4,849 research outputs found
Development of a Human Cytomegalovirus (HCMV)-Based Therapeutic Cancer Vaccine Uncovers a Previously Unsuspected Viral Block of MHC Class I Antigen Presentation
- Author
- Abate
- Ahmed
- Alexandrov
- Alexandrov
- Arnon
- Avdic
- Beyranvand Nejad
- Brown
- Brown
- Browne
- Chang
- Chu
- Cloughesy
- Cobbs
- Dasari
- Dekhtiarenko
- Del Val
- Desjardins
- Doisne
- Dos Santos
- Draper
- Duhen
- Dziurzynski
- Engels
- Fiallos
- Filley
- Fruh
- Galluzzi
- Gilbert
- Gorzer
- Harkins
- Heemskerk
- Howland
- Jarry
- Johnson
- Jutz
- Jutz
- Kern
- Klenerman
- Korn
- Kotenko
- Lauvau
- Le
- Leisegang
- Lim
- Lockridge
- Locy
- Louveau
- Lucas
- Luo
- Malouli
- Martikainen
- Mitchell
- Mocarski
- Nair
- Neefjes
- Odeberg
- Overwijk
- Pardieck
- Polyzoidis
- Potter
- Prins
- Pule
- Raftery
- Raftery
- Raftery
- Raftery
- Rahman
- Ratzinger
- Reap
- Reardon
- Reed
- Ressing
- Riegler
- Rizvi
- Rosato
- Rosskopf
- Sampaio
- Sampson
- Sandalova
- Schempp
- Scheper
- Schmolke
- Schneider
- Schonrich
- Schub
- Sckisel
- Shah
- Simoni
- Sinzger
- Soroceanu
- Soroceanu
- Strang
- Stupp
- Sturm
- Sugawara
- Sylwester
- Thomas
- Tischer
- Tran
- Trgovcich
- Tumeh
- van der Burg
- van Willigen
- Varnum
- Vlahovic
- Wen
- Wills
- Yan
- Zhao
- Publication venue
- Publication date
- 01/01/2019
- Field of study
Human cytomegalovirus (HCMV) induces a uniquely high frequency of virus-specific effector/memory CD8+ T-cells, a phenomenon termed âmemory inflationâ. Thus, HCMV-based vaccines are particularly interesting in order to stimulate a sustained and strong cellular immune response against cancer. Glioblastoma multiforme (GBM) is the most aggressive primary brain tumor with high lethality and inevitable relapse. The current standard treatment does not significantly improve the desperate situation underlining the urgent need to develop novel approaches. Although HCMV is highly fastidious with regard to species and cell type, GBM cell lines are susceptible to HCMV. In order to generate HCMV-based therapeutic vaccine candidates, we deleted all HCMV-encoded proteins (immunoevasins) that interfere with MHC class I presentation. The aim being to use the viral vector as an adjuvant for presentation of endogenous tumor antigens, the presentation of high levels of vector-encoded neoantigens and finally the repurposing of bystander HCMV-specific CD8+ T cells to fight the tumor. As neoantigen, we exemplarily used the E6 and E7 proteins of human papillomavirus type 16 (HPV-16) as a non-transforming fusion protein (E6/E7) that covers all relevant antigenic peptides. Surprisingly, GBM cells infected with E6/E7-expressing HCMV-vectors failed to stimulate E6-specific T cells despite high level expression of E6/E7 protein. Further experiments revealed that MHC class I presentation of E6/E7 is impaired by the HCMV-vector although it lacks all known immunoevasins. We also generated HCMV-based vectors that express E6-derived peptide fused to HCMV proteins. GBM cells infected with these vectors efficiently stimulated E6-specific T cells. Thus, fusion of antigenic sequences to HCMV proteins is required for efficient presentation via MHC class I molecules during infection. Taken together, these results provide the preclinical basis for development of HCMV-based vaccines and also reveal a novel HCMV-encoded block of MHC class I presentation
Performance of CMS muon reconstruction in pp collision events at sqrt(s) = 7 TeV
- Author
- Abbaneo D
- Abbiendi G
- Abbrescia M
- Abdullin S
- Acosta D
- Acosta JG
- Acosta MV
- Adair A
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- Adler V
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- Agram JL
- Aguilar-Benitez M
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- Akchurin N
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- Korablev A
- Korpela A
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- Kreis B
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- 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
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- Raidal M
- Rakness G
- Ralph D
- Rander J
- Ranieri R
- Ranjan K
- Rappoccio S
- Raspereza A
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- Ratti SP
- Raupach F
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- Razis PA
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- Redjimi R
- Redondo I
- Reece W
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- Reithler H
- Rekovic V
- Remington R
- Renker D
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- 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
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- Robles J
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- Rodozov M
- Rodrigo T
- Rodriguez JL
- Rodriguez-Marrero AY
- Roe J
- Roecker S
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- 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
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- Rosin M
- Rosowsky A
- Ross I
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- Rossi AM
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- Rougny R
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- Rudolph M
- Ruiz-Jimeno A
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- Santoro A
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- Savin A
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- Sawley M-C
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- Schaefer C
- Schael S
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- Scheurer A
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- Schlein P
- Schleper P
- Schlieckau E
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- 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
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- Sikler F
- Silkworth C
- Sill A
- Sillou D
- Silva Do Amaral SM
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- Silvers D
- Silverwood H
- Silvestre C
- Silvestris L
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- Simonetto F
- Simonis HJ
- Singh AP
- Singh G
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- Singovsky A
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- Sirois Y
- Siroli G
- Sirunyan AM
- Skhirtladze N
- Skuja A
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- Smirnov I
- Smith J
- Smith JG
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- Smolin D
- Snigirev A
- Snoek H
- Snook B
- Snow GR
- Snowball M
- Soares Jorge L
- Soares MS
- Sobol A
- Sobron Sanudo M
- Soffi L
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- Spiridonov A
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- Stiliaris E
- Stober FM
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- Strobbe N
- Strom 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
- Surat UE
- Svintradze I
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- Tadel M
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- Tapper A
- Taroni S
- Tatarinov A
- Taurok A
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- Thea A
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- Thyssen F
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- Tiras E
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- 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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- Turner M
- Tuuva T
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- 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
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- Vogel H
- Volkov A
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- Vorobiev I
- Vorobyev A
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- Vuosalo C
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- Wakefield S
- Wallny R
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- Waltenberger W
- Walzel G
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- Wardle N
- Wardrope D
- Wasserbaech S
- Wayne M
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- Wehrli L
- Weiler T
- Weinberg M
- Wendland L
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- Weng Y
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- Whyntie T
- Wickens J
- Wickramage N
- Widl E
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- Williams T
- Willmott C
- Wimpenny S
- Winn D
- Winstrom L
- Wissing C
- Wittich P
- Wittmer B
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- Wolf M
- Wolf R
- Womersley WJ
- Won S
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- Wood JS
- Worm SD
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- 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
Performance of CMS muon reconstruction in pp collision events at sqrt(s) = 7 TeV
- Author
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- Romeo F
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- Wissing C
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- Wolf M
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- Womersley WJ
- Won S
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- Wood J
- Wood JS
- Worm SD
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- 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
Constraints on the Ď_(c1) versus Ď_(c2) polarizations in proton-proton collisions at âs = 8 TeV
- Author
- Abbaneo D.
- Abbiendi G.
- Abbrescia M.
- Abdullin S.
- Abercrombie D.
- Acharya H.
- Acosta D.
- Acosta J.âG.
- Adam W.
- Adams M.âR.
- Adams T.
- Adzic P.
- Afanasiev S.
- Agapitos A.
- Agarwal G.
- Aggleton R.
- Agram J.-L.
- Aguilar-Benitez M.
- Ahmad A.
- Ahmad M.
- Ahmad M.
- Ahuja S.
- Akbiyik M.
- Akchurin N.
- Akgun B.
- Albajar C.
- Albergo S.
- Albert A.
- Albrow M.
- Alcaraz Maestre J.
- Aldaya Martin M.
- Aleksandrov A.
- Alexander J.
- Alhusseini M.
- Alimena J.
- Alison J.
- Allen B.
- Almond J.
- Alvarez Gonzalez B.
- Alverson G.
- Alves G.âA.
- Aly R.
- Alyari M.
- Amapane N.
- Ambrogi F.
- Amendola C.
- Amin N.
- Amsler C.
- Anagnostou G.
- Anderson D.
- Andrea J.
- Andreev V.
- Andreev Yu.
- Andrews M.âB.
- Androsov K.
- Ang L.
- Antchev G.
- Antunovic Z.
- Apanasevich L.
- Apollinari G.
- Apresyan A.
- Apyan A.
- Araujo M.
- Arcaro D.
- Arcidiacono R.
- Arenton M.âW.
- Argiro S.
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- Zorbilmez C.
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- Zuolo D.
- Ălvarez FernĂĄndez A.
- Ăzçelik Ă.
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 24/04/2020
- Field of study
The polarizations of promptly produced Ď_(c1) and Ď_(c2) mesons are studied using data collected by the CMS experiment at the LHC, in proton-proton collisions at âs=8ââTeV. The Ď_c states are reconstructed via their radiative decays Ď_c â J/ĎÎł, with the photons being measured through conversions to eâşeâť, which allows the two states to be well resolved. The polarizations are measured in the helicity frame, through the analysis of the Ď_(c2) to Ď_(c1) yield ratio as a function of the polar or azimuthal angle of the positive muon emitted in the J/Ď â ÎźâşÎźâť decay, in three bins of J/Ď transverse momentum. While no differences are seen between the two states in terms of azimuthal decay angle distributions, they are observed to have significantly different polar anisotropies. The measurement favors a scenario where at least one of the two states is strongly polarized along the helicity quantization axis, in agreement with nonrelativistic quantum chromodynamics predictions. This is the first measurement of significantly polarized quarkonia produced at high transverse momentum
Azimuthal anisotropy of charged particles at high transverse momenta in PbPb collisions at sqrt(s[NN]) = 2.76 TeV
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- Wardle N
- Wasserbaech S
- Wayne M
- Weber H
- Weber HA
- Weber M
- Weber M
- Wehrli L
- Weiler T
- Weinberg M
- Wendland L
- Weng Y
- 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
- 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
- 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
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