Search results for "nuclear physics"

showing 10 items of 5307 documents

Precision measurement of the mass difference between light nuclei and anti-nuclei

2015

The measurement of the mass differences for systems bound by the strong force has reached a very high precision with protons and anti-protons. The extension of such measurement from (anti-)baryons to (anti-)nuclei allows one to probe any difference in the interactions between nucleons and anti-nucleons encoded in the (anti-)nuclei masses. This force is a remnant of the underlying strong interaction among quarks and gluons and can be described by effective theories, but cannot yet be directly derived from quantum chromodynamics. Here we report a measurement of the difference between the ratios of the mass and charge of deuterons and anti-deuterons, and $^{3}{\rm He}$ and $^3\overline{\rm He}…

electronQuarkspectroscopyAntiparticleParticle physicsPhysics of Elementary Particles and FieldsCPT symmetryStrong interactionNuclear TheoryantunucleiFOS: Physical sciencesAntiprotonGeneral Physics and Astronomy[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]ElectronHigh Energy Physics - ExperimentNuclear physicsHigh Energy Physics - Experiment (hep-ex)Physics and Astronomy (all)[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]Nuclear Physics - ExperimentNuclear Experiment (nucl-ex)Nuclear ExperimentNuclear ExperimentAntihydrogenSpectroscopyNuclear Physicsantihydrogenmass measurementQuantum chromodynamicsPhysicsanti-nucleita114SPECTROSCOPY; ANTIHYDROGEN; ANTIPROTON; ELECTRONmass difference nuclei antunucleiHigh Energy Physics::Phenomenologymass differenceNATURAL SCIENCES. Physics.3. Good healthGluonPRIRODNE ZNANOSTI. Fizika.antiprotonnucleiQuark–gluon plasmamassmass difference ; nuclei ; anti-nuclei ; ALICE ; CERNHigh Energy Physics::ExperimentNucleon
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Muon-electron lepton-flavor-violating transitions : Shell-model calculations of transitions in 27Al

2018

In this paper we present the results of large-scale shell-model calculations of muon-to-electron lepton-flavorviolating transitions for the case of the target nucleus 27Al. We extend the previous shell-model calculations, done in the sd model space, by including also the p orbitals in order to see whether the negative-parity states produce any significant effect in the conversion rate. The analysis of the results shows the dominance of coherent transitions mediated by isovector operators and going by the ground state of the target, with practically null influence of excited positive- or negative-parity states. peerReviewed

electroweak interactionelectroweak interactions in nuclear physicsnuclear fragmentationydinfysiikkalepton induced nuclear reactionsflavor changing neutral currentsnuclear tests of fundamental interactions
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Analysis of light neutrino exchange and short-range mechanisms in 0νββ decay

2020

Neutrinoless double beta decay (0νββ) is a crucial test for lepton number violation. Observation of this process would have fundamental implications for neutrino physics, theories beyond the Standard Model and cosmology. Focusing on so-called short-range operators of 0νββ and their potential interplay with the standard light Majorana neutrino exchange, we present the first complete calculation of the relevant nuclear matrix elements, performed within the interacting boson model (IBM-2). Furthermore, we calculate the relevant phase space factors using exact Dirac electron wave functions, taking into account the finite nuclear size and screening by the electron cloud. The obtained numerical r…

electroweak interactions in nuclear physicsHigh Energy Physics::PhenomenologyHigh Energy Physics::Experimentsymmetrieshiukkasfysiikkaydinfysiikkanuclear structure and decaysneutrinoless double beta decaynuclear tests of fundamental interactions
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Structure of superheavy nuclei along decay chains of element 115

2014

[Introduction] A recent high-resolution α , X -ray, and γ -ray coincidence-spectroscopy experiment offered the first glimpse of excitation schemes of isotopes along α -decay chains of Z = 115. To understand these observations and to make predictions about shell structure of superheavy nuclei below 288 115, we employ two complementary mean-field models: the self-consistent Skyrme energy density functional approach and the macroscopic-microscopic Nilsson model. We discuss the spectroscopic information carried by the new data. In particular, candidates for the experimentally observed E 1 transitions in 276 Mt are proposed. We find that the presence and nature of low-energy E 1 transitions in w…

element 115PhysicsCouplingNuclear and High Energy Physicsta114IsotopeNuclear TheoryStructure (category theory)Nuclear structureNuclear physicssuperheavy elementsfission-barriersnuclear structuredensity functional calculationsPhysical SciencesSubatomic Physicsheaviest nucleiAlpha decayDecay chainElement (category theory)Nilsson-Strutinsky calculationsquasi-particle statesExcitationPhysical Review C
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Microscopic structure of coexisting $0^+$ states in $^{68}$Ni probed via two-neutron transfer

2019

© 2019 authors. Published by the American Physical Society. Published by the American Physical Society under the terms of the Creative Commons Attribution 4.0 International license. Further distribution of this work must maintain attribution to the author(s) and the published article's title, journal citation, and DOI. The structure of low-spin states originating from shape-coexisting configurations in Ni284068 was directly probed via the two-neutron transfer reaction Ni66(t,p)Ni68 in inverse kinematics using a radioactive ion beam on a radioactive target. The direct feeding to the first excited 0+ state was measured for center-of-mass angles 4-16 and amounts to an integral of 4.2(16)% rela…

energy levels and level densitiestransfer reactionsNuclear Physics - Experimentcollective levels[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]ydinfysiikkaNuclear Structure
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The Large Hadron–Electron Collider at the HL-LHC

2021

The Large Hadron-Electron Collider (LHeC) is designed to move the field of deep inelastic scattering (DIS) to the energy and intensity frontier of particle physics. Exploiting energy-recovery technology, it collides a novel, intense electron beam with a proton or ion beam from the High-Luminosity Large Hadron Collider (HL-LHC). The accelerator and interaction region are designed for concurrent electron-proton and proton-proton operations. This report represents an update to the LHeC's conceptual design report (CDR), published in 2012. It comprises new results on the parton structure of the proton and heavier nuclei, QCD dynamics, and electroweak and top-quark physics. It is shown how the LH…

energy recoverylepton nucleus: scatteringparton: distribution functionhiukkasfysiikka7. Clean energy01 natural sciencesaccelerator physicsHigh Energy Physics - Phenomenology (hep-ph)HEAVY FLAVOR CONTRIBUTIONSenergy-recovery- linacNuclear Experimentcolliding beams [electron p]deep-inelastic scatteringtop and electroweak physicsnew physicsPhysicsSTRUCTURE-FUNCTION RATIOSMonte Carlo [numerical calculations]buildingsprimary [vertex]High Energy Physics - Phenomenologyelectron p: colliding beamskinematicsNuclear Physics - Theoryfinal state: hadronicp: distribution functionbeyond Standard Modelvertex: primarynumerical calculations: Monte Carlodistribution function [parton]High-lumiLHCSTRUCTURE-FUNCTION F-2(X[PHYS.NUCL]Physics [physics]/Nuclear Theory [nucl-th]ion: beam[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]114 Physical sciencesNuclear Theory (nucl-th)deep inelastic scatteringquantum chromodynamicsddc:530010306 general physicsdeep-inelastic scattering; high-lumi LHC; QCD; Higgs; top and electroweak physics; nuclear physics; beyond standard Model; energy-recovery- linac; accelerator physics010308 nuclear & particles physicshigh-lumi LHCresolutionscattering [electron p]structure function [nucleus]sensitivitybeam [electron]energy-recovery-linacHiggsacceptanceNuclear TheoryHIGH-ENERGY FACTORIZATIONdistribution function [p]density [parton]Higgs; High-lumi LHCHigh Energy Physics - Experimentdesign [detector]High Energy Physics - Experiment (hep-ex)electron: linear acceleratorelectron hadron: scatteringCERN LHC Coll: upgrade[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]scattering [electron hadron]FCCelectron: beamNuclear Experiment (nucl-ex)linear accelerator [electron]Nuclear ExperimentlatticesuperconductivityEnergy-recoverylinacBeyond Standard ModeNuclear physics; QCDelectron nucleus: colliding beamsparton: densitycolliding beams [electron nucleus]Particle Physics - ExperimentNUCLEON STRUCTURE FUNCTIONSNuclear and High Energy Physicsscattering [lepton nucleus]beam [ion]FOS: Physical sciencesnucleus: structure functionhadronic [final state]electron p: scatteringTRANSVERSE-MOMENTUM DEPENDENCEnuclear physics0103 physical sciencesNuclear Physics - Experimentstructureupgrade [CERN LHC Coll]detector: designParticle Physics - PhenomenologyDEEP-INELASTIC-SCATTERINGelectroweak interaction3-LOOP SPLITTING FUNCTIONSCLASSICAL RADIATION ZEROScalibrationAccelerators and Storage RingsQCDmagnethigh [current]13. Climate action[PHYS.HPHE]Physics [physics]/High Energy Physics - Phenomenology [hep-ph]LHeCPhysics::Accelerator PhysicsJET CROSS-SECTIONSHigh Energy Physics::Experimentcurrent: highJournal of Physics G: Nuclear and Particle Physics
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Optically pumped Cs magnetometers enabling a high-sensitivity search for the neutron electric dipole moment

2020

An array of 16 laser-pumped scalar Cs magnetometers was part of the neutron electric dipole moment (nEDM) experiment taking data at the Paul Scherrer Institute in 2015 and 2016. It was deployed to measure the gradients of the experiment's magnetic field and to monitor their temporal evolution. The originality of the array lies in its compact design, in which a single near-infrared diode laser drives all magnetometers that are located in a high-vacuum chamber, with a selection of the sensors mounted on a high-voltage electrode. We describe details of the Cs sensors' construction and modes of operation, emphasizing the accuracy and sensitivity of the magnetic-field readout. We present two app…

experimental methodsAtomic Physics (physics.atom-ph)EXPERIMENTAL LIMITPhysics Atomic Molecular & Chemicalnucl-ex01 natural sciencesPhysics - Atomic PhysicsHigh Energy Physics - Experimentlaw.inventionHigh Energy Physics - Experiment (hep-ex)law[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]Nuclear Experiment (nucl-ex)n: spinNuclear ExperimentPhysicsn: electric momentPhysicsincluding interactions with strong fields and short pulsesMagnetic fieldAtomic and molecular processes in external fieldsPhysical SciencesParticle Physics - ExperimentNeutron electric dipole momentMagnetometerOther Fields of PhysicsFOS: Physical sciencesmagnetic field: gradient[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]physics.atom-phOptics0103 physical sciencesNeutronNuclear Physics - ExperimentSensitivity (control systems)010306 general physicsDiodeScience & Technology010308 nuclear & particles physicsbusiness.industryhep-exScalar (physics)OpticssensitivityLaser[PHYS.PHYS.PHYS-GEN-PH]Physics [physics]/Physics [physics]/General Physics [physics.gen-ph]laserfield strengthtime dependencebusinessexperimental results
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First measurement of proton's charge form factor at very low $Q^2$ with initial state radiation

2017

We report on a new experimental method based on initial-state radiation (ISR) in e-p scattering, in which the radiative tail of the elastic e-p peak contains information on the proton charge form factor ($G_E^p$) at extremely small $Q^2$. The ISR technique was validated in a dedicated experiment using the spectrometers of the A1-Collaboration at the Mainz Microtron (MAMI). This provided first measurements of $G_E^p$ for $0.001\leq Q^2\leq 0.004 (GeV/c)^2$.

experimental methodsProtonelastic scattering01 natural sciencesHigh Energy Physics - ExperimentLamb shiftHigh Energy Physics - Experiment (hep-ex)Initial state radiation ; Proton ; Form factor ; Radiative correctionsRadiative transfer[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex][ PHYS.NEXP ] Physics [physics]/Nuclear Experiment [nucl-ex]Nuclear Experiment (nucl-ex)Nuclear ExperimentNuclear ExperimentMicrotronElastic scatteringPhysicsForm factor (quantum field theory)beam: currentRadiative correctionslcsh:QC1-9993. Good healthPRIRODNE ZNANOSTI. Fizika.ProtonNuclear and High Energy PhysicsFOS: Physical sciencesBethe-Heitler25.30.BfRadiation[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]Nuclear physicselectron p: scatteringMainz Linac[ PHYS.HEXP ] Physics [physics]/High Energy Physics - Experiment [hep-ex]12.20.-m0103 physical sciencesradiation: initial-state interaction010306 general physicsnumerical calculationsform factor: charge41.60.-m010308 nuclear & particles physicsScatteringp: chargeNATURAL SCIENCES. Physics.microtronForm factorLamb shiftspectrometerInitial state radiationlcsh:Physicsexperimental results
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Reassigning the shapes of the 0+ states in the 186Pb nucleus

2022

Across the physics disciplines, the 186Pb nucleus is the only known system, where the two first excited states, together with the ground state, form a triplet of zero-spin states assigned with prolate, oblate and spherical shapes. Here we report on a precision measurement where the properties of collective transitions in 186Pb were determined in a simultaneous in-beam γ-ray and electron spectroscopy experiment employing the recoil-decay tagging technique. The feeding of the 0+2 state and the interband 2+2→2+1 transition have been observed. We also present direct measurement of the energies of the electric monopole transitions from the excited 0+ states to the 0+ ground state. In contrast to…

experimental nuclear physicslyijyhiukkasfysiikkaydinfysiikkaphysics3100
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Evaporation channel as a tool to study fission dynamics

2017

The dynamics of the fission process is expected to affect the evaporation residue cross section because of the fission hindrance due to the nuclear viscosity. Systems of intermediate fissility constitute a suitable environment for testing such hypothesis, since they are characterized by evaporation residue cross sections comparable or larger than the fission ones. Observables related to emitted charged particle, due to their relatively high emission probability, can be used to put stringent constraints on models describing the excited nucleus decay and to recognize the effects of fission dynamics. In this work model simulations are compared with the experimental data collected via the ^{32}…

fission dynamics evaporation residues statistical model dynamical fission modelPhysicsNuclear and High Energy PhysicsFissility010308 nuclear & particles physicsFissionFOS: Physical sciencesFusion fissionObservableStatistical model01 natural sciencesCharged particleNuclear physicsExcited nucleus0103 physical sciencesNuclear Experiment (nucl-ex)Nuclear Experiment010306 general physicsNuclear ExperimentNuclear Physics A
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