shell-model calculations of psd -shell nuclei furong xu school of physics, peking university
DESCRIPTION
Shell-model calculations of psd -shell nuclei Furong Xu School of Physics, Peking University. Introduction Shell-model calculations The role of nn interaction and configuration mixing in N=14 and 1 6 shell evolutions; - PowerPoint PPT PresentationTRANSCRIPT
![Page 1: Shell-model calculations of psd -shell nuclei Furong Xu School of Physics, Peking University](https://reader035.vdocument.in/reader035/viewer/2022070422/5681639e550346895dd4985c/html5/thumbnails/1.jpg)
Shell-model calculations of psd-shell nuclei Furong Xu
School of Physics, Peking University
I. Introduction
II. Shell-model calculations
1. The role of nn interaction and configuration mixing in
N=14 and 16 shell evolutions;
2. Increase model space with fitting a new effective
interaction
III. Summary
![Page 2: Shell-model calculations of psd -shell nuclei Furong Xu School of Physics, Peking University](https://reader035.vdocument.in/reader035/viewer/2022070422/5681639e550346895dd4985c/html5/thumbnails/2.jpg)
I. Introduction
N=16
N=14
T. Otsuka et al., PRL 105, 032501 (2010)
![Page 3: Shell-model calculations of psd -shell nuclei Furong Xu School of Physics, Peking University](https://reader035.vdocument.in/reader035/viewer/2022070422/5681639e550346895dd4985c/html5/thumbnails/3.jpg)
8
6 6
16
14
8
0d3/2
0d5/2
0d3/2
0p3/20p3/2
0p1/2
1s1/21s1/2
0d5/2
0p1/2
proton neutron
2+
2+
![Page 4: Shell-model calculations of psd -shell nuclei Furong Xu School of Physics, Peking University](https://reader035.vdocument.in/reader035/viewer/2022070422/5681639e550346895dd4985c/html5/thumbnails/4.jpg)
R.V.F. Janssens, Nature 459, 1069 (2009)
R. Kanungo et al., PRL 102, 152501 (2009)
C.R. Hoffman et al., PLB 672, 17 (2009)
Shell-model calculations are very dependent on interactions used!
Doubly magic nature of 24O
![Page 5: Shell-model calculations of psd -shell nuclei Furong Xu School of Physics, Peking University](https://reader035.vdocument.in/reader035/viewer/2022070422/5681639e550346895dd4985c/html5/thumbnails/5.jpg)
T. Otsuka et al., PRL 105, 032501 (2010)
8
6 6
1614
8
0d3/2
0d5/2
0d3/2
0p3/20p3/2
0p1/2
1s1/21s1/2
0d5/2
0p1/2
proton neutron
Experiments: 0d3/2 neutrons unbound in C, N, O
0d3/2
1s1/2
C.R. Hoffman et al., PRL 100, 152502 (2008)
Unbound
![Page 6: Shell-model calculations of psd -shell nuclei Furong Xu School of Physics, Peking University](https://reader035.vdocument.in/reader035/viewer/2022070422/5681639e550346895dd4985c/html5/thumbnails/6.jpg)
II. Shell-model calculations
1. N=14 and 16 shell closures
Otsuka et al., PRL 87, 082502 (2001).
C.X. Yuan, C. Qi, F.R. Xu, NPA 883, 25 (2012)
![Page 7: Shell-model calculations of psd -shell nuclei Furong Xu School of Physics, Peking University](https://reader035.vdocument.in/reader035/viewer/2022070422/5681639e550346895dd4985c/html5/thumbnails/7.jpg)
+ =0+
+ =2+
core coreV j=0= -2.82MeV V j=0= -2.12MeV
core coreV j=2= -1.00MeV V j=2= -0.82MeV
Interaction matrix elements of couplings Vj=0 and Vj=2
![Page 8: Shell-model calculations of psd -shell nuclei Furong Xu School of Physics, Peking University](https://reader035.vdocument.in/reader035/viewer/2022070422/5681639e550346895dd4985c/html5/thumbnails/8.jpg)
8
6 6
16
14
8
0d3/2
0d5/2
0d3/2
0p3/20p3/2
0p1/2
1s1/2 1s1/2
0d5/2
0p1/2
proton neutron
repulsive tensor
repulsive spin-orbit
attractive tensor
The neutron-proton interaction reduced when going from oxygen to carbon
attractive 5/2 5/2
nnd dV
T. Otsuka et al., PRL 95, 232502 (2005)
![Page 9: Shell-model calculations of psd -shell nuclei Furong Xu School of Physics, Peking University](https://reader035.vdocument.in/reader035/viewer/2022070422/5681639e550346895dd4985c/html5/thumbnails/9.jpg)
attractive , important!
22O: small effect
20C: big (1s1/2 and 0d5/2 degenerate)
1/2 1/2
nns sV
6 6
16
14
8
0d3/2
0p3/20p3/2
0p1/2
1s1/2
0d5/2
0p1/2
proton neutron
repulsiv
e LS
attractive tensor8
C.X. Yuan, C. Qi, F.R. Xu, NPA 883, 25 (2012)
![Page 10: Shell-model calculations of psd -shell nuclei Furong Xu School of Physics, Peking University](https://reader035.vdocument.in/reader035/viewer/2022070422/5681639e550346895dd4985c/html5/thumbnails/10.jpg)
C, N, O wave-function analysis for g.s.
core
coreN=14
N=14
Excited configurations are more important in C isotopes
![Page 11: Shell-model calculations of psd -shell nuclei Furong Xu School of Physics, Peking University](https://reader035.vdocument.in/reader035/viewer/2022070422/5681639e550346895dd4985c/html5/thumbnails/11.jpg)
p n
16
14
14
16
![Page 12: Shell-model calculations of psd -shell nuclei Furong Xu School of Physics, Peking University](https://reader035.vdocument.in/reader035/viewer/2022070422/5681639e550346895dd4985c/html5/thumbnails/12.jpg)
+3/2+ 3/2+
core core
N=11 isotones: 5/2+, 3/2+ inversion related to N=14 shell
![Page 13: Shell-model calculations of psd -shell nuclei Furong Xu School of Physics, Peking University](https://reader035.vdocument.in/reader035/viewer/2022070422/5681639e550346895dd4985c/html5/thumbnails/13.jpg)
From Paul Fallon at LBNL
![Page 14: Shell-model calculations of psd -shell nuclei Furong Xu School of Physics, Peking University](https://reader035.vdocument.in/reader035/viewer/2022070422/5681639e550346895dd4985c/html5/thumbnails/14.jpg)
Carbon
WBT
(2009): Z. Elekes et al., PRC 79, 011302 (R)
(2011): M. Petri et al., PRL 107, 102501
Calculation is sensitive to effective charges used.
![Page 15: Shell-model calculations of psd -shell nuclei Furong Xu School of Physics, Peking University](https://reader035.vdocument.in/reader035/viewer/2022070422/5681639e550346895dd4985c/html5/thumbnails/15.jpg)
21( 2; )2 1i f p p n n
i
B E j j e A e Aj
Ap, An: shell-model quadrupole transition matrix elements.
![Page 16: Shell-model calculations of psd -shell nuclei Furong Xu School of Physics, Peking University](https://reader035.vdocument.in/reader035/viewer/2022070422/5681639e550346895dd4985c/html5/thumbnails/16.jpg)
C isotopes
The effective charges taken from: H. Sagawa et al., PRC 70, 054316 (2004)
![Page 17: Shell-model calculations of psd -shell nuclei Furong Xu School of Physics, Peking University](https://reader035.vdocument.in/reader035/viewer/2022070422/5681639e550346895dd4985c/html5/thumbnails/17.jpg)
The gap is reduced with increasing neutrons on 0d5/2.
This increases the proton excitation.
WBT0hω
attractive tensor
![Page 18: Shell-model calculations of psd -shell nuclei Furong Xu School of Physics, Peking University](https://reader035.vdocument.in/reader035/viewer/2022070422/5681639e550346895dd4985c/html5/thumbnails/18.jpg)
Generally agree well, but still model dependent!
1. Increase model space;
2. Improve interaction.
![Page 19: Shell-model calculations of psd -shell nuclei Furong Xu School of Physics, Peking University](https://reader035.vdocument.in/reader035/viewer/2022070422/5681639e550346895dd4985c/html5/thumbnails/19.jpg)
Our new effective interaction for 0-2 hω
![Page 20: Shell-model calculations of psd -shell nuclei Furong Xu School of Physics, Peking University](https://reader035.vdocument.in/reader035/viewer/2022070422/5681639e550346895dd4985c/html5/thumbnails/20.jpg)
N=11 isotones
![Page 21: Shell-model calculations of psd -shell nuclei Furong Xu School of Physics, Peking University](https://reader035.vdocument.in/reader035/viewer/2022070422/5681639e550346895dd4985c/html5/thumbnails/21.jpg)
III. Summary
1. The nn interaction and configuration mixing
play also important roles in shell evolutions of
N=14, 16.
2. Large model space and suitable effective
interaction are important factors as well.
![Page 22: Shell-model calculations of psd -shell nuclei Furong Xu School of Physics, Peking University](https://reader035.vdocument.in/reader035/viewer/2022070422/5681639e550346895dd4985c/html5/thumbnails/22.jpg)
Collaborators:
C.X. Yuan
C. Qi
T. Otsuka
T. Suzuki
X.B. Wang
N. Tsunoda
![Page 23: Shell-model calculations of psd -shell nuclei Furong Xu School of Physics, Peking University](https://reader035.vdocument.in/reader035/viewer/2022070422/5681639e550346895dd4985c/html5/thumbnails/23.jpg)
Thank you!
NN2012San Antonio, Texas
29 May, 2012