Early onset of deformation in the neutron-deficient polonium isotopes identified by in-source resonant ionization laser spectroscopy

Similar documents
Early onset of deformation in the neutron-deficient polonium isotopes identified by in-source resonant ionization laser spectroscopy

Resonant laser ionization of Po at ISOLDE

LASER SPECTROSCOPIC STUDIES OF NEUTRON-DEFICIENT EUROPIUM AND GADOLINIUM ISOTOPES

In-gas cell laser spectroscopy of neutron-deficient silver isotopes

Opportunities with collinear laser spectroscopy at DESIR:

Laser Spectroscopy on Bunched Radioactive Ion Beams

Results from the collinear laser spectroscopy collaboration at ISOLDE-CERN

Oblate nuclear shapes and shape coexistence in neutron-deficient rare earth isotopes

Study of oblate nuclear shapes and shape coexistence in neutron-deficient rare earth isotopes

Laser spectroscopy and resonant laser ionization atomic tools to probe the nuclear landscape. Iain Moore University of Jyväskylä, Finland

Mapping Fission in Terra Incognita in the neutron-deficient lead region

In-gas jet laser ionization spectroscopy of heavy elements. Piet Van Duppen Department of Physics and Astronomy KU Leuven, Belgium

Radioactivity. (b) Fig shows two samples of the same radioactive substance. The substance emits β-particles. Fig. 12.1

Principle of Resonance Ionization

ISOMER BEAMS. P.M. WALKER Department of Physics, University of Surrey, Guildford GU2 7XH, UK

Recent developments at ISOL-based facilities. Piet Van Duppen KU Leuven, Belgium

In-Gas Laser Ionization and Spectroscopy experiments at S 3 -GANIL

Beta-delayed fission: from neutrondeficient to neutron-rich nuclei

Mass measurements of n-rich nuclei with A~70-150

Laser spectroscopy studies of neutron-rich nuclei

Fission Barriers of Neutron-Deficient Nuclei

Accelerated radioactive beams and the future of nuclear physics. David Jenkins

Nuclear physics: Magdalena Kowalska CERN, PH Dept.

Dipole Response of Exotic Nuclei and Symmetry Energy Experiments at the LAND R 3 B Setup

Shape coexistence in light Krypton isotopes

Coexistence phenomena in neutron-rich A~100 nuclei within beyond-mean-field approach

High-spin studies and nuclear structure in three semi-magic regions of the nuclide chart High-seniority states in Sn isotopes

Introduction to REX-ISOLDE concept and overview of (future) European projects

HEIDI WATKINS. Plunger Measurements of Shape Coexistence in the Neutron Deficient 174 Pt Nuclei

Mapping Low-Energy Fission with RIBs (in the lead region)

Measurement of the g-factors of 2 + states in stable A=112,114,116 Sn isotopes using the transient field technique

Spectroscopic Quadrupole Moment in 96,98 Sr : Shape coexistence at N=60. E.Clément-GANIL IS451 Collaboration

'Nuclear Structure of the Neutron Rich Region around Z=28 towards and beyond N=50' WOG workshop Leuven March 9 11, 2009 Mark Huyse

Probing the evolution of shell structure with in-beam spectroscopy

The Island of of Inversion from a nuclear moments perspective

PHL424: Nuclear Shell Model. Indian Institute of Technology Ropar

Shape Coexistence in Neutron-rich Strontium Isotopes at N=60

c E If photon Mass particle 8-1

FAIR - A Status Report + A Concept for Collinear Spectroscopy at TRIGA Mainz. Wilfried Nörtershäuser GSI Darmstadt & Universität Mainz

Conversion Electron Spectroscopy in Transfermium Nuclei

Perspectives for laser spectroscopy of the heaviest elements

Collinear laser spectroscopy of radioactive isotopes at IGISOL 4 Liam Vormawah

Probing neutron-rich isotopes around doubly closed-shell 132 Sn and doubly mid-shell 170 Dy by combined β-γ and isomer spectroscopy.

Liquid Drop Model From the definition of Binding Energy we can write the mass of a nucleus X Z

Bi β + Po Bismuth-214 is radioactive. It has a half-life of 20 minutes. (a) The nuclide notation for bismuth-214 is Bi.

Novel radioactive ion-beam production techniques Report on new schemes and novel laser-ion-source techniques

Spectroscopy of 252No to Investigate its K-isomer

RFSS: Lecture 8 Nuclear Force, Structure and Models Part 1 Readings: Nuclear Force Nuclear and Radiochemistry:

Alpha decay as a probe of the structure of neutrondeficient. Chong Qi

Ultra-Pure 163 Ho Samples for Neutrino Mass Measurements

Nuclear and Radiation Physics

Radioactivity at the limits of nuclear existence

RFSS: Lecture 6 Gamma Decay

Investigation of Pygmy Dipole Resonance in neutron rich exotic nuclei

Experimental Program on Halo Nuclei with non-accelerated Beams at TRIUMF. stephan ettenauer for the TITAN collaboration

Part II Particle and Nuclear Physics Examples Sheet 4

Lesson 5 The Shell Model

Self-consistent approach to deformation of intruder states in neutron-deficient Pb and Po

Composite Nucleus (Activated Complex)

Present ISOLDE facility Aims of HIE-ISOLDE upgrade First steps towards HIE-ISOLDE

Towards 78 Ni: In-beam γ-ray spectroscopy of the exotic nuclei close to N=50

Role of Hexadecupole Deformation in the Shape Evolution of Neutron-rich Nd Isotopes

"Highlights from radioactive beam experiments using MINIBALL and REX-ISOLDE."

Introduction to Nuclear Science

1. Nuclear Size. A typical atom radius is a few!10 "10 m (Angstroms). The nuclear radius is a few!10 "15 m (Fermi).

Report on Nuclear Spectroscopy at JYFL

The Proper)es of Nuclei. Nucleons

Nuclear structure aspects of Schiff Moments. N.Auerbach Tel Aviv University and MSU

α-decay of the new isotope 187 Po: Probing prolate structures beyond the neutron mid-shell at N = 104

Fission fragment mass distributions via prompt γ -ray spectroscopy

Towards TASCA

The nucleus and its structure

Nuclear Shell model. C. Prediction of spins and Parities: GROUND RULES 1. Even-Even Nuclei. I π = 0 +

Laser spectroscopy of actinides at the IGISOL facility, JYFL. Iain Moore University of Jyväskylä, Finland

Recent Results from ISOLDE and new Opportunities with HIE- ISOLDE

In-trap decay and trap-assisted decay spectroscopy at ISOLTRAP

Magdalena Matejska-Minda HIL, University of Warsaw. NUSPIN 2017, June 2017, GSI

Björn Lehnert. Search for double beta decays of palladium isotopes into excited states

Nuclear Fission Fission discovered by Otto Hahn and Fritz Strassman, Lisa Meitner in 1938

Addendum to the IS534 Proposal

SURROGATE REACTIONS. An overview of papers by Jason Burke from LLNL

arxiv: v1 [nucl-ex] 15 Sep 2012

Silvia M. Lenzi University of Padova and INFN. Silvia Lenzi, 10th Int. Spring Seminar on Nuclear Physics, Vietri sul Mare, May 21-25, 2010

Introduction to Nuclear Science

RFSS: Lecture 2 Nuclear Properties

Shape coexistence and beta decay in proton-rich A~70 nuclei within beyond-mean-field approach

Sunday Monday Thursday. Friday

Shell evolution and pairing in calcium isotopes with two- and three-body forces

Status of the Search for an EDM of 225 Ra

Lecture Series: Atomic Physics Tools in Nuclear Physics IV. High-Precision Penning Trap Mass Spectrometry

PHGN 422: Nuclear Physics Lecture 5: The Liquid Drop Model of the Nucleus

Evolution Of Shell Structure, Shapes & Collective Modes. Dario Vretenar

Nuclear Structure V: Application to Time-Reversal Violation (and Atomic Electric Dipole Moments)

Shell model Monte Carlo level density calculations in the rare-earth region

Fast-Timing with LaBr 3 :Ce Detectors and the Half-life of the I π = 4 Intruder State in 34 P

Introduction to Nuclear Physics

beta-nmr: from nuclear physics to biology

Nucleon Pair Approximation to the nuclear Shell Model

Nuclear spectroscopy with fast exotic beams: News on N = 28 from recent NSCL measurements

Large scale shell model calculations for neutron rich fp-shell nuclei

Transcription:

Early onset of deformation in the neutron-deficient polonium isotopes identified by in-source resonant ionization laser spectroscopy, W. Dexters, M.D. Seliverstov, A.N. Andreyev, S. Antalic, A.E. Barzakh, B. Bastin, J. Büscher, I.G. Darby, D.V. Fedorov, V.N. Fedosseyev, K.T. Flanagan, S. Franchoo, S. Fritzsche, G. Huber, M. Huyse, M. Keupers, U. Köster, Yu. Kudryavtsev, E. Mané, B.A. Marsh, P.L. Molkanov, R.D. Page, A.M. Sjoedin, I. Stefan, J. Van de Walle, P. Van Duppen, M. Venhart, S.G. Zemlyanoy, M. Bender, P.-H. Heenen

Outline I 1 In-Source Spectroscopy at CERN s Isotope Separator On-Line DEvice 2 Shape coexistence in the neutron-deficient 84 Po isotopes 3 & Outlooks

Chart of the nuclides A large world to explore

Shape coexistence around 82Pb isotopes Shape coexistence = proximity of spherical and/or deformed shapes(s) at low energy (E < few MeV) 186 Pb: most dramatic examples where the three lowest lying states are 0 + states of three different shapes within less than 700 kev. More information in D. Jenkins presentation. A.N. Andreyev et al., Nature 405(2000)430

Outline 1 In-Source Spectroscopy at CERN s Isotope Separator On-Line DEvice 2 Shape coexistence in the neutron-deficient 84 Po isotopes 3 & Outlooks

CERN Isotope Separator On-Line DEvice

CERN Isotope Separator On-Line DEvice

CERN Isotope Separator On-Line DEvice

Laser ionisation of polonium essential to all the polonium campaigns at, B.A. Marsh et al., NIMB 266(2008)4403 Challenges of a radioactive element No stable isotope no off-live developments possible; 3 laser ionization schemes were successfully developed; s-electron has the necessary overlap with the nucleus.

Outline 1 In-Source Spectroscopy at CERN s Isotope Separator On-Line DEvice 2 Shape coexistence in the neutron-deficient 84 Po isotopes 3 & Outlooks

In-source laser spectroscopy of Po even-a isotopes from A = 192 up to A = 218; from T 1/2 = 33 ms up to T 1/2 = 3 yr; from 0.3 ion s 1 to over 10 7 ion s 1 ; using α, β, γ and ion (FC) counting.

In-source laser spectroscopy of Po odd-a isotopes A = 191 to A = 211; T 1/2 = 22 ms to T 1/2 = 102 years; 0.01 to over 10 7 ion s 1 ; long-lived ( high-spin 13 +) 2 isomers.

In-source laser spectroscopy of Po odd-a isotopes

191 Po Pushing the limits of the technique 191 Po with only 0.01 ion s 1 very limited production rates due to limited cross section and short half lives; sufficient resolution for clean identification via α decay;

Extracting King at play δν AA = A A AA (m eν + K SMS ) + 0.932 F δ r 2 µδν2 AA = F 2 µδν1 AA + A ref A ref F 1 A ref A K SMS2 F 2 K SMS1 ref F 1, W. Dexters, M.D. Seliverstov Large-scale atomic calculation by S. Fritzsche (GSI) F and K SMS have been calculated; et al., PRL 106(2011)052503 if the y intercept is left free, χ 2 ν 1 can be reached good F 2 F 1 but systematic uncertainty on K SMS.

δ r 2 even-a isotopes δν AA = A A AA (m e ν + K SMS ) + 0.932 F δ r 2, W. Dexters, M.D. Seliverstov et al., PRL 106(2011)052503

δ r 2 all isotopes M.D. Seliverstov, et al., in preparation

δ r 2... compared to the neighbouring nuclei

δ r 2... compared to the neighbouring nuclei

Deformation Consistency check in the β 2 parameter

Outline 1 In-Source Spectroscopy at CERN s Isotope Separator On-Line DEvice 2 Shape coexistence in the neutron-deficient 84 Po isotopes 3 & Outlooks

I from the in-source laser spectroscopy work clean beams of polonium are available (less than 1% contamination in beams of 200 Po); δ r 2 deviate early and strongly from the spherical droplet model; large mixing between the ground and intruder configurations; some uncertainties on the spins challenge the previous nuclear spectroscopic conclusions.

II concerning shape coexistence around Z = 82 low-energy excited 0 + state in even-even nuclei; low-energy excited structure issued from coupling to those states in odd-a nuclei; shape of the ground state;? excitability of the structure and excited levels quadrupole moments Coulomb excitation;? single-particle strength in the different energy levels transfer reactions.

Outlooks Things to look forwards to... Shape coexistence in Po determine the spins of the most neutron-deficient isotopes with a higher resolution technique (CRIS); Coulomb excitation of 196,198,200,202 Po at REX- with MiniBall to determine E 2 matrix elements and quadrupole moments (N. Kesteloot and B. Bastin); HIE- opens new opportunities for transfer reactions on those nuclei.

CRIS Collinear Resonant Ionization Spectroscopy CRIS concepts Collinear Doppler compression of the velocity distribution for resolution. Resonant Ionisation efficient selection of the beam of interest for sensitivity.

CRIS Collinear Resonant Ionization Spectroscopy Achievements CRIS is being developped and tested at CERN. vacuum of 10 9 mbar achieved at the interaction region. non-resonant background suppressed by 1:50 000 on-line. Further suppression can be achieved if ionising ions to a X ++ state.

Collaboration