NSR Query Results
Output year order : Descending NSR database version of March 21, 2024. Search: Author = S.Karataglidis Found 81 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
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
2020AM08 Eur.Phys.J. A 56, 284 (2020) K.Amos, S.Karataglidis, W.A.Richter Charge exchange (p, n) reaction to isobaric analogue states of select nuclei NUCLEAR REACTIONS 90Zr(p, p), (p, n), E=45 MeV; 42,44,48Ca(p, p), (p, n), E=35 MeV; 208Pb(p, p), (p, n), E=45 MeV; analyzed available data; deduced isobaric analogue state (IAS) of ground states of the nuclei, spectroscopic parameters using DWBA98 code.
doi: 10.1140/epja/s10050-020-00278-7
2020KA33 Phys.Rev. C 101, 064316 (2020) Structure of 16C and the B(E2) problem NUCLEAR STRUCTURE 16C; calculated levels, J, π, and B(E2) for the first 2+ state using large scale, no-core, shell-model approach. Comparison with experimental data, and with other theoretical predictions. NUCLEAR REACTIONS 16C(p, p), E=300 MeV; calculated differential σ(θ) using microscopic Melbourne g-folding optical model.
doi: 10.1103/PhysRevC.101.064316
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
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
2017KA20 Eur.Phys.J. A 53, 70 (2017) Electron scattering and reactions from exotic nuclei
doi: 10.1140/epja/i2017-12277-6
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
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
2014GI09 Phys.Scr. 89, 054009 (2014) Symmetries and fluctuations in the nuclear density functional
doi: 10.1088/0031-8949/89/5/054009
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
2013KA21 Phys.Rev. C 87, 054623 (2013) Spin observables in $71A$ MeV 6, 8He-hydrogen scattering NUCLEAR REACTIONS 1H(6He, 6He), (6He, 6He'), (8He, 8He), (8He, 8He'), E=71 MeV/nucleon; analyzed elastic and inelastic scattering σ, σ(θ) and Ay(θ) on polarized hydrogen. The g-folding approach, using multi-phonon no-core shell model wave functions. Neutron skin in 8He.
doi: 10.1103/PhysRevC.87.054623
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
2012FA13 Phys.Rev. C 86, 064606 (2012) Phenomenological pn → ppP- model ofA(p, π-B reactions NUCLEAR REACTIONS 13C(p, π-)14O, E=200 MeV; calculated differential σ(θ), analyzing powers and compared with experimental data. Calculated pn to ppπ- amplitudes, shell model, two-body parentage amplitudes.
doi: 10.1103/PhysRevC.86.064606
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
2011SA39 Phys.Rev. C 84, 024604 (2011) S.Sakaguchi, Y.Iseri, T.Uesaka, M.Tanifuji, K.Amos, N.Aoi, Y.Hashimoto, E.Hiyama, M.Ichikawa, Y.Ichikawa, S.Ishikawa, K.Itoh, M.Itoh, H.Iwasaki, S.Karataglidis, T.Kawabata, T.Kawahara, H.Kuboki, Y.Maeda, R.Matsuo, T.Nakao, H.Okamura, H.Sakai, Y.Sasamoto, M.Sasano, Y.Satou, K.Sekiguchi, M.Shinohara, K.Suda, D.Suzuki, Y.Takahashi, A.Tamii, T.Wakui, K.Yako, M.Yamaguchi, Y.Yamamoto Analyzing power in elastic scattering of 6He from a polarized proton target at 71 MeV/nucleon NUCLEAR REACTIONS 1H(6He, 6He), [6He secondary beam from 9Be(12C, X), E=92 MeV/nucleon primary reaction], E=71 MeV/nucleon; measured 6He and proton spectra, (6He)(p)(q, φ), p(θ), vector analyzing powers, polarized target, σ(θ); deduced optical model parameters. Comparison with semimicroscopic analysis with an α+n+n cluster folding model.
doi: 10.1103/PhysRevC.84.024604
2010AM03 Nucl.Phys. A836, 59 (2010) K.Amos, S.Karataglidis, Y.J.Kim Low excitation structure of 10B probed by scattering of electrons and of 197 MeV polarized protons NUCLEAR REACTIONS 10B(e, e), (e, e'), E≈50-550 MeV; calculated form factors. 10B(polarized p, p), E=197 MeV; 10B(polarized p, p'), E=197, 200 MeV; 10B(polarized p, n), E=186 MeV; calculated σ(θ), Ay(θ), polarization transfer coefficients using a g-folding model and DWA. Comparison with other models and experimental data. NUCLEAR STRUCTURE 10B; calculated levels, J, π, B(E2) using a no-core shell model. Comparison with other models and experimental data.
doi: 10.1016/j.nuclphysa.2010.01.162
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
2010KA39 Nucl.Phys. A848, 110 (2010) S.Karataglidis, K.R.Henninger, W.A.Richter, K.Amos Proton scattering observables from Skyrme-Hartree-Fock densities NUCLEAR REACTIONS 28Si(p, p), E=65, 200 MeV; 32S(p, p), E=29.6, 65 MeV; 40Ar(p, p), E=65 MeV; 40,42,44,48Ca(p, p), E=65 MeV; calculated analyzing powers; 34S(p, p), E=29.8 MeV; 36S(p, p), E=28 MeV; 38S(p, p), E=39 MeV; 40S(p, p), E=30 MeV; 36Ar(p, p), E=33 MeV; 38Ar(p, p), E=33, 65 MeV; 42,44Ar(p, p), E=33 MeV; 46,50,52,54Ca(p, p), E=65 MeV; calculated σ(θ). Shell and Skyrme-Hartree-Fock models. Comparison with data.
doi: 10.1016/j.nuclphysa.2010.08.018
2010UE01 Phys.Rev. C 82, 021602 (2010) T.Uesaka, S.Sakaguchi, Y.Iseri, K.Amos, N.Aoi, Y.Hashimoto, E.Hiyama, M.Ichikawa, Y.Ichikawa, S.Ishikawa, K.Itoh, M.Itoh, H.Iwasaki, S.Karataglidis, T.Kawabata, T.Kawahara, H.Kuboki, Y.Maeda, R.Matsuo, T.Nakao, H.Okamura, H.Sakai, Y.Sasamoto, M.Sasano, Y.Satou, K.Sekiguchi, M.Shinohara, K.Suda, D.Suzuki, Y.Takahashi, M.Tanifuji, A.Tamii, T.Wakui, K.Yako, Y.Yamamoto, M.Yamaguchi Analyzing power for proton elastic scattering from the neutron-rich 6He nucleus NUCLEAR REACTIONS 1H(6He, 6He), E=71 MeV/nucleon; measured σ(θ), vector analyzing power, polarized proton solid target. Comparison with t-matrix and g-matrix microscopic folding calculations. Discussed α-core distribution in 6He.
doi: 10.1103/PhysRevC.82.021602
2008DU10 Phys.Lett. B 665, 152 (2008) M.Dupuis, S.Karataglidis, E.Bauge, J.-P.Delaroche, D.Gogny Challenging nuclear structure models through a microscopic description of proton inelastic scattering off 208Pb NUCLEAR REACTIONS 208Pb(p, p'), E=65-201 MeV; calculated σ(θ). Compared results to available data.
doi: 10.1016/j.physletb.2008.05.061
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
2008KI13 Nucl.Phys. A807, 119 (2008) Y.J.Kim, K.Amos, S.Karataglidis, W.A.Richter Microscopic model analyses of proton scattering from 12C, 20Ne, 24Mg, 28Si and 40Ca NUCLEAR REACTIONS 12C, 20Ne, 24Mg, 28Si, 40Ca(polarized p, p), (polarized p, p'), E=35-250 MeV; analyzed elastic and inelastic σ, analyzing powers using a g-folding approach and DWBA.
doi: 10.1016/j.nuclphysa.2008.04.006
2008OH02 Phys.Rev. C 77, 024605 (2008) A.Ohrn, J.Blomgren, P.Andersson, A.Atac, C.Gustavsson, J.Klug, P.Mermod, S.Pomp, P.Wolniewicz, M.Osterlund, L.Nilsson, B.Bergenwall, K.Elmgren, N.Olsson, U.Tippawan, S.Dangtip, P.Phansuke, P.Nadel-Turonski, O.Jonsson, A.Prokofiev, P.-U.Renberg, V.Blideanu, C.Le Brun, J.F.Lecolley, F.R.Lecolley, M.Louvel, N.Marie-Noury, C.Schweitzer, Ph.Eudes, F.Haddad, C.Lebrun, E.Bauge, J.P.Delaroche, M.Girod, X.Ledoux, K.Amos, S.Karataglidis, R.Crespo, W.Haider Elastic scattering of 96 MeV neutrons from iron, yttrium, and lead NUCLEAR REACTIONS 56Fe, 89Y, 208Pb(n, n), E=96 MeV; measured σ(θ); 12C, 16O; systematics, compared with Wick's limit.
doi: 10.1103/PhysRevC.77.024605
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
2007KA45 Nucl.Phys. A793, 40 (2007) S.Karataglidis, Y.J.Kim, K.Amos Nucleon-nucleus scattering as a test of shell structure of some light mass exotic nuclei NUCLEAR REACTIONS 1H(8He, 8He), E=15.6 MeV/nucleon; 1H(10C, 10C), E=45.3 MeV/nucleon; 1H(11C, 11C), E=40.6 MeV/nucleon; 1H(18O, 18O), 1H(20O, 20O), E=43 MeV/nucleon; 1H(22O, 22O), E=46.6 MeV/nucleon; analyzed elastic and inelastic σ(θ). Microscopic g-folding and distorted wave approximation calculations.
doi: 10.1016/j.nuclphysa.2007.06.006
2007KA50 Phys.Lett. B 650, 148 (2007) Electron scattering form factors from exotic nuclei NUCLEAR REACTIONS 4,6,8He, 7,9,11Li, 8B(e, e), E not given; calculated longitudinal and transverse form factors. Shell model calculations.
doi: 10.1016/j.physletb.2007.04.051
2006AM01 Phys.Rev.Lett. 96, 032503 (2006) K.Amos, W.A.Richter, S.Karataglidis, B.A.Brown Proton Reaction Cross Sections as Measures of the Spatial Distributions of Neutrons in Exotic Nuclei NUCLEAR STRUCTURE A=28-58; calculated proton and neutron densities, radii; deduced optical model parameters, proton scattering σ. NUCLEAR REACTIONS 40Ar(p, p), E=65 MeV; 58Ni(p, p), E=200 MeV; calculated σ(θ), Ay(θ). Comparison with data.
doi: 10.1103/PhysRevLett.96.032503
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
2006DU03 Phys.Rev. C 73, 014605 (2006) M.Dupuis, S.Karataglidis, E.Bauge, J.P.Delaroche, D.Gogny Correlations in microscopic optical model for nucleon elastic scattering off doubly closed-shell nuclei NUCLEAR STRUCTURE 16O, 40,48Ca, 208Pb; calculated neutron and proton radii. Hartree-Fock plus RPA approach, comparison with data. NUCLEAR REACTIONS 208Pb(polarized p, p), E=40-201 MeV; calculated σ(θ), Ay(θ); 16O, 40,48Ca(p, p), E ≈ 200 MeV; calculated σ(θ); deduced role of long-range correlations. Hartree-Fock plus RPA approach, comparison with data.
doi: 10.1103/PhysRevC.73.014605
2006KI17 Nucl.Phys. A779, 82 (2006) Y.J.Kim, K.Amos, S.Karataglidis Properties of effective interactions and the excitation of 6- states in 28Si NUCLEAR REACTIONS 28Si(p, p), (p, p'), E=80, 100, 134, 180 MeV; analyzed σ(θ), Ay(θ). 28Si levels deduced configurations, configuration mixing. Distorted wave analysis.
doi: 10.1016/j.nuclphysa.2006.09.005
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
2005AM11 Nucl.Phys. A762, 230 (2005) K.Amos, S.Karataglidis, Y.J.Kim Complementary reaction analyses and the isospin mixing of the 4- states in 16O NUCLEAR REACTIONS 16O(π+, π+'), (π-, π-'), (e, e'), E not given; analyzed σ(E, θ). 16O(p, p), (p, p'), E=135, 200 MeV; analyzed σ(θ), Ay(θ). 16O levels deduced isospin mixing, related features.
doi: 10.1016/j.nuclphysa.2005.08.015
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
2005DE32 Phys.Rev. C 72, 014608 (2005) P.K.Deb, B.C.Clark, S.Hama, K.Amos, S.Karataglidis, E.D.Cooper Comparison of optical model results from a microscopic Schrodinger approach to nucleon-nucleus elastic scattering with those from a global Dirac phenomenology NUCLEAR REACTIONS 12C, 16O, 40Ca, 90Zr, 208Pb(p, p), E=65, 200 MeV; calculated σ(θ), Ay(θ), other spin observables. 12C, 16O, 40Ca, 90Zr, 208Pb(p, X), (n, X), E=20-800 MeV; calculated total, reaction σ. Comparison of Dirac and Schrodinger approaches, comparison with data.
doi: 10.1103/PhysRevC.72.014608
2005KA21 Phys.Rev. C 71, 064601 (2005) S.Karataglidis, K.Amos, B.G.Giraud Local scale transformations and extended matter distributions in nuclei NUCLEAR REACTIONS 1H(6He, 6He), E=24.5, 40.9, 70.5 MeV/nucleon; 1H(8He, 8He), E=72 MeV/nucleon; 1H(11Li, 11Li), E=62 MeV/nucleon; 40Ca(p, p), E=65 MeV; calculated σ(θ). Local scale transformations to oscillator states. NUCLEAR STRUCTURE 6,8He, 11Li; calculated binding energies, radii, wave functions. Local scale transformations to oscillator states.
doi: 10.1103/PhysRevC.71.064601
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
2004AM11 Phys.Rev. C 70, 024607 (2004) K.Amos, S.Karataglidis, J.Dobaczewski Probing the densities of Sn isotopes NUCLEAR STRUCTURE 100,110,120,130,140,150,160,170Sn; calculated particle density distributions, radii, wave functions. HFB model, Skyrme interaction. NUCLEAR REACTIONS 100,102,104,106,108,110,110,112,114,116,118,120,122,124,126,128,130,132,134,136,138,140,142,144,146,148,150,152,154,156,158,160,162,164,166,168,170,172,174,176Sn(p, p), E=200 MeV; calculated σ, σ(θ). 116,118,120,122,124Sn(p, p), E=39.8, 65 MeV; calculated σ(θ), polarization observables. HFB model, Skyrme interaction.
doi: 10.1103/PhysRevC.70.024607
2004DE51 Phys.Rev. C 70, 057601 (2004) P.K.Deb, K.Amos, S.Karataglidis Simple functional form for the n + 208Pb total cross section between 5 and 600 MeV NUCLEAR REACTIONS 208Pb(n, X), E=5-600 MeV; analyzed total σ; deduced parameters, simple functional form; deduced Ramsauer effect.
doi: 10.1103/PhysRevC.70.057601
2004GI07 Phys.Rev. C 69, 064613 (2004) B.G.Giraud, S.Karataglidis, K.Amos, B.A.Robson Is "friction" responsible for the reduction of fusion rates far below the Coulomb barrier?
doi: 10.1103/PhysRevC.69.064613
2003KL05 Phys.Rev. C 67, 031601 (2003) J.Klug, J.Blomgren, A.Atac, B.Bergenwall, A.Hildebrand, C.Johansson, P.Mermod, L.Nilsson, S.Pomp, U.Tippawan, K.Elmgren, N.Olsson, O.Jonsson, A.V.Prokofiev, P.-U.Renberg, P.Nadel-Turonski, S.Dangtip, P.Phansuke, M.Osterlund, C.Le Brun, J.F.Lecolley, F.R.Lecolley, M.Louvel, N.Marie-Noury, C.Schweitzer, Ph.Eudes, F.Haddad, C.Lebrun, A.J.Koning, E.Bauge, J.P.Delaroche, M.Girod, X.Ledoux, P.Romain, D.G.Madland, K.Amos, P.K.Deb, S.Karataglidis, R.Crespo, A.M.Moro Elastic neutron scattering at 96 MeV from 12C and 208Pb NUCLEAR REACTIONS 12C, 208Pb(n, n), E=96 MeV; measured σ(θ). Comparison with model predictions.
doi: 10.1103/PhysRevC.67.031601
2002AM05 Phys.Rev. C65, 057603 (2002) Total Reaction Cross Sections for Neutron-Nucleus Scattering NUCLEAR REACTIONS 12C, 28Si, 56Fe, 90Zr, 208Pb(n, X), E=45-75 MeV; measured total reaction σ. Comparison with microscopic optical model predictions.
doi: 10.1103/PhysRevC.65.057603
2002AM06 Phys.Rev. C65, 064618 (2002) K.Amos, S.Karataglidis, P.K.Deb Predictions of Total and Total Reaction Cross Sections for Nucleon-Nucleus Scattering up to 300 MeV NUCLEAR REACTIONS 6Li, 9Be, 12C, 16O, 19F, 27Al, 40Ca, 63Cu, 90Zr, 118Sn, 140Ce, 159Tb, 181Ta, 197Au, 208Pb, 238U(p, X), E=0-300 MeV; 6Li, 12C, 19F, 40Ca, 89Y, 184W, 197Au, 208Pb, 238U(n, X), E=0-300 MeV; calculated reaction σ. Various potentials compared. Comparison with data.
doi: 10.1103/PhysRevC.65.064618
2002AM11 Acta Phys.Hung.N.S. 16, 327 (2002) Predictions of a Microscopic Model of p-A Scattering NUCLEAR REACTIONS 208Pb(n, n), (p, p), E=65 MeV; 1H(6He, 6He), (6He, 6He'), E=24.5, 40.9 MeV/nucleon; calculated σ(θ). 12C, 208Pb(n, X), (p, X), E=20-300 MeV; calculated reaction σ. Microscopic model, comparisons with data.
doi: 10.1556/APH.16.2002.1-4.35
2002KA22 Phys.Rev. C65, 044306 (2002) S.Karataglidis, K.Amos, B.A.Brown, P.K.Deb Discerning the Neutron Density Distribution of 208Pb from Nucleon Elastic Scattering NUCLEAR REACTIONS 40Ca, 208Pb(n, n), (p, p), E=40, 65, 200 MeV; analyzed σ(θ). 208Pb deduced neutron density distribution.
doi: 10.1103/PhysRevC.65.044306
2002ST28 Phys.Lett. 542B, 35 (2002) S.V.Stepantsov, D.D.Bogdanov, A.S.Fomichev, A.M.Rodin, S.I.Sidorchuk, R.S.Slepnev, G.M.Ter-Akopian, R.Wolski, M.L.Chelnokov, V.A.Gorshkov, Yu.Ts.Oganessian, N.Alamanos, F.Auger, V.Lapoux, G.Lobo, K.Amos, P.K.Deb, S.Karataglidis, M.S.Golovkov, A.A.Korsheninnikov, I.Tahihata, E.A.Kuzmin, E.Yu.Nikolskii, R.L.Kavalov 24.5 A MeV 6He + p Elastic and Inelastic Scattering NUCLEAR REACTIONS 1H(6He, 6He), (6He, 6He'), (6He, pX), (6He, αX), E=24.5 MeV; measured σ(θ), σ(E), excitation energy spectra. 6He deduced neutron halo features.
doi: 10.1016/S0370-2693(02)02308-0
2001BA17 Phys.Rev. C63, 035803 (2001) N.Bateman, K.Abe, G.Ball, L.Buchmann, J.Chow, J.M.D'Auria, Y.Fuchi, C.Iliadis, H.Ishiyama, K.P.Jackson, S.Karataglidis, S.Kato, S.Kubono, K.Kumagai, M.Kurokawa, X.Liu, S.Michimasa, P.Strasser, M.H.Tanaka Measurement of the 24Mg(p, t)22Mg Reaction and Implications for the 21Na(p, γ)22Mg Stellar Reaction Rate NUCLEAR REACTIONS 24Mg(p, t), E=37.925 MeV; measured particle spectra. 22Mg deduced levels, possible J, π. 21Na(p, γ), E not given; deduced astrophysical reaction rates. Shell model calculations.
doi: 10.1103/PhysRevC.63.035803
2001DE16 Phys.Rev.Lett. 86, 3248 (2001) P.K.Deb, K.Amos, S.Karataglidis, M.B.Chadwick, D.G.Madland Predicting Total Reaction Cross Sections for Nucleon-Nucleus Scattering NUCLEAR REACTIONS 12C, 208Pb(n, X), (p, X), E=0-300 MeV; calculated total reaction σ. Optical potential, comparisons with data.
doi: 10.1103/PhysRevLett.86.3248
2001KA58 Phys.Rev. C64, 064601 (2001) Microscopic Optical Potentials for Nucleon-Nucleus Scattering NUCLEAR REACTIONS 12C, 28Si, 40Ca, 56Fe, 90Zr(n, n), (p, p), E=65 MeV; calculated σ(θ), Ay(θ). 208Pb(n, X), E < 300 MeV; calculated total, reaction σ. Microscopic and phenomenological models compared. Comparisons with data.
doi: 10.1103/PhysRevC.64.064601
2001LA22 Phys.Lett. 518B, 27 (2001) A.Lagoyannis, F.Auger, A.Musumarra, N.Alamanos, E.C.Pollacco, A.Pakou, Y.Blumenfeld, F.Braga, M.La Commara, A.Drouart, G.Fioni, A.Gillibert, E.Khan, V.Lapoux, W.Mittig, S.Ottini-Hustache, D.Pierroutsakou, M.Romoli, P.Roussel-Chomaz, M.Sandoli, D.Santonocito, J.A.Scarpaci, J.L.Sida, T.Suomijarvi, S.Karataglidis, K.Amos Probing the 6He Halo Structure with Elastic and Inelastic Proton Scattering NUCLEAR REACTIONS 1H(6He, 6He), (6He, 6He'), E=40.9 MeV/nucleon; measured excitation energy spectra, σ(θ). 6He deduced halo features. Optical model analysis.
doi: 10.1016/S0370-2693(01)00887-5
2000DE43 Phys.Rev. C62, 037601 (2000) P.K.Deb, K.Amos, S.Karataglidis First Order Optical Potentials and 25 to 40 MeV Proton Elastic Scattering NUCLEAR REACTIONS 6He, 12C, 40Ca, 58Ni, 90Zr, 208Pb(p, p), E=25, 40 MeV; analyzed σ(θ), Ay(θ). Folded optical potentials.
doi: 10.1103/PhysRevC.62.037601
2000DE61 Aust.J.Phys. 53, 767 (2000) P.K.Deb, K.Amos, S.Karataglidis Microscopic Model Analyses of the Elastic Scattering of 25, 30 and 40 MeV Protons from Targets of Diverse Mass NUCLEAR REACTIONS 6,7Li, 12C, 14N, 18O, 24Mg, 27Al, 28Si, 40,48Ca, 58Cu, 88Sr, 89Y, 152Sm, 232Th, 238U(p, p), E=25 MeV; 10B, 13C, 16O, 20Ne, 40Ar, 56Fe, 58Ni, 63Cu, 66Zn, 90Zr, 120Sn, 139La, 144Sm, 176Yb, 208Pb, 209Bi(p, p), E=30 MeV; 6Li, 12C, 16O, 24Mg, 27Al, 28Si, 40Ca, 58Ni, 64Zn, 90Zr, 120Sn, 208Pb(p, p), E=40 MeV; calculated σ(θ), Ay(θ). Optical potential, comparison with data.
2000KA04 Phys.Rev. C61, 024319 (2000) S.Karataglidis, P.J.Dortmans, K.Amos, C.Bennhold Alternative Evaluations of Halos in Nuclei NUCLEAR REACTIONS 1H(6He, 6He), (8He, 8He), E=72 MeV/nucleon; 1H(9Li, 9Li), (11Li, 11Li), E=62 MeV/nucleon; 6Li(γ, π+), E=200 MeV; calculated σ(θ). 6,8He, 9,11Li deduced halo features. Microscopic folding model, comparison with data. NUCLEAR STRUCTURE 6,8He, 9,11Li; calculated levels, J, π, radii, neutron density profiles. Shell model, comparison with data.
doi: 10.1103/PhysRevC.61.024319
1998DO07 Phys.Rev. C57, 2433 (1998) P.J.Dortmans, K.Amos, S.Karataglidis Predictions of the Scattering of 200 and 300 MeV Polarized Protons from Polarized 3He NUCLEAR REACTIONS 3He(polarized p, p), E=200, 300 MeV; calculated σ(θ), A(y)(θ), other polarization observables. Polarized target. Microscopic model, comparison with data.
doi: 10.1103/PhysRevC.57.2433
1998DO16 Phys.Rev. C58, 2249 (1998) P.J.Dortmans, K.Amos, S.Karataglidis, J.Raynal Microscopic Model Analyses of the Elastic Scattering of 65 MeV Protons from Targets of Diverse Mass NUCLEAR REACTIONS 6,7,9,11Li, 11B, 12C, 16O, 20Ne, 24Mg, 28Si, 32S, 40Ar, 40,42,44,48Ca, 46,48,50Ti, 52Cr, 54,56Fe, 59Co, 89Y, 90Zr, 98,100Mo, 118Sn, 144,152,154Sm, 160Gd, 164Dy, 166,168Er, 174,176Yb, 178,180Hf, 182,184W, 192Os, 208Pb, 209Bi, 232Th, 238U(polarized p, p), E=65 MeV; calculated σ(θ), Ay(θ). Comparison with data. Nonlocal coordinate space optical potentials.
doi: 10.1103/PhysRevC.58.2249
1998JE04 Phys.Rev. C58, 579 (1998) B.K.Jennings, S.Karataglidis, T.D.Shoppa Direct Capture Astrophysical S Factors at Low Energy NUCLEAR REACTIONS 16O(p, γ), E < 3 MeV; 7Be(p, γ), E < 0.4 MeV; calculated astrophysical S-factors; deduced low-energy behaviour mechanism.
doi: 10.1103/PhysRevC.58.579
1998JE10 Phys.Rev. C58, 3002 (1998) Seff and the 7Be(p, γ)8B Reaction NUCLEAR REACTIONS 7Be(p, γ), E ≈ 20 keV; calculated effective S-factor using various approximations.
doi: 10.1103/PhysRevC.58.3002
1998JE11 Phys.Rev. C58, 3711 (1998) B.K.Jennings, S.Karataglidis, T.D.Shoppa Extrapolation of the Astrophysical S Factor for 7Be(p, γ)8B to Solar Energies NUCLEAR REACTIONS 7Be(p, γ), E < 3 MeV; calculated astrophysical S-factor; deduced high-energy extrapolation model dependence. Comparisons with data.
doi: 10.1103/PhysRevC.58.3711
1998KA06 Phys.Rev.Lett. 80, 1614 (1998) Probing Proton Halos Through Pion Photoproduction NUCLEAR REACTIONS 17O(γ, π-), E=200 MeV; calculated σ(θ); deduced 17F proton halo dependence.
doi: 10.1103/PhysRevLett.80.1614
1998ST07 Phys.Rev. C57, 1817 (1998) G.F.Steyn, S.V.Fortsch, A.A.Cowley, S.Karataglidis, R.Lindsay, J.J.Lawrie, F.D.Smit, R.T.Newman Single-Nucleon Transfer to Unbound States in the 4He(α, t)5Li Reaction at Incident Energies of 120, 160, and 200 MeV NUCLEAR REACTIONS 4He(α, t), E=120, 160, 200 MeV; measured σ(Et, θ); deduced cluster-core potential parameters. Comparison with 4He(α, 3He) results.
doi: 10.1103/PhysRevC.57.1817
1997DO01 J.Phys.(London) G23, 183 (1997) P.J.Dortmans, K.Amos, S.Karataglidis Fully Microscopic Model Analyses of the Elastic Scattering of 200 MeV Protons from Targets of Diverse Mass NUCLEAR REACTIONS 6,7Li, 9Be, 10B, 12,13C, 27Al, 28Si, 16O, 20Ne, 40,42,44,48Ca, 56Fe, 58Ni, 88Sr, 90Zr, 115In, 120Sn, 197Au, 208Pb(polarized p, p), E=200 MeV; analyzed σ(θ), polarization observables data. Microscopic model.
doi: 10.1088/0954-3899/23/2/006
1997DO02 Phys.Rev. C55, 2723 (1997) P.J.Dortmans, K.Amos, S.Karataglidis Microscopic Model Analyses of Select Scattering of 135 MeV Protons from 12C NUCLEAR REACTIONS 12C(p, p), (p, p'), E=135 MeV; calculated σ(θ); deduced model limitations. Microscopic model analyses.
doi: 10.1103/PhysRevC.55.2723
1997KA24 Phys.Rev. C55, 2826 (1997) S.Karataglidis, B.A.Brown, K.Amos, P.J.Dortmans Shell Model Structures of Low-Lying Excited States in 6,7Li NUCLEAR REACTIONS 6,7Li(polarized p, p), (polarized p, p'), E=200 MeV; analyzed σ(θ), polarizing power vs θ. 6,7Li(e, e), (e, e'), E not given; calculated form factors. 6,7Li level deduced B(λ). Shell model calculations.
doi: 10.1103/PhysRevC.55.2826
1997KA42 Phys.Rev.Lett. 79, 1447 (1997) S.Karataglidis, P.G.Hansen, B.A.Brown, K.Amos, P.J.Dortmans Is There an Excited State in 11Li at E(x) = 1.3 MeV ( Question ) NUCLEAR REACTIONS 11Li(p, p), E=60, 68 MeV; 9Li(p, p), E=62 MeV; 11Li(p, p'), E=68 MeV; analyzed σ(θ); deduced nuclear shakoff mechanism role. 11Li deduced no compelling evidence for 1.3 MeV level.
doi: 10.1103/PhysRevLett.79.1447
1996CS05 Nucl.Phys. A607, 62 (1996); Erratum Nucl.Phys. A609, 601 (1996) Low-Energy M1 Strength in the 7Li(p, γ0)8Be Reaction NUCLEAR REACTIONS, ICPND 7Li(p, γ), E(cm) ≤ 1.1 MeV; calculated astrophysical S-factor vs E. 8Be levels deduced spectroscopic amplitudes, M1 strength distribution. Microscopic cluster model.
doi: 10.1016/S0375-9474(96)00229-1
1996KA01 Phys.Rev. C53, 838 (1996) S.Karataglidis, P.J.Dortmans, K.Amos, R.de Swiniarski Multi-(h-bar)ω Shell Model Analyses of Elastic and Inelastic Proton Scattering from 14N and 16O NUCLEAR REACTIONS 14N, 16O(e, e), 16O(e, e'), E not given; calculated form factors. 12C(polarized p, p), (polarized p, p'), E=160 MeV; 14N(polarized p, p), (polarized p, p'), E=160 MeV; 16O(polarized p, p), (polarized p, p'), E=200 MeV; calculated σ(θ), analyzing power vs θ. Microscopic DWA, large space shell model wave functions.
doi: 10.1103/PhysRevC.53.838
1996KA29 Phys.Rev. C54, 1863 (1996) S.Karataglidis, K.Amos, C.Bennhold, L.Tiator Large Basis Shell Model Analysis of 14N(γ, π+)14C(g.s) Reaction NUCLEAR REACTIONS 14N(γ, π+), E=173 MeV; calculated σ(θ); deduced need for improved elementary pion production process. Shell model wave functions.
doi: 10.1103/PhysRevC.54.1863
1996KA65 Aust.J.Phys. 49, 645 (1996) S.Karataglidis, P.J.Dortmans, K.Amos, R.de Swiniarski Inelastic Proton Scattering Analyses and Ambiguities in Spin-Parity Assignments of States in 12C NUCLEAR REACTIONS 12C(polarized p, p'), E=200, 398 MeV; analyzed σ(θ, Ep'), A(y)(θ, Ep'). 12C deduced levels probable J, π. Fully microscopic distorted wave approximation.
doi: 10.1071/PH960645
1995DO31 Phys.Rev. C52, 3224 (1995) P.J.Dortmans, S.Karataglidis, K.Amos, R.de Swiniarski Fully Microscopic Model Analysis of the Elastic and Inelastic Scattering of Protons from 12C and for Energies in the Range 200 to 800 MeV NUCLEAR REACTIONS 12C(polarized p, p), (polarized p, p'), E=200-800 MeV; calculated σ(θ), analyzing power vs θ. DWA, medium modified effective two nucleon interactions.
doi: 10.1103/PhysRevC.52.3224
1995KA14 Phys.Rev. C51, 2494 (1995) S.Karataglidis, P.Halse, K.Amos Transverse Electric Form Factors for Electron Scattering and Violation of Current Conservation in Nuclear Models NUCLEAR REACTIONS 12C, 20Ne, 24Mg, 28Si(e, e), E not given; calculated transverse electric form factors. Projected Hartree-Fock transition densities, shell model.
doi: 10.1103/PhysRevC.51.2494
1995KA24 Phys.Rev. C52, 861 (1995) S.Karataglidis, P.J.Dortmans, K.Amos, R.de Swiniarski Fully Microscopic Model of 200 MeV Proton-12C Elastic and Inelastic Scattering NUCLEAR REACTIONS 12C(polarized p, p), (polarized p, p'), E=200 MeV; calculated σ(θ), analyzing power vs θ. 12C(e, e), (e, e'), E not given; calculated form factors. Fully microscopic model, realistic effective NN-interaction from Brueckner-Bethe-Goldstone equations.
doi: 10.1103/PhysRevC.52.861
1992SI01 Phys.Rev. C45, 479 (1992) D.A.Sims, S.Karataglidis, G.J.O'Keefe, R.P.Rassool, A.D.Bates, M.N.Thompson, S.Ito, H.Matsuyama, S.Sazaki, O.Konno, T.Terasawa, T.Suda, K.Maeda Comment on the Need to Introduce a T = 1 Quasideuteron NUCLEAR REACTIONS 16O(γ, p), E=42.6-50.2 MeV; measured proton missing energy; analyzed other data on 12C, 40Ca; deduced T=1, quasideuteron or admixed target ground states implications. 15N levels deduced population relative to 6.33 MeV state. Tagged photon beam.
doi: 10.1103/PhysRevC.45.479
1989KA30 Nucl.Phys. A501, 108 (1989) S.Karataglidis, D.Zubanov, P.D.Harty, M.N.Thompson The 7Li(γ, n0)6Li Cross Section Near Threshold NUCLEAR REACTIONS 7Li(γ, n), E=7-9 MeV; measured bremsstrahlung yield; deduced σ(E), solar neutrino implications. Enriched target.
doi: 10.1016/0375-9474(89)90567-8
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