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NSR database version of April 27, 2024.

Search: Author = M.H.Mun

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2023MU15      Eur.Phys.J. A 59, 149 (2023)

M.-H.Mun, I.J.Shin, W.-G.Paeng, M.Harada, Y.Kim

Nuclear structure in parity doublet model

doi: 10.1140/epja/s10050-023-01064-x
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2023ZH15      Phys.Rev. C 107, L041303 (2023)

K.Y.Zhang, P.Papakonstantinou, M.-H.Mun, Y.Kim, H.Yan, X.-X.Sun

Collapse of the N=28 shell closure in the newly discovered ³⁹Na nucleus and the development of deformed halos towards the neutron dripline

NUCLEAR STRUCTURE ³⁹Na; calculated S(n), single-neutron levels, J, π, quadrupole deformation, rms radius. ^{31,33,35,37,39,41}Na; calculated neutron density distributions. Pointed that ³⁹Na could be single nucleus with the coexistence of several exotic structures, including the quenched N=28 shell closure, Borromean structure, deformed halo, and between the core and the halo. Discussed the microscopic mechanisms behind the shape decoupling phenomenon and the development of halos towards dripline. Deformed relativistic Hartree-Bogoliubov theory in continuum.

doi: 10.1103/PhysRevC.107.L041303
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2023ZH35      Phys.Lett. B 844, 138112 (2023)

K.Y.Zhang, S.Q.Yang, J.L.An, S.S.Zhang, P.Papakonstantinou, M.-H.Mun, Y.Kim, H.Yan

Missed prediction of the neutron halo in ³⁷Mg

NUCLEAR STRUCTURE ^35,36,37Mg; calculated neutron density distributions, single-neutron energies, occupation probabilities using a microscopic and self-consistent way using the deformed relativistic Hartree-Bogoliubov theory in continuum; deduced the deformed p-wave halo characteristics of ³⁷Mg.

doi: 10.1016/j.physletb.2023.138112
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2022CH07      Phys.Rev. C 105, 024306 (2022)

Y.-B.Choi, C.-H.Lee, M.-H.Mun, Y.Kim

Bubble nuclei with shape coexistence in even-even isotopes of Hf to Hg

NUCLEAR STRUCTURE ^{152,154,156,158,160,162,164,166,168,170,172,174,176,178,180,182,184,186,188,190,192,194,196,198,200,202,204,206,208,210,212,214,216,218,220,222,224,226,228,230,232,234,236,238,240,242,244,246,248,250,252,254,256}Hf, ^{156,158,160,162,164,166,168,170,172,174,176,178,180,182,184,186,188,190,192,194,196,198,200,202,204,206,208,210,212,214,216,218,220,222,224,226,228,230,232,234,236,238,240,242,244,246,248,250,252,254,256,258}W, ^{162,164,166,168,170,172,174,176,178,180,182,184,186,188,190,192,194,196,198,200,202,204,206,208,210,212,214,216,218,220,222,224,226,228,230,232,234,236,238,240,242,244,246,248,250,252,254,256,258,260}Os, ^{170,172,174,176,178,180,182,184,186,188,190,192,194,196,198,200,202,204,206,208,210,212,214,216,218,220,222,224,226,228,230,232,234,236,238,240,242,244,246,248,250,252,254,256,258,260,262}Pt, ^{172,174,176,178,180,182,184,186,188,190,192,194,196,198,200,202,204,206,208,210,212,214,216,218,220,222,224,226,228,230,232,234,236,238,240,242,244,246,248,250,252,254,256,258,260,262,264}Hg; calculated quadrupole deformation parameters. ²⁵⁶Hf, ²⁵⁸W, ²⁶⁰Os, ²⁵⁶W; calculated neutron, proton and total nuclear densities. ^196,208Os; calculated single-particle energy levels, J, π. ^198,200,256Hf; calculated proton single-particle levels around the Fermi surface. Discussed the bubble structure and shape coexistence. Calculations based on deformed relativistic Hartree-Bogoliubov theory in continuum (DRHBc) and relativistic continuum Hartree-Bogoliubov (RCHB) theory with spherical symmetry. Comparison with experimenatal values.

doi: 10.1103/PhysRevC.105.024306
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2022KI10      Phys.Rev. C 105, 034340 (2022)

S.Kim, M.-H.Mun, M.K.Cheoun, E.Ha

Shape coexistence and neutron skin thickness of Pb isotopes by the deformed relativistic Hartree-Bogoliubov theory in continuum

NUCLEAR STRUCTURE ^{178,180,182,184,186,188,190,192,194,196,198,200,202,204,206,208,210,212,214}Pb; calculated neutron pairing gaps. ^{172,174,176,178,180,182,184,186,188,190,192,194,196,198,200,202,204,206,208,210,212,214,216,218,220,222,224,226,228,230,232,234,236,238,240,242,244,246,248,250,252,254,256,258,260,262,264,266,268,270,272,274,276,278,260,282,284,286,288,290,292,294,296,298,300,302}Pb; calculated deformation parameter by the minimum of the total binding energy. ^{182,184,186,188,208}Pb; calculated neutron single-particle energies for various shape coexistence cases - oblate, spherical, prolate. ^{180,182,184,186,188,190,192,194,196,198,200,202,204,206,208,210,212,214,216,218}Pb; calculated total binding energy dependence on the deformation.^266,268,278Pb; calculated neutron single-particle states occupation probabilities. ^{260,262,264,266,268,270,272,274,276,278,260,282,284,286,288,290,292,294,296,298,300,302,304}Pb; calculated S(2n), Fermi energies, deformation parameters. ²⁰⁸Pb; calculated proton and netron density distributions. ^{174,176,178,180,182,184,186,188,190,192,194,196,198,200,202,204,206,208,210,212,214,216,218,220,222,224,226,228,230,232,234,236,238,240,242,244,246,248,250,252,254,256,258,260,262,264,266}Pb; calculated proton and neutron radii, neutron skin thickness. Deformed relativistic Hartree-Bogoliubov theory in continuum (DRHBc). Comparison to available experimental data.

doi: 10.1103/PhysRevC.105.034340
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2020MU05      Phys.Rev. C 101, 044602 (2020)

M.-H.Mun, K.Kwak, G.G.Adamian, N.V.Antonenko

Possible production of neutron-rich No isotopes

NUCLEAR REACTIONS ^{248,249,250,251}Cf, ²⁵⁴Es(³⁶S, X), (⁴⁰Ar, X), (⁴⁸Ca, X), (⁵⁰Ti, X), ²⁵⁸No/²⁵⁹No/²⁶⁰No/²⁶¹No/²⁶²No/²⁶³No/²⁶⁴No/²⁶⁵No/²⁶⁶No, E(cm)=150-230 MeV; ^249,250,251Cf, (⁴⁸Ca, X), Q=48-70 MeV; ²⁵⁴Es(³⁶S, X), (⁴⁰Ar, X), (⁴⁸Ca, X), (⁵⁰Ti, X), Q=30-55 MeV; calculated production σ(E) in zero-neutron and one-neutron evaporation channels. Comparison of production yields of No and Md isotopes. Dinuclear system (DNS) model.

doi: 10.1103/PhysRevC.101.044602
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2019MU09      Phys.Rev. C 99, 054627 (2019)

M.-H.Mun, K.Kwak, G.G.Adamian, N.V.Antonenko

Possible production of neutron-rich Md isotopes in multinucleon transfer reactions with Cf and Es targets

NUCLEAR REACTIONS ²⁵⁴Es(¹⁴C, X)²⁵⁸Md/²⁵⁹Md/²⁶⁰Md/²⁶¹Md/²⁶²Md, E(cm)=60-80 MeV; ²⁵⁴Es(¹⁸O, X)²⁵⁸Md/²⁵⁹Md/²⁶⁰Md/²⁶¹Md/²⁶²Md, E(cm)=80-95 MeV; ²⁵⁴Es(²²Ne, X)²⁵⁸Md/²⁵⁹Md/²⁶⁰Md/²⁶¹Md/²⁶²Md, E(cm)=100-120 MeV; ²⁵⁴Es(²⁶Mg, X)²⁵⁸Md/²⁵⁹Md/²⁶⁰Md/²⁶¹Md/²⁶²Md, E(cm)=115-140 MeV; ²⁵⁴Es(³⁰Si, X)²⁵⁸Md/²⁵⁹Md/²⁶⁰Md/²⁶¹Md/²⁶²Md, E(cm)=130-160 MeV; ²⁵⁴Es(³⁶S, X)²⁵⁸Md/²⁵⁹Md/²⁶⁰Md/²⁶¹Md/²⁶²Md, E(cm)=155-165 MeV; ²⁵⁴Es(⁴⁰Ar, X)²⁵⁸Md/²⁵⁹Md/²⁶⁰Md/²⁶¹Md/²⁶²Md/²⁶³Md/²⁶⁴Md/²⁶⁵Md, E(cm)=170-210 MeV; ²⁵⁴Es(⁴⁰Ar, X)²⁵⁸Md/²⁵⁹Md/²⁶⁰Md/²⁶¹Md/²⁶²Md/²⁶³Md, E(cm)=210-230 MeV; ²⁴⁹Cf(⁴⁸Ca, X)²⁵⁸Md/²⁵⁹Md/²⁶⁰Md/²⁶¹Md/²⁶²Md, E(cm)=200-210 MeV; ²⁵⁰Cf(⁴⁸Ca, X)²⁵⁸Md/²⁵⁹Md/²⁶⁰Md/²⁶¹Md/²⁶²Md/²⁶³Md, E(cm)=200-210 MeV; ²⁵¹Cf(⁴⁸Ca, X)²⁵⁸Md/²⁵⁹Md/²⁶⁰Md/²⁶¹Md/²⁶²Md/²⁶³Md/²⁶⁴Md, E(cm)=195-212.5 MeV; ²⁵²Cf(⁴⁸Ca, X)²⁵⁸Md/²⁵⁹Md/²⁶⁰Md/²⁶¹Md/²⁶²Md/²⁶³Md/²⁶⁴Md/²⁶⁵Md, E(cm)=195-212.5 MeV; calculated total capture σ(E), maximal production σ(E) for zero- and one-neutron evaporation channels of multinucleon transfer reactions. Dinuclear system (DNS) model.

doi: 10.1103/PhysRevC.99.054627
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2016MU17      Eur.Phys.J. A 52, 363 (2016)

M.-Hw.Mun, G.G.Adamian, N.V.Antonenko, Y.-O.Lee

Possibilities of production of neutron-rich Md isotopes in multi-nucleon transfer reactions

NUCLEAR REACTIONS ²³⁸U(⁴⁸Ca, x)^{259,260,261,262,263}Md, E(cm)=191-197 MeV;^242,244Pu(⁴⁸Ca, x)^{259,260,261,262,263}Md, E(cm)=191-201 MeV;^245,246,248Cm(⁴⁸Ca, x)^{259,260,261,262,263}Md, E(cm)=197-205 MeV; calculated σ.

doi: 10.1140/epja/i2016-16363-y
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2015MU05      Phys.Rev. C 91, 054610 (2015)

M.-H.Mun, G.G.Adamian, N.V.Antonenko, Y.Oh, Y.Kim

Toward neutron-rich nuclei via transfer reactions with stable and radioactive beams

NUCLEAR REACTIONS ¹⁶⁰Gd, ¹⁶⁴Dy, ¹⁷⁰Er, ¹⁷⁶Yb, ¹⁸⁰Hf, ¹⁸⁶W, ¹⁹²Os, ²⁰⁴Hg, ²⁰⁸Pb, ²³²Th(⁴⁸Ca, X)⁵²Ca/⁵⁴Ca/⁵⁶Ca/⁵⁸Ca, E(cm)=150-225 MeV; ^{64,66,68,70,72,74,76,78}Ni, ^{86,88,90,92,94}Kr(¹⁶⁰Gd, X)¹⁶⁶Gd/¹⁶⁸Gd/¹⁷⁰Gd/¹⁷²Gd/¹⁷⁴Gd, E(cm)=145-260 MeV; ⁴⁸Ca, ⁵⁰Ti, ⁵⁴Cr, ⁵⁸Fe, ^{64,66,68,70,72,74,76,78}Ni, ⁷⁰Zn, ⁷⁶Ge, ⁸²Se, ^{86,88,90,92,94}Kr(¹⁶⁴Dy, X)¹⁷⁰Dy/¹⁷²Dy/¹⁷⁴Dy/¹⁷⁶Dy/¹⁷⁸Dy, E(cm)=150-260 MeV; ⁴⁸Ca, ⁵⁰Ti, ⁵⁴Cr, ⁵⁸Fe, ^{64,66,68,70,72,74,76,78}Ni, ⁷⁰Zn, ⁷⁶Ge, ⁸²Se, ^{86,88,90,92,94}Kr(¹⁷⁰Er, X)¹⁷⁶Er/¹⁷⁸Er/¹⁸⁰Er/¹⁸²Er/¹⁸⁴Er, E(cm)=150-270 MeV; ⁴⁸Ca, ⁵⁰Ti, ⁵⁴Cr, ⁵⁸Fe, ^{64,66,68,70,72,74,76,78}Ni, ⁷⁰Zn, ⁷⁶Ge, ⁸²Se, ^{86,88,90,92,94}Kr(¹⁷⁶Yb, X)¹⁸²Yb/¹⁸⁴Yb/¹⁸⁶Yb/¹⁸⁸Yb/¹⁹⁰Yb, E(cm)=160-270 MeV; ^{64,66,68,70,72,74,76,78}Ni(¹⁸⁰Hf, X)¹⁸⁶Hf/¹⁸⁸Hf/¹⁹⁰Hf/¹⁹²Hf/¹⁹⁴Hf, E(cm)=190-230 MeV; ⁴⁸Ca, ⁵⁰Ti, ⁵⁴Cr, ⁵⁸Fe, ^{64,66,68,70,72,74,76,78}Ni, ⁷⁰Zn, ⁷⁶Ge, ⁸²Se(¹⁸⁶W, X)¹⁹²W/¹⁹⁴W/¹⁹⁶W/¹⁹⁸W/²⁰⁰W, E(cm)=170-270 MeV; ⁴⁸Ca, ⁵⁰Ti, ⁵⁴Cr, ⁵⁸Fe, ^{64,66,68,70,72,74,76,78}Ni, ⁷⁰Zn, ⁷⁶Ge, ⁸²Se(¹⁹²Os, X)¹⁹⁶Os/¹⁹⁸Os/²⁰⁰Os/²⁰²Os/²⁰⁴Os, E(cm)=165-270 MeV; ⁴⁸Ca, ^{66,68,70,72,74,76,78}Ni(²⁰⁴Hg, X)²¹⁰Hg/²¹²Hg/²¹⁴Hg/²¹⁶Hg, E(cm)=192-255 MeV; ⁴⁸Ca, ^{66,68,70,72,74,76,78}Ni(²⁰⁸Pb, X)²¹⁴Pb/²¹⁶Pb/²¹⁸Pb/²²⁰Pb, E(cm)=200-268 MeV; ⁴⁸Ca, ^{66,68,70,72,74,76,78}Ni(²³²Th, X)²³⁸Th/²⁴⁰Th/²⁴²Th/²⁴⁴Th, E(cm)=199-261 MeV; calculated σ(E) for production of neutron-rich nuclei close to the neutron drip line in multi-nucleon transfer reactions. Dinuclear system (DNS) approach with synthesis through nucleon transfers and decay into two fragments.

doi: 10.1103/PhysRevC.91.054610
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2014MU02      Phys.Rev. C 89, 034622 (2014)

M.-H.Mun, G.G.Adamian, N.V.Antonenko, Y.Oh, Y.Kim

Production cross section of neutron-rich isotopes with radioactive and stable beams

NUCLEAR REACTIONS ⁴⁸Ca, ⁷⁰Zn, ⁸⁶Kr, ⁸⁸Sr(¹⁴⁴Xe, X)¹⁴⁸Xe/¹⁵⁰Xe/¹⁵²Xe, E(cm)=130-240 MeV; ⁴⁸Ca(¹³⁴Te, X), (¹³⁶Te, X)¹³⁶Te/¹³⁸Te/¹⁴⁰Te/¹⁴²Te, E(cm)=120-170 MeV; ^68,70Zn(¹⁴²Xe, X), (¹⁴⁴Xe, X)⁸²Zn/⁸⁴Zn/⁸⁶Zn, E(cm)=160-195 MeV; ⁴⁸Ca(¹³⁴Te, X), (¹³⁶Te, X)⁵²Ca/⁵⁴Ca/⁵⁶Ca/⁵⁸Ca/⁶⁰Ca, E(cm)=125-165 MeV; ¹⁹⁸Pt(⁴⁸Ca, X), (⁵⁰Ti, X), (⁵⁴Cr, X), (⁵⁸Fe, X), (⁶⁴Ni, X), (⁷⁰Zn, X), (⁷⁶Ge, X)²⁰²Pt/²⁰⁴Pt/²⁰⁶Pt, E(cm)=170-270 MeV; ¹⁹⁸Pt(⁴⁸Ca, X)²⁰²Pt/²⁰³Pt/²⁰⁴Pt/²⁰⁵Pt/²⁰⁶Pt, E(cm)=170-220 MeV; ¹⁹⁸Pt(⁶⁴Ni, X), (⁶⁶Ni, X), (⁶⁸Ni, X), (⁷⁰Ni, X), (⁷²Ni, X)²⁰²Pt/²⁰⁴Pt/²⁰⁶Pt/²⁰⁸Pt/²¹⁰Pt, E(cm)=215-260 MeV; calculated production σ for neutron-rich isotopes close to the neutron drip line using stable and radioactive beams. Diffusive multinucleon transfer reaction model.

doi: 10.1103/PhysRevC.89.034622
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2011KI25      J.Korean Phys.Soc. 59, 1023s (2011)

H.Il.Kim, D.H.Kim, Y.-O.Lee, M.Mun

Nuclear Data Evaluations for Silicon Isotopes Induced by Proton, Deuteron and Alpha

NUCLEAR REACTIONS ^28,29,30Si(p, p'), (d, d'), (α, α'), E=0-200 MeV; calculated, evaluated σ; ²⁸Si(p, p), E=5.93, 17.7, 28.4, 40.2, 51.9, 65, 80, 100, 179 MeV;²⁹Si(p, p), E=10, 40, 80 MeV;³⁰Si(p, p), E=40.8, 180 MeV;²⁸Si(d, d), E=7, 11, 13, 17.9, 29.5, 52, 56 MeV;²⁹Si(d, d), E=10, 12.3 MeV;³⁰Si(d, d), E=10, 11.8, 12.3, 17 MeV;²⁸Si(α, α'), E=5.96, 27, 40, 104, 120, 166 MeV;²⁹Si(α, α'), E=26.3, 28, 41 MeV;³⁰Si(α, α'), E=26.6, 27, 41 MeV; calculated, evaluated σ(θ). TALYS code. Calculations compared to data.

doi: 10.3938/jkps.59.1023
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Note: The following list of authors and aliases matches the search parameter M.H.Mun: , M.H.MUN