1,973 research outputs found
A search for the decay modes B+/- to h+/- tau l
- Author
- Adametz A
- Adye T
- Ahmed H
- Akar S
- Alam MS
- Albert J
- Alwyn KE
- Andreassen R
- Angelini C
- Anulli F
- Arnaud N
- Asgeirsson DJ
- Aston D
- Atmacan H
- Ayad R
- Bailey D
- Baldini-Ferroli R
- Band HR
- Banerjee S
- Bard DJ
- Barlow RJ
- Bartoldus R
- Batignani G
- Behera PK
- Behn E
- Bellis M
- Ben-Haim E
- Benitez JF
- Bernard D
- Bernlochner FU
- Bettarini S
- Bettoni D
- Bevan AJ
- Bhuyan B
- Bianchi F
- Biasini M
- Biassoni P
- Bingham I
- Blinov VE
- Bloom PC
- Bomben M
- Bondioli M
- Bonneaud GR
- Bozzi C
- Brau J
- Briand H
- Brown DN
- Brown DN
- Bunger C
- Burchat PR
- Buzykaev AR
- Calabrese R
- Calcaterra A
- Calderini G
- Campagnari C
- Carpinelli M
- Cartaro C
- Casarosa G
- Cavoto G
- Cenci R
- Cervelli A
- Chauveau J
- Chavez CA
- Chen C
- Cheng CH
- Choi HHF
- Cibinetto G
- Clark PJ
- Cochran J
- Coleman JP
- Contri R
- Convery MR
- Cowan G
- Cowan R
- Cremaldi L
- Dallapiccola C
- Dasu S
- Dauncey PD
- Davier M
- Davis CL
- de Monchenault GH
- De Nardo G
- de Sangro R
- Denig AG
- Di Lodovico F
- Doll DA
- Dorfan J
- Druzhinin VP
- Dubois-Felsmann GP
- Dubrovin MS
- Dujmic D
- Dunwoodie W
- Ebert M
- Echenard B
- Eckmann R
- Edwards AJ
- Eigen G
- Eisner AM
- Emery S
- Ernst JA
- Faccini R
- Feltresi E
- Ferrarotto F
- Ferroni F
- Field RC
- Finocchiaro G
- Fioravanti E
- Flood KT
- Ford WT
- Forti F
- Frey R
- Fritsch M
- Fry JR
- Fulsom BG
- Gabareen AM
- Gabathuler E
- Gagliardi N
- Gamba D
- Gary JW
- Garzia I
- Gaz A
- Gershon TJ
- Gioi LL
- Giorgi MA
- Godang R
- Golubev VB
- Gorodeisky R
- Gradl W
- Graham MT
- Grauges E
- Grenier P
- Gritsan AV
- Grosdidier G
- Grunberg O
- Guido E
- Guo ZJ
- Guttman N
- Hafner A
- Hamilton B
- Hamon O
- Harrison PF
- Hartmann T
- Hast C
- Hearty C
- Hitlin DG
- Hong TM
- Honscheid K
- Huard Z
- Hutchcroft DE
- Innes WR
- Izen JM
- Jackson G
- Jawahery A
- Jessop CP
- Kass R
- Kelsey MH
- Kerth LT
- Khan A
- Kim H
- Kim P
- King GJ
- Kirkby D
- Knoepfel KJ
- Kobel MJ
- Koch H
- Kocian ML
- Kolomensky YG
- Kovalskyi D
- Kowalewski R
- Kravchenko EA
- Kroeger R
- Kroseberg J
- Lacker HM
- Lafferty GD
- Lanceri L
- Lange DJ
- Lankford AJ
- Latham TE
- Lazzaro A
- Le Diberder F
- Leddig T
- Lee CL
- Lees JP
- Leith DWGS
- Leruste P
- Lewczuk MJ
- Lewis P
- Li S
- Lindemann D
- Lindquist B
- Liu F
- Lo Vetere M
- Lockman WS
- Lombardo V
- Long O
- LoSecco JM
- Lou XC
- Lu C
- Lueck T
- Luitz S
- Lund P
- Luppi E
- Lusiani A
- Luth V
- Lutz AM
- Lynch G
- Lynch HL
- MacFarlane DB
- Malaescu B
- Mallik U
- Mandelkern M
- Manoni E
- Marchiori G
- Margoni M
- Marks J
- Martinelli M
- Martinez AJ
- Martinez-Vidal F
- Mattison TS
- Mazzoni MA
- McKenna JA
- Meadows BT
- Meyer WT
- Milanes DA
- Miyashita TS
- Monge MR
- Monorchio D
- Morandin M
- Morii M
- Muller DR
- Munerato M
- Nagel M
- Nauenberg U
- Neal H
- Negrini M
- Nelson S
- Neri N
- Nguyen X
- Nicolaci M
- Nugent IM
- Oberhof B
- Ocariz J
- Ofte I
- Olaiya EO
- Olsen J
- Ongmongkolkul P
- Onorato G
- Onuchin AP
- Oyanguren A
- Pacetti S
- Palano A
- Palombo F
- Pan Y
- Paoloni E
- Pappagallo M
- Park W
- Passaggio S
- Patel PM
- Patrignani C
- Patteri P
- Payne DJ
- Pegna DL
- Peimer DR
- Perez A
- Perl M
- Peruzzi IM
- Piccolo M
- Piemontese L
- Piredda G
- Playfer S
- Poireau V
- Porter FC
- Posocco M
- Prasad V
- Prell S
- Prencipe E
- Prepost R
- Puccio EMT
- Pulliam T
- Purohit MV
- Rakitin AY
- Rama M
- Randle-Conde A
- Ratcliff BN
- Raven G
- Richman JD
- Ritchie JL
- Rizzo G
- Roberts DA
- Robertson SH
- Robutti E
- Roney JM
- Roodman A
- Rosenberg EI
- Rossi A
- Rotondo M
- Roudeau P
- Rubin AE
- Ruland AM
- Sacco R
- Salnikov AA
- Santoro V
- Schalk T
- Schilling CJ
- Schindler RH
- Schram M
- Schroder H
- Schroeder T
- Schubert KR
- Schumm BA
- Schune MH
- Schwierz R
- Schwitters RF
- Sciacca C
- Sciolla G
- Seiden A
- Sekula SJ
- Serednyakov SI
- Sevilla MF
- Sigamani M
- Simi G
- Simonetto F
- Sinev NB
- Sitt S
- Skovpen YI
- Smith AJS
- Smith JG
- Snoek HL
- Snyder A
- Sobie RJ
- Soffer A
- Sokoloff MD
- Solodov EP
- Sonnek P
- Spaan B
- Spanier SM
- Stocchi A
- Stoker DP
- Stracka S
- Stroili R
- Strom D
- Stugu B
- Su D
- Sullivan MK
- Summers DJ
- Sun L
- Taras P
- Tasneem N
- Telnov AV
- Tibbetts M
- Tico JG
- Tisserand V
- Todyshev KY
- Toki WH
- Torrence E
- Touramanis C
- Uwer U
- Va'vra J
- Vasseur G
- Verderi M
- Vitale L
- Vitug GM
- Wagner AP
- Wagner SR
- Waldi R
- Walsh JJ
- Wang WF
- Weaver M
- West CA
- White RM
- Wilson FF
- Wilson JR
- Wisniewski WJ
- Wittgen M
- Wormser G
- Wray BC
- Wright DH
- Wright DM
- Wu SL
- Wulsin HW
- Yarritu AK
- Yeche C
- Young CC
- Yushkov AN
- Zallo A
- Ziegler V
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2012
- Field of study
We present a search for the lepton flavor violating decay modes B+/- to h+/-
tau l (h= K,pi; l= e,mu) using the BaBar data sample, which corresponds to 472
million BBbar pairs. The search uses events where one B meson is fully
reconstructed in one of several hadronic final states. Using the momenta of the
reconstructed B, h, and l candidates, we are able to fully determine the tau
four-momentum. The resulting tau candidate mass is our main discriminant
against combinatorial background. We see no evidence for B+/- to h+/- tau l
decays and set a 90% confidence level upper limit on each branching fraction at
the level of a few times 10^-5.Comment: 15 pages, 7 figures, submitted to Phys. Rev.
Evidence for an excess of B -> D(*) Tau Nu decays
- Author
- Adametz A
- Adye T
- Ahmed H
- Akar S
- Alam MS
- Albert J
- Andreassen R
- ANGELINI CARLO
- Anulli F
- Arnaud N
- Asgeirsson DJ
- Aston D
- Atmacan H
- Ayad R
- Baldini Ferroli R
- Band HR
- Band HR
- Banerjee S
- Banerjee S
- Bard DJ
- Barlow RJ
- Bartoldus R
- BATIGNANI GIOVANNI
- Behn E
- Bellis M
- Ben Haim E
- Benitez JF
- Bernard D
- Bernlochner FU
- BETTARINI STEFANO
- Bettoni D
- Bevan AJ
- Bhuyan B
- Bianchi F
- Biasini M
- Biassoni P
- Blinov VE
- Bloom PC
- Bomben M
- Bondioli M
- Bonneaud GR
- Bozzi C
- Brau J
- Briand H
- Brown DN
- Brown DN
- Bunger C
- Burchat PR
- Buzykaev AR
- Calabrese R
- Calcaterra A
- CALDERINI GIOVANNI
- Campagnari C
- Carpinelli M
- Cartaro C
- Casarosa G
- Cenci R
- Cervelli A
- Chao DS
- Chauveau J
- Chavez CA
- Cheaib R
- Chen C
- Cheng CH
- Choi HHF
- Choi HHF
- Cibinetto G
- Clark PJ
- Cochran J
- Coleman JP
- Contri R
- Convery MR
- Cowan G
- Cowan R
- Cremaldi L
- Dallapiccola C
- Dasu S
- Dasu S
- Dasu S
- Dasu S
- Dauncey PD
- Davier M
- Davis CL
- de Monchenault GH
- De Nardo G
- de Sangro R
- Denig AG
- Derkach D
- Di Lodovico F
- Dorfan J
- Druzhinin VP
- Dubois Felsmann GP
- Dujmic D
- Dunwoodie W
- Ebert M
- Echenard B
- Edwards AJ
- Eigen G
- Eisner AM
- Emery S
- Ernst JA
- Faccini R
- Feltresi E
- Ferrarotto F
- Ferroni F
- Field RC
- Finocchiaro G
- Fioravanti E
- Flood KT
- Ford WT
- FORTI FRANCESCO
- Frey R
- Fritsch M
- Fry JR
- Fulsom BG
- Gabareen AM
- Gabathuler E
- Gagliardi N
- Gamba D
- Gary JW
- Garzia I
- Gaspero M
- Gaz A
- Gershon TJ
- Gershon TJ
- Gioi LL
- GIORGI MARCELLO
- Godang R
- Golubev VB
- Gorodeisky R
- Gradl W
- Graham MT
- Grauges E
- Grenier P
- Griessinger K
- Gritsan AV
- Grosdidier G
- Grunberg O
- Guido E
- Guo ZJ
- Guttman N
- Hafner A
- Hamilton B
- Hamon O
- Harrison PF
- Harrison PF
- Hartmann T
- Hast C
- Hearty C
- Hitlin DG
- Hong TM
- Honscheid K
- Huard Z
- Hutchcroft DE
- Innes WR
- Izen JM
- Jackson G
- Jawahery A
- Jessop CP
- Kass R
- Kelsey MH
- Kerth LT
- Khan A
- Kim P
- King GJ
- King GJ
- Kirkby D
- Koch H
- Kocian ML
- Kolomensky YG
- Kovalskyi D
- Kowalewski R
- Kowalewski R
- Kravchenko EA
- Kroeger R
- Kroseberg J
- Lacker HM
- Lafferty GD
- Lanceri L
- Lange DJ
- Lankford AJ
- Latham TE
- Latham TE
- Le Diberder F
- Leddig T
- Lee CL
- Lees JP
- Leith DWGS
- Leruste P
- Lewczuk MJ
- Lewczuk MJ
- Lewis P
- Lindemann D
- Lindquist B
- Liu F
- Lo Vetere M
- Lockman WS
- Long O
- LoSecco JM
- Lou XC
- Lueck T
- Luitz S
- Lund P
- Luppi E
- Lusiani A
- Luth V
- Lutz AM
- Lynch G
- Lynch HL
- MacFarlane DB
- Malaescu B
- Mallik U
- Mandelkern M
- Manoni E
- Marchiori G
- Margoni M
- Martinelli M
- Martinez AJ
- Martinez Vidal F
- Mattison TS
- Mazzoni MA
- McKenna JA
- Meadows BT
- Meyer WT
- Miyashita TS
- Monge MR
- Monorchio D
- Morandin M
- Morii M
- Muller DR
- Munerato M
- Nauenberg U
- Neal H
- Nelson S
- Neri N
- Nguyen X
- Nugent IM
- Nugent IM
- Oberhof B
- Ocariz J
- Olaiya EO
- Olsen J
- Ongmongkolkul P
- Onorato G
- Onuchin AP
- Oyanguren A
- Pacetti S
- Palano A
- Palombo F
- Pan Y
- Pan Y
- Pan Y
- Pan Y
- Pan Y
- PAOLONI EUGENIO
- Park W
- Passaggio S
- Patel PM
- Patrignani C
- Patteri P
- Payne DJ
- Pegna DL
- Peimer DR
- Perez A
- Perl M
- Peruzzi IM
- Piccolo M
- Piemontese L
- Piredda G
- Playfer S
- Poireau V
- Porter FC
- Posocco M
- Prasad V
- Prell S
- Prencipe E
- Prepost R
- Prepost R
- Prepost R
- Prepost R
- Prepost R
- Puccio EMT
- Puccio EMT
- Pulliam T
- Purohit MV
- Rakitin AY
- Rama M
- Randle Conde A
- Ratcliff BN
- Raven G
- Richman JD
- Ritchie JL
- RIZZO GIULIANA
- Roberts DA
- Robertson SH
- Robutti E
- Roney JM
- Roney JM
- Roodman A
- Rossi A
- Rotondo M
- Roudeau P
- Rubin AE
- Ruland AM
- Sacco R
- Salnikov AA
- Santoro V
- Schindler RH
- Schroder H
- Schroeder T
- Schubert KR
- Schumm BA
- Schune MH
- Schwierz R
- Schwitters RF
- Sciacca C
- Sciolla G
- Seiden A
- Sekula SJ
- Serednyakov SI
- Sevilla MF
- Sigamani M
- Simard M
- Simi G
- Simonetto F
- Sinev NB
- Sitt S
- Skovpen YI
- Smith AJS
- Smith JG
- Snyder A
- So RY
- Sobie RJ
- Sobie RJ
- Soffer A
- Sokoloff MD
- Solodov EP
- Sonnek P
- Spaan B
- Spanier SM
- Stocchi A
- STRACKA SIMONE
- Stroili R
- Strom D
- Stugu B
- Su D
- Sullivan MK
- Summers DJ
- Sun L
- Taras P
- Tasneem N
- Tasneem N
- Telnov AV
- Tico JG
- Tisserand V
- Todyshev KY
- Toki WH
- Torrence E
- Touramanis C
- Uwer U
- Va'vra J
- Vasseur G
- Verderi M
- Vitale L
- Vitug GM
- Voss C
- Vuosalo CO
- Wagner AP
- Wagner SR
- Waldi R
- Walsh JJ
- Wang WF
- West CA
- White RM
- Wilson FF
- Wilson JR
- Wisniewski WJ
- Wittgen M
- Wormser G
- Wray BC
- Wright DH
- Wright DM
- Wu SL
- Wu SL HR
- Wu SLDasu S
- Wu SLR
- Wu SLtti A
- Wulsin HW
- Yeche C
- Young CC
- Yushkov AN
- Zallo A
- Zambito S
- Zhang X
- Ziegler V
- Zucchelli Slbert J
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2012
- Field of study
Based on the full BaBar data sample, we report improved measurements of the
ratios R(D(*)) = B(B -> D(*) Tau Nu)/B(B -> D(*) l Nu), where l is either e or
mu. These ratios are sensitive to new physics contributions in the form of a
charged Higgs boson. We measure R(D) = 0.440 +- 0.058 +- 0.042 and R(D*) =
0.332 +- 0.024 +- 0.018, which exceed the Standard Model expectations by 2.0
sigma and 2.7 sigma, respectively. Taken together, our results disagree with
these expectations at the 3.4 sigma level. This excess cannot be explained by a
charged Higgs boson in the type II two-Higgs-doublet model. We also report the
observation of the decay B -> D Tau Nu, with a significance of 6.8 sigma.Comment: Expanded section on systematics, text corrections, improved the
format of Figure 2 and included the effect of the change of the Tau
polarization due to the charged Higg
Search for the decay modes D^0 → e^+e^-, D^0 → μ^+μ^-, and D^0 → e^±μ∓
- Author
- Adametz A
- Adye T
- Ahmed H
- Akar S
- Alam Ms
- Albert J
- Andreassen R
- Angelini Carlo
- Anulli F
- Arnaud N
- Asgeirsson Dj
- Aston D
- Atmacan H
- Ayad R
- Baldini Ferroli R
- Band Hr
- Band Hr
- Banerjee S
- Banerjee S
- Bard Dj
- Barlow Rj
- Bartoldus R
- Batignani Giovanni
- Behn E
- Bellis M
- Ben Haim E
- Benitez Jf
- Bernard D
- Bernlochner Fu
- Bettarini Stefano
- Bettoni D
- Bevan Aj
- Bhuyan B
- Bianchi F
- Biasini M
- Biassoni P
- Blinov Ve
- Bloom Pc
- Bomben M
- Bondioli M
- Bonneaud Gr
- Bozzi C
- Brau J
- Briand H
- Brown Dn
- Brown Dn
- Bunger C
- Burchat Pr
- Buzykaev Ar
- Calabrese R
- Calcaterra A
- Calderini Giovanni
- Campagnari C
- Carpinelli M
- Cartaro C
- Casarosa G
- Cenci R
- Cervelli A
- Chao Ds
- Chauveau J
- Chavez Ca
- Cheaib R
- Chen C
- Cheng Ch
- Choi Hhf
- Choi Hhf
- Cibinetto G
- Clark Pj
- Cochran J
- Coleman Jp
- Contri R
- Convery Mr
- Cowan G
- Cowan R
- Cremaldi L
- Dallapiccola C
- Dasu S
- Dasu S
- Dasu S
- Dauncey Pd
- Davier M
- Davis Cl
- de Monchenault Gh
- De Nardo G
- De Sangro R
- Denig Ag
- Derkach D
- Di Lodovico F
- Dorfan J
- Druzhinin Vp
- Dubois Felsmann Gp
- Dujmic D
- Dunwoodie W
- Ebert M
- Echenard B
- Edwards Aj
- Eigen G
- Eisner Am
- Emery S
- Ernst Ja
- Faccini R
- Feltresi E
- Ferrarotto F
- Ferroni F
- Field Rc
- Finocchiaro G
- Fioravanti E
- Flood Kt
- Ford Wt
- Forti Francesco
- Frey R
- Fritsch M
- Fry Jr
- Fulsom Bg
- Gabareen Am
- Gabathuler E
- Gagliardi N
- Gamba D
- Gary Jw
- Garzia I
- Gaspero M
- Gaz A
- Gershon Tj
- Gershon Tj
- Gioi Ll
- Giorgi Marcello
- Godang R
- Golubev Vb
- Gorodeisky R
- Gradl W
- Graham Mt
- Grauges E
- Grenier P
- Griessinger K
- Gritsan Av
- Grosdidier G
- Grunberg O
- Guido E
- Guo Zj
- Guttman N
- Hafner A
- Hamilton B
- Hamon O
- Harrison Pf
- Harrison Pf
- Hartmann T
- Hast C
- Hearty C
- Hitlin Dg
- Hong Tm
- Honscheid K
- Huard Z
- Hutchcroft De
- Innes Wr
- Izen Jm
- Jackson G
- Jawahery A
- Jessop Cp
- Kass R
- Kelsey Mh
- Kerth Lt
- Khan A
- Kim P
- King Gj
- King Gj
- Kirkby D
- Koch H
- Kocian Ml
- Kolomensky Yg
- Kovalskyi D
- Kowalewski R
- Kowalewski R
- Kravchenko Ea
- Kroeger R
- Kroseberg J
- Lacker Hm
- Lafferty Gd
- Lanceri L
- Lange Dj
- Lankford Aj
- Latham Te
- Latham Te
- Le Diberder F
- Leddig T
- Lee Cl
- Lees Jp
- Leith Dwgs
- Leruste P
- Lewczuk Mj
- Lewczuk Mj
- Lewis P
- Lindemann D
- Lindquist B
- Liu F
- Lo Vetere M
- Lockman Ws
- Long O
- Losecco Jm
- Lou Xc
- Lueck T
- Luitz S
- Lund P
- Luppi E
- Lusiani A
- Luth V
- Lutz Am
- Lynch G
- Lynch Hl
- Macfarlane Db
- Malaescu B
- Mallik U
- Mandelkern M
- Manoni E
- Marchiori G
- Margoni M
- Martinelli M
- Martinez Vidal F
- Martinez Aj
- Mattison Ts
- Mazzoni Ma
- Mckenna Ja
- Meadows Bt
- Meyer Wt
- Miyashita Ts
- Monge Mr
- Monorchio D
- Morandin M
- Morii M
- Muller Dr
- Mullin E
- Munerato M
- Nauenberg U
- Neal H
- Nelson S
- Neri N
- Nguyen X
- Nugent Im
- Nugent M
- Oberhof B
- Ocariz J
- Olaiya Eo
- Olsen J
- Ongmongkolkul P
- Onorato G
- Onuchin Ap
- Oyanguren A
- Pacetti S
- Palano A
- Palombo F
- Pan Y
- Pan Y
- Pan Y
- Pan Y
- Paoloni Eugenio
- Park W
- Passaggio S
- Patel Pm
- Patrignani C
- Patteri P
- Payne Dj
- Pegna Dl
- Peimer Dr
- Perez A
- Perl M
- Peruzzi Im
- Piccolo M
- Piemontese L
- Piredda G
- Playfer S
- Poireau V
- Porter Fc
- Posocco M
- Prasad V
- Prell S
- Prencipe E
- Prepost R
- Prepost R
- Prepost R
- Prepost R
- Puccio Emt
- Puccio Emt
- Pulliam T
- Purohit Mv
- Rakitin Ay
- Rama M
- Randle Conde A
- Ratcliff Bn
- Raven G
- Richman Jd
- Ritchie Jl
- Rizzo Giuliana
- Roberts Da
- Robertson Sh
- Robutti E
- Roney Jm
- Roney Jm
- Roodman A
- Rossi A
- Rotondo M
- Roudeau P
- Rubin Ae
- Ruland Am
- Sacco R
- Salnikov Aa
- Santoro V
- Schindler Rh
- Schroder H
- Schroeder T
- Schubert Kr
- Schumm Ba
- Schune Mh
- Schwierz R
- Schwitters Rf
- Sciacca C
- Sciolla G
- Seiden A
- Sekula Sj
- Serednyakov Si
- Sevilla Mf
- Sigamani M
- Simard M
- Simi G
- Simonetto F
- Sinev Nb
- Sitt S
- Skovpen Yi
- Smith Ajs
- Smith Jg
- Snyder A
- So Ry
- Sobie Rj
- Sobie Rj
- Soffer A
- Sokoloff Md
- Solodov Ep
- Sonnek P
- Spaan B
- Spanier Sm
- Stocchi A
- Stracka Simone
- Stroili R
- Strom D
- Stugu B
- Su D
- Sullivan Mk
- Summers Dj
- Sun L
- Taras P
- Tasneem N
- Tasneem N
- Telnov Av
- Tico Jg
- Tisserand V
- Todyshev Ky
- Toki Wh
- Torrence E
- Touramanis C
- Uwer U
- Va'Vra J
- Vasseur G
- Verderi M
- Vitale L
- Vitug Gm
- Voss C
- Vuosalo Co
- Wagner Ap
- Wagner Sr
- Waldi R
- Walsh Jj
- Wang Wf
- West Ca
- White Rm
- Wilson Ff
- Wilson Jr
- Wisniewski Wj
- Wittgen M
- Wormser G
- Wray Bc
- Wright Dh
- Wright Dm
- Wu SL Hr
- Wu SLDasu S
- Wu Sl
- Wu Sl
- Wulsin Hw
- Yeche C
- Young Cc
- Yu Ss
- Yun J
- Yushkov An
- Zallo A
- Zambito S
- Zanetti A
- Zhang X
- Ziegler V
- Zucchelli Slbert J
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2012
- Field of study
We present searches for the rare decay modes D^0→e^+e^-, D^0→μ^+μ^-, and D^0→e^±μ^∓ in continuum e^+e^-→cc events recorded by the BABAR detector in a data sample that corresponds to an integrated luminosity of 468 fb^(-1). These decays are highly Glashow–Iliopoulos–Maiani suppressed but may be enhanced in several extensions of the standard model. Our observed event yields are consistent with the expected backgrounds. An excess is seen in the D^0→μ^+μ^- channel, although the observed yield is consistent with an upward background fluctuation at the 5% level. Using the Feldman–Cousins method, we set the following 90% confidence level intervals on the branching fractions: B(D^0→e^+e^-)<1.7×10^(-7), B(D^0→μ^+μ^-) within [0.6,8.1]×10^(-7), and B(D^0→e^±μ^∓)<3.3×10^(-7)
Study of the reaction e^{+}e^{-} -->J/psi\pi^{+}\pi^{-} via initial-state radiation at BaBar
- Author
- Adametz A
- Adye T
- Ahmed H
- Akar S
- Alam MS
- Albert J
- Andreassen R
- Angelini C
- Anulli F
- Arlen T.
- Arnaud N
- Asgeirsson DJ
- Aston D
- Atmacan H
- Aune T.
- Ayad R
- Baldini-Ferroli R
- Band HR
- Banerjee S
- Bard DJ
- Barlow RJ
- Bartoldus R
- Batignani G
- Behera PK
- Behn E
- Beilicke M.
- Bellis M
- Ben-Haim E
- Benbow W.
- Benitez JF
- Bernard D
- Bernlochner FU
- Bettarini S
- Bettoni D
- Bevan AJ
- Bhuyan B
- Bianchi F
- Biasini M
- Biassoni P
- Blinov VE
- Bloom PC
- Bomben M
- Bondioli M
- Bonneaud GR
- Bouvier A.
- Bozzi C
- Bradbury S. M.
- Brau J
- Briand H
- Brown DN
- Brown DN
- Buckley J. H.
- Bugaev V.
- Bunger C
- Burchat PR
- Buzykaev AR
- Byrum K.
- Calabrese R
- Calcaterra A
- Calderini G
- Campagnari C
- Cannon A.
- Cara M.
- Carpinelli M
- Cartaro C
- Casadio C.
- Casarosa G
- Cenci R
- Cervelli A
- Cesarini A.
- Chao DS
- Chauveau J
- Chavez CA
- Cheaib R
- Chen C
- Cheng CH
- Cheung C. C.
- Choi HHF
- Cibinetto G
- Ciupik L.
- Clark PJ
- Cochran J
- Coleman JP
- Connolly M. P.
- Contri R
- Convery MR
- Cowan G
- Cowan R
- Cremaldi L
- Cui W.
- Dallapiccola C
- Dasu S
- Dauncey PD
- Davier M
- Davies F.
- Davis CL
- de Almeida U. Barres
- de Monchenault GH
- De Nardo G
- de Sangro R
- Denig AG
- Derkach D
- Di Lodovico F
- Dickherber R.
- Doi A.
- Dorfan J
- Druzhinin VP
- Dubois-Felsmann GP
- Dujmic D
- Duke C.
- Dunwoodie W
- Ebert M
- Echenard B
- Edwards AJ
- Eigen G
- Eisner AM
- Emery S
- Ernst JA
- Errando M.
- Faccini R
- Falcone A.
- Feltresi E
- Ferrarotto F
- Ferroni F
- Field RC
- Finley J. P.
- Finnegan G.
- Finocchiaro G
- Fioravanti E
- Flood KT
- Ford WT
- Forti F
- Fortson L.
- Frey R
- Fritsch M
- Fry JR
- Fulsom BG
- Furniss A.
- Gabareen AM
- Gabathuler E
- Gagliardi N
- Galante N.
- Gall D.
- Gamba D
- Gary JW
- Garzia I
- Gaspero M
- Gaz A
- Gershon TJ
- Gioi LL
- Giorgi MA
- Giovannini G.
- Giroletti M.
- Godambe S.
- Godang R
- Golubev VB
- Gorodeisky R
- Gradl W
- Graham MT
- Grauges E
- Grenier P
- Griessinger K
- Griffin S.
- Gritsan AV
- Grosdidier G
- Grube J.
- Grunberg O
- Guido E
- Guo ZJ
- Guttman N
- Gyuk G.
- Hada K.
- Hafner A
- Hamilton B
- Hamon O
- Hanna D.
- Hardee P.
- Harris D. E.
- Harrison PF
- Hartmann T
- Hast C
- Hearty C
- Hitlin DG
- Holder J.
- Hong TM
- Honscheid K
- Huan H.
- Huard Z
- Hui C. M.
- Hutchcroft DE
- Innes WR
- Izen JM
- Jackson G
- Jawahery A
- Jessop CP
- Junor W.
- Kaaret P.
- Karlsson N.
- Kass R
- Kelsey MH
- Kerth LT
- Kertzman M.
- Khan A
- Khassen Y.
- Kieda D.
- Kim P
- King GJ
- Kino M.
- Kirkby D
- Koch H
- Kocian ML
- Kolomensky YG
- Kovalskyi D
- Kowalewski R
- Kravchenko EA
- Krawczynski H.
- Krennrich F.
- Kroeger R
- Kroseberg J
- Lacker HM
- Lafferty GD
- Lanceri L
- Lang M. J.
- Lange DJ
- Lankford AJ
- Latham TE
- Le Diberder F
- LeBohec S.
- Leddig T
- Lee CL
- Lee N. P.
- Lees JP
- Leith DWGS
- Leruste P
- Lewczuk MJ
- Lewis P
- Lindemann D
- Lindquist B
- Liu F
- Lo Vetere M
- Lockman WS
- Long O
- LoSecco JM
- Lou XC
- Lueck T
- Luitz S
- Lund P
- Luppi E
- Lusiani A
- Luth V
- Lutz AM
- Ly C.
- Lynch G
- Lynch HL
- MacFarlane DB
- Madrid J.
- Maier G.
- Malaescu B
- Mallik U
- Mandelkern M
- Manoni E
- Marchiori G
- Margoni M
- Martinelli M
- Martinez AJ
- Martinez-Vidal F
- Massaro F.
- Mattison TS
- Mazzoni MA
- McArthur S.
- McCann A.
- McConville W.
- McKenna JA
- Meadows BT
- Meyer WT
- Miyashita TS
- Monge MR
- Monorchio D
- Morandin M
- Moriarty P.
- Morii M
- Mukherjee R.
- Muller DR
- Mundell C. G.
- Munerato M
- Nagai H.
- Nauenberg U
- Neal H
- Negrini M
- Nelson S
- Neri N
- Nguyen X
- Nugent IM
- Nunez P. D.
- Oberhof B
- Ocariz J
- Olaiya EO
- Olsen J
- Ong R. A.
- Ongmongkolkul P
- Onorato G
- Onuchin AP
- Orr M.
- Otte A. N.
- Oyanguren A
- Pacetti S
- Palano A
- Palombo F
- Pan Y
- Paoloni E
- Park N.
- Park W
- Passaggio S
- Patel PM
- Patrignani C
- Patteri P
- Payne DJ
- Pegna DL
- Peimer DR
- Perez A
- Perkins J. S.
- Perl M
- Perlman E. S.
- Peruzzi IM
- Piccolo M
- Pichel A.
- Piemontese L
- Piredda G
- Playfer S
- Pohl M.
- Poireau V
- Porter FC
- Posocco M
- Prasad V
- Prell S
- Prencipe E
- Prepost R
- Prokoph H.
- Puccio EMT
- Pulliam T
- Purohit MV
- Ragan K.
- Rakitin AY
- Rama M
- Randle-Conde A
- Ratcliff BN
- Raven G
- Reyes L. C.
- Reynolds P. T.
- Richman JD
- Ritchie JL
- Rizzo G
- Roache E.
- Roberts DA
- Robertson SH
- Robutti E
- Roney JM
- Roodman A
- Rose H. J.
- Rossi A
- Rotondo M
- Roudeau P
- Rubin AE
- Ruland AM
- Ruppel J.
- Sacco R
- Salnikov AA
- Santoro V
- Schindler RH
- Schroder H
- Schroeder T
- Schroedter M.
- Schubert KR
- Schumm BA
- Schune MH
- Schwierz R
- Schwitters RF
- Sciacca C
- Sciolla G
- Seiden A
- Sekula SJ
- Sembroski G. H.
- Sentuerk G. D.
- Serednyakov SI
- Sevilla MF
- Sigamani M
- Sillanpaa A.
- Simard M
- Simi G
- Simonetto F
- Sinev NB
- Sitarek J.
- Sitt S
- Skovpen YI
- Smith AJS
- Smith JG
- Snyder A
- Sobczynska D.
- Sobie RJ
- Soffer A
- Sokoloff MD
- Solodov EP
- Sonnek P
- Spaan B
- Spanier F.
- Spanier SM
- Spiro S.
- Stamerra A.
- Steele I. A.
- Steinke B.
- Stocchi A
- Storz J.
- Stracka S
- Strah N.
- Stroili R
- Strom D
- Stugu B
- Su D
- Sullivan MK
- Summers DJ
- Sun L
- Suric T.
- Takalo L.
- Takami H.
- Taras P
- Tasneem N
- Tavecchio F.
- Telezhinsky I.
- Telnov AV
- Temnikov P.
- Terzic T.
- Tescaro D.
- Teshima M.
- Tesic G.
- Theiling M.
- Thibadeau S.
- Thom M.
- Tibolla O.
- Tico JG
- Tisserand V
- Todyshev KY
- Toki WH
- Torrence E
- Torres D. F.
- Touramanis C
- Treves A.
- Uwer U
- Va'vra J
- Vankov H.
- Varlotta A.
- Vasseur G
- Vassiliev V. V.
- Verderi M
- Vitale L
- Vitug GM
- Vivier M.
- Vogler P.
- Voss C
- Wagner AP
- Wagner R. M.
- Wagner SR
- Wakely S. P.
- Waldi R
- Walker R. C.
- Walsh JJ
- Wang WF
- Weekes T. C.
- Weitzel Q.
- West CA
- White RM
- Williams D. A.
- Wilson FF
- Wilson JR
- Wisniewski WJ
- Wittgen M
- Wood D. L.
- Wormser G
- Wray BC
- Wright DH
- Wright DM
- Wu SLL S. N.
- Wulsin HW
- Yeche C
- Young CC
- Yushkov AN
- Zabalza V.
- Zallo A
- Zandanel F.
- Zanin R.
- Ziegler V
- Zitzer B.
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2012
- Field of study
We study the process e+e−→J/ψπ+π− with
initial-state-radiation events produced at the PEP-II asymmetric-energy
collider. The data were recorded with the BaBar detector at center-of-mass
energies 10.58 and 10.54 GeV, and correspond to an integrated luminosity of 454
fb−1. We investigate the J/ψπ+π− mass
distribution in the region from 3.5 to 5.5 GeV/c2. Below 3.7
GeV/c2 the ψ(2S) signal dominates, and above 4
GeV/c2 there is a significant peak due to the Y(4260). A fit to
the data in the range 3.74 -- 5.50 GeV/c2 yields a mass value
4244±5 (stat) ±4 (syst)MeV/c2 and a width value 114−15+16 (stat)±7(syst)MeV for this state. We do not
confirm the report from the Belle collaboration of a broad structure at 4.01
GeV/c2. In addition, we investigate the π+π− system
which results from Y(4260) decay
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
Jet energy measurement with the ATLAS detector in proton-proton collisions at root s=7 TeV
- Author
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- Abdallah J
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- Zhemchugov A
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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 rare quark-annihilation decays, B --> Ds(*) Phi
- Author
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- Abrams GS
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- Summers DJ
- Sundermann JE
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- Vasileiadis G
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- Wilden L
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- Wisniewski WJ
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- Xie Y
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- 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
Measurement of the inclusive and dijet cross-sections of b-jets in pp collisions at sqrt(s) = 7 TeV with the ATLAS detector
- 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
- Ackers M
- 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
- Alam MA
- Alam MS
- Albrand S
- Aleksa M
- Aleksandrov IN
- Aleppo M
- Alessandria F
- Alexa C
- Alexander G
- Alexandre G
- Alexopoulos T
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- Alison J
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- Allwood-Spiers SE
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- Zhemchugov A
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- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 31/12/2010
- Field of study
The inclusive and dijet production cross-sections have been measured for jets
containing b-hadrons (b-jets) in proton-proton collisions at a centre-of-mass
energy of sqrt(s) = 7 TeV, using the ATLAS detector at the LHC. The
measurements use data corresponding to an integrated luminosity of 34 pb^-1.
The b-jets are identified using either a lifetime-based method, where secondary
decay vertices of b-hadrons in jets are reconstructed using information from
the tracking detectors, or a muon-based method where the presence of a muon is
used to identify semileptonic decays of b-hadrons inside jets. The inclusive
b-jet cross-section is measured as a function of transverse momentum in the
range 20 < pT < 400 GeV and rapidity in the range |y| < 2.1. The bbbar-dijet
cross-section is measured as a function of the dijet invariant mass in the
range 110 < m_jj < 760 GeV, the azimuthal angle difference between the two jets
and the angular variable chi in two dijet mass regions. The results are
compared with next-to-leading-order QCD predictions. Good agreement is observed
between the measured cross-sections and the predictions obtained using POWHEG +
Pythia. MC@NLO + Herwig shows good agreement with the measured bbbar-dijet
cross-section. However, it does not reproduce the measured inclusive
cross-section well, particularly for central b-jets with large transverse
momenta.Comment: 10 pages plus author list (21 pages total), 8 figures, 1 table, final
version published in European Physical Journal
Measurement of the Bottom-Strange Meson Mixing Phase in the Full CDF Data Set
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- Blumenfeld
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- Bodek
- Bortoletto
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- Yi
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- Yoshida
- Yu
- Yu
- Yu
- Yun
- Z.
- Zanetti
- Zeng
- Zhou
- Zucchelli
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2012
- Field of study
We report a measurement of the bottom-strange meson mixing phase \beta_s
using the time evolution of B0_s -> J/\psi (->\mu+\mu-) \phi (-> K+ K-) decays
in which the quark-flavor content of the bottom-strange meson is identified at
production. This measurement uses the full data set of proton-antiproton
collisions at sqrt(s)= 1.96 TeV collected by the Collider Detector experiment
at the Fermilab Tevatron, corresponding to 9.6 fb-1 of integrated luminosity.
We report confidence regions in the two-dimensional space of \beta_s and the
B0_s decay-width difference \Delta\Gamma_s, and measure \beta_s in [-\pi/2,
-1.51] U [-0.06, 0.30] U [1.26, \pi/2] at the 68% confidence level, in
agreement with the standard model expectation. Assuming the standard model
value of \beta_s, we also determine \Delta\Gamma_s = 0.068 +- 0.026 (stat) +-
0.009 (syst) ps-1 and the mean B0_s lifetime, \tau_s = 1.528 +- 0.019 (stat) +-
0.009 (syst) ps, which are consistent and competitive with determinations by
other experiments.Comment: 8 pages, 2 figures, Phys. Rev. Lett 109, 171802 (2012
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
- Aad G
- Abajyan T
- Abbott B
- Abdallah J
- Abdelalim AA
- Abdinov O
- Abi B
- Abolins M
- AbouZeid OS
- Abramowicz H
- Abreu H
- Acharya BS
- Adam ER
- Adamczyk L
- Adams DL
- Addy TN
- Adelman J
- Adomeit S
- Adragna P
- Adye T
- Aesky S
- Agar-Savedra JA
- Agustoni M
- Ahlen SP
- Ahles F
- Ahmad A
- Ahsan M
- Aielli G
- Akesson TPA
- Akimoto G
- Akimov AV
- Alam MA
- Albert J
- Albrand S
- Aleksa M
- Aleksandrov IN
- Alessandria F
- Alexa C
- Alexander G
- Alexandre G
- Alexopoulos T
- Alhroob M
- Aliev M
- Alimonti G
- Alison J
- Allbrooke BMM
- Allison LJ
- Allport PP
- Allwood-Spiers SE
- Almenar CC
- Almond J
- Aloisio A
- Alon R
- Alonso A
- Alonso F
- Altheimer A
- Alviggi MG
- Amako K
- Amelung C
- Ammosov VV
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- Amorim A
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- Zeitnitz C
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- Zhemchugov A
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- Zinonos Z
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- Zobernig G
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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
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