NSR Query Results
Output year order : Descending NSR database version of May 3, 2024. Search: Author = J.Holden Found 25 matches. 2003KU11 Phys.Lett. B 562, 193 (2003) G.Kumbartzki, N.Benczer-Koller, J.Holden, G.Jakob, T.J.Mertzimekis, M.J.Taylor, K.-H.Speidel, R.Ernst, A.E.Stuchbery, C.W.Beausang, R.Krucken Competition between proton and neutron excitations in 96Zr NUCLEAR REACTIONS C, 24Mg, Cu, Gd, Ta(96Zr, 96Zr'), E=265-274 MeV; measured Eγ, Iγ(θ, H, t), DSA following projectile Coulomb excitation. 96Zr levels deduced T1/2, g factors, configurations, transition B(E3). Transient field technique, comparison with shell model results.
doi: 10.1016/S0370-2693(03)00608-7
2002JA02 Phys.Rev. C65, 024316 (2002) G.Jakob, N.Benczer-Koller, G.Kumbartzki, J.Holden, T.J.Mertzimekis, K.-H.Speidel, R.Ernst, A.E.Stuchbery, A.Pakou, P.Maier-Komor, A.Macchiavelli, M.McMahan, L.Phair, I.Y.Lee Evidence for Proton Excitations in 130, 132, 134, 136Xe Isotopes from Measurements of g Factors of 21+ and 41+ States NUCLEAR REACTIONS Ti(130Xe, 130Xe'), (132Xe, 132Xe'), (134Xe, 134Xe'), (136Xe, 136Xe'), E=485-508 MeV; measured Eγ, Iγ(θ, H, t), (particle)γ-coin, DSA following projectile Coulomb excitation. 130,132,134,136Xe levels deduced g factors, T1/2. Transient field technique, Gd-backed target. Comparison with IBA-II model predictions. NUCLEAR STRUCTURE 130,132,134Te, 132,134,136Xe; calculated g factors. Shell model, comparison with data.
doi: 10.1103/PhysRevC.65.024316
2001HO02 Phys.Rev. C63, 024315 (2001) J.Holden, N.Benczer-Koller, G.Jakob, G.Kumbartzki, T.J.Mertzimekis, K.-H.Speidel, C.W.Beausang, R.Krucken, A.Macchiavelli, M.McMahan, L.Phair, A.E.Stuchbery, P.Maier-Komor, W.Rogers, A.D.Davies Single Particle Degrees of Freedom in the Transition from Deformed to Spherical Nd Nuclei NUCLEAR REACTIONS Si, Ni(144Nd, 144Nd'), (146Nd, 146Nd'), (148Nd, 148Nd'), (150Nd, 150Nd'), E=285, 584-608 MeV; measured Eγ, Iγ(θ, H, t), (particle)γ-coin following projectile Coulomb excitation. 144,146,148,150Nd levels deduced g factors, configurations. Transient field technique.
doi: 10.1103/PhysRevC.63.024315
2001ME20 Phys.Rev. C64, 024314 (2001) T.J.Mertzimekis, N.Benczer-Koller, J.Holden, G.Jakob, G.Kumbartzki, K.-H.Speidel, R.Ernst, A.Macchiavelli, M.McMahan, L.Phair, P.Maier-Komor, A.Pakou, S.Vincent, W.Korten First Measurements of g Factors in the Even Kr Isotopes NUCLEAR REACTIONS 26Mg(78Kr, 78Kr'), (80Kr, 80Kr'), (82Kr, 82Kr'), (84Kr, 84Kr'), (86Kr, 86Kr'), E=220-261 MeV; measured Eγ, Iγ(θ, H, t), (particle)γ-coin following projectile Coulomb excitation. 78,80,82,84,86Kr levels deduced T1/2, B(E2), g factors. Transient field technique, Gd-backed target, IBA-2 calculation.
doi: 10.1103/PhysRevC.64.024314
2000HO25 Phys.Lett. 493B, 7 (2000) J.Holden, N.Benczer-Koller, G.Jakob, G.Kumbartzki, T.J.Mertzimekis, K.-H.Speidel, A.Macchiavelli, M.McMahan, L.Phair, P.Maier-Komor, A.E.Stuchbery, W.F.Rogers, A.D.Davies Evidence for 2f7/2 Neutron Strength in the Low Energy Structure of 144, 146, 148, 150Nd Isotopes NUCLEAR REACTIONS Ni(144Nd, 144Nd'), (146Nd, 146Nd'), (148Nd, 148Nd'), (150Nd, 150Nd'), E=584-608 MeV; measured Eγ, Iγ(θ), precession angles following projectile Coulomb excitation. 144,146,148,150Nd levels deduced g factors, configurations. Deformation effects discussed. Gammasphere array, transient field technique.
doi: 10.1016/S0370-2693(00)01136-9
2000JA11 Phys.Lett. 494B, 187 (2000) G.Jakob, N.Benczer-Koller, J.Holden, G.Kumbartzki, T.J.Mertzimekis, K.-H.Speidel, R.Ernst, P.Maier-Komor, C.W.Beausang, R.Krucken First Measurements of the g Factors of the 21+ and 31+ States of Semi-Magic 4090Zr NUCLEAR REACTIONS 24,26Mg(90Zr, 90Zr'), E=270, 300 MeV; measured Eγ, Iγ(θ, H, t), (recoil)γ-coin, DSA following projectile Coulomb excitation. 90Zr levels deduced g factors, T1/2, configurations. Transient field technique, target backed with Gd, Ta, Cu.
doi: 10.1016/S0370-2693(00)01197-7
1999JA13 Phys.Lett. 468B, 13 (1999) G.Jakob, N.Benczer-Koller, J.Holden, G.Kumbartzki, T.J.Mertzimekis, K.-H.Speidel, C.W.Beausang, R.Krucken Spin Dependence of d5/2 Neutron Configurations in the Wave Functions of 92, 94Zr from g-Factor Measurements NUCLEAR REACTIONS Si(92Zr, 92Zr'), (94Zr, 94Zr'), E=300 MeV; measured Eγ, Iγ(θ, H, t) following projectile Coulomb excitation. 92,94Zr levels deduced g factors, configurations.
doi: 10.1016/S0370-2693(99)01203-4
1999MA06 Phys.Rev. C59, 665 (1999) N.A.Matt, N.Benczer-Koller, J.Holden, G.Kumbartzki, R.H.Mayer, M.Satteson, R.Tanczyn Competition between Single-Particle and Collective Excitations in N = 88 Nuclei: Measurement of g(41+)/g(21+) in 152Gd NUCLEAR REACTIONS 152Gd(32S, 32S'), E=100 MeV; 152Gd(58Ni, 58Ni'), E=180, 212.5 MeV; measured Eγ, Iγ(θ, H, t) following Coulomb excitation. 152Gd levels deduced g factors, single-particle, collective contributions. Transient field technique.
doi: 10.1103/PhysRevC.59.665
1999WE02 Nucl.Phys. A645, 191 (1999) L.Weissman, R.H.Mayer, N.Benczer-Koller, C.Broude, J.A.Cizewski, M.Hass, J.Holden, R.V.F.Janssens, G.Kumbartzki, T.Lauritsen, I.Y.Lee, A.O.Macchiavelli, N.Matt, D.P.McNabb, M.Satteson Time-Decay History of Normal-Deformation High-Spin States in 193, 194Hg NUCLEAR REACTIONS 150Nd(48Ca, 5n), (48Ca, 4n), E=203 MeV; measured Eγ, Iγ, γγ-coin, DSA. 193,194Hg deduced high-spin levels, J, π, T1/2, non-collective configurations. Gammasphere array.
doi: 10.1016/S0375-9474(98)00604-6
1999WE04 Phys.Lett. 446B, 22 (1999) L.Weissman, R.H.Mayer, G.Kumbartzki, N.Benczer-Koller, C.Broude, J.A.Cizewski, M.Hass, J.Holden, R.V.F.Janssens, T.Lauritsen, I.Y.Lee, A.O.Macchiavelli, D.P.McNabb, M.Satteson Single Particle Signatures in High-Spin, Quasicontinuum States in 193, 194Hg from g-Factor Measurements NUCLEAR REACTIONS 150Nd(48Ca, 5n), (48Ca, 4n), E=203 MeV; measured Eγ, Iγ(θ, H, t), γγ-coin. 193,194Hg deduced high-spin, quasicontinuum states average g factors, quasineutron configurations contributions. Gammasphere array.
doi: 10.1016/S0370-2693(98)01514-7
1998MA71 Phys.Rev. C58, R2640 (1998) R.H.Mayer, G.Kumbartzki, L.Weissman, N.Benczer-Koller, C.Broude, J.A.Cizewski, M.Hass, J.Holden, R.V.F.Janssens, T.Lauritsen, I.Y.Lee, A.O.Macchiavelli, D.P.McNabb, M.Satteson First Direct Measurements of g Factors of the Three Superdeformed Bands of 194Hg NUCLEAR REACTIONS 150Nd(48Ca, 4n), E=203 MeV; measured Eγ, Iγ(θ, t), γγ-coin. 194Hg deduced superdeformed bands average g factors. Gammasphere array, transient field technique.
doi: 10.1103/PhysRevC.58.R2640
1998SP03 Phys.Rev. C57, 2181 (1998) K.-H.Speidel, N.Benczer-Koller, G.Kumbartzki, C.Barton, A.Gelberg, J.Holden, G.Jakob, N.Matt, R.H.Mayer, M.Satteson, R.Tanczyn, L.Weissman Shell Closure Effects in the Stable 74-82Se Isotopes from Magnetic Moment Measurements using Projectile Excitation and the Transient Field Technique NUCLEAR REACTIONS Ta(74Se, 74Se'), (76Se, 76Se'), (78Se, 78Se'), (80Se, 80Se'), (82Se, 82Se'), E=230-262 MeV; measured Eγ, Iγ(H, θ) in polarized Gd following projectile Coulomb excitation. 74,76,78,80,82Se deduced g-factors. Multilayer target. Comparison with IBM calculations.
doi: 10.1103/PhysRevC.57.2181
1975LE22 Phys.Rev. C12, 1483 (1975) I.Y.Lee, J.X.Saladin, J.Holden, J.O'Brien, C.Baktash, C.Bemis, Jr., P.H.Stelson, F.K.McGowan, W.T.Milner, J.L.C.Ford, Jr., R.L.Robinson, W.Tuttle Deformation Parameters of the Charge Distribution and the Optical Potential for Some Nuclei in and Near the Rare Earth Region NUCLEAR REACTIONS 154Sm(α, α'), E=11-19 MeV; 166Er(α, α'), E=12.5-19.5 MeV; 182W(α, α'), E=13-21 MeV; measured σ(Eα'). 168Er(α, α'), E=13-19 MeV; 184W(α, α'), E=12.5-19 MeV; 186W(α, α'), E=13.25-19 MeV; measured σ(Eα', θ). 154Sm, 166,168Er, 182,184,186W deduced M(E2), M(E4), charge deformations, optical potential deformations.
doi: 10.1103/PhysRevC.12.1483
1974BA81 Phys.Rev. C10, 2265 (1974) C.Baktash, J.X.Saladin, J.O'Brien, I.Y.Lee, J.E.Holden Determination of B(E2, 0+ → 2+') for Some Even-Even Nuclei in and Near the Rare-Earth Region NUCLEAR REACTIONS 158,160Gd, 162,164Dy, 166,168Er(α, α'), E=11.0-12.5 MeV; 184,186W(α, α'), E=13.25-13.5 MeV; measured σ(E, Eα'). 158,160Gd, 162,164Dy, 166,168Er, 184,186W transitions deduced B(E2).
doi: 10.1103/PhysRevC.10.2265
1974CO06 Phys.Rev. C9, 1025 (1974) B.L.Cohen, J.E.Holden, G.R.Rao High-Resolution Comparison of (p, p') and (d, d') Reactions NUCLEAR REACTIONS 58,64Ni, 124Sn(p, p'), (d, d'), E=12, 17 MeV; measured σ(Ep'), σ(Ed'). 58,64Ni, 124Sn levels deduced relative strengths.
doi: 10.1103/PhysRevC.9.1025
1974LE16 Phys.Rev.Lett. 33, 383 (1974) I.Y.Lee, J.X.Saladin, C.Baktash, J.E.Holden, J.O'Brien Nuclear-Coulomb Interference in Inelastic Scattering of α Particles from 168Er, 184W, and 186W NUCLEAR REACTIONS 168Er, 184,186W(α, α'), E=12.5-19 MeV; measured σ(E, Eα', θ). 168Er, 184,186W deduced charge, optical-potential deformation parameters.
doi: 10.1103/PhysRevLett.33.383
1973HO04 Phys.Rev. C7, 611 (1973) J.E.Holden, D.P.Balamuth, H.T.Fortune, R.W.Zurmuhle Comparison of the 27Al(3He, 3He')27Al and 27Al(3He, t)27Si Reactions at 18 MeV NUCLEAR REACTIONS 27Al(3He, 3He'), (3He, t), E=18 MeV; measured σ(θ). 27Al, 27Si deduced levels, J, π, deformation parameters β(L).
doi: 10.1103/PhysRevC.7.611
1973HO16 Phys.Rev. C8, 2286 (1973) States of 94Mo from the 95Mo(d, t)94Mo Reaction NUCLEAR REACTIONS 95Mo(d, t), Ed=17.0 MeV; measured σ(Et, θ), 8-keV resolution. 94Mo deduced levels, J, π, L(n), S; DWBA analysis. Enriched target.
doi: 10.1103/PhysRevC.8.2286
1972BA06 Phys.Rev. C5, 476 (1972) D.P.Balamuth, J.E.Holden, R.W.Zurmuhle Angular-Correlation Study of 27Si between E = 2.5 and E = 5 MeV Using the Reaction 28Si(3He, αγ)27Si NUCLEAR REACTIONS 28Si(3He, αγ), E=15 MeV; measured σ(Eγ, θ(γγ)). 27Si levels deduced J, π, γ-mixing, γ-branching.
doi: 10.1103/PhysRevC.5.476
1972ER04 Phys.Rev.Lett. 29, 1010 (1972) K.A.Erb, J.E.Holden, I.Y.Lee, J.X.Saladin, T.K.Saylor Quadrupole and Hexadecapole Deformations in Rare-Earth Nuclei NUCLEAR REACTIONS 158,160Gd, 162,164Dy, 166,168,170Er(α, α), (α, α'), E=11-13 MeV; measured σ ratios. 158,160Gd, 162,164Dy , 166,168,170Er deduced B(E2), B(E4), β(L).
doi: 10.1103/PhysRevLett.29.1010
1972HO44 Phys.Rev. C6, 1305 (1972) J.E.Holden, J.J.Kolata, W.W.Daehnick States of 86Rb: the 87Rb(d, t)86Rb Reaction NUCLEAR REACTIONS 87Rb(d, t), E=17.5 MeV; measured σ(Et, θ). 86Rb deduced levels, J, π, S, L(n).
doi: 10.1103/PhysRevC.6.1305
1972KO37 Phys.Rev. C6, 1312 (1972) J.J.Kolata, W.W.Daehnick, J.E.Holden States of 86Rb: the 88Sr(d, α)86Rb Reaction NUCLEAR REACTIONS 88Sr(d, α), E=17 MeV; measured σ(Eα, θ). 86Rb deduced levels, J, π, L.
doi: 10.1103/PhysRevC.6.1312
1971BA33 Phys.Rev.Lett. 26, 1271 (1971) D.P.Balamuth, J.E.Holden, J.W.Noe, R.W.Zurmuhle High-Spin States in 24Mg NUCLEAR REACTIONS 16O(12C, α), E=36 MeV; measured σ(Eα, θ(αα)). 24Mg levels deduced J, π.
doi: 10.1103/PhysRevLett.26.1271
1970HO30 Phys.Rev.Lett. 25, 1677 (1970) J.E.Holden, H.T.Fortune, D.P.Balamuth, R.W.Zurmuhle Sensitivity of the (3He, t) Reaction to Final-State Configurations NUCLEAR REACTIONS 23Na, 27Al(3He, t), E=18 MeV; measured σ(θ); deduced dependence on final-state configuration. 23Mg, 27Si transitions deduced L.
doi: 10.1103/PhysRevLett.25.1677
1970ZU01 Phys.Rev. C2, 1577 (1970) R.W.Zurmuhle, D.P.Balamuth, J.E.Holden New Low-Lying States in 57Ni Observed in the 58Ni(3He, α)57Ni Reaction NUCLEAR REACTIONS 58Ni(3He, α), E=15 MeV; measured σ(Eα, θ). 57Ni deduced levels.
doi: 10.1103/PhysRevC.2.1577
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