Nuclear Science References (NSR)

Indirect Transitions in Two-Nucleon Transfer Reactions between Heavy Ions

NUCLEAR REACTIONS ^60,62,64Ni, ¹²²Sn(¹⁶O, ¹⁸O); calculated σ(θ).

doi: 10.1016/0375-9474(77)90511-5
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1976GL06 Phys.Rev.Lett. 36, 1532 (1976)

Physical Basis for Enhanced Forward Cross Sections in Heavy-Ion Reactions

NUCLEAR REACTIONS ⁶⁰Ni(¹⁸O, ¹⁶O), E=65 MeV; ⁵⁸Ni(¹⁸O, ¹⁸O), (¹⁸O, ¹⁸O'), E=60 MeV; ⁶²Ni(¹⁶O, ¹⁸O), E=70.7 MeV; calculated σ(θ).

doi: 10.1103/PhysRevLett.36.1532
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1976GL08 Nucl.Phys. A269, 223 (1976)

Two-Particle Transfer Contributions to Elastic and Inelastic Heavy Ion Scattering

NUCLEAR REACTIONS ¹⁸O(¹⁶O, ¹⁶O), E=24, 28, 32 MeV; calculated σ(θ).

doi: 10.1016/0375-9474(76)90408-5
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1975GL03 Phys.Rev.Lett. 34, 1642 (1975)

Enhancement of Forward-Angle Cross Sections in Heavy-Ion Reactions Because of Projectile Excitation

NUCLEAR REACTIONS ¹²²Sn(¹⁶O, ¹⁸O), E=62.2, 104 MeV; calculated σ(E(¹⁸O), θ); deduced reaction mechanism.

doi: 10.1103/PhysRevLett.34.1642
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1975SC04 Phys.Rev.Lett. 34, 895 (1975)

D.K.Scott, B.G.Harvey, D.L.Hendrie, U.Jahnke, L.Kraus, C.F.Maguire, J.Mahoney, Y.Terrien, K.Yagi, N.K.Glendenning

Interference between Direct and Indirect Modes in Two-Nucleon Transfer Reactions with Heavy Ions

NUCLEAR REACTIONS ¹²²Sn(¹⁶O, ¹⁸O), E=104 MeV; ¹²²Sn(¹⁸O, ¹⁶O), E=99 MeV; measured σ(θ); deduced reaction mechanism.

doi: 10.1103/PhysRevLett.34.895
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1974AS01 Phys.Lett. 48B, 6 (1974)

The Sensitivity of the Forward Cross Section in Transfer Reactions between Heavy Ions to the Edge of the Nuclear Field

NUCLEAR REACTIONS ¹²⁰Sn(¹⁸O, ¹⁶O); measured nothing, calculated σ(θ).

doi: 10.1016/0370-2693(74)90442-0
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1974BE16 Phys.Rev. C9, 1543 (1974)

F.D.Becchetti, D.G.Kovar, B.G.Harvey, D.L.Hendrie, H.Homeyer, J.Mahoney, W.von Oertzen, N.K.Glendenning

Two-Proton-Transfer Reactions ²⁰⁸Pb(¹²C, ¹⁰Be)²¹⁰Po and ²⁰⁸Pb(¹⁶O, ¹⁴C)²¹⁰Po

NUCLEAR REACTIONS ²⁰⁸Pb(¹²C, ¹⁰Be), (¹⁶O, ¹⁴C), E(¹²C)=78 MeV, E(¹⁶O)=104, 140 MeV; ²⁰⁹Bi(¹²C, ¹¹B), (¹⁶O, ¹⁵N), E(¹²C)=78 MeV, E(¹⁶O)=104 MeV; measured σ(Eout, θ). ²¹⁰Po levels deduced relative strengths.

doi: 10.1103/PhysRevC.9.1543
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1973AS03 Phys.Lett. 45B, 85 (1973)

R.J.Ascuitto, K.Glendenning

The Effect of Indirect Transitions on Two Nucleon Transfer between Heavy Ions and their Q-Dependence

NUCLEAR REACTIONS ¹²⁰Sn(¹⁸O, ¹⁶O), E=100 MeV; measured nothing, calculated σ(θ), form factors.

doi: 10.1016/0370-2693(73)90070-1
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1973AS05 Phys.Lett. 47B, 332 (1973)

On the Systematics of the Interference between Direct and Indirect Modes in Two-Nucleon Pickup and Stripping Reactions between Heavy-Ions

NUCLEAR REACTIONS ^112,120Sn(¹⁸O, ¹⁶O), ^114,122Sn(¹⁶O, ¹⁸O), E=100 MeV; calculated σ(θ).

doi: 10.1016/0370-2693(73)90615-1
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1973SC13 Nucl.Phys. A207, 321 (1973)

R.Schaeffer, N.K.Glendenning

Second-Order Effects in the (³He, t) Reaction

NUCLEAR REACTIONS ^58,60,62,64Ni(³He, t); measured nothing. Calculated σ(θ).

doi: 10.1016/0375-9474(73)90350-3
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1972AS05 Nucl.Phys. A183, 60 (1972)

R.J.Ascuitto, N.K.Glendenning, B.Sorensen

The Importance of Indirect Transitions on (p, t) Reactions on Deformed Nuclei

NUCLEAR REACTIONS ¹⁷⁶Yb, ²⁰⁸Pb, ¹⁵⁴Sm(p, t), E=19 MeV; calculated σ(θ); included indirect contributions.

doi: 10.1016/0375-9474(72)90931-1
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1972AS08 Nucl.Phys. A188, 185 (1972)

R.J.Ascuitto, N.K.Glendenning, B.Sorensen

Quantum Mechanical Treatment of Particle Transfer between Heavy Ions Near the Coulomb Barrier in the Presence of Coulomb Excitation

doi: 10.1016/0375-9474(72)90193-5
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1971AS02 Phys.Lett. 34B, 17 (1971)

Confirmation of Strong Second Order Processes in (p, t) Reactions on Deformed Nuclei

NUCLEAR REACTIONS ¹⁷⁶Yb(p, t), E=19 MeV; calculated σ(θ); deduced second-order processes.

doi: 10.1016/0370-2693(71)90493-X
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1971AS04 Nucl.Phys. A170, 65 (1971)

R.J.Ascuitto, N.K.Glendenning, B.Sorensen

Twice Double-Transfer in Inelastic Proton Scattering Processes Involving Collective Pairing States, Studied in a Coupled Channels Formalism

NUCLEAR REACTIONS ⁴⁸Ca(p, p'), (p, p), E=12, 18, 30 MeV; calculated σ(θ). Coupled-channel formalism.

doi: 10.1016/0375-9474(71)90683-X
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1971GL08 Nucl.Phys. A168, 575 (1971)

N.K.Glendenning, R.S.Mackintosh

Study of Inelastic Processes on (d, p) Reactions in Deformed Nuclei

NUCLEAR REACTIONS ¹⁵⁶Gd, ¹⁶⁶Er(d, p), E=12 MeV; calculated σ(θ).

doi: 10.1016/0375-9474(71)90548-3
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1970AP03 Nucl.Phys. A159, 367 (1970)

A.A.Aponick, Jr., C.M.Chesterfield, D.A.Bromley, N.K.Glendenning

Quadrupole and Hexadecapole Deformations in Rare Earth Nuclei

NUCLEAR REACTIONS ¹⁵⁴Sm, ¹⁶⁶Er, ¹⁷⁶Yb(α, α'), E=27.5, 30.0, 32.5 MeV; measured σ(Eα', θ). ¹⁴⁸Sm(α, α), E=27.5, 30.0, 32.5 MeV; measured σ(θ); deduced optical model parameters. ¹⁵⁴Sm, ¹⁶⁶Er, ¹⁷⁶Yb levels deduced deformation parameters β(L).

doi: 10.1016/0375-9474(70)90713-X
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1970AS07 Phys.Rev. C2, 1260 (1970)

N.K.Glendenning, R.S.Mackintosh

Assessment of Two-Step Processes in (p, t) Reactions

NUCLEAR REACTIONS ⁶²Ni(p, t), E=30 MeV; calculated σ(θ), P(θ).

doi: 10.1103/PhysRevC.2.1260
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1970ST09 Phys. Rev.Lett. 24, 1137 (1970)

F.S.Stephens, R.M.Diamond, N.K.Glendenning, J.de Boer

Electric Hexadecapole Transition Moment in ¹⁵²Sm

NUCLEAR REACTIONS ¹⁵²Sm(α, α'γ), E=10-14 MeV; measured σ(E;Eα, Eγ). ¹⁵²Sm deduced E4 transition moment, deformation parameters β(L).

doi: 10.1103/PhysRevLett.24.1137
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1969GL03 Phys.Letters 29B, 626 (1969)

Non-Rigidity in Alpha Scattering from Deformed Nuclei

doi: 10.1016/0370-2693(69)90091-4
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1968FL02 Phys.Rev. 165, 1153 (1968)

D.G.Fleming, J.Cerny, N.K.Glendenning

Inadequacy of the Simple Distorted-Wave Born-Approximation Treatment of Comparative (p, t) and (p, ³He) Transitions

NUCLEAR STRUCTURE ¹¹B, ¹¹C, ¹³C; measured not abstracted; deduced nuclear properties.

doi: 10.1103/PhysRev.165.1153
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1968FL03 Phys.Rev. 166, 1012 (1968)

D.G.Fleming, J.Cerny, C.C.Maples, N.K.Glendenning

¹⁵N(p, t)¹³N and ¹⁵N(p, ³He)13c Reactions and the Spectroscopy of Levels in Mass 13

NUCLEAR STRUCTURE ¹³C, ¹³N, ¹⁵N; measured not abstracted; deduced nuclear properties.

doi: 10.1103/PhysRev.166.1012
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1968GL05 Phys.Letters 26B, 131 (1968)

N.K.Glendenning, D.L.Hendrie, O.N.Jarvis

Relation between the Optical Potential for Spherical and Deformed Nuclei

NUCLEAR REACTIONS ^148,154Sm(α, α), (α, α'), E=50 MeV; calculated σ(θ). Optical model.

doi: 10.1016/0370-2693(68)90504-2
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1968HE24 Phys.Letters 26B, 127 (1968)

D.L.Hendrie, N.K.Glendenning, B.G.Harvey, O.N.Jarvis, H.H.Duhm, J.Saudinos, J.Mahoney

Determination of Y₄₀ and Y₆₀ Components in the Shapes of Rare Earth Nuclei

NUCLEAR REACTIONS ^152,154Sm, ¹⁵⁸Gd, ¹⁶⁶Er, ^174,176Yb, ¹⁷⁸Hf(α, α'), E=50 MeV; measured σ(θ). Deduced deformation parameters.

doi: 10.1016/0370-2693(68)90502-9
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC2752.

1968MA29 Nucl.Phys. A117, 161(1968)

N.F.Mangelson, B.G.Harvey, N.K.Glendenning

Spectroscopy of ¹⁴N by Use of the ¹²C(³He, p)¹⁴N Reaction

NUCLEAR REACTIONS ¹²C(³He, p), E=20.1 MeV; measured σ(Ep, θ). ¹⁴N levels deduced J, π, L. Natural target.

doi: 10.1016/0375-9474(68)90868-3
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC0933.

1968MA33 Nucl.Phys. A119, 79(1968) Erratum Nucl.Phys. A127, 693(1969)

N.F.Mangelson, B.G.Harvey, N.K.Glendenning

Study of ¹⁸F by Use of (³He, p) and (α, d) Reactions

NUCLEAR REACTIONS ¹⁶O(³He, p), E=19.8 MeV; measured σ(Ep, θ). ¹⁶O(α, d), E=40.3 MeV; measured σ(Ed, θ). ¹⁸F deduced levels, J, π, L. Natural target.

doi: 10.1016/0375-9474(68)90807-5
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC0917.

1967FL09 Phys.Rev.Lett. 19, 798 (1967)

E.R.Flynn, G.J.Igo, R.Woods, P.D.Barnes, N.K.Glendenning

Levels Excited in ²⁰⁶Pb with Both Two-Neutron Stripping and Pickup Reactions

NUCLEAR REACTIONS ²⁰⁴Pb(t, p), E=20 MeV; ²⁰⁸Pb(p, t), E=22 MeV; measured σ(Ep), σ(Et). ²⁰⁶Pb deduced levels.

doi: 10.1103/PhysRevLett.19.798
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1967GL04 Phys.Rev. 156, 1344 (1967)

N.K.Glendenning, K.Harada

Analysis of the ²⁰⁸Pb(p, t) Reaction

NUCLEAR STRUCTURE ²⁰⁶Pb; measured not abstracted; deduced nuclear properties.

doi: 10.1103/PhysRev.156.1344
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1965BU05 Phys.Letters 16, 296 (1965)

A.Bussiere, N.K.Glendenning, B.G.Harvey, J.Mahoney, J.R.Meriwether, D.J.Horen

Octupole States in ¹⁵N and ¹⁶O

NUCLEAR STRUCTURE ¹⁶O, ¹⁵N; measured not abstracted; deduced nuclear properties.

doi: 10.1016/0031-9163(65)90859-0
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1965GL06 Nucl.Phys. 72, 481 (1965)

Shell-Model Calculation for ²¹²Po

NUCLEAR STRUCTURE ²¹²Po; measured not abstracted; deduced nuclear properties.

doi: 10.1016/0029-5582(65)90406-2
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1965GL09 Phys.Rev. 137, B102 (1965)

Nuclear Spectroscopy with Two-Nucleon Transfer Reactions

NUCLEAR REACTIONS ¹²C(α, d), (³He, p); analyzed data. ¹⁴N levels deduced structure amplitudes, L.

doi: 10.1103/PhysRev.137.B102
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1962GL02 Phys.Rev. 127, 923 (1962)

Note on an Isomeric State of Po²¹²

NUCLEAR STRUCTURE ²¹²Po; measured not abstracted; deduced nuclear properties.

doi: 10.1103/PhysRev.127.923
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1962WI19 UCRL-10624, p.159 (1962)

B.D.Wilkins, R.H.Pehl, N.K.Glendenning

Optical-Model Analysis for 10-MeV Protons

1961AL07 Phys.Rev. 122, 862 (1961)

R.D.Albert, S.D.Bloom, N.K.Glendenning

(p, n) Angular Distributions from Mirror Nucleus Targets: C¹³, B¹¹, and Be⁹

NUCLEAR STRUCTURE ⁹Be, ¹¹B, ¹³C; measured not abstracted; deduced nuclear properties.

doi: 10.1103/PhysRev.122.862
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1961CE02 Bull.Am.Phys.Soc. 6, No.6, 507, E11 (1961)

J.Cerny, N.K.Glendenning, B.G.Harvey, R.H.Pehl, E.Rivet

Analysis of the Two-Nucleon Stripping Reaction C¹²(He³, p)N¹⁴

NUCLEAR STRUCTURE ¹²C; measured not abstracted; deduced nuclear properties.

1960GL02 Phys.Rev. 119, 213 (1960)

Theoretical Predictions for the Spectra of the Odd-Mass Xenon and Tellurium Isotopes

NUCLEAR STRUCTURE ¹²⁹Xe, ¹²⁵Te, ¹²³Te, ¹²³Xe; measured not abstracted; deduced nuclear properties.

doi: 10.1103/PhysRev.119.213
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1959GL57 Phys.Rev. 114, 1297 (1959)