clustering in 12 be: determination of the enhanced monopole strength
DESCRIPTION
Clustering in 12 Be: Determination of the Enhanced monopole strength. Yanlin Ye School of Physics and State Key Lab. of Nucl . Phys .&Tech. Peking University. ARIS, 2014.06.02, Tokyo. Collaborators. Outline. I. Some background. II. Observation. Discussion. IV. Summary. - PowerPoint PPT PresentationTRANSCRIPT
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Clustering in Clustering in 1212Be: Be: Determination of the Determination of the Enhanced monopole Enhanced monopole
strengthstrength
Yanlin YeYanlin YeSchool of Physics and State Key School of Physics and State Key
Lab. of Nucl. Phys.&Tech. Peking Lab. of Nucl. Phys.&Tech. Peking
UniversityUniversityARIS, 2014.06.02, Tokyo
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Collaborators
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Outline
I. Some background
II. Observation
III. Discussion
IV. Summary
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alternating independent-particle and clustering structure — a unique feature of nuclear many-body system.
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Idea of the relative tightness of a cluster inside a nucleus
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for unstable nuclei
Unstable nuclei: much more cluster configurations (and thresholds) within a small Ex interval.— richness of nuclear clustering
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Recent progress
Theory: AMD, GCM(RGM), GTCM, FMD, TCSM,
TCHO(DHO), …
Experiment:
0+2 (7.65 MeV) state in 12C,
0+2 (6.05 MeV) and 0+
3 (12.05 MeV) in 16O;
0+4 (8.03 MeV) in 20Ne
…...
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AMD
6He + 6He resonance
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Monopole excitation method
T. Yamada et al., PRC85,034315(2012); PTP120,1139(2008)
Isoscaler monopole excitation, a jump of about 35 MeV in a simple single-particle picture.
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GTCM Explicit cluster-degree of freedomGood up to high excited levels
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Outline
I. Some background
II. Observation
III. Discussion
IV. Summary
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Main experimental observables for determining the cluster formation
i) Ex - spin systematics:
high moment of inertia
ii) Large cluster decay width:
large ΓCluster/Γ ; γ2Cluster ; θ2
Cluster
iii) Characteristic transition strength
large M(IS) !!
M(IS) ΓCluster
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Freer et al., PRL82(1999) 1383; PRC63 (2001)034301Charity et al., PRC76(2007)064313no small angle (low Erel) detection
6He+6He,CH2 4He+8He,with P 4He+8He, with C
Freer
Charity
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A new exp. at RIBLL1@HIRFL, Lanzhou
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Beam : 12Be , 29.0MeV/u , ~3000ppsTarget : Carbon, 100 mg/cm2
DSSD : 32 2mm-stip, 300μm , covering 00-120 Lab.CsI(Tl) : 4 x 4 , 2.5cm*2.5cm*3cm,Detection focused on the most forward angles
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4He 6He
8He
PID for 2-xHe fragments
Uniform calibration of the Si strips and treatment of PID under intense direct beam: [IEEE-NS 61(2014)596, NIMA728(2013)52]
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Ex = Erel + Ethr
* 2
2 2 2 2 22( )( ) 2 ( 2 )( 2 ) cos
rel a b a b
a b a a b b a a a b b b
E M M M M M M
M M M T M T M T T M T T M
*MaM
bM
aT
bT
4He+4He 4He+6He 6He+6He 4He+8He
2-xHe events for 12Be
Reconstruction (insensitive to Ebeam)
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107.6KeV 8Be(g.s)
504.1KeV:9Be->8Be(2+)
Excitation Energy---4He+4He
Ref1: PLB580(04)129-14Be breakup
Ref1
verification for 4He + 4He channel
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Resolution and efficiency
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Our exp: 6He+6He 11.7 13.3 MeV 4He+8He 10.3 12.1 13.6 MeV
Large and unusual 10.3 MeV state;
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Outline
I. Some background
II. Observation
III. Discussion
IV. Summary
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Our exp: 6He+6He 11.7 13.3 MeV 4He+8He 10.3 12.1 13.6 MeV
Large and unsual 10.3 MeV state;pure 0+ !!
Determine the spin and MR band
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Spin: Angular correlation analysis for the 10.3 MeV state in 4He + 8He channel
For small angle inelastic scattering leading to a resonant state with an angular momentum J, which subsequently breaks up into spin-0 fragments, the projected angular correlation spectrum is proportional to | PJ(cos(Ψ) |2, with Ψ being the fragment c.m. angle relative to the beam direction.
Ex: 10.0 - 11.4 MeV
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13.6 MeV state
10.3 MeV state
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|cosΨ| resolution
0.1 0.2 0.4
10.3 MeV state
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10.3 MeV state
Confirming the MR band with large moment of inertia
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Determining the monopole strength
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Fraction: 0.034(10) x 2.2.
EWSR : 6727.9 fm4 MeV,
M(IS) : 7.0 +/- 1.0 fm2,
DWBA calculation
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Determining the cluster decay width
10.3 MeV (0+) state:
1.5(2) MeVii
22
0
ba2
2ΓEE
ΓΓ
ΓΓΓΓΓ pn
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All possible decay channels
10.3 MeV(0+) state: Γ = 1.5(2) MeV; Γ = ΓHe+ΓBe
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Overall dominance of the 0+ state
Kosheninnilov ours
DWBA calculations for the excitation of 12Be from its ground state to the 10.3 MeV excited state, when interacting with a C target.
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10.3 MeV(0+) state: Γ = 1.5(2) MeV; Γ = ΓHe+Γbe
Kosheninnilov[12]: ΓBe/Γ= 0.28±0.12
ΓHe/Γ = 1−ΓBe/Γ = 0.72(12); ΓHe = 1.1(2) MeV
γ2He= 0.50(9); θ2
He= 0.53(10) ( comparable to 8Be)
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Outline
I. Some background
II. Observation
III. Discussion
IV. Summary
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Summary
i) For the first time a strong monopole strength has been determined in unstable nuclei, providing a clear evidence for cluster formation in 12Be.
ii) Angular-correlation method is very sensitive to the spin of the resonance. MR band in 12Be has been justified based on the Ex-spin systematics .
iii) A large cluster-decay width, and consequently a large cluster SF, are obtained for the 10.3 MeV state in 12Be.
All these findings demonstrate a dominating cluster structure in 12Be just above the 4He+8He threshold.
iv) detection around 0-degrees is essential in in order to measure near-threshold resonances in breakup exp.
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3838
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comparison
Freer
Charity
ours
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Korsheninnikov et al., 1995, 50 AMeV 12Be + p; inelastic10 MeV state, L >= 4
Saito et al., 2004, 60 AMeV 12Be + α;
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Recent comprehensive review
238 pages
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