Search results for "Physics::Accelerator Physics"

showing 10 items of 1235 documents

"Table 7" of "Measurement of the low-energy antideuteron inelastic cross section"

2020

Raw primary antiproton-to-proton ratio from Geant4-based MC simulations as a function of the momentum p_primary with sigma_inel(pbar)0.75.

5020.0P PB --> XPhysics::Accelerator PhysicsRAW_PBAR_PHigh Energy Physics::ExperimentNuclear ExperimentRaw antiproton-to-proton ratio
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"Table 5" of "Measurement of the low-energy antideuteron inelastic cross section"

2020

Raw primary antiproton-to-proton ratio from Geant4-based MC simulations as a function of the momentum p_primary with default sigma_inel(pbar).

5020.0P PB --> XPhysics::Accelerator PhysicsRAW_PBAR_PHigh Energy Physics::ExperimentNuclear ExperimentRaw antiproton-to-proton ratio
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"Table 6" of "Measurement of the low-energy antideuteron inelastic cross section"

2020

Raw primary antiproton-to-proton ratio from Geant4-based MC simulations as a function of the momentum p_primary with sigma_inel(pbar)x1.25.

5020.0P PB --> XPhysics::Accelerator PhysicsRAW_PBAR_PHigh Energy Physics::ExperimentNuclear ExperimentRaw antiproton-to-proton ratioPhysics::Atmospheric and Oceanic Physics
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"Table 13" of "Production of charged pions, kaons and (anti-)protons in Pb-Pb and inelastic pp collisions at $\sqrt{s_{\rm{NN}}}$ = 5.02 TeV"

2021

Integrated yield ratios of protons ($p+pbar$) to pions ($\pi^{+}+\pi^{-}$) measured in Pb-Pb collisions at $\sqrt{s_{NN}}$ = 5.02 TeV.

5020.0PB PB --> PBAR XNuclear TheoryPB PB --> PI+ XPB PB --> PI- XDifferential DistributionDN/DPTInclusivePB PB --> P XPhysics::Accelerator PhysicsHigh Energy Physics::ExperimentNuclear ExperimentPB PB --> CHARGED XTransverse Momentum Dependence
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"Table 1" 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 production cross section of heavy-flavour decay muons at forward rapidity (proton-going side) and backward rapidity (Pb-going side)

5020.0p PB --> MUON XHigh Energy Physics::PhenomenologyPhysics::Accelerator PhysicsHigh Energy Physics::ExperimentNuclear ExperimentSIG
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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 6" 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 forward-to-backward ratio of heavy-flavour decay muons

5020.0p PB --> MUON XPhysics::Instrumentation and DetectorsHigh Energy Physics::LatticeHigh Energy Physics::PhenomenologyPhysics::Accelerator PhysicsHigh Energy Physics::ExperimentSIG
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Direct measurement of resonance driving terms in the super proton synchrotron (SPS) of cern using beam position monitors

2003

El objetivo principal de esta tesis consiste en desarrollar un metodo para medir los terminos resonantes del Hamiltoniano de un acelerador mediante la transfomada de Fourier de la posicion del haz vuelta tras vuelta. Dos aspectos fundamentales de este metodo de medida son: el efecto de la decoherencia del haz en el espectro de Fourier y la variacion longitudinal de estos terminos resonantes. Ambos se estudian analiticamente y mediante simulaciones numericas. Con el fin de probar la validez de esta tecnica se realizaron experimentos en dos aceleradores de hadrones: el SPS del CERN y el RHIC del BNL. Por ultimo se estudia como utilizar dipolos AC para que esta tecnica no sea destructiva

53nonePhysics::Accelerator PhysicsFísicaNuclear ExperimentAccelerators and Storage Rings
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Design study for a 500 MeV positron beam at the Mainz Microtron MAMI

2022

A design study has been performed for a positron beam with an energy of 500 MeV to be realized at the applied physics area of the Mainz Microtron MAMI. Positrons will be created after pair conversion of bremsstrahlung, produced by the 855 MeV electron beam af MAMI in a tungsten converter target. From the two conceivable geometries (i) pair conversion in the bremsstrahlung converter target itself, and (ii) bremsstrahlung pair conversion in a separated lead foil, the former was considered in detail. Positrons will be energy selected within an outside open electron beam-line bending magnet, and bent back by an additional sector magnet. Magnetic focusing elements in between are designed to prep…

Accelerator Physics (physics.acc-ph)530 PhysicsPhysics::Instrumentation and DetectorsPhysics::Accelerator PhysicsFOS: Physical sciencesPhysics - Accelerator Physics530 PhysikNuclear ExperimentAtomic and Molecular Physics and Optics
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