structure of even-even nuclei using a mapped collective hamiltonian
DESCRIPTION
Structure of even-even nuclei using a mapped collective hamiltonian and the D1S Gogny interaction. J.-P. Delaroche, M. Girod, H. Goutte, S. Hilaire, S. P é ru, N. Pillet (CEA Bruyères-le-Châtel, France) J. Libert (IPN Orsay, France) G. F. Bertsch (INT, Seattle, USA). Introduction - PowerPoint PPT PresentationTRANSCRIPT
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J.-P. Delaroche Pack Forest , June 2009
Structure of even-even nuclei using a mapped collective hamiltonian
and the D1S Gogny interaction
Structure of even-even nuclei using a mapped collective hamiltonian
and the D1S Gogny interaction
J.-P. Delaroche,M. Girod, H. Goutte, S. Hilaire, S. Péru, N.
Pillet(CEA Bruyères-le-Châtel, France)
J. Libert (IPN Orsay, France)
G. F. Bertsch (INT, Seattle, USA)
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J.-P. Delaroche Pack Forest , June 2009
• Introduction• Reminder of formalism• Ground state properties • Yrast spectrum• Non yrast spectrum• Summary
OutlineOutline
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J.-P. Delaroche Pack Forest , June 2009
• Motivations• Methodology• Calculations for ~1700 nuclei (dripline to dripline) (10<Z<110, N<200)
• Benchmarking• Predictions for future studies (SPIRAL 2, FAIR, RIA, ...)
Computing time : over 25 years of CPU time if calculation were performed on a single processor.
IntroductionIntroduction
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J.-P. Delaroche Pack Forest , June 2009
1) Hartree-Fock-Bogoliubov equations with constraints
0 ZNQ Hii
qZNii
iq =Φλ−λ−λ−Φδ ∑
(Z) N )Z(Nii
qq =ΦΦ
iqiq q Qii
=ΦΦwith
Constraints on
FormalismFormalism
More details in: J. Libert et al., PRC60, 054301 (1999)
0Q and 2Q
2220 yxz2Q −−= 22
2 yxQ −=and
Self-consistent symmetries
2T π and parity
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J.-P. Delaroche Pack Forest , June 2009
•Number of major shells: N0= 6 - 16
•Linear constraints used throughout
FormalismFormalism
•(q0, q2) Bohr coordinates (β, γ)
0 < β < 0.9 0 < γ < π/3
CHFB equations solved by expanding sp states onto triaxial harmonic oscillator basis
•CHFB equations solved on a grid
Δβ = 0.05 Δγ = 10°
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J.-P. Delaroche Pack Forest , June 2009
CHFB -> GCM -> GOA -> 5DCH
No free parameters beyond those in theGogny D1S force.
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J.-P. Delaroche Pack Forest , June 2009
FormalismFormalism
2) Collective Hamiltonian in 5 quadrupole collective coordinates
( ) ( ) ( )20202 and 0nm,
12/12/123
1
22
,,2
ˆ
2ˆ aaVaaV
aBD
aD
J
IH
nmn
mk k
kcoll Δ−+
∂
∂
∂
∂−= ∑∑
=
−−
=
hh
Jk(a0, a2): moment of inertia
)Bdet()a,a(J)a,a(D3,1k
20k20 ∏=
=
qq20 H)a,a(V ΦΦ=
.)vib.rot(ZPE)a,a(V 20 +=Δ ZPEpot neglected
γβ=γβ= sinacosa 20
Bmn(a0, a2): collective mass (vibration)
D(a0, a2): metric
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J.-P. Delaroche Pack Forest , June 2009
FormalismFormalism
Approximations
Bmn(a0, a2): cranking (Inglis-Belyaev)
ValatinThoulessI
limJqkq
0k −⇔ω
ΦΦ=
ωω
→ω
IM)I(EIMHcoll =
∑=K
20IK IMK)a,a(gIM
∫=2
20IK20 )a,a(gdada)K(P
Notations
Correlation energy
DCH5minHFBcorr EEE −=
not fullfilled for ~80 nuclei at (near) double-closed-shells.0Ecorr >
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J.-P. Delaroche Pack Forest , June 2009
FormalismFormalism
3) Limitations of present CHFB+5DCH theory
• Adiabatic approximation low spins only
•Quasiparticle degrees of freedom ignored
•No coupling to other collective modes
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J.-P. Delaroche Pack Forest , June 2009
Shape coexistence
E.Clément et al. PRC75, 054313 (2007)
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J.-P. Delaroche Pack Forest , June 2009
Transitional nucleus
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J.-P. Delaroche Pack Forest , June 2009
GS static and dynamic deformations
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J.-P. Delaroche Pack Forest , June 2009
Frequency distributions of β and γ deformations
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J.-P. Delaroche Pack Forest , June 2009
Rigidity parameters
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J.-P. Delaroche Pack Forest , June 2009
Charge radii
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J.-P. Delaroche Pack Forest , June 2009
Charge radii for Sr isotopes
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J.-P. Delaroche Pack Forest , June 2009
Correlation energy and residuals
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J.-P. Delaroche Pack Forest , June 2009
2-nucleon separation energies
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J.-P. Delaroche Pack Forest , June 2009
Energy weighted sum rules
)20;2E(B)2(ES 111+++ →=
∑ +++ →=i
i1i )20;2E(B)2(E)I(S
2
A
Z)I(S)II(S ⎟
⎠
⎞⎜⎝
⎛=
)X(Se
)20;2E(B)2(E)X(s
2111+++ →
=
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J.-P. Delaroche Pack Forest , June 2009
First 2+ level collective properties
G.F. Bertsch et al., PRL 99, 032502 (2007)
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J.-P. Delaroche Pack Forest , June 2009
Exp. Th.
Frequency distributions of the R42 ratio
R42= E(4+1) / E(2+
1)
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J.-P. Delaroche Pack Forest , June 2009
R42 ratio versus deformation properties
δβ/<β><β>
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J.-P. Delaroche Pack Forest , June 2009
R42: comparison Th. / Exp. R42 frequency distribution
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J.-P. Delaroche Pack Forest , June 2009
R62 versus R42 : comparison Th. / Exp.
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J.-P. Delaroche Pack Forest , June 2009
Probability distribution of K components for 22+ states
∫=2
20IK20 )a,a(gdada)K(P
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J.-P. Delaroche Pack Forest , June 2009
P(K=2) frequency distribution for 22+ and 23
+ states
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J.-P. Delaroche Pack Forest , June 2009
5DCH Systematics for 2+γ levels
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J.-P. Delaroche Pack Forest , June 2009
Comparison Th. / Exp. for 22+ energies
γ vibration
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J.-P. Delaroche Pack Forest , June 2009
Comparison Th. / Exp. for 02+ energies
Cranking masses too small !!!
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J.-P. Delaroche Pack Forest , June 2009
Exp. and Th. for R02 versus R42
R02= E(0+2)/E(2+
1)
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J.-P. Delaroche Pack Forest , June 2009
Energy distribution of 02+ levels
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J.-P. Delaroche Pack Forest , June 2009
Model criteria for the occurrence of β-vibration
Crossover matrix elements
Relationship between quadrupole Transition operator for 21
+ 02+,
23+ 21
+, 23+ 01
+ transitions(Bohr and Mottelson, Eq. 4-219)
gEMJJJJgEMJ ggg 20020ˆ2 ββ ββ
Form the ratio of |M20|, |M02|, |M22| to their total.
Conditions for the existence of β vibration should be quite common.
222002 10
7MMM
10
7
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J.-P. Delaroche Pack Forest , June 2009
Chart of the nuclei in the vicinity of the center of the triangle
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J.-P. Delaroche Pack Forest , June 2009
E0 transition strengths versus neutron number
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J.-P. Delaroche Pack Forest , June 2009
Ratio of transition strengths for excited K=0 over ground state bands versus
neutron number :indicator for shape coexistence
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J.-P. Delaroche Pack Forest , June 2009
• ~1700 nuclei have been studied between drip-lines in the present microscopic model
• Yrast band properties: well described especially for well deformed nuclei
• 22+ levels: energy well described
most of these levels are 2γ + vibrations
• 02+ levels: energy high (cranking masses)
off-band E2 transition: β-vibration? E0 transition strength: high
→CHFB+5DCH questionable for the 02+ excitations.
Extension required to include coupling to quasiparticle and pairing vibration modes.
How with GOA? Better collective masses: Thouless-Valatin, QRPA
• Next to come: γ band properties
Summary and outlookSummary and outlook