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of very neutron deficient heavy nuclei

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1 of very neutron deficient heavy nuclei
In-beam studies of very neutron deficient heavy nuclei Rauno Julin Accelerator Laboratory Department of Physics University of Jyväskylä JYFL Finland

2 Nuclear spectrocopy is required to understand behaviour of nuclei far from stability can reveal unexpected behaviour of nuclei far from stability

3 very neutron deficient heavy nuclei
Probing neutron-deficient and heavy nuclei with Recoil - Decay - Tagging (RDT) very neutron deficient heavy nuclei  can be produced via fusion evaporation with stable-ion beams and stable targets  cross-sections down to 1 nb  short-living alpha or proton emitters → tagging methods Nb 57 first observations of excited states Pb Sn

4 Recoil-Decay-Tagging with JUROGAM + RITU + GREAT
Recoil-Decay-Tagging with JUROGAM + RITU + GREAT , p, β, … e−,  prompt events delayed events Beam Ge array JUROGAM Focal plane Detectors GREAT Separator RITU TDR Total Data Readout

5 TRIPLE - SHAPE COEXISTENCE
Oblate Prolate 186Pb104 Spherical A. Anreyev ... R. Wyss et al. Nature 405, 430 ... but can we identify band structures on top of those ? ... can we see any E0’s ?

6 EXTREMELY CLEAN SPECTRA
RDT γ rays from 186Pb 186Pb 106Pd(83Kr,3n) 186Pb YRAST PROLATE BAND NON-YRAST BAND J. Pakarinen et al. PR C75, , 2009

7 186Pb RDT singles conversion-electron spectrum (SAGE) 2+ - 4+ E0
E0 + E0

8 186Pb Above 1MeV 186Pb looks like any deformed nucleus except ……
OCTUPOLE PROLATE GAMMA GS. BAND 186Pb OBLATE E0 E0 Above 1MeV 186Pb looks like any deformed nucleus except …… J. Pakarinen et al. PR C75, , 2009

9 Verification of prolate shape …… 185Pb
Coupling of the i13/2 neutron ”hole” to the prolate core Strongly coupled band

10 Level systematics of even-A Pb nuclei
Prolate Spherical N = 104 186Pb 186Pb Oblate

11 Polonium systematics (Z=84)
Energy-level systematics vs. Ground-state radia Oblate Spherical Prolate Understanding of ground-state properties

12 → Need B(E2), Qt Moments of Inertia J(1)(rig) = 110 Rigid:
Hydrodynamical: J(1) ~ β2 Need B(E2), Qt PROLATE OBLATE J(1)(rig) = 110

13 In-beam lifetime measuremets far-from-stability
Recoil Distance Doppler-Shift (RDDS) lifetime measurements (plunger). Combined with selective Recoil-Decay-Tagging method.

14 Qt │β2│ = 0.28 │β2│ = 0.17

15 Qt/Z for the prolate and oblate bands in midshell Pb,Hg and Pt nuclei
Is collectivity really decreasing with decreasing Z ?

16 Collectivity vs. neutron number: 76Os case
even-A Os 168Os: B(E2:4+→2+)/B(E2:2+→0+) < 1 1e2b2 = 173Wu ? 166Os: B(E2:2+→0+) = 7 Wu

17 2018: Towards lighter neutron-deficient nuclei with MARA
RITU MARA MARA is a vacuum-mode recoil separator mainly for proton drip-line studies around N~Z nuclei. MARA is a complementary separator to RITU gas-filled recoil separator. MARA is ideal for studies of nuclei produced with symmetric and inverse reactions. RITU is better for heavier products produced with asymmetric reactions.

18 THANK YOU

19

20 Coexistence vs. mass Hg isotopes ∆4

21 Verification of prolate shape in 185Pb
Coupling of the i13/2 neutron ”hole” to the prolate core Strongly coupled band


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