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NSR database version of May 23, 2024.

Search: Author = A.Ercan

Found 9 matches.

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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
Citations: PlumX Metrics

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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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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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