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NSR database version of May 30, 2024.

Search: Author = D.Strottman

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2023RE05      Phys.Rev. C 107, 034915 (2023)

A.Reina Ramirez, V.K.Magas, L.P.Csernai, D.Strottman

Generalized effective string rope model for the initial stages of ultrarelativistic heavy ion collisions

doi: 10.1103/PhysRevC.107.034915
Citations: PlumX Metrics


2018MA34      Phys.Rev. C 97, 064903 (2018)

V.K.Magas, J.Gordillo, D.Strottman, Y.L.Xie, L.P.Csernai

Initial state with shear in peripheral heavy ion collisions

doi: 10.1103/PhysRevC.97.064903
Citations: PlumX Metrics


2012CS03      Phys.Rev. C 85, 054901 (2012)

L.P.Csernai, D.D.Strottman, Cs.Anderlik

Kelvin-Helmholtz instability in high-energy heavy-ion collisions

doi: 10.1103/PhysRevC.85.054901
Citations: PlumX Metrics


2012LE12      Phys.Rev. C 86, 034332 (2012); Erratum Phys.Rev. C 91, 049901 (2015)

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

Effect of pairing correlations on the isospin-mixing parameter in deformed N=Z even-even nuclei

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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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 T1/2 for proton emission from excited states. Time-dependent Schrodinger equation, improved boundary conditions, comparison with data.

doi: 10.1016/j.cpc.2005.07.005
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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 T1/2. Time-dependent Schroedinger equation, comparison with data.

doi: 10.1103/PhysRevC.62.014609
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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, T1/2 vs level energy. One-dimensional time-dependent Schrodinger equation.

doi: 10.1103/PhysRevC.60.054318
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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 T1/2. Relativistic hydrodynamics.

doi: 10.1016/0370-2693(96)00202-X
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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 T1/2. Short-range correlations, finite size nucleon effects.

doi: 10.1016/0370-2693(85)90911-6
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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 117,119,121,123,125,127Cs, 115,117,119,121,123,125,127,129Sb; calculated hole, particle state energy difference. 109,111,113,115In, 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 T1/2; 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