1,179 research outputs found
A Bayesian adaptive design for biomarker trials with linked treatments.
- Author
- A Jimeno
- AD Barker
- Adrian P Mander
- Anne-Laure Vallier
- B Freidlin
- CP Adams
- D Etemadmoghadam
- D Etemadmoghadam
- DJ Stewart
- EL Kwak
- ES Kim
- Helena M Earl
- Ioannis Gournaris
- J Cai
- J Wason
- James D Brenton
- James M S Wason
- Jean E Abraham
- JJ Lee
- JJ Lee
- JM Wason
- JMS Wason
- M Peeters
- P Gallo
- PB Chapman
- R Kaplan
- Richard D Baird
- SM Berry
- TA Yap
- Publication venue
- Br J Cancer
- Publication date
- 11/08/2015
- Field of study
BACKGROUND: Response to treatments is highly heterogeneous in cancer. Increased availability of biomarkers and targeted treatments has led to the need for trial designs that efficiently test new treatments in biomarker-stratified patient subgroups. METHODS: We propose a novel Bayesian adaptive randomisation (BAR) design for use in multi-arm phase II trials where biomarkers exist that are potentially predictive of a linked treatment's effect. The design is motivated in part by two phase II trials that are currently in development. The design starts by randomising patients to the control treatment or to experimental treatments that the biomarker profile suggests should be active. At interim analyses, data from treated patients are used to update the allocation probabilities. If the linked treatments are effective, the allocation remains high; if ineffective, the allocation changes over the course of the trial to unlinked treatments that are more effective. RESULTS: Our proposed design has high power to detect treatment effects if the pairings of treatment with biomarker are correct, but also performs well when alternative pairings are true. The design is consistently more powerful than parallel-groups stratified trials. CONCLUSIONS: This BAR design is a powerful approach to use when there are pairings of biomarkers with treatments available for testing simultaneously.This work was supported by the Medical Research Council (grant number G0800860) and the NIHR Cambridge Biomedical Research Centre.This is the final version of the article. It first appeared from NPG via http://dx.doi.org/10.1038/bjc.2015.27
Angular and Current-Target Correlations in Deep Inelastic Scattering at HERA
- Author
- Abbiendi G
- Abe T
- Abramowicz H
- Acosta D
- Adamczyk L
- Adamus M
- Ahn Sh
- Amelung C
- An Sh
- Anselmo F
- Antonioli P
- Arneodo M
- Bacon Tc
- Badgett Wf
- Bailey Dc
- Bailey Ds
- Bamberger A
- Barbagli G
- Bari G
- Barreiro F
- Barret O
- Bashindzhagyan Gl
- Bashkirov V
- Basile M
- Bauerdick Lat
- Bednarek B
- Behrens U
- Bellagamba L
- Bertolin A
- Bhadra S
- Bienlein Jk
- Blaikley He
- Bohnet I
- Bokel C
- Boogert S
- Bornheim A
- Borzemski P
- Boscherini D
- Botje M
- Breitweg J
- Brock I
- Brook Nh
- Brugnera Riccardo
- Brummer N
- Bruni A
- Bruni G
- Burgard C
- Burow Bd
- Bussey Pj
- Butterworth Jm
- Bylsma B
- CA ZEUS Collaboration
- Caldwell A
- Capua M
- Carlin Roberto
- Cartiglia N
- Cashmore Rj
- Castellini G
- Catterall Cd
- Chapin D
- Chekanov S
- Chwastowski J
- Ciborowski J
- Cifarelli L
- Cindolo F
- Cirio R
- Cloth P
- Coboken K
- Coldewey C
- Cole Je
- Contin A
- COOPER SARKAR Am
- Coppola N
- Cormack C
- Corradi M
- Corriveau F
- Costa M
- Cottingham Wn
- Crittenden J
- Cross R
- D'Agostini G
- Dagan S
- DAL CORSO F
- Dardo M
- DE PASQUALE S
- DE WOLF E
- Deffner R
- DEL PESO J
- Deppe O
- Derrick M
- Deshpande A
- Desler K
- Devenish Rce
- Dhawan S
- Dolgoshein Ba
- Dondana S
- Dosselli U
- Doyle At
- Drews G
- Dulinski Z
- Durkin Ls
- Dusini S
- Eckert M
- Edmonds Jk
- Eisenberg Y
- Eisenhardt S
- Engelen J
- Epperson D
- Ermolov Pf
- Eskreys A
- Fagerstroem Cp
- Fernandez Jp
- Ferrero Mi
- Figiel J
- Filges D
- Foster B
- Foudas C
- FOX MURPHY A
- Fricke U
- Frisken Wr
- Fusayasu T
- Gadaj T
- Galea R
- Gallo E
- Garcia G
- Garcia Yz
- Garfagnini Alberto
- Gendner N
- Gialas I
- Gilmore J
- Ginsburg Cm
- Giusti P
- Gladilin Lk
- Glasman C
- Goebel F
- Golubkov Ya
- Gottlicher P
- Grabosch Hj
- Graciani R
- GROSSE KNETTER J
- Grzelak G
- Haas T
- Hain W
- HALL WILTON R
- Hamatsu R
- Hanna Ds
- Harnew N
- Hart Jc
- Hartmann H
- Hartmann J
- Hartner Gf
- Hasell D
- Hayes Me
- Heapby Ea
- Heath Gp
- Heath Hf
- Hebbel K
- Heinloth K
- Heinz L
- Hernandez Jm
- Heusch C
- Hilger E
- Hirose T
- Hochman D
- Holm U
- Homma K
- Hong Sj
- Howell G
- Hughes Vw
- Iacobucci G
- Iannotti L
- Iga Y
- Inuzuka M
- Ishii T
- Jakob Hp
- Jelen K
- Jeoung Hy
- Jing Z
- Johnson Kf
- Jones Tw
- Kananov S
- Kappes A
- Karshon U
- Kasemann M
- Katz Uf
- Kcira D
- Kerger R
- Khakzad M
- Khein La
- Kim Cl
- Kim Jy
- Kisielewska D
- Kitamura S
- Klanner R
- Klimek K
- Koch W
- Koffeman E
- Kooijman P
- Koop T
- Korotkova Na
- Korzhavina Ia
- Kotanski A
- Kotz U
- Kowal Am
- Kowalski H
- Kowalski T
- Krakauer D
- Kreisel A
- Kuze M
- Kuzmin Va
- Labarga L
- Lamberti L
- Lane Jb
- Laurenti G
- Lee Jh
- Lee Sb
- Lee Sw
- Levi G
- Levman Gm
- Levy A
- Lim H
- Lim It
- Limentani S
- Lindemann L
- Ling Ty
- Liu W
- Lohr B
- Lohrmann E
- Long Kr
- Lukina Oy
- Ma Kj
- Maccarrone G
- Macdonald N
- Magill S
- Mallik U
- Margotti A
- Marini G
- Markun P
- Martin Jf
- Martinez M
- Maselli S
- Massam T
- Mastroberardino A
- Matsushita T
- Mattingly Mck
- Mattingly S
- Mccance Gj
- Mccubbin Na
- Mcfall Jd
- Mellado B
- Menary S
- MEYER LARSEN A
- Meyer A
- Milewski J
- Milite M
- Miller Db
- Monaco V
- Monig K
- Monteiro T
- Morandin M
- Moritz M
- Murray Wn
- Musgrave B
- Nagano K
- Nam Sw
- Nania R
- Nigro A
- Nishimura T
- Notz D
- Nowak Rj
- Noyes Va
- Nylander P
- Ochs A
- Oh By
- Okrasinski Jr
- Olkiewicz K
- Orr Rs
- Pac My
- Padhi S
- Palmonari F
- Park Ih
- Park Sk
- Parsons Ja
- Paul E
- Pavel N
- Pawlak Jm
- Pawlak R
- Pelfer P
- Pellegrino A
- Pelucchi F
- Peroni C
- Pesci A
- Petrucci Mc
- Pfeiffer M
- Piccioni D
- Piotrzkoswski K
- Poelz G
- Polenz S
- Polini A
- Posocco M
- Prinias A
- Proskuryakov As
- Przybycien M
- Przybycien Mb
- Puga J
- Quadt A
- Raach H
- Raso M
- Rautenberg J
- Redondo I
- Reeder Dd
- Repond J
- Ritz S
- Riveline M
- Rohde M
- Romeo Gc
- RULIKOWSKA ZAREBSKA E
- Ruske O
- Ruspa M
- Sabetfakhri A
- Sacchi R
- Sadrozinski Hfw
- Salehi H
- Sampson S
- Sartorelli G
- Saull Prb
- Savin Aa
- Saxon Dh
- Schechter A
- Schioppa M
- Schlenstedt S
- Schmidke Wb
- Schneekloth U
- Schnurbusch H
- Schwarzer O
- Sciulli F
- Scott J
- Sedgbeer Jk
- Seiden A
- Selonke F
- Shah Tp
- Shcheglova Lm
- Sideris D
- Sievers M
- Simmons D
- Sinclair Le
- Skillicorn Io
- Smalska B
- Smith Wh
- Solano A
- Solomin An
- Son D
- ST LAURENT M
- Staiano A
- Stairs Dg
- Stanco L
- Stanek R
- Stifutkin A
- Stonjek S
- Straub Pb
- Strickland E
- Stroili Roberto
- Susinno G
- Suszycki L
- Sutton Mr
- Suzuki I
- Tandler J
- Tapper Ad
- Tapper Rj
- Tassi E
- Terron J
- Tiecke W
- Tokushuku K
- Toothacker Ws
- Tsurugai T
- Tuning N
- Tymieniecka T
- Umemori K
- Vaiciulis A
- VAN SIGHEM A
- Velthuis Jj
- Verkerke W
- Viani Ald
- Voci C
- Vossebeld J
- Votano L
- Walczak R
- Walker R
- Wang Sm
- Waters Ds
- Waugh R
- Weber A
- Whitmore Jj
- Wichmann R
- Wick K
- Wieber H
- Wiggers L
- Wildschek T
- Williams Dc
- Wing M
- Wodarczyk M
- Wolf G
- Wolfle S
- Wollmer U
- Wroblewski Ak
- Yamada S
- Yamashita T
- Yamauchi K
- Yamazaki Y
- Yoshida R
- Youngman C
- Zajac J
- Zakrzewski Ja
- Zarnecki Af
- Zawiejski L
- Zetsche F
- Zeuner W
- Zhu Q
- Zichichi A
- Zotkin Sa
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/1999
- Field of study
Correlations between charged particles in deep inelastic ep scattering have
been studied in the Breit frame with the ZEUS detector at HERA using an
integrated luminosity of 6.4 pb-1. Short-range correlations are analysed in
terms of the angular separation between current-region particles within a cone
centred around the virtual photon axis. Long-range correlations between the
current and target regions have also been measured. The data support
predictions for the scaling behaviour of the angular correlations at high Q2
and for anti-correlations between the current and target regions over a large
range in Q2 and in the Bjorken scaling variable x. Analytic QCD calculations
and Monte Carlo models correctly describe the trends of the data at high Q2,
but show quantitative discrepancies. The data show differences between the
correlations in deep inelastic scattering and e+e- annihilation.Comment: 26 pages including 10 figures (submitted to Eur. J. Phys. C
Measurement of CP-violation asymmetries in D0 to Ks pi+ pi-
- Author
- Aaltonen T
- Ahmed S
- Alam MS
- Albert J
- Amerio S
- Amidei D
- Anastassov A
- Annovi A
- Antos J
- Apollinari G
- Appel JA
- Arisawa T
- Artikov A
- Asaadi J
- Ashmanskas W
- Auerbach B
- Aurisano A
- Azfar F
- Azzolini V
- Badgett W
- Bae T
- Band HR
- Banerjee S
- Barbaro-Galtieri A
- Barnes VE
- Barnett BA
- Barria P
- Bartos P
- Bauce M
- Bedeschi F
- Behari S
- Bellettini G
- Bellinger J
- Benjamin D
- Beretvas A
- Bhatti A
- Bhuyan B
- Bianchi F
- Bisello D
- Bizjak I
- Bland KR
- Blumenfeld B
- Bocci A
- Bodek A
- Bomben M
- Bortoletto D
- Bosisio L
- Boudreau J
- Boveia A
- Brigliadori L
- Bromberg C
- Brucken E
- Budagov J
- Budd HS
- Bula R
- Burchat PR
- Burkett K
- Busetto G
- Bussey P
- Buzatu A
- Calamba A
- Calancha C
- Camarda S
- Campanelli M
- Campbell M
- Canelli F
- Carls B
- Carlsmith D
- Carosi R
- Carrillo S
- Carron S
- Cartaro C
- Casal B
- Casarsa M
- Castro A
- Catastini P
- Cauz D
- Cavaliere V
- Cavalli-Sforza M
- Cerri A
- Cerrito L
- Chen X
- Chen YC
- Chertok M
- Chiarelli G
- Chlachidze G
- Chlebana F
- Cho K
- Chokheli D
- Chung WH
- Chung YS
- Ciocci MA
- Clark A
- Clarke C
- Compostella G
- Convery ME
- Conway J
- Corbo M
- Cordelli M
- Cossutti F
- Cox CA
- Cox DJ
- Crescioli F
- Cuevas J
- Culbertson R
- d'Ascenzo N
- d'Errico M
- D'Onofrio M
- da Costa JG
- Dagenhart D
- Dasu S
- Datta M
- de Barbaro P
- Dell'Orso M
- Della Ricca G
- Demortier L
- Deninno M
- Devoto F
- Di Canto A
- Di Ruzza B
- Dittmann JR
- Donati S
- Dong P
- Dorigo M
- Dorigo T
- Ebina K
- Eckmann R
- Edwards AJ
- Elagin A
- Eppig A
- Erbacher R
- Ernst JA
- Errede S
- Ershaidat N
- Eusebi R
- Farrington S
- Feindt M
- Fernandez JP
- Fernandez PM
- Field R
- Flanagan G
- Flood KT
- Forrest R
- Frank MJ
- Franklin M
- Freeman JC
- Funakoshi Y
- Furic I
- Gallinaro M
- Gallo F
- Gamba D
- Garcia JE
- Garfinkel AF
- Garosi P
- Gerberich H
- Gerchtein E
- Giagu S
- Giakoumopoulou V
- Giannetti P
- Gibson K
- Ginsburg CM
- Giokaris N
- Giromini P
- Giurgiu G
- Glagolev V
- Glenzinski D
- Gold M
- Goldin D
- Goldschmidt N
- Golossanov A
- Gomez G
- Gomez-Ceballos G
- Goncharov M
- Gonzalez BA
- Gonzalez O
- Gorelov I
- Goshaw AT
- Goulianos K
- Grinstein S
- Griso SP
- Grosso-Pilcher C
- Group RC
- Hahn SR
- Halkiadakis E
- Hamaguchi A
- Hamano K
- Han JY
- Happacher F
- Hara K
- Hare D
- Hare M
- Harr RF
- Harrison PF
- Hatakeyama K
- Hays C
- Heck M
- Heinrich J
- Herndon M
- Hewamanage S
- Hocker A
- Hollar JJ
- Hopkins W
- Horn D
- Hou S
- Hughes RE
- Hurwitz M
- Husemann U
- Hussain N
- Hussein M
- Huston J
- Ilic J
- Introzzi G
- Iori M
- Ivanov A
- Izen JM
- Jain V
- James E
- Jang D
- Jayatilaka B
- Jeon EJ
- Jindariani S
- Jones M
- Joo KK
- Jun SY
- Junk TR
- Kamon T
- Karchin PE
- Kasmi A
- Kato Y
- Ketchum W
- Keung J
- Khotilovich V
- Kilminster B
- Kim DH
- Kim HS
- Kim JE
- Kim MJ
- Kim P
- Kim SB
- Kim SH
- Kim YJ
- Kim YK
- Kimura N
- Kirby M
- Klimenko S
- Knoepfel K
- Kocian ML
- Kondo K
- Kong DJ
- Konigsberg J
- Kotwal AV
- Kowalewski R
- Kreps M
- Krishnamurthy M
- Kroll J
- Krop D
- Kruse M
- Krutelyov V
- Kuhr T
- Kurata M
- Kutter PE
- Kwang S
- Laasanen AT
- Lami S
- Lammel S
- Lancaster M
- Lanceri L
- Lander RL
- Lannon K
- Lath A
- Latham TE
- Latino G
- LeCompte T
- Lee E
- Lee HS
- Lee JS
- Lee SW
- Leith DWGS
- Leo S
- Leone S
- Lewis JD
- Li S
- Limosani A
- Lin CJ
- Lindgren M
- Lipeles E
- Lister A
- Litvintsev DO
- Liu C
- Liu H
- Liu Q
- Liu T
- Lockwitz S
- Loginov A
- Lopez-March N
- Lou XC
- Lucchesi D
- Lueck J
- Luitz S
- Lujan P
- Lukens P
- Lungu G
- Luth V
- Lynch HL
- Lys J
- Lysak R
- MacFarlane DB
- Madrak R
- Maeshima K
- Maestro P
- Majewski SA
- Malik S
- Manca G
- Manousakis-Katsikakis A
- Margaroli F
- Marino C
- Marsiske H
- Martinez M
- Martinez-Vidal F
- Mastrandrea P
- Matera K
- Mattson ME
- Mazzacane A
- Mazzanti P
- McFarland KS
- McIntyre P
- McNulty R
- Mehta A
- Mehtala P
- Mesropian C
- Messner R
- Miao T
- Mietlicki D
- Milanes DA
- Mitra A
- Miyake H
- Miyashita TS
- Moed S
- Moggi N
- Mohanty GB
- Mondragon MN
- Moon CS
- Moore R
- Morello MJ
- Morlock J
- Mukherjee A
- Muller DR
- Muller T
- Murat P
- Mussini M
- Nachtman J
- Nagai Y
- Naganoma J
- Nakano I
- Napier A
- Neal H
- Nett J
- Neu C
- Neubauer MS
- Nielsen J
- Nodulman L
- Noh SY
- Norniella O
- Nugent IM
- O'Grady CP
- Oakes L
- Ofte I
- Oh SH
- Oh YD
- Oksuzian I
- Okusawa T
- Orava R
- Ortolan L
- Oyanguren A
- Pagliarone C
- Palencia E
- Pan B
- Pan Y
- Papadimitriou V
- Paramonov AA
- Patrick J
- Pauletta G
- Paulini M
- Paus C
- Pellett DE
- Pelliccioni M
- Penzo A
- Perazzo A
- Perl M
- Petersen BA
- Phillips TJ
- Piacentino G
- Pianori E
- Pierini M
- Pilot J
- Pitts K
- Plager C
- Pondrom L
- Poprocki S
- Potamianos K
- Pranko A
- Prepost R
- Prokoshin F
- Ptohos F
- Pulliam T
- Punzi G
- Rahaman A
- Ramakrishnan V
- Ranjan N
- Ratcliff BN
- Redondo I
- Renton P
- Rescigno M
- Riddick T
- Rimondi F
- Ristori L
- Ritchie JL
- Robson A
- Rodrigo T
- Rodriguez T
- Rogers E
- Rolli S
- Roney JM
- Roodman A
- Roser R
- Ruffini F
- Ruiz A
- Ruland AM
- Russ J
- Rusu V
- Saeed MA
- Safonov A
- Sakumoto WK
- Sakurai Y
- Salnikov AA
- Santi L
- Sato K
- Saveliev V
- Savoy-Navarro A
- Schilling CJ
- Schindler RH
- Schlabach P
- Schmidt A
- Schmidt EE
- Schwarz T
- Schwiening J
- Schwitters RF
- Scodellaro L
- Scribano A
- Scuri F
- Seidel S
- Seiya Y
- Semenov A
- Sforza F
- Shalhout SZ
- Shears T
- Shepard PF
- Shimojima M
- Shochet M
- Shreyber-Tecker I
- Simonenko A
- Sinervo P
- Sliwa K
- Smith JR
- Snider FD
- Snyder A
- Sobie RJ
- Soha A
- Song H
- Sorin V
- Spanier SM
- Squillacioti P
- St Denis R
- Stancari M
- Stelzer B
- Stelzer-Chilton O
- Stentz D
- Strologas J
- Strycker GL
- Su D
- Sudo Y
- Sukhanov A
- Sullivan MK
- Suslov I
- Suzuki K
- Swain SK
- Takemasa K
- Takeuchi Y
- Tang J
- Tecchio M
- Teng PK
- Thom J
- Thome J
- Thompson GA
- Thompson JM
- Thomson E
- Toback D
- Tokar S
- Tollefson K
- Tomura T
- Tonelli D
- Torre S
- Torretta D
- Totaro P
- Trovato M
- Ukegawa F
- Uozumi S
- Va'vra J
- Varganov A
- Vazquez F
- Velev G
- Vellidis C
- Vidal M
- Vila I
- Vilar R
- Vitale L
- Vizan J
- Vogel M
- Volpi G
- Wagner AP
- Wagner P
- Wagner RL
- Wakisaka T
- Wallny R
- Wang SM
- Wappler FR
- Warburton A
- Waters D
- Weaver M
- Wester WC
- Whiteson D
- Wick F
- Wicklund AB
- Wicklund E
- Wilbur S
- Wilden L
- Williams HH
- Wilson JS
- Wilson P
- Winer BL
- Wisniewski WJ
- Wittgen M
- Wittich P
- Wolbers S
- Wolfe H
- Wright DH
- Wright T
- Wu SL
- Wu X
- Wu Z
- Yamamoto K
- Yamato D
- Yang T
- Yang UK
- Yang YC
- Yao WM
- Yarritu AK
- Ye S
- Yeh GP
- Yi K
- Yi K
- Yoh J
- Yorita K
- Yoshida T
- Young CC
- Yu GB
- Yu I
- Yu SS
- Yun JC
- Zain SB
- Zanetti A
- Zeng Y
- Zhou C
- Ziegler V
- Zucchelli S
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2012
- Field of study
We report a measurement of time-integrated CP-violation asymmetries in the
resonant substructure of the three-body decay D0 to Ks pi+ pi- using CDF II
data corresponding to 6.0 invfb of integrated luminosity from Tevatron ppbar
collisions at sqrt(s) = 1.96 TeV. The charm mesons used in this analysis come
from D*+(2010) to D0 pi+ and D*-(2010) to D0bar pi-, where the production
flavor of the charm meson is determined by the charge of the accompanying pion.
We apply a Dalitz-amplitude analysis for the description of the dynamic decay
structure and use two complementary approaches, namely a full Dalitz-plot fit
employing the isobar model for the contributing resonances and a
model-independent bin-by-bin comparison of the D0 and D0bar Dalitz plots. We
find no CP-violation effects and measure an asymmetry of ACP = (-0.05 +- 0.57
(stat) +- 0.54 (syst))% for the overall integrated CP-violation asymmetry,
consistent with the standard model prediction.Comment: 15 page
Observation of associated near-side and away-side long-range correlations in âsNN=5.02ââTeV 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
- Ahmad A
- Ahsan M
- Aielli G
- Akesson TP
- 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 BM
- Allison LJ
- Allport PP
- Allwood-Spiers SE
- Almond J
- Aloisio A
- Alon R
- Alonso A
- Alonso F
- Altheimer A
- Alvarez Gonzalez B
- 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
- Anduaga XS
- Angelidakis S
- Anger P
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- Zemla A
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- Zhemchugov A
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- Zimin NI
- Zimmermann R
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- 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 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
Jet energy measurement with the ATLAS detector in proton-proton collisions at root s=7 TeV
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- Abbott B
- Abdallah J
- Abdelalim AA
- Abdesselam A
- Abdinov O
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- Wiik-Fuchs LAM
- Wijeratne PA
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- Wilkens HG
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- Wosiek BK
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- Yanush S
- Yao Y
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- Yildizb HD
- Yilmaz M
- Yoosootiniya R
- Yorita K
- Yoshida R
- Young C
- Youssef S
- Yu D
- Yu J
- Yu J
- Yuan L
- Yurkewicz A
- Zaets VG
- Zaidan R
- Zaitsev AM
- Zajacova Z
- Zalite YK
- Zanello L
- Zarzhitsky P
- Zaytsev A
- Zeitnitz C
- Zeller M
- Zeman M
- Zemla A
- Zendler C
- Zenin O
- Zenonos Z
- Zenz S
- Zerwas D
- Zhan Z
- Zhang D
- Zhang H
- Zhang J
- Zhang Q
- Zhang X
- Zhang Z
- Zhao L
- Zhao T
- Zhao Z
- Zhemchugov A
- Zheng S
- Zhong J
- Zhou B
- Zhou N
- Zhou Y
- Zhu CG
- Zhu H
- Zhu J
- Zhu Y
- Zhuang X
- Zhuravlov V
- Zieminska D
- Zimmermann R
- Zimmermann S
- Zimmermann S
- Zinonos Z
- Ziolkowski M
- Zitoun R
- Zivkovic L
- Zmouchko VV
- Zobernig G
- Zoccoli A
- Zolnierowski Y
- Zsenei A
- Zutshi V
- Zwalinski L
- 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 âs = 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 pTâ„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 60â€pT<800 GeV, and is maximally 14 % for pT<30 GeV in the most forward region 3. 2â€{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 and study of baryonic B decays: B -> D(*) p pbar, D(*) p pbar pi, and D(*) p pbar pi pi
- Author
- Adametz A
- Adye T
- Ahmed S
- Ahmed S
- Alam MS
- Alam MS
- Albert J
- Albert J
- Allen MT
- Alwyn KE
- Anderson J
- Andreassen R
- Andreotti M
- Angelini C
- Anulli F
- Arnaud N
- Asgeirsson DJ
- Aston D
- Atmacan H
- Ayad R
- Azzolini V
- Bailey D
- Baldini-Ferroli R
- Band HR
- Band HR
- Banerjee S
- Banerjee S
- Baracchini E
- Bard DJ
- Barlow RJ
- Bartoldus R
- Batignani G
- Battaglia M
- Behera PK
- Bellis M
- Ben-Haim E
- Benitez JF
- Bernard D
- Bernlochner FU
- Bettarini S
- Bettoni D
- Bevan AJ
- Bhuyan B
- Bhuyan B
- Bianchi F
- Bianchi F
- Biasini M
- Biassoni P
- Bingham I
- Blinov VE
- Bloom PC
- Blount NL
- Bomben M
- Bomben M
- Bondioli M
- Bonneaud GR
- Bosisio L
- Bozzi C
- Brau J
- Briand H
- Brown DN
- Brown DN
- Bula R
- Burchat PR
- Burchat PR
- Buzykaev AR
- Calabrese R
- Calcaterra A
- Calderini G
- Campagnari C
- Carpinelli M
- Cartaro C
- Cartaro C
- Casarosa G
- Castelli G
- Cavoto G
- Cecchi A
- Cenci R
- Cervelli A
- Chauveau J
- Chavez CA
- Chen C
- Chen X
- Chen XR
- Cheng CH
- Choi HHF
- Cibinetto G
- Clark PJ
- Cochranz J
- Coleman JP
- Contri R
- Convery MR
- Corwin LA
- Cossutti F
- Cowan G
- Cowan R
- Crawley HB
- Cremaldi L
- Curry S
- da Costa JF
- Dallapiccola C
- Dasu S
- Dasu S
- Dauncey PD
- Davier M
- Davis CL
- de Monchenault GH
- De Nardo G
- de Sangro R
- Della Ricca G
- Denig AG
- Derkach D
- Di Lodovico F
- Doll DA
- Dong L
- Dorfan J
- Druzhinin VP
- Dubois-Felsmann GP
- Dubrovin MS
- Dujmic D
- Dunwoodie W
- Ebert M
- Echenard B
- Eckmann R
- Eckmann R
- Edwards AJ
- Edwards AJ
- Eigen G
- Eisner AM
- Emery S
- Ernst JA
- Ernst JA
- Faccini R
- Feltresi E
- Ferrarotto F
- Ferroni F
- Field RC
- Finocchiaro G
- Fioravanti E
- Flanigan JM
- Flood KT
- Flood KT
- Ford WT
- Forti F
- Franchini P
- Franek B
- Frey R
- Fritsch M
- Fry JR
- Fulsom BG
- Gabareen AM
- Gabathuler E
- Gagliardi N
- Gallo F
- Gamba D
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- Gamet R
- Gary JW
- Gaspero M
- Gaz A
- Gershon TJ
- Gioi LL
- Giorgi MA
- Godang R
- Golubev VB
- Gradl W
- Graham MT
- Grauges E
- Grenier P
- Gritsan AV
- Grosdidier G
- Guido E
- Guo ZJ
- Guttman N
- Hafner A
- Hamano K
- Hamano K
- Hamon O
- Harrison PF
- Harrison PF
- Hartmann T
- Hast C
- Hawkes CM
- Hearty C
- Heusch CA
- Hitlin DG
- Hollar JJ
- Hong TM
- Honscheid K
- Hooberman B
- Hutchcroft DE
- Igonkina O
- Ilic J
- Innes WR
- Izen JM
- Izen JM
- Jackson G
- Jain V
- Jasper H
- Jawahery A
- Jessop CP
- Karbach TM
- Kass R
- Kelsey MH
- Kerth LT
- Khan A
- Kim H
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- Kim P
- King GJ
- Kirkby D
- Knoepfel KJ
- Kobel MJ
- Koch H
- Kocian ML
- Kocian ML
- Kolb JA
- Kolomensky YG
- Kovalskyi D
- Kowalewski R
- Kowalewski R
- Krishnamurthy M
- Kroeger R
- Kroseberg J
- Kutter PE
- Lacker HM
- Lafferty GD
- Lanceri L
- Lanceri L
- Lange DJ
- Lankford AJ
- Latham TE
- Latham TE
- Lazzaro A
- Le Diberder F
- Leddig T
- Lee CL
- Lees JP
- Leith DWGS
- Leith DWGS
- Leruste P
- Lewczuk MJ
- Li S
- Li S
- Lindemann D
- Lindquist B
- Liu F
- Lo Vetere M
- Lockman WS
- Lombardo V
- Long O
- Lopez-March N
- Lopez-March N
- LoSecco JM
- Lou XC
- Lou XC
- Lu C
- Lueck T
- Luitz S
- Luitz S
- Lund P
- Luppi E
- Lusiani A
- Luth V
- Luth V
- Lutz AM
- Lynch G
- Lynch HL
- Lynch HL
- MacFarlane DB
- MacFarlane DB
- Majewski SA
- Malaescu B
- Mallik U
- Mancinelli G
- Mandelkern M
- Manoni E
- Marchiori G
- Margoni M
- Marks J
- Marsiske H
- Marsiske H
- Martin EC
- Martinelli M
- Martinez AJ
- Martinez-Vidal F
- Martinez-Vidal F
- Mattison TS
- Mazzoni MA
- McKenna JA
- Meadows BT
- Merkel J
- Messner R
- Meyer WT
- Milanes DA
- Milanes DA
- Miyashita TS
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- Mohanty GB
- Monge MR
- Monorchio D
- Morandin M
- Morii M
- Morris JP
- Muller DR
- Muller DR
- Munerato M
- Nagel M
- Nauenberg U
- Neal H
- Neal H
- Negrini M
- Nelson S
- Neri N
- Nguyen X
- Nicolaci M
- Nugent IM
- Nugent IM
- O'Grady CP
- O'Grady CP
- Ocariz J
- Ofte I
- Ofte I
- Olaiya EO
- Olsen J
- Ongmongkolkul P
- Onorato G
- Onuchin AP
- Osipenkov IL
- Oyanguren A
- Oyanguren A
- Pacetti S
- Palano A
- Palombo F
- Pan B
- Pan B
- Pan Y
- Pan Y
- Paoloni E
- Pappagallo M
- Paramesvaran S
- Park W
- Passaggio S
- Patel PM
- Patrignani C
- Patteri P
- Payne DJ
- Pegna DL
- Pelliccioni M
- Pelliccioni M
- Perazzo A
- Perez A
- Perl M
- Perl M
- Peruzzi IM
- Petersen BA
- Petrella A
- Petzold A
- Piccolo M
- Piemontese L
- Pierini M
- Piredda G
- Playfer S
- Poireau V
- Porter FC
- Posocco M
- Prasad V
- Prell S
- Prencipe E
- Prendki J
- Prepost R
- Prepost R
- Puccio EMT
- Pulliam T
- Pulliam T
- Purohit MV
- Rahmat R
- Rakitin AY
- Rama M
- Randle-Conde A
- Ratcliff BN
- Ratcliff BN
- Raven G
- Renga F
- Richman JD
- Ritchie JL
- Ritchie JL
- Rizzo G
- Roberts DA
- Robertson SH
- Robutti E
- Roney JM
- Roney JM
- Roodman A
- Roodman A
- Rosenberg EI
- Rossi A
- Rotondo M
- Roudeau P
- Rubin AE
- Ruland AM
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- Sacco R
- Saeed MA
- Saeed MA
- Salnikov AA
- Salnikov AA
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- Schalk T
- Schilling CJ
- Schilling CJ
- Schindler RH
- Schindler RH
- Schram M
- Schroeder H
- Schroeder T
- Schubert KR
- Schumm BA
- Schune MH
- Schwiening J
- Schwiening J
- Schwierz R
- Schwitters RF
- Schwitters RF
- Sciacca C
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- Seiden A
- Sekula SJ
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- Skovpen YI
- Smith AJS
- Smith JG
- Snoek HL
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- Snyder A
- Sobie RJ
- Sobie RJ
- Soffer A
- Sokoloff MD
- Solodov EP
- Sonnek P
- Sordini V
- Spaan B
- Spanier SM
- Spanier SM
- Stocchi A
- Stoker DP
- Stracka S
- Stroili R
- Strom D
- Strube J
- Stugu B
- Su D
- Su D
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- Summers DJ
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- Suzuki K
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- Taras P
- Telnov AV
- Thompson JM
- Thompson JM
- Tibbetts M
- Tico JG
- Tisserand V
- Todyshev KY
- Toki WH
- Torrence E
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- Tuggle JM
- Uwer U
- Va'vra J
- Va'vra J
- Vasseur G
- Verderi M
- Vitale L
- Vitale L
- Vitug GM
- Volk A
- Vuosalo CO
- Wacker K
- Wagner AP
- Wagner AP
- Wagner SR
- Waldi R
- Walsh JJ
- Wang L
- Wang WF
- Wappler FR
- Watson AT
- Watson JE
- Weaver M
- Weaver M
- West C
- West CA
- White RM
- Wilden L
- Wilson FF
- Wilson JR
- Wilson P
- Winer BL
- Winstrom LO
- Wisniewski WJ
- Wisniewski WJ
- Wittgen M
- Wittgen M
- Wittich P
- Wolbers S
- Wolfe H
- Wormser G
- Wray BC
- Wren AC
- Wright DH
- Wright DH
- Wright DM
- Wright T
- Wu SL
- Wu SL
- Wu X
- Wu Z
- Wulsin HW
- Yamamoto K
- Yamato D
- Yang T
- Yang UK
- Yang YC
- Yao WM
- Yarritu AK
- Yarritu AK
- Ye S
- Yeche C
- Yeh GP
- Yi K
- Yi K
- Yoh J
- Yorita K
- Yoshida T
- Young CC
- Young CC
- Yu GB
- Yu I
- Yu SS
- Yun JC
- Yushkov AN
- Zain SB
- Zain SB
- Zallo A
- Zanetti A
- Zeng Y
- Zhao M
- Zhou C
- Ziegler V
- Ziegler V
- Zito M
- Zucchelli S
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 15/08/2009
- Field of study
We present a study of ten B-meson decays to a D(*), a proton-antiproton pair,
and a system of up to two pions using BaBar's data set of 455x10^6 BBbar pairs.
Four of the modes (B0bar -> D0 p anti-p, B0bar -> D*0 p anti-p, B0bar -> D+ p
anti-p pi-, B0bar -> D*+ p anti-p pi-) are studied with improved statistics
compared to previous measurements; six of the modes (B- -> D0 p anti-p pi-, B-
-> D*0 p anti-p pi-, B0bar -> D0 p anti-p pi- pi+, B0bar -> D*0 p anti-p pi-
pi+, B- -> D+ p anti-p pi- pi-, B- -> D*+ p anti-p pi- pi-) are first
observations. The branching fractions for 3- and 5-body decays are suppressed
compared to 4-body decays. Kinematic distributions for 3-body decays show
non-overlapping threshold enhancements in m(p anti-p) and m(D(*)0 p) in the
Dalitz plots. For 4-body decays, m(p pi-) mass projections show a narrow peak
with mass and full width of (1497.4 +- 3.0 +- 0.9) MeV/c2, and (47 +- 12 +- 4)
MeV/c2, respectively, where the first (second) errors are statistical
(systematic). For 5-body decays, mass projections are similar to phase space
expectations. All results are preliminary.Comment: 28 pages, 90 postscript figures, submitted to LP0
Search for high-mass resonances decaying to dilepton final states in pp collisions at sâ=7 TeV with the ATLAS detector
- Author
- Aad G
- Abajyan T
- Abbott B
- Abdallah J
- 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
- Aharrouche M
- Ahlen SP
- Ahles R
- Ahmad A
- Ahsan M
- Aielli G
- Akesson TPA
- Akimoto G
- Akimov AV
- 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
- Allbrooke BMM
- 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
- 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
- Arce ATH
- Arfaoui S
- Arguin J-F
- Argyropoulos S
- Arik E
- Arik M
- Armbruster AJ
- Arnaez O
- Arnal V
- Arnault C
- 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
- Avramidou R
- Axen D
- Azuelos G
- Azuma Y
- Baak MA
- Baccaglioni G
- Bacci C
- Bach AM
- Bachacou H
- Bachas K
- Backes M
- Backhaus M
- Badescu E
- Bagnaia P
- Bahinipati S
- Bai Y
- Bailey DC
- Bain T
- Baines JT
- Baker MD
- Baker OK
- Baker S
- Balek P
- Banas E
- Banerjee P
- Banerjee S
- Banfi D
- Bangert A
- Bansal V
- Bansil HS
- Barajas CAC
- Barak L
- Baranov SP
- Barber T
- Barberio EL
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- Zhemchugov A
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- Zobernig G
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- zur Nedden M
- Zutshi V
- Zwalinski L
- Publication venue
- Springer
- Publication date
- 23/11/2012
- 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 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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- Zerwas D
- della Porta GZ
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- Zhemchugov A
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- Zibell A
- Zieminska D
- Zimin NI
- Zimmermann R
- Zimmermann S
- 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 fbâ1 of sâ=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 ÎČ < 40
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
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- Aleksandrov IN
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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
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