Search results for "P PB"

showing 10 items of 405 documents

"Table 47" of "Large-angle production of charged pions by 3 GeV/c - 12.9 GeV/c protons on beryllium, aluminium and lead targets"

2007

Double-differential cross section for PI- production from PB in the LAB system for PI- polar angle from 0.55 to 0.75 radians.

P PB --> PI- XP NUCLEUS --> PI- XInclusiveD2SIG/DP/DTHETADouble Differential Cross SectionAngular Dependence
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"Table 54" of "Large-angle production of charged pions by 3 GeV/c - 12.9 GeV/c protons on beryllium, aluminium and lead targets"

2007

Double-differential cross section for PI- production from PB in the LAB system for PI- polar angle from 1.95 to 2.15 radians.

P PB --> PI- XP NUCLEUS --> PI- XInclusiveD2SIG/DP/DTHETADouble Differential Cross SectionAngular Dependence
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"Table 21" of "Freeze-out radii extracted from three-pion cumulants in pp, p-Pb and Pb-Pb collisions at the LHC"

2014

Exponential radii scaled down by sqrt(pi) and intercept parameters in pPb collisions versus Nch at low KT3.

P PB --> PI- XR lambdaInclusive5020.0Mathematics::Algebraic GeometryPhysics::Instrumentation and DetectorsPhysics::Atomic PhysicsNuclear ExperimentMathematics::Geometric TopologyP PB --> PI+ X
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"Table 24" of "Freeze-out radii extracted from three-pion cumulants in pp, p-Pb and Pb-Pb collisions at the LHC"

2014

Exponential radii scaled down by sqrt(pi) and intercept parameters in pPb collisions versus Nch at high KT3.

P PB --> PI- XR lambdaInclusive5020.0Mathematics::Algebraic GeometryPhysics::Instrumentation and DetectorsPhysics::Atomic PhysicsNuclear ExperimentMathematics::Geometric TopologyP PB --> PI+ X
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"Table 18" of "Freeze-out radii extracted from three-pion cumulants in pp, p-Pb and Pb-Pb collisions at the LHC"

2014

Edgeworth radii and intercept parameters in pPb collisions versus Nch at high KT3.

P PB --> PI- XR lambdaInclusive5020.0P PB --> PI+ X
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"Table 15" of "Freeze-out radii extracted from three-pion cumulants in pp, p-Pb and Pb-Pb collisions at the LHC"

2014

Edgeworth radii and intercept parameters in pPb collisions versus Nch at low KT3.

P PB --> PI- XR lambdaInclusive5020.0P PB --> PI+ X
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"Table 12" of "Freeze-out radii extracted from three-pion cumulants in pp, p-Pb and Pb-Pb collisions at the LHC"

2014

Gaussian radii and intercept parameters in pPb collisions versus Nch at high KT3.

P PB --> PI- XR lambdaInclusive5020.0Physics::Instrumentation and DetectorsAstrophysics::Earth and Planetary AstrophysicsPhysics::Atomic PhysicsNuclear ExperimentP PB --> PI+ XPhysics::Geophysics
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"Table 9" of "Freeze-out radii extracted from three-pion cumulants in pp, p-Pb and Pb-Pb collisions at the LHC"

2014

Gaussian radii and intercept parameters in pPb collisions versus Nch at low KT3.

P PB --> PI- XR lambdaInclusive5020.0Physics::Instrumentation and DetectorsAstrophysics::Earth and Planetary AstrophysicsPhysics::Atomic PhysicsNuclear ExperimentP PB --> PI+ XPhysics::Geophysics
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"Table 10" of "Inclusive $\Upsilon$ production in p-Pb collisions at $\sqrt{s_{\rm NN}}$ = 8.16 TeV"

2020

$\Upsilon$(1S) $R_{\rm pPb}$ as a function of $p_{\rm T}$ at backward rapidity at $\sqrt{s_{\rm NN}}$ = 8.16 TeV. The first uncertainty is statistical, the second is the uncorrelated systematic, while the third one is a correlated systematic uncertainty.

P PB --> UPSILON(1S) X8160.0RPA
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"Table 11" of "Inclusive $\Upsilon$ production in p-Pb collisions at $\sqrt{s_{\rm NN}}$ = 8.16 TeV"

2020

$\Upsilon$(1S) $R_{\rm pPb}$ as a function of $p_{\rm T}$ at forward rapidity at $\sqrt{s_{\rm NN}}$ = 8.16 TeV. The first uncertainty is statistical, the second is the uncorrelated systematic, while the third one is a correlated systematic uncertainty.

P PB --> UPSILON(1S) X8160.0RPA
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