Search results for "fields"

showing 10 items of 575 documents

Physics at CERN's Antiproton Decelerator

2013

The Antiproton Decelerator of CERN began operation in 1999 to serve experiments for studies of CPT invariance by precision laser and microwave spectroscopy of antihydrogen ($\bar{\rm H}$) and antiprotonic helium ($\bar{p}{\rm He}^+$). The first 12 years of operation saw cold $\bar{\rm H}$ synthesized by overlapping clouds of positrons ($e^+$) and antiprotons ($\bar{p}$) confined in magnetic Penning traps. Cold $\bar{\rm H}$ was also produced in collisions between Rydberg positronium atoms and $\bar{p}$. Ground-state $\bar{\rm H}$ was later trapped for up to $\sim 1000$ s in a magnetic bottle trap, and microwave transitions excited between its hyperfine levels. In the $\bar{p}{\rm He}^+$ ato…

Nuclear and High Energy PhysicsAtomic Physics (physics.atom-ph)Other Fields of PhysicsFOS: Physical sciences7. Clean energy01 natural sciencesPhysics - Atomic PhysicsHigh Energy Physics - ExperimentPositroniumHigh Energy Physics - Experiment (hep-ex)0103 physical sciencesPhysics::Atomic PhysicsNuclear Experiment (nucl-ex)010306 general physicsNuclear ExperimentHyperfine structureAntiprotonic heliumPhysicsMagnetic moment010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyMass ratioAntiproton Decelerator13. Climate actionAntiprotonHigh Energy Physics::ExperimentRotational spectroscopyAtomic physics
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Observation of individual spin quantum transitions of a single antiproton

2017

We report on the detection of individual spin quantum transitions of a single trapped antiproton in a Penning trap. The spin-state determination, which is based on the unambiguous detection of axial frequency shifts in presence of a strong magnetic bottle, reaches a fidelity of 92.1% . Spin-state initialization with >99.9% fidelity and an average initialization time of 24 min are demonstrated. This is a major step towards an antiproton magnetic moment measurement with a relative uncertainty on the part-per-billion level. We report on the detection of individual spin quantum transitions of a single trapped antiproton in a Penning trap. The spin-state determination, which is based on the unam…

Nuclear and High Energy PhysicsAtomic Physics (physics.atom-ph)Spin transitionOther Fields of PhysicsInitializationFOS: Physical sciences01 natural sciencesphysics.atom-phPhysics - Atomic Physics010309 optics0103 physical sciencesddc:530Physics::Atomic Physics010306 general physicsQuantumSpin-½PhysicsMeasurement methodMagnetic momentPenning traplcsh:QC1-999AntiprotonDewey Decimal Classification::500 | Naturwissenschaften::530 | PhysikAtomic physicsPräzisionsexperimente - Abteilung Blaumlcsh:Physics
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Measurement of the neutrino-oxygen neutral-current interaction cross section by observing nuclear deexcitation gamma rays

2014

We report the first measurement of the neutrino-oxygen neutral-current quasielastic (NCQE) cross section. It is obtained by observing nuclear deexcitation $\gamma$-rays which follow neutrino-oxygen interactions at the Super-Kamiokande water Cherenkov detector. We use T2K data corresponding to $3.01 \times 10^{20}$ protons on target. By selecting only events during the T2K beam window and with well-reconstructed vertices in the fiducial volume, the large background rate from natural radioactivity is dramatically reduced. We observe 43 events in the $4-30$ MeV reconstructed energy window, compared with an expectation of 51.0, which includes an estimated 16.2 background events. The background …

Nuclear and High Energy PhysicsCherenkov detectorPhysics::Instrumentation and DetectorsC-12FOS: Physical sciencesAstronomy & Astrophysicslaw.inventionHigh Energy Physics - ExperimentPhysics Particles & FieldsNuclear physicsSUPER-KAMIOKANDE DETECTORCross section (physics)High Energy Physics - Experiment (hep-ex)lawEXCITATIONABSORPTION[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]SCATTERINGO-16Nuclear ExperimentPhysicsCALIBRATIONScience & TechnologyNeutral currenthep-exPhysicsGamma rayT2K experimentFísica3. Good healthPhysical SciencesNeutrinoWEAKFiducial markerBeam (structure)
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Dynamical analysis of anisotropic inflation

2016

Inflaton coupling to a vector field via the $f^2(\phi)F_{\mu\nu}F^{\mu\nu}$ term is used in several contexts in the literature, such as to generate primordial magnetic fields, to produce statistically anisotropic curvature perturbation, to support anisotropic inflation and to circumvent the $\eta$-problem. Here, I perform dynamical analysis of such a system allowing for most general Bianchi I initial conditions. I also confirm the stability of attractor equilibrium points in phase-space directions that had not been investigated before.

Nuclear and High Energy PhysicsCosmology and Nongalactic Astrophysics (astro-ph.CO)Dynamical systems theoryFOS: Physical sciencesGeneral Physics and AstronomyGeneral Relativity and Quantum Cosmology (gr-qc)Fixed point01 natural sciencesGeneral Relativity and Quantum CosmologyGeneral Relativity and Quantum CosmologyHigh Energy Physics - Phenomenology (hep-ph)anisotropic Bianchi cosmologies0103 physical sciencesAttractorBoundary value probleminflation010306 general physicsInflation (cosmology)Physicsta114010308 nuclear & particles physicsAstronomy and Astrophysicsdynamical systemsInflatonHigh Energy Physics - PhenomenologyClassical mechanicsPhase spaceVector fieldvector fieldsAstrophysics - Cosmology and Nongalactic AstrophysicsModern Physics Letters A
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Search for the dark photon in π0 decays

2015

A sample of $1.69\times 10^7$ fully reconstructed $\pi^0\to\gamma e^+e^-$ decay candidates collected by the NA48/2 experiment at CERN in 2003--2004 is analysed to search for the dark photon ($A'$) production in the $\pi^0\to\gamma A'$ decay followed by the prompt $A'\to e^+e^-$ decay. No signal is observed, and an exclusion region in the plane of the dark photon mass $m_{A'}$ and mixing parameter $\varepsilon^2$ is established. The obtained upper limits on $\varepsilon^2$ are more stringent than the previous limits in the mass range $9~{\rm MeV}/c^2<m_{A'}<70~{\rm MeV}/c^2$. The NA48/2 sensitivity to the dark photon production in the $K^\pm\to\pi^\pm A'$ decay is also evaluated.

Nuclear and High Energy PhysicsDark matterKAON DECAYSSocio-culturaleAstronomy & Astrophysics01 natural sciencesDark photondark matterHigh Energy Physics - ExperimentPhysics Particles & FieldsNuclear physics0202 Atomic Molecular Nuclear Particle And Plasma Physics0103 physical sciencesdark matter meson decays010306 general physicsDETECTORPhysicsNuclear and High Energy Physics dark photon photon pion neutral pionneutral pionRange (particle radiation)Large Hadron ColliderScience & Technology010308 nuclear & particles physicsPhysicsphotonDark Photon; KAON DECAYSpionmeson decaysNuclear & Particles Physicslcsh:QC1-999Physics NuclearPhysical Sciencesdark photonFotoneHigh Energy Physics::ExperimentParticle Physics - Experimentlcsh:PhysicsHigh Energy Physics - Experiment; Dark Photon
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Magnetic resonance imaging of (1)H long lived states derived from parahydrogen induced polarization in a clinical system.

2015

Hyperpolarization is a powerful tool to overcome the low sensitivity of nuclear magnetic resonance (NMR). However, applications are limited due to the short lifetime of this non equilibrium spin state caused by relaxation processes. This issue can be addressed by storing hyperpolarization in slowly decaying singlet spin states which was so far mostly demonstrated for non-proton spin pairs, e.g. 13C-13C. Protons hyperpolarized by parahydrogen induced polarization (PHIP) in symmetrical molecules, are very well suited for this strategy because they naturally exhibit a long-lived singlet state. The conversion of the NMR silent singlet spin state to observable magnetization can be achieved by ma…

Nuclear and High Energy PhysicsMagnetic Resonance SpectroscopyVinyl CompoundsSpin statesProtonRadio WavesCiencias FísicasBiophysics010402 general chemistrySpin isomers of hydrogen01 natural sciencesBiochemistryMagnetizationNuclear magnetic resonanceElectromagnetic FieldsPARAHYDROGENHyperpolarization (physics)Singlet stateHYPERPOLARIZATIONPHIP010405 organic chemistryChemistryPULSE SEQUENCEPulse sequenceNuclear magnetic resonance spectroscopyCondensed Matter PhysicsMagnetic Resonance Imaging0104 chemical sciencesAstronomíaLONG LIVED STATECondensed Matter::Strongly Correlated ElectronsProtonsCIENCIAS NATURALES Y EXACTASHydrogenJournal of magnetic resonance (San Diego, Calif. : 1997)
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A search for neutron to mirror-neutron oscillations using the nEDM apparatus at PSI

2021

It has been proposed that there could be a mirror copy of the standard model particles, restoring the parity symmetry in the weak interaction on the global level. Oscillations between a neutral standard model particle, such as the neutron, and its mirror counterpart could potentially answer various standing issues in physics today. Astrophysical studies and terrestrial experiments led by ultracold neutron storage measurements have investigated neutron to mirror-neutron oscillations and imposed constraints on the theoretical parameters. Recently, further analysis of these ultracold neutron storage experiments has yielded statistically significant anomalous signals that may be interpreted as …

Nuclear and High Energy PhysicsNeutron electric dipole momentmedia_common.quotation_subjectmagnetic fieldWeak interaction[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]Astronomy & Astrophysics01 natural sciences7. Clean energyAsymmetryrotationPhysics Particles & FieldsELECTRIC-DIPOLE MOMENTweak interaction0103 physical sciencesDark matterDARK-MATTERNeutron010306 general physicsnumerical calculationsmirrorNuclear mattermedia_commonoscillation: timePhysicsn: electric momentProperties of neutrons Ultracold neutrons Nuclear matter Mirror matter Dark matter Particle symmetriesScience & TechnologyProperties of neutronsParticle symmetries010308 nuclear & particles physicsparity: symmetryPhysicsNuclear matter[PHYS.PHYS.PHYS-GEN-PH]Physics [physics]/Physics [physics]/General Physics [physics.gen-ph]lcsh:QC1-999Mirror matterMagnetic fieldMODELPhysics Nuclear[PHYS.HPHE]Physics [physics]/High Energy Physics - Phenomenology [hep-ph]Physical SciencesUltracold neutronsAtomic physicsUltracold neutronsMirror matterasymmetrylcsh:PhysicsPhysics Letters B
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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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Search for Heavy, Long-Lived Neutralinos that Decay to Photons at CDF II Using Photon Timing

2008

We present the results of the first hadron collider search for heavy, long-lived neutralinos that decay via lightest neutralino to gamma gravitino in gauge-mediated supersymmetry breaking models. Using an integrated luminosity of $570\pm34 pb^{-1}$ of $p\bar{p}$ collisions at $\sqrt{s}=1.96$ TeV, we select $\gamma$+jet+missing transverse energy candidate events based on the arrival time of a high-energy photon at the electromagnetic calorimeter as measured with a timing system that was recently installed on the CDF II detector. We find 2 events, consistent with the background estimate of 1.3$\pm$0.7 events. While our search strategy does not rely on model-specific dynamics, we set cross sec…

Nuclear and High Energy PhysicsParticle physicsFOS: Physical sciencesElementary particleddc:500.2Astronomy & Astrophysics;; Physics Particles & Fields7. Clean energy01 natural sciencesHigh Energy Physics - ExperimentNuclear physicsHigh Energy Physics - Experiment (hep-ex)Particle decay0103 physical sciences[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]010306 general physicsPhysicsLarge Hadron ColliderLuminosity (scattering theory)010308 nuclear & particles physicsPhysicsHigh Energy Physics::PhenomenologySupersymmetryMassless particleNeutralino_GravitinoHigh Energy Physics::Experiment13.85.Rm 12.60.Jv 13.85.Qk 14.80.Ly
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