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

Transcription

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

2 Outline I 1 coexistence in the polonium isotopes 2 laser scopy at CERN s Isotope Separator On-Line DEvice coexistence in the neutron-deficient 84 Po isotopes 3

3 Outline 1 coexistence in the polonium isotopes 2 laser scopy at 3

4 Chart of the nuclides A large world to explore

5 coexistence in Pb isotopes 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. A.N. Andreyev et al., Nature 405(2000)430

6 coexistence in Hg isotopes Evidence for shape coexistence in systematic energy levels: flat behaviour of the spherical states against parabolic intrusion of the deformed states with a minimum at mid-shell N = 104.

7 coexistence in Po isotopes From shape coexistence to configuration mixing From N = 126 down, vibrational behaviour with parabolic intrusion of 0 + shape coexistence; From N = 116 down, first 2 +, 4 +,..., go down with intruding configuration configuration mixing?

8 coexistence What are the observables 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 charge distribution δ r 2 ;? excitability of the structure and excited levels quadrupole moments Coulomb excitation;? single-particle strength in the different energy levels transfer reactions.

9 coexistence What are the observables 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 charge distribution δ r 2 ;? excitability of the structure and excited levels quadrupole moments Coulomb excitation;? single-particle strength in the different energy levels transfer reactions.

10 coexistence What are the observables 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 charge distribution δ r 2 ;? excitability of the structure and excited levels quadrupole moments Coulomb excitation;? single-particle strength in the different energy levels transfer reactions.

11 coexistence What are the observables 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 charge distribution δ r 2 ;? excitability of the structure and excited levels quadrupole moments Coulomb excitation;? single-particle strength in the different energy levels transfer reactions.

12 coexistence What are the observables 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 charge distribution δ r 2 ;? excitability of the structure and excited levels quadrupole moments Coulomb excitation;? single-particle strength in the different energy levels transfer reactions.

13 coexistence What are the observables 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 charge distribution δ r 2 ;? excitability of the structure and excited levels quadrupole moments Coulomb excitation;? single-particle strength in the different energy levels transfer reactions.

14 Outline 1 coexistence in the polonium isotopes 2 laser scopy at CERN s Isotope Separator On-Line DEvice coexistence in the neutron-deficient 84 Po isotopes 3

15 CERN Isotope Separator On-Line DEvice

16 CERN Isotope Separator On-Line DEvice

17 CERN Isotope Separator On-Line DEvice

18 Laser ionisation of polonium Light in the dark, 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.

19 laser scopy 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.

20 laser scopy 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.

21 laser scopy 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.

22 laser scopy 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.

23 laser scopy of Po odd-a isotopes

24 α decay of 195 Po... serendipity at play Rich α decay the α decay of the odd-a polonium isotopes has a rich structure, revealing the importance of shape coexistence; a large amount of data on the poorly-known isotope 195 Po was recorded during the study on.

25 α decay of 195 Po... serendipity at play identification of α-γ coincidences; conversion coefficients extracted from branching ratios; E0 components and decay hindrance factors permit spin assignment in many cases.

26 α decay of 195 Po... serendipity at play et al., JPG 37(2010)125103

27 β decay of 199 Po... putting a finger on trouble...

28 β decay of 199 Po... putting a finger on trouble...

29 β decay of 199 Po... and trying to fix it, Ph.D. Thesis (app. B2), KULeuven (2010)

30 β decay of 199 Po... and trying to fix it A linear combination of spectra can yield a purified spectrum. No γ-γ coincidence are available to build up a level scheme.

31 191 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;

32 laser scopy of Po odd-a isotopes

33 laser scopy of Po odd-a isotopes

34 laser scopy of Po odd-a isotopes

35 Extracting King at play again δν AA = A A AA (m eν + K SMS ) 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) 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.

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

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

38 δ r 2... compared to the neighbouring nuclei

39 δ r 2... compared to the neighbouring nuclei

40 Electromagnetic moments... magnetic dipole moments

41 Electromagnetic moments... electric quadrupole moments

42 Deformation Consistency check in the β 2 parameter

43 Outline 1 coexistence in the polonium isotopes 2 laser scopy at 3

44 I from the in-source laser scopy 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 scopic conclusions.

45 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.

46 Things to look forwards to... 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.

47 Coulomb excitation of 200 Po at MiniBall courtesy of B. Bastin

48 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.

49 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: on-line. Further suppression can be achieved if ionising ions to a X ++ state.

50 Collaboration