Search results for "Nuclear Theory"

showing 10 items of 3976 documents

"Table 12" of "$\Upsilon$ production and nuclear modification at forward rapidity in Pb-Pb collisions at $\mathbf{\sqrt{\textit{s}_{\textbf{NN}}}=5.0…

2021

Interpolated $p_{\mathrm{T}}$-differential cross section for $\Upsilon(1\mathrm{S}) \rightarrow \mu^{+}\mu^{-}$ in proton–proton collisions. Results used for the determination of the nuclear modification factor of $\Upsilon(1\mathrm{S})$ as a function of its transverse momentum (Figure 6).

5020.0Proton-Proton ScatteringP P --> UPSI(1S) < MU+ MU- > XD2SIG/DYRAP/DPTNuclear TheoryHigh Energy Physics::ExperimentUpsilonCross SectionNuclear ExperimentTransverse Momentum Dependence
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"Table 13" of "$\Upsilon$ production and nuclear modification at forward rapidity in Pb-Pb collisions at $\mathbf{\sqrt{\textit{s}_{\textbf{NN}}}=5.0…

2021

Interpolated rapidity-differential cross section for $\Upsilon(1\mathrm{S}) \rightarrow \mu^{+}\mu^{-}$ in proton–proton collisions. Results used for the determination of the nuclear modification factor of $\Upsilon(1\mathrm{S})$ as a function of rapidity (Figure 7).

5020.0Proton-Proton ScatteringP P --> UPSI(1S) < MU+ MU- > XRapidity DependenceNuclear TheoryHigh Energy Physics::ExperimentUpsilonDSIG/DYRAPCross SectionNuclear Experiment
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"Table 14" of "$\Upsilon$ production and nuclear modification at forward rapidity in Pb-Pb collisions at $\mathbf{\sqrt{\textit{s}_{\textbf{NN}}}=5.0…

2021

Interpolated rapidity-differential cross section for $\Upsilon(2\mathrm{S}) \rightarrow \mu^{+}\mu^{-}$ in proton–proton collisions. Results used for the determination of the nuclear modification factor of $\Upsilon(2\mathrm{S})$ as a function of rapidity (Figure 7).

5020.0Proton-Proton ScatteringP P --> UPSI(2S) < MU+ MU- > XRapidity DependenceNuclear TheoryHigh Energy Physics::ExperimentUpsilonDSIG/DYRAPCross SectionNuclear Experiment
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"Table 1" of "First measurement of the ${\mathbf{|\textit t|}}$-dependence of coherent $\mathbf{\rm{J/\psi}}$ photonuclear production"

2021

t-dependence of coherent J/psi photonuclear production cross section in Pb-Pb UPC.

5020.0Single Differential Cross SectionDi-Muon ProductionPhotoproductionPhysics::Medical PhysicsNuclear TheoryDSIG/DTMomentum Transfer DependenceHigh Energy Physics::ExperimentPB PB --> PB PB J/PSI(1S)Nuclear ExperimentJ/Psi
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"Table 4" of "Production of muons from heavy-flavour hadron decays in p-Pb collisions at $\mathbf{\sqrt{{\textit s}_{NN}} = 5.02}$ TeV"

2017

pT-differential nuclear modification factor of heavy-flavour decay muons at forward rapidity (proton-going side)

5020.0p PB --> MUON XNuclear TheoryHigh Energy Physics::PhenomenologyPhysics::Accelerator PhysicsHigh Energy Physics::ExperimentNuclear ExperimentSIG
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"Table 2" of "Production of muons from heavy-flavour hadron decays in p-Pb collisions at $\mathbf{\sqrt{{\textit s}_{NN}} = 5.02}$ TeV"

2017

pT-differential nuclear modification factor of heavy-flavour decay muons at forward rapidity (proton-going side)

5020.0p PB --> MUON XNuclear TheoryHigh Energy Physics::PhenomenologyPhysics::Accelerator PhysicsHigh Energy Physics::ExperimentNuclear ExperimentSIG
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"Table 2" of "Charm-quark fragmentation fractions and production cross section at midrapidity in pp collisions at the LHC"

2022

Fragmentation fractions of charm quark to open-charm hadrons $f(\mathrm{c \rightarrow H_c})$ in pp collisions at $\sqrt{s} = 5.02$ TeV.

5020.0pp -> D$_\mathrm{s}^{+}$ + Xpp -> D$^{*+}$ + Xpp -> D$^0$ + XNuclear TheoryHigh Energy Physics::Phenomenologypp -> D$^+$ + XHigh Energy Physics::Experimentpp -> $\Xi_\mathrm{c}^{0}$ + XNuclear Experiment$f(\mathrm{c \rightarrow H_c})$pp -> $\Lambda_\mathrm{c}^{+}$ + X
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"Table 1.4" of "Probing the effects of strong electromagnetic fields with charge-dependent directed flow in Pb-Pb collisions at the LHC"

2020

Directed flow D0 meson 10-40%

5023.0High Energy Physics::LatticeHigh Energy Physics::PhenomenologyNuclear TheoryHigh Energy Physics::ExperimentD0 mesonDirected flowNuclear Experiment
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"Table 1.5" of "Probing the effects of strong electromagnetic fields with charge-dependent directed flow in Pb-Pb collisions at the LHC"

2020

Directed flow D0-bar meson 10-40%

5023.0High Energy Physics::LatticeNuclear TheoryHigh Energy Physics::PhenomenologyD0-bar mesonHigh Energy Physics::ExperimentDirected flowNuclear Experiment
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Evidence of oblate-prolate shape coexistence in the strongly-deformed nucleus 119Cs

2021

International audience; Prolate-oblate shape coexistence close to the ground state in the strongly-deformed proton-rich A≈120 nuclei is reported for the first time. One of the four reported bands in 119Cs, built on a 11/2− state at 670 keV, consists of nearly degenerate signature partners, and has properties which unequivocally indicate the strongly-coupled πh11/2[505]11/2− configuration associated with oblate shape. Together with the decoupled πh11/2[541]3/2− band built on the 11/2− prolate state at 110 keV, for which a half-life of T1/2=55(5)μs has been measured, the new bands bring evidence of shape coexistence at low spin in the proton-rich strongly deformed A≈120 nuclei, a phenomenon p…

58Ni(64Zn3p)119CsNuclear reactionNuclear and High Energy PhysicsQC1-999Nuclear TheoryModel calculation-coincidences[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]01 natural sciencesMolecular physicsMeasured γγγ-coincidencescesium0103 physical sciencesmedicineNuclear reaction:58Ni(64Zn3p)119CsZnCovariant transformationCs010306 general physicsSpin (physics)Ni(PhysicsLinear polarization010308 nuclear & particles physicsLinear polarizationPhysicsDegenerate energy levels3p)Oblate-prolate coexistenceNuclear reactionmedicine.anatomical_structureNuclear reaction:Angular correlationsDensity functional theoryydinfysiikkaGround stateMeasuredNucleusPhysics Letters B
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