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![Page 1: Polarization corrections to single-particle energies · mean-field code HFODD (v2.52k) [46], which is able to solve self-consistent equations in odd nuclei by breaking all symmetries](https://reader036.pdfslide.tips/reader036/viewer/2022071019/5fd365f500bb9b501d380ae6/html5/thumbnails/1.jpg)
Jacek Dobaczewski
1/10
Polarization corrections to
single-particle energies
Jacek DobaczewskiUniversity of Jyväskylä & University of Warsaw
FIDIPRO miniworkshop onQuasiparticle Random Phase Approximation
Jyväskylä, May 7, 2014
![Page 2: Polarization corrections to single-particle energies · mean-field code HFODD (v2.52k) [46], which is able to solve self-consistent equations in odd nuclei by breaking all symmetries](https://reader036.pdfslide.tips/reader036/viewer/2022071019/5fd365f500bb9b501d380ae6/html5/thumbnails/2.jpg)
Jacek Dobaczewski
2/10
![Page 3: Polarization corrections to single-particle energies · mean-field code HFODD (v2.52k) [46], which is able to solve self-consistent equations in odd nuclei by breaking all symmetries](https://reader036.pdfslide.tips/reader036/viewer/2022071019/5fd365f500bb9b501d380ae6/html5/thumbnails/3.jpg)
Jacek Dobaczewski
3/10
![Page 4: Polarization corrections to single-particle energies · mean-field code HFODD (v2.52k) [46], which is able to solve self-consistent equations in odd nuclei by breaking all symmetries](https://reader036.pdfslide.tips/reader036/viewer/2022071019/5fd365f500bb9b501d380ae6/html5/thumbnails/4.jpg)
Jacek Dobaczewski
4/10
Self-interaction
RPA: Self-interaction free
![Page 5: Polarization corrections to single-particle energies · mean-field code HFODD (v2.52k) [46], which is able to solve self-consistent equations in odd nuclei by breaking all symmetries](https://reader036.pdfslide.tips/reader036/viewer/2022071019/5fd365f500bb9b501d380ae6/html5/thumbnails/5.jpg)
Jacek Dobaczewski
5/10
![Page 6: Polarization corrections to single-particle energies · mean-field code HFODD (v2.52k) [46], which is able to solve self-consistent equations in odd nuclei by breaking all symmetries](https://reader036.pdfslide.tips/reader036/viewer/2022071019/5fd365f500bb9b501d380ae6/html5/thumbnails/6.jpg)
Jacek Dobaczewski
6/10
![Page 7: Polarization corrections to single-particle energies · mean-field code HFODD (v2.52k) [46], which is able to solve self-consistent equations in odd nuclei by breaking all symmetries](https://reader036.pdfslide.tips/reader036/viewer/2022071019/5fd365f500bb9b501d380ae6/html5/thumbnails/7.jpg)
Jacek Dobaczewski
7/10
![Page 8: Polarization corrections to single-particle energies · mean-field code HFODD (v2.52k) [46], which is able to solve self-consistent equations in odd nuclei by breaking all symmetries](https://reader036.pdfslide.tips/reader036/viewer/2022071019/5fd365f500bb9b501d380ae6/html5/thumbnails/8.jpg)
Jacek Dobaczewski
8/10
Conclusions
![Page 9: Polarization corrections to single-particle energies · mean-field code HFODD (v2.52k) [46], which is able to solve self-consistent equations in odd nuclei by breaking all symmetries](https://reader036.pdfslide.tips/reader036/viewer/2022071019/5fd365f500bb9b501d380ae6/html5/thumbnails/9.jpg)
Jacek Dobaczewski
9/10
m=p’
p
m=p’
w
m=p’
h
m=p’
w
Particle-vibration coupling (PVC)
![Page 10: Polarization corrections to single-particle energies · mean-field code HFODD (v2.52k) [46], which is able to solve self-consistent equations in odd nuclei by breaking all symmetries](https://reader036.pdfslide.tips/reader036/viewer/2022071019/5fd365f500bb9b501d380ae6/html5/thumbnails/10.jpg)
Jacek Dobaczewski
10/10
-792.5
-792.0
-791.5
0.5 1.5 2.5 3.5 4.5 5.5
En
erg
y (
Me
V)
Eproj
EHF
m
h11/2
?????????????????????
![Page 11: Polarization corrections to single-particle energies · mean-field code HFODD (v2.52k) [46], which is able to solve self-consistent equations in odd nuclei by breaking all symmetries](https://reader036.pdfslide.tips/reader036/viewer/2022071019/5fd365f500bb9b501d380ae6/html5/thumbnails/11.jpg)
Jacek Dobaczewski
11/10
Thank you
