54 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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- R. Santoroce
- R. Schicker bk
- R. Scottdb
- R. Shahoyan f
- R. Singaraju i
- R. Singh av
- R. Smakal ax
- R. Snellings ay
- R. Soltzde
- R. Stockab
- R. Tieulent bp
- R. Turrisi cj
- R. Varmacu
- R. Vernet di
- R. Wan as
- R.A. Ricci bz
- R.P. Scharenbergdh
- S. Aguilar Salazar h
- S. Altinpinar s
- S. Arcelli o
- S. B\uf6ttger v
- S. Bagnascon
- S. Beoleah
- S. Bose be
- S. Chapeland f
- S. Chattopadhyaybe
- S. Chattopadhyayi
- S. Coli n
- S. Dashn
- S. De i
- S. De Pasquale cd
- S. Di Libertoch
- S. Esumi bt
- S. Evrard f
- S. Filchagin bj
- S. Foertsch bl
- S. Fokin m
- S. Gadratac
- S. Gorbunovq
- S. Gotovaccp
- S. Grigoryan aq
- S. Huber s
- S. Jangal as
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- S. Kalcher q
- S. Kimcs
- S. Kirsch f
- S. Kiselevl
- S. Koxac
- S. Kushpil c
- S. Lindal bg
- S. Lohnf
- S. Masciocchi s
- S. Morettoy
- S. Muhuri i
- S. Navin an
- S. Nazarenko bj
- S. Nikolaev m
- S. Nikulin m
- S. Pal aj
- S. Pianocl
- S. Pochybova g
- S. Radomski bk
- S. Raniwala dg
- S. Rossegger f
- S. Rousseau bf
- S. Sadovskybc
- S. Sakai ct
- S. Sambyal av
- S. Sanocr
- S. Schreinerf
- S. Schuchmann ab
- S. Senyukov bx
- S. Serci cf
- S. Sharma av
- S. Vallero bk
- S. Vergara bw
- S. Voloshin at
- S. Yasnopolskiym
- S. Zaporozhets aq
- S.C. Leek
- S.H. Kimk
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- S.K. Pal i
- S.K. Prasadat
- S.P. Jayarathna ba
- S.S. R\ue4s\ue4nen af
- S.U. Ahnk
- T. Altq
- T. Anti\u2c7ci \ub4c x
- T. Aronsson d
- T. Breitner v
- T. Chujo bt
- T. Dietel ap
- T. Dobrowolski cg
- T. Gunji cr
- T. Horaguchi bt
- T. Kalliokoski af
- T. Karavicheva ck
- T. Krawutschkebk
- T. Pawlakcn
- T. Peitzmannbr
- T. Pocheptsov aq
- T. Samanta i
- T. Siemiarczukcg
- T. Sinha be
- T. Steinbeckv
- T. Sugitate dd
- T. Susa x
- T. Traczykcn
- T. Virgili cd
- T.B. Skaali bg
- 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. Tveterbg
- U. Frankenfelds
- U. Fuchsf
- U. Kebschull v
- U. Westerhoffap
- V. Altini r
- V. Anguelov v
- V. Barretak
- V. Canoa Roman f
- V. Catanescu u
- V. Chibante Barroso f
- V. Demanovbj
- V. Feketebi
- V. Grabski h
- V. Grigoriev bb
- V. Ivanov au
- V. Kaplinbb
- V. Kondratiev t
- V. Kushpil c
- V. Lafage bf
- V. Lenti ce
- V. Lindenstruth v
- V. Loginov bb
- V. Mankom
- V. Manzari ce
- V. Muccifora aw
- V. Nikolic x
- V. Nikulin au
- V. Paticchio ce
- V. Peskovf
- V. Petr\ue1\u2c7cek ax
- V. Posp\ued\u161il ax
- V. Puninbj
- V. Samsonov au
- V. Vechernin t
- V. Wagnerax
- V.R. Loggins at
- W. Carenaf
- W. Jungk
- W. Perytcn
- W. Rieglerf
- W.H. Trzaskaaf
- W.J. Parks
- X. Cai bm
- X. Li cz
- X. Lopezak
- X. Yuanbm
- X. Zhang bm
- X.-G. Lubk
- Y. Berdnikovau
- Y. Corrales Morales ah
- Y. Delgado Mercado bn
- Y. Hori cr
- Y. Kharlovbc
- Y. Kucheriaevm
- Y. Kwoncw
- Y. Le Bornec bf
- Y. Maobm
- Y. Martynov p
- Y. Miake bt
- Y. Pachmayerbk
- Y. Pestovdf
- Y. Schutzaa
- Y. Sibiriakm
- Y. Vinogradov bj
- Y. Wangbk
- Y. Wangbm
- Y. Zoccarato bp
- Y.P. Viyogi i
- Y.W. Baekk
- Z. Ahammed i
- Z. Buthelezi bl
- Z. Conesa del Valle aa
- Z. Vilakazi bl
- Z. Yinbm
- Z.L. Matthews an
- 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
Impact of jet-production data on the next-to-next-to-leading-order determination of HERAPDF2.0 parton distributions
- Author
- Abdullah WAT Wan
- Abt I
- Aggarwal R
- Andreev V
- Arratia M
- Aushev V
- Baghdasaryan A
- Baty A
- Begzsuren K
- Behnke O
- Belousov A
- Bertolin A
- Bloch I
- Boudry V
- Brandt G
- Brock I
- Brook NH
- Brugnera R
- Bruni A
- Buniatyan A
- Bussey PJ
- Bystritskaya L
- Caldwell A
- Campbell AJ
- Cantun Avila KB
- Catterall CD
- Cerny K
- Chekelian V
- Chen Z
- Chwastowski J
- Ciborowski J
- Ciesielski R
- Contreras JG
- Cooper-Sarkar AM
- Corradi M
- Currie J
- Cvach J
- Dainton JB
- Daum K
- Dementiev RK
- Deshpande A
- Diaconu C
- Dusini S
- Eckerlin G
- Egli S
- Elsen E
- Favart L
- Fedotov A
- Feltesse J
- Ferrando J
- Fleischer M
- Fomenko A
- Foster B
- Gal C
- Gallo E
- Gangadharan D
- Garfagnini A
- Gayler J
- Gehrmann T
- Gehrmann-De Ridder A
- Geiser A
- Gladilin LK
- Glover EWN
- Goerlich L
- Gogitidze N
- Golubkov Yu A
- Gouzevitch M
- Grab C
- Greenshaw T
- Grindhammer G
- Grzelak G
- Gwenlan C
- Haidt D
- Henderson RCW
- Hladky J
- Hochman D
- Hoffmann D
- Horisberger R
- Hreus T
- Huber F
- Huss A
- Jacobs PM
- Jacquet M
- Janssen T
- Jomhari NZ
- Jung AW
- Jung H
- Kadenko I
- Kapichine M
- Karshon U
- Katzy J
- Kaur P
- Kiesling C
- Klanner R
- Klein M
- Klein U
- Kleinwort C
- Klest HT
- Kogler R
- Korzhavina IA
- Kostka P
- Kovalchuk N
- Kretzschmar J
- Kruecker D
- Kruger K
- Kuze M
- Landon MPJ
- Lange W
- Laycock P
- Lee SH
- Levchenko BB
- Levonian S
- Levy A
- Li W
- Lin J
- Lipka K
- List B
- List J
- Lobodzinski B
- Loehr B
- Lohrmann E
- Long OR
- Longhin A
- Lorkowski F
- Lukina O Yu
- Makarenko I
- Malinovski E
- Malka J
- Martyn H-U
- Masciocchi S
- Maxfield SJ
- Mehta A
- Mendez L Cunqueiro
- Meyer AB
- Meyer J
- Mikocki S
- Mikuni VM
- Mondal MM
- Morgan T
- Morozov A
- Muller K
- Nachman B
- Nagano K
- Nam JD
- Naumann Th
- Newman PR
- Niebuhr C
- Niehues J
- Nowak G
- Olsson JE
- Onishchuk Yu
- Ozerov D
- Park S
- Pascaud C
- Patel GD
- Paul E
- Perez E
- Petrukhin A
- Picuric I
- Pidhurskyi I
- Pires J
- Pitzl D
- Polifka R
- Polini A
- Preins S
- Przybycien M
- Quintero A
- Rabbertz K
- Radescu V
- Raicevic N
- Ravdandorj T
- Reimer P
- Rizvi E
- Robmann P
- Roosen R
- Rostovtsev A
- Rotaru M
- Ruspa M
- Sankey DPC
- Sauter M
- Sauvan E
- Schmitt S
- Schmookler BA
- Schneekloth U
- Schoeffel L
- Schoening A
- Schoerner-Sadenius T
- Sefkow F
- Selyuzhenkov I
- Shchedrolosiev M
- Shcheglova LM
- Shushkevich S
- Skillicorn IO
- Slominski W
- Solano A
- Soloviev Y
- Sopicki P
- South D
- Spaskov V
- Specka A
- Stanco L
- Steder M
- Stefaniuk N
- Stella B
- Straumann U
- Sun C
- Surrow B
- Sutton MR
- Sykora T
- Thompson PD
- Tokushuku K
- Traynor D
- Tseepeldorj B
- Tu Z
- Turkot O
- Tymieniecka T
- Valkarova A
- Vallee C
- Van Mechelen P
- Verbytskyi A
- Wegener D
- Wichmann K
- Wing M
- Wunsch E
- Yamada S
- Yamazaki Y
- Zacek J
- Zarnecki AF
- Zenaiev O
- Zhang J
- Zhang Z
- Zlebcik R
- Zohrabyan H
- Zomer F
- Publication venue
- 'Springer Fachmedien Wiesbaden GmbH'
- Publication date
- 21/03/2022
- Field of study
The HERAPDF2.0 ensemble of parton distribution functions (PDFs) was introduced in 2015. The final stage is presented, a next-to-next-to-leading-order (NNLO) analysis of the HERA data on inclusive deep inelastic ep scattering together with jet data as published by the H1 and ZEUS collaborations. A perturbative QCD fit, simultaneously of αs(M2Z) and the PDFs, was performed with the result αs(M2Z)=0.1156±0.0011 (exp) +0.0001−0.0002 (model +parameterisation) ±0.0029 (scale). The PDF sets of HERAPDF2.0Jets NNLO were determined with separate fits using two fixed values of αs(M2Z), αs(M2Z)=0.1155 and 0.118, since the latter value was already chosen for the published HERAPDF2.0 NNLO analysis based on HERA inclusive DIS data only. The different sets of PDFs are presented, evaluated and compared. The consistency of the PDFs determined with and without the jet data demonstrates the consistency of HERA inclusive and jet-production cross-section data. The inclusion of the jet data reduced the uncertainty on the gluon PDF. Predictions based on the PDFs of HERAPDF2.0Jets NNLO give an excellent description of the jet-production data used as input
Evidence for tWZ production in proton-proton collisions at √s=13 TeV in multilepton final states
- Author
- Aarrestad TK
- Aarup Petersen H
- Abbaneo D
- Abbiendi G
- Abbott S
- Abbrescia M
- Abdullin S
- Abreu A
- Abu Zeid S
- Acharya H
- Acharya S
- Acosta D
- Adam W
- Adamidis K
- Adams E
- Adams MR
- Adams T
- Addesa FM
- Adloff C
- Adzic P
- Aebi D
- Afanasiev S
- Agapitos A
- Agarwal G
- Agram J-L
- Aguilar-Benitez M
- Agyel D
- Ahmad A
- Ahmad M
- Ahmed A
- Aimè C
- Ajmal S
- Akchurin N
- Akgun B
- Akpinar A
- Al Kadhim A
- Albert A
- Albrecht A
- Albrecht S
- Albrow M
- Alcaraz Maestre J
- Alcerro Alcerro LF
- Aldaya Martin M
- Aldá Júnior WL
- Aleksandrov A
- Alexander J
- Alhusseini M
- Alimena J
- Alison J
- Allmond B
- Ally D
- Almond J
- Alpana A
- Alsufyani B
- Alvarez Gonzalez B
- Alves Gallo Pereira M
- Alves GA
- Aly R
- Alyari M
- Amapane N
- Ambrozas M
- Ameen MM
- Amendola C
- Amoroso S
- Amram O
- Amsler C
- An S
- An Y
- Anagnostou G
- Andrea J
- Andreev V
- Andreev Y
- Andrejkovic JW
- Andrews MB
- Androsov K
- Anguiano J
- Antchev G
- Anthony D
- Antonello M
- Apollinari G
- Apparu D
- Appelt E
- Apresyan A
- Araujo M
- Aravind A
- Arcaro D
- Arcidiacono R
- Ardino R
- Argiro S
- Arneodo M
- Aruta C
- Asawatangtrakuldee C
- Asenov P
- Asghar MI
- Asilar E
- Askew A
- Assiouras P
- Atakisi IO
- Attikis A
- Auffray E
- Aushev T
- Auzinger G
- Avati V
- Avery P
- Avila C
- Awais A
- Awan MIM
- Ayala E
- Ayala G
- Aydilek O
- Azarkin M
- Aziz T
- Azzi P
- Azzurri P
- Baarmand MM
- Babaev A
- Babbar J
- Bacchetta N
- Bachtis M
- Backhaus M
- Baden A
- Baechler J
- Bagliesi G
- Bahinipati S
- Bainbridge R
- Bak G
- Bakas G
- Bakhshiansohi H
- Bakshi AS
- Bala A
- Baldenegro Barrera C
- Ball AH
- Ban Y
- Band R
- Bandyopadhyay H
- Banerjee S
- Banerjee S
- Bansal S
- Baradia S
- Barbagli G
- Barberis E
- Barbosa Trujillo DA
- Bardelli G
- Bargassa P
- Baringer P
- Barman S
- Barnes VE
- Barney D
- Baron O
- Barria P
- Barroso Ferreira Filho M
- Bartek R
- Bartosik N
- Bartók M
- Barzdukas A
- Basnet A
- Bastos D
- Battilana C
- Baty A
- Bauer G
- Bauerdick LAT
- Bautista I
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- Bayatmakou M
- Bean A
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- Becerril Gonzalez H
- Bedoya CF
- Behera PK
- Behera SC
- Behnke O
- Bein S
- Beirão Da Cruz E Silva C
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- Bestintzanos I
- Bethani A
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- Bilin B
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- Blinov V
- Bloch D
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- Bloom K
- Bluj M
- Blumenfeld B
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- Bocci A
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- Boletti A
- Bols ES
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- Bonilla J
- Boos E
- Boran F
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- Bornheim A
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- Buontempo S
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- Bury F
- Busson P
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- Butalla S
- Butler JN
- Butler PH
- Butz E
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- Cabrera A
- Cabrillo IJ
- Cacchio V
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- Cagnotta A
- Caillol C
- Cakir A
- Calandri A
- Calderon De La Barca Sanchez M
- Calderon A
- Cali IA
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- Calzaferri S
- Camaiani B
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- Camporesi T
- Candelise V
- Canelli MF
- Canepa A
- Cankocak K
- Capiluppi P
- Cappati A
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- Cardini A
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- Carrigan M
- Carrillo Montoya CA
- Cartiglia N
- Carvalho W
- Casarsa M
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- Castaldi R
- Castaneda Hernandez A
- Castells S
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- Castro A
- Cavallari F
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- Cavanaugh R
- Cazzaniga C
- Ceard L
- Ceccarelli R
- Cepeda M
- Cerati GB
- Cerci S
- Cerminara G
- Cerrada M
- Cerri O
- Cetorelli F
- Chabert EC
- Chahal GS
- Chandra S
- Chang P
- Chanon N
- Chao Y
- Charlot C
- Chatagnon P
- Chatterjee RM
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- Chatterjee S
- Chatzistavrou T
- Chaudhary G
- Chauhan S
- Chawla R
- Checchia P
- Chekhovsky V
- Chen GM
- Chen HS
- Chen KF
- Chen M
- Chen PS
- Chen X
- Chen Y
- Chen YM
- Chen Z
- Chen ZG
- Chenarani S
- Cheng C
- Cheng T
- Cherepanov V
- Chernyavskaya N
- Chertok M
- Cheung HWK
- Chhetri A
- Chiarito B
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- Chistov R
- Chitroda BK
- Chlebana F
- Choi J
- Choi J
- Choi M
- Choi S
- Chou JP
- Choudhary BC
- Christoforou K
- Chudasama R
- Chwalek T
- Ciangottini D
- Ciocci MA
- Cipriani M
- Citron M
- Cittolin S
- Ciulli V
- Civinini C
- Claes DR
- Clare R
- Clement E
- Clerbaux B
- Cockerill DJA
- Coelho E
- Colaleo A
- Coldham K
- Cole JE
- Colino N
- Collard C
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- Colombina F
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- Consuegra Rodríguez S
- Contardo D
- Conway J
- Cooke C
- Cooper SI
- Cooperstein S
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- Correia Silva G
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- Costa S
- Coubez X
- Couderc F
- Cousins R
- Covarelli R
- Cox B
- Cox PT
- Cranshaw DJ
- Creanza D
- Cremaldi LM
- Cremonesi M
- Crossman B
- Csanád M
- Csorgo T
- Cuevas J
- Cuffiani M
- Cumalat JP
- Cummings G
- Cunqueiro Mendez L
- Cussans D
- Cutts D
- Czellar S
- D'Alessandro R
- D'Alfonso M
- D'Amante V
- D'Anzi B
- d'Enterria D
- D'Hondt J
- Da Costa EM
- Da Silveira GG
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- Dallavalle GM
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- Damas F
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- Dancu JS
- Danilov M
- Dansana S
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- Dasu S
- Datta A
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- Davies G
- Davies J
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- Davis J
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- De Bruyn I
- De Coen M
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- De Guio F
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- De Jesus Damiao D
- De La Cruz B
- De La Cruz-Burelo E
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- De Leo K
- De Moor A
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- De Roeck A
- De Silva M
- de Trocóniz JF
- De Wit A
- Defranchis MM
- Deile M
- Dejardin M
- Del Burgo R
- Del Re D
- Delaere C
- Delannoy AG
- Delcourt M
- Delgado Peris A
- Dell'Orso R
- Della Negra M
- Della Ricca G
- Demaria N
- Demina R
- Demiragli Z
- Demiroglu ZS
- Denegri D
- Depasse P
- Dermenev A
- Dewanjee RK
- Dezoort G
- Dharmaratna WGD
- Dhingra N
- Di Florio A
- Di Marco E
- Di Mattia A
- Diaz D
- Dickinson J
- Diekmann S
- Diemoz M
- Dierlamm A
- Dildick S
- Dilsiz K
- Dimitrov A
- Dimova T
- Dinardo ME
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- Diotalevi T
- Dissertori G
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- Dittmer S
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- Dobur D
- Dodonova A
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- Dolek F
- Dolen J
- Dominguez A
- Donato S
- Donegà M
- Donertas IS
- Dordevic M
- Dorigo T
- Doroba K
- Dorsett A
- Dozen C
- Dragicevic M
- Dreimanis K
- Droll A
- Druzhkin D
- Duarte Campderros J
- Duarte J
- Dube S
- Dubinin M
- Dudko L
- Dugad S
- Dulemba JL
- Dumanoglu I
- Durkin LS
- Dutta I
- Dutta S
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- Yuldashev BS
- Yusuff I
- Zabi A
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- Zuolo D
- Zygala L
- Publication venue
- Elsevier BV
- Publication date
- 21/06/2024
- Field of study
Data availability - https://www.sciencedirect.com/science/article/pii/S0370269324003733?via%3Dihub#dav0001 [Release and preservation of data used by the CMS Collaboration as the basis for publications is guided by the CMS data preservation, re-use and open access policy (https://cms-docdb.cern.ch/cgi-bin/PublicDocDB/RetrieveFile?docid=6032&filename=CMSDataPolicyV1.2.pdf&version=2)]The first evidence for the standard model production of a top quark in association with a W boson and a Z boson is reported. The measurement is performed in multilepton final states, where the Z boson is reconstructed via its decays to electron or muon pairs. At least one W boson, associated or from top quark decay, decays leptonically, too. The analysed data were recorded by the CMS experiment at the CERN LHC in 2016–2018 in proton-proton collisions at √s=13 TeV, and correspond to an integrated luminosity of 138 fb−1. The measured cross section is 354±54(stat)±95(syst) fb, and corresponds to a statistical significance of 3.4 standard deviations.SCOAP
Measurement of the Higgs boson production via vector boson fusion and its decay into bottom quarks in proton-proton collisions at s = 13 TeV
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- Aarup Petersen H
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- Publication venue
- Springer Nature on behalf of SISSA
- Publication date
- 30/01/2024
- Field of study
A preprint version of the article is available at arXiv:2308.01253v2 [hep-ex], https://arxiv.org/abs/2308.01253v2 . Comments: Replaced with the published version. Added the journal reference and the DOI. All the figures and tables can be found at https://cms-results.web.cern.ch/cms-results/public-results/publications/HIG-22-009 (CMS Public Pages). Report number: CMS-HIG-22-009, CERN-EP-2023-110.A measurement of the Higgs boson (H) production via vector boson fusion (VBF) and its decay into a bottom quark-antiquark pair (bb¯) is presented using proton-proton collision data recorded by the CMS experiment at s√ = 13 TeV and corresponding to an integrated luminosity of 90.8 fb−1. Treating the gluon-gluon fusion process as a background and constraining its rate to the value expected in the standard model (SM) within uncertainties, the signal strength of the VBF process, defined as the ratio of the observed signal rate to that predicted by the SM, is measured to be μqqHHbb¯ = 1.01 +0.55−0.46. The VBF signal is observed with a significance of 2.4 standard deviations relative to the background prediction, while the expected significance is 2.7 standard deviations. Considering inclusive Higgs boson production and decay into bottom quarks, the signal strength is measured to be μincl.Hbb¯ = 0.99 +0.48−0.41, corresponding to an observed (expected) significance of 2.6 (2.9) standard deviations.SCOAP3, STFC; Marie-Curie program and the European Research Council and Horizon 2020 Gran
Search for long-lived heavy neutral leptons with lepton flavour conserving or violating decays to a jet and a charged lepton
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- Publication venue
- Springer Nature on behalf of SISSA
- Publication date
- 19/03/2024
- Field of study
A preprint version of the article is available at arXiv:2312.07484v3 [hep-ex], https://arxiv.org/abs/2312.07484 . Comments: Replaced with the published version. Added the journal reference and the DOI. All the figures and tables can be found at https://cms-results.web.cern.ch/cms-results/public-results/publications/EXO-21-013 (CMS Public Pages)A search for long-lived heavy neutral leptons (HNLs) is presented, which considers the hadronic final state and coupling scenarios involving all three lepton generations in the 2-20 GeV HNL mass range for the first time. Events comprising two leptons (electrons or muons) and jets are analyzed in a data sample of proton-proton collisions, recorded with the CMS experiment at the CERN LHC at a centre-of-mass energy of 13 TeV, corresponding to an integrated luminosity of 138 fb−1. A novel jet tagger, based on a deep neural network, has been developed to identify jets from an HNL decay using various features of the jet and its constituent particles. The network output can be used as a powerful discriminating tool to probe a broad range of HNL lifetimes and masses. Contributions from background processes are determined from data. No excess of events in data over the expected background is observed. Upper limits on the HNL production cross section are derived as functions of the HNL mass and the three coupling strengths VℓN to each lepton generation ℓ and presented as exclusion limits in the coupling-mass plane, as lower limits on the HNL lifetime, and on the HNL mass. In this search, the most stringent limit on the coupling strength is obtained for pure muon coupling scenarios; values of |VμN|2 > 5 (4) × 10−7 are excluded for Dirac (Majorana) HNLs with a mass of 10 GeV at a confidence level of 95% that correspond to proper decay lengths of 17 (10) mm.SCOAP3
Search for direct production of GeV-scale resonances decaying to a pair of muons in proton-proton collisions at s = 13 TeV
- Author
- Aarrestad TK
- Aarup Petersen H
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- Abbiendi G
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- Publication venue
- Springer Nature on behalf of SISSA
- Publication date
- 30/11/2023
- Field of study
A preprint version of the article is available at arXiv:2309.16003v2 [hep-ex], https://arxiv.org/abs/2309.16003v2 . Comments: Replaced with the published version. Added the journal reference and the DOI. All the figures and tables, including additional supplementary figures, can be found at https://cms-results.web.cern.ch/cms-results/public-results/publications/EXO-21-005 (CMS Public Pages). Report number: CMS-EXO-21-005, CERN-EP-2023-165.A search for direct production of low-mass dimuon resonances is performed using s√ = 13 TeV proton-proton collision data collected by the CMS experiment during the 2017-2018 operation of the CERN LHC with an integrated luminosity of 96.6 fb−1. The search exploits a dedicated high-rate trigger stream that records events with two muons with transverse momenta as low as 3 GeV but does not include the full event information. The search is performed by looking for narrow peaks in the dimuon mass spectrum in the ranges of 1.1-2.6 GeV and 4.2-7.9 GeV. No significant excess of events above the expectation from the standard model background is observed. Model-independent limits on production rates of dimuon resonances within the experimental fiducial acceptance are set. Competitive or world's best limits are set at 90% confidence level for a minimal dark photon model and for a scenario with two Higgs doublets and an extra complex scalar singlet (2HDM+S). Values of the squared kinetic mixing coefficient ε2 in the dark photon model above 10−6 are excluded over most of the mass range of the search. In the 2HDM+S, values of the mixing angle sin(θH) above 0.08 are excluded over most of the mass range of the search with a fixed ratio of the Higgs doublets vacuum expectation tanβ = 0.5.SCOAP3
Search for W′ bosons decaying to a top and a bottom quark in leptonic final states in proton-proton collisions at s = 13 TeV
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- Aarrestad TK
- Aarup Petersen H
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- Publication venue
- Springer Nature
- Publication date
- 05/04/2024
- Field of study
A preprint version of the article is available at arXiv:2310.19893v1 [hep-ex], https://arxiv.org/abs/2310.19893v1 . Comments: Submitted to the Journal of High Energy Physics. All figures and tables can be found at https://cms-results.web.cern.ch/cms-results/public-results/publications/B2G-20-012 (CMS Public Pages). Report number: CMS-B2G-20-012, CERN-EP-2023-213.A search for W' bosons decaying to a top and a bottom quark in final states including an electron or a muon is performed with the CMS detector at the LHC. The analyzed data correspond to an integrated luminosity of 138 fb^{-1} of proton-proton collisions at a center-of-mass energy of 13 Tev. Good agreement with the standard model expectation is observed and no evidence for the existence of the W' boson is found over the mass range examined. The largest observed deviation from the standard model expectation is found for a W' boson mass (mW′) hypothesis of 3.8 TeV with a relative decay width of 1%, with a local (global) significance of 2.6 (2.0) standard deviations. Upper limits on the production cross sections of W' bosons decaying to a top and a bottom quark are set. Left- and right-handed W' bosons with mW′ below 3.9 and 4.3 TeV, respectively, are excluded at the 95% confidence level, under the assumption that the new particle has a narrow decay width. Limits are also set for relative decay widths up to 30%. These are the most stringent limits to date on this W' boson decay channel.SCOAP3
Measurement of energy correlators inside jets and determination of the strong coupling αS(mZ)
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- Publication venue
- American Physical Society (APS)
- Publication date
- 14/08/2024
- Field of study
A preprint version of this article is available at arXiv:2402.13864v2 [hep-ex], https://arxiv.org/abs/2402.13864 . Comments: Replaced with the published version. Added the journal reference and the DOI. All the figures and tables can be found at https://cms-results.web.cern.ch/cms-results/public-results/publications/SMP-22-015 (CMS Public Pages). Report number: CMS-SMP-22-015, CERN-EP-2024-010 .Energy correlators that describe energy-weighted distances between two or three particles in a hadronic jet are measured using an event sample of √ = 13 TeV proton-proton collisions collected by the CMS experiment and corresponding to an integrated luminosity of 36.3 fb^−1. The measured distributions are consistent with the trends in the simulation that reveal two key features of the strong interaction: confinement and asymptotic freedom. By comparing the ratio of the measured three- and two-particle energy correlator distributions with theoretical calculations that resum collinear emissions at approximate next-to-next-to-leading-logarithmic accuracy matched to a next-to-leading-order calculation, the strong coupling is determined at the boson mass: () = 0.1229+0.0040 −0.0050, the most precise () value obtained using jet substructure observables.SCOAP3
Search for new Higgs bosons via same-sign top quark pair production in association with a jet in proton-proton collisions at √s = 13 TeV
- Author
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- Sharma A
- Sharma A
- Sharma A
- Sharma R
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- Sharma V
- Shchedrolosiev M
- Shchelina K
- Sheldon P
- Sheokand T
- Shepherd-Themistocleous CH
- Sheplock J
- Shevelev A
- Shi K
- Shi Z
- Shmatov S
- Shopova M
- Shukla R
- Shulha S
- Shumka E
- Shvetsov I
- Si W
- Siado JE
- Siamarkou E
- Siikonen H
- Sikdar AK
- Sikler F
- Silva P
- Silvestris L
- Simkina P
- Simone FM
- Simonetto F
- Simonis HJ
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- Singh JB
- Singla A
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- Siroli GP
- Siviero F
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- Smirnov V
- Smith C
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- Smith VJ
- Smith WH
- Snyder C
- Soeiro M
- Soffi L
- Soha A
- Sola V
- Solano A
- Somalwar S
- Sommerhalder M
- Sonawane M
- Song JN
- Sonnadara DUJ
- Sorrentino G
- Sosa Ricardo RE
- Sosnov D
- Soto Rodríguez A
- Spagnolo P
- Spah JL
- Spanier S
- Sperka D
- Sphicas P
- Spiegel L
- Spiga D
- Spiropulu M
- Spitzbart D
- Srimanobhas N
- Stadie H
- Stafford D
- Stahl Leiton AG
- Stahl A
- Staiano A
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- Strologas J
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- Su XF
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- Sulimov V
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- Summers S
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- Sznajder A
- Sánchez Hernández A
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- Tabarelli de Fatis T
- Tabb W
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- Takahashi Y
- Tali B
- Taliercio A
- Tamulaitis G
- Tani L
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- Tapper A
- Tarabini A
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- Taus R
- Tavernier S
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- Townsend A
- Tramontano R
- Tran NV
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- Trevisani N
- Tricomi A
- Triossi A
- Trocino D
- Tropea P
- Tsai LS
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- Tsatsos A
- Tsipolitis G
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- Usai E
- Uslan E
- Uttley GP
- Uvarov L
- Uzunian A
- Vaandering EW
- Vage LH
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- Vai I
- Valencia Palomo L
- Valsecchi D
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- Van Onsem GP
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- Wulff JW
- Wulz C-E
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- Wyslouch B
- Würthwein F
- Xiang Y
- Xiao J
- Xiao M
- Xie S
- Xie W
- Yagil A
- Yalvac M
- Yan F
- Yan X
- Yanes E
- Yang H
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- Yang UK
- Yang Y
- Yang YC
- Yao Y
- Yarar H
- Yates BR
- Yazgan E
- Ye Z
- Yi K
- Yi R
- Yigitbasi E
- Yockey H
- Yohay R
- Yoo HD
- Yoo J
- Yoo J
- Yoon I
- You Z
- Yu D
- Yu I
- Yu SS
- Yuan L
- Yuan S
- Yuldashev BS
- Yusuff I
- Zabi A
- Zabolotny W
- Zacharopoulou A
- Zaleski S
- Zalewski P
- Zanetti M
- Zarubin A
- Zarucki M
- Zaza A
- Zecchinelli AG
- Zehetner P
- Zeinali M
- Zejdl P
- Zeuner WD
- Zghiche A
- Zhang F
- Zhang H
- Zhang J
- Zhang L
- Zhang W
- Zhang Y
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- Zhizhin I
- Zhokin A
- Zhou C
- Zhu RY
- Ziemons T
- Zilizi G
- Zimermmane Castro Santos A
- Zipper N
- Zisopoulos I
- Zoi I
- Zolkapli Z
- Zorbakir IS
- Zorbilmez C
- Zotto P
- Zotz A
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- Zucchetta A
- Zumerle G
- Zuo X
- Zuolo D
- Zygala L
- Publication venue
- Elsevier
- Publication date
- 02/02/2024
- Field of study
Data availability:
Release and preservation of data used by the CMS Collaboration as the basis for publications is guided by the CMS policy as stated in “CMS data preservation, re-use and open access policy” available online at: https://cms-docdb.cern.ch/cgi-bin/PublicDocDB/RetrieveFile?docid=6032&filename=CMSDataPolicyV1.2.pdf&version=2 .A preprint of this article is available online at arXiv:2311.03261v2 [hep-ex] https://arxiv.org/abs/2311.03261v2 . Comments: Replaced with the published version. Added the journal reference and the DOI. All the figures and tables can be found at https://cms-results.web.cern.ch/cms-results/public-results/publications/TOP-22-010 (CMS Public Pages)A search is presented for new Higgs bosons in proton-proton (pp) collision events in which a same-sign top quark pair is produced in association with a jet, via the pp → tH/A → tt¯c and pp → tH/A → tt¯u processes. Here, H and A represent the extra scalar and pseudoscalar boson, respectively, of the second Higgs doublet in the generalized two-Higgs-doublet model (g2HDM). The search is based on pp collision data collected at a center-of-mass energy of 13 TeV with the CMS detector at the LHC, corresponding to an integrated luminosity of 138 fb−1. Final states with a same-sign lepton pair in association with jets and missing transverse momentum are considered. New Higgs bosons in the 200-1000 GeV mass range and new Yukawa couplings between 0.1 and 1.0 are targeted in the search, for scenarios in which either H or A appear alone, or in which they coexist and interfere. No significant excess above the standard model prediction is observed. Exclusion limits are derived in the context of the g2HDM.SCOAP3
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