908 research outputs found
Measurement of CP-violation asymmetries in D0 to Ks pi+ pi-
- Author
- Aaltonen T
- Ahmed S
- Alam MS
- Albert J
- Amerio S
- Amidei D
- Anastassov A
- Annovi A
- Antos J
- Apollinari G
- Appel JA
- Arisawa T
- Artikov A
- Asaadi J
- Ashmanskas W
- Auerbach B
- Aurisano A
- Azfar F
- Azzolini V
- Badgett W
- Bae T
- Band HR
- Banerjee S
- Barbaro-Galtieri A
- Barnes VE
- Barnett BA
- Barria P
- Bartos P
- Bauce M
- Bedeschi F
- Behari S
- Bellettini G
- Bellinger J
- Benjamin D
- Beretvas A
- Bhatti A
- Bhuyan B
- Bianchi F
- Bisello D
- Bizjak I
- Bland KR
- Blumenfeld B
- Bocci A
- Bodek A
- Bomben M
- Bortoletto D
- Bosisio L
- Boudreau J
- Boveia A
- Brigliadori L
- Bromberg C
- Brucken E
- Budagov J
- Budd HS
- Bula R
- Burchat PR
- Burkett K
- Busetto G
- Bussey P
- Buzatu A
- Calamba A
- Calancha C
- Camarda S
- Campanelli M
- Campbell M
- Canelli F
- Carls B
- Carlsmith D
- Carosi R
- Carrillo S
- Carron S
- Cartaro C
- Casal B
- Casarsa M
- Castro A
- Catastini P
- Cauz D
- Cavaliere V
- Cavalli-Sforza M
- Cerri A
- Cerrito L
- Chen X
- Chen YC
- Chertok M
- Chiarelli G
- Chlachidze G
- Chlebana F
- Cho K
- Chokheli D
- Chung WH
- Chung YS
- Ciocci MA
- Clark A
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- Convery ME
- Conway J
- Corbo M
- Cordelli M
- Cossutti F
- Cox CA
- Cox DJ
- Crescioli F
- Cuevas J
- Culbertson R
- d'Ascenzo N
- d'Errico M
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- da Costa JG
- Dagenhart D
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- Datta M
- de Barbaro P
- Dell'Orso M
- Della Ricca G
- Demortier L
- Deninno M
- Devoto F
- Di Canto A
- Di Ruzza B
- Dittmann JR
- Donati S
- Dong P
- Dorigo M
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- Ebina K
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- Edwards AJ
- Elagin A
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- Errede S
- Ershaidat N
- Eusebi R
- Farrington S
- Feindt M
- Fernandez JP
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- Flood KT
- Forrest R
- Frank MJ
- Franklin M
- Freeman JC
- Funakoshi Y
- Furic I
- Gallinaro M
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- Garfinkel AF
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- Gerberich H
- Gerchtein E
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- Golossanov A
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- Goncharov M
- Gonzalez BA
- Gonzalez O
- Gorelov I
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- Goulianos K
- Grinstein S
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- Grosso-Pilcher C
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- Halkiadakis E
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- Hatakeyama K
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- Jain V
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- Ketchum W
- Keung J
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- Kilminster B
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- Luitz S
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- Mattson ME
- Mazzacane A
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- McFarland KS
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- Okusawa T
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- Redondo I
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- Rimondi F
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- Russ J
- Rusu V
- Saeed MA
- Safonov A
- Sakumoto WK
- Sakurai Y
- Salnikov AA
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- Saveliev V
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- Schilling CJ
- Schindler RH
- Schlabach P
- Schmidt A
- Schmidt EE
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- Schwiening J
- Schwitters RF
- Scodellaro L
- Scribano A
- Scuri F
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- Shalhout SZ
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- Shepard PF
- Shimojima M
- Shochet M
- Shreyber-Tecker I
- Simonenko A
- Sinervo P
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- Smith JR
- Snider FD
- Snyder A
- Sobie RJ
- Soha A
- Song H
- Sorin V
- Spanier SM
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- Teng PK
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- Thompson GA
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- Trovato M
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- Uozumi S
- Va'vra J
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- Wallny R
- Wang SM
- Wappler FR
- Warburton A
- Waters D
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- Wicklund E
- Wilbur S
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- Wisniewski WJ
- Wittgen M
- Wittich P
- Wolbers S
- Wolfe H
- Wright DH
- Wright T
- Wu SL
- Wu X
- Wu Z
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- Yamato D
- Yang T
- Yang UK
- Yang YC
- Yao WM
- Yarritu AK
- Ye S
- Yeh GP
- Yi K
- Yi K
- Yoh J
- Yorita K
- Yoshida T
- Young CC
- Yu GB
- Yu I
- Yu SS
- Yun JC
- Zain SB
- Zanetti A
- Zeng Y
- Zhou C
- Ziegler V
- Zucchelli S
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2012
- Field of study
We report a measurement of time-integrated CP-violation asymmetries in the
resonant substructure of the three-body decay D0 to Ks pi+ pi- using CDF II
data corresponding to 6.0 invfb of integrated luminosity from Tevatron ppbar
collisions at sqrt(s) = 1.96 TeV. The charm mesons used in this analysis come
from D*+(2010) to D0 pi+ and D*-(2010) to D0bar pi-, where the production
flavor of the charm meson is determined by the charge of the accompanying pion.
We apply a Dalitz-amplitude analysis for the description of the dynamic decay
structure and use two complementary approaches, namely a full Dalitz-plot fit
employing the isobar model for the contributing resonances and a
model-independent bin-by-bin comparison of the D0 and D0bar Dalitz plots. We
find no CP-violation effects and measure an asymmetry of ACP = (-0.05 +- 0.57
(stat) +- 0.54 (syst))% for the overall integrated CP-violation asymmetry,
consistent with the standard model prediction.Comment: 15 page
Search for new phenomena in final states with an energetic jet and large missing transverse momentum in pp collisions at √ s = 8 TeV with the ATLAS detector
- Author
- Aad G
- Abbott B
- Abbott DC
- Abeling K
- Abhayasinghe DK
- Abidi SH
- AbouZeid OS
- Abraham NL
- Abramowicz H
- Abreu H
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- Acharya BS
- Achkar B
- Adachi S
- Adam L
- Adamczyk L
- Adamek L
- Adelman J
- Adersberger M
- Adiguzel A
- Adorni S
- Adye T
- Affolder AA
- Afik Y
- Agapopoulou C
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- Alberghi GL
- Albert J
- Alderweireldt S
- Aleksa M
- Aleksandrov IN
- Alexa C
- Alexopoulos T
- Alfonsi A
- Alfonsi F
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- Ali B
- Aliev M
- Alimonti G
- Allaire C
- Allbrooke BMM
- Allen BW
- Allport PP
- Aloisio A
- Alonso F
- Alpigiani C
- Alshehri AA
- Alvarez Estevez M
- Alviggi MG
- Amaral Coutinho Y
- Ambler A
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- de Renstrom PAB
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- De Salvo A
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- Denisov SP
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- Zhemchugov A
- Zheng Z
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- Zimmermann S
- Zinonos Z
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- Zou R
- Zu Theenhausen HM
- Zwalinski L
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2015
- Field of study
Results of a search for new phenomena in final states with an energetic jet and large missing transverse momentum are reported. The search uses 20.3 fb−1 of √ s = 8 TeV data collected in 2012 with the ATLAS detector at the LHC. Events are required to have at least one jet with pT > 120 GeV and no leptons. Nine signal regions are considered with increasing missing transverse momentum requirements between Emiss T > 150 GeV and Emiss T > 700 GeV. Good agreement is observed between the number of events in data and Standard Model expectations. The results are translated into exclusion limits on models with either large extra spatial dimensions, pair production of weakly interacting dark matter candidates, or production of very light gravitinos in a gauge-mediated supersymmetric model. In addition, limits on the production of an invisibly decaying Higgs-like boson leading to similar topologies in the final state are presente
Search for rare quark-annihilation decays, B --> Ds(*) Phi
- Author
- Abe T
- Abrams GS
- Adye T
- Ahmed M
- Ahmed S
- Alam MS
- Albert J
- Aleksan R
- Allen MT
- Allison J
- Allmendinger T
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- Andreassen R
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- Arnaud N
- Aston D
- Aubert B
- Azzolini V
- Baak M
- Back JJ
- Baldini-Ferroli R
- Band HR
- Banerjee S
- Barate R
- Bard DJ
- Barlow NR
- Barlow RJ
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- Bartoldus R
- Batignani G
- Battaglia M
- Bauer JM
- Beck TW
- Behera PK
- Bellini F
- Benayoun M
- Benelli G
- Berger N
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- Berryhill JW
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- Bettoni D
- Bevan AJ
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- Bhuyan B
- Bianchi F
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- Blanc F
- Blaylock G
- Blinov AE
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- Bloom PC
- Blount NL
- Bomben M
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- Bondioli M
- Bonneaud GR
- Bosisio L
- Boutigny D
- Bowerman DA
- Boyarski AM
- Boyd JT
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- Breon AB
- Brose J
- Brown CL
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- Brunet S
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- Bukin AD
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- Bulten H
- Buono LD
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- Burke JP
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- Calcaterra A
- Calderini G
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- Cenci R
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- D'Orazio A
- Dahmes B
- Dallapiccola C
- Danielson N
- Dasu S
- Datta M
- Dauncey PD
- David P
- Davier M
- Davis CL
- Day CT
- de la Vaissiere C
- de Monchenault GH
- de Sangro R
- del Re D
- Diberder FL
- Dickopp M
- Dingfelder JC
- Dittongo S
- Dong D
- Dong L
- Dorfan J
- Druzhinin VP
- Dubitzky RS
- Dubois-Felsmann GP
- Dujmic D
- Dunwoodie W
- Dvoretskii A
- Eckhart EA
- Eckmann R
- Edgar CL
- Edwards AJ
- Egede U
- Eichenbaum AM
- Eigen G
- Eisner AM
- Elmer P
- Emery S
- Ernst JA
- Eschenburg V
- Eschrich I
- Eyges V
- Fabozzi F
- Faccini R
- Fan S
- Feltresi E
- Ferrarotto F
- Ferroni F
- Field RC
- Finocchiaro G
- Flacco CJ
- Flack RL
- Flaecher HU
- Flood KT
- Ford KE
- Ford WT
- Forster IJ
- Forti F
- Fortin D
- Foulkes SD
- Franek B
- Frey R
- Fritsch M
- Fry JR
- Fulsom BG
- Gabathuler E
- Gaidot A
- Gaillard JR
- Galeazzi F
- Gallo F
- Gamba D
- Gamet R
- Gan KK
- Ganzhur SF
- Gary JW
- Gaspero M
- Gatto C
- George KA
- Gill MS
- Gioi LL
- Giorgi MA
- Giroux X
- Gladney L
- Glanzman T
- Godang R
- Goetzen K
- Golubev VB
- Gopal GP
- Gowdy SJ
- Gradl W
- Graham MT
- Grancagnolo S
- Grauges E
- Graziani G
- Green MG
- Grenier P
- Gritsan AV
- Groot ND
- Grosdidier G
- Groysman Y
- Guo QH
- Hadavand HK
- Hadig T
- Haire M
- Halyo V
- Hamano K
- Hamon O
- Harrison PF
- Harrison TJ
- Hart AJ
- Hartfiel BL
- Hast C
- Hauke A
- Hawkes CM
- Hearty C
- Held T
- Hertzbach SS
- Heusch CA
- Hill EJ
- Hirschauer JF
- Hitlin DG
- Hocker A
- Hodgkinson MC
- Hollar JJ
- Hong TM
- Honscheid K
- Hopkins DA
- Hryn'ova T
- Hufnagel D
- Hulsbergen WD
- Hutchcroft DE
- Igonkina O
- Innes WR
- Izen JM
- Jackson PD
- Jackson PS
- Jacobsen RG
- Jawahery A
- Jessop CP
- John MJJ
- Johnson JR
- Judd D
- Kadel RW
- Kadyk J
- Kagan H
- Karyotakis Y
- Kass R
- Kelly MP
- Kelsey MH
- Kerth LT
- Khan A
- Kim H
- Kim P
- Kirkby D
- Kitayama I
- Klose V
- Knecht NS
- Koch H
- Kocian ML
- Koeneke K
- Kofler R
- Kolomensky YG
- Kovalskyi D
- Kowalewski R
- Kozanecki W
- Kravchenko EA
- Kreisel A
- Krishnamurthy M
- Kroeger R
- Kroseberg J
- Kukartsev G
- Kutter PE
- Kyberd P
- Lacker HM
- Lae CK
- Lafferty GD
- Lanceri L
- Lange DJ
- Langenegger U
- Lankford AJ
- Latham TE
- Latour E
- Lau YP
- Lazzaro A
- Lees JP
- Legendre M
- Leith DWGS
- Lepeltier V
- Leruste P
- Lewandowski B
- Li H
- Li X
- Libby J
- Lista L
- Liu R
- Lockman WS
- Lodovico FD
- Lombardo V
- London GW
- Long O
- LoSecco JM
- Lou XC
- Lu C
- Lu M
- Luitz S
- Lund P
- Luppi E
- Lusiani A
- Luth V
- Lutz AM
- Lynch G
- Lynch HL
- MacFarlane DB
- Macri MM
- Mader WF
- Majewski SA
- Malcles J
- Mallik U
- Mancinelli G
- Mandelkern M
- Marchiori G
- Marco ED
- Margoni M
- Marks J
- Marsiske H
- Martinez-Vidal F
- Mattison TS
- Mayer B
- Mazur MA
- Mazzoni MA
- McKenna JA
- McMahon TR
- Meadows BT
- Mellado B
- Menges W
- Messner R
- Meyer WT
- Mihalyi A
- Minamora JS
- Mir LM
- Mohanty GB
- Mohapatra AK
- Mommsen RK
- Monge MR
- Monorchio D
- Moore TB
- Morandin M
- Morgan SE
- Morganti M
- Morganti S
- Morii M
- Muheim F
- Muller DR
- Naisbit MT
- Nardo GD
- Narsky I
- Nash JA
- Nauenberg U
- Neal H
- Negrini M
- Neri N
- Nesom G
- Nicholson H
- Nikolich MB
- Nogowski R
- Nugent IM
- O'Grady CP
- Ocariz J
- Oddone PJ
- Ofte I
- Olaiya EO
- Olivas A
- Olsen J
- Onuchin AP
- Orimoto TJ
- Otto S
- Oyanguren A
- Ozcan VE
- Paar HP
- Pacetti S
- Palano A
- Palombo F
- Pan Y
- Panetta J
- Panvini RS
- Paoloni E
- Paolucci P
- Pappagallo M
- Parry RJ
- Passaggio S
- Patel PM
- Patrignani C
- Patteri P
- Payne DJ
- Pelizaeus M
- Perazzo A
- Perl M
- Peruzzi IM
- Peters K
- Petersen BA
- Petersen TC
- Petzold A
- Piatenko T
- Piccolo D
- Piccolo M
- Piemontese L
- Pierini M
- Pioppi M
- Piredda G
- Plaszczynski S
- Playfer S
- Poireau V
- Polci F
- Pompili A
- Porter FC
- Posocco M
- Potter CT
- Prell S
- Prepost R
- Pripstein M
- Pulliam T
- Purohit MV
- Qi ND
- Rahatlou S
- Rahimi AM
- Rahmat R
- Rama M
- Ratcliff BN
- Raven G
- Reidy J
- Ricca GD
- Ricciardi S
- Richman JD
- Ritchie JL
- Rizzo G
- Roat C
- Roberts DA
- Robertson SH
- Robutti E
- Rodier S
- Roe NA
- Roethel W
- Ronan MT
- Roney JM
- Rong G
- Roodman A
- Roos L
- Rosenberg EI
- Rotondo M
- Roudeau P
- Rubin AE
- Ruddick WO
- Ryd A
- Sacco R
- Saeed MA
- Saleem M
- Salnikov AA
- Salvatore F
- Samuel A
- Sanders DA
- Santroni A
- Saremi S
- Satpathy A
- Schalk T
- Schenk S
- Schindler RH
- Schofield KC
- Schott G
- Schrenk S
- Schroder H
- Schroeder T
- Schubert J
- Schubert KR
- Schumm BA
- Schune MH
- Schwiening J
- Schwierz R
- Schwitters RF
- Sciacca C
- Sciolla G
- Seiden A
- Sekula SJ
- Serednyakov SI
- Sharma V
- Shen BC
- Simi G
- Simonetto F
- Sinev NB
- Skovpen YI
- Smith AJS
- Smith JG
- Snoek HL
- Snyder A
- Sobie RJ
- Soffer A
- Sokoloff MD
- Solodov EP
- Spaan B
- Spanier SM
- Spitznagel M
- Spradlin P
- Staengle H
- Steinke M
- Stelzer J
- Stocchi A
- Stoker DP
- Stroili R
- Strom D
- Strube J
- Stugu B
- Su D
- Sullivan MK
- Summers DJ
- Sundermann JE
- Suzuki K
- Swain SK
- Tan P
- Taras P
- Taylor F
- Tehrani FS
- Telnov AV
- Teodorescu L
- Ter-Antonyan R
- Therin G
- Thiebaux C
- Thompson JM
- Tisserand V
- Toki WH
- Torrence E
- Tosi S
- Touramanis C
- Ulmer KA
- Uwer U
- Va'vra J
- van Bakel N
- Vasileiadis G
- Vasseur G
- Vazquez WP
- Verderi M
- Verkerke W
- Vetere ML
- Viaud FB
- Vitale L
- Voci C
- Voena C
- Wagner SR
- Wagoner DE
- Waldi R
- Walsh J
- Wang K
- Wang P
- Wang WF
- Wappler FR
- Watson AT
- Weaver M
- Weidemann AW
- Weinstein AJR
- Wenzel WA
- Wilden L
- Williams DC
- Williams JC
- Willocq SY
- Wilson FF
- Wilson JR
- Wilson MG
- Wilson RJ
- Winklmeier F
- Wisniewski WJ
- Wittgen M
- Wong QK
- Wormser G
- Wright DH
- Wright DM
- Wu J
- Wu SL
- Xie Y
- Yamamoto RK
- Yarritu AK
- Ye S
- Yeche C
- Yi JI
- Yi K
- Young CC
- Yu Z
- Yushkov AN
- Zain SB
- Zallo A
- Zeng Q
- Zghiche A
- Zhang J
- Zhang L
- Zhao HW
- Zhu YS
- Ziegler V
- Zito M
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 12/12/2005
- Field of study
We report on searches for B- --> Ds- Phi and B- --> Ds*- Phi. In the context
of the Standard Model, these decays are expected to be highly suppressed since
they proceed through annihilation of the b and u-bar quarks in the B- meson.
Our results are based on 234 million Upsilon(4S) --> B Bbar decays collected
with the BABAR detector at SLAC. We find no evidence for these decays, and we
set Bayesian 90% confidence level upper limits on the branching fractions BF(B-
--> Ds- Phi) Ds*- Phi)<1.2x10^(-5). These results
are consistent with Standard Model expectations.Comment: 8 pages, 3 postscript figues, submitted to Phys. Rev. D (Rapid
Communications
Observation and study of baryonic B decays: B -> D(*) p pbar, D(*) p pbar pi, and D(*) p pbar pi pi
- Author
- Adametz A
- Adye T
- Ahmed S
- Ahmed S
- Alam MS
- Alam MS
- Albert J
- Albert J
- Allen MT
- Alwyn KE
- Anderson J
- Andreassen R
- Andreotti M
- Angelini C
- Anulli F
- Arnaud N
- Asgeirsson DJ
- Aston D
- Atmacan H
- Ayad R
- Azzolini V
- Bailey D
- Baldini-Ferroli R
- Band HR
- Band HR
- Banerjee S
- Banerjee S
- Baracchini E
- Bard DJ
- Barlow RJ
- Bartoldus R
- Batignani G
- Battaglia M
- Behera PK
- Bellis M
- Ben-Haim E
- Benitez JF
- Bernard D
- Bernlochner FU
- Bettarini S
- Bettoni D
- Bevan AJ
- Bhuyan B
- Bhuyan B
- Bianchi F
- Bianchi F
- Biasini M
- Biassoni P
- Bingham I
- Blinov VE
- Bloom PC
- Blount NL
- Bomben M
- Bomben M
- Bondioli M
- Bonneaud GR
- Bosisio L
- Bozzi C
- Brau J
- Briand H
- Brown DN
- Brown DN
- Bula R
- Burchat PR
- Burchat PR
- Buzykaev AR
- Calabrese R
- Calcaterra A
- Calderini G
- Campagnari C
- Carpinelli M
- Cartaro C
- Cartaro C
- Casarosa G
- Castelli G
- Cavoto G
- Cecchi A
- Cenci R
- Cervelli A
- Chauveau J
- Chavez CA
- Chen C
- Chen X
- Chen XR
- Cheng CH
- Choi HHF
- Cibinetto G
- Clark PJ
- Cochranz J
- Coleman JP
- Contri R
- Convery MR
- Corwin LA
- Cossutti F
- Cowan G
- Cowan R
- Crawley HB
- Cremaldi L
- Curry S
- da Costa JF
- Dallapiccola C
- Dasu S
- Dasu S
- Dauncey PD
- Davier M
- Davis CL
- de Monchenault GH
- De Nardo G
- de Sangro R
- Della Ricca G
- Denig AG
- Derkach D
- Di Lodovico F
- Doll DA
- Dong L
- Dorfan J
- Druzhinin VP
- Dubois-Felsmann GP
- Dubrovin MS
- Dujmic D
- Dunwoodie W
- Ebert M
- Echenard B
- Eckmann R
- Eckmann R
- Edwards AJ
- Edwards AJ
- Eigen G
- Eisner AM
- Emery S
- Ernst JA
- Ernst JA
- Faccini R
- Feltresi E
- Ferrarotto F
- Ferroni F
- Field RC
- Finocchiaro G
- Fioravanti E
- Flanigan JM
- Flood KT
- Flood KT
- Ford WT
- Forti F
- Franchini P
- Franek B
- Frey R
- Fritsch M
- Fry JR
- Fulsom BG
- Gabareen AM
- Gabathuler E
- Gagliardi N
- Gallo F
- Gamba D
- Gamba D
- Gamet R
- Gary JW
- Gaspero M
- Gaz A
- Gershon TJ
- Gioi LL
- Giorgi MA
- Godang R
- Golubev VB
- Gradl W
- Graham MT
- Grauges E
- Grenier P
- Gritsan AV
- Grosdidier G
- Guido E
- Guo ZJ
- Guttman N
- Hafner A
- Hamano K
- Hamano K
- Hamon O
- Harrison PF
- Harrison PF
- Hartmann T
- Hast C
- Hawkes CM
- Hearty C
- Heusch CA
- Hitlin DG
- Hollar JJ
- Hong TM
- Honscheid K
- Hooberman B
- Hutchcroft DE
- Igonkina O
- Ilic J
- Innes WR
- Izen JM
- Izen JM
- Jackson G
- Jain V
- Jasper H
- Jawahery A
- Jessop CP
- Karbach TM
- Kass R
- Kelsey MH
- Kerth LT
- Khan A
- Kim H
- Kim P
- Kim P
- King GJ
- Kirkby D
- Knoepfel KJ
- Kobel MJ
- Koch H
- Kocian ML
- Kocian ML
- Kolb JA
- Kolomensky YG
- Kovalskyi D
- Kowalewski R
- Kowalewski R
- Krishnamurthy M
- Kroeger R
- Kroseberg J
- Kutter PE
- Lacker HM
- Lafferty GD
- Lanceri L
- Lanceri L
- Lange DJ
- Lankford AJ
- Latham TE
- Latham TE
- Lazzaro A
- Le Diberder F
- Leddig T
- Lee CL
- Lees JP
- Leith DWGS
- Leith DWGS
- Leruste P
- Lewczuk MJ
- Li S
- Li S
- Lindemann D
- Lindquist B
- Liu F
- Lo Vetere M
- Lockman WS
- Lombardo V
- Long O
- Lopez-March N
- Lopez-March N
- LoSecco JM
- Lou XC
- Lou XC
- Lu C
- Lueck T
- Luitz S
- Luitz S
- Lund P
- Luppi E
- Lusiani A
- Luth V
- Luth V
- Lutz AM
- Lynch G
- Lynch HL
- Lynch HL
- MacFarlane DB
- MacFarlane DB
- Majewski SA
- Malaescu B
- Mallik U
- Mancinelli G
- Mandelkern M
- Manoni E
- Marchiori G
- Margoni M
- Marks J
- Marsiske H
- Marsiske H
- Martin EC
- Martinelli M
- Martinez AJ
- Martinez-Vidal F
- Martinez-Vidal F
- Mattison TS
- Mazzoni MA
- McKenna JA
- Meadows BT
- Merkel J
- Messner R
- Meyer WT
- Milanes DA
- Milanes DA
- Miyashita TS
- Miyashita TS
- Mohanty GB
- Monge MR
- Monorchio D
- Morandin M
- Morii M
- Morris JP
- Muller DR
- Muller DR
- Munerato M
- Nagel M
- Nauenberg U
- Neal H
- Neal H
- Negrini M
- Nelson S
- Neri N
- Nguyen X
- Nicolaci M
- Nugent IM
- Nugent IM
- O'Grady CP
- O'Grady CP
- Ocariz J
- Ofte I
- Ofte I
- Olaiya EO
- Olsen J
- Ongmongkolkul P
- Onorato G
- Onuchin AP
- Osipenkov IL
- Oyanguren A
- Oyanguren A
- Pacetti S
- Palano A
- Palombo F
- Pan B
- Pan B
- Pan Y
- Pan Y
- Paoloni E
- Pappagallo M
- Paramesvaran S
- Park W
- Passaggio S
- Patel PM
- Patrignani C
- Patteri P
- Payne DJ
- Pegna DL
- Pelliccioni M
- Pelliccioni M
- Perazzo A
- Perez A
- Perl M
- Perl M
- Peruzzi IM
- Petersen BA
- Petrella A
- Petzold A
- Piccolo M
- Piemontese L
- Pierini M
- Piredda G
- Playfer S
- Poireau V
- Porter FC
- Posocco M
- Prasad V
- Prell S
- Prencipe E
- Prendki J
- Prepost R
- Prepost R
- Puccio EMT
- Pulliam T
- Pulliam T
- Purohit MV
- Rahmat R
- Rakitin AY
- Rama M
- Randle-Conde A
- Ratcliff BN
- Ratcliff BN
- Raven G
- Renga F
- Richman JD
- Ritchie JL
- Ritchie JL
- Rizzo G
- Roberts DA
- Robertson SH
- Robutti E
- Roney JM
- Roney JM
- Roodman A
- Roodman A
- Rosenberg EI
- Rossi A
- Rotondo M
- Roudeau P
- Rubin AE
- Ruland AM
- Ruland AM
- Sacco R
- Saeed MA
- Saeed MA
- Salnikov AA
- Salnikov AA
- Salvati E
- Sanchez PDA
- Santoro V
- Schalk T
- Schilling CJ
- Schilling CJ
- Schindler RH
- Schindler RH
- Schram M
- Schroeder H
- Schroeder T
- Schubert KR
- Schumm BA
- Schune MH
- Schwiening J
- Schwiening J
- Schwierz R
- Schwitters RF
- Schwitters RF
- Sciacca C
- Sciolla G
- Seiden A
- Sekula SJ
- Serednyakov SI
- Serrano J
- Sevilla MF
- Sigamani M
- Simard M
- Simi G
- Simonetto F
- Sinev NB
- Sitt S
- Skovpen YI
- Smith AJS
- Smith JG
- Snoek HL
- Snyder A
- Snyder A
- Sobie RJ
- Sobie RJ
- Soffer A
- Sokoloff MD
- Solodov EP
- Sonnek P
- Sordini V
- Spaan B
- Spanier SM
- Spanier SM
- Stocchi A
- Stoker DP
- Stracka S
- Stroili R
- Strom D
- Strube J
- Stugu B
- Su D
- Su D
- Sullivan MK
- Sullivan MK
- Summers DJ
- Sun L
- Sun S
- Suzuki K
- Suzuki K
- Swain SK
- Tanabe T
- Taras P
- Telnov AV
- Thompson JM
- Thompson JM
- Tibbetts M
- Tico JG
- Tisserand V
- Todyshev KY
- Toki WH
- Torrence E
- Tosi S
- Touramanis C
- Tuggle JM
- Uwer U
- Va'vra J
- Va'vra J
- Vasseur G
- Verderi M
- Vitale L
- Vitale L
- Vitug GM
- Volk A
- Vuosalo CO
- Wacker K
- Wagner AP
- Wagner AP
- Wagner SR
- Waldi R
- Walsh JJ
- Wang L
- Wang WF
- Wappler FR
- Watson AT
- Watson JE
- Weaver M
- Weaver M
- West C
- West CA
- White RM
- Wilden L
- Wilson FF
- Wilson JR
- Wilson P
- Winer BL
- Winstrom LO
- Wisniewski WJ
- Wisniewski WJ
- Wittgen M
- Wittgen M
- Wittich P
- Wolbers S
- Wolfe H
- Wormser G
- Wray BC
- Wren AC
- Wright DH
- Wright DH
- Wright DM
- Wright T
- Wu SL
- Wu SL
- Wu X
- Wu Z
- Wulsin HW
- Yamamoto K
- Yamato D
- Yang T
- Yang UK
- Yang YC
- Yao WM
- Yarritu AK
- Yarritu AK
- Ye S
- Yeche C
- Yeh GP
- Yi K
- Yi K
- Yoh J
- Yorita K
- Yoshida T
- Young CC
- Young CC
- Yu GB
- Yu I
- Yu SS
- Yun JC
- Yushkov AN
- Zain SB
- Zain SB
- Zallo A
- Zanetti A
- Zeng Y
- Zhao M
- Zhou C
- Ziegler V
- Ziegler V
- Zito M
- Zucchelli S
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 15/08/2009
- Field of study
We present a study of ten B-meson decays to a D(*), a proton-antiproton pair,
and a system of up to two pions using BaBar's data set of 455x10^6 BBbar pairs.
Four of the modes (B0bar -> D0 p anti-p, B0bar -> D*0 p anti-p, B0bar -> D+ p
anti-p pi-, B0bar -> D*+ p anti-p pi-) are studied with improved statistics
compared to previous measurements; six of the modes (B- -> D0 p anti-p pi-, B-
-> D*0 p anti-p pi-, B0bar -> D0 p anti-p pi- pi+, B0bar -> D*0 p anti-p pi-
pi+, B- -> D+ p anti-p pi- pi-, B- -> D*+ p anti-p pi- pi-) are first
observations. The branching fractions for 3- and 5-body decays are suppressed
compared to 4-body decays. Kinematic distributions for 3-body decays show
non-overlapping threshold enhancements in m(p anti-p) and m(D(*)0 p) in the
Dalitz plots. For 4-body decays, m(p pi-) mass projections show a narrow peak
with mass and full width of (1497.4 +- 3.0 +- 0.9) MeV/c2, and (47 +- 12 +- 4)
MeV/c2, respectively, where the first (second) errors are statistical
(systematic). For 5-body decays, mass projections are similar to phase space
expectations. All results are preliminary.Comment: 28 pages, 90 postscript figures, submitted to LP0
Development of estimates of dietary nitrates, nitrites, and nitrosamines for use with the short willet food frequency questionnaire
- Author
- A Petersen
- A Pomeranz
- A Wawrzniak
- A Wawrzyniak
- AJ Vecchio
- Antonio A Rene
- AR Tricker
- AR Tricker
- B Spiegelhalder
- B Thomson
- BC Choi
- BG Osterdahl
- BJ Canas
- CL Walters
- D Klein
- D Pobel
- DC Havery
- DC Havery
- DC Paik
- DP Huang
- E Pedersen
- EF Binkerd
- Food Standards Agency: Joint Food Safety Standards Group
- French National Inventory
- G Saccani
- GR Howe
- H Bartsch
- H Mahieu
- I Stepanov
- J Brender
- J Cornee
- J Farrell
- J Siciliano
- Jean D Brender
- JH Hotchkiss
- John C Huber
- John S Griesenbeck
- Joseph R Sharkey
- JT Bernert
- KA Walters
- L Lakritz
- L Merino
- LM Libbey
- M Dietrich
- M Inouye
- M Matsui
- M Siddiqi
- M Yamamoto
- MH Ward
- Michelle D Steck
- MJ Dennis
- MP Longnecker
- MR Ashton
- National Academy of Sciences
- National Academy of Sciences
- NB Kyriakidis
- NP Sen
- NP Sen
- P Jakszyn
- P VonCollett
- PE Key
- PW Yoon
- R Fudge
- RA Bloomfield
- RA Scanlan
- S Westmoreland
- StataCorp
- SY Chung
- T Koyama
- T Maki
- T Tamme
- TM Knight
- W Lijinsky
- WC Willett
- WC Willett
- Publication venue
- BioMed Central
- Publication date
- 01/01/2009
- Field of study
<p>Abstract</p> <p>Background</p> <p>Studies have suggested that nitrates, nitrites, and nitrosamines have an etiologic role in adverse pregnancy outcomes and chronic diseases such as cancer. Although an extensive body of literature exists on estimates of these compounds in foods, the extant data varies in quality, quantified estimates, and relevance.</p> <p>Methods</p> <p>We developed estimates of nitrates, nitrites, and nitrosamines for food items listed in the Short Willet Food Frequency Questionnaire (WFFQ) as adapted for use in the National Birth Defects Prevention Study. Multiple reference databases were searched for published literature reflecting nitrate, nitrite, and nitrosamine values in foods. Relevant published literature was reviewed; only publications reporting results for items listed on the WFFQ were selected for inclusion. The references selected were prioritized according to relevance to the U.S. population.</p> <p>Results</p> <p>Based on our estimates, vegetable products contain the highest levels of nitrate, contributing as much as 189 mg/serving. Meat and bean products contain the highest levels of nitrites with values up to 1.84 mg/serving. Alcohol, meat and dairy products contain the highest values of nitrosamines with a maximum value of 0.531 μg/serving. The estimates of dietary nitrates, nitrites, and nitrosamines generated in this study are based on the published values currently available.</p> <p>Conclusion</p> <p>To our knowledge, these are the only estimates specifically designed for use with the adapted WFFQ and generated to represent food items available to the U.S. population. The estimates provided may be useful in other research studies, specifically in those exploring the relation between exposure to these compounds in foods and adverse health outcomes.</p
Economic and sociodemographic inequalities in complete denture need among older Brazilian adults: a cross-sectional population-based study
- Author
- A Andreas Zenthöfer
- AG Roncalli
- AG Roncalli
- AMEB Martins
- Angelo Giuseppe Roncalli
- Daniela Mendes da Veiga Pessoa
- G Piuvezam
- GA Pucca Junior
- J Harford
- J Nadgere
- JA Haro
- JMA Giordani
- Kenio Costa de Lima
- M Marmot
- MA Peres
- MA Peres
- National Commission on the Social Determinants of Health
- P Hersch-Martínez
- PE Petersen
- PR Barbato
- R Mariño
- RK Saarela
- RS Moreira
- S Listl
- T Yamamoto
- VR Aguiar
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- Field of study
Observation of the Decay B=> J/psi eta K and Search for X(3872)=> J/psi eta
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- Abe K
- Abe T
- Abrams GS
- Adye T
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- Albert J
- Aleksan R
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- Andreotti M
- Angelini C
- Anulli F
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- von Wimmersperg-Toeller JH
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- Yun JC
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- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2004
- Field of study
We report the observation of the B meson decay B±→J/ψηK±
and evidence for the decay B0→J/ψηKS0, using {90} million
BBbar events collected at the \ensuremath{\Upsilon{(4S)}}\xspace resonance
with the BaBar detector at the PEP-II e+e− asymmetric-energy storage
ring. We obtain branching fractions of B(B±→J/ψηK±)=(10.8±2.3(stat.)±2.4(syst.))×10−5 and
B(B0→J/ψηKS0)=(8.4±2.6(stat.)±2.7(syst.))×10−5. We search for the new narrow mass state, the
X(3872), recently reported by the Belle Collaboration, in the decay B^\pm\to
X(3872)K^\pm, X(3872)\to \jpsi \eta and determine an upper limit of
B(B^\pm \to X(3872) K^\pm \to \jpsi \eta K^\pm) <7.7×10−6
at 90% C.L.Comment: 7 pages and two figures, submitted to Phys. Rev. Lett
Search for the direct production of charginos and neutralinos in final states with tau leptons in √s=13 TeV collisions with the ATLAS detector
- Author
- Aaboud M
- Aad G
- Abbott B
- Abdinov O
- Abeloos B
- Abidi SH
- AbouZeid OS
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- Zhang Y
- Zhang Z
- Zhao X
- Zhao Y
- Zhao Z
- Zhemchugov A
- Zhou B
- Zhou C
- Zhou L
- Zhou M
- Zhou M
- Zhou N
- Zhu CG
- Zhu H
- Zhu J
- Zhu Y
- Zhuang X
- Zhukov K
- Zibell A
- Zieminska D
- Zimine NI
- Zimmermann C
- Zimmermann S
- Zinonos Z
- Zinser M
- Ziolkowski M
- Zivkovic L
- Zobernig G
- Zoccoli A
- Zou R
- zur Nedden M
- Zwalinski L
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2017
- Field of study
A search for the direct production of charginos and neutralinos in final states with at least two hadronically decaying tau leptons is presented. The analysis uses a dataset of pp collisions corresponding to an integrated luminosity of 36.1 fb−1, recorded with the ATLAS detector at the Large Hadron Collider at a centre-of-mass energy of 13TeV.Nosignificant deviation from the expected Standard Model background is observed. Limits are derived in scenarios of ˜χ+1 ˜χ−1 pair production and of ˜χ±1 ˜χ02 and ˜χ+1 ˜χ−1 production in simplified models where the neutralinos and charginos decay solely via intermediate left-handed staus and tau sneutrinos, and the mass of the ˜ τL state is set to be halfway between the masses of the ˜χ±1 and the ˜χ01. Chargino masses up to 630 GeV are excluded at 95% confidence level in the scenario of direct production of ˜χ+1 ˜χ−1 for a massless ˜χ01. Common ˜χ±1 and ˜χ02 masses up to 760 GeV are excluded in the case of production of ˜χ±1 ˜χ02 and ˜χ+1 ˜χ−1 assuming a massless ˜χ01. Exclusion limits for additional benchmark scenarios with large and small mass-splitting between the ˜χ±1 and the ˜χ01 are also studied by varying the ˜ τL mass between the masses of the ˜χ±1 and the ˜χ01
Combined measurement of differential and total cross sections in the H → γγ and the H → ZZ* → 4ℓ decay channels at s=13 TeV with the ATLAS detector
- Author
- Aaboud M
- Aad G
- Abbott B
- Abdinov O
- Abeloos B
- Abhayasinghe DK
- Abidi SH
- Abouzeid OS
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- Zhulanov V
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- Zobernig G
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- Álvarez Piqueras D
- Åkesson TPA
- Šfiligoj T
- Ženiš T
- Živković L
- Publication venue
- Elsevier
- Publication date
- 01/01/2018
- Field of study
A combined measurement of differential and inclusive total cross sections of Higgs boson production is performed using 36.1 fb−1 of 13 TeV proton–proton collision data produced by the LHC and recorded by the ATLAS detector in 2015 and 2016. Cross sections are obtained from measured H→γγ and H→ZZ*(→4ℓ event yields, which are combined taking into account detector efficiencies, resolution, acceptances and branching fractions. The total Higgs boson production cross section is measured to be 57.0−5.9 +6.0 (stat.) −3.3 +4.0 (syst.) pb, in agreement with the Standard Model prediction. Differential cross-section measurements are presented for the Higgs boson transverse momentum distribution, Higgs boson rapidity, number of jets produced together with the Higgs boson, and the transverse momentum of the leading jet. The results from the two decay channels are found to be compatible, and their combination agrees with the Standard Model predictions
Search for anomalous couplings in the W tb vertex from the measurement of double differential angular decay rates of single top quarks produced in the t-channel with the ATLAS detector
- Author
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- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 13/10/2015
- Field of study
The electroweak production and subsequent decay of single top quarks is determined by the properties of the Wtb vertex. This vertex can be described by the complex parameters of an effective Lagrangian. An analysis of angular distributions of the decay products of single top quarks produced in the t -channel constrains these parameters simultaneously. The analysis described in this paper uses 4.6 fb−1 of proton-proton collision data at √s =7 TeV collected with the ATLAS detector at the LHC. Two parameters are measured simultaneously in this analysis. The fraction f 1 of decays containing transversely polarised W bosons is measured to be 0.37 ± 0.07 (stat.⊕syst.). The phase δ − between amplitudes for transversely and longitudinally polarised W bosons recoiling against left-handed b-quarks is measured to be −0.014π ± 0.036π (stat.⊕syst.). The correlation in the measurement of these parameters is 0.15. These values result in two-dimensional limits at the 95% confidence level on the ratio of the complex coupling parameters g R and V L, yielding Re[g R /V L] ∈ [−0.36, 0.10] and Im[g R /V L] ∈ [−0.17, 0.23] with a correlation of 0.11. The results are in good agreement with the predictions of the Standard Model
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