigiani C
- Altheimer A
- Alviggi MG
- Amako K
- Amaral Coutinho Y
- Amelung C
- Amidei D
- Amor Dos Santos SP
- Amorim A
- Amoroso S
- Amram N
- Amundsen G
- Anastopoulos C
- Ancu LS
- Andari N
- Andeen T
- Anders CF
- Anders G
- Anderson KJ
- Andreazza A
- Andrei V
- Anduaga XS
- Angelidakis S
- Angelozzi I
- Anger P
- Angerami A
- Anghinolfi F
- Anh TV
- Anisenkov AV
- Anjos N
- Annovi A
- Antonaki A
- Antonelli M
- Antonov A
- Antos J
- Anulli F
- Aoki M
- Apolle R
- Arabidze G
- Aracena I
- Arai Y
- Araque JP
- Arce ATH
- Arguin J-F
- Argyropoulos S
- Arik M
- Armbruster AJ
- Arnaez O
- Arnal V
- Arnold H
- Arratia M
- Arslan O
- Artamonov A
- Artoni G
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- Zurzolo G
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- Zwalinski L
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2014
- Field of study
The results of a search for direct pair production of the scalar partner to the top quark using an integrated luminosity of 20.1fbâ1 of protonâproton collision data at âs = 8 TeV recorded with the ATLAS detector at the LHC are reported. The top squark is assumed to decay via tËâtÏË01 or tËâ bÏ˱1 âbW(â)ÏË01 , where ÏË01 (Ï˱1 ) denotes the lightest neutralino (chargino) in supersymmetric models. The search targets a fully-hadronic final state in events with four or more jets and large missing transverse momentum. No significant excess over the Standard Model background prediction is observed, and exclusion limits are reported in terms of the top squark and neutralino masses and as a function of the branching fraction of tË â tÏË01 . For a branching fraction of 100%, top squark masses in the range 270â645 GeV are excluded for ÏË01 masses below 30 GeV. For a branching fraction of 50% to either tË â tÏË01 or tË â bÏ˱1 , and assuming the Ï˱1 mass to be twice the ÏË01 mass, top squark masses in the range 250â550 GeV are excluded for ÏË01 masses below 60 GeV
Search for pair-produced long-lived neutral particles decaying to jets in the ATLAS hadronic calorimeter in ppcollisions at âs=8TeV
- Author
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- zur Nedden M
- Zurzolo G
- Zutshi V
- Zwalinski L
- Publication venue
- 'Elsevier BV'
- Publication date
- 01/01/2014
- Field of study
The ATLAS detector at the Large Hadron Collider at CERN is used to search for the decay of a scalar boson to a pair of long-lived particles, neutral under the Standard Model gauge group, in 20.3fbâ1of data collected in protonâproton collisions at âs=8TeV. This search is sensitive to long-lived particles that decay to Standard Model particles producing jets at the outer edge of the ATLAS electromagnetic calorimeter or inside the hadronic calorimeter. No significant excess of events is observed. Limits are reported on the product of the scalar boson production cross section times branching ratio into long-lived neutral particles as a function of the proper lifetime of the particles. Limits are reported for boson masses from 100 GeVto 900 GeV, and a long-lived neutral particle mass from 10 GeVto 150 GeV
Measurements of normalized differential cross sections for ttÌ production in pp collisions at â(s)=7ââTeV using the ATLAS detector
- Author
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- Abajyan T
- Abbott B
- Abdallah J
- Abdinov O
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- Wu SL
- Wu X
- Wu Y
- Wulf E
- Wyatt TR
- Wynne BM
- Xella S
- Xiao M
- Xu D
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- Yacoob S
- Yamada M
- Yamaguchi H
- Yamaguchi Y
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- Yao L
- Yao W-M
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- Yen AL
- Yildirim E
- Yildiz HD
- Yilmaz M
- Yoosoofmiya R
- Yorita K
- Yoshida R
- Yoshihara K
- Young C
- Young CJS
- Youssef S
- Yu DR
- Yu J
- Yu J
- Yu JM
- Yuan L
- Yurkewicz A
- Zabinski B
- Zaidan R
- Zaitsev AM
- Zaman A
- Zambito S
- Zanello L
- Zanzi D
- Zaytsev A
- Zeitnitz C
- Zeman M
- Zemla A
- Zengel K
- Zenin O
- Zenis T
- Zerwas D
- Zhang D
- Zhang F
- Zhang H
- Zhang J
- Zhang L
- Zhang X
- Zhang Z
- Zhao Z
- Zhemchugov A
- Zhong J
- Zhou B
- Zhou L
- Zhou N
- Zhu CG
- Zhu H
- Zhu J
- Zhu Y
- Zhuang X
- Zibell A
- Zieminska D
- Zimine NI
- Zimmermann C
- Zimmermann R
- Zimmermann S
- Zimmermann S
- Zinonos Z
- Ziolkowski M
- Zitoun R
- Zobernig G
- Zoccoli A
- Zurzolo G
- Zutshi V
- Zwalinski L
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2014
- Field of study
Measurements of normalized differential cross sections for top-quark pair production are presented as a function of the top-quark transverse momentum, and of the mass, transverse momentum, and rapidity of the tÂŻt system, in protonâproton collisions at a center-of-mass energy of âs=7ââTeV. The data set corresponds to an integrated luminosity of 4.6ââfbâ1, recorded in 2011 with the ATLAS detector at the CERN Large Hadron Collider. Events are selected in the lepton+jets channel, requiring exactly one lepton and at least four jets with at least one of the jets tagged as originating from a b-quark. The measured spectra are corrected for detector efficiency and resolution effects and are compared to several Monte Carlo simulations and theory calculations. The results are in fair agreement with the predictions in a wide kinematic range. Nevertheless, data distributions are softer than predicted for higher values of the mass of the tÂŻt system and of the top-quark transverse momentum. The measurements can also discriminate among different sets of parton distribution functions
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
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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 4.5ââfb[superscript â1] of proton-proton collisions data at âs=7ââTeV and 20.3ââfb[superscript â1] at âs=8ââTeV 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 ÎŒ=1.17±0.27 at the value of the Higgs boson mass measured by ATLAS, m[subscript H]=125.4ââGeV. 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 ÎŒ[subscript ggF]=1.32±0.38, ÎŒ[subscript VBF]=0.8±0.7, ÎŒ[subscript WH]=1.0±1.6, ÎŒ[subscript ZH]=0.1[superscript +3.7 subscript â0.1], and ÎŒ[subscript t [bar over t] H] =1.6[superscript +2.7 subscript â1.8], 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
Flavor tagged time-dependent angular analysis of the B0s â J/ÏÏ decay and extraction of ÎÎs and the weak phase Ïs in ATLAS
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- Aad G
- Abajyan T
- Abbott B
- Abdallah J
- Abdinov O
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- Yang Y
- Yanush S
- Yao L
- Yao W-M
- Yasu Y
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- Ye J
- Ye S
- Yen AL
- Yildirim E
- Yildiz HD
- Yilmaz M
- Yoosoofmiya R
- Yorita K
- Yoshida R
- Yoshihara K
- Young C
- Young CJS
- Youssef S
- Yu DR
- Yu J
- Yu J
- Yu JM
- Yuan L
- Yurkewicz A
- Zabinski B
- Zaidan R
- Zaitsev AM
- Zaman A
- Zambito S
- Zanello L
- Zanzi D
- Zaytsev A
- Zeitnitz C
- Zeman M
- Zemla A
- Zengel K
- Zenin O
- Zenis T
- Zerwas D
- Zhang D
- Zhang F
- Zhang H
- Zhang J
- Zhang L
- Zhang X
- Zhang Z
- Zhao Z
- Zhemchugov A
- Zhong J
- Zhou B
- Zhou L
- Zhou N
- Zhu CG
- Zhu H
- Zhu J
- Zhu Y
- Zhuang X
- Zibell A
- Zieminska D
- Zimine NI
- Zimmermann C
- Zimmermann R
- Zimmermann S
- Zimmermann S
- Zinonos Z
- Ziolkowski M
- Zitoun R
- 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 measurement of the B0sâJ/ÏÏ decay parameters, updated to include flavor tagging is reported using 4.9ââfbâÂč of integrated luminosity collected by the ATLAS detector from âs=7ââTeV pp collisions recorded in 2011 at the LHC. The values measured for the physical parameters are
Ïs=0.12±0.25(stat)±0.05(syst)âârad
ÎÎs=0.053±0.021(stat)±0.010(syst)ââpsâÂč
Îs=0.677±0.007(stat)±0.004(syst)ââpsâÂč
|Aâ„(0)|2=0.220±0.008(stat)±0.009(syst)
|A0(0)|2=0.529±0.006(stat)±0.012(syst)
ÎŽâ„=3.89±0.47(stat)±0.11(syst)âârad
where the parameter ÎÎs is constrained to be positive. The S-wave contribution was measured and found to be compatible with zero. Results for Ïs and ÎÎs are also presented as 68% and 95% likelihood contours, which show agreement with the Standard Model expectations
Search for high-mass dilepton resonances in pp collisions at sâ=8ââTeV 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
- Adamczyk L
- Adams DL
- Adelman J
- Adomeit S
- Adye T
- Agatonovic-Jovin T
- Aguilar-Saavedra JA
- Agustoni M
- Ahlen SP
- Ahmadov F
- Aielli G
- Akerstedt H
- Akesson TPA
- Akimoto G
- Akimov AV
- Alberghi GL
- Albert J
- Albrand S
- Alconada Verzini MJ
- Aleksa M
- Aleksandrov IN
- Alexa C
- Alexander G
- Alexandre G
- Alexopoulos T
- Alhroob M
- Alimonti G
- Alio L
- Alison J
- Allbrooke BMM
- Allen K
- Allison LJ
- Allport PP
- Almond J
- Aloisio A
- Alonso A
- Alonso F
- Alpigiani C
- Altheimer A
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- Terzo S
- Testa M
- Teuscher RJ
- Therhaag J
- Theveneaux-Pelzer T
- Thomas JP
- Thomas-Wilsker J
- Thompson AS
- Thompson EN
- Thompson PD
- Thompson PD
- Thomsen LA
- Thomson E
- Thomson M
- Thong WM
- Thun RP
- Tian F
- Tibbetts MJ
- Tikhomirov VO
- Tikhonov YA
- Timoshenko S
- Tiouchichine E
- Tipton P
- Tisserant S
- Todorov T
- Todorova-Nova S
- Toggerson B
- Tojo J
- Tokar S
- Tokushuku K
- Tollefson K
- Tomlinson L
- Tomoto M
- Tompkins L
- Toms K
- Topilin ND
- Toro RC
- Torregrosa EF
- Torrence E
- Torres H
- Torro Pastor E
- Toth J
- Touchard F
- Tovey DR
- Tran HL
- Trefzger T
- Tremblet L
- Tricoli A
- Trigger IM
- Trincaz-Duvoid S
- Tripiana MF
- Triplett N
- Trischuk W
- Trocme B
- Troncon C
- Trottier-McDonald M
- Trovatelli M
- True P
- Trzebinski M
- Trzupek A
- Tsarouchas C
- Tseng JC-L
- Tsiareshka PV
- Tsionou D
- Tsipolitis G
- Tsirintanis N
- Tsiskaridze S
- Tsiskaridze V
- Tskhadadze EG
- Tsukerman II
- Tsulaia V
- Tsuno S
- Tsybychev D
- Tudorache A
- Tudorache V
- Tuna AN
- Tupputi SA
- Turchikhin S
- Turecek D
- Turra R
- Tuts PM
- Tykhonov A
- Tylmad M
- Tyndel M
- Uchida K
- Ueda I
- Ueno R
- Ughetto M
- Ugland M
- Uhlenbrock M
- Ukegawa F
- Unal G
- Undrus A
- Unel G
- Ungaro FC
- Unno Y
- Urbaniec D
- Urquijo P
- Usai G
- Usanova A
- Vacavant L
- Vacek V
- Vachon B
- Valencic N
- Valentinetti S
- Valero A
- Valery L
- Valkar S
- Valladolid Gallego E
- Vallecorsa S
- Valls Ferrer JA
- Van Der Deijl PC
- Van der Geer R
- Van der Graaf H
- Van der Leeuw R
- Van der Ster D
- van Eldik N
- van Gemmeren P
- van Huysduynen LH
- Van Nieuwkoop J
- van Vulpen I
- van Woerden MC
- Vanadia M
- Vandelli W
- Vanguri R
- Vaniachine A
- Vankov P
- Vannucci F
- Vaque FV
- Vardanyan G
- Vari R
- Varnes EW
- Varol T
- Varouchas D
- Vartapetian A
- Varvell KE
- Vazeille F
- Vazquez JGP
- Veatch J
- Veloso F
- Veneziano S
- Ventura A
- Ventura D
- Venturi M
- Venturi N
- Venturini A
- Vercesi V
- Verducci M
- Verkerke W
- Vermeulen JC
- Vest A
- Vetterli MC
- Viazlo O
- Vichou I
- Vickey T
- Viehhauser GHA
- Viel S
- Vigne R
- Villa M
- Vilucchi E
- Vincter MG
- Vinogradov VB
- Virzi J
- Vivarelli I
- Vlachos S
- Vladoiu D
- Vlasak M
- Vogel A
- Vogel M
- Vokac P
- Volpi G
- Volpi M
- von der Schmitt H
- von Radziewski H
- von Toerne E
- Vorobel V
- Vorobev K
- Vos M
- Voss R
- Vossebeld JH
- Vranjes N
- Vrba V
- Vreeswijk M
- Vuillermet R
- Vukotic I
- Vykydal Z
- Wagner P
- Wagner W
- Wahlberg H
- Wahrmund S
- Wakabayashi J
- Walder J
- Walker R
- Walkowiak W
- Wall R
- Waller P
- Walls FMG
- Walsh B
- Wang C
- Wang C
- Wang F
- Wang H
- Wang H
- Wang J
- Wang J
- Wang K
- Wang R
- Wang SM
- Wang T
- Wang X
- Wanotayaroj C
- Warburton A
- Ward CP
- Wardrope DR
- Warsinsky M
- Washbrook A
- Wasicki C
- Watanabe I
- Watkins PM
- Watson AT
- Watson IJ
- Watson MF
- Watts G
- Watts S
- Waugh BM
- Webb S
- Weber MS
- Weber SW
- Webster JS
- Weidberg AR
- Weigell P
- Weinert B
- Weingarten J
- Weiser C
- Weits H
- Wells PS
- Wemans ADV
- Wenaus T
- Wendland D
- Weng Z
- Wengler T
- Wenig S
- Wermes N
- Werner M
- Werner P
- Wessels M
- Wetter J
- Whalen K
- White A
- White MJ
- White R
- White S
- Whiteson D
- Wicke D
- Wickens FJ
- Wiedenmann W
- Wielers M
- Wienemann P
- Wiglesworth C
- Wiik-Fuchs LAM
- Wijeratne PA
- Wildauer A
- Wildt MA
- Wilkens HG
- Will JZ
- Williams HH
- Williams S
- Willis C
- Willocq S
- Wilson A
- Wilson JA
- Wingerter-Seez I
- Winklmeier F
- Winter BT
- Wittgen M
- Wittig T
- Wittkowski J
- Wollstadt SJ
- Wolter MW
- Wolters H
- Wong KHY
- Wosiek BK
- Wotschack J
- Woudstra MJ
- Wozniak KW
- Wright M
- Wu M
- Wu SL
- Wu X
- Wu Y
- Wulf E
- Wyatt TR
- Wynne BM
- Xella S
- Xiao M
- Xu D
- Xu L
- Yabsley B
- Yacoob S
- Yamada M
- Yamaguchi H
- Yamaguchi Y
- Yamamoto A
- Yamamoto K
- Yamamoto S
- Yamamura T
- Yamanaka T
- Yamauchi K
- Yamazaki Y
- Yan Z
- Yang H
- Yang H
- Yang UK
- Yang Y
- Yanush S
- Yao L
- Yao W-M
- Yasu Y
- Yatsenko E
- Ye J
- Ye S
- Yeletskikh I
- Yen AL
- Yildirim E
- Yildiz HD
- Yilmaz M
- Yoosoofmiya R
- Yorita K
- Yoshida R
- Yoshihara K
- Young C
- Young CJS
- Youssef S
- Yu DR
- Yu J
- Yu J
- Yu JM
- Yuan L
- Yurkewicz A
- Zabinski B
- Zaidan R
- Zaitsev AM
- Zaman A
- Zambito S
- Zanello L
- Zanzi D
- Zeitnitz C
- Zeman M
- Zemla A
- Zengel K
- Zenin O
- Zenis T
- Zerwas D
- Zhang D
- Zhang F
- Zhang H
- Zhang J
- Zhang L
- Zhang X
- Zhang Z
- Zhao Z
- Zhemchugov A
- Zhong J
- Zhou B
- Zhou L
- Zhou N
- Zhu CG
- Zhu H
- Zhu J
- Zhu Y
- Zhuang X
- Zibell A
- Zieminska D
- Zimine NI
- Zimmermann C
- Zimmermann R
- Zimmermann S
- Zimmermann S
- Zinonos Z
- Zinser M
- Ziolkowski M
- 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
The ATLAS detector at the Large Hadron Collider is used to search for high-mass resonances decaying to dielectron or dimuon final states. Results are presented from an analysis of proton-proton (pp) collisions at a center-of-mass energy of 8 TeV corresponding to an integrated luminosity of 20.3ââfbâ1 in the dimuon channel. A narrow resonance with Standard Model Z couplings to fermions is excluded at 95% confidence level for masses less than 2.79 TeV in the dielectron channel, 2.53 TeV in the dimuon channel, and 2.90 TeV in the two channels combined. Limits on other model interpretations are also presented, including a grand-unification model based on the E6 gauge group, Zâ bosons, minimal Z' models, a spin-2 graviton excitation from Randall-Sundrum models, quantum black holes, and a minimal walking technicolor model with a composite Higgs boson
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