NSR Query Results
Output year order : Descending NSR database version of April 11, 2024. Search: Author = I.J.Thompson Found 195 matches. Showing 1 to 100. [Next]2023HE08 J.Phys.(London) G50, 060501 (2023) C.Hebborn, F.M.Nunes, G.Potel, W.H.Dickhoff, J.W.Holt, M.C.Atkinson, R.B.Baker, C.Barbieri, G.Blanchon, M.Burrows, R.Capote, P.Danielewicz, M.Dupuis, C.Elster, J.E.Escher, L.Hlophe, A.Idini, H.Jayatissa, B.P.Kay, K.Kravvaris, J.J.Manfredi, A.Mercenne, B.Morillon, G.Perdikakis, C.D.Pruitt, G.H.Sargsyan, I.J.Thompson, M.Vorabbi, T.R.Whitehead Optical potentials for the rare-isotope beam era
doi: 10.1088/1361-6471/acc348
2021HO15 Phys.Lett. B 822, 136710 (2021) M.Holl, R.Kanungo, Z.H.Sun, G.Hagen, J.A.Lay, A.M.Moro, P.Navratil, T.Papenbrock, M.Alcorta, D.Connolly, B.Davids, A.Diaz Varela, M.Gennari, G.Hackman, J.Henderson, S.Ishimoto, A.I.Kilic, R.Krucken, A.Lennarz, J.Liang, J.Measures, W.Mittig, O.Paetkau, A.Psaltis, S.Quaglioni, J.S.Randhawa, J.Smallcombe, I.J.Thompson, M.Vorabbi, M.Williams Proton inelastic scattering reveals deformation in 8He NUCLEAR REACTIONS 1H(8He, p), E=8.25 MeV/nucleon; measured reaction products, Ep, Ip. 8He; deduced σ(θ), resonance parameters, first 2+ state, quadrupole deformation parameter. Comparison with no-core shell model predictions. Charged particle spectroscopy station IRIS at TRIUMF in Canada.
doi: 10.1016/j.physletb.2021.136710
2020DE12 Phys.Rev. C 101, 045802 (2020) R.J.deBoer, C.R.Brune, M.Febrarro, J.Gorres, I.J.Thompson, M.Wiescher Sensitivity of the 13C(α, n)16O S factor to the uncertainty in the level parameters of the near-threshold state NUCLEAR REACTIONS 13C(α, n)16O, E(cm)<1.2 MeV; calculated astrophysical S factors and reaction rates by R-matrix theory using the AZURE2 code for different sets of level parameters for the near-threshold 1/2+ resonance at 6356 keV in 17O; analyzed theory and available experimental data to investigate the sensitivity of the low-energy extrapolation to the associated uncertainties and discrepancies. Relevance to s process in asymptotic giant branch (AGB) stars and i process in carbon-enhanced metal-poor (CEMP) stars.
doi: 10.1103/PhysRevC.101.045802
2019RA06 Phys.Rev. C 99, 021301 (2019) J.S.Randhawa, R.Kanungo, M.Holl, J.D.Holt, P.Navratil, S.R.Stroberg, G.Hagen, G.R.Jansen, M.Alcorta, C.Andreoiu, C.Barnes, C.Burbadge, D.Burke, A.A.Chen, A.Chester, G.Christian, S.Cruz, B.Davids, J.Even, G.Hackman, J.Henderson, S.Ishimoto, P.Jassal, S.Kaur, M.Keefe, D.Kisliuk, R.Krucken, J.Liang, J.Lighthall, E.McGee, J.Measures, M.Moukaddam, E.Padilla-Rodal, A.Shotter, I.J.Thompson, J.Turko, M.Williams, O.Workman Observation of excited states in 20Mg sheds light on nuclear forces and shell evolution NUCLEAR REACTIONS 2H(20Mg, d), (20Mg, d'), E=8.5 MeV/nucleon, [secondary 20Mg beam produced in Si(p, X), E=480 MeV fragmentation reaction using SiC target at ISAC-II facility]; measured scattered deuteron spectra, differential σ(θ) using annular single-sided silicon strip detector array and CsI(Tl) detectors (IRIS reaction spectroscopy facility) at TRIUMF. 20Mg; deduced levels, J, π, proton-unbound resonances. Comparison with ab initio calculations using the valence-space in-medium similarity renormalization-group (VS-IMSRG) approach.
doi: 10.1103/PhysRevC.99.021301
2019TH03 Eur.Phys.J. A 55, 92 (2019) I.J.Thompson, R.J.deBoer, P.Dimitriou, S.Kunieda, M.T.Pigni, G.Arbanas, H.Leeb, T.Srdinko, G.Hale, P.Tamagno, P.Archier Verification of R-matrix calculations for charged-particle reactions in the resolved resonance region for the 7Be system NUCLEAR REACTIONS 4He(3He, 3He)4He; 6Li(p, α0)3He; 6Li(p, p0)6Li, E* below 8 MeV; calculated σ using different R-code algorithms; compared results and possibilities both for total σ and for the individual l-waves.
doi: 10.1140/epja/i2019-12753-y
2017LO03 Phys.Rev. C 95, 034605 (2017) A.E.Lovell, F.M.Nunes, I.J.Thompson Three-body model for the two-neutron emission of 16Be RADIOACTIVITY 16Be(2n); calculated resonance energy, phase shifts, and density distributions. Three-body calculation in the continuum using hyperspherical harmonics and the R-matrix method with n-14Be interactions for dineutron emission.
doi: 10.1103/PhysRevC.95.034605
2016SA13 Phys.Lett. B 755, 481 (2016) A.Sanetullaev, R.Kanungo, J.Tanaka, M.Alcorta, C.Andreoiu, P.Bender, A.A.Chen, G.Christian, B.Davids, J.Fallis, J.P.Fortin, N.Galinski, A.T.Gallant, P.E.Garrett, G.Hackman, B.Hadinia, S.Ishimoto, M.Keefe, R.Krucken, J.Lighthall, E.McNeice, D.Miller, J.Purcell, J.S.Randhawa, T.Roger, A.Rojas, H.Savajols, A.Shotter, I.Tanihata, I.J.Thompson, C.Unsworth, P.Voss, Z.Wang Investigation of the role of 10Li resonances in the halo structure of 11Li(p, d)10Li through the transfer reaction NUCLEAR REACTIONS 1H(11Li, d), (11Li, p), E=5.7 MeV/nucleon; measured reaction products; deduced resonance parameters, spectroscopic factor, σ(θ). DWBA analysis.
doi: 10.1016/j.physletb.2016.02.060
2015GO13 Phys.Rev. C 92, 014613 (2015) M.Gomez-Ramos, A.M.Moro, J.Gomez-Camacho, I.J.Thompson Transfer induced by core excitation within an extended distorted-wave Born approximation method NUCLEAR REACTIONS 10Be(d, p)11Be, E=21.4 MeV; 30Ne(d, p)31Ne, E=30 MeV; calculated spectroscopic factors for 11Be, σ(θ) for ground and excited states of 11Be and 31Ne, cross sections excluding and including prompt core-excitation (PCE) effects. Extended distorted-wave Born approximation (DWBA) formalism. Comparison with available experimental data.
doi: 10.1103/PhysRevC.92.014613
2015KA15 Phys.Rev.Lett. 114, 192502 (2015) R.Kanungo, A.Sanetullaev, J.Tanaka, S.Ishimoto, G.Hagen, T.Myo, T.Suzuki, C.Andreoiu, P.Bender, A.A.Chen, B.Davids, J.Fallis, J.P.Fortin, N.Galinski, A.T.Gallant, P.E.Garrett, G.Hackman, B.Hadinia, G.Jansen, M.Keefe, R.Krucken, J.Lighthall, E.McNeice, D.Miller, T.Otsuka, J.Purcell, J.S.Randhawa, T.Roger, A.Rojas, H.Savajols, A.Shotter, I.Tanihata, I.J.Thompson, C.Unsworth, P.Voss, Z.Wang Evidence of Soft Dipole Resonance in 11Li with Isoscalar Character NUCLEAR REACTIONS 2H(11Li, X)7Li/8Li/9Li/10Li/11Li, E=5.5 MeV/nucleon; measured reaction products. 11Li; deduced yields, σ(θ), excitation energy, soft dipole resonance. Comparison with ab initio calculations in the coupled cluster framework.
doi: 10.1103/PhysRevLett.114.192502
2015OT02 Phys.Rev. C 92, 054603 (2015) S.Ota, J.T.Burke, R.J.Casperson, J.E.Escher, R.O.Hughes, J.J.Ressler, N.D.Scielzo, I.J.Thompson, R.A.E.Austin, B.Abromeit, N.J.Foley, E.McCleskey, M.McCleskey, H.I.Park, A.Saastamoinen, T.J.Ross Spin differences in the 90Zr compound nucleus induced by (p, p'), (p, d), and (p, t) surrogate reactions NUCLEAR REACTIONS 90Zr(p, p'), (p, np), 91Zr(p, d), 92Zr(p, t), E=28.56 MeV; measured light-ion particle spectra, angular distributions, Eγ, Iγ, (particle)γ-coin, using STARLiTeR detector system at Texas A and M cyclotron facility; deduced γ-decay probabilities as functions of 90Zr excitation energy, angular momentum, and particle scattering angle. Enriched targets. 89,90Zr; deduced levels, J, π. 89Zr(n, γ); discussed relevance to determination of σ by surrogate reaction approach.
doi: 10.1103/PhysRevC.92.054603
2015PO07 Phys.Rev. C 92, 034611 (2015) G.Potel, F.M.Nunes, I.J.Thompson Establishing a theory for deuteron-induced surrogate reactions NUCLEAR REACTIONS 93Nb(d, p), E=15, 25 MeV; calculated energy distributions of the detected protons, and total σ(E) as function of proton energy for elastic breakup and inelastic processes. Post- and prior-form distorted wave Born approximation formalism. Surrogate reaction for neutron capture into compound states. Comparison with experimental data.
doi: 10.1103/PhysRevC.92.034611
2014AD07 Phys.Rev. C 89, 044618 (2014) S.Adhikari, C.Basu, I.J.Thompson, P.Sugathan, A.Jhinghan, K.S.Golda, A.Babu, D.Singh, S.Ray, A.K.Mitra Observation of a breakup-induced α-transfer process for some bound states of 16O populated by the 12C6Li, d)16O* reaction NUCLEAR REACTIONS 12C(6Li, d)16O*, E=20 MeV; measured deuteron spectra, σ(θ) at 15UD Pelletron facility of IUAC. 16O; deduced levels, α-unbound states, J, π, spectroscopic amplitudes, S(α) spectroscopic factors. 12C(α, γ); deduced astrophysical E2 S factor. Comparison with R-matrix FR-DWBA, Hauser-Feshbach, and Continuum discretized coupled-channel coupled reaction channel (CDCC-CRC) calculations with and without the inclusion of the breakup of 6Li. Comparison with previous experimental results.
doi: 10.1103/PhysRevC.89.044618
2014CA36 Phys.Rev. C 90, 044304 (2014); Pub.Note Phys.Rev. C 94, 069903 (2016) J.Casal, M.Rodriguez-Gallardo, J.M.Arias, I.J.Thompson Astrophysical reaction rate for 9Be formation within a three-body approach NUCLEAR STRUCTURE 9Be; calculated ground-state energy, matter and charge radii, sum rule ST(E1) using α+α+n three body approach and analytical transformed harmonic oscillator method for 9Be Borromean nucleus. NUCLEAR REACTIONS 8Be(n, γ)9Be; calculated photodissociation σ(E)for α+α+n --> 9Be+γ reaction, reaction rate dependence on temperature, contribution of resonances to total photodissociation cross section, total astrophysical reaction rates using α+α+n three body approach and analytical transformed harmonic oscillator method. Comparison with experimental results.
doi: 10.1103/PhysRevC.90.044304
2014ES03 Phys.Rev. C 89, 054605 (2014) J.E.Escher, I.J.Thompson, G.Arbanas, Ch.Elster, V.Eremenko, L.Hlophe, F.M.Nunes Reexamining surface-integral formulations for one-nucleon transfers to bound and resonance states NUCLEAR REACTIONS 90Zr(d, p), E=11 MeV; 48Ca(d, p), E=13, 19.3, 56 MeV; 20O(d, p), E=21 MeV; calculated σ(θ, E), interior, surface, and exterior contributions to the transfer reaction for bound states and resonances. Improvements to surface-integral approach. R-matrix theory, and finite range distorted-wave Born approximation (DWBA) calculations using reaction code FRESCO. Comparison with experimental data.
doi: 10.1103/PhysRevC.89.054605
2014HL01 Phys.Rev. C 90, 061602 (2014) L.Hlophe, V.Eremenko, Ch.Elster, F.M.Nunes, G.Arbanas, J.E.Escher, I.J.Thompson, for the TORUS Collaboration Separable representation of proton-nucleus optical potentials NUCLEAR REACTIONS 12C, 48Ca(p, p), E=38 MeV; 208Pb(p, p), E=45 MeV; calculated S-matrix elements and σ(θ); deduced effects of the short-range Coulomb potential on the proton-nucleus form factor. Comparison with coordinate space calculations. Generalization of the Ernst-Shakin-Thaler (EST) scheme.
doi: 10.1103/PhysRevC.90.061602
2014HU12 Phys.Rev. C 90, 014304 (2014) R.O.Hughes, C.W.Beausang, T.J.Ross, J.T.Burke, R.J.Casperson, N.Cooper, J.E.Escher, K.Gell, E.Good, P.Humby, M.McCleskey, A.Saastimoinen, T.D.Tarlow, I.J.Thompson 236Pu(n, f), 237Pu(n, f), and 238Pu(n, f) cross sections deduced from (p, t), (p, d), and (p, p') surrogate reactions NUCLEAR REACTIONS 235U, 239Pu(p, t), (p, d), (p, p'), E=28.5 MeV; measured particle and γ spectra, (particle)γ-, (particle)(particle)-, (d)(fission)-coin, cross sections using STARLiTeR array at Texas A-M cyclotron facility. 232,233U, 236,237Pu(n, F), E=0.5-7.5 MeV; deduced σ(E) ratios. 238Pu(n, F), E=0.5-10.5 MeV; deduced σ(E) from (p, p') and σ for 234U(n, F) in ENDF/B-VII evaluation. Surrogate ratio method. Comparison with ENSDF/B-VII evaluations, and some previous experimental results.
doi: 10.1103/PhysRevC.90.014304
2014KW03 Phys.Lett. B 732, 210 (2014) E.Kwan, C.Y.Wu, N.C.Summers, G.Hackman, T.E.Drake, C.Andreoiu, R.Ashley, G.C.Ball, P.C.Bender, A.J.Boston, H.C.Boston, A.Chester, A.Close, D.Cline, D.S.Cross, R.Dunlop, A.Finlay, A.B.Garnsworthy, A.B.Hayes, A.T.Laffoley, T.Nano, P.Navratil, C.J.Pearson, J.Pore, S.Quaglioni, C.E.Svensson, K.Starosta, I.J.Thompson, P.Voss, S.J.Williams, Z.M.Wang Precision measurement of the electromagnetic dipole strengths in 11Be NUCLEAR REACTIONS 196Pt(11Be, 11Be'), E=1.73, 2.09 MeV/nucleon;measured reaction products, Eγ, Iγ. 11Be; deduced yields, B(E1). Comparison with FRESCO code calculations.
doi: 10.1016/j.physletb.2014.03.049
2014MC03 Phys.Rev. C 89, 044605 (2014) M.McCleskey, A.M.Mukhamedzhanov, L.Trache, R.E.Tribble, A.Banu, V.Eremenko, V.Z.Goldberg, Y.-W.Lui, E.McCleskey, B.T.Roeder, A.Spiridon, F.Carstoiu, V.Burjan, Z.Hons, I.J.Thompson Determination of the asymptotic normalization coefficients for 14C + n ←→ 15C, the (+14)C(n, γ)15C reaction rate, and evaluation of a new method to determine spectroscopic factors NUCLEAR REACTIONS 13C(14C, 14C), (14C, 15C)12C, E=12 MeV/nucleon; 2H(14C, p)15C, E=11.7 MeV/nucleon; 14C(d, p), E=60 MeV; measured particle spectra, σ(θ) using MDM spectrometer at Texas A-M Cyclotron Institute. 15C; deduced levels, asymptotic normalization coefficient (ANC) and spectroscopic factors for g.s. and first excited state. 13C, 17O; population of g.s. in both and excited levels in 13C. DWBA analysis with Woods-Saxon and doublefolding (DF) potentials for 13C+14C reaction. FRESCO code and adiabatic distorted wave approximation (ADWA) used for analysis of σ(θ) data in 2H+14C reactions. 15C, 15F; analyzed mirror analogy for spectroscopic factors. Deuteron stripping theory. 14C(n, γ), E=10 keV-1 MeV; deduced astrophysical direct-capture rate σ(E) to g.s. and first excited state using RADCAP code and ANCs from the present work. Comparison with previous experimental results.
doi: 10.1103/PhysRevC.89.044605
2014TH05 Nucl.Data Sheets 118, 292 (2014) I.J.Thompson, J.E.Escher, G.Arbanas Coupled-Channel Models of Direct-Semidirect Capture via Giant-Dipole Resonances NUCLEAR REACTIONS 208Pb(n, γ), E=1-20 MeV; calculated capture σ using second-order DWBA implemented in FRESSCO and in CUPIDO codes. Compared with data. 130Sn(n, γ), E=0.01-6 MeV; calculated direct-semidirect σ using CUPIDO code with phenomenological optical model potential. Compared with other calculations.
doi: 10.1016/j.nds.2014.04.061
2014TH06 Nucl.Data Sheets 118, 298 (2014) Coupled-channel Treatment of Isobaric Analog Resonances in (p, p') Capture Processes NUCLEAR REACTIONS 208Pb(p, p'γ), E=12-20 MeV; calculated proton inelastic σ to specified state, IAR neutron bound state using CC code FRESCO.
doi: 10.1016/j.nds.2014.04.063
2014UP02 Phys.Rev. C 90, 014615 (2014) N.J.Upadhyay, V.Eremenko, L.Hlophe, F.M.Nunes, Ch.Elster, G.Arbanas, J.E.Escher, I.J.Thompson Coulomb problem in momentum space without screening NUCLEAR REACTIONS 2H(12C, p), E(cm)=30 MeV; 2H(48Ca, p), E(cm)=36 MeV; 2H(208Pb, p), E(cm)=36, 39 MeV; calculated Coulomb-distorted form factors for (d, p) reactions and dependence on charge, angular momentum, and energy. Regularization techniques using a separable interaction derived from realistic nucleon-nucleus optical potential
doi: 10.1103/PhysRevC.90.014615
2013AL09 Phys.Lett. B 721, 224 (2013) H.Al Falou, R.Kanungo, C.Andreoiu, D.S.Cross, B.Davids, M.Djongolov, A.T.Gallant, N.Galinski, D.Howell, R.Kshetri, D.Niamir, J.N.Orce, A.C.Shotter, S.Sjue, I.Tanihata, I.J.Thompson, S.Triambak, M.Uchida, P.Walden, R.B.Wiringa Inelastic scattering of 9Li and excitation mechanism of its first excited state NUCLEAR REACTIONS C, 2H(9Li, 8Li), (9Li, X), (9Li, 9Li), E=5 MeV/nucleon; measured reaction products. 9Li; deduced σ(θ), quadrupole deformation parameter, B(E2). DWUCK4, FRESCO calculations, comparison with available data.
doi: 10.1016/j.physletb.2013.03.018
2013GU02 Phys.Rev. C 87, 012801 (2013) M.Gulino, C.Spitaleri, X.D.Tang, G.L.Guardo, L.Lamia, S.Cherubini, B.Bucher, V.Burjan, M.Couder, P.Davies, R.deBoer, X.Fang, V.Z.Goldberg, Z.Hons, V.Kroha, L.Lamm, M.La Cognata, C.Li, C.Ma, J.Mrazek, A.M.Mukhamedzhanov, M.Notani, S.O'Brien, R.G.Pizzone, G.G.Rapisarda, D.Roberson, M.L.Sergi, W.Tan, I.J.Thompson, M.Wiescher Suppression of the centrifugal barrier effects in the off-energy-shell neutron + 17O interaction NUCLEAR REACTIONS 2H(17O, α14C), E=41, 43.5 MeV; measured α and 14C particle spectra, (14C)α-coin, angular distributions, yields using position-sensitive silicon detectors (PSD) at LNS, Catania, and at NSL, Notre Dame. CD2 target; deduced momentum distributions, Q value. DWBA analysis. 17O(n, α)14C, E(cm)=0-350 keV; deduced yields, angular distributions, neutron from quasifree breakup of deuteron. 18O; deduced resonances, J, π, and excitation functions. Trojan Horse method (THM), and suppression of centrifugal barrier. Comparison with previous studies. Relevance to neutron-induced reactions in nuclear reactors, and nucleosynthesis in astrophysics.
doi: 10.1103/PhysRevC.87.012801
2013HL01 Phys.Rev. C 88, 064608 (2013) L.Hlophe, Ch.Elster, R.C.Johnson, N.J.Upadhyay, F.M.Nunes, G.Arbanas, V.Eremenko, J.E.Escher, I.J.Thompson Separable representation of phenomenological optical potentials of Woods-Saxon type NUCLEAR REACTIONS 48Ca, 132Sn, 208Pb(n, X), E=0-50 MeV; calculated partial wave S matrices, separable representations of two-body transition matrix elements and potentials. Ernst-Shakin-Thaler (EST) scheme with CH89 potential.
doi: 10.1103/PhysRevC.88.064608
2013HO15 Phys.Rev. C 88, 025804 (2013) D.Howell, B.Davids, J.P.Greene, R.Kanungo, S.Mythili, C.Ruiz, G.Ruprecht, I.J.Thompson First determination of the 8Li valence neutron asymptotic normalization coefficient using the 7Li(8Li, 7Li)8Li reaction NUCLEAR REACTIONS 7Li(8Li, 7Li)8Li, E=11 MeV; measured 8Li particle spectra, (7Li)(8Li)-coin, σ(θ) using TUDA array at ISAC-TRIUMF. 8Li; deduced valence neutron asymptotic normalization coefficient (ANC) using DWBA analysis. 8B; deduced valence proton ANC from isospin asymmetry. 7Be (p, γ)8B; deduced astrophysical S-factor (S17(0)). Comparison with previous data.
doi: 10.1103/PhysRevC.88.025804
2013NG01 Phys.Rev. C 87, 054615 (2013) N.B.Nguyen, F.M.Nunes, I.J.Thompson Investigation of the triple-α reaction in a full three-body approach NUCLEAR STRUCTURE 12C; calculated triple-α reaction rates at temperature T<0.1 GK, binding energies, density distributions, and rms radius of first 2+ and second 0+ states, quadrupole transition strength as function of three-α kinetic energy. Three-body Borromean system. Combination of the R-matrix expansion and R-matrix propagation in hyperspherical harmonics (HH) method. Long-range Coulomb effects. Comparison with NACRE, the CDCC, and the three-body Breit Wigner calculations.
doi: 10.1103/PhysRevC.87.054615
2012DI07 Phys.Rev. C 85, 044611 (2012) F.S.Dietrich, I.J.Thompson, T.Kawano Target-state dependence of cross sections for reactions on statically deformed nuclei NUCLEAR REACTIONS 233,235,238U, 239Pu, 165Ho, 169Tm, 170Yb, 20Ne(n, X), E<20 MeV; calculated compound nucleus formation cross section for ground and excited states of different K quantum numbers, cross section ratios for adiabatic to nonadiabatic approximations. Coupled-channels calculations. Application to transmission coefficients in Hauser-Feshbach calculations.
doi: 10.1103/PhysRevC.85.044611
2012ES03 Rev.Mod.Phys. 84, 353 (2012) J.E.Escher, J.T.Burke, F.S.Dietrich, N.D.Scielzo, I.J.Thompson, W.Younes Compound-nuclear reaction cross sections from surrogate measurements
doi: 10.1103/RevModPhys.84.353
2012RO14 Phys.Rev. C 85, 051304 (2012) T.J.Ross, C.W.Beausang, R.O.Hughes, J.M.Allmond, C.T.Angell, M.S.Basunia, D.L.Bleuel, J.T.Burke, R.J.Casperson, J.E.Escher, P.Fallon, R.Hatarik, J.Munson, S.Paschalis, M.Petri, L.Phair, J.J.Ressler, N.D.Scielzo, I.J.Thompson Measurement of the entry-spin distribution imparted to the high excitation continuum region of gadolinium nuclei via (p, d) and (p, t) reactions NUCLEAR REACTIONS 154,158Gd(p, d), (p, t), E=25 MeV; measured particle and γ spectra, pγ-, dγ-, tγ-coin, σ(θ) using STARS-LIBERACE array; deduced entry spin distribution for the highly excited quasicontinuum in light-ion transfer reactions. DWBA analysis of σ(θ) data. 153,156Gd; deduced levels, J, π, l-transfer.
doi: 10.1103/PhysRevC.85.051304
2012SC10 Phys.Rev. C 85, 054619 (2012) N.D.Scielzo, J.E.Escher, J.M.Allmond, M.S.Basunia, C.W.Beausang, L.A.Bernstein, D.L.Bleuel, J.T.Burke, R.M.Clark, F.S.Dietrich, P.Fallon, J.Gibelin, B.L.Goldblum, S.R.Lesher, M.A.McMahan, E.B.Norman, L.Phair, E.Rodriguez-Vieitez, S.A.Sheets, I.J.Thompson, M.Wiedeking Statistical γ rays in the analysis of surrogate nuclear reactions NUCLEAR REACTIONS 154,155,156,158Gd(p, p'), E=21.7 MeV; measured Ep, Ip, Eγ, Iγ, pγ-coin using STARS-LiBerACE at LBNL cyclotron facility; deduced γ-ray emission probability. 155,157Gd(n, γ), E<3.5 MeV; deduced cross section ratios by surrogate analyses using statistical and discrete γ-rays. Comparison with reaction theory. Surrogate nuclear reaction technique.
doi: 10.1103/PhysRevC.85.054619
2012TH05 Nucl.Sci.Eng. 171, 85 (2012) I.J.Thompson, Y.M.X.M.Dardenne, J.M.Kenneally, A.Robertson, L.E.Ahle, C.A.Hagmann, R.A.Henderson, D.Vogt, C.-Y.Wu, W.Younes Evaluations of Fission Chain Yields for 239Pu from Fission-Spectrum Neutrons NUCLEAR REACTIONS 239Pu(n, F)95Zr/97Zr/95Nb/97Nb/99Mo/144Ce/146Nd/147Nd/148Nd/150Nd/155Eu/156Eu/140Ba/90Sr/103Ru/131I/140La, E<10 MeV; analyzed available data; deduced fission chain yields.
doi: 10.13182/NSE10-101
2011BU11 J.Korean Phys.Soc. 59, 1892s (2011) J.T.Burke, J.J.Ressler, J.E.Escher, N.D.Scielzo, I.J.Thompson, R.Henderson, J.Gostic, L.Bernstein, D.Bluel, M.Weideking, V.Meot, O.Roig, L.W.Phair, R.Hatarik, J.Munson, C.Angell, B.Goldblum, C.W.Beausang, T.Ross, R.Hughes, M.Aiche, G.Barreau, N.Cappelan, S.Czajkowski, B.Hass, B.Jurado, L.Mathieu, I.Companis Experimental Approaches to Studying the Fission Process Using the Surrogate Reaction Technique NUCLEAR REACTIONS 235,236U, 239Pu(α, α'), E=55 MeV; measured E(charged particle), I(charged particle), Eγ, Iγ(θ), γγ-coin, fission products using STARS (Silicon Telescope Array for Reaction Studies), LIBERACE, HYDRA; deduced σ 238Pu(n, F) below 20 MeV using surrogate reactions. Comparison with other data.
doi: 10.3938/jkps.59.1892
2011CH57 Nucl.Data Sheets 112, 2887 (2011) M.B.Chadwick, M.Herman, P.Oblozinsky, M.E.Dunn, Y.Danon, A.C.Kahler, D.L.Smith, B.Pritychenko, G.Arbanas, R.Arcilla, R.Brewer, D.A.Brown, R.Capote, A.D.Carlson, Y.S.Cho, H.Derrien, K.Guber, G.M.Hale, S.Hoblit, S.Holloway, T.D.Johnson, T.Kawano, B.C.Kiedrowski, H.Kim, S.Kunieda, N.M.Larson, L.Leal, J.P.Lestone, R.C.Little, E.A.McCutchan, R.E.MacFarlane, M.MacInnes, C.M.Mattoon, R.D.McKnight, S.F.Mughabghab, G.P.A.Nobre, G.Palmiotti, A.Palumbo, M.T.Pigni, V.G.Pronyaev, R.O.Sayer, A.A.Sonzogni, N.C.Summers, P.Talou, I.J.Thompson, A.Trkov, R.L.Vogt, S.C.van der Marck, A.Wallner, M.C.White, D.Wiarda, P.G.Young ENDF/B-VII.1 Nuclear Data for Science and Technology: Cross Sections, Covariances, Fission Product Yields and Decay Data COMPILATION Z=1-118; compiled, analyzed decay data, Maxwellian averaged neutron capture σ, neutron-induced fission σ. NUCLEAR REACTIONS 1,2H, 3He, 6,7Li, 7,9Be, 10,11B, C, 14,15N, 16,17O, 19F, 22,23Na, 24,25,26Mg, 27Al, 28,29,30Si, 31P, 32,33,34,36S, 35,37Cl, 36,38,40Ar, 39,40,41K, 40,42,43,44,46,48Ca, 45Sc, 46,47,48,49,50Ti, 50,51V, 50,52,53,54Cr, 55Mn, 54,56,57,58Fe, 58,59Co, 58,59,60,61,62,64Ni, 63,65Cu, 65,66,67,68,70Zn, 69,71Ga, 70,72,73,74,76Ge, 74,75As, 74,76,77,78,79,80,82Se, 79,81Br, 78,80,82,83,84,85,86Kr, 85,86,87Rb, 84,86,87,88,89,90Sr, 89,90,91Y, 90,91,92,93,94,95,96Zr, 93,94,95Nb, 92,94,95,96,97,98,99,100Mo, 99Tc, 96,98,99,100,101,102,103,104,105,106Ru, 103,105Rh, 102,104,105,106,107,108,110Pd, 107,109,110,111Ag, 106,108,110,111,112,113,114,115,116Cd, 113,115In, 112,113,114,115,116,117,118,119,120,122,123,124,125,126Sn, 121,123,124,125,126Sb, 120,122,123,124,125,126,127,128,129,130,132Te, 127,129,130,131,135I, 123,124,126,128,129,130,131,132,133,134,135,136Xe, 133,134,135,136,137Cs, 130,132,133,134,135,136,137,138,140Ba, 138,139,140La, 136,138,139,140,141,142,143,144Ce, 141,142,143Pr, 142,143,144,145,146,147,148,150Nd, 147,148,149,151Pm, 144,147,148,149,150,151,152,153,154Sm, 151,152,153,154,155,156,157Eu, 152,153,154,155,156,157,158,160Gd, 159,160Tb, 156,158,160,161,162,163,164Dy, 165,166Ho, 162,164,166,167,168,170Er, 168,169,170Tm, 175,176Lu, 174,176,177,178,179,180Hf, 180,181,182Ta, 180,182,183,184,186W, 185,187Re, 191,193Ir, 197Au, 196,198,199,200,201,202,204Hg, 203,205Tl, 204,206,207,208Pb, 209Bi, 223,224,225,226Ra, 225,226,227Ac, 227,228,229,230,231,232,233,234Th, 229,230,231,232,233Pa, 230,231,232,233,234,235,236,237,238,239,240,241U, 234,235,236,237,238,239Np, 236,237,238,239,240,241,242,243,244,246Pu, 240,241,242,243,244Am, 240,241,242,243,244,245,246,247,248,249,250Cm, 245,246,247,249,250Bk, 246,248,249,250,251,252,253,254Cf, 251,252,253,254,255Es, 255Fm(n, γ), E=30 keV; calculated Maxwellian-averaged σ using ENDF/B-VII.1 evaluated neutron library. Comparison with ENDF/B-VII.0 and KADONIS values. NUCLEAR REACTIONS 227,228,229,230,231,232,233,234Th, 229,230,231,232,233Pa, 230,231,232,233,234,235,236,237,238,239,240,241U, 234,235,236,237,238,239Np, 236,237,238,239,240,241,242,243,244,246Pu, 240,241,242,243,244Am, 240,241,242,243,244,245,246,247,248,249,250Cm, 245,246,247,249,250Bk, 246,248,249,250,251,252,253,254Cf, 251,252,253,254,255Es, 255Fm(n, γ), (n, F), E=thermal; calculated thermal σ. Comparison with ENDF/B-VII.0, JENDL-4.0 and Atlas of Neutron Resonances values.
doi: 10.1016/j.nds.2011.11.002
2011NO17 Phys.Rev. C 84, 064609 (2011) G.P.A.Nobre, F.S.Dietrich, J.E.Escher, I.J.Thompson, M.Dupuis, J.Terasaki, J.Engel Toward a microscopic reaction description based on energy-density-functional structure models NUCLEAR REACTIONS 90Zr(n, X), E=10, 20, 30 MeV; 58Ni(n, X), E=20, 30 MeV; 58Ni(p, X), E=10-70 MeV; 48Ca(p, X), E=10-50 MeV; 40,48Ca, 58Ni, 144Sm(n, X), (p, X), E=30 MeV; 90Zr(p, X), E=20-70 MeV; calculated reaction cross section. 90Zr(p, p), E=40, 65 MeV; calculated σ(θ). Random-phase, Hartree-Fock-Bogoliubov (HFB) framework and Skyrme density functional with coupling to all RPA and QRPA inelastic channels including deuteron formation. Assessed effects of couplings between inelastic resonances from higher-order channels. Comparison with experimental data.
doi: 10.1103/PhysRevC.84.064609
2011NO18 J.Phys.:Conf.Ser. 312, 082033 (2011) G.P.A.Nobre, I.J.Thompson, J.E.Escher, F.S.Dietrich Reaction cross-section predictions for nucleon induced reactions NUCLEAR REACTIONS 58Ni(n, X), E=20, 30 MeV;90Zr(n, X), E=10, 20, 40 MeV;144Sm(n, X), E=30 MeV;40,48Ca, 58Ni(p, X), E=10, 20, 30, 40 MeV;90Zr(p, X), E=10, 20, 30, 40, 50, 60, 70 MeV;144Sm(p, X), E=30 MeV; calculated reaction σ using optical model with QRPA target excitations and coupling to inelastic and transfer channels. Proton reactions compared to data.
doi: 10.1088/1742-6596/312/4/082033
2011RE09 Phys.Rev. C 83, 054610 (2011) J.J.Ressler, J.T.Burke, J.E.Escher, C.T.Angell, M.S.Basunia, C.W.Beausang, L.A.Bernstein, D.L.Bleuel, R.J.Casperson, B.L.Goldblum, J.Gostic, R.Hatarik, R.Henderson, R.O.Hughes, J.Munson, L.W.Phair, T.J.Ross, N.D.Scielzo, E.Swanberg, I.J.Thompson, M.Wiedeking Surrogate measurement of the 238Pu(n, f) cross section NUCLEAR REACTIONS 239Pu(α, α'F), 235U(α, α'F), 236U(α, α'F), E=20-55 MeV; measured particle and fission fragment spectra, α-fission coincidences, cross sections, fission fragment anisotropy ratios. 238Pu, 234,235U(n, F), E=5-20 MeV; deduced fission cross sections using surrogate ratio method. Comparison with previous experimental data and evaluated libraries. Data needs for following reactions for next-generation reactors: 241Pu, 241,242Am, 243,244,245Cm(n, F), E.1 MeV. Potential surrogate and ratio reactions listed.
doi: 10.1103/PhysRevC.83.054610
2011TH05 J.Phys.:Conf.Ser. 312, 082041 (2011) The Theory of Partial Fusion NUCLEAR REACTIONS 239Pu(d, p), E=15 MeV; calculated partial fusion σ, breakup escape σ; deduced competition between neutron absorption and escape.
doi: 10.1088/1742-6596/312/4/082041
2010NO06 Phys.Rev.Lett. 105, 202502 (2010) G.P.A.Nobre, F.S.Dietrich, J.E.Escher, I.J.Thompson, M.Dupuis, J.Terasaki, J.Engel Coupled-Channel Calculation of Nonelastic Cross Sections Using a Density-Functional Structure Model NUCLEAR REACTIONS 40,48Ca, 58Ni, 90Zr, 144Sm(p, X), (n, X), E<40 MeV; calculated total reaction σ. Complete microscopic calculation, comparison with experimental data.
doi: 10.1103/PhysRevLett.105.202502
2010SC06 Phys.Rev. C 81, 034608 (2010) N.D.Scielzo, J.E.Escher, J.M.Allmond, M.S.Basunia, C.W.Beausang, L.A.Bernstein, D.L.Bleuel, J.T.Burke, R.M.Clark, F.S.Dietrich, P.Fallon, J.Gibelin, B.L.Goldblum, S.R.Lesher, M.A.McMahan, E.B.Norman, L.Phair, E.Rodriquez-Vieitez, S.A.Sheets, I.J.Thompson, M.Wiedeking Measurement of γ-emission branching ratios for 154, 156, 158Gd compound nuclei: Tests of surrogate nuclear reaction approximations for (n, γ) cross sections NUCLEAR REACTIONS 154,156,158Gd(p, p'γ), E=22 MeV; measured Eγ, Iγ, proton spectra, γ-ray emission probabilities using STARS/LiBerACE array. 155,157Gd(n, γ), E=0.01-4 MeV; deduced σ by surrogate reaction method using Weisskopf-Ewing and ratio approximations.
doi: 10.1103/PhysRevC.81.034608
2010YA03 Few-Body Systems 47, 213 (2010) A.Yakhelef, N.K.Timofeyuk, J.S.Al-Khalili, I.J.Thompson Three-Body Spectrum of 18C and its Relevance to r-Process Nucleosynthesis NUCLEAR STRUCTURE 16,17,18C; calculated energy levels, transition strengths, two-neutron separation energy. NUCLEAR REACTIONS 17C(n, γ), E not given; calculated B(M1), astrophysical reaction rate, σ.
doi: 10.1007/s00601-010-0086-8
2009RO26 Phys.Rev. C 80, 051601 (2009) M.Rodriguez-Gallardo, J.M.Arias, J.Gomez-Camacho, A.M.Moro, I.J.Thompson, J.A.Tostevin Four-body continuum-discretized coupled-channels calculations NUCLEAR REACTIONS 208Pb(6He, X), E=22 MeV; calculated σ(θ), angular distributions , B(E1) and B(E2) distributions using continuum-discretized coupled channels calculations. calculated . Comparison with experimental data.
doi: 10.1103/PhysRevC.80.051601
2008BA46 Phys.Rev. C 78, 054603 (2008) A.J.Bartlett, J.A.Tostevin, I.J.Thompson R-matrix and dynamical model calculations of three-body resonance decay widths RADIOACTIVITY 6He(n); calculated resonance decay widths, channel resonance energy, probability densities. R-matrix and dynamical three-body theoretical models.
doi: 10.1103/PhysRevC.78.054603
2008RO16 Phys.Rev. C 77, 064609 (2008) M.Rodriguez-Gallardo, J.M.Arias, J.Gomez-Camacho, R.C.Johnson, A.M.Moro, I.J.Thompson, J.A.Tostevin Four-body continuum-discretized coupled-channels calculations using a transformed harmonic oscillator basis NUCLEAR REACTIONS 12C(6He, 6He), E=229.8 MeV; 64Zn(6He, 6He), E=10.0, 13.6 MeV; 208Pb(6He, 6He), E=22 MeV; calculated energy spectra, σ(θ). Comparison with experimental data.
doi: 10.1103/PhysRevC.77.064609
2008TA13 Phys.Rev.Lett. 100, 192502 (2008) I.Tanihata, M.Alcorta, D.Bandyopadhyay, R.Bieri, L.Buchmann, B.Davids, N.Galinski, D.Howell, W.Mills, S.Mythili, R.Openshaw, E.Padilla-Rodal, G.Ruprecht, G.Sheffer, A.C.Shotter, M.Trinczek, P.Walden, H.Savajols, T.Roger, M.Caamano, W.Mittig, P.Roussel-Chomaz, R.Kanungo, A.Gallant, M.Notani, G.Savard, I.J.Thompson Measurement of the Two-Halo Neutron Transfer Reaction 1H(11Li, 9Li)3H at 3 A MeV NUCLEAR REACTIONS 1H(11Li, 9Li)3H, E=3 MeV/nucleon; measured σ(θ), proton-Li-coin using gas-Si-CsI target-detection system (MAYA active target); deduced spectroscopic factors. Comparison with Optical Model calculations.
doi: 10.1103/PhysRevLett.100.192502
2008TI07 Phys.Rev. C 78, 044323 (2008) N.K.Timofeyuk, P.Descouvemont, I.J.Thompson Threshold effects in the 27P(3/2+) → 26Si + p and 27Mg(3/2+) → 26Mg + n mirror decays and the stellar reaction 26Si(p, γ)27P NUCLEAR REACTIONS 26Mg(t, d), E=36 MeV; analyzed cross sections, ANCs; 26Si(p, γ); deduced astrophysical S-factors. NUCLEAR STRUCTURE 27Mg, 27P; calculated resonance energies, widths, particle separation energies. Shell model calculations.
doi: 10.1103/PhysRevC.78.044323
2008TI09 Phys.Rev. C 78, 054322 (2008) Spectroscopic factors and asymptotic normalization coefficients in mirror three-body systems NUCLEAR STRUCTURE 6He, 6Be, 9Li, 9C, 18O, 18Ne; calculated spectroscopic factors, asymptotic normalization coefficients.
doi: 10.1103/PhysRevC.78.054322
2007AL08 Phys.Rev. C 75, 024608 (2007) J.S.Al-Khalili, R.Crespo, R.C.Johnson, A.M.Moro, I.J.Thompson Few-body multiple scattering calculations for 6He on protons NUCLEAR REACTIONS 1H(α, α), E=699 MeV/nucleon; 1H(6He, 6He), E=717 MeV/nucleon; calculated elastic σ(θ). Multiple scattering expansion, comparison with data.
doi: 10.1103/PhysRevC.75.024608
2007BE18 Phys.Lett. B 645, 128 (2007); Erratum Phys.Lett. B 671, 496 (2009) F.Beck, D.Frekers, P.von Neumann-Cosel, A.Richter, N.Ryezayeva, I.J.Thompson Spectroscopic factor of the 7He ground state NUCLEAR REACTIONS 7Li(d, 2p), E=171 MeV; analysed σ(E, θ); deduced resonance width, spectroscopic factor. R-matrix analysis.
doi: 10.1016/j.physletb.2006.12.036
2007CR07 Eur.Phys.J. Special Topics 150, 13 (2007) R.Crespo, A.M.Moro, I.J.Thompson, M.Rodriguez-Gallardo, J.Gomez-Camacho, J.M.Arias Exploring the 6He continuum sea through proton inelastic collisions NUCLEAR REACTIONS 6He(p, p'), E=717 MeV; calculated σ(θ) using the MST framework.
doi: 10.1140/epjst/e2007-00253-1
2007DA30 Phys.Rev. C 76, 064612 (2007) B.V.Danilin, J.S.Vaagen, T.Rogde, S.N.Ershov, I.J.Thompson, M.V.Zhukov, and the RNBT Collaboration Three-body continuum energy correlations in Borromean halo nuclei. III. Short-range external fields NUCLEAR STRUCTURE 6He, 11Li; calculated energy correlations using three-body cluster model for halo nuclides.
doi: 10.1103/PhysRevC.76.064612
2007MO02 Phys.Rev. C 75, 017603 (2007) A.M.Moro, M.Rodriguez-Gallardo, R.Crespo, I.J.Thompson Continuum description with pseudostate wave functions NUCLEAR REACTIONS 1H(6He, 6He'), E=717 MeV/nucleon; calculated σ(θ). Comparison of two pseudostate bases.
doi: 10.1103/PhysRevC.75.017603
2007NO06 Nucl.Phys. A786, 90 (2007) G.P.A.Nobre, L.C.Chamon, B.V.Carlson, I.J.Thompson, L.R.Gasques Tunneling through a parabolic barrier coupled to an oscillatory degree of freedom: Application to heavy-ion fusion at sub-barrier energies NUCLEAR REACTIONS 58,64Ni(58Ni, X), (64Ni, X), E(cm)=85-115 MeV; calculated fusion excitation functions.
doi: 10.1016/j.nuclphysa.2007.02.005
2007NO08 Phys.Rev. C 75, 044606 (2007) G.P.A.Nobre, L.C.Chamon, L.R.Gasques, B.V.Carlson, I.J.Thompson Consistent analysis of fusion data without adjustable parameters for a wide variety of heavy-ion systems NUCLEAR REACTIONS 12C, 92Zr, 208Pb(12C, X), 16O, 144,148,152,154Sm, 182,186W, 208Pb, 238U(16O, X), 208Pb(18O, X), 68Zn, 92Zr, 100Mo, 144Sm, 208Pb(28Si, X), 92,94,98,100Mo, 104Ru, 108,110Pd, 182W, 208Pb(32S, X), 90,98Zr, 92,100Mo, 104Ru, 108,110Pd(36S, X), 112,122Sn, 144,148,154Sm(40Ar, X), 40,48Ca, 48Ti, 90,98Zr, 192Os, 194Pt(40Ca, X), 90,98Zr(48Ca, X), 58,64Ni, 74Ge, 112,124Sn(58Ni, X), 64Ni, 74Ge, 100Mo(64Ni, X), 70,76Ge, 92Mo, 104Ru(86Kr, X), 90,96Zr(90Zr, X), E ≈ barrier; calculated fusion σ. Sao Paolo potential, comparison with data.
doi: 10.1103/PhysRevC.75.044606
2007RO29 Eur.Phys.J. Special Topics 150, 51 (2007) M.Rodriguez-Gallardo, J.M.Arias, J.Gomez-Camacho, R.C.Johnson, A.M.Moro, I.J.Thompson, J.A.Tostevin Continuum effects: Structure and reactions of 6He NUCLEAR STRUCTURE 6He; calculated B(E1), B(E2) distributions using the Transformed Harmonic Oscillator method. NUCLEAR REACTIONS 12C(6He, 6He), E=229.8 MeV; calculated elastic scattering σ(θ).
doi: 10.1140/epjst/e2007-00264-x
2007SU17 Nucl.Phys. A788, 325c (2007) N.C.Summers, F.M.Nunes, I.J.Thompson The effects of core excitation in the breakup of exotic nuclei
doi: 10.1016/j.nuclphysa.2007.01.095
2007SU18 Phys.Lett. B 650, 124 (2007) N.C.Summers, S.D.Pain, N.A.Orr, W.N.Catford, J.C.Angelique, N.I.Ashwood, V.Bouchat, N.M.Clarke, N.Curtis, M.Freer, B.R.Fulton, F.Hanappe, M.Labiche, J.L.Lecouey, R.C.Lemmon, D.Mahboub, A.Ninane, G.Normand, F.M.Nunes, N.Soic, L.Stuttge, C.N.Timis, I.J.Thompson, J.S.Winfield, V.Ziman B(E1) strengths from Coulomb excitation of 11Be NUCLEAR REACTIONS 208Pb(11Be, 11Be'), E=38.6 MeV/nucleon; measured Coulomb excitation σ. 11Be deduced B(E1) strengths; calculated σ. Extended continuum discretized coupled channels method. Comparison with previous data.
doi: 10.1016/j.physletb.2007.05.003
2006CR01 Nucl.Phys. A771, 26 (2006) R.Crespo, A.M.Moro, I.J.Thompson Few body impulse and fixed scatterer approximations for high energy scattering NUCLEAR REACTIONS 4He(p, p), E=700, 800 MeV; 6He(p, p), E=717 MeV; calculated σ(θ). Comparison with data, cluster effects. Factorized impulse approximation, fixed scatterer approximation.
doi: 10.1016/j.nuclphysa.2006.02.015
2006CR02 Phys.Atomic Nuclei 69, 1254 (2006) R.Crespo, A.M.Moro, I.J.Thompson Four-Body Multiple-Scattering Expansion of the Total Transition Amplitude-MST NUCLEAR REACTIONS 4,6He(p, p), E=717 MeV; calculated σ(θ). Factorized impulse approximations, comparison with data.
doi: 10.1134/S1063778806070258
2006CR03 Phys.Rev. C 74, 044616 (2006) R.Crespo, I.J.Thompson, A.M.Moro Excitation modes of 6He from proton collisions NUCLEAR REACTIONS 4,6He(p, p), (p, p'), E=700 MeV; calculated σ(θ). Multiple scattering expansion of total transition amplitude.
doi: 10.1103/PhysRevC.74.044616
2006DA13 Phys.Rev. C 73, 054002 (2006) B.V.Danilin, J.S.Vaagen, T.Rogde, S.N.Ershov, I.J.Thompson, M.V.Zhukov, and the Russian-Nordic-British Theory (RNBT) Collaboration Three-body continuum energy correlations in Borromean halo nuclei. II NUCLEAR STRUCTURE 6He; calculated energy correlations in three-body continuum, resonance features.
doi: 10.1103/PhysRevC.73.054002
2006HU12 Phys.Lett. B 640, 91 (2006) M.S.Hussein, R.Lichtenthaler, F.M.Nunes, I.J.Thompson Scaling and interference in the dissociation of halo nuclei NUCLEAR REACTIONS 12C, 40Ca, 120Sn, 208Pb(8B, X), E=44, 70 MeV/nucleon; 12C, 40Ca, 120Sn, 208Pb(11Be, X), E=44, 70, 200 MeV/nucleon; 12C, 40Ca, 120Sn, 208Pb(7Be, X), E=100 MeV/nucleon; calculated elastic nuclear breakup σ; deduced target mass dependence, Coulomb-nuclear interference. Continuum discretized coupled channels calculations, other targets also considered.
doi: 10.1016/j.physletb.2006.07.046
2006SU05 Phys.Rev. C 73, 031603 (2006) N.C.Summers, F.M.Nunes, I.J.Thompson Core transitions in the breakup of exotic nuclei NUCLEAR REACTIONS 9Be(11Be, 10BeX), E=60 MeV/nucleon; calculated break-up and stripping σ, role of dynamical core excitation. Extended continuum discretized coupled channels method, comparison with data.
doi: 10.1103/PhysRevC.73.031603
2006SU11 Phys.Rev. C 74, 014606 (2006); Erratum Phys.Rev. C 89, 069901 (2014) N.C.Summers, F.M.Nunes, I.J.Thompson Extended continuum discretized coupled channels method: Core excitation in the breakup of exotic nuclei NUCLEAR REACTIONS 9Be(11Be, n10Be), (17C, n16C), E=60 MeV/nucleon; calculated breakup σ, σ(E), core excitation effects. Extended continuum discretized coupled channels method.
doi: 10.1103/PhysRevC.74.014606
2006TI05 Phys.Rev.Lett. 96, 162501 (2006) N.K.Timofeyuk, D.Baye, P.Descouvemont, R.Kamouni, I.J.Thompson 15C-15F Charge symmetry and the 14C(n, γ)15C Reaction Puzzle NUCLEAR REACTIONS 14C(n, γ), E ≈ 10-1000 keV; analyzed σ, asymptotic normalization coefficients, E1 component, charge symmetry features in 15C, 15F nucleon decay.
doi: 10.1103/PhysRevLett.96.162501
2005BA54 Phys.Rev. C 71, 064608 (2005) P.Batham, I.J.Thompson, J.A.Tostevin Dynamical core deformation effects on single-nucleon knockout reactions at fragmentation beam energies NUCLEAR REACTIONS 9Be(11Be, 10BeX), E=60 MeV/nucleon; 9Be(17C, 16CX), E=62 MeV/nucleon; calculated σ, dynamical core deformation effects. Comparison with data.
doi: 10.1103/PhysRevC.71.064608
2005CH49 Nucl.Phys. A759, 23 (2005) L.V.Chulkov, H.Simon, I.J.Thompson, T.Aumann, M.J.G.Borge, Th.W.Elze, H.Emling, H.Geissel, L.V.Grigorenko, M.Hellstrom, B.Jonson, J.W.V.Kratz, R.Kulessa, K.Markenroth, M.Meister, G.Munzenberg, F.Nickel, T.Nilsson, G.Nyman, V.Pribora, A.Richter, K.Riisager, C.Scheidenberger, G.Schrieder, O.Tengblad, M.V.Zhukov Three-body correlations in electromagnetic dissociation of Borromean nuclei: The 6He case NUCLEAR REACTIONS Pb(6He, 2nα), E=240 MeV/nucleon; measured Eα, En, three-body energy and angular correlations; deduced role of final state interactions, other reaction mechanism features. 6He deduced possible resonance.
doi: 10.1016/j.nuclphysa.2005.05.001
2005GI07 Phys.Rev. C 71, 064311 (2005) L.Giot, P.Roussel-Chomaz, C.E.Demonchy, W.Mittig, H.Savajols, N.Alamanos, F.Auger, A.Gillibert, C.Jouanne, V.Lapoux, L.Nalpas, E.C.Pollacco, J.L.Sida, F.Skaza, M.D.Cortina-Gil, J.Fernandez-Vazquez, R.S.Mackintosh, A.Pakou, S.Pita, A.Rodin, S.Stepantsov, G.M.Ter-Akopian, K.Rusek, I.J.Thompson, R.Wolski Investigation of 6He cluster structures NUCLEAR REACTIONS 1H(6He, α), E=25 MeV/nucleon; measured σ(θ); deduced particle transfer contributions, entrance potential dependence. 6He deduced spectroscopic factors for t+t and α+2n cluster configurations. 1H(6He, p), E=25 MeV/nucleon; measured σ(θ). 3He(α, α), E(cm)=28.7 MeV; calculated σ(θ). SPEG spectrometer and MUST array at GANIL. DWBA and coupled-channels calculations.
doi: 10.1103/PhysRevC.71.064311
2005HO12 J.Phys.(London) G31, 309 (2005) S.Hossain, M.N.A.Abdullah, S.K.Das, M.A.Uddin, A.K.Basak, H.M.Sen Gupta, I.J.Thompson, F.B.Malik Band mixing in 29Si and 29P NUCLEAR REACTIONS 28Si(α, t), (α, 3He), E=45 MeV; analyzed σ(E, θ). 29P, 29Si deduced configurations, band-mixing effects. Coupled channels approach, finite-range transfer theory, Nilsson model.
doi: 10.1088/0954-3899/31/5/003
2005RO27 Phys.Rev. C 72, 024007 (2005) M.Rodriguez-Gallardo, J.M.Arias, J.Gomez-Camacho, A.M.Moro, I.J.Thompson, J.A.Tostevin Three-body continuum discretization in a basis of transformed harmonic oscillator states NUCLEAR STRUCTURE 6He; calculated B(E1), B(E2) distributions, sum rules. Transformed harmonic oscillator method, three-body continuum.
doi: 10.1103/PhysRevC.72.024007
2004BR08 Phys.Rev. C 69, 024608 (2004) B.Braizinha, C.R.Brune, A.M.Eiro, B.M.Fisher, H.J.Karwowski, D.S.Leonard, E.J.Ludwig, F.D.Santos, I.J.Thompson Resonant and direct components in the 3He(d, p)4He reaction at low energies NUCLEAR REACTIONS 3He(polarized d, p), E=0.52, 0.89, 1.49 MeV; measured σ(θ=0°), analyzing power; deduced scattering matrix elements.
doi: 10.1103/PhysRevC.69.024608
2004DA07 Phys.Rev. C 69, 024609 (2004) B.V.Danilin, T.Rogde, J.S.Vaagen, I.J.Thompson, M.V.Zhukov, and the RNBT Collaboration Three-body continuum spatial correlations in Borromean halo nuclei NUCLEAR STRUCTURE 6He; calculated low-lying resonance features, spatial correlations in three-body continuum. Hyperspherical harmonics method.
doi: 10.1103/PhysRevC.69.024609
2004DI16 Acta Phys.Hung.N.S. 19, 7 (2004) A.Diaz-Torres, I.J.Thompson, W.Scheid Fusion of Weakly Bound Projectiles around the Coulomb Barrier NUCLEAR REACTIONS 208Pb(11Be, X), 209Bi(9Be, X), E(cm) ≈ 35-50 MeV; analyzed fusion excitation functions, continuum-continuum coupling effects.
doi: 10.1556/APH.19.2004.1-2.2
2004ER07 Phys.Rev. C 70, 054608 (2004) S.N.Ershov, B.V.Danilin, J.S.Vaagen, A.A.Korsheninnikov, I.J.Thompson Structure of the 11Li continuum from breakup on proton target NUCLEAR REACTIONS 1H(11Li, 11Li'), E=68 MeV/nucleon; calculated σ(E, θ), energy and angular correlations. 11Li deduced continuum features. Microscopic four-body distorted-wave model, comparisons with data.
doi: 10.1103/PhysRevC.70.054608
2004MA99 Nucl.Phys. A746, 497c (2004) M.Mazzocco, P.Scopel, C.Signorini, L.Fortunato, F.Soramel, I.J.Thompson, A.Vitturi, M.Barbui, A.Brondi, M.Cinausero, D.Fabris, E.Fioretto, G.La Rana, M.Lunardon, R.Moro, A.Ordine, G.F.Prete, V.Rizzi, L.Stroe, M.Trotta, E.Vardaci, G.Viesti 6Li breakup from 208Pb target at Coulomb barrier energies: doorway to reaction mechanism induced by loosely bound/halo nuclei NUCLEAR REACTIONS 208Pb(6Li, dα), (6Li, npα), E=31, 33, 35, 39 MeV; measured particle spectra, excitation energy distributions; deduced breakup mechanism features.
doi: 10.1016/j.nuclphysa.2004.09.076
2004NU05 Nucl.Phys. A746, 61c (2004) What are the advantages of a three body model with core excitation for 21Ne and 21Na? NUCLEAR STRUCTURE 21Ne, 21Na; calculated level energies. Three-body model with core excitation, comparison with data.
doi: 10.1016/j.nuclphysa.2004.09.136
2004TA03 Nucl.Phys. A733, 53 (2004) T.Tarutina, I.J.Thompson, J.A.Tostevin Study of 14Be with core excitation NUCLEAR STRUCTURE 12,13,14Be; calculated ground-state energies, deformations, resonance features, related parameters. Particle-rotor model with core excitation, hyperspherical harmonics method.
doi: 10.1016/j.nuclphysa.2003.12.003
2004TH08 Prog.Theor.Phys.(Kyoto), Suppl. 154, 69 (2004) Modelling Effects of Halo Breakup on Fusion
doi: 10.1143/PTPS.154.69
2004TO24 Nucl.Phys. A746, 166c (2004) J.A.Tostevin, P.Batham, G.Podolyak, I.J.Thompson Direct reaction spectroscopy of exotic nuclei NUCLEAR REACTIONS 12C(12C, 10BeX), (12C, 10CX), E=0.25, 1.05, 2.1 GeV; calculated inclusive two-nucleon knockout σ. 9Be(28Mg, 26NeX), E=82 MeV/nucleon; calculated two-proton knockout σ(E). Comparison with model predictions.
doi: 10.1016/j.nuclphysa.2004.09.071
2003DI07 Phys.Rev. C 68, 044607 (2003) A.Diaz-Torres, I.J.Thompson, C.Beck How does breakup influence the total fusion of 6, 7Li at the Coulomb barrier? NUCLEAR REACTIONS 59Co(6Li, X), (7Li, X), E(cm)=8-24 MeV; 209Bi(6Li, X), (7Li, X), E(cm)=28-48 MeV; calculated fusion σ, breakup channels contributions. Coupled-channels approach, comparison with data.
doi: 10.1103/PhysRevC.68.044607
2003MA85 Eur.Phys.J. A 18, 583 (2003) M.Mazzocco, P.Scopel, C.Signorini, L.Fortunato, F.Soramel, I.J.Thompson, A.Vitturi, M.Barbui, A.Brondi, M.Cinausero, D.Fabris, E.Fioretto, G.La Rana, M.Lunardon, R.Moro, A.Ordine, G.F.Prete, V.Rizzi, L.Stroe, M.Trotta, E.Vardaci, G.Viesti Excitation of 6Li above the breakup threshold in the 6Li + 208Pb system around the Coulomb barrier NUCLEAR REACTIONS 208Pb(6Li, 6Li'), (6Li, dα), E=31, 33, 35, 39 MeV; measured outgoing particles invariant mass spectra, σ(E, θ); deduced breakup mechanism features.Coupled-channels analysis.
doi: 10.1140/epja/i2003-10097-y
2003MO07 Phys.Rev. C 67, 047602 (2003) A.M.Moro, R.Crespo, F.M.Nunes, I.J.Thompson Breakup and core coupling in 14N(7Be, 8B)13C NUCLEAR REACTIONS 14N(7Be, 8B), E=84 MeV; calculated σ(E), σ(θ), core coupling and breakup channel effects. Continuum discretized coupled channels Born approximation.
doi: 10.1103/PhysRevC.67.047602
2003MO37 Nucl.Phys. A722, 455c (2003) A.M.Moro, R.Crespo, F.Nunes, I.J.Thompson Continuum effects in reactions involving weakly bound nuclei NUCLEAR REACTIONS 13C(8B, 8B), E=78 MeV; 14N(7Be, 8B), E=84 MeV; calculated σ(θ); deduced continuum coupling effects.
doi: 10.1016/S0375-9474(03)01407-6
2003PE08 Eur.Phys.J. A 16, 509 (2003) I.Peter, W.von Oertzen, S.Thummerer, H.G.Bohlen, B.Gebauer, J.Gerl, M.Kaspar, I.Kozhoukharov, T.Kroll, M.Rejmund, H.J.Wollersheim, I.J.Thompson Enhanced neutron pair transfer and collective excitations in the system 206Pb + 118Sn at barrier energies NUCLEAR REACTIONS 208Pb(118Sn, 116Sn), (118Sn, 117Sn), (118Sn, 118Sn'), (118Sn, 119Sn), (118Sn, 120Sn), E=5.14, 5.32 MeV/nucleon; measured Eγ, Iγ, (particle)γ-coin; deduced one- and two-neutron transfer probabilities, spectroscopic amplitudes, σ(θ), enhancement factors. Semi-classical analysis, comparison with model predictions.
doi: 10.1140/epja/i2002-10124-7
2003SI02 Phys.Rev. C 67, 044607 (2003) C.Signorini, A.Edifizi, M.Mazzocco, M.Lunardon, D.Fabris, A.Vitturi, P.Scopel, F.Soramel, L.Stroe, G.Prete, E.Fioretto, M.Cinausero, M.Trotta, A.Brondi, R.Moro, G.La Rana, E.Vardaci, A.Ordine, G.Inglima, M.La Commara, D.Pierroutsakou, M.Romoli, M.Sandoli, A.Diaz-Torres, I.J.Thompson, Z.H.Liu Exclusive breakup of 6Li by 208Pb at Coulomb barrier energies NUCLEAR REACTIONS 208Pb(6Li, αX), (6Li, dα), (6Li, npα), E=31-39 MeV; measured Eα, dα-, pα-coin, σ(E, θ), σ; deduced reaction mechanism features. Continuum discretized coupled channels calculations.
doi: 10.1103/PhysRevC.67.044607
2002CR06 Phys.Rev. C66, 021002 (2002) R.Crespo, I.J.Thompson, A.A.Korsheninnikov Excitation modes of 11Li at Ex ∼ 1.3 MeV from proton collisions NUCLEAR REACTIONS 11Li(p, p'), E=68 MeV/nucleon; calculated, analyzed σ(E), σ(θ). 11Li deduced excited states features. Multiple scattering expansion of total transition amplitude.
doi: 10.1103/PhysRevC.66.021002
2002DA26 Eur.Phys.J. A 15, 65 (2002) B.Davids, S.M.Austin, D.Bazin, H.Esbensen, B.M.Sherrill, I.J.Thompson, J.A.Tostevin Coulomb breakup of 8B and the flux of 8B neutrinos from the Sun NUCLEAR REACTIONS Pb(8B, p7Be), E=83 MeV/nucleon; measured σ. 7Be(p, γ), E=low; deduced astrophysical S-factor. Continuum-discretized coupled-channels analysis.
doi: 10.1140/epja/i2001-10227-7
2002DI02 Phys.Rev. C65, 024606 (2002) Effect of Continuum Couplings in Fusion of Halo 11Be on 208Pb Around the Coulomb Barrier NUCLEAR REACTIONS 208Pb(11Be, X), E(cm) ≈ 30-50 MeV; calculated complete and incomplete fusion σ; deduced role of continuum couplings. Three-body model, comparison with data.
doi: 10.1103/PhysRevC.65.024606
2002DI13 Nucl.Phys. A703, 83 (2002) A.Diaz-Torres, I.J.Thompson, W.Scheid Breakup of 9Be on 209Bi Above and Near the Coulomb Barrier as a Molecular Single-Particle Effect: Its influence on complete fusion and scattering NUCLEAR REACTIONS 209Bi(9Be, X), E(cm) ≈ 40-50 MeV; calculated fusion σ, elastic and inelastic σ(θ), breakup channel contributions. Adiabatic two-center shell model approach, molecular single-particle effect.
doi: 10.1016/S0375-9474(01)01335-5
2002DI15 Phys.Lett. 533B, 265 (2002) A.Diaz-Torres, I.J.Thompson, W.Scheid Alpha Particle Production by Molecular Single-Particle Effect in Reactions of 9Be Just Above the Coulomb Barrier NUCLEAR REACTIONS 209Bi(9Be, n2α), E(cm)=44-57 MeV; calculated dissociation probability, σ. 64Zn(9Be, X), E(cm)=18-25 MeV; calculated fusion σ. Adiabatic two-center shell model, molecular single-particle effects.
doi: 10.1016/S0370-2693(02)01676-3
2002GR03 Phys.Rev.Lett. 88, 042502 (2002) L.V.Grigorenko, I.G.Mukha, I.J.Thompson, M.V.Zhukov Two-Proton Widths of 12O, 16Ne, and Three-Body Mechanism of Thomas-Ehrman Shift NUCLEAR STRUCTURE 12O, 16Ne; calculated levels J, π, widths, IAS features, two-proton decay widths. Three-body mechanism, comparison with data.
doi: 10.1103/PhysRevLett.88.042502
2002GR10 Phys.Rev. C65, 044612 (2002) L.V.Grigorenko, R.C.Johnson, I.J.Thompson, M.V.Zhukov Two-Proton Events in the 17F(p, 2p)16O Reaction NUCLEAR REACTIONS 1H(17F, 16O), E=33, 44 MeV; calculated two-proton production σ, contribution from 18Ne excited state decay. Comparison with data.
doi: 10.1103/PhysRevC.65.044612
2002GR25 Eur.Phys.J. A 15, 125 (2002) L.V.Grigorenko, R.C.Johnson, I.G.Mukha, I.J.Thompson, M.V.Zhukov Three-body decays of light nuclei: 6Be, 8Li, 9Be, 12O, 16Ne, and 17Ne NUCLEAR STRUCTURE 8Li, 6,9Be, 12O, 16Ne; calculated two-proton decay related particle spectra, level widths. Comparisons with data. RADIOACTIVITY 8Li, 6,9Be, 12O, 16Ne(2p); calculated two-proton decay related particle spectra, level widths. Comparisons with data.
doi: 10.1140/epja/i2001-10239-3
2002LI34 Phys.Rev. C65, 051603 (2002) J.F.Liang, J.R.Beene, H.Esbensen, A.Galindo-Uribarri, J.Gomez del Campo, C.J.Gross, M.L.Halbert, P.E.Mueller, D.Shapira, D.W.Stracener, I.J.Thompson, R.L.Varner Elastic Scattering and Breakup of 17F at 10 MeV/nucleon NUCLEAR REACTIONS 208Pb(17F, 17F), (17F, 16O), E=170 MeV; measured σ(θ); deduced reaction mechanism features. Comparison with optical model predictions.
doi: 10.1103/PhysRevC.65.051603
2002MO21 Phys.Rev. C65, 064619 (2002) J.Mortimer, I.J.Thompson, J.A.Tostevin Higher-Order and E2 Effects in Medium Energy 8B Breakup NUCLEAR REACTIONS Pb(8B, p7Be), E=44, 81 MeV/nucleon; calculated fragments parallel momentum distributions; deduced E1/E2 interference effects. Coupled discretized continuum channels method, comparisons with data.
doi: 10.1103/PhysRevC.65.064619
2002MO28 Phys.Rev. C66, 024612 (2002) A.M.Moro, R.Crespo, F.Nunes, I.J.Thompson 8B breakup in elastic and transfer reactions NUCLEAR REACTIONS 13C(p, p), E=10 MeV; 13C(7Be, 7Be), E=68 MeV; 13C(8B, 8B), E=78 MeV; 14N(7Be, 8B), E=84 MeV; calculated σ(θ); deduced continuum effects. Continuum discretized coupled channels formalism.
doi: 10.1103/PhysRevC.66.024612
2002NU01 Nucl.Phys. A703, 593 (2002) F.M.Nunes, I.J.Thompson, J.A.Tostevin Core Excitation in 12Be NUCLEAR STRUCTURE 11,12Be; calculated levels, J, π, radii, configurations, spectroscopic factors, B(E1), B(E2). Three-body model with core excitations, comparison with data.
doi: 10.1016/S0375-9474(01)01667-0
2002TH07 Nucl.Phys. A701, 7c (2002) Halo Physics
doi: 10.1016/S0375-9474(01)01537-8
2002TO23 Prog.Theor.Phys.(Kyoto), Suppl. 146, 338 (2002) J.A.Tostevin, J.M.Brooke, J.Mortimer, I.J.Thompson Eikonal and Coupled-Channels Reaction Methods Applied to Studies of Weakly Bound Nuclei NUCLEAR REACTIONS 9Be(15C, n14C), E=54 MeV/nucleon; 208Pb(8B, p7Be), E=44.1 MeV/nucleon; calculated fragments parallel momentum distributions, elastic breakup contribution. Coupled discretized continuum channels method, comparison with data.
doi: 10.1143/PTPS.146.338
2002WA08 Phys.Rev. C65, 044617 (2002) R.E.Warner, I.J.Thompson, J.A.Tostevin Effects of the In-Medium NN Interaction on Total Reaction and Neutron Removal Cross Sections NUCLEAR REACTIONS 12C(12C, X), E=10-1000 MeV/nucleon; 12C(6Li, X), (7Li, X), (8Li, X), (9Li, X), (11Li, X), E=800 MeV/c; calculated total reaction σ; 12C(11Li, X), E=800 MeV/c; calculated two-neutron removal σ; deduced in-medium effects.
doi: 10.1103/PhysRevC.65.044617
2001CR02 Phys.Rev. C63, 044003 (2001) Effects on p-11Li Elastic Scattering of Core Recoil and Virtual 2-n Halo Breakup NUCLEAR REACTIONS 1H(11Li, 11Li), E=800 MeV/nucleon; calculated σ(θ); deduced core recoil and virtual breakup effects. Kerman-McManus-Thaler, T matrix formalisms. Comparison between different calculations.
doi: 10.1103/PhysRevC.63.044003
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