Search results for "Atomic Physics"

showing 10 items of 5530 documents

Johnson-Nyquist Noise Effects in Neutron Electric-Dipole-Moment Experiments

2021

Magnetic Johnson-Nyquist noise (JNN) originating from metal electrodes, used to create a static electric field in neutron electric-dipole-moment (nEDM) experiments, may limit the sensitivity of measurements. We present here the first dedicated study on JNN applied to a large-scale long-measurement-time experiment with the implementation of a co-magnetometry. In this study, we derive surface- and volume-averaged root-mean-square normal noise amplitudes at a certain frequency bandwidth for a cylindrical geometry. In addition, we model the source of noise as a finite number of current dipoles and demonstrate a method to simulate temporal and three-dimensional spatial dependencies of JNN. The c…

noiseNeutron electric dipole momentMagnetometerAtomic Physics (physics.atom-ph)FOS: Physical sciencesNeutron Physics[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]01 natural sciencesNoise (electronics)010305 fluids & plasmaslaw.inventionPhysics - Atomic PhysicslawElectric field0103 physical sciencesNeutronNuclear Experiment (nucl-ex)010306 general physicsNuclear ExperimentPhysicshigh-precision experimentsprecision measurementJohnson–Nyquist noiseAtomic and molecular structure and dynamics[PHYS.PHYS.PHYS-GEN-PH]Physics [physics]/Physics [physics]/General Physics [physics.gen-ph]Computational physicsDipoleNuclear Spin ResonanceAmplitudeElectromagnetic Field Calculations
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Shape staggering of midshell mercury isotopes from in-source laser spectroscopy compared with density-functional-theory and Monte Carlo shell-model c…

2019

Neutron-deficient Hg177-185 isotopes were studied using in-source laser resonance-ionization spectroscopy at the CERN-ISOLDE radioactive ion-beam facility in an experiment combining different detection methods tailored to the studied isotopes. These include either α-decay tagging or multireflection time-of-flight gating for isotope identification. The endpoint of the odd-even nuclear shape staggering in mercury was observed directly by measuring for the first time the isotope shifts and hyperfine structures of Hg177-180. Changes in the mean-square charge radii for all mentioned isotopes, magnetic dipole, and electric quadrupole moments of the odd-A isotopes and arguments in favor of I=7/2 s…

nucl-thNuclear Theory[PHYS.NUCL]Physics [physics]/Nuclear Theory [nucl-th]3106ResearchInstitutes_Networks_Beacons/photon_science_instituteharmonic-oscillator basisMonte Carlo methodFOS: Physical sciencesPhoton Science Institute[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]nucl-exNuclear Structure01 natural sciences7. Clean energyodd-massNuclear Theory (nucl-th)Atomic orbitalCharge radius0103 physical sciencesNuclear Physics - ExperimentDalton Nuclear InstituteNeutronneutron-deficient hgNuclear Experiment (nucl-ex)nuclear charge-distribution010306 general physicsNuclear ExperimentNuclear ExperimentHyperfine structurePhysics010308 nuclear & particles physicsGénéralitésexcited structuresstatesResearchInstitutes_Networks_Beacons/dalton_nuclear_institutehyperfine-structure13. Climate actionNuclear Physics - Theoryoblate-prolate transitionaxially deformed solutionQuadrupolemomentsDensity functional theoryAtomic physicsPräzisionsexperimente - Abteilung BlaumMagnetic dipole
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Penning-trap mass measurements on 92, 94-98, 100Mo with JYFLTRAP

2012

Penning-trap measurements on stable 92, 94-98, 100Mo isotopes have been performed with relative accuracy of \ensuremath1⋅10−8\ensuremath1⋅10−8 with the JYFLTRAP Penning-trap mass spectrometer by using 85Rb as a reference. The Mo isotopes have been found to be about 3keV more bound than given in the Atomic Mass Evaluation 2003 (AME03). The results confirm that the discrepancy between the ISOLTRAP and JYFLTRAP data for 101-105Cd isotopes was due to an erroneous value in the AME03 for 96Mo used as a reference at JYFLTRAP. The measured frequency ratios of Mo isotopes have been used to update mass-excess values of 30 neutron-deficient nuclides measured at JYFLTRAP. peerReviewed

nuclear spectroscopyPhysicsNuclear and High Energy PhysicsMass excessIsotopeaccelerator-based physicsPenning trapMass spectrometrykiihdytinpohjainen fysiikkaISOLTRAPAtomic massNuclear physicsydinrakennenuclear structureydinspektroskopiaNuclear fusionNuclideAtomic physicsydinfysiikkaThe European Physical Journal A
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Nuclear mean-square charge radii of $^{63,64,66,68−82}$Ga nuclei: No anomalous behavior at N=32

2012

Collinear laser spectroscopy was performed on the 63,64,66,68−82Ga isotopes with neutron numbers from N = 32 to N = 51. These measurements were carried out at the ISOLDE radioactive ion beam facility at CERN. Here we present the nuclear mean-square charge radii extracted from the isotope shifts and, for the lighter isotopes, new spin and moment values. New ground-state nuclear spin and moments were extracted from the hyperfine spectra of 63,70Ga, measured on an atomic transition in the neutral atom. The ground-state spin of 63Ga is determined to be I = 3/2. Analysis of the trend in the change in mean-square charge radii of the gallium isotopes demonstrates that there is no evidence of anoma…

nuclear spectroscopyydinrakenneaccelerator-based physicsnuclear structureydinspektroskopiaddc:530Physics::Atomic PhysicsNuclear Experimentydinfysiikkakiihdytinpohjainen fysiikka
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High-resolution spectrum of La and Ar

2013

A high-resolution spectrum of lanthanum has been recorded by a Fourier Transform spectrometer in the wavelength range from 833nm to 1666nm (6000/cm to 12000/cm) using as light source a hollow cathode lamp operated with argon as the discharge carrier gas. In total, 2386 spectral lines were detected in this region, of which 555 lines could be classified as La I transitions and 10 lines as La II transitions. All La II transitions and 534 of these La I transitions were classified for the first time, and 6 of the La II transitions and 433 of the classified La I transitions appear to be new lines, which could not be found in the literature. The corresponding energy level data of classified lines …

observational astronomyAstrophysics and AstronomyInfrared astronomyPhysicsNatural SciencesSpectroscopyInterdisciplinary AstronomyAtomic physics
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Spectra of a Holmium in the near-UV. II.

2017

Fourier Transform spectra of Holmium (Ho) in the UV spectral range from 31530 to 25000cm^-1^ (317 to 400nm) have been investigated, particularly focusing on the ionic lines. The distinction between the different degrees of ionization (I, II, and III) is based on differences in signal-to-noise ratios from two Ho spectra, which have been measured with different buffer gases, i.e., neon and argon. Based on 106 known Ho II and 126 known Ho III energy levels, 97 lines could be classified as transitions of singly ionized Ho and 9 lines could be classified as transitions of doubly ionized Ho. Of the 97 Ho II lines, 6 have not been listed in the extant literature. Another 215 lines have been assign…

observational astronomyUltraviolet astronomyAstrophysics and AstronomyPhysicsNatural SciencesSpectroscopyAtomic physicsInterdisciplinary Astronomy
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Spectra of a Holmium in the near-UV. I. Ho I.

2017

The Fourier Transform spectra of a Holmium hollow cathode discharge lamp have been investigated in the UV spectral range from 25000 up to 31530cm^-1^ (317 to 400nm). Two Ho spectra have been measured with neon and argon as buffer gases. Based on the intensity ratios from these two spectra, a distinction was made between atomic and ionic lines (ionic lines are discussed in an accompanying paper). Using the known Ho I energy levels, 71 lines could be classified as transitions of atomic Ho, 34 of which have not been published previously. Another 32 lines, which could not be classified, are listed in the literature and assigned as atomic Ho. An additional 370 spectral lines have been assigned t…

observational astronomyUltraviolet astronomyAstrophysics and AstronomyPhysicsPhysics::Atomic and Molecular ClustersPhysics::Atomic PhysicsNatural SciencesSpectroscopyAtomic physicsInterdisciplinary Astronomy
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Experimental investigation of the optical Kerr effect at large laser intensity: impact on the propagation of a short and intense laser pulse

2010

Talk given by O. Faucher; International audience

optical Kerr effect[PHYS.PHYS.PHYS-ATOM-PH]Physics [physics]/Physics [physics]/Atomic Physics [physics.atom-ph]laser filamenation[ PHYS.PHYS.PHYS-ATOM-PH ] Physics [physics]/Physics [physics]/Atomic Physics [physics.atom-ph]nonlinear propagation[PHYS.PHYS.PHYS-ATOM-PH] Physics [physics]/Physics [physics]/Atomic Physics [physics.atom-ph]ComputingMilieux_MISCELLANEOUS
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Negative and positive Kerr nonlinearity of air calibrated with transient molecular alignment

2009

Talk given by O. Faucher; International audience; Nonlinear electronic Kerr index of the major air constituents has been measured up to high order terms using transient molecular alignment as a reference. Sign reversal associated to negative nonlinearity is observed above a pulse intensity of 26 TW/cm^.2

optical Kerr effectfilamentation[PHYS.PHYS.PHYS-ATOM-PH]Physics [physics]/Physics [physics]/Atomic Physics [physics.atom-ph][ PHYS.PHYS.PHYS-ATOM-PH ] Physics [physics]/Physics [physics]/Atomic Physics [physics.atom-ph]nonlinear optics(320.2250) Femtosecond phenomena; (350.5400) Plasmas; (190.7110) Ultrafast nonlinear optics; (260.5950) Self-focusing[PHYS.PHYS.PHYS-ATOM-PH] Physics [physics]/Physics [physics]/Atomic Physics [physics.atom-ph]femtosecondmolecular alignment
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Higher-order Kerr terms allow ionization-free filamentation in gases

2010

Talk given by J. Kasparian; International audience; Higher-order nonlinear indices, rather than plasma, provide the main defocusing contribution to filamentation in gases at 800 nm. Developing generalized Miller formulae, we discuss the generality of this as a function of the laser wavelength

optical Kerr effectlaser filamenation[PHYS.PHYS.PHYS-ATOM-PH]Physics [physics]/Physics [physics]/Atomic Physics [physics.atom-ph][ PHYS.PHYS.PHYS-ATOM-PH ] Physics [physics]/Physics [physics]/Atomic Physics [physics.atom-ph]laser filamentationPhysics::Opticsnonlinear propagation42.65.Jx 37.10.Vz 42.65.Tg 78.20.Ci[PHYS.PHYS.PHYS-ATOM-PH] Physics [physics]/Physics [physics]/Atomic Physics [physics.atom-ph]ComputingMilieux_MISCELLANEOUS
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