745 research outputs found
Long-term subjective outcomes of barbed reposition pharyngoplasty for obstructive sleep apnea syndrome treatment
- Author
- Publication venue
- 'MDPI AG'
- Publication date
- 01/01/2020
- Field of study
Background: The purpose of this study was to evaluate long-term subjective outcomes of barbed reposition pharyngoplasty for obstructive sleep apnea syndrome (OSAS) treatment using a specific questionnaire, the Palate Postoperative Problem Score (PPOPS). Methods: 140 patients who underwent barbed reposition pharyngoplasty (BRP) surgery in the Morgagni Pierantoni Hospital of Forlì, Italy were enrolled in the study. Postoperative outcomes were evaluated in a short- and long-term follow-up using the PPOPS questionnaire. The average period of follow-up was 26 months. All patients received the PPOPS questionnaire by telephone in a period between April and August 2019. Results: 51% of patients complained of swallowing problems after surgery. In 91% of cases, the problem cleared up spontaneously. At the time of the interview, only 9% of patients had a residual swallowing difficult. At the time of PPOPS evaluation, rhinolalia was observed in 8% of patients, whereas nose regurgitation was present in 2% of patients. In 20% of patients, the foreign body sensation was present during follow-up. The value of apnea-hypopnea index (AHI) reduced from the preoperative value of 31.5 to the postoperative value of 11.4. Conclusions: BRP surgery proved to be an effective technique, appreciated by the majority of patients. Use of the PPOPS questionnaire has demonstrated that the BRP technique seems to ensure efficacy and lower morbidity, with few complications after surgery
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
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
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- Zhemchugov A
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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
Jet energy measurement with the ATLAS detector in proton-proton collisions at root s=7 TeV
- Author
- Aad G
- Abbott B
- Abdallah J
- Abdelalim AA
- Abdesselam A
- Abdinov O
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- Yoosootiniya R
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- Zarzhitsky P
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- Zerwas D
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- Zhemchugov A
- Zheng S
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- Zieminska D
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- Zitoun R
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- Zwalinski L
- 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 direct pair production of the top squark in all-hadronic final states in proton-proton collisions at s√=8 TeV with the ATLAS detector
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- Zhemchugov A
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- Zurzolo G
- Zutshi V
- Zwalinski L
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2014
- Field of study
The results of a search for direct pair production of the scalar partner to the top quark using an integrated luminosity of 20.1fb−1 of proton–proton collision data at √s = 8 TeV recorded with the ATLAS detector at the LHC are reported. The top squark is assumed to decay via t˜→tχ˜01 or t˜→ bχ˜±1 →bW(∗)χ˜01 , where χ˜01 (χ˜±1 ) denotes the lightest neutralino (chargino) in supersymmetric models. The search targets a fully-hadronic final state in events with four or more jets and large missing transverse momentum. No significant excess over the Standard Model background prediction is observed, and exclusion limits are reported in terms of the top squark and neutralino masses and as a function of the branching fraction of t˜ → tχ˜01 . For a branching fraction of 100%, top squark masses in the range 270–645 GeV are excluded for χ˜01 masses below 30 GeV. For a branching fraction of 50% to either t˜ → tχ˜01 or t˜ → bχ˜±1 , and assuming the χ˜±1 mass to be twice the χ˜01 mass, top squark masses in the range 250–550 GeV are excluded for χ˜01 masses below 60 GeV
Search for pair-produced long-lived neutral particles decaying to jets in the ATLAS hadronic calorimeter in ppcollisions at √s=8TeV
- Author
- Aad G
- Abbott B
- Abdallah J
- Abdinov O
- Aben R
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- Zenis T
- Zerwas D
- Zhang D
- Zhang F
- Zhang H
- Zhang J
- Zhang L
- Zhang X
- Zhang Z
- Zhao Z
- Zhemchugov A
- Zhong J
- Zhou B
- Zhou L
- Zhou N
- Zhu CG
- Zhu H
- Zhu J
- Zhu Y
- Zhuang X
- Zhukov K
- Zibell A
- Zieminska D
- Zimine NI
- Zimmermann C
- Zimmermann R
- Zimmermann S
- Zimmermann S
- Zinonos Z
- Ziolkowski M
- Zobernig G
- Zoccoli A
- zur Nedden M
- Zurzolo G
- Zutshi V
- Zwalinski L
- Publication venue
- 'Elsevier BV'
- Publication date
- 01/01/2014
- Field of study
The ATLAS detector at the Large Hadron Collider at CERN is used to search for the decay of a scalar boson to a pair of long-lived particles, neutral under the Standard Model gauge group, in 20.3fb−1of data collected in proton–proton collisions at √s=8TeV. This search is sensitive to long-lived particles that decay to Standard Model particles producing jets at the outer edge of the ATLAS electromagnetic calorimeter or inside the hadronic calorimeter. No significant excess of events is observed. Limits are reported on the product of the scalar boson production cross section times branching ratio into long-lived neutral particles as a function of the proper lifetime of the particles. Limits are reported for boson masses from 100 GeVto 900 GeV, and a long-lived neutral particle mass from 10 GeVto 150 GeV
Spread of Epidemic MRSA-ST5-IV Clone Encoding PVL as a Major Cause of Community Onset Staphylococcal Infections in Argentinean Children
- Author
- A Corso
- A Tristan
- Alejandro J. Moyano
- Ana L. Egea
- Ana Vindel
- Analia Garnero
- AS Rossney
- B Goldstein
- B Limbago
- BE Gonzalez
- BP Howden
- C Liu
- C Milheirico
- C Milheirico
- C Sola
- C Sola
- C Sola
- C Sola
- C Sola
- Catalina Culasso
- CL Maree
- Claudia Sola
- D Bhattacharya
- D Harmsen
- DC Oliveira
- E Cercenado
- E Rodriguez-Noriega
- FR Deleo
- H Paganini
- Horacio Lopardo
- Hugo Paganini
- I Niniou
- Ines Kevric
- J Reyes
- José L. Bocco
- JS Gerber
- K Chua
- K Hiramatsu
- K Okuma
- Laurence Van Melderen
- M Wootton
- MA Morrison
- MB Tokumoto
- MC Enright
- MJ Ellington
- MZ David
- MZ David
- N Gardella
- O Dauwalder
- R Blanco
- R Heusser
- RC Orscheln
- RH Deurenberg
- RM Klevens
- RM Klevens
- S Breurec
- S Monecke
- S Monecke
- S Monecke
- SL Kaplan
- SR Benoit
- SW Satola
- TE Zaoutis
- U Nubel
- XX Ma
- Publication venue
- Public Library of Science
- Publication date
- 01/01/2012
- Field of study
BACKGROUND: Community-associated methicillin-resistant Staphylococcus aureus-(CA-MRSA) strains have emerged in Argentina. We investigated the clinical and molecular evolution of community-onset MRSA infections (CO-MRSA) in children of Córdoba, Argentina, 2005-2008. Additionally, data from 2007 were compared with the epidemiology of these infections in other regions of the country. METHODOLOGY/PRINCIPAL FINDINGS: Two datasets were used: i) lab-based prospective surveillance of CA-MRSA isolates from 3 Córdoba pediatric hospitals-(CBAH1-H3) in 2007-2008 (compared to previously published data of 2005) and ii) a sampling of CO-MRSA from a study involving both, healthcare-associated community-onset-(HACO) infections in children with risk-factors for healthcare-associated infections-(HRFs), and CA-MRSA infections in patients without HRFs detected in multiple centers of Argentina in 2007. Molecular typing was performed on the CA-MRSA-(n: 99) isolates from the CBAH1-H3-dataset and on the HACO-MRSA-(n: 51) and CA-MRSA-(n: 213) isolates from other regions. Between 2005-2008, the annual proportion of CA-MRSA/CA-S. aureus in Córdoba hospitals increased from 25% to 49%, P<0.01. Total CA-MRSA infections increased 3.6 fold-(5.1 to 18.6 cases/100,000 annual-visits, P<0.0001), associated with an important increase of invasive CA-MRSA infections-(8.5 fold). In all regions analyzed, a single genotype prevailed in both CA-MRSA (82%) and HACO-MRSA(57%), which showed pulsed-field-gel electrophoresis-(PFGE)-type-"I", sequence-type-5-(ST5), SCCmec-type-IVa, spa-t311, and was positive for PVL. The second clone, pulsotype-N/ST30/CC30/SCCmecIVc/t019/PVL(+), accounted for 11.5% of total CA-MRSA infections. Importantly, the first 4 isolates of Argentina belonging to South American-USA300 clone-(USA300/ST8/CC8/SCCmecIVc/t008/PVL(+)/ACME(-)) were detected. We also demonstrated that a HA-MRSA clone-(pulsotype-C/ST100/CC5) caused 2% and 10% of CA-MRSA and HACO-MRSA infections respectively and was associated with a SCCmec type closely related to SCCmecIV(2B&5). CONCLUSIONS/SIGNIFICANCE: The dissemination of epidemic MRSA clone, ST5-IV-PVL(+) was the main cause of increasing staphylococcal community-onset infections in Argentinean children (2003-2008), conversely to other countries. The predominance of this clone, which has capacity to express the h-VISA phenotype, in healthcare-associated community-onset cases suggests that it has infiltrated into hospital-settings
Performance of the CMS Cathode Strip Chambers with Cosmic Rays
- Author
- Abadjiev K
- Abbaneo D
- Abbiendi G
- Abbrescia M
- Abdullin S
- Abelev B
- Acosta D
- Acosta JG
- Acosta MV
- Actis O
- Adam N
- Adam W
- Adams MR
- Adams T
- Adiguzel A
- Adler V
- Adolphi R
- Adzic P
- Afaq MA
- Agostino L
- Agram JL
- Aguilar-Benitez M
- Ahmad M
- Ahmad WH
- Ahmed I
- Ahmed W
- Ahuja S
- Aisa D
- Aisa S
- Akchurin N
- Akgun B
- Akgun U
- Akimenko S
- Akin IV
- Alagoz E
- Alampi G
- Albajar C
- Albayrak EA
- Alberdi J
- Albergo S
- Albert E
- Albrow M
- Alexander J
- Alidra M
- Aliev T
- Allfrey P
- Almeida N
- Altenhofer G
- Altsybeev I
- Alver B
- Alverson G
- Alves GA
- Amaglobeli N
- Amapane N
- Ambroglini F
- Amsler C
- Anagnostou G
- Ananthan B
- Anastassov A
- Andelin D
- Anderson M
- Andrea J
- Andreev V
- Andreev Y
- Anghel IM
- Anguelov T
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- Anisimov A
- Antillon E
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- Antunes JR
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- Apollinari G
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- Publication date
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- Field of study
The Cathode Strip Chambers (CSCs) constitute the primary muon tracking device
in the CMS endcaps. Their performance has been evaluated using data taken
during a cosmic ray run in fall 2008. Measured noise levels are low, with the
number of noisy channels well below 1%. Coordinate resolution was measured for
all types of chambers, and fall in the range 47 microns to 243 microns. The
efficiencies for local charged track triggers, for hit and for segments
reconstruction were measured, and are above 99%. The timing resolution per
layer is approximately 5 ns
The use of the Airtraq® optical laryngoscope for routine tracheal intubation in high-risk cardio-surgical patients
- Author
- A Friedrich
- A Vlatten
- AI Brain
- AI Brain
- B Holst
- BK Fung
- Britta Fiedler
- CH Maharaj
- CH Maharaj
- CH Maharaj
- CH Maharaj
- CT Buschmann
- DK Rose
- DZ Ferson
- G Dhonneur
- G Landesberg
- G Serocki
- Gereon Schälte
- GL Savoldelli
- GN Peterson
- H Trimmel
- IL López-Negrete
- IL López-Negrete
- J Horak
- J McElwain
- K Nishikawa
- L Liu
- LM Pott
- Mark Coburn
- MC Newland
- N Ueda
- Norbert Zoremba
- O Chalkeidis
- PA Modesti
- R Singh
- RM Corso
- Rolf Rossaint
- S Khalil
- S Kheterpal
- SK Ndoko
- SK Pittman
- Steffen Rex
- SY Thong
- T Gaszyński
- Ulrike Scheid
- Y Hirabayashi
- Y Lu
- Z Kayhan
- Publication venue
- BioMed Central
- Publication date
- 01/01/2011
- Field of study
<p>Abstract</p> <p>Background</p> <p>The Airtraq<sup>® </sup>optical laryngoscope (Prodol Ltd., Vizcaya, Spain) is a novel disposable device facilitating tracheal intubation in routine and difficult airway patients. No data investigating routine tracheal intubation using the Airtaq<sup>® </sup>in patients at a high cardiac risk are available at present. Purpose of this study was to investigate the feasibility and hemodynamic implications of tracheal intubation with the Aitraq<sup>® </sup>optical laryngoscope, in high-risk cardio-surgical patients.</p> <p>Methods</p> <p>123 consecutive ASA III patients undergoing elective coronary artery bypass grafting were routinely intubated with the Airtraq<sup>® </sup>laryngoscope. Induction of anesthesia was standardized according to our institutional protocol. All tracheal intubations were performed by six anesthetists trained in the use of the Airtraq<sup>® </sup>prior.</p> <p>Results</p> <p>Overall success rate was 100% (n = 123). All but five patients trachea could be intubated in the first attempt (95,9%). 5 patients were intubated in a 2nd (n = 4) or 3rd (n = 1) attempt. Mean intubation time was 24.3 s (range 16-128 s). Heart rate, arterial blood pressure and SpO<sub>2 </sub>were not significantly altered. Minor complications were observed in 6 patients (4,8%), i.e. two lesions of the lips and four minor superficial mucosal bleedings. Intubation duration (p = 0.62) and number of attempts (p = 0.26) were independent from BMI and Mallampati score.</p> <p>Conclusion</p> <p>Tracheal intubation with the Airtraq<sup>® </sup>optical laryngoscope was feasible, save and easy to perform in high-risk patients undergoing cardiac surgery. In all patients, a sufficient view on the vocal cords could be obtained, independent from BMI and preoperative Mallampati score.</p> <p>Trial Registration</p> <p>DRKS 00003230</p
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