538 research outputs found
Observation of associated near-side and away-side long-range correlations in √sNN=5.02 TeV proton-lead collisions with the ATLAS detector
- Author
- Aad G
- Abajyan T
- Abbott B
- Abdallah J
- Abdel Khalek S
- Abdelalim AA
- Abdinov O
- Aben R
- Abi B
- Abolins M
- Abouzeid OS
- Abramowicz H
- Abreu H
- Acharya BS
- Adamczyk L
- Adams DL
- Addy TN
- Adelman J
- Adomeit S
- Adragna P
- Adye T
- Aefsky S
- Aguilar-Saavedra JA
- Agustoni M
- Ahlen SP
- Ahles F
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- Ahsan M
- Aielli G
- Akesson TP
- Akimoto G
- Akimov AV
- Alam MA
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- Aleksa M
- Aleksandrov IN
- Alessandria F
- Alexa C
- Alexander G
- Alexandre G
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- Alimonti G
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- Allbrooke BM
- Allison LJ
- Allport PP
- Allwood-Spiers SE
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- Angelidakis S
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- Arguin JF
- Argyropoulos S
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- Armbruster AJ
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- Arutinov D
- Asai S
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- Asman B
- Asquith L
- Assamagan K
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- ATLAS Collaboration The
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- Stanecka E
- Stanek RW
- Stanescu C
- Stanescu-Bellu M
- Stanitzki MM
- Stapnes S
- Starchenko EA
- Stark J
- Staroba P
- Starovoitov P
- Staszewski R
- Staude A
- Stavina P
- Steele G
- Steinbach P
- Steinberg P
- Stekl I
- Stelzer B
- Stelzer HJ
- Stelzer-Chilton O
- Stenzel H
- Stern S
- Stewart GA
- Stillings JA
- Stockton MC
- Stoebe M
- Stoerig K
- Stoicea G
- Stonjek S
- Strachota P
- Stradling AR
- Straessner A
- Strandberg J
- Strandberg S
- Strandlie A
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- Strauss E
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- Strong JA
- Stroynowski R
- Ströhmer R
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- Stupak J
- Sturm P
- Styles NA
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- Subramania H
- Subramaniam R
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- Sulin VV
- Sultansoy S
- Sumida T
- Sun X
- Sundermann JE
- Suruliz K
- Susinno G
- Sutton MR
- 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
- Tanaka R
- Tanaka S
- Tanaka S
- Tanasijczuk AJ
- Tani K
- Tannoury N
- Tapprogge S
- Tardif D
- Tarem S
- Tarrade F
- Tartarelli GF
- Tas P
- Tasevsky M
- Tassi E
- Tayalati Y
- Taylor C
- Taylor FE
- Taylor GN
- Taylor W
- Teinturier M
- Teischinger FA
- Teixeira Dias Castanheira M
- Teixeira-Dias P
- Temming KK
- Ten Kate H
- Teng PK
- Terada S
- Terashi K
- Terron J
- 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
- Toms K
- Tonoyan A
- Topfel C
- Topilin ND
- Torrence E
- Torres H
- Torró 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
- Trocmé B
- Troncon C
- Trottier-McDonald M
- Trovatelli M
- True P
- Trzebinski M
- Trzupek A
- Tsarouchas C
- Tseng JC
- Tsiakiris M
- Tsiareshka PV
- Tsionou D
- Tsipolitis G
- Tsiskaridze S
- Tsiskaridze V
- Tskhadadze EG
- Tsukerman II
- Tsulaia V
- Tsung JW
- Tsuno S
- Tsybychev D
- Tua A
- Tudorache A
- Tudorache V
- Tuggle JM
- Turala M
- Turecek D
- 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
- Vacek V
- Vachon B
- Vahsen S
- Valencic N
- Valentinetti S
- Valero A
- Valery L
- Valkar S
- Valladolid Gallego E
- Vallecorsa S
- Valls Ferrer JA
- Van Berg R
- Van Der Deijl 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 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
- Wall R
- Waller P
- Walsh B
- Wang C
- Wang H
- Wang H
- Wang J
- Wang J
- Wang K
- Wang R
- Wang SM
- Wang T
- Wang X
- 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 LA
- 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
- 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
Shape similarity, better than semantic membership, accounts for the structure of visual object representations in a population of monkey inferotemporal neurons
- Author
- A Alemi-Neissi
- A Clarke
- AC Connolly
- AH Bell
- AK Jain
- Alireza Alemi-Neissi
- BDB Willmore
- BJ Frey
- BZ Mahon
- BZ Mahon
- Carlo Baldassi
- CE Connor
- CL Wiggs
- CP Hung
- D Ringach
- D Zoccolan
- D Zoccolan
- DA Leopold
- Davide Zoccolan
- DD Cox
- DJ Freedman
- DJ Freedman
- DY Tsao
- DY Tsao
- DY Tsao
- EM Meyers
- ET Rolls
- ET Rolls
- ET Rolls
- F Gosselin
- F Iorio
- G Kayaert
- G Kayaert
- GA Orban
- GC Baylis
- H Op de Beeck
- I Biederman
- ID Popivanov
- J Mutch
- James J. DiCarlo
- JJ DiCarlo
- JK Fitzgerald
- K Lindorff-Larsen
- K Sakai
- K Tanaka
- KJ Nielsen
- L Fei-Fei
- M Bailly-Bechet
- M Bar
- M Bayati
- M Leone
- M Riesenhuber
- Marino Pagan
- MJ Garnett
- N Kanwisher
- N Kanwisher
- N Kriegeskorte
- N Li
- N Li
- N Li
- NC Rust
- NK Logothetis
- O Schwartz
- PE Downing
- R Kiani
- RF Murray
- Riccardo Zecchina
- RQ Quiroga
- RQ Quiroga
- RQ Quiroga
- RQ Quiroga
- S Higuchi
- S Suzuki
- S Tafazoli
- S-R Afraz
- SL Brincat
- SL Brincat
- T Naselaris
- T Serre
- Wolfgang Einhäuser
- Y Agam
- Y Miyashita
- Y Miyashita
- Y Yamane
- Z Kourtzi
- Publication venue
- 'Public Library of Science (PLoS)'
- Publication date
- 01/01/2013
- Field of study
The anterior inferotemporal cortex (IT) is the highest stage along the hierarchy of visual areas that, in primates, processes visual objects. Although several lines of evidence suggest that IT primarily represents visual shape information, some recent studies have argued that neuronal ensembles in IT code the semantic membership of visual objects (i.e., represent conceptual classes such as animate and inanimate objects). In this study, we investigated to what extent semantic, rather than purely visual information, is represented in IT by performing a multivariate analysis of IT responses to a set of visual objects. By relying on a variety of machine-learning approaches (including a cutting-edge clustering algorithm that has been recently developed in the domain of statistical physics), we found that, in most instances, IT representation of visual objects is accounted for by their similarity at the level of shape or, more surprisingly, low-level visual properties. Only in a few cases we observed IT representations of semantic classes that were not explainable by the visual similarity of their members. Overall, these findings reassert the primary function of IT as a conveyor of explicit visual shape information, and reveal that low-level visual properties are represented in IT to a greater extent than previously appreciated. In addition, our work demonstrates how combining a variety of state-of-the-art multivariate approaches, and carefully estimating the contribution of shape similarity to the representation of object categories, can substantially advance our understanding of neuronal coding of visual objects in cortex
Model-free model-fitting and predictive distributions
- Author
- A DasGupta
- A Pagan
- AC Atkinson
- AC Davison
- AK Gangopadhyay
- AP Dawid
- AS Goldberger
- B Efron
- B Efron
- B Efron
- C Loader
- D Ruppert
- DA Freedman
- Dimitris N. Politis
- DJ Olive
- DN Politis
- DN Politis
- DN Politis
- DN Politis
- DR Cox
- EA Nadaraya
- GAF Seber
- GEP Box
- GS Watson
- J Dai
- J Fan
- J Hahn
- J Horowitz
- J Shao
- J Wolfowitz
- JD Hart
- JD Hart
- JK Patel
- L Breiman
- L Wang
- M Neumann
- M Rosenblatt
- NR Draper
- NS Altman
- OB Linton
- P Bickel
- P Hall
- P Hall
- P Hall
- P McCullagh
- PS Carmack
- Q Li
- R Beran
- R Koenker
- R Tibshirani
- R Tibshirani
- RA Stine
- RJ Carroll
- RJ Carroll
- RL Schmoyer
- S Geisser
- SG Shi
- T McMurry
- T McMurry
- W Härdle
- W Härdle
- W Härdle
- WR Schucany
- Y Hong
- Y Hong
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- Field of study
Fighting Capital Flight in Africa: Evidence from Bundling and Unbundling Governance
- Author
- A Dixit
- A Gani
- A Moulemvo
- A Pagan
- AHT Mpenya
- AS Ndiaye
- BH Baltagi
- CR McKenzie
- D Kaufmann
- D Kaufmann
- D Kelsey
- D Roodman
- D Roodman
- DN Muchai
- F Fukuyama
- FL Bartels
- HF Kaiser
- I Kolstad
- I Love
- IT Jolliffe
- J Ba
- J Bai
- J Bai
- J Christensen
- J Weeks
- J Weeks
- J Westerlund
- J Westerlund
- J Westerlund
- J-M Gankou
- Jacinta C. Nwachukwu
- JH Stock
- JK Boyce
- JK Boyce
- JK Boyce
- JK Boyce
- JW Musila
- K Tuomi
- L Ndikumana
- L Ndikumana
- L Oxley
- M Arellano
- M Arellano
- M Kurtz
- M Kurtz
- M Kwaramba
- MH Pesaran
- OT Ramiandrisoa
- P Collier
- QV Le
- R Blundell
- R Drogendijk
- R Greenaway-McGrevy
- R Lensink
- RA Andrés
- RA Andrés
- RF Tusalem
- S Asongu
- S Dewan
- S Oluwatobi
- S Yerrabati
- SA Asongu
- SA Asongu
- SA Asongu
- SA Asongu
- SA Asongu
- SA Asongu
- Simplice A. Asongu
- T Beck
- T Kangoye
- U Efobi
- V Davies
- WK Darley
- X Lin
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2016
- Field of study
This study investigates the effect of governance on capital flight by bundling and unbundling governance. The empirical evidence is based on 37 African countries for the period 1996–2010 and the Generalised Method of Moments. Governance is bundled by principal component analysis, namely: (i) political governance from political stability and ‘voice and accountability’; (ii) economic governance from government effectiveness and regulation quality and (iii) institutional governance from corruption-control and the rule of law. The following findings are established. (i) Political stability and ‘voice and accountability’ reduce capital flight while the collective effect of political governance is not significant. (ii) Economic governance increases capital flight whereas the individual effects of regulation quality and government effectiveness are not significant. (iii) Corruption-control and institutional governance negatively affect capital flight whereas the impact of the rule of law is not significant. (iv) Taken together, Corruption-control is the most effective governance weapon in the fight against capital flight. (v) Priority in the Washington Consensus is more effective at fighting capital flight compared to the Beijing Model. Policy implications are discussed
Anatomy of the sign-problem in heavy-dense QCD
- Author
- Adam E Romero
- Aranda C Padilla
- Arjanovic MM
- Armadans R Caminal
- Astigarraga ME Pozo
- Barajas CA Chavez
- Bechtle P
- Beck HP
- Becker K
- Becker M
- Beckingham M
- Becot C
- Beddall A
- Beddall AJ
- Bednyakov VA
- Bedognetti M
- Bee CP
- Beemster LJ
- Beermann TA
- Begel M
- Behr JK
- Belanger-Champagne C
- Bell AS
- Bella G
- Bellagamba L
- Bellerive A
- Bellomo M
- Belotskiy K
- Beltramello O
- Belyaev NL
- Benary O
- Benchekroun D
- Bender M
- Bendtz K
- Benekos N
- Benhammou Y
- Benitez J
- Benjamin DP
- Bensinger JR
- Bentvelsen S
- Beresford L
- Beretta M
- Berge D
- Berger N
- Berghaus F
- Beringer J
- Berlendis S
- Berlingen J Montejo
- Bernard NR
- Bernius C
- Bernlochner FU
- Berry T
- Berta P
- Bertella C
- Bertoli G
- Bertolucci F
- Bertram IA
- Bertsche C
- Bertsche D
- Besjes GJ
- Bessner M
- Besson N
- Betancourt C
- Bethke S
- Bevan AJ
- Bhimji W
- Bianchi RM
- Bianchini L
- Bianco M
- Biebel O
- Biedermann D
- Bielski R
- Biesuz NV
- Biglietti M
- Bilokon H
- Bindi M
- Binet S
- Bingul A
- Bini C
- Biondi S
- Bjergaard DM
- Black CW
- Black JE
- Black KM
- Blackburn D
- Blair RE
- Blanchard J-B
- Blanco JE
- Blazek T
- Bloch I
- Blocker C
- Blum W
- Blumenschein U
- Blunier S
- Bobbink GJ
- Bobrovnikov VS
- Bocchetta SS
- Bocci A
- Bock C
- Boehler M
- Boeriu OE Vickey
- Boerner D
- Bogaerts JA
- Bogavac D
- Bogdanchikov AG
- Bohm C
- Boisvert V
- Bold T
- Boldea V
- Boldyrev AS
- Bomben M
- Bona M
- Boonekamp M
- Borisov A
- Borissov G
- Bortfeldt J
- Bortoletto D
- Bortolotto V
- Bos K
- Boscherini D
- Bosman M
- Bossio Sola JD
- Boudreau J
- Bouffard J
- Bouhova-Thacker EV
- Boumediene D
- Bourdarios C
- Bousson N
- Boutle SK
- Boveia A
- Boyd J
- Boyko IR
- Bracinik J
- Brandt A
- Brandt G
- Brandt O
- Bratzler U
- Brau B
- Brau JE
- Braun HM
- Bravo A Gascon
- Brendlinger K
- Brennan AJ
- Brenner L
- Brenner R
- Bressler S
- Bret M Cano
- Bristow TM
- Britton D
- Britzger D
- Brochu FM
- Brock I
- Brock R
- Brooijmans G
- Brooks T
- Brooks WK
- Brosamer J
- Brost E
- Broughton JH
- Bruncko D
- Bruneliere R
- Bruni A
- Bruni G
- Brunt BH
- Bruschi M
- Bruscino N
- Bryant P
- Bryngemark L
- Buanes T
- Buat Q
- Buchholz P
- Buckley AG
- Budagov IA
- Buehrer F
- Buescher D
- Buesher V
- Bugge MK
- Bulekov O
- Bullock D
- Burckhart H
- Burdin S
- Burgard CD
- Burghgrave B
- Burka K
- Burke S
- Burmeister I
- Busato E
- Bussey P
- Butler JM
- Butt AI
- Buttar CM
- Butterworth JM
- Butti P
- Buttinger W
- Buzatu A
- Buzykaev AR
- Bylund O Bessidskaia
- Cabrera Urban S
- Caforio D
- Cairo VM
- Cakir O
- Calace N
- Calafiura P
- Calandri A
- Calderini G
- Calfayan P
- Caloba LP
- Calvet D
- Calvet S
- Calvet TP
- Camarda S
- Camarri P
- Cameron D
- Camincher C
- Campana S
- Campanelli M
- Campoverde A
- Canale V
- Canepa A
- Cantero J
- Cantrill R
- Cao T
- Caprini I
- Caprini M
- Capua M
- Caputo R
- Carbone RM
- Cardarelli R
- Cardillo F
- Carli I
- Carli T
- Carlino G
- Carminati L
- Caron S
- Carquin E
- Carrillo-Montoya GD
- Carter JR
- Carvalho J
- Casadei D
- Casado MP
- Casolino M
- Casper DW
- Castaneda-Miranda E
- Castelli A
- Castillo Gimenez V
- Castillo I Santoyo
- Castilloa LR Flores
- Castro NF
- Catinaccio A
- Catmore JR
- Cattai A
- Caudron J
- Cavaliere V
- Cavalli D
- Cavalli-Sforza M
- Cavasinni V
- Ceradini F
- Cerda Alberich L
- Cerio BC
- Cerqueira AS
- Cerri A
- Cerrito L
- Cerutti F
- Cerv M
- Cervelli A
- Cetin SA
- Chafaq A
- Chakraborty D
- Chan SK
- Chan YL
- Chang P
- Chapman JD
- Charlton DG
- Chatterjee A
- Chau CC
- Che S
- Cheatham S
- Chegwidden A
- Chekanov S
- Chekulaev SV
- Chelkov GA
- Chelstowska MA
- Chen C
- Chen H
- Chen K
- Chen S
- Chen S
- Chen X
- Chen Y
- Cheng HC
- Cheng HJ
- Cheng Y
- Cheplakov A
- Cheremushkina E
- Cherkaoui El Moursli R
- Chernyatin V
- Cheu E
- Chevalier L
- Chiarella V
- Chiarelli G
- Chiodini G
- Chisholm AS
- Chitan A
- Chizhov MV
- Choi K
- Chomont AR
- Chouridou S
- Chow BKB
- Christodoulou V
- Chromek-Burckhart D
- Chudoba J
- Chuinard AJ
- Chwastowski JJ
- Chytka L
- Ciapetti G
- Ciftci AK
- Cinca D
- Cindro V
- Cioara IA
- Ciocio A
- Cirotto F
- Citron ZH
- Ciubancan M
- Clark A
- Clark BL
- Clark PJ
- Clarke RN
- Clement C
- Coadou Y
- Cobal M
- Coccaro A
- Cochran J
- Codina E Perez
- Coffey L
- Colasurdo L
- Cole B
- Cole S
- Colijn AP
- Collot J
- Colombo T
- Compostella G
- Conde Muino P
- Coniavitis E
- Connell SH
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- Yildiz H Duran
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- Zhemchugov A
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- Zibell A
- Zieminska D
- Zimine NI
- Zimmermann C
- Zimmermann S
- Zinonos Z
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- Zivkovic L
- Zobernig G
- Zoccoli A
- zur Nedden M
- Zurzolo G
- Zwalinski L
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2016
- Field of study
QCD at finite densities of heavy quarks is investigated
using the density-of-states method. The phase factor
expectation value of the quark determinant is calculated to
unprecedented precision as a function of the chemical potential.
Results are validated using those from a reweighting
approach where the latter can produce a significant signalto-noise
ratio. We confirm the particle–hole symmetry at low
temperatures, find a strong sign problem at intermediate values
of the chemical potential, and an inverse Silver Blaze
feature for chemical potentials close to the onset value: here,
the phase-quenched theory underestimates the density of the
full theory
Search for the direct production of charginos and neutralinos in final states with tau leptons in √s=13 TeV collisions with the ATLAS detector
- Author
- Aaboud M
- Aad G
- Abbott B
- Abdinov O
- Abeloos B
- Abidi SH
- AbouZeid OS
- Abraham NL
- Abramowicz H
- Abreu H
- Abreu R
- Abulaiti Y
- Acharya BS
- Adachi S
- Adamczyk L
- Adelman J
- Adersberger M
- Adye T
- Affolder AA
- Afik Y
- Agatonovic-Jovin T
- Agheorghiesei C
- Aguilar-Saavedra JA
- Ahlen SP
- Ahmadov F
- Aielli G
- Akatsuka S
- Akerstedt H
- Akesson TPA
- Akilli E
- Akimov AV
- Albergh GL
- Albert J
- Albicocco P
- Alconada Verzini MJ
- Alderweireldt SC
- Aleksa M
- Aleksandrov IN
- Alexa C
- Alexander G
- Alexopoulos T
- Alhroob M
- Ali B
- Aliev M
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- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2017
- Field of study
A search for the direct production of charginos and neutralinos in final states with at least two hadronically decaying tau leptons is presented. The analysis uses a dataset of pp collisions corresponding to an integrated luminosity of 36.1 fb−1, recorded with the ATLAS detector at the Large Hadron Collider at a centre-of-mass energy of 13TeV.Nosignificant deviation from the expected Standard Model background is observed. Limits are derived in scenarios of ˜χ+1 ˜χ−1 pair production and of ˜χ±1 ˜χ02 and ˜χ+1 ˜χ−1 production in simplified models where the neutralinos and charginos decay solely via intermediate left-handed staus and tau sneutrinos, and the mass of the ˜ τL state is set to be halfway between the masses of the ˜χ±1 and the ˜χ01. Chargino masses up to 630 GeV are excluded at 95% confidence level in the scenario of direct production of ˜χ+1 ˜χ−1 for a massless ˜χ01. Common ˜χ±1 and ˜χ02 masses up to 760 GeV are excluded in the case of production of ˜χ±1 ˜χ02 and ˜χ+1 ˜χ−1 assuming a massless ˜χ01. Exclusion limits for additional benchmark scenarios with large and small mass-splitting between the ˜χ±1 and the ˜χ01 are also studied by varying the ˜ τL mass between the masses of the ˜χ±1 and the ˜χ01
Measurement of the photon identification efficiencies with the ATLAS detector using LHC Run-1 data
- Author
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- Aad G
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- Abdallah J
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- Zobernig G
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- zur Nedden M
- Zurzolo G
- Zwalinski L
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2016
- Field of study
© 2016, CERN for the benefit of the ATLAS collaboration.The algorithms used by the ATLAS Collaboration to reconstruct and identify prompt photons are described. Measurements of the photon identification efficiencies are reported, using 4.9 fb- 1 of pp collision data collected at the LHC at s=7 TeV and 20.3 fb- 1 at s=8 TeV. The efficiencies are measured separately for converted and unconverted photons, in four different pseudorapidity regions, for transverse momenta between 10 GeV and 1.5 TeV. The results from the combination of three data-driven techniques are compared to the predictions from a simulation of the detector response, after correcting the electromagnetic shower momenta in the simulation for the average differences observed with respect to data. Data-to-simulation efficiency ratios used as correction factors in physics measurements are determined to account for the small residual efficiency differences. These factors are measured with uncertainties between 0.5% and 10% in 7 TeV data and between 0.5% and 5.6% in 8 TeV data, depending on the photon transverse momentum and pseudorapidity
Study of ordered hadron chains with the ATLAS detector
- Author
- Aaboud M
- Aad G
- Abbott B
- Abdinov O
- Abeloos B
- Abidi SH
- AbouZeid OS
- Abraham NL
- Abramowicz H
- Abreu H
- Abreu R
- Abulaiti Y
- Acharya BS
- Adachi S
- Adamczyk L
- Adelman J
- Adersberger M
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- Ahlen SP
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- Akerstedt H
- Akesson TPA
- Akilli E
- Akimov AV
- Alberghi GL
- Albert J
- Albicocco P
- Alderweireldt SC
- Aleksa M
- Aleksandrov IN
- Alexa C
- Alexander G
- Alexopoulos T
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- Alkire SP
- Allbrooke BMM
- Allen BW
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- Yoshihara K
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- Zieminska D
- Zimine NI
- Zimmermann C
- Zimmermann S
- Zinonos Z
- Zinser M
- Ziolkowski M
- Zivkovic L
- Zobernig G
- Zoccoli A
- Zou R
- Zu Theenhausen H Meyer
- zur Nedden M
- Zwalinski L
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2017
- Field of study
The analysis of the momentum difference between charged hadrons in high-energy proton-proton collisions is performed in order to study coherent particle production. The observed correlation pattern agrees with a model of a helical QCD string fragmenting into a chain of ground-state hadrons. A threshold momentum difference in the production of adjacent pairs of charged hadrons is observed, in agreement with model predictions. The presence of low-mass hadron chains also explains the emergence of charge-combination-dependent two-particle correlations commonly attributed to Bose-Einstein interference. The data sample consists of 190 μb−1 of minimum-bias events collected with proton-proton collisions at a center-of-mass energy √s=7 TeV in the early low-luminosity data taking with the ATLAS detector at the LHC
Combined measurement of differential and total cross sections in the H → γγ and the H → ZZ* → 4ℓ decay channels at s=13 TeV with the ATLAS detector
- Author
- Aaboud M
- Aad G
- Abbott B
- Abdinov O
- Abeloos B
- Abhayasinghe DK
- Abidi SH
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- Zobernig G
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- Zorbas TG
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- Zwalinski L
- Álvarez Piqueras D
- Åkesson TPA
- Šfiligoj T
- Ženiš T
- Živković L
- Publication venue
- Elsevier
- Publication date
- 01/01/2018
- Field of study
A combined measurement of differential and inclusive total cross sections of Higgs boson production is performed using 36.1 fb−1 of 13 TeV proton–proton collision data produced by the LHC and recorded by the ATLAS detector in 2015 and 2016. Cross sections are obtained from measured H→γγ and H→ZZ*(→4ℓ event yields, which are combined taking into account detector efficiencies, resolution, acceptances and branching fractions. The total Higgs boson production cross section is measured to be 57.0−5.9 +6.0 (stat.) −3.3 +4.0 (syst.) pb, in agreement with the Standard Model prediction. Differential cross-section measurements are presented for the Higgs boson transverse momentum distribution, Higgs boson rapidity, number of jets produced together with the Higgs boson, and the transverse momentum of the leading jet. The results from the two decay channels are found to be compatible, and their combination agrees with the Standard Model predictions
Search for High-Mass Resonances Decaying to τν in pp Collisions at √s=13 TeV with the ATLAS Detector
- Author
- Aaboud M
- Aad G
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- Zorbas TG
- Zou R
- Zu Theenhausen H Meyer
- zur Nedden M
- Zwalinski L
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2018
- Field of study
A search for high-mass resonances decaying to τν using proton-proton collisions at √s=13 TeV produced by the Large Hadron Collider is presented. Only τ-lepton decays with hadrons in the final state are considered. The data were recorded with the ATLAS detector and correspond to an integrated luminosity of 36.1 fb−1. No statistically significant excess above the standard model expectation is observed; model-independent upper limits are set on the visible τν production cross section. Heavy W′ bosons with masses less than 3.7 TeV in the sequential standard model and masses less than 2.2–3.8 TeV depending on the coupling in the nonuniversal G(221) model are excluded at the 95% credibility level
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