Search results for "LEA"

showing 10 items of 41122 documents

"9-antideuterons_3" of "Multiplicity dependence of light (anti-)nuclei production in p-Pb collisions at $\sqrt{s_{\rm{NN}}}$ = 5.02 TeV"

2019

Transverse momentum distributions of anti-deuterons in the 40-60% V0A multiplicity class

$1/N_{\mathrm{ev}}\mathrm{d}^{2}N/(\mathrm{d}y\mathrm{d}p_{T})$Nuclear TheoryNuclear Experiment
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"17-3He" of "Multiplicity dependence of light (anti-)nuclei production in p-Pb collisions at $\sqrt{s_{\rm{NN}}}$ = 5.02 TeV"

2019

Transverse momentum distribution of $^{3}\mathrm{He}$ for all non single diffractive (NSD) p-Pb collisions.

$1/N_{\mathrm{ev}}\mathrm{d}^{2}N/(\mathrm{d}y\mathrm{d}p_{T})$Physics::OpticsNuclear Experiment
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"Table 3" of "The ALICE Transition Radiation Detector: construction, operation, and performance"

2017

Most probable charge deposit signal normalised to that of minimum ionising particles as a function of $\beta\gamma$ for $\pi$, $\it{e}$ and proton in pp collisions ($\sqrt{s} = 7$ TeV). Statistical uncertainties as vertical error bars. Uncertainties in momentum and thus $\beta \gamma$ determination are drawn as horizontal error bars.

$Q_{\rm MPV}/Q_{\rm MPV}^{\rm mip}$Astrophysics::High Energy Astrophysical PhenomenaNuclear Experiment
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"12-ratio_1" of "Multiplicity dependence of light (anti-)nuclei production in p-Pb collisions at $\sqrt{s_{\rm{NN}}}$ = 5.02 TeV"

2019

$\bar{d}$/d ratio as a function of transverse momentum in the 10-20% V0A multiplicity class

$\bar{d}/d$Nuclear Experiment
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"11-ratio_0" of "Multiplicity dependence of light (anti-)nuclei production in p-Pb collisions at $\sqrt{s_{\rm{NN}}}$ = 5.02 TeV"

2019

$\bar{d}$/d ratio as a function of transverse momentum in the 0-10% V0A multiplicity class

$\bar{d}/d$Nuclear Experiment
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"14-ratio_3" of "Multiplicity dependence of light (anti-)nuclei production in p-Pb collisions at $\sqrt{s_{\rm{NN}}}$ = 5.02 TeV"

2019

$\bar{d}$/d ratio as a function of transverse momentum in the 40-60% V0A multiplicity class

$\bar{d}/d$Nuclear Experiment
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"13-ratio_2" of "Multiplicity dependence of light (anti-)nuclei production in p-Pb collisions at $\sqrt{s_{\rm{NN}}}$ = 5.02 TeV"

2019

$\bar{d}$/d ratio as a function of transverse momentum in the 20-40% V0A multiplicity class

$\bar{d}/d$Nuclear Experiment
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"15-ratio_4" of "Multiplicity dependence of light (anti-)nuclei production in p-Pb collisions at $\sqrt{s_{\rm{NN}}}$ = 5.02 TeV"

2019

$\bar{d}$/d ratio as a function of transverse momentum in the 60-100% V0A multiplicity class

$\bar{d}/d$Nuclear Experiment
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"Table 4" of "Multiplicities of charged pions and unidentified charged hadrons from deep-inelastic scattering of muons off an isoscalar target"

2017

Multiplicities of unidentified negatively charged hadrons from semi-inclusive deep-inelastic scattering of muons off an isoscalar target, $M^{h^{-}}$, in bins of $x$, $y$, and $z$. Also given are the diffractive vector meson correction to the hadron count, $DVM^{h^{-}}$, and DIS count, $DVM^{DIS}$, as well as the radiative correction factors to the hadron count, $\eta^{h^{-}}$, and DIS count, $\eta^{DIS}$. The correction factors were applied to the raw multiplicity to arrive at the final multiplicity given in the table, $M^{h^{-}}$, as follows: $M^{h^{-}}$ = $M_{raw}^{h^{-}}$ * $\frac{\eta^{h^{-}}} {\eta^{DIS}}$ * $\frac{ DVM^{h^{-}} } {DVM^{DIS} }$.

$\mu^{+}$ d --> $\mu'^{+}$ $h^{-}$ XHigh Energy Physics::ExperimentNuclear ExperimentMULT
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"Table 2" of "Multiplicities of charged pions and unidentified charged hadrons from deep-inelastic scattering of muons off an isoscalar target"

2017

Multiplicities of negatively charged pions from semi-inclusive deep-inelastic scattering of muons off an isoscalar target, $M^{\pi^{-}}$, in bins of $x$, $y$, and $z$. Also given are the diffractive vector meson correction to the pion count, $DVM^{\pi^{-}}$, and DIS count, $DVM^{DIS}$, as well as the radiative correction factors to the pion count, $\eta^{\pi^{-}}$, and DIS count, $\eta^{DIS}$. The correction factors were applied to the raw multiplicity to arrive at the final multiplicity given in the table, $M^{\pi^{-}}$, as follows: $M^{\pi^{-}}$ = $M_{raw}^{\pi^{-}}$ * $\frac{\eta^{\pi^{-}}} {\eta^{DIS}}$ * $\frac{ DVM^{\pi^{-}} } {DVM^{DIS} }$.

$\mu^{+}$ d --> $\mu^{+}$ $\pi^{-}$ XNuclear TheoryHigh Energy Physics::ExperimentNuclear ExperimentMULT
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