Giant Dipole Resonance â tool for hot nuclei studies Giant Dipole ...
Giant Dipole Resonance â tool for hot nuclei studies Giant Dipole ...
Giant Dipole Resonance â tool for hot nuclei studies Giant Dipole ...
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LSD calculations<br />
thermal shape<br />
fluctuations +<br />
Coriolis splitting<br />
P(β,γ) ∝ exp(-F(b,g)/T)<br />
46<br />
Ti<br />
β 2<br />
sin(γ+30 o )<br />
γ = 60 o<br />
0.75<br />
0.50<br />
0.25<br />
0.00<br />
0.0<br />
0.5<br />
γ = 0 o<br />
I = 24<br />
1.0<br />
β 2<br />
cos(γ+30 o )<br />
γ = 60 o<br />
0.75<br />
0.50<br />
0.25<br />
1.5<br />
0.00<br />
0.0<br />
γ = 0 o<br />
I = 28 - 34<br />
1.0<br />
0.5<br />
β 2<br />
cos(γ+30 o )<br />
1.5<br />
f<br />
av<br />
GDR<br />
∫∫<br />
−F(<br />
T,<br />
I;<br />
γ γ<br />
T I f β γ ω e<br />
β , )/ T ( I;<br />
= β , ) 4<br />
( , ) ( , , )<br />
β sin(3 γ)<br />
dβdγ<br />
GDR<br />
Jacobi shape transition and<br />
indicated <strong>for</strong> the first time<br />
Coriolis effect<br />
[a. u.]<br />
Y γ<br />
Exp. LSD (I = 28-34) LSD (I = 24)<br />
with Coriolis<br />
A. Maj et al., Nucl. Phys. A731, 319c (2004)<br />
0 5 10 15 20 25 30 35<br />
E [MeV] γ<br />
Maria Kmiecik<br />
International Workshop on Acceleration and Applications of Heavy Ions, Warszawa 2011
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