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NSR database version of April 11, 2024.

Search: Author = J.Holden

Found 25 matches.

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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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1973HO16      Phys.Rev. C8, 2286 (1973)

J.E.Holden, W.W.Daehnick

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
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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
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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
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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
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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
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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
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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
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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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Note: The following list of authors and aliases matches the search parameter J.Holden: , J.E.HOLDEN