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1.Description of correlations in mean-field and beyond mean-field methods. Variational multiparticle-multihole configuration mixing method N.Pillet (1) , J.-F.Berger (1) , E.Caurier (2) , H.Goutte (1) , N.Vinh Mau (3) , F.Chappert (1). Spatial structure of Cooper pairs in HFB approach - PowerPoint PPT Presentation
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1.Description of correlations in mean-field and beyond mean-field
methods
Spatial structure of Cooper pairs in HFB approach
N.Pillet(1), N.Sandulescu(4), P.Schuck(3)
2.Nuclear excitations in plasmas
G.Gosselin(1), V.Méot(1), N.Pillet(1)
Jeunots 2008, February 4-6 (2008), Saclay
Variational multiparticle-multihole configuration mixing method
N.Pillet(1), J.-F.Berger(1), E.Caurier(2), H.Goutte(1),
N.Vinh Mau(3), F.Chappert(1)
(1) SPN,CEA-Bruyères-le-Châtel (3) IPN, Orsay
(2) IPHC, Strasbourg (4) IPNE, Bucharest
Variational multiparticle-multihole configuration mixing
Motivations:
• Towards a unified description of correlations in the context of beyond mean- field method {essentially Pairing + RPA + particle-vibration coupling}
• Conservation of particle numbers + enforced Pauli principle
• Description on the same footing of even-even, odd and odd-odd nuclei
• Description of both ground states and excited states
Description of correlations in mean field and beyond mean field methods
Jeunots 2008, February 4-6 (2008), Saclay
Formalism:
• Trial wave function: Superposition of Slater determinants corresponding to mpmh excitations built upon a given state of HF type
Description of correlations in mean field and beyond mean field methods
Variational multiparticle-multihole configuration mixing method
Jeunots 2008, February 4-6 (2008), Saclay
h2p2
h2p2
h1p1
h1p1h0p0 AAA
N
1ii 0a
m
1)kl(lkaawith an
d
+ + + …
• Variational principle
o Optimized single particle states:
o Mixing coefficients:
Description of correlations in mean field and beyond mean field methods
Variational multiparticle-multihole configuration mixing method
Jeunots 2008, February 4-6 (2008), Saclay
o Functional: )(H)(
0A
)(*
A)(H)(HA
0)(
*i
),(G),(h
Simultaneous solution of both equations (iterative):self-consistent procedure and renormalization of the
HF field
ˆwith
(*) N.Pillet, J-F.Berger and E.Caurier, under submission to PRC.
N.Pillet, N.Sandulescu, Nguyen Van Giai and J-F.Berger, Phys.Rev.C71, 044306 (2005).
Current study:
Description of correlations in mean field and beyond mean field methods
Variational multiparticle-multihole configuration mixing method
Jeunots 2008, February 4-6 (2008), Saclay
Pairing correlations and link with projection on particle
number methods-Applications to Sn isotope ground states(*)
Structure of correlated wave functions
Correlation energy (MeV) Only configurations
with excited pairs
D1S Gogny force
ij 2
A)j,i(T
Description of correlations in mean field and beyond mean field methods
Variational multiparticle-multihole configuration mixing method
Jeunots 2008, February 4-6 (2008), Saclay
Effect of correlations on single particle spectra
Charge radii
Future studies:
• Link with RPA – How to simulate RPA calculation with mp-mh method?
Which one-body density should be used?
• Description of light exotic nuclei (B, Li, Be, C, N, O, F) – PhD Proposal
Application of the mp-mh method to odd and odd-odd nuclei
Effect of general correlations on single particle spectra
Applications to island of inversionRe-fit of Gogny interaction (D2)?
Need for experimental data on masses, spins, parities… towards drip lines
Description of correlations in mean field and beyond mean field methods
Variational multiparticle-multihole configuration mixing method
Jeunots 2008, February 4-6 (2008), Saclay
Spatial structure of Cooper pairs in HFB approach
(*) N. Pillet, N. Sandulescu and P. Schuck, Phys. Rev. C76, 024310 (2007).
• Method: HFB with D1S Gogny interaction
• Spherical nuclei: O, Ca, Ni, Sn, Pb isotopic chains
Jeunots 2008, February 4-6 (2008), Saclay
Description of correlations in mean field and beyond mean field methods
Brody-Moshinsky transformation K(R,r) (R: center of mass, r: relative coordinates)
Two-body correlated wave function (J=0):
)(cosP)()r()r(K)1j2(41
)r,r(K 12ll
2l2n1l1nlj2n1n
lj1n2n0S21
0;lnln0;nlNl)(cosP)R2()2/r()l2
1l2()(
K)1j2(41
)r,R(K
1211lNlnNl
nl2/1
1
l
1j1l2n1n
1j1l
1n2n10S
2rr
R 21
21 rrr
and
Size of Cooper pairs:
2/122
2/124
dsindr,r,RKr
dsindr,r,RKr)R(
Jeunots 2008, February 4-6 (2008), Saclay
Description of correlations in mean field and beyond mean field methods
Spatial structure of Cooper pairs in HFB approach
Strong coupling behavior of Cooper pairs on the surface of superfluid nuclei
Probability Distribution
222 )r,R(KRr)r,R(P
Jeunots 2008, February 4-6 (2008), Saclay
Description of correlations in mean field and beyond mean field methods
Spatial structure of Cooper pairs in HFB approach
Future study: Generalization to deformed nuclei where the parity mixing is expected to be stronger + nucleon pair transfer
Nuclear excitations in plasmas
Photon absorption
NEEC
(nuclear excitation by electron capture)
NEET
(nuclear excitation by electronic transition)
Inelastic electron scattering
Jeunots 2008, February 4-6 (2008), Saclay
Main excitation processes
Corresponding de-excitation processes Photon emission
spontaneous+ stimulated
IC
(internal conversion)
BIC
(bound internal conversion)
(*) P.Morel, V.Méot, G.Gosselin, D.Gogny and W.Younes, Phys.Rev.A69, 063414 (2004).
(*) G. Gosselin, V. Méot and P. Morel, Phys.Rev.C76, 044611 (2007).(*) G. Gosselin, V. Méot and P. Morel, Phys.Rev.C70, 064603 (2004).
•Photon absorption, NEET and NEEC mechanisms (*):
First order perturbation theory Fermi golden rule
Method for transition rate calculation:
•Inelastic electron scattering: (under development)
Second order perturbation theory
PWBA, WKB, DWBA (radial transition matrix element)
Jeunots 2008, February 4-6 (2008), Saclay
Nuclear excitations in plasmas
201Hgm
Two level model
Photon+NEEC/IC+NEET/BIC
(thermodynamical equilibrium)
(*) V.Méot, J.Aupiais, P.Morel, G.Gosselin, F.Gobet, J.N.Scheurer and M.Tarisien, Phys. Rev. C75, 064306 (2007).
201Hg
g.s.0 keV
1.56 keV
26.27 keV
81ns(*)3/2-
1/2-
5/2- 630ps
Jeunots 2008, February 4-6 (2008), Saclay
Nuclear excitations in plasmas
Lifetime of first 201Hgm
Future: inclusion of inelastic electron scattering
Jeunots 2008, February 4-6 (2008), Saclay
Future
• Variational multiparticle-multihole configuration mixing method
• Spatial structure of Cooper pairs
• Nuclear excitations in plasmas
Link with RPA
Study of light nuclei- PhD proposal
Test and possible re-fit of Gogny interaction (D2)
Generalization to deformed nuclei + pair transfer
Inclusion of inelastic electron scattering
Κ2(R,r) in Sn isotopes and Parity mixing effect
Jeunots 2008, February 4-6 (2008), Saclay
Description of correlations in mean field and beyond mean field methods
Spatial structure of Cooper pairs in HFB approach
Shell effects + Parity mixing effects
Probability Distribution 222 )r,R(KRr)r,R(P
Jeunots 2008, February 4-6 (2008), Saclay
Description of correlations in mean field and beyond mean field methods
Spatial structure of Cooper pairs in HFB approach
dr)r,R(Kr
)r,R(Kr)r,R(W 22
22
Future study: Generalization to deformed nuclei where the parity mixing is expected to be stronger + nucleon pair transfer