121 research outputs found
Multiplicity dependence of inclusive J/psi production at midrapidity in pp collisions at root s=13 TeV
- Author
- Acharya S.
- AdamovĂĄ D.
- Adler A.
- Adolfsson J.
- Aggarwal M.M.
- Aglieri Rinella G.
- Agnello M.
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- Ahammed Z.
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- Albuquerque D.S.D.
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- Winn M.
- Witt W.E.
- Wright J.R.
- Wu Y.
- Xu R.
- Yalcin S.
- Yamaguchi Y.
- Yamakawa K.
- Yang S.
- Yano S.
- Yin Z.
- Yokoyama H.
- Yoo I.-K.
- Yoon J.H.
- Yuan S.
- Yuncu A.
- Yurchenko V.
- Zaccolo V.
- Zaman A.
- Zampolli C.
- Zanoli H.J.C.
- Zardoshti N.
- Zarochentsev A.
- Zaviyalov N.
- Zbroszczyk H.
- Zhalov M.
- Zhang S.
- Zhang X.
- Zhang Z.
- Zherebchevskii V.
- Zhi Y.
- Zhou D.
- Zhou Y.
- Zhou Z.
- Zhu J.
- Zhu Y.
- Zichichi A.
- Zinovjev G.
- Zurlo N.
- ZĂĄvada P.
- Ć afaĆĂk K.
- Ć umbera M.
- Publication venue
- Publication date
- 01/01/2019
- Field of study
Measurements of the inclusive J/psi yield as a function of charged-particle pseudorapidity density dN(ch)/d eta in pp collisions at root s = 13 TeV with ALICE at the LHC are reported. The J/psi meson yield is measured at midrapidity (vertical bar y vertical bar <0.9) in the dielectron channel, for events selected based on the charged-particle multiplicity at midrapidity (vertical bar eta vertical bar <1) and at forward rapidity (-3.7 <eta <-1.7 and 2.8 <eta <5.1); both observables are normalized to their corresponding averages in minimum bias events. The increase of the normalized J/psi yield with normalized dN(ch)/d eta is significantly stronger than linear and dependent on the transverse momentum. The data are compared to theoretical predictions, which describe the observed trends well, albeit not always quantitatively. (C) 2020 European Organization for Nuclear Research. Published by Elsevier B.V.Peer reviewe
First measurement of Ωc0 production in pp collisions at s=13 TeV
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- ZĂĄvada P.
- Ć afaĆĂk K.
- Ć erkĆĄnytÄ L.
- Publication venue
- Elsevier BV
- Publication date
- 01/01/2023
- Field of study
The inclusive production of the charmâstrange baryon 0 c is measured for the first time via its hadronic â decay into âÏ+ at midrapidity (|y| <0.5) in protonâproton (pp) collisions at the centre-of-mass energy s =13 TeV with the ALICE detector at the LHC. The transverse momentum (pT) differential cross section multiplied by the branching ratio is presented in the interval 2 < pT < 12 GeV/c. The pT dependence of the 0 c-baryon production relative to the prompt D0-meson and to the prompt 0 c-baryon production is compared to various models that take different hadronisation mechanisms into consideration. In the measured pT interval, the ratio of the pT-integrated cross sections of 0 c and prompt + c baryons multiplied by the âÏ+ branching ratio is found to be larger by a factor of about 20 with a significance of about 4Ï when compared to e+eâ collisions
Elliptic flow of charged particles at midrapidity relative to the spectator plane in PbâPb and XeâXe collisions
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- Ć erkĆĄnytÄ L.
- Publication venue
- Elsevier BV
- Publication date
- 01/01/2023
- Field of study
Measurements of the elliptic flow coefficient relative to the collision plane defined by the spectator neutrons v2{ SP} in collisions of Pb ions at center-of-mass energy per nucleonânucleon pair â 2.76 TeV and Xe ions at â sNN = sNN =5.44 TeV are reported. The results are presented for charged particles produced at midrapidity as a function of centrality and transverse momentum for the 5â70% and 0.2â6 GeV/c ranges, respectively. The ratio between v2{ SP} and the elliptic flow coefficient relative to the participant plane v2{4}, estimated using four-particle correlations, deviates by up to 20% from unity depending on centrality. This observation differs strongly from the magnitude of the corresponding eccentricity ratios predicted by the TRENTo and the elliptic power models of initial state fluctuations that are tuned to describe the participant plane anisotropies. The differences can be interpreted as a decorrelation of the neutron spectator plane and the reaction plane because of fragmentation of the remnants from the colliding nuclei, which points to an incompleteness of current models describing the initial state fluctuations. A significant transverse momentum dependence of the ratio v2{ SP}/v2{4} is observed in all but the most central collisions, which may help to understand whether momentum anisotropies at low and intermediate transverse momentum have a common origin in initial state f luctuations. The ratios of v2{ SP} and v2{4} to the corresponding initial state eccentricities for XeâXe and PbâPb collisions at similar initial entropy density show a difference of (7.0 ±0.9)%with an additional variation of +1.8% when including RHIC data in the TRENTo parameter extraction. These observations provide new experimental constraints for viscous effects in the hydrodynamic modeling of the expanding quarkâgluon plasma produced in heavy-ion collisions at the LHC
Production of Î and KS0 in jets in pâPb collisions at sNN=5.02 TeV and pp collisions at s=7 TeV
- Publication venue
- Publication date
- 01/01/2022
- Field of study
The production of Î baryons and KS0 mesons (V0 particles) was measured in pâPb collisions at sNN=5.02 TeV and pp collisions at s=7 TeV with ALICE at the LHC. The production of these strange particles is studied separately for particles associated with hard scatterings and the underlying event to shed light on the baryon-to-meson ratio enhancement observed at intermediate transverse momentum (pT) in high multiplicity pp and pâPb collisions. Hard scatterings are selected on an event-by-event basis with jets reconstructed with the anti-kT algorithm using charged particles. The production of strange particles associated with jets pT,jetch&gt;10 and pT,jetch&gt;20 GeV/c in pâPb collisions, and with jet pT,jetch&gt;10 GeV/c in pp collisions is reported as a function of pT. Its dependence on angular distance from the jet axis, R(V0,jet), for jets with pT,jetch&gt;10 GeV/c in pâPb collisions is reported as well. The pT-differential production spectra of strange particles associated with jets are found to be harder compared to that in the underlying event and both differ from the inclusive measurements. In events containing a jet, the density of the V0 particles in the underlying event is found to be larger than the density in the minimum bias events. The Î/KS0 ratio associated with jets in pâPb collisions is consistent with the ratio in pp collisions and follows the expectation of jets fragmenting in vacuum. On the other hand, this ratio within jets is consistently lower than the one obtained in the underlying event and it does not show the characteristic enhancement of baryons at intermediate pT often referred to as âbaryon anomalyâ in the inclusive measurements. © 2022 European Organization for Nuclear Research, ALIC
Anisotropic flow and flow fluctuations of identified hadrons in PbâPb collisions at sNNââ = 5.02 TeV
- Author
- Acharya S
- AdamovĂĄ D
- Adler A
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- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2023
- Field of study
International audienceThe first measurements of elliptic flow of ϱ, K±, p+pâ, KS0â, Î+Î, Ï, Îâ+Î+, and Ωâ+Ω+ using multiparticle cumulants in PbâPb collisions at sNNââ = 5.02 TeV are resented. Results obtained with two- (v2â{2}) and four-particle cumulants (v2â{4}) are shown as a function of transverse momentum, pTâ, for various collision centrality intervals. Combining the data for both v2â{2} and v2â{4} also allows us to report the first measurements of the mean elliptic flow, elliptic flow fluctuations, and relative elliptic flow fluctuations for various hadron species. These observables probe the event-by-event eccentricity fluctuations in the initial state and the contributions from the dynamic evolution of the expanding quarkâgluon plasma. The characteristic features observed in previous pTâ-differential anisotropic flow measurements for identified hadrons with two-particle correlations, namely the mass ordering at low pTâ and the approximate scaling with the number of constituent quarks at intermediate pTâ, are similarly present in the four-particle correlations and the combinations of v2â{2} and v2â{4}. In addition, a particle species dependence of flow fluctuations is observed that could indicate a significant contribution from final state hadronic interactions. The comparison between experimental measurements and CoLBT model calculations, which combine the various physics processes of hydrodynamics, quark coalescence, and jet fragmentation, illustrates their importance over a wide pTâ range.[graphic not available: see fulltext
ÎŁ(1385)± resonance production in PbâPb collisions at sNNââ = 5.02 TeV
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- Acharya S
- AdamovĂĄ D
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- Ć erkĆĄnytÄ L
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2023
- Field of study
International audienceHadronic resonances are used to probe the hadron gas produced in the late stage of heavy-ion collisions since they decay on the same timescale, of the order of 1â10 fm/c, as the decoupling time of the system. In the hadron gas, (pseudo)elastic scatterings among the products of resonances that decayed before the kinetic freeze-out and regeneration processes counteract each other, the net effect depending on the resonance lifetime, the duration of the hadronic phase, and the hadronic cross sections at play. In this context, the ÎŁ(1385)± particle is of particular interest as models predict that regeneration dominates over rescattering despite its relatively short lifetime of about 5.5 fm/c. The first measurement of the ÎŁ(1385)± resonance production at midrapidity in PbâPb collisions at sNNââ=5.02 TeV with the ALICE detector is presented in this Letter. The resonances are reconstructed via their hadronic decay channel, ÎÏ, as a function of the transverse momentum (pTâ) and the collision centrality. The results are discussed in comparison with the measured yield of pions and with expectations from the statistical hadronization model as well as commonly employed event generators, including PYTHIA8/Angantyr and EPOS3 coupled to the UrQMD hadronic cascade afterburner. None of the models can describe the data. For ÎŁ(1385)±, a similar behaviour as Kâ(892)0 is observed in data unlike the predictions of EPOS3 with afterburner
Constraining the KN coupled channel dynamics using femtoscopic correlations at the LHC
- Author
- Acharya S
- AdamovĂĄ D
- Adler A
- Aglieri Rinella G
- Agnello M
- Agrawal N
- Ahammed Z
- Ahmad S
- Ahn S.U
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- Ć erkĆĄnytÄ L
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2023
- Field of study
International audienceThe interaction of Kâwith protons is characterised by the presence of several coupled channels, systems like K0n and \uppi \Sigma with a similar mass and the same quantum numbers as the Kâp state. The strengths of these couplings to the Kâp system are of crucial importance for the understanding of the nature of the Î(1405) resonance and of the attractive Kâp strong interaction. In this article, we present measurements of the Kâp correlation functions in relative momentum space obtained in pp collisions at sâ = 13 Te, in pâPb collisions at sNNââ = 5.02 Te, and (semi)peripheral PbâPb collisions at sNNââ = 5.02 Te. The emitting source size, composed of a core radius anchored to the K+p correlation and of a resonance halo specific to each particle pair, varies between 1 and 2 fm in these collision systems. The strength and the effects of the K0n and \uppi \Sigma inelastic channels on the measured Kâp correlation function are investigated in the different colliding systems by comparing the data with state-of-the-art models of chiral potentials. A novel approach to determine the conversion weights Ï, necessary to quantify the amount of produced inelastic channels in the correlation function, is presented. In this method, particle yields are estimated from thermal model predictions, and their kinematic distribution from blast-wave fits to measured data. The comparison of chiral potentials to the measured Kâp interaction indicates that, while the \uppi \Sigma âKâp dynamics is well reproduced by the model, the coupling to the K0n channel in the model is currently underestimated
Measurements of the groomed jet radius and momentum splitting fraction with the soft drop and dynamical grooming algorithms in pp collisions at sâ = 5.02 TeV
- Author
- Acharya S
- AdamovĂĄ D
- Adler A
- Aglieri Rinella G
- Agnello M
- Agrawal N
- Ahammed Z
- Ahmad S
- Ahn S.U
- Ahuja I
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- Alfanda H.M
- Alfaro Molina R
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- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2023
- Field of study
International audienceThis article presents measurements of the groomed jet radius and momentum splitting fraction in pp collisions at sâ = 5.02 TeV with the ALICE detector at the Large Hadron Collider. Inclusive charged-particle jets are reconstructed at midrapidity using the anti-kTâ algorithm for transverse momentum 60<pTchjetâ<80 GeV/c. We report results using two different grooming algorithms: soft drop and, for the first time, dynamical grooming. For each grooming algorithm, a variety of grooming settings are used in order to explore the impact of collinear radiation on these jet substructure observables. These results are compared to perturbative calculations that include resummation of large logarithms at all orders in the strong coupling constant. We find good agreement of the theoretical predictions with the data for all grooming settings considered.[graphic not available: see fulltext
Measurement of Ï(2S) production as a function of charged-particle pseudorapidity density in pp collisions at sâ = 13 TeV and p-Pb collisions at sNNââ = 8.16 TeV with ALICE at the LHC
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- AdamovĂĄ D
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- Silvermyr D
- Simantathammakul T
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- Simonetti G
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- Yoo I.K
- Yoon J.H
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- Zaccolo V
- Zampolli C
- Zanoli H.J. C
- Zanone F
- Zardoshti N
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- Zaviyalov N
- Zhalov M
- Zhang B
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- Zhao M
- Zherebchevskii V
- Zhi Y
- Zhigareva N
- Zhou D
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- ZĂĄvada P
- Ć afaĆĂk K
- Ć erkĆĄnytÄ L
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 21/04/2022
- Field of study
International audienceProduction of inclusive charmonia in pp collisions at center-of-mass energy of sâ = 13 TeV and pâPb collisions at center-of-mass energy per nucleon pair of sNNââ = 8.16 TeV is studied as a function of charged-particle pseudorapidity density with ALICE. Ground and excited charmonium states (J/Ï, Ï(2S)) are measured from their dimuon decays in the interval of rapidity in the center-of-mass frame 2.5 < ycmsâ< 4.0 for pp collisions, and 2.03 < ycmsâ< 3.53 and â4.46 < ycmsâ< â2.96 for pâPb collisions. The charged-particle pseudorapidity density is measured around midrapidity (|η| < 1.0). In pp collisions, the measured charged-particle multiplicity extends to about six times the average value, while in p-Pb collisions at forward (backward) rapidity a multiplicity corresponding to about three (four) times the average is reached. The Ï(2S) yield increases with the charged-particle pseudorapidity density. The ratio of Ï(2S) over J/Ï yield does not show a significant multiplicity dependence in either colliding system, suggesting a similar behavior of J/Ï and Ï(2S) yields with respect to charged-particle pseudorapidity density. Results for the Ï(2S) yield and its ratio with respect to J/Ï agree with available model calculations.[graphic not available: see fulltext
Measurement of inclusive and leading subjet fragmentation in pp and PbâPb collisions at sNNââ = 5.02 TeV
- Author
- Acharya S
- AdamovĂĄ D
- Adler A
- Aglieri Rinella G
- Agnello M
- Agrawal N
- Ahammed Z
- Ahmad S
- Ahn S.U
- Ahuja I
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- Aleksandrov D
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- Alfanda H.M
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- Storehaug I
- Storetvedt M.M
- Stratmann P
- Strazzi S
- Stylianidis C.P
- Suaide A.A. P
- Suire C
- Sukhanov M
- Suljic M
- Sumberia V
- Sumowidagdo S
- Swain S
- Szabo A
- Szarka I
- Tabassam U
- Taghavi S.F
- Taillepied G
- Takahashi J
- Tambave G.J
- Tang S
- Tang Z
- Tapia Takaki J.D
- Tapus N
- Tarasovicova L.A
- Tarzila M.G
- Tauro A
- Telesca A
- Terlizzi L
- Terrevoli C
- Tersimonov G
- Thakur S
- Thomas D
- Tieulent R
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- Timmins A.R
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- Tkacik T
- Toia A
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- Torales-Acosta F
- Tork T
- Torres Ramos A.G
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- Trubnikov V
- Trzaska W.H
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- Ulukutlu B
- Uras A
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- Usai G.L
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- Vallero S
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- van Leeuwen M
- van Veen C.A
- van Weelden R.J. G
- Vande Vyvre P
- Varga D
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- Varga-Kofarago M
- Vasileiou M
- Vasiliev A
- Vechernin V
- Vercellin E
- Vergara LimĂłn S
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- Vino G
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- Volkel B
- Voloshin K
- Voloshin S.A
- Volpe G
- von Haller B
- Vorobyev I
- Vozniuk N
- VrlĂĄkovĂĄ J
- VĂĄzquez Doce O
- VĂ©rtesi R
- Völkl M.A
- Wagner B
- Wang C
- Wang D
- Weber M
- 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.K
- Yalcin S
- Yamaguchi Y
- Yamakawa K
- Yang S
- Yano S
- Yin Z
- Yoo I.K
- Yoon J.H
- Yuan S
- Yuncu A
- Zaccolo V
- Zampolli C
- Zanoli H.J. C
- Zanone F
- Zardoshti N
- Zarochentsev A
- Zaviyalov N
- Zhalov M
- Zhang B
- Zhang S
- Zhang X
- Zhang Y
- Zhao M
- Zherebchevskii V
- Zhi Y
- Zhigareva N
- Zhou D
- Zhou Y
- Zhu J
- Zhu Y
- Zinovjev G
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- Ć afaĆĂk K
- Ć erkĆĄnytÄ L
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2023
- Field of study
International audienceThis article presents new measurements of the fragmentation properties of jets in both protonâproton (pp) and heavy-ion collisions with the ALICE experiment at the Large Hadron Collider (LHC). We report distributions of the fraction zrâ of transverse momentum carried by subjets of radius r within jets of radius R. Charged-particle jets are reconstructed at midrapidity using the anti-kTâ algorithm with jet radius R = 0.4, and subjets are reconstructed by reclustering the jet constituents using the anti-kTâ algorithm with radii r = 0.1 and r = 0.2. In protonâproton collisions, we measure both the inclusive and leading subjet distributions. We compare these measurements to perturbative calculations at next-to-leading logarithmic accuracy, which suggest a large impact of threshold resummation and hadronization effects on the zrâ distribution. In heavy-ion collisions, we measure the leading subjet distributions, which allow access to a region of harder jet frag- mentation than has been probed by previous measurements of jet quenching via hadron fragmentation distributions. The zrâ distributions enable extraction of the parton-to-subjet fragmentation function and allow for tests of the universality of jet fragmentation functions in the quarkâgluon plasma (QGP). We find no significant modification of zrâ distributions in PbâPb compared to pp collisions. However, the distributions are also consistent with a hardening trend for zrâ< 0.95, as predicted by several jet quenching models. As zrâ â 1 our results indicate that any such hardening effects cease, exposing qualitatively new possibilities to disentangle competing jet quenching mechanisms. By comparing our results to theoretical calculations based on an independent extraction of the parton-to-jet fragmentation function, we find consistency with the universality of jet fragmentation and no indication of factorization breaking in the QGP.[graphic not available: see fulltext
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