• Nenhum resultado encontrado

[PDF] Top 20 Relative Modification of Prompt ψ(2S) and J/ψ Yields from pp to PbPb Collisions at $\sqrt{s_{NN}}=5.02$ TeV

Has 10000 "Relative Modification of Prompt ψ(2S) and J/ψ Yields from pp to PbPb Collisions at $\sqrt{s_{NN}}=5.02$ TeV" found on our website. Below are the top 20 most common "Relative Modification of Prompt ψ(2S) and J/ψ Yields from pp to PbPb Collisions at $\sqrt{s_{NN}}=5.02$ TeV".

Relative Modification of Prompt ψ(2S) and J/ψ Yields from pp to PbPb Collisions at $\sqrt{s_{NN}}=5.02$ TeV

Relative Modification of Prompt ψ(2S) and J/ψ Yields from pp to PbPb Collisions at $\sqrt{s_{NN}}=5.02$ TeV

... D. Abbaneo, E. Auffray, G. Auzinger, M. Bachtis, P. Baillon, A.H. Ball, D. Barney, P. Bloch, A. Bocci, A. Bonato, C. Botta, T. Camporesi, R. Castello, M. Cepeda, G. Cerminara, D. d’Enterria, A. Dabrowski, V. Daponte, A. ... See full document

28

Nuclear modification factor of D$^0$ mesons in PbPb collisions at  $\sqrt{s_\mathrm{NN}} = 5.02$ TeV

Nuclear modification factor of D$^0$ mesons in PbPb collisions at $\sqrt{s_\mathrm{NN}} = 5.02$ TeV

... information from the HF calorimeters and the beam pickup ...designed to identify online events with a D 0 ...expected to leave large energy deposits in HCAL, HLT algorithms were run on events ... See full document

23

Study of $W$ boson production in PbPb and $pp$ collisions at $\sqrt{s_{NN}}=2.76$ TeV

Study of $W$ boson production in PbPb and $pp$ collisions at $\sqrt{s_{NN}}=2.76$ TeV

... hot and dense matter produced in heavy-ion (AA) collisions can be studied in a variety of ...is to compare AA to proton-proton (pp) collisions as well as to ... See full document

33

Charged-particle nuclear modification factors in XeXe collisions at $ \sqrt{s_{\mathrm{NN}}} = 5.44 $ TeV

Charged-particle nuclear modification factors in XeXe collisions at $ \sqrt{s_{\mathrm{NN}}} = 5.44 $ TeV

... likely to decay into secondary particles which then contaminate the ...lead to a model dependence of the total tracking correction, because different MC event generators predict dissimilar ... See full document

41

Suppression of non-prompt $J/\psi$, prompt $J/\psi$, and Y(1S) in PbPb collisions at $\sqrt{s_{NN}}=2.76$ TeV

Suppression of non-prompt $J/\psi$, prompt $J/\psi$, and Y(1S) in PbPb collisions at $\sqrt{s_{NN}}=2.76$ TeV

... fit to the µ + µ − invari- ant mass spectrum between 7 and 14 GeV/c 2 is performed, integrated over p T , rapidity, and centrality, as shown in the left panel of ...Fig. 5. The measured ... See full document

51

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

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

... due to electron contamination is evaluated by repeating the analysis without applying electron rejection, and scaling the difference in the final observ- ables to the residual electron contamination ... See full document

38

Charged-particle nuclear modification factors in PbPb and pPb collisions at $ \sqrt{s_{\mathrm{N}\;\mathrm{N}}}=5.02 $ TeV

Charged-particle nuclear modification factors in PbPb and pPb collisions at $ \sqrt{s_{\mathrm{N}\;\mathrm{N}}}=5.02 $ TeV

... amination of the relative difference between pp and PbPb of MC/data tracking ef- ficiency discrepancies is ...ratio of the uncorrected track spectra in data in the 30–100% ... See full document

38

Modification of jet shapes in PbPb collisions at $\sqrt {s_{NN}} = 2.76$ TeV

Modification of jet shapes in PbPb collisions at $\sqrt {s_{NN}} = 2.76$ TeV

... cross-check of the background subtraction ...considered to be representative of the back- ...matched to ten minimum bias PbPb events that are required to have similar global ... See full document

29

Measurement of the groomed jet mass in PbPb and pp collisions at $ \sqrt{s_{\mathrm{NN}}}=5.02 $ TeV

Measurement of the groomed jet mass in PbPb and pp collisions at $ \sqrt{s_{\mathrm{NN}}}=5.02 $ TeV

... measurement of the groomed jet mass in PbPb and pp collisions at a nucleon- nucleon center-of-mass energy of ...5.02 TeV with the CMS detector at the ... See full document

35

Comparing transverse momentum balance of b jet pairs in pp and PbPb collisions at $ \sqrt{s_{\mathrm{NN}}}=5.02 $ TeV

Comparing transverse momentum balance of b jet pairs in pp and PbPb collisions at $ \sqrt{s_{\mathrm{NN}}}=5.02 $ TeV

... type of parton that initiates the jet is difficult to determine ...fragmentation of bottom ...presence of a soft lepton or a displaced vertex inside the ...measurement of the b quark ... See full document

34

Jet properties in PbPb and pp collisions at $ \sqrt{s_{\mathrm{N}\;\mathrm{N}}}=5.02 $ TeV

Jet properties in PbPb and pp collisions at $ \sqrt{s_{\mathrm{N}\;\mathrm{N}}}=5.02 $ TeV

... mance of the LHC and thank the technical and administrative staffs at CERN and at other CMS institutes for their contributions to the success of the CMS ...centres ... See full document

34

Modification of jet shapes in PbPb collisions at root s(NN)=2.76 TeV

Modification of jet shapes in PbPb collisions at root s(NN)=2.76 TeV

... expected to lose energy while traversing the hot and dense medium created in these collisions [1,2] ...discovered at the Relativistic Heavy Ion Collider (RHIC) [3–5] through the ... See full document

22

Centrality dependence of dihadron correlations and azimuthal anisotropy harmonics in PbPb collisions at $\sqrt{s_{NN}}=2.76$ TeV

Centrality dependence of dihadron correlations and azimuthal anisotropy harmonics in PbPb collisions at $\sqrt{s_{NN}}=2.76$ TeV

... D. Abbaneo, E. Auffray, G. Auzinger, P. Baillon, A.H. Ball, D. Barney, C. Bernet 5 , W. Bialas, G. Bianchi, P. Bloch, A. Bocci, H. Breuker, K. Bunkowski, T. Camporesi, G. Cerminara, T. Christiansen, J.A. Coarasa ... See full document

39

Azimuthal anisotropy of charged particles at high transverse momenta in PbPb collisions at $\sqrt{s_{NN}}=2.76$ TeV

Azimuthal anisotropy of charged particles at high transverse momenta in PbPb collisions at $\sqrt{s_{NN}}=2.76$ TeV

... reconstruction of the primary event vertex and the trajectories of charged particles in PbPb collisions is based on signals in the silicon pixel and strip detectors and ... See full document

27

Measurement of higher-order harmonic azimuthal anisotropy in PbPb collisions at $\sqrt{s_{NN}}$ = 2.76 TeV

Measurement of higher-order harmonic azimuthal anisotropy in PbPb collisions at $\sqrt{s_{NN}}$ = 2.76 TeV

... found to have their maximum values near η ≈ 0 (see Section ...selection of both particles in a pair from the mid-rapidity, maximum v 3 region, thus assuring a somewhat smaller v 3 result as compared ... See full document

61

Studies of azimuthal dihadron correlations in ultra-central PbPb collisions at $\sqrt{s_{NN}} =$ 2.76 TeV

Studies of azimuthal dihadron correlations in ultra-central PbPb collisions at $\sqrt{s_{NN}} =$ 2.76 TeV

... extraction of η/s from the anisotropy data is crucial for investigating the transport prop- erties of the hot and dense medium created in heavy-ion collisions in detail ...understanding ... See full document

37

Measurement of the azimuthal anisotropy of neutral pions in PbPb collisions at $\sqrt{s_{NN}}=2.76$ TeV

Measurement of the azimuthal anisotropy of neutral pions in PbPb collisions at $\sqrt{s_{NN}}=2.76$ TeV

... mance of the LHC machine. We thank the technical and administrative staff at CERN and other CMS institutes, and acknowledge support from: BMWF and FWF (Austria); FNRS ... See full document

27

Study of Z production in PbPb and pp collisions at $ \sqrt{s_{\mathrm{NN}}}=2.76 $ TeV in the dimuon and dielectron decay channels

Study of Z production in PbPb and pp collisions at $ \sqrt{s_{\mathrm{NN}}}=2.76 $ TeV in the dimuon and dielectron decay channels

... lifetime of 0.1 fm/c and their leptonic decays are of particu- lar interest since leptons pass through the medium being probed without interacting ...Dileptons from Z boson decays can thus ... See full document

37

Prompt and non-prompt $J/\psi $ elliptic flow in Pb+Pb collisions at $\sqrt{s_{_\text {NN}}} = 5.02$ Tev with the ATLAS detector

Prompt and non-prompt $J/\psi $ elliptic flow in Pb+Pb collisions at $\sqrt{s_{_\text {NN}}} = 5.02$ Tev with the ATLAS detector

... J.J. Kempster 21 , J. Kendrick 21 , O. Kepka 137 , S. Kersten 179 , B.P. Kerševan 89 , R.A. Keyes 101 , M. Khader 170 , F. Khalil-Zada 13 , A. Khanov 125 , A.G. Kharlamov 120b,120a , T. Kharlamova 120b,120a , E.E. ... See full document

34

Suppression of $\Upsilon(1S), \Upsilon(2S)$ and $\Upsilon(3S)$ production in PbPb collisions at $\sqrt{s_{\rm NN}}$ = 2.76 TeV

Suppression of $\Upsilon(1S), \Upsilon(2S)$ and $\Upsilon(3S)$ production in PbPb collisions at $\sqrt{s_{\rm NN}}$ = 2.76 TeV

... hadronic PbPb collisions, contributions from ultraperipheral collisions and noncollision beam backgrounds are removed, as described in ...built from at least two tracks, ... See full document

23

Show all 10000 documents...

temas relacionados