6533b86dfe1ef96bd12c9621

RESEARCH PRODUCT

High-resolution laser system for the S3-Low Energy Branch

Jekabs RomansAnjali AjayakumarMartial AuthierFrederic BoumardLucia CaceresJean-françois CamArno ClaessensSamuel DamoyPierre DelahayePhilippe DesruesWenling DongAntoine DrouartPatricia DuchesneRafael FerrerXavier FléchardSerge FranchooPatrice GangnantSarina GeldhofRuben P. De GrooteNathalie LecesneRenan LeroyJulien LoryFranck LuttonVladimir ManeaYvan MerrerIain MooreAlejandro Ortiz-cortesBenoit OsmondJulien PiotOlivier PochonSebastian RaederAntoine De RoubinHervé SavajolsSimon SelsDominik StuderEmil TraykovJuha UusitaloChristophe VandammeMarine VandebrouckPaul Van Den BerghPiet Van DuppenKlaus Wendt

subject

Resonance ionization laser spectroscopyNuclear and High Energy PhysicsIsotope shiftAtomic Physics (physics.atom-ph)FOS: Physical sciencesHyperfine structureNuclear Experiment (nucl-ex)[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]Nuclear ground state propertiesNuclear ExperimentInstrumentation[PHYS.PHYS.PHYS-GEN-PH]Physics [physics]/Physics [physics]/General Physics [physics.gen-ph]Physics - Atomic Physics

description

International audience; In this paper we present the first high-resolution laser spectroscopy results obtained at the GISELE laser laboratory of the GANIL-SPIRAL2 facility, in preparation for the first experiments with the S$^3$-Low Energy Branch. Studies of neutron-deficient radioactive isotopes of erbium and tin represent the first physics cases to be studied at S$^3$. The measured isotope-shift and hyperfine structure data are presented for stable isotopes of these elements. The erbium isotopes were studied using the $4f^{12}6s^2$$^3H_6 \rightarrow 4f^{12}(^3 H)6s6p$$J = 5$ atomic transition (415 nm) and the tin isotopes were studied by the $5s^25p^2 (^3P_0) \rightarrow 5s^25p6s (^3P_1)$ atomic transition (286.4 nm), and are used as a benchmark of the laser setup. Additionally, the tin isotopes were studied by the $5s^25p6s (^3P_1) \rightarrow 5s^25p6p (^3P_2)$ atomic transition (811.6 nm), for which new isotope-shift data was obtained and the corresponding field-shift $F_{812}$ and mass-shift $M_{812}$ factors are presented.

10.1016/j.nimb.2022.12.012https://hal.science/hal-03910507