1,066 research outputs found
The in vivo properties of STX243: a potent angiogenesis inhibitor in breast cancer
- Author
- A Passaniti
- A Purohit
- A Tsukamoto
- AJ Leo
- B Raobaikady
- B V L Potter
- C Bubert
- C Sweeney
- CR Ireson
- E Ryschich
- F Loganzo
- FALM Eskens
- GL Scheffer
- J Folkman
- J Folkman
- JM Day
- L Wood
- M F C Parsons
- M J Reed
- M P Leese
- M Prewett
- MJ Newman
- MP Leese
- MP Leese
- MVJ Mustonen
- NJ Lakhani
- P A Foster
- P Workman
- PA Foster
- R Jhalli
- R Kerbel
- RN Suzuki
- S K Chander
- S P Newman
- SK Chander
- SP Newman
- SP Newman
- SP Newman
- T Fotsis
- T Utsumi
- WL Dahut
- Publication venue
- Nature Publishing Group
- Publication date
- 01/01/2008
- Field of study
The steroidal-based drug 2-ethyloestradiol-3,17-O,O-bis-sulphamate (STX243) has been developed as a potent antiangiogenic and antitumour compound. The objective of this study was to ascertain whether STX243 is more active in vivo than the clinically relevant drug 2-methoxyoestradiol (2-MeOE2) and the structurally similar compound 2-MeOE2-3,17-O,O-bis-sulphamate (STX140). The tumour growth inhibition efficacy, antiangiogenic potential and pharmacokinetics of STX243 were examined using four in vivo models. Both STX243 and STX140 were capable of retarding the growth of MDA-MB-231 xenograft tumours (72 and 63%, respectively), whereas no inhibition was observed for animals treated with 2-MeOE2. Further tumour inhibition studies showed that STX243 was also active against MCF-7 paclitaxel-resistant tumours. Using a Matrigel plug-based model, in vivo angiogenesis was restricted with STX243 and STX140 (50 and 72%, respectively, using a 10 mg kg−1 oral dose), thereby showing the antiangiogenic activity of both compounds. The pharmacokinetics of STX243 were examined at two different doses using adult female rats. The compound was orally bioavailable (31% after a single 10 mg kg−1 dose) and resistant to metabolism. These results show that STX243 is a potent in vivo drug and could be clinically effective at treating a number of oncological conditions
Measurement of the branching fraction and CP content for the decay B(0) -> D(*+)D(*-)
- Author
- Abe K
- Abrams GS
- Adam I
- Adye T
- Albert J
- Aleksan R
- Allison J
- Alsmiller JRG
- Angelini C
- Anjomshoaa A
- Anulli F
- Arisaka K
- Aspinwall ML
- Aston D
- Aubert B
- BABAR Collaboration
- Back JJ
- Bagnasco S
- Baldini-Ferroli R
- Band HR
- Barillari T
- Barlow NR
- Barlow RJ
- Bartoldus R
- Batignani G
- Bauer JM
- Bellodi G
- Benayoun M
- Berger N
- Beringer J
- Bernard D
- Bernet R
- Best D
- Bettarini S
- Bevan AJ
- Bhimji W
- Bianchi F
- Bionta RM
- Blaylock G
- Blinov VE
- Bloom P
- Blouw J
- Bona M
- Bondioli M
- Bonneaud GR
- Borean C
- Borgland AW
- Bosisio L
- Boutigny D
- Bowerman DA
- Boyarski AM
- Boyd JT
- Bozzi C
- Brandt T
- Brau B
- Brau J
- Breon AB
- Briand H
- Brigljevic V
- Brochard F
- Brose J
- Brown CM
- Brown D
- Brown DN
- Bucci F
- Buchanan C
- Bugg W
- Bukin AD
- Bukin DA
- Burchat PR
- Button-Shafer J
- Buzykaev AR
- Buzzo A
- Cahn RN
- Calcaterra A
- Calderini G
- Campagna E
- Campagnari C
- Carpinelli M
- Cartaro C
- Cavallo N
- Cavoto G
- Chao M
- Charles E
- Chauveau J
- Chen E
- Chen GP
- Chen JC
- Cheng CH
- Chevalier N
- Christ S
- Chun S
- Clark PJ
- Cochran J
- Cohen-Tanugi J
- Cohn H
- Colberg T
- Colecchia F
- Contri R
- Convery MR
- Cottingham WN
- Coupal DP
- Cowan G
- Cowan R
- Crawley HB
- Cremaldi L
- Crosetti G
- Dahmes B
- Dal Corso F
- Dallapiccola C
- Dasu S
- Datta M
- Dauncey PD
- David P
- Davis CL
- De Groot N
- De Nardo G
- de Sangro R
- de Vaissiere C
- Del Buono L
- del Re D
- Della Ricca G
- Deppermann T
- Devmal S
- Di Lodovico F
- Dickopp M
- Dittongo S
- Dixon P
- Dong D
- Dorfan J
- Dorigo A
- Dubitzky RS
- Dubois-Felsmann GP
- Dunwoodie W
- Dvoretskii A
- Egede U
- Eichenbaum AM
- Eigen G
- Eisner AM
- Emery S
- Eschenburg V
- Eschrich I
- Fabozzi F
- Faccini R
- Falbo M
- Falciai D
- Farbin A
- Ferrag S
- Ferrarotto F
- Ferroni F
- Field RC
- Finocchiaro G
- Fischer PA
- Flood K
- Ford WT
- Forti AC
- Forti F
- Foster B
- Franek B
- Frank ED
- Frey R
- Fry JR
- Gabathuler E
- Gabriel TA
- Gaidot A
- Gaillard JM
- Galeazzi F
- Gamba D
- Gamet R
- Ganzhur SF
- Gatto C
- Geddes NI
- George M
- George S
- Gill MS
- Giorgi MA
- Giraud PF
- Gladney L
- Glanzman T
- Goetzen K
- Golubev VB
- Gopal GP
- Gowdy S
- Grauges E
- Green MG
- Gritsan AV
- Grosdidier G
- Grothe M
- Groysman Y
- Guo QH
- Haas T
- Haire M
- Halyo V
- Hamilton R
- Hamon O
- Harrison PF
- Harrison TJ
- Hart PA
- Harton JL
- Hast C
- Hauke A
- Hawkes CM
- Hearty C
- Henderson R
- Hertzbach SS
- Heusch CA
- Hicheur A
- Himel T
- Hitlin DG
- Hocker A
- Hryn'ova T
- Hu H
- Huffer ME
- Innes WR
- Ivanchenko VN
- Iwasaki M
- Izen JM
- Jackson F
- Jackson PD
- Jacobsen RG
- Jawahery A
- Jayatilleke S
- Jessop C
- Johnson JR
- Jolly S
- Judd D
- Kadel RW
- Kadyk J
- Karyotakis Y
- Kay M
- Kelsey MH
- Kerth LT
- Khan A
- Kim P
- Kirkby D
- Kitayama I
- Knowles DJ
- Koch H
- Kocian ML
- Kofler R
- Kolomensky YG
- Koptchev VB
- Kordich TMB
- Korol AA
- Kowalewski R
- Kozanecki W
- Kral JF
- Kravchenko EA
- Krishnamurthy M
- Kroeger R
- Kunze M
- Kurup A
- Kuznetsova N
- Lacker HM
- Lafferty GD
- Lamsa J
- Lanceri L
- Lange D
- Langenegger U
- Langer M
- Lankford AJ
- Laplace S
- Lavin D
- Le Diberder F
- LeClerc C
- Lees JP
- Leith DWGS
- Lepeltier V
- Leruste P
- Levi ME
- Levy SL
- Lewandowski B
- Lillard V
- Lista L
- Liu R
- Lo Vetere M
- Lockman WS
- London GW
- Long O
- LoSecco JM
- Lou XC
- Lu A
- Lu C
- Luitz S
- Lusiani A
- Luth V
- Lutz AM
- Lynch G
- Lynch HL
- MacFarlane DB
- Mackay C
- Macri M
- Mallik U
- Maly E
- Mancinelli G
- Mandelkern M
- Manfredi PF
- Marchiori G
- Margoni M
- Marker CE
- Marsiske H
- Martinez-Vidal F
- Mattison TS
- Mayer B
- Mazur MA
- Mazzoni MA
- McKemey AK
- McKenna JA
- McMahon S
- McMahon TR
- Meadows BT
- Menke S
- Messner R
- Metzler S
- Meyer TI
- Meyer WT
- Michelon G
- Miftakov V
- Milek M
- Monchenault GH
- Monge MR
- Moore TB
- Morandin M
- Morganti M
- Morganti S
- Morii M
- Morton GW
- Mugge M
- Muheim F
- Muller DR
- Muller-Pfefferkorn R
- Nash JA
- Nauenberg U
- Neal H
- Neri N
- Nicholson H
- Nief JY
- O'Grady CP
- O'Neale SW
- Ocariz J
- Oddone PJ
- Olivas A
- Olsen J
- Onuchin AP
- Otto S
- Oyang J
- Ozcan VE
- Paick K
- Palano A
- Palombo F
- Pan Y
- Panetta J
- Panvini RS
- Paoloni E
- Paolucci P
- Passaggio S
- Pastore FC
- Patel PM
- Patrignani C
- Patteri P
- Payne DJ
- Penny RC
- Perazzo A
- Perl M
- Peruzzi IM
- Peters K
- Petrak S
- Piccolo D
- Piccolo M
- Piemontese L
- Piredda G
- Pivk M
- Plaszczynski S
- Playfer S
- Pompili A
- Poropat P
- Porter FC
- Posocco M
- Potter RJL
- Prell S
- Prepost R
- Pripstein M
- Pulliam T
- Purohit MV
- Qi ND
- Quinn H
- Rahatlou S
- Rama M
- Rankin P
- Ratcliff BN
- Raven G
- Re V
- Reidy J
- Ricciardi S
- Richman JD
- Rizzo G
- Roat C
- Robbe P
- Roberts DA
- Robertson SH
- Robutti E
- Roe NA
- Romosan A
- Ronan MT
- Roney JM
- Rong G
- Roodman A
- Roos L
- Rosenberg EI
- Rotondo M
- Roy J
- Ryd A
- Salnikov AA
- Salvatore F
- Samuel A
- Sanders DA
- Sanders P
- Sandrelli F
- Santroni A
- Savvas N
- Schaffner SF
- Schalk T
- Schieck JR
- Schietinger T
- Schindler RH
- Schmitz RE
- Schmuecker H
- Schubert KR
- Schumm BA
- Schune MH
- Schwiening J
- Schwierz R
- Sciacca C
- Sciolla G
- Scott IJ
- Seiden A
- Sekula SJ
- Serednyakov SI
- Serfass B
- Serra M
- Sharma V
- Shelkov VG
- Shorthouse HW
- Simi G
- Simonetto F
- Sinev NB
- Singh H
- Skovpen YI
- Sloane RJ
- Smith AJS
- Smith D
- Smith JG
- Snyder A
- Soffer A
- Soha A
- Sokoloff MD
- Spaan B
- Spanier SM
- Speziali V
- Staengle H
- Stark J
- Steinke M
- Stelzer J
- Stoker DP
- Stroili R
- Strom D
- Strother P
- Stugu B
- Su D
- Sullivan MK
- Summers DJ
- Swain JE
- T'Jampens S
- Tanaka HA
- Taras P
- Taylor F
- Telnov AV
- Telnov VI
- Thiebaux C
- Thiessen D
- Tinslay J
- Tisserand V
- Toki WH
- Torassa E
- Tosi S
- Touramanis C
- Treadwell E
- Triggiani G
- Trincaz-Duvoid S
- Tumanov A
- Turnbull L
- Turri M
- Va'vra J
- Vaitsas G
- van Bibber K
- van Hoek WC
- Varnes EW
- Vasileiadis G
- Vasseur G
- Verderi M
- Verkerke W
- Vidal PB
- Voci C
- Voena C
- von Wimmersperg-Toeller JH
- Vuagnin G
- Wagner SR
- Wagoner DE
- Waldi R
- Walkowiak W
- Walsh J
- Wang P
- Watson AT
- Watson NK
- Weatherall JH
- Weaver M
- Weidemann AW
- Weinstein AJR
- Wenzel WA
- Wilden L
- Williams DC
- Williams JC
- Willocq S
- Wilson FF
- Wilson MG
- Wilson RJ
- Wisniewski WJ
- Wormser G
- Wright DH
- Wright DM
- Wu SL
- Xella SM
- Xie Y
- Yamamoto RK
- Yang S
- Yeche C
- Yi J
- Young CC
- Yu Z
- Yumiceva FX
- Yushkov AN
- Zallo A
- Zghiche A
- Zhang J
- Zhang L
- Zhu RY
- Zhu YS
- Zito M
- Publication venue
- American Physical Society
- Publication date
- 01/01/2002
- Field of study
This is the pre-print version of the Article. The official published version can be accessed from the links below. Copyright @ 2002 APS.We report a measurement of the branching fraction of the decay B0→D*+D*- and of the CP-odd component of its final state using the BABAR detector. With data corresponding to an integrated luminosity of 20.4 fb-1 collected at the Υ(4S) resonance during 1999–2000, we have reconstructed 38 candidate signal events in the mode B0→D*+D*- with an estimated background of 6.2±0.5 events. From these events, we determine the branching fraction to be B(B0→D*+D*-)=[8.3±1.6(stat)±1.2(syst)]×10-4. The measured CP-odd fraction of the final state is 0.22±0.18(stat)±0.03(syst).This work is supported by DOE and NSF (USA), NSERC (Canada), IHEP (China), CEA and CNRS-IN2P3 (France), BMBF (Germany), INFN (Italy), NFR (Norway), MIST (Russia), and PPARC (United Kingdom). Individuals have received support from the A.P. Sloan Foundation, Research Corporation, and Alexander von Humboldt Foundation
Measurement of D-s(+) and D-s(*+) production in B meson decays and from continuum e(+)e(-) annihilation at √s=10.6 GeV
- Author
- Abe K
- Abrams GS
- Adam I
- Adye T
- Albert J
- Aleksan R
- Allison J
- Alsmiller JRG
- Andress JC
- Angelini C
- Anjomshoaa A
- Anthony PL
- Anulli F
- Arisaka K
- Aspinwall ML
- Aston D
- Aubert B
- Azzopardi DE
- BABAR Collaboration
- Back JJ
- Bagnasco S
- Baird K
- Baldini-Ferroli R
- Band HR
- Barillari T
- Barlow NR
- Barlow RJ
- Bartoldus R
- Batignani G
- Bauer JM
- Benayoun M
- Berger N
- Beringer J
- Bernard D
- Bernet R
- Best D
- Bettarini S
- Bhimji W
- Bianchi F
- Bionta RM
- Blaylock G
- Blinov VE
- Bloom E
- Bloom P
- Blouw J
- Bona M
- Bondioli M
- Bonneaud GR
- Borean C
- Borgland AW
- Bosisio L
- Boutigny D
- Bowerman DA
- Boyarski AM
- Boyd JT
- Bozzi C
- Brandt T
- Brau B
- Brau J
- Breon AB
- Briand H
- Bright-Thomas PG
- Brigljevic V
- Brochard F
- Brose J
- Brown CM
- Brown D
- Brown DN
- Buchanan C
- Bugg W
- Bukin AD
- Bukin DA
- Bulos F
- Burchat PR
- Button-Shafer J
- Buzykaev AR
- Buzzo A
- Cahn RN
- Calcaterra A
- Calderini G
- Campagnari C
- Carpinelli M
- Carroll M
- Cartaro C
- Cavallo N
- Cavoto G
- Chao M
- Charles E
- Chauveau J
- Chen E
- Chen GP
- Chen JC
- Cheng CH
- Chevalier N
- Christ S
- Chun S
- Clark AR
- Clark PJ
- Cochran J
- Cohen-Tanugi J
- Cohn H
- Colberg T
- Colecchia F
- Contri R
- Convery MR
- Copty N
- Cottingham WN
- Coupal DP
- Cowan G
- Cowan R
- Coward DH
- Crawley HB
- Cremaldi L
- Crosetti G
- Dahmes B
- Dal Corso F
- Dallapiccola C
- Dasu S
- Dauncey PD
- David P
- Davis CL
- De Groot N
- de la Vaissiere C
- de Lesquen A
- de Monchenault GH
- De Nardo G
- de Sangro R
- Del Buono L
- del Re D
- Della Ricca G
- Deppermann T
- Devmal S
- Di Lodovico F
- Dickopp M
- Dima MO
- Dittongo S
- Dixon P
- Dorfan DE
- Dorfan J
- Dorigo A
- Dubitzky RS
- Dubois-Felsmann GP
- Dunwoodie W
- Dvoretskii A
- Dyce N
- Egede U
- Eichenbaum AM
- Eigen G
- Eisner AM
- Elmer P
- Emery S
- Eschenburg V
- Eschrich I
- Fabozzi F
- Faccini R
- Fahey S
- Falbo M
- Falciai D
- Farbin A
- Ferrag S
- Ferrarotto F
- Ferroni F
- Field RC
- Finocchiaro G
- Fischer PA
- Flood K
- Ford WT
- Forti AC
- Forti F
- Foster B
- Franek B
- Frank ED
- Frey R
- Fry JR
- Fullwood J
- Gabathuler E
- Gabriel TA
- Gaidot A
- Gaillard JM
- Galeazzi F
- Gamba D
- Gamet R
- Ganzhur SF
- Gatto C
- Geddes NI
- Geld TL
- George M
- George S
- Gill MS
- Giorgi MA
- Giraud PF
- Gladney L
- Glanzman T
- Godfrey GL
- Goetzen K
- Golubev VB
- Gopal GP
- Gowdy S
- Green MG
- Grillo AA
- Gritsan AV
- Grosdidier G
- Grosso P
- Grothe M
- Groysman Y
- Gunawardane NJW
- Guo QH
- Haas T
- Haire M
- Hamilton R
- Hamon O
- Handler T
- Harrison PF
- Harrison TJ
- Hart PA
- Harton JL
- Hast C
- Hauke A
- Hawkes CM
- Hearty C
- Henderson R
- Hertzbach SS
- Heusch CA
- Hicheur A
- Himel T
- Hitlin DG
- Hocker A
- Hryn'ova T
- Hu H
- Huffer ME
- Innes WR
- Ivanchenko VN
- Iwasaki M
- Izen JM
- Jackson F
- Jackson PD
- Jacobsen RG
- Jawahery A
- Jayatilleke S
- Jessop C
- Johnson DR
- Johnson JR
- Johnson RP
- Jolly S
- Judd D
- Kadel RW
- Kadyk J
- Karyotakis Y
- Kay M
- Kelsey MH
- Kerth LT
- Khan A
- Kim P
- Kirkby D
- Kitayama I
- Knowles DJ
- Koch H
- Kocian ML
- Kofler R
- Kolomensky YG
- Koptchev VG
- Kordich TMB
- Korol AA
- Kowalewski R
- Kozanecki W
- Kral JF
- Kravchenko EA
- Krishnamurthy M
- Kroeger R
- Kunze M
- Kurup A
- Kuznetsova N
- Lacker HM
- Lafferty GD
- Lamanna E
- Lamsa J
- Lanceri L
- Lange D
- Langenegger U
- Langer M
- Lankford AJ
- Laplace S
- Lavin D
- Le Diberder F
- LeClerc C
- Lees JP
- Leith DWGS
- Leonardi E
- Lepeltier V
- Leruste P
- Levi ME
- Levy SL
- Lewandowski B
- Lillard V
- Lista L
- Liu R
- Lo Vetere M
- Lockman WS
- London GW
- Long O
- LoSecco JM
- Lou XC
- Lu A
- Lu C
- Luitz S
- Lusiani A
- Luth V
- Lutz AM
- Lynch G
- Lynch HL
- MacFarlane DB
- Mackay C
- Macri M
- Mallik U
- Maly E
- Mancinelli G
- Mandelkern M
- Manfredi PF
- Margoni M
- Marker CE
- Marsiske H
- Martin JP
- Martinez-Vidal F
- Mattison TS
- Mayer B
- Mazzoni MA
- McDonald KT
- McGrath P
- McKemey AK
- McKenna JA
- McMahon S
- McMahon TR
- Meadows BT
- Menke S
- Messner R
- Metzler S
- Meyer TI
- Meyer WT
- Michelon G
- Miftakov V
- Milek M
- Moffeit KC
- Monge MR
- Moore TB
- Morandin M
- Morganti M
- Morganti S
- Morii M
- Mount R
- Mugge M
- Muheim F
- Muller DR
- Muller-Pfefferkorn R
- Nash JA
- Nauenberg U
- Neal H
- Neri N
- Nicholson H
- Nief JY
- O'Grady CP
- O'Neale SW
- Ocariz J
- Oddone PJ
- Olivas A
- Olsen J
- Onuchin AP
- Otto S
- Oyang J
- Ozcan VE
- Paick K
- Palano A
- Palombo F
- Pan Y
- Panetta J
- Panvini RS
- Paoloni E
- Paolucci P
- Passaggio S
- Pastore FC
- Patel PM
- Patrignani C
- Patteri P
- Payne DJ
- Penny RC
- Perazzo A
- Perl M
- Peruzzi IM
- Peters K
- Petrak S
- Pia MG
- Piccolo D
- Piccolo M
- Piemontese L
- Piredda G
- Plaszczynski S
- Playfer S
- Pompili A
- Poropat P
- Porter FC
- Posocco M
- Potter RJL
- Prell S
- Prepost R
- Pripstein M
- Pulliam T
- Purohit MV
- Qi ND
- Quinn H
- Rahatlou S
- Rama M
- Rankin P
- Ratcliff BN
- Raven G
- Re V
- Reidy J
- Ricciardi S
- Richman JD
- Rizzo G
- Roat C
- Robbe P
- Roberts DA
- Robertson SH
- Robutti E
- Rochester LS
- Roe NA
- Romosan A
- Ronan MT
- Roney JM
- Rong G
- Roodman A
- Roos L
- Rosenberg EI
- Rotondo M
- Roussot E
- Roy J
- Ryd A
- Sadrozinski H
- Salnikov AA
- Salvatore F
- Samuel A
- Sanders DA
- Sanders P
- Sandrelli F
- Santroni A
- Savvas N
- Schaffner SF
- Schalk T
- Schieck JR
- Schietinger T
- Schindler RH
- Schmitz RE
- Schmuecker H
- Schubert KR
- Schumm BA
- Schune MH
- Schwiening J
- Schwierz R
- Sciacca C
- Sciolla G
- Scott I
- Scott IJ
- Seiden A
- Seitz R
- Sekula SJ
- Sen S
- Serbo VV
- Serednyakov SI
- Serfass B
- Serra M
- Sharma V
- Shelkov VG
- Shorthouse HW
- Simi G
- Simonetto F
- Simopoulos ET
- Sinev NB
- Singh H
- Skovpen YI
- Sloane RJ
- Smith AJS
- Smith D
- Smith JG
- Smol A
- Snyder A
- Soffer A
- Soha A
- Sokoloff MD
- Spaan B
- Spanier SM
- Speziali V
- Staengle H
- Stark J
- Steinke M
- Stelzer J
- Stoker DP
- Stroili R
- Strom D
- Strother P
- Stugu B
- Su D
- Sullivan MK
- Summers DJ
- Sutton CS
- Swain JE
- T'Jampens S
- Tanaka HA
- Taras P
- Taylor F
- Tehrani FS
- Telnov AV
- Telnov VI
- Thiebaux C
- Thiessen D
- Tinslay J
- Tisserand V
- Toki WH
- Torassa E
- Tosi S
- Touramanis C
- Treadwell E
- Triggiani G
- Trincaz-Duvoid S
- Tumanov A
- Turnbull L
- Turri M
- Va'vra J
- Vaitsas G
- van Bibber K
- van Hoek WC
- Varnes EW
- Vasileiadis G
- Vasseur G
- Verderi M
- Verkerke W
- Versille S
- Vidal PB
- Voci C
- Voena C
- von Wimmersperg-Toeller JH
- Vuagnin G
- Wagner DL
- Wagner SR
- Wagoner DE
- Waldi R
- Walkowiak W
- Wallom D
- Walsh J
- Wang P
- Watson AT
- Watson NK
- Weatherall JH
- Weaver M
- Weidemann AW
- Weinstein AJR
- Wenzel WA
- Wilden L
- Williams DC
- Williams MI
- Willocq S
- Wilson FF
- Wilson MG
- Wilson RJ
- Wisniewski WJ
- Witherell M
- Wormser G
- Wright DH
- Wright DM
- Wu SL
- Xella SM
- Xie Y
- Yamamoto RK
- Yang S
- Yeche C
- Yellin S
- Young CC
- Yu Z
- Yumiceva FX
- Yushkov AN
- Zacek V
- Zallo A
- Zhang J
- Zhu RY
- Zhu YS
- Zito M
- Publication venue
- American Physical Society
- Publication date
- 01/01/2002
- Field of study
This is the pre-print version of the Article. The official published version can be accessed from the links below. Copyright @ 2002 APSNew measurements of Ds+ and Ds*+ meson production rates from B decays and from qq̅ continuum events near the Υ(4S) resonance are presented. Using 20.8 fb-1 of data on the Υ(4S) resonance and 2.6 fb-1 off-resonance, we find the inclusive branching fractions B(B⃗Ds+X)=(10.93±0.19±0.58±2.73)% and B(B⃗Ds*+X)=(7.9±0.8±0.7±2.0)%, where the first error is statistical, the second is systematic, and the third is due to the Ds+→φπ+ branching fraction uncertainty. The production cross sections σ(e+e-→Ds+X)×B(Ds+→φπ+)=7.55±0.20±0.34pb and σ(e+e-→Ds*±X)×B(Ds+→φπ+)=5.8±0.7±0.5pb are measured at center-of-mass energies about 40 MeV below the Υ(4S) mass. The branching fractions ΣB(B⃗Ds(*)+D(*))=(5.07±0.14±0.30±1.27)% and ΣB(B⃗Ds*+D(*))=(4.1±0.2±0.4±1.0)% are determined from the Ds(*)+ momentum spectra. The mass difference m(Ds+)-m(D+)=98.4±0.1±0.3MeV/c2 is also measured.This work was supported by DOE and NSF (USA), NSERC (Canada), IHEP (China), CEA and CNRS-IN2P3 (France), BMBF (Germany), INFN (Italy), NFR (Norway), MIST (Russia), and PPARC (United Kingdom). Individuals have received support from the Swiss NSF, A. P. Sloan Foundation, Research Corporation, and Alexander von Humboldt Foundation
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
- Altenburg D
- Andreassen R
- Andreotti M
- Angelini C
- Anulli F
- 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
- Barrett M
- Bartoldus R
- Batignani G
- Battaglia M
- Bauer JM
- Beck TW
- Behera PK
- Bellini F
- Benayoun M
- Benelli G
- Berger N
- Bernard D
- Berryhill JW
- Best D
- Bettarini S
- Bettoni D
- Bevan AJ
- Bhimji W
- Bhuyan B
- Bianchi F
- Biasini M
- Biesiada J
- Blanc F
- Blaylock G
- Blinov AE
- Blinov VE
- Bloom PC
- Blount NL
- Bomben M
- Bona M
- Bondioli M
- Bonneaud GR
- Bosisio L
- Boutigny D
- Bowerman DA
- Boyarski AM
- Boyd JT
- Bozzi C
- Brandenburg G
- Brandt T
- Brau J
- Breon AB
- Brose J
- Brown CL
- Brown CM
- Brown DN
- Brown DN
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- Bucci F
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- Buono LD
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- Burke JP
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- Buzzo A
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- Calderini G
- Campagnari C
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- Chai X
- Chaisanguanthum KS
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- Wisniewski WJ
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- Xie Y
- Yamamoto RK
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- Yeche C
- Yi JI
- Yi K
- Young CC
- Yu Z
- Yushkov AN
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- Zallo A
- Zeng Q
- Zghiche A
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- 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 of associated near-side and away-side long-range correlations in √sNN=5.02 TeV proton-lead collisions with the ATLAS detector
- Author
- Aad G
- Abajyan T
- Abbott B
- Abdallah J
- Abdel Khalek S
- Abdelalim AA
- Abdinov O
- Aben R
- Abi B
- Abolins M
- Abouzeid OS
- Abramowicz H
- Abreu H
- Acharya BS
- Adamczyk L
- Adams DL
- Addy TN
- Adelman J
- Adomeit S
- Adragna P
- Adye T
- Aefsky S
- Aguilar-Saavedra JA
- Agustoni M
- Ahlen SP
- Ahles F
- Ahmad A
- Ahsan M
- Aielli G
- Akesson TP
- 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 BM
- Allison LJ
- Allport PP
- Allwood-Spiers SE
- Almond J
- Aloisio A
- Alon R
- Alonso A
- Alonso F
- Altheimer A
- Alvarez Gonzalez B
- Alviggi MG
- Amako K
- Amelung C
- Ammosov VV
- Amor Dos Santos SP
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- Zhu J
- Zhu Y
- Zhuang X
- Zhuravlov V
- Zibell A
- Zieminska D
- Zimin NI
- Zimmermann R
- Zimmermann S
- Zimmermann S
- Zinonos Z
- Ziolkowski M
- Zitoun R
- Zivković L
- Zmouchko VV
- Zobernig G
- Zoccoli A
- Zur Nedden M
- Zutshi V
- Zwalinski L
- Publication venue
- American Physical Society
- Publication date
- 01/01/2012
- Field of study
Two-particle correlations in relative azimuthal angle (Δϕ) and pseudorapidity (Δη) are measured in √sNN=5.02 TeV p+Pb collisions using the ATLAS detector at the LHC. The measurements are performed using approximately 1 μb-1 of data as a function of transverse momentum (pT) and the transverse energy (ΣETPb) summed over 3.1<η<4.9 in the direction of the Pb beam. The correlation function, constructed from charged particles, exhibits a long-range (2<|Δη|<5) “near-side” (Δϕ∼0) correlation that grows rapidly with increasing ΣETPb. A long-range “away-side” (Δϕ∼π) correlation, obtained by subtracting the expected contributions from recoiling dijets and other sources estimated using events with small ΣETPb, is found to match the near-side correlation in magnitude, shape (in Δη and Δϕ) and ΣETPb dependence. The resultant Δϕ correlation is approximately symmetric about π/2, and is consistent with a dominant cos2Δϕ modulation for all ΣETPb ranges and particle pT
Measurements of fiducial and differential cross sections for Higgs boson production in the diphoton decay channel at s√=8 TeV with ATLAS
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- A Djouadi
- A Idilbi
- A. A. E. Bannoura
- A. A. Grillo
- A. A. Komar
- A. A. Korol
- A. A. Maier
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- A. A. Snesarev
- A. A. Solodkov
- A. A. Talyshev
- A. Aloisio
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- A. Andreazza
- A. Angerami
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- A. Antonaki
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- A. Artamonov
- A. Ashkenazi
- A. B. Fenyuk
- A. Baas
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- A. Bellerive
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- A. Borisov
- A. Boveia
- A. Brandt
- A. Bruni
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- A. C. Bundock
- A. C. Daniells
- A. C. Florez Bustos
- A. C. König
- A. C. Martyniuk
- A. C. Schaffer
- A. Calandri
- A. Campoverde
- A. Canepa
- A. Castelli
- A. Catinaccio
- A. Cattai
- A. Cerri
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- A. Cortes-Gonzalez
- A. D. Hawkins
- A. D. Pilkington
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- Z. Hajduk
- Z. Hubacek
- Z. J. Grout
- Z. Kohout
- Z. L. Ren
- Z. Liang
- Z. M. Karpova
- Z. Marshall
- Z. Rurikova
- Z. V. Krumshteyn
- Z. Vykydal
- Z. Weng
- Z. Yan
- Z. Zhang
- Z. Zhao
- Z. Zinonos
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2014
- Field of study
Measurements of fiducial and differential cross sections are presented for Higgs boson production in proton-proton collisions at a centre-of-mass energy of s√=8 TeV. The analysis is performed in the H → γγ decay channel using 20.3 fb−1 of data recorded by the ATLAS experiment at the CERN Large Hadron Collider. The signal is extracted using a fit to the diphoton invariant mass spectrum assuming that the width of the resonance is much smaller than the experimental resolution. The signal yields are corrected for the effects of detector inefficiency and resolution. The pp → H → γγ fiducial cross section is measured to be 43.2 ±9.4(stat.) − 2.9 + 3.2 (syst.) ±1.2(lumi)fb for a Higgs boson of mass 125.4GeV decaying to two isolated photons that have transverse momentum greater than 35% and 25% of the diphoton invariant mass and each with absolute pseudorapidity less than 2.37. Four additional fiducial cross sections and two cross-section limits are presented in phase space regions that test the theoretical modelling of different Higgs boson production mechanisms, or are sensitive to physics beyond the Standard Model. Differential cross sections are also presented, as a function of variables related to the diphoton kinematics and the jet activity produced in the Higgs boson events. The observed spectra are statistically limited but broadly in line with the theoretical expectations
Search for R-parity-violating supersymmetry in events with four or more leptons in sqrt(s) =7 TeV pp collisions with the ATLAS detector
- Author
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- della Porta GZ
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- Zhemchugov A
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- Zivkovic L
- Zmouchko VV
- Zobernig G
- Zoccoli A
- zur Nedden M
- Zutshi V
- Zwalinski L
- Collaboration ATLAS
- Publication venue
- Springer Verlag
- Publication date
- 01/01/2008
- Field of study
A search for new phenomena in final states with four or more leptons (electrons or muons) is presented. The analysis is based on 4.7 fb−1 of s=7TeV proton-proton collisions delivered by the Large Hadron Collider and recorded with the ATLAS detector. Observations are consistent with Standard Model expectations in two signal regions: one that requires moderate values of missing transverse momentum and another that requires large effective mass. The results are interpreted in a simplified model of R-parity-violating supersymmetry in which a 95% CL exclusion region is set for charged wino masses up to 540 GeV. In an R-parity-violating MSUGRA/CMSSM model, values of m 1/2 up to 820 GeV are excluded for 10 < tan β < 40
Search for high-mass resonances decaying to dilepton final states in pp collisions at s√=7 TeV with the ATLAS detector
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- Yanush S
- Yao L
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- Yilmaz M
- Yoosoofmiya R
- Yorita K
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- Yoshihara K
- Young C
- Young CJ
- Youssef S
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- Yurkewicz A
- Zabinski B
- Zaidan R
- Zaitsev AM
- Zajacova Z
- Zanello L
- Zanzi D
- Zaytsev A
- Zeitnitz C
- Zeman M
- Zemla A
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- Zenin O
- Zenis T
- Zerwas D
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- Zhao L
- Zhao Z
- Zhemchugov A
- Zhong J
- Zhou B
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- Zhu CG
- Zhu H
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- Zhu Y
- Zhuang X
- Zhuravlov V
- Zibell A
- Zieminska D
- Zimin NI
- Zimmermann R
- Zimmermann S
- Zimmermann S
- Zinonos Z
- Ziolkowski M
- Zitoun R
- Zivkovic L
- Zmouchko VV
- Zobernig G
- Zoccoli A
- zur Nedden M
- Zutshi V
- Zwalinski L
- Publication venue
- Springer
- Publication date
- 01/01/2012
- Field of study
The ATLAS detector at the Large Hadron Collider is used to search for high-mass resonances decaying to an electron-positron pair or a muon-antimuon pair. The search is sensitive to heavy neutral Z′ gauge bosons, Randall-Sundrum gravitons, Z * bosons, techni-mesons, Kaluza-Klein Z/γ bosons, and bosons predicted by Torsion models. Results are presented based on an analysis of pp collisions at a center-of-mass energy of 7 TeV corresponding to an integrated luminosity of 4.9 fb−1 in the e + e − channel and 5.0 fb−1 in the μ + μ −channel. A Z ′ boson with Standard Model-like couplings is excluded at 95 % confidence level for masses below 2.22 TeV. A Randall-Sundrum graviton with coupling k/MPl=0.1 is excluded at 95 % confidence level for masses below 2.16 TeV. Limits on the other models are also presented, including Technicolor and Minimal Z′ Models
Measurement of the cross-section of high transverse momentum vector bosons reconstructed as single jets and studies of jet substructure in pp collisions at √s = 7 TeV with the ATLAS detector
- Author
- Aad G
- Abajyan T
- Abbott B
- Abdallah J
- Abdinov O
- Aben R
- Abi B
- Abolins M
- AbouZeid OS
- Abramowicz H
- Abreu H
- Abulaitia Y
- Acharya BS
- Adamczyk L
- Adams DL
- Addy TN
- Adelman J
- Adomeit S
- Adye T
- Agatonovic-Jovin T
- Aguilar-Saavedra JA
- Agustoni M
- Ahlen SP
- Ahmadov F
- Aielli G
- Akesson TP
- Akimoto G
- Akimov AV
- Albert J
- Albrand S
- Alconada Verzini MJ
- Aleksa M
- Aleksandrov IN
- Alexa C
- Alexander G
- Alexandre G
- Alexopoulos T
- Alhroob M
- Alimonti G
- Alio L
- Alison J
- Allbrooke BMM
- Allison LJ
- Allport PP
- Allwood-Spiers SE
- Almond J
- Aloisio A
- Alon R
- Alonso A
- Alonso F
- Alpigiani C
- Altheimer A
- Alviggi MG
- Amako K
- Amelung C
- Ammosov VV
- Amor Dos Santos SP
- Amorim A
- Amoroso S
- Amram N
- Amundsen G
- Anastopoulos C
- Ancu LS
- Andari N
- Andeen T
- Anders CF
- Anders G
- Anderson KJ
- Andreazza A
- Andrei V
- Anduaga XS
- Angelidakis S
- Anger P
- Angerami A
- Anghinolfi F
- Anh TV
- Anisenkov AV
- Anjos N
- Annovi A
- Antonaki A
- Antonelli M
- Antonov A
- Antos J
- Anulli F
- Aoki M
- Apolle R
- Arabidze G
- Aracena I
- Arai Y
- Arce ATH
- Arguin J-F
- Argyropoulos S
- Arik E
- Arik M
- Armbruster AJ
- Arnaez O
- Arnal V
- Arslan O
- Artamonov A
- Artoni G
- Asai S
- Asbah N
- Ask S
- Asman B
- Asquith L
- Assamagan K
- Astalos R
- Astbury A
- Atkinson M
- Atlay NB
- Auerbach B
- Auge E
- Augsten K
- Aurousseau M
- Avolio G
- Azuelos G
- Azuma Y
- Baak MA
- Bacci C
- Bach AM
- Bachacou H
- Bachas K
- Backes M
- Backhaus M
- Badescua E
- Bagiacchi P
- Bagnaia P
- Bai Y
- Bailey DC
- Bain T
- Baines JT
- Baker OK
- Baker S
- Balek P
- Balli F
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- Bessidskaia O
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- Bloch I
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- Buckley AG
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- Budagov IA
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- Bugge L
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- Bundock AC
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- Burghgrave B
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- Burmeister I
- Busato E
- Bussey P
- Bustos ACF
- Buszello CP
- Butler B
- Butler JM
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- Buttar CM
- Butterworth JM
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- Caforio D
- Cakir IT
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- Calderini G
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- Camillocci ES
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- Caminal Armadans R
- Campana S
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- Castanheira MTD
- Castelli A
- Castillo Gimenez V
- Castillo IS
- Castillo LRF
- Castillo LRF
- Castro NF
- Catastini P
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- Catmore JR
- Cattai A
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- Chalupkova I
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- Chekulaev SV
- Chelkov GA
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- Chen C
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- Chen Y
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- Cheng Y
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- Chernyatin V
- Cheu E
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- Chilingarov A
- Chiodini G
- Chisholm AS
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- Chromek-Burckhart D
- Chu ML
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- Cortes-Gonzalez A
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- Da Costa JGPF
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- Da Cunha Sargedas De Sousa MJ
- Da Via C
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- Dafinca A
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- de Jong P
- De la Taille C
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- de Lima DEF
- de Lima DEF
- De Lorenzi F
- De Mendizabal JB
- De Nooij L
- De Pedis D
- De Regie JBDV
- de Renstrom PAB
- De Salvo A
- De Sanctis U
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- Degenhardt J
- Deigaard I
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- Del Prete T
- Delemontex T
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- Dell'Acqua A
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- Della Pietra M
- della Porta GZ
- della Volpe D
- Delmastro M
- Delsart PA
- Deluca C
- Demers S
- Demichev M
- Demilly A
- Demirkoz B
- Denisov SP
- Derendarz D
- Derkaoui JE
- Derue F
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- Deviveiros PO
- Dewhurst A
- Dhaliwal S
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- Di Domenico A
- Di Donato C
- Di Girolamo A
- Di Girolamo B
- Di Mattia A
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- Di Nardo R
- Di Simone A
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- Di Valentino D
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- Dionisi C
- Dita P
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- Djama F
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- do Vale MAB
- Doan TKO
- Dobos D
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- Doglioni C
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- Dohmae T
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- Dubreuil E
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- Dueren M
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- Dunford M
- Dwuznik M
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- Edson W
- Edwards NC
- Ehrenfeld W
- Eifert T
- Eigen G
- Einsweiler K
- Ekelof T
- El Kacimi M
- El Moursli A
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- Ellert M
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- Elmsheuser J
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- Emeliyanov D
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- Enari Y
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- Endner OC
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- Endo M
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- Engelmann R
- Engelmann R
- Erdmann J
- Erdmann J
- Ereditato A
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- Eriksson D
- Eriksson D
- Ernis G
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- Ernst J
- Ernst J
- Ernst M
- Ernst M
- Ernwein J
- Ernwein J
- Errede D
- Errede D
- Errede S
- Errede S
- Ertel E
- Ertel E
- Escalier M
- Escalier M
- Esch H
- Esch H
- Escobar C
- Escobar C
- Espinal Curull X
- Espinal Curull X
- Esposito B
- Esposito B
- Etienne F
- Etienne F
- Etienvre AI
- Etienvre AI
- Etzion E
- Etzion E
- Evans H
- Evans H
- Fabbri L
- Fabbri L
- Facini G
- Facini G
- Fajardo LSG
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- Fakhrutdinov RM
- Fakhrutdinov RM
- Falciano S
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- Faltova J
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- Fang Y
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- Fanti M
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- Farbin A
- Farbin A
- Farilla A
- Farilla A
- Farooque T
- Farooque T
- Farrell S
- Farrell S
- Farrington SM
- Farrington SM
- Farthouat P
- Farthouat P
- Fassi F
- Fassi F
- Fassnacht P
- Fassnacht P
- Fassouliotis D
- Fassouliotis D
- Favareto A
- Favareto A
- Fayard L
- Fayard L
- Federic P
- Federic P
- Fedin OL
- Fedin OL
- Fedorko W
- Fedorko W
- Fehling-Kaschek M
- Fehling-Kaschek M
- Feigl S
- Feigl S
- Feligioni L
- Feligioni L
- Feng C
- Feng C
- Feng EJ
- Feng EJ
- Feng H
- Feng H
- Fenyuk AB
- Fenyuk AB
- Fernando W
- Fernando W
- Ferrag S
- Ferrag S
- Ferrando BMS
- Ferrando J
- Ferrando J
- Ferrara V
- Ferrara V
- Ferrari A
- Ferrari A
- Ferrari P
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- Ferrari R
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- Ferrer A
- Ferrer A
- Ferrere D
- Ferrere D
- Ferretti C
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- Fiascaris M
- Fiascaris M
- Fiedler F
- Fiedler F
- Filipcic A
- Filipcic A
- Filipuzzi M
- Filipuzzi M
- Filthaut F
- Filthaut F
- Fincke-Keeler M
- Fincke-Keeler M
- Finelli KD
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- Fiolhais MCN
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- Fiorini L
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- Firan A
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- Fischer J
- Fischer J
- Fisher MJ
- Fisher MJ
- Fitzgerald EA
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- Flechl M
- Flechl M
- Fleck I
- Fleck I
- Fleischmann P
- Fleischmann P
- Fleischmann S
- Fleischmann S
- Fletcher G
- Fletcher G
- Fletcher GT
- Fletcher GT
- Flick T
- Flick T
- Floderus A
- Floderus A
- Florez Bustos AC
- Flowerdew MJ
- Flowerdew MJ
- Formica A
- Formica A
- Forti A
- Forti A
- Fortin D
- Fortin D
- Fournier D
- Fournier D
- Fox H
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- Francavilla P
- Francavilla P
- Franchini M
- Franchini M
- Franchino S
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- Francis D
- Francis D
- Franklin M
- Franklin M
- Franz S
- Franz S
- Fraternali M
- Fraternali M
- Fratin S
- Fratina S
- French ST
- French ST
- Friedrich C
- Friedrich C
- Friedrich F
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- Froidevaux D
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- Frost JA
- Frost JA
- Fukunaga C
- Fukunaga C
- Fulsom BG
- Fulsom BG
- Fuster J
- Fuster J
- Gabaldon C
- Gabaldon C
- Gabizon O
- Gabizon O
- Gabrielli A
- Gabrielli A
- Gabrielli A
- Gabrielli A
- Gadatsch S
- Gadatsch S
- Gadomski S
- Gadomski S
- Gagliardi G
- Gagliardi G
- Gagnon P
- Gagnon P
- Galea C
- Galea C
- Galhardo B
- Galhardo B
- Gallas EJ
- Gallas EJ
- Gallo V
- Gallo V
- Gallop BJ
- Gallop BJ
- Gallus P
- Gallus P
- Galster G
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- Gan KK
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- Gandrajula RP
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- Gao J
- Gao YS
- Gao YS
- Gaob J
- Garberson F
- Garberson F
- Garcia Navarro JE
- Garcia Navarro JE
- Garcia BRM
- Garcia C
- Garcia C
- Garcia JAB
- Garcia-Sciveres M
- Garcia-Sciveres M
- Gardner RW
- Gardner RW
- Garelli N
- Garelli N
- Garonne V
- Garonne V
- Garrido MDMC
- Gatti C
- Gatti C
- Gaudio G
- Gaudio G
- Gaur B
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- Gauthier L
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- Gauzzi P
- Gauzzi P
- Gavrilenko IL
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- Gay C
- Gay C
- Gaycken G
- Gaycken G
- Gazis EN
- Gazis EN
- Ge P
- Ge P
- Gecse Z
- Gecse Z
- Gee CNP
- Gee CNP
- Geerts DAA
- Geerts DAA
- Geich-Gimbel C
- Geich-Gimbel C
- Gellerstedt K
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- Gemme C
- Gemme C
- Gemmell A
- Gemmell A
- Genest MH
- Genest MH
- Gentile S
- Gentile S
- George M
- George M
- George S
- George S
- Gerbaudo D
- Gerbaudo D
- Gershon A
- Gershon A
- Ghazlane H
- Ghazlane H
- Ghodbane N
- Ghodbane N
- Giacobbe B
- Giacobbe B
- Giagu S
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- Giangiobbe V
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- Giannetti P
- Giannetti P
- Gianotti F
- Gianotti F
- Gibbard B
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- Gibson SM
- Gibson SM
- Gilchriese M
- Gilchriese M
- Gillam TPS
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- Gillberg D
- Gillberg D
- Gillman AR
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- Gingrich DM
- Gingrich M
- Giokaris N
- Giokaris N
- Giordani MP
- Giordani MP
- Giordano R
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- Giorgi FM
- Giorgi FM
- Giraud PF
- Giraud PF
- Giugni D
- Giugni D
- Giuliani C
- Giuliani C
- Giunta M
- Giunta M
- Gjelsten BK
- Gjelsten BK
- Gkialas I
- Gkialas I
- Gladilin LK
- Gladilin LK
- Glasman C
- Glasman C
- Glatzer J
- Glatzer J
- Glazov A
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- Goddard JR
- Goddard JR
- Godfrey J
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- Goeringer C
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- Goessling C
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- Gonalo R
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- Gonzalez Parra G
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- Goossens L
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- Gorbounov PA
- Gorbounov PA
- Gordon HA
- Gordon HA
- Gorelov I
- Gorelov I
- Gorini B
- Gorini B
- Gorini E
- Gorini E
- Gorisek A
- Gorisek A
- Gornicki E
- Gornicki E
- Goshaw AT
- Goshaw AT
- Gostkin MI
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- Gouighri M
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- Goujdami D
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- Goulette MP
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- Goussiou AG
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- Goy C
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- Gozpinar S
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- Grabas HMX
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- Graber L
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- Grafstroem P
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- Grassi V
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- Gratchev V
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- Gray HM
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- Grebenyuk OG
- Grebenyuk OG
- Greenwood ZD
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- Griffiths J
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- Grillo AA
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- Griso SP
- Grivaz J-F
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- Gross E
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- Guyot C
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- Haas A
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- Haddad N
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- Publication venue
- 'IOP Publishing'
- Publication date
- 01/01/2014
- Field of study
This paper presents a measurement of the cross-section for high transverse momentum W and Z bosons produced in pp collisions and decaying to all-hadronic final states. The data used in the analysis were recorded by the ATLAS detector at the CERN Large Hadron Collider at a centre-of-mass energy of √s = 7 TeV;{\rm Te}{\rm V}andcorrespondtoanintegratedluminosityof4.6\;{\rm f}{{{\rm b}}^{-1}}.ThemeasurementisperformedbyreconstructingtheboostedWorZbosonsinsinglejets.ThereconstructedjetmassisusedtoidentifytheWandZbosons,andajetsubstructuremethodbasedonenergyclusterinformationinthejetcentre−of−massframeisusedtosuppressthelargemulti−jetbackground.Thecross−sectionforeventswithahadronicallydecayingWorZboson,withtransversemomentum{{p}_{{\rm T}}}\gt 320\;{\rm Ge}{\rm V}andpseudorapidity|\eta |\lt 1.9,ismeasuredtobe{{\sigma }_{W+Z}}=8.5\pm 1.7$ pb and is compared to next-to-leading-order calculations. The selected events are further used to study jet grooming techniques
Search for the neutral Higgs bosons of the minimal supersymmetric standard model in pp collisions at root s=7 TeV with the ATLAS detector
- Author
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- Publication venue
- Publication date
- 01/02/2013
- Field of study
A search for neutral Higgs bosons of the Minimal Supersymmetric Standard Model (MSSM) is reported. The analysis is based on a sample of proton-proton collisions at a centre-of-mass energy of 7TeV recorded with the ATLAS detector at the Large Hadron Collider. The data were recorded in 2011 and correspond to an integrated luminosity of 4.7 fb-1 to 4.8 fb-1. Higgs boson decays into oppositely-charged muon or τ lepton pairs are considered for final states requiring either the presence or absence of b-jets. No statistically significant excess over the expected background is observed and exclusion limits at the 95% confidence level are derived. The exclusion limits are for the production cross-section of a generic neutral Higgs boson, φ, as a function of the Higgs boson mass and for h/A/H production in the MSSM as a function of the parameters mA and tan β in the mhmax scenario for mA in the range of 90GeV to 500 GeV. Copyright CERN
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