337 research outputs found
Measurement of the Bottom-Strange Meson Mixing Phase in the Full CDF Data Set
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- Tomura
- Tonelli
- Tooze SA
- Torre
- Torretta
- Totaro
- Tournier C
- Tower J
- Towns R
- Trajkovic V
- Travassos LH
- Trovato
- Tsai TF
- Tschan MP
- Tsubata T
- Tsung A
- Turk B
- Turner LS
- Tyagi SC
- Tönges L
- U.
- U.K.
- Uchiyama Y
- Ueno T
- Ukegawa
- Umekawa M
- Umemiya-Shira
- Uozumi
- V.
- V.
- V.
- V.
- V.
- V.
- V.
- V.
- V.
- V.
- V.E.
- Varganov
- Velev
- Vellidis
- Vidal
- Vila
- Vilar
- Vizán
- Vogel
- Volpi
- Vázquez
- W.
- W.
- W.
- W.
- W.-M.
- W.C.
- W.H.
- W.K.
- Wagner
- Wagner
- Wakisaka
- Wallny
- Wang
- Warburton
- Waters
- Wester
- Whiteson
- Wick
- Wicklund
- Wicklund
- Wilbur
- Williams
- Wilson
- Wilson
- Winer
- Wittich
- Wolbers
- Wolfe
- Wright
- Wu
- Wu
- X.
- Y.
- Y.
- Y.
- Y.
- Y.
- Y.
- Y.
- Y.
- Y.C.
- Y.C.
- Y.D.
- Y.J.
- Y.K.
- Y.S.
- Yamamoto
- Yamato
- Yang
- Yang
- Yang
- Yao
- Yeh
- Yi
- Yoh
- Yorita
- Yoshida
- Yu
- Yu
- Yu
- Yun
- Z.
- Zanetti
- Zeng
- Zhou
- Zucchelli
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2012
- Field of study
We report a measurement of the bottom-strange meson mixing phase \beta_s
using the time evolution of B0_s -> J/\psi (->\mu+\mu-) \phi (-> K+ K-) decays
in which the quark-flavor content of the bottom-strange meson is identified at
production. This measurement uses the full data set of proton-antiproton
collisions at sqrt(s)= 1.96 TeV collected by the Collider Detector experiment
at the Fermilab Tevatron, corresponding to 9.6 fb-1 of integrated luminosity.
We report confidence regions in the two-dimensional space of \beta_s and the
B0_s decay-width difference \Delta\Gamma_s, and measure \beta_s in [-\pi/2,
-1.51] U [-0.06, 0.30] U [1.26, \pi/2] at the 68% confidence level, in
agreement with the standard model expectation. Assuming the standard model
value of \beta_s, we also determine \Delta\Gamma_s = 0.068 +- 0.026 (stat) +-
0.009 (syst) ps-1 and the mean B0_s lifetime, \tau_s = 1.528 +- 0.019 (stat) +-
0.009 (syst) ps, which are consistent and competitive with determinations by
other experiments.Comment: 8 pages, 2 figures, Phys. Rev. Lett 109, 171802 (2012
A Study of B0 -> J/psi K(*)0 pi+ pi- Decays with the Collider Detector at Fermilab
- Author
- Affolder T
- Akimoto H
- Akopian A
- Albrow MG
- Amaral P
- Amidei D
- Anikeev K
- Anthony PL
- Antos J
- Apollinari G
- Arisawa T
- Artikov A
- Asakawa T
- Ashmanskas W
- Aston D
- Azfar F
- Azzi-Bacchetta P
- Bacchetta N
- Bachacou H
- Bailey S
- Baird K
- Band HR
- Barbaro-Galtieri A
- Barnes VE
- Barnett BA
- Baroiant S
- Barone M
- Bauer G
- Bedeschi F
- Belforte S
- Bell WH
- Bellettini G
- Bellinger J
- Benjamin D
- Bensinger J
- Beretvas A
- Berge JP
- Berryhill J
- Bhatti A
- Bianchi F
- Binkley M
- Bisello D
- Bishai M
- Blair RE
- Blocker C
- Bloom E
- Bloom K
- Blumenfeld B
- Blusk SR
- Bocci A
- Bodek A
- Bokhari W
- Bolla G
- Bona M
- Bonushkin Y
- Bortoletto D
- Boudreau J
- Boyarski AM
- Brandl A
- Bromberg C
- Brown CM
- Brozovic M
- Brubaker E
- Bruner N
- Buckley-Geer E
- Budagov J
- Budd HS
- Bugg W
- Bulos F
- Burchat PR
- Burkett K
- Busetto G
- Byon-Wagner A
- Byrum KL
- Cabrera S
- Calafiura P
- Calderini G
- Campbell M
- Carithers W
- Carlsmith D
- Carlson J
- Caskey W
- Castro A
- Cauz D
- Cerri A
- Chan AW
- Chang PS
- Chang PT
- Chapman J
- Charles E
- Chen C
- Chen YC
- Cheng CH
- Cheng MT
- Chertok M
- Chiarelli G
- Chirikov-Zorin I
- Chlachidze G
- Chlebana F
- Christofek L
- Chu ML
- Chung YS
- Ciobanu CI
- Clark AG
- Claus R
- Cohn H
- Colijn AP
- Connolly A
- Convery MR
- Conway J
- Cordelli M
- Coupal DP
- Coward DH
- Cranshaw J
- Cropp R
- Culbertson R
- D'Auria S
- D'Onofrio M
- da Costa JG
- Dagenhart D
- Dasu S
- de Barbaro P
- De Silva A
- de Troconiz JF
- DeJongh F
- Dell'Agnello S
- Dell'Orso M
- Demortier L
- Deninno M
- Derwent PF
- Devlin T
- Di Girolamo B
- Di Lodovico F
- Dittmann JR
- Dominguez A
- Donati S
- Done J
- Dorfan J
- Dorigo T
- Doser M
- Dunwoodie W
- Eddy N
- Eichenbaum AM
- Einsweiler K
- Elias JE
- Engels E
- Erbacher R
- Errede D
- Errede S
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- Ferretti C
- Field RC
- Field RD
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- Flaugher B
- Foster GW
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- Freeman J
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- Fukui Y
- Furic I
- Galeotti S
- Gallas A
- Gallinaro M
- Gamba D
- Gao T
- Garcia-Sciveres M
- Garfinkel AF
- Gatti P
- Gay C
- Gerdes DW
- Giannetti P
- Giromini P
- Glagolev V
- Glanzman T
- Glenzinski D
- Godfrey L
- Gold M
- Goldstein J
- Gorelov I
- Goshaw AT
- Gotra Y
- Goulianos K
- Gowdy SJ
- Green C
- Grim G
- Gris P
- Groer L
- Grosso P
- Grosso-Pilcher C
- Guenther M
- Guillian G
- Haas RM
- Haber C
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- Hao W
- Happacher F
- Hara K
- Hardman AD
- Harris RM
- Hartmann F
- Hatakeyama K
- Hauser J
- Heinrich J
- Heiss A
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- Hill C
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- Hoffman KD
- Holck C
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- Hu H
- Huffer ME
- Huffman BT
- Hughes R
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- Ikeda H
- Incandela J
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- Introzzi G
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- Izen JM
- James E
- Jessop CP
- Johnson JR
- Jones M
- Joshi U
- Kambara H
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- Kato Y
- Keaffaber TA
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- Kilminster B
- Kim BJ
- Kim DH
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- Kirkby D
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- Kitayama I
- Klimenko S
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- Kondo K
- Konigsberg J
- Kordich TMB
- Korn A
- Korytov A
- Kovacs E
- Kowalewski R
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- Kruse M
- Kuhlmann SE
- Kurino K
- Kuwabara T
- Laasanen AT
- Lai N
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- Lancaster J
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- Langenegger U
- Lath A
- Latino G
- LeCompte T
- Lee AM
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- Leith DWGS
- Leone S
- Lewis JD
- Lindgren M
- Liss TM
- Litvintsev DO
- Liu JB
- Liu R
- Liu YC
- Lobban O
- Lockyer N
- Loken J
- Loreti M
- Lou XC
- Lucchesi D
- Luitz S
- Lukens P
- Lusin S
- Luth V
- Lynch HL
- Lyons L
- Lys J
- Madrak R
- Maeshima K
- Maksimovic P
- Malferrari L
- Mangano M
- Mariotti M
- Marsiske H
- Martignon G
- Martin A
- Matthews JAJ
- Mayer J
- Mazzanti P
- McFarland KS
- McIntyre P
- McKigney E
- Menguzzato M
- Menke S
- Menzione A
- Merkel P
- Mesropian C
- Messner R
- Meyer A
- Meyer TI
- Miao T
- Miller JS
- Miller R
- Minato H
- Miscetti S
- Mishina M
- Mitselmakher G
- Moffeit KC
- Moggi N
- Moore E
- Moore R
- Morita Y
- Moulik T
- Mount R
- Mukherjee A
- Mulhearn M
- Muller DR
- Muller T
- Munar A
- Murat P
- Murgia S
- Nachtman J
- Nagaslaev V
- Nahn S
- Nakada H
- Nakano I
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- Newman-Holmes C
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- Nielsen J
- Niu H
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- Nomerotski A
- O'Grady CP
- Oh SH
- Oh YD
- Ohmoto T
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- Oishi R
- Okusawa T
- Olsen J
- Orejudos W
- Pagliarone C
- Palmonari F
- Pan Y
- Panvini RS
- Paoletti R
- Papadimitriou V
- Partos D
- Patrick J
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- Paus C
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- Phillips TJ
- Piacentino G
- Pitts KT
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- Proudfoot J
- Ptohos F
- Pukhov O
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- Rakitine A
- Ratcliff BN
- Ratnikov F
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- Reichold A
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- Rimondi F
- Ristori L
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- Roat C
- Robertson SH
- Robertson WJ
- Robinson A
- Rochester LS
- Rodrigo T
- Rolli S
- Roney JM
- Roodman A
- Rosenson L
- Roser R
- Rossin R
- Rott C
- Roy A
- Ruiz A
- Safonov A
- Sakumoto WK
- Saltzberg D
- Sanchez C
- Sansoni A
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- Savard P
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- Schindler RH
- Schlabach P
- Schmidt EE
- Schmidt MP
- Schmitt M
- Schwiening J
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- Scott A
- Scott IJ
- Scribano A
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- Semenov A
- Semeria F
- Serbo VV
- Shah T
- Shapiro MD
- Shepard PF
- Shibayama T
- Shimojima M
- Shochet M
- Sidoti A
- Siegrist J
- Sill A
- Sinervo P
- Singh P
- Slaughter AJ
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- Tanaka HA
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- Tannenbaum B
- Tecchio M
- Teng PK
- Terashi K
- Tesarek R
- Tether S
- Thompson AS
- Thurman-Keup R
- Tipton P
- Tkaczyk S
- Toback D
- Tollefson K
- Tollestrup A
- Tonelli D
- Toyoda H
- Trischuk W
- Tseng J
- Turcotte M
- Turini N
- Ukegawa F
- Va'vra J
- Vaiciulis T
- Valls J
- van den Brink S
- Vejcik S
- Velev G
- Veramendi G
- Vidal R
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- Vilar R
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- von der Mey M
- von Wimmerspeig-Toeller JH
- Vuagnin G
- Vucinic D
- Wagner RG
- Wagner RL
- Wagner SR
- Wallace NB
- Wan Z
- Wang C
- Wang MJ
- Ward B
- Waschke S
- Watanabe T
- Waters D
- Watts T
- Webb R
- Weidemann AW
- Weinstein AJR
- Wenzel H
- Wester WC
- Wicklund AB
- Wicklund E
- Wilkes T
- Williams HH
- Wilson P
- Winer BL
- Winn D
- Wisniewski WJ
- Wolbers S
- Wolbers S
- Wolinski D
- Wolinski D
- Wolinski J
- Wolinski J
- Wolinski S
- Wolinski S
- Worm S
- Worm S
- Wright DH
- Wu SL
- Wu X
- Wu X
- Wu X
- Wuerthwein F
- Wyss J
- Wyss J
- Wyss J
- Yang UK
- Yao W
- Yao W
- Yao W
- Yeh GP
- Yeh GP
- Yeh GP
- Yeh P
- Yeh P
- Yeh P
- Yi K
- Yoh J
- Yoh J
- Yoh J
- Yosef C
- Yosef C
- Yosef C
- Yoshida T
- Yoshida T
- Yoshida T
- Young CC
- Yu I
- Yu I
- Yu I
- Yu S
- Yu S
- Yu S
- Yu S
- Yu Z
- Yu Z
- Yu Z
- Yu Z
- Yu Z
- Yun JC
- Zanetti A
- Zanetti A
- Zanetti A
- Zanetti A
- Zanin D
- Zetti F
- Zetti F
- Zetti F
- Zetti F
- Zetti F
- Zetti Fi A
- Zobernig H
- Zucchelli S
- Zucchelli S Yu I
- Zucchelli Scchelli Sam I
- Zucchelli Sm S
- Zucchelli Snetti A
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 09/08/2001
- Field of study
We report a study of the decays B0 -> J/psi K(*)0 pi+ pi-, which involve the
creation of a u u-bar or d d-bar quark pair in addition to a b-bar -> c-bar(c
s-bar) decay. The data sample consists of 110 1/pb of p p-bar collisions at
sqrt{s} = 1.8 TeV collected by the CDF detector at the Fermilab Tevatron
collider during 1992-1995. We measure the branching ratios to be BR(B0 -> J/psi
K*0 pi+ pi-) = (8.0 +- 2.2 +- 1.5) * 10^{-4} and BR(B0 -> J/psi K0 pi+ pi-) =
(1.1 +- 0.4 +- 0.2) * 10^{-3}. Contributions to these decays are seen from
psi(2S) K(*)0, J/psi K0 rho0, J/psi K*+ pi-, and J/psi K1(1270)
Precise measurement of the W-boson mass with the CDF II detector
- Author
- Aaltonen T.
- Abbaneo D
- Adzic P
- Aguilar-Benitez M
- Ahmad M
- Ahmed I
- Albajar C
- Allfrey P
- Almeida N
- Alvarez Gonzalez B.
- Amerio S.
- Amidei D.
- Anastassov A.
- Andreev V
- Andreev Y
- Annovi A.
- Antos J.
- Apollinari G.
- Appel J. A.
- Arce P
- Arisawa T.
- Artikov A.
- Asaadi J.
- Asghar MI
- Ashmanskas W.
- Auerbach B.
- Auffray E
- Aurisano A.
- Auzinger G
- Azarkin M
- Azfar F.
- Azhgirey I
- Badgett W.
- Bae T.
- Baillon P
- Ball AH
- Barbaro-Galtieri A.
- Barnes V. E.
- Barnett B. A.
- Barney D
- Barria P.
- Bartos P.
- Battilana C
- Bauce M.
- Bedeschi F.
- Bedoya CF
- Beecher D.
- Behari S.
- Bell AJ
- Bellettini G.
- Bellinger J.
- Belotelov I
- Benedetti D
- Benjamin D.
- Beretvas A.
- Bernet C
- Bhatti A.
- Bialas W
- Bilinskas MJ
- Binkley M.
- Bisello D.
- Bitioukov S
- Bizjak I.
- Bland K. R.
- Bloch P
- Blumenfeld B.
- Bocci A
- Bocci A.
- Bodek A.
- Bolognesi S
- Bondar N
- Boos E
- Bortoletto D.
- Boudreau J.
- Boveia A.
- Breuker H
- Brigliadori L.
- Bromberg C.
- Brona G
- Brucken E.
- Budagov J.
- Budd H. S.
- Bunin P
- Bunkowski K
- Burelo ED
- Burkett K.
- Busetto G.
- Bussey P.
- Butler PH
- Buzatu A.
- Caballero IG
- Cabrillo IJ
- Calamba A.
- Calancha C.
- Calderon A
- Calvo E
- Camarda S.
- Campanelli M.
- Campbell M.
- Campderros JD
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- Canelli F.
- Cano E
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- Carlsmith D.
- Carosi R.
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- Cavaliere V.
- Cavalli-Sforza M.
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- Cerrito L.
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- Cho K.
- Choi M
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- Chung Y. S.
- Cifuentes JAB
- Ciocci M. A.
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- Compostella G.
- Convery M. E.
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- Corbo M.
- Cordelli M.
- Cortabitarte RV
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- Crescioli F.
- Cuevas J
- Cuevas J.
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- Cure B
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- d'Errico M.
- D'Onofrio M.
- da Costa J. Guimaraes
- Dagenhart D.
- Datta M.
- David A
- de Barbaro P.
- De La Cruz B
- De Roeck A
- de Troconiz JF
- Dell'Orso M
- Demortier L.
- Deninno M.
- Devoto F.
- Di Canto A.
- Di Ruzza B.
- Dittmann J. R.
- Djordjevic M
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- Dremin I
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- Garfinkel A. F.
- Garosi P.
- Garrido RGR
- Gavrilov V
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- Georgiou G
- Gerberich H.
- Gerchtein E.
- Gerwig H
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- Giakoumopoulou V.
- Giannetti P.
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- Gigi D
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- Ginsburg C. M.
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- Hoffmann HF
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- Huston J.
- Ibarguen HAS
- Iglesias LL
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- Jeon E. J.
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- Yao W. -M.
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- Zhou C.
- Zucchelli S..
- Zucchelli S..ng S
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2012
- Field of study
We have measured the W-boson mass MW using data corresponding to 2.2/fb of
integrated luminosity collected in proton-antiproton collisions at 1.96 TeV
with the CDF II detector at the Fermilab Tevatron collider. Samples consisting
of 470126 W->enu candidates and 624708 W->munu candidates yield the measurement
MW = 80387 +- 12 (stat) +- 15 (syst) = 80387 +- 19 MeV. This is the most
precise measurement of the W-boson mass to date and significantly exceeds the
precision of all previous measurements combined
Performance of CMS muon reconstruction in pp collision events at sqrt(s) = 7 TeV
- Author
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- Abbiendi G
- Abbrescia M
- Abdullin S
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- Yildirim E
- Yilmaz Y
- Yohay R
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- Yumiceva F
- Yun JC
- Zabel J
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- Zakaria M
- Zalewski P
- Zanetti M
- Zang J
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- Zatserklyaniy A
- Zeinali M
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- Zeyrek M
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- Zoeller MH
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- 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
Compressed representation of a partially defined integer function over multiple arguments
- Author
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- Abbiendi G
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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
Performance of CMS muon reconstruction in pp collision events at sqrt(s) = 7 TeV
- Author
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- Kreczko L
- Kreis B
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- Newman HB
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- Perelygin V
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- Perez JAC
- Perfilov M
- Perieanu A
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- Pesaresi M
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- Polatoz A
- Polese G
- Polic D
- Poll A
- Pollack B
- Pompili A
- Pooth O
- Popov V
- Pordes R
- Potenza A
- Potenza R
- Pozdnyakov A
- Pozzobon N
- Prado Da Silva WL
- Primavera F
- Prokofyev O
- Prosper H
- Ptochos F
- Puerta Pelayo J
- Pugliese G
- Puigh D
- Puljak I
- Qazi S
- Qian SJ
- Quan X
- Quast G
- Quertenmont L
- Rabbertz K
- Racz A
- Radburn-Smith BC
- Radi A
- Ragazzi S
- Rahatlou S
- Rahbaran B
- Rahmat R
- Raics P
- Raidal M
- Rakness G
- Ralph D
- Rander J
- Ranieri R
- Ranjan K
- Rappoccio S
- Raspereza A
- Ratnikov F
- Ratnikova N
- Ratti SP
- Raupach F
- Raval A
- Raymond DM
- Razis PA
- Rebane L
- Rebassoo F
- Redaelli N
- Redjimi R
- Redondo I
- Reece W
- Reid ID
- Reithler H
- Rekovic V
- Remington R
- Renker D
- Rennefeld J
- Renz M
- Reucroft S
- Reyes-Santos MA
- Ribeiro PQ
- Ribnik J
- Riccardi C
- Richards A
- Richman J
- Rikova MI
- Rinkevicius A
- Rios AAO
- Rizzi A
- Ro SR
- Roberts J
- Robles J
- Robmann P
- Rodenburg M
- Rodozov M
- Rodrigo T
- Rodriguez JL
- Rodriguez-Marrero AY
- Roe J
- Roecker S
- Rogan C
- Rogerson S
- Roh Y
- Rohe T
- Rohlf J
- Rohringer C
- Rohringer H
- Roland B
- Roland C
- Roland G
- Rolandi G
- Romano F
- Romanowska-Rybinska K
- Romeo F
- Romero A
- Romero L
- Rommerskirchen T
- Rompotis N
- Ronchese P
- Ronga FJ
- Rose A
- Rose K
- Rosin M
- Rosowsky A
- Ross I
- Rossato K
- Rossi AM
- Rossin R
- Rossini M
- Rougny R
- Rovelli C
- Rovelli T
- Rovere M
- Ruchti R
- Rudolph M
- Ruiz-Jimeno A
- Rumerio P
- Rusack R
- Rusakov SV
- Ruspa M
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- Sala S
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- Santocchia A
- Santoro A
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- Sarycheva L
- Sasseville M
- Sauerland P
- Savin A
- Savrin V
- Sawley M-C
- Scarborough T
- Schaefer C
- Schael S
- Schettler H
- Scheurer A
- Schieferdecker P
- Schilling F-P
- Schlein P
- Schleper P
- Schlieckau E
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- Schmitt M
- Schmitt M
- Schmitz SA
- Schnetzer S
- Schoefbeck R
- Schoerner-Sadenius T
- Schott G
- Schroeder M
- Schul N
- Schum T
- Schwarz T
- Schwick C
- Scodellaro L
- Scurlock B
- Searle M
- Seez C
- Segala M
- Segoni I
- Seitz C
- Seixas J
- Sekmen S
- Sellers P
- Selvaggi G
- Selvaggi M
- Semenov S
- Sen N
- Sen S
- Sengupta S
- Senkin S
- Seo E
- Seo H
- Serban AT
- Serin M
- Sever R
- Sexton-Kennedy E
- Sfiligoi I
- Sguazzoni G
- Shah MA
- Sharma A
- Sharma A
- Sharma S
- Sharma V
- Sharma V
- Sharp P
- Sheldon P
- Shepherd-Themistocleous CH
- Shi X
- Shipkowski SP
- Shipsey I
- Shiu JG
- Shivpuri RK
- Shmatov S
- Shoaib M
- Shrestha S
- Shreyber I
- Shukla P
- Shumeiko N
- Sibille J
- Siegrist P
- Sierra RV
- Sigamani M
- Sikler F
- Silkworth C
- Sill A
- Sillou D
- Silva Do Amaral SM
- Silva P
- Silvers D
- Silverwood H
- Silvestre C
- Silvestris L
- Sim KS
- Simon M
- Simon S
- Simonetto F
- Simonis HJ
- Singh AP
- Singh G
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- Singh SP
- Singovsky A
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- Sirois Y
- Siroli G
- Sirunyan AM
- Skhirtladze N
- Skuja A
- Slaunwhite J
- Smirnov I
- Smith J
- Smith JG
- Smith K
- Smith VJ
- Smith WH
- Smolin D
- Snigirev A
- Snoek H
- Snook B
- Snow GR
- Snowball M
- Soares Jorge L
- Soares MS
- Sobol A
- Sobron Sanudo M
- Soffi L
- Sogut K
- Sola V
- Solano A
- Somalwar S
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- Spiropulu M
- Sprenger D
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- Stadie H
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- Stephans GSF
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- Stieger B
- Stiliaris E
- Stober FM
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- Stoynev S
- Strauss J
- Stringer R
- Strobbe N
- Strom D
- Stuart D
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- Suarez I
- Suarez RG
- Sudano E
- Sudhakar K
- Sulak L
- Sulimov V
- Sultanov G
- Summers D
- Sumorok K
- Sumowidagdo S
- Sun W
- Sung K
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- Svintradze I
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- Swartz M
- Symonds P
- Szillasi Z
- Szleper M
- Sznajder A
- Tadel M
- Takahashi M
- Tali B
- Tambe N
- Tan P
- Tao J
- Tapper A
- Taroni S
- Tatarinov A
- Taurok A
- Tauscher L
- Taylor L
- Tcholakov V
- Teischinger F
- Temple J
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- Teo WD
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- Teyssier D
- Thea A
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- Thomsen J
- Thyssen F
- Tiko A
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- Tiras E
- Titov M
- Tkaczyk S
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- Toback D
- Tomalin IR
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- Tonelli G
- Tonjes MB
- Tonwar SC
- Topakli H
- Topaksu AK
- Torassa E
- Toropin A
- Torre P
- Tosi M
- Tosi S
- Tourneur S
- Tourtchanovitch L
- Traczyk P
- Tran NV
- Travaglini R
- Trayanov R
- Treille D
- Triantis FA
- Tricomi A
- Tripathi M
- Trocino D
- Trocsanyi ZL
- Troendle D
- Troitsky S
- Tropiano A
- Troshin S
- Tsang KV
- Tschudi Y
- Tsirou A
- Tu Y
- Tucker J
- Tully C
- Tumasyan A
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- Tuominen E
- Tuominiemi J
- Tuovinen E
- Tupputi S
- Turkewitz J
- Turner M
- Tuuva T
- Tuve C
- Twedt E
- Tytgat M
- Tyurin N
- Tzeng YM
- Ujvari B
- Ulmer KA
- Ungaro D
- Uplegger L
- Urscheler C
- Uvarov L
- Uzun D
- Uzunian A
- Vaandering EW
- Valdata M
- Valls N
- Valuev V
- Van Doninck W
- Van Haevermaet H
- Van Hove P
- Van Mechelen P
- Van Mulders P
- Van Onsem GP
- Van Remortel N
- Van Spilbeeck A
- Vander Velde C
- Vanelderen L
- Vanini S
- Vanlaer P
- Varela J
- Varelas N
- Vargas JER
- Vartak A
- Vasil'ev S
- Vaughan J
- Vavilov S
- Vazquez Valencia F
- Veelken C
- Veeraraghavan V
- Velasco M
- Velicanu D
- Velkovska J
- Ventura S
- Venturi A
- Verdier P
- Verdini PG
- Veres GI
- Vergili LN
- Vergili M
- Verwilligen P
- Verzetti M
- Veszpremi V
- Vesztergombi G
- Veverka J
- Vichoudis P
- Vidal R
- Vila I
- Vilar Cortabitarte R
- Villasenor-Cendejas LM
- Villella I
- Vinogradov A
- Virdee T
- Viret S
- Vischia P
- Vishnevskiy D
- Vitulo P
- Viviani C
- Vizan Garcia JM
- Vlasov E
- Vlimant JR
- Vodopiyanov I
- Vogel H
- Volkov A
- Volobouev I
- Volpe R
- Vorobiev I
- Vorobyev A
- Vorobyev A
- Voutilainen M
- Vuosalo C
- Vutova M
- Wagner P
- Wagner SR
- Wagner-Kuhr J
- Wakefield S
- Wallny R
- Walsh R
- Walsh S
- Waltenberger W
- Walzel G
- Wan Z
- Wang D
- Wang J
- Wang J
- Wang M
- Wang S
- Wang X
- Wang Z
- Wardle N
- Wardrope D
- Wasserbaech S
- Wayne M
- Weber H
- Weber HA
- Weber M
- Weber M
- Wehrli L
- Weiler T
- Weinberg M
- Wendland L
- Weng J
- Weng Y
- Wenger EA
- Werner JS
- West C
- Wetzel J
- Whitbeck A
- Whitmore J
- Whyntie T
- Wickens J
- Wickramage N
- Widl E
- Wigmans R
- Wilken R
- Wilkinson R
- Williams G
- Williams T
- Willmott C
- Wimpenny S
- Winn D
- Winstrom L
- Wissing C
- Wittich P
- Wittmer B
- Woehri HK
- Wolf M
- Wolf R
- Womersley WJ
- Won S
- Wood D
- Wood J
- Wood JS
- Worm SD
- Wright D
- Wrochna G
- Wu W
- Wuerthwein F
- Wulz C-E
- Wyslouch B
- Xiao H
- Xie S
- Xu M
- Yagil A
- Yalvac M
- Yang F
- Yang M
- Yang Y
- Yang ZC
- Yazgan E
- 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
- 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
Azimuthal anisotropy of charged particles at high transverse momenta in PbPb collisions at sqrt(s[NN]) = 2.76 TeV
- Author
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- Wissing C
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- Wood JS
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- Wulz C-E
- Wyslouch B
- Xiao H
- Xie S
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- Yalvac M
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- Yang M
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- Yang ZC
- 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
- Ziegler J
- Zielinski M
- Zito G
- Zotto P
- 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
- Abbaneo D
- Abbiendi G
- Abbrescia M
- Abdullin S
- Abdulsalam A
- Acosta D
- Acosta JG
- Adair A
- Adam N
- Adam W
- Adams JR
- Adams MR
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- Adiguzel A
- Adler V
- Adzic P
- 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
- Aldaya Martin M
- Alexander J
- Aliev T
- Alimena J
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- Alverson G
- Alves GA
- Amapane N
- Amsler C
- Anagnostou G
- Anastassov A
- Anderson J
- Anderson M
- Andrea J
- Andreev V
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- Andreev Y
- Andrews W
- Anghel IM
- Antonelli L
- Antunovic Z
- Apanasevich L
- Appelt E
- Apresyan A
- Arce P
- Arcidiacono R
- Arenton MW
- Arfaei H
- Argiro S
- Arneodo M
- Arora S
- Asawatangtrakuldee C
- Asghar MI
- Askew A
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- Ata M
- Attikis A
- Auffray E
- Autermann C
- Auzinger G
- Avdeeva E
- Avery P
- Avetisyan A
- Avila C
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- Azhgirey I
- Aziz T
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- Azzolini V
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- Baarmand MM
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- Baden A
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- Baffioni S
- Bagliesi G
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- Bainbridge R
- Bakhshiansohi H
- Bakirci MN
- Balazs M
- Ball AH
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- Barbagli G
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- Bauerdick LAT
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- Beernaert K
- Behr J
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- Behrens U
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- Belotelov I
- Belyaev A
- Belyaev A
- Benaglia A
- Bencze G
- Bendavid J
- Benedetti D
- Benelli G
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- Beni N
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- Yilmaz Y
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- 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
Measurement of jet fragmentation into charged particles in pp and PbPb collisions at sqrt(s[NN]) = 2.76 TeV
- Author
- Abbaneo D
- Abbiendi G
- Abbrescia M
- Abdullin S
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- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2012
- Field of study
Jet fragmentation in pp and PbPb collisions at a centre-of-mass energy of
2.76 TeV per nucleon pair was studied using data collected with the CMS
detector at the LHC. Fragmentation functions are constructed using
charged-particle tracks with transverse momenta pt > 4 GeV for dijet events
with a leading jet of pt > 100 GeV. The fragmentation functions in PbPb events
are compared to those in pp data as a function of collision centrality, as well
as dijet-pt imbalance. Special emphasis is placed on the most central PbPb
events including dijets with unbalanced momentum, indicative of energy loss of
the hard scattered parent partons. The fragmentation patterns for both the
leading and subleading jets in PbPb collisions agree with those seen in pp data
at 2.76 TeV. The results provide evidence that, despite the large parton energy
loss observed in PbPb collisions, the partition of the remaining momentum
within the jet cone into high-pt particles is not strongly modified in
comparison to that observed for jets in vacuum.Comment: Submitted to the Journal of High Energy Physic
The impact of surgical delay on resectability of colorectal cancer: An international prospective cohort study
- Author
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- Publication venue
- 'Royal College of Obstetricians & Gynaecologists (RCOG)'
- Publication date
- 01/06/2022
- Field of study
AIM: The SARS-CoV-2 pandemic has provided a unique opportunity to explore the impact of surgical delays on cancer resectability. This study aimed to compare resectability for colorectal cancer patients undergoing delayed versus non-delayed surgery. METHODS: This was an international prospective cohort study of consecutive colorectal cancer patients with a decision for curative surgery (January-April 2020). Surgical delay was defined as an operation taking place more than 4 weeks after treatment decision, in a patient who did not receive neoadjuvant therapy. A subgroup analysis explored the effects of delay in elective patients only. The impact of longer delays was explored in a sensitivity analysis. The primary outcome was complete resection, defined as curative resection with an R0 margin. RESULTS: Overall, 5453 patients from 304 hospitals in 47 countries were included, of whom 6.6% (358/5453) did not receive their planned operation. Of the 4304 operated patients without neoadjuvant therapy, 40.5% (1744/4304) were delayed beyond 4 weeks. Delayed patients were more likely to be older, men, more comorbid, have higher body mass index and have rectal cancer and early stage disease. Delayed patients had higher unadjusted rates of complete resection (93.7% vs. 91.9%, P = 0.032) and lower rates of emergency surgery (4.5% vs. 22.5%, P < 0.001). After adjustment, delay was not associated with a lower rate of complete resection (OR 1.18, 95% CI 0.90-1.55, P = 0.224), which was consistent in elective patients only (OR 0.94, 95% CI 0.69-1.27, P = 0.672). Longer delays were not associated with poorer outcomes. CONCLUSION: One in 15 colorectal cancer patients did not receive their planned operation during the first wave of COVID-19. Surgical delay did not appear to compromise resectability, raising the hypothesis that any reduction in long-term survival attributable to delays is likely to be due to micro-metastatic disease
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