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NSR database version of April 27, 2024.

Search: Author = J.Holden

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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 T_1/2, 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, 136}Xe 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. ^{130,132,134,136}Xe levels deduced g factors, T_1/2. 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. ^{144,146,148,150}Nd 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. ^{78,80,82,84,86}Kr levels deduced T_1/2, 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 2f_7/2 Neutron Strength in the Low Energy Structure of ^{144, 146, 148, 150}Nd 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. ^{144,146,148,150}Nd 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, T_1/2, 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 d_5/2 Neutron Configurations in the Wave Functions of ^{92, 94}Zr 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, 194}Hg

NUCLEAR REACTIONS ¹⁵⁰Nd(⁴⁸Ca, 5n), (⁴⁸Ca, 4n), E=203 MeV; measured Eγ, Iγ, γγ-coin, DSA. ^193,194Hg deduced high-spin levels, J, π, T_1/2, 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, 194}Hg 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. ^{74,76,78,80,82}Se 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