2020
DOI: 10.1088/1674-1137/abb4d1
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Finite particle number description of neutron matter using the unitary correlation operator and high-momentum pair methods *

Abstract: By using bare Argonne V4' (AV4'), V6' (AV6'), and V8' (AV8') nucleon-nucleon (N N) interactions respectively, the nuclear equations of state (EOSs) for neutron matter are calculated with the unitary correlation operator and high-momentum pair methods. The neutron matter is described under a finite particle number approach with magic number N = 66 under a periodic boundary condition. The central short-range correlation coming from the short-range repulsion in the N N interaction is treated by the unitary correl… Show more

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Cited by 10 publications
(10 citation statements)
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“…[16,17]. This technique has been applied to the calculations of both finite nuclei [16,17,18,20,19] and nuclear matters [21,22]. Hybridizing the TOAMD and HM-AMD methods, the "Tensor-optimized High-momentum Antisymmetrized Molecular Dynamics" (TO-HMAMD) approach is formulated, which also provides the same quality of the nuclear properties of 3 H [23] and 4 He [24] as other ab initio calculations in TOAMD or GFMC frameworks.…”
Section: Introductionmentioning
confidence: 99%
“…[16,17]. This technique has been applied to the calculations of both finite nuclei [16,17,18,20,19] and nuclear matters [21,22]. Hybridizing the TOAMD and HM-AMD methods, the "Tensor-optimized High-momentum Antisymmetrized Molecular Dynamics" (TO-HMAMD) approach is formulated, which also provides the same quality of the nuclear properties of 3 H [23] and 4 He [24] as other ab initio calculations in TOAMD or GFMC frameworks.…”
Section: Introductionmentioning
confidence: 99%
“…The symmetric nuclear matter is described by the finite particle-number approach, where the periodical boundary condition is employed for the single-nucleon wave function as φ(r) = φ(r + Lx). Under this description, the infinite nuclear matter can be divided into identical cubic boxes with finite size L. The 0p0h state of the cubic box is defined by the Slater determinant as [64,65]…”
Section: B 2p2h Excitation Modes and Total Wave Functionmentioning
confidence: 99%
“…The HM component in symmetric nuclear matter is described by introducing 2p2h excitations of nucleon pairs, which can be written as [64,65]…”
Section: B 2p2h Excitation Modes and Total Wave Functionmentioning
confidence: 99%
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