909 research outputs found
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
Performance of CMS muon reconstruction in pp collision events at sqrt(s) = 7 TeV
- Author
- Abbaneo D
- Abbiendi G
- Abbrescia M
- Abdullin S
- Acosta D
- Acosta JG
- Acosta MV
- Adair A
- Adam N
- Adam W
- Adams MR
- Adams T
- Adiguzel A
- Adler V
- Adzic P
- Agostino L
- Agram JL
- Aguilar-Benitez M
- Aguilo E
- Ahmad M
- Ahmad WH
- Ahuja S
- Akchurin N
- Akgun B
- Akgun U
- Akin IV
- Alagoz E
- Albajar C
- Albayrak EA
- Albergo S
- Albrow M
- Alda Junior WL
- Alexander J
- Aliev T
- Almeida N
- Alver B
- Alverson G
- Alves GA
- Amapane N
- Amsler C
- Anagnostou G
- Anastassov A
- Anderson J
- Anderson M
- Andrea J
- Andreev V
- Andreev V
- Andreev Y
- Andrews W
- Anghel IM
- Anjos TS
- Antonelli L
- Antunes JR
- Antunovic Z
- Apanasevich L
- Apollinari G
- Appelt E
- Apresyan A
- Aranyi A
- Arce P
- Arcidiacono R
- Arenton MW
- Arfaei H
- Argiro S
- Arisaka K
- Arneodo M
- Arora S
- Asawatangtrakuldee C
- Asghar MI
- Askew A
- Assran Y
- Ata M
- Atac M
- Atramentov O
- Attikis A
- Auffray E
- Autermann C
- Auzinger G
- Avdeeva E
- Avery P
- Avetisyan A
- Azarkin M
- Azhgirey I
- Aziz T
- Azzi P
- Azzolini V
- Azzurri P
- Baarmand MM
- Babb J
- Bacchetta N
- Bachtis M
- Baden A
- Baeni L
- Baesso P
- Baffioni S
- Bagliesi G
- Bai Y
- Baillon P
- Bainbridge R
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- Bakken JA
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- Barbagli G
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- Barfuss AF
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- Baringer P
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- Barnett BA
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- Battilana C
- Baty C
- Bauer G
- Bauerdick LAT
- Baumgartel D
- Baur U
- Bayshev I
- Bazterra VE
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- Beauceron S
- Beaudette F
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- Bedjidian M
- Beernaert K
- Behrenhoff W
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- Bernardes CA
- Bernardini J
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- Berryhill J
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- Besancon M
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- Betts RR
- Beuselinck R
- Bhat PC
- Bhatnagar V
- Bhattacharya S
- Bhattacharya S
- Bhatti A
- Bialas W
- Bialkowska H
- Bian JG
- Bianchi G
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- Bianco S
- Biasini M
- Biino C
- Bilei GM
- Bilin B
- Bilinskas MJ
- Bilki B
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- Biselli A
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- Bitioukov S
- Blekman F
- Blobel V
- Bloch D
- Bloch I
- Bloch P
- Bloom K
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- Blumenfeld B
- Blyweert S
- Bobrovskyi S
- Boccali T
- Bocci A
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- Bodek A
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- Boimska B
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- Calderon De La Barca Sanchez M
- Calderon A
- Cali IA
- Calligaris L
- Callner J
- Calvert B
- Calvo E
- Campagnari C
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- Camporesi T
- Capiluppi P
- Caponeri B
- Cappello G
- Cardaci M
- Carlin R
- Carlsmith D
- Carrillo Moreno S
- Carroll R
- Cartiglia N
- Carvalho W
- Casal B
- Casimiro Linares E
- Castaldi R
- Castello R
- Castilla-Valdez H
- Castro A
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- Caudron J
- Caulfield M
- Cavallari F
- Cavallo FR
- Cavallo N
- Cavanaugh R
- Ceard L
- Ceballos GG
- Cepeda M
- Cerati GB
- Cerci DS
- Cerci S
- Cerizza G
- Cerminara G
- Cerrada M
- Chabert EC
- Chadwick M
- Chakaberia I
- Chamizo Llatas M
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- Chang YH
- Chang YH
- Chang YW
- Chanon N
- Chao Y
- Charaf O
- Charlot C
- Chasco M
- Chasserat J
- Chatrchyan S
- Chatterjee A
- Chauhan S
- Checchia P
- Chen GM
- Chen HS
- Chen J
- Chen KF
- Chen KH
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- Chen Y
- Chen Z
- Cherepanov V
- Chertok M
- Chetluru V
- Cheung HWK
- Chhibra SS
- Chierici R
- Chiochia V
- Chiorboli M
- Chlebana F
- Cho Y
- Choi M
- Choi S
- Choi Y
- Choi YK
- Chou JP
- Choudhary BC
- Choudhury RK
- Choudhury S
- Christiansen T
- Chuang SH
- Chung J
- Chung YS
- Chwalek T
- Ciesielski R
- Cihangir S
- Cimmino A
- Cipriano PMR
- Cirino G
- Cittolin S
- Ciulli V
- Civinini C
- Claes DR
- Clare R
- Clarida W
- Clement E
- Clerbaux B
- Cline D
- CMS Collaboration
- Cockerill DJA
- Codispoti G
- Colafranceschi S
- Colaleo A
- Cole JE
- Colino N
- Collard C
- Colling D
- Conetti S
- Contardo D
- Conte E
- Contreras-Campana C
- Contreras-Campana E
- Conway J
- Conway R
- Cooper SI
- Cooper W
- Cornelis T
- Correa Martins Junior M
- Cortezon EP
- Cossutti F
- Costa M
- Costa S
- Costantini S
- Coughlan JA
- Cousins R
- Covarelli R
- Cox B
- Cox PT
- Creanza D
- Cremaldi LM
- Cripps N
- Cuevas J
- Cuffiani M
- Cumalat JP
- Cuplov V
- Cure B
- Cushman P
- Cussans D
- Custodio A
- Cutajar M
- Cutts D
- Cwiok M
- Czellar S
- D'Agnolo RT
- D'Alessandro R
- D'Alfonso M
- D'Enterria D
- D'Hondt J
- Da Costa EM
- Daci N
- Dahmes B
- Dahms T
- Dallavalle GM
- Damgov J
- Damiao DD
- Dammann D
- Danielson T
- Das S
- Daskalakis G
- Dasu S
- Daubie E
- Dauncey P
- David A
- Davids M
- Davies G
- de Barbaro P
- De Benedetti A
- De Boer W
- de Cassagnac RG
- De Cosa A
- de Fatis TT
- De Filippis N
- De Gruttola M
- De Guio F
- De Jeneret JD
- De La Cruz B
- De La Cruz-Burelo E
- De Lentdecker G
- De Mattia M
- de Monchenault GH
- De Oliveira Martins C
- De Palma M
- De Roeck A
- de Troconiz JF
- De Visscher S
- De Wolf EA
- Deisher A
- Deiters K
- Dejardin M
- del Arbol PMR
- Del Re D
- Delaere C
- Delgado Peris A
- Deliomeroglu M
- Dell'Orso R
- Della Negra M
- Della Ricca G
- Demaria N
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- Depasse P
- Dermenev A
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- Di Giovanni GP
- Di Guida S
- Di Marco E
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- Diamond B
- Dias FA
- Diemoz M
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- Dietz C
- Dietz-Laursonn E
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- Dimitrov A
- Dinardo ME
- Dirkes G
- Dissertori G
- Dittmar M
- Djordjevic M
- Dobrzynski L
- Dobson M
- Dobur D
- Doesburg R
- Dogangun O
- Dolen J
- Dominguez Vazquez D
- Dominguez A
- Dominik W
- Don CKK
- Dorigo T
- Dorney B
- Doroba K
- Dozen C
- Draeger J
- Dragicevic M
- Dragoiu C
- Drell BR
- Dremin I
- Drouhin F
- Drozdetskiy A
- du Pree T
- Duarte Campderros J
- Duarte J
- Dubinin M
- Dudero PR
- Dudko L
- Duenser M
- Dugad S
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- Dumanoglu I
- Dupont-Sagorin N
- Duric S
- Duris J
- Durkin LS
- Duru F
- Dutta D
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- Dzelalija M
- Eads M
- Eartly DP
- Eckerlin G
- Ecklund KM
- Eckstein D
- Edelhoff M
- Edelmaier CJ
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- Zatserklyaniy A
- Zeinali M
- Zeise M
- Zeuner WD
- Zeyrek M
- Zhang J
- Zhang Z
- Zheng Y
- Zhokin A
- Zhu B
- Zhu RY
- Zhukov V
- Zhukova V
- Ziebarth EB
- Ziegler J
- Zielinski M
- Zito G
- Zoeller MH
- Zotto P
- Zou W
- Zumerle G
- Zuranski A
- Publication venue
- 'IOP Publishing'
- Publication date
- 01/01/2012
- Field of study
The performance of muon reconstruction, identification, and triggering in CMS
has been studied using 40 inverse picobarns of data collected in pp collisions
at sqrt(s) = 7 TeV at the LHC in 2010. A few benchmark sets of selection
criteria covering a wide range of physics analysis needs have been examined.
For all considered selections, the efficiency to reconstruct and identify a
muon with a transverse momentum pT larger than a few GeV is above 95% over the
whole region of pseudorapidity covered by the CMS muon system, abs(eta) < 2.4,
while the probability to misidentify a hadron as a muon is well below 1%. The
efficiency to trigger on single muons with pT above a few GeV is higher than
90% over the full eta range, and typically substantially better. The overall
momentum scale is measured to a precision of 0.2% with muons from Z decays. The
transverse momentum resolution varies from 1% to 6% depending on pseudorapidity
for muons with pT below 100 GeV and, using cosmic rays, it is shown to be
better than 10% in the central region up to pT = 1 TeV. Observed distributions
of all quantities are well reproduced by the Monte Carlo simulation.Comment: Replaced with published version. Added journal reference and DO
Performance of CMS muon reconstruction in pp collision events at sqrt(s) = 7 TeV
- Author
- Abbaneo D
- Abbiendi G
- Abbrescia M
- Abdullin S
- Acosta D
- Acosta JG
- Acosta MV
- Adair A
- Adam N
- Adam W
- Adams MR
- Adams T
- Adiguzel A
- Adler V
- Adzic P
- Agostino L
- Agram JL
- Aguilar-Benitez M
- Aguilo E
- Ahmad M
- Ahmad WH
- Ahuja S
- Akchurin N
- Akgun B
- Akgun U
- Akin IV
- Alagoz E
- Albajar C
- Albayrak EA
- Albergo S
- Albrow M
- Alda Junior WL
- Alexander J
- Aliev T
- Almeida N
- Alver B
- Alverson G
- Alves GA
- Amapane N
- Amsler C
- Anagnostou G
- Anastassov A
- Anderson J
- Anderson M
- Andrea J
- Andreev V
- Andreev V
- Andreev Y
- Andrews W
- Anghel IM
- Anjos TS
- Antonelli L
- Antunes JR
- Antunovic Z
- Apanasevich L
- Apollinari G
- Appelt E
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- Xiao H
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- Yelton J
- Yetkin T
- Yi K
- Yildirim E
- Yilmaz Y
- Yohay R
- Yoo HD
- Yoo J
- Yoon AS
- York A
- Yu I
- Yu SS
- Yumiceva F
- Yun JC
- Zabel J
- Zabi A
- Zablocki J
- Zaganidis N
- Zakaria M
- Zalewski P
- Zanetti M
- Zang J
- Zang SL
- Zarubin A
- Zatserklyaniy A
- Zeinali M
- Zeise M
- Zeuner WD
- Zeyrek M
- Zhang J
- Zhang Z
- Zheng Y
- Zhokin A
- Zhu B
- Zhu RY
- Zhukov V
- Zhukova V
- Ziebarth EB
- Ziegler J
- Zielinski M
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- Zoeller MH
- Zotto P
- Zou W
- Zumerle G
- Zuranski A
- Publication venue
- 'IOP Publishing'
- Publication date
- 01/01/2012
- Field of study
The performance of muon reconstruction, identification, and triggering in CMS
has been studied using 40 inverse picobarns of data collected in pp collisions
at sqrt(s) = 7 TeV at the LHC in 2010. A few benchmark sets of selection
criteria covering a wide range of physics analysis needs have been examined.
For all considered selections, the efficiency to reconstruct and identify a
muon with a transverse momentum pT larger than a few GeV is above 95% over the
whole region of pseudorapidity covered by the CMS muon system, abs(eta) < 2.4,
while the probability to misidentify a hadron as a muon is well below 1%. The
efficiency to trigger on single muons with pT above a few GeV is higher than
90% over the full eta range, and typically substantially better. The overall
momentum scale is measured to a precision of 0.2% with muons from Z decays. The
transverse momentum resolution varies from 1% to 6% depending on pseudorapidity
for muons with pT below 100 GeV and, using cosmic rays, it is shown to be
better than 10% in the central region up to pT = 1 TeV. Observed distributions
of all quantities are well reproduced by the Monte Carlo simulation.Comment: Replaced with published version. Added journal reference and DO
Azimuthal anisotropy of charged particles at high transverse momenta in PbPb collisions at sqrt(s[NN]) = 2.76 TeV
- Author
- Abbaneo D
- Abbiendi G
- Abbrescia M
- Abdullin S
- Abdulsalam A
- Acosta D
- Acosta JG
- Acosta MV
- Adair A
- Adam N
- Adam W
- Adams MR
- Adams T
- Adiguzel A
- Adler V
- Adzic P
- Afanasiev S
- Agostino L
- Agram JL
- Aguilar-Benitez M
- Aguilo E
- Ahmad M
- Ahmad WH
- Ahuja S
- Akchurin N
- Akgun B
- Akgun U
- Akin IV
- Alagoz E
- Albajar C
- Albayrak EA
- Albergo S
- Albrow M
- Alcaraz Maestre J
- Alda Junior WL
- Alexander J
- Aliev T
- Alimena J
- Almeida N
- Alverson G
- Alves GA
- Amapane N
- Amsler C
- Anagnostou G
- Anastassov A
- Anderson J
- Anderson M
- Andrea J
- Andreev V
- Andreev V
- Andreev Y
- Andrews W
- Anghel IM
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- Wyslouch B
- Xiao H
- Xie S
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- Yang M
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- Yazgan E
- Yelton J
- Yetkin T
- Yi K
- Yildirim E
- Yilmaz Y
- Yohay R
- Yoo HD
- Yoo J
- Yoon AS
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- Yu I
- Yu SS
- Yumiceva F
- Yun JC
- Zabel J
- Zabi A
- Zablocki J
- Zaganidis N
- Zakaria M
- Zalewski P
- Zanetti M
- Zang J
- Zarubin A
- Zatserklyaniy A
- Zeinali M
- Zeise M
- Zeuner WD
- Zeyrek M
- Zhang J
- Zhang Z
- Zheng Y
- Zhokin A
- Zhu B
- Zhu RY
- Zhukov V
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- Ziebarth EB
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- Zito G
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- Zou W
- Zumerle G
- Zuranski A
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2012
- Field of study
The azimuthal anisotropy of charged particles in PbPb collisions at
nucleon-nucleon center-of-mass energy of 2.76 TeV is measured with the CMS
detector at the LHC over an extended transverse momentum (pt) range up to
approximately 60 GeV. The data cover both the low-pt region associated with
hydrodynamic flow phenomena and the high-pt region where the anisotropies may
reflect the path-length dependence of parton energy loss in the created medium.
The anisotropy parameter (v2) of the particles is extracted by correlating
charged tracks with respect to the event-plane reconstructed by using the
energy deposited in forward-angle calorimeters. For the six bins of collision
centrality studied, spanning the range of 0-60% most-central events, the
observed v2 values are found to first increase with pt, reaching a maximum
around pt = 3 GeV, and then to gradually decrease to almost zero, with the
decline persisting up to at least pt = 40 GeV over the full centrality range
measured.Comment: Replaced with published version. Added journal reference and DO
Search for new physics with same-sign isolated dilepton events with jets and missing transverse energy
- Author
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- Abbiendi G
- Abbrescia M
- Abdullin S
- Abdulsalam A
- Acosta D
- Acosta JG
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- Aguilo E
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- Akin IV
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- Aldaya Martin M
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- Yilmaz Y
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- Zielinski M
- Zito G
- Zou W
- Zucchetta A
- Zumerle G
- Zuranski A
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2012
- Field of study
A search for new physics is performed in events with two same-sign isolated
leptons, hadronic jets, and missing transverse energy in the final state. The
analysis is based on a data sample corresponding to an integrated luminosity of
4.98 inverse femtobarns produced in pp collisions at a center-of-mass energy of
7 TeV collected by the CMS experiment at the LHC. This constitutes a factor of
140 increase in integrated luminosity over previously published results. The
observed yields agree with the standard model predictions and thus no evidence
for new physics is found. The observations are used to set upper limits on
possible new physics contributions and to constrain supersymmetric models. To
facilitate the interpretation of the data in a broader range of new physics
scenarios, information on the event selection, detector response, and
efficiencies is provided.Comment: Published in Physical Review Letter
Compressed representation of a partially defined integer function over multiple arguments
- Author
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- Abbiendi G
- Abbrescia M
- Abdelalim AA
- Abdullin S
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- Cepeda M
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- Cimmino A
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- Cittolin S
- Ciulli V
- Civinini C
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- Cline D
- CMS Collaboration
- Coarasa Perez JA
- Cockerill DJA
- Colafranceschi S
- Colaleo A
- Cole JE
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- Colling D
- Contardo D
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- Costantini S
- Costanza F
- Couderc F
- Coughlan JA
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- Cremaldi LM
- Cripps N
- Cuevas J
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- Cumalat JP
- Cussans D
- Custodio A
- Cutajar M
- Cutts D
- Cwiok M
- Czellar S
- D'Agnolo RT
- D'Alessandro R
- D'Alfonso M
- d'Enterria D
- D'Hondt J
- Da Costa EM
- Dabrowski A
- Daci N
- Dahmes B
- Dahms T
- Dalchenko M
- Dallavalle GM
- Damgov J
- Danielson T
- Das S
- Daskalakis G
- Dasu S
- Daubie E
- Dauncey P
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- De Boer W
- de Cassagnac RG
- De Cosa A
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- Publication venue
- Publication date
- 01/01/2013
- Field of study
In OLAP (OnLine Analitical Processing) data are analysed in an n-dimensional cube. The cube may be represented as a partially defined function over n arguments. Considering that often the function is not defined everywhere, we ask: is there a known way of representing the function or the points in which it is defined, in a more compact manner than the trivial one
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