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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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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
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.
Light Pb isotopesLight Pb isotopes
Andrew Robinson - INTC: 11th February 2008Andrew Robinson - INTC: 11th February 2008
Mercury IsotopesMercury Isotopes
Andrew Robinson - INTC: 11th February 2008Andrew Robinson - INTC: 11th February 2008
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
+)
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
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
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
Light Polonium IsotopesLight Polonium Isotopes
Andrew Robinson - INTC: 11th February 2008Andrew Robinson - INTC: 11th February 2008
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
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).
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
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
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
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
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
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)
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
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
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.