NSR Query Results
Output year order : Descending NSR database version of April 27, 2024. Search: Author = A.Ercan Found 9 matches. 1993LA10 Z.Phys. A345, 427 (1993) M.Lach, P.Kleinheinz, J.Blomqvist, A.Ercan, H.J.Hahn, D.Wahner, R.Julin, M.Zupancic, F.Cigoroglu, G.de Angelis Shell Model Yrast States in the N = 79 Nuclei 141Sm and 143Gd NUCLEAR REACTIONS 142Nd, 144Sm(α, 5n), E=77, 80 MeV; measured Eγ, Iγ, γ(θ), I(ce), γγ-coin. 144Sm(α, 6n), E=95 MeV; measured γγ-coin. 141Sm, 143Gd deduced levels, J, π, band structure, configuration. Shell model.
doi: 10.1007/BF01282905
1988ER02 Z.Phys. A329, 63 (1988) A.Ercan, R.Broda, P.Kleinheinz, M.Piiparinen, R.Julin, J.Blomqvist The Two Particle-Phonon Multiplet (πh11/2νf7/2)x3- and Higher-Lying Four-Nucleon Yrast States in the Doubly-Odd Nucleus 63146Eu83 NUCLEAR REACTIONS 147Sm(α, 4np), E=76 MeV; measured Eγ, Iγ, γ(θ). 146Eu deduced levels, J, π, B(λ), configurations, γ-multipolarity. Model calculations.
1986BO17 Nucl.Instrum.Methods Phys.Res. A245, 393 (1986); see 1986Bo23 G.L.Borchert, J.Bojowald, A.Ercan, H.Labus, Th.Rose, O.W.B.Schult Curved Crystal Spectrometer for High-Resolution In-Beam Spectroscopy of X-Rays and Low-Energy Gamma Rays
doi: 10.1016/0168-9002(86)91274-X
1986BO23 Nucl.Instrum.Methods Phys.Res. A245, 393 (1986) G.L.Borchert, J.Bojowald, A.Ercan, H.Labus, Th.Rose, O.W.B.Schult Curved Crystal Spectrometer for High-Resolution In-Beam Spectroscopy of X-Rays and Low-Energy Gamma Rays NUCLEAR REACTIONS 147Sm(p, 2n), E=22 MeV; measured Eγ, Iγ. 181Ta(p, 3n), E=26 MeV; measured Eγ, Iγ, E X-ray, I X-ray. 179W deduced transition energies. High resolution curved crystal spectrometer.
doi: 10.1016/0168-9002(86)91274-X
1986LU07 Z.Phys. A324, 433 (1986) S.Lunardi, F.Soramel, W.Starzecki, W.Meczynski, R.Julin, M.Lach, A.Ercan, P.Kleinheinz First Observation of Yrast γ-Rays in the N = 78 Nuclei 142Gd and 141Eu NUCLEAR REACTIONS, ICPND 142Nd, 144Sm(α, 6n), (α, 6np), (α, 5n), (α, 4n), (α, 3n), (α, 2n), E=65-107 MeV; measured Eγ, Iγ, σ(E), σ(θ), γ(θ), γγ-coin. 110Cd(35Cl, 2np), (35Cl, 2n2p), E=138 MeV; 112Cd(32S, 2np), (32S, 2n2p), E=132 MeV; 106Pd(37Cl, 2np), (37Cl, 2n2p), (37Cl, 2n), E=148 MeV; measured Eγ, Iγ, γγ-coin. 145Tb, 144Gd, 143Eu deduced exit channel σ ratio. 141Eu, 142Gd deduced levels, yrast cascade. Ge detectors.
1986RU04 Z.Phys. A324, 27 (1986) B.Rubio, A.Ercan, G.de Angelis, P.Kleinheinz, J.L.Tain, B.Brinkmoller, D.Paul, J.Meissburger, L.G.Mann, D.J.Decman, T.N.Massey, G.L.Struble, H.J.Scheerer, J.Blomqvist The Ground State Mass of 147Gd from Single-Neutron-Transfer Reactions and Its Impact on Derived Mass Values NUCLEAR REACTIONS 148Gd(p, d), E=25 MeV; 148Gd(d, t), E=22 MeV; 148Gd(3He, α), E=30 MeV; measured σ(Ed), σ(Et), σ(Eα); deduced Q-value differences. 147Gd deduced mass. 148Gd deduced neutron separation energy. Shell model comparison.
1983SO13 Z.Phys. A314, 127 (1983) F.Soramel-Stanco, R.Julin, J.Styczen, P.T.Prokofjev, A.Ercan, P.Kleinheinz A 45 ns 8+ Isomer in the Doubly Odd 150Eu Nucleus NUCLEAR REACTIONS 152Sm(p, 3n), E=29 MeV; measured Eγ, Iγ, I(ce), γγ(t). 150Eu deduced levels, J, π, ICC, δ, γ-branching.
1983ST03 Phys.Rev.Lett. 50, 1752 (1983) J.Styczen, Y.Nagai, M.Piiparinen, A.Ercan, P.Kleinheinz Deformed Ground-Band States in the N = 86 Nucleus 152Dy NUCLEAR REACTIONS 152Gd(α, 4n), E=60 MeV; measured γγ-coin, γ(θ), I(ce). 156Dy deduced levels, J, π, isomer, γ-multipolarities, γ-branching, backbending characteristics, configurations.
doi: 10.1103/PhysRevLett.50.1752
1980ER04 Z.Phys. A295, 197 (1980) A.Ercan, R.Broda, M.Piiparinen, Y.Nagai, R.Pengo, P.Kleinheinz The 235 μs 9+ Isomer in 146Eu NUCLEAR REACTIONS 147Sm(p, 2n), E=19-22 MeV; measured I(ce), Eγ, Iγ, γγ-coin with, without pulsed beam. 146Eu deduced levels, γ-branching, multipolarity, J, π, configuration.
doi: 10.1007/BF01413077
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