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Search for 28 Si cluster states through the 12 C+ 16 O radiative capture
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Transcript of Search for 28 Si cluster states through the 12 C+ 16 O radiative capture
Sandrine CourtinSan Antonio May 29th, 2012
Search for 28Si cluster states through the 12C+16O radiative capture
Sandrine Courtin
Institut Pluridisciplinaire Hubert Curien,and University of Strasbourg
France
Sandrine CourtinSan Antonio May 29th, 2012
Cluster bands → 16O(12C+), 18O(14C+), 20Ne(16O+), 44Ti(40Ca+)
→ Be and C neutron-rich isotopes with 2xn and 3xn configurations W. Von Oertzen, HMI (dimers and polymers, Nucl.Phys. A734(2004)) M. Freer, Charissa (Nucl.Phys. A738(2004))
Stars examples of α clustering : → 8Be(0+) Ex = 0.0 MeV → 9Be(3/2-, 5/2-) Ex = 0.0, 2.43 MeV E2(5/2- → 3/2-) : 24 W.u. → 12C(0+) Ex = 7.65 MeV E2(0+ → 2+) : 8 W.u. → 16O(0+, 2+, 4+) Ex = 6.05, 6.92, 10.36 MeV (4p-4h) E2(2+ → 0+) : 27 W.u., E2(4+ → 2+) : 65 W.u.
α clusters in light heavy-ionsα clusters in light heavy-ions
Sandrine CourtinSan Antonio May 29th, 2012
In the sd shell, based on 12C, 16O CN at high excitation energy, narrow resonances… Width = 100-200 keV, striking examples: 12C+12C and 12C+16O
12C+16O : collision at CB and below, low spin (0+-4+), Ex(28Si) ~ 25 MeV Radiative capture reaction 12C(16O,)28Si, gamma decay via ‘doorway’ states… cluster states, deformed
Heavier clusters
Sandrine CourtinSan Antonio May 29th, 2012
12C+16O breakup states in 28Si
Excitation energy (MeV)25
• 12C+16O ‘breakup’ states in 28Si up to E* = 45 MeV C.J. Metelko et al., J. Phys. G29 (2003), 697 • Reaction 12C(20Ne,12C16O)@ ANL
• Position Sensitive Double-Sided Silicon Strip Detectors for coincident particle detection
RC
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Radiative Capture and heavy-ions
Nuclear astrophysics, light particles, inverse kinematics
Heavy-ionsHeavy-ions
GSI (J.G. Keller, K.H. Schmidt et al. PRC 29, 1569 (1984)) 90Zr(358 MeV)+90Zr -> 180Hg + σ= 40 pb More recently at Argonne (F. Camera et al., PLB 560, 155 (2003)) 89Y(352 MeV)+90Zr -> 179Au + Light heavy-ions: : 1212C+C+1212C -> C -> 2424Mg + Mg + Sandorfi et al. (Brookhaven) : Sandorfi et al. (Brookhaven) : large NaI detectorlarge NaI detector (~ 1980) (~ 1980) ResonancesResonances
EE > 18 MeV, decay to low-lying states of > 18 MeV, decay to low-lying states of 2424MgMgSame results for Same results for 1212C+C+1616O -> O -> 2828Si + Si +
Sandrine CourtinSan Antonio May 29th, 2012
To the 28Si prolate excited band
A.M. Sandorfi, in Treatise on Heavy-Ion Science, D.A. Bromley, Vol II, sec. 3.M.T. Collins, A.M. Sandorfi and D.H. Hoffmann, Phys.Rev. Lett. 49 (1982), 155P.R. Christensen et al., Nucl.Phys. A 280 (1977) 189.
radiative capture resonances
To the 28Si ground state band
… … Capture Radiative and light heavy-ions / Decay studiesCapture Radiative and light heavy-ions / Decay studies1212C+C+1616O at 5 energiesO at 5 energies
CB
fusion
Ec.m. = 6.6, 7.2, 8.5, 8.8 and 9 MeV
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First stageFirst stage
Second stageSecond stage
D.A
. H
utc
he
on
et
al.,
NIM
A 4
98
, 1
90
(2
00
3).
ISAC I : RNBs / Stable (OLIS) 0° spectrometer Tof : 21 m Beam rejection: 10Beam rejection: 101313
Acceptance : cone ½ angle 20 mrad
gaz/solid target focal plane (DSSSD, …) BGO ( = 50 % @ 5 MeV)
… … Capture Radiative and light heavy-ions/ Decay studies Capture Radiative and light heavy-ions/ Decay studies 1212C+C+1616OO
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12C+16ORecoil spectrum vs ToF (28Si)
12C+16OGamma spectrum (28Si)2+ → 0+
4+ → 2+
3+,0+, 3-
~14 MeV
12C+16OHighest energy -ray
~14 MeV
25 MeV
~ 11 MeV
0 MeV28Si
S. Courtin et al., Fusion 06, San Servolo, AIP Conf. Proc. 853 (2006)
12C+16O/ Results
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What is the structure of these states?What is the structure of these states?
28Si(12C-160) Ohkubo and Yamashita, Phys.Lett. B 578 (2004) 304.
→ → Links between cluster bands?Links between cluster bands?
… … Capture Radiative and light heavy-ions/ Decay studiesCapture Radiative and light heavy-ions/ Decay studies1212C+C+1212C and C and 1212C+C+1616OO
T. Ichikawa, Y. Kanada-En’yo and P. Möller, Phys. Rev. C 83 (2011)
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simulation
experiment
19.3 MeV
p
n
24Mg
Resonance J = 0+,1-, 2+, 3-, 4+, 5-, 6+
28Si
20Ne
10 MeV
g.s.
25 MeV
Very well known sd shell nucleus
E0(MeV)
Co
un
ts
E0(MeV) 9.3 MeV
0+ only
Ex : J = 0+
12C+16O resonance spin ? / MC simulations
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12C+16O / statistical vs structural effects
E = 8.5 MeV E = 9 MeV
D. Lebhertz, S. Courtin et al. Phys.Rev. C 85, 034333 (2012)
J = 5- (44%),6+ (56%) J = 5- (8%),6+ (86%) + stat. background
in good agreement with fusion resonance work(E. Schloemer et al. Phys. Rev. Lett. 51 (1983))
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Direct feeding of 31- (deformed) at 6.9 MeV
3-1
25.3 MeV
6.9 MeV
28Sig.s.
E0(MeV)
E1(
MeV
)
Direct feeding of the 43+ (prolate) at 9.2 MeV
2+1
4+3
25.7 MeV
9.4 MeV
1.8 MeV
28Sig.s.
12C+16O / statistical vs structural effects
E = 9 MeVE = 8.5 MeV
E = 9 MeV
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12C+16O below CB
A. Goasduff, PhD Thesis Université de Strasbourg 2012
E = 6.6 MeV, strong feeding of J= 1+,T=1 states
Decay scenario L = 1 transition from 0+, 1-, 2+ resonancecf 12C+12C, E = 6 MeV (D.G. Jenkins et al, Phys. Rev. C76 (2007))
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12C+16O radiative capture cross-sections from our 2 experimental campaigns
12C+16O radiative capture cross-sections from our 2 experimental campaigns
D. Lebhertz, PhD Thesis University of Strasbourg, 2009
Larger cross-sections due to new decays paths
A. Goasduff, PhD Thesis University of Strasbourg, 2012
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Future: radiative capture with the PARIS arrayFuture: radiative capture with the PARIS array
Experimental : Better resolution array (100 keV to 50 MeV), LaBr3 + NaI phoswichescoupled to a large acceptance spectrometer or used in a calorimeter mode
→ Individual peaks can be resolved
12C(12C,γ)24Mg, GEANT4 simulations for PARIS (200 LaBr3 spherical configuration)
12C+12C24Mgtoday
12C+12C24Mgtomorrow
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this work
Metelko et al. data
ConclusionsConclusions
• Radiative capture reactions around CB 28Si(12C-16O), doorway states 11 MeV, (∼ +24Mg = 9.99 MeV) ➜ impact on the capture cross-section
• Results compared to simulations • above CB, 5-, 6+ spins for the resonance and feeding
of specific states• below CB, large feeding of 1+, T = 1 states (11.45 MeV),
like in 24Mg (10.70 MeV). Isovector M1 transitions, spin-flip excitations give rise to 1+,T=1 states in the N=Z nuclei 24Mg and 28Si (same states strongly observed in (e,e’), (’), (p, p’), (p,n)).2+ resonance for 28Si and 24Mgin C+C, it is proposed that the resonance is connected with the 24Mg ISGQR (on 24Mg g.s.)in C+O, the 2+ resonant state could be connected with the 28Si ISGQR built on the prolate structure (~ 7MeV). Just N=Z selection rule ?
• Decay scenarios will be confirmed with better resolution data with the PARIS detector
Sandrine CourtinSan Antonio May 29th, 2012
S.Courtin, A. Goasduff, D. Lebhertz, A. Michalon, F. Haas et al., Department of Subatomic Research, IPHC, Strasbourg, France
D.G. Jenkins, P.A. Marley et al., Physics Department, University of York, UK
D.A Hutcheon, C. Ruiz, J. Fallis et al.,TRIUMF, Vancouver, Canada
CollaborationCollaboration