about
The ALICE experiment at the CERN LHCCharged-particle multiplicity measurement in proton–proton collisions at $\sqrt{s}=0.9$ and 2.36 TeV with ALICE at LHCSearch for slowly moving magnetic monopoles with the MACRO detectorStudy of the isospin symmetry breaking in the light quark sea of the nucleon from the Drell-Yan processCharmonium and e (+) e (-) pair photoproduction at mid-rapidity in ultra-peripheral Pb-Pb collisions at [Formula: see text].Energy dependence of the transverse momentum distributions of charged particles in pp collisions measured by ALICE.Measurement of inelastic, single- and double-diffraction cross sections in proton-proton collisions at the LHC with ALICE.D meson elliptic flow in noncentral Pb-Pb collisions at sqrt[sNN]=2.76 Tev.Directed flow of charged particles at midrapidity relative to the spectator plane in Pb-Pb collisions at √(s(NN))=2.76 TeV.K(S)0 and Λ production in Pb-Pb collisions at √(s(NN))=2.76 TeV.Net-charge fluctuations in Pb-Pb collisions at sqrt[sNN]=2.76 TeV.Transverse momentum distribution and nuclear modification factor of charged particles in p+Pb collisions at sqrt[s(NN)] = 5.02 TeV.J/ψ elliptic flow in Pb-Pb collisions at √(s(NN))=2.76 TeV.Charge separation relative to the reaction plane in Pb-Pb collisions at sqrt[s(NN)] = 2.76 TeV.Pseudorapidity density of charged particles in p+Pb collisions at √(s(NN))=5.02 TeV.Measurement of the cross section for electromagnetic dissociation with neutron emission in Pb-Pb collisions at sqrt[s(NN)] = 2.76 TeV.Pion, kaon, and proton production in central Pb-Pb collisions at sqrt[s(NN)] = 2.76 TeV.J/ψ suppression at forward rapidity in Pb-Pb collisions at √s(NN) = 2.76 TeV.Particle-yield modification in jetlike azimuthal dihadron correlations in Pb-Pb collisions at √s(NN)=2.76 TeV.Centrality dependence of the charged-particle multiplicity density at midrapidity in Pb-Pb collisions at sqrt[s(NN)] = 2.76 TeV.Elliptic flow of charged particles in Pb-Pb collisions at sqrt[S(NN)] = 2.76 TeV.Charged-particle multiplicity density at midrapidity in central Pb-Pb collisions at sqrt[S(NN)] = 2.76 TeV.Midrapidity antiproton-to-proton ratio in pp collisons at sqrt[s]=0.9 and 7 TeV measured by the ALICE experiment.Evidence for deconfinement of quarks and gluons from the J/ψ suppression pattern measured in Pb-Pb collisions at the CERN-SPSObservation of Higgs Boson Decay to Bottom QuarksMulti-strange baryon production at mid-rapidity in Pb–Pb collisions at s NN = 2.76 TeVMultiplicity dependence of pion, kaon, proton and lambda production in p–Pb collisions at s NN = 5.02 TeVAnisotropic flow of charged hadrons, pions and (anti-)protons measured at high transverse momentum in Pb–Pb collisions at s NN = 2.76 TeVCentrality dependence of the pseudorapidity density distribution for charged particles in Pb–Pb collisions at s NN = 2.76 TeVCentrality dependence ofπ,K, andpproduction in Pb-Pb collisions atsNN=2.76TeVCentrality determination of Pb-Pb collisions atsNN=2.76TeV with ALICECharged kaon femtoscopic correlations inppcollisions ats=7 TeVCoherent J / ψ photoproduction in ultra-peripheral Pb–Pb collisions at s NN = 2.76 TeVLong-range angular correlations of π, K and p in p–Pb collisions at s NN = 5.02 TeVLong-range angular correlations on the near and away side in p–Pb collisions at s NN = 5.02 TeVMid-rapidity anti-baryon to baryon ratios in pp collisions at $\sqrt{s} = 0.9,\ 2.76\mbox{ and }7\mbox{ TeV}$ measured by ALICEMultiplicity dependence of the average transverse momentum in pp, p–Pb, and Pb–Pb collisions at the LHCMultiplicity dependence of two-particle azimuthal correlations in pp collisions at the LHCD s + meson production at central rapidity in proton–proton collisions at s = 7 TeVErratum to “Rapidity and transverse momentum dependence of inclusive J / ψ production in pp collisions at s = 7 TeV ” [Phys. Lett. B 704 (5) (2011) 442]
P50
Q21994529-EEEA1A65-FC1D-4A6E-AEF6-422EAACCE0ACQ27011928-D1AA36CB-A3A6-4E7B-BDB7-514391952D01Q27450464-A21DDE54-BA23-44D4-A448-724DAFD27DF9Q29299793-CF930119-837A-4221-9FFF-90C5052CB64CQ35210219-652347E4-D3A8-4BB4-95E5-48553802CCD5Q35210247-3E1FFA58-DB88-45D2-82CB-2DE29796705EQ35210525-8E0F2B01-9F04-4994-A45A-C54585D09846Q51047580-C8982106-6D1B-4DE0-A613-51C922CC1A3EQ51118264-A4E4033F-85E7-479D-B187-8BC565244258Q51133659-B66C02C7-8A6A-4787-81B1-EBD27A05D39DQ51232750-5F622A0B-C343-4599-8AEE-96187AAEBFF9Q53115887-1F3204D7-3795-4040-8D19-42BF145E5C6DQ53310087-B28068C9-54FC-4CFC-B57F-CE64B0B4E44FQ53342414-1A46A573-AA27-4B8A-B941-D680F145574EQ53342875-36990B46-56DC-4B59-9611-45F9C1FB56EDQ53343178-4586FF7A-1B8B-4C68-8B53-DB0021ADD4DCQ53343198-5E65FA96-F280-4DAC-8908-2C2732EEA13EQ53359562-045BFFD0-8B3C-494D-BEDD-DAB022C6470EQ53382181-133867D3-0D76-4949-B30B-C361E8D77949Q53433893-2DE95BAC-1ABF-4F46-8BD3-B3423316B6C6Q53442713-3463D55D-5037-4C6D-89D2-9B969EDF2A4EQ53442731-8D363D02-DA63-4540-B011-6159D370917EQ53457062-D9ED7408-F4CE-403D-A40E-E93CEB4ABB12Q56048771-69F9F770-DCFB-4A24-9E91-171E36E1743BQ57191597-F6F57CE5-EB50-4126-A9E4-389F021E6FB3Q57718212-C6FABD87-0C2E-45F6-97C5-04CCABB2BA0DQ57718223-83959323-5F3A-4618-9B0E-DF67E143B54AQ57718286-A5215BE5-F1CF-410D-ACF5-F4FF20066F0FQ57718291-F51189DC-56A6-4A02-90EC-ACB565A45C28Q57718296-5C1FF27B-E245-4C1B-807B-F0C032D0E0E7Q57718301-7E18572E-E6DC-40B6-9BA5-65ED6BA23843Q57718311-E0C1D41E-8494-4D82-ADAF-0B2AA26EF1FBQ57718323-7C920FB7-BBD1-4301-BE8A-BC1FCCBF48B3Q57718341-856ED87B-A95B-4539-B0FA-6FD412BB085BQ57718347-0A86212C-44FF-491C-9D11-307C7B30C938Q57718356-800E216F-3605-4B3D-B814-4EB2B9E9F934Q57718360-C1C37FAE-9B9B-4395-A33C-1449E868C9EFQ57718366-18DCE237-9EC6-4228-8CC8-E3F0D0BEE6FAQ57718386-10315C5D-DEA1-4DCE-A076-BDE2D08C23CDQ57718389-DD730822-8427-474F-B20F-467F13FE4C7B
P50
description
hulumtues
@sq
researcher
@en
wetenschapper
@nl
հետազոտող
@hy
name
M Monteno
@nl
M Monteno
@sl
Marco Monteno
@en
Marco Monteno
@es
type
label
M Monteno
@nl
M Monteno
@sl
Marco Monteno
@en
Marco Monteno
@es
altLabel
M Monteno
@en
prefLabel
M Monteno
@nl
M Monteno
@sl
Marco Monteno
@en
Marco Monteno
@es
P106
P1153
7004262162
P21
P31
P496
0000-0002-3521-6333