Nuclear Science References (NSR)

NUCLEAR STRUCTURE ²⁸Si, ⁴⁸Cr, ⁶⁸Se, ⁷⁶Sr; calculated isospin mixing parameters in the ground states. Particle-number conserving highly truncated diagonalization approach (HTDA) and Skyrme SIII effective interaction.

doi: 10.1103/PhysRevC.86.034332
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2012WA37 Eur.Phys.J. A 48, 168 (2012)

D.J.Wang, L.P.Csernai, D.Strottman, Cs.Anderlik, Y.Cheng, D.M.Zhou, Y.L.Yan, X.Cai, B.H.Sa

QGP flow fluctuations and the characteristics of higher moments

doi: 10.1140/epja/i2012-12168-4
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2011CS03 Phys.Rev. C 84, 024914 (2011)

L.P.Csernai, V.K.Magas, H.Stocker, D.D.Strottman

Fluid dynamical prediction of changed ν₁ flow at energies available at the CERN Large Hadron Collider

doi: 10.1103/PhysRevC.84.024914
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2010CH23 Phys.Rev. C 81, 064910 (2010)

Y.Cheng, L.P.Csernai, V.K.Magas, B.R.Schlei, D.Strottman

Matching stages of heavy-ion collision models

doi: 10.1103/PhysRevC.81.064910
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2010CS01 Nucl.Phys. A834, 261c (2010)

L.P.Csernai, Y.Cheng, V.K.Magas, I.N.Mishustin, D.Strottman

Collective Flow in Ultra-relativistic Collisions

doi: 10.1016/j.nuclphysa.2009.12.054
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2010LE06 Int.J.Mod.Phys. E19, 568 (2010)

J.Le Bloas, L.Bonneau, P.Quentin, J.Bartel, D.Strottman

Effects of vibrational and pairing correlations on isospin mixing in the Higher Tamm-Dancoff Approximation

doi: 10.1142/S0218301310014984
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2009BO22 Int.J.Mod.Phys. E18, 951 (2009)

L.Bonneau, J.Le Bloas, P.Quentin, J.Bartel, D.Strottman

Isospin mixing in the higher Tamm-Dancoff approximation

NUCLEAR STRUCTURE ¹⁶O, ⁴⁰Ca, ⁵⁶Ni, ¹⁰⁰Sn; calculated mass excess; ¹⁰⁰Sn; calculated isospin mixing.

doi: 10.1142/S0218301309013099
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2007BA81 J.Phys.(London) G34, S1077 (2007)

B.Bauchle, Y.Cheng, L.P.Csernai, V.K.Magas, D.D.Strottman, P.Van, M.Zetenyi

Fluid dynamics as a diagnostic tool for heavy-ion collisions

doi: 10.1088/0954-3899/34/8/S160
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2006DO08 Phys.Rev. C 73, 045209 (2006)

M.Doring, E.Oset, D.Strottman

Chiral dynamics in the γp → π⁰ηp and γp → π⁰K⁰Σ⁺ reactions

NUCLEAR REACTIONS ¹H(γ, π⁰X), E ≈ 1000-1700 MeV; calculated σ, invariant mass spectra for various channels; deduced resonance contributions. Chiral unitary approach.

doi: 10.1103/PhysRevC.73.045209
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2006DO16 Phys.Lett. B 639, 59 (2006)

M.Doring, E.Oset, D.Strottman

Clues to the nature of the Δ^*(1700) resonance from pion- and photon-induced reactions

NUCLEAR REACTIONS ¹H(π^-, π⁰X), (π⁺, π⁺X), (π⁺, K⁺X), E(cm)=1.75-2.1 GeV; calculated total reaction σ, invariant mass spectra. ¹H(γ, π⁺X), (γ, π⁰X), (γ, π^-X), E=1.0-2.0 GeV; calculated strange and η particle production σ.Chiral unity approach, comparison with data.

doi: 10.1016/j.physletb.2006.06.022
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2006DO18 Acta Phys.Slovaca 56, 221 (2006)

M.Doring, E.Oset, D.Strottman

Chiral dynamics in γp → π⁰ηp and related reactions

NUCLEAR REACTIONS ¹H(γ, π⁰X), E=1000-1700 MeV; calculated η-meson and hyperon production invariant mass spectra, σ. Chiral unitary approach.

2005CA46 Comput.Phys.Commun. 173, 41 (2005)

N.Carjan, M.Rizea, D.Strottman

Improved boundary conditions for the decay of low lying metastable proton states in a time-dependent approach

RADIOACTIVITY ^109mIn, ^147mTm, ^166mIr, ^171mAu(p); calculated T_1/2 for proton emission from excited states. Time-dependent Schrodinger equation, improved boundary conditions, comparison with data.

doi: 10.1016/j.cpc.2005.07.005
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2005VE05 Int.J.Mod.Phys. E14, 751 (2005)

J.D.Vergados, P.Quentin, D.Strottman

Direct detection of supersymmetric dark matter: theoretical rates for transitions to excited states

NUCLEAR STRUCTURE ¹²⁷I; calculated matrix elements, transition rate for interaction with light supersymmetric particle.

doi: 10.1142/S0218301305003508
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2002MA63 Nucl.Phys. A712, 167 (2002)

V.K.Magas, L.P.Csernai, D.Strottman

Effective string rope model for the initial stages of ultra-relativistic heavy ion collisions

doi: 10.1016/S0375-9474(02)01073-4
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2001MA54 Phys.Rev. C64, 014901 (2001)

V.K.Magas, L.P.Csernai, D.D.Strottman

Initial State of Ultrarelativistic Heavy Ion Collisions

doi: 10.1103/PhysRevC.64.014901
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2000ST22 Phys.Scr. T88, 148 (2000)

D.Strottman, N.Carjan, P.Talou

New Aspects in the Decay of Quasi-Stationary Proton States by Mutidimensional Tunneling

doi: 10.1238/Physica.Topical.088a00148
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2000TA23 Phys.Rev. C62, 014609 (2000)

P.Talou, N.Carjan, C.Negrevergne, D.Strottman

Exact Dynamical Approach to Spherical Ground-State Proton Emitters

RADIOACTIVITY ¹⁰⁵Sb, ¹¹³Cs, ¹⁴⁷Tm, ¹⁵¹Lu, ¹⁵⁷Ta, ¹⁸⁵Bi(p); calculated T_1/2. Time-dependent Schroedinger equation, comparison with data.

doi: 10.1103/PhysRevC.62.014609
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1999SC01 Phys.Rev. C59, R9 (1999)

B.R.Schlei, D.Strottman

Predictions for √ s = 200A GeV Au + Au Collisions from Relativistic Hydrodynamics

NUCLEAR REACTIONS ¹⁹⁷Au(¹⁹⁷Au, X), E(cm)=200 GeV/nucleon; calculated pions, kaons, protons yields, rapidity, transverse momentum spectra. Relativistic hydrodynamical model.

doi: 10.1103/PhysRevC.59.R9
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1999SC42 Eur.Phys.J. C 10, 483 (1999)

B.R.Schlei, D.Strottman, J.P.Sullivan, H.W.van Hecke

Bose-Einstein Correlations and the Equation of State of Nuclear Matter

NUCLEAR REACTIONS Pb(Pb, X), E=158 GeV/nucleon; analyzed Bose-Einstein correlations for pion pairs; deduced sensitivity to equation of state.

doi: 10.1007/s100520050771
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1999TA06 Nucl.Phys. A647, 21 (1999)

P.Talou, N.Carjan, D.Strottman

Time-Dependent Approach to Bidimensional Quantum Tunneling: Application to the proton emission from deformed nuclei

NUCLEAR STRUCTURE ²⁰⁸Pb; calculated decay rates, tunneling probability for proton emission from deformed, excited states. Time-dependent two-dimensional Schrodinger equation.

doi: 10.1016/S0375-9474(99)00005-6
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1999TA30 Phys.Rev. C60, 054318 (1999)

P.Talou, D.Strottman, N.Carjan

Exact Calculation of Proton Decay Rates from Excited States in Spherical Nuclei

RADIOACTIVITY ¹⁰⁹I(p); calculated proton decay rates, T_1/2 vs level energy. One-dimensional time-dependent Schrodinger equation.

doi: 10.1103/PhysRevC.60.054318
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1998ME24 Phys.Rev. C58, 3627 (1998)

A.Z.Mekjian, B.R.Schlei, D.Strottman

Various Models for Pion Probability Distributions from Heavy-Ion Collision

doi: 10.1103/PhysRevC.58.3627
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1998SC10 Phys.Rev.Lett. 80, 3467 (1998)

B.R.Schlei, D.Strottman, N.Xu

Equation of State of Nuclear Matter in 158A GeV Pb + Pb Collisions

NUCLEAR REACTIONS Pb(Pb, X), E=158; calculated energy density, rapidity, transverse mass spectra. Comparison with data. Three equations of state compared.

doi: 10.1103/PhysRevLett.80.3467
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1998SC16 Phys.Lett. 420B, 1 (1998)

B.R.Schlei, D.Strottman, N.Xu

The Linear Correlation Coefficient vs. the Cross Term in Bose-Einstein Correlations

NUCLEAR REACTIONS S(S, X), Pb(Pb, X), E=high; calculated meson pairs rapidity spectra, linear correlation coefficients; deduced features of Bose-Einstein correlations in chaotic hadron sources.

doi: 10.1016/S0370-2693(97)01523-2
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1998TA25 Phys.Rev. C58, 3280 (1998)

P.Talou, N.Carjan, D.Strottman

Time-Dependent Properties of Proton Decay from Crossing Single-Particle Metastable States in Deformed Nuclei

doi: 10.1103/PhysRevC.58.3280
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1997OR06 Phys.Rev. C56, 412 (1997)

U.Ornik, M.Plumer, B.R.Schlei, D.Strottman, R.M.Weiner

Effects of Bose Condensates on Single Inclusive Spectra and Bose-Einstein Correlations

doi: 10.1103/PhysRevC.56.412
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1996OR05 Phys.Rev. C54, 1381 (1996)

U.Ornik, M.Plumer, B.R.Schlei, D.Strottman, R.M.Weiner

Hydrodynamical Analysis of Symmetric Nucleus-Nucleus Collisions Near 200A GeV

NUCLEAR REACTIONS S(S, X), E=200 GeV/nucleon; Pb(Pb, X), E=160 GeV/nucleon; analyzed data; deduced quark-gluon plasma volume, life-time. Hydrodynamical analysis.

doi: 10.1103/PhysRevC.54.1381
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1996SC12 Phys.Lett. 376B, 212 (1996)

B.R.Schlei, U.Ornik, M.Plumer, D.Strottman, R.M.Weiner

Hydrodynamical Analysis of Single Inclusive Spectra and Bose-Einstein Correlations for Pb + Pb at 160 AGeV

NUCLEAR REACTIONS Pb(Pb, X), E=160 GeV/nucleon; analyzed data; deduced quark-gluon plasma T_1/2. Relativistic hydrodynamics.

doi: 10.1016/0370-2693(96)00202-X
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1994BR24 Phys.Rev. C50, 2161 (1994)

L.Bravina, L.P.Csernai, P.Levai, D.Strottman

Collective Global Dynamics in Au + Au Collisions at the BNL AGS

NUCLEAR REACTIONS ¹⁹⁷Au(¹⁹⁷Au, X), E=11.6 GeV/nucleon; calculated protons transverse flow, collective effects signatures. Quark gluon string model.

doi: 10.1103/PhysRevC.50.2161
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1994CA36 Z.Phys. A349, 353 (1994)

N.Carjan, O.Serot, D.Strottman

Time-Dependent Schrodinger Approach to Sub-Barrier Fission

NUCLEAR STRUCTURE ²¹³At; calculated fission rates at saddle, scission points. Time-dependent Schrodinger approach.

doi: 10.1007/BF01288994
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1994SE02 Nucl.Phys. A569, 562 (1994)

O.Serot, N.Carjan, D.Strottman

Transient Behaviour in Quantum Tunneling: Time-dependent approach to alpha decay

doi: 10.1016/0375-9474(94)90319-0
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1993OS01 Phys.Rev.Lett. 70, 146 (1993)

E.Oset, D.Strottman

High-Energy Pion-Induced Double Charge Exchange and Isovector Renormalization

NUCLEAR REACTIONS ¹⁴C, ¹⁸O(π⁺, π^-), E=300-525 MeV; analyzed σ(θ); deduced unconventional mechanisms role.

doi: 10.1103/PhysRevLett.70.146
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1993OS07 Phys.Rev. C48, 2395 (1993)

E.Oset, D.Strottman, H.Toki, J.Navarro

Core Polarization Phenomena in Pion-Nucleus Charge-Exchange Reactions Above the Delta Resonance

NUCLEAR REACTIONS ¹⁴C(π⁺, π⁰), E=250-650 MeV; calculated σ(θ)=0°. ¹⁴C, ⁴²Ca, ¹⁸O(π⁺, π^-), E=400 MeV; calculated σ(θ). Microscopic, parameter free Glauber approach.

doi: 10.1103/PhysRevC.48.2395
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1992MA46 Chin.J.Nucl.Phys. 14, No 3, 197 (1992)

W.Ma, D.Strottman, Q.Wu, L.S.Kisslinger, S.Wang

A Good Place for Dibaryon to Manifest Itself

NUCLEAR REACTIONS ¹⁸O(π⁺, π^-), E=164 MeV; calculated σ(θ); deduced dibaryon state role.

1992MI01 Phys.Rev. C45, 473 (1992)

D.J.Millener, A.C.Hayes, D.Strottman

Comment on ' p-Shell Nuclei in a (0+2)(h-bar x Omega) Model Space. I. Method ' and on ' p-Shell nuclei in a (0+2)(h-bar x Omega) Model Space. II. Results '

NUCLEAR STRUCTURE ¹⁶O; analyzed other model calculation results; deduced effective interaction inconsistencies.

doi: 10.1103/PhysRevC.45.473
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1992OS01 Phys.Rev. C45, 662 (1992)

E.Osnes, D.Strottman

Spin-Tensor Analysis of Realistic Shell Model Interactions

NUCLEAR STRUCTURE ¹⁸O; calculated levels. Realistic shell model interactions, spin-tensor analysis.

doi: 10.1103/PhysRevC.45.662
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1992SI14 J.Phys.(London) G18, 1377 (1992)

J.Sinatkas, L.D.Skouras, D.Strottman, J.D.Vergados

Shell-Model Calculations in the A = 80-100 Mass Region: I. A study of the N = 50 nuclei

NUCLEAR STRUCTURE ⁹⁴Ru, ⁹²Mo, ⁹⁰Zr, ⁸⁸Sr, ⁸⁶Kr, ⁸⁴Se, ⁹³Tc, ⁹¹Nb, ⁸⁹Y, ⁸⁷Rb, ⁹⁵Rh; calculated levels, B(λ). ⁹⁶Pd; calculated levels. Shell model.

doi: 10.1088/0954-3899/18/8/012
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1992SI15 J.Phys.(London) G18, 1401 (1992)

J.Sinatkas, L.D.Skouras, D.Strottman, J.D.Vergados

Shell-Model Calculations in the A = 80-100 Mass Region: II. A study of the N = 49, 48 nuclei

NUCLEAR STRUCTURE ⁹¹Mo, ⁸⁹Zr, ⁹³Ru, ⁸⁷Sr, ⁹⁰Nb, ⁸⁸Y, ⁹²Ru, ⁹⁰Mo, ⁸⁸Zr, ⁸⁶Sr, ⁹¹Tc, ⁸⁹Nb; calculated levels, B(λ). ⁸⁷Y; caluclated levels. Shell model.

doi: 10.1088/0954-3899/18/8/013
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1991GA07 Nucl.Phys. A526, 685 (1991)

C.Garcia-Recio, E.Oset, L.L.Salcedo, D.Strottman, M.J.Lopez

Pion-Nucleus Elastic Scattering in a Local Approximation to the Delta-Hole Model

NUCLEAR REACTIONS ¹⁶O(π⁺, π⁺), E=163 MeV; ⁴⁰Ca(π⁺, π⁺), (π^-, π^-), E=116-292 MeV; ²⁰⁸Pb(π⁺, π⁺), (π^-, π^-), E=162 MeV; calculated σ(θ). Isobar-hole model.

doi: 10.1016/0375-9474(91)90438-C
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1991MA25 Phys.Rev. C44, 615 (1991)

W.-H.Ma, D.Strottman

Antiproton-Induced Elastic and Inelastic Scattering at Intermediate Energies

NUCLEAR REACTIONS ¹²C, ¹⁶O, ⁴⁰Ca(p-bar, p-bar), (p-bar, p-bar'), E=0.232-1.83 GeV; calculated σ(θ). Glauber model, microscopic shell model wave functions.

doi: 10.1103/PhysRevC.44.615
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1991OS01 Phys.Rev. C44, 468 (1991)

E.Oset, D.Strottman

Pion-Induced Elastic and Inelastic Scattering Above the 3, 3 Resonance

NUCLEAR REACTIONS ¹²C, ¹⁸O, ^40,48Ca(π⁺, π⁺), (π⁺, π⁺'), E=0.2-1.4 GeV; calculated σ(θ). Glauber model.

doi: 10.1103/PhysRevC.44.468
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1990HA10 Phys.Rev. C41, 1727 (1990)

A.C.Hayes, J.L.Friar, D.Strottman

Two-Photon Decay of the First Excited 0⁺ State in ¹⁶O

NUCLEAR STRUCTURE ¹⁶O; calculated 2γ decay rate, matrix elements, GDR resonances, B(λ). Shell model, large SU(3) basis.

doi: 10.1103/PhysRevC.41.1727
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1990HA33 Phys.Rev. C42, 2248 (1990)

A.C.Hayes, D.Strottman

Soft Giant Dipole Mode of ¹¹Li

NUCLEAR STRUCTURE ¹¹Li; calculated B(E1), transition strength distribution, Coulomb excitation σ.

doi: 10.1103/PhysRevC.42.2248
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1990OS01 Phys.Rev. C42, 2454 (1990)

E.Oset, D.Strottman

Pion-Nucleus Single-Charge Exchange above the Resonance

NUCLEAR REACTIONS ⁷Li, ¹⁴C(π⁺, π⁰), E=250-650 MeV; analyzed σ(θ) vs E; deduced two-, three-body pion absorption role. Glauber model.

doi: 10.1103/PhysRevC.42.2454
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1988OS02 Nucl.Phys. A483, 514 (1988)

E.Oset, M.J.Vicente-Vacas, M.B.Johnson, D.Strottman, H.T.Fortune, R.Gilman

The Δ Interaction Contribution to Double Charge Exchange

NUCLEAR REACTIONS ¹⁸O(π⁺, π^-), E=130-230 MeV; calculated σ(θ); deduced isobar interaction contribution.

doi: 10.1016/0375-9474(88)90082-6
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1986OS06 Phys.Rev. C34, 2349 (1986)

E.Oset, D.Strottman, M.J.Vicente Vacas, Ma Wei-hsing

Comment on ' Comparison of Approximate Chiral-Dynamical πN → ππN Models used in A(π, 2π) Calculations '

NUCLEAR REACTIONS ¹⁸O(π⁺, π^-), E not given; calculated forward σ(θ); deduced vanishing contact term.

doi: 10.1103/PhysRevC.34.2349
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1985OS08 Phys.Lett. 165B, 13 (1985)

E.Oset, L.L.Salcedo, D.Strottman

A Theoretical Approach to Pion Nuclear Reactions in the Resonance Region

NUCLEAR REACTIONS ⁹³Nb(π⁺, π⁺), (π⁺, π⁺'), (π⁺, X), (π⁺, π^-), E=85-315 MeV; calculated σ(E). ¹²C, ²⁷Al, ⁵⁶Fe, ⁹³Nb, ²⁰⁸Bi(π⁺, π⁺), (π⁺, π⁺'), (π⁺, X), (π⁺, π^-), E=165 MeV; calculated σ. Microscopic isobar-hole model.

doi: 10.1016/0370-2693(85)90681-1
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1985WU05 Phys.Lett. 162B, 227 (1985)

H.F.Wu, H.Q.Song, T.T.S.Kuo, W.K.Cheng, D.Strottman

Majorana Neutrino and Lepton-Number Non-Conservation in ⁴⁸Ca Nuclear Double Beta Decay

RADIOACTIVITY ⁴⁸Ca(2β); calculated neutrinoless decay T_1/2. Short-range correlations, finite size nucleon effects.

doi: 10.1016/0370-2693(85)90911-6
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1983OS09 Nucl.Phys. A408, 461 (1983)

E.Oset, D.Strottman, M.J.Vicente-Vacas, W.-H.Ma

Meson-exchange currents in pion-nucleus double-charge-exchange reactions

NUCLEAR REACTIONS ¹⁸O(π⁺, π^-), E<250 MeV; analyzed available data; deduced σ(θ), at large angles the meson-exchange contribution changes the σ appreciably and can become the dominant mechanism.

doi: 10.1016/0375-9474(83)90240-3
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1983SH32 Nucl.Phys. A408, 310 (1983)

J.Shurpin, T.T.S.Kuo, D.Strottman

Folded Diagrams and 1s-0d Effective Interactions Derived from Reid and Paris Nucleon-Nucleon Potentials

NUCLEAR STRUCTURE ^18,20O, ^18,19F, ^20,22Ne, ²²Na, ²⁴Mg; calculated levels. Folded diagrams, Reid, Paris potential based effective interactions.

doi: 10.1016/0375-9474(83)90586-9
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1982OS01 Nucl.Phys. A377, 297 (1982)

E.Oset, D.Strottman

Elastic and Inelastic Pion Scattering and Nuclear Structure

NUCLEAR REACTIONS ¹²C, ⁷Li(π⁺, π⁺), (π⁺, π⁺'), E=160 MeV; ²⁴Mg(π⁺, π⁺), E=180 MeV; ²⁰Ne, ¹⁵N(π⁺, π⁺'), (π^-, π^-'), E=160 MeV; calculated σ(θ); deduced structure effects. Glauber theory, shell model wave functions.

doi: 10.1016/0375-9474(82)90043-4
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1981GA24 Phys.Lett. 106B, 6 (1981)

M.Gai, A.Arima, D.Strottman

Generalized Seniority Scheme for the Systematics of Single-Particle States

NUCLEAR STRUCTURE ^{117,119,121,123,125,127}Cs, ^{115,117,119,121,123,125,127,129}Sb; calculated hole, particle state energy difference. ^{109,111,113,115}In, ^115,117,119Sb, ¹¹⁹I, ^129,131Cs; calculated stretched spin state μ deviation from Schmidt limit. Generalized seniority scheme.

doi: 10.1016/0370-2693(81)91068-6
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1981HA21 Phys.Rev.Lett. 47, 153 (1981)

W.C.Haxton, G.J.Stephenson, Jr., D.Strottman

Double Beta Decay and the Majorana Mass of the Electron Neutrino

RADIOACTIVITY ⁷⁶Ge, ⁸²Se; calculated double β-decay T_1/2; deduced ν(e) Majorana mass constraint. Two-neutrino, neutrinoless decay mechanisms.

doi: 10.1103/PhysRevLett.47.153
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1981KA08 Phys.Rev. C23, 1282 (1981)

J.I.Kapusta, D.Strottman

Entropy Generation and Hydrodynamic Flow in Relativistic Heavy Ion Collisions

NUCLEAR REACTIONS K, Cl(Ar, π⁺), (Ar, π^-), (Ar, π⁰), (Ar, p), (Ar, d), (Ar, t), E=800 MeV/nucleon; calculated particle spectra, entropy per nucleon vs time. Hydrodynamic model, equation of state.

doi: 10.1103/PhysRevC.23.1282
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1981OS04 Nucl.Phys. A355, 437 (1981)

E.Oset, D.Strottman

Pion-Induced Single Charge Exchange and Nuclear Structure

NUCLEAR REACTIONS ⁷Li, ¹³C, ¹⁵N, ^16,17O, ³⁹K(π⁺, π⁰), ¹³C, ¹⁵N, ¹⁷O(π^-, π⁰), E=130-250 MeV; calculated total σ(E), σ(θ); deduced importance of Δ-isobar property renormalizations. Glauber theory, shell model configurations, Woods-Saxon single particle functions.

doi: 10.1016/0375-9474(81)90536-4
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1981ST26 Phys.Rev.Lett. 47, 1807 (1981)

H.Stocker, C.Riedel, Y.Yariv, L.P.Csernai, G.Buchwald, G.Graebner, J.A.Maruhn, W.Greiner, K.Frankel, M.Gyulassy, B.Schurmann, G.Westfall, J.D.Stevenson, J.R.Nix, D.Strottman

Nuclear Fluid Dynamics Versus Intranuclear Cascade- Possible Evidence for Collective Flow in Central High-Energy Nuclear Collisions

NUCLEAR REACTIONS ²³⁸U(²⁰Ne, p), E=393 MeV/nucleon; calculated σ(θ, Ep); deduced collective flow effects. Different collision models.

doi: 10.1103/PhysRevLett.47.1807
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1980AR12 Phys.Lett. B96, 23 (1980)

A.Arima, D.Strottman

Magnetic Dipole Strength in ¹⁶O

NUCLEAR STRUCTURE ¹⁶O; calculated M1 transition strength fragmentation. Shell model.

doi: 10.1016/0370-2693(80)90203-8
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1979FA12 Nucl.Phys. A330, 333 (1979)

A.Faessler, D.J.Millener, P.Paul, D.Strottman

Alpha and Proton Decay of the Isoscalar E2 Resonance in ¹⁶O and ⁴⁰Ca

NUCLEAR STRUCTURE ¹⁶O, ⁴⁰Ca; calculated Γα/Γp for T=0, GQR. SU(3) framework, 1p-1h excitations.

doi: 10.1016/0375-9474(79)90058-7
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1979OS05 Phys.Lett. 84B, 396 (1979)

E.Oset, D.Strottman

Core Polarisation Effects in Inelastic Pion-Nucleus Scattering

NUCLEAR REACTIONS ¹⁸O(π⁺, π⁺), (π^-, π^-'), E=160, 230 MeV; calculated σ(θ). Glauber theory, core polarization introduced as a renormalization constant.

doi: 10.1016/0370-2693(79)91224-3
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1979ST11 Phys.Rev. C20, 1150 (1979)

D.Strottman

Weak Coupling Calculation of ²¹²Po Using Realistic Matrix Elements

NUCLEAR STRUCTURE ²¹²Po; calculated levels, J, π. Weak coupling model, realistic interaction.

doi: 10.1103/PhysRevC.20.1150
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1978AN15 Nucl.Phys. A306, 201 (1978)

N.Anyas-Weiss, D.Strottman

Influence of Non-Central Interactions on 1s-0d Nuclei

NUCLEAR STRUCTURE ^21,19F, ^20,21,22Ne, ²²Na; calculated levels, noncentral interactions.

doi: 10.1016/0375-9474(78)90323-8
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1978GR02 Nucl.Phys. A295, 319 (1978)

H.D.Graf, H.Feldmeier, P.Manakos, A.Richter, E.Spamer, D.Strottman

Study of Electic Monopole Transitions between the Ground State and the First Excited 0⁺ State in ^40,42,44,48Ca with High Resolution Inelastic Electron Scattering

NUCLEAR REACTIONS ^40,42,44,48Ca(e, e'), E=31-67 MeV; measured σ(E;Ee';θ). ^40,42,44,48Ca 0+ level deduced E0 matrix elements. Shell model calculation.

doi: 10.1016/0375-9474(78)90120-3
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1978OS02 Phys.Lett. 73B, 393 (1978)

E.Oset, D.Strottman, G.E.Brown

Nuclear Structure Effects in Pion Double Charge Exchange

NUCLEAR REACTIONS ¹⁸O(π⁺, π^-), E=187 MeV; calculated σ(θ).

doi: 10.1016/0370-2693(78)90748-7
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1977GR01 Nucl.Phys. A276, 130 (1977)

L.R.Grisham, D.Strottman

Alpha Strength Factors in Medium Nuclei

NUCLEAR STRUCTURE ⁵⁸Ni; calculated α-strengths.

doi: 10.1016/0375-9474(77)90163-4
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1977SH11 Phys.Lett. 69B, 395 (1977)

J.Shurpin, D.Strottman, T.T.S.Kuo, M.Conze, P.Manakos

Folded Diagrams and s-d Shell Effective Interactions

NUCLEAR STRUCTURE ¹⁸O, ^18,19F; calculated levels.

doi: 10.1016/0370-2693(77)90828-0
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1977ST08 Nucl.Phys. A279, 45 (1977)

D.Strottman

Validity of Pseudo SU(3) for Rare Earth Nuclei

NUCLEAR STRUCTURE ¹⁴³Pr; calculated levels. Pseudo SU(3) calculations.

doi: 10.1016/0375-9474(77)90419-5
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1976CO17 Phys.Lett. 62B, 131 (1976)

P.J.Cooney, D.Geesaman, D.Strottman

The Fragmentation of d-State Antianalogue Single Particle Strength in Odd A Nb Isotopes

NUCLEAR STRUCTURE ^90,92,94,96Zr, ⁹¹Nb; calculated single-particle strength.

doi: 10.1016/0370-2693(76)90485-8
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1976EN01 Phys.Lett. 60B, 321 (1976)

T.Engeland, E.Osnes, D.Strottman

Nuclear Structure Aspects of the g-Factor of the 3.83 MeV (15/2+) Level in ⁴¹Ca

NUCLEAR STRUCTURE ⁴¹Ca level; calculated g.

doi: 10.1016/0370-2693(76)90739-5
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1976NA22 Phys.Rev. C14, 2133 (1976)

K.Nagatani, C.W.Towsley, K.G.Nair, R.Hanus, M.Hamm, D.Strottman

Alpha Transfer Reaction ¹⁶O(¹⁴N, ¹⁰B)²⁰Ne and High-Spin States in ²⁰Ne

NUCLEAR REACTIONS ¹⁶O(¹⁴N, ¹⁰B), E=155 MeV; measured σ; deduced α-transfer mechanism. ²⁰Ne deduced levels, K.

doi: 10.1103/PhysRevC.14.2133
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1975AR30 Phys.Lett. 60B, 1 (1975)

A.Arima, P.Manakos, D.Strottman

The Isospin Forbidden 1^- → 0⁺ Transition in ¹⁶O

NUCLEAR STRUCTURE ¹⁶O; calculated Coulomb form factor. 1p-1h model.

doi: 10.1016/0370-2693(75)90512-2
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1975YO05 Phys.Rev. C12, 1358 (1975)

L.E.Young, G.D.Sprouse, D.Strottman

g Factor of the 3.830 MeV (15/2⁺) Level in ⁴¹Ca

NUCLEAR REACTIONS ²⁷Al(¹⁶O, pnγ), E=48 MeV; measured γ(θ, H, t). ⁴¹Ca level deduced g.

doi: 10.1103/PhysRevC.12.1358
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1974AN36 Phys.Rep. 12, 201 (1974)

N.Anyas-Weiss, J.C.Cornell, P.S.Fisher, P.N.Hudson, A.Menchaca-Rocha, D.J.Millener, A.D.Panagiotou, D.K.Scott, D.Strottman, D.M.Brink, B.Buck, P.J.Ellis, T.Engeland

Nuclear structure of light nuclei using the selectivity of high energy transfer reactions with heavy ions

NUCLEAR REACTIONS ¹²C, ¹⁶O, ⁴⁰Ca(¹²C, ¹¹B), (¹²C, ¹¹C), (¹²C, ¹⁰B), (¹²C, ¹⁰Be), (¹²C, ¹⁰C), (¹²C, ⁹Be), E=114 MeV; ^12,13C(¹¹B, ⁹Li), E=114 MeV; ¹³C(¹¹B, ¹⁰B), E=114 MeV; measured particle spectra, σ(E, θ). ^13,14C, ^13,14,15N, ^14,15O deduced levels, J, π, spectroscopic amplitudes.

doi: 10.1016/0370-1573(74)90045-3
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1973ST24 Phys.Lett. 47B, 16 (1973)

D.Strottman, N.Anyas-Weiss, J.C.Cornell, P.S.Fisher, P.N.Hudson, A.Menchaca-Rocha, A.D.Panagiotou, D.K.Scott

Structure of States in ²⁰Ne from the Reactions ¹⁸O(¹¹B, ⁹Li)²⁰Ne and ¹⁶O(¹¹B, ⁷Li)²⁰Ne

NUCLEAR REACTIONS ¹⁶O(¹¹B, ⁷Li), ¹⁸O(¹¹B, ⁹Li), E=114 MeV; measured σ(E(⁷Li), E(⁹Li)). ²⁰Ne deduced levels.

doi: 10.1016/0370-2693(73)90557-1
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1973ST25 Phys.Lett. 47B, 215 (1973)

D.Strottman

Pseudo SU(3) and the Extension of the Ground State Rotational Band

NUCLEAR STRUCTURE ²⁰Ne; levels calculated B(E2).

doi: 10.1016/0370-2693(73)90712-0
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1973ST32 Part.Nucl. 6, 55 (1973)

D.Strottman

Renormalization of Two Body Matrix Elements and the Quadrupole-Quadrupole Force in the sd Shell

NUCLEAR STRUCTURE ¹⁹O, ^20,21Ne, ¹⁹F; calculated levels.

1972ST11 Phys.Lett. 39B, 457 (1972)

D.Strottman

SU(3) Calculations in ²⁴Mg

NUCLEAR STRUCTURE ²⁴Mg; calculated levels, B(E2), μ, quadrupole moment. Su(3) formalism; realistic matrix elements.

doi: 10.1016/0370-2693(72)90317-6
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1972ST13 Nucl.Phys. A188, 488 (1972)

D.Strottman

On the Validity of the Pseudo SU(3) for A = 59 and 60

NUCLEAR STRUCTURE ⁶⁰Zn, ⁶⁰Ni; A=59-60; calculated levels, energy centroids. Pseudo SU₃.

doi: 10.1016/0375-9474(72)90215-1
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1971AR05 Nucl.Phys. A162, 423 (1971)

A.Arima, D.Strottman

The Structure of Positive Parity States of ²⁰Ne

NUCLEAR STRUCTURE ²⁰Ne; calculated levels, B(E2).

doi: 10.1016/0375-9474(71)90996-1
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1971ST04 Nucl.Phys. A162, 605 (1971)

D.Strottman, A.Arima

Stabilization of the Axially Symmetric Shape and (pf)² Mixing in sd Shell Nuclei

NUCLEAR STRUCTURE ²²Ne, ²⁴Mg; calculated levels, B(E2).

doi: 10.1016/0375-9474(71)90259-4
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1971ST36 Phys.Lett. 36B, 321 (1971)

D.Strottman

Low Lying 8 and 12 Hole States in Light Nuclei

NUCLEAR STRUCTURE ²⁰Ne, ²⁴Mg, ²⁸Si, ³²S, ³⁶Ar, ⁴⁰Ca, ⁴⁴Ti, ⁴⁸Cr, ⁵²Fe; calculated mp-mh(M < 13) states, B(E2). Shell model, monopole-monopole interaction.

doi: 10.1016/0370-2693(71)90714-3
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Note: The following list of authors and aliases matches the search parameter D.Strottman: , D.D.STROTTMAN