Search results for "Color"

showing 10 items of 2721 documents

Glueball enhancement by color deconfinement

2007

5 pages, 4 figures.-- PACS nrs.: 14.80.-j; 24.80.+y; 25.75.Nq.-- ISI Article Identifier: 000245333000063.-- ArXiv pre-print available at: http://arxiv.org/abs/hep-ph/0609219

Nuclear and High Energy PhysicsParticle physics[PACS] Nuclear tests of fundamental interactions and symmetriesNuclear Theory[PACS] Quark deconfinement quark-gluon plasma production and phase transitions in heavy-ion collisionsHigh Energy Physics::LatticeFOS: Physical sciencesDeconfinementQuantum chromodynamics (QCD)Nuclear Theory (nucl-th)Nuclear physicsHigh Energy Physics - Phenomenology (hep-ph)Color confinementNuclear ExperimentNuclear theoryQuantum chromodynamicsPhysicsQuark confinementGlueball[PACS] Other particles (including hypothetical)High Energy Physics::PhenomenologyFísicaHigh Energy Physics - PhenomenologyColor modelHeavy ion-nucleus reactions
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The physics programme of the MoEDAL experiment at the LHC

2014

The MoEDAL experiment at Point 8 of the LHC ring is the seventh and newest LHC experiment. It is dedicated to the search for highly ionizing particle avatars of physics beyond the Standard Model, extending significantly the discovery horizon of the LHC. A MoEDAL discovery would have revolutionary implications for our fundamental understanding of the Microcosm. MoEDAL is an unconventional and largely passive LHC detector comprised of the largest array of Nuclear Track Detector stacks ever deployed at an accelerator, surrounding the intersection region at Point 8 on the LHC ring. Another novel feature is the use of paramagnetic trapping volumes to capture both electrically and magnetically ch…

Nuclear and High Energy PhysicsParticle physicsphysics beyond the Standard ModelAtomic and Molecular Physics and Opticdoubly charged particlePhysics::Instrumentation and DetectorsPhysics beyond the Standard Modelmagnetic monopoleFOS: Physical sciencesLHC magnetic monopoletechnicolor01 natural sciencesdark matterData acquisitionHigh Energy Physics - Phenomenology (hep-ph)0103 physical sciences(pseudo-)stable massive charged particle010306 general physicsNuclear and High Energy PhysicParticle Physics - PhenomenologyPhysicsLarge Hadron Collider010308 nuclear & particles physicsDetectorsupersymmetryFísicaAstronomy and AstrophysicsMoEDALAtomic and Molecular Physics and Opticsextra dimensionmonopoliumHigh Energy Physics - PhenomenologyMoEDAL experimentNuclear trackhighly ionizing particlesupersymmetrydyonINTERNATIONAL JOURNAL OF MODERN PHYSICS A
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Azimuthal harmonics of color fields in a high energy nucleus

2015

Recent experimental results have revealed a surprisingly rich structure of multiparticle azimuthal correlations in high energy proton-nucleus collisions. Final state collective effects can be responsible for many of the observed effects, but it has recently been argued that a part of these correlations are present already in the wavefunctions of the colliding particles. We evaluate the momentum space 2-particle cumulant azimuthal anisotropy coefficients v_n{2}, n=2,3,4 from fundamental representation Wilson line distributions describing the high energy nucleus. These would correspond to the flow coefficients in very forward proton nucleus scattering. We find significant differences beteen W…

Nuclear and High Energy PhysicsWilson loopNuclear TheoryGLASMA FLUX TUBESFOS: Physical sciencesPosition and momentum space114 Physical sciences01 natural sciencesColor-glass condensateNuclear Theory (nucl-th)GLUON DISTRIBUTION-FUNCTIONSHigh Energy Physics - Phenomenology (hep-ph)CONDENSATE0103 physical sciencesSIDEproton-nucleus collisionsMultiplicity (chemistry)LONG-RANGE010306 general physicsAnisotropyWave functionNuclear ExperimentPhysicsta114010308 nuclear & particles physicsScatteringPB COLLISIONSTRANSVERSE-MOMENTUMMULTIPLICITYPPB COLLISIONSANGULAR-CORRELATIONSlcsh:QC1-999High Energy Physics - PhenomenologyQuantum electrodynamicsmultiparticle azimuthal correlationsColor chargelcsh:PhysicsPhysics Letters B
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On the use of a running coupling in the calculation of forward hadron production at next-to-leading order

2018

We study a puzzle raised recently regarding the running coupling prescription used in the calculation of forward particle production in proton-nucleus collisions at next-to-leading order: using a coordinate space prescription which is consistent with the one used in the high energy evolution of the target leads to results which can be two orders of magnitude larger than the ones obtained with a momentum space prescription. We show that this is an artefact of the Fourier transform involved when passing between coordinate and momentum space and propose a new coordinate space prescription which avoids this problem.

Nuclear and High Energy Physicslead: targetHadronFOS: Physical sciencesPosition and momentum spacehiukkasfysiikka114 Physical sciences01 natural sciencesColor-glass condensatesymbols.namesakecoupling constant: energy dependenceHigh Energy Physics - Phenomenology (hep-ph)0103 physical sciencesStatistical physicshadron: productionCoordinate space010306 general physicsCouplingPhysicsenergy: highta114010308 nuclear & particles physicssaturationhigher-order: 1Order (ring theory)High Energy Physics - Phenomenology* Automatic Keywords *Fourier transform[PHYS.HPHE]Physics [physics]/High Energy Physics - Phenomenology [hep-ph]Color Glass Condensatesymbolsp nucleusOrder of magnitudeNuclear Physics A
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The search for dark matter gauge bosons with the Mainz Microtron

2011

Abstract A pilot experiment in the search for light gauge bosons at the spectrometer setup of the A1 collaboration at MAMI is presented. Light gauge bosons arise naturally in a wide range of theoretical approaches beyond the standard model and are in accordance with several pieces of experimental evidence not yet understood in the standard model. A first test measurement at MAMI showed that existing limits on the coupling of such a light gauge boson can be improved by nearly an order of magnitude by fixed target experiments at existing electron accelerators.

Nuclear physicsHidden sectorPhysicsNuclear and High Energy PhysicsGauge bosonParticle physicsSpectrometerPhysics beyond the Standard ModelHigh Energy Physics::PhenomenologyDark matterTechnicolorMicrotronStandard ModelProgress in Particle and Nuclear Physics
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A Method for Measurements of the Total 2H(γ,π−)PP Cross Sections at Threshold

1979

In recent years measurements of the total cross section for the reactions 2H(γ,π+ nn) and 2H(γ,π0)2H close to the production threshold were performed1. For the 2H(γ,π−)pp reaction data of similar good quality doesn’t exist. In this paper a method is prescribed and the feasibility for the reaction 2H(γ,π−)pp is demonstrated. Figure 1 shows the principle: The photon beam hits a liquid or high pressured gas target of 2H. π− are created on the deuteron and stopped in the same target cell. The major part of the tt are captured π− are captured by deuterons via the reaction 2H(π−,n)n. The energy is shared equally by the two neutrons (En= 68.2 MeV). One of these monochromatic neutrons is detected b…

Nuclear physicsPhysicsCross section (physics)Time of flightQuality (physics)DeuteriumNeutron detectionNeutronMonochromatic colorPhoton beam
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Dipole amplitude with uncertainty estimate from HERA data and applications in Color Glass Condensate phenomenology

2014

We determine the initial condition for the small-x evolution equation (BK) from the HERA deep inelastic scattering data using a new parametrization that also keeps the unintegrated gluon distribution positive. The obtained dipole amplitude and its uncertainty estimate can be used to compute single inclusive particle production in proton-proton and proton-nucleus collisions. We argue that one has to use consistently the proton transverse area measured in DIS and the total inelastic cross section when calculating the single inclusive cross section. This leads to a midrapidity nuclear modification factor RpA that approaches unity at large transverse momentum, independently of the center-of-mas…

Nuclear physicsPhysicsDipoleAmplitudeNuclear TheoryInitial value problemHERANuclear ExperimentDeep inelastic scatteringPhenomenology (particle physics)Color-glass condensateGluonProceedings of XXII. International Workshop on Deep-Inelastic Scattering and Related Subjects — PoS(DIS2014)
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European Hadron Facility

1989

In this contribution we survey the physics potential of a facility such as EHF in somewhat general terms. In other words, we outline some fundamental questions in nuclear physics and low energy particle physics to whose advancement EHF can and will make substantial contributions, without going into specific experiments needed to answer them. It is the role of the case studies, presented in the EHF proposal(1), to illustrate the kind of experimental effort (typical beam requirements, characteristic detectors, size of experiments, etc.) needed at EHF for the physics one wishes to clarify.

Nuclear physicsPhysicsLow energyHadronColor confinementBeam (structure)
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Next-to-next-to-leading order corrections to three-jet observables in electron-positron annihilation.

2008

I report on a numerical program, which can be used to calculate any infrared safe three-jet observable in electron-positron annihilation to next-to-next-to-leading order in the strong coupling constant ${\ensuremath{\alpha}}_{s}$. The results are compared to a recent calculation by another group. Numerical differences in three color factors are discussed and explained.

Nuclear physicsQuantum chromodynamicsPhysicsRenormalizationParticle physicsColor modelAnnihilationElectron–positron annihilationGeneral Physics and AstronomyOrder (ring theory)ObservableJet (particle physics)Physical review letters
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A novel approach to measure the cross section of the 18O(p, α)15N resonant reaction in the 0-200 keV energy range

2009

The 18O(p, ?)15N reaction is of primary importance to pin down the uncertainties, due to nuclear physics input, affecting present-day models of asymptotic giant branch stars. Its reaction rate can modify both fluorine nucleosynthesis inside such stars and oxygen and nitrogen isotopic ratios, which allow one to constrain the proposed astrophysical scenarios. Thus, an indirect measurement of the low-energy region of the 18O(p, ?)15N reaction has been performed to access, for the first time, the range of relevance for astrophysical application. In particular, a full, high-accuracy spectroscopic study of the 20 and 90 keV resonances has been performed and the strengths deduced to evaluate the r…

Nuclear reactionstars: abundances7. Clean energy01 natural sciencesReaction rateNuclear physicsNucleosynthesis0103 physical sciencesAsymptotic giant branchAstrophysics::Solar and Stellar AstrophysicsNuclear Experiment010303 astronomy & astrophysicsnuclear reactionsPhysics010308 nuclear & particles physicsabundances[SDU.ASTR.SR]Sciences of the Universe [physics]/Astrophysics [astro-ph]/Solar and Stellar Astrophysics [astro-ph.SR]stars: AGB and post-AGB Online-only material: color figuresnucleosynthesisAstronomy and AstrophysicsAlpha particle[PHYS.ASTR.SR]Physics [physics]/Astrophysics [astro-ph]/Solar and Stellar Astrophysics [astro-ph.SR]Charged particleStars13. Climate actionSpace and Planetary ScienceAtomic physicsDimensionless quantity
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