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NSR database version of April 11, 2024.

Search: Author = J.P.Svenne

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2019FR03      Phys.Rev. C 100, 024609 (2019)

P.R.Fraser, K.Amos, L.Canton, S.Karataglidis, D.van der Knijff, J.P.Svenne

Mass-15 nuclei and predicting narrow states beyond the proton drip line

NUCLEAR STRUCTURE 15C, 15N, 15O, 15F; calculated levels, J, π and widths using multichannel algebraic scattering (MCAS) technique, and n+14O or p+14C and p+14O or n+14C mirror systems. Comparison with experimental data.

NUCLEAR REACTIONS 1H(14O, 15F), E=E=95 MeV/nucleon; calculated cross sections for population of levels in 15F using multichannel algebraic scattering (MCAS) technique, and using the vibrational model for the interaction potential for p+14O cluster. Comparison with experimental data.

doi: 10.1103/PhysRevC.100.024609
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2017AM02      Eur.Phys.J. A 53, 72 (2017)

K.Amos, L.Canton, P.R.Fraser, S.Karataglidis, J.P.Svenne, D.van der Knijff

A multi-channel model for an α plus 6He nucleus cluster

NUCLEAR REACTIONS 4He(6He, 6He'), E=2-6 MeV(10Be E*=9.4-13.4 MeV); calculated σ(θ). Compared with data.

NUCLEAR STRUCTURE 10Be; calculated levels, J, πi, charge distribution using three- and five-state MCAS (Multi-Channel Algebraic Scattering). Compared with data.

doi: 10.1140/epja/i2017-12270-1
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2017SV01      Phys.Rev. C 95, 034305 (2017)

J.P.Svenne, L.Canton, K.Amos, P.R.Fraser, S.Karataglidis, G.Pisent, D.van der Knijff

Very low-energy nucleon-16O coupled-channel scattering: Results with a phenomenological vibrational model

NUCLEAR STRUCTURE 17O, 17F; calculated levels, J, π, widths. 16O; calculated B(E2) for the first 2+ and B(E3) for the first 3- state, ρ2(E0) for the first excited 0+ state. Multichannel algebraic scattering method (MCAS)for bound states and resonances. Comparison with experimental data.

NUCLEAR REACTIONS 16O(n, X), E=0.001-8.5 MeV; calculated total σ(E). 16O(p, X), E<4.5 MeV; calculated differential σ(E, θ). Multichannel algebraic scattering method (MCAS) for nucleon-16O cluster systems. Comparison with experimental data.

doi: 10.1103/PhysRevC.95.034305
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2016FR09      Phys.Rev. C 94, 034603 (2016)

P.R.Fraser, K.Massen-Hane, K.Amos, I.Bray, L.Canton, R.Fossion, A.S.Kadyrov, S.Karataglidis, J.P.Svenne, D.van der Knijff

Importance of resonance widths in low-energy scattering of weakly bound light-mass nuclei

NUCLEAR STRUCTURE 9Be; calculated levels, resonances J, π, widths of a compound nucleus with 8Be+n cluster by solving the Lippmann-Schwinger equations in momentum space. Comparison with multichannel algebraic scattering (MCAS) calculations with target states.

NUCLEAR REACTIONS 8Be(n, n), E<5.5 MeV; 12C(n, n), (n, X), E<6.5 MeV; calculated elastic and reaction σ(E) coupled to first 0+, 2+ and 4+ states in 8Be, reaction σ with particle emission widths of 12C coupled to g.s., first 2+ and first excited 0+ states in 12C; deduced effect of particle-emitting resonances on the scattering cross section. Method involved choosing an appropriate target-state resonance shape, modifying a Lorentzian by use of widths dependent on projectile energy, with a correction to target-state centroid energy.

doi: 10.1103/PhysRevC.94.034603
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2015FR04      Eur.Phys.J. A 51, 110 (2015)

P.R.Fraser, K.Amos, L.Canton, S.Karataglidis, D.van der Knijff, J.P.Svenne

A collective coupled-channel model and mirror state energy displacements

NUCLEAR STRUCTURE 12C; calculated charge distribution, radius; deduced interaction parameters. 13,15C, 13,15,16N, 15,16O, 15F; calculated energy levels, J, π; deduced interaction parameters. MCAS (multi-channel algebraic scattering) method; compared to data.

NUCLEAR REACTIONS 1H(14O, 14O'), E(cm)=0.3-9 MeV; calculated σ(θ) using MCAS (multi-channel algebraic scattering) method; compared to data.

doi: 10.1140/epja/i2015-15110-4
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2014FR08      Phys.Rev. C 90, 024616 (2014)

P.R.Fraser, L.Canton, K.Amos, S.Karataglidis, J.P.Svenne, D.van der Knijff

Coupling to two target-state bands in the study of the n+22Ne system at low energy

NUCLEAR STRUCTURE 22Ne; calculated low-lying levels, J, π, dominant partition percentages, β2, B(E2) using large-space shell-model. 23Ne; calculated levels, resonances, J, π by coupling to low-lying states in 22Ne using multichannel algebraic scattering (MCAS) formalism for n+22Ne system; comparison with experimental spectrum of 23Ne.

NUCLEAR REACTIONS 22Ne(n, n), E<4.5 MeV; calculated elastic σ(E), resonances, J, π using multichannel algebraic scattering (MCAS) formalism. Comparison with experimental data.

doi: 10.1103/PhysRevC.90.024616
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2014NA25      Nucl.Data Sheets 119, 98 (2014)

N.Nankov, A.J.M.Plompen, S.Kopecky, K.S.Kozier, D.Roubtsov, R.Rao, R.Beyer, E.Grosse, R.Hannaske, A.R.Junghans, R.Massarczyk, R.Schwengner, D.Yakorev, A.Wagner, M.Stanoiu, L.Canton, R.Nolte, S.Rottger, J.Beyer, J.Svenne

The Angular Distribution of Neutrons Scattered from Deuterium below 2 MeV

NUCLEAR REACTIONS 2H(n, n), E=0.1-2 MeV; Measured En, In(θ=150), In(θ=1650) using nELBE neutron ToF facility; deduced neutron spectra, deuteron counts at forward and backward directions.

doi: 10.1016/j.nds.2014.08.028
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2014RO12      Nucl.Data Sheets 118, 414 (2014)

D.Roubtsov, K.S.Kozier, J.C.Chow, A.J.M.Plompen, S.Kopecky, J.P.Svenne, L.Canton

Reactivity Impact of 2H and 16O Elastic Scattering Nuclear Data on Critical Systems with Heavy Water

NUCLEAR REACTIONS 2H, 16O(n, n), E=0.0001 eV-2 MeV; evaluated elastic scattering σ for critical systems with heavy water, influence on reactivity.

doi: 10.1016/j.nds.2014.04.094
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2013AM01      Nucl.Phys. A912, 7 (2013)

K.Amos, L.Canton, P.R.Fraser, S.Karataglidis, J.P.Svenne, D.van der Knijff

Analysis of a coupled-channel continuum approach for spectra of mass-17 compound systems

NUCLEAR STRUCTURE 17C, 17Na; calculated levels, J, π, level widths using MCAS (multi-channel algebraic scattering).

doi: 10.1016/j.nuclphysa.2013.05.008
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2012AM01      Nucl.Phys. A879, 132 (2012)

K.Amos, L.Canton, P.R.Fraser, S.Karataglidis, J.P.Svenne, D.van der Knijff

Linking the exotic structure of 17C to its unbound mirror 17Na

NUCLEAR STRUCTURE 17C, 17Na; calculated low-lying resonances, deformation using MCAS (multichannel algebraic scattering) method to coupled Lippmann-Schwinger equation in momentum space and CC model of nucleon-nucleus structure; deduced parameters.

doi: 10.1016/j.nuclphysa.2012.01.022
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2012AM06      Europhys.Lett. 99, 12001 (2012)

K.Amos, D.van der Knijff, L.Canton, P.R.Fraser, S.Karataglidis, J.P.Svenne

Linking nuclear masses with nucleon-removal thresholds and the mass of the proton-emitter 17Na

NUCLEAR STRUCTURE 6,7Li, 8,9Be, 10,11B, 12,13,17C, 14,15,17N, 16,17O, 17,18,19F, 17,20Ne, 17Na; calculated ground state gap energies, masses, nucleon removal thresholds. Comparison with available data.

doi: 10.1209/0295-5075/99/12001
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2011CA10      Phys.Rev. C 83, 047603 (2011)

L.Canton, P.R.Fraser, J.P.Svenne, K.Amos, S.Karataglidis, D.van der Knijff

Energy-dependent target widths in a coupled-channel scattering study

NUCLEAR REACTIONS 8Be(n, n), (n, n'), E=0-6 MeV; calculated σ(E). 9Be; calculated resonances, J, π, width using multichannel algebraic scattering formalism for particle emitting resonances. Comparison with experimental data.

doi: 10.1103/PhysRevC.83.047603
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2011ST25      J.Korean Phys.Soc. 59, 1825s (2011)

M.Stanoiu, N.Nankov, A.J.M.Plompen, C.Rouki, K.Kozier, R.Rao, D.Roubtsov, J.P.Svenne, L.Canton

Neutron-Deuteron Elastic Scattering Measurements

doi: 10.3938/jkps.59.1825
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2010CA20      Int.J.Mod.Phys. E19, 1435 (2010)

L.Canton, K.Amos, S.Karataglidis, J.P.Svenne

Coupled-channel calculation of bound and resonant spectra of 9ΛBe and 13ΛC hypernuclei

NUCLEAR STRUCTURE 9Be, 13C; analyzed hypernucleus spectra; deduced splitting of levels, spin-orbit, spin-spin, low-lying resonance states. Multi-channel algebraic scattering (MCAS).

doi: 10.1142/S0218301310015849
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2008FR02      Eur.Phys.J. A 35, 69 (2008)

P.Fraser, K.Amos, S.Karataglidis, L.Canton, G.Pisent, J.P.Svenne

Two causes of nonlocalities in nucleon-nucleus potentials and their effects in nucleon-nucleus scattering

NUCLEAR REACTIONS 12C(n, n), (n, n'), E=40.3, 95 MeV; 12C(p, p), (p, p'), E=200 MeV; calculated σ(θ), Ay(θ). 12C(e, e), E not given; calculated longitudinal and transverse form factors. Coupled channel calculations, comparison with data.

doi: 10.1140/epja/i2007-10524-1
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2008FR11      Phys.Rev.Lett. 101, 242501 (2008)

P.Fraser, K.Amos, L.Canton, G.Pisent, S.Karataglidis, J.P.Svenne, D.van der Knijff

Coupled-Channel Evaluations of Cross Sections for Scattering Involving Particle-Unstable Resonances

NUCLEAR REACTIONS 12C(n, n'), E < 6 MeV; 8Be(n, n'), E < 4 MeV; calculated cross sections using a multichannnel algebraic scattering approach; 9Be; calculated levels energies, widths. Compared results to available data.

doi: 10.1103/PhysRevLett.101.242501
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2008KA39      Nucl.Phys. A813, 235 (2008)

S.Karataglidis, K.Amos, P.Fraser, L.Canton, J.P.Svenne

Constraints on the spectra of 17, 19C

NUCLEAR STRUCTURE 17,19C; analyzed levels, J, radii with shell model and coupled-channel approach, scattering data.

NUCLEAR REACTIONS 1H(17C, 17C), (19C, 19C), E=70 MeV/nucleon; analyzed elastic and inelastic σ(θ). 17,19C(p, p'), E=70 MeV; analyzed σ(θ). Microscopic g-folding and distorted wave approximation calculations.

doi: 10.1016/j.nuclphysa.2008.09.007
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2008SV02      Few-Body Systems 44, 31 (2008)

J.P.Svenne, L.Canton, K.S.Kozier

Neutron-deuteron scattering calculation for evaluated neutron data libraries

doi: 10.1007/s00601-008-0250-6
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2007CA31      Nucl.Phys. A790, 251c (2007)

L.Canton, K.Amos, S.Karataglidis, G.Pisent, J.P.Svenne, D.van der Knijff

Particle-unstable and weakly-bound light nuclei with a Sturmian approach that preserves the Pauli principle

NUCLEAR REACTIONS 12C(n, n), E≈0.001-5 MeV; calculated σ. Coupled channel calculation. Comparison with data.

NUCLEAR STRUCTURE 7He, 7Li, 7Be, 7B, 15C, 15F; calculated levels, J, π, scattering data. Collective-coupling analysis.

doi: 10.1016/j.nuclphysa.2007.03.148
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2006CA08      Phys.Rev.Lett. 96, 072502 (2006)

L.Canton, G.Pisent, J.P.Svenne, K.Amos, S.Karataglidis

Predicting Narrow States in the Spectrum of a Nucleus beyond the Proton Drip Line

NUCLEAR STRUCTURE 14,15C, 14O; analyzed levels, scattering data. 15F calculated resonance energies, widths. Multichannel algebraic scattering theory.

doi: 10.1103/PhysRevLett.96.072502
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2006CA35      Phys.Rev.C 74, 064605 (2006)

L.Canton, G.Pisent, K.Amos, S.Karataglidis, J.P.Svenne, D.van der Knijff

Collective-coupling analysis of spectra of mass-7 isobars: 7He, 7Li, 7Be, and 7B

NUCLEAR REACTIONS 3H(α, α), E=3-14 MeV; 4He(3He, 3He), E=3-14 MeV; calculated σ(θ). Collective-coupling analysis.

NUCLEAR STRUCTURE 7He, 7Li, 7Be, 7B; calculated levels, J, π. Collective-coupling analysis.

doi: 10.1103/PhysRevC.74.064605
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2006SV01      Phys.Rev. C 73, 027601 (2006)

J.P.Svenne, K.Amos, S.Karataglidis, D.van der Knijff, L.Canton, G.Pisent

Low-energy neutron-12C analyzing powers: Results from a multichannel algebraic scattering theory

NUCLEAR REACTIONS 12C(polarized n, n), E=1.9-4 MeV; calculated σ(θ), Ay(θ). Multichannel algebraic scattering theory, comparison with data.

doi: 10.1103/PhysRevC.73.027601
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2005AM12      Phys.Rev. C 72, 064604 (2005)

K.Amos, S.Karataglidis, D.van der Knijff, L.Canton, G.Pisent, J.P.Svenne

Comparison between two methods of solution of coupled equations for low-energy scattering

NUCLEAR REACTIONS 12C(n, X), E=0.1-4 MeV; analyzed total σ. Comparison of two coupled-channels approaches.

doi: 10.1103/PhysRevC.72.064604
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2005CA16      Phys.Rev.Lett. 94, 122503 (2005)

L.Canton, G.Pisent, J.P.Svenne, D.van der Knijff, K.Amos, S.Karataglidis

Role of the Pauli Principle in Collective-Model Coupled-Channel Calculations

NUCLEAR REACTIONS 12C(n, n), E=low; analyzed σ(θ), role of Pauli principle. Multichannel algebraic scattering theory.

doi: 10.1103/PhysRevLett.94.122503
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2005PI16      Phys.Rev. C 72, 014601 (2005)

G.Pisent, J.P.Svenne, L.Canton, K.Amos, S.Karataglidis, D.van der Knijff

Compound and quasicompound states in low-energy scattering of nucleons from 12C

NUCLEAR REACTIONS 12C(n, n), E ≈ 0-5 MeV; analyzed elastic σ. 12C(p, p), E ≈ 1-7 MeV; analyzed σ(θ), Ay(θ), σ. 13C, 13N deduced sub-threshold bound state and resonance features. Multichannel algebraic scattering theory.

doi: 10.1103/PhysRevC.72.014601
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2003AM08      Nucl.Phys. A728, 65 (2003)

K.Amos, L.Canton, G.Pisent, J.P.Svenne, D.van der Knijff

An algebraic solution of the multichannel problem applied to low energy nucleon-nucleus scattering

NUCLEAR REACTIONS 12C(n, n), E=0-5 MeV; calculated elastic σ, polarization, resonance effects. Sturmian expansions of multichannel interactions. Comparison with data.

doi: 10.1016/j.nuclphysa.2003.08.019
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2002ME21      Few-Body Systems 32, 143 (2002)

T.Melde, L.Canton, J.P.Svenne

Three-Body Dynamics in One Dimension: A Test Model for the Three-Nucleon System with Irreducible Pionic Diagrams

NUCLEAR STRUCTURE A=3; calculated binding energy. Spinless, one-dimensional model.

doi: 10.1007/s00601-002-0114-4
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2001CA10      Phys.Rev. C63, 034004 (2001)

L.Canton, T.Melde, J.P.Svenne

Practical Approximation Scheme for the Pion Dynamics in the Three-Nucleon System

doi: 10.1103/PhysRevC.63.034004
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2001CA19      Nucl.Phys. A684, 417c (2001)

L.Canton, G.Pisent, W.Schadow, J.P.Svenne

Spin Observables for Pion Production from pd Collisions

NUCLEAR REACTIONS 2H(polarized p, π0), E ≈ threshold; calculated Ay(θ). Comparison with data.

doi: 10.1016/S0375-9474(01)00442-0
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1998CA09      Phys.Rev. C57, 1588 (1998)

L.Canton, G.Cattapan, G.Pisent, W.Schadow, J.P.Svenne

Spin Observables for the pd ← → π+t Reaction Around the Δ Resonance

NUCLEAR REACTIONS 2H(polarized p, π+), E=350 MeV; calculated σ(θ), A(y0)(θ), T(20)(θ); deduced reaction mechanism, Δ resonance role. Comparison with data.

doi: 10.1103/PhysRevC.57.1588
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1996CA26      Can.J.Phys. 74, 209 (1996)

L.Canton, G.Cattapan, P.J.Dortmans, G.Pisent, J.P.Svenne

A Meson-Exchange Isobar Model for the π+d → pp, pp ← π+d Reaction

NUCLEAR REACTIONS 2H(π+, p), E=145 MeV; analyzed σ(θ), polarization observables. Meson-exchange isobar model.

doi: 10.1139/p96-033
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1995PI08      Phys.Rev. C51, 3211 (1995)

G.Pisent, J.P.Svenne

Analysis of Compound and Quasicompound Resonances in a Multichannel, Finite-Rank Model

doi: 10.1103/PhysRevC.51.3211
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1993CA29      Phys.Rev. C48, 1562 (1993)

L.Canton, J.P.Svenne, G.Cattapan

Pion Absorption on 3He. II. Antisymmetrization and Angular Decomposition of the Faddeev-Based Amplitude

doi: 10.1103/PhysRevC.48.1562
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1990WA26      Can.J.Phys. 68, 1200 (1990)

W.B.Wango, J.Birchall, J.S.C.McKee, J.P.Svenne

Evidence for Three-Body Forces in p-d Breakup at 25 MeV ( Question )

NUCLEAR REACTIONS 2H(p, 2p), E=25.05 MeV; measured σ(θ1, θ2, E1) vs arc length following target breakup; deduced three-body force evidence. Faddeev calculations. Collinear geometry.

doi: 10.1139/p90-170
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1989AB06      Phys.Rev. D39, 2464 (1989)

R.Abegg, D.Bandyopadhyay, J.Birchall, E.B.Cairns, H.Coombes, C.A.Davis, N.E.Davison, P.P.J.Delheij, P.W.Green, L.G.Greeniaus, H.P.Gubler, D.C.Healey, C.Lapointe, W.P.Lee, W.J.McDonald, C.A.Miller, G.A.Moss, G.R.Plattner, P.R.Poffenberger, W.D.Ramsay, G.Roy, J.Soukup, J.P.Svenne, R.R.Tkachuk, W.T.H.van Oers, G.D.Wait, Y.P.Zhang

Charge-Symmetry Breaking in np Elastic Scattering at 477 MeV

NUCLEAR REACTIONS 1H(polarized n, n), E=477 MeV; measured neutron, proton analyzing power difference; deduced isospin violating, charge symmetry breaking effects role.

doi: 10.1103/PhysRevD.39.2464
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Data from this article have been entered in the EXFOR database. For more information, access X4 dataset13181.


1989AB11      Phys.Rev. C40, 2406 (1989)

R.Abegg, M.Ahmad, D.Bandyopadhyay, J.Birchall, E.B.Cairns, K.Chantziantoniou, H.Coombes, C.A.Davis, N.E.Davison, P.P.J.Delheij, P.W.Green, L.G.Greeniaus, H.P.Gubler, D.C.Healey, C.Lapointe, W.P.Lee, W.J.McDonald, C.A.Miller, G.A.Moss, S.A.Page, G.R.Plattner, P.R.Poffenberger, W.D.Ramsay, N.L.Rodning, G.Roy, J.Soukup, J.P.Svenne, R.R.Tkachuk, W.T.H.van Oers, G.D.Wait, J.W.Watson, Y.Ye, Y.P.Zhang

np Elastic Scattering Analyzing Power Characteristics at Intermediate Energies

NUCLEAR REACTIONS 1H(polarized n, n), E=220-477 MeV; measured polarization observables; deduced analyzing power. Other data input.

doi: 10.1103/PhysRevC.40.2406
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1986LE02      Phys.Rev. C33, 417 (1986)

Lei Ge, J.P.Svenne

Charge-Symmetry Breaking in Neutron-Proton Scattering: Isospin-mixing parameter

NUCLEAR REACTIONS 1n(p, p), E=100-400 MeV; calculated isospin mixing parameter; deduced analyzing power difference.

doi: 10.1103/PhysRevC.33.417
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1985AB05      Nucl.Instrum.Methods 234, 20 (1985)

R.Abegg, J.Birchall, E.Cairns, H.Coombes, C.A.Davis, N.E.Davison, P.W.Green, L.G.Greeniaus, H.P.Gubler, W.P.Lee, W.J.McDonald, C.A.Miller, G.A.Moss, G.R.Plattner, P.R.Poffenberger, G.Roy, J.Soukup, J.P.Svenne, R.Tkachuk, W.T.H.van Oers, Y.P.Zhang

Detection Equipment For A Test of Charge Symmetry in n-p Elastic Scattering

NUCLEAR REACTIONS 1H(polarized n, n), E=150-500 MeV; measured neutron, recoil proton analyzing power, difference.

doi: 10.1016/0168-9002(85)90804-6
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1985AB06      Nucl.Instrum.Methods 234, 11 (1985)

R.Abegg, J.Birchall, E.Cairns, H.Coombes, C.A.Davis, N.E.Davison, P.W.Green, L.G.Greeniaus, H.P.Gubler, W.P.Lee, W.J.McDonald, C.A.Miller, G.A.Moss, G.R.Plattner, P.R.Poffenberger, G.Roy, J.Soukup, J.P.Svenne, R.Tkachuk, W.T.H.Van Oers, Y.P.Zhang

The Neutron Beam Facility at TRIUMF

NUCLEAR REACTIONS 1H(polarized n, n), E=480 MeV; measured effective analyzing power. High precision experiments.


1985AB18      J.Phys.(Paris), Colloq.C-2, 467 (1985)

R.Abegg, J.Birchall, E.Cairns, H.Coombes, C.A.Davis, N.E.Davison, P.P.J.Delheij, P.W.Green, L.G.Greeniaus, H.P.Gubler, D.C.Healey, W.P.Lee, W.J.McDonald, C.A.Miller, G.A.Moss, G.R.Plattner, P.R.Poffenberger, G.Roy, J.Soukup, J.P.Svenne, R.Tkachuk, W.T.H.van Oers, G.D.Wait, Y.P.Zhang

Test of Charge Symmetry in n-p Elastic Scattering at 480 MeV

NUCLEAR REACTIONS 1H(polarized n, n), E=480 MeV; measured neutron, proton analyzing power difference.


1982SV01      Phys.Lett. 119B, 269 (1982)

J.P.Svenne, J.Birchall, J.S.C.McKee

Possible Evidence for Sensitivity to the Two-Body Tensor Force in the Reaction d + p → p + p + n

NUCLEAR REACTIONS 2H(p, 2p), E=25.7 MeV; measured σ(θ1, θ2, E1); deduced breakup sensitivity to two-body tensor force. 1H(polarized d, 2p), E=51.4 MeV; calculated tensor analyzing power vs θ. Three-body model.

doi: 10.1016/0370-2693(82)90667-0
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1980AY01      Can.J.Phys. 58, 1026 (1980)

T.Aytimur, J.P.Svenne

Three-Body Calculations of Elastic Scattering and Stripping of Deuterons on 16O

NUCLEAR REACTIONS 16O(d, d), (d, n), (d, p), E=20, 45 MeV; 16O(polarized d, d), (polarized d, p), (polarized d, n), E=20 MeV; calculated σ(θ), vector, tensor analyzing power vs θ. Three-body calculations, no Coulomb effects, separable interactions.

doi: 10.1139/p80-141
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1980SV01      J.Phys.(London) G6, 465 (1980)

J.P.Svenne

A Relation between Average Kinetic Energy and Mean-Square Radius in Nuclei

NUCLEAR STRUCTURE 16O, 208Pb; calculated average kinetic energy, single-particle sum rule. Hartree-Fock, Hartree-Fock-Bogoliubov theories.

doi: 10.1088/0305-4616/6/4/015
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1979BI07      Phys.Rev. C20, 1585 (1979)

J.Birchall, J.P.Svenne, M.S.de Jong, J.S.C.McKee, W.D.Ramsay, M.S.A.L.Al-Ghazi, N.Videla

Proton-Deuteron Breakup Cross Sections in Collinear Geometry at 28.6 MeV

NUCLEAR REACTIONS 2H(p, 2p), E=28.6 MeV; measured σ. Collinear geometry, exact three-body calculation.

doi: 10.1103/PhysRevC.20.1585
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1978SV01      Phys.Rev. C18, 983 (1978)

J.P.Svenne, R.S.Mackintosh

Spin-Orbit Force and the Deformation of 12C

NUCLEAR STRUCTURE 12C; calculated deformation.

doi: 10.1103/PhysRevC.18.983
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1975BE48      Phys.Rev. C12, 2067 (1975)

R.L.Becker, J.P.Svenne

Interpretation of Inversions of Single-Particle Levels in Self-Consistent Field Theories

NUCLEAR STRUCTURE 15N, 15,16O; calculated single-particle energies, level inversion.

doi: 10.1103/PhysRevC.12.2067
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1974RE03      Phys.Rev. C9, 1882 (1974)

N.E.Reid, N.E.Davison, J.P.Svenne

Variational Calculation of Light Nuclei Using Nearly Orthogonal Functions

NUCLEAR STRUCTURE 16O, 20Ne, 24Mg, 28Si, 32S, 36Ar, 40Ca; calculated binding energies, radii, moments, density distributions. Variational method. Density-dependent interaction.

doi: 10.1103/PhysRevC.9.1882
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1972PA21      Phys.Rev. C6, 34 (1972)

J.C.Parikh, J.P.Svenne

How Good Is the Hartree-Fock Approximation for 16O (Question)

NUCLEAR STRUCTURE 16O; analyzed intrinsic states; tested Hartree-Fock approximation.

doi: 10.1103/PhysRevC.6.34
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1971CA24      Can.J.Phys. 49, 2028 (1971)

B.Castel, J.P.Svenne

Compressibility under Deformation of the Hartree-Fock Field

NUCLEAR STRUCTURE 44Ca, 50Cr, 56,58Ni; calculated rms radius, compressibility under deformation. Deformed Hartree-Fock model.

doi: 10.1139/p71-245
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1971LA05      Nucl.Phys. A164, 49 (1971)

A.Lande, J.P.Svenne

The Proton Densities in 40Ca and 48Ca in the Hartree-Fock Approximation

NUCLEAR STRUCTURE 40,48Ca; calculated rms proton radii. Hartree-Fock theory.

doi: 10.1016/0375-9474(71)90842-6
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1970BR37      Nucl.Phys. A154, 449 (1970)

D.M.Brink, J.P.Svenne

Isospin Mixing of Hartree-Fock Solutions

NUCLEAR STRUCTURE 40,48Ca; calculated ground-state energy, proton, mass radii. Constrained Hartree-Fock method, isospin mixing.

doi: 10.1016/0375-9474(70)90117-X
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1969CA08      Can.J.Phys. 47, 1393 (1969)

B.Castel, J.P.Svenne

Octupole Deformations in the 2s-1d Shell

NUCLEAR STRUCTURE 30Si, 32,34S, 36,38Ar; calculated levels, deformation parameters.

doi: 10.1139/p69-178
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