24 research outputs found
Evidence for the h_b(1P) meson in the decay Upsilon(3S) --> pi0 h_b(1P)
- Author
- Adametz A.
- Adye T.
- Ahmed H.
- Alam M. S.
- Albert J.
- Allen M. T.
- Alwyn K. E.
- Andreassen R.
- Angelini C.
- Anh TV
- Anulli F.
- Arnaud N.
- Asgeirsson D. J.
- Aston D.
- Atmacan H.
- Ayad R.
- Bailey D.
- Baldini-Ferroli R.
- Band H. R.
- Banerjee Sw.
- Bard D. J.
- Barlow R. J.
- Bartoldus R.
- Batignani G.
- Behera P. K.
- Bellis M.
- Ben-Haim E.
- Benitez J. F.
- Bernard D.
- Bernlochner F. U.
- Bettarini S.
- Bettoni D.
- Bevan A. J.
- Bhuyan B.
- Bianchi F.
- Biasini M.
- Biassoni P.
- Bingham I.
- Blinov V. E.
- Bloom P. C.
- Blount N. L.
- Bomben M.
- Bondioli M.
- Bonneaud G. R.
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- Briand H.
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- Burchat P. R.
- Buzykaev A. R.
- Cakir IT
- Calabrese R.
- Calcaterra A.
- Calderini G.
- Campagnari C.
- Carpinelli M.
- Cartaro C.
- Casarosa G.
- Castanheira MTD
- Castelli G.
- Cavoto G.
- Cenci R.
- Cervelli A.
- Chauveau J.
- Chavez C. A.
- Chen C.
- Chen X. R.
- Cheng C. H.
- Choi H. H. F.
- Cibinetto G.
- Clark P. J.
- Cochran J.
- Coleman J. P.
- Contri R.
- Convery M. R.
- Corwin L. A.
- Cowan G.
- Cowan R.
- Crawley H. B.
- Cremaldi L.
- Curry S.
- Dallapiccola C.
- Dasu S.
- Dauncey P. D.
- Davier M.
- Davis C. L.
- de Monchenault G. Hamel
- De Nardo G.
- de Sangro R.
- Denig A. G.
- Derkach D.
- Di Lodovico F.
- Doll D. A.
- Dorfan J.
- Druzhinin V. P.
- Dubois-Felsmann G. P.
- Dubrovin M. S.
- Dujmic D.
- Dunwoodie W.
- Ebert M.
- Echenard B.
- Eckmann R.
- Edwards A. J.
- Eigen G.
- Eisner A. M.
- Emery S.
- Ernst J. A.
- Faccini R.
- Feltresi E.
- Ferrarotto F.
- Ferrer JAV
- Ferroni F.
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- Finocchiaro G.
- Fioravanti E.
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- Ford W. T.
- Forti F.
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- Fritsch M.
- Fry J. R.
- Fulsom B. G.
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- Gabathuler E.
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- Grenier P.
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- Schwierz R.
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- Sevilla M. Franco
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- Simi G.
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- Skovpen Yu. I.
- Smith A. J. S.
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- Strandlie A
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- Sundermann JE
- Suruliz K
- Sushkov S
- Susinno G
- Sutton MR
- Suzuki K.
- Suzuki Y
- Sviridov YM
- Swedish S
- Sykora I
- Sykora T
- Szeless B
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- Taffard A
- Tafirout R
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- Taiblum N
- Takahashi Y
- Takai H
- Takashima R
- Takeda H
- Takeshita T
- Talby M
- Talyshev A
- Tamsett MC
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- Traynor D
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- Wisniewski W. J.
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- Yao W. -M.
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- Yeche Ch.
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- Yi K.
- Yoh J
- Yoh J.
- Yorita K
- Yorita K.
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- Yoshida T.
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- Yu G B
- Yu G. B.
- Yu I
- Yu I.
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- Yun J. C.
- Yushkov A. N.
- Zallo A.
- Zanetti A
- Zanetti A.
- Zanetti A.
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- Ziegler V.
- Zucchelli S.
- Zucchelli S. Stradling AR
- Zucchelli SVazquez F.
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2011
- Field of study
Using a sample of 122 million Upsilon(3S) events recorded with the BaBar
detector at the PEP-II asymmetric-energy e+e- collider at SLAC, we search for
the hb(1P) spin-singlet partner of the P-wave chi_{bJ}(1P) states in the
sequential decay Upsilon(3S) --> pi0 h_b(1P), h_b(1P) --> gamma eta_b(1S). We
observe an excess of events above background in the distribution of the recoil
mass against the pi0 at mass 9902 +/- 4(stat.) +/- 2(syst.) MeV/c^2. The width
of the observed signal is consistent with experimental resolution, and its
significance is 3.1sigma, including systematic uncertainties. We obtain the
value (4.3 +/- 1.1(stat.) +/- 0.9(syst.)) x 10^{-4} for the product branching
fraction BF(Upsilon(3S)-->pi0 h_b) x BF(h_b-->gamma eta_b).Comment: 8 pages, 4 postscript figures, submitted to Phys. Rev. D (Rapid
Communications
Search for high-mass resonances decaying to dilepton final states in pp collisions at s√=7 TeV with the ATLAS detector
- Author
- Aad G
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- Abdallah J
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- 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
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- Akimov AV
- Alam MA
- Alam MS
- Albert J
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- Aleksa M
- Aleksandrov IN
- Alessandria F
- Alexa C
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- Yoosoofmiya R
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- Zabinski B
- Zaidan R
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- Zemla A
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- Zerwas D
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- Zhang H
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- Zhang X
- Zhang Z
- Zhao L
- Zhao Z
- Zhemchugov A
- Zhong J
- Zhou B
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- Zhou Y
- Zhu CG
- Zhu H
- Zhu J
- Zhu Y
- Zhuang X
- Zhuravlov V
- Zibell A
- Zieminska D
- Zimin NI
- Zimmermann R
- Zimmermann S
- Zimmermann S
- Zinonos Z
- Ziolkowski M
- Zitoun R
- Zivkovic L
- Zmouchko VV
- Zobernig G
- Zoccoli A
- zur Nedden M
- Zutshi V
- Zwalinski L
- Publication venue
- Springer
- Publication date
- 01/01/2012
- Field of study
The ATLAS detector at the Large Hadron Collider is used to search for high-mass resonances decaying to an electron-positron pair or a muon-antimuon pair. The search is sensitive to heavy neutral Z′ gauge bosons, Randall-Sundrum gravitons, Z * bosons, techni-mesons, Kaluza-Klein Z/γ bosons, and bosons predicted by Torsion models. Results are presented based on an analysis of pp collisions at a center-of-mass energy of 7 TeV corresponding to an integrated luminosity of 4.9 fb−1 in the e + e − channel and 5.0 fb−1 in the μ + μ −channel. A Z ′ boson with Standard Model-like couplings is excluded at 95 % confidence level for masses below 2.22 TeV. A Randall-Sundrum graviton with coupling k/MPl=0.1 is excluded at 95 % confidence level for masses below 2.16 TeV. Limits on the other models are also presented, including Technicolor and Minimal Z′ Models
Measurement of the Top Pair Production Cross Section in the Dilepton Decay Channel in ppbar Collisions at sqrt s = 1.96 TeV
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- Aaltonen T
- Almenar CC
- Amerio S
- Amidei D
- Anastassov A
- Anh TV
- 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
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- Barnes VE
- Barnett BA
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- Blocker C
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- 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
- Cakir IT
- Calancha C
- Camarda S
- Camillocci ES
- Campanelli M
- Campbell M
- Canelli F
- Canepa A
- Canto A
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- Carlsmith D
- Carosi R
- Carrillo S
- Carron S
- Casal B
- Casarsa M
- Castanheira MTD
- 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
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- De Barbaro P
- De Cecco S
- De Lorenzo G
- DELL'ORSO MAURO
- Deluca C
- Demortier L
- Deng J
- Deninno M
- Denis RS
- Devoto F
- Di Ruzza B
- Dittmann JR
- DONATI SIMONE
- 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 PM
- Ferrazza C
- Ferrer JAV
- Field R
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- Forrest R
- Frank MJ
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- Freeman JC
- Furic I
- Gallego EV
- Gallinaro M
- Galyardt J
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- 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 Ceballos G
- Gomez G
- Goncharov M
- Gonzalez BA
- Gonzalez O
- Gorelov I
- Goshaw AT
- Goulianos K
- Gresele A
- Grinstein S
- Griso SP
- Grosso Pilcher C
- Group RC
- Gunay Unalan Z
- Haber C
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- Hamaguchi A
- Han JY
- Happacher F
- Hara K
- Hare D
- Hare M
- Harr RF
- Hatakeyama K
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- Hughes RE
- Hurwitz M
- Husemann U
- Hussain N
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- Huston J
- Introzzi G
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- Ivanov A
- James E
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- Jayatilaka B
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- Jha MK
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- Krop D
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- Kuhr T
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- Maeshima K
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- Malik S
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- Manousakis Katsikakis A
- Margaroli F
- Marino C
- Martinez Ballarin R
- Martinez M
- Mastrandrea P
- Mathis M
- Mattson ME
- Mazzanti P
- McFarland KS
- McIntyre P
- McNulty R
- Mehta A
- Mehtala P
- Menzione A
- Mesropian C
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- PUNZI GIOVANNI
- Pursley J
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- Ramakrishnan V
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- Shepard PF
- Shimojima M
- Shiraishi S
- Shochet M
- Shreyber I
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- Solodkov AA
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- Sondericker J
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- Spousta M
- Spreitzer T
- Spurlock B
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- St Denis RD
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- Stavina P
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- Stekl I
- Stelzer B
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- Stewart GA
- Stillings JA
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- Thompson GA
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- Timmermans CJWP
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- Vermeulen JC
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- Viehhauser GHA
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- von der Schmitt H
- von Loeben J
- von Radziewski H
- von Toerne E
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- Vorobiev AP
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- Vossebeld JH
- Vovenko AS
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- Vreeswijk M
- Vuillermet R
- Vukotic I
- Wagner P
- Wagner P
- Wagner RL
- Wagner W
- Wahlen H
- Wakabayashi J
- Wakisaka T
- Walbersloh J
- Walch S
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- Walker R.
- Wallny R
- Wang SM
- Warburton A
- Waters D
- Weinberger M
- Wester WC
- Whitehouse B
- Whiteson D
- Wick F
- Wicklund AB
- Wicklund E
- Wilbur S
- Williams HH
- Wilson JS
- Wilson P
- Winer BL
- Wittich P
- Wolbers S
- Wolfe H
- Wright T
- Wu X
- Wu Z
- Yamamoto K
- Yamaoka J
- Yang UK
- Yang YC
- Yao WM
- Yeh GP
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- Yoh J
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- Yu GB
- Yu I
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- Yun JC
- Zanetti A
- Zeng Y
- Zucchelli S. Snesarev AA
- Publication venue
- Publication date
- 01/01/2010
- Field of study
Submitted to Phys. Rev. DA measurement of the \ttbar production cross section in \ppbar collisions at s = 1.96 TeV using events with two leptons, missing transverse energy, and jets is reported. The data were collected with the CDF II Detector. The result in a data sample corresponding to an integrated luminosity 2.8 fb−1 is: \sigma_{\ttbar} = 6.27 ± 0.73(stat) ± 0.63(syst) ± 0.39(lum) pb. for an assumed top mass of 175 GeV/c2.A measurement of the tt̅ production cross section in pp̅ collisions at √s=1.96 TeV using events with two leptons, missing transverse energy, and jets is reported. The data were collected with the CDF II detector. The result in a data sample corresponding to an integrated luminosity 2.8 fb-1 is σtt̅ =6.27±0.73(stat)±0.63(syst)±0.39(lum) pb. for an assumed top mass of 175 GeV/c2.Peer reviewe
Measurement of the cross-section for b-jets produced in association with a Z boson at root s=7 TeV with the ATLAS detector ATLAS Collaboration
- 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
- Akdogan T
- Akesson TPA
- Akimoto G
- Akimov AV
- Akiyama 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
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- Zhemchugov A
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- Zivkovic L
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- Zobernig G
- Zoccoli A
- Zolnierowski Y
- Zsenei A
- zur Nedden M
- Zutshi V
- Zwalinski L
- Publication venue
- 'Elsevier BV'
- Publication date
- 01/01/2011
- Field of study
A measurement is presented of the inclusive cross-section for b-jet production in association with a Z boson in pp collisions at a centre-of-mass energy of root s = 7 TeV. The analysis uses the data sample collected by the ATLAS experiment in 2010, corresponding to an integrated luminosity of approximately 36 pb(-1). The event selection requires a Z boson decaying into high P-T electrons or muons, and at least one b-jet, identified by its displaced vertex, with transverse momentum p(T) > 25 GeV and rapidity vertical bar y vertical bar < 2.1. After subtraction of background processes, the yield is extracted from the vertex mass distribution of the candidate b-jets. The ratio of this cross-section to the inclusive Z cross-section (the average number of b-jets per Z event) is also measured. Both results are found to be in good agreement with perturbative QCD predictions at next-to-leading order
Compound effect of EHD and surface roughness in pool boiling and CHF with R-123
- Author
- Aad G
- Abbott B
- Abdallah J
- Abdelalim AA
- Abdesselam A
- Abdinov O
- Abi B
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- 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
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- Zwalinski L
- Publication venue
- 'Elsevier BV'
- Publication date
- 01/01/2011
- Field of study
This article is a post-print version of the fianl published article which may be accessed at the link below.Saturated pool boiling of R-123 at 1 bar, including the critical heat flux (CHF), was enhanced by modifying the surface characteristics and applying a high intensity electrostatic field, the latter termed electrohydrodynamic (and abbreviated EHD) enhancement. The heat flux was varied from very low values in the natural convection regime up to CHF. Experiments were performed with increasing and decreasing heat flux to study boiling hysteresis without and with EHD. Boiling occurred on the sand blasted surface of a
cylindrical copper block with embedded electrical heating elements, with standardized surface parameter Pa = 3.5 μm. The electric field was generated by a potential of 5 kV to 25 kV, applied through a 40 mm diameter circular electrode of ss-304 wire mesh, aperture size 5.1 mm, located at distances of 5 - 60 mm from the surface, with most of the data obtained for 20 mm. The data for the rough surface were compared with earlier data for a smooth surface and indicated a significant increase in the heat transfer rates. EHD produced a further increase in the heat transfer rates, particularly at low heat flux values and near the CHF. Boiling hysteresis was reduced progressively by EHD and eliminated at high field strength.This work was supported by Government of Pakistan under a scholarship programme
Myocardial infarct size and mortality in diabetic patients.
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- Allison S.P.
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- B L Pentecost
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- D J Gwilt
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- Flint E.J.
- Fuller J.H.
- FV Jr, Crall
- Garcia M.J.
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- Oswald G.A.
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- Shell W.E.
- Sobel B.E.
- Soler N.G.
- T III, Killip
- true
- Vague P.
- Publication venue
- 'BMJ'
- Publication date
- Field of study
Search for the Higgs boson in the all-hadronic final state using the CDF II detector
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- Aaltonen T.
- Almenar C. Cuenca
- Alvarez Gonzalez B.
- Amerio S.
- Amidei D.
- Anastassov A.
- Anh TV
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- Whitehouse B.
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- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2011
- Field of study
We report on a search for the production of the Higgs boson decaying to two bottom quarks accompanied by two additional quarks. The data sample used corresponds to an integrated luminosity of approximately 4 fb(-1) of p (p) over bar collisions at root s = 1.96 TeV recorded by the CDF II experiment. This search includes twice the integrated luminosity of the previous published result, uses analysis techniques to distinguish jets originating from light flavor quarks and those from gluon radiation, and adds sensitivity to a Higgs boson produced by vector boson fusion. We find no evidence of the Higgs boson and place limits on the Higgs boson production cross section for Higgs boson masses between 100 GeV/c(2) and 150 GeV/c(2) at the 95% confidence level. For a Higgs boson mass of 120 GeV/c(2), the observed (expected) limit is 10.5 (20.0) times the predicted standard model cross section
Searches for rare or forbidden semileptonic charm decays
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- Adametz A.
- Adye T.
- Ahmed H.
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- Albert J.
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- Angelini C.
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- Bard D. J.
- Barlow R. J.
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- Batignani G.
- Behera P. K.
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- Yao W. -M.
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- Yeche Ch
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- Yeh G. P.
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- Yi K.
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- Yoh J.
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- Yorita K.
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- Yoshida T.
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- Zanetti A
- Zanetti A.
- Zanetti A.
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- Zeng Y.
- Zeng Y.
- Ziegler V.
- Zucchelli S.
- Zucchelli S. Stradling AR
- Zucchelli SVazquez F.
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2011
- Field of study
We present searches for rare or forbidden charm decays of the form X(c)(+) -> h(+/-)l(+/-)l((l)+), where X(c)(+) is a charm hadron (D(+), D(s)(+), or A(c)(+)), h +/- is a pion, kaon, or proton, and l((l)+/-) is an electron or muon. The analysis is based on 384 fb(-1) of e(+)e(-) annihilation data collected at or close to the gamma(4S) resonance with the BABAR detector at the SLAC National Accelerator Laboratory. No significant signal is observed for any of the 35 decay modes that are investigated. We establish 90% confidence-level upper limits on the branching fractions between 1 x 10(-6) and 44 x 10(-6) depending on the channel. In most cases, these results represent either the first limits or significant improvements on existing limits for the decay modes studied
Analysis of the D^{+}→K^{-}π^{+}e^{+}ν_{e} decay channel
- Author
- Adametz A.
- Adye T.
- Ahmed S.
- Alam M. S.
- Albert J.
- Allen M. T.
- Alwyn K. E.
- Anderson J.
- Andreassen R.
- Andreotti M.
- Angelini C.
- Anh TV
- Anulli F.
- Arnaud N.
- Asgeirsson D. J.
- Aston D.
- Atmacan H.
- Ayad R.
- Bailey D.
- Baldini-Ferroli R.
- Band H. R.
- Banerjee S. W.
- Baracchini E.
- Bard D. J.
- Barlow R. J.
- Bartoldus R.
- Batignani G.
- Battaglia M.
- Behera P. K.
- Bellis M.
- Ben-Haim E.
- Benitez J. F.
- Bernard D.
- Bernlochner F. U.
- Bettarini S.
- Bettoni D.
- Bevan A. J.
- Bhuyan B.
- Bianchi F.
- Biasini M.
- Biassoni P.
- Bingham I.
- Blinov V. E.
- Bloom P. C.
- Blount N. L.
- Bomben M.
- Bondioli M.
- Bonneaud G. R.
- Bozzi C.
- Brau J.
- Briand H.
- Brown D. N.
- Brown D. N.
- Burchat P. R.
- Buzykaev A. R.
- Cakir IT
- Calabrese R.
- Calcaterra A.
- Calderini G.
- Campagnari C.
- Carpinelli M.
- Cartaro C.
- Casarosa G.
- Castanheira MTD
- Castelli G.
- Cavoto G.
- Cecchi A.
- Cenci R.
- Cervelli A.
- Chauveau J.
- Chavez C. A.
- Chen C.
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- Cheng C. H.
- Choi H. H. F.
- Cibinetto G.
- Clark P. J.
- Cochran J.
- Coleman J. P.
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- Curry S.
- da Costa J. Firmino
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- Dasu S.
- Dauncey P. D.
- Davier M.
- Davis C. L.
- de Monchenault G. Hamel
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- de Sangro R.
- Denig A. G.
- Derkach D.
- Di Lodovico F.
- Doll D. A.
- Dong L.
- Dorfan J.
- Druzhinin V. P.
- Dubois-Felsmann G. P.
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- Dunwoodie W.
- Ebert M.
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- Eigen G.
- Eisner A. M.
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- Ernst J. A.
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- Ferrarotto F.
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- Ferroni F.
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- Franchini P.
- Franek B.
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- Fritsch M.
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- Gabareen A. M.
- Gabathuler E.
- Gagliardi N.
- Gallego EV
- Gamba D.
- Gamet R.
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- Gaspero M.
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- Gershon T. J.
- Gioi L. Li
- Giorgi M. A.
- Godang R.
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- Gradl W.
- Graham M. T.
- Grauges E.
- Grenier P.
- Gritsan A. V.
- Grosdidier G.
- Guido E.
- Guo Z. J.
- Guttman N.
- Hafner A.
- Hamano K.
- Hamon O.
- Harrison P. F.
- Hartmann T.
- Hast C.
- Hawkes C. M.
- Hearty C.
- Heusch C. A.
- Hitlin D. G.
- Hong T. M.
- Honscheid K.
- Hooberman B.
- Hutchcroft D. E.
- Igonkina O.
- Innes W. R.
- Izen J. M.
- Jackson G.
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- Kolomensky Yu. G.
- Kovalskyi D.
- Kowalewski R.
- Kroeger R.
- Kroseberg J.
- Lacker H. M.
- Lafferty G. D.
- Lanceri L.
- Lange D. J.
- Lankford A. J.
- Latham T. E.
- Lazzaro A.
- Le Diberder F.
- Leddig T.
- Lee C. L.
- Lees J. P.
- Leith D. W. G. S.
- Leruste Ph.
- Lewczuk M. J.
- Li S.
- Lindemann D.
- Lindquist B.
- Liu F.
- Lo Vetere M.
- Lockman W. S.
- Lombardo V.
- Long O.
- Lopez-March N.
- LoSecco J. M.
- Lou X. C.
- Lu C.
- Lueck T.
- Luitz S.
- Lund P.
- Luppi E.
- Lusiani A.
- Luth V.
- Lutz A. M.
- Lynch G.
- Lynch H. L.
- MacFarlane D. B.
- Malaescu B.
- Mallik U.
- Mancinelli G.
- Mandelkern M.
- Manoni E.
- Marchiori G.
- Margoni M.
- Marks J.
- Marsiske H.
- Martin E. C.
- Martinelli M.
- Martinez A. J.
- Martinez-Vidal F.
- Mattison T. S.
- Mazzoni M. A.
- McKenna J. A.
- Meadows B. T.
- Merkel J.
- Meyer W. T.
- Milanes D. A.
- Milosavljevic MV
- Miyashita T. S.
- Monge M. R.
- Monorchio D.
- Morandin M.
- Morii M.
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- Muller D. R.
- Munerato M.
- Nagel M.
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- Neal H.
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- Nguyen X.
- Nicolaci M.
- Nugent I. M.
- O'Grady C. P.
- Ocariz J.
- Ofte I.
- Olaiya E. O.
- Olsen J.
- Ongmongkolkul P.
- Onorato G.
- Onuchin A. P.
- Osipenkov I. L.
- Oyanguren A.
- Pacetti S.
- Palano A.
- Palombo F.
- Pan B.
- Pan Y.
- Paoloni E.
- Pappagallo M.
- Paramesvaran S.
- Park W.
- Passaggio S.
- Pastor ET
- Patel P. M.
- Patrignani C.
- Patteri P.
- Payne D. J.
- Pegna D. Lopes
- Pelliccioni M.
- Perez A.
- Perez MV
- Perl M.
- Peruzzi I. M.
- Petrella A.
- Petzold A.
- Piccolo M.
- Piemontese L.
- Piredda G.
- Playfer S.
- Poireau V.
- Porter F. C.
- Posocco M.
- Prasad V.
- Prell S.
- Prencipe E.
- Prendki J.
- Prepost R.
- Puccio E. M. T.
- Pulliam T.
- Purohit M. V.
- Rahmat R.
- Rakitin A. Y.
- Rama M.
- Randle-Conde A.
- Ratcliff B. N.
- Raven G.
- Renga F.
- Richman J. D.
- Ritchie J. L.
- Rizzo G.
- Roberts D. A.
- Robertson S. H.
- Robutti E.
- Rodriguez FV
- Roney J. M.
- Roodman A.
- Rosenberg E. I.
- Rossi A.
- Rotondo M.
- Roudeau P.
- Rubin A. E.
- Ruland A. M.
- Sacco R.
- Saeed M. A.
- Salnikov A. A.
- Salvati E.
- Sanchez J
- Sanchez P. del Amo
- Santoro V.
- Schalk T.
- Schilling C. J.
- Schindler R. H.
- Schram M.
- Schroeder H.
- Schroeder T.
- Schubert K. R.
- Schumm B. A.
- Schune M. H.
- Schwiening J.
- Schwierz R.
- Schwitters R. F.
- Sciacca C.
- Sciolla G.
- Seiden A.
- Sekula S. J.
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- Strandberg J
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- Sundermann JE
- Suruliz K
- Sushkov S
- Susinno G
- Sutton MR
- Suzuki K.
- Suzuki Y
- Sviridov YM
- Swedish S
- Sykora I
- Sykora T
- Szeless B
- Ta D
- Tackmann K
- Taffard A
- Tafirout R
- Taga A
- Taiblum N
- Takahashi Y
- Takai H
- Takashima R
- Takeda H
- Takeshita T
- Talby M
- Talyshev A
- Tamsett MC
- Tanabe T.
- Tanaka J
- Tanaka R
- Tanaka S
- Tanaka S
- Tanaka Y
- Tani K
- Tannoury N
- Tappern GP
- Tapprogge S
- Taras P.
- Tardif D
- Tarem S
- Tarrade F
- Tartarelli GF
- Tas P
- Tasevsky M
- Tassi E
- Tatarkhanov M
- Taylor C
- Taylor FE
- Taylor GN
- Taylor W
- Teixeira-Dias P
- Telnov A. V.
- Temming KK
- Ten Kate H
- Teng PK
- Tenon J
- Terada S
- Terashi K
- Terwort M
- Testa M
- Teuscher RJ
- Tevlin CM
- Thadome J
- Therhaag J
- Theveneaux-Pelzer T
- Thioye M
- Thoma S
- Thomas JP
- Thompson AS
- Thompson EN
- Thompson J. M.
- Thompson PD
- Thompson PD
- Thomson E
- Thomson M
- Thun RP
- Tibbetts M.
- Tic T
- Tico J. Garra
- Tikhomirov V
- Tikhonov YA
- Timmermans CJWP
- Tipton P
- Tisserand V.
- Tisserant S
- Tobias J
- Toczek B
- Todorov T
- Todorova-Nova S
- Todyshev K. Yu.
- Toggerson B
- Tojo J
- Tokar S
- Toki W. H.
- Tokunaga K
- Tokushuku K
- Tollefson K
- Tomoto M
- Tompkins L
- Toms K
- Tonazzo A
- Tong G
- Tonoyan A
- Topfel C
- Topilin ND
- Torchiani I
- Torrence E
- Torrence E.
- Tosi S.
- Toth J
- Touchard F
- Touramanis C.
- Tovey DR
- Traynor D
- Trefzger T
- Treis J
- Tremblet L
- Tricoli A
- Trigger IM
- Trincaz-Duvoid S
- Trinh TN
- Tripiana MF
- Triplett N
- Trischuk W
- Trivedi A
- Trocme B
- Troncon C
- Trottier-McDonald M
- Trzupek A
- Tsarouchas C
- Tseng JCL
- Tsialciris M
- Tsiareshka PV
- Tsionou D
- Tsipolitis G
- Tsiskaridze V
- Tskhadadze EG
- Tsukerman O
- Tsulaia V
- Tsung JW
- Tsuno S
- Tsybychev D
- Tua A
- Tuggle J. M.
- Tuggle JM
- Turala M
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- Turlay E
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- Tykhonov A
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- Typaldos D
- Tyrvainen H
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- Uchida K
- Ueda I
- Ueno R
- Ugland M
- Uhlenbrock M
- Uhrmacher M
- Ukegawa F
- Unal G
- Underwood DG
- Undnis A
- Unel G
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- Urkovsky E
- Urrejola P
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- Wakisaka T.
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- Wang W. F.
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- Watson J. E.
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- Weinberger M.
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- West C. A.
- West T. J.
- Wester W. C. III
- White R. M.
- Whitehouse B.
- Whiteson D.
- Wick F.
- Wicklund A. B.
- Wicklund E.
- Wilbur S.
- Williams H. H.
- Wilson F. F.
- Wilson J. R.
- Wilson J. S.
- Wilson P.
- Winer B. L.
- Winstrom L. O.
- Wisniewski W. J.
- Wittgen M.
- Wittich P.
- Wolbers S.
- Wolfe H.
- Wormser G.
- Wray B. C.
- Wren A. C.
- Wright D. H.
- Wright D. M.
- Wright T.
- Wu S. L. Y
- Wu X.
- Wu Z.
- Wulsin H. W.
- Yamamoto K.
- Yamaoka J.
- Yang T.
- Yang U. K.
- Yang Y. C.
- Yao W. -M.
- Yarritu A. K.
- Yeche Ch.
- Yeh G. P.
- Yi K.
- Yoh J.
- Yorita K.
- Yoshida T.
- Young C. C.
- Yu G. B.
- Yu I.
- Yu S. S.
- Yun J. C.
- Yun J. C.
- Yushkov A. N.
- Zain S. B.
- Zallo A.
- Zanetti A.
- Zanetti A.
- Zeng Y.
- Zeng Y.
- Zhao M.
- Ziegler V.
- Zito M.
- Zucchelli S.
- Zucchelli S. Stradling AR
- Zucchelli SVazquez F.
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/11/2010
- Field of study
Using 347.5 fb-1 of data recorded by the BABAR detector at the PEP-II electron-positron collider, 244×103 signal events for the D+→K-π+e+νe decay channel are analyzed. This decay mode is dominated by the K̅ *(892)0 contribution. We determine the K̅ *(892)0 parameters: mK*(892)0=(895.4±0.2±0.2) MeV/c2, ΓK*(892)00=(46.5±0.3±0.2) MeV/c2, and the Blatt-Weisskopf parameter rBW=2.1±0.5±0.5 (GeV/c)-1, where the first uncertainty comes from statistics and the second from systematic uncertainties. We also measure the parameters defining the corresponding hadronic form factors at q2=0 (rV=V(0)/A1(0)=1.463±0.017±0.031, r2=A2(0)/A1(0)=0.801±0.020±0.020) and the value of the axial-vector pole mass parametrizing the q2 variation of A1 and A2: mA=(2.63±0.10±0.13) GeV/c2. The S-wave fraction is equal to (5.79±0.16±0.15)%. Other signal components correspond to fractions below 1%. Using the D+→K-π+π+ channel as a normalization, we measure the D+ semileptonic branching fraction: B(D+→K-π+e+νe)=(4.00±0.03±0.04±0.09)×10-2, where the third uncertainty comes from external inputs. We then obtain the value of the hadronic form factor A1 at q2=0: A1(0)=0.6200±0.0056±0.0065±0.0071. Fixing the P-wave parameters, we measure the phase of the S wave for several values of the Kπ mass. These results confirm those obtained with Kπ production at small momentum transfer in fixed target experiments
A study of radiative bottomonium transitions using converted photons
- Author
- Adametz A.
- Adye T.
- Ahmed H.
- Alam M. S.
- Albert J.
- Alwyn K. E.
- Andreassen R.
- ANGELINI CARLO
- Anh TV
- Anulli F.
- Arnaud N.
- Asgeirsson D. J.
- Aston D.
- Atmacan H.
- Ayad R.
- Bailey D.
- Baldini Ferroli R.
- Band H. R.
- Band H. R.
- Banerjee S.w.
- Bard D. J.
- Barlow R. J.
- Bartoldus R.
- BATIGNANI GIOVANNI
- Behera P. K.
- Bellis M.
- Ben Haim E.
- Benitez J. F.
- Bernard D.
- Bernlochner F. U.
- BETTARINI STEFANO
- Bettoni D.
- Bevan A. J.
- Bhuyan B.
- Bianchi F.
- Biasini M.
- Biassoni P.
- Bingham I.
- Blinov V. E.
- Bloom P. C.
- Bomben M.
- Bondioli M.
- Bonneaud G. R.
- Bozzi C.
- Brau J.
- Briand H.
- Brown D. N.
- Brown D. N.
- Buenger C.
- Burchat P. R.
- Buzykaev A. R.
- Cakir IT
- Calabrese R.
- Calcaterra A.
- CALDERINI GIOVANNI
- Campagnari C.
- Carpinelli M.
- Cartaro C.
- Casarosa G.
- Castanheira MTD
- Cavoto G.
- Cenci R.
- Cervelli A.
- Chauveau J.
- Chavez C. A.
- Chen C.
- Cheng C. H.
- Choi H. H. F.
- Choi H. H. F.
- Cibinetto G.
- Clark P. J.
- Cochran J.
- Coleman J. P.
- Contri R.
- Convery M. R.
- Cowan G.
- Cowan R.
- Crawley H. B.
- Cremaldi L.
- Curry S.
- Dallapiccola C.
- Dasu S.
- Dasu S.
- Dauncey P. D.
- Davier M.
- Davis C. L.
- de Monchenault G. Hamel
- De Nardo G.
- de Sangro R.
- Denig A. G.
- Derkach D.
- Di Lodovico F.
- Doll D. A.
- Dorfan J.
- Druzhinin V. P.
- Dubois Felsmann G. P.
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- Dujmic D.
- Dunwoodie W.
- Ebert M.
- Echenard B.
- Eckmann R.
- Edwards A. J.
- Eigen G.
- Eisner A. M.
- Emery S.
- Ernst J. A.
- Faccini R.
- Feltresi E.
- Ferrarotto F.
- Ferrer JAV
- Ferroni F.
- Field R. C.
- Finocchiaro G.
- Fioravanti E.
- Flood K. T.
- Ford W. T.
- FORTI FRANCESCO
- Frey R.
- Fritsch M.
- Fry J. R.
- Fulsom B. G.
- Gabareen A. M.
- Gabathuler E.
- Gagliardi N.
- Gallego EV
- Gamba D.
- Gary J. W.
- Garzia I.
- Gaspero M.
- Gaz A.
- Gershon T. J.
- Gershon T. J.
- Gioi L. Li
- GIORGI MARCELLO
- Godang R.
- Golubev V. B.
- Gorodeisky R.
- Gradl W.
- Graham M. T.
- Grauges E.
- Grenier P.
- Gritsan A. V.
- Grosdidier G.
- Guido E.
- Guo Z. J.
- Guttman N.
- Hafner A.
- Hamano K.
- Hamilton B.
- Hamon O.
- Harrison P. F.
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- Hartmann T.
- Hast C.
- Hearty C.
- Hitlin D. G.
- Hong T. M.
- Honscheid K.
- Hutchcroft D. E.
- Innes W. R.
- Izen J. M.
- Jackson G.
- Jawahery A.
- Jessop C. P.
- Kass R.
- Kelsey M. H.
- Kerth L. T.
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- Kim H.
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- Kirkby D.
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- Kobel M. J.
- Koch H.
- Kocian M. L.
- Kolomensky Y.u. G.
- Kovalskyi D.
- Kowalewski R.
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- Kroeger R.
- Kroseberg J.
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- Lanceri L.
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- Latham T. E.
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- Lazzaro A.
- Le Diberder F.
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- Lindquist B.
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- Liu F.
- Lo Vetere M.
- Lockman W. S.
- Lombardo V.
- Long O.
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- LoSecco J. M.
- Lou X. C.
- Lu C.
- Lueck T.
- Luitz S.
- Lund P.
- Luppi E.
- Lusiani A.
- Luth V.
- Lutz A. M.
- Lynch G.
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- MacFarlane D. B.
- Malaescu B.
- Mallik U.
- Mandelkern M.
- Manoni E.
- Marchiori G.
- Margoni M.
- Marks J.
- Martinelli M.
- Martinez A. J.
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- Mattison T. S.
- Mazzoni M. A.
- McKenna J. A.
- Meadows B. T.
- Meyer W. T.
- Milanes D. A.
- Milosavljevic MV
- Miyashita T. S.
- Monge M. R.
- Monorchio D.
- Morandin M.
- Morii M.
- Muller D. R.
- Munerato M.
- Nagel M.
- Nauenberg U.
- Neal H.
- Negrini M.
- Nelson S.
- Neri N.
- Nguyen X.
- Nicolaci M.
- Nugent I. M.
- Nugent I. M.
- Oberhof B.
- Ocariz J.
- Ofte I.
- Olaiya E. O.
- Olsen J.
- Ongmongkolkul P.
- Onorato G.
- Onuchin A. P.
- Oyanguren A.
- Pacetti S.
- Palano A.
- Palombo F.
- Pan Y.
- Pan Y.
- PAOLONI EUGENIO
- Pappagallo M.
- Paramesvaran S.
- Park W.
- Passaggio S.
- Pastor ET
- Patel P. M.
- Patrignani C.
- Patteri P.
- Payne D. J.
- Pegna D. Lopes
- Peimer D. R.
- Perez A.
- Perez MV
- Perl M.
- Peruzzi I. M.
- Piccolo M.
- Piemontese L.
- Piredda G.
- Playfer S.
- Poireau V.
- Porter F. C.
- Posocco M.
- Prasad V.
- Prell S.
- Prencipe E.
- Prepost R.
- Prepost R.
- Puccio E. M. T.
- Puccio E. M. T.
- Pulliam T.
- Purohit M. V.
- Rakitin A. Y.
- Rama M.
- Randle Conde A.
- Ratcliff B. N.
- Raven G.
- Richman J. D.
- Ritchie J. L.
- RIZZO GIULIANA
- Roberts D. A.
- Robertson S. H.
- Robutti E.
- Rodriguez FV
- Roney J. M.
- Roney J. M.
- Roodman A.
- Rosenberg E. I.
- Rossi A.
- Rotondo M.
- Roudeau P.
- Rubin A. E.
- Ruland A. M.
- Sacco R.
- Salnikov A. A.
- Salvati E.
- Sanchez J
- Santoro V.
- Schalk T.
- Schilling C. J.
- Schindler R. H.
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- Schroeder H.
- Schroeder T.
- Schubert K. R.
- Schumm B. A.
- Schune M. H.
- Schwierz R.
- Schwitters R. F.
- Sciacca C.
- Sciolla G.
- Seiden A.
- Sekula S. J.
- Serednyakov S. I.
- Sevilla M. Franco
- Sigamani M.
- Simi G.
- Simonetto F.
- Sinev N. B.
- Sitt S.
- Skovpen Y.u. I.
- Smith A. J. S.
- Smith J. G.
- Snoek H. L.
- Snyder A.
- Sobie R. J.
- Sobie R. J.
- Soffer A.
- Soh DA
- Sokoloff M. D.
- Solodov E. P.
- Sonnek P.
- Spaan B.
- Spanier S. M.
- Stocchi A.
- Stoker D. P.
- Stracka S.
- Straessner A
- Strandberg J
- Strandberg S
- Strandlie A
- Strang M
- Strauss E
- Strauss M
- Strizenec P
- Strohmer R
- Stroili R.
- Strom D.
- Strom DM
- Strong JA
- Stroynowski R
- Strube J
- Stugu B
- Stugu B.
- Stumer O
- Stupak J
- Sturm P
- Su D
- Su D.
- Subramania HS
- Sugaya Y
- Sugimoto T
- Suhr C
- Suita K
- Suk M
- Sulin VV
- Sullivan M. K.
- Sultansoy S
- Sumida T
- Summers D. J.
- Sun L.
- Sun X
- Sundermann JE
- Suruliz K
- Sushkov S
- Susinno G
- Sutton MR
- Suzuki Y
- Sviridov YM
- Swedish S
- Sykora I
- Sykora T
- Szeless B
- Ta D
- Tackmann K
- Taffard A
- Tafirout R
- Taga A
- Taiblum N
- Takahashi Y
- Takai H
- Takashima R
- Takeda H
- Takeshita T
- Talby M
- Talyshev A
- Tamsett MC
- Tanaka J
- Tanaka R
- Tanaka S
- Tanaka S
- Tanaka Y
- Tani K
- Tannoury N
- Tappern GP
- Tapprogge S
- Taras P.
- Tardif D
- Tarem S
- Tarrade F
- Tartarelli GF
- Tas P
- Tasevsky M
- Tassi E
- Tatarkhanov M
- Taylor C
- Taylor FE
- Taylor GN
- Taylor W
- Teixeira Dias P
- Telnov A. V.
- Temming KK
- Ten Kate H
- Teng PK
- Tenon J
- Terada S
- Terashi K
- Terwort M
- Testa M
- Teuscher RJ
- Tevlin CM
- Thadome J
- Therhaag J
- Theveneaux Pelzer T
- Thioye M
- Thoma S
- Thomas JP
- Thompson AS
- Thompson EN
- Thompson PD
- Thompson PD
- Thomson E
- Thomson M
- Thun RP
- Tibbetts M.
- Tic T
- Tico J. Garra
- Tikhomirov V
- Tikhonov YA
- Timmermans CJWP
- Tipton P
- Tisserand V.
- Tisserant S
- Tobias J
- Toczek B
- Todorov T
- Todorova Nova S
- Todyshev K. Y.u.
- Toggerson B
- Tojo J
- Tokar S
- Toki W. H.
- Tokunaga K
- Tokushuku K
- Tollefson K
- Tomoto M
- Tompkins L
- Toms K
- Tonazzo A
- Tong G
- Tonoyan A
- Topfel C
- Topilin ND
- Torchiani I
- Torrence E
- Torrence E.
- Toth J
- Touchard F
- Touramanis C.
- Tovey DR
- Traynor D
- Trefzger T
- Treis J
- Tremblet L
- Tricoli A
- Trigger IM
- Trincaz Duvoid S
- Trinh TN
- Tripiana MF
- Triplett N
- Trischuk W
- Trivedi A
- Trocme B
- Troncon C
- Trottier McDonald M
- Trzupek A
- Tsarouchas C
- Tseng JCL
- Tsialciris M
- Tsiareshka PV
- Tsionou D
- Tsipolitis G
- Tsiskaridze V
- Tskhadadze EG
- Tsukerman O
- Tsulaia V
- Tsung JW
- Tsuno S
- Tsybychev D
- Tua A
- Tuggle JM
- Turala M
- Turecek D
- Turlay E
- Turra R
- Tuts PM
- Tykhonov A
- Tylmad M
- Tyndel M
- Typaldos D
- Tyrvainen H
- Tzanakos G
- Uchida K
- Ueda I
- Ueno R
- Ugland M
- Uhlenbrock M
- Uhrmacher M
- Ukegawa F
- Unal G
- Underwood DG
- Undnis A
- Unel G
- Unno Y
- Urbaniec D
- Urkovsky E
- Urrejola P
- Usai G
- Uslenghi M
- Uwer U.
- Va'vra J.
- Vacavant L
- Vacek V
- Vachon B
- Vague FV
- Vahsen S
- Valderanis C
- Valenta J
- Valente P
- Valentinetti S
- Valkar S
- Vallecorsa S
- van der Graaf H
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- van Eldik N
- van Gemmeren P
- van Kesteren Z
- van Vulpen I
- Vandelli W
- Vandoni G
- Vaniachine A
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- Varnes EW
- Varouchas D
- Vartapetian A
- Varvell KE
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- Vassilakopoulos VI
- Vazeille F
- Vegni G
- Veillet JJ
- Velev G.
- Vellidis C
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- Verderi M.
- Verducci M.
- Verkerke W
- Vermeulen JC
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- Vetterli MC
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- Vickey T
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- Vorobiev AP
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- Vossebeld JH
- Vovenko AS
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- Wester W. C. III
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- Wisniewski W. J.
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- Wu S. L. Wallny R
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- Yamaoka J
- Yamaoka J.
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- Yang Y. C
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- Yao W. M
- Yao W. M.
- Yarritu A. K.
- Yeche C.h.
- Yeh G. P
- Yeh G. P.
- Yi K
- Yi K.
- Yoh J
- Yoh J.
- Yorita K
- Yorita K.
- Yoshida T
- Yoshida T.
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- Yu I
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- Yushkov A. N.
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- Zanetti A
- Zanetti A.
- Zanetti A.
- Zeng Y
- Zeng Y.
- Zeng Y.
- Ziegler V.
- Zucchelli S.
- Zucchelli S. Stradling AR
- Zucchelli SVazquez F.
- Publication venue
- American Physical Society
- Publication date
- 01/01/2011
- Field of study
19 pages, 7 figures, submitted to Phys. Rev. DWe use 111+/-1 million Upsilon(3S) and 89+/-1 million Upsilon(2S) events recorded by the BaBar detector at the PEP-II B-factory at SLAC to perform a study of radiative transitions between bottomonium states using photons that have been converted to e+e- pairs by the detector material. We observe Upsilon(3S) -> gamma chi_b0,2(1P) decay, make precise measurements of the branching fractions for chi_b1,2(1P,2P) -> gamma Upsilon(1S) and chi_b1,2(2P) -> gamma Upsilon(2S) decays, and search for radiative decay to the eta_b(1S) and eta_b(2S) states