NSR Query Results
Output year order : Descending NSR database version of April 11, 2024. Search: Author = H.M.Sengupta Found 102 matches. Showing 1 to 100. [Next]2016MA38 Pramana 86, 1275 (2016) U.K.Mazumder, A.Somadder, E.Hoque, Y.Haque, S.K.Das, H.M.Sen Gupta Analysis of the normal optical, Michel and molecular potentials on the 40Ca(6Li, d)44 Ti reaction NUCLEAR REACTIONS 40Ca(6Li, d), E=28 MeV; analyzed σ(θ) using full finite-range (FFR) distorted-wave Born approximation (DWBA) method for the 22 transitions involving both the bound and unbound states of 44Ti by using the normal optical, Michel and molecular potentials; deduced spectroscopic factors for the three optical potentials. Comparison with available data.
doi: 10.1007/s12043-016-1195-9
2010SA34 Int.J.Mod.Phys. E19, 2167 (2010) D.R.Sarker, M.A.Rahman, H.M.Sen Gupta A study of scattering of alpha particles from nuclei NUCLEAR REACTIONS 16O, 24,26Mg, 28,30Si, 34S, 40,48Ca, 46,50Ti, 52Cr, 56Fe, 58,60,62,64Ni, 90Zr, 120Sn, 148,150,152,154Sm, 208Pb(α, α), E=100-172.5 MeV; calculated σ(θ), interaction radius, surface diffuseness, deformation lengths leading to 2+, 3- states. Strong absorption model due to Frahn and Venter.
doi: 10.1142/S0218301310016570
2006AB32 Nucl.Phys. A775, 1 (2006) M.N.A.Abdullah, M.S.Sabra, M.M.Rashid, Z.Shehadeh, M.M.Billah, S.K.Das, M.A.Uddin, A.K.Basak, I.Reichstein, H.M.Sen Gupta, F.B.Malik Alpha-alpha potential up to 47.3 MeV bombarding energy NUCLEAR REACTIONS 4He(α, α), E=2.0-47.3 MeV; analysed σ, σ(θ); deduced parameters. 8Be deduced decay width. Various non-monotonic and Woods-Saxon α-nucleus potentials compared, phase shift effects discussed.
doi: 10.1016/j.nuclphysa.2006.06.007
2005AB24 Nucl.Phys. A760, 40 (2005) M.N.A.Abdullah, A.B.Idris, A.S.B.Tariq, M.S.Islam, S.K.Das, M.A.Uddin, A.S.Mondal, A.K.Basak, I.Reichstein, H.M.Sen Gupta, F.B.Malik Potentials for the α- 40, 44, 48Ca elastic scattering NUCLEAR REACTIONS 40,44,48Ca(α, α), E=10-180 MeV; analyzed σ(θ); deduced parameters. Non-monotonic and Squared Woods-Saxon α-nucleus potentials compared, dispersion effects discussed.
doi: 10.1016/j.nuclphysa.2005.05.149
2005BI23 Nucl.Phys. A762, 50 (2005) M.M.Billah, M.N.A.Abdullah, S.K.Das, M.A.Uddin, A.K.Basak, I.Reichstein, H.M.Sen Gupta, F.B.Malik Alpha-Ni optical model potentials NUCLEAR REACTIONS 58,60,62,64Ni(α, α), E ≈ 15-166 MeV; calculated σ(θ). Four optical potentials compared with data.
doi: 10.1016/j.nuclphysa.2005.07.020
2005HO12 J.Phys.(London) G31, 309 (2005) S.Hossain, M.N.A.Abdullah, S.K.Das, M.A.Uddin, A.K.Basak, H.M.Sen Gupta, I.J.Thompson, F.B.Malik Band mixing in 29Si and 29P NUCLEAR REACTIONS 28Si(α, t), (α, 3He), E=45 MeV; analyzed σ(E, θ). 29P, 29Si deduced configurations, band-mixing effects. Coupled channels approach, finite-range transfer theory, Nilsson model.
doi: 10.1088/0954-3899/31/5/003
2004SA28 Int.J.Mod.Phys. E13, 505 (2004) D.R.Sarker, L.Begum, Md.A.Rahman, H.M.Sen Gupta Strong absorption model studies of pion-nucleus scattering around the Δ resonance NUCLEAR REACTIONS 7Li, 9Be, 10B, 12,13C, 14N, 16O, 28Si, 40,42,44,48Ca, 51V, 54Fe, 58,60,62,64Ni, 104,106,108,110Pd, 118Sn, 206,208Pb(π+, π+), (π-, π-), E ≈ 80-800 MeV; analyzed σ(θ); deduced strong absorption model parameters. 28Si, 40,42,44,48Ca, 54Fe, 58,60,62,64Ni, 104,106,108,110Pd, 206,208Pb; deduced deformation parameters.
doi: 10.1142/S0218301304002314
2004SU22 Phys.Rev. C 70, 034612 (2004) S.A.Sultana, D.Maki, G.Wakabayashi, Y.Uozumi, N.Ikeda, Syafarudin, F.Aramaki, T.Kawaguchi, M.Matoba, H.M.Sen Gupta The 96Mo((p(pol)), d)95Mo reaction at 50 MeV NUCLEAR REACTIONS 96Mo(polarized p, d), E=50 MeV; measured deuteron spectra, σ(E, θ), analyzing powers. 95Mo deduced levels, J, π, spectroscopic factors. Comparison with model predictions.
doi: 10.1103/PhysRevC.70.034612
2003AB11 J.Phys.(London) G29, 1259 (2003) M.N.A.Abdullah, S.K.Das, A.S.B.Tariq, M.S.Mahbub, A.S.Mondal, M.A.Uddin, A.K.Basak, H.M.Sen Gupta, F.B.Malik Molecular versus squared Woods-Saxon α-nucleus potentials in the 27Al(α, t)28Si reaction NUCLEAR REACTIONS 27Al(α, t), (α, α), E=64.5 MeV; calculated σ(θ), σ(E, θ). Comparison of Woods-Saxon and molecular potentials, comparison with data.
doi: 10.1088/0954-3899/29/6/323
2003AB22 Phys.Lett. B 571, 45 (2003) M.N.A.Abdullah, M.S.I.Sarker, S.Hossain, S.K.Das, A.S.B.Tariq, M.A.Uddin, A.S.Mondal, A.K.Basak, S.Ali, H.M.Sen Gupta, F.B.Malik Cluster structure of 40, 44, 48Ca NUCLEAR REACTIONS 40,44,48Ca(α, α), E=22-166 MeV; analyzed σ(θ); deduced parameters. 40,44,48Ca deduced α-cluster structure. Folded potential.
doi: 10.1016/j.physletb.2003.08.014
2003AB24 Eur.Phys.J. A 18, 65 (2003) M.N.A.Abdullah, S.Hossain, M.S.I.Sarker, S.K.Das, A.S.B.Tariq, M.A.Uddin, A.K.Basak, S.Ali, H.M.Sen Gupta, F.B.Malik Cluster structure of 16O NUCLEAR REACTIONS 16O(α, α), E=25.4-146.0 MeV; calculated σ(θ). 16O deduced radius. Folding model, α-cluster configurations, comparisons with data.
doi: 10.1140/epja/i2003-10068-7
2002AB22 Eur.Phys.J. A 15, 477 (2002) M.N.A.Abdullah, M.S.Mahbub, S.K.Das, A.S.B.Tariq, M.A.Uddin, A.K.Basak, H.M.Sen Gupta, F.B.Malik Investigation of α-nucleus interaction in the 27Al(α, α)27Al scattering and 27Al(α, d)29Si reaction NUCLEAR REACTIONS 27Al(α, α), E=22.3-64.5 MeV; analyzed σ(θ); deduced potential parameters. 27Al(α, d), E=26.5, 27.2 MeV; calculated spectroscopic factors, σ(θ). Molecular and Michel potentials, DWBA.
doi: 10.1140/epja/i2002-10066-0
2002AF05 J.Phys.(London) G28, 223 (2002) S.Afroze Sultana, H.M.Sen Gupta A Study of the Inelastic Scattering of Pions from 40, 42, 44, 48Ca and 54Fe NUCLEAR REACTIONS 40,42,44,46,48Ca, 54Fe(π+, π+'), (π-, π-'), E=116-292.5 MeV; calculated σ(θ). 40,42,44,46,48Ca, 54Fe deduced levels deformation parameters following DWBA fit to inelastic data.
doi: 10.1088/0954-3899/28/2/303
2002SA49 Int.J.Mod.Phys. E11, 403 (2002) D.R.Sarker, H.Kabir, Md.A.Rahman, H.M.Sen Gupta Generalized Diffraction Model Study of Intermediate Energy Proton-Nucleus Scattering NUCLEAR REACTIONS 12C, 14N, 16O, 24,26Mg, 28Si, 32S, 40Ar, 40,42,44,48Ca, 48Ti, 58,60,62,64Ni, 90Zr, 120Sn, 144Sm, 208Pb(p, p), (p, p'), E ≈ 150-1000 MeV; analyzed σ(θ); deduced parameters. Optical and diffraction models.
doi: 10.1142/S0218301302000922
2001AK03 J.Phys.(London) G27, 755 (2001) Md.A.E.Akhter, S.Afroze Sultana, H.M.Sen Gupta, R.J.Peterson Local Optical Model Studies of Pion-Nucleus Scattering NUCLEAR REACTIONS 40,42,44,48Ca, 54Fe(π+, π+), (π-, π-), (π+, π+'), (π-, π-'), E=116, 180, 292.5 MeV; analyzed elastic and inelastic σ(θ); deduced optical model parameters.
doi: 10.1088/0954-3899/27/4/302
2001BB08 Eur.Phys.J. A 12, 387 (2001) A.K.Basak, M.N.A.Abdullah, A.S.B.Tariq, S.K.Das, A.F.M.M.Rahman, A.S.Mondal, H.M.Sen Gupta, F.B.Malik Investigation of Inelastic α-Scattering on 24Mg and 28Si NUCLEAR REACTIONS 24Mg(α, α'), E=54 MeV; 28Si(α, α'), E=26 MeV; measured σ(E, θ); deduced potential parameters. Coupled channels analysis.
doi: 10.1007/s10050-001-8662-4
2001DA19 Phys.Rev. C64, 034605 (2001) S.K.Das, A.S.B.Tariq, A.F.M.M.Rahman, S.Hossain, A.S.Mondal, A.K.Basak, H.M.Sen Gupta, F.B.Malik Effect of the α-Nucleus Interaction on the 29, 30Si(α, d)31, 32P Reaction NUCLEAR REACTIONS 29,30Si(α, d), E=25 MeV; calculated σ(E, θ), spectroscopic factors. Microscopic and macroscopic DWBA calculations, comparison of molecular, standard and squared Woods-Saxon α-nucleus potentials.
doi: 10.1103/PhysRevC.64.034605
2001SE01 Phys.Rev. C63, 017601 (2001) H.M.Sen Gupta, Syafarudin, S.Aoki, F.Aramaki, M.Matoba, Y.Uozumi, G.Wakabayashi, T.Sakae, N.Koori, T.Maki, M.Nakano, Y.Fujita, M.Fujiwara, H.Ikegami, I.Katayama, S.Morinobu, T.Yamazaki Isobaric Analog States Observed in the 58Ni(p, d)57Ni Reaction with 65 MeV Polarized Protons NUCLEAR REACTIONS 58Ni(polarized p, d), E=65 MeV; measured σ(θ), analyzing powers, deuteron spectra. 57Ni deduced levels, J, π, isobaric analog states, deviation from Coulomb displacement energy calculation. Finite range DWBA calculations.
doi: 10.1103/PhysRevC.63.017601
2000DA28 Phys.Rev. C62, 054605 (2000) S.K.Das, A.S.B.Tariq, M.A.Uddin, A.S.Mondal, A.K.Basak, K.M.Rashid, H.M.Sen Gupta, F.B.Malik Effect of α-Nucleus Potential on the 28Si(α, d)30P Reaction NUCLEAR REACTIONS 28Si(α, d), E=26 MeV; analyzed σ(E, θ). 30P level deduced J, π. DWBA calculations, several potentials compared.
doi: 10.1103/PhysRevC.62.054605
2000DA29 Phys.Rev. C62, 054606 (2000) S.K.Das, A.K.Basak, K.Banu, A.S.Mondal, A.S.B.Tariq, A.F.M.M.Rahman, H.M.Sen Gupta, F.B.Malik Effect of the α-Nucleus Potential on the 28Si(α, p)31P Reaction NUCLEAR REACTIONS 28Si(α, α), (α, p), E=26 MeV; analyzed σ(E, θ). DWBA calculations, several potentials compared.
doi: 10.1103/PhysRevC.62.054606
1999DA20 Phys.Rev. C60, 044617 (1999); Comment Phys.Rev. C62, 049801 (2000) S.K.Das, A.S.B.Tariq, A.F.M.Rahman, R.K.Roy, M.N.Huda, A.S.Mondal, A.K.Basak, H.M.Sen Gupta, F.B.Malik Effect of α-Nucleus Potential on the 27Al(α, t)28Si Reaction NUCLEAR REACTIONS 27Al(α, α), E=64.5 MeV; analyzed σ(θ); deduced parameters. 27Al(α, t), E=64.5 MeV; calculated σ(E, θ). 28Si deduced spectroscopic factors. Finite-range DWBA, molecular and Michel optical potentials. Comparisons with data.
doi: 10.1103/PhysRevC.60.044617
1999DA24 Nuovo Cim. 112A, 661 (1999) S.K.Das, A.K.Basak, A.S.Mondal, A.S.B.Tariq, A.F.M.Rahman, D.R.Sarker, H.M.Sen Gupta Normalization Constant of the (α, t) Reaction NUCLEAR REACTIONS 16O, 19F, 25Mg, 27Al, 30Si, 40Ca, 51V, 55Mn, 54Fe, 59Co, 64Ni, 116Sn, 144Sm, 208Pb(α, t), E=25-104 MeV; analyzed σ(θ); deduced normalization constant. DWBA analysis.
doi: 10.1007/BF03035876
1999HA66 Nuovo Cim. 112A, 1049 (1999) E.Hai, S.Soheli, Md.A.Rahman, H.M.Sen Gupta Inelastic Scattering of Pion Leading to the Lowest Octupole States in Nuclei NUCLEAR REACTIONS 18O, 28Si, 40,42,44,48Ca, 58Ni, 208Pb(π+, π+'), (π-, π-'), E=164-292 MeV; analyzed σ(E, θ) for transitions to lowest octupole state; deduced parameters. Strong absorption model.
doi: 10.1007/BF03035911
1999RA24 Nuovo Cim. 112A, 587 (1999) Md.A.Rahman, Md.Sirajum Munir, H.M.Sen Gupta Heavy Ion Nucleus Scattering NUCLEAR REACTIONS 24Mg, 40Ca(6Li, 6Li), E=20 MeV; 28Si(6Li, 6Li), E=20, 318 MeV; 16O, 28Si(7Li, 7Li), E=20 MeV; 28Si(12C, 12C), E=40.2 MeV; 12C, 16O, 28Si, 32S(13C, 13C), E=36 MeV; 40Ca, 88Sr(14C, 14C), E=51 MeV; 24Mg, 27Al, 28Si(14N, 14N), E ≈ 53 MeV; 40Ca(16O, 16O), E=104, 214, 310 MeV; 208Pb(28Si, 28Si), E=209.8 MeV; analyzed σ(θ); deduced parameters. Strong absorption model.
doi: 10.1007/BF03035870
1999RO27 Nuovo Cim. 112A, 1041 (1999) J.Roy, S.Soheli, Md.A.Rahman, H.M.Sen Gupta The Antiproton-Nucleus Scattering NUCLEAR REACTIONS 12C, 16,18O, 27Al, 40Ca, Cu, 208Pb(p-bar, p-bar), E ≈ 47-180 MeV; 12C, 18O(p-bar, p-bar'), E ≈ 47, 180 MeV; analyzed σ(θ), σ(E, θ); deduced parameters. 12C, 18O deduced deformation lengths. Strong absorption model.
doi: 10.1007/BF03035910
1999TA13 Phys.Rev. C59, 2558 (1999) A.S.B.Tariq, A.F.M.M.Rahman, S.K.Das, A.S.Mondal, M.A.Uddin, A.K.Basak, H.M.Sen Gupta, F.B.Malik Potential Description of Anomalous Large Angle Scattering of α Particles NUCLEAR REACTIONS 28Si(α, α), E=14.47-45 MeV; 30Si(α, α), E=26.6 MeV; 24Mg(α, α), E=22-120 MeV; analyzed σ(θ); deduced potential parameters. Michel, molecular potentials, anomalous large angle scattering.
doi: 10.1103/PhysRevC.59.2558
1998AH06 Nuovo Cim. 111A, 113 (1998) M.Ahmed, Md.A.E.Akhter, Md.A.Rahman, H.M.Sen Gupta, M.Rahman Scattering of Pions from Light Nuclei NUCLEAR REACTIONS 6Li, 12,14C, 13N(π+, π+), (π-, π-), E=100-280 MeV; 16O(π+, π+), E=114-343 MeV; analyzed σ(θ); deduced parameters. Generalized diffraction model.
1998HA68 Nuovo Cim. 111, 1131 (1998) M.Haque, S.K.Das, A.K.Basak, H.M.Sen Gupta Anomaly in the Normalization Constant of the (3He, p) Reaction NUCLEAR REACTIONS 62Ni(3He, p), E not given; calculated DWBA normalization constants; deduced dependence on final level, possible multi-step mechanisms.
1997AH09 Nuovo Cim. 110A, 1393 (1997) M.Ahmed, Md.A.Rahman, H.M.Sen Gupta Scattering of Pions from 90Zr and 118Sn Around the Δ Resonance NUCLEAR REACTIONS 90Zr, 118Sn(π+, π+), (π+, π+'), (π-, π-), (π-, π-'), E=163 MeV; analyzed σ(θ); deduced interaction radius, surface diffuseness, deformation parameters. Generalized diffraction model.
1997BA60 Phys.Rev. C56, 1983 (1997) A.K.Basak, M.A.Basher, A.S.Mondal, M.A.Uddin, S.Bhattacherjee, A.Husain, S.K.Das, M.Haque, H.M.Sen Gupta 64Cu Levels from the 62Ni(3He, p) Reaction at 18 MeV NUCLEAR REACTIONS 62Ni(3He, p), E=18 MeV; measured proton spectra, σ(Ep, θ); deduced optical model parameters. 64Cu levels deduced J, π. Shell model analysis.
doi: 10.1103/PhysRevC.56.1983
1996MA11 Phys.Rev. C53, 1792 (1996) M.Matoba, K.Kurohmaru, O.Iwamoto, A.Nohtomi, Y.Uozumi, T.Sakae, N.Koori, H.Ohgaki, H.Ijiri, T.Maki, M.Nakano, H.M.Sen Gupta (p, d) Reaction on 62Ni at 65 MeV NUCLEAR REACTIONS 62Ni(polarized p, d), E=65 MeV; measured σ(Ed, θ), analyzing power vs Ed, θ. 61Ni deduced levels, J, π. DWBA analyses. Enriched target. Other data discussed, analyzed.
doi: 10.1103/PhysRevC.53.1792
1994SO26 J.Phys.Soc.Jpn. 63, 2572 (1994) S.Soheli, E.Hai, Md.A.Rahman, H.M.Sen Gupta, M.Rahman The Triton-Nucleus Scattering NUCLEAR REACTIONS 9Be, 30Si, 32S, 40Ca, 46,48Ti, 54,56Fe, 58,60Ni, 68Zn, 90,94Zr, 116Sn, 140Ce, 208Pb(t, t), E=17 MeV; 40Ca, 52Cr, 54Fe, 62,64Ni, 90,92,94,96Zr, 116,118,120,122,124Sn, 182W, 207,208Pb(t, t), E=20 MeV; 19F, 24Mg, 40,48Ca, 51V, 56Fe, 58Ni, 89Y(t, t), E=33 MeV; analyzed σ(θ). 30Si(t, t'), E=17 MeV; 90,92,94,96Zr(t, t'), E=20 MeV; analyzed σ(θ); deduced model parameters. 30Si, 32S, 90,92,94,96Zr levels deduced deformation parameters β2. Strong absorption model.
doi: 10.1143/JPSJ.63.2572
1992BA16 Phys.Rev. C45, 1575 (1992) M.A.Basher, H.R.Siddique, A.Husain, A.K.Basak, H.M.Sen Gupta Level Structure of 52Cr from the 51V(3He, d) Reaction NUCLEAR REACTIONS 51V(3He, d), E=15 MeV; measured σ(θ). 52Cr deduced levels, L, J, π, spectroscopic factors. DWBA analysis.
doi: 10.1103/PhysRevC.45.1575
1992CH39 Phys.Rev. C46, 2273 (1992) M.S.Chowdhury, M.A.Zaman, H.M.Sen Gupta 18O(3He, p)20F Reaction NUCLEAR REACTIONS 18O(3He, p), E=18 MeV; measured σ(E, θ). 20F deduced levels, L, J, π limits. Enriched tatget. DWBA analysis.
doi: 10.1103/PhysRevC.46.2273
1992RA15 Nuovo Cim. 105A, 729 (1992) Nuclear Inelastic-Scattering Cross-Section for Transitions L = 2 and 3 in the Strong-Absorption Model NUCLEAR REACTIONS 48Ti(α, α'), E=28 MeV; analyzed σ(θ). Strong absorption model.
doi: 10.1007/BF02730779
1992RA21 Nuovo Cim. 105A, 851 (1992) Md.A.Rahman, S.C.Paul, H.M.Sen Gupta, M.Rahman Strong-Absorption Model Analysis of Alpha Scattering NUCLEAR REACTIONS 20Ne, 24Mg, 27Al, 28Si, 48Ti, 59Co, 60,58Ni, Ag, 113Cd, 119Sn(α, α), E=28 MeV; 46Ti, 58Fe, 58,62,64Ni, 64Zn, 40Ca, 58Ni(α, α), E ≈ 21-85.6 MeV; analyzed σ(θ); deduced interaction radius, surface diffuseness parameters. Strong absorption model.
doi: 10.1007/BF02799100
1992RA31 Nuovo Cim. 105A, 1767 (1992) Md.A.Rahman, S.K.Sarker, H.M.Sen Gupta Deuteron-Nucleus Scattering at E(d) = 34 and 80 MeV NUCLEAR REACTIONS, ICPND 48,49,50Ti, 63,65Cu, 92,94Zr(d, d), E=34 MeV; 120Sn, 208Pb(d, d), 68Zn, 120Sn(d, d'), E=80 MeV; 12C, 58Ni, 68Zn, 120Sn(d, d'), E=82 MeV; analyzed σ(θ); deduced model parameters, reaction σ. 12C, 58Ni, 68Zn, 120Sn level deduced deformation parameter. Strong absorption model.
doi: 10.1007/BF02740926
1992RO12 Phys.Rev. C46, 144 (1992) J.N.Roy, A.R.Majumder, H.M.Sen Gupta 45Sc(d, p)46Sc Reaction NUCLEAR REACTIONS 45Sc(d, p), E=12 MeV; measured σ(θ). 46Sc deduced levels, L, J, π, spectroscopic factors. Nonlocal finite-range DWBA analysis.
doi: 10.1103/PhysRevC.46.144
1991RA22 Phys.Rev. C44, 2484 (1991) Md.A.Rahman, H.M.Sen Gupta, M.Rahman Strong Absorption Model for Pion-Nucleus Scattering Around the (3, 3) Resonance NUCLEAR REACTIONS 18O, 24,26Mg, 56,54Fe, 48,50Ti, 40,44Ca, 52Cr(π+, π+), (π-, π-), E=180 MeV; 18O(π+, π+), (π-, π-), E=164, 230 MeV; 40,48,44Ca(π+, π+), (π-, π-), E=116 MeV; 28Si, 58Ni, 208Pb(π+, π+), (π-, π-), E=162 MeV; 40,42,44,48Ca, 54Fe(π+, π+), (π-, π-), E=292.5 MeV; analyzed σ(θ); deduced model parameters. 24,26Mg, 42,44,48Ca, 48Ti, 54,56Fe, 18O, 24,26Mg, 28Si, 58Ni, 52Cr levels deduced β2. Strong absorption model.
doi: 10.1103/PhysRevC.44.2484
1990BE19 Nuovo Cim. 103A, 865 (1990) R.Begum, D.K.Banik, Md.A.Rahman, A.R.Majumder, H.M.Sen Gupta Low-Lying Levels in 44Sc Populated in the (d, t) Reaction on 45Sc NUCLEAR REACTIONS 45Sc(d, t), E=12 MeV; measured σ(θ). 44Sc levels deduced spectroscopic factors. DWBA analysis.
doi: 10.1007/BF02799233
1990RA09 Phys.Rev. C41, 2305 (1990); Erratum Phys.Rev. C44, 566 (1991) Md.A.Rahman, H.M.Sen Gupta, M.Rahman Pion-Nucleus Scattering Around the (3, 3) Resonance NUCLEAR REACTIONS 28Si, 40Ar, 40,48Ca, 208Pb(π+, π+), (π-, π-), E=80-230 MeV; 28Si(π+, π+'), (π-, π-'), E=130-226 MeV; calculated σ(θ); deduced model parameters. 28Si level deformation parameter. Strong absorption model.
doi: 10.1103/PhysRevC.41.2305
1990SE03 Nucl.Phys. A512, 97 (1990) H.M.Sen Gupta, J.B.A.England, F.Khazaie, E.M.E.Rawas, G.T.A.Squier Level Structure of 61Cu from the (3He, d) Reaction on 60Ni NUCLEAR REACTIONS 60Ni(3He, d), E=33 MeV; measured σ(Ed, θ). 61Cu deduced levels, L, S. Enriched target.
doi: 10.1016/0375-9474(90)90005-7
1990SE07 J.Phys.(London) G16, 1039 (1990) H.M.Sen Gupta, J.B.A.England, E.M.E.Rawas, F.Khazaie, G.T.A.Squier A Study of the (3He, α) Reaction on 60Ni NUCLEAR REACTIONS 60Ni(3He, α), E=33 MeV; measured σ(Eα), σ(θ). 59Ni deduced levels, spectroscopic factors.
doi: 10.1088/0954-3899/16/7/015
1990SE12 Nucl.Phys. A517, 82 (1990) H.M.Sen Gupta, J.B.A.England, F.Khazaie, E.M.W.Rawas, G.T.A.Squier A Study of the (3He, p) Reaction on 60Ni NUCLEAR REACTIONS 60Ni(3He, p), E=33 MeV; measured σ(Ep, θ). 62Cu deduced levels, L, J, π. Enriched targets.
doi: 10.1016/0375-9474(90)90261-J
1988RA20 Nuovo Cim. 99A, 317 (1988) Md.A.Rahman, S.N.Rahman, H.M.Sen Gupta, H.-J.Trost, P.Lezoch, U.Strohbusch Alpha-Spectroscopic Factors from (d, 6Li) and (3He, 7Be) Reaction on 12C, 24Mg, 40Ca and 58Ni NUCLEAR REACTIONS 12C, 24Mg, 40Ca, 58Ni(3He, 7Be), E=41 MeV; measured σ(E(7Be)), σ(θ). 12C, 24Mg, 40Ca, 58Ni deduced α spectroscopic factors. Analysis of (d, 6Li) data.
doi: 10.1007/BF02733824
1988RA28 Nuovo Cim. 100A, 427 (1988) Md.A.Rahman, H.M.Sen Gupta, U.Strohbusch (7Li, t) Reaction on 40Ca, 44Ca and 58Ni NUCLEAR REACTIONS 40,44Ca, 58Ni(7Li, t), E=34 MeV; analyzed σ(θ); deduced model parameters. 44,48Ti, 62Zn levels deduced relative Sα.
doi: 10.1007/BF02812970
1987MO17 Nuovo Cim. 97A, 211 (1987) N.I.Molla, M.Rahman, S.Khatun, H.M.Sen Gupta A Study of (p, γ) Resonance Reactions on 27Al and 45Sc NUCLEAR REACTIONS 27Al, 45Sc(p, γ), E=1026-2044 keV; measured Eγ, Iγ, γ(θ). 28Si, 46Ti deduced levels, J, π, γ-branching. NaI detector.
doi: 10.1007/BF02734932
1987RA36 Nuovo Cim. 98A, 513 (1987) M.Rahman, H.M.Sen Gupta, Md.A.Rahman, Abu Bakar Siddique Strong-Absorption Model Analysis of 3He Scattering NUCLEAR REACTIONS 10B, 12,13C, 58Ni, 56Fe, 144Sm(3He, 3He), E=41 MeV; 16,18O, 23Na, 24,25,26Mg, 27Al, 40Ca(3He, 3He), E=25, 41 MeV; 28,29,30Si, 31P, 35,37Cl, 39K(3He, 3He), E=25 MeV; 19F(3He, 3He), E=25 MeV; analyzed σ(θ); deduced model parameters. 18O, 24Mg, 56Fe level deduced deformation parameter.
doi: 10.1007/BF02902093
1987SE17 Nuovo Cim. 98A, 715 (1987) H.M.Sen Gupta, M.S.Chowdhury, F.Watt, M.J.Hurst A Study of Some (sd)4 Shell Model States in 20F via the 18O(3He, p) Reaction NUCLEAR REACTIONS 18O(3He, p), E=18 MeV; analyzed σ(θ); deduced model parameters. Microscopic two-particle DWBA.
1986RA15 Nuovo Cim. 93A, 236 (1986) Spectroscopic Information from (3He, 7Be) Reaction on 12C and 24Mg NUCLEAR REACTIONS 12C, 24Mg(3He, 7Be), E=41 MeV; measured σ(θ); deduced model parameters. 24Mg, 12C deduced relative spectroscopic factor Sα. DWBA analysis.
doi: 10.1007/BF02773652
1986RA19 Nuovo Cim. 93A, 373 (1986) M.Rahman, N.I.Molla, S.Khatun, H.M.Sen Gupta A Study of Some Proton Capture Resonance Reactions on 52Cr and 56Fe NUCLEAR REACTIONS 52Cr(p, γ), E=1388, 1395, 1608, 1901 keV; 56Fe(p, γ), E=1248, 1652, 2065 keV; measured Eγ, Iγ, γ(θ). 53Mn, 57Co deduced levels, J, π, γ-multipolarity, δ. Enriched 52Cr, natural iron target, Ge(Li), NaI(Tl) detectors.
doi: 10.1007/BF02780654
1986SE08 Nuovo Cim. 93A, 217 (1986) H.M.Sen Gupta, M.A.Zaman, F.Watt, M.J.Hurst A Study of the 17O(3He, p)19F Reaction NUCLEAR REACTIONS 17O(3He, p), E=18 MeV; measured σ(Ep), σ(θ); deduced model parameters. 19F levels deduced L, configuration, normalization factor. DWBA, two-nucleon spectroscopic amplitudes.
1985FO02 Phys.Rev. C31, 392 (1985) H.T.Fortune, M.Carchidi, H.Banu, H.M.Sen Gupta Level Structures of 61Co via the Reaction 59Co(t, p)61Co NUCLEAR REACTIONS 59Co(t, p), E=15 MeV; measured σ(E), σ(θ); deduced optical model parameters. 61Co levels deduced, L. DWBA analysis.
doi: 10.1103/PhysRevC.31.392
1984CH29 Nuovo Cim. 82A, 292 (1984) M.S.Chowdhury, H.M.Sen Gupta, M.A.M.Shahabuddin Bound Levels in 29P Populated in the 28Si(3He, d) Reaction NUCLEAR REACTIONS 28Si(3He, d), E=17 MeV; measured σ(θd); deduced reaction mechanism. 29P levels deduced J, π, C2S. Single-step DWBA analysis.
doi: 10.1007/BF02773556
1982HA11 Nucl.Phys. A378, 11 (1982) Hamida Banu, H.M.Sen Gupta, F.Watt Level Structure of 46Ti from the (τ, d) Reaction on 45Sc NUCLEAR REACTIONS 45Sc(3He, d), E=16 MeV; measured σ(Ed, θ). 46Ti deduced levels, L, π, C2S. Natural target.
doi: 10.1016/0375-9474(82)90380-3
1981RA05 Lett.Nuovo Cim. 30, 259 (1981) Strong-Absorption Model for Scattering of 3He Particles. NUCLEAR REACTIONS 89Y, 27Al, 51V(3He, 3He), E=29.6 MeV; 59Co, 60Ni, 116Sn(3He, 3He), E=29.6 MeV; 90Zr, 115In(3He, 3He), E=29.8 MeV; 114Cd(3He, 3He), E=29.7 MeV; 59Co(3He, 3He), E=34.8 MeV; 60Ni(3He, 3He), E=35.1 MeV; 115In(3He, 3He), E=35.3 MeV; 116Sn(3He, 3He), E=35.2 MeV; calculated σ(θ). 56,58Fe, 58Ni(3He, 3He'), E=22 MeV; 24Mg(3He, 3He'), E=29 MeV; analyzed σ(θ). 24Mg, 56,58Fe, 58Ni level deduced β2. Strong absorption model.
1981ZA04 Lett.Nuovo Cim. 30, 279 (1981) M.A.Zaman, A.R.Majumder, M.S.Chowdhury, H.M.Sen Gupta A Study of the (d, t) Reaction on 56Fe NUCLEAR REACTIONS 56Fe(d, t), E=12 MeV; measured σ(θ). 55Fe levels deduced L, C2S. Local, zero-range DWBA analysis. Enriched targets, multichannel magnetic spectrograph.
doi: 10.1007/BF02759276
1980UL01 Nucl.Phys. A337, 231 (1980) A Study of Some Resonances in the 54Fe(p, γ)55Co Reaction NUCLEAR REACTIONS 54Fe(p, γ), E=1.100-1.760 MeV; measured σ(E; Eγ, θ). 55Co deduced levels, IAR, J, δ, resonance strengths, Γγ. Enriched target.
doi: 10.1016/0375-9474(80)90053-6
1980ZA05 J.Phys.(London) G6, 1119 (1980) M.A.Zaman, H.M.Sen Gupta, F.Watt A Study of the (τ, α) Reaction on 56Fe NUCLEAR REACTIONS 56Fe(3He, α), E=18 MeV; measured σ(Eα, θ). 56Fe deduced levels, L, J, π, C2S. Enriched target, DWBA analysis.
doi: 10.1088/0305-4616/6/9/009
1979AW02 Nuovo Cim. 52A, 175 (1979) N.A.Awal, W.M.Zuk, H.M.Sen Gupta The Gamma-Decay of the 1644 and 1650 keV Resonances in the 44Ca(p, γ)45Sc Reaction NUCLEAR REACTIONS 44Ca(p, γ), E=1644, 1650 keV; measured γ(θ). 45Sc deduced levels, J, π.
doi: 10.1007/BF02902044
1978BA51 Nucl.Phys. A307, 106 (1978) A Study of the Level Properties of 57Co from the (τ, d) Reaction on 56Fe NUCLEAR REACTIONS 56Fe(3He, d), E=18 MeV; measured σ(Ed, θ). 57Co deduced levels, L, J, π, C2S. Enriched target.
doi: 10.1016/0375-9474(78)90430-X
1978HA16 Nucl.Phys. A299, 99 (1978) S.J.Hall, H.R.Siddique, H.M.Sen Gupta Elastic Scattering of Neutrons from 28Si and 32S NUCLEAR REACTIONS 28Si, 32S(n, n), E=0.6-3.6 MeV; measured σ(E, θ). Optical model analysis. Natural targets.
doi: 10.1016/0375-9474(78)90211-7
1978RO18 J.Phys.(London) G4, 1469 (1978) J.N.Roy, H.M.Sen Gupta, A.R.Majumder, T.Congedo, J.E.Alzona Level Properties of 60Co from the (d, p) Reaction on 59Co NUCLEAR REACTIONS 59Co(d, p), E=14 MeV; measured σ(Ep, θ). 60Co deduced levels, L, J, π, C2S. Natural target. DWBA analysis.
doi: 10.1088/0305-4616/4/9/018
1978UL03 Nucl.Sci.Appl., Ser.B 11, 8 (1978) The Gamma Decay Properties of the Resonance State at Ep = 1679 keV in The 54Fe(p, γ)55Co Reaction NUCLEAR REACTIONS 54Fe(p, γ), E=1679 keV; measured Eγ, Iγ, γ(θ). 55Co deduced resonance strength, Γγ, J, π, levels, δ. Legendre polynomial analysis.
1978ZA03 Nuclear Phys. A295, 451 (1978) M.A.Zaman, H.M.Sen Gupta, F.Watt, M.J.Hurst A Study of the (τ, α) Reaction on 50Cr NUCLEAR REACTIONS 50Cr(3He, α), E=16 MeV; measured σ(Eα, θ). 49Cr deduced levels, L, J, π, C2S. Enriched target.
doi: 10.1016/0375-9474(78)90186-0
1977CH12 Nucl.Phys. A282, 87 (1977) M.S.Chowdhury, A.R.Majumder, H.M.Sen Gupta Level Structure of 51Cr from the (d, p) Reaction on 50Cr NUCLEAR REACTIONS 50Cr(d, p), E=12 MeV; measured σ(Ep, θ). 51Cr deduced levels, L, J, π, C2S. Enriched target.
doi: 10.1016/0375-9474(77)90173-7
1977EN01 Nucl.Phys. A284, 29 (1977) J.B.A.England, E.Casal, A.Garcia, T.Picazo, J.Aguilar, H.M.Sen Gupta Optical Model Analysis of the Elastic Scattering of 20-24 MeV α-Particles by 12C, 14N, 16O, and 20Ne NUCLEAR REACTIONS 12C, 14N, 16O, 20Ne(α, α), E=20-24 MeV; measured σ(E, θ). Optical model analysis.
doi: 10.1016/0375-9474(77)90683-2
1977RA21 Pramana 8, 478 (1977) M.A.Rahman, M.A.Awal, M.Rahman, H.M.Sengupta, S.K.Gupta High Resolution Gamma-Ray Spectroscopy of the 27Al(p, γ)28Si Resonance Reaction NUCLEAR REACTIONS 27Al(p, γ), E=2.4-2.75 MeV; measured Eγ, Iγ. 28Si deduced resonances, J, π, γ-branching.
doi: 10.1007/BF02862903
1977SE08 Nucl.Phys. A285, 45 (1977) H.M.Sen Gupta, A.R.Majumder, M.S.Chowdhury A Study of the (τ, α) Reaction on 54Fe NUCLEAR REACTIONS 54Fe(3He, α), E=18 MeV; measured σ(Eα, θ). 53Fe deduced levels, L, C2S, J, π. Enriched target.
doi: 10.1016/0375-9474(77)90145-2
1976AH08 Nuovo Cim. 33A, 592 (1976) N.Ahmed, M.A.Rahman, S.Khatun, M.A.Awal, M.Rahman, A.K.M.Siddiq, H.M.Sen Gupta Isobaric Analogue States in 60Ni from (p, γ) and (p, n) Reactions in 59Co NUCLEAR REACTIONS 59Co(p, γ), (p, n), E=2.43-3.05 MeV; measured σ(E). 60Co deduced levels, resonances, Γ.
doi: 10.1007/BF02729874
1976AW02 Nucl.Sci.Appl., Ser.B 9, 1 (1976) M.A.Awal, H.M.Sen Gupta, G.U.Din Energy Levels of 55Co from 54Fe(p, γ)55Co Reaction NUCLEAR REACTIONS 54Fe(p, γ), E=1286, 1680, 1747 keV; measured Eγ, Iγ. 55Co deduced levels, transitions.
1976AW03 Nucl.Sci.Appl., Ser.B 9, 7 (1976) M.A.Awal, M.A.Rahman, M.Rahman, H.M.Sen Gupta Probable Isobaric Analogue States in 57Co from (p, γ) Reaction in 56Fe NUCLEAR REACTIONS 56Fe(p, γ), E=1.2-3.03 MeV; measured σ(E, Eγ). 57Co deduced IAS.
1976RA39 Lett.Nuovo Cim. 15, 27 (1976) M.Rahman, M.Salimullah, H.M.Sen Gupta On Possible Magicity of Superheavy Nuclei NUCLEAR STRUCTURE A > 200; calculated possible magicity.
doi: 10.1007/BF02725374
1976SE10 Nucl.Phys. A267, 205 (1976) H.M.Sen Gupta, T.A.Belote, D.Roaf A Study of the Level Structure of 20Ne from the (3He, d) Reaction on 19F NUCLEAR REACTIONS 19F(3He, d), E=16 MeV; measured σ(Ed, θ). 20Ne levels deduced C2S.
doi: 10.1016/0375-9474(76)90712-0
1976SE12 J.Phys.(London) G2, 935 (1976) H.M.Sen Gupta, M.J.Hurst, F.Watt A Study of the Reaction 16O(3He, p)18F NUCLEAR REACTIONS 16O(3He, p), E=18 MeV; measured σ(Ep, θ). 18F deduced levels, J, π. DWBA analysis.
doi: 10.1088/0305-4616/2/12/010
1975MA06 Nucl.Phys. A238, 1 (1975) A.R.Majumder, M.S.Chowdhury, H.M.Sen Gupta, A.Guichard Level Properties of 50V Through the 51V(τ, α) Reaction NUCLEAR REACTIONS 51V(3He, α), E=18.0 MeV; measured σ(Eα, θ). 50V deduced levels, L, C2S, π. Natural target.
doi: 10.1016/0375-9474(75)90337-1
1975RA04 Lett.Nuovo Cim. 12, 290 (1975) M.A.Rahman, M.A.Awal, M.Rahman, H.M.Sen Gupta, S.K.Gupta A Note on the Possible 4+ Analogue-Antianalogue States in 28Si NUCLEAR REACTIONS 27Al(p, γ), E > 2 MeV; measured σ(E, Eγ, θ). 28Si deduced resonance, J, π, L.
doi: 10.1007/BF02790602
1974CH41 Nucl.Phys. A229, 484 (1974) Level Structure of 47Ti from the (d, p) Reaction in 46Ti NUCLEAR REACTIONS 46Ti(d, p), E=10 MeV; measured σ(Ep, θ). 47Ti deduced levels, L, J, π, C2S. Enriched target.
doi: 10.1016/0375-9474(74)90666-6
1974RA32 Nucl.Sci.Appl., Ser.B 7, 5 (1974) M.Rahman, H.M.Sen Gupta, D.Husain Two-Particle (γ, n) Photodisintegration of the Alpha Particle NUCLEAR REACTIONS 4He(γ, n), E < 100 MeV; calculated σ(E).
1974RA33 Nucl.Sci.Appl., Ser.B 7, 21 (1974) M.A.Rahman, M.A.Awal, M.Rahman, H.M.Sen Gupta Isobaric Analogue States in 46Ti from (p, γ) Reaction in 45Sc NUCLEAR REACTIONS 45Sc(p, γ), E < 3 MeV; measured σ(E, Eγ); deduced Coulomb displacement energy. 46Ti deduced resonances.
1973AH03 J.Phys.Soc.Jap. 35, 348 (1973) N.Ahmed, M.A.Rahman, M.A.Awal, M.Rahman, S.Khatun, H.M.Sen Gupta A Study of the Isobaric Analogue States in 56Fe from (p, γ) and (p, n) Reactions in 55Mn NUCLEAR REACTIONS 55Mn(p, γ), (p, n), E=1.3-3.012 MeV; measured σ(E), Eγ. 55,56Fe resonances deduced level-width. Coulomb displacement energy.
doi: 10.1143/JPSJ.35.348
1973CH11 Nucl.Phys. A205, 454 (1973) A Study of Nuclear Structure in 59Ni from the (d, p) Reaction on 58Ni NUCLEAR REACTIONS 58Ni(d, p), E=10 MeV; measured σ(Ep', θ). 59Ni deduced levels, L, J, π, S. Enriched target.
doi: 10.1016/0375-9474(73)90699-4
1973CH30 Lett.Nuovo Cim. 6, 587 (1973) Evidence for f7/2 Neutron Holes in the Ground-State Configuration of 58Ni from the 58Ni(d, p) Reaction NUCLEAR REACTIONS 58Ni(d, p), E=10 MeV; measured σ(Ep, θ). 59Ni deduced levels, J, π, L, S.
doi: 10.1007/BF02827077
1973MA25 Nucl.Phys. A209, 615 (1973) A.R.Majumder, H.M.Sen Gupta, A.Guichard A Study of the (d, α) Reaction in 56Fe at 12 MeV NUCLEAR REACTIONS 56Fe(d, α), E=12 MeV; measured σ(Eα', θ). 54Mn deduced levels, J, π, L. Enriched target.
doi: 10.1016/0375-9474(73)90850-6
1973MA58 Indian J.Phys. 47, 396 (1973) A Study of the Low-Lying Levels in 55Fe from the (d, t) Reaction on 56Fe NUCLEAR REACTIONS 56Fe(d, t), E=12 MeV; measured σ(Et, θ). 55Fe levels deduced J, π, S, L.
1972AH01 Lett.Nuovo Cim. 3, 299 (1972); Erratum Lett.Nuovo Cim. 6, 388 (1973) N.Ahmed, M.A.Rahman, S.Khatun, M.A.Awal, H.M.Sen Gupta Evidence for Some Isobaric Analogue States in 55Co from (p, γ) Reaction NUCLEAR REACTIONS 54Fe(p, γ), E < 3 MeV; measured σ(E;Eγ). 55Co deduced isobaric analog resonances. 55Co - 55Fe deduced Coulomb displacement energy.
doi: 10.1007/BF02780737
1972AH08 Nuovo Cim. 11A, 476 (1972); Erratum Nuovo Cim. 14A, 224 (1973) N.Ahmed, M.A.Rahman, M.Rahman, H.M.Sen Gupta A Study of the Low-Lying Isobaric Analogue States in 52Cr from (p, γ) and (p, n) Reactions in 51V NUCLEAR REACTIONS 51V(p, γ), (p, n), E < 3.12 MeV; measured σ(E). 52Cr deduced IAR, level-width, Coulomb displacement energy.
doi: 10.1007/BF02728888
1972AH09 Z.Phys. 257, 380 (1972) N.Ahmed, M.A.Rahman, S.Khatun, M.A.Awal, M.Rahman, H.M.Sen Gupta Isobaric Analogue States in 28Si from (p, γ) Reaction in 27Al NUCLEAR REACTIONS 27Al(p, γ), E=0.85-3.0 MeV; measured σ(E;Eγ). 28Si deduced analog resonances, Coulomb displacement energy.
doi: 10.1007/BF01401521
1971AH02 Lett.Nuovo Cim. 1, 327 (1971) N.Ahmed, M.A.Rahman, M.Rahman, H.M.Sen Gupta, M.A.S.Khan, T.Hossain Isobaric Analogue States in 52Cr from (p, γ) and (p, n) Reactions in 51V NUCLEAR REACTIONS 51V(p, γ), (p, n), E=2-3 MeV; measured σ(E;Eγ), σ(E;En). 52Cr deduced resonances, isobaric analog. 52Cr-52V deduced Coulomb energy difference.
doi: 10.1007/BF02784684
1971RA11 Nucl.Phys. A168, 314 (1971) M.Rahman, H.M.Sen Gupta, D.Husain Two-Particle (γ, n) Photodisintegration of the Triton NUCLEAR REACTIONS 3H(γ, n), E < 30 MeV; calculated σ(E). Modified Irving wave function, final-state interaction.
doi: 10.1016/0375-9474(71)90796-2
1971RA32 Nuovo Cim. 4A, 588 (1971) M.Rahman, A.J.H.Begum, H.M.Sen Gupta Strong-Absorption Model for Scattering of Deuterons NUCLEAR REACTIONS Mg, Fe, Ni, Zn, Zr, Ag, Ce, Ta, Au(d, d), E=26 MeV; analyzed σ(θ). Strong absorption model. 24Mg, 56Fe, 58Ni, Zn, 140Ce(d, d'), E=26 MeV; analyzed σ(θ). 24Mg, 56Fe, 58Ni, Zn, 140Ce deduced deformation parameter β2.
doi: 10.1007/BF02731374
1971SE01 Nucl.Phys. A160, 529 (1971) H.M.Sen Gupta, A.R.Majumder, E.K.Lin A Study of the Level Structure in 57Fe from the (d, p) Reaction on 56Fe NUCLEAR REACTIONS 56Fe(d, p), E=12 MeV; measured σ(Ep', θ). 57Fe deduced levels, J, π, S. Enriched target.
doi: 10.1016/0375-9474(71)90096-0
1970RA27 Nuovo Cimento 68A, 397 (1970) M.Rahman, M.U.Ahmed, H.M.Sen Gupta Strong-Absorption Model for Scattering of Helions and Tritons NUCLEAR REACTIONS 24Mg(3He, 3He'), E=29 MeV; 56,58Fe, 58Ni(3He, 3He'), E=22 MeV; measured nothing; analyzed σ(θ) data. 24Mg, 56,58Fe, 58Ni deduced deformation parameters β2.
1969RA36 Nucl.Sci.Appl. 5, 4 (1969) Quasi-Elastic (p, n) Scattering NUCLEAR REACTIONS 9Be, 11B, 13C, 15N, 27Al, 93Nb, 120Sn, 165Ho, 208Pb(p, n), E approx 20 MeV; surveyed quasi-elastic σ(θ) data.
1968AH03 Nucl.Sci.Appl. 4B, 22 (1968) R.Ahmed, H.M.Sen Gupta, M.A.Awal, M.Mohsen The (d, p) Reaction in 27Al at 2 MeV NUCLEAR REACTIONS 27Al(d, p), E=2 MeV; measured σ(Ep, θ). 28Al deduced levels.
1968MA21 Australian J.Phys. 21, 235 (1968) Inelastic Scattering of Deuterons from 56Fe NUCLEAR STRUCTURE 56Fe; measured not abstracted; deduced nuclear properties.
doi: 10.1071/PH680235
1968MA36 Nucl.Phys. A118, 151 (1968) A Study of the Levels in 56Fe from Inelastic Scattering of Deuterons NUCLEAR REACTIONS 56Fe(d, d'), E=12.0 MeV; measured σ(Ed', θ). 56Fe deduced levels, deformations. Enriched target.
doi: 10.1016/0375-9474(68)90193-0
1967KH02 Nucl.Sci.Appl. 3, No.2, 51 (1967) A.H.Khan, A.Hossain, H.M.Sen Gupta, A.H.M.A.Hannan Angular Distribution of Protons from (d, p) Reactions in Fe56 NUCLEAR STRUCTURE 57Fe; measured not abstracted; deduced nuclear properties.
1967SE06 Nuovo Cimento 49B, 207 (1967) H.M.Sen Gupta, A.H.M.A.Hannan, A.H.Khan, A.Hossain Angular Distribution of Protons from the (d, p) Reaction in 56Fe NUCLEAR STRUCTURE 57Fe; measured not abstracted; deduced nuclear properties.
1966DA18 J.Natur.Sci.Math. 6, 33 (1966) Energy Spectrum of Neutrons from (p, n) Reaction in 9Be NUCLEAR REACTIONS 9Be(p, n), E=7.5 MeV; measured σ(En, θ). 9B deduced levels.
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