0000000000900001

AUTHOR

C. Henrich

showing 18 related works from this author

High-Statistics Sub-Barrier Coulomb Excitation of $^{106,108,110}$Sn

2020

International audience; A Coulomb excitation campaign on $^{106,108,110}$Sn at 4.4–4.5 MeV/u was launched at the HIE-ISOLDE facility at CERN. Larger excitation cross sections and γ-ray statistics were achieved compared to previous experiments at ∼2.8 MeV/u. More precise $(B(E2;0_{1}^{ + } \to 2_{1}^{ + }))$ values, lifetimes of states via the Doppler shift attenuation method, and new $(B(E2;0_{1}^{ + } \to 2_{x}^{ + })), (B(E2;2_{1}^{ + } \to 4_{1}^{ + }))$ and $(Q(2_{1}^{ + }))$ values from the new Miniball data will be obtained and applied to test modern nuclear structure theories.

Physics010308 nuclear & particles physicsCoulomb excitation0103 physical sciencesshell modelNuclear Physics - ExperimentCoulomb excitationAtomic physics[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]010306 general physics01 natural sciencesnuclear collectivity
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Lifetime measurements in Ti52,54 to study shell evolution toward N=32

2019

Lifetimes of the excited states in the neutron-rich Ti-52,Ti-54 nuclei, produced in a multinucleon-transfer reaction, were measured by employing the Cologne plunger device and the recoil-distance D ...

PlungerPhysics010308 nuclear & particles physicsExcited stateNuclear Theory0103 physical sciencesShell (structure)Atomic physicsNuclear Experiment010306 general physics7. Clean energy01 natural sciencesPhysical Review C
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Coulomb Excitation of (142) Xe

2017

5 pags., 2 figs. -- Open Access funded by Creative Commons Atribution Licence 4.0. -- Presented at the XXXV Mazurian Lakes Conference on Physics, Piaski, Poland, September 3–9, 2017.

PhysicsLarge Hadron ColliderSpectrometerta114010308 nuclear & particles physicsDetectorNuclear TheoryGeneral Physics and AstronomyksenonCoulomb excitation[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]01 natural sciencesxenonNuclear physicsnuclear physics0103 physical sciencesQuadrupolePhysics::Accelerator PhysicsNuclear Physics - ExperimentMAGIC (telescope)ydinfysiikkaNuclear ExperimentBeam (structure)
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Lifetime measurements of excited states in $^{163}$W and the implications for the anomalous B(E2) ratios in transitional nuclei

2019

Grahn, Tuomas/0000-0002-6255-2279; Herzan, Andrej/0000-0002-6736-7638; Cullen, Dave/0000-0002-0041-1606; Barber, Liam/0000-0002-7409-9352; Keatings, James Michael/0000-0003-4271-8021; SAYGI, BAHADIR/0000-0001-5406-506X; Greenlees, Paul/0000-0002-5986-5274; Spagnoletti, Pietro/0000-0002-7674-989X; Parr, Edward/0000-0001-6204-4461; Bondili, S Nara Singh/0000-0002-4096-2429

Nuclear and High Energy PhysicsspektroskopiaNuclear TheoryMean lifetimes[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]7. Clean energy01 natural sciencessymbols.namesake0103 physical sciencesCollective modelmedicineNeutronGamma spectroscopy010306 general physicsNuclear ExperimentPhysicsmean lifetimes010308 nuclear & particles physicsRecoil-distance Doppler-shift methodlcsh:QC1-999Nuclear deformationGamma-ray SpectroscopyCore (optical fiber)Rotational modelmedicine.anatomical_structureB(E2) reduced transition probabilitiesgamma-ray spectroscopyExcited statesymbolsAtomic physicsydinfysiikkaNucleusDoppler effectlcsh:Physics
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Enhanced Quadrupole and Octupole Strength in Doubly Magic Sn132

2018

The first 2+ and 3- states of the doubly magic nucleus Sn132 are populated via safe Coulomb excitation employing the recently commissioned HIE-ISOLDE accelerator at CERN in conjunction with the highly efficient MINIBALL array. The Sn132 ions are accelerated to an energy of 5.49 MeV/nucleon and impinged on a Pb206 target. Deexciting γ rays from the low-lying excited states of the target and the projectile are recorded in coincidence with scattered particles. The reduced transition strengths are determined for the transitions 0g.s.+→21+, 0g.s.+→31-, and 21+→31- in Sn132. The results on these states provide crucial information on cross-shell configurations which are determined within large-sca…

PhysicsLarge Hadron Collider010308 nuclear & particles physicsProjectileMonte Carlo methodGeneral Physics and AstronomyCoulomb excitation01 natural sciencesIonExcited state0103 physical sciencesQuadrupoleAtomic physicsNuclear Experiment010306 general physicsNucleonPhysical Review Letters
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Evolution of Octupole Deformation in Radium Nuclei from Coulomb Excitation of Radioactive Ra222 and Ra228 Beams

2020

There is sparse direct experimental evidence that atomic nuclei can exhibit stable "pear" shapes arising from strong octupole correlations. In order to investigate the nature of octupole collectivity in radium isotopes, electric octupole (E3) matrix elements have been determined for transitions in ^{222,228}Ra nuclei using the method of sub-barrier, multistep Coulomb excitation. Beams of the radioactive radium isotopes were provided by the HIE-ISOLDE facility at CERN. The observed pattern of E3 matrix elements for different nuclear transitions is explained by describing ^{222}Ra as pear shaped with stable octupole deformation, while ^{228}Ra behaves like an octupole vibrator.

PhysicsIsotopeNuclear TheoryGeneral Physics and Astronomychemistry.chemical_elementCoulomb excitation01 natural sciencesRadiumMatrix (mathematics)chemistryExcited state0103 physical sciencesAtomic nucleusCoulombPhysics::Accelerator PhysicsPhysics::Atomic PhysicsAtomic physicsDeformation (engineering)Nuclear Experiment010306 general physicsPhysical Review Letters
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β decay of In133 : γ emission from neutron-unbound states in Sn133

2019

Excited states in Sn-133 were investigated through the beta decay of In-133 at the ISOLDE facility. The ISOLDE Resonance Ionization Laser Ion Source (RILIS) provided isomer-selective ionization for In-133, allowing us to study separately, and in detail, the beta-decay branch of In-133 J(pi)= (9/2(+)) ground state and its J(pi) = (1/2(-)) isomer.Thanks to the large spin difference of the two beta-decaying states of In-133, it is possible to investigate separately the lower and higher spin states in the daughter, Sn-133, and thus to probe independently different single-particle and single-hole levels. We report here new gamma transitions observed in the decay of In-133, including those assign…

PhysicsSpin states010308 nuclear & particles physicsGamma ray01 natural sciences7. Clean energyBeta decayIon source3. Good healthIonizationExcited state0103 physical sciencesNeutronAtomic physics010306 general physicsGround statePhysical Review C
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The observation of vibrating pear-shapes in radon nuclei

2019

6 pags., 4 fig.s, 1 tab. -- Open Access funded by Creative Commons Atribution Licence 4.0

Physics beyond the Standard ModelScienceNuclear TheoryGeneral Physics and Astronomychemistry.chemical_elementRadon[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]01 natural sciencesArticleGeneral Biochemistry Genetics and Molecular BiologyRadiumQuantum state0103 physical sciencesCP: violationground stateNuclear Physics - ExperimentPhysics::Atomic PhysicsExperimental nuclear physicslcsh:Science010306 general physicsnumerical calculationsNuclear ExperimentPhysicsMultidisciplinaryIsotope010308 nuclear & particles physicsnew physicsnucleusQradonGeneral ChemistryPublisher Correctionradiumexotic nucleielectric momentchemistryradioactivityMoment (physics)Atomic nucleusCP violationlcsh:QExotic atoms and moleculesAtomic physicsydinfysiikka
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Coulomb excitation of pear-shaped nuclei

2019

There is a large body of evidence that atomic nuclei can undergo octupole distortion and assume the shape of a pear. This phenomenon is important for measurements of electric-dipole moments of atoms, which would indicate CP violation and hence probe physics beyond the Standard Model of particle physics. Isotopes of both radon and radium have been identified as candidates for such measurements. Here, we have observed the low-lying quantum states in 224Rn and 226Rn by accelerating beams of these radioactive nuclei. We show that radon isotopes undergo octupole vibrations but do not possess static pear-shapes in their ground states. We conclude that radon atoms provide less favourable condition…

PhysicsIsotope010308 nuclear & particles physicsPhysicsQC1-999Physics beyond the Standard Modelchemistry.chemical_elementRadonCoulomb excitation[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]01 natural scienceschemistryQuantum state0103 physical sciencesMoment (physics)Atomic nucleusCP violationNuclear Physics - ExperimentPhysics::Atomic PhysicsAtomic physics010306 general physicsydinfysiikka
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Enhanced Quadrupole and Octupole Strength in Doubly Magic ^{132}Sn.

2018

International audience; The first $2^+$ and $3^-$ states of the doubly magic nucleus $^{132}$Sn are populated via safe Coulomb excitation employing the recently commissioned HIE-ISOLDE accelerator at CERN in conjunction with the highly efficient MINIBALL array. The $^{132}$Sn ions are accelerated to an energy of 5.49  MeV/nucleon and impinged on a $^{206}$Pb target. Deexciting $\gamma$ rays from the low-lying excited states of the target and the projectile are recorded in coincidence with scattered particles. The reduced transition strengths are determined for the transitions $0_{g.s.}^+ \rightarrow 2_1^+$, $0_{g.s.}^+ \rightarrow 3_1^-$, and $2_1^+ \rightarrow 3_1^-$ in $^{132}$Sn. The res…

nuclear physics[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]ydinfysiikkaNuclear PhysicsPhysical review letters
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Lifetime measurements of excited states in ¹⁶³W and the implications for the anomalous B(E2) ratios in transitional nuclei

2019

This letter reports lifetime measurements of excited states in the odd-N nucleus $^{163}$W using the recoil-distance Doppler shift method to probe the core polarising effect of the i13/2 neutron orbital on the underlying soft triaxial even-even core. The ratio B(E2:21/2+→17/2+)/B(E2:17/2+→13/2+) is consistent with the predictions of the collective rotational model. The deduced B(E2) values provide insights into the validity of collective model predictions for heavy transitional nuclei and a geometric origin for the anomalous B(E2) ratios observed in nearby even-even nuclei is proposed.

Nuclear Experiment
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Coulomb excitation of Rn-222

2022

The nature of quadrupole and octupole collectivity in 222Rn was investigated by determining the electric-quadrupole (E2) and octupole (E3) matrix elements using subbarrier, multistep Coulomb excitation. The radioactive 222Rn beam, accelerated to 4.23 MeV/u, was provided by the HIE-ISOLDE facility at CERN. Data were collected in the Miniball γ-ray spectrometer following the bombardment of two targets, 120Sn and 60Ni. Transition E2 matrix elements within the ground-state and octupole bands were measured up to 10ℏ and the results were consistent with a constant intrinsic electric-quadrupole moment, 518(11)efm2. The values of the intrinsic electric-octupole moment for the 0+→3− and 2+→5− transi…

Science & TechnologyPhysics NuclearSTATESPhysicsSHAPESPhysical SciencesISOTOPESRADON
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First ß-decay spectroscopy of 135In and new ß-decay branches of 134In

2021

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First β-decay spectroscopy of $^{135}$In and new $β$-decay branches of $^{134}$In

2021

International audience; The $\beta$ decay of the neutron-rich $^{134}$In and $^{135}$In was investigated experimentally in order to provide new insights into the nuclear structure of the tin isotopes with magic proton number $Z=50$ above the $N=82$ shell. The $\beta$-delayed $\gamma$-ray spectroscopy measurement was performed at the ISOLDE facility at CERN, where indium isotopes were selectively laser-ionized and on-line mass separated. Three $\beta$-decay branches of $^{134}$In were established, two of which were observed for the first time. Population of neutron-unbound states decaying via $\gamma$ rays was identified in the two daughter nuclei of $^{134}$In, $^{134}$Sn and $^{133}$Sn, at…

isotoopitmittausAstrophysics::High Energy Astrophysical PhenomenaspektroskopiaNuclear TheoryNuclear Physics - Experimentneutronit[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]fysiikkaydinfysiikkaNuclear ExperimentNuclear Experiment
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First β -decay spectroscopy of In 135 and new β -decay branches of In 134

Physical Review C
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Detailed spectroscopy of doubly magic $^{132}$Sn

2020

The structure of the doubly magic $^{132}_{50}$Sn$_{82}$ has been investigated at the ISOLDE facility at CERN, populated both by the $\beta^-$decay of $^{132}$In and $\beta^-$-delayed neutron emission of $^{133}$In. The level scheme of $^{132}$Sn is greatly expanded with the addition of 68 $\gamma$-transitions and 17 levels observed for the first time in the $\beta$ decay. The information on the excited structure is completed by new $\gamma$-transitions and states populated in the $\beta$-n decay of $^{133}$In. Improved delayed neutron emission probabilities are obtained both for $^{132}$In and $^{133}$In. Level lifetimes are measured via the Advanced Time-Delayed $\beta\gamma\gamma$(t) fas…

Astrophysics::High Energy Astrophysical PhenomenaFOS: Physical sciencesNuclear Physics - Experiment[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]Nuclear Experiment (nucl-ex)nucl-exNuclear StructureNuclear Experiment
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First -decay spectroscopy of and new -decay branches of

2021

19 pags., 14 figs., 3 tabs.

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Coulomb excitation of 222Rn

2022

International audience; The nature of quadrupole and octupole collectivity in $^{222}$Rn was investigated by determining the electric-quadrupole (E2) and octupole (E3) matrix elements using subbarrier, multistep Coulomb excitation. The radioactive $^{222}$Rn beam, accelerated to 4.23 MeV/u, was provided by the HIE-ISOLDE facility at CERN. Data were collected in the Miniball $\gamma$ -ray spectrometer following the bombardment of two targets, $^{120}$Sn and $^{60}$Ni. Transition E2 matrix elements within the ground-state and octupole bands were measured up to 10 ¯h and the results were consistent with a constant intrinsic electric-quadrupole moment, 518(11) $e$ fm$^2$ . The values of the int…

A ≥ 220electromagnetic transitionsnuclear structure & decaysNuclear Physics - Experimentradon[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]ydinfysiikka114 Physical sciences
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