Search results for "BT"

showing 10 items of 1498 documents

Electromagnetic moments of scandium isotopes and $N=28$ isotones in the distinctive $0f_{7/2}$ orbit

2022

The electric quadrupole moment of $^{49}$Sc was measured by collinear laser spectroscopy at CERN-ISOLDE to be $Q_{\rm s}=-0.159(8)$ $e$b, and a nearly tenfold improvement in precision was reached for the electromagnetic moments of $^{47,49}$Sc. The single-particle behavior and nucleon-nucleon correlations are investigated with the electromagnetic moments of $Z=21$ isotopes and $N=28$ isotones as valence neutrons and protons fill the distinctive $0f_{7/2}$ orbit, respectively, located between magic numbers, 20 and 28. The experimental data are interpreted with shell-model calculations using an effective interaction, and ab-initio valence-space in-medium similarity renormalization group calcu…

Nuclear and High Energy PhysicsNuclear Theorynucl-thCollinear laser spectroscopyNuclear TheoryFOS: Physical sciencesAstronomy & Astrophysicsnucl-exComputer Science::Digital LibrariesPhysics Particles & FieldsElectromagnetic momentsNuclear Theory (nucl-th)Nuclear Physics - ExperimentNuclear Experiment (nucl-ex)Nuclear ExperimentNuclear ExperimentisotoopitScience & TechnologyPhysicsNUCLEAR MOMENTSQUADRUPOLE-MOMENTSPhysics NuclearNucleon-nucleon correlationNuclear Physics - TheoryPhysical SciencesSHELL-MODELCOLLECTIVITYPräzisionsexperimente - Abteilung BlaumydinfysiikkaskandiumAb-initio calculation
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Measurement of CP asymmetries in the decays B0 → K*0 μ+μ- and B+ → K+ μ+μ-

2014

The direct CP asymmetries of the decays B 0 → K *0 μ + μ − and B + → K + μ + μ − are measured using pp collision data corresponding to an integrated luminosity of 3.0 fb−1 collected with the LHCb detector. The respective control modes B 0 → J/ψK *0 and B + → J/ψK + are used to account for detection and production asymmetries. The measurements are made in several intervals of μ + μ − invariant mass squared, with the ϕ(1020) and charmonium resonance regions excluded. Under the hypothesis of zero CP asymmetry in the control modes, the average values of the asymmetries are ACP(B0→K∗0μ+μ−)=−0.035±0.024±0.003,ACP(B+→K+μ+μ−)=0.012±0.017±0.001, where the first uncertainties are statistical and the …

Nuclear and High Energy PhysicsParticle physicsB physicmedia_common.quotation_subject14.40.NdFlavour Changing Neutral CurrentsLHCb - Abteilung HofmannHadrons01 natural sciencesAsymmetryB physicsNOPhysics Particles & FieldsLuminosityStandard Model0103 physical sciencesLeptonic semileptonic and radiative decays of bottom mesonInvariant mass010306 general physicsLarge Hadron Collider (France and Switzerland)QCmedia_commonPhysicsFlavour Changing Neutral CurrentScience & TechnologyHadron-Hadron Scattering010308 nuclear & particles physicsPhysicsHigh Energy Physics::PhenomenologyGran Col·lisionador d'HadronsParticle physicsResonanceCharge conjugation parity time reversal and other discrete symmetrieLHCbCP violationRare decay13.20.HePhysical SciencesBottom mesons (|B|>0)11.30.ErFísica nuclearB physics; CP violation; Flavour Changing Neutral Currents; Hadron-Hadron Scattering; Rare decayProduction (computer science)High Energy Physics::ExperimentLHCFísica de partículesExperiments
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Observation of charmonium pairs produced exclusively in $pp$ collisions

2014

A search is performed for the central exclusive production of pairs of charmonia produced in proton-proton collisions. Using data corresponding to an integrated luminosity of $3{\rm\ fb}^{-1}$ collected at centre-of-mass energies of 7 and 8 TeV, $J/\psi J/\psi$ and $J/\psi\psi(2S)$ pairs are observed, which have been produced in the absence of any other activity inside the LHCb acceptance that is sensitive to charged particles in the pseudorapidity ranges $(-3.5,-1.5)$ and $(1.5,5.0)$. Searches are also performed for pairs of P-wave charmonia and limits are set on their production. The cross-sections for these processes, where the dimeson system has a rapidity between 2.0 and 4.5, are measu…

Nuclear and High Energy PhysicsParticle physicsNuclear TheorydiffractionFOS: Physical sciencesLHCb - Abteilung HofmannHEAVY-ION COLLISIONSQCD diffraction charmoniaNOHigh Energy Physics - ExperimentLuminosityHigh Energy Physics - Experiment (hep-ex)[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]Quantum chromodynamiccharmonia; diffraction; QCDcharmonia; diffraction; QCD; Nuclear and High Energy PhysicsRapiditySDG 7 - Affordable and Clean EnergyNuclear ExperimentQCPhysics/dk/atira/pure/sustainabledevelopmentgoals/affordable_and_clean_energyhep-ex12.38.-tParticle physicsHadron-induced high- and super-high-energy interactions (energy > 10 GeV): Inclusive production with identified hadronHEAVY-ION COLLISIONS; 450 GEV/C; DIFFRACTION; LHCQCDCromodinàmica quànticaLHCbDifracció450 GEV/CPseudorapidityPhysics::Accelerator PhysicscharmoniaFísica nuclearHigh Energy Physics::ExperimentProduction (computer science)LHCHEAVYFísica de partículesExperiments13.85.NiDiffractionQuantum chromodynamicsParticle Physics - ExperimentJournal of Physics G: Nuclear and Particle Physics
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Search for CP violation in D (+/-) -> (KSK +/-)-K-0 and D-s(+/-) -> K-S(0)pi(+/-) decays

2014

A search for \CP violation in Cabibbo-suppressed $D^{\pm}\rightarrow K^0_{\mathrm{S}} K^{\pm}$ and $D^{\pm}_{s}\rightarrow K^0_{\mathrm{S}} \pi^{\pm}$ decays is performed using $pp$ collision data, corresponding to an integrated luminosity of 3~fb$^{-1}$, recorded by the LHCb experiment. The individual $CP$-violating asymmetries are measured to be \begin{eqnarray*} \mathcal{A}_{CP}^{D^{\pm}\rightarrow K^0_{\mathrm{S}} K^{\pm}} & = & (+0.03 \pm 0.17 \pm 0.14) \% \mathcal{A}_{CP}^{D^{\pm}_{s}\rightarrow K^0_{\mathrm{S}} \pi^{\pm}} & = & (+0.38 \pm 0.46 \pm 0.17) \%, \end{eqnarray*} assuming that $CP$ violation in the Cabibbo-favoured decays is negligible. A combination of the measured asymmet…

Nuclear and High Energy PhysicsParticle physicsSDG 16 - Peacemedia_common.quotation_subjectCP violation; Hadron-Hadron ScatteringDalitz plotLHCb - Abteilung HofmannHadrons01 natural sciencesAsymmetryNOSettore FIS/04 - Fisica Nucleare e SubnucleareNuclear physicsTEV PP COLLISIONS; PRODUCTION ASYMMETRY0103 physical sciencesCP violation hadron-hadron scatteringPiTEV PP COLLISIONS010306 general physicsLarge Hadron Collider (France and Switzerland)PRODUCTION ASYMMETRYQCmedia_commonPhysicsLuminosity (scattering theory)Hadron-Hadron Scattering010308 nuclear & particles physicshep-exSDG 16 - Peace Justice and Strong InstitutionsHigh Energy Physics::PhenomenologyGran Col·lisionador d'HadronsParticle physicsPhi meson/dk/atira/pure/sustainabledevelopmentgoals/peace_justice_and_strong_institutionsJustice and Strong InstitutionsCP violationCP violationHigh Energy Physics::ExperimentFísica nuclearFísica de partículesExperimentsParticle Physics - Experiment
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Pileup and underlying event mitigation with iterative constituent subtraction

2019

Abstract The hard-scatter processes in hadronic collisions are often largely contaminated with soft background coming from pileup in proton-proton collisions, or underlying event in heavy-ion collisions. This paper presents a new background subtraction method for jets and event observables (such as missing transverse energy) which is based on the previously published Constituent Subtraction algorithm. The new subtraction method, called Iterative Constituent Subtraction, applies event-wide implementation of Constituent Subtraction iteratively in order to fully equilibrate the background subtraction across the entire event. Besides documenting the new method, we provide guidelines for setting…

Nuclear and High Energy PhysicsParticle physicsSubtraction methodFOS: Physical sciences01 natural sciencesMinimum biasHigh Energy Physics - ExperimentHigh Energy Physics - Experiment (hep-ex)High Energy Physics - Phenomenology (hep-ph)Hadron-Hadron scattering (experiments)0103 physical sciencesJetslcsh:Nuclear and particle physics. Atomic energy. RadioactivityHardware_ARITHMETICANDLOGICSTRUCTURES010306 general physicsNuclear ExperimentEvent (probability theory)PhysicsBackground subtractionHard scattering010308 nuclear & particles physicsSubtractionObservableHigh Energy Physics - Phenomenologylcsh:QC770-798AlgorithmJet substructureEnergy (signal processing)Underlying eventFree parameterJournal of High Energy Physics
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Evidence for Increased neutron and proton excitations between 51−63 Mn

2015

The hyperfine structures of the odd-even 51−63Mnatoms (N=26 −38) were measured using bunched beam collinear laser spectroscopy at ISOLDE, CERN. The extracted spins and magnetic dipole moments have been compared to large-scale shell-model calculations using different model spaces and effective interactions. In the case of 61,63Mn, the results show the increasing importance of neutron excitations across the N=40subshell closure, and of proton excitations across the Z=28shell gap. These measurements provide the first direct proof that proton and neutron excitations across shell gaps are playing an important role in the ground state wave functions of the neutron-rich Mn isotopes. publisher: Els…

Nuclear and High Energy PhysicsProtonNuclear TheoryMagnetic dipole momentsMagnetic dipole momentNuclear Physics - ExperimentNeutronPhysics::Atomic PhysicsNuclear ExperimentWave functionHyperfine structurePhysicsManganeseta114SpinsMagnetic momentMagnetic dipole moment; Manganese; Spin determination; Nuclear and High Energy Physicsmangaanilcsh:QC1-999Spin determinationPhysics::Accelerator PhysicsPräzisionsexperimente - Abteilung BlaumAtomic physicsGround stateMagnetic dipolelcsh:PhysicsPhysics Letters B
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Nuclear charge radii of 62−80Zn and their dependence on cross-shell proton excitations

2019

Nuclear charge radii of 62−80Zn have been determined using collinear laser spectroscopy of bunched ion beams at CERN-ISOLDE. The subtle variations of observed charge radii, both within one isotope and along the full range of neutron numbers, are found to be well described in terms of the proton excitations across the Z=28 shell gap, as predicted by large-scale shell model calculations. It comprehensively explains the changes in isomer-to-ground state mean square charge radii of 69−79Zn, the inversion of the odd-even staggering around N=40 and the odd-even staggering systematics of the Zn charge radii. With two protons above Z=28, the observed charge radii of the Zn isotopic chain show a cum…

Nuclear and High Energy PhysicsProtonShell closureNuclear TheoryAstronomy & Astrophysics[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]530ISOTOPE SHIFTS01 natural sciences7. Clean energyMolecular physicsEffective nuclear chargePhysics Particles & FieldsIonNaturvetenskap0103 physical sciencesNuclear Physics - Experimentddc:530Neutron010306 general physicsSpectroscopyNuclear ExperimentCumulative effectPhysicsScience & TechnologyIsotopeCorrelations010308 nuclear & particles physicsPhysicsNuclear structurelcsh:QC1-999Physique atomique et nucléaireNuclear deformationZincPhysics NuclearNuclear charge radiiPhysical SciencesCorrelations ; Nuclear charge radii ; Nuclear deformation ; Shell closure ; ZincPräzisionsexperimente - Abteilung BlaumNatural Scienceslcsh:Physics
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Simulation studies of the laser ablation ion source at the SHIPTRAP setup

2020

Hyperfine interactions 241(1), 46 (2020). doi:10.1007/s10751-020-01708-0

Nuclear and High Energy PhysicsSpeichertechnik - Abteilung BlaumMaterials scienceMultiphysicsNuclear engineeringPenning trapsMass spectrometry01 natural sciences530IonPhysics::Plasma Physics0103 physical sciencesSample preparationddc:530Physical and Theoretical Chemistry010306 general physicsSurface ionization ion sourceLaser ablationMass spectrometry010308 nuclear & particles physicsLaser ablation ion sourceCondensed Matter PhysicsAtomic and Molecular Physics and OpticsIon sourceThermalisationQuadrupole
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High-resolution spectroscopy of gaseous $^\mathrm{83m}$Kr conversion electrons with the KATRIN experiment

2020

In this work, we present the first spectroscopic measurements of conversion electrons originating from the decay of metastable gaseous $^\mathrm{83m}$Kr with the Karlsruhe Tritium Neutrino (KATRIN) experiment. The results obtained in this calibration measurement represent a major commissioning milestone for the upcoming direct neutrino mass measurement with KATRIN. The successful campaign demonstrates the functionalities of the full KATRIN beamline. The KATRIN main spectrometer's excellent energy resolution of ~ 1 eV made it possible to determine the narrow K-32 and L$_3$-32 conversion electron line widths with an unprecedented precision of ~ 1 %.

Nuclear and High Energy PhysicsSpeichertechnik - Abteilung BlaumPhysics - Instrumentation and DetectorsResolution (mass spectrometry)Physics::Instrumentation and Detectorsenergy resolutionFOS: Physical sciencesElectron[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]KATRIN7. Clean energy01 natural sciencesAtomicneutrino massNuclear physicsParticle and Plasma Physicsconversion electronsMetastability0103 physical sciencesNuclearddc:530[PHYS.PHYS.PHYS-INS-DET]Physics [physics]/Physics [physics]/Instrumentation and Detectors [physics.ins-det]Nuclear Experiment (nucl-ex)010306 general physicsSpectroscopyNuclear ExperimentPhysicsSpectrometerelectrostatic spectrometer010308 nuclear & particles physicsPhysicskrypton: decayMolecularInstrumentation and Detectors (physics.ins-det)krypton: nuclide530 PhysikcalibrationNuclear & Particles Physicsddc:3. Good healthBeamlineelectron: energy spectrumNeutrinoperformanceKATRIN
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The nuclear magnetic moment of 208Bi and its relevance for a test of bound-state strong-field QED

2018

Physics letters / B 779, 324 - 330 (2018). doi:10.1016/j.physletb.2018.02.024

Nuclear and High Energy Physicschemistry.chemical_elementHyperfine anomaly53001 natural sciencesBismuth0103 physical sciencesBound stateNuclear Physics - Experimentddc:530Physics::Atomic PhysicsLaser spectroscopy010306 general physicsSpectroscopyHyperfine structureQuantum electrodynamicsPhysicsSpecific difference010308 nuclear & particles physicsNuclear structurelcsh:QC1-999chemistryNuclear magnetic momentNuclear magnetic momentPräzisionsexperimente - Abteilung BlaumAtomic physicsAnomaly (physics)Bismuthlcsh:PhysicsOrder of magnitudePhysics Letters B
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