Search results for "protons"

showing 10 items of 158 documents

High-precision mass measurements for the rp-process at JYFLTRAP

2017

The double Penning trap JYFLTRAP at the University of Jyvaskyla has been successfully used to achieve high-precision mass measurements of nuclei involved in the rapid proton-capture (rp) process. A precise mass measurement of 31 Cl is essential to estimate the waiting point condition of 30 S in the rp-process occurring in type I x-ray bursts (XRBs). The mass-excess of 31 C1 measured at JYFLTRAP, -7034.7(3.4) keV, is 15 more precise than the value given in the Atomic Mass Evaluation 2012. The proton separation energy S p determined from the new mass-excess value confirmed that 30 S is a waiting point, with a lower-temperature limit of 0.44 GK. The mass of 52 Co effects both 51 Fe( p,γ ) 52 C…

PhysicsIon Traps (Instrumentation)protonitProtonta114protons010308 nuclear & particles physicsPhysicsQC1-999Analytical chemistryAntiprotonsrp-processPenning trapatomipainot01 natural sciencesMass measurementAtomic massnukleonitnucleons0103 physical sciencesmassamass010306 general physicsAtomic Weights
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Fine structure in the beta-delayed proton decay of 33Ar

1996

9 pages, 2 figures, 2 tables.-- PACS nrs.: 21.60.Cs; 23.40.−s; 27.30.+t; 29.30.Ep.

PhysicsMeasured beta-delayed protons Ep IpNuclear and High Energy PhysicsDeduced relative spectroscopic amplitudesAr-33 (from 1 GeV p on Nb-foil target selective mass separation)Proton decaySHELL modelShell nucleiShell-model calculationGas-Si telescope spectrometerShell modelEmissionBeta-delayed proton decayAmplitudeAtomic orbitalExcited stateBeta (plasma physics)Nuclear Physics - ExperimentAtomic physicsNuclear Physics A
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The polarized double cell target of the SMC

1999

The polarized target of the Spin Muon Collaboration at CERN was used for deep inelastic muon scattering experiments during 1993-1996 with a polarized muon beam to investigate the spin structure of the nucleon. Most of the experiments were carried out with longitudinal target polarization and 190 GeV muons, and some were done with transverse polarization and 100 GeV muons. Protons as well as deuterons were polarized by dynamic nuclear polarization (DNP) in three kinds of solid materials - butanol, ammonia, and deuterated butanol - with maximum degrees of polarization of 94%, 91% and 60%, respectively. Considerable attention was paid to the accuracies of the NMR polarization measurements and …

PhysicsNuclear and High Energy PhysicsDISLarge Hadron ColliderMuonanalysisScatteringSMCPolarized targetSpin structurepolarized protons and deuteronsPolarization (waves)Deep inelastic scatteringNMRdynamic nuclear polarizationSMC; DIS; Polarized targetNuclear physicsDeuteriumPhysics::Accelerator PhysicsHigh Energy Physics::ExperimentDetectors and Experimental TechniquesNuclear ExperimentNucleonInstrumentation
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Direct evidence of secondary recoiled nuclei from high energy protons

2008

The production of secondary recoiled particles from interactions between high energy protons and microelectronics devices was investigated. By using NAND Flash memories, we were able to directly obtain analog information on recoil characteristics. While our results qualitatively confirm the role of nuclear reactions, in particular of those with tungsten, a quantitative model based on Monte Carlo and device-level simulations cannot describe the observed results in terms of recoils from proton-W reactions. © 2006 IEEE.

PhysicsNuclear reactionNuclear and High Energy Physicsbusiness.industryDirect evidencePhysics::Instrumentation and DetectorsMonte Carlo methodNAND gatechemistry.chemical_elementHigh energy protonsSingle event effectsTungstenFlash memorySpace radiationNuclear physicsRecoilNuclear Energy and EngineeringchemistryFloating gate memoriesMicroelectronicsElectrical and Electronic EngineeringAtomic physicsbusinessNuclear Experiment
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Predictions of covariant chiral perturbation theory for nucleon polarisabilities and polarised Compton scattering

2015

We update the predictions of the SU(2) baryon chiral perturbation theory for the dipole polarisabilities of the proton, $\{\alpha_{E1},\,\beta_{M1}\}_p=\{11.2(0.7),\,3.9(0.7)\}\times10^{-4}$fm$^3$, and obtain the corresponding predictions for the quadrupole, dispersive, and spin polarisabilities: $\{\alpha_{E2},\,\beta_{M2}\}_p=\{17.3(3.9),\,-15.5(3.5)\}\times10^{-4}$fm$^5$, $\{\alpha_{E1\nu},\,\beta_{M1\nu}\}_p=\{-1.3(1.0),\,7.1(2.5)\}\times10^{-4}$fm$^5$, and $\{\gamma_{E1E1},\,\gamma_{M1M1},\,\gamma_{E1M2},\,\gamma_{M1E2}\}_p=\{-3.3(0.8),\,2.9(1.5),\,0.2(0.2),\,1.1(0.3)\}\times10^{-4}$fm$^4$. The results for the scalar polarisabilities are in significant disagreement with semi-empirical …

PhysicsParticle physicsChiral perturbation theoryNuclear TheoryPhysics and Astronomy (miscellaneous)ProtonFOS: Physical sciencesCompton scattering Protons and neutron polarisabilitiesNuclear Theory (nucl-th)BaryonHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)PionProduction (computer science)Sensitivity (control systems)Sum rule in quantum mechanicsNucleonEngineering (miscellaneous)The European Physical Journal C
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Monte Carlo study of microdosimetric diamond detectors

2015

Ion-beam therapy provides a high dose conformity and increased radiobiological effectiveness with respect to conventional radiation-therapy. Strict constraints on the maximum uncertainty on the biological weighted dose and consequently on the biological weighting factor require the determination of the radiation quality, defined as the types and energy spectra of the radiation at a specific point. However the experimental determination of radiation quality, in particular for an internal target, is not simple and the features of ion interactions and treatment delivery require dedicated and optimized detectors. Recently chemical vapor deposition (CVD) diamond detectors have been suggested as …

PhysicsPhotonsWork (thermodynamics)PhotonRadiological and Ultrasound Technologybusiness.industryDetectorMonte Carlo methodUncertaintyDiamondRadiationengineering.materialIonOpticsengineeringRadiometryRadiology Nuclear Medicine and imagingDiamondProtonsRadiometrybusinessMonte Carlo MethodPhysics in Medicine and Biology
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Effect of a Triaxial Nuclear Shape on Proton Tunneling: The Decay and Structure of 145Tm

2007

Gamma rays deexciting states in the proton emitter 145Tm were observed using the recoil-decay tagging method. The 145Tm ground-state rotational band was found to exhibit the properties expected for an h{11/2} proton decoupled band. In addition, coincidences between protons feeding the 2{+} state in 144Er and the 2{+}-->0{+} gamma-ray transition were detected, the first measurement of this kind, leading to a more precise value for the 2{+} excitation energy of 329(1) keV. Calculations with the particle-rotor model and the core quasiparticle coupling model indicate that the properties of the pi{11/2} band and the proton-decay rates in 145Tm are consistent with the presence of triaxiality with…

PhysicsProton010308 nuclear & particles physicsAstrophysics::High Energy Astrophysical PhenomenaHadronGamma rayGeneral Physics and Astronomy[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]Coupling (probability)01 natural sciencesGamma RaysExcited state0103 physical sciencesQuasiparticle23.20.Lv 23.50.+z 27.60.+jAtomic physicsProtons010306 general physicsNucleonRadioactive decay
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Energy loss measurement of protons in liquid water

2011

The proton stopping power of liquid water was, for the first time, measured in the energy range 4.7-15.2 MeV. The proton energies were determined by the time-of-flight transmission technique with the microchannel plate detectors, which were especially developed for timing applications. The results are compared to the literature values (from ICRU Report 49 (1993) and Janni's tabulation (1982 At. Data Nucl. Data Tables 27 147-339)) which are based on Bethe's formula and an agreement is found within the experimental uncertainty of 4.6%. Thus, earlier reported discrepancy between the experimental and literature stopping power values at lower energies was not observed at the energies considered …

PhysicsRange (particle radiation)Energy lossTime FactorsRadiological and Ultrasound TechnologyProtonLiquid waterDetectorWaterNuclear physicsExperimental uncertainty analysisSolventsStopping power (particle radiation)Computer SimulationLinear Energy TransferRadiology Nuclear Medicine and imagingMicrochannel plate detectorProtonsAtomic physicsRadiometryPhysics in Medicine and Biology
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Confronting the impact parameter dependent JIMWLK evolution with HERA data

2018

The small-$x$ evolution of protons is determined from numerical solutions of the JIMWLK equations, starting from an initial condition at moderate $x$ for a finite size proton. The resulting dipole amplitude is used to calculate the total reduced cross section $\sigma_r$ and charm reduced cross section $\sigma_{rc}$, as well as diffractive vector meson production. We compare results to experimental data from HERA and discuss fundamental problems arising from the regime sensitive to non-perturbative physics. We emphasize that information on the gluonic content of the proton, gluon spatial distributions and correlations over wide ranges in $x$, which can in principle be constrained by our stud…

Physicsparton densitiesParticle physicsprotonitta114protons010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyNuclear TheoryHERAhiukkasfysiikka7. Clean energy01 natural sciencesGluonColor-glass condensateHigh Energy Physics - Phenomenology0103 physical sciencesContent (measure theory)Saturation (graph theory)High Energy Physics::ExperimentProduction (computer science)Vector mesonImpact parameter010306 general physicsNuclear ExperimentPhysical Review D
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Metal coordination of azurin in the unfolded state.

1998

Abstract1H NMR data applied to the paramagnetic cobalt(II) derivative of azurin from Pseudomonas aeruginosa have made it possible to show that the metal ion is bound to the protein in the unfolded state. The relaxation data as well as the low magnetic anisotropy of the metal ion indicate that the cobalt ion is tetrahedral in the unfolded form. The cobalt ligands have been identified as the residues Gly45, His46, Cys112 and His117. Met121 is not coordinated in the unfolded state. In this state, the metal ion is not constrained to adopt a bipyramidal geometry, as imposed by the protein when it is folded. This is clear confirmation of the rack-induced bonding mechanism previously proposed for …

Protein FoldingBlue copper proteinProtein ConformationRack mechanismBiophysicschemistry.chemical_elementLigandsBiochemistryNuclear magnetic resonanceMetalParamagnetismProtein structureStructural BiologyAzurinNickelGeneticsMolecular BiologyNuclear Magnetic Resonance BiomolecularGuanidineBinding SitesCell BiologyCobaltCrystallographyNickelchemistryvisual_artPseudomonas aeruginosaProton NMRvisual_art.visual_art_mediumProtein foldingAzurinProtonsCobaltFEBS letters
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