0000000001315000

AUTHOR

Magdalena Kowalska

showing 28 related works from this author

Evolution of nuclear structure in neutron-rich odd-Zn isotopes and isomers

2017

Collinear laser spectroscopy was performed on Zn (Z=30) isotopes at ISOLDE, CERN. The study of hyperfine spectra of nuclei across the Zn isotopic chain, N=33–49, allowed the measurement of nuclear spins for the ground and isomeric states in odd-A neutron-rich nuclei up to N=50. Exactly one long-lived (&

Nuclear and High Energy Physicsshell closureShell closureNuclear TheoryLasermagnetic dipole moment[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]7. Clean energy01 natural sciencesQuadrupole momentMagnetic dipole momentNaturvetenskap0103 physical sciencesPhysics::Atomic and Molecular ClustersDalton Nuclear InstituteNuclear Physics - Experimentddc:530NeutronPhysics::Atomic Physics010306 general physicsNuclear ExperimentHyperfine structurePhysicsValence (chemistry)quadrupole momentMagnetic moment010308 nuclear & particles physicsNuclear structurePhysique atomique et nucléairelcsh:QC1-999laserZincResearchInstitutes_Networks_Beacons/dalton_nuclear_instituteZinc ; Magnetic dipole moment ; Quadrupole moment ; Laser ; Shell closureQuadrupoleNuclear magnetic momentPräzisionsexperimente - Abteilung BlaumAtomic physicsNatural SciencesMagnetic dipolelcsh:Physics
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Measurement of the Spin and Magnetic Moment ofMg31: Evidence for a Strongly Deformed Intruder Ground State

2005

Unambiguous values of the spin and magnetic moment of $^{31}\mathrm{M}\mathrm{g}$ are obtained by combining the results of a hyperfine-structure measurement and a $\ensuremath{\beta}$-NMR measurement, both performed with an optically polarized ion beam. With a measured nuclear $g$ factor and spin $I=1/2$, the magnetic moment $\ensuremath{\mu}(^{31}\mathrm{M}\mathrm{g})=\ensuremath{-}0.88355(15){\ensuremath{\mu}}_{N}$ is deduced. A revised level scheme of $^{31}\mathrm{M}\mathrm{g}$ ($Z=12$, $N=19$) with ground state spin/parity ${I}^{\ensuremath{\pi}}=1/{2}^{+}$ is presented, revealing the coexistence of 1p-1h and 2p-2h intruder states below 500 keV. Advanced shell-model calculations and th…

PhysicsMagnetic momentIsland of inversionNuclear structureGeneral Physics and AstronomyParity (physics)Prolate spheroidAtomic physicsGround stateSpectroscopyIntruder statePhysical Review Letters
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2-Acylamino-6-pyridones: breaking of an intramolecular hydrogen bond by self-association and complexation with double and triple hydrogenbonding coun…

2012

2-Acylamino-6-pyridones (acyl = RCO, where R = Me, Et, i-Pr, t-Bu, and 1-adamantyl) were previously characterized by X-ray diffractometry and solid-state NMR techniques by us. One of these compounds was used recently in organocatalysis. The series is now studied in solution and by computational methods recommended for noncovalent interactions (DFT/M05). These compounds showed interesting behavior during dilution and titration experiments monitored by (1)H NMR. 2-Acylamino-6-pyridones change their conformation at higher concentrations, forming double hydrogen-bonded dimers and trimers in which an uncommon steric effect is observed. To the best of our knowledge, this is the first example of s…

Steric effectschemistry.chemical_classificationStereochemistryHydrogen bondOrganic ChemistryIntermolecular forceTautomerCrystallographychemistryIntramolecular forceProton NMRMoleculeNon-covalent interactionsta116Journal of Organic Chemistry
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The influence of CH bond polarization on the self-association of 2-acylaminopyrimidines by NH/CH···O/N interactions: XRD, NMR, DFT, and AIM study

2013

The single crystal structures of two 2-acylaminopyrimidines, where alkyl groups in acyl moiety are iso-propyl (1) and dichloromethyl (2), were solved by X-ray diffraction method. The strength of intermolecular hydrogen bonding interactions depends on the C–H bond polarization increased by exchanging two methyl groups by chlorine atoms in the adjacent substituent. The computational methods provide an additional insight into the intermolecular interactions and are utilized in explaining the differences in the observed crystal structures. The experimental and computational data together explain the differences in the formed aggregates and revealed that these simple substitutions cause crucial …

chemistry.chemical_classification010405 organic chemistryStereochemistryHydrogen bondIntermolecular forceSubstituentCrystal structure010402 general chemistryCondensed Matter Physics01 natural sciences0104 chemical scienceschemistry.chemical_compoundCrystallographychemistryMoietyPhysical and Theoretical ChemistryPolarization (electrochemistry)Single crystalAlkylStructural Chemistry
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Billion-Fold Enhancement in Sensitivity of Nuclear Magnetic Resonance Spectroscopy for Magnesium Ions in Solution

2014

Beta-nuclear magnetic resonance (NMR) spectroscopy is highly sensitive compared to conventional NMR spectroscopy, and may be applied for several elements across the periodic table. Beta-NMR has previously been successfully applied in the fields of nuclear and solid-state physics. In this work, beta-NMR is applied, for the first time, to record an NMR spectrum for a species in solution. 31Mg b-NMR spectra are measured for as few as 10^7 magnesium ions in ionic liquid (EMIM-Ac) within minutes, as a prototypical test case. Resonances are observed at 3882.9 and 3887.2 kHz in an external field of 0.3 T. The key achievement of the current work is to demonstrate that beta-NMR is applicable for the…

RadioisotopesMagnetic Resonance SpectroscopyChemistryCarbon-13 NMR satelliteIonic liquid (EMIM-Ac)Analytical chemistryIonic Liquids31MgNuclear magnetic resonance spectroscopyFluorine-19 NMRNuclear magnetic resonance crystallographyCarbon-13 NMRAtomic and Molecular Physics and OpticsSolutionsnucelar magnetci resonanceSolid-state nuclear magnetic resonanceMagnesiumPräzisionsexperimente - Abteilung BlaumPhysical and Theoretical ChemistryTwo-dimensional nuclear magnetic resonance spectroscopyEarth's field NMR
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Precision Measurement ofLi11Moments: Influence of Halo Neutrons on theLi9Core

2008

The electric quadrupole moment and the magnetic moment of the 11Li halo nucleus have been measured with more than an order of magnitude higher precision than before, |Q| = 33.3(5) mb and mu = +3.6712(3)muN, revealing a 8.8(1.5)% increase of the quadrupole moment relative to that of 9Li. This result is compared to various models that aim at describing the halo properties. In the shell model an increased quadrupole moment points to a significant occupation of the 1d orbits, whereas in a simple halo picture this can be explained by relating the quadrupole moments of the proton distribution to the charge radii. Advanced models so far fail to reproduce simultaneously the trends observed in the r…

PhysicsMagnetic momentProtonIsotopes of lithiumNuclear TheoryNuclear structureGeneral Physics and AstronomyHalo nucleusNuclear physicsQuadrupolePhysics::Accelerator PhysicsNeutronPhysics::Atomic PhysicsHaloAtomic physicsPhysical Review Letters
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Ground-state spins and moments of72,74,76,78Ga nuclei

2011

Laser spectroscopy was performed on the ${}^{72,74,76,78}$Ga isotopes at On-Line Isotope Mass Separator (ISOLDE) facility, CERN. Ground-state nuclear spins and moments were extracted from the measured hyperfine spectra. The results are compared to shell-model calculations, which provide a detailed probe of the nuclear wave function. The spin is established from the shape of the hyperfine structure and the parity inferred from a comparison of shell-model calculations with the measured nuclear moments. The ground states of ${}^{76,78}$Ga are both assigned a spin and parity of ${I}^{\ensuremath{\pi}}={2}^{\ensuremath{-}}$, while ${}^{74}$Ga is tentatively assigned as ${I}^{\ensuremath{\pi}}={3…

PhysicsNuclear and High Energy PhysicsAngular momentumSpinsMagnetic moment010308 nuclear & particles physics01 natural sciences7. Clean energySpectral line0103 physical sciencesAtomic physicsNuclear Experiment010306 general physicsWave functionGround stateSpectroscopyHyperfine structurePhysical Review C
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Association of N-(Pyridin-2-yl),N′-substituted Ureas with 2-Amino-1,8-naphthyridines and Benzoates: NMR and Quantum Chemical Studies of the Substitue…

2013

Association of four N-(pyridin-2-yl),N'-R(1)-ureas (R(1) = ethyl, n-butyl, phenyl, and tert-butyl) with substituted 2-amino-1,8-naphthyridines and benzoates were studied by (1)H NMR spectroscopic titrations and quantum chemical calculations. The benzoates and 2-amino-1,8-naphthyridines were selected as representatives of double and triple hydrogen bonding counterparts, respectively. The classical substituent effect on the association was studied. A prerequisite and a crucial step for the complex formation was the breaking of the intramolecular hydrogen bond in urea derivatives. The QTAIM calculation method was employed to explain the hydrogen bonding within complexes. In the case of benzoat…

Quantum chemicalMagnetic Resonance SpectroscopyMolecular StructureStereochemistryHydrogen bondOrganic ChemistryComplex formationSubstituentHydrogen BondingBenzoatesMedicinal chemistryBenzoateschemistry.chemical_compoundchemistryIntramolecular forceProton NMRQuantum TheoryUreaTitrationNaphthyridinesta116The Journal of Organic Chemistry
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Nuclear ground-state spins and magnetic moments ofMg27,Mg29, andMg31

2008

The ground-state spins and magnetic moments of neutron-rich {sup 27}Mg, {sup 29}Mg, and {sup 31}Mg were measured for the first time with laser and {beta}-NMR spectroscopy at ISOLDE/CERN. The hyperfine structure of {sup 27}Mg--observed in fluorescence--confirms previous assignments of the spin I=1/2 and reveals the magnetic moment {mu}{sub I}({sup 27}Mg)=-0.4107(15){mu}{sub N}. The hyperfine structure and nuclear magnetic resonance of optically polarized {sup 29}Mg--observed in the asymmetry of its {beta} decay after implantation in a cubic crystal--give I=3/2 and {mu}{sub I}({sup 29}Mg)=+0.9780(6){mu}{sub N}. For {sup 31}Mg they yield together I=1/2 and {mu}{sub I}({sup 31}Mg)=-0.88355(15){…

PhysicsNuclear and High Energy PhysicsMagnetic momentIsland of inversionHadronAtomic physicsNucleonGround stateIsotopes of magnesiumHyperfine structureRadioactive decayPhysical Review C
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Charge radius changes of even-even neutron-rich Tellurium isotopes

2005

Laser spectroscopy based on resonant ionization of laser-desorbed atoms has been used to study the neutron-rich tellurium isotopes with the COMPLIS facility at ISOLDE-CERN. The isotope shift and the hyperfine structure of several neutron-rich Te isotopes: $^{120–136}$Te and $^{123m–133m}$Te have been measured. From the hyperfine structure and the isotope shift we can extract the magnetic and quadrupole moments and the change in the mean square charge radius respectively. The mean square charge radii of the even-even isotopes have been deduced and their comparison with the known data for the other elements near Z=50 is presented. The experimental $\delta$ is compared with that obtained from …

spectroscopyIsotope27.60.+j 29.30.-h010308 nuclear & particles physicsChemistryNuclear structure[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]01 natural sciences7. Clean energyCharge radiusIonizationtellurium0103 physical sciencesQuadrupolenuclear structureNuclei with mass number 90 to 149NeutronPhysics::Atomic Physicslaser beam applicationsAtomic physics010306 general physicsSpectroscopyNuclear ExperimentHyperfine structure
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Approaching theN=82shell closure with mass measurements of Ag and Cd isotopes

2010

Mass measurements of neutron-rich Cd and Ag isotopes were performed with the Penning trap mass spectrometer ISOLTRAP. The masses of ${}^{112,114\ensuremath{-}124}$Ag and ${}^{114,120,122\ensuremath{-}124,126,128}$Cd, determined with relative uncertainties between $2\ifmmode\times\else\texttimes\fi{}{10}^{\ensuremath{-}8}$ and $2\ifmmode\times\else\texttimes\fi{}{10}^{\ensuremath{-}7}$, resulted in significant corrections and improvements of the mass surface. In particular, the mass of $^{124}\mathrm{Ag}$ was previously unknown. In addition, other masses that had to be inferred from $Q$ values of nuclear decays and reactions have now been measured directly. The analysis includes various mass…

PhysicsNuclear reactionNuclear and High Energy Physics010308 nuclear & particles physicsQ value21.10.Dr 21.30.Fe 27.60.+jHadron[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]01 natural sciencesISOLTRAPIsotopes of cadmium0103 physical sciencesIsotopes of tinNuclear Physics - ExperimentAtomic physics010306 general physicsNucleonEnergy (signal processing)Physical Review C
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Mg isotopes and the disappearance of magic N=20 Laser and β-NMR studies

2007

Collinear laser spectroscopy and β-NMR spectroscopy with optical pumping were applied at ISOLDE/CERN to measure for the first time the magnetic moments of neutron-rich 27Mg, 29Mg, 31Mg and 33Mg, along with the spins of the two latter. The magnetic moment of 27Mg was derived from its hyperfine structure detected in UV fluorescent light, whereas the nuclear magnetic resonance observed in β-decay asymmetry from a polarised ensemble of nuclei gave the magnetic moment of 29Mg. For 31Mg and 33Mg, the hyperfine structure and nuclear magnetic resonance gave the spin and the magnetic moment. The preliminary results for 27Mg and 29Mg are consistent with a large neutron shell gap at N=20, whereas data…

Optical pumpingMagnetic momentIsotopeSpinsChemistryNuclear magnetic momentNeutronAtomic physicsNuclear ExperimentSpectroscopyHyperfine structure
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Magnetic and quadrupole moments of neutron deficient 58-62Cu isotopes

2011

Abstract This paper reports on the ground state nuclear moments measured in 58–62Cu using collinear laser spectroscopy at the ISOLDE facility. The quadrupole moments for 58–60Cu have been measured for the first time as Q ( Cu 58 ) = − 15 ( 3 ) efm 2 , Q ( Cu 59 ) = − 19.3 ( 19 ) efm 2 , Q ( Cu 60 ) = + 11.6 ( 12 ) efm 2 and with higher precision for 61,62Cu as Q ( Cu 61 ) = − 21.1 ( 10 ) efm 2 , Q ( Cu 62 ) = − 2.2 ( 4 ) efm 2 . The magnetic moments of 58,59Cu are measured with a higher precision as μ ( Cu 58 ) = + 0.570 ( 2 ) μ N and μ ( Cu 59 ) = + 1.8910 ( 9 ) μ N . The experimental nuclear moments are compared to large-scale shell-model calculations with the GXPF1 and GXPF1A effective i…

PhysicsNuclear and High Energy Physicsnuclear-structureIsotopeMagnetic momentNuclear moments010308 nuclear & particles physicsshell-modelNuclear structureN=287. Clean energy01 natural sciencesShell modelCu58Cu59Cu60Cu61Cu620103 physical sciencesQuadrupoleNuclear spinNeutronHyperfine structureAtomic physicsLaser spectroscopy010306 general physicsGround stateSpectroscopyHyperfine structure
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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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Damping effects in Penning trap mass spectrometry

2011

Abstract Collisions of ions with residual gas atoms in a Penning trap can have a strong influence on the trajectories of the ions, depending on the atom species and the gas pressure. We report on investigations of damping effects in time-of-flight ion-cyclotron resonance mass spectrometry with the Penning trap mass spectrometers ISOLTRAP at ISOLDE/CERN (Geneva, Switzerland) and SHIPTRAP at GSI (Darmstadt, Germany). The work focuses on the interconversion of the magnetron and cyclotron motional modes, in particular the modification of the resonance profiles for quadrupolar excitation due to the damping effect of the residual gas. Extensive experiments have been performed with standard and Ra…

ChemistryCyclotronResonanceCondensed Matter PhysicsMass spectrometryPenning trapISOLTRAPFourier transform ion cyclotron resonancelaw.inventionPhysics::Plasma PhysicslawPhysics::Atomic PhysicsIon trapPhysical and Theoretical ChemistryAtomic physicsNuclear ExperimentInstrumentationSpectroscopyIon cyclotron resonanceInternational Journal of Mass Spectrometry
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Trap-assisted decay spectroscopy with ISOLTRAP

2012

Penning traps are excellent high-precision mass spectrometers for radionuclides. The high-resolving power used for cleaning isobaric and even isomeric contaminants can be exploited to improve decay-spectroscopy studies by delivering purified samples. An apparatus allowing trap-assisted decay spectroscopy has been coupled to the ISOLTRAP mass spectrometer at ISOLDE/CERN. The results from studies with stable and radioactive ions show that the setup can be used to perform decay studies on purified short-lived nuclides and to assist mass measurements. (C) 2012 Elsevier B.V. All rights reserved.

PhysicsNuclear and High Energy PhysicsRadionuclideStudies at ISOL-type facilitiesPenning trap mass spectrometers010308 nuclear & particles physics[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]Trap (plumbing)Mass spectrometry01 natural sciencesISOLTRAPIonNuclear physicsTrap-assisted decay spectroscopy0103 physical sciencesIsobaric processNuclideNuclear Experiment010306 general physicsSpectroscopyInstrumentation
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Precision Test of Many-Body QED in theBe+2pFine Structure Doublet Using Short-Lived Isotopes

2015

Absolute transition frequencies of the $2s\text{ }{^{2}S}_{1/2}\ensuremath{\rightarrow}2p\text{ }{^{2}P}_{1/2,3/2}$ transitions in ${\mathrm{Be}}^{+}$ were measured for the isotopes $^{7,9--12}\mathrm{Be}$. The fine structure splitting of the $2p$ state and its isotope dependence are extracted and compared to results of ab initio calculations using explicitly correlated basis functions, including relativistic and quantum electrodynamics effects at the order of $m{\ensuremath{\alpha}}^{6}$ and $m{\ensuremath{\alpha}}^{7} \mathrm{ln} \ensuremath{\alpha}$. Accuracy has been improved in both the theory and experiment by 2 orders of magnitude, and good agreement is observed. This represents on…

PhysicsOrders of magnitude (time)Ab initio quantum chemistry methodsShort lived isotopesStructure (category theory)General Physics and AstronomyOrder (ring theory)Fine structureState (functional analysis)Atomic physicsHyperfine structurePhysical Review Letters
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The MORA project

2018

The MORA (Matter's Origin from the RadioActivity of trapped and oriented ions) project aims at measuring with unprecedented precision the D correlation in the nuclear beta decay of trapped and oriented ions. The D correlation offers the possibility to search for new CP-violating interactions, complementary to searches done at the LHC and with Electric Dipole Moments. Technically, MORA uses an innovative in-trap orientation method which combines the high trapping efficiency of a transparent Paul trap with laser orientation techniques. The trapping, detection, and laser setups are under development, for first tests at the Accelerator laboratory, JYFL, in the coming years.

Physics - Instrumentation and Detectorsexperimental methodsPhysics beyond the Standard Model42.25.Janucl-ex01 natural sciences7. Clean energylaw.invention23.40.-slawPhysics::Atomic PhysicsNuclear Experiment (nucl-ex)Detectors and Experimental TechniquesNuclear Experimentphysics.ins-detPhysicsLarge Hadron Colliderion trapsOrientation (computer vision)Instrumentation and Detectors (physics.ins-det)Condensed Matter PhysicsComputer Science::Computers and SocietyAtomic and Molecular Physics and OpticsIon trapydinfysiikkaNuclear and High Energy PhysicsFOS: Physical sciencesTrapping[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]Computer Science::Digital LibrariesIonFundamental symmetriesNuclear physics0103 physical sciencesCP: violation37.10.TyNuclear Physics - Experiment[PHYS.PHYS.PHYS-INS-DET]Physics [physics]/Physics [physics]/Instrumentation and Detectors [physics.ins-det]Physical and Theoretical Chemistry010306 general physicsactivity reportion: capturenucleus: semileptonic decayCondensed Matter::Quantum Gases010308 nuclear & particles physicsBeta DecayLaserlaserDipoleefficiencycorrelationfundamental symmetries11.30.Erbeta decayIon traps
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First operational experience of HIE-ISOLDE

2016

The High Intensity and Energy ISOLDE project (HIE-ISOLDE)* is a major upgrade of the ISOLDE facility at CERN. The energy range of the post-accelerator will be extended from 2.85 MeV/u to 9.3 MeV/u for beams with A/q = 4.5 (and to 14.3 MeV/u for A/q = 2.5) once all the cryomodules of the superconducting accelerator are in place. The project has been divided into different phases, the first of which (phase 1a) finished in October 2015 after the hardware and beam commissioning were completed**. The physics campaign followed with the delivery of both radioactive and stable beams to two different experimental stations. The characteristics of the beams (energies, intensities, time structure and b…

kokeiludetectorexperimentdetector; dipole; ion; experiment; targetPhysics::Accelerator Physicsion04 Hadron AcceleratorsNuclear ExperimentAccelerators and Storage RingsdipoletargetAccelerator Physics
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Charge radii of neon isotopes across the sd neutron shell

2011

We report on the changes in mean square charge radii of unstable neon nuclei relative to the stable Ne-20, based on the measurement of optical isotope shifts. The studies were carried out using collinear laser spectroscopy on a fast beam of neutral neon atoms. High sensitivity on short-lived isotopes was achieved thanks to nonoptical detection based on optical pumping and state-selective collisional ionization, which was complemented by an accurate determination of the beam kinetic energy. The new results provide information on the structural changes in the sequence of neon isotopes all across the neutron sd shell, ranging from the proton drip line nucleus and halo candidate Ne-17 up to the…

Nuclear and High Energy PhysicsProtonNuclear Theoryquadrupole collectivitychemistry.chemical_elementXXargon isotopesNeonCharge radiusrich nucleiNeutronPhysics::Atomic PhysicsNuclear Experimentcluster statesMagic number (physics)Physicslaser-spectroscopy measurementssodium isotopesIsland of inversionintruder configurationsmean-field theorychemistryIsotopes of neonlight-nucleiAtomic physicsmass shiftNucleon
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Nuclear Charge Radii ofMg21−32

2012

Charge radii of all magnesium isotopes in the sd shell have been measured, revealing evolution of the nuclear shape throughout two prominent regions of assumed deformation centered on (24)Mg and (32)Mg. A striking correspondence is found between the nuclear charge radius and the neutron shell structure. The importance of cluster configurations towards N=8 and collectivity near N=20 is discussed in the framework of the fermionic molecular dynamics model. These essential results have been made possible by the first application of laser-induced nuclear orientation for isotope shift measurements.

PhysicsIsotopeIsland of inversionNuclear TheoryGeneral Physics and AstronomyCharge densityCharge (physics)NeutronRadiusAtomic physicsNuclear ExperimentIsotopes of magnesiumEffective nuclear chargePhysical Review Letters
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Nuclear spins, magnetic moments, and quadrupole moments of Cu isotopes fromN=28toN=46: Probes for core polarization effects

2010

Measurements of the ground-state nuclear spins and magnetic and quadrupole moments of the copper isotopes from $^{61}\mathrm{Cu}$ up to $^{75}\mathrm{Cu}$ are reported. The experiments were performed at the CERN online isotope mass separator (ISOLDE) facility, using the technique of collinear laser spectroscopy. The trend in the magnetic moments between the $N=28$ and $N=50$ shell closures is reasonably reproduced by large-scale shell-model calculations starting from a $^{56}\mathrm{Ni}$ core. The quadrupole moments reveal a strong polarization of the underlying Ni core when the neutron shell is opened, which is, however, strongly reduced at $N=40$ due to the parity change between the $\mat…

PhysicsNuclear and High Energy PhysicsSpinsMagnetic moment010308 nuclear & particles physicsIsotopes of copperNuclear TheoryHadron01 natural sciences7. Clean energyBaryon0103 physical sciencesQuadrupoleNeutronAtomic physics010306 general physicsNucleonPhysical Review C
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Spin and magnetic moment of23Mg

2017

A negative magnetic moment of 23Mg has been determined by collinear laser spectroscopy at CERN-ISOLDE. The absolute value is in agreement with previous measurements by nuclear magnetic resonance while the sign points at high-seniority configurations. The result is consistent with shell-model predictions for nuclei with valence nucleons in the sd shell. ispartof: Journal of Physics G, Nuclear and Particle Physics vol:44 issue:7 status: published

PhysicsNuclear and High Energy PhysicsAngular momentumValence (chemistry)[PHYS.NUCL]Physics [physics]/Nuclear Theory [nucl-th]Magnetic moment010308 nuclear & particles physicsNuclear TheoryHadronElementary particleFermion01 natural sciencesNuclear magnetic resonance0103 physical sciencesPhysics::Atomic and Molecular ClustersPräzisionsexperimente - Abteilung BlaumAtomic physicsNuclear Experiment010306 general physicsNucleonSpectroscopyJournal of Physics G: Nuclear and Particle Physics
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Tuning the hydrogen bonding strength in 2,6-bis(cycloalkylcarbonylamino)pyridine assemblies by variable flexibility. Association constants measured b…

2011

International audience; The association of 2,6-bis(cycloalkylcarbonyloamino)pyridines with rigid and non-rigid counterparts was studied in chloroform solution by 1H NMR and computational methods. The angles within the cycloalkyl ring and rotation of these substituents determine the strength of the association via triple hydrogen-bonding. The dimerization and methyl-methyl repulsion have been addressed as mechanisms restricting heterocomplexation of diacetamide. The association constants obtained by the shift changes of hydrogen-bonded protons are in agreement with those of methine protons. This "dual shift" method was proposed as an additional verification of association constants obtained …

Steric effectsFlexibility (anatomy)ChloroformHydrogen010405 organic chemistryStereochemistryHydrogen bondchemistry.chemical_elementGeneral Chemistry010402 general chemistryRing (chemistry)01 natural sciences0104 chemical scienceschemistry.chemical_compoundCrystallographymedicine.anatomical_structurechemistryPyridinePhysical SciencesmedicineProton NMR[CHIM.OTHE]Chemical Sciences/Other
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g factors of $^{31,32,33}$Al: Indication for intruder configurations in the $^{33}$Al ground state

2006

Abstract The g factors of 31,32,33 Al have been measured using the β -nuclear magnetic resonance ( β -NMR) technique on spin-polarized beams produced in the fragmentation of a 36 S (77.5 MeV/u) beam on a 9 Be target. Nearly pure beams of Al ( Z = 13 ) isotopes were selected with the high-resolution fragment separator LISE at GANIL. An asymmetry as high as 6% has been observed in the β -NMR curve for 32 Al implanted in a Si single crystal. The magnetic moment of the N = 20 nucleus 33 Al is obtained for the first time: μ ( Al 33 , I π = 5 / 2 + ) = 4.088 ( 5 ) μ N , while those of 31,32 Al are obtained with improved accuracy: μ ( Al 31 , I π = 5 / 2 + ) = 3.830 ( 5 ) μ N and μ ( Al 32 , I π =…

Nuclear reactionPhysicsNuclear and High Energy PhysicsMagnetic momentNUCLEISTABILITY010308 nuclear & particles physicsLandé g-factorMG-32[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]01 natural sciencesN=20 SHELL CLOSUREMODELMAGNETIC DIPOLEPhysics and AstronomyELECTRIC QUADRUPOLE-MOMENTS0103 physical sciencesSPECTROMETERAtomic physics010306 general physicsGround stateWave functionMagnetic dipoleSingle crystalDimensionless quantity
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CCDC 1422861: Experimental Crystal Structure Determination

2015

Related Article: Borys Ośmiałowski, Karina Mroczyńska, Erkki Kolehmainen, Magdalena Kowalska, Arto Valkonen, Marek Pietrzak, and Kari Rissanen|2013|J.Org.Chem.|78|7582|doi:10.1021/jo4011393

Space GroupCrystallography1-phenyl-3-pyridin-2-ylureaCrystal SystemCrystal StructureCell ParametersExperimental 3D Coordinates
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CCDC 1422862: Experimental Crystal Structure Determination

2015

Related Article: Borys Ośmiałowski, Karina Mroczyńska, Erkki Kolehmainen, Magdalena Kowalska, Arto Valkonen, Marek Pietrzak, and Kari Rissanen|2013|J.Org.Chem.|78|7582|doi:10.1021/jo4011393

Space GroupCrystallographyCrystal SystemCrystal Structure1-ethyl-3-pyridin-2-ylureaCell ParametersExperimental 3D Coordinates
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CCDC 1422860: Experimental Crystal Structure Determination

2015

Related Article: Borys Ośmiałowski, Karina Mroczyńska, Erkki Kolehmainen, Magdalena Kowalska, Arto Valkonen, Marek Pietrzak, and Kari Rissanen|2013|J.Org.Chem.|78|7582|doi:10.1021/jo4011393

Space GroupCrystallographyCrystal SystemCrystal StructureCell Parameters1-butyl-3-pyridin-2-ylureaExperimental 3D Coordinates
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