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Evolution of nuclear Evolution of nuclear shape in the light Radon shape in the light Radon isotopes isotopes University of York University of Jyväskylä Instituut voor Kern- en Stralingsfysica, KU Leuven CERN Institut fuer kernphyysik, Universitaet zu Koeln University of Liverpool University of Manchester University of Edinburgh Technische Universität München Ludwig-Maximilians-Universita Muenchen Technische Universität Darmstadt University of Sofia Weizmann Institute of Science The Miniball Collaboration

Evolution of nuclear shape in the light Radon isotopes

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Evolution of nuclear shape in the light Radon isotopes. University of York University of Jyväskylä Instituut voor Kern- en Stralingsfysica, KU Leuven CERN Institut fuer kernphyysik, Universitaet zu Koeln University of Liverpool University of Manchester University of Edinburgh - PowerPoint PPT Presentation

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Page 1: Evolution of nuclear shape in the light Radon isotopes

Evolution of nuclear shape in the Evolution of nuclear shape in the light Radon isotopeslight Radon isotopes

University of York

University of Jyväskylä

Instituut voor Kern- en Stralingsfysica, KU Leuven

CERN

Institut fuer kernphyysik, Universitaet zu Koeln

University of Liverpool

University of Manchester

University of Edinburgh

Technische Universität München

Ludwig-Maximilians-Universita Muenchen

Technische Universität Darmstadt

University of Sofia

Weizmann Institute of Science

The Miniball Collaboration

Page 2: Evolution of nuclear shape in the light Radon isotopes

Andrew Robinson - INTC: 11th February 2008Andrew Robinson - INTC: 11th February 2008

Shape CoexistenceShape Coexistence

Atomic nucleus minimises its energy by adopting different deformed mean-field shapes.

Page 3: Evolution of nuclear shape in the light Radon isotopes

Light Pb isotopesLight Pb isotopes

Andrew Robinson - INTC: 11th February 2008Andrew Robinson - INTC: 11th February 2008

Page 4: Evolution of nuclear shape in the light Radon isotopes

Mercury IsotopesMercury Isotopes

Andrew Robinson - INTC: 11th February 2008Andrew Robinson - INTC: 11th February 2008

Page 5: Evolution of nuclear shape in the light Radon isotopes

Coulomb Excitation (Coulex)Coulomb Excitation (Coulex)

Coulex with radioactive beams is a highly successful method for establishing the evolution of nuclear shape

74,7674,76KrKr at SPIRALSPIRAL

E. Clement et al., PRC 75, 054313 (2007)

7070SeSe at REX-ISOLDEREX-ISOLDE

A.M. Hurst et al., PRL 98, 072501 (2007)

Andrew Robinson - INTC: 11th February 2008Andrew Robinson - INTC: 11th February 2008

d

d >1.25(Ap1/ 3 + AT

1/ 3) + 5 [fm]€

B(E2, 01+ → 21

+)∝ I2+ M(E2) I

0+

2

dσ CEdΩ

∝ B(E2, 01+ → 21

+)

β2 ∝ B(E2, 01+ → 21

+)

Page 6: Evolution of nuclear shape in the light Radon isotopes

Coulex of Hg Isotopes - IS452Coulex of Hg Isotopes - IS452

non Doppler corrected γ spectrumDoppler corrected γ spectrum

0+

2+

4+

0

367

1089

375

534653

0+

2+4+

N. Bree & A. Petts et al., IS452

Andrew Robinson - INTC: 11th February 2008Andrew Robinson - INTC: 11th February 2008

Page 7: Evolution of nuclear shape in the light Radon isotopes

Coulex of Hg Isotopes - IS452Coulex of Hg Isotopes - IS452

Doppler corrected γ spectrum

0+

2+

4+

0

405

1080

523621

808

0+2+

4+

403

N. Bree & A. Petts et al., IS452

Andrew Robinson - INTC: 11th February 2008Andrew Robinson - INTC: 11th February 2008

Page 8: Evolution of nuclear shape in the light Radon isotopes

Coulex of Hg Isotopes - IS452Coulex of Hg Isotopes - IS452

Doppler corrected γ spectrum

0+

2+

4+

0+2+

4+

0

413

1005

824881

1208

N. Bree & A. Petts et al., IS452

Andrew Robinson - INTC: 11th February 2008Andrew Robinson - INTC: 11th February 2008

Page 9: Evolution of nuclear shape in the light Radon isotopes

Light Polonium IsotopesLight Polonium Isotopes

Andrew Robinson - INTC: 11th February 2008Andrew Robinson - INTC: 11th February 2008

Page 10: Evolution of nuclear shape in the light Radon isotopes

Radon IsotopesRadon Isotopes

PoloniumPolonium

RadonRadonMacroscopic-microscopic models predict that deformed ground statesdeformed ground states exist beyond 202Rn.

E(4E(4++)/E(2)/E(2++)) ratio for 198,200,202198,200,202RnRn typical of ananharmonic vibrationalanharmonic vibrational system.S.J. Freeman et al., PRC 50 R1754 (1994)

R.B.E. Taylor et al., PRC 54, 2926 (1996); PRC 59, 673 (1999)

Evidence found for deformed intruder states in 202,204202,204RnRn which coexist with spherical ground state.D.J. Dobson et al., PRC 66 064321 (2002)

Andrew Robinson - INTC: 11th February 2008Andrew Robinson - INTC: 11th February 2008

Page 11: Evolution of nuclear shape in the light Radon isotopes

Low Lying Levels in Rn IsotopesLow Lying Levels in Rn Isotopes

Andrew Robinson - INTC: 11th February 2008Andrew Robinson - INTC: 11th February 2008

Study Coulex of 202Rn and 204Rn

•Obtain B(E2) values.

•Search for excited 0+ and other non-yrast states.

•Infer the sign of nuclear deformation (with RDM measurement).

Page 12: Evolution of nuclear shape in the light Radon isotopes

Experimental TechniqueExperimental Technique

Light Radon isotopes acceleratedfrom REX-ISOLDEREX-ISOLDE.

202,204202,204RnRn produced with goodyields from ThTh primary targets.

PS Booster and ThC target:202202Rn - 9 x 10Rn - 9 x 1055 ions/ ions/CC204204Rn - 2 x 10Rn - 2 x 1077 ions/ ions/CC

Plasma cooled transfer line provides Isobarically pure beamIsobarically pure beam.

208Pb has recently been accelerated as a preparatory step for light Hg nuclei at REX-ISOLDE.

Andrew Robinson - INTC: 11th February 2008Andrew Robinson - INTC: 11th February 2008

Page 13: Evolution of nuclear shape in the light Radon isotopes

x8 Miniball clustersx8 Miniball clusters

120120SnSn2 mgcm2 mgcm-2-2

202,204202,204Rn from Rn from REX-ISOLDEREX-ISOLDE

CD detectorCD detector(16(16oo-53-53oo))

Experimental TechniqueExperimental Technique

Andrew Robinson - INTC: 11th February 2008Andrew Robinson - INTC: 11th February 2008

Page 14: Evolution of nuclear shape in the light Radon isotopes

YieldsYields

E n e r g y V e r s u s L a b o r a t o r y A n g l e

0

1 0 0

2 0 0

3 0 0

4 0 0

5 0 0

6 0 0

0 1 0 2 0 3 0 4 0 5 0 6 0 7 0 8 0 9 0

L a b o r a t o r y A n g l e ( d e g )

Energy (MeV)

P r o j e c t i l e E n e r g y

T a r g e t E n e r g y

3 MeV/u 3 MeV/u 202202RnRn beam on 120120SnSn Target (550 MeV centre of target)

2%2% transmission efficiency

Beam Current of 2x102x104 4 ion/sion/s

State (mb)-ray yields

21+ 2.55 32000

41+ 0.1 1200

23+ 0.009 100

02+ 0.22 2700

22+ 0.019 2500

42+ 0.00068 <10

Estimate using CLX code assuming standard Miniball setup (8 triple cluster Ge detectors and CD detector)

Andrew Robinson - INTC: 11th February 2008Andrew Robinson - INTC: 11th February 2008

Page 15: Evolution of nuclear shape in the light Radon isotopes

Programmatic AspectsProgrammatic Aspects

First of a proposed programme of complementary complementary measurementsmeasurements using the unique facilitiesunique facilities at ISOLDEISOLDE and at the University of JyväskyläUniversity of Jyväskylä.

Andrew Robinson - INTC: 11th February 2008Andrew Robinson - INTC: 11th February 2008

Conversion electronConversion electron studies at ISOLDEISOLDE or SAGE SpectrometerSAGE Spectrometer at Jyväskylä. Help to determine properties of excited 0excited 0++ states and E0E0 content of j j j j transitions, related to rms charge radius.rms charge radius.

Recoil Distance Method (RDM)Recoil Distance Method (RDM) measurements with plunger to obtain independent lifetimesindependent lifetimes. Allow full extraction of the diagonal matrix diagonal matrix elementselements, allowing the sign of the deformationsign of the deformation to be extracted

Page 16: Evolution of nuclear shape in the light Radon isotopes

SummarySummary

Andrew Robinson - INTC: 11th February 2008Andrew Robinson - INTC: 11th February 2008

Coulomb Excitation of 202,204202,204RnRn using REX-ISOLDEREX-ISOLDE and Miniball + CDMiniball + CD.

•Obtain B(E2)B(E2) values.

•Search for excited 0excited 0++ and other non-yrastnon-yrast states.

•Infer the sign of nuclear deformation (with RDM measurement).

BeamMin.

IntensityTarget Ion Source Shifts

202Rn 9 x 105 / c ThCPlasma Cooled

15

204Rn 2 x 107 / c ThCPlasma Cooled

6

Page 17: Evolution of nuclear shape in the light Radon isotopes
Page 18: Evolution of nuclear shape in the light Radon isotopes

INTC - 11th February 2008INTC - 11th February 2008

Radon IsotopesRadon Isotopes

Macroscopic-microscopic models predict that deformed ground statesdeformed ground states exist beyond 202Rn.

E(4E(4++)/E(2)/E(2++)) ratio for 198,200,202198,200,202RnRn typical of ananharmonic vibrationalanharmonic vibrational system.S.J. Freeman et al., PRC 50 R1754 (1994)

R.B.E. Taylor et al., PRC 54, 2926 (1996); PRC 59, 673 (1999)

Evidence found for deformed intruder states in 202,204202,204RnRn which coexist with spherical ground state.D.J. Dobson et al., PRC 66 064321 (2002)

Page 19: Evolution of nuclear shape in the light Radon isotopes

INTC - 11th February 2008INTC - 11th February 2008

YieldsYields

Calculations

Beam current etcE n e r g y V e r s u s L a b o r a t o r y A n g l e

0

1 0 0

2 0 0

3 0 0

4 0 0

5 0 0

6 0 0

0 1 0 2 0 3 0 4 0 5 0 6 0 7 0 8 0 9 0

L a b o r a t o r y A n g l e ( d e g )

Energy (MeV)

P r o j e c t i l e E n e r g y

T a r g e t E n e r g y

Page 20: Evolution of nuclear shape in the light Radon isotopes

INTC - 11th February 2008INTC - 11th February 2008

Coulomb ExcitationCoulomb Excitation

Why is it good ?

Details of recent successes at ISOLDE

What will it allow us to extract ?

Hg Data - similar quailty

Page 21: Evolution of nuclear shape in the light Radon isotopes

INTC - 11th February 2008INTC - 11th February 2008

Programmatic AspectsProgrammatic Aspects

Programs etc.

SAGE this year

2+-2+ / 0+s

First of a proposed programme of complementary measurementscomplementary measurements using the unique facilitiesunique facilities at ISOLDEISOLDE and at the University of JyvaskylaUniversity of Jyvaskyla.