ning wang 1, min liu 1, xi-zhen wu 2, jie meng 3 isospin effects in nuclear mass models nuclear...
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Ning Wang1, Min Liu1, Xi-Zhen Wu2, Jie Meng3
Isospin effects in nuclear mass models
Nuclear Structure and Related Topics (NSRT15), 2015.7.14-18, DUBNA
1 Guangxi Normal University, Guilin, China2 China Institute of Atomic Energy, Beijing, China3 Peking University, Beijing, China
Introduction Weizsaecker-Skyrme mass formula Shell gaps and symmetry energy coefficients Summary
N. Wang, M. Liu, X. Z. Wu, J. Meng, Phys. Lett. B 734, 215 (2014)
Super-heavy nuclei
r-process 、symmetry energy
known masses: 2438unmeasured ~ 4000
Nuclear mass models play an important role for the study of super-heavy nuclei, nuclear astrophysics, and nuclear symmetry energy. Popular mass models with rms error of ~300-600keV
Yu. Oganessian. SKLTP/CAS - BLTP/JINR July 16, 2014, Dubna
neutrons →
1. Central position of the island for SHE ?
N. Wang, M. Liu, X. Wu, PRC 82 (2010) 044304
Courtesy of Qiu-Hong Mo
Why is the difference so large for neutron-rich nuclei ?
Macro-micro concept & Skyrme energy density functional
Liquid drop Deformation Shell Residual
Residual : Mirror 、 pairing 、 Wigner corrections...
PRC81-044322 ; PRC82-044304 ; PRC84-014333
Skyrme EDF plus extended Thomas-Fermi approach,significantly reduces CPU time
Parabolic approx. for the deformation energies
Shell corrections
symmetry potential
Deformed Woods-Saxon potential
Isospin dependence of model parameters
1. Symmetry energy coefficient
2. Symmetry potential
3. Strength of spin-orbit potential
4. Pairing corr. term
symmetry potential
WS3 : Phys.Rev.C84_014333
5. Isospin dependence of surface diffuseness
N. Wang, M. Liu, X. Z. Wu, and J. Meng, Phys. Lett. B 734 (2014) 215
Rms (keV)
FRDM HFB24 WS WS4
To known masses 654 549 525 298
Number of model para. 31 30 13 18
9 y 13 y 4 yRm
s e
rro
r
Predictive power for new masses AME2012
rmsD (in keV) WS3 FRDM DZ28 HFB17
sigma (M)2149 336 656 360 581
sigma (M)219 424 765 673 648
M(WS3) – M(exp.)
For new masses after 2012
Xu and Qi, Phys. Lett. B724 (2013) 247
KSO = -1 KSO = 1
WS4, Phys. Lett. B 734 (2014) 215
FRDM
WS*
Wienholtz, et al., Nature 498 (2013)346
New magic numbers
Mo, Liu, Wang, Phys. Rev. C 90, 024320 (2014)
Shell structure in heavy and super-heavy nuclei
108
142 152 162
Kowal,et al., Phys. Rev. C 82_014303
H. F. Zhang, et al., Phys. Rev. C 85_014325
178
WS*
162
Symmetry energy coefficients of nuclei
Parabolic law for drip line nuclei?
Liu, Wang, Li, Zhang, Phys. Rev. C 82_064306
Symmetry energy coefficients of finite nuclei from Skryme energy density functional + ETF
N. Wang, M. Liu, H. Jiang, J. L. Tian, Y. M. Zhao, Phys. Rev. C 91, 044308 (2015)
Inspired by the Skyrme energy-density functional, we propose a new
macro-micro mass formula with an rms error of 298 keV, considering the
isospin dependence of model parameters.
The shell gaps from WS formula indicate that N=32 could be new magic
number in neutron-rich region, and N=142, 152, 162, 178;
Z=92, 100, 108, 120 could be sub-shell closure in super-heavy region.
The symmetry energy coefficients of nuclei are extracted from nuclear
masses and Skyrme energy density functional. The opposite values for the
coefficient of I^4 term used in the HFB17 and WS4 models may result in
the large difference at the predictions of the masses of neutron-rich nuclei.
Summary
Thank you for your attention
Codes & Nuclear mass tables :www.ImQMD.com/mass
Guilin, China
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Quadrupole Deformations
Prolate
Oblate
Mo, Liu, Wang , Phys. Rev. C 90, 024320 (2014)
原子核壳能隙可以给出子壳信息
Volume term
Surface energy term
Coulomb energy term
Symmetry energy term
Nuclear surface diffuseness results in the deformation energies being complicated
Isospin dependence of the surface diffuseness Deformation dependence of the symmetry energy coefficients of nuclei
Skyrme energy density functional + ETF2
Mo, Liu, Chen, Wang, Sci. China Phys. Mech. & Astron. 58 (2015) 082001
Nuclear deformations
Prolate
Oblate
N. Wang, T. Li, Phys. Rev. C88, 011301(R)
Rms charge radii
RMF: Lalazissis, Raman, and Ring, At. Data Nucl. Data Tables 71, 1 (1999)