177 research outputs found
Two-pion Bose-Einstein correlations in central Pb-Pb collisions at sNN = 2.76 TeV
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- T. Sugitate dd
- T. Susa x
- T. Traczykcn
- T. Virgili ce
- T.B. Skaali bh
- T.C. Awesae
- T.J. Humanicw
- T.J.M. Symons ct
- T.K. Nayaki
- T.M. Cormier at
- T.S. R\ue4ih\ue4af
- T.S. Tveterbh
- U. Frankenfelds
- U. Fuchsf
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- U. Westerhoffap
- V. Altini r
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- V. Catanescu u
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- V. Demanovbk
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- V. Puninbk
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- Venaruzzo M.
- W. Carena f
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- W. Perytcn
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- W.H. Trzaskaaf
- W.J. Parks
- X. Cai bn
- X. Li cz
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- X. Zhang bn
- X. Zhubn
- X.-G. Lu bl
- Y. Berdnikov au
- Y. Corrales Morales ah
- Y. Delgado Mercado bo
- Y. Hori cr
- Y. Kharlovbd
- Y. Kucheriaevm
- Y. Kwoncw
- Y. Le Bornec bg
- Y. Maobn
- Y. Martynov p
- Y. Miake bu
- Y. Pachmayerbl
- Y. Pestovdf
- Y. Schutzaa
- Y. Sibiriakm
- Y. Vinogradov bk
- Y. Wangbl
- Y. Wangbn
- Y. Zoccarato bq
- Y.P. Viyogi i
- Y.W. Baekk
- Z. Ahammed i
- Z. Buthelezi bm
- Z. Conesa del Valle aa
- Z. Vilakazi bm
- Z. Yinbn
- Z.L. Matthews an
- Publication venue
- 'Elsevier BV'
- Publication date
- 21/12/2010
- Field of study
The first measurement of two-pion Bose-Einstein correlations in central Pb-Pb
collisions at sNN=2.76 TeV at the Large Hadron Collider is
presented. We observe a growing trend with energy now not only for the
longitudinal and the outward but also for the sideward pion source radius. The
pion homogeneity volume and the decoupling time are significantly larger than
those measured at RHIC.Comment: 17 pages, 5 captioned figures, 1 table, authors from page 12,
published version, figures at
http://aliceinfo.cern.ch/ArtSubmission/node/388
Suppression of charged particle production at large transverse momentum in central Pb-Pb collisions at sNN=2.76 TeV
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- A. Abrahantes Quintana b
- A. Ahmad Masoodi j
- A. Akindinov l
- A. Alici o
- A. Alkinp
- A. Andronic s
- A. Arendab
- A. Asryant
- A. Augustinus f
- A. Badal\ue0 ag
- A. Baldisseri aj
- A. Baldit ak
- A. Bercuci u
- A. Bhasinav
- A. Bilandzic ay
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- A. Bogdanovbb
- A. Casanova D\uedaz aw
- A. Dainesebz
- A. Danuca
- A. Dashcb
- A. De Azevedo Moregula aw
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- A. De Falco cf
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- A. Deppman cc
- A. Di Maurof
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- A. Fedunovaq
- A. Fern\ue1ndez T\ue9llez bw
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- A. Grigorasf
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- A. Herghelegiu u
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- A. Kalweitcv
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- A. Khanzadeev au
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- A. Klovning a
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- A. Kuryakinbj
- A. Maevskayack
- A. Maireas
- A. Mamonovbj
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- A. Margotti z
- A. Mart\uednez Davalos h
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- A. Mastroserio f
- A. Matyja ao
- A. Menchaca-Rocha h
- A. Mischke br
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- A. Ochirovt
- A. Ortiz Velasquez by
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- A. Pavlinovat
- A. Pesci z
- A. Piccotti n
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- A. Pulvirenti am
- A. Rachevski cl
- A. Rademakers f
- A. Rakotozafindrabe aj
- A. Ram\uedrez Reyesbv
- A. Reshetinck
- A. Rivetti n
- A. Rossi y
- A. Rybicki ao
- A. Sandoval h
- A. Sevcencoca
- A. Silenzi o
- A. Soloviev bc
- A. Szanto de Toledocc
- A. Szostaka
- A. Taurof
- A. Telesca f
- A. Toia f
- A. Tumkinbj
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- A. Vacchi cl
- A. Vargasbw
- A. Vasilievm
- A. Vinogradovm
- A. Vodopyanov aq
- A. Wilk ap
- A. Zarochentsev t
- A. Zeninbc
- A. Zichichi o
- A.A.P. Suaide cc
- A.B. Kurepin ck
- A.G. Agocs g
- A.J. Peters f
- A.J. Rubio Montero az
- A.J. Turveybo
- A.K. Bhati e
- A.K. Dubeyi
- A.K. Dutta Majumdar be
- A.M. Adared
- A.R. Reolonaw
- A.R. Timmins at
- B. Alessandro n
- B. Bathenap
- B. Batyunyaaq
- B. Boyerbf
- B. Chang af
- B. Cheynis bp
- B. D\uf6nigus s
- B. Espagnonbf
- B. Ghidini r
- B. Grinyovp
- B. Guerzoni o
- B. Hicksd
- B. Hippolyte as
- B. Kileng ci
- B. Mohantyi
- B. Polichtchouk bc
- B. Potukuchi av
- B. Sitarbi
- B. von Haller f
- B. Vulpescu ak
- B. Wagnera
- B. Windelband bk
- B.C. Sinha i
- B.K. Nandi cu
- B.K. Srivastavadh
- B.S. Nielsenar
- B.S. Nilsen bo
- C. Andrei u
- C. Anson w
- C. Baumannab
- C. Bianchin y
- C. Blumeab
- C. Bombonati y
- C. Bortoliny
- C. Cavicchioli f
- C. Cheshkovbp
- C. Cicalo bu
- C. Di Giglio r
- C. Furgetac
- C. Garabatos s
- C. Geuna aj
- C. Grigorasf
- C. Guerra Gutierrez bn
- C. Hadjidakisbf
- C. Hern\ue1ndez s
- C. Ivans
- C. Klein-B\uf6sing ap
- C. Kottachchi Kankanamge Don at
- C. Kuhn as
- C. Larav
- C. Lazzeroni an
- C. Lippmann f
- C. Loizidesct
- C. Luzzi f
- C. Mitu ca
- C. Nattrass db
- C. Nygaard ar
- C. Oppedisano n
- C. Pajaresad
- C. Pettaam
- C. Royaa
- C. S\uf8gaard ar
- C. Schiauau
- C. Schmidts
- C. Soos f
- C. Suire bf
- C. Tagridis cm
- C. Terrevoli r
- C. Zampolli f
- C.A. Pruneau at
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- C.E. P\ue9rez Lara ay
- C.H. Christensen ar
- C.W. Fabjanf
- D. Adamov\ue1c
- D. Aleksandrovm
- D. Blaum
- D. Budnikovbj
- D. Caffarri y
- D. Dasbe
- D. De Gruttolacd
- D. Di Bari r
- D. Eliace
- D. Emschermann ap
- D. Evansan
- D. Fabriscj
- D. Falchieri o
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- D. Hasegan ca
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- D. Krumbhorn bk
- D. Lohner bk
- D. Mal\u2019Kevich l
- D. Mayani by
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- D. Peresunkom
- D. Perini f
- D. Perrino r
- D. R\uf6hrich a
- D. Rohr q
- D. Sakata bt
- D. Silvermyr ae
- D. Stocco aa
- D. Swobodaf
- D. Thomasbr
- D. Tlusty ax
- D. Truesdale w
- D. Vranics
- D. Wangbm
- D. Zhoubm
- D.A. Moreira De Godoy cc
- D.B. Piyarathna at
- D.D. Chinellato bq
- D.J. Kimaf
- D.M. Madagodahettige-Don ba
- D.P. Mahapatra cb
- D.S. Hwangcs
- D.S. Kimk
- D.T. Larsen a
- D.W. Kim k
- E. Almar\ue1z Avi\uf1a h
- E. Belmont-Moreno h
- E. Berdermanns
- E. Biolcati ah
- E. Bruna d
- E. Calvo Villar bn
- E. Chiavassa n
- E. Cresciobv
- E. Cuautle by
- E. D\ue9nes g
- E. Fragiacomo cl
- E. Gladysz-Dziadus ao
- E. Incani cf
- E. Kang k
- E. Karpechevck
- E. Korna\ub4s ao
- E. Kryshenau
- E. L\uf3pez Torres b
- E. Montesaz
- E. Mudniccp
- E. Nappi ce
- E. Quercigh f
- E. Ryabinkin m
- E. Scapparone z
- E. Scomparinn
- E. Serradilla az
- E. Sickingf
- E. Stenlundbs
- E. Vercellin ah
- E. Zabrodin bg
- E.M. Fiore r
- F. Antinori y
- F. Barile r
- F. Bellini o
- F. Blanco az
- F. Blancoba
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- F. Carenaf
- F. Carminati f
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- F. Coccetti ai
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- F. Kramerab
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- F. Navachr
- F. Nendazbp
- F. Noferini z
- F. Padilla ah
- F. Painkeq
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- F. Prino n
- F. Rettig q
- F. Riggi am
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- F. Roukoutakis cm
- F. Scarlassara y
- F. Soramel y
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- G. Cara Romeoz
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- G. Contin bh
- G. de Cataldo ce
- G. Dellacasa bx
- G. Eyyubova bg
- G. Feofilovt
- G. Giraudon
- G. Hamar g
- G. Herrera Corral bv
- G. L\uf8vh\uf8iden bg
- G. Luparello ah
- G. Mart\uednez Garc\ueda aa
- G. Mazza n
- G. Nazarov bj
- G. Nooren br
- G. Ortonaah
- G. Pai\ub4c by
- G. Puddu cf
- G. Scioli o
- G. Segato y
- G. Shabratova aq
- G. Simonetti f
- G. Stefanek cg
- G. Stefanini f
- G. Steynbl
- G. Tejeda Mu\uf1oz bw
- G. Viesti y
- G. Volpe r
- G. Wilk cg
- G. Zinovjev p
- G.D. Erasmo r
- G.E. Bruno r
- G.G. Barnaf\uf6ldi g
- G.L. Usai cf
- G.M. Innocenti ah
- G.M. Urciuoli ch
- G.O.V. de Barros cc
- G.S. Pappalardo ag
- G.T. Jonesan
- G.V. Margagliotti bh
- H. Appelsh\ue4user ab
- H. B\uf8ggild ar
- H. Beck ab
- H. Borel aj
- H. Buesching ab
- H. Cainesd
- H. Delagrange aa
- H. Engel v
- H. Gonz\ue1lez Santosbw
- H. Gutbrods
- H. Hamagaki cr
- H. Helstrupci
- H. Jungk
- H. Le\uf3n Vargasab
- H. M\ufcller f
- H. Obayashi dd
- H. Oeschlercv
- H. Qvigstad bg
- H. Ricaud cv
- H. Soncs
- H. Torii dd
- H. Yang aj
- H. Yokoyamabt
- H. Zbroszczyk cn
- H.A. Erdal ci
- H.H. Dalsgaard ar
- H.N. Kimk
- H.R. Schmidt s
- I. Altsybeevt
- I. Belikovas
- I. Berceanuu
- I. Cort\ue9s Maldonado bw
- I. Dasbe
- I. Dom\uednguez by
- I. H\u2c7rivn\ue1\u2c7cov\ue1 bf
- I. Ilkivcg
- I. Kisel v
- I. Kr\ue1likal
- I. Krauscv
- I. Le\uf3n Monz\uf3nco
- I. Maldonado Cervantes by
- I. Martashvili db
- I. Otterlundbs
- I. Pshenichnov ck
- I. Rusanovf
- I. Stanca
- I. Szarkabi
- I. Yushmanovm
- I. Zguraca
- I.-K. Yoo dj
- I.C. Arsene s
- I.G. Bearden ar
- J. \uc4yst\uf6af
- J. B\ue1nal
- J. Bartkeao
- J. Biel\u2c7c\uedk ax
- J. Biel\u2c7c\uedkov\ue1 c
- J. Book ab
- J. Castillo Castellanos aj
- J. Cleymansbl
- J. de Cuveland q
- J. Dubuisson f
- J. Faivre ac
- J. Gerhardq
- J. Kleinbk
- J. Kral af
- J. Lehnert ab
- J. Mare\u161da
- J. Mercado P\ue9rezbk
- J. Midori dd
- J. Milosevic bg
- J. Mlynarz at
- J. Munozbw
- J. Newbyde
- J. Nystranda
- J. Oleniaczcn
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- J. Pluta cn
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- J. Rakaf
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- J. Yi dj
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- J.H. Kimcs
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- J.J. Gaardh\uf8je ar
- J.L. Charvet aj
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- J.W. Harris d
- K. \u160afa\u2c7r\uedk f
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- K. Gulbrandsen ar
- K. Kanaki a
- K. Kochbk
- K. Kozlovm
- K. Mabm
- K. Oyamabk
- K. Ozawacr
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- K. Reygersbk
- K. Schwarzs
- K. Schwedabk
- K. Shigaki dd
- K. Shtejer b
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- K. Watanabe bt
- K.F. Hetland ci
- K.F. Readdb
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- L. Aphecetcheaa
- L. Betevf
- L. Bianchi ah
- L. Boldizs\ue1rg
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- L. Cifarelli o
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- L. Liua
- L. Luquin aa
- L. Manceauak
- L. Mangotra av
- L. Massacrier bp
- L. Milano ah
- L. Molnarf
- L. Monta\uf1o Zetinabv
- L. Musaf
- L. Pinsky ba
- L. Ramello bx
- L. Riccati n
- L. Toscano f
- L. Valencia Palomo bf
- L. Vannucci bz
- L. Vickovic cp
- L. Vinogradov t
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- L.S. Barnby an
- M. \u160umbera c
- M. Bachq
- M. Basile o
- M. Boccioli f
- M. Bogolyubsky bc
- M. Bombarabd
- M. Botjeay
- M. Bregant bh
- M. Brozbi
- M. Caselle f
- M. Cherney bo
- M. Chojnacki br
- M. Estienne aa
- M. Fasel s
- M. Florisf
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- M. Fusco Girard cd
- M. Gagliardi ah
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- M. Germainaa
- M. Gheataf
- M. Haiducca
- M. Hartigab
- M. Heideap
- M. Heinz d
- M. Huang a
- M. Inababt
- M. Ippolitov m
- M. Irfanj
- M. Ivanovs
- M. Kaliskyap
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- M. Kimk
- M. Kliemantab
- M. Kowalski ao
- M. Kretz q
- M. Krivda an
- M. Krusax
- M. Krzewicki ay
- M. L\uf3pez Noriega bf
- M. Lenhardt aa
- M. Lunardony
- M. Magerf
- M. Malaev au
- M. Maseraah
- M. Mastromarco ce
- M. Montenon
- M. Morando y
- M. Nicassio r
- M. P\u142oskon\ub4 ct
- M. Pachr ax
- M. Petrisu
- M. Petrovici u
- M. Pikna bi
- M. Puti\u161bd
- M. Rammler ap
- M. Richtera
- M. Rodr\uedguez Cahuantzi bw
- M. Sano bt
- M. Shimomura bt
- M. Siciliano ah
- M. Sittabx
- M. Songcw
- M. Spyropoulou-Stassinaki cm
- M. Stolpovskiy bc
- M. Tavletf
- M. Valaaq
- M. van Leeuwen br
- M. Vasileioucm
- M. Venaruzzo bh
- M. Verweij br
- M. Wildeap
- M. Zhalovau
- M. Zynovyev p
- M.A. Lisa w
- M.A. Mazzoni ch
- M.A. Subieta V\ue1squez ah
- M.A.S. Figueredo cc
- M.C.S. Williams z
- M.D. Azmi j
- M.E. Cotallo az
- M.G. Munhoz cc
- M.G. Poghosyan ah
- M.I. Mart\uednez bw
- M.J. Kweonbk
- M.K. K\uf6hlers
- M.L. Knichel s
- M.M. Aggarwal e
- M.M. Khanj
- M.R. Cosentino bq
- M.R. Dutta Majumdar i
- M.R. Girard cn
- M.S. Nilsson bg
- N. Ahmadj
- N. Arborac
- N. Armestoad
- N. Bastidak
- N. Bianchi aw
- N. Bockw
- N. De Marcon
- N. Grioncl
- N. Herrmannbk
- N. Kondratyeva bb
- N. Novitzky af
- N. Pitz ab
- N. Sharma e
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- O. Busch bk
- O. Dordic bg
- O. Driga aa
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- O. Pinazza f
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- P. Braun-Munzinger s
- P. Camerini bh
- P. Cerello n
- P. Chochulaf
- P. Christakoglou br
- P. Christiansen bs
- P. Constantinbk
- P. Cortese bx
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- P. Ghosh i
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- P. Hristovf
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- P. Riedlerf
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- P. Saturnini ak
- P. Strmenbi
- P. Vande Vyvre f
- P. Z\ue1vadada
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- P.M. Jacobsct
- P.T. Hille d
- R. Alfaro Molina h
- R. Arnaldi n
- R. Averbecks
- R. Bailhache ab
- R. Balaah
- R. Baldini Ferroli ai
- R. Barberaam
- R. Bellwied at
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- R. De Remigis n
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- R. Fearickbl
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- X. Zhang bm
- X.-G. Lubk
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- Y. Kucheriaevm
- Y. Kwoncw
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- Y. Maobm
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- Publication venue
- 'Elsevier BV'
- Publication date
- 07/12/2010
- Field of study
Inclusive transverse momentum spectra of primary charged particles in Pb-Pb
collisions at sNN = 2.76 TeV have been measured by the ALICE
Collaboration at the LHC. The data are presented for central and peripheral
collisions, corresponding to 0-5% and 70-80% of the hadronic Pb-Pb cross
section. The measured charged particle spectra in ∣η∣<0.8 and 0.3<pT<20 GeV/c are compared to the expectation in pp collisions at the same
sNN, scaled by the number of underlying nucleon-nucleon
collisions. The comparison is expressed in terms of the nuclear modification
factor RAA. The result indicates only weak medium effects (RAA≈ 0.7) in peripheral collisions. In central collisions, RAA
reaches a minimum of about 0.14 at pT=6-7GeV/c and increases
significantly at larger pT. The measured suppression of high-pT particles is stronger than that observed at lower collision energies,
indicating that a very dense medium is formed in central Pb-Pb collisions at
the LHC.Comment: 15 pages, 5 captioned figures, 3 tables, authors from page 10,
published version, figures at http://aliceinfo.cern.ch/ArtSubmission/node/98
Measurement of the inclusive and differential Higgs boson production cross sections in the decay mode to a pair of τ Leptons in pp collisions at sqrt[s]=13 TeV
- Author
- Aarrestad TK
- Aarup Petersen H
- Abbaneo D
- Abbiendi G
- Abbrescia M
- Abdalla H
- Abdelalim AA
- Abdullin S
- Abercrombie D
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- Chhibra SS
- Chiarito B
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- Chou JP
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- Christoforou K
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- Ciangottini D
- Ciocci MA
- Cipriani M
- Citron M
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- Cornelis T
- Correia Silva G
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- Dallavalle GM
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- De Wolf EA
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- Defranchis MM
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- Del Burgo R
- Del Re D
- Delaere C
- Delannoy AG
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- Delgado Peris A
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- Demiroglu ZS
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- Dewanjee RK
- Dezoort G
- Dharmaratna WGD
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- Di Petrillo KF
- Di Pilato A
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- Diamantopoulou M
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- Yusli MN
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- Zahid S
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- Zecchinelli AG
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- Zorbilmez C
- Zotto P
- Zotz A
- Zou D
- Zou R
- Zucchetta A
- Zumerle G
- Zuo X
- Zuolo D
- Zygala L
- Álvarez Fernández A
- Özçelik Ö
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2022
- Field of study
Measurements of the inclusive and differential fiducial cross sections of the Higgs boson are presented, using the τ lepton decay channel. The differential cross sections are measured as functions of the Higgs boson transverse momentum, jet multiplicity, and transverse momentum of the leading jet in the event, if any. The analysis is performed using proton-proton collision data collected with the CMS detector at the LHC at a center-of-mass energy of 13 TeV and corresponding to an integrated luminosity of 138 fb^{-1}. These are the first differential measurements of the Higgs boson cross section in the final state of two τ leptons. In final states with a large jet multiplicity or with a Lorentz-boosted Higgs boson, these measurements constitute a significant improvement over measurements performed in other final states
Observation of a New Excited Beauty Strange Baryon Decaying to Ξb- π+π-
- Author
- Aarrestad TK
- Aarup Petersen H
- Abbaneo D
- Abbiendi G
- Abbrescia M
- Abdullin S
- Abercrombie D
- Abu Zeid S
- Acharya H
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- Yi K
- Yigitbasi E
- Yohay R
- Yoo HD
- Yoo J
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- Yu I
- Yu PR
- Yu SS
- Yuan L
- Yuan S
- Yumiceva F
- Yusli MN
- Zabi A
- Zacharopoulou A
- Zahid S
- Zaleski S
- Zalewski P
- Zanetti M
- Zarubin A
- Zarucki M
- Zecchinelli AG
- Zeinali M
- Zeuner WD
- Zghiche A
- Zhang F
- Zhang H
- Zhang J
- Zhang S
- Zhang W
- Zhang Y
- Zhang Z
- Zhao J
- Zhizhin I
- Zhokin A
- Zhu DH
- Zhu RY
- Ziemons T
- Zientek M
- Zlebcik R
- Zoi I
- Zolkapli Z
- Zorbakir IS
- Zorbilmez C
- Zotto P
- Zou D
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- Zumerle G
- Zuo X
- Zuolo D
- Zygala L
- Álvarez Fernández A
- Özçelik Ö
- Publication venue
- American Physical Society
- Publication date
- 01/01/2021
- Field of study
The Ξb-π+π- invariant mass spectrum is investigated with an event sample of proton-proton collisions at s=13 TeV, collected by the CMS experiment at the LHC in 2016-2018 and corresponding to an integrated luminosity of 140 fb-1. The ground state Ξb- is reconstructed via its decays to J/ψΞ- and J/ψΛK-. A narrow resonance, labeled Ξb(6100)-, is observed at a Ξb-π+π- invariant mass of 6100.3±0.2(stat)±0.1(syst)±0.6(Ξb-) MeV, where the last uncertainty reflects the precision of the Ξb- baryon mass. The upper limit on the Ξb(6100)- natural width is determined to be 1.9 MeV at 95% confidence level. The low Ξb(6100)- signal yield observed in data does not allow a measurement of the quantum numbers of the new state. However, following analogies with the established excited Ξc baryon states, the new Ξb(6100)- resonance and its decay sequence are consistent with the orbitally excited Ξb- baryon, with spin and parity quantum numbers JP=3/2-
First measurement of the |t|-dependence of coherent J/ψ photonuclear production
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- Yoon JH
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- Zaman A
- Zampolli C
- Zanoli HJC
- Zardoshti N
- Zarochentsev A
- Zavada P
- Zaviyalov N
- Zbroszczyk H
- Zhalov M
- Zhang X
- Zhang Y
- Zhang Z
- Zhao C
- Zherebchevskii V
- Zhigareva N
- Zhou D
- Zhou Y
- Zhou Z
- Zhu H
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- Zhu Y
- Zichichi A
- Zimmermann MB
- Zinovjev G
- Zmeskal J
- Publication venue
- 'Elsevier BV'
- Publication date
- 01/01/2021
- Field of study
The first measurement of the cross section for coherent J/ψ photoproduction as a function of |t|, the square of the momentum transferred between the incoming and outgoing target nucleus, is presented. The data were measured with the ALICE detector in ultra-peripheral Pb–Pb collisions at a centre-of-mass energy per nucleon pair sNN=5.02TeV with the J/ψ produced in the central rapidity region |y|<0.8, which corresponds to the small Bjorken-x range (0.3−1.4)×10−3.
The measured |t|-dependence is not described by computations based only on the Pb nuclear form factor, while the photonuclear cross section is better reproduced by models including shadowing according to the leading-twist approximation, or gluon-saturation effects from the impact-parameter dependent Balitsky–Kovchegov equation. These new results are therefore a valid tool to constrain the relevant model parameters and to investigate the transverse gluonic structure at very low Bjorken-x.publishedVersio
Search for strongly interacting massive particles generating trackless jets in proton-proton collisions at s = 13 TeV
- Author
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- Yang UK
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- Zanetti M
- Zarubin A
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- Zecchinelli AG
- Zeinali M
- Zenaiev O
- Zeuner WD
- Zghiche A
- Zhang F
- Zhang H
- Zhang J
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- Zhokin A
- Zhu DH
- Zhu RY
- Zich J
- Zielinski K
- Ziemons T
- Zientek M
- Zlebcik R
- Zoi I
- Zolkapli Z
- Zorbakir IS
- Zorbilmez C
- Zotto P
- Zou D
- Zucchetta A
- Zumerle G
- Zuo X
- Zuolo D
- Zygala L
- Álvarez Fernández A
- Österberg K
- Özçelik Ö
- Široký J
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2022
- Field of study
A search for dark matter in the form of strongly interacting massive particles (SIMPs) using the CMS detector at the LHC is presented. The SIMPs would be produced in pairs that manifest themselves as pairs of jets without tracks. The energy fraction of jets carried by charged particles is used as a key discriminator to suppress efficiently the large multijet background, and the remaining background is estimated directly from data. The search is performed using proton-proton collision data corresponding to an integrated luminosity of 16.1 fb - 1 , collected with the CMS detector in 2016. No significant excess of events is observed above the expected background. For the simplified dark matter model under consideration, SIMPs with masses up to 100 GeV are excluded and further sensitivity is explored towards higher masses
Search for Higgs Boson Pair Production in the Four b Quark Final State in Proton-Proton Collisions at root s=13 TeV
- Author
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- Abbaneo D
- Abbiendi G
- Abbrescia M
- Abdullah WW
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- Zeinali M
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- Álvarez CR
- Özçelik Ö
- Publication venue
- Publication date
- 01/01/2022
- Field of study
Observation of the B-s(0) -> X(3872)phi Decay
- Author
- Aarrestad TK
- Aarup Petersen H
- Abbaneo D
- Abbiendi G
- Abbrescia M
- Abdullin S
- Abercrombie D
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- Publication venue
- Publication date
- 01/01/2020
- Field of study
Using a data sample of proton-proton collisions at root s = 13 TeV, corresponding to an integrated luminosity of 140 fb(-1) collected by the CMS experiment in 2016-2018, the B-s(0) -> X(3872)phi decay is observed. Decays into J/psi pi(+)pi(-) and K+K- are used to reconstruct, respectively, the X(3872) and phi. The ratio of the product of branching fractions B[B-s(0) -> X(3872)phi]B[X(3872) -> J/psi pi(+)pi(-)] to the product B[B-s(0) ->psi(2S)phi]B[psi(2S) -> J/psi pi(+)pi(-)] is measured to be [2.21 +/- 0.29(stat) +/- 0.17(syst)]%. The ratio B[B-s(0) -> X(3872)phi]/B[B-0 -> X(3872)K-0] is found to be consistent with one, while the ratio B[B-s(0) -> X(3872)phi]/B[B+-> X(3872)K+] is two times smaller. This suggests a difference in the production dynamics of the X(3872) in B-0 and B(0)s meson decays compared to B+. The reported observation may shed new light on the nature of the X(3872) particle.Peer reviewe
Search for invisible decays of the Higgs boson produced via vector boson fusion in proton-proton collisions at root s=13 TeV
- Author
- Aarrestad T
- Abbaneo D
- Abbiendi G
- Abbrescia M
- Abdelalim A
- Abdullin S
- Abercrombie D
- Abreu A
- Acharya H
- Acosta D
- Acosta HE
- Adam W
- Adamidis K
- Adams E
- Adams M
- Adams T
- Addesa F
- Adloff C
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- Yohay R
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- Yoon I
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- Yu D
- Yu G
- Yu I
- Yu Pr
- Yu S
- Yuan L
- Yuan S
- Yuldashev B
- Yumiceva F
- Yzquierdo AP
- Zabi A
- Zacharopoulou A
- Zahid S
- Zaleski S
- Zalewski P
- Zanetti M
- Zarubin A
- Zarucki M
- Zecchinelli A
- Zeinali M
- Zeuner W
- Zghiche A
- Zhang F
- Zhang H
- Zhang J
- Zhang L
- Zhang W
- Zhang Y
- Zhang Z
- Zhao J
- Zhizhin I
- Zhokin A
- Zhu R
- Ziemons T
- Zipper N
- Zoi I
- Zolkapli Z
- Zorbakir I
- Zorbilmez C
- Zotto P
- Zotz A
- Zou D
- Zou R
- Zucchetta A
- Zumerle G
- Zuo X
- Zuolo D
- Zygala L
- Álvarez CR
- Özçelik Ö
- Publication venue
- Publication date
- 01/01/2022
- Field of study
Search for dark matter produced in association with a Higgs boson decaying to a pair of bottom quarks in proton-proton collisions at root s=13TeV
- Author
- Aarrestad TK
- Abbaneo D
- Abbiendi G
- Abbrescia M
- Abdullah WATW
- Abdullin S
- Abercrombie D
- Acharya H
- Acosta D
- Acosta JG
- Adam W
- Adams E
- Adams MR
- Adams T
- Adloff C
- Adzic P
- Adán DP
- Afanasiev S
- Agapitos A
- Agarwal G
- Aggleton R
- Agram J-L
- Aguilar-Benitez M
- Ahmad A
- Ahmad M
- Ahmad WH
- Ahmed A
- Ahuja S
- Aime' C
- Akchurin N
- Akgun B
- Akpinar A
- Albajar C
- Albergo S
- Albert A
- Albrow M
- Aleksandrov A
- Alexander J
- Alhusseini M
- Alimena J
- Alison J
- Allen B
- Almond J
- Alonso AG
- Alvarez JDR
- Alverson G
- Alves GA
- Aly R
- Alyari M
- Amapane N
- Amaral SMSD
- Amendola C
- Amin N
- Amram O
- Amsler C
- Anagnostou G
- Anampa KH
- Anderson D
- Andrea J
- Andreev V
- Andreev Y
- Andrews MB
- Androsov K
- Angioni GLP
- Antchev G
- Antunovic Z
- Anuar AAB
- Apanasevich L
- Apollinari G
- Appelt E
- Apresyan A
- Apyan A
- Araujo M
- Arbelaez NV
- Arbol PMRD
- Arcaro D
- Arcidiacono R
- Arenton MW
- Argiro S
- Arneodo M
- Aruta C
- Asavapibhop B
- Asawatangtrakuldee C
- Asenov P
- Asghar MI
- Asilar E
- Askew A
- Asmuss P
- Atakisi IO
- Atanasov I
- Ather MW
- Attikis A
- Auffray E
- Aushev T
- Auzinger G
- Avati V
- Avery P
- Avila C
- Awan MIM
- Ayala E
- Ayala G
- Azarkin M
- Azhgirey I
- Aziz T
- Azzi P
- Azzurri P
- Baarmand MM
- Babaev A
- Babounikau I
- Bacchetta N
- Bachiller I
- Bachtis M
- Backhaus M
- Baden A
- Baechler J
- Bagliesi G
- Bahinipati S
- Baillon P
- Bainbridge R
- Bakas G
- Bakhshiansohi H
- Ball AH
- Ban Y
- Band R
- Bandyopadhyay H
- Banerjee S
- Banerjee S
- Banos LIE
- Bansal S
- Barbagli G
- Barberis E
- Bargassa P
- Baringer P
- Barnes VE
- Barney D
- Baron O
- Barrera CB
- Barrera CO
- Bartek R
- Bartosik N
- Bartók M
- Bastos D
- Battilana C
- Baty A
- Bauerdick LAT
- Baur S
- Baxter S
- Bayshev I
- Bean A
- Beauceron S
- Beaudette F
- Becerra DAS
- Bechtel J
- Bedoya CF
- Beghin D
- Behera PK
- Behera SC
- Behnke O
- Bein S
- Belforte S
- Bell KW
- Bellan R
- Belloni A
- Bellora A
- Belyaev A
- Belyaev A
- Benaglia A
- Benato L
- Bencze G
- Bendavid J
- Benecke A
- Benelli G
- Beni N
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- Özçelik Ö
- Publication venue
- Publication date
- 01/01/2018
- Field of study
A search for dark matter produced in association with a Higgs boson decaying to a pair of bottom quarks is performed in proton-proton collisions at a center-of-mass energy of 13 TeV collected with the CMS detector at the LHC. The analyzed data sample corresponds to an integrated luminosity of 35.9 fb(-1). The signal is characterized by a large missing transverse momentum recoiling against a bottom quark-antiquark system that has a large Lorentz boost. The number of events observed in the data is consistent with the standard model background prediction. Results are interpreted in terms of limits both on parameters of the type-2 two-Higgs doublet model extended by an additional light pseudoscalar boson a (2HDM+a) and on parameters of a baryonic Z simplified model. The 2HDM+a model is tested experimentally for the first time. For the baryonic Z model, the presented results constitute the most stringent constraints to date.Peer reviewe
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