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NSR database version of April 11, 2024.

Search: Author = J.N.Ginocchio

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2006GI05      Int.J.Mod.Phys. E15, 1843 (2006)


Pseudospin symmetry in nuclei as a relativistic symmetry

doi: 10.1142/S0218301306004879
Citations: PlumX Metrics

2005GI05      Int.J.Mod.Phys. E14, 105 (2005)


Pseudospin symmetry and the nucleon-nucleon interaction

doi: 10.1142/S0218301305002825
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2005GI06      Phys.Rep. 414, 165 (2005)


Relativistic symmetries in nuclei and hadrons

doi: 10.1016/j.physrep.2005.04.003
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2005GI08      Phys.Rev. C 71, 064325 (2005)


Critical point symmetry in a fermion monopole and quadrupole pairing model

NUCLEAR STRUCTURE Xe; analyzed B(E2); deduced symmetry features. Fermion monopole and quadrupole pairing model.

doi: 10.1103/PhysRevC.71.064325
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2005GI19      Phys.Rev.Lett. 95, 252501 (2005)


U(3) and Pseudo-U(3) Symmetry of the Relativistic Harmonic Oscillator

doi: 10.1103/PhysRevLett.95.252501
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2004GI01      Phys.Rev. C 69, 034303 (2004)

J.N.Ginocchio, A.Leviatan, J.Meng, S.-G.Zhou

Test of pseudospin symmetry in deformed nuclei

NUCLEAR STRUCTURE 168Er; calculated single-particle energies, wave functions, role of pseudospin symmetry.

doi: 10.1103/PhysRevC.69.034303
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2004GI02      Phys.Rev. C 69, 034318 (2004)


Relativistic harmonic oscillator with spin symmetry

doi: 10.1103/PhysRevC.69.034318
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2003LE10      Phys.Rev.Lett. 90, 212501 (2003)

A.Leviatan, J.N.Ginocchio

Critical-Point Symmetry in a Finite System

doi: 10.1103/PhysRevLett.90.212501
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2003ZH35      Phys.Rev. C 68, 044320 (2003)

Y.M.Zhao, A.Arima, J.N.Ginocchio, N.Yoshinaga

General pairing interactions and pair truncation approximations for fermions in a single-j shell

doi: 10.1103/PhysRevC.68.044320
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2002GI07      Phys.Rev. C65, 054002 (2002)


Pseudospin and Spin Symmetry in Nucleon-Nucleon Scattering

doi: 10.1103/PhysRevC.65.054002
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2002GI13      Phys.Rev. C 66, 064312 (2002)


Pseudospin symmetry and relativistic mean field eigenfunctions

doi: 10.1103/PhysRevC.66.064312
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2002SM01      Phys.Rev. C65, 024319 (2002)

N.A.Smirnova, N.Pietralla, A.Leviatan, J.N.Ginocchio, C.Fransen

Extended M1 Sum Rule for Excited Symmetric and Mixed-Symmetry States in Nuclei

NUCLEAR STRUCTURE 94Mo; analyzed mixed-symmetry states B(M1) transition rates; deduced quadrupole d-boson ratio. Interacting boson model, generalized sum rule.

doi: 10.1103/PhysRevC.65.024319
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2001GI07      Nucl.Phys. A690, 41c (2001)


A Relativistic Symmetry in Nuclei: Its origins and consequences

doi: 10.1016/S0375-9474(01)00929-0
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2001GI08      Phys.Rev.Lett. 87, 072502 (2001)

J.N.Ginocchio, A.Leviatan

Test of Nuclear Wave Functions for Pseudospin Symmetry

doi: 10.1103/PhysRevLett.87.072502
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2001LE35      Phys.Lett. 518B, 214 (2001)

A.Leviatan, J.N.Ginocchio

Consequences of a Relativistic Pseudospin Symmetry for Radial Nodes and Intruder Levels in Nuclei

doi: 10.1016/S0370-2693(01)01039-5
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2000LE04      Phys.Rev. C61, 024305 (2000)

A.Leviatan, J.N.Ginocchio

F Spin as a Partial Symmetry

NUCLEAR STRUCTURE 148,150Nd, 148,150,154Sm, 154,160Gd, 160,162,164Dy, 166,168,170Er, 172,174Yb; analyzed levels, B(M1); deduced F-spin symmetry. Scissors modes, IBM-2 Hamiltonians.

doi: 10.1103/PhysRevC.61.024305
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2000VO12      Phys.Rev. C62, 014308 (2000)

P.von Neumann-Cosel, J.N.Ginocchio

l-Forbidden M1 Transitions and Pseudospin Symmetry

NUCLEAR STRUCTURE 37Ar, 39Ca, 53Cr, 57,59Ni, 57Fe, 67Ga, 91Zr, 95Mo, 97Ru, 121Sb, 127,129,131I, 139Ce, 141,145Nd, 203,205Tl, 207,209Pb; calculated transitions B(M1), spectroscopic factors for pseudospin partners. Comparison with data.

doi: 10.1103/PhysRevC.62.014308
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1999GI06      Phys.Rev. C59, 2487 (1999)


Implications of Pseudospin Symmetry on Relativistic Magnetic Properties and Gamow-Teller Transitions in Nuclei

RADIOACTIVITY 39Ca(β+); calculated l-forbidden transition Gamow-Teller strength; deduced pseudospin symmetry effects.

doi: 10.1103/PhysRevC.59.2487
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1999GI07      J.Phys.(London) G25, 617 (1999)


On the Relativistic Origins of Pseudo-Spin Symmetry in Nuclei

doi: 10.1088/0954-3899/25/4/008
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1999GI08      Phys.Rev.Lett. 82, 4599 (1999)


Resurrection of a Symmetry in Nucleon-Nucleon Scattering

NUCLEAR REACTIONS 208Pb(polarized p, p), E=800 MeV; analyzed σ(θ); deduced pseudospin symmetry features.

doi: 10.1103/PhysRevLett.82.4599
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1999GI10      Phys.Rep. 315, 231 (1999)


A Relativistic Symmetry in Nuclei

doi: 10.1016/S0370-1573(99)00021-6
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1999GI19      Nucl.Phys. (Supplement) A654, 663c (1999)


The Relativistic Foundations of Pseudospin Symmetry in Nuclei

NUCLEAR STRUCTURE 208Pb; calculated levels, J, π, pseudospin doublet level energy splitting. Comparison with data.

doi: 10.1016/S0375-9474(00)88522-X
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1998GI04      Phys.Rev. C57, 1167 (1998)

J.N.Ginocchio, D.G.Madland

Pseudospin Symmetry and Relativistic Single-Nucleon Wave Functions

NUCLEAR STRUCTURE 208Pb; calculated neutron, proton pseudospin doublets wavefunctions, levels; deduced pseudospin symmetry effects. Realistic relativistic mean fields.

doi: 10.1103/PhysRevC.57.1167
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1998GI08      Phys.Lett. 425B, 1 (1998)

J.N.Ginocchio, A.Leviatan

On the Relativistic Foundations of Pseudospin Symmetry in Nuclei

doi: 10.1016/S0370-2693(98)00188-9
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1997GI01      Phys.Rev.Lett. 78, 436 (1997)


Pseudospin as a Relativistic Symmetry

doi: 10.1103/PhysRevLett.78.436
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1997GI05      Phys.Rev.Lett. 79, 813 (1997)

J.N.Ginocchio, A.Leviatan

Magnetic Dipole Sum Rules for Odd-Mass Nuclei

NUCLEAR STRUCTURE 161Dy, 167Er; calculated total B(M1) strength; deduced sum rules physical content, geometric interpretation.

doi: 10.1103/PhysRevLett.79.813
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1996GI07      Phys.Rev.Lett. 77, 28 (1996)


New Type of Collective Motion for N ∼ Z Nuclei

NUCLEAR STRUCTURE 64Ge; calculated lowest levels; deduced quantum numbers. 44Ti, 48Cr; calculated levels, B(λ). New α-type collective motion.

doi: 10.1103/PhysRevLett.77.28
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1996WU06      Phys.Rev. C54, 1208 (1996)

H.C.Wu, J.N.Ginocchio, A.E.L.Dieperink, O.Scholten

Double Charge Exchange on Te Isotopes in the Generalized Seniority Scheme

NUCLEAR STRUCTURE 128,130Te; calculated double IAS, ground state double charge exchange transition σ leading to 128,130Xe. Generalized seniority scheme, pion double charge exchange reactions.

doi: 10.1103/PhysRevC.54.1208
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1995GI03      Phys.Rev. C51, 1861 (1995)

J.N.Ginocchio, C.W.Johnson

Unified Theory of Fermion Pair to Boson Mappings in Full and Truncated Spaces

doi: 10.1103/PhysRevC.51.1861
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1995VO10      Phys.Rev.Lett. 75, 4178 (1995)

P.von Neumann-Cosel, J.N.Ginocchio, H.Bauer, A.Richter

Relation between the Scissors Mode and the Interacting Boson Model Deformation

NUCLEAR STRUCTURE 146,148,150Nd, 148,150,152,154Sm, 156,158,160Gd, 160,162,164Dy, 166,168,170Er, 172,174,176Yb, 182,184,186W; analyzed B(M1); deduced relation between scissors mode and model deformation. Interacting boson model sum rule strength.

doi: 10.1103/PhysRevLett.75.4178
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1994GI11      Phys.Rev.Lett. 73, 1903 (1994)

J.N.Ginocchio, A.Leviatan

Quadrupole Collectivity with Isospin

doi: 10.1103/PhysRevLett.73.1903
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1994JO06      Phys.Rev. C50, R571 (1994)

C.W.Johnson, J.N.Ginocchio

Hermitian Boson Mapping and Finite Truncation

doi: 10.1103/PhysRevC.50.R571
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1994OT06      Nucl.Phys. A577, 197c (1994)

T.Otsuka, J.N.Ginocchio

M1 Excitation of Deformed Nuclei and Proton-Neutron Correction

NUCLEAR STRUCTURE 156Sm; calculated (J(π), J(ν)) matrix element vs J; deduced M1 excitation features. Nilsson, interacting boson models.

doi: 10.1016/0375-9474(94)90855-9
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1993GI05      Phys.Rev. C48, 1460 (1993)


Test of Generalized Seniority with Pion Double Charge Exchange on the Nickel Isotopes

NUCLEAR REACTIONS Ni(π+, π-), E=35, 292 MeV; Sn(π+, π-), E=35 MeV; analyzed σ(θ) vs valence neutron pair number. Generalized seniority model.

doi: 10.1103/PhysRevC.48.1460
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1992BA15      Phys.Rev. C45, R1417 (1992)

B.R.Barrett, R.F.Casten, J.N.Ginocchio, T.Seligman, H.A.Weidenmuller

Is there Incomplete Mixing of States with Different K Quantum Numbers in the Neutron Resonance Region ( Question )

NUCLEAR STRUCTURE 168Er, 178Hf; analyzed primary transitions Iγ; deduced incomplete K-mixing evidence.

doi: 10.1103/PhysRevC.45.R1417
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1991GI08      Phys.Lett. 265B, 6 (1991)


A Sum Rule for B(M1) Strength

NUCLEAR STRUCTURE 168Er, 160,164Dy, 154,160Gd, 148,154Sm, 146,150Nd; calculated quadrupole bosons average number; deduced B(M1) strength sum rule.

doi: 10.1016/0370-2693(91)90003-9
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1990LE21      Phys.Rev.Lett. 65, 2853 (1990)

A.Leviatan, J.N.Ginocchio, M.W.Kirson

Proton-Neutron Deformations and F-Spin Symmetry in Nuclei

NUCLEAR STRUCTURE 165Ho; calculated ground state band F-spin mixing; deduced proton, neutron deformations role.

doi: 10.1103/PhysRevLett.65.2853
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1988AU05      Phys.Rev. C38, 1277 (1988)

N.Auerbach, W.R.Gibbs, J.N.Ginocchio, W.B.Kaufmann

Pion-Nucleus Double Charge Exchange and the Nuclear Shell Model

NUCLEAR REACTIONS 42,44,46,48Ca, 46,48,50Ti, 52Cr, 54Fe(π+, π-), E=35, 45, 292 MeV; calculated ground, IAS transition σ(θ). Shell model.

doi: 10.1103/PhysRevC.38.1277
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1988WE05      J.Phys.(London) G14, Supplement S65 (1988)

G.Wenes, J.N.Ginocchio

An Algebraic Approach to Medium Energy Proton Scattering

NUCLEAR REACTIONS 154Gd(p, p'), E=650 MeV; calculated σ(θ). Glauber model.

doi: 10.1088/0305-4616/14/1/010
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1988WE08      Phys.Rev. C37, 1878 (1988)

G.Wenes, T.Otsuka, J.N.Ginocchio

F-Spin Vector Effects in Inelastic Electron Scattering from Low-Lying Collective States of 154Gd

NUCLEAR REACTIONS 154Gd(e, e'), E not given; analyzed data; deduced boson form factors. 154Gd levels deduced neutron-proton asymmetry. Interacting boson model.

NUCLEAR STRUCTURE 154Gd; calculated levels, B(λ). Interacting boson model.

doi: 10.1103/PhysRevC.37.1878
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1987GI08      Phys.Rev. C36, 2436 (1987)

J.N.Ginocchio, G.Wenes, R.D.Amado, D.C.Cook, N.M.Hintz, M.M.Gazzaly

Medium Energy Proton Scattering from 154Gd and the Interacting Boson Model of Nuclei

NUCLEAR REACTIONS 154Gd(p, p'), E=650 MeV; measured σ(θ). 154Gd levels deduced B(λ). Interacting boson model quadrupole hadronic transition operator, compared to boson electromagnetic operator.

doi: 10.1103/PhysRevC.36.2436
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1987GU06      Phys.Lett. 187B, 210 (1987)

M.W.Guidry, C.-L.Wu, Z.-P.Li, D.H.Feng, J.N.Ginocchio

An Algerbraic Fermion Description of Band Termination and Loss of Collectivity in Heavy Nuclei

NUCLEAR STRUCTURE 162Dy, 160,166,174,176Yb, 168,172W; calculated B(E2) ratio relative to rigid rotor value. Algebraic fermion model.

doi: 10.1016/0370-2693(87)91082-3
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1987HA41      Phys.Rev. C36, 2611 (1987)

P.Halse, J.N.Ginocchio

SU(3) X SU(4) Limit of an Isospin Invariant Fermion Dynamical Symmetry Model

NUCLEAR STRUCTURE 20,22Ne, 24Mg, 16O; calculated levels, band structure; deduced symmetry classification.

doi: 10.1103/PhysRevC.36.2611
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1986CA10      Phys.Rev.Lett. 56, 2578 (1986)

R.F.Casten, C.-L.Wu, Da Hsuan Feng, J.N.Ginocchio, Xiao-Ling Han

Empirical Evidence for an SO(7) Fermion Dynamical Symmetry in Nuclei

NUCLEAR STRUCTURE 98,100,102,104,106Pd, 104,106,108,110,112Pd; calculated levels, B(E2) ratios; deduced dynamical symmetry evidence. Ginocchio model, SO(7) fermion dynamical symmetry.

doi: 10.1103/PhysRevLett.56.2578
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1986GI01      Phys.Rev. C33, 247 (1986)

J.N.Ginocchio, T.Otsuka, R.D.Amado, D.A.Sparrow

Medium Energy Probes and the Interacting Boson Model of Nuclei

NUCLEAR REACTIONS Sm(p, p), (p, p'), E=800 MeV; calculated σ(θ). Glauber approximation plus interacting boson model.

doi: 10.1103/PhysRevC.33.247
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1986GI02      Phys.Rev. C33, 365 (1986)

J.N.Ginocchio, P.Van Isacker

Determination of the Neutron and Proton Effective Charges in the Quadrupole Operator of Nuclear Collective Models

NUCLEAR STRUCTURE 104,106,108,110Pd; calculated electric quadrupole transition matrix elements; deduced neutron, proton effective charges. Interacting boson model.

doi: 10.1103/PhysRevC.33.365
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1986GI11      Phys.Rev. C34, 1127 (1986)

J.N.Ginocchio, G.Wenes

Electromagnetic and Hadronic Form Factors and Operators in the Interacting Boson Model

NUCLEAR REACTIONS 154Sm(p, p'), E=800 MeV; calculated σ(θ). Interacting boson model transition form factors.

doi: 10.1103/PhysRevC.34.1127
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1986GU11      Phys.Lett. 176B, 1 (1986)

M.W.Guidry, C.-L.Wu, D.H.Feng, J.N.Ginocchio, X.-G.Chen, J.-Q.Chen

A Fermion Dynamical Symmetry Model for High-Spin Physics

NUCLEAR STRUCTURE 232Th; calculated levels, E2 matrix elements. 160Yb; calculated levels, alignment. Interacting boson model, dynamical symmetry.

doi: 10.1016/0370-2693(86)90913-5
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1986WE12      Nucl.Phys. A459, 631 (1986)

G.Wenes, J.N.Ginocchio, A.E.L.Dieperink, B.van der Cammen

Algebraic Treatment of Multistep Exciation Processes in Collective Nuclei. (III). Medium Energy Proton Scattering

NUCLEAR REACTIONS 154Sm(p, p'), E=800 MeV; calculated σ(θ). Glauber theory, collective state excitation, channel coupling.

doi: 10.1016/0375-9474(86)90165-X
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1985GI03      Ann.Phys.(New York) 159, 467 (1985)


A Class of Exactly Solvable Potentials II. The Three-Dimensional Schrodinger Equation

NUCLEAR STRUCTURE 208Pb; calculated charge density. Three-dimensional Schrodinger equation, effective mass.

doi: 10.1016/0003-4916(85)90120-4
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1985OT01      Phys.Rev.Lett. 54, 777 (1985)

T.Otsuka, J.N.Ginocchio

Low-Lying Isovector Collective States and the Interacting-Boson Model

NUCLEAR STRUCTURE 148,150,152,154Sm; calculated levels, β(E2), F-boson charges, proton-neutron matrix element ratio.

doi: 10.1103/PhysRevLett.54.777
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1985OT03      Phys.Rev.Lett. 55, 276 (1985)

T.Otsuka, J.N.Ginocchio

Renormalization of g-Boson Effects in the Interacting-Boson Hamiltonian

NUCLEAR STRUCTURE 158Gd; calculated levels; deduced g-boson renormalization effects. Interacting boson model.

doi: 10.1103/PhysRevLett.55.276
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1984GI12      Nucl.Phys. A421, 369c (1984)


Medium Energy Probes and Nuclear Structure

NUCLEAR REACTIONS 154Sm(p, p'), E=800 MeV; analyzed σ(θ). Multiple scattering theory, summing to all orders.

doi: 10.1016/0375-9474(84)90354-3
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1980GI01      Phys.Rev. C21, 1056 (1980)

J.N.Ginocchio, M.B.Johnson

Effect of the Pion and Δ Optical Potential on Deep Inelastic Pion-Nuclear Reactions

NUCLEAR REACTIONS 1H(p, π+n), (p, π0p), (p, π+), E=300-1200 MeV; calculated production σ. 12C(π-, X), (π+, X), E=50-250 MeV; calculated total reaction σ, absorption σ. 62Ni(π+, X), E=220 MeV; calculated spallation σ. Semiclassical transport model, pion, isobar optical potentials.

doi: 10.1103/PhysRevC.21.1056
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1980GI08      Nucl.Phys. A350, 31 (1980)

J.N.Ginocchio, M.W.Kirson

An Intrinsic State for the Interacting Boson Model and Its Relationship to the Bohr-Mottelson Model

NUCLEAR STRUCTURE 148,150,152,154Sm, 186,188,190,192,194,196Pt, 112,124,134,136Ce; calculated energy surfaces vs shape variables, intrinsic state orientation; deduced relation to Bohr-Mottelson model. Interacting boson approximation.

doi: 10.1016/0375-9474(80)90387-5
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1980OR02      Phys.Rev. C21, 2524 (1980)

C.J.Orth, W.R.Daniels, B.J.Dropesky, R.A.Williams, G.C.Giesler, J.N.Ginocchio

Products of Stopped-Pion Interactions with Cu and Ta

NUCLEAR REACTIONS Cu, Ta(π-, X), E at rest; measured cumulative yields for 55,56,57,61Co, 52,59Fe, 48,49,51Cr, 48V, 43K, 41Ar, 24Na, 169Lu, 166,169Yb, 165,167Tm, independent yields for 56,57Ni, 58,60Co, 52,54Mn, 44,46,47,48Sc, 170,171,172,173,175,177,179Hf, 167,170,171,172,173,174,176,177,178,179Lu, 175,177Yb, 166,168,170,172,173Tm, 169,171Er. Three-step model calculations.

doi: 10.1103/PhysRevC.21.2524
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1978GI01      Phys.Rev. C17, 195, (1978)


Deep Inelastic Pion-Induced Nuclear Reactions in the Isobar Model

NUCLEAR REACTIONS 27Al(π+, p), (π-, p), E=100 MeV; 62Ni(π+, p), (π-, p), E=220 MeV; calculated σ. Cu(π+, X), (π-, X), E=100, 190 MeV; 62Ni(π+, X), (π-, X), E=220 MeV; calculated σ(A).

doi: 10.1103/PhysRevC.17.195
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1977AM01      Phys.Rev.Lett. 38, 1055 (1977)

A.A.Amsden, J.N.Ginocchio, F.H.Harlow, J.R.Nix, M.Danos, E.C.Halbert, R.K.Smith, Jr.

Comparison of Macroscopic and Microscopic Calculations of High-Energy 20Ne + 238U Collisions

NUCLEAR REACTIONS 238U(20Ne, X), E=250 MeV/nucleon; calculated σ(θ) for outgoing protons.

doi: 10.1103/PhysRevLett.38.1055
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1977SI01      Phys.Rev. C15, 371 (1977)

R.R.Silbar, J.N.Ginocchio, M.M.Sternheim

Dramatic Nuclear Structure Effects in (π, πN) Reactions

NUCLEAR REACTIONS 11B, 12C, 16,17,18O, 19F, 31P, 58,60,62,64Ni, 64,66,68,70Zn(π, X), E ≈ 190 MeV; calculated pion induced nucleon knockout σ.

doi: 10.1103/PhysRevC.15.371
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1975GI03      Nucl.Phys. A239, 365 (1975)

J.N.Ginocchio, M.M.Yen

The Dependence of Shell Model State Densities on Angular Momentum

NUCLEAR STRUCTURE 20Ne, 21F, 62Ni, 62,63,64Cu, 68Zn calculated angular momentum, level densities.

doi: 10.1016/0375-9474(75)90373-5
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1974AY02      Nucl.Phys. A234, 13 (1974)

S.Ayik, J.N.Ginocchio

Shell Model Level Densities for Light Nuclei

NUCLEAR STRUCTURE 23Na, 23Mg, 26Al, 28Si; calculated yrast lines. 23Na, 23Mg, 27Al, 27,29Si, 29P; calculated levels.

doi: 10.1016/0375-9474(74)90376-5
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1973GI09      Phys.Rev.Lett. 31, 1260 (1973)


Angular-Momentum Dependence of the Density of States

NUCLEAR STRUCTURE 20Ne, 62Ni; calculated levels, level-width.

doi: 10.1103/PhysRevLett.31.1260
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1972VA13      Nucl.Phys. A185, 349 (1972)

J.Vary, R.J.Ascuitto, J.N.Ginocchio

Approximate Treatment of Correlations in Nuclear Spectroscopy (II). Two-Nucleon Transfer in the Lead Region

NUCLEAR REACTIONS 208Pb(p, t), E=20 MeV; 208Pb(t, p), E=20 MeV; 208Pb(3He, n), E=30 MeV; calculated σ(θ); analyzed ground-state correlation effects.

doi: 10.1016/0375-9474(72)90018-8
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1971VA13      Nucl.Phys. A166, 479 (1971)

J.Vary, J.N.Ginocchio

Approximate Treatment of Correlations in Nuclear Spectroscopy (I). Structure of the Lead Isotopes

NUCLEAR STRUCTURE 206,210Pb; calculated levels, S, B(λ). 2N RPA.

doi: 10.1016/0375-9474(71)90902-X
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1966GI01      Phys.Rev. 144, 952 (1966)


f7/2 Model of V46,47, Cr49, and Mn50

NUCLEAR STRUCTURE 49Cr, 47V, 46V, 50Mn; measured not abstracted; deduced nuclear properties.

doi: 10.1103/PhysRev.144.952
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