<em>Ab initio</em> many-body perturbation theory and no-core shell model

B. S. Hu; Q. Wu; F. R. Xu

doi:10.1088/1674-1137/41/10/104101

Chinese Physics C> 2017, Vol. 41> Issue(10) : 104101 DOI: 10.1088/1674-1137/41/10/104101

Ab initio many-body perturbation theory and no-core shell model

1.
State Key Laboratory of Nuclear Physics and Technology, School of Physics, Peking University, Beijing 100871, China

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Abstract：
In many-body perturbation theory (MBPT) we always introduce a parameter N_shell to measure the maximal allowed major harmonic-oscillator (HO) shells for the single-particle basis, while the no-core shell model (NCSM) uses N_max hΩ HO excitation truncation above the lowest HO configuration for the many-body basis. It is worth comparing the two different methods. Starting from "bare" and Okubo-Lee-Suzuki renormalized modern nucleon-nucleon interactions, NNLO_opt and JISP16, we show that MBPT within Hartree-Fock bases is in reasonable agreement with NCSM within harmonic oscillator bases for ⁴He and ¹⁶O in "close" model space. In addition, we compare the results using "bare" force with the Okubo-Lee-Suzuki renormalized force.
- MBPT ,
- NCSM ,
- Okubo-Lee-Suzuki ,
- nuclear force

References

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B. S. Hu, Q. Wu and F. R. Xu. Ab initio many-body perturbation theory and no-core shell model[J]. Chinese Physics C, 2017, 41(10): 104101. doi: 10.1088/1674-1137/41/10/104101

B. S. Hu, Q. Wu and F. R. Xu. Ab initio many-body perturbation theory and no-core shell model[J]. Chinese Physics C, 2017, 41(10): 104101. doi: 10.1088/1674-1137/41/10/104101 shu

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Received: 2017-05-16

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Supported by National Key Basic Research Program of China (2013CB834402), National Natural Science Foundation of China (11235001, 11320101004, 11575007) and the CUSTIPEN (China-U.S. Theory Institute for Physics with Exotic Nuclei) funded by the U.S. Department of Energy, Office of Science (DE-SC0009971)

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沈阳化工大学材料科学与工程学院沈阳 110142

Ab initio many-body perturbation theory and no-core shell model

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