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NSR database version of April 11, 2024.

Search: Author = S.Karataglidis

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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
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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
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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
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2020KA33      Phys.Rev. C 101, 064316 (2020)

S.Karataglidis, K.Murulane

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
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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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2017KA20      Eur.Phys.J. A 53, 70 (2017)

S.Karataglidis

Electron scattering and reactions from exotic nuclei

doi: 10.1140/epja/i2017-12277-6
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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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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
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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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2014GI09      Phys.Scr. 89, 054009 (2014)

B.G.Giraud, S.Karataglidis

Symmetries and fluctuations in the nuclear density functional

doi: 10.1088/0031-8949/89/5/054009
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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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2013KA21      Phys.Rev. C 87, 054623 (2013)

S.Karataglidis, K.Amos

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
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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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2012FA13      Phys.Rev. C 86, 064606 (2012)

W.R.Falk, S.Karataglidis

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
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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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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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetE2287.


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
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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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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
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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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetE2287.


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
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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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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
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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
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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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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
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2007KA50      Phys.Lett. B 650, 148 (2007)

S.Karataglidis, K.Amos

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
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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
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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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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
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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
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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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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
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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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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
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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
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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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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
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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
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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
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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
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2002AM05      Phys.Rev. C65, 057603 (2002)

K.Amos, S.Karataglidis

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
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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
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2002AM11      Acta Phys.Hung.N.S. 16, 327 (2002)

K.Amos, S.Karataglidis

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
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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
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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
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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
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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
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2001KA58      Phys.Rev. C64, 064601 (2001)

S.Karataglidis, M.B.Chadwick

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
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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
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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
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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
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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
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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
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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
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1998JE10      Phys.Rev. C58, 3002 (1998)

B.K.Jennings, S.Karataglidis

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
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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
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1998KA06      Phys.Rev.Lett. 80, 1614 (1998)

S.Karataglidis, C.Bennhold

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
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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
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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
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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
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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
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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
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1996CS05      Nucl.Phys. A607, 62 (1996); Erratum Nucl.Phys. A609, 601 (1996)

A.Csoto, S.Karataglidis

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
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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
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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
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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
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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
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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
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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
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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
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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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