58 research outputs found
A(c)(+) Production and Baryon-to-Meson Ratios in pp and p-Pb Collisions at root S-NN=5.02 TeV at the LHC
- Author
- A G Clai
- Acharya S
- Adamova D
- Adler A
- Adolfsson J
- Agnello M
- Agrawal N
- Ahammed Z
- Ahmad S
- Ahn SU
- Akbar Z
- Akindinov A
- Al-Turany M
- Albuquerque DSD
- Aleksandrov D
- Alessandro B
- Alfanda HM
- Alfaro Molina R
- Ali B
- Ali Y
- Alici A
- Alizadehvandchali N
- Alkin A
- Alme J
- Alt T
- Altenkamper L
- Altsybeev I
- Anaam MN
- Andrei C
- Andreou D
- Andronic A
- Angeletti M
- Anguelov V
- Anticic T
- Antinori F
- Antonioli P
- Apadula N
- Aphecetche L
- Appelshaeuser H
- Arcelli S
- Arnaldi R
- Arratia M
- Arsene IC
- Arslandok M
- Augustinus A
- Averbeck R
- Aziz S
- Azmi MD
- Badala A
- Baek YW
- Bai X
- Bailhache R
- Baillie O Villalobos
- Bala R
- Balbastre G Conesa
- Balbino A
- Baldisseri A
- Ball M
- Banerjee D
- Barbera R
- Barioglio L
- Barlou M
- Barnafoldi GG
- Barnby LS
- Barret V
- Barroso V Chibante
- Bartels C
- Barth K
- Bartsch E
- Baruffaldi F
- Bastid N
- Basu S
- Batigne G
- Batyunya B
- Bauri D
- Bazo Alba JL
- Bearden IG
- Beattie C
- Belikov I
- Bellini F
- Bellwied R
- Belokurova S
- Belyaev V
- Bencedi G
- Beole S
- Bercuci A
- Berdnikov Y
- Berdnikova A
- Berenyi D
- Bergmann L
- Besoiu MG
- Betev L
- Bhaduri PP
- Bhasin A
- Bhat IR
- Bhat MA
- Bhattacharjee B
- Bhattacharya P
- Bianchi A
- Bianchi L
- Bianchi N
- Bielcik J
- Bielcikova J
- Bilandzic A
- Biro G
- Biswas S
- Blair JT
- Blau D
- Blidaru MB
- Blume C
- Boca G
- Bock F
- Bogdanov A
- Boi S
- Bok J
- Boldizsar L
- Bolozdynya A
- Bombara M
- Bonomi G
- Borel H
- Borissov A
- Bossi H
- Botta E
- Bratrud L
- Braun-Munzinger P
- Bregant M
- Broz M
- Bruno GE
- Buckland MD
- Budnikov D
- Buesching H
- Bufalino S
- Bugnon O
- Buhler P
- Buncic P
- Buthelezi Z
- Butt JB
- Bysiak SA
- Caffarri D
- Caliva A
- Calvo Villar E
- Camacho JMM
- Camacho RS
- Camerini P
- Canedo FDM
- Capon AA
- Carnesecchi F
- Caron R
- Castellanos J Castillo
- Casula EAR
- Catalano F
- Chakraborty P
- Chandra S
- Chang W
- Chapeland S
- Chartier M
- Chattopadhyay S
- Chattopadhyay S
- Chauvin A
- Cheshkov C
- Cheynis B
- Chinellato DD
- Cho S
- Chochula P
- Christakoglou P
- Christensen CH
- Christiansen P
- Chujo T
- Cicalo C
- Cifarelli L
- Cindolo F
- Ciupek MR
- Cleymans J
- Colamaria F
- Colburn JS
- Colella D
- Collaboration ALICE
- Collu A
- Colocci M
- Concas M
- Contin G
- Contreras JG
- Cormier TM
- Corral G Herrera
- Cortese P
- Cosentino MR
- Costa F
- Costanza S
- Crochet P
- Cuautle E
- Cui P
- Cunqueiro L
- Da Costa H Pereira
- Da Silva AC Oliveira
- Dahms T
- Dainese A
- Damas FPA
- Danisch MC
- Danu A
- Das D
- Das I
- Das P
- Das P
- Das S
- Dash S
- De Caro A
- de Cataldo G
- De Cilladi L
- de Cuveland J
- De Falco A
- De Godoy DA Moreira
- De Gruttola D
- De Marco N
- De Martin C
- De Pasquale S
- De S
- Deb S
- Degenhardt HF
- Deja KR
- del Valle Z Conesa
- Delsanto S
- Deng W
- Dhankher P
- Di Bari D
- Di Mauro A
- Diaz RA
- Dietel T
- Dillenseger P
- Ding Y
- Divia R
- Dixit DU
- Djuvsland O
- Dmitrieva U
- Do J
- Dobrin A
- Doce O Vazquez
- Doenigus B
- Dordic O
- Dubey AK
- Dubla A
- Ducati MB Gay
- Dudi S
- Dukhishyam M
- Dupieux P
- Eder TM
- Ehlers RJ
- Eikeland VN
- Elia D
- Erazmus B
- Erhardt F
- Erokhin A
- Ersdal MR
- Espagnon B
- Eulisse G
- Evans D
- Evdokimov S
- Fabbietti L
- Faggin M
- Faivre J
- Fan F
- Fantoni A
- Fasel M
- Fecchio P
- Feliciello A
- Feofilov G
- Fernandez Tellez A
- Ferrero A
- Ferretti A
- Festanti A
- Feuillard VJG
- Figiel J
- Filchagin S
- Finogeev D
- Fionda FM
- Fiorenza G
- Flor F
- Flores AN
- Foertsch S
- Foka P
- Fokin S
- Fragiacomo E
- Fuchs U
- Furget C
- Furs A
- Gaardhoje JJ
- Gagliardi M
- Gago AM
- Gajdosova K Krizkova
- Gal A
- Galvan CD
- Ganoti P
- Garabatos C
- Garcia G Martinez
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- Garibli A
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- Gauger EF
- Germain M
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- Ghosh SK
- Giacalone M
- Gianotti P
- Girard M Fusco
- Giubellino P
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- Glaenzer AMC
- Glaessel P
- Gonzalez V
- Gonzalez-Trueba LH
- Gorbunov S
- Gorlich L
- Gotovac S
- Grabski V
- Graczykowski LK
- Graham KL
- Greiner L
- Grelli A
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- Grigoriev V
- Grigoryan A
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- Groettvik OS
- Grosa F
- Grosse-Oetringhaus JF
- Grosso R
- Guernane R
- Guilbaud M
- Guittiere M
- Gulbrandsen K
- Gunji T
- Gupta A
- Gupta R
- Guzman IB
- Haake R
- Habib MK
- Hadjidakis C
- Hamagaki H
- Hamar G
- Hamid M
- Hannigan R
- Haque MR
- Harlenderova A
- Harris JW
- Harton A
- Hasenbichler JA
- Hassan H
- Hatzifotiadou D
- Hauer P
- Havener LB
- Hayashi S
- Hechavarria ADC Bell
- Heckel ST
- Hellbaer E
- Helstrup H
- Herman T
- Hernandez EG
- Herrmann F
- Hetland KF
- Hillemanns H
- Hills C
- Hippolyte B
- Hohlweger B
- Honermann J
- Hong GH
- Horak D
- Hornung S
- Hosokawa R
- Hristov P
- Huang C
- Hughes C
- Huhn P
- Humanic TJ
- Hushnud H
- Husova LA
- Hussain N
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- Iddon JP
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- Inaba M
- Innocenti GM
- Ippolitov M
- Isakov A
- Islam MS
- Ivanov M
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- Izucheev V
- Jacak B
- Jacazio N
- Jacobs PM
- Jadlovska S
- Jadlovsky J
- Jaelani S
- Jahnke C
- Jakubowska MJ
- Janik MA
- Janson T
- Jercic M
- Jevons O
- Jin M
- Jonas F
- Jones PG
- Jung J
- Jung M
- Jusko A
- Kalinak P
- Kalweit A
- Kaplin V
- Kar S
- Karatovic D
- Karavichev O
- Karavicheva T
- Karczmarczyk P
- Karpechev E
- Kazantsev A
- Kebschull U
- Keidel R
- Keil M
- Ketzer B
- Khabanova Z
- Khan AM
- Khan M Mohisin
- Khan S
- Khanzadeev A
- Kharlov Y
- Khatun A
- Khuntia A
- Kileng B
- Kim B
- Kim D
- Kim DJ
- Kim EJ
- Kim H
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- Kim J
- Kim JS
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- Kirsch S
- Kisel I
- Kiselev S
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- Klay JL
- Klein J
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- Kleiner M
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- Kluge A
- Knospe AG
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- Konigstorfer SA
- Konopka PJ
- Kornakov G
- Koryciak SD
- Koska L
- Kovalenko O
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- Kowalski M
- Kralik I
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- Krzewicki M
- Kucera V
- Kuhn C
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- Margotti A
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- Marquard M
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- Masera M
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- Mathis AM
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- Matuoka PFT
- Matyja A
- Mayer C
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- Mechler AF
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- Melikyan Y
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- Mengke C
- Meninno E
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- Meres M
- Mhlanga S
- Miake Y
- Micheletti L
- Migliorin LC
- Mihaylov DL
- Mikhaylov K
- Mishra AN
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- Mohanty AP
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- Monzon I Leon
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- Mulligan JD
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- van der Kolk N
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- Varga D
- Varga Z
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- Willems GA
- Willsher E
- Windelband B
- Winn M
- Witt WE
- Wright JR
- Wu Y
- Xu R
- Yalcin S
- Yamaguchi Y
- Yamakawa K
- Yang S
- Yano S
- Yin Z
- Yokoyama H
- Yoo I-K
- Yoon JH
- Yuan S
- Yuncu A
- Yurchenko V
- Zaccolo V
- Zaman A
- Zampolli C
- Zanoli HJC
- Zardoshti N
- Zarochentsev A
- Zavada P
- Zaviyalov N
- Zbroszczyk H
- Zhalov M
- Zhang S
- Zhang X
- Zhang Y
- Zherebchevskii V
- Zhi Y
- Zhou D
- Zhou Y
- Zhu J
- Zhu Y
- Zichichi A
- Zinovjev G
- Zurlo N
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2021
- Field of study
The prompt production of the charm baryon \u39bc+ and the \u39bc+/D0 production ratios were measured at midrapidity with the ALICE detector in pp and p-Pb collisions at sNN=5.02 TeV. These new measurements show a clear decrease of the \u39bc+/D0 ratio with increasing transverse momentum (pT) in both collision systems in the range 2<12 GeV/c, exhibiting similarities with the light-flavor baryon-to-meson ratios p/\u3c0 and \u39b/KS0. At low pT, predictions that include additional color-reconnection mechanisms beyond the leading-color approximation, assume the existence of additional higher-mass charm-baryon states, or include hadronization via coalescence can describe the data, while predictions driven by charm-quark fragmentation processes measured in e+e- and e-p collisions significantly underestimate the data. The results presented in this Letter provide significant evidence that the established assumption of universality (colliding-system independence) of parton-to-hadron fragmentation is not sufficient to describe charm-baryon production in hadronic collisions at LHC energies
A(c)(+) Production and Baryon-to-Meson Ratios in pp and p-Pb Collisions at root S-NN=5.02 TeV at the LHC
- Author
- A G Clai
- Acharya S
- Adamova D
- Adler A
- Adolfsson J
- Agnello M
- Agrawal N
- Ahammed Z
- Ahmad S
- Ahn SU
- Akbar Z
- Akindinov A
- Al-Turany M
- Albuquerque DSD
- Aleksandrov D
- Alessandro B
- Alfanda HM
- Alfaro Molina R
- Ali B
- Ali Y
- Alici A
- Alizadehvandchali N
- Alkin A
- Alme J
- Alt T
- Altenkamper L
- Altsybeev I
- Anaam MN
- Andrei C
- Andreou D
- Andronic A
- Angeletti M
- Anguelov V
- Anticic T
- Antinori F
- Antonioli P
- Apadula N
- Aphecetche L
- Appelshaeuser H
- Arcelli S
- Arnaldi R
- Arratia M
- Arsene IC
- Arslandok M
- Augustinus A
- Averbeck R
- Aziz S
- Azmi MD
- Badala A
- Baek YW
- Bai X
- Bailhache R
- Baillie O Villalobos
- Bala R
- Balbastre G Conesa
- Balbino A
- Baldisseri A
- Ball M
- Banerjee D
- Barbera R
- Barioglio L
- Barlou M
- Barnafoldi GG
- Barnby LS
- Barret V
- Barroso V Chibante
- Bartels C
- Barth K
- Bartsch E
- Baruffaldi F
- Bastid N
- Basu S
- Batigne G
- Batyunya B
- Bauri D
- Bazo Alba JL
- Bearden IG
- Beattie C
- Belikov I
- Bellini F
- Bellwied R
- Belokurova S
- Belyaev V
- Bencedi G
- Beole S
- Bercuci A
- Berdnikov Y
- Berdnikova A
- Berenyi D
- Bergmann L
- Besoiu MG
- Betev L
- Bhaduri PP
- Bhasin A
- Bhat IR
- Bhat MA
- Bhattacharjee B
- Bhattacharya P
- Bianchi A
- Bianchi L
- Bianchi N
- Bielcik J
- Bielcikova J
- Bilandzic A
- Biro G
- Biswas S
- Blair JT
- Blau D
- Blidaru MB
- Blume C
- Boca G
- Bock F
- Bogdanov A
- Boi S
- Bok J
- Boldizsar L
- Bolozdynya A
- Bombara M
- Bonomi G
- Borel H
- Borissov A
- Bossi H
- Botta E
- Bratrud L
- Braun-Munzinger P
- Bregant M
- Broz M
- Bruno GE
- Buckland MD
- Budnikov D
- Buesching H
- Bufalino S
- Bugnon O
- Buhler P
- Buncic P
- Buthelezi Z
- Butt JB
- Bysiak SA
- Caffarri D
- Caliva A
- Calvo Villar E
- Camacho JMM
- Camacho RS
- Camerini P
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- Zanoli HJC
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- Zichichi A
- Zinovjev G
- Zurlo N
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2021
- Field of study
The prompt production of the charm baryon Λ_{c}^{+} and the Λ_{c}^{+}/D^{0} production ratios were measured at midrapidity with the ALICE detector in pp and p-Pb collisions at sqrt[s_{NN}]=5.02 TeV. These new measurements show a clear decrease of the Λ_{c}^{+}/D^{0} ratio with increasing transverse momentum (p_{T}) in both collision systems in the range 2<p_{T}<12 GeV/c, exhibiting similarities with the light-flavor baryon-to-meson ratios p/π and Λ/K_{S}^{0}. At low p_{T}, predictions that include additional color-reconnection mechanisms beyond the leading-color approximation, assume the existence of additional higher-mass charm-baryon states, or include hadronization via coalescence can describe the data, while predictions driven by charm-quark fragmentation processes measured in e^{+}e^{-} and e^{-}p collisions significantly underestimate the data. The results presented in this Letter provide significant evidence that the established assumption of universality (colliding-system independence) of parton-to-hadron fragmentation is not sufficient to describe charm-baryon production in hadronic collisions at LHC energies
Suppression in Pb-Pb Collisions at the LHC.
- Author
- Acharya S
- Adamová D
- Adler A
- Aglieri Rinella G
- Agnello M
- Agrawal N
- Ahammed Z
- Ahmad S
- Ahn SU
- Ahuja I
- Akindinov A
- Al-Turany M
- Aleksandrov D
- Alessandro B
- Alfanda HM
- Alfaro Molina R
- Ali B
- ALICE Collaboration
- Alici A
- Alizadehvandchali N
- Alkin A
- Alme J
- Alocco G
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The production of the ψ(2S) charmonium state was measured with ALICE in Pb-Pb collisions at sqrt[s_{NN}]=5.02 TeV, in the dimuon decay channel. A significant signal was observed for the first time at LHC energies down to zero transverse momentum, at forward rapidity (2.5<y<4). The measurement of the ratio of the inclusive production cross sections of the ψ(2S) and J/ψ resonances is reported as a function of the centrality of the collisions and of transverse momentum, in the region p_{T}<12 GeV/c. The results are compared with the corresponding measurements in pp collisions, by forming the double ratio [σ^{ψ(2S)}/σ^{J/ψ}]_{Pb-Pb}/[σ^{ψ(2S)}/σ^{J/ψ}]_{pp}. It is found that in Pb-Pb collisions the ψ(2S) is suppressed by a factor of ∼2 with respect to the J/ψ. The ψ(2S) nuclear modification factor R_{AA} was also obtained as a function of both centrality and p_{T}. The results show that the ψ(2S) resonance yield is strongly suppressed in Pb-Pb collisions, by a factor of up to ∼3 with respect to pp. Comparisons of cross section ratios with previous Super Proton Synchrotron findings by the NA50 experiment and of R_{AA} with higher-p_{T} results at LHC energy are also reported. These results and the corresponding comparisons with calculations of transport and statistical models address questions on the presence and properties of charmonium states in the quark-gluon plasma formed in nuclear collisions at the LHC
Measurement of prompt J/psi and beauty hadron production cross sections at mid-rapidity in pp collisions at root s=7 TeV
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- VYUSHIN A
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- WAGNER V
- WAN RZ
- WANG D
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- WATANABE K
- WEBER M
- WESSELS J
- WESTERHOFF U
- WIECHULA J
- WIKNE J
- WILDE MR
- WILK A
- WILK GA
- WILLIAMS C
- WINDELBAND BS
- YALDO CG
- YAMAGUCHI Y
- YANG HY
- YANG SM
- YASNOPOLSKY S
- YI JG
- YIN ZB
- YOO IK
- YOON J
- YU WL
- YUAN XB
- YUSHMANOV I
- ZACH C
- ZAMPOLLI C
- ZAPOROZHETS S
- ZAROCHENTSEV A
- ZAVADA P
- ZAVIYALOV N
- ZBROSZCZYK HP
- ZELNICEK P
- ZETINA LMM
- ZGURA SI
- ZHALOV M
- ZHANG HT
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- ZHOU FC
- ZHOU Y
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- ZYZAKBZ M
- Publication venue
- 'Springer Fachmedien Wiesbaden GmbH'
- Publication date
- 01/01/2012
- Field of study
The ALICE experiment at the LHC has studied J/psi production at mid-rapidity in pp collisions at root s = 7 TeV through its electron pair decay on a data sample corresponding to an integrated luminosity L-int = 5.6 nb(-1). The fraction of J/psi from the decay of long-lived beauty hadrons was determined for J/psi candidates with transverse momentum p(t) > 1,3 GeV/c and rapidity vertical bar y vertical bar 1.3 GeV/c, vertical bar y vertical bar 1.3 GeV/c and vertical bar y vertical bar 1.3 GeV/c, vertical bar y vertical bar < 0.9) = 1.46 +/- 0.38 (stat.)(-0.32)(+0.26) (syst.) mu b. The results are compared to QCD model predictions. The shape of the p(t) and y distributions of b-quarks predicted by perturbative QCD model calculations are used to extrapolate the measured cross section to derive the b (b) over bar pair total cross section and d sigma/dy at mid-rapidity
Underlying Event measurements in pp collisions at root s=0.9 and 7 TeV with the ALICE experiment at the LHC
- Author
- Abelev B
- Adamova D
- Adare AM
- Aggarwal M
- Agocs AG
- Agostinelli A
- Ahammed Z
- Ahmad A
- Ahmad N
- Ahn SU
- Akindinov A
- Alaniz EC
- Aleksandrov D
- Alessandro B
- Alici A
- Alkin A
- Alt T
- Altini V
- Altinpinar S
- Altsybeev I
- Andrei C
- Andronic A
- Anguelov V
- Anson CD
- Anticic T
- Antinori F
- Antonioli P
- Aphecetche LB
- Appelshauser H
- Arbor N
- Arcelli S
- Arend A
- Armesto N
- Arnaldi R
- Aronsson TR
- Arsene IC
- Arslandok M
- Asryan A
- Augustinus A
- Averbeck RP
- Avina EJA
- Awes T
- Aysto JH
- Azmi MD
- Bach MJ
- Badala A
- Baek YW
- Bailhache RM
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- Barret V
- Barroso VMC
- Bartke JG
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- Bearden IG
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- Beole S
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- Bercuci A
- Berdnikov Y
- Berenyi D
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- Betev L
- Bhasin A
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- Bilandzic A
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- Buthelezi EZ
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- Cai X
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- Casula EAR
- Catanescu V
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- Cervantes IAM
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- Christensen CH
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- Cicalo C
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- Colamaria F
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- Corral GAH
- Cortese P
- Cosentino MR
- Costa F
- Cotallo ME
- Crescio E
- Crochet P
- Cuautle E
- Cunqueiro L
- D'Erasmo G
- Dainese A
- Dalsgaard HH
- Danu A
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- Davalos AM
- de Barros G
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- Irfan M
- Ivan CG
- Ivanov A
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- Ivanov V
- Ivanytskyi O
- Jacholkowski AW
- Jacobs P
- Jancurova L
- Jang HJ
- Jangal SG
- Janik MA
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- Jayarathna S
- Jena S
- Jirden L
- Jones PG
- Jung HT
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- Jusko A
- Kaidalov A
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- Kalcher S
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- Kalisky M
- Kalliokoski TEA
- Kalweit AP
- Kanaki K
- Kang JH
- Kaplin V
- Karampatsos LX
- Karavichev O
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- Karpechev E
- Kazantsev A
- Kebschull UW
- Keidel R
- Khan MM
- Khan P
- Khan SA
- Khanzadeev A
- Kharlov Y
- Kileng B
- Kim B
- Kim DJ
- Kim DW
- Kim J
- Kim JS
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- Kim SH
- Kim SY
- Kim T
- Kirsch S
- Kisel I
- Kiselev S
- Kisiel AR
- Klay JL
- Klein J
- Klein-Bosing C
- Kliemant M
- Kluge A
- Knichel ML
- Koch K
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- Kolojvari A
- Kondratiev V
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- Konevskih A
- Korneev A
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- Kowalski M
- Kox S
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- Wilk GA
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- Yang HY
- Yang SM
- Yano S
- Yasnopolsky S
- Yi J
- Yin ZB
- Yokoyama H
- Yoo IK
- Yoon J
- Yu WL
- Yuan XB
- Yushmanov I
- Zach C
- Zampolli C
- Zaporozhets S
- Zarochentsev A
- Zavada P
- Zaviyalov N
- Zbroszczyk HP
- Zelnicek P
- Zetina LMM
- Zgura SI
- Zhalov M
- Zhang XM
- Zhou DC
- Zhou FC
- Zhou Y
- Zhu XR
- Zichichi A
- Zimmermann A
- Zinovjev G
- Zoccarato YD
- Zynovyev M
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2012
- Field of study
We present measurements of Underlying Event observables in pp collisions at root s = 0 : 9 and 7 TeV. The analysis is performed as a function of the highest charged-particle transverse momentum p(T),L-T in the event. Different regions are defined with respect to the azimuthal direction of the leading (highest transverse momentum) track: Toward, Transverse and Away. The Toward and Away regions collect the fragmentation products of the hardest partonic interaction. The Transverse region is expected to be most sensitive to the Underlying Event activity. The study is performed with charged particles above three different p(T) thresholds: 0.15, 0.5 and 1.0 GeV/c. In the Transverse region we observe an increase in the multiplicity of a factor 2-3 between the lower and higher collision energies, depending on the track p(T) threshold considered. Data are compared to PYTHIA 6.4, PYTHIA 8.1 and PHOJET. On average, all models considered underestimate the multiplicity and summed p(T) in the Transverse region by about 10-30%
Underlying Event measurements in pp collisions at root s=0.9 and 7 TeV with the ALICE experiment at the LHC
- Author
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- ADAMOVA D
- ADARE AM
- AGGARWAL M
- AGOCS AG
- AGOSTINELLI A
- AHAMMED Z
- AHMAD A
- AHMAD N
- AHN SU
- AKINDINOV A
- ALANIZ EC
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- ALESSANDRO B
- ALICI A
- ALKIN A
- ALT T
- ALTINI V
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- ANDREI C
- ANDRONIC A
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- ANSON CD
- ANTICIC T
- ANTINORI F
- ANTONIOLI P
- APHECETCHE LB
- APPELSHAUSER H
- ARBOR N
- ARCELLI S
- AREND A
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- ARSENE IC
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- AZMI MD
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- BEARDEN IG
- BECK H
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- VARGAS HL
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- VASILEIOU M
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- VASQUEZ MAS
- VECHERNIN V
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- WIKNE J
- WILDE MR
- WILK A
- WILK GA
- WILLIAMS C
- WINDELBAND BS
- YANG HY
- YANG SM
- YANO S
- YASNOPOLSKY S
- YI J
- YIN ZB
- YOKOYAMA H
- YOO IK
- YOON J
- YU WL
- YUAN XB
- YUSHMANOV I
- ZACH C
- ZAMPOLLI C
- ZAPOROZHETS S
- ZAROCHENTSEV A
- ZAVADA P
- ZAVIYALOV N
- ZBROSZCZYK HP
- ZELNICEK P
- ZETINA LMM
- ZGURA SI
- ZHALOV M
- ZHANG XM
- ZHOU DC
- ZHOU FC
- ZHOU Y
- ZHU XR
- ZICHICHI A
- ZIMMERMANN A
- ZINOVJEV G
- ZOCCARATO YD
- ZYNOVYEV M
- Publication venue
- 'Springer Fachmedien Wiesbaden GmbH'
- Publication date
- 01/01/2012
- Field of study
We present measurements of Underlying Event observables in pp collisions at root s = 0 : 9 and 7 TeV. The analysis is performed as a function of the highest charged-particle transverse momentum p(T),L-T in the event. Different regions are defined with respect to the azimuthal direction of the leading (highest transverse momentum) track: Toward, Transverse and Away. The Toward and Away regions collect the fragmentation products of the hardest partonic interaction. The Transverse region is expected to be most sensitive to the Underlying Event activity. The study is performed with charged particles above three different p(T) thresholds: 0.15, 0.5 and 1.0 GeV/c. In the Transverse region we observe an increase in the multiplicity of a factor 2-3 between the lower and higher collision energies, depending on the track p(T) threshold considered. Data are compared to PYTHIA 6.4, PYTHIA 8.1 and PHOJET. On average, all models considered underestimate the multiplicity and summed p(T) in the Transverse region by about 10-30%
Measurements of mixed harmonic cumulants in Pb-Pb collisions at root s(NN)=5.02 TeV
- Author
- Acharya S
- Adamova D
- Adler A
- Adolfsson J
- Agnello M
- Agrawal N
- Ahammed Z
- Ahmad S
- Ahn SU
- Akbar Z
- Akindinov A
- Al-Turany M
- Alba JLB
- Aleksandrov D
- Alessandro B
- Alfanda HM
- Ali B
- Ali Y
- Alici A
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- Alkin A
- Alme J
- Alt T
- Altenkamper L
- Altsybeev I
- Anaam MN
- Andrei C
- Andreou D
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- Anguelov V
- Antinori F
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- Appelshauser H
- Arcelli S
- Arnaldi R
- Arsene IC
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- Augustinus A
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- Aziz S
- Azmi MD
- Badala A
- Baek YW
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- Barlou M
- Barnafoldi GG
- Barnby LS
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- Bauri D
- Bearden IG
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- Belyaev V
- Bencedi G
- Beole S
- Bercuci A
- Berdnikov Y
- Berdnikova A
- Berenyi D
- Bergmann L
- Besoiu MG
- Betev L
- Bhaduri PP
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- Braun-Munzinger P
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- Bruno GE
- Buckland MD
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- Bysiak SA
- Caffarri D
- Cahuantzi MR
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- Camacho JMM
- Camacho RS
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- Zichichi A
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- Publication venue
- 'Elsevier BV'
- Publication date
- 01/01/2021
- Field of study
Correlations between moments of different flow coefficients are measured in Pb-Pb collisions at root s(NN) = 5.02 TeV recorded with the ALICE detector. These new measurements are based on multiparticle mixed harmonic cumulants calculated using charged particles in the pseudorapidity region vertical bar eta vertical bar < 0.8 with the transverse momentum range 0.2 < p(T) < 5.0 GeV/c. The centrality dependence of correlations between two flow coefficients as well as the correlations between three flow coefficients, both in terms of their second moments, are shown. In addition, a collection of mixed harmonic cumulants involving higher moments of v(2) and v(3) is measured for the first time, where the characteristic signature of negative, positive and negative signs of four-, six- and eight-particle cumulants are observed, respectively. The measurements are compared to the hydrodynamic calculations using iEBE-VISHNU with AMPT and TRENTo initial conditions. It is shown that the measurements carried out using the LHC Run 2 data in 2015 have the precision to explore the details of initial-state fluctuations and probe the nonlinear hydrodynamic response of v(2) and v(3) to their corresponding initial anisotropy coefficients epsilon(2) and epsilon(3). These new studies on correlations between three flow coefficients as well as correlations between higher moments of two different flow coefficients will pave the way to tighten constraints on initial-state models and help to extract precise information on the dynamic evolution of the hot and dense matter created in heavy-ion collisions at the LHC. (C) 2021 The Author. Published by Elsevier B.V
Underlying Event measurements in pp collisions at root s=0.9 and 7 TeV with the ALICE experiment at the LHC
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- Sukhorukov M
- Sultanov R
- Sumbera M
- Susa T
- Szarka I
- Szostak AK
- Tagridis C
- Takahashi J
- Takaki DJT
- Tauro A
- Telesca A
- Tellez AF
- TERREVOLI CRISTINA
- Thader JM
- Thomas D
- Thomas J
- Tieulent RN
- Timmins A
- Tlusty D
- Toia A
- Torii H
- Torres EL
- Toscano L
- Tosello F
- Traczyk T
- Truesdale DC
- Trzaska WH
- Tsuji T
- Tumkin A
- Turrisi R
- Tveter TS
- Ulery JG
- Ullaland K
- Ulrich J
- Uras A
- Urban J
- Urciuoli GM
- USAI GIANLUCA
- Uysal AK
- Vajzer M
- Vala M
- Vallero S
- van der Kolk N
- van Leeuwen M
- Vannucci L
- Vargas AD
- Vargas HL
- Varma R
- Vasileiou M
- Vasiliev A
- Vasquez MAS
- Vechernin V
- Velasquez AO
- Veldhoen M
- Venaruzzo M
- Vercellin E
- Vergara S
- Vernekohl DC
- Vernet R
- Verweij M
- Vickovic L
- Viesti G
- Vikhlyantsev O
- Vilakazi Z
- Villar EC
- Vinogradov A
- Vinogradov L
- Vinogradov Y
- Virgili T
- Viyogi Y
- Vodopianov A
- Voloshin K
- Voloshin S
- Volpe G
- von Haller B
- Vranic D
- Vrebekk G
- Vrlakova J
- Vulpescu B
- Vyushin A
- Vyvre PV
- Wagner B
- Wagner V
- Wan RZ
- Wang D
- Wang ML
- Wang YF
- Wang YP
- Watanabe K
- Wessels J
- Westerhoff U
- Wiechula J
- Wikne J
- Wilde MR
- Wilk A
- Wilk GA
- Williams C
- Windelband BS
- Yang HY
- Yang SM
- Yano S
- Yasnopolsky S
- Yi J
- Yin ZB
- Yokoyama H
- Yoo IK
- Yoon J
- Yu WL
- Yuan XB
- Yushmanov I
- Zach C
- Zampolli C
- Zaporozhets S
- Zarochentsev A
- Zavada P
- Zaviyalov N
- Zbroszczyk HP
- Zelnicek P
- Zetina LMM
- Zgura SI
- Zhalov M
- Zhang XM
- Zhou DC
- Zhou FC
- Zhou Y
- Zhu XR
- Zichichi A
- Zimmermann A
- Zinovjev G
- Zoccarato YD
- Zynovyev M.
- Publication venue
- Publication date
- 01/01/2012
- Field of study
We present measurements of Underlying Event observables in pp collisions at root s = 0 : 9 and 7 TeV. The analysis is performed as a function of the highest charged-particle transverse momentum p(T),L-T in the event. Different regions are defined with respect to the azimuthal direction of the leading (highest transverse momentum) track: Toward, Transverse and Away. The Toward and Away regions collect the fragmentation products of the hardest partonic interaction. The Transverse region is expected to be most sensitive to the Underlying Event activity. The study is performed with charged particles above three different p(T) thresholds: 0.15, 0.5 and 1.0 GeV/c. In the Transverse region we observe an increase in the multiplicity of a factor 2-3 between the lower and higher collision energies, depending on the track p(T) threshold considered. Data are compared to PYTHIA 6.4, PYTHIA 8.1 and PHOJET. On average, all models considered underestimate the multiplicity and summed p(T) in the Transverse region by about 10-30%
Multiplicity dependence of charged-particle jet production in pp collisions at root s=13 TeV
- Author
- Acharya S
- Adamova D
- Adler A
- Adolfsson J
- Agnello M
- Agrawal N
- Ahammed Z
- Ahmad S
- Ahn SU
- Ahuja I
- Akbar Z
- Akindinov A
- Al-Turany M
- Alam SN
- Aleksandrov D
- Alessandro B
- Alfanda HM
- Alfaro Molina R
- Ali B
- Ali Y
- Alici A
- Alizadehvandchali N
- Alkin A
- Alme J
- Alocco G
- Alt T
- Altsybeev I
- Anaam MN
- Andrei C
- Andreou D
- Andronic A
- Anguelov V
- Antinori F
- Antonioli P
- Anuj C
- Apadula N
- Aphecetche L
- Appelshaeuser H
- Arcelli S
- Arnaldi R
- Arsene IC
- Arslandok M
- Augustinus A
- Averbeck R
- Aziz S
- Azmi MD
- Badala A
- Baek YW
- Bai X
- Bailhache R
- Baillie OV
- Bailung Y
- Bala R
- Balbastre GC
- Balbino A
- Baldisseri A
- Balis B
- Banerjee D
- Banoo Z
- Barbera R
- Barioglio L
- Barlou M
- Barnafoldi GG
- Barnby LS
- Barret V
- Barroso VC
- Bartels C
- Barth K
- Bartsch E
- Baruffaldi F
- Bastid N
- Basu S
- Batigne G
- Battistini D
- Batyunya B
- Bauri D
- Bazo Alba JL
- Bearden IG
- Beattie C
- Becht P
- Belikov I
- Bellini F
- Bellwied R
- Belokurova S
- Belyaev V
- Bencedi G
- Beole S
- Bercuci A
- Berdnikov Y
- Berdnikova A
- Bergmann L
- Besoiu MG
- Betev L
- Bhaduri PP
- Bhasin A
- Bhat IR
- Bhat MA
- Bhattacharjee B
- Bhattacharya P
- Bianchi L
- Bianchi N
- Biernat J
- Bilandzic A
- Biro G
- Biswas S
- Blair JT
- Blau D
- Blidaru MB
- Blume C
- Boca G
- Bock F
- Bogdanov A
- Boi S
- Bok J
- Boldizsar L
- Bolozdynya A
- Bombara M
- Bond PM
- Bonomi G
- Borel H
- Borissov A
- Bossi H
- Botta E
- Bratrud L
- Braun-Munzinger P
- Bregant M
- Broz M
- Bruno GE
- Buckland MD
- Budnikov D
- Buesching H
- Bufalino S
- Bugnon O
- Buhler P
- Buthelezi Z
- Butt JB
- Bylinkin A
- Bysiak SA
- Cai M
- Caines H
- Caliva A
- Calvo Villar E
- Camacho JMM
- Camacho RS
- Canedo FDM
- Carabas M
- Carnesecchi F
- Caron R
- Castellanos JC
- Casula EAR
- Catalano F
- Chakaberia I
- Chakraborty P
- Chandra S
- Chapeland S
- Chartier M
- Chattopadhyay S
- Chavez TG
- Cheng T
- Cheshkov C
- Cheynis B
- Chinellato DD
- Cho S
- Chochula P
- Christakoglou P
- Christensen CH
- Christiansen P
- Chujo T
- Cicalo C
- Cifarelli L
- Cindolo F
- Ciupek MR
- Clai G
- Cleymans J
- Colburn JS
- Colella D
- Collaboration A
- Collu A
- Colocci M
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- Contin G
- Contreras JG
- Coquet ML
- Cormier TM
- Cortese P
- Cosentino MR
- Costanza S
- Crochet P
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- Cuautle E
- Cui P
- Cunqueiro L
- Da Costa HP
- Da Silva ACO
- Dainese A
- Danisch MC
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- de Cataldo G
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- de Cuveland J
- De Falco A
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- Vergara Limon S
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- Virgili T
- Vislavicius V
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- Witt WE
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- Wu Y
- Xu R
- Yadav AK
- Yalcin S
- Yamaguchi Y
- Yamakawa K
- Yang S
- Yano S
- Yin Z
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- Yoon JH
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- Zaccolo V
- Zampolli C
- Zanoli HJC
- Zanone F
- Zardoshti N
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- Zaviyalov N
- Zhalov M
- Zhang B
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- Zhou Y
- Zhu J
- Zhu Y
- Zinovjev G
- Zurlo N
- Publication venue
- Publication date
- 01/01/2022
- Field of study
Jet-associated deuteron production in pp collisions at s=13 TeV
- Author
- a
- A
- A Adler
- A Akindinov
- A Alici
- A Alkin
- A Augustinus
- A Badalà
- A Balbino
- A Baldisseri
- A Bercuci
- A Berdnikova
- A Bhasin
- A Bianchi
- A Bil
- A Bogdanov
- A Bolozdynya
- A Borissov
- A Chauvin
- A Collu
- A Dainese
- A Danu
- A De Caro
- A De Falco
- A Di Mauro
- A Dobrin
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- Publication venue
- Publication date
- 01/01/2021
- Field of study
Deuteron production in high-energy collisions is sensitive to the space–time evolution of the collision system, and is typically described by a coalescence mechanism. For the first time, we present results on jet-associated deuteron production in pp collisions at s=13 TeV, providing an opportunity to test the established picture for deuteron production in events with a hard scattering. Using a trigger particle with high transverse-momentum (pT>5 GeV/c) as a proxy for the presence of a jet at midrapidity, we observe a measurable population of deuterons being produced around the jet proxy. The associated deuteron yield measured in a narrow angular range around the trigger particle differs by 2.4–4.8 standard deviations from the uncorrelated background. The data are described by PYTHIA model calculations featuring baryon coalescence
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