NSR Query Results
Output year order : Descending NSR database version of April 11, 2024. Search: Author = S.Hamada Found 69 matches. 2024MO06 Chin.Phys.C 48, 024103 (2024) A.Morzabayev, N.Amangeldi, A.A.Ibraheem, D.Soldatkhan, G.Yergaliuly, B.Mauyey, A.A.Orazalievna, Sh.Hamada Dynamics of 7Li breakup and its influence on elastic scattering: a study of 7Li + 144Sm system NUCLEAR REACTIONS 144Sm(7Li, 7Li), E=21.6-52 MeV; analyzed available data; deduced σ(θ), optical model potential parameters.
doi: 10.1088/1674-1137/ad1029
2024NA03 Eur.Phys.J. A 60, 30 (2024) M.Nassurlla, N.Burtebayev, S.B.Sakuta, Sh.Hamada, S.V.Artemov, K.Rusek, N.Marzhan, N.Amangeldi, B.Mauyey, G.Yergaliuly, F.Ergashev, A.Sabidolda, R.Khojayev, Y.B.Mukanov, E.Piasecki, A.A.Ibraheem Scattering of 10B ions on 11B nuclei at an energy of 41.3 MeV NUCLEAR REACTIONS 11B(10B, 10B), E=41.3 MeV; measured reaction products. 10B; deduced σ(θ), σ, excited states J, π, spectroscopic amplitude value, optical model potential parameters. A cyclotron U-200P at the Heavy Ion Laboratory of Warsaw University.
doi: 10.1140/epja/s10050-023-01220-3
2023AL19 Int.J.Mod.Phys. E32, 2350029 (2023) W.Alharbi, A.A.Ibraheem, S.Hamada New microscopic analysis for 15N(d, p)16N neutron transfer reaction at 15 MeV NUCLEAR REACTIONS 15N(d, p), E=15 MeV; analyzed available data; deduced spectroscopic factors using the continuum discretized coupled channel (CDCC) method.
doi: 10.1142/S0218301323500295
2023AM05 Eur.Phys.J. A 59, 182 (2023) Effects of deuteron breakup and nucleon-transfer reactions on d+11B elastic scattering NUCLEAR REACTIONS 11B(d, d), (d, d'), (d, t), E=14.5 MeV; analyzed available data; deduced σ(θ), spectroscopic factors. Comparison with the continuum-discretized coupled-channel (CDCC) and coupled-reaction channel (CRC) methods.
doi: 10.1140/epja/s10050-023-01094-5
2023HA03 Nucl.Phys. A1030, 122590 (2023) Phenomenological and microscopic analysis for the 7Li + 12C system NUCLEAR REACTIONS 12C(7Li, 7Li), E=5.8-350 MeV; analyzed available data; deduced σ, potential parameters. The fully microscopic continuum discretized coupled channel (CDCC) method.
doi: 10.1016/j.nuclphysa.2022.122590
2023HA05 Pramana 97, 39 (2023) S.Hamada, N.A.M.Alsaif, M.El-Azab Farid, B.M.Alotaibi, M.Alotiby, A.A.Ibraheem Elastic scattering analysis using different phenomenological and microscopic potentials for 7Li + 27Al system NUCLEAR REACTIONS 27Al(7Li, 7Li), E=6-89 MeV; analyzed available data using different phenomenological and microscopic potentials to investigate the cluster nature of the weakly-bound 7Li projectile and the associated break-up effect on the elastic scattering data; deduced optical model potential parameters, σ incorporating microscopic potentials such as SPP, DF using the CDM3Y6 interaction and CFP without and with repulsive DPP.
doi: 10.1007/s12043-023-02515-2
2023HA22 Int.J.Mod.Phys. E32, 2350015 (2023) Sh.Hamada, A.H.Al-Ghamdi, A.A.Alholaisi, A.A.Ibraheem, N.Amangeldi, Y.Abdou Analysis of elastic scattering of 6, 7Li and 20Ne from 24Mg nucleus using microscopic potentials NUCLEAR REACTIONS 24Mg(6Li, 6Li), E=20, 88, 240 MeV; 24Mg(7Li, 7Li), E=20, 34, 88 MeV; 24Mg(20Ne, 20Ne), E=50, 60, 80, 90, 100 MeV; analyzed available data; deduced optical model parameters, σ, volume integrals.
doi: 10.1142/S0218301323500155
2023KU27 Eur.Phys.J. A 59, 282 (2023) Z.Kurmanaliyev, B.Mauyey, Awad A.Ibraheem, K.W.Kemper, S.Hamada Behavior of 6Li+144Sm elastic and inelastic angular distributions in the region of the Coulomb barrier NUCLEAR REACTIONS 144Sm(6Li, 6Li'), E=21-45 MeV; analyzed available data with a Woods-Saxon phenomenological and two microscopic optical potentials; deduced σ, energy-dependent real and imaginary potential volume integrals, normal threshold anomaly of strong coupling between the real and imaginary potentials.
doi: 10.1140/epja/s10050-023-01191-5
2022HA12 Int.J.Mod.Phys. E31, 2250019 (2022) Anomaly in weakly bound 7Li nucleus in the field of 208Pb target NUCLEAR REACTIONS 208Pb(7Li, 7Li), E=23.67, 39, 52, 63 MeV; analyzed available data. 7Li; deduced threshold anomaly. Continuum discretized coupled channel (CDCC) calculations.
doi: 10.1142/S0218301322500197
2022HA34 Phys.Scr. 97, 125303 (2022) Extensive investigation of the 6Li + 27Al and 6He + 27Al systems using different models NUCLEAR REACTIONS 27Al(6Li, 6Li), E=7-88 MeV; 27Al(6He, 6He), E=9.5-13.4 MeV; analyzed available data; deduced optical model and double folding potentials, cluster folding potential, σ within the framework of various potentials and methods.
doi: 10.1088/1402-4896/ac9dc9
2022IB01 Phys.Scr. 97, 085304 (2022) A.A.Ibraheem, M.Aygun, N.A.M.Alsaif, A.Alghamdi, S.Hamada Analysis of d + 6, 7, 9, 11Li elastic scattering using different densities and calculation procedures NUCLEAR REACTIONS 6,7Li(d, d), 2H(9Li, 9Li), (11Li, 11Li), E<10 MeV; analyzed available data; deduced σ(θ).
doi: 10.1088/1402-4896/ac824e
2022NA26 Phys.Scr. 97, 045302 (2022) M.Nassurlla, N.Burtebayev, B.K.Karakozov, S.B.Sakuta, D.Janseitov, M.Nassurlla, D.Alimov, J.Burtebayeva, A.Sabidolda, K.W.Kemper, R.Khojayev, S.Hamada Study of the 13C(3He, α)12C reaction at energies of 50 and 60 MeV NUCLEAR REACTIONS 13C(3He, α)12C, E=50, 60 MeV; measured reaction products, Eα, Iα; deduced σ(θ), σ, energy levels. The Coupled Channels Born Approximation method. The U-150M isochronous cyclotron at the Institute of Nuclear Physics (Almaty, Kazakhstan).
doi: 10.1088/1402-4896/ac5af6
2021HA51 Phys.Scr. 96, 055306 (2021) S.Hamada, N.A.M.Alsaif, A.A.Ibraheem Detailed analysis for 6Li+40Ca elastic scattering using different potentials NUCLEAR REACTIONS 40Ca(6Li, 6Li), E=20-240 MeV; analyzed available data. 6Li; deduced σ(θ) using the framework of the phenomenological optical model (OM), the semi-microscopic cluster folding optical model (CFOM), and the microscopic cluster folding model (CFM) motivated by the well-known cluster structure of 6Li.
doi: 10.1088/1402-4896/abeba6
2021IB01 Phys.Scr. 96, 115307 (2021) A.A.Ibraheem, N.A.M.Alsaif, M.Al-Ahmari, S.Hamada Further investigation of 10, 11B + 58Ni elastic scattering NUCLEAR REACTIONS 58Ni(10B, 10B), (11B, 11B), E=23, 24, 25, 35 MeV; analyzed available data; deduced σ, σ(θ), potential parameters using optical, double folding as well as cluster folding potentials.
doi: 10.1088/1402-4896/ac183f
2021NA14 Eur.Phys.J. A 57, 231 (2021) M.Nassurlla, N.Burtebayev, B.K.Karakozov, S.B.Sakuta, I.Boztosun, N.Amangeldi, A.K.Morzabayev, G.Yergaliuly, D.K.Alimov, J.Burtebayeva, M.Nassurlla, B.Mauyey, Y.Kucuk, Sh.Hamada, A.Sabidolda, R.Khojayev New measurements and analysis of elastic scattering of 13C by 9Be nuclei in a wide energy range NUCLEAR REACTIONS 9Be(13C, 13C), E=16.25, 19.5, 22.75, 28.12, 36.15, 57.77, 72.88 MeV; measured reaction products; deduced σ, σ(θ). OM and DWBA method, FRESCO program.
doi: 10.1140/epja/s10050-021-00539-z
2020AM07 Int.J.Mod.Phys. E29, 2050086 (2020) A.H.Amer, Yu.E.Penionzhkevich, A.A.Ibraheem, Sh.Hamada Comparison between the elastic scattering of 12C(α, α)12C and 12C(6He, 6He)12C using different nuclear potentials NUCLEAR REACTIONS 12C(α, α), E=48.7-386 MeV; 12C(6He, 6He), E=5.9-493.8 MeV; analyzed available data; deduced σ(θ) using the framework of both optical model (OM) and double folding optical model (DFOM).
doi: 10.1142/S021830132050086X
2020JA05 Acta Phys.Pol. B51, 745 (2020) D.M.Janseitov, N.Burtebayev, Z.Kerimkulov, D.Alimov, M.Nassurlla, B.Mauyey, D.S.Valiolda, A.S.Demyanova, A.Danilov, S.Hamada, A.Aimaganbetov Investigation of Deuteron Scattering from 13C at Low Energy
doi: 10.5506/APhysPolB.51.745
2020NA30 Chin.Phys.C 44, 104103 (2020) M.Nassurlla, N.Burtebayev, T.Kh.Sadykov, I.Boztosun, N.Amangeldi, D.Alimov, Z.Kerimkulov, J.Burtebayeva, M.Nassurlla, A.Kurakhmedov, S.B.Sakuta, M.Karakoc, A.A.Ibraheem, K.W.Kemper, S.Hamada New measurements and reanalysis of 14N elastic scattering on 10B target NUCLEAR REACTIONS 10B(14N, 14N), E= 38-94.0 MeV; measured reaction products; deduced σ(θ), possible contribution of the α-cluster exchange mechanism, spectroscopic amplitudes using the optical model and the distorted waves Born approximation method.
doi: 10.1088/1674-1137/abab89
2019BU13 Int.J.Mod.Phys. E28, 1950028 (2019) N.Burtebayev, M.Nassurlla, A.Sabidolda, S.B.Sakuta, A.A.Karakhodjaev, F.X.Ergashev, K.Rusek, E.Piasecki, A.Trzcinska, M.Wolinska-Cichocka, M.Kowalczyk, B.Mauyey, D.Janseitov, B.Zalewski, Sh.Hamada, K.W.Kemper, A.A.Ibraheem Measurement and analysis of 10B + 12C elastic scattering at energy of 41.3 MeV NUCLEAR REACTIONS 12C(10B, 10B), E=41.3 MeV; measured reaction products; deduced σ(θ), optical model parameters.
doi: 10.1142/S0218301319500289
2019BU18 Acta Phys.Pol. B50, 1423 (2019) N.Burtebayev, Sh.Hamada, A.A.Ibraheem, K.Rusek, M.Wolinska-Cichocka, J.Burtebayeva, N.Amangeldi, M.Nassurlla, M.Nassurlla, A.Sabidolda Effect of the Transfer Reactions for 16O+10B Elastic Scattering NUCLEAR REACTIONS 10B(16O, 16O), E=24 MeV; measured reaction products; deduced σ, optimal potential parameters. Comparison with available data.
doi: 10.5506/aphyspolb.50.1423
2019HA36 Phys.Part. and Nucl.Lett. 16, 602 (2019) Coupled Reaction Channels and Cluster Folding Analysis for 3He + 20Ne Elastic and Inelastic Scattering
doi: 10.1134/S1547477119060189
2019HA37 Int.J.Mod.Phys. E28, 1950108 (2019) Peculiarities of 6Li +12C elastic scattering NUCLEAR REACTIONS 12C(6Li, 6Li), E=50-600 MeV; analyzed available data using the phenomenological optical potential and two different semi-microscopic potentials, namely double folding and cluster folding (CF).
doi: 10.1142/S0218301319501088
2018HA20 Phys.Part. and Nucl.Lett. 15, 143 (2018) Single Folding Optical Potential for Elastic Scattering of Protons from 14N and 16O in a Wide Range of Energies NUCLEAR REACTIONS 14N, 16O(p, p), E=8.6-14.6 MeV; analyzed available data; calculated σ(θ).
doi: 10.1134/S1547477118020073
2018HA22 Phys.Rev. C 97, 054609 (2018) Sh.Hamada, N.Keeley, K.W.Kemper, K.Rusek Cluster folding analysis of 20Ne + 16O elastic transfer NUCLEAR REACTIONS 16O(20Ne, 16O)20Ne, E(cm)=24.5, 24.7, 27.9, 28.2, 29.1, 31.7, 32.1, 33.0, 35.5 MeV; analyzed experimental σ(θ, E) data using optical model cluster folding including elastic transfer process via DWBA; deduced σ, spectroscopic factors, and real and imaginary volume integrals per nucleon pair. Relevance to α-particle structure of nuclei.
doi: 10.1103/PhysRevC.97.054609
2016HA42 Braz.J.Phys. 46, 740 (2016) Sh.Hamada, I.Bondok, M.Abdelmoatmed Double Folding Potential of Different Interaction Models for 16O + 12C Elastic Scattering NUCLEAR REACTIONS 12C(16O, 16O), E=115.9-230 MeV; calculated σ(θ); deduced renormalization factor for the different interaction models.
doi: 10.1007/s13538-016-0450-3
2015HA17 Int.J.Mod.Phys. E24, 1550047(2015); Erratum Int.J.Mod.Phys. E24, 1592001 (2015) One-two step transfer observed in16O+11B nuclear system NUCLEAR REACTIONS 11B(16O, 16O), E=22.4 MeV; measured reaction products; deduced yields, σ(θ), optical model parameters. Comparison with distorted wave Born approximation method implemented in FRESCO code.
doi: 10.1142/S0218301315500470
2014HA34 Int.J.Mod.Phys. E23, 1450061 (2014) Sh.Hamada, N.Burtebayev, N.Amangeldi Detailed study for 16O → 12C + α and 12C → 11B + p spectroscopic factors NUCLEAR REACTIONS 12C(16O, 16O), E=28 MeV; 11B(12C, 12C), E=18 MeV; measured reaction products; deduced σ(θ), optical model potential parameters, spectroscopic factors. Comparison with DWBA and CCBA calculations.
doi: 10.1142/S021830131450061X
2013HA01 Phys.Rev. C 87, 024311 (2013) Sh.Hamada, Y.Hirabayashi, N.Burtebayev, S.Ohkubo Observation of an Airy minimum in elastic and inelastic scattering of 3He from 12C at 50.5 and 60 MeV, and α-particle condensation in 12C NUCLEAR REACTIONS 12C(3He, 3He), (3He, 3He'), E=50.5, 60 MeV;measured particle spectra, energy loss, σ(θ, E) for Hoyle state and other levels. 12C; deduced levels, angular position of Airy minimum A1. Hoyle state interpreted as three α-particle condensate with dilute density. Coupled-channel analysis with double folding model.
doi: 10.1103/PhysRevC.87.024311
2013HA22 Int.J.Mod.Phys. E22, 1350058 (2013) Sh.Hamada, N.Burtebayev, N.Amangeldi Detailed study for 16O elastically scattered from 16O at energies 20, 24 and 28 MeV NUCLEAR REACTIONS 16O(16O, 16O), E=20, 24, 28 MeV; measured reaction products; deduced σ(θ). Comparison with optical model calculations.
doi: 10.1142/S0218301313500584
2012GR16 Bull.Rus.Acad.Sci.Phys. 76, 934 (2012); Izv.Akad.Nauk RAS, Ser.Fiz 76, 1038 (2012) K.A.Gridnev, N.A.Maltsev, N.Burtebaev, N.Amangeldy, Sh.Hamada Role of the inelastic transfer channel in elastic 16O + 12C scattering over a wide range of energies NUCLEAR REACTIONS 12C(16O, 16O), E<200 MeV; calculated σ(θ), α-cluster transfer. DWBA and CCBA calculations.
doi: 10.3103/S106287381208014X
2012HA45 J.Phys.:Conf.Ser. 381, 012130 (2012) S.Hamada, N.Burtebayev, N.Amangeldi, K.A.Gridnev, K.Rusek, Zh.Kerimkulov, N.Maltsev Phenomenological and semi-microscopic analysis for 16O and 12C elastically scattering on the nucleus of 16O and 12C at Energies near the Coulomb barrier NUCLEAR REACTIONS 12C(12C, 12C), E=18, 21 MeV;16O(16O, 16O), E=24, 28 MeV; measured E(particle), I(particle, θ); deduced σ(θ); calculated σ(θ) using phenomenological optical potential using SPI-GENDA code and using double-folding potential code FRESCO; deduced potential parameters.
doi: 10.1088/1742-6596/381/1/012130
2011AM02 Int.J.Mod.Phys. E20, 980 (2011) A.Amar, S.Hamada, N.Burtebayev, N.Amangeldy Study of scattering 1H, 12C and 16O nuclei on 1P-shell at energy near the Coulomb barrier NUCLEAR REACTIONS 6,7Li, 10,11B(p, p), E=300-1050 keV; measured proton spectrum; deduced σ(θ), optical model parameters. Comparison with code SPIVAL and DWBA calculations.
doi: 10.1142/S0218301311019106
2011GR11 Bull.Rus.Acad.Sci.Phys. 75, 961 (2011) K.A.Gridnev, N.Burtebayev, N.A.Maltsev, N.Amangeldi, Sh.Hamada Investigating the 16O + 12C reaction over a wide range of energies NUCLEAR REACTIONS 12C(16O, 16O), (16O, 12C), E=28 MeV; measured reaction products; deduced σ(θ). α-cluster transfer, DWBA model, DWUCK5 program.
doi: 10.3103/S1062873811070173
2011HA23 Nucl.Phys. A859, 29 (2011) Sh.Hamada, N.Burtebayev, K.A.Gridnev, N.Amangeldi Analysis of alpha-cluster transfer in 16O+ 12C and 12C+ 16O at energies near Coulomb barrier NUCLEAR REACTIONS 12C(16O, 12C), E=20, 24, 28 MeV; 16O(12C, 16O), E=21 MeV; measured E(particle), I(particle, θ); deduced σ(θ), optical potential parameters; calculated σ(θ) using optical model DWUCK5 and SPI-GENOA code.
doi: 10.1016/j.nuclphysa.2011.04.006
2011HA47 Phys.Scr. 84, 045201 (2011) Sh.Hamada, N.Burtebayev, K.A.Gridnev, N.Amangeldi Further investigation of the elastic scattering of 16O, 14N and 12C on the nucleus of 27Al at low energies NUCLEAR REACTIONS 27Al(16O, 16O), (14N, 14N), (12C, 12C), E=1.75 MeV/nucleon; measured reaction products; deduced σ, σ(θ). Comparison with optical model calculations.
doi: 10.1088/0031-8949/84/04/045201
2003GU06 Phys.Rev. C 67, 064601 (2003) V.Guimaraes, S.Kubono, F.C.Barker, M.Hosaka, S.C.Jeong, I.Katayama, T.Miyachi, T.Nomura, M.H.Tanaka, Y.Fuchi, H.Kawashima, S.Kato, C.C.Yun, K.Ito, H.Orihara, T.Terakawa, T.Kishida, Y.Pu, S.Hamada, M.Hirai, H.Miyatake Structure of the unbound 11N nucleus by the (3He, 6He) reaction NUCLEAR REACTIONS 14N(3He, 6He), E=73.4 MeV; measured σ(E, θ). 11N deduced levels, J, π, resonance widths. DWBA analysis.
doi: 10.1103/PhysRevC.67.064601
2003GU30 Braz.J.Phys. 33, 263 (2003) V.Guimaraes, S.Kubono, F.C.Barker, M.Hosaka, S.C.Jeong, I.Katayama, T.Miyachi, T.Nomura, M.H.Tanaka, Y.Fuchi, H.Kawashima, S.Kato, T.Kishida, Y.Pu, S.Hamada Spectroscopic Study of the Unbound 11N Nucleus NUCLEAR REACTIONS 14N(3He, 6He), E=73.4 MeV; measured particle spectra, σ(E, θ). 11N deduced resonance energies, J, π, widths. DWBA analysis.
doi: 10.1590/s0103-97332003000200017
2002FU14 Phys.Rev. C66, 024609 (2002); Erratum Phys.Rev. C 68, 019904 (2003) H.Fujita, M.Hijiya, Y.Inotani, T.Mukae, K.Koga, M.Koga, F.Nakamura, S.Koto, T.Sugimitsu, N.Ikeda, S.Morinobu, Y.Sugiyama, Y.Tomita, H.Ikezoe, Y.Yamanouti, K.Ideno, S.Hamada, T.Ikuta Intermediate structures in 12C(16O, 12C[2+])16O studied with the γ-ray recoil method NUCLEAR REACTIONS 12C(16O, 12C), E(cm) ≈ 30 MeV; measured particle momentum spectra, σ(E, θ); deduced resonance structures J, π.
doi: 10.1103/PhysRevC.66.024609
2001DA31 Hyperfine Interactions 132, 133 (2001) C.N.Davids, P.J.Woods, J.C.Batchelder, C.R.Bingham, D.J.Blumenthal, L.T.Brown, B.C.Busse, M.P.Carpenter, L.F.Conticchio, T.Davinson, J.Deboer, S.J.Freeman, S.Hamada, D.J.Henderson, R.J.Irvine, R.V.F.Janssens, H.J.Maier, L.Muller, R.D.Page, H.T.Penttila, G.L.Poli, D.Seweryniak, F.Soramel, K.S.Toth, W.B.Walters, B.E.Zimmerman Masses and Proton Separation Energies Obtained from Qα and Qp Measurements ATOMIC MASSES 151Tm, 155Lu, 159Ta, 163,165Re, 166Os, 167,169Ir, 170Pt, 171,173Au, 174,176Hg, 177Tl, 180Pb; analyzed α-decay and proton-decay data; deduced mass excesses. Tm, Lu, Ta, Re, Ir, Au, Tl; deduced proton separation energies.
doi: 10.1023/A:1011941605006
1999ID01 Eur.Phys.J. A 6, 387 (1999) E.Ideguchi, X.H.Zhou, Y.Gono, S.Mitarai, T.Morikawa, M.Kidera, H.Tsuchida, M.Shibata, H.Watanabe, M.Miyake, A.Odahara, M.Oshima, Y.Hatsukawa, S.Hamada, H.Iimura, M.Shibata, T.Ishii, T.Kishida, M.Ishihara A New High Spin Isomer in 146Eu NUCLEAR REACTIONS 140Ce(10B, 4n), E=50 MeV; 139La(13C, 6n), E=98 MeV; measured Eγ, Iγ(t), γγ-coin. 146Eu deduced high-spin levels, J, π, configurations, high-spin isomer T1/2. Comparison with deformed independent particle model.
doi: 10.1007/s100500050360
1999PO09 Phys.Rev. C59, R2979 (1999) G.L.Poli, C.N.Davids, P.J.Woods, D.Seweryniak, J.C.Batchelder, L.T.Brown, C.R.Bingham, M.P.Carpenter, L.F.Conticchio, T.Davinson, J.DeBoer, S.Hamada, D.J.Henderson, R.J.Irvine, R.V.F.Janssens, H.J.Maier, L.Muller, F.Soramel, K.S.Toth, W.B.Walters, J.Wauters Proton and α Radioactivity below the Z = 82 Shell Closure RADIOACTIVITY 177Tl, 171Au(p) [from 96Ru, 102Pd(78Kr, xnyp)]; measured Ep, T1/2 from ground, isomeric levels. 177Tl, 173Au, 169Ir(α); measured Eα, T1/2 from ground, isomeric levels. 177Tl, 171Au levels deduced J, π, spectroscopic factors. 177,177mTl, 173,173mAu, 169,169mIr, 165,165mRe, 171Au; deduced proton separation energies. RADIOACTIVITY 176Hg(α); measured decay products, Eα, Iα; deduced %α branch, T1/2.
doi: 10.1103/PhysRevC.59.R2979
1999UT03 Nucl.Phys. (Supplement) A654, 928c (1999) H.Utsunomiya, Y.Tokimoto, T.Yamagata, M.Ohta, Y.Aoki, K.Hirota, K.Ieki, Y.Iwata, K.Katori, S.Hamada, Y.-W.Lui, R.P.Schmitt, S.Typel, G.Baur Excitation of Continuum States in 7Li and Their Decay by Quantum Tunneling NUCLEAR REACTIONS 27Al, 58Ni, 64Zn, 90Zr, 120Sn, 144Sm, 197Au(7Li, tα), E=42 MeV; measured particle spectra, forward-backward asymmetry; deduced E1, E2, higher-order effects in Coulomb breakup.
doi: 10.1016/S0375-9474(00)88575-9
1998SE20 Phys.Rev. C58, 2710 (1998) D.Seweryniak, D.Ackermann, H.Amro, L.T.Brown, M.P.Carpenter, L.Conticchio, C.N.Davids, S.M.Fischer, G.Hackman, S.Hamada, D.J.Henderson, R.V.F.Janssens, D.Nisius, P.Reiter, W.B.Walters, P.J.Woods In-Beam γ-Ray Spectroscopy of Pt Isotopes Located at the Proton Drip Line NUCLEAR REACTIONS 96Mo(78Kr, 2n), (78Kr, 3n), E=345 MeV; 96Ru(78Kr, 2n2p), E=385 MeV; measured Eγ, Iγ, (recoil)γ-coin. 170,171,172Pt deduced levels, J, π. Comparison with neighboring isotopes, isotones. Recoil-decay tagging technique.
doi: 10.1103/PhysRevC.58.2710
1998UT01 Phys.Lett. 416B, 43 (1998) H.Utsunomiya, Y.Tokimoto, H.Mabuchi, K.Osada, T.Yamagata, M.Ohta, Y.Aoki, K.Hirota, K.Ieki, Y.Iwata, K.Katori, S.Hamada, Y.-W.Lui, R.P.Schmitt Strongly-Suppressed Post-Coulomb Acceleration in Non-Resonant Breakup of 7Li NUCLEAR REACTIONS 27Al, 58Ni, 90Zr, 120Sn, 144Sm, 197Au(7Li, tα), E=42 MeV; measured tα-coin, σ(θ, Et, Eα); deduced no evidence for fragment post-acceleration. Non-resonant breakup, Coulomb dissociation, astrophysical implications.
doi: 10.1016/S0370-2693(97)01328-2
1998UT03 Nucl.Instrum.Methods Phys.Res. A402, 417 (1998) H.Utsunomiya, Y.Tokimoto, K.Osada, T.Yamagata, M.Ohta, Y.Aoki, K.Hirota, K.Ieki, Y.Iwata, K.Katori, S.Hamada, Y.-W.Lui, R.P.Schmitt Method of Coulomb Breakup Probing Primordial 7Li Synthesis NUCLEAR REACTIONS 90Zr(7Li, tα), E=42 MeV; measured t-, α-spectra, tα-coin; deduced astrophysical S-factors. Comparison with direct capture data.
doi: 10.1016/S0168-9002(97)00883-8
1998UT04 J.Phys.(London) G24, 1637 (1998) H.Utsunomiya, Y.Tokimoto, K.Osada, T.Yamagata, M.Ohta, Y.Aoki, K.Hirota, K.Ieki, Y.Iwata, K.Katori, S.Hamada, Y.-W.Lui, R.P.Schmitt Astrophysical Implications of Non-Resonant Break-Up of 7Li NUCLEAR REACTIONS 90Zr, 197Au(7Li, tα), E not given; analyzed nonresonant breakup data; deduced role of post-Coulomb acceleration.
doi: 10.1088/0954-3899/24/8/044
1997OD01 Nucl.Phys. A620, 363 (1997) A.Odahara, Y.Gono, S.Mitarai, T.Morikawa, T.Shizuma, M.Kidera, M.Shibata, T.Kishida, E.Ideguchi, K.Morita, A.Yoshida, H.Kumagai, Y.H.Zhang, A.Ferragut, T.Murakami, M.Oshima, H.Iimura, M.Shibata, S.Hamada, H.Kusakari, M.Sugawara, M.Ogawa, M.Nakajima, B.J.Min, J.C.Kim, S.J.Chae, H.Sagawa High-Spin Isomer and Level Structure of 145Sm NUCLEAR REACTIONS 20Ne(136Xe, 7nα), E=8.2 MeV/nucleon; 16O(136Xe, 7n), E=7.4 MeV/nucleon; 139La(10B, 4n), E=47 MeV; 138Ba(13C, 6n), E=95, 98 MeV; measured Eγ, Iγ, γγ-coin, γγ(t), Iγ(θ). 145Sm deduced high-spin levels, J, π, isomer T1/2.
doi: 10.1016/S0375-9474(97)00189-9
1997SU01 Phys.Rev. C55, R5 (1997) Y.Sugiyama, Y.Tomita, Y.Yamanouti, S.Hamada, T.Ikuta, H.Fujita, D.R.Napoli Elastic Two-Neutron Transfer Reactions of 58Ni + 60Ni and 62Ni + 64Ni Around the Coulomb Barrier NUCLEAR REACTIONS 60Ni(58Ni, 58Ni), E=204-250 MeV; 62Ni(64Ni, 64Ni), E=250 MeV; measured σ(θ) vs E; deduced pair deformation parameter, optical model parameters. Coupled-channels, DWBA analyses.
doi: 10.1103/PhysRevC.55.R5
1997SU22 J.Phys.(London) G23, 1393 (1997) Y.Sugiyama, S.Hamada, T.Ikuta, A.Yamazaki Elastic Two-Neutron Transfer Reaction of 58Ni + 60Ni and 62Ni + 64Ni Around the Coulomb Barrier NUCLEAR REACTIONS 60Ni(58Ni, 58Ni), E(cm)=103.7, 111.9, 120.0, 127.1 MeV; 64Ni(62Ni, 62Ni), E(cm)=108.2, 123.0 MeV; 64Ni(58Ni, 58Ni), E(cm)=99.8, 118.8 MeV; 64Ni(58Ni, 60Ni), E(cm)=118.8 MeV; measured σ(θ); deduced parameters, two-neutron transfer role. Coupled-channels, DWBA analyses.
doi: 10.1088/0954-3899/23/10/029
1997ZH15 Z.Phys. A358, 285 (1997) X.H.Zhou, E.Ideguchi, Y.Gono, T.Kishida, S.Mitarai, T.Morikawa, H.Tsuchida, M.Shibata, H.Watanabe, M.Miyake, A.Odahara, M.Oshima, Y.Hatsukawa, S.Hamada, H.Iimura, M.Shibata, T.Ishii, M.Ishihara Study of High-Lying States in 147Eu NUCLEAR REACTIONS 139La(13C, 5n), E=98 MeV; measured γγ(t), Iγ(θ). 147Eu deduced high-spin levels, J, π.
doi: 10.1007/s002180050331
1996IK01 Phys.Rev. C54, 2043 (1996) H.Ikezoe, T.Ikuta, S.Hamada, Y.Nagame, I.Nishinaka, K.Tsukada, Y.Oura, T.Ohtsuki α Decay of a New Isotope 209Th RADIOACTIVITY 209Th(α) [from 182W(32S, X), E=171 MeV]; 210,211,212Th, 208,209Ac(α), 208Ac(IT); measured decay products, Eα, αα-correlations, αα-coin; deduced α-particle energies, reduced width, T1/2. Recoil mass separator, the JAERI-tandem accelerator.
doi: 10.1103/PhysRevC.54.2043
1996IK03 Nucl.Instrum.Methods Phys.Res. A376, 420 (1996) H.Ikezoe, Y.Nagame, T.Ikuta, S.Hamada, I.Nishinaka, T.Ohtsuki JAERI Recoil Mass Separator NUCLEAR REACTIONS 89Y, Ag, I, 59Co(28Si, X), E=130 MeV; measured fusion residues energy, yield vs position; deduced recoil mass separator characteristics. JAERI recoil mass separator.
doi: 10.1016/0168-9002(96)00183-0
1996KO04 Phys.Lett. 365B, 17 (1996) Y.Kondo, Y.Sugiyama, Y.Tomita, Y.Yamanouchi, H.Ikezoe, K.Ideno, S.Hamada, T.Sugimitsu, M.Hijiya, H.Fujita Airy Minimum Crossing θ(cm) = 90° at E(lab) = 124 MeV for the 16O + 16O System NUCLEAR REACTIONS 16O(16O, 16O), E=124 MeV; measured σ(θ); deduced Airy minimum related features.
doi: 10.1016/0370-2693(95)01305-9
1995GU08 Nucl.Phys. A588, 161c (1995) V.Guimaraes, S.Kubono, M.Hosaka, N.Ikeda, S.C.Jeong, I.Katayama, T.Miyachi, T.Nomura, M.H.Tanaka, Y.Fuchi, H.Kawashima, S.Ohkawa, S.Kato, H.Toyokawa, C.C.Yun, T.Niizeki, K.Ito, T.Kishida, T.Kubo, Y.Pu, M.Ohura, H.Orihara, T.Terakawa, S.Hamada, M.Hirai, H.Miyatake Structure of Light Proton-Rich Nuclei on the Drip-Line NUCLEAR REACTIONS 14N, 20Ne(3He, 6He), E=70.08 MeV; measured 6He energy spectra; deduced isobaric multiplet mass equation. 11N, 17Ne deduced levels, J, π, configuration.
doi: 10.1016/0375-9474(95)00117-J
1995ID01 Z.Phys. A352, 363 (1995) E.Ideguchi, Y.Gono, S.Mitarai, T.Morikawa, A.Odahara, M.Kidera, M.Sibata, H.Tsuchida, K.Miyazaki, M.Oshima, Y.Hatsukawa, S.Hamada, H.Iimura, M.Shibata, T.Ishii, T.Murakami, H.Kusakari, M.Sugawara, T.Kishida, K.Morita, H.Kumagai, M.Ishihara High-Spin States in 148Tb NUCLEAR REACTIONS 141Pr(13C, 6n), E=95-108 MeV; 27Al(130Te, 9n), E=7.5 MeV/nucleon; measured γγ-coin. 148Tb deduced high-spin levels, J, π.
doi: 10.1007/BF01299753
1994HA16 Phys.Rev. C49, 3192 (1994) S.Hamada, M.Yasue, S.Kubono, M.H.Tanaka, R.J.Peterson Cluster Structure in 10Be from the 7Li(α, p)10Be Reaction NUCLEAR REACTIONS 7Li(α, p), (α, α), E=65 MeV; measured spectra, σ(θ); deduced model parameters. 10Be levels deduced cluster spectroscopic factors, particle decay widths. Cluster model.
doi: 10.1103/PhysRevC.49.3192
1994IK01 Phys.Rev. C49, 968 (1994) H.Ikezoe, Y.Nagame, I.Nishinaka, Y.Sugiyama, Y.Tomita, K.Ideno, S.Hamada, N.Shikazono, A.Iwamoto, T.Ohtsuki Prescission and Postscission Charge Particle Emissions from the 19F + 159Tb Reaction NUCLEAR REACTIONS 159Tb(19F, F), E=124.1, 159.1 MeV; measured fission (fragment)p-, (fragment)α-coin, prescission, postscission p-, α-multiplicities; deduced fission fragment temperatures. Statistical model.
doi: 10.1103/PhysRevC.49.968
1994OD02 Z.Phys. A350, 185 (1994) A.Odahara, Y.Gono, S.Mitarai, E.Ideguchi, M.Kidera, M.Shibata, T.Morikawa, T.Kishida, K.Morita, A.Yoshida, H.Kumagai, Y.H.Zhang, A.Ferragut, T.Murakami, M.Oshima, H.Iimura, M.Shibata, S.Hamada, H.Kusakari, M.Sugawara, M.Ogawa, M.Nakajima, B.J.Min, J.C.Kim, S.J.Chae, H.Sagawa High-Spin States of 145Sm NUCLEAR REACTIONS 20Ne(136Xe, 7nα), E=8.2 MeV/nucleon; 139La(10B, 4n), E=47 MeV; 138Ba(13C, 6n), E=95, 98 MeV; measured γγ-coin, γ(θ). 145Sm deduced high-spin levels, J, π, isomer. Deformed independent particle model comparison.
doi: 10.1007/BF01289580
1994SU09 Phys.Rev. C49, 3305 (1994) Y.Sugiyama, Y.Tomita, H.Ikezoe, Y.Yamanouchi, K.Ideno, S.Hamada, M.Hijiya, T.Sugimitsu, T.Mukae, K.Nakamoto, K.Utsunomiya, T.Okamoto, S.Mitsuoka, M.Matsuo, H.Fujita New Appraoch to Spin Assignments of Intermediate Structures in 12C(16O, 12C[2+1])16O NUCLEAR REACTIONS 12C(16O, 16O'), E(cm)=28.5-33.5 MeV; measured recoil 12C spectra, σ(θ) vs E, magnetic substate population; deduced intermediate structure resonances, J.
doi: 10.1103/PhysRevC.49.3305
1993SU11 Phys.Lett. 312B, 35 (1993) Y.Sugiyama, Y.Tomita, H.Ikezoe, Y.Yamanouchi, K.Ideno, S.Hamada, T.Sugimitsu, M.Hijiya, Y.Kondo Observation of Airy Oscillation for the 16O + 16O System at E(lab) = 145 MeV NUCLEAR REACTIONS 16O(16O, 16O), E=145 MeV; measured σ(θ); deduced Airy oscillation evidence, model parameters. Optical model.
doi: 10.1016/0370-2693(93)90482-W
1992MA52 Hyperfine Interactions 74, 223 (1992) S.Matsuki, K.Shimomura, I.Ogawa, K.Suzuki, S.Hamada, T.Nakamura, H.Okuno, M.Koizumi, N.Inabe, Y.Fukashiro, H.Sunaoshi, M.Wada, T.Murayama, T.Kohmoto, M.Kitano, T.Kubo, T.Shinozuka, K.Asahi, Y.Kido, T.T.Inamura, T.Nomura, M.Ishihara, M.Fujioka, H.T.Duong, H.Haas, and the ISOLDE Collaboration Radiation-Detected Optical Pumping in Solids NUCLEAR REACTIONS 160Gd(12C, 5np), E=100 MeV; measured residual nucleus polarization. 160Gd(12C, 6n), E=100 MeV; measured nuclear polarization following residual decay. Optical pumping in SrF, crystal. RADIOACTIVITY 164Tm(β+) [from 164Yb-decay following production in 158Gd(12C, 6n), E=100 MeV]; measured β+ asymmetry. On-line polarization, implantation in CaF2 host crystal. 114mIn(IT); measured β+ asymmetry of 114In decay vs exciting laser wavelength. Polarization of 114In in GaAs crystal, Ti-saphire excited laser for optical pumping. 33Si(β-) [from 9Be(Ar, X), E=94 MeV/nucleon]; measured β-asymmetry, NMR vs exciting laser wavelength. Ion implantation in GaAs host crystal.
doi: 10.1007/BF02398632
1992SH23 Hyperfine Interactions 74, 317 (1992) K.Shimomura, T.Nakamura, H.Okuno, M.Koizumi, S.Hamada, N.Inabe, I.Ogawa, K.Suzuki, M.Wada, H.Sunaoshi, Y.Fukashiro, T.Murayama, T.Kohmoto, T.Shinozuka, T.Kubo, K.Asahi, T.Inamura, M.Ishihara, M.Fujioka, S.Matsuki Nuclear Polarization and Magnetic Resonance of 33Si with Optical Pumping in Solids RADIOACTIVITY 33Si(β-) [from 9Be(Ar, X), E=80, 95 MeV/nucleon]; measured β-asymmetry, more precise T1/2; deduced polarization, magnetic resonance. Scintillation-counter telescopes, implantation into liquid He cooled GaAs crystal.
doi: 10.1007/BF02398646
1992SH31 Nucl.Instrum.Methods Phys.Res. B70, 513 (1992) K.Shimomura, I.Ogawa, K.Suzuki, S.Hamada, T.Nakamura, H.Okuno, M.Koizumi, N.Inabe, Y.Fukashiro, H.Sunaoshi, M.Wada, S.Hatori, T.Murayama, T.Kohmoto, Y.Fukuda, T.Kubo, T.Shinozuka, K.Asahi, S.Morinobu, T.T.Inamura, M.Ishihara, M.Fujioka, M.Kondo, S.Matsuki OPERA: An On-Line System of Optical Pumping in Solids for Unstable Nuclei RADIOACTIVITY 166Tm(β+), (EC) [from 166Yb(EC-decay) following 160Gd(12C, 6n), E=100 MeV; 160Gd(12C, 5np), E=100 MeV]; 114In(β-), (β+), (EC) [from 114mIn(IT)]; 33Si(β-) [from 9Be(Ar, X), E=94 MeV/nucleon]; measured β asymmetry, NMR, polarized nuclei. On-line system, optical pumping in solids.
doi: 10.1016/0168-583X(92)95975-W
1990YA07 Phys.Rev. C42, 1279 (1990) M.Yasue, K.Ogawa, T.Niizeki, J.Takamatsu, M.Ohura, A.Terakawa, T.Nakagawa, T.Hasegawa, H.Ohnuma, H.Toyokawa, S.Hamada Spectroscopy of Positive Parity States in 26Mg and 26Al via the (α, 3He) and (α, t) Reactions NUCLEAR REACTIONS 25Mg(α, 3He), (α, t), E=50 MeV; measured σ(θ). 26Mg, 26Al deduced levels, spectroscopic factors. Enriched target. Exact finite-range DWBA analysis.
doi: 10.1103/PhysRevC.42.1279
1989AH01 J.Phys.(London) G15, 93 (1989) S.T.Ahmad, W.D.Hamilton, P.Van Isacker, S.A.Hamada, S.J.Robinson Mixed-Symmetry States and the Structure of 200Hg NUCLEAR REACTIONS 199Hg(n, γ), E=thermal; measured E(γ), I(γ), γγ-coin, γγ(θ). 200Hg deduced levels, J, π, δ(E2/M1), X(E0/E2), mixed-symmetry. Enriched target, Ge(Li) detectors.
doi: 10.1088/0954-3899/15/1/010
1989CO01 J.Phys.(London) G15, 321 (1989) S.P.Collins, S.A.Eid, S.A.Hamada, W.D.Hamilton, F.Hoyler A Search for Mixed-Symmetry States in the Mass A ≈ 50 Region RADIOACTIVITY 56Mn(β-); measured γ(θ). 56Fe levels deduced δ. Cryogenically oriented nuclei. NUCLEAR REACTIONS 47Ti, 53Cr, 57Fe(n, γ), E=thermal; measured γγ(θ). 48Ti, 54Cr, 58Fe levels deduced δ, μ, B(λ). Enriched target, on-line directional correlations.
doi: 10.1088/0954-3899/15/3/010
1988HA28 J.Phys.(London) G14, 1237 (1988) S.A.Hamada, W.D.Hamilton, B.More Gamma-Gamma Directional Correlation Measurements in 130,132Xe following Thermal Neutron Capture by Natural Xenon NUCLEAR REACTIONS 129,131Xe(n, γ), E=thermal; measured E(γ), I(γ), γγ(θ). 130,132Xe deduced levels, J, π, δ, B(λ). Model comparisons. NUCLEAR STRUCTURE 122,124,126,128,130,132Xe; calculated levels, δ, B(λ), potential energy surfaces. Interacting boson, dynamic deformation models.
doi: 10.1088/0305-4616/14/9/009
1987HA21 J.Phys.(London) G13, 1143 (1987) S.A.Hamada, W.D.Hamilton, F.Hoyler Gamma-Gamma Directional Correlation Measurements in 84Kr following Thermal Neutron Capture by Natural Krypton NUCLEAR STRUCTURE 82,84,86Kr; calculated levels, quadrupole moments, B(λ), δ, potential energy surfaces. Interacting boson model. NUCLEAR REACTIONS 83Kr(n, γ), E=thermal; measured Eγ, Iγ, γγ(θ). 84Kr deduced levels, J, π, δ. Natural gas target, directonal correlation system. Interacting boson model.
doi: 10.1088/0305-4616/13/9/015
1985SH04 Phys.Lett. 153B, 221 (1985) T.L.Shaw, V.R.Green, N.J.Stone, J.Rikovska, P.M.Walker, S.Collins, S.A.Hamada, W.D.Hamilton, I.S.Grant On-Line Nuclear Orientation of 118I and the Identification of the g9/2 Intruder Orbital RADIOACTIVITY 118,118mI(β+), (EC) [from 93Nb(32S, xnyp), E=175 MeV]; measured γγ-coin, γγ(θ), γ(θ), oriented nuclei; deduced μ. 118Te deduced level, J, π, K, γ-multipolarity, possible shape coexistence role.
doi: 10.1016/0370-2693(85)90535-0
Back to query form Note: The following list of authors and aliases matches the search parameter S.Hamada: , S.A.HAMADA |