572 research outputs found
Refined physical map of the human PAX2/HOX11/NFKB2 cancer gene region at 10q24 and relocalization of the HPV6AI1 viral integration site to 14q13.3-q21.1
- Author
- A Neri
- AH Parmiter
- AK Virmani
- B Khoubehi
- B Leube
- BJ Trask
- C Kahl
- C Lo Nigro
- C Morris
- C Nobile
- C Nobile
- Consortium IHGS
- CW Roberts
- D Cappellen
- D Heckel
- DM Stone
- EC Thorland
- EV Prochownik
- F Chen
- F Luft
- G Senger
- GB Silberstein
- GR Dressler
- IC Gray
- IC Gray
- J Jonkers
- J Reifenberger
- J Richter
- J ten Hoeve
- JC Alers
- JJ Scarisbrick
- JM Morante-Redolat
- JR Korenberg
- K Nikali
- K Verhoeven
- K Yoshiura
- KE Kim
- KS Wilson
- LA Koopman
- M Durst
- M Hatano
- M Karin
- MA Kennedy
- MH Einstein
- MR Eccles
- MR Eccles
- N Wentzensen
- NS Fracchiolla
- O Chernova
- OB Chernova
- PD Salvati
- PD Salvati
- PE Crossen
- PM Watt
- R Lundgren
- R Simon
- S Ford
- S Jeon
- S Kalachikov
- S Porteous
- S Reuter
- SL Speaks
- SR Vincent
- T Kahn
- T Saitoh
- T Saitoh
- TN Dear
- TN Dear
- X Sastre-Garau
- X Zhou
- Y Cabeza-Arvelaiz
- Publication venue
- BioMed Central
- Publication date
- 01/01/2003
- Field of study
BACKGROUND: Chromosome band 10q24 is a gene-rich domain and host to a number of cancer, developmental, and neurological genes. Recurring translocations, deletions and mutations involving this chromosome band have been observed in different human cancers and other disease conditions, but the precise identification of breakpoint sites, and detailed characterization of the genetic basis and mechanisms which underlie many of these rearrangements has yet to be resolved. Towards this end it is vital to establish a definitive genetic map of this region, which to date has shown considerable volatility through time in published works of scientific journals, within different builds of the same international genomic database, and across the differently constructed databases. RESULTS: Using a combination of chromosome and interphase fluorescent in situ hybridization (FISH), BAC end-sequencing and genomic database analysis we present a physical map showing that the order and chromosomal orientation of selected genes within 10q24 is CEN-CYP2C9-PAX2-HOX11-NFKB2-TEL. Our analysis has resolved the orientation of an otherwise dynamically evolving assembly of larger contigs upstream of this region, and in so doing verifies the order and orientation of a further 9 cancer-related genes and GOT1. This study further shows that the previously reported human papillomavirus type 6a DNA integration site HPV6AI1 does not map to 10q24, but that it maps at the interface of chromosome bands 14q13.3-q21.1. CONCLUSIONS: This revised map will allow more precise localization of chromosome rearrangements involving chromosome band 10q24, and will serve as a useful baseline to better understand the molecular aetiology of chromosomal instability in this region. In particular, the relocation of HPV6AI1 is important to report because this HPV6a integration site, originally isolated from a tonsillar carcinoma, was shown to be rearranged in other HPV6a-related malignancies, including 2 of 25 genital condylomas, and 2 of 7 head and neck tumors tested. Our finding shifts the focus of this genomic interest from 10q24 to the chromosome 14 site
Evidence for the h_b(1P) meson in the decay Upsilon(3S) --> pi0 h_b(1P)
- Author
- Adametz A.
- Adye T.
- Ahmed H.
- Alam M. S.
- Albert J.
- Allen M. T.
- Alwyn K. E.
- Andreassen R.
- Angelini C.
- Anh TV
- Anulli F.
- Arnaud N.
- Asgeirsson D. J.
- Aston D.
- Atmacan H.
- Ayad R.
- Bailey D.
- Baldini-Ferroli R.
- Band H. R.
- Banerjee Sw.
- Bard D. J.
- Barlow R. J.
- Bartoldus R.
- Batignani G.
- Behera P. K.
- Bellis M.
- Ben-Haim E.
- Benitez J. F.
- Bernard D.
- Bernlochner F. U.
- Bettarini S.
- Bettoni D.
- Bevan A. J.
- Bhuyan B.
- Bianchi F.
- Biasini M.
- Biassoni P.
- Bingham I.
- Blinov V. E.
- Bloom P. C.
- Blount N. L.
- Bomben M.
- Bondioli M.
- Bonneaud G. R.
- Bozzi C.
- Brau J.
- Briand H.
- Brown D. N.
- Brown D. N.
- Buenger C.
- Burchat P. R.
- Buzykaev A. R.
- Cakir IT
- Calabrese R.
- Calcaterra A.
- Calderini G.
- Campagnari C.
- Carpinelli M.
- Cartaro C.
- Casarosa G.
- Castanheira MTD
- Castelli G.
- Cavoto G.
- Cenci R.
- Cervelli A.
- Chauveau J.
- Chavez C. A.
- Chen C.
- Chen X. R.
- Cheng C. H.
- Choi H. H. F.
- Cibinetto G.
- Clark P. J.
- Cochran J.
- Coleman J. P.
- Contri R.
- Convery M. R.
- Corwin L. A.
- Cowan G.
- Cowan R.
- Crawley H. B.
- Cremaldi L.
- Curry S.
- Dallapiccola C.
- Dasu S.
- Dauncey P. D.
- Davier M.
- Davis C. L.
- de Monchenault G. Hamel
- De Nardo G.
- de Sangro R.
- Denig A. G.
- Derkach D.
- Di Lodovico F.
- Doll D. A.
- Dorfan J.
- Druzhinin V. P.
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- Dujmic D.
- Dunwoodie W.
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- Eigen G.
- Eisner A. M.
- Emery S.
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- Ferrarotto F.
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- Weinberger M.
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- Wester W. C. III
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- Whitehouse B.
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- Whiteson D.
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- Wicklund E.
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- Wu X.
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- Yao W. -M.
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- Yeche Ch.
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- Yi K.
- Yoh J
- Yoh J.
- Yorita K
- Yorita K.
- Yoshida T
- Yoshida T.
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- Yushkov A. N.
- Zallo A.
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- Ziegler V.
- Zucchelli S.
- Zucchelli S. Stradling AR
- Zucchelli SVazquez F.
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2011
- Field of study
Using a sample of 122 million Upsilon(3S) events recorded with the BaBar
detector at the PEP-II asymmetric-energy e+e- collider at SLAC, we search for
the hbâ(1P) spin-singlet partner of the P-wave chi_{bJ}(1P) states in the
sequential decay Upsilon(3S) --> pi0 h_b(1P), h_b(1P) --> gamma eta_b(1S). We
observe an excess of events above background in the distribution of the recoil
mass against the pi0 at mass 9902 +/- 4(stat.) +/- 2(syst.) MeV/c^2. The width
of the observed signal is consistent with experimental resolution, and its
significance is 3.1sigma, including systematic uncertainties. We obtain the
value (4.3 +/- 1.1(stat.) +/- 0.9(syst.)) x 10^{-4} for the product branching
fraction BF(Upsilon(3S)-->pi0 h_b) x BF(h_b-->gamma eta_b).Comment: 8 pages, 4 postscript figures, submitted to Phys. Rev. D (Rapid
Communications
Observation and study of baryonic B decays: B -> D(*) p pbar, D(*) p pbar pi, and D(*) p pbar pi pi
- Author
- Adametz A
- Adye T
- Ahmed S
- Ahmed S
- Alam MS
- Alam MS
- Albert J
- Albert J
- Allen MT
- Alwyn KE
- Anderson J
- Andreassen R
- Andreotti M
- Angelini C
- Anulli F
- Arnaud N
- Asgeirsson DJ
- Aston D
- Atmacan H
- Ayad R
- Azzolini V
- Bailey D
- Baldini-Ferroli R
- Band HR
- Band HR
- Banerjee S
- Banerjee S
- Baracchini E
- Bard DJ
- Barlow RJ
- Bartoldus R
- Batignani G
- Battaglia M
- Behera PK
- Bellis M
- Ben-Haim E
- Benitez JF
- Bernard D
- Bernlochner FU
- Bettarini S
- Bettoni D
- Bevan AJ
- Bhuyan B
- Bhuyan B
- Bianchi F
- Bianchi F
- Biasini M
- Biassoni P
- Bingham I
- Blinov VE
- Bloom PC
- Blount NL
- Bomben M
- Bomben M
- Bondioli M
- Bonneaud GR
- Bosisio L
- Bozzi C
- Brau J
- Briand H
- Brown DN
- Brown DN
- Bula R
- Burchat PR
- Burchat PR
- Buzykaev AR
- Calabrese R
- Calcaterra A
- Calderini G
- Campagnari C
- Carpinelli M
- Cartaro C
- Cartaro C
- Casarosa G
- Castelli G
- Cavoto G
- Cecchi A
- Cenci R
- Cervelli A
- Chauveau J
- Chavez CA
- Chen C
- Chen X
- Chen XR
- Cheng CH
- Choi HHF
- Cibinetto G
- Clark PJ
- Cochranz J
- Coleman JP
- Contri R
- Convery MR
- Corwin LA
- Cossutti F
- Cowan G
- Cowan R
- Crawley HB
- Cremaldi L
- Curry S
- da Costa JF
- Dallapiccola C
- Dasu S
- Dasu S
- Dauncey PD
- Davier M
- Davis CL
- de Monchenault GH
- De Nardo G
- de Sangro R
- Della Ricca G
- Denig AG
- Derkach D
- Di Lodovico F
- Doll DA
- Dong L
- Dorfan J
- Druzhinin VP
- Dubois-Felsmann GP
- Dubrovin MS
- Dujmic D
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- Flood KT
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- Fulsom BG
- Gabareen AM
- Gabathuler E
- Gagliardi N
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- Gamba D
- Gamba D
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- Hamano K
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- Harrison PF
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- Izen JM
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- Wisniewski WJ
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- Wulsin HW
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- Yang UK
- Yang YC
- Yao WM
- Yarritu AK
- Yarritu AK
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- Yeh GP
- Yi K
- Yi K
- Yoh J
- Yorita K
- Yoshida T
- Young CC
- Young CC
- Yu GB
- Yu I
- Yu SS
- Yun JC
- Yushkov AN
- Zain SB
- Zain SB
- Zallo A
- Zanetti A
- Zeng Y
- Zhao M
- Zhou C
- Ziegler V
- Ziegler V
- Zito M
- Zucchelli S
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 15/08/2009
- Field of study
We present a study of ten B-meson decays to a D(*), a proton-antiproton pair,
and a system of up to two pions using BaBar's data set of 455x10^6 BBbar pairs.
Four of the modes (B0bar -> D0 p anti-p, B0bar -> D*0 p anti-p, B0bar -> D+ p
anti-p pi-, B0bar -> D*+ p anti-p pi-) are studied with improved statistics
compared to previous measurements; six of the modes (B- -> D0 p anti-p pi-, B-
-> D*0 p anti-p pi-, B0bar -> D0 p anti-p pi- pi+, B0bar -> D*0 p anti-p pi-
pi+, B- -> D+ p anti-p pi- pi-, B- -> D*+ p anti-p pi- pi-) are first
observations. The branching fractions for 3- and 5-body decays are suppressed
compared to 4-body decays. Kinematic distributions for 3-body decays show
non-overlapping threshold enhancements in m(p anti-p) and m(D(*)0 p) in the
Dalitz plots. For 4-body decays, m(p pi-) mass projections show a narrow peak
with mass and full width of (1497.4 +- 3.0 +- 0.9) MeV/c2, and (47 +- 12 +- 4)
MeV/c2, respectively, where the first (second) errors are statistical
(systematic). For 5-body decays, mass projections are similar to phase space
expectations. All results are preliminary.Comment: 28 pages, 90 postscript figures, submitted to LP0
Performance of CMS muon reconstruction in pp collision events at sqrt(s) = 7 TeV
- Author
- Abbaneo D
- Abbiendi G
- Abbrescia M
- Abdullin S
- Acosta D
- Acosta JG
- Acosta MV
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- Zanetti M
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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
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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- Yetkin T
- Yi K
- Yildirim E
- Yilmaz Y
- Yohay R
- Yoo HD
- Yoo J
- Yoon AS
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- 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
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- Zhu RY
- Zhukov V
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- 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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- Abbiendi G
- Abbrescia M
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- Acosta MV
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- Afanasiev S
- Agostino L
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- Kharchilava A
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- Khukhunaishvili A
- Khurana R
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- Kirakosyan M
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- Klingebiel D
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- Kodolova O
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- Kreis B
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- Kroeger R
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- Kubik A
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- Polatoz A
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- Pooth O
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- 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
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- Qian SJ
- Quan X
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- Redondo I
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- Rikova MI
- Rinkevicius A
- Rios AAO
- Rizzi A
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- Roberts J
- Robles J
- Robmann P
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- Rodozov M
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- Rodrigues Antunes J
- Rodriguez JL
- Rodriguez-Marrero AY
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- Schleper P
- Schlieckau E
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- Schoerner-Sadenius T
- Schott G
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- Shukla P
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- Tsang KV
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- Tuuva T
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- Ujvari B
- Ulmer KA
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- Urscheler C
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- Veverka J
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- Vila I
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- Villella I
- Vinogradov A
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- Vogel H
- Volkov A
- Volobouev I
- Volodko A
- Volpe R
- Vorobiev I
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- Vorobyev A
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- Wagner SR
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- Wakefield S
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- Walzel G
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- Warchol J
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- Wayne M
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- Weber HA
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- Weber M
- Wehrli L
- Weiler T
- Weinberg M
- Wendland L
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- Wenger EA
- Werner JS
- West C
- Wetzel J
- Whitbeck A
- Whitmore J
- Whyntie T
- Wickramage N
- Widl E
- Wilken R
- Wilkinson R
- Williams G
- Williams T
- Willmott C
- Wimpenny S
- Winer BL
- Winn D
- Winstrom L
- Wissing C
- Wittich P
- Wittmer B
- Woehri HK
- Wolf M
- Wolf R
- Womersley WJ
- Won S
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- Wood J
- Wood JS
- Worm SD
- Wright D
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- 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
- 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
- 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
- Adams T
- Adiguzel A
- Adler V
- Adzic P
- Agram JL
- Aguilar-Benitez M
- Aguilo E
- Ahmad M
- Ahmad WH
- Ahuja S
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- Akgun B
- Akgun U
- Akin IV
- Alagoz E
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- Albayrak EA
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- Aldaya Martin M
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- Xiao H
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- Yilmaz Y
- Yohay R
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- Yumiceva F
- Yun JC
- Zabel J
- Zabi A
- Zablocki J
- Zaganidis N
- Zakaria M
- Zalewski P
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- Zatserklyaniy A
- Zeinali M
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- Zheng Y
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- Zhu B
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- Zhukov V
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- Zielinski M
- Zito G
- Zou W
- Zucchetta A
- Zumerle G
- Zuranski A
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2012
- Field of study
A search for new physics is performed in events with two same-sign isolated
leptons, hadronic jets, and missing transverse energy in the final state. The
analysis is based on a data sample corresponding to an integrated luminosity of
4.98 inverse femtobarns produced in pp collisions at a center-of-mass energy of
7 TeV collected by the CMS experiment at the LHC. This constitutes a factor of
140 increase in integrated luminosity over previously published results. The
observed yields agree with the standard model predictions and thus no evidence
for new physics is found. The observations are used to set upper limits on
possible new physics contributions and to constrain supersymmetric models. To
facilitate the interpretation of the data in a broader range of new physics
scenarios, information on the event selection, detector response, and
efficiencies is provided.Comment: Published in Physical Review Letter
Compressed representation of a partially defined integer function over multiple arguments
- Author
- Abbaneo D
- Abbiendi G
- Abbrescia M
- Abdelalim AA
- Abdullin S
- Abdulsalam A
- Acosta D
- Acosta MV
- Adair A
- Adam W
- Adams MR
- Adams T
- Adiguzel A
- Adler V
- Adzic P
- Agram J-L
- Aguilar-Benitez M
- 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
- Alderweireldt S
- Alexander J
- Aliev T
- Alimena J
- Almeida N
- Alverson G
- Alves GA
- Amapane N
- Amsler C
- Anagnostou G
- Anastassov A
- Anderson J
- Andrea J
- Andreev V
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- Andreev Y
- Andrews W
- Androsov K
- Antonelli L
- Antunovic Z
- Apanasevich L
- Apollinari G
- Appelt E
- Apresyan A
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- Arcidiacono R
- Arenton MW
- Arfaei H
- Argiro S
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- Arora S
- Asavapibhop B
- Asawatangtrakuldee C
- Asghar MI
- Asin I
- Askew A
- Aslanoglou X
- Assran Y
- Ata M
- Attikis A
- Auffray E
- Autermann C
- Auzinger G
- Avdeeva E
- Avery P
- Avetisyan A
- Avila C
- Azarkin M
- Azhgirey I
- Aziz T
- Azzi P
- Azzolini V
- Azzurri P
- Baarmand MM
- Babb J
- Bacchetta N
- Bachmair F
- Bachtis M
- Baden A
- Baeni L
- Baffioni S
- Bagliesi G
- Bahtiyar H
- Baillon P
- Bainbridge R
- Bakhshiansohi H
- Bakirci MN
- Ball AH
- Ban Y
- Banerjee S
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- Bansal M
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- Barbagli G
- Barberis E
- Barbone L
- Barfuss AF
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- Barnett BA
- Barney D
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- Bauerdick LAT
- Baumgartel D
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- Bayshev I
- Bazterra VE
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- Beauceron S
- Beaudette F
- Beaupere N
- Beernaert K
- Behr J
- Behrenhoff W
- Behrens U
- Beirao Da Cruz E Silva C
- Belforte S
- Beliy N
- Belknap DA
- Bell AJ
- Bell KW
- Bellan R
- Beluffi C
- Belyaev A
- Belyaev A
- Benaglia A
- Bencze G
- Bendavid J
- Benedetti D
- Benelli G
- Benhabib L
- Beni N
- Benitez JF
- Benucci L
- Benussi L
- Benvenuti AC
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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
Measurement of jet fragmentation into charged particles in pp and PbPb collisions at sqrt(s[NN]) = 2.76 TeV
- Author
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- Zucchetta A
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- Zuranski A
- 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
Planck 2018 results. VII. Isotropy and Statistics of the CMB
- Author
- Akrami Y
- Ashdown M
- Aumont J
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- Ballardini M
- Banday AJ
- Barreiro RB
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- Chiang HC
- Colombo LPL
- Combet C
- Contreras D
- Crill BP
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- Delouis J-M
- Diego JM
- DorĂŠ O
- Douspis M
- Ducout A
- Dupac X
- Efstathiou G
- Elsner F
- EnĂlin TA
- Eriksen HK
- Fantaye Y
- Fernandez-Cobos R
- Finelli F
- Frailis M
- Fraisse AA
- Franceschi E
- Frolov A
- Galeotta S
- Galli S
- Ganga K
- Gerbino M
- Ghosh T
- GonzĂĄlez-Nuevo J
- Gruppuso A
- Gudmundsson JE
- GĂŠnova-Santos RT
- GĂłrski KM
- Hamann J
- Handley W
- Hansen FK
- Herranz D
- Hivon E
- Huang Z
- Jaffe AH
- Jeune ML
- Jones WC
- Keihänen E
- Keskitalo R
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- Kim J
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- Kunz M
- Kurki-Suonio H
- Lagache G
- Lamarre J-M
- Lasenby A
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- Lawrence CR
- Levrier F
- Liguori M
- Lilje PB
- Lindholm V
- LĂłpez-Caniego M
- Ma Y-Z
- MacĂas-PĂŠrez JF
- Maggio G
- Maino D
- Mandolesi N
- Mangilli A
- Marcos-Caballero A
- Maris M
- Martin PG
- MartĂnez-GonzĂĄlez E
- Matarrese S
- Mauri N
- McEwen JD
- Meinhold PR
- Mennella A
- Migliaccio M
- Miville-DeschĂŞnes M-A
- Molinari D
- Moneti A
- Montier L
- Moss A
- Natoli P
- Pagano L
- Paoletti D
- Partridge B
- Perrotta F
- Pettorino V
- Piacentini F
- Polenta G
- Puget J-L
- Rachen JP
- Reinecke M
- Remazeilles M
- Renzi A
- Rocha G
- Rosset C
- Roudier G
- RubiĂąo-MartĂn JA
- Ruiz-Granados B
- Salvati L
- Savelainen M
- Scott D
- Shellard EPS
- Sirignano C
- Sunyaev R
- Suur-Uski A-S
- Tauber JA
- Tavagnacco D
- Tent BV
- Tenti M
- Toffolatti L
- Tomasi M
- Trombetti T
- Valentino ED
- Valenziano L
- Valiviita J
- Vielva P
- Villa F
- Vittorio N
- Wandelt BD
- Wehus IK
- Zacchei A
- Zibin JP
- Zonca A
- Zotti GD
- Publication venue
- Publication date
- 01/09/2020
- Field of study
Analysis of the Planck 2018 data set indicates that the statistical properties of the cosmic microwave background (CMB) temperature anisotropies are in excellent agreement with previous studies using the 2013 and 2015 data releases. In particular, they are consistent with the Gaussian predictions of the ÎCDM cosmological model, yet also confirm the presence of several so-called "anomalies" on large angular scales. The novelty of the current study, however, lies in being a first attempt at a comprehensive analysis of the statistics of the polarization signal over all angular scales, using either maps of the Stokes parameters, Q and U, or the E-mode signal derived from these using a new methodology (which we describe in an appendix). Although remarkable progress has been made in reducing the systematic effects that contaminated the 2015 polarization maps on large angular scales, it is still the case that residual systematics (and our ability to simulate them) can limit some tests of non-Gaussianity and isotropy. However, a detailed set of null tests applied to the maps indicates that these issues do not dominate the analysis on intermediate and large angular scales (i.e., ââ˛400). In this regime, no unambiguous detections of cosmological non-Gaussianity, or of anomalies corresponding to those seen in temperature, are claimed. Notably, the stacking of CMB polarization signals centred on the positions of temperature hot and cold spots exhibits excellent agreement with the ÎCDM cosmological model, and also gives a clear indication of how Planck provides state-of-the-art measurements of CMB temperature and polarization on degree scales
- âŚ