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NSR database version of April 25, 2024.

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2024ZH14      Phys.Lett. B 850, 138511 (2024)

Q.Zhao, M.Kimura, B.Zhou, S.-h.Shin

Microscopic investigation of one- and two-proton decay from the excited states of ¹⁰C

RADIOACTIVITY ¹⁰C(p), (2p), ⁹B(p); calculated decay widths with R-matrix method. Comparison with experimental data. Microscopic cluster model.

doi: 10.1016/j.physletb.2024.138511
Citations: PlumX Metrics

2023NA30      Eur.Phys.J. A 59, 249 (2023)

H.Naik, G.N.Kim, R.Schwengner, W.Jang, T.H.Nguyen, S.G.Shin, Y.Kye, R.Massarczyk, R.John, A.Junghans, A.Wagner, M.H.Cho

Measurement of the flux-weighted cross-sections for the ^natYb(γ, xn)^{175, 169, 167}Yb reactions in the Bremsstrahlung end-point energies of 12-16 MeV and 60-70 MeV

NUCLEAR REACTIONS Yb(γ, xn)¹⁷⁵Yb/¹⁶⁹Yb/¹⁶⁷Yb, ²⁷Al(γ, n2p), ¹⁹⁷Au(γ, n), E<70 MeV; measured reaction products, Eγ, Iγ; deduced flux-weighted average σ, normalised activation yields. Comparison with the EXFOR library, TALYS 1.9 calculations. The 20 MeV electron linac (ELBE) at Helmholtz-Zentrum Dresden-Rossendorf (HZDR), Dresden, Germany, and 100 MeV electron linac at the Pohang Accelerator Laboratory (PAL), Korea.

doi: 10.1140/epja/s10050-023-01137-x
Citations: PlumX Metrics

2022NA24      Eur.Phys.J. A 58, 92 (2022)

H.Naik, G.N.Kim, R.Schwengner, W.Jang, T.H.Nguyen, S.G.Shin, Y.Kye, R.Massavczyh, R.John, A.Junghans, A.Wagner, M.-H.Cho

Photo-neutron cross-section of ^natGd in the bremsstrahlung end-point energies of 12-16 MeV and 60-70 MeV

NUCLEAR REACTIONS Gd(γ, xn)¹⁵⁹Gd/¹⁵³Gd, E<70 MeV; measured reaction products, Eγ, Iγ; deduced spectrum-averaged σ. Comparison with TALYS-1.9 calculations. The 20 MeV electron linac (ELBE) at HZDR, Dresden, Germany, and 100 MeV electron linac at Pohang Accelerator Laboratory, Korea.

doi: 10.1140/epja/s10050-022-00736-4
Citations: PlumX Metrics

2022ZH11      Eur.Phys.J. A 58, 25 (2022)

Q.Zhao, B.Zhou, M.Kimura, H.Motoki, S.-h.Shin

Microscopic calculations of ⁶He and ⁶Li with real-time evolution method

NUCLEAR STRUCTURE ⁶He, ⁶Li; calculated low-lying cluster states, J, π, rms radii by the real-time evolution method (REM) which generates basis wave functions for the generator coordinate method (GCM) from the equation of motion of Gaussian wave packets.

doi: 10.1140/epja/s10050-021-00648-9
Citations: PlumX Metrics

2022ZH64      Phys.Rev. C 106, 054313 (2022)

Q.Zhao, M.Kimura, B.Zhou, S.-h.Shin

α-formation probability in ¹⁰Be and ¹²Be within a microscopic cluster model

NUCLEAR STRUCTURE ^4,6,8He, ^10,12Be; calculated ground state energy. ^10,12Be; calculated rms radii of point neutron and proton distributions, charge radius, reduced width amplitude, spectroscopic factors. Calculations within the framework of generator coordinates method (GCM) with the real-time evolution method (REM) where the equation of motion of the Gaussian wave packets is used to generate basis wave functions, with various cluster configurations. Comparison with experimental data and other theoretical calculations.

doi: 10.1103/PhysRevC.106.054313
Citations: PlumX Metrics

2021SH20      Phys.Rev. C 103, 054313 (2021)

S.Shin, B.Zhou, M.Kimura

Shape of ¹³C studied by the real-time evolution method

NUCLEAR STRUCTURE ¹³C; calculated levels, J, π, B(E2), bands based on E2 transition strengths, energies and radii of the first 1/2- and 5/2+ states, overlap between REM wave function and the basis wave function for 1/2- and 1/2+ states, density distributions of the basis wave functions for 1/2- and 1/2+ states; deduced the ground band as a rigid-body rotational band manifesting triangular symmetry. Real-time evolution method (REM) using the equation-of-motion of cluster of 3α+n system without any assumption of symmetry. Comparison of level structures with the experimental data.

doi: 10.1103/PhysRevC.103.054313
Citations: PlumX Metrics

2021SH42      Few-Body Systems 62, 93 (2021)

S.Shin, B.Zhou, M.Kimura

The Isoscalar Monopole Strength of ¹³C

NUCLEAR STRUCTURE ¹³C; calculated energy levels, J, π, density distributions of the Brink-Bloch wave functions, monopole strengths, radii, extra neutron causes the shrinkage of 3α.

doi: 10.1007/s00601-021-01671-8
Citations: PlumX Metrics

2020KY01      Eur.Phys.J. A 56, 30 (2020)

Y.-u.Kye, S.-g.Shin, M.-h.Cho, W.Namkung, G.Kim, P.Schillebeeckx, C.Paradela, S.Kopecky

Resonance parameters of Gd isotopes derived from capture measurements at GELINA

doi: 10.1140/epja/s10050-020-00047-6
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 dataset23720.

2020NA15      J.Radioanal.Nucl.Chem. 324, 837 (2020)

H.Naik, G.Kim, T.H.Nguyen, K.Kim, S.-G.Shin, Y.-u.Kye, M-H.Cho

Measurement of ^natNi(γ, xn)^{57, 56}Ni and ^natNi(γ, pxn)^58-55Co reaction cross sections in bremsstrahlung with end-point energies of 65 and 75 MeV

NUCLEAR REACTIONS Ni(γ, X)⁵⁷Ni/⁵⁶Ni/⁵⁸Co/⁵⁷Co/⁵⁶Co/⁵⁵Co, E<75 MeV; measured reaction products, Eγ, Iγ; deduced σ. Comparison with TALYS nuclear model calculations, experimental data.

doi: 10.1007/s10967-020-07105-9
Citations: PlumX Metrics

2020NA36      Eur.Phys.J. A 56, 264 (2020)

H.Naik, G.N.Kim, R.Schwengner, W.Jang, N.T.Hien, K.Kim, S.G.Shin, Y.Kye, A.Junghans, A.Wagner, M.-H.Cho

Photo-neutron cross-section of ^natDy in the bremsstrahlung end-point energies of 12, 14, 16, 65, and 75 MeV

NUCLEAR REACTIONS Dy(γ, xn)¹⁵⁵Dy/¹⁵⁷Dy/¹⁵⁹Dy, E<12, 14, 16, 65, 75 MeV; measured reaction products, Eγ, Iγ; deduced flux-weighted average σ. Comparison with TALYS-1.9 calculations.

doi: 10.1140/epja/s10050-020-00268-9
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetG0079.

2020NG01      Eur.Phys.J.Plus 135, 384 (2020)

T.H.Nguyen, V.D.Nguyen, G.Kim, Y.-u.Kye, S.-G.Shin, M-H.Cho

Measurement of the thermal neutron cross section and resonance integral of the ¹⁸⁷Re(n, γ)¹⁸⁸Re reaction

NUCLEAR REACTIONS ¹⁸⁷Re(n, γ), E thermal; measured reaction products, Eγ, Iγ; deduced σ and resonance integrals. Comparison with available data.

doi: 10.1140/epjp/s13360-020-00406-8
Citations: PlumX Metrics

2020RA19      Eur.Phys.J. A 56, 235 (2020)

M.S.Rahman, K.Kim, T.H.Nguyen, G.Kim, H.Naik, S.-C.Yang, S.-G.Shin, Y.-u.Kye, M.-H.Cho

Measurement of flux-weighted average cross sections of ^natIn(γ, xn) reactions and isomeric yield ratios of ^{112mg, 111m, g, 110m, g}In with bremsstrahlung

NUCLEAR REACTIONS In(γ, xN)¹¹⁰In/¹¹¹In/¹¹²In, ¹⁹⁷Au(γ, n), E<50, 60, 70 MeV; measured reaction products, Eγ, Iγ; deduced σ, isomeric ratios. Comparison with TALYS-1.9 calculations.

doi: 10.1140/epja/s10050-020-00245-2
Citations: PlumX Metrics

2020ZH45      Eur.Phys.J. A 56, 298 (2020)

B.Zhou, M.Kimura, Q.Zhao, S.-h.Shin

Microscopic calculations for Be isotopes within real-time evolution method

NUCLEAR STRUCTURE ^9,10,12Be; calculated energy levels, J, π within the Real-time Evolution Method (REM).

doi: 10.1140/epja/s10050-020-00306-6
Citations: PlumX Metrics

2019NA29      Eur.Phys.J. A 55, 217 (2019)

H.Naik, G.Kim, M.Zaman, W.Jang, K.Kim, N.T.Hien, S.-G.Shin, Y.-uk.Kye, M.-H.Cho

Photo-neutron reaction cross-sections of ⁵⁹Co in the bremsstrahlung end-point energies of 65 and 75 MeV

doi: 10.1140/epja/i2019-12915-y
Citations: PlumX Metrics

2018HI05      Nucl.Instrum.Methods Phys.Res. B424, 37 (2018)

N.T.Hien, G.Kim, K.Kim, N.V.Do, P.D.Khue, K.T.Thanh, S.-G.Shin, M.-Hy.Cho

Measurements of the thermal neutron cross-section and resonance integral for the ¹⁰⁸Pd(n, γ)¹⁰⁹Pd reaction

NUCLEAR REACTIONS ¹⁰⁸Pd(n, γ), E thermal; measured reaction products, Eγ, Iγ; deduced σ, resonance integrals.

doi: 10.1016/j.nimb.2018.03.031
Citations: PlumX Metrics

2018SH43      Eur.Phys.J. A 54, 226 (2018)

S.G.Shin, Y.U.Kye, W.Namkung, M.H.Cho, Y.-R.Kang, M.W.Lee, G.N.Kim, T.-I.Ro, J.E.Lee, T.Katabuchi, K.Terada

Neutron capture yields and resonance parameters of dysprosium isotopes measured at Japan Proton Accelerator Research Complex

NUCLEAR REACTIONS ^{161,162,163,164}Dy(n, γ), E=0.1-300 eV; measured En using ToF method; deduced counting rates vs neutron energy; calculated counting rates using multilevel R-matrix Bayesian code SAMMY; deduced resonances, resonance parameters Γ_n, Γ_γ, yields, cumulative radiation width distribution, other parameters employing Reich-Moore approximation, considering self-shielding, multiple scattering and Doppler broadening effects. Compared with ENDF/B-VII.1 and RPI.

doi: 10.1140/epja/i2018-12653-8
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 dataset23462.

2018ZA04      Nucl.Phys. A978, 173 (2018)

M.Zaman, G.Kim, H.Naik, K.Kim, M.Shahid, M.Nadeem, S.-G.Shin, M.-H.Cho

Flux weighted average cross-sections of ^natNi(γ, x) reactions with the bremsstrahlung end-point energies of 55, 59, 61 and 65 MeV

NUCLEAR REACTIONS Ni(γ, xn), (γ, xnp), E=55, 59, 61, 65 MeV[bremsstrahlung end-point energies]; measured Eγ, Iγ using energy and efficiency-calibrated HPGe, also for ²⁷Al(γ, 2pn)²⁴Na as the monitor reaction; deduced γ-ray energy spectrum. ^55,56,57,58Co, ^56,57Ni; deduced yields, production σ; compared with published data, TALYS-1.8 calculations and TENDL-2015.

doi: 10.1016/j.nuclphysa.2018.07.017
Citations: PlumX Metrics

2017DO08      Appl.Radiat.Isot. 128, 148 (2017)

N.V.Do, P.D.Khue, K.T.Thanh, N.T.Hien, G.Kim, K.Kim, S.-G.Shin, Y.-U.Kye, M.-H.Cho

Measurement of isomeric yield ratios of ^{99m, g;101m, g;102m, g}Rh in the ^natPd(γ, pxn) reactions with the bremsstrahlung end-point energies of 50-70 MeV

NUCLEAR REACTIONS Pd(γ, XNP)⁹⁹Rh/¹⁰¹Rh/¹⁰²Rh, E<70 MeV; measured reaction products, Eγ, Iγ; deduced isomeric yield ratios. Comparison with TALYS-1.6 calculations.

doi: 10.1016/j.apradiso.2017.06.024
Citations: PlumX Metrics

2017HI01      J.Radioanal.Nucl.Chem. 311, 1559 (2017)

N.T.Hien, G.Kim, K.Kim, M.Nadeem, M.S.Rahman, N.V.Do, P.D.Khue, K.T.Thanh, S.-G.Shin, M.-H.Cho

Measurement of isomeric yield ratios for the ¹¹⁰Pd(γ, n)^{109m, g}Pd reaction

NUCLEAR REACTIONS ¹¹⁰Pd(γ, n), E<70 MeV; measured reaction products, Eγ, Iγ; deduced isomeric yield ratio.

doi: 10.1007/s10967-016-5124-7
Citations: PlumX Metrics

2017SH50      Eur.Phys.J. A 53, 203 (2017); Erratum Eur.Phys.J. A 53, 235 (2017)

S.G.Shin, Y.U.Kye, W.Namkung, M.H.Cho, Y.-R.Kang, M.W.Lee, G.N.Kim, T.-I.Ro, Y.Danon, D.Williams, G.Leinweber, R.C.Block, D.P.Barry, M.J.Rapp

Neutron capture measurements and resonance parameters of dysprosium

NUCLEAR REACTIONS Dy, ^{161,162,163,164}Dy(n, γ), E=10-1000 eV; measured Eγ, Iγ, energies of neutron resonances using NaI(Tl) multiplicity detector divided into 16 optically isolated segments at Gaerttner LINAC Center of Rensselaer Polytechnic Institute; deduced resonance parameters, Γ_n, Γ_γ, capture resonance integrals, level densities, cumulative radiation. Comparison with results in ENDF/B-VII.1 evaluation, and with Porter-Thomas distribution.

doi: 10.1140/epja/i2017-12402-7
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 dataset14514.

2017TA23      Radiochim.Acta 105, 789 (2017)

M.Tatari, H.Naik, G.Kim, K.Kim, S.-G.Shin, M.-H.Cho

Measurement of photo-neutron cross sections and isomeric yield ratios in the ⁸⁹Y(γ, xn)^89-xY reactions at the bremsstrahlung end-point energies of 65, 70 and 75 MeV

NUCLEAR REACTIONS ⁸⁹Y(γ, xn)⁸⁸Y/⁸⁷Y/⁸⁶Y/⁸⁵Y, E<75 MeV; measured reaction products, Eγ, Iγ; deduced σ, isomeric yield ratios. Comparison with experimental data, TALYS 1.6 calculations.

doi: 10.1515/ract-2016-2741
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetG3136.

2017ZA03      Nucl.Phys. A960, 22 (2017)

M.Zaman, G.Kim, H.Naik, K.Kim, Y.-S.Cho, Y.-O.Lee, S.-G.Shin, M.-H.Cho, Y.-R.Kang, M.-W.Lee

Measurement of flux-weight average cross-sections of ^natZn(γ, xn) reactions in the bremsstrahlung end-point energies of 50, 55, 60, and 65 MeV

NUCLEAR REACTIONS Zn(γ, xn), E₀=50, 55, 60, 65 MeV[bremsstrahlung end-point energy, (x=1-5)]; measured bremsstrahlung induced products using off-line γ-ray activation spectroscopic technique; deduced γ-ray spectrum, σ vs Eγ, σ vs bremsstrahlung end-point energy. Compared with data and with TENDL-2014 calculated by TALYS 1.6.

doi: 10.1016/j.nuclphysa.2017.01.008
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetG3126.

2016NA07      Nucl.Phys. A948, 28 (2016)

H.Naik, G.Kim, K.Kim, M.Zaman, A.Goswami, M.W.Lee, S.-C.Yang, Y.-O.Lee, S.-G.Shin, M.-H.Cho

Measurement of flux-weighted average cross sections for ¹⁹⁷Au(γ, xn) reactions and isomeric yield ratios of ^{196m, g}Au with bremsstrahlung

NUCLEAR REACTIONS ¹⁹⁷Au(γ, xn), E=50, 60, 70 MeV [bremsstrahlung end-point energy]; measured bremsstrahlung induced activation Eγ, Iγ; deduced flux-weighted σ vs bremsstrahlung end-point energy. ^196m,196gAu deduced isomeric σ, yields. Compared with available literature data, TENDL2014 library and published TALYS-1.6 calculations.

doi: 10.1016/j.nuclphysa.2016.01.015
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetG3122.

2016NA11      Eur.Phys.J. A 52, 47 (2016)

H.Naik, G.N.Kim, R.Schwengner, K.Kim, M.Zaman, S.C.Yang, S.G.Shin, Y.-U.Kye, R.Massarczyk, R.John, A.Junghans, A.Wagner, A.Goswami, M.-H.Cho

Measurement of isomeric ratios for ^{89g, m}Zr, ^{91g, m}Mo, and ^{97g, m}Nb in the bremsstrahlung end-point energies of 16 and 45-70 MeV

NUCLEAR REACTIONS Zr(γ, xn), Mo(γ, x), E=16, 45, 50, 55, 60, 70 MeV[bremsstrahlung end-point energy]; measured bremsstrahlung induced off-line Eγ, Iγ; deduced ^89g,89mZr, ^91g,91mMo, ^97g,97mNb isomeric σ ratios, isomeric yield ratios; calculated isomeric σ ratios using TALYS 1.6. Compared also with published data.

doi: 10.1140/epja/i2016-16047-8
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetG3121.

2016NA25      Eur.Phys.J. A 52, 195 (2016)

H.Naik, G.N.Kim, R.Capote Noy, R.Schwengner, K.Kim, M.Zaman, S.G.Shin, Y.Gey, R.Massarczyk, R.John, R.John, A.Junghans, A.Wagner, M.-H.Cho

Photo-neutron reaction cross-sections for ^natMo in the bremsstrahlung end-point energies of 12-16 and 45-70 MeV

NUCLEAR REACTIONS Mo(γ, xn)^90,91,99Mo, E=12-16, 45-70 MeV[end-point energy]; measured bremsstrahlung induced Eγ, Iγ using activation and γ-ray spectrometric technique; deduced σ (separated metastable and gs for ⁹¹Mo); calculated σ using TALYS 1.6 (complemented by some other Mo(γ, xn) reactions from literature). (Results for ⁹¹Mo of the authors already published in Eur.Phys.J. A52, p.47.)

doi: 10.1140/epja/i2016-16195-9
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetG3132.

2016NA44      Eur.Phys.J. A 52, 339 (2016)

H.Naik, G.Kim, K.Kim, M.Zaman, M.Shahid, Y.-R.Kang, M.W.Lee, S.-G.Shin, M.-H.Cho

Determination of flux-weighted average cross-sections of ^natPb(γ, xn), ²⁰⁸Pb(γ, xn), and ²⁰⁹Bi(γ, xn) reactions using bremsstrahlung end-point energies of 50-70 MeV

NUCLEAR REACTIONS Pb, ²⁰⁸Pb, ²⁰⁹Bi(γ, xn), E=50-70 MeV[bremsstrahlung end-point energy]; measured bremsstrahlung induced reaction activation and off-line Eγ, Iγ; deduced photo-neutron σ for x=3-6; calculated photo-neutron σ using TALYS 1.6. Compared with other data and published calculations.

doi: 10.1140/epja/i2016-16339-y
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetG3134.

2016RA23      Eur.Phys.J. A 52, 194 (2016)

Md.S.Rahman, K.Kim, G.Kim, H.Naik, M.Nadeem, N.T.Hien, M.Shahid, S.-C.Yang, Y.-S.Cho, Y.-O.Lee, Y.-O.Lee, S.-G.Shin, M.-H.Cho, M.W.Lee, Y.-R.Kang, G.-M.Yang, T.-I.Ro

Measurement of flux-weighted average cross-sections and isomeric yield ratios for ¹⁰³Rh(γ, xn) reactions in the bremsstrahlung end-point energies of 55 and 60 MeV

NUCLEAR REACTIONS ¹⁰³Rh(γ, xn), E=55, 60 MeV[end-point energy]; measured bremsstrahlung induced Eγ, Iγ; deduced ¹⁰³Rh(γ, xn, x=1-4) reaction flux-weighted average σ, isomeric ratios; calculated σ using TALYS 1.6. For comparison of data with calculations, present data are complemented by those of Lepretre (at lower energies).

doi: 10.1140/epja/i2016-16194-x
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetG3131.

2015KI03      Nucl.Instrum.Methods Phys.Res. B349, 141 (2015)

H.Kim, S.J.Noh, Y.-R.Kang, M.Lee, D.H.Jeong, J.K.Kim, K.Yang, T.-I.Ro, S.G.Shin, Y.U.Kye, M.-H.Cho, G.Kim

Measurement of isomeric yield ratios in the photo-production of ^{133m, g;137m, g}Ce from ^natCe using 55-, 60-, and 65-MeV bremsstrahlung

NUCLEAR REACTIONS Ce(γ, xn)¹³³Ce/¹³⁷Ce, E=55, 60, 65 MeV; measured reaction products, Eγ, Iγ; deduced isomeric yield ratios. Comparison with available data.

doi: 10.1016/j.nimb.2015.02.055
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetG3129.

2015KY01      Nucl.Instrum.Methods Phys.Res. B351, 35 (2015)

Yo.-U.Kye, S.-G.Shin, M.-H.Cho, K.S.Kim, W.Namkung, G.Kim, K.Kim, Y.-R.Kang, M.-W.Lee, S.-C.Yang, V.D.Nguyen, D.K.Pham, T.T.Kim, H.Naik

Measurement of isomeric yield ratios of ^{197m, g}Pt and ^{190m2, g+m1}Ir from the ¹⁹⁸Pt(γ, n) and ^natPt(γ, xn1p) reactions induced by 55-, 60-, and 65-MeV bremsstrahlung

NUCLEAR REACTIONS ¹⁹⁸Pt(γ, n)¹⁹⁷Pt, Pt(γ, xnp)¹⁹⁰Ir, E<65 MeV; measured reaction products, Eγ, Iγ; deduced isomeric yield ratios. Comparison with available data.

doi: 10.1016/j.nimb.2015.03.079
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetG3130.

2015NG01      Nucl.Instrum.Methods Phys.Res. B362, 9 (2015)

Nguyen Van Do, Pham Duc Khue, Kim Tien Thanh, N.T.Hien, G.Kim, K.Kim, S.-G.Shin, M.-H.Cho, M.Lee

Thermal neutron capture and resonance integral cross sections of ⁴⁵Sc

NUCLEAR REACTIONS ⁴⁵Sc(n, γ), E thermal; measured reaction products, Eγ, Iγ; deduced σ, resonance integrals. Comparison with available data.

doi: 10.1016/j.nimb.2015.08.075
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 dataset30837.

2015TA02      Nucl.Instrum.Methods Phys.Res. B344, 76 (2015)

M.Tatari, G.Kim, H.Naik, K.Kim, S.C.Yang, M.Zaman, S.G.Shin, Y.-U.Kye, M.-H.Cho

Measurement of isomeric yield ratios of ^{86m, g}Y, ^{87m, g}Y, and ^{89m, g}Zr in the photonuclear reactions of ⁸⁹Y and ^natZr at the end-point bremsstrahlung energies of 45 and 55 MeV

NUCLEAR REACTIONS ⁸⁹Y(γ, xn)⁸⁶Y/⁸⁷Y, Zr(γ, X)⁸⁹Zr, E<100 MeV; measured reaction products, Eγ, Iγ; deduced isomeric yield ratios and their uncertainties. Comparison with available data.

doi: 10.1016/j.nimb.2014.12.019
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetG3125.

2015ZA01      Eur.Phys.J. A 51, 5 (2015)

M.Zaman, G.Kim, H.Naik, K.Kim, S.-C.Yang, M.Shahid, S.-G.Shin, M.-H.Cho

Flux-weighted average cross-sections of ^natAg(γ, xn)^103-106Ag reactions with end-point bremsstrahlung energies of 45-0 MeV

NUCLEAR REACTIONS Ag(γ, xn), E=45-60 MeV (bremsstrahlung end-point energy); measured activation and off-line Eγ, Iγ using 100 MeV electron linac; deduced σ, flux-weighted σ. Compared with TENDL-2013 and data.

doi: 10.1140/epja/i2015-15005-4
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetG3114.

2014DO07      Nucl.Instrum.Methods Phys.Res. B335, 1 (2014)

N.V.Do, P.D.Khue, K.T.Thanh, N.T.Hien, G.Kim, S.Yang, Y.-S.Cho, T.-Y.Song, Y.-O.Lee, S.G.Shin, M.-H.Cho, M.W.Lee

Thermal neutron capture cross section and resonance integral of the ¹³⁹La(n, γ)¹⁴⁰La reaction

NUCLEAR REACTIONS ¹³⁹La(n, γ), E thermal; measured reaction products, Eγ, Iγ; deduced σ, resonance integral. Comparison with available data.

doi: 10.1016/j.nimb.2014.05.018
Citations: PlumX Metrics

2014DO17      Nucl.Instrum.Methods Phys.Res. B342, 188 (2014)

N.V.Do, P.D.Khue, K.T.Thanh, N.T.Hien, B.V.Loat, S.-C.Yang, K.Kim, G.Kim, T.-Y.Song, S.-G.Shin, M.-H.Cho, Y.-U.Kye, M.-W.Lee

Isomeric yield ratios for the ^natAg(γ, xn)^{106m, g;104m, g}Ag photonuclear reactions induced by 40-, 45-, 50-, 55-, and 60-MeV bremsstrahlung

NUCLEAR REACTIONS Ag(γ, xn)¹⁰⁶Ag/¹⁰⁴Ag, E=40-60 MeV; measured reaction products, Eγ, Iγ; deduced isomeric yield ratios. Comparison with available data.

doi: 10.1016/j.nimb.2014.09.034
Citations: PlumX Metrics

2014NA07      J.Radioanal.Nucl.Chem. 299, 1335 (2014)

H.Naik, A.Goswami, G.Kim, K.Kim, S.-C.Yang, M.Sahid, M.Zaman, M.Lee, S.G.Shin, M.-H.Cho

Independent isomeric-yield ratio of ^{89m, g}Nb from ⁹³Nb(γ, 4n), ^natZr(p, xn), and ⁸⁹Y(α, 4n) reactions

NUCLEAR REACTIONS ⁹³Nb(γ, 4n), E=45-70 MeV; ⁸⁹Y(α, 4n), E=38.9-42.5 MeV; Zr(p, xn)⁸⁹Nb, E-19.4-44.7 MeV; measured reaction products, Eγ, Iγ; deduced σ, isomeric yield ratio. TALYS nuclear model code calculations, comparison with available data.

doi: 10.1007/s10967-013-2848-5
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD7011.

2014NA16      J.Radioanal.Nucl.Chem. 300, 1121 (2014)

H.Naik, G.Kim, K.Kim, M.Zaman, S.-C.Yang, M.Sahid, M.Lee, S.-G.Shin, A.Goswami, M.-H.Cho

Independent isomeric yield ratios of ^{95m, g}Nb in the ^natMo(γ, pxn) and ^natZr(p, xn) reactions

NUCLEAR REACTIONS Mo(γ, xnp)⁹⁵Nb, E<70 MeV; measured reaction products, Eγ, Iγ; deduced independent isomeric yield ratios, σ. Comparison with available data, TALYS-1.4 nuclear model code calculations.

doi: 10.1007/s10967-014-3045-x
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD7012.

2014NA17      Eur.Phys.J. A 50, 83 (2014)

H.Naik, G.N.Kim, R.Schwengner, K.Kim, M.Zaman, S.C.Yang, M.W.Lee, S.G.Shin, Y.Gey, R.Massarczyk, R.John, A.Junghans, A.Wagner, A.Goswami, M.-H.Cho

Photo-neutron reaction cross-sections for ^natZr in the bremsstrahlung end-point energies of 12-16 and 45-70 MeV

NUCLEAR REACTIONS Zr(γ, xn), E=12-16, 45-70 MeV bremsstrahlung end-point; measured off-line Eγ, Iγ; deduced σ; calculated σ using TALYS-1.4. Compared with data.

doi: 10.1140/epja/i2014-14083-0
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetG0509.

2014NA23      Eur.Phys.J. A 50, 117 (2014)

H.Naik, G.N.Kim, K.Kim, M.Zaman, M.Sahid, S.-C.Yang, M.W.Lee, Y.R.Kang, S.G.Shin, M.-H.Cho, A.Goswami, T.Y.Song

Isomeric yield ratios of ^{87m, g}Y from different nuclear reactions

NUCLEAR REACTIONS Zr(γ, xnp), E=0-70 MeV;⁹³Nb(γ, 2nα), E=0-70 MeV[bremsstrahlung end-point energy given];⁸⁹Y(p, p2n), E=15-45 MeV;Zr(p, xnα), E=15-45 MeV;⁸⁹Y(α, 2nα), E=32-43 MeV; measured off-line Eγ, Iγ using HPGe. ^87g,87gY deduced isomeric σ_h to σ_l ratio, yield ratio; calculated σ_h to σ_l ratio using TALYS. Compared with published available data.

doi: 10.1140/epja/i2014-14117-7
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD7010.

2014TA08      J.Radioanal.Nucl.Chem. 300, 269 (2014)

M.Tatari, G.Kim, H.Naik, A.Hoseini Ranjbar, K.Kim, S.C.Yang, M.Zaman, M.Sahid, S.G.Shin, Y.U.Kye, Moo-Hyun Cho

Measurement of isomeric yield ratios of the ^{104m, g, 106m, g}Ag in the 45- and 55-MeV bremsstrahlung induced reactions of natural silver

NUCLEAR REACTIONS Ag(γ, xn)¹⁰⁴Ag/¹⁰⁶Ag, E<55 MeV; measured reaction products, Eγ, Iγ; deduced normalized yields, isomeric yield ratios and their uncertainties. Comparison with available data.

doi: 10.1007/s10967-014-3008-2
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetG3117.

2014YA06      J.Radioanal.Nucl.Chem. 300, 367 (2014)

S.Yang, K.Kim, M.Zaman, H.Naik, G.Kim, T.-Y.Song, Y.-O.Lee, S.Gy.Shin, Y.-U.Key, Moo-Hyun Cho

Isomeric yield ratios for the ^natNd(γ, xn)^{139m, g; 141m, g}Nd reactions in the bremsstrahlung energy region from 45 to 60 MeV

NUCLEAR REACTIONS Nd(γ, X)¹³⁹Nd/¹⁴¹Nd, E<60 MeV; measured reaction products, Eγ, Iγ; deduced normalized yields, isomeric yield ratios and their uncertainties. Comparison with available data.

doi: 10.1007/s10967-014-3008-2
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetG3118.

2014YA17      Nucl.Data Sheets 119, 314 (2014)

S.C.Yang, K.Kim, G.N.Kim, H.I.Kim, Y.O.Lee, M.W.Lee, D.K.Pham, V.D.Nguyen, S.G.Shin, M.H.Cho

Measurement of Isomeric Yield Ratio of ^{143m, g}Sm from ^natSm(γ, xn) Reaction with End-Point Bremsstrahlung Energies of 40-60 MeV

NUCLEAR REACTIONS Sm(γ, xn), E=40, 50, 60 MeV; measured bremsstrahlung induced activation Eγ, Iγ; deduced isomeric yield ratio for each energy; calculated isomeric yield ratio using TALYS-1.4. Compared to other data.

doi: 10.1016/j.nds.2014.08.086
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetG3123.

2014YA24      J.Radioanal.Nucl.Chem. 302, 467 (2014)

S.C.Yang, G.Kim, M.Zaman, K.Kim, T.-Y.Song, Y.-O.Lee, S.G.Shin, Y.-U.Key, M.-H.Cho, D.K.Pham, V.D.Nguyen, H.Naik, T.-I.Ro

Isomeric yield ratios of ¹⁴⁸Pm from the ^natSm(γ, x) and the natNd(p, xn) reactions

NUCLEAR REACTIONS Sm(γ, X)¹⁴⁸Pm/¹⁵¹Pm/¹⁵³Sm, E=45-64 MeV; Nd(p, xn)¹⁴⁸Pm/¹⁵⁰Pm/¹⁴¹Nd, E=5.08-44.72 MeV; measured reaction products, Eγ, Iγ. ¹⁴⁸Pm; deduced isomeric yields ratio and uncertainties. Comparison with TALYS 1.4 nuclear model code calculations, available data.

doi: 10.1007/s10967-014-3284-x
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD7013.

2014ZA03      J.Radioanal.Nucl.Chem. 299, 1739 (2014)

M.Zaman, G.Kim, H.Naik, K.Kim, S.-G.Shin, M.Tatari, M.-H.Cho

Measurement of photo-neutron cross-sections of ⁸⁹Y with bremsstrahlung energies of 45 and 55 MeV

NUCLEAR REACTIONS ⁸⁹Y(γ, n), (γ, 2n), (γ, 3n), (γ, 4n), E<55 MeV; measured reaction products, Eγ, Iγ; deduced σ. TALYS 1.4 nuclear model code calculations, comparison with available data.

doi: 10.1007/s10967-013-2914-z
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetG3116.

2013DO16      Nucl.Instrum.Methods Phys.Res. B310, 10 (2013)

N.V.Do, P.D.Khue, K.T.Thanh, N.G.Hein, G.Kim, S.Yang, K.S.Kim, S.G.Shin, M.-H.Cho, M.W.Lee

Measurement of thermal neutron cross section and resonance integral for the ¹⁷⁰Er(n, γ)¹⁷¹Er reaction by using a gold monitor

NUCLEAR REACTIONS ¹⁷⁰Er(n, γ), ¹⁹⁷Au(n, γ), E thermal; measured reaction products, Eγ, Iγ; deduced σ, resonance integral. Comparison with available data.

doi: 10.1016/j.nimb.2013.05.013
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2013NA30      Nucl.Phys. A916, 168 (2013)

H.Naik, G.N.Kim, R.Schwengner, K.Kim, M.Zaman, M.Tatari, M.Sahid, S.C.Yang, R.John, R.Massavczyk, A.Junghans, S.G.Shin, Y.Key, A.Wagner, M.W.Lee, A.Goswami, M.-H.Cho

Photo-neutron reaction cross-section for ⁹³Nb in the end-point bremsstrahlung energies of 12-16 and 45-70 MeV

NUCLEAR REACTIONS ²⁷Al(γ, 2pn), ⁹³Nb(γ, n), (γ, 2n), (γ, 3n), (γ, 4n), ¹⁹⁷Au(γ, n), E=12, 14, 16, 45, 50, 55, 60, 70 MeV; measured bremsstrahlung induced photoproduction Eγ, Iγ; deduced σ, metastable-state σ; calculated σ, metastable-state σ using TALYS 1.4. Compared also with other data.

doi: 10.1016/j.nuclphysa.2013.08.003
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetG3111.

2012NA26      Phys.Rev. C 86, 054607 (2012)

H.Naik, A.Goswami, G.N.Kim, M.W.Lee, K.S.Kim, S.V.Suryanarayana, E.A.Kim, S.G.Shin, M.-H.Cho

Mass-yield distributions of fission products from photofission of ²³²Th induced by 45- and 80-MeV bremsstrahlung

NUCLEAR REACTIONS ²³²Th(γ, F), E=45, 80 MeV bremmstrahlung; measured Eγ, Iγ, fission product yields of ^77,78Ge, ⁸⁴Br, ^85,87,88Kr, ⁸⁹Rb, ^91,92Sr, ^94,94Y, ^95,97Zr, ^99,101Mo, ^103,105Ru, ¹⁰⁴Tc, ^105,107Rh, ¹¹²Ag, ^115,117Cd, ^{127,128,129,131}Sb, ^{131,133,134,135}I, ^132,134Te, ¹³⁸Xe, ¹³⁸Cs, ^139,140,142Ba, ^{141,143,144,146}Ce, ¹⁴²La, ¹⁴⁶Pr, ^147,149Nd, ¹⁴⁹Pm, ¹⁵³Sm, A=133, 134, 138, 139, 143, 144 using a recoil catcher and an offline γ-ray spectrometric technique; deduced average heavy mass, and light mass, Peak-to-valley (P/V) ratio. Comparison with fission yields in ²³²Th, ²³⁸U(n, F) and ²³⁸U(γ, F) reactions.

doi: 10.1103/PhysRevC.86.054607
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetG3110.

2011KI42      J.Korean Phys.Soc. 59, 2029s (2011)

H.W.Kim, B.N.Lee, S.H.Lee, H.J.Choi, Y.S.Lee, H.S.Song, T.Zhou, Kh M.Gad, Y.H.Yeon, J.H.Oh, K.H.Park, S.H.Shin, M.H.Yoon, J.S.Chai

Magnet Design of 4 MeV Cyclotron for the BNCT

doi: 10.3938/jkps.59.2029
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2011SH42      J.Korean Phys.Soc. 59, 2075s (2011)

S.S.Shin, A.M.Kim, O.B.Gwun

Radiation Simulator Generator for GEANT4 Applications

doi: 10.3938/jkps.59.2075
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2010BH10      Int.J.Mod.Phys. E19, 2558 (2010)

H.Bhang, S.Ajimura, K.Aoki, A.Banu, T.Fukuda, O.Hashimoto, J.I.Hwang, S.Kameoka, B.H.Kang, E.Kim, J.H.Kim, M.Kim, T.Maruta, Y.Miura, Y.Miyake, T.Nagae, M.Nakamura, S.N.Nakamura, H.Noumi, S.Okada, Y.Okayasu, H.Outa, H.Park, P.K.Saha, Y.Sato, M.Sekimoto, S.Shin, T.Takahashi, H.Tamura, K.Tanida, A.Toyota, K.Tsukata, T.Watanabe, H.J.Yim

Recent progresses in the study of nonmesonic weak decay of Λ hypernuclei

RADIOACTIVITY ¹²C(π^-); measured decay products in Λ hypernuclei; deduced nonmesonic weak decay proton and neutron energy spectra, momentum sum yields. asymmetry parameter. Comparison with theoretical calculations.

doi: 10.1142/S0218301310017083
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2007BH06      Eur.Phys.J. A 33, 259 (2007)

H.Bhang, S.Ajimura, K.Aoki, A.Banu, T.Fukuda, O.Hashimoto, J.I.Hwang, S.Kameoka, B.H.Kang, E.H.Kim, J.H.Kim, M.Kim, T.Maruta, Y.Miura, Y.Miyake, T.Nagae, M.Nakamura, S.N.Nakamura, H.Noumi, S.Okada, Y.Okayasu, H.Outa, H.Park, P.K.Saha, Y.Sato, M.Sekimoto, S.Shin, T.Takahashi, H.Tamura, K.Tanida, A.Toyota, K.Tsukada, T.Watanabe, H.J.Yim

The quenching of nucleon yields in the nonmesonic weak decay of Λ-hypernuclei and the three-body weak decay process

NUCLEAR REACTIONS ⁵He, ¹²C(π⁺, K⁺), E at 1.05 GeV/c; measured Ep, En and angular distributions in hypernuclei decay and discussed quenching effect. Comparison with intra-nuclear cascade calculations.

doi: 10.1140/epja/i2007-10470-x
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2006KI14      Phys.Lett. B 641, 28 (2006)

M.J.Kim, S.Ajimura, K.Aoki, A.Banu, H.Bhang, T.Fukuda, O.Hashimoto, J.I.Hwang, S.Kameoka, B.H.Kang, E.H.Kim, J.H.Kim, T.Maruta, Y.Miura, Y.Miyake, T.Nagae, M.Nakamura, S.N.Nakamura, H.Noumi, S.Okada, Y.Okayasu, H.Outa, H.Park, P.K.Saha, Y.Sato, M.Sekimoto, S.Shin, T.Takahashi, H.Tamura, K.Tanida, A.Toyoda, K.Tsukada, T.Watanabe, H.J.Yim

Coincidence measurement of the nonmesonic weak decay of ¹²_ΛC

NUCLEAR REACTIONS ¹²C(π⁺, K⁺), E at 1.05 GeV/c; measured excitation energy spectra, Ep, En, np-, nn-coin, angular correlations. ¹²C deduced hypernucleus nonmesonic weak decay widths.

doi: 10.1016/j.physletb.2006.08.012
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1997PU01      Z.Phys. A357, 1 (1997)

Y.H.Pu, K.Morita, M.G.Hies, K.O.Lee, A.Yoshida, T.Nomura, Y.Tagaya, T.Motobayashi, M.Kurokawa, H.Minemura, T.Uchibori, T.Ariga, K.Sueki, S.A.Shin

New α-Decaying Neutron-Deficient Isotope ¹⁹⁶Rn

NUCLEAR REACTIONS ¹⁶⁶Er(³⁶Ar, 6n), (³⁶Ar, xnypzα), E=208 MeV; measured Eα, αα-correlations; deduced ¹⁹⁶Rn production σ. ¹⁹⁶Rn deduced α-decay T_1/2.

RADIOACTIVITY ^197,197m,196Rn(α) [from ¹⁶⁶Er(³⁶Ar, xn), E=208 MeV]; ¹⁹²Po(α) [from ¹⁹⁶Rn(α-decay)]; measured Eα, α-correlation. ¹⁹⁶Rn deduced T_1/2.

doi: 10.1007/s002180050203
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1995GO18      Nucl.Phys. A588, 241c (1995)

Y.Gono, T.Morikawa, T.Kishida, K.Morita, A.Odahara, E.Ideguchi, T.Murakami, M.Oshima, M.Sugawara, H.Kusakari, H.Kumagai, H.Tsuchida, M.Ogawa, M.Kidera, M.Shibata, K.Miyazaki, S.Mitarai, Y.H.Zhang, A.Ferragut, G.H.Liu, Y.Hatsukawa, J.C.Kim, S.A.Shin, M.Ishihara

Gamma-Ray Spectroscopy with High-Spin Isomer Beams

NUCLEAR REACTIONS ²⁰⁸Pb(¹⁷⁴Hf, ¹⁷⁴Hf'), E ≈ 5.4 MeV/nucleon; measured Eγ, Iγ following projectile isomer Coulomb excitation. ¹⁷⁴Hf deduced transition, B(λ). High-K isomer beam from ⁹Be(¹⁷⁰Er, 5n) reaction. Other aspects of high-spin isomer beams discussed.

doi: 10.1016/0375-9474(95)00146-R
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1995MO14      Z.Phys. A352, 7 (1995)

K.Morita, Y.H.Pu, J.Feng, M.G.Hies, K.O.Lee, A.Yoshida, S.C.Jeong, S.Kubono, T.Nomura, Y.Tagaya, M.Wada, M.Kurokawa, T.Motobayashi, H.Ogawa, T.Uchibori, K.Sueki, T.Ishizuka, K.Uchiyama, Y.Fujita, H.Miyatake, T.Shimoda, T.Shinozuka, H.Kudo, Y.Nagai, S.A.Shin

New α-Decaying Neutron Deficient Isotopes ¹⁹⁷Rn and ²⁰⁰Fr

NUCLEAR REACTIONS ¹⁶⁶Er(³⁶Ar, 5n), E=186, 200 MeV; ¹⁶⁹Tm(³⁶Ar, 5n), E=186 MeV; measured Eα, Iα; deduced evidence for ^197,197mRn, ²⁰⁰Fr. Evaporation residues obtained from gas-filled recoil separator, implanted onto position sensitive solid state detector.

RADIOACTIVITY ^197,197mRn(α) [from ¹⁶⁶Er(³⁶Ar, 5n), E=186, 200 MeV]; ²⁰⁰Fr(α) [from ¹⁶⁹Tm(³⁶Ar, 5n), E=186 MeV]; ^193,193mPo(α) [from ^197,197mRn(α-decay)]; ¹⁹⁶Rn(α) [from ¹⁶⁶Er(³⁶Ar, 6n)]; ¹⁹²Po(α) [from ¹⁹⁶Rn(α-decay)]; ²⁰⁰Fr(α) [from ¹⁶⁹Tm(³⁶Ar, 5n), E=186 MeV]; ¹⁹⁶At(α) [from ²⁰⁰Fr(α-decay)]; measured Eα, Iα, T_1/2, αα-energy correlations. Evaporation residues obtained from gas-filled recoil separator, implanted onto position sensitive solid state detector.

Note: The following list of authors and aliases matches the search parameter S.Shin: , S.A.SHIN, S.G.SHIN, S.H.SHIN, S.S.SHIN