203 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
- Almenar CC
- Almond J
- Aloisio A
- Alon R
- 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
- Annovi A
- 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
- Astvatsatourov A
- Atoian G
- Aubert B
- Auge E
- Augsten K
- Aurousseau M
- Austin N
- Avolio G
- Avramidou R
- Axen D
- Ay C
- Azuelos G
- Azuma Y
- Baak MA
- Baccaglioni G
- Bacci C
- Bach AM
- Bachacou H
- Bachas K
- Bachy G
- Backes M
- Backhaus M
- Badescu E
- Bagnaia P
- Bahinipati S
- Bai Y
- Bailey DC
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- Baker MD
- Baker OK
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- Bangert A
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- Boorman G
- Booth CN
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- Borjanovic I
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- Boscherini D
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- Botterill D
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- Boudreau J
- Bouhova-Thacker EV
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- Brandenburg GW
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- Brodet E
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- Brooijmans G
- Brooks WK
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- Buckingham RM
- Buckley AG
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- Budagov IA
- Budick B
- Bueso XP
- Bugge L
- Buira-Clark D
- Bulekov O
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- Butterworth JM
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- Castanheira MTD
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- Castro NF
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- Chapleau B
- Chapman JD
- Chapman JW
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- Charlton DG
- Chavda V
- Cheatham S
- Chekanov S
- Chekulaev SV
- Chelkov GA
- Chelstowska MA
- Chen C
- Chen H
- Chen S
- Chen T
- Chen X
- Cheng S
- Cheong ALF
- Cheplakov A
- Chepurnov VF
- Chernyatin V
- Cheu E
- Cheung SL
- Chevalier L
- Chiefari G
- Chikovani L
- Childers JT
- Chilingarov A
- Chiodini G
- Chizhov MV
- Choudalakis G
- Chouridou S
- Christidi IA
- Christov A
- Chromek-Burckhart D
- Chu ML
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- Cioccaa C
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- Collaboration ATLAS
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- Da Costa JBG
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- Damazio DO
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- De Graat J
- De Groot N
- De Jong P
- De la Hoz SG
- De la Taille C
- De la Torre H
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- De Nooij L
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- Debbe R
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- Degenhardt J
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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
Observation of associated near-side and away-side long-range correlations in √sNN=5.02 TeV proton-lead collisions with the ATLAS detector
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- Schoening A
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- Schäfer U
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- Sedov G
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- Sekhniaidze G
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- Shamim M
- Shan LY
- Shank JT
- Shao QT
- Shapiro M
- Shatalov PB
- Shaw K
- Sherwood P
- Shimizu S
- Shimojima M
- Shin T
- Shiyakova M
- Shmeleva A
- Shochet MJ
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- Shrestha S
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- Sicho P
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- Sipica V
- Siragusa G
- Sircar A
- Sisakyan AN
- Sivoklokov SY
- Sjursen TB
- Sjölin J
- Skinnari LA
- Skottowe HP
- Skovpen K
- Skubic P
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- Slavicek T
- Sliwa K
- Smakhtin V
- Smart BH
- Smestad L
- Smirnov SY
- Smirnov Y
- Smirnova LN
- Smirnova O
- Smith BC
- Smith KM
- Smizanska M
- Smolek K
- Snesarev AA
- Snidero G
- Snow J
- Snow SW
- Snyder S
- Sobie R
- Sodomka J
- Soffer A
- Soh DA
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- Soldatov EY
- Soldevila U
- Solfaroli Camillocci E
- Solodkov AA
- Solovyanov OV
- Solovyev V
- Soni N
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- Spanò F
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- Spigo G
- Spiwoks R
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- Stanitzki MM
- Stapnes S
- Starchenko EA
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- Staroba P
- Starovoitov P
- Staszewski R
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- Steinberg P
- Stekl I
- Stelzer B
- Stelzer HJ
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- Stradling AR
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- Strandberg S
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- Ströhmer R
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- Sturm P
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- Subramaniam R
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- Sundermann JE
- Suruliz K
- Susinno G
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- Suzuki Y
- Suzuki Y
- Svatos M
- Swedish S
- Swiatlowski M
- Sykora I
- Sykora T
- Sánchez J
- Ta D
- Tackmann K
- Taffard A
- Tafirout R
- Taiblum N
- Takahashi Y
- Takai H
- Takashima R
- Takeda H
- Takeshita T
- Takubo Y
- Talby M
- Talyshev A
- Tam JY
- Tamsett MC
- Tan KG
- Tanaka J
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- Tanasijczuk AJ
- Tani K
- Tannoury N
- Tapprogge S
- Tardif D
- Tarem S
- Tarrade F
- Tartarelli GF
- Tas P
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- Tayalati Y
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- Teixeira-Dias P
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- Testa M
- Teuscher RJ
- Therhaag J
- Theveneaux-Pelzer T
- Thoma S
- Thomas JP
- Thompson AS
- Thompson EN
- Thompson PD
- Thompson PD
- Thomsen LA
- Thomson E
- Thomson M
- Thong WM
- Thun RP
- Tian F
- Tibbetts MJ
- Tic T
- Tikhomirov VO
- Tikhonov YA
- Timoshenko S
- Tiouchichine E
- Tipton P
- Tisserant S
- Todorov T
- Todorova-Nova S
- Toggerson B
- Tojo J
- Tokushuku K
- Tokár S
- Tollefson K
- Tomlinson L
- Tomoto M
- Tompkins L
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- Tonoyan A
- Topfel C
- Topilin ND
- Torrence E
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- Trzebinski M
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- Tsarouchas C
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- Tsiareshka PV
- Tsionou D
- Tsipolitis G
- Tsiskaridze S
- Tsiskaridze V
- Tskhadadze EG
- Tsukerman II
- Tsulaia V
- Tsung JW
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- Tsybychev D
- Tua A
- Tudorache A
- Tudorache V
- Tuggle JM
- Turala M
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- Turk Cakir I
- Turra R
- Tuts PM
- Tykhonov A
- Tylmad M
- Tyndel M
- Tzanakos G
- 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
- Vacavant L
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- Vachon B
- Vahsen S
- Valencic N
- Valentinetti S
- Valero A
- Valery L
- Valkar S
- Valladolid Gallego E
- Vallecorsa S
- Valls Ferrer JA
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- van der Geer R
- van der Graaf H
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- van der Poel E
- van der Ster D
- van Eldik N
- van Gemmeren P
- Van Nieuwkoop J
- van Vulpen I
- Vanadia M
- Vandelli W
- Vaniachine A
- Vankov P
- Vannucci F
- Vari R
- Varnes EW
- Varol T
- Varouchas D
- Vartapetian A
- Varvell KE
- Vassilakopoulos VI
- Vazeille F
- Vazquez Schroeder T
- Veloso F
- Veneziano S
- Ventura A
- Ventura D
- Venturi M
- Venturi N
- Vercesi V
- Verducci M
- Verkerke W
- Vermeulen JC
- Vest A
- Vetterli MC
- Vichou I
- Vickey Boeriu OE
- Vickey T
- Viehhauser GH
- Viel S
- Villa M
- Villaplana Perez M
- Vilucchi E
- Vincter MG
- Vinek E
- Vinogradov VB
- Virzi J
- Vitells O
- Viti M
- Vivarelli I
- Vives Vaque F
- Vlachos S
- Vladoiu D
- Vlasak M
- Vogel A
- Vokac P
- Volpi G
- Volpi M
- Volpini G
- von der Schmitt H
- von Radziewski H
- von Toerne E
- Vorobel V
- Vorwerk V
- Vos M
- Voss R
- Vossebeld JH
- Vranjes Milosavljevic M
- Vranjes N
- Vrba V
- Vreeswijk M
- Vu Anh T
- Vuillermet R
- Vukotic I
- Vykydal Z
- Wagner P
- Wagner W
- Wahlen H
- Wahrmund S
- Wakabayashi J
- Walch S
- Walder J
- Walker R
- Walkowiak W
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- Warburton A
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- Wardrope DR
- Warsinsky M
- Washbrook A
- Wasicki C
- Watanabe I
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- Waugh AT
- Waugh BM
- Weber MS
- Webster JS
- Weidberg AR
- Weigell P
- Weingarten J
- Weiser C
- Wells PS
- Wenaus T
- Wendland D
- Weng Z
- Wengler T
- Wenig S
- Wermes N
- Werner M
- Werner P
- Werth M
- Wessels M
- Wetter J
- Weydert C
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- Wiedenmann W
- Wielers M
- Wienemann P
- Wiglesworth C
- Wiik-Fuchs LA
- Wijeratne PA
- Wildauer A
- Wildt MA
- Wilhelm I
- Wilkens HG
- Will JZ
- Williams E
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- Willis W
- Willocq S
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- Wilson JA
- Wilson MG
- Wingerter-Seez I
- Winkelmann S
- Winklmeier F
- Wittgen M
- Wittig T
- Wittkowski J
- Wollstadt SJ
- Wolter MW
- Wolters H
- Wong WC
- Wooden G
- Wosiek BK
- Wotschack J
- Woudstra MJ
- Wozniak KW
- Wraight K
- Wright M
- Wrona B
- Wu SL
- Wu X
- Wu Y
- Wulf E
- Wynne BM
- Xella S
- Xiao M
- Xie S
- Xu C
- Xu D
- Xu L
- Yabsley B
- Yacoob S
- Yamada M
- Yamaguchi H
- Yamamoto A
- Yamamoto K
- Yamamoto S
- Yamamura T
- Yamanaka T
- Yamauchi K
- Yamazaki T
- Yamazaki Y
- Yan Z
- Yang H
- Yang H
- Yang UK
- Yang Y
- Yang Z
- Yanush S
- Yao L
- Yasu Y
- Yatsenko E
- Ye J
- Ye S
- Yen AL
- Yilmaz M
- Yoosoofmiya R
- Yorita K
- Yoshida R
- Yoshihara K
- Young C
- 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
- Zeniš 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
- Zivković 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 (Δϕ) and pseudorapidity (Δη) are measured in √sNN=5.02 TeV p+Pb collisions using the ATLAS detector at the LHC. The measurements are performed using approximately 1 μb-1 of data as a function of transverse momentum (pT) and the transverse energy (ΣETPb) 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<|Δη|<5) “near-side” (Δϕ∼0) correlation that grows rapidly with increasing ΣETPb. A long-range “away-side” (Δϕ∼π) correlation, obtained by subtracting the expected contributions from recoiling dijets and other sources estimated using events with small ΣETPb, is found to match the near-side correlation in magnitude, shape (in Δη and Δϕ) and ΣETPb dependence. The resultant Δϕ correlation is approximately symmetric about π/2, and is consistent with a dominant cos2Δϕ modulation for all ΣETPb ranges and particle pT
Search for R-parity-violating supersymmetry in events with four or more leptons in sqrt(s) =7 TeV pp collisions with the ATLAS detector
- Author
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- Abajyan T
- Abbott B
- Abdallah J
- Khalek SA
- Abdelalim AA
- Abdinov O
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- Yilmaz M
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- della Porta GZ
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- Zhemchugov A
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- Zibell A
- Zieminska D
- Zimin NI
- Zimmermann R
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- Zimmermann S
- Ziolkowski M
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- Zivkovic L
- Zmouchko VV
- Zobernig G
- Zoccoli A
- zur Nedden M
- Zutshi V
- Zwalinski L
- Collaboration ATLAS
- Publication venue
- Springer Verlag
- Publication date
- 01/01/2008
- Field of study
A search for new phenomena in final states with four or more leptons (electrons or muons) is presented. The analysis is based on 4.7 fb−1 of s=7TeV proton-proton collisions delivered by the Large Hadron Collider and recorded with the ATLAS detector. Observations are consistent with Standard Model expectations in two signal regions: one that requires moderate values of missing transverse momentum and another that requires large effective mass. The results are interpreted in a simplified model of R-parity-violating supersymmetry in which a 95% CL exclusion region is set for charged wino masses up to 540 GeV. In an R-parity-violating MSUGRA/CMSSM model, values of m 1/2 up to 820 GeV are excluded for 10 < tan β < 40
Search for high-mass resonances decaying to dilepton final states in pp collisions at s√=7 TeV with the ATLAS detector
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- Yanush S
- Yao L
- Yao Y
- Yasu Y
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- Yildiz HD
- Yilmaz M
- Yoosoofmiya R
- Yorita K
- Yoshida R
- Yoshihara K
- Young C
- Young CJ
- Youssef S
- Yu D
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- Yu J
- Yu J
- Yuan L
- Yurkewicz A
- Zabinski B
- Zaidan R
- Zaitsev AM
- Zajacova Z
- Zanello L
- Zanzi D
- Zaytsev A
- Zeitnitz C
- Zeman M
- Zemla A
- Zendler C
- Zenin O
- Zenis T
- Zerwas D
- Zhang D
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- Zhang Z
- Zhao L
- Zhao Z
- Zhemchugov A
- Zhong J
- Zhou B
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- 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
- 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 Z′ gauge bosons, Randall-Sundrum gravitons, Z * bosons, techni-mesons, Kaluza-Klein Z/γ 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 fb−1 in the e + e − channel and 5.0 fb−1 in the μ + μ −channel. A Z ′ 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 Z′ 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
- Aad G
- Abajyan T
- Abbott B
- Abdallah J
- Abdelalim AA
- Abdinov O
- Abi B
- Abolins M
- AbouZeid OS
- Abramowicz H
- Abreu H
- Acharya BS
- Adam ER
- Adamczyk L
- Adams DL
- Addy TN
- Adelman J
- Adomeit S
- Adragna P
- Adye T
- Aesky S
- Agar-Savedra JA
- Agustoni M
- Ahlen SP
- Ahles F
- Ahmad A
- Ahsan M
- Aielli G
- Akesson TPA
- Akimoto G
- Akimov AV
- Alam MA
- 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
- Allbrooke BMM
- Allison LJ
- Allport PP
- Allwood-Spiers SE
- Almenar CC
- Almond J
- Aloisio A
- Alon R
- Alonso A
- Alonso F
- Altheimer A
- Alviggi MG
- Amako K
- Amelung C
- Ammosov VV
- Amor Dos Santos SP
- Amorim A
- Amoroso S
- 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
- Angelidakis S
- Anger P
- Angerami A
- Anghinolfi F
- Anh TV
- Anisenkov A
- Anjos N
- Annovi A
- Antonaki A
- Antonelli M
- Antonov A
- Antos J
- Anulli F
- Aoki M
- Aoun S
- Apolle R
- Arabidze G
- Aracena I
- Arai Y
- Aranda CP
- Arce ATH
- Arfaoui S
- Arguin J-F
- Argyropoulos S
- Arik E
- Arik M
- Armbruster AJ
- Arnaez O
- Arnal V
- Artamonov A
- Artoni G
- Arutinov D
- Asai S
- Ask S
- Asman B
- Asquith L
- Assamagan K
- Astbury A
- Atkinson M
- Aubert B
- Auge E
- Augsten K
- Aurousseau M
- Avolio G
- Axen A
- Azuelos G
- Azuma Y
- Baak MA
- Baccaglioni G
- Bacci C
- Bach AM
- Bachacou H
- Bachas K
- Backes M
- Backhaus M
- Badescu E
- Bagnaia P
- Bai Y
- Bailey DC
- Bain T
- Baines JT
- Baker OK
- Baker S
- Balek P
- Banas E
- Banerjee P
- Banerjee S
- Banfi D
- Bangert A
- Bansal V
- Bansil HS
- Barak L
- Baranov SP
- Barber T
- Barberio EL
- Barberis D
- Barbero N
- Bardin DY
- Barillari T
- Barisonzi M
- Barklow T
- Barlow N
- Barnett BM
- Barnett RM
- Barojas CAC
- Baroncelli A
- Barone G
- Barr AJ
- Barreiro F
- Barrera CO
- Bartoldus R
- Barton AE
- Bartsch V
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- Uchida K
- Ueda I
- Ueno R
- Ughetto N
- Ugland M
- Uhlenbrock M
- Ukegawa F
- Unal G
- Undrus A
- Unel G
- Unno Y
- Urbaniec D
- Urquijo P
- Usai G
- Vacavant L
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- Van der Deij PC
- van der Geer R
- van der Graaf H
- Van der Leeuw R
- van der Poel E
- van der Ster D
- van Eldik N
- van Gemmeren P
- van Huysduynen LH
- Van Nieuwkoop J
- Van Vulpen I
- Vanadia M
- Vandelli W
- Vaniachine A
- Vankov P
- Vannucci F
- Vaque FV
- Vari R
- Varnes EW
- Varol T
- Varouchas D
- Vartapetian A
- Varvell KE
- Vassilakopoulos VI
- Vazeille F
- Vazquez JGP
- Vegni G
- Veillet JJ
- Veloso F
- Veness R
- Veneziano S
- Ventura A
- Ventura D
- Venturi M
- Venturi N
- Vercesi V
- Verducci M
- Verkerke W
- Vermeulen JC
- Vest A
- Vetterli MC
- Vickey T
- Viehhauser GHA
- Viehou I
- Viel S
- Villa M
- Vilucchi E
- Vincter MG
- Vinek E
- Vinogradov VB
- Virchaux M
- Virzi J
- Vitells O
- Viti M
- Vivarelli I
- Vlachos S
- Vladoiu D
- Vlasak M
- Vogel A
- Vokac P
- Volpi G
- Volpi M
- Volpini G
- von der Schmitt H
- von Radziewski H
- von Toerne E
- Vorobel V
- Vorwerk V
- Vos M
- Voss R
- Vossebeld JH
- Vranjes N
- Vrba V
- Vreeswijk M
- Vuillermet R
- Vukotic I
- Wagner P
- Wagner W
- Wahlen H
- Wahrmund S
- Wakabayashi J
- Walch S
- Walder J
- Walker R
- Walkowiak W
- Wall R
- Waller P
- Walsh B
- Wang C
- Wang H
- Wang H
- Wang J
- Wang J
- Wang R
- Wang SM
- Wang T
- 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 AT
- Waugh BM
- Weber MS
- Webster JS
- Weidberg AR
- Weigell P
- Weingarten J
- Weiser C
- Wells PS
- Wenaus T
- Wendland D
- Weng Z
- Wengler T
- Wenig S
- Wermes N
- Werner M
- Werner P
- Werth M
- Wessels M
- Wetter J
- Weydert C
- Whalen K
- White A
- White MJ
- White S
- Whitehead SR
- Whiteson D
- Whittington D
- Wicke D
- Wickens FJ
- Wiedenmann W
- Wielers M
- Wienemann P
- Wiglesworth C
- Wiik-Fuchs LAM
- Wijeratne PA
- Wildauer A
- Wildt MA
- Wilhelm I
- Wilkens HG
- Will JZ
- Williams E
- Williams HH
- Williams S
- Willis W
- Willocq S
- Wilson A
- Wilson JA
- Wilson MG
- Wingerter-Seez I
- Winkelmann S
- Winklmeier F
- Wittgen M
- Wollstadt SJ
- Wolter MW
- Wolters H
- Wong WC
- Wooden G
- Wosiek BK
- Wotschack J
- Woudstra MJ
- Wozniak KW
- Wraight K
- Wright M
- Wrona B
- Wu SL
- Wu X
- Wu Y
- Wulf E
- Wynne BM
- Xella S
- Xiao M
- Xie S
- Xu C
- Xu D
- Xu L
- Yabsley B
- Yacoob S
- Yagci KD
- Yamada N
- Yamaguchi H
- Yamamoto A
- Yamamoto K
- Yamamoto S
- Yamamura T
- Yamanaka T
- Yamauchi K
- Yamazaki T
- Yamazaki Y
- Yan Z
- Yang H
- Yang H
- Yang UK
- Yang Y
- Yang Z
- Yanush S
- Yao L
- Yasu Y
- Yatsenko E
- Ye J
- Ye S
- Yen AL
- Yilmaz M
- Yoosoofmiya R
- Yorita K
- Yoshida R
- Yoshihara K
- Young C
- Young CJ
- Youssef S
- Yu D
- Yu DR
- Yu J
- Yu J
- Yuan L
- Yurkewicz A
- Zabinski B
- Zaidan R
- Zaitsev AM
- Zanello L
- Zanzi D
- Zaytsev A
- Zeitnitz C
- Zeman M
- Zemla A
- Zenin O
- Zenis T
- Zerwas D
- Zhang D
- Zhang H
- Zhang J
- 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
- Zivkovic L
- Zmouchko VV
- Zobernig G
- Zoccoli A
- zur Nedden M
- Zutshi V
- Zwalinski L
- 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
Polyploidization as a Retraction Force in Plant Genome Evolution: Sequence Rearrangements in Triticale
- Author
- A Baumel
- A Baumel
- A Belyayev
- A Kumar
- A Madlung
- A Merker
- A Suoniemi
- B Liu
- C Vitte
- D Sandhu
- DR Corbin
- EV Boyko
- H Ozkan
- H Ozkan
- H Shaked
- H. Sofia Pereira
- HE Varmus
- HS Pereira
- IJ Leitch
- James Fraser
- JC Peng
- JP Gustafson
- K Kashkush
- K Kashkush
- KL Adams
- KL Wycoff
- KM Devos
- KM Song
- M Berenyi
- M Feldman
- M Rocheta
- MA Saghai-Maroof
- Manuela Silva
- Margarida Rocheta
- MD Bennett
- MD Bennett
- Miguel Bento
- N Neves
- N Saitou
- O Pontes
- O Pontes
- P Smykal
- Perry Gustafson
- PS Perlman
- R Kalendar
- T Schwarzacher
- W Viegas
- Wanda Viegas
- WL Gerlach
- XF Ma
- XF Ma
- XF Ma
- ZJ Chen
- Publication venue
- Public Library of Science
- Publication date
- 01/01/2008
- Field of study
BACKGROUND: Polyploidization is a major evolutionary process in plants where hybridization and chromosome doubling induce enormous genomic stress and can generate genetic and epigenetic modifications. However, proper evaluation of DNA sequence restructuring events and the precise characterization of sequences involved are still sparse. METHODOLOGY/PRINCIPAL FINDINGS: Inter Retrotransposons Amplified Polymorphism (IRAP), Retrotransposons Microsatellite Amplified Polymorphism (REMAP) and Inter Simple Sequence Repeat (ISSR) largely confirmed the absence of any intraspecific variation in wheat, rye and triticale. The comparative analysis of banding profiles between wheat and rye inbred lines revealed 34% of monomorphic (common to both parental species) bands for the ten different primer combinations used. The analysis of triticale plants uncovered nearly 51% of rearranged bands in the polyploid, being the majority of these modifications, due to the loss of rye bands (83%). Sequence analysis of rye fragments absent in triticale revealed for instance homology with hydroxyproline-rich glycoproteins (HRGP), a protein that belongs to a major family of inducible defence response proteins. Conversely, a wheat-specific band absent in triticale comprises a nested structure of copia-like retrotransposons elements, namely Claudia and Barbara. Sequencing of a polyploid-specific band (absent in both parents) revealed a microsatellite related sequence. Cytological studies using Fluorescent In Situ Hybridization (FISH) with REMAP products revealed a widespread distribution of retrotransposon and/or microsatellite flanking sequences on rye chromosomes, with a preferential accumulation in heterochromatic sub-telomeric domains. CONCLUSIONS/SIGNIFICANCE: Here, we used PCR-based molecular marker techniques involving retrotransposons and microsatellites to uncover polyploidization induced genetic restructuring in triticale. Sequence analysis of rearranged genomic fragments either from rye or wheat origin showed these to be retrotransposon-related as well as coding sequences. Further FISH analysis revealed possible chromosome hotspots for sequence rearrangements. The role of chromatin condensation on the origin of genomic rearrangements mediated by polyploidization in triticale is also discussed
Post-meiotic transcription in mouse testes detected with spermatid cDNA clones
- Author
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/12/1984
- Field of study
cDNA clones to poly(A) + mRNA from spermatids have been obtained to study gene transcription in post-meiotic germ cells. Four cDNA clones detect mRNAs that increase in abundance in post-meiotic germ cells. One clone, pPM459, was shown to correspond to an mRNA that is transcribed after meiosis. Pulse-labelling experiments demonstrate transcription o5 the message in spermatids. These data constitute further evidence for post-meiotic gene transcription in spermatids.Peer Reviewedhttp://deepblue.lib.umich.edu/bitstream/2027.42/44190/1/10540_2005_Article_BF01116696.pd
Taxonomy based on science is necessary for global conservation
- Author
- Ahyong ST
- Alonso-Zarazaga M
- Ammirati J
- Araya JF
- Ascher JS
- Audisio TL
- Azevedo-Santos VM
- Bailly N
- Baker WJ
- Balke M
- Barclay MVL
- Barrett RL
- Benine RC
- Bickerstaff JRM
- Bouchard P
- Bour R
- Bourgoin T
- Boyko CB
- Breure ASH
- Brothers DJ
- Byng JW
- Campbell D
- Cernák I
- Cerretti P
- Ceríaco LMP
- Chang CH
- Cho S
- Copus JM
- Costello MJ
- Cseh A
- Csuzdi C
- Culham A
- Daneliya ME
- Dekker R
- Dickinson EC
- Dickinson TA
- Dijkstra KDB
- Dima B
- Dmitriev DA
- Duistermaat L
- Dumbacher JP
- D’Elía G
- d’Udekem d’Acoz C
- Eiserhardt WL
- Ekrem T
- Evenhuis NL
- Faille A
- Fernández-Triana JL
- Fiesler E
- Fishbein M
- Fordham BG
- Freitas AVL
- Friol NR
- Fritz U
- Frøslev T
- Funk VA
- Gaimari SD
- Garbino GST
- Garraffoni ARS
- Geml J
- Gill AC
- Gray A
- Grazziotin FG
- Greenslade P
- Gutiérrez EE
- Harvey MS
- Hazevoet CJ
- He K
- He X
- Helfer S
- Helgen KM
- Hita Garcia F
- Holstein N
- Horváth MK
- Hovenkamp PH
- Hwang WS
- Hyvönen J
- Islam MB
- Iverson JB
- Ivie MA
- Jaafar Z
- Jackson MD
- Jayat JP
- Johnson NF
- Kaiser H
- Klitgård BB
- Knapp DG
- Kojima JI
- Kontschán J
- Krell FT
- Krisai-Greilhuber I
- Kullander S
- Kõljalg U
- Latella L
- Lattke JE
- Lencioni V
- Pyle RL
- Thomson SA
- van Dijk PP
- van Heteren AH
- Publication venue
- Public Library of Science (PLoS)
- Publication date
- 14/03/2018
- Field of study
First observation of the decays χcJ→π0π0π0π0
- Author
- Ablikim M
- Achasov MN
- An L
- An Q
- An ZH
- Bai JZ
- Baldini R
- Ban Y
- Becker J
- Berger N
- Bertani M
- Bian JM
- Boyko I
- Briere RA
- Bytev V
- Cai X
- Cao GF
- Cao XX
- Chang JF
- Chelkov G
- Chen G
- Chen HS
- Chen JC
- Chen ML
- Chen SJ
- Chen Y
- Chen YB
- Cheng HP
- Chu YP
- CroninHennessy D
- Dai HL
- Dai JP
- Dedovich D
- Deng ZY
- Denysenko I
- Destefanis M
- Ding Y
- Dong LY
- Dong MY
- Du SX
- Duan MY
- Fan RR
- Fang J
- Fang SS
- Feldbauer F
- Feng CQ
- Fu CD
- Fu JL
- Gao Y
- Geng C
- Goetzen K
- Gong WX
- Greco M
- Grishin S
- Gu MH
- Gu YT
- Guan YH
- Guo AQ
- Guo LB
- Guo YP
- Hao XQ
- Harris FA
- He KL
- He M
- He ZY
- Heng YK
- Hou ZL
- Hu HM
- Hu JF
- Hu T
- Huang B
- Huang GM
- Huang JS
- Huang XT
- Huang YP
- Hussain T
- Ji CS
- Ji Q
- Ji XB
- Ji XL
- Jia LK
- Jiang LL
- Jiang XS
- Jiao JB
- Jiao Z
- Jin DP
- Jin S
- Jing FF
- Kavatsyuk M
- Komamiya S
- Kuehn W
- Lange JS
- Leung JKC
- Li C
- Li C
- Li DM
- Li F
- Li G
- Li HB
- Li JC
- Li L
- Li NB
- Li QJ
- Li WD
- Li WG
- Li XL
- Li XN
- Li XQ
- Li XR
- Li ZB
- Liang H
- Liang YF
- Liang YT
- Liao GR
- Liao XT
- Liu BJ
- Liu BJ
- Liu CL
- Liu CX
- Liu CY
- Liu F
- Liu F
- Liu FH
- Liu GC
- Liu H
- Liu HB
- Liu HM
- Liu HW
- Liu JP
- Liu K
- Liu KY
- Liu Q
- Liu SB
- Liu X
- Liu XH
- Liu Y
- Liu YB
- Liu YW
- Liu ZA
- Liu ZQ
- Loehner H
- Lu GR
- Lu HJ
- Lu JG
- Lu QW
- Lu XR
- Lu YP
- Luo CL
- Luo MX
- Luo T
- Luo XL
- Ma CL
- Ma FC
- Ma HL
- Ma QM
- Ma T
- Ma X
- Ma XY
- Maggiora M
- Malik QA
- Mao H
- Mao YJ
- Mao ZP
- Messchendorp JG
- Min J
- Mitchell RE
- Mo XH
- Motzko C
- Muchnoi NY
- Nefedov Y
- Ning Z
- Olsen SL
- Ouyang Q
- Pacetti S
- Pelizaeus M
- Peters K
- Ping JL
- Ping RG
- Poling R
- Pun CSJ
- Qi M
- Qian S
- Qiao CF
- Qin XS
- Qiu JF
- Rashid KH
- Rong G
- Ruan XD
- Sarantsev A
- Schulze J
- Shao M
- Shen CP
- Shen XY
- Sheng HY
- Shepherd MR
- Song XY
- Sonoda S
- Spataro S
- Spruck B
- Sun DH
- Sun GX
- Sun JF
- Sun SS
- Sun XD
- Sun YJ
- Sun YZ
- Sun ZJ
- Sun ZT
- Tang CJ
- Tang X
- Tang XF
- Tian HL
- Toth D
- Varner GS
- Wan X
- Wang BQ
- Wang K
- Wang LL
- Wang LS
- Wang M
- Wang P
- Wang PL
- Wang Q
- Wang SG
- Wang XL
- Wang YD
- Wang YF
- Wang YQ
- Wang Z
- Wang ZG
- Wang ZY
- Wei DH
- Wen SP
- Wiedner U
- Wu LH
- Wu N
- Wu W
- Wu Z
- Xiao ZJ
- Xie YG
- Xu GF
- Xu GM
- Xu H
- Xu Y
- Xu ZR
- Xu ZZ
- Xue Z
- Yan L
- Yan WB
- Yan YH
- Yang HX
- Yang M
- Yang T
- Yang Y
- Yang YX
- Ye M
- Ye MH
- Yu BX
- Yu CX
- Yu L
- Yuan CZ
- Yuan WL
- Yuan Y
- Zafar AA
- Zallo A
- Zeng Y
- Zhang BX
- Zhang BY
- Zhang CC
- Zhang DH
- Zhang HH
- Zhang HY
- Zhang J
- Zhang JW
- Zhang JY
- Zhang JZ
- Zhang L
- Zhang SH
- Zhang TR
- Zhang XJ
- Zhang XY
- Zhang Y
- Zhang YH
- Zhang ZP
- Zhang ZY
- Zhao G
- Zhao HS
- Zhao J
- Zhao J
- Zhao L
- Zhao L
- Zhao MG
- Zhao Q
- Zhao SJ
- Zhao TC
- Zhao XH
- Zhao YB
- Zhao ZG
- Zhao ZL
- Zhemchugov A
- Zheng B
- Zheng JP
- Zheng YH
- Zheng ZP
- Zhong B
- Zhong J
- Zhong L
- Zhou L
- Zhou XK
- Zhou XR
- Zhu C
- Zhu K
- Zhu KJ
- Zhu SH
- Zhu XL
- Zhu XW
- Zhu YS
- Zhu ZA
- Zhuang J
- Zou BS
- Zou JH
- Zuo JX
- Zweber P
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2011
- Field of study
We present a study of the P-wave spin-triplet charmonium χ cJ decays (J=0, 1, 2) into π0π0π0π0. The analysis is based on 106×106 ψ⊃′ decays recorded with the BESIII detector at the BEPCII electron positron collider. The decay into the π0π0π0π0 hadronic final state is observed for the first time. We measure the branching fractions B(χ c0→π0π0π0π0)=(3.34±0. 06±0.44)×10⊃-3, B(χ c1→π0π0π0π0) =(0.57±0.03±0.08)×10⊃-3, and B(χ c2→π0π0π0π0)=(1.21±0.05±0.16) ×10⊃-3, where the uncertainties are statistical and systematical, respectively. © 2011 American Physical Society.published_or_final_versio
Measurement of the matrix element for the decay η′→ηπ +π -
- Author
- Ablikim M
- Achasov MN
- An L
- An Q
- An ZH
- Bai JZ
- Baldini R
- Ban Y
- Becker J
- Berger N
- Bertani M
- Bian JM
- Bondarenko O
- Boyko I
- Briere RA
- Bytev V
- Cai X
- Cao GF
- Cao XX
- Chang JF
- Chelkov G
- Chen G
- Chen HS
- Chen JC
- Chen ML
- Chen SJ
- Chen Y
- Chen YB
- Cheng HP
- Chu YP
- CroninHennessy D
- Dai HL
- Dai JP
- Dedovich D
- Deng ZY
- Denysenko I
- Destefanis M
- Ding Y
- Dong LY
- Dong MY
- Du SX
- Duan MY
- Fan RR
- Fang J
- Fang SS
- Feng CQ
- Fu CD
- Fu JL
- Gao Y
- Geng C
- Goetzen K
- Gong WX
- Greco M
- Grishin S
- Gu MH
- Gu YT
- Guan YH
- Guo AQ
- Guo LB
- Guo YP
- Hao XQ
- Harris FA
- He KL
- He M
- He ZY
- Heng YK
- Hou ZL
- Hu HM
- Hu JF
- Hu T
- Huang B
- Huang GM
- Huang JS
- Huang XT
- Huang YP
- Hussain T
- Ji CS
- Ji Q
- Ji XB
- Ji XL
- Jia LK
- Jiang LL
- Jiang XS
- Jiao JB
- Jiao Z
- Jin DP
- Jin S
- Jing FF
- Kavatsyuk M
- Komamiya S
- Kuehn W
- Lange JS
- Leung JKC
- Li C
- Li C
- Li DM
- Li F
- Li G
- Li HB
- Li JC
- Li L
- Li NB
- Li QJ
- Li WD
- Li WG
- Li XL
- Li XN
- Li XQ
- Li XR
- Li ZB
- Liang H
- Liang YF
- Liang YT
- Liao GR
- Liao XT
- Liu BJ
- Liu BJ
- Liu CL
- Liu CX
- Liu CY
- Liu F
- Liu F
- Liu FH
- Liu GC
- Liu H
- Liu HB
- Liu HM
- Liu HW
- Liu JP
- Liu K
- Liu KY
- Liu Q
- Liu SB
- Liu X
- Liu XH
- Liu Y
- Liu YB
- Liu YW
- Liu ZA
- Liu ZQ
- Loehner H
- Lu GR
- Lu HJ
- Lu JG
- Lu QW
- Lu XR
- Lu YP
- Luo CL
- Luo MX
- Luo T
- Luo XL
- Ma CL
- Ma FC
- Ma HL
- Ma QM
- Ma T
- Ma X
- Ma XY
- Maggiora M
- Malik QA
- Mao H
- Mao YJ
- Mao ZP
- Messchendorp JG
- Min J
- Mitchell RE
- Mo XH
- Muchnoi NY
- Nefedov Y
- Ning Z
- Olsen SL
- Ouyang Q
- Pacetti S
- Pelizaeus M
- Peters K
- Ping JL
- Ping RG
- Poling R
- Pun CSJ
- Qi M
- Qian S
- Qiao CF
- Qin XS
- Qiu JF
- Rashid KH
- Rong G
- Ruan XD
- Sarantsev A
- Schulze J
- Shao M
- Shen CP
- Shen XY
- Sheng HY
- Shepherd MR
- Song XY
- Sonoda S
- Spataro S
- Spruck B
- Sun DH
- Sun GX
- Sun JF
- Sun SS
- Sun XD
- Sun YJ
- Sun YZ
- Sun ZJ
- Sun ZT
- Tang CJ
- Tang X
- Tang XF
- Tian HL
- Toth D
- Varner GS
- Wan X
- Wang BQ
- Wang K
- Wang LL
- Wang LS
- Wang M
- Wang P
- Wang PL
- Wang Q
- Wang SG
- Wang XL
- Wang YD
- Wang YF
- Wang YQ
- Wang Z
- Wang ZG
- Wang ZY
- Wei DH
- Wen QG
- Wen SP
- Wiedner U
- Wu LH
- Wu N
- Wu W
- Wu Z
- Xiao ZJ
- Xie YG
- Xu GF
- Xu GM
- Xu H
- Xu Y
- Xu ZR
- Xu ZZ
- Xue Z
- Yan L
- Yan WB
- Yan YH
- Yang HX
- Yang M
- Yang T
- Yang Y
- Yang YX
- Ye M
- Ye MH
- Yu BX
- Yu CX
- Yu L
- Yuan CZ
- Yuan WL
- Yuan Y
- Zafar AA
- Zallo A
- Zeng Y
- Zhang BX
- Zhang BY
- Zhang CC
- Zhang DH
- Zhang HH
- Zhang HY
- Zhang J
- Zhang JW
- Zhang JY
- Zhang JZ
- Zhang L
- Zhang SH
- Zhang TR
- Zhang XJ
- Zhang XY
- Zhang Y
- Zhang YH
- Zhang ZP
- Zhang ZY
- Zhao G
- Zhao HS
- Zhao J
- Zhao J
- Zhao L
- Zhao L
- Zhao MG
- Zhao Q
- Zhao SJ
- Zhao TC
- Zhao XH
- Zhao YB
- Zhao ZG
- Zhao ZL
- Zhemchugov A
- Zheng B
- Zheng JP
- Zheng YH
- Zheng ZP
- Zhong B
- Zhong J
- Zhong L
- Zhou L
- Zhou XK
- Zhou XR
- Zhu C
- Zhu K
- Zhu KJ
- Zhu SH
- Zhu XL
- Zhu XW
- Zhu YS
- Zhu ZA
- Zhuang J
- Zou BS
- Zou JH
- Zuo JX
- Zweber P
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2011
- Field of study
The Dalitz plot of η⊃′→ηπ⊃+π⊃- decay is studied using (225.2±2.8)×106 J/ψ events collected with the BESIII detector at the BEPCII e⊃+e⊃- collider. With the largest sample of η⊃′ decays to date, the parameters of the Dalitz plot are determined in a generalized and a linear representation. Also, the branching fraction of J/ψ→γη⊃′ is determined to be (4.84±0.03±0.24)×10⊃-3, where the first error is statistical and the second systematic. © 2011 American Physical Society.published_or_final_versio
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