1,100 research outputs found
Strong interface-induced spin-orbit coupling in graphene on WS2
- Author
- Agashe K
- Aielli G
- Amsler C
- Anderson J
- Antonelli M
- Asner DM
- Baer H
- Banerjee Sw
- Barnett RM
- Basaglia T
- Bauer CW
- Beatty JJ
- Belousov VI
- Beringer J
- Bethke S
- Bichsel H
- Biebel O
- Blucher E
- Brooijmans G
- Buchmueller O
- Burkert V
- Bychkov MA
- Cahn RN
- Carena M
- Ceccucci A
- Cerri A
- Chakraborty D
- Chen M-C
- Chivukula RS
- Copic K
- Cowan G
- D'Ambrosio G
- D'Onofrio M
- Dahl O
- Damour T
- de Florian D
- de Gouvea A
- de Jong P
- DeGrand T
- Dissertori G
- Dobrescu BA
- Doser M
- Drees M
- Dreiner HK
- Dwyer DA
- Eerola P
- Eidelman S
- Ellis J
- Erler J
- Ezhela VV
- Fetscher W
- Fields BD
- Foster B
- Freitas A
- Gallagher H
- Garren L
- Gerber H-J
- Gerbier G
- Gershon T
- Gherghetta T
- Godizov AA
- Goodman M
- Grab C
- Griso S Pagan
- Gritsan AV
- Grojean C
- Groom DE
- Grp Particle Data
- Gruenewald M
- Gurtu A
- Gutsche T
- Haber HE
- Hagiwara K
- Hanhart C
- Harper G
- Hashimoto S
- Hayato Y
- Hayes KG
- Hebecker A
- Heltsley B
- Hernandez-Rey JJ
- Hikasa K
- Hisano J
- Hoecker A
- Holder J
- Holtkamp A
- Huston J
- Hyodo T
- Irwin K
- Jackson JD
- Johnson KF
- Kado M
- Karliner M
- Katz UF
- Klein SR
- Klempt E
- Kowalewski RV
- Krauss F
- Kreps M
- Krusche B
- Kuyanov Yu V
- Kwon Y
- Lahav O
- Laiho J
- Langacker P
- Liddle A
- Ligeti Z
- Lin C-J
- Lippmann C
- Liss TM
- Littenberg L
- Lugovsky KS
- Lugovsky SB
- Lugovsky VS
- Lusiani A
- Makida Y
- Maltoni F
- Mannel T
- Manohar AV
- Marciano WJ
- Martin AD
- Masoni A
- Matthews J
- Meissner U-G
- Milstead D
- Mitchell RE
- Molaro P
- Monig K
- Moortgat F
- Mortonson MJ
- Murayama H
- Nakamura K
- Narain M
- Nason P
- Navas S
- Neubert M
- Nevski P
- Nir Y
- Olive KA
- Parsons J
- Patrignani C
- Peacock JA
- Pennington M
- Petcov ST
- Petrov VA
- Piepke A
- Pomarol A
- Quadt A
- Raby S
- Rademacker J
- Raffelt G
- Ratcliff BN
- Richardson P
- Ringwald A
- Roesler S
- Rolli S
- Romaniouk A
- Rosenberg LJ
- Rosner JL
- Rybka G
- Ryutin RA
- Sachrajda CT
- Sakai Y
- Salam GP
- Sarkar S
- Sauli F
- Schaffner P
- Schneider O
- Scholberg K
- Schwartz AJ
- Scott D
- Sharma V
- Sharpe SR
- Shutt T
- Silari M
- Sjostrand T
- Skands P
- Skwarnicki T
- Smith JG
- Smoot GF
- Spanier S
- Spieler H
- Spiering C
- Stahl A
- Stone SL
- Sumino Y
- Sumiyoshi T
- Syphers MJ
- Takahashi F
- Tanabashi M
- Terashi K
- Terning J
- Thorne RS
- Tiator L
- Titov M
- Tkachenko NP
- Tornqvist NA
- Tovey D
- Valencia G
- Van de Water R
- Varelas N
- Venanzoni G
- Vincter MG
- Vogel P
- Vogt A
- Wakely SP
- Walkowiak W
- Walter CW
- Wands D
- Ward DR
- Wascko MO
- Weiglein G
- Weinberg DH
- Weinberg EJ
- White M
- Wiencke LR
- Wiliocq S
- Wohl CC
- Wolfenstein L
- Womersley J
- Woody CL
- Workman RL
- Yao W-M
- Zeller GP
- Zenin OV
- Zhu R-Y
- Zimmermann F
- Zyla PA
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2015
- Field of study
Interfacial interactions allow the electronic properties of graphene to be
modified, as recently demonstrated by the appearance of satellite Dirac cones
in the band structure of graphene on hexagonal boron nitride (hBN) substrates.
Ongoing research strives to explore interfacial interactions in a broader class
of materials in order to engineer targeted electronic properties. Here we show
that at an interface with a tungsten disulfide (WS2) substrate, the strength of
the spin-orbit interaction (SOI) in graphene is very strongly enhanced. The
induced SOI leads to a pronounced low-temperature weak anti-localization (WAL)
effect, from which we determine the spin-relaxation time. We find that
spin-relaxation time in graphene is two-to-three orders of magnitude smaller on
WS2 than on SiO2 or hBN, and that it is comparable to the intervalley
scattering time. To interpret our findings we have performed first-principle
electronic structure calculations, which both confirm that carriers in
graphene-on-WS2 experience a strong SOI and allow us to extract a
spin-dependent low-energy effective Hamiltonian. Our analysis further shows
that the use of WS2 substrates opens a possible new route to access topological
states of matter in graphene-based systems.Comment: Originally submitted version in compliance with editorial guidelines.
Final version with expanded discussion of the relation between theory and
experiments to be published in Nature Communication
Studying the Underlying Event in Drell-Yan and High Transverse Momentum Jet Production at the Tevatron
- Author
- Aaltonen T
- Adelman J
- Almenar CC
- Amerio S
- Amidei D
- Anastassov A
- Annovi A
- Antos J
- Apollinari G
- Apresyan A
- Arisawa T
- Artikov A
- Asaadi J
- Ashmanskas W
- Attal A
- Aurisano A
- Azfar F
- Badgett W
- Barbaro-Galtieri A
- Barnes VE
- Barnett BA
- Barria P
- Bartos P
- Bauer G
- Beauchemin PH
- Bedeschi F
- Beecher D
- Behari S
- Bellettini G
- Bellinger J
- Benjamin D
- Beretvas A
- Berge D
- Bhatti A
- Binkley M
- Bisello D
- Bizjak I
- Blair RE
- Blocker C
- Blumenfeld B
- Bocci A
- Bodek A
- Boisvert V
- Bortoletto D
- Boudreau J
- Boveia A
- Brau B
- Bridgeman A
- Brigliadori L
- Bromberg C
- Brubaker E
- Budagov J
- Budd HS
- Budd S
- Burkett K
- Busetto G
- Bussey P
- Buzatu A
- Byrum KL
- Cabrera S
- Calancha C
- Camarda S
- Campanelli M
- Campbell M
- Canelli F
- Canepa A
- Carls B
- Carlsmith D
- Carosi R
- Carrillo S
- Carron S
- Casal B
- Casarsa M
- Castro A
- Catastini P
- Cauz D
- Cavaliere V
- Cavalli-Sforza M
- Cerri A
- Cerrito L
- Chang SH
- Chen YC
- Chertok M
- Chiarelli G
- Chlachidze G
- Chlebana F
- Cho K
- Chokheli D
- Chou JP
- Chung K
- Chung WH
- Chung YS
- Chwalek T
- Ciobanu CI
- Ciocci MA
- Clark A
- Clark D
- Compostella G
- Convery ME
- Conway J
- Corbo M
- Cordelli M
- Cox CA
- Cox DJ
- Crescioli F
- Cuevas J
- Culbertson R
- Cully JC
- d'Errico M
- D'Onofrio M
- da Costa JG
- Dagenhart D
- Datta M
- Davies T
- de Barbaro P
- De Cecco S
- De Lorenzo G
- Deisher A
- Dell'Orso M
- della Porta G. Zevi
- Deluca C
- Demortier L
- Deng J
- Deninno M
- Denis RS
- Di Canto A
- di Giovanni GP
- Di Ruzza B
- Dittmann JR
- Donati S
- Dong P
- Dorigo T
- Dube S
- Ebina K
- Elagin A
- Erbacher R
- Errede D
- Errede S
- Ershaidat N
- Eusebi R
- Fang HC
- Farrington S
- Fedorko WT
- Feild RG
- Feindt M
- Fernandez JP
- Fernandez PM
- Ferrazza C
- Field R
- Flanagan G
- Forrest R
- Frank MJ
- Franklin M
- Freeman JC
- Furic I
- Gallinaro M
- Galyardt J
- Garberson F
- Garcia JE
- Garfinkel AF
- Garosi P
- Gerberich H
- Gerdes D
- Gessler A
- Giagu S
- Giakoumopoulou V
- Giannetti P
- Gibson K
- Gimmell JL
- Ginsburg CM
- Giokaris N
- Giordani M
- Giromini P
- Giunta M
- Giurgiu G
- Glagolev V
- Glenzinski D
- Gold M
- Goldschmidt N
- Golossanov A
- Gomez G
- Gomez-Ceballos G
- Goncharov M
- Gonzalez BA
- Gonzalez O
- Gorelov I
- Goshaw AT
- Goulianos K
- Gresele A
- Grinstein S
- Griso SP
- Grosso-Pilcher C
- Group RC
- Grundler U
- Gunay-Unalan Z
- Haber C
- Hahn SR
- Halkiadakis E
- Han BY
- Han JY
- Happacher F
- Hara K
- Hare D
- Hare M
- Harr RF
- Hartz M
- Hatakeyama K
- Hays C
- Heck M
- Heinrich J
- Herndon M
- Heuser J
- Hewamanage S
- Hickman M
- Hidas D
- Hill CS
- Hirschbuehl D
- Hocker A
- Hou S
- Houlden M
- Hsu SC
- Hughes RE
- Hurwitz M
- Husemann U
- Hussein M
- Huston J
- Incandela J
- Introzzi G
- Iori M
- Ivanov A
- James E
- Jang D
- Jayatilaka B
- Jeon EJ
- Jha MK
- Jindariani S
- Johnson W
- Jones M
- Joo KK
- Jun SY
- Jung JE
- Junk TR
- Kamon T
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- Kato Y
- Kephart R
- Ketchum W
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- Kim MJ
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- Oh YD
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- Okusawa T
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- Papadimitriou V
- Papaikonomou A
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- Potamianos K
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- Pursley J
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- Redondo I
- Renton P
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- Rescigno M
- Richter S
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- Safonov A
- Sakumoto WK
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- Savoy-Navarro A
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- Scribano A
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- Tsai SY
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- van Remortel N
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- Vataga E
- Vazquez F
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- Volpi G
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- Wakisaka T
- Wallny R
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- Waters D
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- Weinelt J
- Wester WC
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- Wicklund AB
- Wicklund E
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- Williams G
- Williams HH
- Wilson MG
- Wilson P
- Winer BL
- Wittich P
- Wolbers S
- Wolfe C
- Wolfe H
- Wright T
- Wu X
- Wurthwein F
- Yagil A
- Yamamoto K
- Yamaoka J
- Yang UK
- Yang YC
- Yao WM
- Yeh GP
- Yi K
- Yilmaz M.
- Yoh J
- Yoosoofmiya R.
- Yorita K
- Yorita K.
- Yoshida R.
- Yoshida T
- Young C.
- Youssef S.
- Yu D.
- Yu GB
- Yu I
- Yu J.
- Yu J.
- Yu SS
- Yuan L.
- Yun JC
- Yurkewicz A.
- Zaets V. G.
- Zaidan R.
- Zaitsev A. M.
- Zajacova Z.
- Zalite Yo. K.
- Zanello L.
- Zanetti A
- Zarzhitsky P.
- Zaytsev A.
- Zdrazil M.
- Zeitnitz C.
- Zeller M.
- Zema P. F.
- Zemla A.
- Zendler C.
- Zeng Y
- Zenin A. V.
- Zenin O.
- Zenis T.
- Zenonos Z.
- Zenz S.
- Zerwas D.
- Zhan Z.
- Zhang D.
- Zhang H.
- Zhang J.
- Zhang X
- Zhang X.
- Zhang Z.
- Zhao L.
- Zhao T.
- Zhao Z.
- Zhemchugov A.
- Zheng S.
- Zheng Y
- Zhong J.
- Zhou B.
- Zhou N.
- Zhou Y.
- Zhu C. G.
- Zhu H.
- Zhu Y.
- Zhuang X.
- Zhuravlov V.
- Zieminska D.
- Zilka B.
- Zimmermann R.
- Zimmermann S.
- Zimmermann S.
- Ziolkowski M.
- Zitoun R.
- Zivkovic L.
- Zmouchko V. V.
- Zobernig G.
- Zoccoli A.
- Zolnierowski Y.
- Zsenei A.
- Zucchelli Se S.
- zur Nedden M.
- Zutshi V.
- Zwalinski L.
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2010
- Field of study
We study the underlying event in proton-antiproton collisions by examining
the behavior of charged particles (transverse momentum pT > 0.5 GeV/c,
pseudorapidity |\eta| < 1) produced in association with large transverse
momentum jets (~2.2 fb-1) or with Drell-Yan lepton-pairs (~2.7 fb-1) in the
Z-boson mass region (70 < M(pair) < 110 GeV/c2) as measured by CDF at 1.96 TeV
center-of-mass energy. We use the direction of the lepton-pair (in Drell-Yan
production) or the leading jet (in high-pT jet production) in each event to
define three regions of \eta-\phi space; toward, away, and transverse, where
\phi is the azimuthal scattering angle. For Drell-Yan production (excluding the
leptons) both the toward and transverse regions are very sensitive to the
underlying event. In high-pT jet production the transverse region is very
sensitive to the underlying event and is separated into a MAX and MIN
transverse region, which helps separate the hard component (initial and
final-state radiation) from the beam-beam remnant and multiple parton
interaction components of the scattering. The data are corrected to the
particle level to remove detector effects and are then compared with several
QCD Monte-Carlo models. The goal of this analysis is to provide data that can
be used to test and improve the QCD Monte-Carlo models of the underlying event
that are used to simulate hadron-hadron collisions.Comment: Submitted to Phys.Rev.
Observation of the Baryonic Flavor-Changing Neutral Current Decay Lambda_b -> Lambda mu+ mu-
- Author
- Aaltonen T
- Almenar CC
- Amerio S
- Amidei D
- Anastassov A
- Annovi A
- Antos J
- Apollinari G
- Appel JA
- Apresyan A
- Arisawa T
- Artikov A
- Asaadi J
- Ashmanskas W
- Auerbach B
- Aurisano A
- Azfar F
- Badgett W
- Barbaro-Galtieri A
- Barnes VE
- Barnett BA
- Barria P
- Bartos P
- Bauce M
- Bauer G
- Bedeschi F
- Beecher D
- Behari S
- Bellettini G
- Bellinger J
- Benjamin D
- Beretvas A
- Bhatti A
- Binkley M
- Bisello D
- Bizjak I
- Bland KR
- Blocker C
- Blumenfeld B
- Bocci A
- Bodek A
- Bortoletto D
- Boudreau J
- Boveia A
- Brau B
- Brigliadori L
- Brisuda A
- Bromberg C
- Brucken E
- Bucciantonio M
- Budagov J
- Budd HS
- Budd S
- Burkett K
- Busetto G
- Bussey P
- Buzatu A
- Cabrera S
- Calancha C
- Camarda S
- Campanelli M
- Campbell M
- Canelli F
- Canepa A
- Carls B
- Carlsmith D
- Carosi R
- Carrillo S
- Carron S
- Casal B
- Casarsa M
- Castro A
- Catastini P
- Cauz D
- Cavaliere V
- Cavalli-Sforza M
- Cerri A
- Cerrito L
- Chen YC
- Chertok M
- Chiarelli G
- Chlachidze G
- Chlebana F
- Cho K
- Chokheli D
- Chou JP
- Chung WH
- Chung YS
- Ciobanu CI
- Ciocci MA
- Clark A
- Clark D
- Compostella G
- Convery ME
- Conway J
- Corbo M
- Cordelli M
- Cox CA
- Cox DJ
- Crescioli F
- Cuevas J
- Culbertson R
- d'Ascenzo N
- d'Errico M
- D'Onofrio M
- da Costa JG
- Dagenhart D
- Datta M
- De Barbaro P
- De Cecco S
- De Lorenzo G
- Dell'Orso M
- Deluca C
- Demortier L
- Deng J
- Deninno M
- Denis RS
- Devoto F
- Di Canto A
- Di Ruzza B
- Dittmann JR
- Donati S
- Dong P
- Dorigo T
- Ebina K
- Elagin A
- Eppig A
- Erbacher R
- Errede D
- Errede S
- Ershaidat N
- Eusebi R
- Fang HC
- Farrington S
- Feindt M
- Fernandez JP
- Fernandez P. Movilla
- Fernandez PM
- Ferrazza C
- Field R
- Flanagan G
- Forrest R
- Frank MJ
- Franklin M
- Freeman JC
- Furic I
- Gallinaro M
- Galyardt J
- Garcia JE
- Garfinkel AF
- Garosi P
- Gerberich H
- Gerchtein E
- Giagu S
- Giakoumopoulou V
- Giannetti P
- Gibson K
- Ginsburg CM
- Giokaris N
- Giromini P
- Giunta M
- 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
- Gresele A
- Grinstein S
- Griso S. Pagan
- Griso SP
- Grosso-Pilcher C
- Group RC
- Gunay-Unalan Z
- Haber C
- Hahn SR
- Halkiadakis E
- Hamaguchi A
- Han JY
- Happacher F
- Hara K
- Hare D
- Hare M
- Harr RF
- Hatakeyama K
- Hays C
- Heck M
- Heinrich J
- Herndon M
- Hewamanage S
- Hidas D
- Hocker A
- Hopkins W
- Horn D
- Hou S
- Hughes RE
- Hurwitz M
- Husemann U
- Hussain N
- Hussein M
- Huston J
- Introzzi G
- Iori M
- Ivanov A
- James E
- Jang D
- Jayatilaka B
- Jeon EJ
- Jha MK
- Jindariani S
- Johnson W
- Jones M
- Jonsson P.
- Joo K. K.
- Joo KK
- Jun S. Y.
- Jun SY
- Jung J. E.
- Junk T. R.
- Junk TR
- Juste A.
- Kaadze K.
- Kajfasz E.
- Kamon T
- Kamon T.
- Kar D.
- Karchin P. E.
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- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2011
- Field of study
We report the first observation of the baryonic flavor-changing neutral
current decay Lambda_b -> Lambda mu+ mu- with 24 signal events and a
statistical significance of 5.8 Gaussian standard deviations. This measurement
uses ppbar collisions data sample corresponding to 6.8fb-1 at sqrt{s}=1.96TeV
collected by the CDF II detector at the Tevatron collider. The total and
differential branching ratios for Lambda_b -> Lambda mu+ mu- are measured. We
find B(Lambda_b -> Lambda mu+ mu-) = [1.73+-0.42(stat)+-0.55(syst)] x 10^{-6}.
We also report the first measurement of the differential branching ratio of B_s
-> phi mu+ mu- using 49 signal events. In addition, we report branching ratios
for B+ -> K+ mu+ mu-, B0 -> K0 mu+ mu-, and B -> K*(892) mu+ mu- decays.Comment: 8 pages, 2 figures, 4 tables. Submitted to Phys. Rev. Let
Measurement of Lifetime and Decay-Width Difference in B0s -> J/psi phi Decays
- Author
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- Orava R
- Osterberg K
- Pagliarone C
- Palencia E
- Papadimitriou V
- Papaikonomou A
- Paramonov AA
- Parks B
- Pashapour S
- Patrick J
- Pauletta G
- Paulini M
- Paus C
- Pellett DE
- Penzo A
- Phillips TJ
- Piacentino G
- Piedra J
- Pinera L
- Pitts K
- Plager C
- Pondrom L
- Portell X
- Poukhov O
- Pounder N
- Prakoshyn F
- Pronko A
- Proudfoot J
- Ptohos F
- Punzi G
- Pursley J
- Rademacker J
- Rahaman A
- Ramakrishnan V
- Ranjan N
- Redondo I
- Reisert B
- Rekovic V
- Renton P
- Rescigno M
- Richter S
- Rimondi F
- Ristori L
- Robson A
- Rodrigo T
- Rogers E
- Rolli S
- Roser R
- Rossi M
- Rossin R
- Roy P
- Ruiz A
- Russ J
- Rusu V
- Saarikko H
- Safonov A
- Sakumoto WK
- Salamanna G
- Salto O
- Santi L
- Sarkar S
- Sartori L
- Sato K
- Savard P
- Savoy-Navarro A
- Scheidle T
- Schlabach P
- Schmidt EE
- Schmidt MA
- Schmidt MP
- Schmitt M
- Schwarz T
- Scodellaro L
- Scott AL
- Scribano A
- Scuri F
- Sedov A
- Seidel S
- Seiya Y
- Semenov A
- Sexton-Kennedy L
- Sfyrla A
- Shalhout SZ
- Shapiro MD
- Shears T
- Shepard PF
- Sherman D
- Shimojima M
- Shochet M
- Shon Y
- Shreyber I
- Sidoti A
- Sinervo P
- Sisakyan A
- Slaughter AJ
- Slaunwhite J
- Sliwa K
- Smith JR
- Snider FD
- Snihur R
- Soderberg M
- Soha A
- Somalwar S
- Sorin V
- Spalding J
- Spinella F
- Spreitzer T
- Squillacioti P
- Stanitzki M
- Stelzer B
- Stelzer-Chilton O
- Stentz D
- Strologas J
- Stuart D
- Suh JS
- Sukhanov A
- Sun H
- Suslov I
- Suzuki T
- Taffard A
- Takashima R
- Takeuchi Y
- Tanaka R
- Tecchio M
- Teng PK
- Terashi K
- Thom J
- Thompson AS
- Thompson GA
- Thomson E
- Tipton P
- Tiwari V
- Tkaczyk S
- Toback D
- Tokar S
- Tollefson K
- Tomura T
- Tonelli D
- Torre S
- Torretta D
- Tourneur S
- Trischuk W
- Tu Y
- Turini N
- Ukegawa F
- Uozumi S
- Vallecorsa S
- van Remortel N
- Varganov A
- Vataga E
- Vazquez F
- Velev G
- Vellidis C
- Veszpremi V
- Vidal M
- Vidal R
- Vila I
- Vilar R
- Vine T
- Vogel M
- Volobouev I
- Volpi G
- Wagner J
- Wagner P
- Wagner RG
- Wagner RL
- Wagner W
- Wakisaka T
- Wallny R
- Wang SM
- Warburton A
- Waters D
- Weinberger M
- Wester WC
- Whitehouse B
- Whiteson D
- Wicklund AB
- Wicklund E
- Williams G
- Williams HH
- Wilson P
- Winer BL
- Wittich P
- Wolbers S
- Wolfe C
- Wright T
- Wu X
- Wurthwein F
- Wynne SM
- Yagil A
- Yamamoto K
- Yamaoka J
- Yamashita T
- Yang C
- Yang UK
- Yang YC
- Yao WM
- Yeh GP
- Yoh J
- Yorita K
- Yoshida T
- Yu GB
- Yu I
- Yu SS
- Yun JC
- Zanello L
- Zanetti A
- Zaw I
- Zaw I
- Zhang X
- Zhang X
- Zheng Y
- Zheng Y
- Zucchelli S S
- Zucchelli Sanetti A
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2007
- Field of study
We measure the mean lifetime, tau=2/(Gamma_L+Gamma_H), and the width
difference, DeltaGamma=Gamma_L-Gamma_H, of the light and heavy mass eigenstates
of the B0s meson, B0sL and B0sH, in B0s -> J/psi phi decays using 1.7 fb^-1 of
data collected with the CDF II detector at the Fermilab Tevatron ppbar
collider. Assuming CP conservation, a good approximation for the B0s system in
the Standard Model, we obtain DeltaGamma = 0.076^+0.059_-0.063 (stat.) +- 0.006
(syst.) ps^-1 and tau = 1.52 +- 0.04 (stat.) +- 0.02 (syst.) ps, the most
precise measurements to date. Our constraints on the weak phase and DeltaGamma
are consistent with CP conservation.
Dedicated to the memory of our dear friend and colleague, Michael P. Schmid
Forward-Backward Asymmetry in Top Quark Production in ppbar Collisions at sqrt{s}=1.96 TeV
- Author
- Aaltonen T
- Adelman J
- Akimoto T
- Albrow MG
- Almenar CC
- Amerio S
- Amidei D
- Anastassov A
- Annovi A
- Antos J
- Apollinari G
- Apresyan A
- Arisawa T
- Artikov A
- Ashmanskas W
- Attal A
- Aurisano A
- Azfar F
- Azzurri P
- Badgett W
- Barbaro P
- Barbaro-Galtieri A
- Barnes VE
- Barnett BA
- Bartsch V
- Bauer G
- Beauchemin PH
- Bedeschi F
- Bednar P
- Beecher D
- Behari S
- Bellettini G
- Bellinger J
- Benjamin D
- Beretvas A
- Beringer J
- Bhatti A
- Binkley M
- Bisello D
- Bizjak I
- Blair RE
- Blocker C
- Blumenfeld B
- Bocci A
- Bodek A
- Boisvert V
- Bolla G
- Bortoletto D
- Boudreau J
- Boveia A
- Brau B
- Bridgeman A
- Brigliadori L
- Bromberg C
- Brubaker E
- Budagov J
- Budd HS
- Budd S
- Burkett K
- Busetto G
- Bussey P
- Buzatu A
- Byrum KL
- Cabrera S
- Calancha C
- Campanelli M
- Campbell M
- Canelli F
- Canepa A
- Carlsmith D
- Carosi R
- Carrillo S
- Carron S
- Casal B
- Casarsa M
- Castro A
- Catastini P
- Cauz D
- Cavaliere V
- Cavalli-Sforza M
- Cecco S
- Cerri A
- Cerrito L
- Chang SH
- Chen YC
- Chertok M
- Chiarelli G
- Chlachidze G
- Chlebana F
- Cho K
- Chokheli D
- Chou JP
- Choudalakis G
- Chuang SH
- Chung K
- Chung WH
- Chung YS
- Chwalek T
- Ciobanu CI
- Ciocci MA
- Clark A
- Clark D
- Compostella G
- Convery ME
- Conway J
- Copic K
- Cordelli M
- Cortiana G
- Cox DJ
- Crescioli F
- Cuevas J
- Culbertson R
- Cully JC
- D'Onofrio M
- da Costa JG
- Dagenhart D
- Datta M
- Davies T
- Deisher A
- Dell'Orso M
- Deluca C
- Demortier L
- Deng J
- Deninno M
- Denis RS
- Derwent PF
- Dionisi C
- Dittmann JR
- Donati S
- Dong P
- Donini J
- Dorigo T
- Dube S
- Efron J
- Elagin A
- Erbacher R
- Errede D
- Errede S
- Eusebi R
- Fang HC
- Farrington S
- Fedorko WT
- Feild RG
- Feindt M
- Fernandez JP
- Fernandez PM
- Ferrazza C
- Field R
- Flanagan G
- Forrest R
- Franklin M
- Freeman JC
- Furic I
- Gallinaro M
- Galyardt J
- Garberson F
- Garcia JE
- Garfinkel AF
- Genser K
- Gerberich H
- Gerdes D
- Gessler A
- Giagu S
- Giakoumopoulou V
- Giannetti P
- Gibson K
- Gimmell JL
- Ginsburg CM
- Giokaris N
- Giordani M
- Giovanni GP
- Giromini P
- Giunta M
- Giurgiu G
- Glagolev V
- Glenzinski D
- Gold M
- Goldschmidt N
- Golossanov A
- Gomez G
- Gomez-Ceballos G
- Goncharov M
- Gonzalez BA
- Gonzalez O
- Gorelov I
- Goshaw AT
- Goulianos K
- Gresele A
- Grinstein S
- Griso SP
- Grosso-Pilcher C
- Group RC
- Grundler U
- Gunay-Unalan Z
- Haber C
- Hahn K
- Hahn SR
- Halkiadakis E
- Han BY
- Han JY
- Handler R
- Happacher F
- Hara K
- Hare D
- Hare M
- Harper S
- Harr RF
- Harris RM
- Hartz M
- Hatakeyama K
- Hauser J
- Hays C
- Heck M
- Heijboer A
- Heinemann B
- Heinrich J
- Henderson C
- Herndon M
- Heuser J
- Hewamanage S
- Hidas D
- Hill CS
- Hirschbuehl D
- Hocker A
- Hou S
- Houlden M
- Hsu SC
- Huffman BT
- Hughes RE
- Husemann U
- Huston J
- Incandela J
- Introzzi G
- Iori M
- Ivanov A
- James E
- Jayatilaka B
- Jeon EJ
- Jha MK
- Jindariani S
- Johnson W
- Jones M
- Joo KK
- Jun SY
- Jung JE
- Junk TR
- Kamon T
- Kar D
- Karchin PE
- Kato Y
- Kephart R
- Keung J
- Khotilovich V
- Kilminster B
- Kim DH
- Kim HS
- Kim JE
- Kim MJ
- Kim SB
- Kim SH
- Kim YK
- Kimura N
- Kirsch L
- Klimenko S
- Knuteson B
- Ko BR
- Koay SA
- Kondo K
- Kong DJ
- Konigsberg J
- Korytov A
- Kotwal AV
- Kreps M
- Kroll J
- Krop D
- Krumnack N
- Kruse M
- Krutelyov V
- Kubo T
- Kuhr T
- Kulkarni NP
- Kurata M
- Kusakabe Y
- Kwang S
- Laasanen AT
- Lami S
- Lammel S
- Lancaster M
- Lander RL
- Lannon K
- Lath A
- Latino G
- Lazzizzera I
- LeCompte T
- Lee E
- Lee SW
- Leone S
- Lewis JD
- Lin CS
- Linacre J
- Lindgren M
- Lipeles E
- Lister A
- Litvintsev DO
- Liu C
- Liu T
- Lockyer NS
- Loginov A
- Lorenzo G
- Loreti M
- Lovas L
- Lu RS
- Lucchesi D
- Luci C
- Lueck J
- Lujan P
- Lukens P
- Lungu G
- Lyons L
- Lys J
- Lysak R
- Lytken E
- Mack P
- MacQueen D
- Madrak R
- Maeshima K
- Makhoul K
- Maki T
- Maksimovic P
- Malde S
- Malik S
- Manca G
- Manousakis-Katsikakis A
- Margaroli F
- Marino C
- Marino CP
- Martin A
- Martin V
- Martinez M
- Martinez-Ballarin R
- Maruyama T
- Mastrandrea P
- Masubuchi T
- Mattson ME
- Mazzanti P
- McFarland KS
- McIntyre P
- McNulty R
- Mehta A
- Mehtala P
- Menzione A
- Merkel P
- Mesropian C
- Miao T
- Miladinovic N
- Miller R
- Mills C
- Milnik M
- Mitra A
- Mitselmakher G
- Miyake H
- Moggi N
- Moon CS
- Moore R
- Morello MJ
- Morlok J
- Mukherjee A
- Muller T
- Mulmenstadt J
- Mumford R
- Murat P
- Mussini M
- Nachtman J
- Nagai Y
- Nagano A
- Naganoma J
- Nakamura K
- Nakano I
- Napier A
- Necula V
- Neu C
- Neubauer MS
- Nielsen J
- Nodulman L
- Norman M
- Norniella O
- Nurse E
- Oakes L
- Oh SH
- Oh YD
- Oksuzian I
- Okusawa T
- Orava R
- Osterberg K
- Pagliarone C
- Palencia E
- Papadimitriou V
- Papaikonomou A
- Paramonov AA
- Parks B
- Pashapour S
- Patrick J
- Pauletta G
- Paulini M
- Paus C
- Peiffer T
- Pellett DE
- Penzo A
- Phillips TJ
- Piacentino G
- Pianori E
- Pinera L
- Pitts K
- Plager C
- Pondrom L
- Poukhov O
- Pounder N
- Prakoshyn F
- Pronko A
- Proudfoot J
- Ptohos F
- Pueschel E
- Punzi G
- Pursley J
- Rademacker J
- Rahaman A
- Ramakrishnan V
- Ranjan N
- Redondo I
- Reisert B
- Rekovic V
- Remortel N
- Renton P
- Rescigno M
- Richter S
- Rimondi F
- Ristori L
- Robson A
- Rodrigo T
- Rodriguez T
- Rogers E
- Rolli S
- Roser R
- Rossi M
- Rossin R
- Roy P
- Ruiz A
- Russ J
- Rusu V
- Ruzza B
- Saarikko H
- Safonov A
- Sakumoto WK
- Salto O
- Santi L
- Sarkar S
- Sartori L
- Sato K
- Savoy-Navarro A
- Scheidle T
- Schlabach P
- Schmidt A
- Schmidt EE
- Schmidt MA
- Schmidt MP
- Schmitt M
- Schwarz T
- Scodellaro L
- Scott AL
- Scribano A
- Scuri F
- Sedov A
- Seidel S
- Seiya Y
- Semenov A
- Sexton-Kennedy L
- Sfyrla A
- Shalhout SZ
- Shears T
- Shepard PF
- Sherman D
- Shimojima M
- Shiraishi S
- Shochet M
- Shon Y
- Shreyber I
- Sidoti A
- Sinervo P
- Sisakyan A
- Slaughter AJ
- Slaunwhite J
- Sliwa K
- Smith JR
- Snider FD
- Snihur R
- Soha A
- Somalwar S
- Sorin V
- Spalding J
- Spreitzer T
- Squillacioti P
- Stanitzki M
- Stelzer B
- Stelzer-Chilton O
- Stentz D
- Strologas J
- Stuart D
- Suh JS
- Sukhanov A
- Suslov I
- Suzuki T
- Taffard A
- Takashima R
- Takeuchi Y
- Tanaka R
- Tecchio M
- Teng PK
- Terashi K
- Thom J
- Thompson AS
- Thompson GA
- Thomson E
- Tipton P
- Tiwari V
- Tkaczyk S
- Toback D
- Tokar S
- Tollefson K
- Tomura T
- Tonelli D
- Torre S
- Torretta D
- Totaro P
- Tourneur S
- Tu Y
- Turini N
- Ukegawa F
- Vallecorsa S
- Varganov A
- Vataga E
- Vazquez F
- Velev G
- Vellidis C
- Veszpremi V
- Vidal M
- Vidal R
- Vila I
- Vilar R
- Vine T
- Vogel M
- Volobouev I
- Volpi G
- Wagner P
- Wagner RG
- Wagner RL
- Wagner W
- Wagner-Kuhr J
- Wakisaka T
- Wallny R
- Wang SM
- Warburton A
- Waters D
- Weinberger M
- Weinelt J
- Wester WC
- Whitehouse B
- Whiteson D
- Wicklund AB
- Wicklund E
- Williams G
- Williams HH
- Wilson P
- Winer BL
- Wittich P
- Wolbers S
- Wolfe C
- Wright T
- Wu X
- Wurthwein F
- Wynne SM
- Wynne SM
- Yagil A
- Yagil A
- Yamamoto K
- Yamamoto K
- Yamaoka J
- Yamaoka J
- Yamashita T
- Yang C
- Yang UK
- Yang UK
- Yang YC
- Yang YC
- Yao WM
- Yao WM
- Yeh GP
- Yeh GP
- Yoh J
- Yoh J
- Yorita K
- Yorita K
- Yoshida T
- Yoshida T
- Yu GB
- Yu GB
- Yu I
- Yu I
- Yu SS
- Yu SS
- Yun JC
- Yun JC
- Zanello L
- Zanello L
- Zanetti A
- Zanetti A
- Zaw I
- Zaw I
- Zhang X
- Zhang X
- Zheng Y
- Zheng Y
- Zucchelli S
- Zucchelli S Wu X
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2008
- Field of study
Reconstructable final state kinematics and charge assignment in the reaction
ppbar->ttbar allows tests of discrete strong interaction symmetries at high
energy. We define frame dependent forward-backward asymmetries for the outgoing
top quark in both the ppbar and ttbar rest frames, correct for experimental
distortions, and derive values at the parton-level. Using 1.9/fb of ppbar
collisions at sqrt{s}=1.96 TeV recorded with the CDF II detector at the
Fermilab Tevatron, we measure forward-backward top quark production asymmetries
in the ppbar and ttbar rest frames of A_{FB,pp} = 0.17 +- 0.08 and A_{FB,tt} =
0.24 +- 0.14.Comment: 7 pages, 2 figures, submitted to Phys.Rev.Lett, corrected references
and change of tex
Search for Pair Production of Scalar Top Quarks Decaying to a tau Lepton and a b Quark in ppbar Collisions at sqrt{s}=1.96 TeV
- Author
- Aaltonen T
- Adelman J
- Akimoto T
- Albrow MG
- Almenar CC
- Amerio S
- Amidei D
- Anastassov A
- Annovi A
- Antos J
- Aoki M
- Apollinari G
- Apresyan A
- Arisawa T
- Artikov A
- Ashmanskas W
- Attal A
- Aurisano A
- Azfar F
- Azzi-Bacchetta P
- Azzurri P
- Bacchetta N
- Badgett W
- Barbaro-Galtieri A
- Barnes VE
- Barnett BA
- Baroiant S
- Bartsch V
- Bauer G
- Beauchemin PH
- Bedeschi F
- Bednar P
- Behari S
- Bellettini G
- Bellinger J
- Belloni A
- Benjamin D
- Beretvas A
- Beringer J
- Berry T
- Bhatti A
- Binkley M
- Bisello D
- Bizjak I
- Blair RE
- Blocker C
- Blumenfeld B
- Bocci A
- Bodek A
- Boisvert V
- Bolla G
- Bolshov A
- Bortoletto D
- Boudreau J
- Boveia A
- Brau B
- Bridgeman A
- Brigliadori L
- Bromberg C
- Brubaker E
- Budagov J
- Budd HS
- Budd S
- Burkett K
- Busetto G
- Bussey P
- Buzatu A
- Byrum KL
- Cabrera S
- Campanelli M
- Campbell M
- Canelli F
- Canepa A
- Carlsmith D
- Carosi R
- Carrillo S
- Carron S
- Casal B
- Casarsa M
- Castro A
- Catastini P
- Cauz D
- Cavalli-Sforza M
- Cerri A
- Cerrito L
- Chang SH
- Chen YC
- Chertok M
- Chiarelli G
- Chlachidze G
- Chlebana F
- Cho K
- Chokheli D
- Chou JP
- Choudalakis G
- Chuang SH
- Chung K
- Chung WH
- Chung YS
- Ciobanu CI
- Ciocci MA
- Clark A
- Clark D
- Compostella G
- Convery ME
- Conway J
- Cooper B
- Copic K
- Cordelli M
- Cortiana G
- Crescioli F
- Cuevas J
- Culbertson R
- Cully JC
- D'Onofrio M
- Da Costa JG
- Dagenhart D
- Datta M
- Davies T
- De Barbaro P
- De Cecco S
- De Lentdecker G
- De Lorenzo G
- De Pedis D
- Deisher A
- Dell'Orso M
- Demortier L
- Deng J
- Deninno M
- Denis RS
- Derwent PF
- Di Giovanni GP
- Di Ruzza B
- Dionisi C
- Dittmann JR
- Donati S
- Dong P
- Donini J
- Dorigo T
- Dube S
- Efron J
- Erbacher R
- Errede D
- Errede S
- Eusebi R
- Fang HC
- Farrington S
- Fedorko WT
- Feild RG
- Feindt M
- Fernandez JP
- Fernandez PM
- Ferrazza C
- Field R
- Flanagan G
- Forrest R
- Forrester S
- Franklin M
- Freeman JC
- Furic I
- Gallinaro M
- Galyardt J
- Garberson F
- Garcia JE
- Garfinkel AF
- Genser K
- Gerberich H
- Gerdes D
- Giagu S
- Giakoumopolou V
- Giannetti P
- Gibson K
- Gimmell JL
- Ginsburg CM
- Giokaris N
- Giordani M
- Giromini P
- Giunta M
- Glagolev V
- Glenzinski D
- Gold M
- Goldschmidt N
- Golossanov A
- Gomez G
- Gomez-Ceballos G
- Goncharov M
- Gonzalez BA
- Gonzalez O
- Gorelov I
- Goshaw AT
- Goulianos K
- Gresele A
- Grinstein S
- Griso SP
- Grosso-Pilcher C
- Group RC
- Grundler U
- Gunay-Unalan Z
- Haber C
- Hahn K
- Hahn SR
- Halkiadakis E
- Hamilton A
- Han BY
- Han JY
- Handler R
- Happacher F
- Hara K
- Hare D
- Hare M
- Harper S
- Harr RF
- Harris RM
- Hartz M
- Hatakeyama K
- Hauser J
- Hays C
- Heck M
- Heijboer A
- Heinemann B
- Heinrich J
- Henderson C
- Herndon M
- Heuser J
- Hewamanage S
- Hidas D
- Hill CS
- Hirschbuehl D
- Hocker A
- Hou S
- Houlden M
- Hsu SC
- Huffman BT
- Hughes RE
- Husemann U
- Huston J
- Incandela J
- Introzzi G
- Iori M
- Ivanov A
- Iyutin B
- James E
- Jayatilaka B
- Jeans D
- Jeon EJ
- Jindariani S
- Johnson W
- Jones M
- Joo KK
- Jun SY
- Jung JE
- Junk TR
- Kamon T
- Kar D
- Karchin PE
- Kato Y
- Kephart R
- Kerzel U
- Khotilovich V
- Kilminster B
- Kim DH
- Kim HS
- Kim JE
- Kim MJ
- Kim SB
- Kim SH
- Kim YK
- Kimura N
- Kirsch L
- Klimenko S
- Klute M
- Knuteson B
- Ko BR
- Koay SA
- Kondo K
- Kong DJ
- Konigsberg J
- Korytov A
- Kotwal AV
- Kraus J
- Kreps M
- Kroll J
- Krumnack N
- Kruse M
- Krutelyov V
- Kubo T
- Kuhlmann SE
- Kuhr T
- Kulkarni NP
- Kusakabe Y
- Kwang S
- Laasanen AT
- Lai S
- Lami S
- Lammel S
- Lancaster M
- Lander RL
- Lannon K
- Lath A
- Latino G
- Lazzizzera I
- LeCompte T
- Lee J
- Lee J
- Lee SW
- Lee YJ
- Leonardo N
- Leone S
- Levy S
- Lewis JD
- Lin C
- Lin CS
- Linacre J
- Lindgren M
- Lipeles E
- Liss TM
- Lister A
- Litvintsev DO
- Liu T
- Lockyer NS
- Loginov A
- Loreti M
- Lovas L
- Lu RS
- Lucchesi D
- Luci C
- Lueck J
- Lujan P
- Lukens P
- Lungu G
- Lyons L
- Lys J
- Lysak R
- Lytken E
- Mack P
- MacQueen D
- Madrak R
- Maeshima K
- Makhoul K
- Maki T
- Maksimovic P
- Malde S
- Malik S
- Manca G
- Manousakis A
- Margaroli F
- Marino C
- Marino CP
- Martin A
- Martin M
- Martin V
- Martinez M
- Martinez-Ballarin R
- Maruyama T
- Mastrandrea P
- Masubuchi T
- Mattson ME
- Mazzanti P
- McFarland KS
- McIntyre P
- McNulty R
- Mehta A
- Mehtala P
- Menzemer S
- Menzione A
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- Milnik M
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- Mitselmakher G
- Miyake H
- Moed S
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- Moore R
- Morello M
- Mukherjee A
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- Mulmenstadt J
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- Prakoshyn F
- Pronko A
- Proudfoot J
- Ptohos F
- Punzi G
- Pursley J
- Rademacker J
- Rahaman A
- Ramakrishnan V
- Ranjan N
- Redondo I
- Reisert B
- Rekovic V
- Renton P
- Rescigno M
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- Saarikko H
- Safonov A
- Sakumoto WK
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- Scheidle T
- Schlabach P
- Schmidt EE
- Schmidt MA
- Schmidt MP
- Schmitt M
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- Scott AL
- Scribano A
- Scuri F
- Sedov A
- Seidel S
- Seiya Y
- Semenov A
- Sexton-Kennedy L
- Sfyrla A
- Shalhout SZ
- Shapiro MD
- Shears T
- Shepard PF
- Sherman D
- Shimojima M
- Shochet M
- Shon Y
- Shreyber I
- Sidoti A
- Sinervo P
- Sisakyan A
- Slaughter AJ
- Slaunwhite J
- Sliwa K
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- Snihur R
- Soderberg M
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- Somalwar S
- Sorin V
- Spalding J
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- Stanitzki M
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- Stentz D
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- van Remortel N.
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- Veszpremi V.
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- Vidal M.
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- Vidal R.
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- Vila I.
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- Vilar R.
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- Vine T.
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- Vogel M.
- Volobouev I
- Volobouev I.
- Volpi G
- Volpi G.
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- Wagner P
- Wagner P.
- Wagner R. G.
- Wagner R. L.
- Wagner RG
- Wagner RL
- Wagner W
- Wagner W.
- Wagner-Kuhr J
- Wakisaka T
- Wakisaka T.
- Wallny R
- Wallny R.
- Wang S. M.
- Wang SM
- Warburton A
- Warburton A.
- Waters D
- Waters D.
- Weinberger M
- Weinberger M.
- Wester W. C. III
- Wester WC
- Whitehouse B
- Whitehouse B.
- Whiteson D
- Whiteson D.
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- Wicklund AB
- Wicklund E
- Wicklund E.
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- Williams G.
- Williams H. H.
- Williams HH
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- Wilson P.
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- Winer BL
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- Wittich P.
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- Wolbers S.
- Wolfe C
- Wolfe C.
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- Wright T.
- Wu X
- Wu X.
- Wurthwein F
- Wurthwein F.
- Wynne S. M.
- Wynne SM
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- Yagil A.
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- Yamamoto K.
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- Yamaoka J.
- Yamashita T
- Yamashita T.
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- Yang C.
- Yang U. K.
- Yang UK
- Yang Y. C.
- Yang YC
- Yao W. M.
- Yao WM
- Yeh G. P.
- Yeh GP
- Yoh J
- Yoh J.
- Yorita K
- Yorita K.
- Yoshida T
- Yoshida T.
- Yu G. B.
- Yu GB
- Yu I
- Yu I.
- Yu S. S.
- Yu SS
- Yun J. C.
- Yun JC
- Zanello L
- Zanello L.
- Zanetti A
- Zanetti A.
- Zaw I
- Zaw I.
- Zaw I.
- Zhang X
- Zhang X.
- Zhang X.
- Zheng Y
- Zheng Y.
- Zheng Y.
- Zucchelli S.
- Zucchelli S. S.Zucchelli S.
- Zucchelli Sneur S.
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2008
- Field of study
We search for pair production of supersymmetric top quarks (~t_1), followed
by R-parity violating decay ~t_1 -> tau b with a branching ratio beta, using
322 pb^-1 of ppbar collisions at sqrt{s}=1.96 TeV collected by the CDF II
detector at Fermilab. Two candidate events pass our final selection criteria,
consistent with the standard model expectation. We set upper limits on the
cross section sigma(~t_1 ~tbar_1)*beta^2 as a function of the stop mass
m(~t_1). Assuming beta=1, we set a 95% confidence level limit m(~t_1)>153
GeV/c^2. The limits are also applicable to the case of a third generation
scalar leptoquark (LQ_3) decaying LQ_3 -> tau b.Comment: 7 pages, 2 eps figure
Measurement of the W+W− Production Cross Section and Search for Anomalous WWγ and WWZ Couplings in ppˉ Collisions at s=1.96 TeV
- Author
- Aaltonen T
- Adelman J
- Almenar CC
- Amerio S
- Amidei D
- Anastassov A
- Annovi A
- Antos J
- Apollinari G
- Apresyan A
- Arisawa T
- Artikov A
- Asaadi J
- Ashmanskas W
- Attal A
- Aurisano A
- Azfar F
- Badgett W
- Barbaro-Galtieri A
- Barnes VE
- Barnett BA
- Barria P
- Bartos P
- Bauer G
- Beauchemin PH
- Bedeschi F
- Beecher D
- Behari S
- Bellettini G
- Bellinger J
- Benjamin D
- Beretvas A
- Bhatti A
- Binkley M
- Bisello D
- Bizjak I
- Blair RE
- Blocker C
- Blumenfeld B
- Bocci A
- Bodek A
- Boisvert V
- Bortoletto D
- Boudreau J
- Boveia A
- Brau B
- Bridgeman A
- Brigliadori L
- Bromberg C
- Brubaker E
- Budagov J
- Budd HS
- Budd S
- Burkett K
- Busetto G
- Bussey P
- Buzatu A
- Byrum KL
- Cabrera S
- Calancha C
- Camarda S
- Campanelli M
- Campbell M
- Canelli F
- Canepa A
- Carls B
- Carlsmith D
- Carosi R
- Carrillo S
- Carron S
- Casal B
- Casarsa M
- Castro A
- Catastini P
- Cauz D
- Cavaliere V
- Cavalli-Sforza M
- Cerri A
- Cerrito L
- Chang SH
- Chen YC
- Chertok M
- Chiarelli G
- Chlachidze G
- Chlebana F
- Cho K
- Chokheli D
- Chou JP
- Chung K
- Chung WH
- Chung YS
- Chwalek T
- Ciobanu CI
- Ciocci MA
- Clark A
- Clark D
- Compostella G
- Convery ME
- Conway J
- Corbo M
- Cordelli M
- Cox CA
- Cox DJ
- Crescioli F
- Cuevas J
- Culbertson R
- Cully JC
- d'Errico M
- D'Onofrio M
- da Costa JG
- Dagenhart D
- Datta M
- Davies T
- de Barbaro P
- De Cecco S
- De Lorenzo G
- Deisher A
- Dell'Orso M
- della Porta G. Zevi
- Deluca C
- Demortier L
- Deng J
- Deninno M
- Denis RS
- Di Canto A
- di Giovanni GP
- Di Ruzza B
- Dittmann JR
- Donati S
- Dong P
- Dorigo T
- Dube S
- Ebina K
- Elagin A
- Erbacher R
- Errede D
- Errede S
- Ershaidat N
- Eusebi R
- Fang HC
- Farrington S
- Fedorko WT
- Feild RG
- Feindt M
- Fernandez JP
- Fernandez PM
- Ferrazza C
- Field R
- Flanagan G
- Forrest R
- Frank MJ
- Franklin M
- Freeman JC
- Furic I
- Gallinaro M
- Galyardt J
- Garberson F
- Garcia JE
- Garfinkel AF
- Garosi P
- Gerberich H
- Gerdes D
- Gessler A
- Giagu S
- Giakoumopoulou V
- Giannetti P
- Gibson K
- Gimmell JL
- Ginsburg CM
- Giokaris N
- Giordani M
- Giromini P
- Giunta M
- Giurgiu G
- Glagolev V
- Glenzinski D
- Gold M
- Goldschmidt N
- Golossanov A
- Gomez G
- Gomez-Ceballos G
- Goncharov M
- Gonzalez BA
- Gonzalez O
- Gorelov I
- Goshaw AT
- Goulianos K
- Gresele A
- Grinstein S
- Griso SP
- Grosso-Pilcher C
- Group RC
- Grundler U
- Gunay-Unalan Z
- Haber C
- Hahn SR
- Halkiadakis E
- Han BY
- Han JY
- Happacher F
- Hara K
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- Harr RF
- Hartz M
- Hatakeyama K
- Hays C
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- Heinrich J
- Herndon M
- Heuser J
- Hewamanage S
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- Hill CS
- Hirschbuehl D
- Hocker A
- Hou S
- Houlden M
- Hsu SC
- Hughes RE
- Hurwitz M
- Husemann U
- Hussein M
- Huston J
- Incandela J
- Introzzi G
- Iori M
- Ivanov A
- James E
- Jang D
- Jayatilaka B
- Jeon EJ
- Jha MK
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- Johnson W
- Jones M
- Joo KK
- Jun SY
- Jung JE
- Junk TR
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- Karchin PE
- Kato Y
- Kephart R
- Ketchum W
- Keung J
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- Kilminster B
- Kim DH
- Kim HS
- Kim HW
- Kim JE
- Kim MJ
- Kim SB
- Kim SH
- Kim YK
- Kimura N
- Kirsch L
- Klimenko S
- Kondo K
- Kong DJ
- Konigsberg J
- Korytov A
- Kotwal AV
- Kreps M
- Kroll J
- Krop D
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- Krutelyov V
- Kuhr T
- Kulkarni NP
- Kurata M
- Kwang S
- Laasanen AT
- Lami S
- Lammel S
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- Lander RL
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- Lazzizzera I
- LeCompte T
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- Lin CJ
- Linacre J
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- Lungu G
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- Madrak R
- Maeshima K
- Makhoul K
- Maksimovic P
- Malde S
- Malik S
- Manca G
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- Margaroli F
- Marino C
- Marino CP
- Martin A
- Martin V
- Martinez M
- Martinez-Ballarin R
- Mastrandrea P
- Mathis M
- Mattson ME
- Mazzanti P
- McFarland KS
- McIntyre P
- McNulty R
- Mehta A
- Mehtala P
- Menzione A
- Mesropian C
- Miao T
- Mietlicki D
- Miladinovic N
- Miller R
- Mills C
- Milnik M
- Mitra A
- Mitselmakher G
- Miyake H
- Moed S
- Moggi N
- Mondragon MN
- Moon CS
- Moore R
- Morello MJ
- Morlock J
- Mukherjee A
- Muller T
- Mulmenstadt J
- Murat P
- Mussini M
- Nachtman J
- Nagai Y
- Naganoma J
- Nakamura K
- Nakano I
- Napier A
- Nett J
- Neu C
- Neubauer MS
- Neubauer S
- Nielsen J
- Nodulman L
- Norman M
- Norniella O
- Nurse E
- Oakes L
- Oh SH
- Oh YD
- Oksuzian I
- Okusawa T
- Orava R
- Osterberg K
- Pagliarone C
- Palencia E
- Papadimitriou V
- Papaikonomou A
- Paramanov AA
- Parks B
- Pashapour S
- Patrick J
- Pauletta G
- Paulini M
- Paus C
- Peiffer T
- Pellett DE
- Penzo A
- Phillips TJ
- Piacentino G
- Pianori E
- Pinera L
- Pitts K
- Plager C
- Pondrom L
- Potamianos K
- Poukhov O
- Prokoshin F
- Pronko A
- Ptohos F
- Pueschel E
- Punzi G
- Pursley J
- Rademacker J
- Rahaman A
- Ramakrishnan V
- Ranjan N
- Redondo I
- Renton P
- Renz M
- Rescigno M
- Richter S
- Rimondi F
- Ristori L
- Robson A
- Rodrigo T
- Rodriguez T
- Rogers E
- Rolli S
- Roser R
- Rossi M
- Rossin R
- Roy P
- Ruiz A
- Russ J
- Rusu V
- Rutherford B
- Saarikko H
- Safonov A
- Sakumoto WK
- Santi L
- Sartori L
- Sato K
- Savoy-Navarro A
- Schlabach P
- Schmidt A
- Schmidt EE
- Schmidt MA
- Schmidt MP
- Schmitt M
- Schwarz T
- Scodellaro L
- Scribano A
- Scuri F
- Sedov A
- Seidel S
- Seiya Y
- Semenov A
- Sexton-Kennedy L
- Sforza F
- Sfyrla A
- Shalhout SZ
- Shears T
- Shepard PF
- Shimojima M
- Shiraishi S
- Shochet M
- Shon Y
- Shreyber I
- Simonenko A
- Sinervo P
- Sisakyan A
- Slaughter AJ
- Slaunwhite J
- Sliwa K
- Smith JR
- Snider FD
- Snihur R
- Soha A
- Somalwar S
- Sorin V
- Squillacioti P
- Stanitzki M
- Stelzer B
- Stelzer-Chilton O
- Stentz D
- Strologas J
- Strycker GL
- Suh JS
- Sukhanov A
- Suslov I
- Taffard A
- Takashima R
- Takeuchi Y
- Tanaka R
- Tang J
- Tecchio M
- Teng PK
- Thom J
- Thome J
- Thompson GA
- Thomson E
- Tipton P
- Tkaczyk S
- Toback D
- Tokar S
- Tollefson K
- Tomura T
- Tonelli D
- Torre S
- Torretta D
- Totaro P
- Tourneur S
- Trovato M
- Tsai SY
- Ttito-Guzman P
- Tu Y
- Turini N
- Ukegawa F
- Uozumi S
- van Remortel N
- Varganov A
- Vataga E
- Vazquez F
- Velev G
- Vellidis C
- Vidal M
- Vila I
- Vilar R
- Vogel M
- Volobouev I
- Volpi G
- Wagner P
- Wagner RG
- Wagner RL
- Wagner W
- Wagner-Kuhr J
- Wakisaka T
- Wallny R
- Wang SM
- Warburton A
- Waters D
- Weinberger M
- Weinelt J
- Wester WC
- Whitehouse B
- Whiteson D
- Wicklund AB
- Wicklund E
- Wilbur S
- Williams G
- Williams HH
- Wilson P
- Winer BL
- Wittich P
- Wolbers S
- Wolfe C
- Wolfe H
- Wright T
- Wu X
- Wurthwein F
- Yagil A
- Yamamoto K
- Yamaoka J
- Yang UK
- Yang YC
- Yao WM
- Yeh GP
- Yi K
- Yilmaz M.
- Yoh J
- Yoosoofmiya R.
- Yorita K
- Yorita K.
- Yoshida R.
- Yoshida T
- Young C.
- Youssef S.
- Yu D.
- Yu GB
- Yu I
- Yu J.
- Yu J.
- Yu SS
- Yuan L.
- Yun JC
- Yurkewicz A.
- Zaets V. G.
- Zaidan R.
- Zaitsev A. M.
- Zajacova Z.
- Zalite Yo. K.
- Zanello L.
- Zanetti A
- Zarzhitsky P.
- Zaytsev A.
- Zdrazil M.
- Zeitnitz C.
- Zeller M.
- Zema P. F.
- Zemla A.
- Zendler C.
- Zeng Y
- Zenin A. V.
- Zenin O.
- Zenis T.
- Zenonos Z.
- Zenz S.
- Zerwas D.
- Zhan Z.
- Zhang D.
- Zhang H.
- Zhang J.
- Zhang X
- Zhang X.
- Zhang Z.
- Zhao L.
- Zhao T.
- Zhao Z.
- Zhemchugov A.
- Zheng S.
- Zheng Y
- Zheng Y
- Zhong J.
- Zhou B.
- Zhou N.
- Zhou Y.
- Zhu C. G.
- Zhu H.
- Zhu Y.
- Zhuang X.
- Zhuravlov V.
- Zieminska D.
- Zilka B.
- Zimmermann R.
- Zimmermann S.
- Zimmermann S.
- Ziolkowski M.
- Zitoun R.
- Zivkovic L.
- Zmouchko V. V.
- Zobernig G.
- Zoccoli A.
- Zolnierowski Y.
- Zsenei A.
- Zucchelli S
- Zucchelli Se S.
- Zucchelli SX
- zur Nedden M.
- Zutshi V.
- Zwalinski L.
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/12/2009
- Field of study
This Letter describes the current most precise measurement of the W boson
pair production cross section and most sensitive test of anomalous WWγ
and WWZ couplings in ppˉ collisions at a center-of-mass energy of 1.96
TeV. The WW candidates are reconstructed from decays containing two charged
leptons and two neutrinos, where the charged leptons are either electrons or
muons. Using data collected by the CDF II detector from 3.6 fb−1 of
integrated luminosity, a total of 654 candidate events are observed with an
expected background contribution of 320±47 events. The measured total
cross section is σ(ppˉ→W+W−+X)=12.1±0.9(stat)−1.4+1.6(syst) pb, which is in good agreement
with the standard model prediction. The same data sample is used to place
constraints on anomalous WWγ and WWZ couplings.Comment: submitted to Phys. Rev. Let
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
- Bain T
- Baines JT
- Baker MD
- Baker OK
- Baker S
- Banas E
- Banerjee P
- Banerjee S
- Banfi D
- Bangert A
- Bansal V
- Bansil HS
- Barajas CAC
- Barak L
- Baranov SP
- Barashkou A
- Barber T
- Barberio EL
- Barberis D
- Barbero M
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- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/03/2013
- Field of study
The jet energy scale and its systematic uncertainty are determined for jets measured with the ATLAS detector at the LHC in proton-proton collision data at a centre-of-mass energy of √s = 7TeV corresponding to an integrated luminosity of 38 pb-1. Jets are reconstructed with the anti-kt algorithm with distance parameters R=0. 4 or R=0. 6. Jet energy and angle corrections are determined from Monte Carlo simulations to calibrate jets with transverse momenta pT≥20 GeV and pseudorapidities {pipe}η{pipe}<4. 5. The jet energy systematic uncertainty is estimated using the single isolated hadron response measured in situ and in test-beams, exploiting the transverse momentum balance between central and forward jets in events with dijet topologies and studying systematic variations in Monte Carlo simulations. The jet energy uncertainty is less than 2. 5 % in the central calorimeter region ({pipe}η{pipe}<0. 8) for jets with 60≤pT<800 GeV, and is maximally 14 % for pT<30 GeV in the most forward region 3. 2≤{pipe}η{pipe}<4. 5. The jet energy is validated for jet transverse momenta up to 1 TeV to the level of a few percent using several in situ techniques by comparing a well-known reference such as the recoiling photon pT, the sum of the transverse momenta of tracks associated to the jet, or a system of low-pT jets recoiling against a high-pT jet. More sophisticated jet calibration schemes are presented based on calorimeter cell energy density weighting or hadronic properties of jets, aiming for an improved jet energy resolution and a reduced flavour dependence of the jet response. The systematic uncertainty of the jet energy determined from a combination of in situ techniques is consistent with the one derived from single hadron response measurements over a wide kinematic range. The nominal corrections and uncertainties are derived for isolated jets in an inclusive sample of high-pT jets. Special cases such as event topologies with close-by jets, or selections of samples with an enhanced content of jets originating from light quarks, heavy quarks or gluons are also discussed and the corresponding uncertainties are determined. © 2013 CERN for the benefit of the ATLAS collaboration
Search for the neutral Higgs bosons of the minimal supersymmetric standard model in pp collisions at root s=7 TeV with the ATLAS detector
- Author
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- Publication venue
- Publication date
- 01/02/2013
- Field of study
A search for neutral Higgs bosons of the Minimal Supersymmetric Standard Model (MSSM) is reported. The analysis is based on a sample of proton-proton collisions at a centre-of-mass energy of 7TeV recorded with the ATLAS detector at the Large Hadron Collider. The data were recorded in 2011 and correspond to an integrated luminosity of 4.7 fb-1 to 4.8 fb-1. Higgs boson decays into oppositely-charged muon or τ lepton pairs are considered for final states requiring either the presence or absence of b-jets. No statistically significant excess over the expected background is observed and exclusion limits at the 95% confidence level are derived. The exclusion limits are for the production cross-section of a generic neutral Higgs boson, φ, as a function of the Higgs boson mass and for h/A/H production in the MSSM as a function of the parameters mA and tan β in the mhmax scenario for mA in the range of 90GeV to 500 GeV. Copyright CERN
Search for direct pair production of the top squark in all-hadronic final states in proton-proton collisions at s√=8 TeV with the ATLAS detector
- Author
- Aad G
- Abbott B
- Abdallah J
- Abdinov O
- Aben R
- Abi B
- Abolins M
- AbouZeid OS
- Abramowicz H
- Abreu H
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- Acharya BS
- Adamczyk L
- Adams DL
- Adelman J
- Adomeit S
- Adye T
- Agatonovic-Jovin T
- Aguilar-Saavedra JA
- Agustoni M
- Ahlen SP
- Ahmadov F
- Aielli G
- Akerstedt H
- Akesson TPA
- Akimoto G
- Akimov AV
- Alberghi GL
- Albert J
- Albrand S
- Alconada Verzini MJ
- Aleksa M
- Aleksandrov IN
- Alexa C
- Alexander G
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- Allbrooke BMM
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- Zhemchugov A
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- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2014
- Field of study
The results of a search for direct pair production of the scalar partner to the top quark using an integrated luminosity of 20.1fb−1 of proton–proton collision data at √s = 8 TeV recorded with the ATLAS detector at the LHC are reported. The top squark is assumed to decay via t˜→tχ˜01 or t˜→ bχ˜±1 →bW(∗)χ˜01 , where χ˜01 (χ˜±1 ) denotes the lightest neutralino (chargino) in supersymmetric models. The search targets a fully-hadronic final state in events with four or more jets and large missing transverse momentum. No significant excess over the Standard Model background prediction is observed, and exclusion limits are reported in terms of the top squark and neutralino masses and as a function of the branching fraction of t˜ → tχ˜01 . For a branching fraction of 100%, top squark masses in the range 270–645 GeV are excluded for χ˜01 masses below 30 GeV. For a branching fraction of 50% to either t˜ → tχ˜01 or t˜ → bχ˜±1 , and assuming the χ˜±1 mass to be twice the χ˜01 mass, top squark masses in the range 250–550 GeV are excluded for χ˜01 masses below 60 GeV
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