22 research outputs found
First measurement of <math><msubsup><mi mathvariant="normal">Λ</mi><mrow><mi>c</mi></mrow><mo>+</mo></msubsup></math> production down to <math><mrow><msub><mi>p</mi><mi>T</mi></msub><mo>=</mo><mn>0</mn></mrow></math> in <math><mrow><mi>p</mi><mi>p</mi></mrow></math> and <math><mi>p</mi></math>-Pb collisions at <math><mrow><msqrt><msub><mi>s</mi><mrow><mi>N</mi><mi>N</mi></mrow></msub></msqrt><mo>=</mo><mn>5.02</mn></mrow></math> TeV
- Author
- Acharya S
- Adamová D
- Adler A
- Aglieri Rinella G
- Agnello M
- Agrawal N
- Ahammed Z
- Ahmad S
- Ahn S.U
- Ahuja I
- Akindinov A
- Al-Turany M
- Aleksandrov D
- Alessandro B
- Alfanda H.M
- Alfaro Molina R
- Ali B
- Alici A
- Alizadehvandchali N
- Alkin A
- Alme J
- Alocco G
- Alt T
- Altsybeev I
- Anaam M.N
- Andrei C
- Andronic A
- Anguelov V
- Antinori F
- Antonioli P
- Apadula N
- Aphecetche L
- Appelshäuser H
- Arata C
- Arcelli S
- Aresti M
- Arnaldi R
- Arneiro J.G.M.C.A
- Arsene I.C
- Arslandok M
- Augustinus A
- Averbeck R
- Azmi M.D
- Badalà A
- Bae J
- Baek Y.W
- Bai X
- Bailhache R
- Bailung Y
- Balbino A
- Baldisseri A
- Balis B
- Banerjee D
- Banoo Z
- Barbera R
- Barile F
- Barioglio L
- Barlou M
- Barnaföldi G.G
- Barnby L.S
- Barret V
- Barreto L
- Bartels C
- Barth K
- Bartsch E
- Bastid N
- Basu S
- Batigne G
- Battistini D
- Batyunya B
- Bauri D
- Bazo Alba J.L
- Bearden I.G
- Beattie C
- Becht P
- Behera D
- Belikov I
- Bell Hechavarria A.D.C
- Bellini F
- Bellwied R
- Belokurova S
- Belyaev V
- Bencedi G
- Beole S
- Bercuci A
- Berdnikov Y
- Berdnikova A
- Bergmann L
- Besoiu M.G
- Betev L
- Bhaduri P.P
- Bhasin A
- Bhat M.A
- Bhattacharjee B
- Bianchi L
- Bianchi N
- Bielčík J
- Bielčíková J
- Biernat J
- Bigot A.P
- Bilandzic A
- Biro G
- Biswas S
- Bize N
- Blair J.T
- Blau D
- Blidaru M.B
- Bluhme N
- Blume C
- Boca G
- Bock F
- Bodova T
- Bogdanov A
- Boi S
- Bok J
- Boldizsár L
- Bolozdynya A
- Bombara M
- Bond P.M
- Bonomi G
- Borel H
- Borissov A
- Borquez Carcamo A.G
- Bossi H
- Botta E
- Bouziani Y.E.M
- Bratrud L
- Braun-Munzinger P
- Bregant M
- Broz M
- Bruno G.E
- Buckland M.D
- Budnikov D
- Buesching H
- Bufalino S
- Bugnon O
- Buhler P
- Buthelezi Z
- Bysiak S.A
- Cai M
- Caines H
- Caliva A
- Calvo Villar E
- Camacho J.M.M
- Camerini P
- Canedo F.D.M
- Carabas M
- Carballo A.A
- Carnesecchi F
- Caron R
- Carvalho L.A.D
- Castillo Castellanos J
- Catalano F
- Ceballos Sanchez C
- Chakaberia I
- Chakraborty P
- Chandra S
- Chapeland S
- Chartier M
- Chattopadhyay S
- Chattopadhyay S
- Chavez T.G
- Cheng T
- Cheshkov C
- Cheynis B
- Chibante Barroso V
- Chinellato D.D
- Chizzali E.S
- Cho J
- Cho S
- Chochula P
- Christakoglou P
- Christensen C.H
- Christiansen P
- Chujo T
- Ciacco M
- Cicalo C
- Cindolo F
- Ciupek M.R
- Clai G
- Colamaria F
- Colburn J.S
- Colella D
- Colocci M
- Concas M
- Conesa Balbastre G
- Conesa del Valle Z
- Contin G
- Contreras J.G
- Coquet M.L
- Cormier T.M
- Cortese P
- Cosentino M.R
- Costa F
- Costanza S
- Cot C
- Crkovská J
- Crochet P
- Cruz-Torres R
- Cuautle E
- Cui P
- Dainese A
- Danisch M.C
- Danu A
- Das P
- Das P
- Das S
- Dash A.R
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- de Caro A
- de Cataldo G
- de Cuveland J
- de Falco A
- de Gruttola D
- de Marco N
- de Martin C
- de Pasquale S
- Deb S
- Debski R.J
- Deja K.R
- del Grande R
- Dello Stritto L
- Deng W
- Dhankher P
- Di Bari D
- Di Mauro A
- Diaz R.A
- Dietel T
- Ding Y
- Divià R
- Dixit D.U
- Djuvsland Ø
- Dmitrieva U
- Dobrin A
- Dubinski J.M
- Dubla A
- Dudi S
- Dupieux P
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- Dönigus B
- Eder T.M
- Ehlers R.J
- Eikeland V.N
- Eisenhut F
- Elia D
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- Ercolessi F
- Erhardt F
- Ersdal M.R
- Espagnon B
- Eulisse G
- Evans D
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- Fabbietti L
- Faggin M
- Faivre J
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- Fantoni A
- Fasel M
- Fecchio P
- Feliciello A
- Feofilov G
- Fernández Téllez A
- Ferrandi L
- Ferrer M.B
- Ferrero A
- Ferrero C
- Ferretti A
- Feuillard V.J.G
- Filova V
- Finogeev D
- Fionda F.M
- Flor F
- Flores A.N
- Foertsch S
- Fokin I
- Fokin S
- Fragiacomo E
- Frajna E
- Fuchs U
- Funicello N
- Furget C
- Furs A
- Fusayasu T
- Gaardhøje J.J
- Gagliardi M
- Gago A.M
- Galvan C.D
- Gangadharan D.R
- Ganoti P
- Garabatos C
- Garcia J.R.A
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- Gay Ducati M.B
- Germain M
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- Ghosh C
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- Gonzalez V
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- Gotovac S
- Grabski V
- Graczykowski L.K
- Grecka E
- Grelli A
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- Grigoriev V
- Grigoryan S
- Grosa F
- Gross-Bolting S.J
- Grosse-Oetringhaus J.F
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- Guardiano G.G
- Guernane R
- Guilbaud M
- Gulbrandsen K
- Gundem T
- Gunji T
- Guo W
- Gupta A
- Gupta R
- Guzman S.P
- Gyulai L
- Habib M.K
- Hadjidakis C
- Haider F.U
- Hamagaki H
- Hamdi A
- Hamid M
- Han Y
- Hannigan R
- Haque M.R
- Harris J.W
- Harton A
- Hassan H
- Hatzifotiadou D
- Hauer P
- Havener L.B
- Heckel S.T
- Hellbär E
- Helstrup H
- Hemmer M
- Herman T
- Herrera Corral G
- Herrmann F
- Herrmann S
- Hetland K.F
- Heybeck B
- Hillemanns H
- Hills C
- Hippolyte B
- Hoffmann F.W
- Hofman B
- Hohlweger B
- Hong G.H
- Horst M
- Horzyk A
- Hosokawa R
- Hou Y
- Hristov P
- Hughes C
- Huhn P
- Huhta L.M
- Hulse C.V
- Humanic T.J
- Hutson A
- Hutter D
- Iddon J.P
- Ilkaev R
- Ilyas H
- Inaba M
- Innocenti G.M
- Ippolitov M
- Isakov A
- Isidori T
- Islam M.S
- Ivanov M
- Ivanov M
- Ivanov V
- Jablonski M
- Jacak B
- Jacazio N
- Jacobs P.M
- Jadlovska S
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- Jaelani S
- Jaffe L
- Jahnke C
- Jakubowska M.J
- Janik M.A
- Janson T
- Jercic M
- Jia S
- Jimenez A.A.P
- Jonas F
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- Jung J
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- Junique A
- Jusko A
- Kabus M.J
- Kaewjai J
- Kalinak P
- Kalteyer A.S
- Kalweit A
- Kaplin V
- Karasu Uysal A
- Karatovic D
- Karavichev O
- Karavicheva T
- Karczmarczyk P
- Karpechev E
- Kebschull U
- Keidel R
- Keijdener D.L.D
- Keil M
- Ketzer B
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- Khatun A
- Khuntia A
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- Likmeta I
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- von Haller B
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- Wenzel S.C
- Wessels J.P
- Weyhmiller S.L
- Wiechula J
- Wikne J
- Wilk G
- Wilkinson J
- Willems G.A
- Windelband B
- Winn M
- Wright J.R
- Wu W
- Wu Y
- Xu R
- Yadav A
- Yadav A.K
- Yalcin S
- Yamaguchi Y
- Yang S
- Yano S
- Yin Z
- Yoo I.-K
- Yoon J.H
- Yuan S
- Yuncu A
- Zaccolo V
- Zampolli C
- Zanone F
- Zardoshti N
- Zarochentsev A
- Zaviyalov N
- Zhalov M
- Zhang B
- Zhang L
- Zhang S
- Zhang X
- Zhang Y
- Zhang Z
- Zhao M
- Zherebchevskii V
- Zhi Y
- Zhou D
- Zhou Y
- Zhu J
- Zhu Y
- Zugravel S.C
- Zurlo N
- Závada P
- Šafařík K
- Šerkšnytė L
- Publication venue
- HAL CCSD
- Publication date
- 01/01/2023
- Field of study
International audienceThe production of prompt Λc+ baryons has been measured at midrapidity in the transverse momentum interval 0<pT<1 GeV/c for the first time, in pp and p–Pb collisions at a center-of-mass energy per nucleon-nucleon collision sNN=5.02TeV. The measurement was performed in the decay channel Λc+→pKS0 by applying new decay reconstruction techniques using a Kalman-Filter vertexing algorithm and adopting a machine-learning approach for the candidate selection. The pT-integrated Λc+ production cross sections in both collision systems were determined and used along with the measured yields in Pb–Pb collisions to compute the pT-integrated nuclear modification factors RpPb and RAA of Λc+ baryons, which are compared to model calculations that consider nuclear modification of the parton distribution functions. The Λc+/D0 baryon-to-meson yield ratio is reported for pp and p–Pb collisions. Comparisons with models that include modified hadronization processes are presented, and the implications of the results on the understanding of charm hadronization in hadronic collisions are discussed. A significant (3.7σ) modification of the mean transverse momentum of Λc+ baryons is seen in p–Pb collisions with respect to pp collisions, while the pT-integrated Λc+/D0 yield ratio was found to be consistent between the two collision systems within the uncertainties
Exclusive and dissociative <math display="inline"><mi>J</mi><mo>/</mo><mi>ψ</mi></math> photoproduction, and exclusive dimuon production, in p-Pb collisions at <math display="inline"><mrow><msqrt><mrow><msub><mrow><mi>s</mi></mrow><mrow><mi>NN</mi></mrow></msub></mrow></msqrt><mo>=</mo><mn>8.16</mn><mtext> </mtext><mtext> </mtext><mi>TeV</mi></mrow></math>
- Author
- Acharya S
- Adamová D
- Adler A
- Aglieri Rinella G
- Agnello M
- Agrawal N
- Ahammed Z
- Ahmad S
- Ahn S.U
- Ahuja I
- Akindinov A
- Al-Turany M
- Aleksandrov D
- Alessandro B
- Alfanda H.M
- Alfaro Molina R
- Ali B
- Alici A
- Alizadehvandchali N
- Alkin A
- Alme J
- Alocco G
- Alt T
- Altsybeev I
- Anaam M.N
- Andrei C
- Andronic A
- Anguelov V
- Antinori F
- Antonioli P
- Apadula N
- Aphecetche L
- Appelshäuser H
- Arata C
- Arcelli S
- Aresti M
- Arnaldi R
- Arneiro J.G.M.C.A
- Arsene I.C
- Arslandok M
- Augustinus A
- Averbeck R
- Azmi M.D
- Badalà A
- Bae J
- Baek Y.W
- Bai X
- Bailhache R
- Bailung Y
- Balbino A
- Baldisseri A
- Balis B
- Banerjee D
- Banoo Z
- Barbera R
- Barile F
- Barioglio L
- Barlou M
- Barnaföldi G.G
- Barnby L.S
- Barret V
- Barreto L
- Bartels C
- Barth K
- Bartsch E
- Bastid N
- Basu S
- Batigne G
- Battistini D
- Batyunya B
- Bauri D
- Bazo Alba J.L
- Bearden I.G
- Beattie C
- Becht P
- Behera D
- Belikov I
- Bell Hechavarria A.D.C
- Bellini F
- Bellwied R
- Belokurova S
- Bencedi G
- Beole S
- Bercuci A
- Berdnikov Y
- Berdnikova A
- Bergmann L
- Besoiu M.G
- Betev L
- Bhaduri P.P
- Bhasin A
- Bhat M.A
- Bhattacharjee B
- Bianchi L
- Bianchi N
- Bielčík J
- Bielčíková J
- Biernat J
- Bigot A.P
- Bilandzic A
- Biro G
- Biswas S
- Bize N
- Blair J.T
- Blau D
- Blidaru M.B
- Bluhme N
- Blume C
- Boca G
- Bock F
- Bodova T
- Bogdanov A
- Boi S
- Bok J
- Boldizsár L
- Bombara M
- Bond P.M
- Bonomi G
- Borel H
- Borissov A
- Borquez Carcamo A.G
- Bossi H
- Botta E
- Bouziani Y.E.M
- Bratrud L
- Braun-Munzinger P
- Bregant M
- Broz M
- Bruno G.E
- Buckland M.D
- Budnikov D
- Buesching H
- Bufalino S
- Buhler P
- Buthelezi Z
- Bylinkin A
- Bysiak S.A
- Cai M
- Caines H
- Caliva A
- Calvo Villar E
- Camacho J.M.M
- Camerini P
- Canedo F.D.M
- Carabas M
- Carballo A.A
- Carnesecchi F
- Caron R
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- Castillo Castellanos J
- Catalano F
- Ceballos Sanchez C
- Chakaberia I
- Chakraborty P
- Chandra S
- Chapeland S
- Chartier M
- Chattopadhyay S
- Chattopadhyay S
- Chavez T.G
- Cheng T
- Cheshkov C
- Cheynis B
- Chibante Barroso V
- Chinellato D.D
- Chizzali E.S
- Cho J
- Cho S
- Chochula P
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- Christensen C.H
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- Colburn J.S
- Colella D
- Colocci M
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- Contin G
- Contreras J.G
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- Cortese P
- Cosentino M.R
- Costa F
- Costanza S
- Cot C
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- de Caro A
- de Cataldo G
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- de Falco A
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- del Grande R
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- Feliciello A
- Feofilov G
- Fernández Téllez A
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- Ferrer M.B
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- Ferretti A
- Feuillard V.J.G
- Filova V
- Finogeev D
- Fionda F.M
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- Fokin I
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- Gaardhøje J.J
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- Haider F.U
- Hamagaki H
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- Hippolyte B
- Hoffmann F.W
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- Jakubowska M.J
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- Wenzel S.C
- Wessels J.P
- Weyhmiller S.L
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- Wikne J
- Wilk G
- Wilkinson J
- Willems G.A
- Windelband B
- Winn M
- Wright J.R
- Wu W
- Wu Y
- Xu R
- Yadav A
- Yadav A.K
- Yalcin S
- Yamaguchi Y
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- Yano S
- Yin Z
- Yoo I.-K
- Yoon J.H
- Yu H
- Yuan S
- Yuncu A
- Zaccolo V
- Zampolli C
- Zanone F
- Zardoshti N
- Zarochentsev A
- Zaviyalov N
- Zhalov M
- Zhang B
- Zhang L
- Zhang S
- Zhang X
- Zhang Y
- Zhang Z
- Zhao M
- Zherebchevskii V
- Zhi Y
- Zhou D
- Zhou Y
- Zhu J
- Zhu Y
- Zugravel S.C
- Zurlo N
- Závada P
- Šafařík K
- Šerkšnytė L
- Publication venue
- HAL CCSD
- Publication date
- 01/01/2023
- Field of study
International audienceThe ALICE Collaboration reports three measurements in ultraperipheral proton-lead collisions at forward rapidity. The exclusive two-photon process γγ→μ+μ- and the exclusive photoproduction of J/ψ are studied. J/ψ photoproduction with proton dissociation is measured for the first time at a hadron collider. The cross section for the two-photon process of dimuons in the invariant mass range from 1 to 2.5 GeV/c2 agrees with leading-order quantum electrodynamics calculations. The exclusive and dissociative cross sections for J/ψ photoproductions are measured for photon-proton center-of-mass energies from 27 to 57 GeV. They are in good agreement with HERA results
Symmetry plane correlations in Pb-Pb collisions at sNN=2.76TeV
- Author
- Acharya S
- Adamová D
- Adler A
- Aglieri Rinella G
- Agnello M
- Agrawal N
- Ahammed Z
- Ahmad S
- Ahn S.U
- Ahuja I
- Akindinov A
- Al-Turany M
- Aleksandrov D
- Alessandro B
- Alfanda H.M
- Alfaro Molina R
- Ali B
- Alici A
- Alizadehvandchali N
- Alkin A
- Alme J
- Alocco G
- Alt T
- Altsybeev I
- Anaam M.N
- Andrei C
- Andronic A
- Anguelov V
- Antinori F
- Antonioli P
- Apadula N
- Aphecetche L
- Appelshäuser H
- Arata C
- Arcelli S
- Aresti M
- Arnaldi R
- Arneiro J.G. M.C. A
- Arsene I.C
- Arslandok M
- Augustinus A
- Averbeck R
- Azmi M.D
- Badalà A
- Bae J
- Baek Y.W
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- Willems G.A
- Windelband B
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- Wu W
- Wu Y
- Xu R
- Yadav A
- Yadav A.K
- Yalcin S
- Yamaguchi Y
- Yang S
- Yano S
- Yin Z
- Yoo I.K
- Yoon J.H
- Yuan S
- Yuncu A
- Zaccolo V
- Zampolli C
- Zanone F
- Zardoshti N
- Zarochentsev A
- Zaviyalov N
- Zhalov M
- Zhang B
- Zhang L
- Zhang S
- Zhang X
- Zhang Y
- Zhang Z
- Zhao M
- Zherebchevskii V
- Zhi Y
- Zhou D
- Zhou Y
- Zhu J
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- Zugravel S.C
- Zurlo N
- Závada P
- Šafařík K
- Šerkšnytė L
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2023
- Field of study
International audienceA newly developed observable for correlations between symmetry planes, which characterize the direction of the anisotropic emission of produced particles, is measured in Pb–Pb collisions at sNN = 2.76 TeV with ALICE. This so-called Gaussian Estimator allows for the first time the study of these quantities without the influence of correlations between different flow amplitudes. The centrality dependence of various correlations between two, three and four symmetry planes is presented. The ordering of magnitude between these symmetry plane correlations is discussed and the results of the Gaussian Estimator are compared with measurements of previously used estimators. The results utilizing the new estimator lead to significantly smaller correlations than reported by studies using the Scalar Product method. Furthermore, the obtained symmetry plane correlations are compared to state-of-the-art hydrodynamic model calculations for the evolution of heavy-ion collisions. While the model predictions provide a qualitative description of the data, quantitative agreement is not always observed, particularly for correlators with significant non-linear response of the medium to initial state anisotropies of the collision system. As these results provide unique and independent information, their usage in future Bayesian analysis can further constrain our knowledge on the properties of the QCD matter produced in ultrarelativistic heavy-ion collisions
Measurements of azimuthal anisotropies at forward and backward rapidity with muons in high-multiplicity p–Pb collisions at sNN=8.16 TeV
- Author
- A. Adler
- A. Akindinov
- A. Alici
- A. Alkin
- A. Andronic
- A. Augustinus
- A. Badalà
- A. Balbino
- A. Baldisseri
- A. Bercuci
- A. Berdnikova
- A. Bhasin
- A. Bilandzic
- A. Bogdanov
- A. Bolozdynya
- A. Borissov
- A. Caliva
- A. Dainese
- A. Danu
- A. De Caro
- A. De Falco
- A. Di Mauro
- A. Dobrin
- A. Dubla
- A. Fantoni
- A. Feliciello
- A. Fernández Téllez
- A. Ferrero
- A. Ferretti
- A. Furs
- A. Garibli
- A. Gautam
- A. Grelli
- A. Gupta
- A. Hamdi
- A. Harton
- A. Horzyk
- A. Hutson
- A. Isakov
- A. Junique
- A. Jusko
- A. Kalweit
- A. Karasu Uysal
- A. Khanzadeev
- A. Khatun
- A. Khuntia
- A. Kisiel
- A. Kluge
- A. Kondratyev
- A. Kotliarov
- A. Kravčáková
- A. Kurepin
- A. Kuryakin
- A. Lakrathok
- A. Lindner
- A. Liu
- A. Maevskaya
- A. Maire
- A. Margotti
- A. Marín
- A. Masoni
- A. Mastroserio
- A. Matyja
- A. Menchaca-Rocha
- A. Modak
- A. Morsch
- A. Mulliri
- A. Nath
- A. Neagu
- A. Negru
- A. Nyanin
- A. Ohlson
- A. Onnerstad
- A. Ortiz Velasquez
- A. Palasciano
- A. Pop
- A. Rakotozafindrabe
- A. Rehman
- A. Riabov
- A. Rosano
- A. Rossi
- A. Roy
- A. Rustamov
- A. Rybicki
- A. Schmah
- A. Schröter
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- U. Dmitrieva
- U. Fuchs
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- U. Sharma
- V. Anguelov
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- V.K. Singh
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- W. Deng
- W. Fan
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- W. Riegler
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- W. Wu
- W.H. Trzaska
- X. Bai
- X. Li
- X. Lopez
- X. Peng
- X. Zhang
- X.L. Li
- Y. Bailung
- Y. Berdnikov
- Y. Ding
- Y. Han
- Y. Hou
- Y. Kharlov
- Y. Kwon
- Y. Mao
- Y. Melikyan
- Y. Miake
- Y. Pachmayer
- Y. Pestov
- Y. Ryabov
- Y. Sekiguchi
- Y. Sibiriak
- Y. Wang
- Y. Wu
- Y. Yamaguchi
- Y. Zhang
- Y. Zhi
- Y. Zhou
- Y. Zhu
- Y.E.M. Bouziani
- Y.G. Ma
- Y.S. Lai
- Y.W. Baek
- Z. Ahammed
- Z. Banoo
- Z. Buthelezi
- Z. Conesa del Valle
- Z. Moravcova
- Z. Pugelova
- Z. Rescakova
- Z. Tang
- Z. Varga
- Z. Vilakazi
- Z. Yin
- Z. Zhang
- Ø. Djuvsland
- Publication venue
- Elsevier
- Publication date
- 01/01/2023
- Field of study
The study of the azimuthal anisotropy of inclusive muons produced in p–Pb collisions at sNN=8.16 TeV, using the ALICE detector at the LHC is reported. The measurement of the second-order Fourier coefficient of the particle azimuthal distribution, v2, is performed as a function of transverse momentum pT in the 0–20% high-multiplicity interval at both forward (2.032 GeV/c. The v2 coefficient of inclusive muons is extracted using two different techniques, namely two-particle cumulants, used for the first time for heavy-flavour measurements, and forward–central two-particle correlations. Both techniques give compatible results. A positive v2 is measured at both forward and backward rapidities with a significance larger than 4.7σ and 7.6σ, respectively, in the interval 2<pT<6 GeV/c. Comparisons with previous measurements in p–Pb collisions at sNN=5.02 TeV, and with AMPT and CGC-based theoretical calculations are discussed. The findings impose new constraints on the theoretical interpretations of the origin of the collective behaviour in small collision systems
Skewness and kurtosis of mean transverse momentum fluctuations at the LHC energies
- Author
- A. Akindinov
- A. Alici
- A. Alkin
- A. Andronic
- A. Augustinus
- A. Badalà
- A. Balbino
- A. Baldisseri
- A. Berdnikova
- A. Bhasin
- A. Bilandzic
- A. Bogdanov
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- V.K. Singh
- V.M. Sarti
- V.V. Torres
- W. Deng
- W. Fan
- W. Guo
- W. Riegler
- W. Rzesa
- W. Wu
- W.H. Trzaska
- X. Bai
- X. Li
- X. Lopez
- X. Peng
- X. Zhang
- Y. Bailung
- Y. Berdnikov
- Y. Ding
- Y. Han
- Y. Hou
- Y. Kharlov
- Y. Kwon
- Y. Mao
- Y. Melikyan
- Y. Miake
- Y. Pachmayer
- Y. Patley
- Y. Pestov
- Y. Ryabov
- Y. Sekiguchi
- Y. Sibiriak
- Y. Wang
- Y. Wang
- Y. Wu
- Y. Yamaguchi
- Y. Zhang
- Y. Zhi
- Y. Zhou
- Y. Zhu
- Y.A.V. Beltran
- Y.E.M. Bouziani
- Y.G. Ma
- Y.W. Baek
- Z. Ahammed
- Z. Banoo
- Z. Buthelezi
- Z. Conesa del Valle
- Z. Pugelova
- Z. Rescakova
- Z. Tang
- Z. Varga
- Z. Vilakazi
- Z. Yin
- Z. Zhang
- Ø. Djuvsland
- Publication venue
- Elsevier
- Publication date
- 01/01/2024
- Field of study
The first measurements of skewness and kurtosis of mean transverse momentum (〈pT〉) fluctuations are reported in Pb–Pb collisions at sNN = 5.02 TeV, Xe–Xe collisions at sNN = 5.44 TeV and pp collisions at s=5.02 TeV using the ALICE detector. The measurements are carried out as a function of system size 〈dNch/dη〉|η|<0.51/3, using charged particles with transverse momentum (pT) and pseudorapidity (η), in the range 0.2<pT<3.0 GeV/c and |η|<0.8, respectively. In Pb–Pb and Xe–Xe collisions, positive skewness is observed in the fluctuations of 〈pT〉 for all centralities, which is significantly larger than what would be expected in the scenario of independent particle emission. This positive skewness is considered a crucial consequence of the hydrodynamic evolution of the hot and dense nuclear matter created in heavy-ion collisions. Furthermore, similar observations of positive skewness for minimum bias pp collisions are also reported here. Kurtosis of 〈pT〉 fluctuations is found to be in good agreement with the kurtosis of Gaussian distribution, for most central Pb–Pb collisions. Hydrodynamic model calculations with MUSIC using Monte Carlo Glauber initial conditions are able to explain the measurements of both skewness and kurtosis qualitatively from semicentral to central collisions in Pb–Pb system. Color reconnection mechanism in PYTHIA8 model seems to play a pivotal role in capturing the qualitative behavior of the same measurements in pp collisions
Accessing the strong interaction between Λ baryons and charged kaons with the femtoscopy technique at the LHC
- Author
- A. Adler
- A. Akindinov
- A. Alici
- A. Alkin
- A. Andronic
- A. Augustinus
- A. Badalà
- A. Balbino
- A. Baldisseri
- A. Bercuci
- A. Berdnikova
- A. Bhasin
- A. Bilandzic
- A. Bogdanov
- A. Borissov
- A. Bylinkin
- A. Caliva
- A. Dainese
- A. Danu
- A. De Caro
- A. De Falco
- A. Di Mauro
- A. Dobrin
- A. Dubla
- A. Fantoni
- A. Feliciello
- A. Fernández Téllez
- A. Ferrero
- A. Ferretti
- A. Furs
- A. Gautam
- A. Ghimouz
- A. Grelli
- A. Gupta
- A. Hamdi
- A. Harton
- A. Horzyk
- A. Hutson
- A. Isakov
- A. Junique
- A. Jusko
- A. Kalweit
- A. Karasu Uysal
- A. Khanzadeev
- A. Khatun
- A. Khuntia
- A. Kisiel
- A. Kluge
- A. Kondratyev
- A. Kotliarov
- A. Kravčáková
- A. Kurepin
- A. Kuryakin
- A. Lakrathok
- A. Lindner
- A. Liu
- A. Maire
- A. Margotti
- A. Marín
- A. Masoni
- A. Mastroserio
- A. Matyja
- A. Menchaca-Rocha
- A. Modak
- A. Morsch
- A. Mulliri
- A. Nath
- A. Neagu
- A. Negru
- A. Nyanin
- A. Ohlson
- A. Onnerstad
- A. Ortiz Velasquez
- A. Palasciano
- A. Pop
- A. Rakotozafindrabe
- A. Rehman
- A. Riabov
- A. Rosano
- A. Rossi
- A. Roy
- A. Rustamov
- A. Rybicki
- A. Schmah
- A. Schröter
- A. Sevcenco
- A. Shabetai
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- S. Yang
- S. Yano
- S. Yuan
- S. Zhang
- S.A. Bysiak
- S.A. Konigstorfer
- S.A. Voloshin
- S.A.R. Ramirez
- S.C. Wenzel
- S.C. Zugravel
- S.D. Koryciak
- S.F. Stiefelmaier
- S.F. Taghavi
- S.H. Lim
- S.K. Malik
- S.K. Mandal
- S.K. Prasad
- S.K. Saha
- S.L. La Pointe
- S.L. Weyhmiller
- S.P. Guzman
- S.S. Khade
- S.S. Räsänen
- S.T. Heckel
- S.U. Ahn
- T. Alt
- T. Bodova
- T. Cheng
- T. Chujo
- T. Dietel
- T. Fusayasu
- T. Gahlaut
- T. Gundem
- T. Gunji
- T. Herman
- T. Hyodo
- T. Isidori
- T. Janson
- T. Karavicheva
- T. Kim
- T. Klemenz
- T. Kollegger
- T. Kumaoka
- T. Mrnjavac
- T. Peitzmann
- T. Siemiarczuk
- T. Simantathammakul
- T. Sinha
- T. Tkacik
- T. Tork
- T. Tripathy
- T. Virgili
- T.A. Rancien
- T.B. Saramela
- T.B. Skaali
- T.F. Silva
- T.G. Chavez
- T.J. Humanic
- T.J. Shaba
- T.M. Eder
- T.M. Lelek
- T.P. Trzcinski
- T.S. Rogoschinski
- T.S. Tveter
- U. Dmitrieva
- U. Fuchs
- U. Kebschull
- U. Sharma
- V. Anguelov
- V. Barret
- V. Chibante Barroso
- V. Filova
- V. Gonzalez
- V. Grabski
- V. Grigoriev
- V. Ivanov
- V. Kaplin
- V. Kovalenko
- V. Kozhuharov
- V. Kučera
- V. Lindenstruth
- V. Manko
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- V. Nikulin
- V. Petrov
- V. Pozdniakov
- V. Riabov
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- V. Singhal
- V. Sumberia
- V. Trubnikov
- V. Vechernin
- V. Vislavicius
- V. Zaccolo
- V. Zherebchevskii
- V.A. Okorokov
- V.J.G. Feuillard
- V.K. Singh
- V.M. Sarti
- V.V. Torres
- W. Deng
- W. Fan
- W. Guo
- W. Riegler
- W. Rzesa
- W. Wu
- W.H. Trzaska
- X. Bai
- X. Li
- X. Lopez
- X. Peng
- X. Zhang
- X.L. Li
- Y. Bailung
- Y. Berdnikov
- Y. Ding
- Y. Han
- Y. Hou
- Y. Kamiya
- Y. Kharlov
- Y. Kwon
- Y. Mao
- Y. Melikyan
- Y. Miake
- Y. Pachmayer
- Y. Patley
- Y. Pestov
- Y. Ryabov
- Y. Sekiguchi
- Y. Sibiriak
- Y. Wang
- Y. Wang
- Y. Wu
- Y. Yamaguchi
- Y. Zhang
- Y. Zhi
- Y. Zhou
- Y. Zhu
- Y.E.M. Bouziani
- Y.G. Ma
- Y.W. Baek
- Z. Ahammed
- Z. Banoo
- Z. Buthelezi
- Z. Conesa del Valle
- Z. Moravcova
- Z. Pugelova
- Z. Rescakova
- Z. Tang
- Z. Varga
- Z. Vilakazi
- Z. Yin
- Z. Zhang
- Ø. Djuvsland
- Publication venue
- Elsevier
- Publication date
- 01/10/2023
- Field of study
The interaction between Λ baryons and kaons/antikaons is a crucial ingredient for the strangeness S=0 and S=−2 sector of the meson–baryon interaction at low energies. In particular, the ΛK‾ might help in understanding the origin of states such as the Ξ(1620), whose nature and properties are still under debate. Experimental data on Λ–K and Λ–K‾ systems are scarce, leading to large uncertainties and tension between the available theoretical predictions constrained by such data. In this Letter we present the measurements of Λ–K⊕+Λ‾–K− and Λ–K⊕−Λ‾–K+ correlations obtained in the high-multiplicity triggered data sample in pp collisions at s=13 TeV recorded by ALICE at the LHC. The correlation function for both pairs is modeled using the Lednický–Lyuboshits analytical formula and the corresponding scattering parameters are extracted. The Λ–K⊕−Λ‾–K+ correlations show the presence of several structures at relative momenta k⁎ above 200 MeV/c, compatible with the Ω baryon, the Ξ(1690), and Ξ(1820) resonances decaying into Λ–K− pairs. The low k⁎ region in the Λ–K⊕−Λ‾–K+ also exhibits the presence of the Ξ(1620) state, expected to strongly couple to the measured pair. The presented data allow to access the ΛK+ and ΛK− strong interaction with an unprecedented precision and deliver the first experimental observation of the Ξ(1620) decaying into ΛK−
Production of pions, kaons, and protons as a function of the relative transverse activity classifier in pp collisions at s = 13 TeV
- Author
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- Tambave G.J
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- Tarzila M.G
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- Weiglhofer F.T
- Wenzel S.C
- Wessels J.P
- Weyhmiller S.L
- Wiechula J
- Wikne J
- Wilk G
- Wilkinson J
- Willems G.A
- Windelband B
- Winn M
- Wright J.R
- Wu W
- Wu Y
- Xu R
- Yadav A
- Yadav A.K
- Yalcin S
- Yamaguchi Y
- Yang S
- Yano S
- Yin Z
- Yoo I.K
- Yoon J.H
- Yuan S
- Yuncu A
- Zaccolo V
- Zampolli C
- Zanone F
- Zardoshti N
- Zarochentsev A
- Zaviyalov N
- Zhalov M
- Zhang B
- Zhang L
- Zhang S
- Zhang X
- Zhang Y
- Zhang Z
- Zhao M
- Zherebchevskii V
- Zhi Y
- Zhou D
- Zhou Y
- Zhu J
- Zhu Y
- Zugravel S.C
- Zurlo N
- Závada P
- Šafařík K
- Šerkšnytė L
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2023
- Field of study
International audienceThe production of π±, K±, and (p)p is measured in pp collisions at s = 13 TeV in different topological regions of the events. Particle transverse momentum (pT) spectra are measured in the “toward”, “transverse”, and “away” angular regions defined with respect to the direction of the leading particle in the event. While the toward and away regions contain the fragmentation products of the near-side and away-side jets, respectively, the transverse region is dominated by particles from the Underlying Event (UE). The relative transverse activity classifier, RT = NT/〈NT〉, is used to group events according to their UE activity, where NT is the measured charged-particle multiplicity per event in the transverse region and 〈NT〉 is the mean value over all the analysed events. The first measurements of identified particle pT spectra as a function of RT in the three topological regions are reported. It is found that the yield of high transverse momentum particles relative to the RT-integrated measurement decreases with increasing RT in both the toward and the away regions, indicating that the softer UE dominates particle production as RT increases and validating that RT can be used to control the magnitude of the UE. Conversely, the spectral shapes in the transverse region harden significantly with increasing RT. This hardening follows a mass ordering, being more significant for heavier particles. Finally, it is observed that the pT-differential particle ratios \left(\textrm{p}+\overline{\textrm{p}}\right)/\left({\uppi}^{+}+{\uppi}^{-}\right) and (K+ + K−)/(π+ + π−) in the low UE limit (RT → 0) approach expectations from Monte Carlo generators such as PYTHIA 8 with Monash 2013 tune and EPOS LHC, where the jet-fragmentation models have been tuned to reproduce e+e− results.[graphic not available: see fulltext
Measurement of the non-prompt D-meson fraction as a function of multiplicity in proton-proton collisions at s = 13 TeV
- Author
- Acharya S
- Adamová D
- Adler A
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- Topilskaya N
- Toppi M
- Torales-Acosta F
- Tork T
- Torres Ramos A.G
- Trifiró A
- Triolo A.S
- Tripathy S
- Tripathy T
- Trogolo S
- Trubnikov V
- Trzaska W.H
- Trzcinski T.P
- Tumkin A
- Turrisi R
- Tveter T.S
- Ullaland K
- Ulukutlu B
- Uras A
- Urioni M
- Usai G.L
- Vala M
- Valle N
- van Doremalen L.V. R
- van Leeuwen M
- van Veen C.A
- van Weelden R.J. G
- Vande Vyvre P
- Varga D
- Varga Z
- Vasileiou M
- Vasiliev A
- Vazquez Rueda O
- Vechernin V
- Vercellin E
- Vergara Limón S
- Vermunt L
- Verweij M
- Vickovic L
- Vilakazi Z
- Villalobos Baillie O
- Villani A
- Vino G
- Vinogradov A
- Virgili T
- Virta M.M. O
- Vislavicius V
- Vodopyanov A
- Volkel B
- Voloshin K
- Voloshin S.A
- Volpe G
- von Haller B
- Vorobyev I
- Vozniuk N
- Vrláková J
- Vázquez Doce O
- Vértesi R
- Völkl M.A
- Wang C
- Wang D
- Wang Y
- Wegrzynek A
- Weiglhofer F.T
- Wenzel S.C
- Wessels J.P
- Weyhmiller S.L
- Wiechula J
- Wikne J
- Wilk G
- Wilkinson J
- Willems G.A
- Windelband B
- Winn M
- Wright J.R
- Wu W
- Wu Y
- Xu R
- Yadav A
- Yadav A.K
- Yalcin S
- Yamaguchi Y
- Yang S
- Yano S
- Yin Z
- Yoo I.K
- Yoon J.H
- Yuan S
- Yuncu A
- Zaccolo V
- Zampolli C
- Zanone F
- Zardoshti N
- Zarochentsev A
- Zaviyalov N
- Zhalov M
- Zhang B
- Zhang L
- Zhang S
- Zhang X
- Zhang Y
- Zhang Z
- Zhao M
- Zherebchevskii V
- Zhi Y
- Zhou D
- Zhou Y
- Zhu J
- Zhu Y
- Zugravel S.C
- Zurlo N
- Závada P
- Šafařík K
- Šerkšnytė L
- Publication venue
- HAL CCSD
- Publication date
- 01/01/2023
- Field of study
International audienceThe fractions of non-prompt (i.e. originating from beauty-hadron decays) D0 and D+ mesons with respect to the inclusive yield are measured as a function of the charged-particle multiplicity in proton-proton collisions at a centre-of-mass energy of s = 13 TeV with the ALICE detector at the LHC. The results are reported in intervals of transverse momentum (pT) and integrated in the range 1 < pT< 24 GeV/c. The fraction of non-prompt D0 and D+ mesons is found to increase slightly as a function of pT in all the measured multiplicity intervals, while no significant dependence on the charged-particle multiplicity is observed. In order to investigate the production and hadronisation mechanisms of charm and beauty quarks, the results are compared to PYTHIA 8 as well as EPOS 3 and EPOS 4 Monte Carlo simulations, and to calculations based on the colour glass condensate including three-pomeron fusion.[graphic not available: see fulltext
The ALICE experiment: a journey through QCD
- Author
- Acharya S
- Adamová D
- Adler A
- Aglieri Rinella G
- Agnello M
- Agrawal N
- Ahammed Z
- Ahmad S
- Ahn S.U
- Ahuja I
- Akindinov A
- Al-Turany M
- Aleksandrov D
- Alessandro B
- Alfanda H.M
- Alfaro Molina R
- Ali B
- Alici A
- Alizadehvandchali N
- Alkin A
- Alme J
- Alocco G
- Alt T
- Altsybeev I
- Alvarado J.R
- Anaam M.N
- Andrei C
- Andronic A
- Anguelov V
- Antinori F
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- Aphecetche L
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- Arata C
- Arcelli S
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- Baek Y.W
- Bai X
- Bailhache R
- Bailung Y
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- Barnaföldi G.G
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- Belyaev V
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- Vermunt L
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- Vickovic L
- Vilakazi Z
- Villalobos Baillie O
- Vino G
- Vinogradov A
- Virgili T
- Vislavicius V
- Vodopyanov A
- Volkel B
- Voloshin K
- Voloshin S.A
- Volpe G
- von Haller B
- Vorobyev I
- Vozniuk N
- Vrláková J
- Vázquez Doce O
- Vértesi R
- Völkl M.A
- Wang C
- Wang D
- Wang Y
- Weber M
- Wegrzynek A
- Weiglhofer F.T
- Wenzel S.C
- Wessels J.P
- Wiechula J
- Wikne J
- Wilk G
- Wilkinson J
- Willems G.A
- Windelband B
- Winn M
- Wright J.R
- Wu W
- Wu Y
- Xu R
- Yadav A
- Yadav A.K
- Yalcin S
- Yamaguchi Y
- Yang S
- Yano S
- Yin Z
- Yoo I.K
- Yoon J.H
- Yuan S
- Yuncu A
- Zaccolo V
- Zampolli C
- Zanone F
- Zardoshti N
- Zarochentsev A
- Zaviyalov N
- Zhalov M
- Zhang B
- Zhang L
- Zhang S
- Zhang X
- Zhang Y
- Zhang Z
- Zhao M
- Zherebchevskii V
- Zhi Y
- Zhou D
- Zhou Y
- Zhu J
- Zhu Y
- Zugravel S.C
- Zurlo N
- Závada P
- Šafařík K
- Šerkšnytė L
- Publication venue
- HAL CCSD
- Publication date
- 01/01/2024
- Field of study
CERN-EP-2022-227International audienceThe ALICE experiment was proposed in 1993, to study strongly-interacting matter at extreme energy densities and temperatures. This proposal entailed a comprehensive investigation of nuclear collisions at the LHC. Its physics programme initially focused on the determination of the properties of the quark–gluon plasma (QGP), a deconfined state of quarks and gluons, created in such collisions. The ALICE physics programme has been extended to cover a broader ensemble of observables related to Quantum Chromodynamics (QCD), the theory of strong interactions. The experiment has studied Pb–Pb, Xe–Xe, p–Pb and pp collisions in the multi-TeV centre of mass energy range, during the Run 1–2 data-taking periods at the LHC (2009–2018). The aim of this review is to summarise the key ALICE physics results in this endeavor, and to discuss their implications on the current understanding of the macroscopic and microscopic properties of strongly-interacting matter at the highest temperatures reached in the laboratory. It will review the latest findings on the properties of the QGP created by heavy-ion collisions at LHC energies, and describe the surprising QGP-like effects in pp and p–Pb collisions. Measurements of few-body QCD interactions, and their impact in unraveling the structure of hadrons and hadronic interactions, will be discussed. ALICE results relevant for physics topics outside the realm of QCD will also be touched upon. Finally, prospects for future measurements with the ALICE detector in the context of its planned upgrades will also be briefly described
Azimuthal correlations of heavy-flavor hadron decay electrons with charged particles in pp and p–Pb collisions at sNN = 5.02 TeV
- Author
- Acharya S
- Adamová D
- Adler A
- Aglieri Rinella G
- Agnello M
- Agrawal N
- Ahammed Z
- Ahmad S
- Ahn S.U
- Ahuja I
- Akindinov A
- Al-Turany M
- Aleksandrov D
- Alessandro B
- Alfanda H.M
- Alfaro Molina R
- Ali B
- Alici A
- Alizadehvandchali N
- Alkin A
- Alme J
- Alocco G
- Alt T
- Altsybeev I
- Anaam M.N
- Andrei C
- Andronic A
- Anguelov V
- Antinori F
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- Aphecetche L
- Appelshäuser H
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- Arcelli S
- Aresti M
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- Arneiro J.G. M.C. A
- Arsene I.C
- Arslandok M
- Augustinus A
- Averbeck R
- Azmi M.D
- Badalà A
- Bae J
- Baek Y.W
- Bai X
- Bailhache R
- Bailung Y
- Balbino A
- Baldisseri A
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- Banoo Z
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- Barile F
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- Barlou M
- Barnaföldi G.G
- Barnby L.S
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- Barreto L
- Bartels C
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- Bauri D
- Bazo Alba J.L
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- Wright J.R
- Wu W
- Wu Y
- Xu R
- Yadav A
- Yadav A.K
- Yalcin S
- Yamaguchi Y
- Yang S
- Yano S
- Yin Z
- Yoo I.K
- Yoon J.H
- Yuan S
- Yuncu A
- Zaccolo V
- Zampolli C
- Zanone F
- Zardoshti N
- Zarochentsev A
- Zaviyalov N
- Zhalov M
- Zhang B
- Zhang L
- Zhang S
- Zhang X
- Zhang Y
- Zhang Z
- Zhao M
- Zherebchevskii V
- Zhi Y
- Zhou D
- Zhou Y
- Zhu J
- Zhu Y
- Zugravel S.C
- Zurlo N
- Závada P
- Šafařík K
- Šerkšnytė L
- Publication venue
- HAL CCSD
- Publication date
- 01/01/2023
- Field of study
International audienceThe azimuthal (Δφ) correlation distributions between heavy-flavor decay electrons and associated charged particles are measured in pp and p–Pb collisions at sNN=5.02 TeV. Results are reported for electrons with transverse momentum 4<pT<16GeV/c and pseudorapidity ∣η∣<0.6. The associated charged particles are selected with transverse momentum 1<pT<7GeV/c, and relative pseudorapidity separation with the leading electron ∣Δη∣<1. The correlation measurements are performed to study and characterize the fragmentation and hadronization of heavy quarks. The correlation structures are fitted with a constant and two von Mises functions to obtain the baseline and the near- and away-side peaks, respectively. The results from p–Pb collisions are compared with those from pp collisions to study the effects of cold nuclear matter. In the measured trigger electron and associated particle kinematic regions, the two collision systems give consistent results. The Δφ distribution and the peak observables in pp and p–Pb collisions are compared with calculations from various Monte Carlo event generators