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[PDF] Top 20 $\Lambda_{\rm c}^+$ production in pp collisions at $\sqrt{s} = 7$ TeV and in p-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV

Has 10000 "$\Lambda_{\rm c}^+$ production in pp collisions at $\sqrt{s} = 7$ TeV and in p-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV" found on our website. Below are the top 20 most common "$\Lambda_{\rm c}^+$ production in pp collisions at $\sqrt{s} = 7$ TeV and in p-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV".

$\Lambda_{\rm c}^+$ production in pp collisions at $\sqrt{s} = 7$ TeV and in p-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV

$\Lambda_{\rm c}^+$ production in pp collisions at $\sqrt{s} = 7$ TeV and in p-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV

... fractions in the beauty sector [ 11 , 12 ]. In Monte Carlo generators, hadronisation is imple- mented via formation of strings as in pythia, via ropes [ 13 ] as in dipsy [ 14 ] or via clusters ... Voir le document complet

49

One-dimensional charged kaon femtoscopy in p-Pb collisions at $\sqrt{s_{\rm NN}}$ = 5.02 TeV

One-dimensional charged kaon femtoscopy in p-Pb collisions at $\sqrt{s_{\rm NN}}$ = 5.02 TeV

... [11] and PHENIX [12] collaborations and in pp collisions at √ s = 7 TeV and PbPb collisions at √s NN = ...2.76 TeV ... Voir le document complet

23

Inclusive J/$\psi$ production at forward and backward rapidity in p-Pb collisions at $\sqrt{s_{\rm NN}}$ = 8.16 TeV

Inclusive J/$\psi$ production at forward and backward rapidity in p-Pb collisions at $\sqrt{s_{\rm NN}}$ = 8.16 TeV

... ies at this energy is threefold: first, a significantly larger integrated luminosity with respect to studies performed at √ s NN = ...5.02 TeV [27–29] has become available in ALICE, ... Voir le document complet

24

Measurements of inclusive jet spectra in pp and central Pb-Pb collisions at $\sqrt{s_{\rm{NN}}}$ = 5.02 TeV

Measurements of inclusive jet spectra in pp and central Pb-Pb collisions at $\sqrt{s_{\rm{NN}}}$ = 5.02 TeV

... jets in pp collisions at √ s = 5.02 TeV and PbPb collisions at √ s NN = ...5.02 TeV, as well as the jet nuclear modification factor (R ... Voir le document complet

31

Production of the $\rho$(770)${^{0}}$ meson in pp and Pb-Pb collisions at $\sqrt{s_{\rm NN}}$ = 2.76 TeV

Production of the $\rho$(770)${^{0}}$ meson in pp and Pb-Pb collisions at $\sqrt{s_{\rm NN}}$ = 2.76 TeV

... 2.76 TeV. The shaded regions in the two panels correspond to a ±20% variation of the ratio, see text for ...kaon and (anti)proton production spectra [60, 61] with Tsallis Blast-Wave (TBW) ... Voir le document complet

33

Measurement of $\Upsilon(1{\rm S})$ elliptic flow at forward rapidity in Pb-Pb collisions at $\sqrt{s_{\rm{NN}}}=5.02$ TeV

Measurement of $\Upsilon(1{\rm S})$ elliptic flow at forward rapidity in Pb-Pb collisions at $\sqrt{s_{\rm{NN}}}=5.02$ TeV

... Charm and beauty quarks are important probes of the ...predominantly in hard- scattering processes at the early collision stage and therefore experience the entire evolution of the ...2 ... Voir le document complet

17

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

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

... Y. Sekiguchi 127 , D. Sekihata 47 , I. Selyuzhenkov 96 , K. Senosi 65 , S. Senyukov 3 ,36 , E. Serradilla 10 ,64 , A. Sevcenco 62 , A. Shabanov 56 , A. Shabetai 113 , O. Shadura 3 , R. Shahoyan 36 , A. Shangaraev 111 , ... Voir le document complet

27

Coherent $\rm{J/\psi}$ and $\rm{\psi'}$ photoproduction at midrapidity in ultra-peripheral Pb-Pb collisions at $\sqrt{s_{\mathrm{NN}}}~=~5.02$ TeV

Coherent $\rm{J/\psi}$ and $\rm{\psi'}$ photoproduction at midrapidity in ultra-peripheral Pb-Pb collisions at $\sqrt{s_{\mathrm{NN}}}~=~5.02$ TeV

... MeV/c). In the first case, the nu- clei usually do not dissociate, but the electromagnetic fields of ultrarelativistic heavy nuclei are strong enough to develop other independent soft electromagnetic interactions ... Voir le document complet

28

J/$\psi$ suppression at forward rapidity in Pb-Pb collisions at $\mathbf{\sqrt{s_{{\rm NN}}} = 5.02}$ TeV

J/$\psi$ suppression at forward rapidity in Pb-Pb collisions at $\mathbf{\sqrt{s_{{\rm NN}}} = 5.02}$ TeV

... effects at high energy, followed by an increase, re- lated to the effect of regeneration, which acts in the opposite direction and becomes dominant for central ...central collisions, while for ... Voir le document complet

14

J/$\psi$ production as a function of charged-particle pseudorapidity density in p-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV

J/$\psi$ production as a function of charged-particle pseudorapidity density in p-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV

... C. Bianchin 141 , J. Bielˇc´ık 38 , J. Bielˇc´ıkov´a 87 , A. Bilandzic 35,97 , G. Biro 142 , R. Biswas 4 , S. Biswas 4 , J.T. Blair 121 , D. Blau 83 , C. Blume 60 , G. Boca 136 , F. Bock 75,96 , A. Bogdanov 76 , L. ... Voir le document complet

24

Exclusive $\mathrm{J/}\psi$ photoproduction off protons in ultra-peripheral p-Pb collisions at $\sqrt{s_{\rm NN}}=5.02$ TeV

Exclusive $\mathrm{J/}\psi$ photoproduction off protons in ultra-peripheral p-Pb collisions at $\sqrt{s_{\rm NN}}=5.02$ TeV

... presented. and are listed in Table 2. The hW γ p i is calculated by weighting with the product of the photon spectrum and the cross section σ ( γ p ) from ...calculated in impact ... Voir le document complet

17

Centrality and transverse momentum dependence of inclusive J/$\psi$ production at midrapidity in Pb-Pb collisions at $\sqrt{s_{\rm NN}}$ = 5.02 TeV

Centrality and transverse momentum dependence of inclusive J/$\psi$ production at midrapidity in Pb-Pb collisions at $\sqrt{s_{\rm NN}}$ = 5.02 TeV

... presented in this paper are obtained using the MB trigger data collected during the 2015 LHC PbPb run at a center-of-mass energy per nucleon pair of ...V0 and Zero Degree Calorimeters ... Voir le document complet

24

Coherent J/$\psi$ photoproduction at forward rapidity in ultra-peripheral Pb-Pb collisions at $\sqrt{s_{\rm{NN}}}=5.02$ TeV

Coherent J/$\psi$ photoproduction at forward rapidity in ultra-peripheral Pb-Pb collisions at $\sqrt{s_{\rm{NN}}}=5.02$ TeV

... enriched in coherent candidates was obtained by selecting dimuons with transverse momentum p T < ...shown in Fig. 1, left, in the full dimuon rapidity range ...−2.5 and in ... Voir le document complet

22

Azimuthal Anisotropy of Heavy-Flavor Decay Electrons in $p$-Pb Collisions at $ \sqrt{s_{\rm NN}}$ = 5.02 TeV

Azimuthal Anisotropy of Heavy-Flavor Decay Electrons in $p$-Pb Collisions at $ \sqrt{s_{\rm NN}}$ = 5.02 TeV

... ated in ultra-relativistic collisions of protons or ...differences in the azimuthal angle (∆ϕ) and in pseudorapidity (∆η) between a reference (“trigger”) particle and other ... Voir le document complet

18

Production of (anti-)$^3$He and (anti-)$^3$H in p-Pb collisions at $\sqrt{s_{\rm{NN}}}$ = 5.02 TeV

Production of (anti-)$^3$He and (anti-)$^3$H in p-Pb collisions at $\sqrt{s_{\rm{NN}}}$ = 5.02 TeV

... Science and Technology for Sustainable Development in the South (COMSATS), Pakistan; Pontificia Universidad Católica del Perú, Peru; Ministry of Science and Higher Education and National ... Voir le document complet

30

$\Upsilon$ suppression at forward rapidity in Pb-Pb collisions at $\sqrt{s_{\rm NN}}$ = 5.02 TeV

$\Upsilon$ suppression at forward rapidity in Pb-Pb collisions at $\sqrt{s_{\rm NN}}$ = 5.02 TeV

... Education and Science of the Russian Federation and National Research Centre Kurchatov Institute, Russia; Ministry of Education, Science, Research and Sport of the Slovak Re- public, Slovakia; ... Voir le document complet

21

Measurement of $\Lambda$(1520) production in pp collisions at $\sqrt{s}$ = 7 TeV and p-Pb collisions at $\sqrt{s_{\rm{NN}}}$ = 5.02 TeV

Measurement of $\Lambda$(1520) production in pp collisions at $\sqrt{s}$ = 7 TeV and p-Pb collisions at $\sqrt{s_{\rm{NN}}}$ = 5.02 TeV

... intervals in pPb ...summarized in Table ...budget) and the hadronic interaction cross-section in the detector ...observed in pPb data, thus the ... Voir le document complet

26

$\rm \Lambda_{c}^{+}$ production and baryon-to-meson ratios in pp and p-Pb collisions at $\sqrt{s_\mathrm{NN}} = 5.02$ TeV at the LHC

$\rm \Lambda_{c}^{+}$ production and baryon-to-meson ratios in pp and p-Pb collisions at $\sqrt{s_\mathrm{NN}} = 5.02$ TeV at the LHC

... , E. Cuautle 70 , P. Cui 7 , L. Cunqueiro 98 , T. Dahms 107 , A. Dainese 58 , F.P.A. Damas 117,139 , M.C. Danisch 106 , A. Danu 68 , D. Das 112 , I. Das 112 , P. Das 88 , P. Das 4 , S. Das 4 ... Voir le document complet

18

Measurement of electrons from beauty-hadron decays in p-Pb collisions at $\mathbf{\sqrt{s_{\rm NN}}=5.02}$ TeV and Pb-Pb collisions at $\mathbf{\sqrt{s_{\rm NN}}=2.76}$ TeV

Measurement of electrons from beauty-hadron decays in p-Pb collisions at $\mathbf{\sqrt{s_{\rm NN}}=5.02}$ TeV and Pb-Pb collisions at $\mathbf{\sqrt{s_{\rm NN}}=2.76}$ TeV

... summarized in table 2 ...found in figure 3 ...(hits in both SPD layers) does not depend strongly on the particle ...rapidity and azimuthal angle) regions where the efficiency was close to ... Voir le document complet

41

Jet fragmentation transverse momentum distributions in pp and p-Pb collisions at $\sqrt{s_{\rm NN}}$ = 5.02 TeV

Jet fragmentation transverse momentum distributions in pp and p-Pb collisions at $\sqrt{s_{\rm NN}}$ = 5.02 TeV

... uncertainties in this analysis come from the background estimation, the unfolding proce- dure and the uncertainties related to track and cluster ...uncertainty in the tracking efficiency is ... Voir le document complet

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