NSR Query Results
Output year order : Descending NSR database version of April 27, 2024. Search: Author = A.M.Haque Found 19 matches. 1995BR34 Z.Phys. A353, 141 (1995) F.Brandolini, D.Bazzacco, A.M.I.Haque, M.Ionescu-Bujor, P.Pavan, M.De Poli, R.V.Ribas, C.Rossi-Alvarez g-Factors of the Lowest 2+ and 4+ States in 198,200,202Hg NUCLEAR REACTIONS 198,200,202Hg(58Ni, 58Ni'), E=217 MeV; measured Eγ, Iγ, γγ(θ, H) following Coulomb excitation. 198,200,202Hg levels deduced g factors. Models comparison.
doi: 10.1007/BF01295891
1993BI13 Z.Phys. A346, 181 (1993) A.M.Bizzeti-Sona, A.A.Stefanini, F.Brandolini, P.Pavan, A.M.I.Haque The g-Factor of the 8+ Isomer of 142Eu NUCLEAR REACTIONS 114Cd(32S, 3np), E=155 MeV; measured Eγ, Iγ, γ(θ, H, t). 142Eu deduced isomer g factor, configuration.
doi: 10.1007/BF01306076
1992BR03 Nucl.Phys. A536, 366 (1992) F.Brandolini, M.Ionescu-Bujor, P.Pavan, D.Bazzacco, C.Rossi-Alvarez, M.De Poli, A.M.I.Haque, R.V.Ribas Gyromagnetic Ratios of Low-Lying States in 192,194,196Pt NUCLEAR REACTIONS 192,194,196Pt(58Ni, 58Ni'), E=180-210 MeV; measured γ(θ, H, T) in polarized Gd, Fe, (particle)-γ coin, Coulomb excitation. 192,194,196Pt levels deduced g-factors. Enriched targets, thin foil transient-field IMPAC technique. NUCLEAR STRUCTURE 192,194,198Pt; calculated g-factors. Pairing-plus-quadrupole, dynamical deformation, interacting bosons models.
doi: 10.1016/0375-9474(92)90388-Z
1992BR07 Phys.Rev. C45, 1549 (1992) F.Brandolini, P.Pavan, D.Bazzacco, C.Rossi-Alvarez, R.V.Ribas, M.De Poli, A.M.I.Haque g Factors for Yrast States in Isotopic Doublets 156,158Gd and 166,168Er NUCLEAR REACTIONS 156,158Gd(58Ni, 58Ni'), 166,168Er(58Ni, 58Ni'), E=130-217 MeV; measured γ(θ, H, T) in polarized Gd, Fe, (particle)γ-coin, following Coulomb excitation. 156,158Gd, 166,168Er levels deduced g-factors of ground state rotational bands. Cranked shell model and cranked HFB calculations. Thin foil transient-field IMPAC technique.
doi: 10.1103/PhysRevC.45.1549
1991BA38 Nucl.Phys. A533, 541 (1991) D.Bazzacco, F.Brandolini, K.Loewenich, P.Pavan, C.Rossi-Alvarez, E.Maglione, M.De Poli, A.M.I.Haque Transient-Field g-Factor Measurement of the First 2+ States in the N = 82 Nuclei 140Ce, 142Nd and 144Sm NUCLEAR REACTIONS 140Ce, 142Nd, 144Sm(32S, 32S'), E=110-116 MeV; measured γ(θ, H, t) in polarized Fe, (particle)γ-coin, Coulomb excitation. 140Ce, 142Nd, 144Sm deduced 2+ level, g. Enriched targets, thin foil technique. NUCLEAR STRUCTURE 140Ce, 142Nd, 144Sm; calculated levels, g. Shell model, quasiparticle random phase approximation.
doi: 10.1016/0375-9474(91)90532-B
1991BR29 Nuovo Cim. 104A, 1413 (1991); Erratum Nuovo Cim. 104A, 1587 (1991) T.Bressani, D.Calvo, A.Feliciello, C.Lamberti, F.Iazzi, B.Minetti, R.Cherubini, A.M.I.Haque, R.A.Ricci Observation of 2.5 MeV Neutrons Emitted from a Titanium-Deuterium System NUCLEAR REACTIONS 2H(d, d), E=low; measured neutron emission, energy. Ti(metal)/D(gas) system, double scattering spectrometer.
doi: 10.1007/BF02789584
1990BA39 Hyperfine Interactions 59, 125 (1990) D.Bazzacco, F.Brandolini, K.Loewenich, P.Pavan, C.Rossi Alvarez, M.De Poli, A.M.I.Haque g-Factors of the First Excited 4+ States in 156Gd and 158Gd NUCLEAR REACTIONS 156,158Gd(58Ni, 58Ni'), E=117 MeV; measured γ(58Ni)-coin, γ-precession following Coulomb excitation. 156,158Gd level deduced g. Transient field technique.
doi: 10.1007/BF02401205
1990BA40 Hyperfine Interactions 59, 129 (1990) D.Bazzacco, F.Brandolini, K.Loewenich, P.Pavan, C.Rossi Alvarez, M.De Poli, A.M.I.Haque g-Factor Measurements in Stable Hg Isotopes NUCLEAR REACTIONS 198,200,202Hg(58Ni, 58Ni'), E=217 MeV; measured γ(58Ni)-coin, γ-precession following Coulomb excitation. 198,200,202Hg level deduced g. Transient field technique.
doi: 10.1007/BF02401206
1990BA41 Hyperfine Interactions 59, 133 (1990) D.Bazzacco, F.Brandolini, K.Loewenich, P.Pavan, C.Rossi Alvarez, M.De Poli, A.M.I.Haque Transient Field g-Factor Measurement of the First 3- State in 144Sm NUCLEAR REACTIONS 144Sm(58Ni, 58Ni'), E=217 MeV; measured γ(58Ni)-coin, γ-precession following Coulomb excitation. 144Sm level deduced g. Transient field technique.
doi: 10.1007/BF02401207
1990BI03 Z.Phys. A335, 365 (1990) A.M.Bizzeti-Sona, P.Blasi, M.Donvito, A.A.Stefanini, D.Bazzacco, F.Brandolini, K.Loewenich, P.Pavan, C.Rossi-Alvarez, M.De Poli, A.M.I.Haque The g Factor of the Lowest 7+ State in 100Rh and 6- State in 104Rh NUCLEAR REACTIONS 96,100Mo(7Li, 3n), E=30 MeV; measured γ(θ, H, t). 100,104Rh deduced isomer g, configuration. Shell model comparison.
1989RI03 Nucl.Phys. A499, 221 (1989) R.Richter, I.Forster, A.Gelberg, A.M.I.Haque, P.von Brentano, R.F.Casten, H.G.Borner, G.G.Colvin, K.Schreckenbach, G.Barreau, S.A.Kerr, H.H.Schmidt, P.Hungerford, H.J.Scheerer, T.von Egidy, R.Rascher Nuclear Structure of 179Hf Studied with (n, γ), (d, p) and (d, t) Reactions NUCLEAR REACTIONS 178Hf(n, γ)(n, e-), E=thermal; measured Eγ, Iγ. 178Hf(n, e-), E=thermal; measured I(ce). 178Hf(d, p), 180Hf(d, t), E=15, 23 MeV; measured σ(Ep), σ(Et). 179Hf deduced levels, J, π, ICC, γ-multipolarity, Nilsson assignments.
doi: 10.1016/0375-9474(89)90045-6
1988BA11 Z.Phys. A329, 429 (1988) D.Bazzacco, F.Brandolini, K.Loewenich, P.Pavan, C.Rossi-Alvarez, M.De Poli, A.M.I.Haque, A.M.Bizzeti Sona, P.Blasi, A.A.Stefanini TDPAD g-Factor Measurement of the (21/2)+ State in 89Zr NUCLEAR REACTIONS 85Rb(7Li, 3n), E=28 MeV; measured γ(θ, H, t). 89Zr level deduced g.
1988BA22 Phys.Lett. 206B, 404 (1988) D.Bazzacco, F.Brandolini, K.Loewenich, S.Lunardi, P.Pavan, C.Rossi-Alvarez, F.Soramel, M.De Poli, A.M.I.Haque, G.de Angelis g-Factor Measurement of the Two Lowest 10+ States in 140Sm NUCLEAR REACTIONS 116Cd(28Si, 4n), E=125 MeV; measured γ(θ, H, t). 140Sm levels deduced g, configuration.
doi: 10.1016/0370-2693(88)91600-0
1986HA22 Nucl.Phys. A455, 231 (1986) A.M.I.Haque, R.F.Casten, I.Forster, A.Gelberg, R.Rascher, R.Richter, P.von Brentano, G.Barreau, H.G.Borner, S.A.Kerr, K.Schreckenbach, D.D.Warner A Study of the Low-Lying States in 178Hf through the (n, γ) Reaction NUCLEAR REACTIONS 177Hf(n, γ), E=thermal, resonance; measured Eγ, Iγ, I(ce). 178Hf deduced levels, J, π, γ-branching, γ-multipolarity, δ, B(λ), band structure, neutron binding energy.
doi: 10.1016/0375-9474(86)90018-7
1985CA20 Phys.Rev. C31, 1991 (1985) R.F.Casten, P.Von Brentano, A.M.I.Haque Evidence for an Underlying SU(3) Structure near Neutron Number N = 104 NUCLEAR STRUCTURE 158,160,162,164Dy, 162,164,166,168,170Er, 162,166,168,170,172Yb, 176,178,182Hf, 180,182,184,186,188Os, 182,184,186W; analyzed levels, B(E2); deduced SU(3) limit of interacting boson approximation.
doi: 10.1103/PhysRevC.31.1991
1985RI09 Z.Phys. A322, 43 (1985) R.Richter, I.Forster, A.Gelberg, A.M.I.Haque, P.von Brentano, R.F.Casten, H.G.Borner, G.G.Colvin, K.Schreckenbach, P.Hungerford, H.J.Scheerer, H.H.Schmidt, T.von Egidy, R.Rascher, G.Barreau, S.A.Kerr An Unusual M1 Electromagnetic Transition Connecting Octupole and Quadrupole Vibrations in 179Hf NUCLEAR REACTIONS 178Hf(n, γ), E=thermal; measured Eγ, Iγ. 178Hf(n, e-), E=thermal; measured I(ce). 178Hf(d, p), E=15, 23 MeV; 180Hf(d, t), E=15 MeV; measured not abstracted. 179Hf deduced levels, J, π, Nilsson assignments, E1 hindrance factors, T1/2, octupole-quadrupole vibration coupling role.
doi: 10.1007/BF01412016
1983BA10 Z.Phys. A310, 65 (1983) D.Bazzacco, A.M.I.Haque, K.O.Zell, W.Neumann, J.Eberth, P.von Brentano, C.Protop Excited States in 145Gd from the (3He, 2n) Reaction NUCLEAR REACTIONS, ICPND 144Sm(3He, 2nγ), E=18-26 MeV, measured Eγ, Iγ(E), Iγ(θ), γγ-coin, I(ce), γ yields. 145Gd deduced levels J, π, ICC. Enriched targets, Ge(Li) detectors. Weak coupling model.
doi: 10.1007/BF01433612
1980BA01 Phys.Rev. C21, 222 (1980) D.Bazzacco, A.M.I.Haque, K.O.Zell, P.von Brentano, C.Protop Core Coupled States in 145Eu NUCLEAR REACTIONS 142Nd(6Li, 3nγ), E=25-33 MeV; measured Eγ, Iγ, σ(E, Eγ, θ), γγ-coin. 145Eu deduced levels, J, π. Enriched targets. Ge-Li detectors.
doi: 10.1103/PhysRevC.21.222
1977HA50 Nucl.Sci.Appl., Ser.B 10, 38 (1977) Nuclear Level Density of a Few Iron Isotopes NUCLEAR STRUCTURE 53,56,57Fe; calculated single particle level density with respect to nuclear level density from energy levels of Fe isotopes. Method of Lang, Le-Couteur.
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