Everything is coupled: reactions with weakly bound projectiles
Transcript of Everything is coupled: reactions with weakly bound projectiles
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Everything is coupled: reactions with weakly bound
projectilesKrzysztof Rusek
Heavy Ion Laboratory, University of Warsaw
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• National nuclear physics laboratory open
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Heavy Ion Laboratory, University of
Warsaw :
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Overview
Investigation of coupling effects has a long history,
as long as nuclear physics, beginning with deuteron
induced reactions. This contribution is not meant as
a review but rather as a presentation of a few
examples where the couplings play an important
role.
- Elastic scattering and coupling with the continuum
(effect of breakup)
- Elastic scattering and transfer reactions
- Fusion and direct reactions
- Effect on the Coulomb barrier distribution
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Real and virtual processes
Targetcore
Virtual couplings (polarizability) – processes whereby, for
example, the projectile nucleus is raised to an excited
state which then decays back to the ground state before
the projectile has traversed the field of the target nucleus.
N.Keeley et al. Progress in
Particle and Nuclear Physics
63,396 (2009)
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6Li + 58Ni
El. scatt. and effect of breakup
α+d
breakup
threshold
g.s.
6Li
resonance?
H. Nishioka et al., NPA 415,
230 (1984)
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Couplings with resonant and non-
resonant states
α+d
breakup
threshold
g.s.
6Li
resonance
K.R. et al. PRC 50, 2010 (1994)
Resonant only
full
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6Li - no E1
Electric dipole transition:
= 0 for λ = 1
Where „effective charge” is:
B. Buck, A.A. Pilt, NPA280, 133 (1977)
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Comparison of 6Li-6He
Reduced Coulomb-nuclear interference peak for 6He,
caused by Coulomb dipole couplings to the continuum
No E1
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Interaction distance from el. scattering
D
6He + 208Pb
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Comparison for various projectiles
6He: D=18 fm
A. Pakou, K.R.
6Li: D=14.7 fm
209Bi, 208Pb targetsReduced int. distance
d = D / (Ap1/3+At1/3)
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Coulomb post-acceleration6He + 206Pb at 18 MeV, L. Standylo et al. PRC 87, 064603
6He el.
4He from
breakup
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Coulomb post-acceleration
α energy at the detector:
4/6 ED + Z1Z2e2/D
= 4/6 E + 1/3 Z1Z2e2/D
6He energy at D:
ED = E – Z1Z2e2/D
D
Z2
Z1
Breakup occurs at D ~ 25 fm
~3 MeV
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Model: Continuum-Discretized
Coupled-ChannelsAn extension of coupled channels technique to allow the
treatment of couplings to unbound states, both resonances and
non-resonant continuum. It was first developed to describe the
effect of breakup couplings on deuteron elastic scattering.
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CDCC in action
Dot-dashed: no dipole couplings
Dashed: no couplings to the continuum
L. Acosta et al.
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Effect of breakup on el. scattering,
summary
Coupling to the continuum is clearly
observed in experiments. It affects
seriously the elastic scattering cross
section and contributes to the
generation of analysing powers
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Coupling with reaction channelsCoupled-Reaction-Channels method
K. Zerva et al. PRC82,
044607
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El. scatt. and coupling with reaction
channels
?
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6Li+18O el. scattering - summary
↓
↑
K. Rusek et al. PRC 91, 044612 (2015)
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6He+206Pb el. scattering
L. Standylo et al. PRC 87,064603
Coupling
effects
make 6He
look larger.
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Effect of transfer on el. scattering,
summary
For the cross section, effect of transfer on the
elastic scattering is opposite to that of breakup. It
is especially strong at backward angles.
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Effect on fusion
CDCC and CRC models are well suited to
calculate direct reactions while fusion
cross section is calculated by means of
simple potential models, like Wong model.
Thus, in order to study an effect of direct
reactions on fusion one has to find how
the direct reactions affect the effective
nucleus-nucleus potential.
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Dynamic Polarization Potential
V = Vo + i W + DPP
High energy exp.
Low energy exp.
From CDCC, CRC calculations
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Fusion – an enhancement below the
Coulomb barrier
6He – EPJA 47 111; PRL81 4580
6Li – PRC68 044605; PRC66 041602
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Effect on fusion, summary
Direct reaction channels (breakup,
transfer) may significantly affect the
fusion cross section with respect to the
predictions based on a simple potential
model (e.g. enhance the fusion c.s.
below the Coulomb barrier and
suppress it above).
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Effect on the Coulomb barrier
distribution
pro
babili
ty
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Effect on the Coulomb barrier
distributions
6Li+28Si
K. Zerva et al. PRC 82, 044607 J.P. Fernandez-Garcia et al. PRC 92, 054602
Dot-dash - no coupling
Solid – coupl. to breakup only
Dotted – coupl. to breakup and transf.
Dashed- no coupling
Solid – coupl. to breakup only
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Effect on barrier distribution,
summary
Breakup tends to broaden the barrier
distribution and to increase its average
energy while the transfer acts opposite,
similar as it was observed for elastic
scattering.
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Weakly bound light nuclei are ideal to study coupling
effects. These effects are clearly observed in
experiments measuring elastic scattering, transfer
reactions and fusion providing that the
measurements are precise. It helps, if such a study
is complex – a set of experiments devoted to
different processes. In fact there are not many data
sets existing that cover all possible reaction
channels for a given pair of scattered nuclei. Good
example of such a set is the data for 6,7Li + 28Si
collected in complementary experiments by Prof.
Athena Pakou and her team.
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7Li + 28Si
El. scattering
A. Pakou et al.
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Alpha-production c.s.
A.Pakou et al. PRC71,
064602
Open triangles and
crosses - 6He,
Other symbols – 6,7Li
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6Li exclusive breakup
A. Pakou et al. PLB
633, 691
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Reaction cross section
Triangles – theory
Symbols – el. scattering
Solid curves - experiment
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Thank you all for your attention
and for the invitation to this
meeting
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mazurian.fuw.edu.pl
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Thank you all for your attention!