Shell Model in Complex Energy Plane
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Shell Model in Complex Energy Plane
Institute of Atomic Physics, Bucharest
• Resonances and virtual states: Berggren representation
• Shell model with resonances and virtual states
• Application: the structure of 11Li
N. Sandulescu
Espace de Structure Nucleaire Theorique, Saclay
**Similar work: N. Michel, W.Nazarewicz, M. Ploszajczak, K. Bennaceur,…
*Collaborators: R.Id. Betan (Rosario) , R.J.Liotta (Stockholm), T. Vertse (Debrecen)
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Resonances and virtual states
10Li
virtual stateresonances
9Li
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Single-particle resonant states
79Ni
78Ni
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Resonant states
Decaying state (Gamow,1928)
2En
nn iE
divergence !
« Capturing » state: tt *nn kk
tEi n
e ri ne
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General defintion ( Siegert, 1939)
0),()](2)1(
[22
22
2
krurVh
M
r
llk
dr
dl
« Resonances »: out-going solutions
Time-reversed solutions : ),(~),( * rkurku nln
),( rku nl
0),()( lll OuWky
;)()(),( lllll IkyOkxrku
Resonant states
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Poles of S-matrix
Re k
Im k• k-plane :
• energy plane: ;2
iE );(
222
2
M
M
2
ik
« resonance »
« anti-resonance »
« crazy »
« anti-bound » Re E
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Gamow states : normalisation
• Bi-orthogonal set : ),( rku nl ),(),(~ * rkurku nn
• Regularisation: Zeldovich (’60) ; Gyarmati & Vertse (1971)
drrkurkueuu r ),(),(~lim|~ *
0
2
• Matrix elements: uAu ||~ complex quantity !
•Note : Gamow functions rigged Hilbert space
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Berggren representation
• Real-energy axis:
• Complex-energy plane:
L
Re k
(T. Berggren, Nucl. Phys. A108,265,1968)
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Two-particle resonances
)2,1()2(ˆ)1(ˆˆ VhhH
iiih ˆ)()(),( 2121 rrXrr jiij
kljilkijji XVX ||~~)(
)()( klfXijGf kl
ji
ijf
G )(1 2
;
Re
Im
(R.Betan, R.J.Liotta, N.S., T. Vertse, Phys.Rev. Lett. 89, 042501, 2002)
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Single-particle states
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Two-particle states
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Two-particle resonant states
80Ni
78Ni
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Two-particle resonant states
( R.Betan, R.J.Liotta, N.S., T. Vertse, Phys. Rev. Lett. 89, 042501, 2002 )
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Two-particle resonant states
( R.Betan, R.J.Liotta, N.S., T. Vertse, Phys. Rev. Lett. 89, 042501,2002 )
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Resonances and anti-bound states
10Li
anti-boundresonances
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Anti-bound states
• definition: ;nn ik 22
2 nn ME
Re k
Im k
• wave function:
),()(),( 2/122
riuk
krk n
nscat
);( riu n
(A.B.Migdal et al, Sov.J.Nucl.Phys. 14, 488, 1872 )
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Energy contours in Berggren representation
Re
Im
L
Anti-bound state
Resonant states
Re
2/1s
2/1p2/3d
L
Im
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Resonances and anti-bound states
10Li
anti-bound
Note: does a unique mean field exist ? NO !
resonances
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Effective mean fields for 10Li
J.C.Pacheco, N. Vinh Mau, Pys.Rev.C65(2002)044004
H. Esbensen, G.F. Bertsch, K. Hencken, Phys.Rev.C56(1997)3054
N. Vinh Mau, Nucl. Phys. A592(1995)33
Particle-vibration couplings:
F. Barranco et al, Eur. Phys. J. A11(2001)385
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Ground state of 11Li: pole structure
Re
(R.Betan, R.J.Liotta, N.S., T. Vertse, Phys. Lett. B584, 48, 2004 )
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Two-particle resonant states in 11Li
(R.Betan, R.J.Liotta, N.S., T. Vertse, Phys. Lett. B584, 48, 2004 )
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Conclusions
Main advantages of shell model in complex energy plane:
• based on relevant continuum configurations
• direct access to multi-particle resonant states
Open problems :
• multi-particle resonant states: decays channels ?
• efficient truncation schemes for large systems ?
- Density Matrix Renormalisation Group
( N. Michel, W. Nazarewicz, M. Ploszajczak, J. Rotureau, nucl-th/0401036)
( G.Hagen, M.Hjorth-Jensen, J. Vagen, nucl-th/0410114 )
- Lee-Suzuki similarity transformation - Multi-reference perturbation method
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)()(),( 2121 rrXrr jiij
Rr
ikre iKRe
Decay channels
1r
2r
11rike
22rike
…………….…………….
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Localisation of scattering states
( R.Betan, R.J.Liotta, N.S., T. Vertse, Phys. Lett. B584, 48, 2004 )
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Anti-bound states: trajectories