Abstract: CERN-LHC. Measurements of the transverse momentum multiplicity dependences of Pion, Kaon, Proton and Lambda production in Proton-Lead collisions at a centre-of-mass energy/nucleon of 5.02 TeV. The dependences of the multiplicity and mean transverse momentum on the charged particle multiplicity density dN/dETARAP is also presented.

Multiplicity Dependence of Pion, Kaon, Proton and Lambda Production in p--Pb Collisions at sqrt(s_NN) = 5.02 TeV;ALICE Collaboration;2020;HEPData


Abstract: No data abstract available.

High precision measurements of Z boson production in PbPb collisions at $\sqrt{s_\mathrm{NN}} =$ 5.02 TeV;CMS Collaboration;2023;HEPData


Stress induces oxytocin–Gαi-dependent remodeling of astrocytes to shape neuronal response in the amygdala;Angel BAUDON;2024;Zenodo


Abstract: No data abstract available.

Elliptic anisotropy measurement of the f$_0$(980) hadron in proton-lead collisions and evidence for its quark-antiquark composition;CMS Collaboration;2024;HEPData


Abstract: The azimuthal anisotropy of $\mathrm{\Upsilon(1S)}$ mesons in high-multiplicity pPb collisions is studied using data collected by the CMS experiment at a nucleon-nucleon center-of-mass energy of 8.16 TeV. The $\mathrm{\Upsilon(1S)}$ mesons are reconstructed using the dimuon decay channel. The anisotropy, characterized by the second Fourier harmonic coefficient $v_2^{\mathrm{sub}}$, is determined using the two-particle correlation technique, in which the $\mathrm{\Upsilon(1S)}$ mesons are correlated with charged hadrons. A large psuedorapidity gap is used to suppress short-range correlations. The $v_2^{\mathrm{sub}}$ values are measured in four transverse momentum intervals in the range from 0 - 30 GeV/c. No azimuthal anisotropy is observed for the $\mathrm{\Upsilon(1S)}$ mesons in high-multiplicity pPb collisions, which is consistent with previous PbPb collision results. The results suggest that any collectivity on bottomonia is smaller than that of charmonia in pPb collisions.

Study of azimuthal anisotropy of $\Upsilon$(1S) mesons in pPb collisions at $\sqrt{s_\mathrm{NN}}$ = 8.16 TeV;CMS Collaboration;2024;HEPData


Abstract: The hydrodynamic flow-like behavior of charged hadrons in high-energy lead-lead collisions is studied through multiparticle correlations. The elliptic anisotropy values based on different orders of multiparticle cumulants, $v_{2}\{2k\}$, are measured up to the tenth order ($k = 5$) as functions of the collision centrality at a nucleon-nucleon center-of-mass energy of $\sqrt{s_{\rm{NN}}}=5.02~\textrm{Te}\textrm{V}$. The data were recorded by the CMS experiment at the LHC and correspond to an integrated luminosity of $0.607~\textrm{nb}^{-1}$. A hierarchy is observed between the coefficients, with $v_{2}\{2\} > v_{2}\{4\} \gtrsim v_{2}\{6\} \gtrsim v_{2}\{8\} \gtrsim v_{2}\{10\}$. Based on these results, centrality-dependent moments for the fluctuation-driven event-by-event $v_{2}$ distribution are determined, including the skewness, kurtosis and, for the first time, superskewness. Assuming a hydrodynamic expansion of the produced medium, these moments directly probe the initial-state geometry in high-energy nucleus-nucleus collisions.

Higher-order moments of the elliptic flow distribution in PbPb collisions at $\sqrt{s_\mathrm{NN}}$ = 5.02 TeV;CMS Collaboration;2024;HEPData


Abstract: The production of prompt $\Lambda_c^+$ baryons is measured via the exclusive decay channel $\Lambda_c^+ \to \mathrm{p} \mathrm{K}^- \pi^+$ at a center-of-mass energy per nucleon pair of $5.02~\mathrm{TeV}$ using $252~\mathrm{nb}^{-1}$ proton-proton (pp) and $0.607~\mathrm{nb}^{-1}$ lead-lead (PbPb) collisions collected at the CERN LHC in 2017 and 2018, respectively. The measurements are performed within the $\Lambda_c^+$ rapidity interval $|y|<1.0$ with transverse momentum ($p_\mathrm{T}$) ranges of 3--30 and 6--40 $\mathrm{GeV}/c$ for pp and PbPb collisions, respectively. Compared to pp collisions scaled by the number of nucleon-nucleon interactions, the observed yields of $\Lambda_c^+$ with $p_\mathrm{T}>10~\mathrm{GeV}/c$ are strongly suppressed in PbPb collisions. The level of suppression depends significantly on both the collision centrality and the $p_\mathrm{T}$ of the $\Lambda_c^+$ baryon. The $\Lambda_c^+/\mathrm{D}^0$ production ratio in PbPb collisions is consistent with the result in pp collisions for $p_\mathrm{T}>10~\mathrm{GeV}/c$, suggesting that the coalescence process of hadronization is not significant for PbPb collisions in the higher $p_\mathrm{T}$ region.

Study of charm hadronization with prompt $\Lambda^+_\mathrm{c}$ baryons in proton-proton and lead-lead collisions at $\sqrt{s_\mathrm{NN}}$ = 5.02 TeV;CMS Collaboration;2023;HEPData


Abstract: The first study in heavy ion collisions of the shapes of jets arising from bottom (b) quarks is presented. Jet shapes are studied using charged hadron constituents as a function of their radial distance from the jet axis. Lead-lead (PbPb) collision data at a nucleon-nucleon center-of-mass energy of $\sqrt{s_{NN}}=5.02$~TeV were recorded by the CMS detector at the LHC, with an integrated luminosity of $1.69~\mathrm{nb}^{-1}$. Compared to proton-proton collisions, the quark-gluon plasma (QGP) created in PbPb collisions causes a redistribution of the energy in b jets to larger distances from the jet axis. This QGP-induced redistribution is substantially larger for b jets than for inclusive jets.

Search for medium effects using jets from bottom quarks in PbPb collisions at $\sqrt{s_\mathrm{NN}}$ = 5.02 TeV;CMS Collaboration;2022;HEPData


Abstract: No data abstract available.

Multiplicity and transverse momentum dependence of charge-balance functions in pPb and PbPb collisions at LHC energies;CMS Collaboration;2024;HEPData


Abstract: Jet production in lead-lead (PbPb) and proton-proton (pp) collisions at a nucleon-nucleon center-of-mass energy of 5.02 TeV is studied with the CMS detector at the LHC, using PbPb and pp data samples corresponding to integrated luminosities of 404/μb and 27.4/pb, respectively. Jets with different areas are reconstructed using the anti-kT algorithm by varying the distance parameter R. The measurements are performed using jets with transverse momenta (pT) greater than 200 GeV and in a pseudorapidity range of |eta|< 2. To reveal the medium modification of the jet spectra in PbPb collisions, the properly normalized ratio of spectra from PbPb and pp data is used to extract jet nuclear modification factors as functions of the PbPb collision centrality, pT and, for the first time, as a function of R up to 1.0. For the most central collisions, a strong suppression is observed for high-pT jets reconstructed with all distance parameters, implying that a significant amount of jet energy is scattered to large angles. The dependence of jet suppression on R is expected to be sensitive to both the jet energy loss mechanism and the medium response, and so the data are compared to several modern event generators and analytic calculations. The models considered do not fully reproduce the data.

First measurement of large area jet transverse momentum spectra in heavy-ion collisions;CMS Collaboration;2021;HEPData


Abstract: A new algorithm is presented to discriminate reconstructed hadronic decays of tau leptons (tau_h) that originate from genuine tau leptons in the CMS detector against tau_h candidates that originate from quark or gluon jets, electrons, or muons. The algorithm inputs information from all reconstructed particles in the vicinity of a tau_h candidate and employs a deep neural network with convolutional layers to efficiently process the inputs. This algorithm leads to a significantly improved performance compared with the previously used one. For example, the efficiency for a genuine tau_h to pass the discriminator against jets increases by 10-30% for a given efficiency for quark and gluon jets. Furthermore, a more efficient tau_h reconstruction is introduced that incorporates additional hadronic decay modes. The superior performance of the new algorithm to discriminate against jets, electrons, and muons and the improved tau_h reconstruction method are validated with LHC proton-proton collision data at sqrt(s) = 13 TeV.

Identification of hadronic tau lepton decays using a deep neural network;CMS Collaboration;2022;HEPData


Abstract: No data abstract available.

Two-particle azimuthal correlations in $\gamma$p interactions using pPb collisions at $\sqrt{s_\mathrm{NN}}$ = 8.16 TeV;CMS Collaboration;2022;HEPData


Abstract: Production cross sections of $\Upsilon(1S)$, $\Upsilon(2S)$, and $\Upsilon(3S)$ states decaying into $\mu^{+}\mu^{-}$ in proton-lead (pPb) collisions are reported using data collected by the CMS experiment at $\sqrt{s_{_{\mathrm{NN}}}} = $ 5.02 TeV. A comparison is made with corresponding cross sections obtained with pp data measured at the same collision energy and scaled by the Pb nucleus mass number. The nuclear modification factor for $\Upsilon(1S)$ is found to be $R_{\mathrm{pPb}}(\Upsilon(1S)) = $ 0.806 $ \pm\ $ 0.024 (stat) $ \pm\ $ 0.059 (syst). Similar results for the excited states indicate a sequential suppression pattern, such that $R_{\mathrm{pPb}}(\Upsilon(1S)) > R_{\mathrm{pPb}}(\Upsilon(2S)) > R_{\mathrm{pPb}}(\Upsilon(3S))$. The suppression is much less pronounced in pPb than in PbPb collisions, and independent of transverse momentum $p^{\Upsilon}_{T}$ and center-of-mass rapidity $y^{\Upsilon}_{CM}$ of the individual $\Upsilon$ state in the studied range $p^{\Upsilon}_{T} < $ 30 GeV/c and $|y^{\Upsilon}_{CM}| < $ 1.93. Models that incorporate sequential suppression of bottomonia in pPb collisions are in better agreement with the data than those which only assume initial-state modifications.

Nuclear modification of $\Upsilon$ states in pPb collisions at $\sqrt{s_\mathrm{NN}}$ = 5.02 TeV;CMS Collaboration;2022;HEPData


Abstract: No data abstract available.

Observation of the B$_\mathrm{c}^+$ meson in PbPb and pp collisions at $\sqrt{s_{\mathrm{NN}}}$ = 5.02 TeV;CMS Collaboration;2022;HEPData


Abstract: Measurements of the second Fourier harmonic coefficient ($v_2$) of the azimuthal distributions of prompt and nonprompt D$^{0}$ mesons produced in pp and pPb collisions are presented. Nonprompt D$^{0}$ mesons come from beauty hadron decays. The data samples are collected by the CMS experiment at nucleon-nucleon center-of-mass energies of 13 and 8.16 TeV, respectively. In high multiplicity pp collisions, $v_2$ signals for prompt charm hadrons are reported for the first time, and are found to be comparable to those for light-flavor hadron species over a transverse momentum ($p_{\mathrm{T}}$) range of 2-6 GeV. Compared at similar event multiplicities, the prompt D$^{0}$ meson $v_2$ values in pp and pPb collisions are similar in magnitude. The $v_2$ values for open beauty hadrons are extracted for the first time via nonprompt D$^{0}$ mesons in D$^{0}$ collisions. For $p_{\mathrm{T}}$ in the range of 2-5 GeV, the results suggest that $v_2$ for nonprompt D$^{0}$ mesons is smaller than that for prompt D$^{0}$ mesons. These new measurements indicate a positive charm hadron $v_2$ in pp collisions and suggest a mass dependence in $v_2$ between charm and beauty hadrons in the pPb system. These results provide insights into the origin of heavy-flavor quark collectivity in small systems.

Studies of charm and beauty hadron long-range correlations in pp and pPb collisions at LHC energies;CMS Collaboration;2021;HEPData


Abstract: No data abstract available.

Fragmentation of jets containing a prompt J$/\psi$ meson in PbPb and pp collisions at $\sqrt{s_\mathrm{NN}} =$ 5.02 TeV;CMS Collaboration;2021;HEPData


Abstract: No data abstract available.

Using Z boson events to study parton-medium interactions in PbPb collisions;CMS Collaboration;2021;HEPData


Abstract: No data abstract available.

Studies of beauty suppression via nonprompt D$^0$ mesons in PbPb collisions at $\sqrt{s_\mathrm{NN}}=$ 5.02 TeV;CMS Collaboration;2020;HEPData


Abstract: CERN-LHC. The second-order Fourier coefficients ($v_{2}$) characterizing the azimuthal distribution of $\Upsilon(\mathrm{1S})$ and $\Upsilon(\mathrm{2S})$ mesons arising from PbPb collisions at $ {\sqrt {\smash [b]{s_{_{\mathrm {NN}}}}}} = $ 5.02 TeV are studied. The $\Upsilon$ mesons are reconstructed in their $\mathrm{dimuon}$ decay channel, as measured by the CMS detector. The data set was collected in 2018 and corresponds to an integrated luminosity of 1.7$\smash{\,\text{nb}^{-1}}$. The scalar product method is used to extract the $v_{2}$ coefficients of the azimuthal distribution. Results are reported for the rapidity range $|y|<2.4$, with the transverse momentum $0 < $ ${p_{\mathrm{T}}}$ $ < 50\smash{\,\text{GeV/c}}$, and in three centrality ranges of 10-30, 30-50 and 50-90%. In contrast to the J/$\psi$ mesons, no azimuthal anisotropy is observed for the $\Upsilon$ mesons.

Measurement of the azimuthal anisotropy of $\Upsilon$(1S) and $\Upsilon$(2S) mesons in PbPb collisions at $\sqrt{s_\mathrm{NN}} =$ 5.02 TeV;CMS Collaboration;2020;HEPData


Abstract: Azimuthal correlations of charged particles in xenon-xenon collisions at a center-of-mass energy per nucleon pair of $ \sqrt{s_{_\mathrm{NN}}} = 5.44~$TeV are studied. The data were collected by the CMS experiment at the LHC with a total integrated luminosity of $3.42~\mathrm{\mu b}^{-1}$. The collective motion of the system formed in the collision is parameterized by a Fourier expansion of the azimuthal particle density distribution. The azimuthal anisotropy coefficients $v_{2}$, $v_{3}$, and $v_{4}$ are obtained by the scalar-product, two-particle correlation, and multiparticle correlation methods. Within a hydrodynamic picture, these methods have different sensitivities to non-collective and fluctuation effects. The dependence of the Fourier coefficients on the size of the colliding system is explored by comparing the xenon-xenon results with equivalent lead-lead data. Model calculations that include initial-state fluctuation effects are also compared to the experimental results. The observed angular correlations provide new constraints on the hydrodynamic description of heavy ion collisions.

Charged-particle angular correlations in XeXe collisions at $\sqrt{s_{_\mathrm{NN}}}=$ 5.44 TeV;CMS Collaboration;2022;HEPData


Abstract: No data abstract available.

Production of $\Lambda_\mathrm{c}^+$ baryons in proton-proton and lead-lead collisions at $\sqrt{s_\mathrm{NN}}=$ 5.02 TeV;CMS Collaboration;2020;HEPData


Abstract: No data abstract available.

Measurement of B$^0_\mathrm{s}$ meson production in pp and PbPb collisions at $\sqrt{s_\mathrm{NN}} =$ 5.02 TeV;CMS Collaboration;2019;HEPData


Abstract: Ultrarelativistic heavy ion collisions recreate in the laboratory the thermodynamical conditions prevailing in the early universe up to $10^{-6}$ seconds, thereby allowing the study of the quark-gluon plasma (QGP), a state of quantum chromodynamics (QCD) matter with deconfined partons. The top quark, the heaviest elementary particle known, is accessible in nucleus-nucleus collisions at the CERN LHC, and constitutes a novel probe of the QGP. Here, we report the first-ever evidence for the production of top quarks in nucleus-nucleus collisions, using lead-lead collision data at a nucleon-nucleon centre-of-mass energy of 5.02 TeV recorded by the CMS experiment. Two methods are used to measure the cross section for top quark pair production ($\sigma_{\mathrm{t\bar{t}}}$) via the decay into charged leptons (electrons or muons) and bottom quarks. One method relies on the leptonic information alone, and the second one exploits, in addition, the presence of bottom quarks. The measured cross sections, $\sigma_{\mathrm{t\bar{t}}} = 2.54^{+0.84}_{-0.74}$ and $2.03^{+0.71}_{-0.64}\,\mu$b, respectively, are compatible with expectations from scaled proton-proton data and QCD predictions.

Evidence for top quark production in nucleus-nucleus collisions;CMS Collaboration;2020;HEPData


Abstract: No data abstract available.

Jet properties in PbPb and pp collisions at $\sqrt{s_\mathrm{NN}} =$ 5.02 TeV;CMS Collaboration;2019;HEPData


Abstract:
Measurement of the fiducial cross section of light-by-light scattering and exclusion limits on axion-like-particles in lead-lead collisions at a centre-of-mass energy of 5.02 TeV with 390 mub^-1 of data collected in 2015.

The fiducial region is defined as:
- 2Gamma
- pt_Gamma > 2 GeV
- $|\eta_{\gamma}| < 2.4$
- exluding 1.444<|$\eta$|<1.566 region
- m_GammaGamma > 5 GeV
- pt_GammaGamma < 1 GeV
- aco_GammaGamma < 0.01

Evidence for light-by-light scattering and searches for axion-like particles in ultraperipheral PbPb collisions at $\sqrt{s_\mathrm{NN}} =$ 5.02 TeV;CMS Collaboration;2020;HEPData


Abstract: CERN-LHC. The relative yields of Υ mesons produced in pp and PbPb collisions at 5.02TeV and reconstructed via the dimuon decay channel are measured using data collected by the CMS experiment. Double ratios are formed by comparing the yields of the excited states, Υ(2S) and Υ(3S), to the ground state, Υ(1S), in both PbPb and pp collisions at the same center-of-mass energy, in data collected in 2015. The double ratios are studied as a function of collision centrality, as well as Υ transverse momentum and rapidity.

Suppression of excited Upsilon states relative to the ground state in PbPb collisions at sqrt(sNN) = 5.02 TeV;CMS Collaboration;2018;HEPData


Abstract: No data abstract available.

Non-Gaussian elliptic-flow fluctuations in PbPb collisions at $\sqrt{\smash[b]{s_{_\text{NN}}}} = 5.02$ TeV;CMS Collaboration;2018;HEPData


Abstract: No data abstract available.

Study of jet quenching with Z+jet correlations in PbPb and pp collisions at sqrt(s[NN]) = 5.02 TeV;CMS Collaboration;2017;HEPData


Abstract: CERN-LHC. Measurement of leading and subleading modes using PCA and two-particle correlations for PbPb and pPb at centre-mass energy 2.76 TeV and 5.02 TeV respectively.

Principal-component analysis of two-particle azimuthal correlations in PbPb and pPb collisions at CMS;CMS Collaboration;2018;HEPData


Abstract: CERN-LHC. Inclusive jet spectra from pp and PbPb collisions at 2.76 TeV collected by the CMS experiment. Jets are reconstructed with three different distance parameters (R=0.2, 0.3, and 0.4) for transverse momentum pT>70GeV/c and pseudorapidity |eta|<2. The production cross sections and nuclear modification factor RAA is presented as function of pT and event centrality, for each R.

Measurement of inclusive jet cross-sections in pp and PbPb collisions at sqrt(s[NN])=2.76 TeV;CMS Collaboration;2018;HEPData


Abstract: Modifications to the distribution of charged particles with respect to high transverse momentum $(p_{\mathrm{T}})$ jets passing through a quark-gluon plasma are explored using the CMS detector. Back-to-back dijets are analyzed in lead-lead and proton-proton collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV via correlations of charged particles in bins of relative pseudorapidity and angular distance from the leading and subleading jet axes. In comparing the lead-lead and proton-proton collision results, modifications to the charged-particle relative distance distribution and to the momentum distributions around the jet axis are found to depend on the dijet momentum balance $x_{j}$, which is the ratio between the subleading and leading jet $p_{\mathrm{T}}$. For events with $x_{j} \approx 1$, these modifications are observed for both the leading and subleading jets. However, while subleading jets show significant modifications for events with a larger dijet momentum imbalance, much smaller modifications are found for the leading jets in these events.

In-medium modification of dijets in PbPb collisions at $\sqrt{s_\mathrm{NN}} =$ 5.02 TeV;CMS Collaboration;2021;HEPData


Abstract:
Objectives: As X-linked myotubular myopathy (XLMTM) is a rare
 neuromuscular disease caused by mutations in the MTM1 gene with a large
 phenotypic heterogeneity, to ensure clinical trial readiness, it was
 mandatory to better quantify disease burden and determine best outcomes
 measures. Methods: We designed an international prospective and
 longitudinal natural history study in patients with XLMTM and assessed
 muscle strength and motor and respiratory functions over the first year of
 follow-up. The humoral immunity against adeno-associated virus serotype 8
 was also monitored. Results: Forty-five male patients aged 3.5 months to
 56.8 years were enrolled between May 2014 and May 2017. Thirteen patients
 had a mild phenotype (no ventilation support), seven had an intermediate
 phenotype (ventilation support less than 12 hours a day), and twenty-five
 had a severe phenotype (ventilation support equal to or greater than 12
 hours a day). Most strength and motor function assessments could be
 performed even in very weak patients. MFM32 total score, grip and pinch
 strengths, and FVC, FEV1 and PCF measures discriminated the three groups
 of patients. Disease history revealed motor milestone loss in several
 patients. Longitudinal data on 37 patients shown a MFM32 total score
 significantly decreased by 2%. Of the 38 patients evaluated, anti-AAV8
 neutralizing activity was detected in 26% with two patients having an
 inhibitory titer >1:10. Conclusions: Our data confirm that XLMTM is
 slowly progressive for male survivors regardless of their phenotype and
 provide outcome validation and natural history data that can support
 clinical development in this population. NCT02057705.

Data from: X-linked myotubular myopathy: a prospective international natural history study;Mélanie Annoussamy;2019;Dryad

[ 23 ] Clinical trials Observational study (Cohort

Clinical trials Observational study Cohort

Quality of
 lifeQuality of life based on
 the PROMIS® systemNatHis-MTM_art-Neurol-Figure-e1.pdf


Abstract:
Objective: We took advantage of a large multinational recruitment to
 delineate genotype-phenotype correlations in a large, trans-European
 multicenter cohort of patients with spastic paraplegia gene 7 (SPG7).
 Methods: We analyzed clinical and genetic data from 241 patients with
 SPG7, integrating neurologic follow-up data. One case was examined
 neuropathologically. Results: Patients with SPG7 had a mean age of 35.5 ±
 14.3 years (n = 233) at onset and presented with spasticity (n = 89),
 ataxia (n = 74), or both (n = 45). At the first visit, patients with a
 longer disease duration (>20 years, n = 62) showed more cerebellar
 dysarthria (p < 0.05), deep sensory loss (p < 0.01), muscle
 wasting (p < 0.01), ophthalmoplegia (p < 0.05), and
 sphincter dysfunction (p < 0.05) than those with a shorter duration
 (<10 years, n = 93). Progression, measured by Scale for the
 Assessment and Rating of Ataxia evaluations, showed a mean annual increase
 of 1.0 ± 1.4 points in a subgroup of 30 patients. Patients homozygous for
 loss of function (LOF) variants (n = 65) presented significantly more
 often with pyramidal signs (p < 0.05), diminished visual acuity due
 to optic atrophy (p < 0.0001), and deep sensory loss (p <
 0.0001) than those with at least 1 missense variant (n = 176). Patients
 with at least 1 Ala510Val variant (58%) were older (age 37.6 ± 13.7 vs
 32.8 ± 14.6 years, p < 0.05) and showed ataxia at onset (p <
 0.05). Neuropathologic examination revealed reduction of the pyramidal
 tract in the medulla oblongata and moderate loss of Purkinje cells and
 substantia nigra neurons. Conclusions: This is the largest SPG7 cohort
 study to date and shows a spasticity-predominant phenotype of LOF variants
 and more frequent cerebellar ataxia and later onset in patients carrying
 at least 1 Ala510Val variant.

Data from: Loss of paraplegin drives spasticity rather than ataxia in a cohort of 241 patients with SPG7;Giulia Coarelli;2019;Dryad

Coarelli et al., Table
 4Table 4. New SPG7
 variants found in the analyzed cohort.Coarelli_Table
 4.docx


Abstract:
Biological invasions offer interesting situations to observe how novel
 interactions between closely related, formerly allopatric species may
 trigger phenotypic evolution in situ. Assuming that successful invaders
 are usually filtered to be competitively dominant, invasive and native
 species may follow different trajectories. Natives may evolve traits that
 minimize the negative impact of competition, while trait shifts in
 invasives should mostly reflect expansion dynamics, through selection for
 colonization ability and transiently enhanced mutation load at the
 colonization front. These ideas were tested through a large-scale
 common-garden experiment measuring life-history traits in two closely
 related snail species, one invasive and one native, co-occurring in a
 network of freshwater ponds in Guadeloupe. We looked for evidence of
 recent evolution by comparing uninvaded or recently invaded with
 long-invaded sites. The native species adopted a life history favoring
 rapid population growth (i.e. increased fecundity, earlier reproduction
 and increased juvenile survival) that may increase its prospects of
 coexistence with the more competitive invader. We discuss why these
 effects are more likely to result from genetic change than from maternal
 effects. The invader exhibited slightly decreased overall performances in
 recently colonized sites, consistent with a moderate expansion load
 resulting from local founder effects. Our study highlights a rare example
 of rapid life-history evolution following invasion.

data Physa acuta Aplexa
 marmoratamain
 dataappendix data_length of
 Pysa a and Aplexa m.appendix data on
 lengthappendix
 data_fecundity_Physa a. Aplexa m.appendix data on
 fecundity

Data from: Bioinvasion triggers rapid evolution of life-histories in freshwater snails;Elodie Chapuis;2017;Dryad


Abstract: No data abstract available.

Study of same-sign W boson scattering and anomalous couplings in events with one tau lepton from pp collisions at $\sqrt{s} $ = 13 TeV;CMS Collaboration;2024;HEPData


MATLAS ultra diffuse galaxies

MATLAS ultra diffuse galaxies;F.R. Marleau;2021;Centre de Donnees Strasbourg (CDS)

VizieR online Data Catalogue associated with article published in journal Astronomy and Astrophysics with title ' Ultra diffuse galaxies in the MATLAS low-to-moderate density fields.' (bibcode: 2021A&A...654A.105M)


Abstract: No data abstract available.

Pseudorapidity distributions of charged hadrons in lead-lead collisions at $\sqrt{s_\mathrm{NN}}$ = 5.36 TeV;CMS Collaboration;2024;HEPData


Abstract: In particle collider experiments, elementary particle interactions with large momentum transfer produce quarks and gluons (known as partons) whose evolution is governed by the strong force, as described by the theory of quantum chromodynamics (QCD). These partons subsequently emit further partons in a process that can be described as a parton shower which culminates in the formation of detectable hadrons. Studying the pattern of the parton shower is one of the key experimental tools for testing QCD. This pattern is expected to depend on the mass of the initiating parton, through a phenomenon known as the dead-cone effect, which predicts a suppression of the gluon spectrum emitted by a heavy quark of mass $m_{\rm{Q}}$ and energy $E$, within a cone of angular size $m_{\rm{Q}}$/$E$ around the emitter. Previously, a direct observation of the dead-cone effect in QCD had not been possible, owing to the challenge of reconstructing the cascading quarks and gluons from the experimentally accessible hadrons. We report the direct observation of the QCD dead cone by using new iterative declustering techniques to reconstruct the parton shower of charm quarks. This result confirms a fundamental feature of QCD. Furthermore, the measurement of a dead-cone angle constitutes a direct experimental observation of the non-zero mass of the charm quark, which is a fundamental constant in the standard model of particle physics.

Direct observation of the dead-cone effect in QCD;ALICE Collaboration;2022;HEPData


Abstract: No data abstract available.

First measurement of the absorption of $^{3}\overline{\rm He}$ nuclei in matter and impact on their propagation in the galaxy;ALICE Collaboration;2022;HEPData


Abstract: No data abstract available.

Strange hadron collectivity in pPb and PbPb collisions;CMS Collaboration;2022;HEPData


Abstract: The production of the charm-strange baryon $\Xi_{\rm c}^{0}$ is measured for the first time at the LHC via its semileptonic decay into e$^+\Xi^-\nu_{\rm e}$ in pp collisions at $\sqrt{s}=7$ TeV with the ALICE detector. The transverse momentum ($p_{\rm T}$) differential cross section multiplied by the branching ratio is presented in the interval 1 $<$ $p_{\rm T}$ $<$ 8~GeV/$c$ at mid-rapidity, $|y|$ $<$ 0.5. The transverse momentum dependence of the $\Xi_{\rm c}^{0}$ baryon production relative to the ${\rm D}^0$ meson production is compared to predictions of event generators with various tunes of the hadronisation mechanism, which are found to underestimate the measured cross-section ratio.

First measurement of $\Xi_{\rm c}^0$ production in pp collisions at $\mathbf{\sqrt{s}}$ = 7 TeV;ALICE Collaboration;2018;HEPData


Abstract: CERN-LHC. First results on K/pi, p/pi and K/p fluctuations are obtained with the ALICE detector at the CERN LHC as a function of centrality in Pb--Pb collisions at sqrt(s) = 2.76. The observable nu_dyn, which is defined in terms of the moments of particle multiplicity distributions, is used to quantify the magnitude of dynamical fluctuations of relative particle yields and also provides insight into the correlation between particle pairs. This study is based on a novel experimental technique, called the Identity Method, which allows one to measure the moments of multiplicity distributions in case of incomplete particle identification. The results for p/pi show a change of sign in nu_dyn from positive to negative towards more peripheral collisions. For central collisions, the results follow the smooth trend of the data at lower energies and nu_dyn exhibits a change in sign for p/pi and K/p.

Relative particle yield fluctuations in Pb-Pb collisions at ${\mathbf{\sqrt{s_{\rm NN}}=2.76}}$ TeV;ALICE Collaboration;2018;HEPData


Abstract:
The production of Z-bosons at large rapidities in Pb-Pb collisions at $\sqrt{s_{\rm NN}}=5.02$ TeV is reported.

Z-boson candidates are reconstructed in the dimuon decay channel (${\rm Z}^{0} \rightarrow \mu^{+}\mu^{-}$), based on muons selected with pseudo-rapidity $-4.0<\eta_{\mu}<-2.5$ and $p_{\rm T}^\mu>20$ GeV/$c$.

The invariant yield and the nuclear modification factor, $R_{AA}$, are presented as a function of rapidity and collision centrality.

The value of $R_{\rm AA}$ for the 0-20% central Pb-Pb collisions is $0.67 \pm 0.11 \, \mbox{(stat.)} \, \pm 0.03 \, \mbox{(syst.)} \, \pm 0.06 \, \mbox{(corr. syst.)}$, exhibiting a deviation of $2.6 \sigma$ from unity.

The results are well-described by calculations that include nuclear modifications of the parton distribution functions, while the predictions using vacuum PDFs deviate from data by $2.3\sigma$ in the 0-90% centrality class and by $3\sigma$ in the 0-20% central collisions.

Measurement of Z$^0$-boson production at large rapidities in Pb-Pb collisions at $\sqrt{s_{\rm NN}}=5.02$ TeV;ALICE Collaboration;2018;HEPData


Abstract: CERN-LHC. The Transition Radiation Detector (TRD) was designed and built to enhance the capabilities of the ALICE detector at the Large Hadron Collider (LHC). While aimed at providing electron identification and triggering, the TRD also contributes significantly to the track reconstruction and calibration in the central barrel of ALICE. In this paper the design, construction, operation, and performance of this detector are discussed. A pion rejection factor of up to 410 is achieved at a momentum of 1 GeV/$c$ in p-Pb collisions and the resolution at high transverse momentum improves by about 40% when including the TRD information in track reconstruction. The triggering capability is demonstrated both for jet, light nuclei, and electron selection.

The ALICE Transition Radiation Detector: construction, operation, and performance;ALICE Collaboration;2017;HEPData


Abstract: The transverse momentum ($p_{\mathrm{T}}$) spectra and elliptic flow coefficient ($v_{2}$) of deuterons and anti-deuterons at mid-rapidity ($|y|<0.5$) are measured with the ALICE detector at the LHC in Pb-Pb collisions at $\sqrt{s_{\mathrm{NN}}}$ = 2.76 TeV. The measurement of the $p_{\mathrm{T}}$ spectra of (anti-)deuterons is done up to 8 GeV/$c$ in 0-10\% centrality class and up to 6 GeV/$c$ in 10-20\% and 20-40\% centrality classes. The $v_{2}$ is measured in the 0.8 $<$ $p_{\mathrm{T}}$ $< $5 GeV/$c$ interval and in six different centrality intervals (0-5\%, 5-10\%, 10-20\%, 20-30\%, 30-40\% and 40-50\%) using the scalar product technique. Measured \pio$^{\pm}$, K$^{\pm}$ and p+$\overline{\mathrm{p}}$ transverse-momentum spectra and $v_{2}$ are used to predict the deuteron $p_{\mathrm{T}}$ spectra and $v_{2}$ within the Blast-Wave model. The predictions are able to reproduce the $v_{2}$ coefficient in the measured $p_{\mathrm{T}}$ range and the transverse-momentum spectra for $p_{\mathrm{T}}$ $>$ 1.8 GeV/$c$ within the experimental uncertainties. The measurement of the coalescence parameter $B_2$ is performed, showing a $p_{\mathrm{T}}$ dependence in contrast with the simplest coalescence model, which fails to reproduce also the measured $v_{2}$ coefficient. In addition, the coalescence parameter $B_2$ and the elliptic flow coefficient in the 20-40\% centrality interval are compared with the AMPT model which is able, in its version without string melting, to reproduce the measured $v_{2}$($p_{\mathrm{T}}$) and the $B_2$($p_{\mathrm{T}}$) trend.

Measurement of deuteron spectra and elliptic flow in Pb-Pb collisions at $\mathbf{\sqrt{s_{\rm NN}}}$ = 2.76 TeV at the LHC;ALICE Collaboration;2017;HEPData


Abstract: CERN-LHC. The production of muons from heavy-flavour hadron decays in p--Pb collisions at $\sqrt{s_{\rm NN}}=5.02$~TeV was studied for $2

Production of muons from heavy-flavour hadron decays in p-Pb collisions at $\mathbf{\sqrt{{\textit s}_{NN}} = 5.02}$ TeV;ALICE Collaboration;2017;HEPData


Abstract: CERN-LHC. We report a precise measurement of the J/$\psi$ elliptic flow in Pb-Pb collisions at $\sqrt{s_{\rm NN}}=5.02$ TeV with the ALICE detector at the LHC. The J/$\psi$ mesons are reconstructed at mid-rapidity ($|y| < 0.9$) in the dielectron decay channel and at forward rapidity ($2.5

J/$\psi$ elliptic flow in Pb-Pb collisions at $\mathbf{\sqrt{s_{\rm NN}}}$ = 5.02 TeV;ALICE Collaboration;2017;HEPData


Abstract: No data abstract available.

First measurement of jet mass in Pb-Pb and p-Pb collisions at the LHC;ALICE Collaboration;2017;HEPData


Abstract: CERN-LHC. The azimuthal anisotropy coefficient $v_2$ of prompt $D^0$, $D^+$, $D^{*+}$ and $D_s^+$ mesons was measured in mid-central (30-50% centrality class) Pb-Pb collisions at a centre-of-mass energy per nucleon pair $\sqrt{s_{\rm NN}}$ = 5.02 TeV, with the ALICE detector at the LHC. The D mesons were reconstructed via their hadronic decays at mid-rapidity, |$y$|<0.8, in the transverse momentum interval 1<$p_{\rm T}$<24 GeV/$c$. The measured D-meson $v_2$ has similar values as that of charged pions. The $D_s^+$ $v_2$, measured for the first time, is found to be compatible with that of non-strange D mesons. The measurements are compared with theoretical calculations of charm-quark transport in a hydrodynamically expanding medium and have the potential to constrain medium parameters.

D-meson azimuthal anisotropy in mid-central Pb-Pb collisions at $\mathbf{\sqrt{s_{\rm NN}}=5.02}$ TeV;ALICE Collaboration;2017;HEPData


Abstract:
CERN-LHC. We present the charged-particle pseudorapidity density in Pb-Pb collisions at $\sqrt{s_{_{\mathrm{NN}}}}=5.02\,\mathrm{TeV}$ in centrality classes measured by ALICE. The measurement covers a wide pseudorapidity range from $-3.5$ to $5$, which is sufficient for reliable estimates of the total number of charged particles produced in the collisions. For the most central collisions we find $21\,400\pm 1\,300$ while for the most peripheral we find $230\pm 38$. This corresponds to an increase of $(27\pm4)\%$ over the results at $\sqrt{s_{_{\mathrm{NN}}}}=2.76\,\mathrm{TeV}$ previously reported by ALICE. The energy dependence of the total number of charged particles produced in heavy-ion collisions is found to obey a modified power-law like behaviour. The charged-particle
pseudorapidity density of the most central collisions is compared to model calculations - none of which fully describes the measured distribution. We also present an estimate of the rapidity density of charged particles. The width of that distribution is found to exhibit a remarkable proportionality to the beam rapidity, independent of the collision energy from the top SPS to LHC energies.

Centrality dependence of the pseudorapidity density distribution for charged particles in Pb-Pb collisions at $\sqrt{s_{\rm NN}}=5.02$ TeV;ALICE Collaboration;2017;HEPData


Abstract:
Measuring K$^0_{\rm S}$K$^0_{\rm S}$ and K$^{\rm \pm}$K$^{\rm \pm}$
three-dimensional femtoscopic correlations using Pb-Pb collisions at
$\mathbf {\sqrt{s_{\rm NN}}=2.76}$ TeV

LHC ALICE collaboration
KchKch and K0sK0s femtoscopy from 2.76 TeV/nucleon Pb-Pb collision
0-10%, 10-30% and 30-50% centrality, -0.8 < eta < 0.8

We present the results of three-dimensional femtoscopic analyses for charged and neutral kaons recorded by ALICE in Pb-Pb collisions at $\sqrt{s_{\rm{NN}}}$ = 2.76 TeV. The $m_{\mathrm{T}}$ scaling predicted by pure hydrodynamic models appears to be broken in our data, which indicates the importance of the hadronic rescattering phase at LHC energies. A $k_{\mathrm{T}}$ scaling of pion and kaon source radii is observed instead. The time of maximal emission of the system is estimated using the three-dimensional femtoscopic analysis for kaons. The measured emission time is larger than that of pions. Our observations are well supported by the hydrokinetic model predictions.
For correlation functions (Figure 2, Figure 3) the errors are statistical only, systematic uncertainties are equal to or less than the statistical errors.
For all other figures total errors are presented.

Kaon femtoscopy in Pb-Pb collisions at $\sqrt{s_{\rm{NN}}}$ = 2.76 TeV;ALICE Collaboration;2017;HEPData


Abstract: The measurement of azimuthal correlations of charged particles is presented for Pb–Pb collisions at 2.76 TeV and p–Pb collisions at 5.02 TeV with the ALICE detector at the CERN Large Hadron Collider. These correlations are measured for the second, third and fourth order flow vector in the pseudorapidity region eta < 0.8 as a function of centrality and transverse momentum pT using two observables, to search for evidence of pT-dependent flow vector fluctuations. For Pb–Pb collisions at 2.76 TeV, the measurements indicate that pT-dependent fluctuations are only present for the second order flow vector. Similar results have been found for p–Pb collisions at 5.02 TeV. These measurements are compared to hydrodynamic model calculations with event-by-event geometry fluctuations in the initial state to constrain the initial conditions and transport properties of the matter created in Pb–Pb and p–Pb collisions.

Searches for transverse momentum dependent flow vector fluctuations in Pb-Pb and p-Pb collisions at the LHC;ALICE Collaboration;2017;HEPData


Abstract: CERN-LHC. The elliptic flow of electrons from heavy-flavour hadron decays at mid-rapidity ($|y|$ $<$ 0.7) is measured in Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 2.76$ TeV with ALICE at the LHC. The particle azimuthal distribution with respect to the reaction plane can be parametrized with a Fourier expansion, where the second coefficient ($v_{\rm 2}$) represents the elliptic flow. The $v_{\rm 2}$ coefficient of inclusive electrons is measured in three centrality classes (0-10%, 10-20% and 20-40%) with the event plane and the scalar product methods in the transverse momentum ($p_{\rm T}$) intervals 0.5-13 GeV/$c$ and 0.5-8 GeV/$c$, respectively. After subtracting the background, mainly from photon conversions and Dalitz decays of neutral mesons, a positive $v_{\rm 2}$ of electrons from heavy-flavour hadron decays is observed in all centrality classes, with a maximum significance of $5.9\sigma$ in the interval $2 <$ $p_{\rm T}$ $<$ 2.5 GeV/$c$ in semi-central collisions (20-40%). The value of $v_{\rm 2}$ decreases towards more central collisions at low and intermediate $p_{\rm T}$ (0.5 $<$ $p_{\rm T}$ $<$ 3 GeV/$c$). The $v_{\rm 2}$ of electrons from heavy-flavour hadron decays at mid-rapidity is found to be similar to the one of muons from heavy-flavour hadron decays at forward rapidity (2.5 $<$ $y$ $<$ 4). The results are described within uncertainties by model calculations including substantial elastic interactions of heavy quarks with an expanding strongly-interacting medium.

Elliptic flow of electrons from heavy-flavour hadron decays at mid-rapidity in Pb-Pb collisions at $\mathbf{\sqrt{s_\mathrm{NN}}}$ = 2.76 TeV;ALICE Collaboration;2016;HEPData


Abstract:
The W and Z boson production was measured via the muonic decay channel in p-Pb collisions at $\sqrt{s_{\rm NN}}=5.02$ TeV at the Large Hadron Collider with the ALICE detector.
The measurement covers backward ($-4.46 < y_{\rm cms} < -2.96$) and forward ($2.03 < y_{\rm cms} < 3.53$) rapidity regions, corresponding to Pb-going and p-going directions, respectively.
The Z-boson production cross section, with dimuon invariant mass of $6010$ GeV/$c$ are determined.
The W-boson production is also studied as a function of the collision centrality: the cross section of muons from W-boson decays is found to scale with the average number of binary nucleon-nucleon collisions within uncertainties.

W and Z boson production in p-Pb collisions at $\sqrt{s_{\rm NN}}$ = 5.02 TeV;ALICE Collaboration;2017;HEPData


Abstract: CERN-LHC. The pseudorapidity density of charged particles ($\mathrm{d}N_\mathrm{ch}/\mathrm{d}\eta$) at mid-rapidity in Pb-Pb collisions has been measured at a center-of-mass energy per nucleon pair of $\sqrt{s_{\rm NN}}$ = 5.02 TeV.

Centrality dependence of the charged-particle multiplicity density at mid-rapidity in Pb-Pb collisions at $\sqrt{s_{\rm NN}}$ = 5.02 TeV;ALICE Collaboration;2016;HEPData


Abstract: CERN-LHC. The inclusive production of the $\psi$(2S) charmonium state was studied as a function of centrality in p-Pb collisions at the nucleon-nucleon center of mass energy $\sqrt{s_{\rm NN}}$ = 5.02 TeV at the CERN LHC. The measurement was performed with the ALICE detector in the center of mass rapidity ranges $-4.46

Centrality dependence of $\mathbf{\psi}$(2S) suppression in p-Pb collisions at $\mathbf{\sqrt{{\textit s}_{\rm NN}}}$ = 5.02 TeV;ALICE Collaboration;2016;HEPData


Abstract: The production of K$^{*0}$ and $\phi$ mesons are measured with the ALICE detector in pp and Pb-Pb collisions at the centre-of-mass energy per nucleon pair, $\sqrt{s_{\rm NN}}$ = 2.76 TeV. The invariant yield of K$^{*0}$ and $\phi$ for rapidity $|y|<0.5$ are presented as a function of transverse momentum ($p_{\rm T}$). The K$^{*0}$ and $\phi$ invariant yields are compared with model calculation for inelastic pp collisions. The $p_{\rm T}$ dependent particle ratios such K$^{*0}$/K, K$^{*0}/\pi$, $\phi$/K, $\phi/\pi$, p/K$^{*0}$ and p/$\phi$ in inelastic pp and Pb--Pb collisions are obtained. The nuclear modification factor $R_{\rm AA}$ was computed using a proton-proton reference at $\sqrt{s} = 2.76$ TeV.

K$^{*}(892)^{0}$ and $\phi(1020)$ meson production at high transverse momentum in pp and Pb-Pb collisions at $\sqrt{s_\mathrm{NN}}$ = 2.76 TeV;ALICE Collaboration;2017;HEPData


Abstract: CERN-LHC. An invariant differential cross section measurement of inclusive $\pi^{0}$ and $\eta$ meson production at mid-rapidity in pp collisions at $\sqrt{s}=8$~TeV was carried out by the ALICE experiment at the LHC. The spectra of $\pi^{0}$ and $\eta$ mesons are measured in transverse momentum ranges of $0.33.5$~GeV/$c$. However, a deviation from this empirical scaling rule is observed for transverse momenta below $p_{\rm T}<3.5$~GeV/$c$ in the $\eta/\pi^{0}$ ratio with a significance of $6.2\sigma$.

$\pi^0$ and $\eta$ meson production in proton-proton collisions at $\sqrt{s}=8$ TeV;ALICE Collaboration;2018;HEPData


Abstract: CERN-LHC. The evolution of the near-side jet peak is studied in Pb-Pb collisions at 2.76 TeV as a function of centrality and $p_{\rm T}$ and in pp collisions at the same energy as a function of $p_{\rm T}$.

Evolution of the longitudinal and azimuthal structure of the near-side jet peak in Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 2.76$ TeV;ALICE Collaboration;2018;HEPData


Abstract: CERN-LHC. Direct photon production at mid-rapidity in Pb-Pb collisions at $\sqrt{s_{_{\mathrm{NN}}}} = 2.76$ TeV was studied in the transverse momentum range $0.9 < p_\mathrm{T} < 14$ GeV$/c$. Photons were detected with the highly segmented electromagnetic calorimeter PHOS and via conversions in the ALICE detector material with the $e^+e^-$ pair reconstructed in the central tracking system. The results of the two methods were combined and direct photon spectra were measured for the 0-20%, 20-40%, and 40-80% centrality classes. For all three classes, agreement was found with perturbative QCD calculations for $p_\mathrm{T} \gtrsim 5$ GeV$/c$. Direct photon spectra down to $p_\mathrm{T} \approx 1$ GeV$/c$ could be extracted for the 20-40% and 0-20% centrality classes. The significance of the direct photon signal for $0.9 < p_\mathrm{T} < 2.1$ GeV$/c$ is $2.6\sigma$ for the 0-20% class. The spectrum in this $p_\mathrm{T}$ range and centrality class can be described by an exponential with an inverse slope parameter of $(297 \pm 12^\mathrm{stat}\pm 41^\mathrm{syst})$ MeV. State-of-the-art models for photon production in heavy-ion collisions agree with the data within uncertainties.

Direct photon production in Pb-Pb collisions at $\sqrt{s_\rm{NN}}$ = 2.76 TeV;ALICE Collaboration;2016;HEPData


Abstract:
CERN-LHC.

We present measurements of the azimuthal dependence of charged jet production in central and semi-central $\sqrt{s}_{NN}$ = 2.76 TeV Pb--Pb collisions with respect to the second harmonic event plane, quantified as $v_2^{ch~jet}$. Jet finding is performed employing the anti-$k_{T}$ algorithm with a resolution parameter $R$ = 0.2 using charged tracks from the ALICE tracking system. The contribution of the azimuthal anisotropy of the underlying event is taken into account event-by-event. The remaining (statistical) region-to-region fluctuations are removed on an ensemble basis by unfolding the jet spectra for different event plane orientations independently.

Azimuthal anisotropy of charged jet production in $\sqrt{s_{\rm NN}}$ = 2.76 TeV Pb-Pb collisions;ALICE Collaboration;2016;HEPData


Abstract: No description provided.

Azimuthally differential pion femtoscopy in Pb-Pb collisions at $\sqrt{s_{\rm NN}}=2.76$ TeV;ALICE Collaboration;2017;HEPData


Abstract: In ultrarelativistic heavy-ion collisions, the event-by-event variation of the elliptic flow $v_2$ reflects fluctuations in the shape of the initial state of the system. This allows us to systematically study events corresponding to the same centrality but different initial geometry. This selection technique, Event Shape Engineering, has been used in the analysis of charge-dependent two- and three-particle correlations in Pb—Pb collisions at $\sqrt{s_{\rm NN}} = 2.76$ TeV. The two-particle correlator $\langle \cos(\varphi_{\alpha} - \varphi_{\beta}) \rangle$, calculated for different combinations of charges $\alpha$ and $\beta$, is almost independent of $v_2$ (for a given centrality), while the three-particle correlator $\langle \cos(\varphi_{\alpha} + \varphi_{\beta} - 2\Psi_2) \rangle$ scales almost linearly both with the event $v_2$ and charged-particle pseudorapidity density. The charge dependence of the three-particle correlator is often interpreted as evidence for the Chiral Magnetic Effect (CME), a parity violating effect of the strong interaction. However, its measured dependence on $v_2$ points to a large non-CME contribution to the correlator. Comparing the results with Monte Carlo calculations including a magnetic field due to the spectators, the upper limit of the CME signal contribution to the three-particle correlator in the 10-50% centrality interval is found to be 26-33% at 95% confidence level.

Constraining the magnitude of the Chiral Magnetic Effect with Event Shape Engineering in Pb-Pb collisions at $\sqrt{s_{\rm NN}}$ = 2.76$ TeV;ALICE Collaboration;2017;HEPData


Abstract: CERN-LHC. The production of prompt D$_s^+$ mesons was measured for the first time in collisions of heavy nuclei with the ALICE detector at the LHC. The analysis was performed on a data sample of Pb-Pb collisions at a centre-of-mass energy per nucleon pair, $\sqrt{s_{\rm NN}}$, of 2.76 TeV in two different centrality classes, namely 0-10% and 20-50%. The nuclear modification factor $R_{\rm AA}$ was computed by comparing the $p_{\rm T}$-differential production yields in Pb-Pb collisions to those in proton-proton (pp) collisions at the same energy. The production ratios D$_s^+$/D$^0$ and D$_s^+$\D$^+$ were also measured in Pb-Pb collisions and compared to their values in proton-proton collisions.

Measurement of D$_s^+$ production and nuclear modification factor in Pb-Pb collisions at $\sqrt{s_{\rm NN}}=2.76$ TeV;ALICE Collaboration;2016;HEPData


Abstract: CERN-LHC. Measurements of charged jet production as a function of centrality are presented for p-Pb collisions recorded at $\sqrt{s_{\rm NN}} = 5.02$ TeV with the ALICE detector. Centrality classes are determined via the energy deposit in neutron calorimeters at zero degree, close to the beam direction, to minimise dynamical biases of the selection. The corresponding number of participants or binary nucleon-nucleon collisions is determined based on the particle production in the Pb-going rapidity region. Jets have been reconstructed in the central rapidity region from charged particles with the anti-$k_{\rm T}$ algorithm for resolution parameters $R = 0.2$ and $R = 0.4$ in the transverse momentum range 20 to 120 GeV/$c$. The reconstructed jet momentum and yields have been corrected for detector effects and underlying-event background.

Centrality dependence of charged jet production in p-Pb collisions at $\sqrt{s_\mathrm{NN}}$ = 5.02 TeV;ALICE Collaboration;2016;HEPData


Abstract: CERN-LHC. Two-particle angular correlations between trigger particles in the forward pseudorapidity range ($2.5 < |\eta| < 4.0$) and associated particles in the central range ($|\eta| < 1.0$) are measured with the ALICE detector in p-Pb collisions at a nucleon-nucleon centre-of-mass energy of 5.02 TeV. The trigger particles are reconstructed using the muon spectrometer, and the associated particles by the central barrel tracking detectors. In high-multiplicity events, the double-ridge structure, previously discovered in two-particle angular correlations at midrapidity, is found to persist to the pseudorapidity ranges studied in this Letter. The second-order Fourier coefficients for muons in high-multiplicity events are extracted after jet-like correlations from low-multiplicity events have been subtracted. The coefficients are found to have a similar transverse momentum ($p_{\rm T}$) dependence in p-going (p-Pb) and Pb-going (Pb-p) configurations, with the Pb-going coefficients larger by about $16\pm6$%, rather independent of $p_{\rm T}$ within the uncertainties of the measurement.

Forward-central two-particle correlations in p-Pb collisions at $\sqrt{s_{\rm NN}}$ = 5.02 TeV;ALICE Collaboration;2016;HEPData


Abstract: CERN-LHC. The yields of strange (${\rm K}^{0}_{S}$, $\Lambda$, $\bar{\Lambda}$) and multi-strange ($\Xi^{-}$, $\bar{\Xi}^{+}$, $\Omega^{-}$, $\bar{\Omega}^{+}$) hadrons are measured at midrapidity in proton-proton (pp) collisions at $\sqrt{s}$ = 7 TeV as a function of the charged-particle multiplicity density (${\rm d}N_{\rm ch}/{\rm d}\eta$).The production rate of strange particles increases faster than that of non-strange hadrons, leading to an enhancement of strange particles relative to pions, similar to that found in nucleus-nucleus collisions as well as in proton-nucleus collisions at the LHC. This is the first observation of an enhanced production of strange particles in high-multiplicity pp collisions. The magnitude of this strangeness enhancement increases with the event activity, quantified by ${\rm d}N_{\rm ch}/{\rm d}\eta$, and with hadron strangeness. It reaches almost a factor of two for the $\Omega$ at the highest multiplicity presented. No enhancement is observed for particles with no strange quark content, demonstrating that the observed effect is strangeness rather than mass related. The results are not reproduced by any of the Monte Carlo models commonly used at the LHC, suggesting that further developments are needed for a complete microscopic understanding of strangeness production and indicating the presence of a phenomenon novel in high-multiplicity pp collisions.

Enhanced production of multi-strange hadrons in high-multiplicity proton-proton collisions;ALICE Collaboration;2017;HEPData


Abstract: The azimuthal correlations of D mesons and charged particles were measured with the ALICE detector in pp collisions at $\sqrt{s}=7$ TeV and p-Pb collisions at $\sqrt{s_{\rm NN}}=5.02$ TeV at the Large Hadron Collider. D$^0$, D$^+$, and D$^{*+}$ mesons with transverse momentum $3<~p_{\rm T}<~16$ GeV/$c$ and rapidity in the nucleon-nucleon centre-of-mass system $|y_{\rm cms}|<~0.5$ (pp collisions) and $-0.96<~y_{\rm cms}<~0.04$ (p-Pb collisions) were correlated to charged particles with $p_{\rm T}>0.3$ Gev/$c$. The properties of the correlation peak induced by the jet containing the D meson, described in terms of the yield of charged particles in the peak and peak width, are compatible within uncertainties between the two collision systems, and described by Monte-Carlo simulations based on the PYTHIA and POWHEG event generators.

Measurement of azimuthal correlations of D mesons and charged particles in pp collisions at $\sqrt{s}=7$ TeV and p-Pb collisions at $\sqrt{s_{\rm NN}}=5.02$ TeV;ALICE Collaboration;2017;HEPData


Abstract: CERN-LHC. The anisotropic flow coefficients relative to the second, third and fourth harmonic ($v_2$, $v_3$ and $v_4$, respectively) are measured with two- and multi-particle correlation techniques in Pb-Pb collisions at 5.02 TeV, recorded in November 2015 with the ALICE detector at the CERN Large Hadron Collider. The measurements are performed in the central pseudorapidity region (|$\eta$| < 0.8) and transverse momentum range 0.2 < $p_{\rm T}$ < 5.0 GeV/$c$.

Anisotropic flow of charged particles in Pb-Pb collisions at $\sqrt{s_{\rm NN}}=5.02$ TeV;ALICE Collaboration;2017;HEPData


Abstract: CERN-LHC. The production of J/$\psi$ and $\psi$(2S) was studied with the ALICE detector in Pb-Pb collisions at the LHC. The measurement was performed at forward rapidity ($2.5

Differential studies of inclusive J/$\psi$ and $\psi$(2S) production at forward rapidity in Pb-Pb collisions at $\mathbf{\sqrt{{\textit s}_{_{NN}}}}$ = 2.76 TeV;ALICE Collaboration;2016;HEPData


Abstract:
Measurements of charged particle pseudorapidity densities and multiplicities in pp collisions at centre-of-mass energies from 900 to 8000 GeV in the pseudorapidity range -2 to 2.

Results are given for three normalizations:

- INEL -the sum of all inelastic interactions
- NSD -non-single diffractive, i.e. non-diffractive and double processes only
- INEL > 0 class of events, which requires at least one charged particle in the final state in the pseudorapidiy range -1 to 1.

Charged-particle multiplicities in proton-proton collisions at $\sqrt{s}$ = 0.9 to 8 TeV;ALICE Collaboration;2017;HEPData


Abstract: CERN-LHC. We report on results obtained with the Event Shape Engineering technique applied to Pb-Pb collisions at $\sqrt{s_\rm{NN}}=2.76$ TeV. By selecting events in the same centrality interval, but with very different average flow, different initial state conditions can be studied. We find the effect of the event-shape selection on the elliptic flow coefficient $v_2$ to be almost independent of transverse momentum $p_\rm{T}$, as expected if this effect is due to fluctuations in the initial geometry of the system. Charged hadron, pion, kaon, and proton transverse momentum distributions are found to be harder in events with higher-than-average elliptic flow, indicating an interplay between radial and elliptic flow.

Event shape engineering for inclusive spectra and elliptic flow in Pb-Pb collisions at $\sqrt{s_\rm{NN}}=2.76$ TeV;ALICE Collaboration;2016;HEPData


Abstract: This represents the first experimental evidence of the attractive strong interaction between a proton and a $\phi$ meson. The result is obtained from two-particle correlations of combined $\mathrm{p}-\phi\oplus\mathrm{\overline{p}}-\phi$ pairs measured in high-multiplicity pp collisions at $\sqrt{s} = 13$ TeV by the ALICE collaboration. The spin-averaged scattering length and effective range of the $\mathrm{p}-\phi$ interaction are extracted from the fully corrected correlation function employing the Lednick'y-Lyuboshits approach. In particular, the imaginary part of the scattering length vanishes within uncertainties, indicating that inelastic processes do not play a prominent role for the $\mathrm{p}-\phi$ interaction. These data demonstrate that the interaction is dominated by elastic $\mathrm{p}-\phi$ scattering. Furthermore, an analysis employing phenomenological Gaussian- and Yukawa-type potentials is conducted. This work provides valuable experimental input to accomplish a self-consistent description of the N-$\phi$ interaction, which is particularly relevant for the more fundamental studies on partial restoration of chiral symmetry in nuclear medium.

Experimental evidence for an attractive p-$\phi$ interaction;ALICE Collaboration;2021;HEPData


Abstract: The production of electrons from beauty-hadron decays was measured at midrapidity in proton--proton (pp) and central Pb--Pb collisions at center-of-mass energy per nucleon--nucleon pair $\sqrt{s_{\rm{NN}}} = 5.02~{\rm TeV}$, using the ALICE detector at the LHC. The cross section measured in pp collisions in the transverse momentum interval $2< p_{T} < 8$ GeV/c was compared with models based on perturbative quantum chromodynamics calculations. The yield in the 10% most central Pb--Pb collisions, measured in the interval $2< p_{T} < 26$ GeV/c, was used to compute the nuclear modification factor $R_{AA}$, extrapolating the pp reference cross section to $p_{T}$ larger than 8 GeV/c. The measured $R_{AA}$ shows significant suppression of the yield of electrons from beauty-hadron decays at high $p_{T}$ and does not show a significant dependence on $p_{T}$ above 8 GeV/c within uncertainties. The results are described by several theoretical models based on different implementations of the interaction of heavy quarks with a quark--gluon plasma, which predict a smaller energy loss for beauty quarks compared to light and charm quarks.

Measurement of electrons from beauty-hadron decays in pp and Pb-Pb collisions at $\sqrt{s_{\rm NN}}$ = 5.02 TeV;ALICE Collaboration;2023;HEPData


Abstract: No data abstract available.

Inclusive and multiplicity dependent production of electrons from heavy-flavour hadron decays in pp and p$-$Pb collisions;ALICE Collaboration;2023;HEPData


Abstract: The ALICE Collaboration reports the first fully-corrected measurements of the $N$-subjettiness observable for track-based jets in heavy-ion collisions. This study is performed using data recorded in pp and Pb--Pb collisions at centre-of-mass energies of $\sqrt{s}= 7$ TeV and $\sqrt{s_{\rm NN}} = 2.76$ TeV, respectively. In particular the ratio of 2-subjettiness to 1-subjettiness, $\tau_{2}/\tau_{1}$, which is sensitive to the rate of two-pronged jet substructure, is presented. Energy loss of jets traversing the strongly interacting medium in heavy-ion collisions is expected to change the rate of two-pronged substructure relative to vacuum. The results are presented for jets with a resolution parameter of $R = 0.4$ and charged jet transverse momentum of $40 \leq p_{\rm T,\rm jet} \leq 60$ GeV/$c$, which constitute a larger jet resolution and lower jet transverse momentum interval than previous measurements in heavy-ion collisions. This has been achieved by utilising a semi-inclusive hadron-jet coincidence technique to suppress the larger jet combinatorial background in this kinematic region. No significant modification of the $\tau_{2}/\tau_{1}$ observable for track-based jets in Pb--Pb collisions is observed relative to vacuum PYTHIA6 and PYTHIA8 references at the same collision energy. The measurements of $\tau_{2}/\tau_{1}$, together with the splitting aperture angle $\Delta R$, are also performed in pp collisions at $\sqrt{s}=7$ TeV for inclusive jets. These results are compared with PYTHIA calculations at $\sqrt{s}=7$ TeV, in order to validate the model as a vacuum reference for the Pb--Pb centre-of-mass energy. The PYTHIA references for $\tau_{2}/\tau_{1}$ are shifted to larger values compared to the measurement in pp collisions. This hints at a reduction in the rate of two-pronged jets in Pb--Pb collisions compared to pp collisions.

First measurements of N-subjettiness in central Pb-Pb collisions at $ \sqrt{s_{\mathrm{NN}}} $ = 2.76 TeV;ALICE Collaboration;2021;HEPData


Abstract: No data abstract available.

Production of K$^{*}(892)^{0}$ and $\phi(1020)$ in pp and Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV;ALICE Collaboration;2023;HEPData


Abstract:
CERN-LHC. The first results on K*(892)$^{\pm}$ resonance production in inelastic pp collisions at LHC energies of $\sqrt{s}$ = 5.02, 8, and 13 TeV are reported. The K*(892)$^{\pm}$ has been reconstructed via its hadronic decay channel K*(892)$^{\pm} \rightarrow$ $\mathrm {K^0_S}$ $~+~\pi^{\pm}$ with the ALICE detector. Transverse momentum distributions measured at mid-rapidity, integrated yields, and mean transverse momenta are presented.
The ratio of each measured p$_{T}$ distribution for K*(892)$^{\pm}$ mesons at $\sqrt{s}$ = 5.02, 8 and 13 TeV to the K*(892)$^{0}$ spectrum at the same collision energy is reported. The ratio of each measured p$_{T}$ distribution for K*(892)$^{\pm}$ mesons at
$\sqrt{s}$ = 5.02 and 13 TeV to the K spectrum at the same collision energy is also reported. The pp data at $\sqrt{s}$ = 5.02 and 13 TeV were collected in 2015 while data at $\sqrt{s}$ = 8 TeV were collected in 2012, with integrated luminosities of 2.12, 0.92 and 1.25 nb$^{-1}$, respectively.

Measurement of K$^{*}$(892)$^{\mathrm{\pm}}$ production in inelastic pp collisions at the LHC;ALICE Collaboration;2022;HEPData


Abstract: The path-length dependent parton energy loss within the quark-gluon plasma created in lead-lead collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV is studied by determining the azimuthal anisotropies for high-$p_{\mathrm{T}}$ dijets. The anisotropies are expressed as the Fourier expansion coefficients $v_{2}$, $v_{3}$, and $v_{4}$. The data were collected by the CMS experiment in 2018 and correspond to an integral luminosity of 1.7 $\mathrm{nb}^{-1}$. Jet-hadron and hadron-hadron correlations from events with back-to-back dijets are constructed as functions of relative azimuthal angle and pseudorapidity between a jet and a hadron and between two hadrons, respectively. Together, these correlations allow for a determination of the dijet $v_{n}$ values assuming factorization. Restricting the analysis to long-range components of the correlations provides robust suppression of background contributions from fragmentation processes. Positive dijet $v_{2}$ values are found that show a strong centrality dependence, consistent with previous high-$p_{\mathrm{T}}$ hadron and inclusive jet measurements. The dijet $v_{3}$ and $v_{4}$ values are consistent with zero, which is also seen for high-$p_{\mathrm{T}}$ hadron $v_{3}$ values in previous studies.

Azimuthal anisotropy of dijet events in PbPb collisions at $\sqrt{s_\mathrm{NN}}$ = 5.02 TeV;CMS Collaboration;2022;HEPData


Abstract: CERN-LHC-CMS. Observation of double $\mathrm{J}\mspace{-2mu}/\mspace{-2mu}\psi$ meson production in pPb collisions at $\sqrt{s_\mathrm{NN}} = 8.16\,\mathrm{TeV}$.

Observation of double J/$\psi$ meson production in pPb collisions at $\sqrt{s_\mathrm{NN}}$ = 8.16 TeV;CMS Collaboration;2024;HEPData


Abstract: The total charm-quark production cross section per unit of rapidity $\mathrm{d}\sigma(\mathrm{c\bar{c}})/\mathrm{d}y$, and the fragmentation fractions of charm quarks to different charm-hadron species $f(\mathrm{c}\rightarrow \mathrm{h}_\mathrm{c})$, are measured for the first time in p-Pb collisions at $\sqrt{s_\mathrm{NN}}=5.02\,$TeV at midrapidity ($-0.96

Charm fragmentation fractions and ${\rm c\overline{c}}$ cross section in p$-$Pb collisions at $\sqrt{s_{\rm NN}}=5.02$ TeV;ALICE Collaboration;2024;HEPData


Abstract: Transverse momentum spectra of antideuterons as a function of rapidity, measured in pp collisions at centre-of-mass per nucleon-nucleon energy of 13 TeV, are shown in Fig. 1. The coalescence parameters B2 as a function of the transverse momentum per nucleon are reported in Fig. 2.

Rapidity dependence of antideuteron coalescence in pp collisions at $\sqrt{s}$ = 13 TeV with ALICE;ALICE Collaboration;2024;HEPData


Abstract: The first measurement of $_{\Lambda}^{3}\mathrm{H}$ and $^3_ {\overline{\Lambda}}\overline{\mathrm{H}}$ differential production with respect to transverse momentum and centrality in Pb$-$Pb collisions at $\sqrt{s_{\mathrm{NN}}}=5.02$ TeV is presented. The $_{\Lambda}^{3}\mathrm{H}$ has been reconstructed via its two-charged-body decay channel, i.e., $_{\Lambda}^{3}\mathrm{H} \rightarrow {}^{3}\mathrm{He} + \pi^{-}$. A Blast-Wave model fit of the $p_{\rm T}$-differential spectra of all nuclear species measured by the ALICE collaboration suggests that the $_{\Lambda}^{3}\mathrm{H}$ kinetic freeze-out surface is consistent with that of other nuclei. The ratio between the integrated yields of $_{\Lambda}^{3}\mathrm{H}$ and $^3\mathrm{He}$ is compared to predictions from the statistical hadronisation model and the coalescence model, with the latter being favoured by the presented measurements.

Measurement of ${}_{\Lambda}^{3}\mathrm{H}$ production in Pb-Pb collisions at $\sqrt{s_{\mathrm{NN}}}$ = 5.02 TeV;ALICE Collaboration;2024;HEPData


Abstract: A study of strange hadron production associated with hard scattering processes and with the underlying event is conducted to investigate the origin of the enhanced production of strange hadrons in small collision systems characterised by large charged-particle multiplicities. The production of the single-strange meson ${\rm K}^{0}_{\rm{S}}$ and the double-strange baryon $\Xi^{\pm}$ is measured, in each event, in the azimuthal direction of the highest-$p_{\rm T}$ particle (trigger particle), related to hard scattering processes, and in the direction transverse to it in azimuth, associated with the underlying event, in pp collisions at $\sqrt{s}=5.02$ TeV and $\sqrt{s}=13$ TeV using the ALICE detector at the LHC. The per-trigger yields of ${\rm K}^{0}_{\rm{S}}$ and $\Xi^{\pm}$ are dominated by the transverse-to-leading production (i.e., in the direction transverse to the trigger particle), whose contribution relative to the toward-leading production is observed to increase with the event charged-particle multiplicity. The transverse-to-leading and the toward-leading $\Xi^{\pm}$/${\rm K}^{0}_{\rm{S}}$ yield ratios increase with the multiplicity of charged particles, suggesting that strangeness enhancement with multiplicity is associated with both hard scattering processes and the underlying event. The relative production of $\Xi^{\pm}$ with respect to ${\rm K}^{0}_{\rm{S}}$ is higher in transverse-to-leading processes over the whole multiplicity interval covered by the measurement. The ${\rm K}^{0}_{\rm{S}}$ and $\Xi^{\pm}$ per-trigger yields and yield ratios are compared with predictions of three different phenomenological models, namely Pythia8.2 with the Monash tune, Pythia8.2 with ropes and EPOS LHC. The comparison shows that none of them can quantitatively describe either the transverse-to-leading or the toward-leading yields of ${\rm K}^{0}_{\rm{S}}$ and $\Xi^{\pm}$.

Investigating strangeness enhancement with multiplicity in pp collisions using angular correlations;ALICE Collaboration;2024;HEPData


Abstract: The inclusive production of the charm-strange baryon $\Omega^0_{\rm c}$ is measured for the first time via its semileptonic decay into $\Omega^{-}\rm e^{+}\nu_{e}$ at midrapidity ($|y|<0.8$) in proton proton (pp) collisions at the centre-of-mass energy $\sqrt{s}=13$ TeV with the ALICE detector at the LHC. The transverse momentum ($p_{\rm T}$) differential cross section multiplied by the branching ratio is presented in the interval $2

Measurement of $\Omega^0_{\rm c}$ baryon production and branching-fraction ratio ${\rm BR(\Omega^0_c \rightarrow \Omega^- e^+\nu_e)} / {\rm BR(\Omega^0_c \rightarrow \Omega^- \pi^+)}$ in pp collisions at $\sqrt{s}$ = 13 TeV;ALICE Collaboration;2024;HEPData


Abstract: The two-particle momentum correlation functions between charm mesons (D$^{*\pm}$ and D$^{\pm}$) and charged light-flavor mesons ($\uppi^{\pm}$ and K$^{\pm}$) in all charge-combinations are measured for the first time by the ALICE Collaboration in high-multiplicity proton--proton collisions at a center-of-mass energy of $\sqrt(s)=13$ TeV. For DK and D$^*$K pairs, the experimental results are in agreement with theoretical predictions of the residual strong interaction based on quantum chromodynamics calculations on the lattice and chiral effective field theory. In the case of D$\uppi$ and D$^*\uppi$ pairs, tension between the calculations including strong interactions and the measurement is observed. For all particle pairs, the data can be adequately described by Coulomb interaction only, indicating a shallow interaction between charm and light-flavor mesons. Finally, the scattering lengths governing the residual strong interaction of the D$\uppi$ and D$^*\uppi$ systems are determined by fitting the experimental correlation functions with a model that employs a Gaussian potential. The extracted values are small and compatible with zero.

Studying the interaction between charm and light-flavor mesons;ALICE Collaboration;2024;HEPData


Abstract: First measurements of hadron(h)-$\Lambda$ azimuthal angular correlations in p--Pb collisions at $\sqrt{s_{\text{NN}}}= 5.02$ TeV using the ALICE detector at the LHC are presented. These correlations are used to separate the production of associated $\Lambda$ baryons into three different kinematic regions, namely those produced in the direction of the trigger particle (near-side), those produced in the opposite direction (away-side), and those whose production is uncorrelated with the jet-axis (underlying event). The per-trigger associated $\Lambda$ yields in these regions are extracted, along with the near- and away-side azimuthal peak widths, and the results are studied as a function of associated particle $p_{\text{T}}$ and event multiplicity. Comparisons with the DPMJET event generator and previous measurements of the $\phi(1020)$ meson are also made. The final results indicate that strangeness production in the highest multiplicity p-Pb collisions is enhanced relative to low multiplicity collisions in the jet-like regions, as well as the underlying event. The production of $\Lambda$ relative to charged hadrons is also enhanced in the underlying event when compared to the jet-like regions. Additionally, the results hint that strange quark production in the away-side of the jet is modified by soft interactions with the underlying event.

Investigating $\Lambda$ baryon production in p-Pb collisions in jets and the underlying event using angular correlations;ALICE Collaboration;2024;HEPData


Abstract: The $p_{T}$-differential production cross sections of non-prompt $D^{0}$, $D^{+}$, and $D^{+}_{s}$ mesons originating from beauty-hadron decays are measured in proton--proton collisions at a centre-of-mass energy $\sqrt{s}$ of 13 TeV. The measurements are performed at midrapidity, $|y| < 0.5$, with the data sample collected by ALICE from 2016 to 2018. The results are in agreement with predictions from several perturbative QCD calculations. The fragmentation fraction of beauty quarks to strange mesons divided by the one to non-strange mesons, $f_{s}/(f_{u}+f_{d})$, is found to be $0.114 \pm 0.016~{\mathrm (stat.)} \pm 0.006~{\mathrm (syst.)} \pm 0.003~{\mathrm (BR)} \pm 0.003~{\mathrm (extrap.)}$. This value is compatible with previous measurements at lower centre-of-mass energies and in different collision systems in agreement with the assumption of universality of fragmentation functions. In addition, the dependence of the non-prompt D meson production on the centre-of-mass energy is investigated by comparing the results obtained at $\sqrt{s} = 5.02$ and 13~TeV, showing a hardening of the non-prompt D-meson $p_{T}$-differential production cross section at higher $\sqrt{s}$. Finally, the ${\mathrm b\overline{b}}$ production cross section per unit of rapidity at midrapidity is calculated from the non-prompt $D^{0}$, $D^{+}$, $D^{+}_{s}$, and $\Lambda_{c}$ hadron measurements, obtaining $\mathrm{d}\sigma/{\mathrm d}y = 75.2\pm 3.2~(\mathrm{stat.}) \pm 5.2~(\mathrm{syst.})^{+12.3}_{-3.2} ~(\mathrm{extrap.})$$\mu$b

Measurement of beauty-quark production in pp collisions at $\sqrt{s}=13$ TeV via non-prompt D mesons;ALICE Collaboration;2024;HEPData


Abstract: In this letter, measurements of (anti)alpha production in central (0-10%) Pb--Pb collisions at a center-of-mass energy per nucleon--nucleon pair of $\sqrt{s_{\mathrm{NN}}}$ = 5.02 TeV are presented, including the first measurement of an antialpha transverse-momentum spectrum. Owing to its large mass, (anti)alpha production yields and transverse-momentum spectra are of particular interest because they provide a stringent test of particle production models. The averaged antialpha and alpha spectrum is included into a common blast-wave fit with lighter particles, indicating that the (anti)alpha also participates in the collective expansion of the medium created in the collision. A blast-wave fit including only protons, (anti)alpha, and other light nuclei results in a similar flow velocity as the fit that includes all particles. A similar flow velocity, but a significantly larger kinetic freeze-out temperature is obtained when only protons and light nuclei are included in the fit. The coalescence parameter $B_4$ is well described by calculations from a statistical hadronization model but significantly underestimated by calculations assuming nucleus formation via coalescence of nucleons. Similarly, the (anti)alpha-to-proton ratio is well described by the statistical hadronization model. On the other hand, coalescence calculations including approaches with different implementations of the (anti)alpha substructure tend to underestimate the data.

Measurement of (anti)alpha production in central Pb-Pb collisions at $\sqrt{s_{\rm NN}}$ = 5.02 TeV;ALICE Collaboration;2024;HEPData


Abstract:
The measurement of coherent $K^+K^-$ photoproduction
in ultra-peripheral Pb$-$Pb collisions at $\sqrt{s_\mathrm{NN}}$ = 5.02 TeV is presented. These
results are based on the data sample collected by the ALICE detector during the
2015 LHC Pb$-$Pb run.

Photoproduction of K$^{+}$K$^{-}$ pairs in ultra-peripheral collisions;ALICE Collaboration;2024;HEPData


Abstract: No data abstract available.

Probing the Chiral Magnetic Wave with charge-dependent flow measurements in Pb-Pb collisions at the LHC;ALICE Collaboration;2023;HEPData


Abstract: Measurements of higher-order fluctuations of $\langle p_\mathrm{T}\rangle$ distribution in Pb$-$Pb collisions, Xe$-$Xe collisions at $\sqrt{s_\mathrm{NN}}$ = 5.02 TeV and in pp collisions at at $\sqrt{s}$ = 5.02 TeV using the ALICE detector at the CERN LHC. Standardized skewness, intensive skewness and kurtosis of $\langle p_\mathrm{T}\rangle$ are presented as a function of $\langle\mathrm{d}N_\mathrm{ch}/\mathrm{d}\eta\rangle^{1/3}_{|\eta|<0.5}$ for all the collision systems. The charged particles are selected in the transverse momentum range, 0.2 < $p_\mathrm{T}$ (GeV/c) < 3.0 and pseudorapidity range, $|\eta|$ < 0.8.

Skewness and kurtosis of mean transverse momentum fluctuations at the LHC energies;ALICE Collaboration;2024;HEPData


Abstract: No data abstract available.

Study of flavor dependence of the baryon-to-meson ratio in proton-proton collisions at $\sqrt{s} = 13$ TeV;ALICE Collaboration;2023;HEPData


Abstract: The first measurement of the multiplicity dependence of intra-jet properties of leading charged-particle jets in proton-proton (pp) collisions is reported. The mean charged-particle multiplicity and jet fragmentation distributions are measured in minimum-bias and high-multiplicity pp collisions at center-of-mass energy $\sqrt{s}$ = 13 TeV using the ALICE detector. Jets are reconstructed from charged particles produced in the midrapidity region ($|\eta| < 0.9$) using the sequential recombination anti-$k_{\rm T}$ algorithm with jet resolution parameters $R$ = 0.2, 0.3, and 0.4 for the transverse momentum ($p_{\rm T}$) interval 5$-$110 GeV/$c$. The high-multiplicity events are selected by the forward V0 scintillator detectors. The mean charged-particle multiplicity inside the leading jet cone rises monotonically with increasing jet $p_{\rm T}$ in qualitative agreement with previous measurements at lower energies. The distributions of jet fragmentation function variables $z^{\rm ch}$ and $\xi^{\rm ch}$ are measured for different jet-$p_{\rm T}$ intervals. Jet-$p_{\rm T}$ independent fragmentation of leading jets is observed for wider jets except at high- and low-$z^{\rm ch}$ values. The observed ``hump-backed plateau'' structure in the $\xi^{\rm ch}$ distribution indicates suppression of low-$p_{\rm T}$ particles. In high-multiplicity events, an enhancement of the fragmentation probability of low-$z^{\rm ch}$ particles accompanied by a suppression of high-$z^{\rm ch}$ particles is observed compared to minimum-bias events. This behavior becomes more prominent for low-$p_{\rm T}$ jets with larger jet radius. The results are compared with predictions of QCD-inspired event generators, PYTHIA 8 with Monash 2013 tune and EPOS LHC. It is found that PYTHIA 8 qualitatively reproduces the jet modification in high-multiplicity events except at high jet $p_{\rm T}$. These measurements provide important constraints to models of jet fragmentation.

Multiplicity dependence of charged-particle intra-jet properties in pp collisions at $\sqrt{s}$ = 13 TeV;ALICE Collaboration;2024;HEPData


Abstract: The ALICE Collaboration reports a search for jet quenching effects in high-multiplicity (HM) proton--proton collisions at $\sqrt{s} = 13$ TeV, using the semi-inclusive azimuthal-difference distribution $\Delta\varphi$ of charged-particle jets recoiling from a high transverse momentum (high-$p_{\mathrm{T,trig}}$) trigger hadron. Jet quenching may broaden the $\Delta\varphi$ distribution measured in HM events compared to that in minimum bias (MB) events. The measurement employs a $p_{\mathrm{T,trig}}$-differential observable for data-driven suppression of the contribution of multiple partonic interactions, which is the dominant background. While azimuthal broadening is indeed observed in HM compared to MB events, similar broadening for HM events is observed for simulations based on the PYTHIA 8 Monte Carlo generator, which does not incorporate jet quenching. We elucidate the origin of the broadening by comparing biases induced by HM selection in the data and simulations, and discuss its implications for the study of jet quenching in small collision systems.

Search for jet quenching effects in high-multiplicity pp collisions at $\sqrt{s}$ = 13 TeV via di-jet acoplanarity;ALICE Collaboration;2024;HEPData


Abstract:
CERN-LHC. Measurement of inclusive J/$\psi$ pair production cross section in pp collisions at $\sqrt{s}$ = 13 TeV.

Quarkonia:
- in their dimuon decay
- pT>0

Measurement of inclusive J/$\psi$ pair production cross section in pp collisions at $\sqrt{s} = 13$ TeV;ALICE Collaboration;2023;HEPData


Abstract: No data abstract available.

Modification of charged-particle jets in event-shape engineered Pb$-$Pb collisions at $\sqrt{s_{\rm NN}} = 5$ TeV;ALICE Collaboration;2024;HEPData


Abstract: The femtoscopic study of pairs of identical pions is particularly suited to investigate the effective source function of particle emission, due to the resulting Bose--Einstein correlation signal. In small collision systems at the LHC, pp in particular, the majority of the pions are produced in resonance decays, which significantly affect the profile and size of the source. In this work, we explicitly model this effect in order to extract the primordial source in pp collisions at $\sqrt{s}~=~13~$TeV from charged $\pi$$-$$\pi$ correlations measured by ALICE. We demonstrate that the assumption of a Gaussian primordial source is compatible with the data and that the effective source, resulting from modifications due to resonances, is approximately exponential, as found in previous measurements at the LHC. The universality of hadron emission in pp collisions is further investigated by applying the same methodology to characterize the primordial source of K$-$p pairs. The size of the primordial source is evaluated as a function of the transverse mass ($m_{\mathrm{T}}$) of the pairs, leading to the observation of a common scaling for both $\pi$$-$$\pi$ and K$-$p, suggesting a collective effect. Further, the present results are compatible with the $m_{\mathrm{T}}$ scaling of the $\mathrm{p\mbox{-}p}$ and p$-\Lambda$ primordial source measured by ALICE in high multiplicity pp collisions, providing compelling evidence for the presence of a common emission source for all hadrons in small collision systems at the LHC. This will allow the determination of the source function for any hadron--hadron pairs with high precision, granting access to the properties of the possible final-state interaction among pairs of less abundantly produced hadrons, such as strange or charmed particles.

Common femtoscopic hadron-emission source in pp collisions at the LHC;ALICE Collaboration;2024;HEPData


Abstract: 'Measurements of inclusive charged-particle jet production in pp and p-Pb collisions at center-of-mass energy per nucleon-nucleon collision $\sqrt{s_{\rm NN}} = 5.02$ TeV and the corresponding nuclear modification factor $R_{\rm pPb}^{\rm ch~jet}$ are presented, using data collected with the ALICE detector at the LHC. Jets are reconstructed in the central rapidity region $|\eta_{\rm jet}| < 0.5$ from charged particles using the anti-$k_{\rm T}$ algorithm with resolution parameters $R = 0.2$, $0.3$, and $0.4$. The $p_{\rm T}$-differential inclusive production cross section of charged-particle jets, as well as the corresponding cross-section ratios, are reported for pp and p-Pb collisions in the transverse momentum range $10

Measurement of inclusive charged-particle jet production in pp and p-Pb collisions at $\sqrt{s_{\rm NN}}=5.02$ TeV;ALICE Collaboration;2024;HEPData


Abstract: Recent measurements of charm-baryon production in hadronic collisions have questioned the universality of charm-quark fragmentation across different collision systems. In this work the fragmentation of charm quarks into charm baryons is probed, by presenting the first measurement of the longitudinal jet momentum fraction carried by $\Lambda_{\rm{c}}^{+}$ baryons, $z_{\parallel}$, in hadronic collisions. The results are obtained in proton--proton (pp) collisions at $\sqrt{s}=13$ TeV at the LHC, with $\Lambda_{\rm{c}}^{+}$ baryons and track-based jets reconstructed in the transverse momentum intervals of $3 \leq p_{\rm{T}}^{\Lambda_{\rm{c}}^{+}} < 15$ GeV$/\it{c}$ and $7 \leq p_{\rm{T}}^{\rm{jet,ch}} < 15$ GeV$/\it{c}$, respectively. The $z_{\parallel}$ distribution is compared to a measurement of D$^{0}$-tagged charged jets in pp collisions as well as to PYTHIA 8 simulations. The data hints that the fragmentation of charm quarks into charm baryons is softer with respect to charm mesons, as predicted by hadronisation models which include colour correlations beyond leading-colour in the string formation.

Exploring the non-universality of charm hadronisation through the measurement of the fraction of jet longitudinal momentum carried by $\Lambda_{\rm c}^+$ baryons in pp collisions;ALICE Collaboration;2024;HEPData


Abstract: Exclusive and dissociative J/psi photoproduction, and exclusive dimuon production, in p–Pb collisions at sqrt(s_NN) = 8.16 TeV

Exclusive and dissociative J/$\psi$ photoproduction, and exclusive dimuon production, in p$-$Pb collisions at $\sqrt{s_{\rm NN}} = 8.16$ TeV;ALICE Collaboration;2023;HEPData


Abstract: CERN-LHC. The measurement of the production of $\rm{f}_{0}(980)$ in inelastic pp collisions at $\sqrt{s}$ = 5.02 TeV is presented. This is the first reported measurement of inclusive $\rm{f}_{0}(980)$ yield at LHC energies. The production is measured at midrapidity, $\left | y \right | < 0.5$, in a wide transverse momentum range, $0

${\rm f}_{0}(980)$ production in inelastic pp collisions at $\sqrt{s} = 5.02$ TeV;ALICE Collaboration;2023;HEPData


Abstract: No data abstract available.

Measurements of chemical potentials in Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV;ALICE Collaboration;2024;HEPData


Abstract: The ALICE Collaboration reports measurements of the semi-inclusive distribution of charged-particle jets recoiling from a high transverse momentum (high $p_\mathrm{T}$) charged hadron, in pp and central Pb--Pb collisions at center of mass energy per nucleon--nucleon collision $\sqrt{s_\mathrm{NN}}=5.02$ TeV. The large uncorrelated background in central Pb--Pb collisions is corrected using a data-driven statistical approach, which enables precise measurement of recoil jet distributions over a broad range in $p_\mathrm{T,ch jet}$ and jet resolution parameter $R$. Recoil jet yields are reported for $R=$ 0.2, 0.4, and 0.5 in the range $7

Measurements of jet quenching using semi-inclusive hadron+jet distributions in pp and central Pb$-$Pb collisions at $\sqrt{s_{\rm NN}}=5.02$ TeV;ALICE Collaboration;2024;HEPData


Abstract: Measurements of the production cross sections of prompt $\mathrm{D}^0$, $\mathrm{D}^+$, $\mathrm{D}^{*+}$, $\mathrm{D}^+_\mathrm{c}$, $\Lambda^+_\mathrm{c}$, and $\Xi^+_\mathrm{c}$ charm hadrons at midrapidity in proton$-$proton collisions at $\sqrt{s}=13$ TeV with the ALICE detector are presented. The D-meson cross sections as a function of transverse momentum ($p_\mathrm{T}$) are provided with improved precision and granularity. The ratios of $p_\mathrm{T}$-differential meson production cross sections based on this publication and on measurements at different rapidity and collision energy provide a constraint on gluon parton distribution functions at low values of Bjorken-$x$ ($10^{-5}-10^{-4}$). The measurements of $\Lambda^+_\mathrm{c}$ ($\Xi^+_\mathrm{c}$) baryon production extend the measured $p_\mathrm{T}$ intervals down to $p_\mathrm{T}=0(3)$~GeV$/c$. These measurements are used to determine the charm-quark fragmentation fractions and the $\mathrm{c}\bar{\mathrm{c}}$ production cross section at midrapidity ($|y|<0.5$) based on the sum of the cross sections of the weakly-decaying ground-state charm hadrons $\mathrm{D}^0$, $\mathrm{D}^+$, $\mathrm{D}^+_\mathrm{c}$, $\Lambda^+_\mathrm{c}$, $\Xi^0_\mathrm{c}$ and, for the first time, $\Xi^+_\mathrm{c}$, and of the strongly-decaying $J/\psi$ mesons. The first measurements of $\Xi^+_\mathrm{c}$ and $\Sigma_\mathrm{c}^{0,+,++}$ fragmentation fractions at midrapidity are also reported. A significantly larger fraction of charm quarks hadronising to baryons is found compared to $\mathrm{e}^+\mathrm{e}^-$ and ep collisions. The $\mathrm{c}\bar{\mathrm{c}}$ production cross section at midrapidity is found to be at the upper bound of state-of-the-art perturbative QCD calculations.

Charm production and fragmentation fractions at midrapidity in pp collisions at $\sqrt{s} = 13$ TeV;ALICE Collaboration;2023;HEPData


Abstract: The azimuthal ($\Delta\varphi$) correlation distributions between heavy-flavor decay electrons and associated charged particles are measured in pp and p$\textendash$Pb collisions at $\sqrt{s_{\rm{NN}}} = 5.02$ TeV. Results are reported for electrons with transverse momentum $4

Azimuthal correlations of heavy-flavor hadron decay electrons with charged particles in pp and p-Pb collisions at $\sqrt{s_{\rm NN}}$ = 5.02 TeV;ALICE Collaboration;2023;HEPData


Abstract: Two-particle transverse momentum differential correlators, recently measured in Pb$-$Pb collisions at LHC energies, provide an additional tool to gain insights into particle production mechanisms and infer transport properties, such as the ratio of shear viscosity to entropy density, of the medium created in Pb$-$Pb collisions. The longitudinal long-range correlations and the large azimuthal anisotropy measured at low transverse momenta in small collision systems, namely pp and p$-$Pb, at LHC energies resemble manifestations of collective behaviour. This suggests that locally equilibrated matter may be produced in these small collision systems, similar to what is observed in Pb$-$Pb collisions. In this work, the same two-particle transverse momentum differential correlators are exploited in pp and p$-$Pb collisions at $\sqrt{s} = 7\;\text{TeV}$ and $\sqrt{s_{\rm NN}} = 5.02\;\text{TeV}$, respectively, to seek evidence for viscous effects. Specifically, the strength and shape of the correlators are studied as a function of the produced particle multiplicity to identify evidence for longitudinal broadening that might reveal the presence of viscous effects in these smaller systems. The measured correlators and their evolution from pp and p$-$Pb to Pb$-$Pb collisions are additionally compared to predictions from Monte Carlo event generators, and the potential presence of viscous effects is discussed.

Two-particle transverse momentum correlations in pp and p-Pb collisions at LHC energies;ALICE Collaboration;2023;HEPData


Abstract: CERN-LHC. Fluctuation measurements are important sources of information on the mechanism of particle production at LHC energies. This article reports the first experimental results on third-order cumulants of the net-proton distributions in Pb--Pb collisions at a center-of-mass energy 5.02 TeV recorded by the ALICE detector. The results on the second-order cumulants of net-proton distributions at 2.76 and 5.02 TeV are also discussed in view of effects due to the global and local baryon number conservation. The results demonstrate the presence of long-range rapidity correlations between protons and antiprotons. Such correlations originate from the early phase of the collision. The experimental results are compared with HIJING and EPOS model calculations, and the dependence of the fluctuation measurements on the phase-space coverage is examined in the context of lattice quantum chromodynamics (LQCD) and hadron resonance gas (HRG) model estimations. The measured third-order cumulants are consistent with zero within experimental uncertainties of about 4% and are described well by LQCD and HRG predictions.

Closing in on critical net-baryon fluctuations at LHC energies: cumulants up to third order in Pb$-$Pb collisions;ALICE Collaboration;2022;HEPData


Abstract: Charge-dependent two- and three-particle correlations measured in Xe-Xe collisions at $\sqrt{s_{\mathrm{NN}}} = 5.44$ TeV are presented. Results are obtained for charged particles in the pseudorapidity range $|\eta|<0.8$ and transverse momentum interval $0.2 \le p_{\rm T} < 5.0$ GeV/$c$ for different collision centralities. The three-particle correlator $\gamma_{\alpha\beta} \equiv \langle \cos(\varphi_\alpha + \varphi_\beta - 2\Psi_2) \rangle$, calculated for different combinations of charge sign $\alpha$ and $\beta$, is expected to be sensitive to the presence of the Chiral Magnetic Effect (CME). Its magnitude is similar to the one observed in Pb-Pb collisions in contrast to a smaller CME signal in Xe-Xe collisions than in Pb-Pb collisions predicted by Monte Carlo (MC) calculations including a magnetic field induced by the spectator protons. These observations point to a large non-CME contribution to the correlator. Furthermore, the charge dependence of $\gamma_{\alpha\beta}$ can be described by a blast wave model calculation that incorporates background effects and by the Anomalous Viscous Fluid Dynamics model with values of the CME signal consistent with zero. The Xe-Xe and Pb-Pb results are combined with the expected CME signal dependence on the system size from the MC calculations including a magnetic field to obtain the fraction of CME contribution in $\gamma_{\alpha\beta}$, $f_{\rm CME}$. The CME fraction is compatible with zero for the most 30% central events in both systems and then becomes positive; averaging over the 0-70% centrality interval yields an upper limit of 2% (3%) and 25% (32%) at 95% (99.7%) confidence level for the CME signal contribution to $\gamma_{\alpha\beta}$ in Xe-Xe and Pb-Pb collisions, respectively.

Search for the Chiral Magnetic Effect with charge-dependent azimuthal correlations in Xe-Xe collisions at $\sqrt{s_{\mathrm{NN}}} = 5.44$ TeV;ALICE Collaboration;2024;HEPData


Abstract: No data abstract available.

Measurement of the radius dependence of charged-particle jet suppression in Pb-Pb collisions at $\sqrt{s_{\rm NN}}$ = 5.02 TeV;ALICE Collaboration;2024;HEPData


Abstract: The interaction of K$^-$ with protons is characterised by the presence of several coupled channels, systems like $\mathrm{\overline{K}^0 n}$ and $\pi \Sigma$ with a similar mass and the same quantum numbers as the K$^-$p state. The strengths of these couplings to the K$^-$p system are of crucial importance for the understanding of the nature of the $\Lambda(1405)$ resonance and of the attractive K$^-$p strong interaction. In this article, we present measurements of the K$^-$p correlation functions in relative momentum space obtained in pp collisions at $\sqrt{s}$ = 13 TeV, in p-Pb collisions at $\sqrt{s_{\mathrm{NN}}}$ = 5.02 TeV, and (semi)peripheral Pb-Pb collisions at $\sqrt{s_{\mathrm{NN}}}$ = 5.02 TeV. 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 $\mathrm{\overline{K}^0 n}$ and $\pi \Sigma$ inelastic channels on the measured K$^-$p 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 $\omega$, 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 K$^-$p interaction indicates that, while the $\pi \Sigma$-K$^-$p dynamics is well reproduced by the model, the coupling to the $\mathrm{\overline{K}^0 n}$ channel in the model is currently underestimated.

Constraining the ${\rm\overline{K}N}$ coupled channel dynamics using femtoscopic correlations at the LHC;ALICE Collaboration;2022;HEPData


Abstract:
This article reports about the properties of the underlying event measured with ALICE at
the LHC in pp and p-Pb collisions at $\sqrt{s_{\rm NN}}= 5.02$ TeV. The event activity, quantified by charged-particle number and summed-$p_{\rm T}$ densities, is measured
as a function of the leading-particle transverse momentum ($p_{\rm T}^{\rm trig}$). These quantities are studied in three azimuthal-angle regions relative to the leading particle in the event: toward, away, and transverse. Results are presented for
three different $p_{\rm T}$ thresholds (0.15, 0.5 and 1 GeV/$c$) at mid-pseudorapidity ($|\\eta|<0.8$).
The event activity in the transverse region, which is the most sensitive to the underlying event, exhibits similar behaviour in both pp and p-Pb
collisions, namely, a steep increase with $p_{\rm T}^{\rm trig}$ for low $p_{\rm T}^{\rm trig}$, followed by a saturation at $p_{\rm T}^{\rm trig} \approx 5$ GeV/$c$. The results from pp collisions are
compared with existing measurements at other centre-of-mass energies. The quantities in the toward and away regions are also analyzed after
the subtraction of the contribution measured in the transverse region. The remaining jet-like particle densities are consistent in pp and p-Pb
collisions for $p_{\rm T}^{\rm trig}>10$ GeV/$c$, whereas for lower $p_{\rm T}^{\rm trig}$ values
the event activity is slightly higher in pPb than in pp collisions. The measurements are compared with predictions from the Monte Carlo event generators.

Underlying-event properties in pp and p$-$Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV;ALICE Collaboration;2022;HEPData


Abstract: No data abstract available.

Measurements of the groomed jet radius and momentum splitting fraction with the soft drop and dynamical grooming algorithms in pp collisions at $\sqrt{s}=5.02$ TeV;ALICE Collaboration;2022;HEPData


Abstract: No data abstract available.

Multiplicity dependence of charged-particle jet production in pp collisions at $\sqrt{s} = 13$ TeV;ALICE Collaboration;2022;HEPData


Abstract: No data abstract available.

Dielectron production in proton-proton and proton-lead collisions at $\sqrt{s_{\rm{NN}}}$ = 5.02 TeV;ALICE Collaboration;2020;HEPData


Abstract: No data abstract available.

Measurement of the angle between jet axes in pp collisions at $\sqrt{s} = 5.02$ TeV;ALICE Collaboration;2023;HEPData


Pristine survey DR1

Pristine survey DR1;N.F. Martin;2024;Centre de Donnees Strasbourg (CDS)

VizieR online Data Catalogue associated with article published in journal Astronomy and Astrophysics with title ' The Pristine survey. XXIII. Data Release 1 and an all-sky metallicity catalogue based on Gaia DR3 BP/RP spectro-photometry.' (bibcode: 2024A&A...692A.115M)


Abstract: No data abstract available.

Study of jet quenching with isolated-photon+jet correlations in PbPb and pp collisions at $\sqrt{s_{_{\mathrm{NN}}}} =$ 5.02 TeV;CMS Collaboration;2018;HEPData


Abstract: No data abstract available.

Observation of medium induced modifications of jet fragmentation in PbPb collisions using isolated-photon-tagged jets;CMS Collaboration;2018;HEPData


Abstract: No data abstract available.

Nuclear modification factor of D0 mesons in PbPb collisions at sqrt(s[NN]) = 5.02 TeV;CMS Collaboration;2018;HEPData