NSR Query Results
Output year order : Descending NSR database version of April 29, 2024. Search: Author = H.Ropke Found 51 matches. 2004RO39 Eur.Phys.J. A 22, 213 (2004) Systematics of deformed states around doubly-magic 40Ca NUCLEAR STRUCTURE 36,37,38,39,40,41,42Ar, 38,39,40,41,42,43K, 40,41,42,43,44Ca, 42,43,44,45Sc, 44,45,46Ti, 46,47V, 48Cr; analyzed levels, J, π, rotational bands.
doi: 10.1140/epja/i2004-10045-5
2002RO24 Eur.Phys.J. A 14, 159 (2002) H.Ropke, J.Brenneisen, M.Lickert High-Spin States in 36Ar and Their Underlying Shell Model Configurations NUCLEAR REACTIONS 33S(α, nγ), E=13.4, 14.4 MeV; 35Cl(p, γ), E=1209, 1462 keV; measured Eγ, (neutron)γ-coin, γ angular distributions . 36Ar deduced high-spin levels, J, π, resonance properties. Comparison with Shell model results.
doi: 10.1140/epja/i2001-10201-5
2000RO18 Nucl.Phys. A674, 95 (2000) Alignment of Individual-Particle Angular Momenta Along the Deformation Axis in Light Nuclei NUCLEAR STRUCTURE 23Ne, 23,25Na, 24,25,26,27Mg, 26,27,28Al, 28,29Si; calculated levels, J, π, high-K rotational bands, configurations; deduced residual interaction features.
doi: 10.1016/S0375-9474(00)00161-5
1998RO10 Nucl.Phys. A632, 173 (1998) Renaissance of the Nilsson-Model Approach to Light Nuclei: The case of A = 26 system NUCLEAR STRUCTURE 26Al; calculated levels, J, π, rotational bands, B(E2), spectroscopic factors. Nilsson model.
doi: 10.1016/S0375-9474(97)00624-6
1997BR07 Z.Phys. A357, 157 (1997) J.Brenneisen, B.Erhardt, F.Glatz, Th.Kern, R.Ott, H.Ropke, J.Schmalzlin, P.Siedle, B.H.Wildenthal The Structure of 32S I. Spectroscopy of the Highly-Excited States NUCLEAR REACTIONS 29Si(α, n), E=14.4 MeV; measured neutron spectra, γn-coin, γn(θ). 31P(p, γ), E=2-3.3 MeV; measured Eγ, Iγ, γ(θ). 32S deduced high-spin levels, J, π, T, γ-branching ratios, T1/2, δ, B(M1). Other data input.
doi: 10.1007/s002180050231
1997BR12 Z.Phys. A357, 377 (1997) J.Brenneisen, B.Erhardt, F.Glatz, Th.Kern, R.Ott, H.Ropke, J.Schmalzlin, P.Siedle, B.H.Wildenthal The Structure of 32S II. Shell Model Interpretation NUCLEAR STRUCTURE 32S; calculated levels, Γγ, branching ratios, other aspects. Shell model.
doi: 10.1007/s002180050257
1996BR06 Z.Phys. A354, 301 (1996) J.Brenneisen, D.Grathwohl, B.Ehrhard, P.M.Endt, S.Fischer, M.Lickert, R.Ott, H.Ropke, J.Schmalzlin, P.Siedle, B.H.Wildenthal Quantum Numbers of 26Al Levels Above 6 MeV Excitation Energy NUCLEAR REACTIONS, ICPND 25Mg(p, γ), E=2-4 MeV; measured Eγ, Iγ, γ yield, γ(θ), anisotropies, resonance strengths. 26Al deduced levels, J, π, T, δ, IAR features.
doi: 10.1007/s002180050049
1995BR16 Z.Phys. A352, 149 (1995) J.Brenneisen, D.Grathwohl, M.Lickert, R.Ott, H.Ropke, J.Schmalzlin, P.Siedle, B.H.Wildenthal The Structure of 28Si Above 10 MeV Excitation Energy I: Gamma-decay modes and radiative widths of levels NUCLEAR REACTIONS 27Al(p, γ), E=1.097-4.492 MeV; 24Mg(α, γ), E=1.5-4 MeV; measured Eγ, Iγ. 27Al(d, nγ), E=4-6 MeV; measured nγ-coin, Eγ, Iγ. 28Si deduced levels, Γ, γ-branching ratios, resonance strengths.
doi: 10.1007/BF01298901
1995BR17 Z.Phys. A352, 279 (1995) J.Brenneisen, D.Grathwohl, M.Lickert, R.Ott, H.Ropke, J.Schmalzlin, P.Siedle, B.H.Wildenthal The Structure of 28Si Above 10 MeV Excitation Energy II: Assignments of quantum numbers NUCLEAR REACTIONS 27Al(p, γ), E not given; 24Mg(α, γ), E=3.355 MeV; measured Eγ, Iγ(θ). 28Si deduced levels, J, π, δ, T.
doi: 10.1007/BF01289501
1995BR32 Z.Phys. A352, 403 (1995) J.Brenneisen, D.Grathwohl, M.Lickert, R.Ott, H.Ropke, J.Schmalzlin, P.Siedle, B.H.Wildenthal The Structure of 28Si Above 10 MeV Excitation Energy III: Level scheme and shell model interpretation NUCLEAR STRUCTURE 28Si; analyzed data; deduced level scheme, J, π, T, γ-branching ratio. Shell model.
doi: 10.1007/BF01299758
1991HE05 Z.Phys. A338, 23 (1991) F.Heidinger, P.Betz, W.Brendler, F.Glatz, A.Hoffmann, H.Ropke, B.H.Wildenthal The Structure of 25Mg NUCLEAR REACTIONS 24Mg(d, p), E=6.5 MeV; measured σ(Ep). 22Ne(α, nγ), E=11.8-15.5 MeV; measured Eγ, Iγ, nγ-coin, nγ(θ). 25Mg deduced levels, J, π, branching ratio, δ, T1/2, B(λ), T. Shell model.
doi: 10.1007/BF01279113
1989HO07 Z.Phys. A332, 289 (1989) A.Hoffmann, P.Betz, H.Ropke, B.H.Wildenthal Structure of the Mirror Nuclei 21Ne and 21Na NUCLEAR REACTIONS 18O(α, nγ), E=12-15.4 MeV; measured nγ(θ), σ(En), nγ-coin. 18O(α, 2nγ), E=13.4 MeV; measured σ(En). 21Ne deduced levels, J, π, δ. Shell model comparison. NUCLEAR STRUCTURE 21Ne, 21Na; calculated levels, Gamow-Teller matrix elements, T1/2. Shell model.
1988LI31 Z.Phys. A331, 409 (1988) M.Lickert, J.Brenneisen, F.Glatz, D.Grathwohl, A.Martinez v.Remisowski, H.Ropke, J.Siefert, B.H.Wildenthal The Structure of 27Al NUCLEAR REACTIONS 24Mg(α, pγ), E=14.2, 15, 15.6 MeV; measured proton spectra, Eγ, Iγ, pγ-coin, pγ(θ). 26Mg(p, γ), E=1.82-2.574 MeV; measured γ(θ). 27Al deduced levels, J, π, δ, γ-branching ratios, B(λ), T1/2. Shell model. NUCLEAR STRUCTURE 27Al; calculated levels, γ-branching ratios, T1/2, B(λ). Shell model.
1986GL05 Z.Phys. A324, 173 (1986) F.Glatz, M.Lickert, A.Burkard, Th.Kern, R.Lehmann, S.Norbert, H.Ropke, J.Siefert, B.H.Wildenthal Search for Missing Predicted High-Spin States in 28Si NUCLEAR REACTIONS 27Al(p, γ), E=1.911, 2.073 keV; measured Eγ, Iγ, γ(θ), linear polarization, DSA. 28Si deduced levels, J, π, T, K, rotational band structure, Γγ. Shell model comparison.
1986GL06 Z.Phys. A324, 187 (1986) F.Glatz, S.Norbert, E.Bitterwolf, A.Burkard, F.Heidinger, Th.Kern, R.Lehmann, H.Ropke, J.Siefert, C.Schneider, B.H.Wildenthal High-Spin States in 26Mg NUCLEAR REACTIONS 23Na(α, pγ), E=14.2, 16 MeV; measured σ(Ep), pγ-coin, pγ(θ), DSA. 26Mg deduced levels, J, π, T1/2, K, γ-branching, δ, B(λ), intrinsic quadrupole moments, rotational band structure, prolate to oblate deformation transition.
1983BI08 Z.Phys. A313, 123 (1983) E.Bitterwolf, A.Burkard, P.Betz, F.Glatz, F.Heidinger, Th.Kern, R.Lehmann, S.Norbert, H.Ropke, C.Schneider, J.Siefert Shape Coexistence and Other Aspects of Nuclear Structure in 40Ar NUCLEAR REACTIONS 37Cl(α, pγ), E=12, 13 MeV; measured pγ-coin, γ linear polarization, DSA. 40Ar deduced levels, J, π, γ branching, T1/2, δ, quadrupole moment, shape coexistence. Weak coupling model.
doi: 10.1007/BF02115850
1982BE52 Z.Phys. A309, 163 (1982) P.Betz, E.Bitterwolf, A.Burkard, F.Glatz, F.Heidinger, Th.Kern, R.Lehmann, S.Norbert, H.Ropke, C.Schneider, J.Siefert Spectroscopy of Highly Excited States in 29Si NUCLEAR REACTIONS 28Si(d, pγ), E=6.5, 7 MeV; 26Mg(α, nγ), E=12, 14, 15 MeV; 27Al(3He, pγ), E=9 MeV; measured σ(Ep), σ(En), γp(θ), γp-coin. 29Si deduced levels, J, π, K, deformation, rotational band structure. Shell model.
doi: 10.1007/BF01414978
1981GL01 Phys.Rev.Lett. 46, 1559 (1981) F.Glatz, P.Betz, J.Siefert, F.Heideniger, H.Ropke Excited Kπ = 0+ Rotational Band in 28Si NUCLEAR REACTIONS 25Mg(α, n), E=14.5 MeV; measured nγ(θ); 27Al(p, γ), E=2160, 2312 keV; measured Eγ, Iγ, DSA. 28Si deduced levels, J, π, K, rotational band structure, ground state quadrupole moments, B(λ). Ge(Li) detectors, tof.
doi: 10.1103/PhysRevLett.46.1559
1981GL05 Z.Phys. A303, 239 (1981) F.Glatz, J.Siefert, P.Betz, E.Bitterwolf, A.Burkard, F.Heidinger, Th.Kern, R.Lehmann, S.Norbert, H.Ropke Structure of 28Si from the Spectroscopy of High-Spin States NUCLEAR REACTIONS 25Mg(α, nγ), E=14, 15.5 MeV; measured nγ-coin, nγ(θ), DSA. 27Al(p, γ), E=2.16, 2.312 MeV; measured Eγ, Iγ, DSA. 28Si deduced levels, J, π, rotational bands, T1/2, B(λ), δ, Γp, Γ, intrinsic quadrupole moments. Shell model.
doi: 10.1007/BF01424765
1980BI14 Z.Phys. A298, 279 (1980) E.Bitterwolf, P.Betz, A.Burkard, F.Glatz, F.Heidinger, T.Kern, R.Lehmann, S.Norbert, J.Siefert, H.Ropke Structure of 30Si from the Spectroscopy of Highly Excited States NUCLEAR REACTIONS 27Al(α, pγ), E=12, 14.1, 15 MeV; measured pγ(θ), linearly polarized γp-coin, DSA. 30Si deduced levels, T1/2, J, π, rotational bands, intrinsic quadrupole moments, K, Nilsson assignments. Collective, shell models.
doi: 10.1007/BF01425158
1980KE01 Z.Phys. A294, 51 (1980) T.Kern, P.Betz, E.Bitterwolf, F.Glatz, H.Ropke Density of High-Spin States in 38Ar and 42Ca NUCLEAR REACTIONS 35Cl(α, pγ), E=16 MeV; 39K(α, pγ), E=15.14 MeV; measured pγ-coin. 42Ca, 38Ar deduced levels, π, γ-branching, high J state density. Weak coupling model.
doi: 10.1007/BF01473121
1979GL07 Z.Phys. A293, 57 (1979) F.Glatz, P.Betz, E.Bitterwolf, A.Burkard, F.Heidinger, T.Kern, R.Lehmann, S.Norbert, H.Ropke High-Spin States in 48Ti NUCLEAR REACTIONS 45Sc(α, pγ), E=11, 12, 13 MeV; measured pγ(θ), DSA, Eγ, Iγ, σ(Ep). 48Ti deduced levels, J, π, γ-branching ratio. Shell-model interpretation.
doi: 10.1007/BF01414785
1978GL05 Fizika, Suppl. 10, 9 (1978) High-Spin States in 48Ti NUCLEAR REACTIONS 45Sc(α, pγ), E=11 MeV; measured pγ(θ), DSA. 48Ti deduced high spin states, T1/2, B(λ). Shell model.
1977BR07 Z.Phys. A281, 75 (1977) W.Brendler, P.Betz. E.Bitterwolf, H.Ropke The Structure of 27Mg from the 26Mg(d, pγ) Reaction NUCLEAR REACTIONS 26Mg(d, pγ), E=5.5, 6.5 MeV; measured pγ(θ), DSA. 27Mg deduced levels, J, π, γ-branching, T1/2, δ.
doi: 10.1007/BF01408616
1976BE13 Z.Phys. A276, 295 (1976) P.Betz, E.Bitterwolf, B.Busshardt, H.Ropke Deformed States of High Spin in 42Ca NUCLEAR REACTIONS 39K(α, pγ), E=14, 15 MeV; measured pγ(θ), DSA. 42Ca deduced levels, K, J, π, T1/2, quadrupole moment, γ-branching, δ, B(λ).
doi: 10.1007/BF01412107
1976BI15 J.Phys.(London) G2, L171 (1976) Collective Structure of Negative Parity States in 42Ca NUCLEAR REACTIONS 39K(α, pγ), E=14, 15 MeV; measured σ(Ep, Eγ), DSA. 42Ca levels deduced J, π, T1/2, γ-branching, δ.
doi: 10.1088/0305-4616/2/3/009
1976GL10 Z.Phys. A278, 319 (1976) F.Glatz, G.Pappert, A.Brachat, P.Betz, H.Ropke High-Spin States in 38Ar NUCLEAR REACTIONS 35Cl(α, pγ), E=14 MeV; measured Eγ, Iγ, γγ(θ), γ(t). 38Ar deduced levels, J, π, T1/2, δ, γ-branching.
1974BE68 Z.Phys. 271, 195 (1974) P.Betz, H.Ropke, F.Glatz, G.Hammel, V.Glattes, W.Brendler Evidence for the Coexistence of Spherical and Deformed States in 38Ar NUCLEAR REACTIONS 35Cl(α, pγ), E=14, 14.5 MeV; measured pγ(θ), DSA. 38Ar deduced levels, K, J, π, T1/2, E2 strengths.
doi: 10.1007/BF01676390
1974RO10 Z.Phys. 266, 55 (1974) H.Ropke, G.Hammel, W.Brendler, P.Betz, V.Glattes New Aspects of the Rotational Model in 25Mg NUCLEAR REACTIONS 22Ne(α, nγ), E=8.0, 8.8 MeV; 24Mg(d, pγ), E=6 MeV; measured γ(θ), pγ(θ), DSA. 25Mg levels deduced T1/2, J, π, γ-mixing.
1974RO24 Z.Phys. 268, 391 (1974) H.Ropke, P.Betz, G.Bender, V.Glattes, G.Hammel, W.Brendler High-Spin States in 27Al NUCLEAR REACTIONS 26Mg(p, γ), E=2174 keV; measured σ(Eγ, θ). 24Mg(α, pγ), E=13, 15, 15.2 MeV; measured DSA, pγ-coin, pγ(θ), σ(Ep, Eγ). 27Al deduced levels, T1/2, J, π, γ-mixing, γ-width. Data from this article have been entered in the EXFOR database. For more information, access X4 datasetF0664. 1974RO39 Z.Phys. 271, 59 (1974) H.Ropke, W.Brendler, P.Betz, V.Glattes, G.Hammel Lifetime Measurements in 25Mg NUCLEAR REACTIONS 24Mg(d, pγ), E=6 MeV; measured DSA, pγ-coin. 25Mg levels deduced T1/2, K, J, π, transition rates.
1973BE28 Z.Phys. 261, 351 (1973) Search for High-Spin States in 29Si Using a Neutron Time-of-Flight Spectrometer NUCLEAR REACTIONS 26Mg(α, nγ), E=11, 12, 13, 14 MeV; measured nγ-coin, Eγ, Iγ, DSA. 29Si deduced levels, J, π, T1/2.
doi: 10.1007/BF01399333
1973RO17 Z.Phys. 260, 67 (1973) H.Ropke, V.Glattes, H.J.Brundiers, G.Hammel The γ-Decay of 25Mg NUCLEAR REACTIONS 24Mg(d, pγ), 27Al(d, αγ), E=5.2 MeV; measured Eγ, Iγ. 25Mg deduced levels, γ-branching, J, π, K.
1972RO38 Phys.Lett. 41B, 565 (1972) Spectroscopic Factors of γ-Vibrational Like States in Odd-A s-d Shell Nuclei NUCLEAR STRUCTURE 22Ne, 24,26Mg, 25Mg, 23Na; calculated levels, S for γ-vibrational states.
doi: 10.1016/0370-2693(72)90634-X
1971RO22 Nucl.Phys. A172, 499 (1971) Investigation of the 6477 keV State in 27Al with a Ge(Li) γ-Ray Polarimeter NUCLEAR REACTIONS 26Mg(p, γ), E=2293 keV; measured dσ(θ(γ)), γ-ray polarization, Doppler shift. 27Al levels deduced J, π, γ-mixing, T1/2. Enriched target.
doi: 10.1016/0375-9474(71)90040-6
1971RO23 Nucl.Phys. A172, 506 (1971) The Kπ = 1/2-, [330] Rotational Band in A = 21-27 Nucleides NUCLEAR STRUCTURE 21Na, 21Ne, 23Ne, 25Al, 25Mg, 27Al, 27Mg; surveyed experimental data; calculated levels, level-width, S.
doi: 10.1016/0375-9474(71)90041-8
1970RO19 Nucl.Phys. A153, 211 (1970) H.Ropke, H.J.Brundiers, G.Hammel Further Evidence of a Kπ = 3/2+ Band in the Mirror Nuclei 25Al and 25Mg NUCLEAR REACTIONS 24Mg(p, p'γ), E=2.9-4.28 MeV; measured resonance energy σ(E;Ep', Eγ, θ(p'), θ(γ)). 25Al deduced resonances, level-width, J. Enriched, natural targets. 23Na(3He, p), E=7.5, 8.0 MeV; measured σ(Ep, θ(p)). 25Mg level deduced L. Natural targets.
doi: 10.1016/0375-9474(70)90766-9
1970RO25 Nucl.Phys. A156, 477 (1970) Rotation-Vibration Interaction in 27Al NUCLEAR STRUCTURE 27Al; calculated levels, E2 transition strengths. Rotation-vibration model.
doi: 10.1016/0375-9474(70)90245-9
1969HA02 Nucl.Phys. A123, 437(1969) Electric Quadrupole Transitions in 42Ca NUCLEAR REACTIONS 39K(α, pγ), E=7.5, 9.0, 10.6 MeV; measured Doppler shift attenuation, pγ-delay. 42Ca levels deduced T1/2. Natural target, Ge(Li) detector.
doi: 10.1016/0375-9474(69)90512-0
1969RO28 Can.J.Phys. 47, 1545 (1969) The 23Na(α, γ)27Al Reaction. A Survey of the Reaction and Some Properties of the 27Al Nucleus NUCLEAR REACTIONS 23Na(α, γ), E = 2-3 MeV; measured σ(E;Eγ, θ(γ)). 27Al deduced resonances, J, π, level-width, γ-branching. 27Al deduced levels, J, π.
1968AN06 Phys.Letters 27B, 161(1968) N.Anyas-Weiss, A.E.Litherland, H.Ropke Resonance Width Measurements Using the Doppler Shift Attenuation Method NUCLEAR REACTIONS 24Mg(p, γ), E=1.2, 1.823 MeV; 27Al(p, γ), E=0.612 MeV; measured Doppler shift. 25Al, 28Si levels, deduced level-width.
doi: 10.1016/0370-2693(68)90059-2
1968LI04 Nucl.Phys. A108, 233(1968) K.P.Lieb, H.Ropke, H.Grawe, H.J.Brundiers, O.Klepper Lifetime Measurements in 38Ar NUCLEAR REACTIONS 35Cl(α, pγ), E = 5.9, 10.5 MeV; measured σ(Eγ), Doppler-shift attenuation, pγ-delay. 38Ar deduced levels, T1/2. Natural target, Ge(Li) detector.
doi: 10.1016/0375-9474(68)90156-5
1968RO04 Z.Physik 210, 179 (1968) The Lifetime of the 5.14 MeV State in 22Ne NUCLEAR STRUCTURE 22Ne; measured not abstracted; deduced nuclear properties.
1968RO10 Phys.Letters 27B, 368 (1968) H.Ropke, N.Anyas-Weiss, A.E.Litherland Investigation of a New E = 4 507 keV State in 25Al NUCLEAR STRUCTURE 25Al; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0370-2693(68)90185-8
1968RO11 Can.J.Phys. 46, 1649 (1968) A Study of the 4.509-MeV State in 27Al by the 26Mg(p, γ) Reaction NUCLEAR STRUCTURE 27Al; measured not abstracted; deduced nuclear properties.
1968RO17 Can.J.Phys. 46, 2789(1968) H.Ropke, N.Anyas-Weiss, A.E.Litherland Properties of the 4.038 MeV State in 25Al NUCLEAR REACTIONS 24Mg(p, γ), E=1.824 MeV; measured σ(Eγ, θ), Doppler-shift attenuation. 25Al deduced resonances, levels, J, π, T1/2, level-width, γ-mixing ratios. Ge(Li) detector.
1967LI05 Nucl.Phys. A98, 145(1967) Lifetime Measurements in 30Si NUCLEAR REACTIONS 27Al(α, pγ), E = 3.47, 4.55 MeV; measured Doppler-shift attenuation. 30Si levels deduced T1/2.
doi: 10.1016/0375-9474(67)90906-2
1967RO10 Nucl.Phys. A97, 609(1967) A Resonance in the 16O + 3He Reactions at 5.05 MeV Bombarding Energy NUCLEAR REACTIONS 16O(3He, 3He), (3He, p), (3He, α), E = 3.5-5.6 MeV; measured σ(E;Ep, θ). 19Ne deduced level, level-width, J, π, L. Natural target.
doi: 10.1016/0375-9474(67)90525-8
1967RO16 Nucl.Phys. A104, 529(1967) H.Ropke, K.P.Lieb, H.Brundiers The 4.88 and 5.36 MeV States in 38Ar NUCLEAR REACTIONS 35Cl(α, pγ), E=10.6 MeV; measured σ(Ep, Eγ, θ). 38Ar deduced levels, J, π, delta. Natural target.
doi: 10.1016/0375-9474(67)90471-X
1966RO03 Nucl.Phys. 80, 476(1966) Perturbation of the Angular Correlation of the 1.35 Mev-0.198 MeV γ-γ Cascade in 19F NUCLEAR REACTIONS 19F(p, p'γ), E = 4.3 MeV; measured γ γ(θ, t); deduced angular correlation attenuation factors.
doi: 10.1016/0029-5582(66)90105-2
1965SP03 Nucl.Phys. 63, 477 (1965); H.Spehl - Priv.Comm. (April 1972) The Gyromagnetic Ratio of the First Excited 2+ State of Pt194 NUCLEAR REACTIONS 194Pt(p, p'γ), E=2.55 MeV; measured pγ(θ, H). 194Pt deduced g(328.5 keV level). Enriched target.
doi: 10.1016/0029-5582(65)90477-3
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