NSR Query Results
Output year order : Descending NSR database version of April 27, 2024. Search: Author = L.Canton Found 61 matches. 2022AM07 Eur.Phys.J. A 58, 181 (2022) K.Amos, S.Karataglidis, L.Canton, P.R.Fraser, K.Murulane Coupled-channel description for mirror mass-11 nuclei compared to shell-model structures NUCLEAR STRUCTURE 10,11Be, 10,11C, 10,11B, 11N; calculated energy levels, J, π; deduced parameter values used in the coupled-channel evaluations. The Multi-Channel Algebraic Scattering method (MCAS).
doi: 10.1140/epja/s10050-022-00828-1
2022CO03 Nucl.Technology 208, 735 (2022) A.Colombi, M.P.Carante, F.Barbaro, L.Canton, A.Fontana Production of High-Purity 52gMn from natV Targets with Alpha Beams at Cyclotrons NUCLEAR REACTIONS V(α, X)52Mn, E<100 MeV; analyzed available data; deduced recommended integral yields, need for σ measurements. Talys, Empire, and Fluka nuclear reaction model codes.
doi: 10.1080/00295450.2021.1947122
2021AM03 Eur.Phys.J. A 57, 165 (2021) K.Amos, P.R.Fraser, S.Karataglidis, L.Canton Low-energy spectra of mirror mass-19 nuclei with a collective coupled-channel scattering model NUCLEAR STRUCTURE 3H, 3,4He, 15N, 15,16,18,19O, 19Na, 19F, 18,19Ne; analyzed available data for mirror pairs; deduced low-excitation states the Multi-Channel Algebraic Scattering (MCAS) method.
doi: 10.1140/epja/s10050-021-00479-8
2021BA44 Phys.Rev. C 104, 044619 (2021) F.Barbaro, L.Canton, M.P.Carante, A.Colombi, L.De Dominicis, A.Fontana, F.Haddad, L.Mou, G.Pupillo New results on proton-induced reactions on vanadium for 47Sc production and the impact of level densities on theoretical cross sections NUCLEAR REACTIONS V(p, X)47Sc/43Sc/44mSc/44gSc/46Sc/48Sc/42K/43K/48V/48Cr/49Cr/51Cr, E=26-70 MeV; measured Eγ, Iγ, activation σ(E) using stacked-foils natural vanadium targets, and off-line γ-ray spectroscopy; deduced impact of tuning of the theoretical level density parameters to obtain accurate cross sections. Comparison with the theoretical σ(E) using the TALYS code, and level-density parameters of the microscopic models, and with previous experimental σ(E) results. Relevance to production of 47Sc, a β--emitter for radiotheranostic applications in nuclear medicine.
doi: 10.1103/PhysRevC.104.044619
2020PU01 Nucl.Instrum.Methods Phys.Res. B464, 32 (2020) G.Pupillo, L.Mou, F.Haddad, A.Fontana, L.Canton New results on the natV(p, x)43Sc cross section: Analysis of the discrepancy with previous data NUCLEAR REACTIONS V(p, X)43Sc/43K, E<65 MeV; measured reaction products, Eγ, Iγ; deduced σ. Comparison with FLUKA, EMPIRE and TALYS calculations, EXFOR database.
doi: 10.1016/j.nimb.2019.11.032
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
2019PU03 J.Radioanal.Nucl.Chem. 322, 1711 (2019); Erratum J.Radioanal.Nucl.Chem. 328, 1407 (2021) G.Pupillo, L.Mou, A.Boschi, S.Calzaferri, L.Canton, S.Cisternino, L.De Dominicis, A.Duatti, A.Fontana, F.Haddad, P.Martini, M.Pasquali, H.Skliarova, J.Esposito Production of 47Sc with natural vanadium targets: results of the PASTA project NUCLEAR REACTIONS V(p, X)46Sc/47Sc, E=34-70 MeV; measured reaction products, Eγ, Iγ; deduced σ. Comparison with TALYS, EMPIRE and FLUKA calculations.
doi: 10.1007/s10967-019-06844-8
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
2017FR05 Phys.Rev. C 96, 014619 (2017) P.R.Fraser, K.Massen-Hane, A.S.Kadyrov, K.Amos, I.Bray, L.Canton Effective two-body model for spectra of clusters of 2H, 3H, 3He and 4He with 4He, and 2H - 4He scattering NUCLEAR REACTIONS 4He(t, X)7Li, 4He(3He, X)7Be, 4He(α, X)8Be, 4He(d, X)6Li; calculated low-energy spectra of 6Li, 7Li, 7Be and 8Be, considering 7Li as cluster of 4He with 3H, 7Be as cluster of 4He with 3He, 8Be as cluster of 4He with 4He, and 6Li as cluster of 4He with 2H. 4He(d, d), E=0.6-11 MeV; calculated σ(E, θ). Comparison with experimental data. Solution of single-channel Lippmann-Schwinger equations.
doi: 10.1103/PhysRevC.96.014619
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
2016FR07 J.Phys.(London) G43, 095104 (2016) P.R.Fraser, A.S.Kadyrov, K.Massen-Hane, K.Amos, L.Canton, S.Karataglidis, D.van der Knijff, I.Bray Structure of 23Al from a multi-channel algebraic scattering model based on mirror symmetry NUCLEAR REACTIONS 22Mg(p, X)23Al, E(cm)<4 MeV; calculated σ(θ). Comparison with experimental data. NUCLEAR STRUCTURE 23Al; calculated energy levels, J, π. Comparison with experimental data.
doi: 10.1088/0954-3899/43/9/095104
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
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
2015LA13 Ukr.J.Phys. 60, 406 (2015) Y.A.Lashko, G.F.Filippov, L.Canton Scattering of 6He on α-Particle: Microscopic Guidance for Orthogonalizing Pseudopotentials NUCLEAR REACTIONS 4He(6He, 6He), E<200 MeV; calculated phase shifts. Microscopic two-cluster model.
doi: 10.15407/ujpe60.05.0406
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
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
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
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
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
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
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
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
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
2008CA14 Nucl.Phys. A808, 192 (2008) Low-energy radiative-capture reactions within two-cluster coupled-channel description NUCLEAR REACTIONS 3He(α, γ), E(cm)=0-2.0 MeV; calculated σ; deduced astrophysical S-factor using a multichannel algebraic scattering approach. 7Be deduced levels, J, π.
doi: 10.1016/j.nuclphysa.2008.05.006
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
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
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
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
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
2007KO11 Ann.Phys.(New York) 322, 736 (2007) V.Yu.Korda, L.Canton, A.V.Shebeko Relativistic interactions for the meson-two-nucleon system in the clothed-particle unitary representation
doi: 10.1016/j.aop.2006.07.010
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
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
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
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
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
2005CA20 Phys.Rev. C 71, 041001 (2005) Polarized proton pionic capture in deuterium as a probe of 3N dynamics NUCLEAR REACTIONS 2H(polarized p, π0), E=350-500 MeV; calculated σ(θ), Ay(θ); deduced role of three-nucleon dynamics in initial state. Comparison with data.
doi: 10.1103/PhysRevC.71.041001
2005ME15 Eur.Phys.J. A 25, 97 (2005) T.Melde, L.Canton, W.Plessas, R.F.Wagenbrunn Spectator-model operators in point-form relativistic quantum mechanics
doi: 10.1140/epja/i2004-10276-4
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
2004CA27 Nucl.Phys. A737, 200 (2004) What can we learn from an explicit treatment of the π in the three-nucleon system? NUCLEAR REACTIONS 2H(n, n), E=8.5-18 MeV; analyzed σ(θ), analyzing powers, role of pion dynamics.
doi: 10.1016/j.nuclphysa.2004.03.064
2004LE23 Eur.Phys.J. A 21, 29 (2004) L.Levchuk, L.Canton, A.Shebeko Nuclear effects in positive pion electroproduction on the deuteron near threshold NUCLEAR REACTIONS 1H(e, e'π+), E ≈ threshold; analyzed σ(E, θ); deduced nuclear medium effects. Unitary transformation method.
doi: 10.1140/epja/i2003-10184-1
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
2002CA32 Eur.Phys.J. A 14, 225 (2002) L.Canton, W.Schadow, J.Haidenbauer Irreducible Pionic Effects in Nucleon-Deuteron Scattering Below 20 MeV NUCLEAR REACTIONS 2H(p, p), (n, n), E=3-19 MeV; calculated σ(θ), analyzing powers, spin transfer coefficients, polarization transfer coefficients. Comparison with data and between different potentials.
doi: 10.1140/epja/i2001-10122-3
2002ME21 Few-Body Systems 32, 143 (2002) 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
2001CA10 Phys.Rev. C63, 034004 (2001) Practical Approximation Scheme for the Pion Dynamics in the Three-Nucleon System
doi: 10.1103/PhysRevC.63.034004
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
2001CA44 Phys.Rev. C64, 031001 (2001) One-Pion-Exchange Three-Nucleon Force and the Ay Puzzle NUCLEAR REACTIONS 2H(n, n), E=3-30 MeV; calculated σ(θ), analyzing powers; deduced three-nucleon force effects. Comparisons with data.
doi: 10.1103/PhysRevC.64.031001
2000CA23 Phys.Rev. C61, 064009 (2000) Isoscalar Off-Shell Effects in Threshold Pion Production from pd Collisions NUCLEAR REACTIONS 2H(p, π+), E ≈ threshold; calculated σ(θ), tensor analyzing power; deduced off-shell effects. Comparisons with data.
doi: 10.1103/PhysRevC.61.064009
2000CA39 Phys.Rev. C62, 044005 (2000) Why is the Three-Nucleon Force so Odd ?
doi: 10.1103/PhysRevC.62.044005
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
1998CA39 Phys.Rev. C58, 1929 (1998) L.Canton, A.Davini, P.J.Dortmans pp ← → π+ d Process at Low Energy: Interplay between s- and p-wave mechanisms NUCLEAR REACTIONS 1H(p, π+), E ≈ threshold; calculated production σ, σ(θ), analyzing power. Meson-exchange isobar model. Comparison with data.
doi: 10.1103/PhysRevC.58.1929
1998CA48 Phys.Rev. C58, 3121 (1998) Pion-Three-Nucleon Problem with Two-Cluster Connected-Kernel Equations
doi: 10.1103/PhysRevC.58.3121
1997CA28 Phys.Rev. C56, 689 (1997) πNNN-NNN Problem: Connectedness, transition amplitudes, and quasiparticle approximation
doi: 10.1103/PhysRevC.56.689
1997CA37 Phys.Rev. C56, 1231 (1997) pd → π+t Reaction Around the Δ Resonance NUCLEAR REACTIONS 2H(p, X), E=300-605 MeV; analyzed π+ production σ vs π momentum, other observables; deduced reaction mechanism related features. Three-body mechanisms.
doi: 10.1103/PhysRevC.56.1231
1997DO03 J.Phys.(London) G23, 479 (1997) P.J.Dortmans, L.Canton, K.Amos Cross Sections, Spin Observables, and Helicity Amplitudes of the π+d → pp pp ← π+d Reaction at the Isobar Resonance and Below NUCLEAR REACTIONS 2H(π+, p), E=145 MeV; analyzed σ(θ). 2H(π+, p), E=112, 180 MeV; analyzed σ(θ), polarization observables, helicity amplitudes. Impluse mechanism, Δ-rescattering, s-wave πN-scattering mechisms included.
doi: 10.1088/0954-3899/23/4/008
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
1994CA31 Phys.Rev. C50, 2761 (1994) Theory of Coupled π-Trinucleon Systems
doi: 10.1103/PhysRevC.50.2761
1994DO12 Phys.Rev. C49, 2828 (1994) P.J.Dortmans, L.Canton, G.Pisent, K.Amos Complex Conjugate Pairs in Stationary Sturmian Eigenstates
doi: 10.1103/PhysRevC.49.2828
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
1991CA04 Phys.Rev. C43, 1395 (1991) G.Cattapan, L.Canton, G.Pisent Analysis of the Optical Potential with Coupled-Channel Scattering Equations: Energy dependence and coordinate-space behavior NUCLEAR REACTIONS 208Pb(n, n), E not given; calculated dynamic polarization potential, radial dependence. Sturmian expansion method.
doi: 10.1103/PhysRevC.43.1395
1991CA22 Phys.Rev. C44, 1784 (1991) Pion Absorption on 3He: Absorption amplitude in the Faddeev-quasiparticle scheme NUCLEAR REACTIONS 3He(π, X), E not given; calculated pion-induced target breakup amplitudes. Faddeev-quasiparticle scheme.
doi: 10.1103/PhysRevC.44.1784
1987CA17 Nuovo Cim. 97A, 319 (1987) L.Canton, G.Cattapan, G.Pisent Separable Expansions for Realistic Multichannel Scattering Problems NUCLEAR REACTIONS 4He(n, n), E ≤ 20; calculated phase shifts. 4He(n, n), E=6 MeV; calculated polarization vs θ. 4He(n, n), E ≈ 24-34 MeV; calculated absorptive scattering phase shift vs E. Realistic multi-channel approach, separable expansions.
doi: 10.1007/BF02734941
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