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NSR database version of April 24, 2024.

Search: Author = G.F.Steyn

Found 88 matches.

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2023BR04      Phys.Rev. C 107, 055802 (2023)

J.W.Brummer, P.Adsley, T.Rauscher, F.D.Smit, C.P.Brits, M.Kohne, N.A.Khumalo, K.C.W.Li, D.J.Marin-Lambarri, N.J.Mukwevho, F.Nemulodi, R.Neveling, P.Papka, L.Pellegri, V.Pesudo, B.M.Rebeiro, G.F.Steyn, W.Yahia-Cherif

Proton decays from α-unbound states in 22Mg and the 18Ne(α, p0)21Na cross section

NUCLEAR REACTIONS 24Mg(p, t)22Mg, E=100 MeV; measured reaction products, triton spectra, Ep, Ip. 22Mg; deduced levels, branching ratios for proton decay of the excited states. 18Ne(α, p)21Na, E(cm)=1-3 MeV; calculated exclusive σ(E) to the ground state with SMARAGD code using deduced p0 width. Comparison to TALYS, NON-SMOKER and SMARAGD calculations and other experimental results. K600 magnetic spectrometer and CAKE (Coincidence Array for K600 Experiments) array 5 double-sided silicon strip detectors at Separated-Sector Cyclotron (iThemba LABS).

doi: 10.1103/PhysRevC.107.055802
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Data from this article have been entered in the XUNDL database. For more information, click here.


2022LI08      Phys.Rev. C 105, 024308 (2022)

K.C.W.Li, P.Adsley, R.Neveling, P.Papka, F.D.Smit, E.Nikolskii, J.W.Brummer, L.M.Donaldson, M.Freer, M.N.Harakeh, F.Nemulodi, L.Pellegri, V.Pesudo, M.Wiedeking, E.Z.Buthelezi, V.Chudoba, S.V.Fortsch, P.Jones, M.Kamil, J.P.Mira, G.G.O'Neill, E.Sideras-Haddad, B.Singh, S.Siem, G.F.Steyn, J.A.Swartz, I.T.Usman, J.J.van Zyl

Multiprobe study of excited states in 12C: Disentangling the sources of monopole strength between the energy of the Hoyle state and ex = 13 MeV

NUCLEAR REACTIONS 12C(α, α'), E=118, 160, 196, 200; 14C(p, t), E=67.5, 100 MeV; measured reaction products, Eα, Iα, (particle)α-coin; deduced excitation energy spectra. 12C; deduced levels, J, π, resonances, resonance widths, monopole strength distribution. Discussed the nature of monopole strength excess at around 9 MeV as possible breathing-mode excitation of the Hoyle state. CAKE-array of double-sided silicon strip detectors coupled with K600 magnetic spectrometer at iThemba LABS.

doi: 10.1103/PhysRevC.105.024308
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2022LI13      Phys.Lett. B 827, 136928 (2022)

K.C.W.Li, F.D.Smit, P.Adsley, R.Neveling, P.Papka, E.Nikolskii, J.W.Brummer, L.M.Donaldson, M.Freer, M.N.Harakeh, F.Nemulodi, L.Pellegri, V.Pesudo, M.Wiedeking, E.Z.Buthelezi, V.Chudoba, S.V.Fortsch, P.Jones, M.Kamil, J.P.Mira, G.G.O'Neill, E.Sideras-Haddad, B.Singh, S.Siem, G.F.Steyn, J.A.Swartz, I.T.Usman, J.J.van Zyl

Investigating the predicted breathing-mode excitation of the Hoyle state

NUCLEAR REACTIONS 12C(α, α'), E=200 MeV; 14C(p, t)12C, E not given; measured reaction products. 12C; deduced experimentally observed inclusive yields, monopole resonance as the breathing-mode excitation of the Hoyle state. The K600 spectrometer at the iThemba Laboratory for Accelerator-Based Sciences (iThemba LABS) in South Africa.

doi: 10.1016/j.physletb.2022.136928
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2022OL03      Phys.Rev. C 105, 054319 (2022)

S.D.Olorunfunmi, R.Neveling, J.Carter, P.von Neumann-Cosel, I.T.Usman, P.Adsley, A.Bahini, L.P.L.Baloyi, J.W.Brummer, L.M.Donaldson, H.Jivan, N.Y.Kheswa, K.C.W.Li, D.J.Marin-Lambarri, P.T.Molema, C.S.Moodley, G.G.O'Neill, P.Papka, L.Pellegri, V.Pesudo, E.Sideras-Haddad, F.D.Smit, G.F.Steyn, A.A.Avaa, F.Diel, F.Dunkel, P.Jones, V.Karayonchev

Evolution of the isoscalar giant monopole resonance in the Ca isotope chain

NUCLEAR REACTIONS Ca, 42,44,48Ca(α, α'), E=196 MeV; measured Eα, Iα; deduced σ(θ), isoscalar giant monopole resonance strength distribution in the 9.5-25.5 MeV range, nucleus incompressibility KA. Analysis with difference-of-spectra (DoS) technique using measurements at 2 different angular covege settings of the spectrometer. Comparison to previous experimental results. K600 magnetic spectrometer at iThemba LABS.

doi: 10.1103/PhysRevC.105.054319
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD1023.


2021ST01      Appl.Radiat.Isot. 168, 109469 (2021)

G.F.Steyn, T.N.van der Walt, F.Szelecsenyi, C.Perrang, J.W.Brummer, C.Vermeulen, N.P.van der Meulen, M.A.Motetshwane, M.R.van Heerden

Large-scale production of 88Y and 88Zr/88Y generators: A proof of concept study for a 70 MeV H- cyclotron

NUCLEAR REACTIONS Sr, 89Y, Zr, 93Nb(p, X)88Y, 89Y, Zr, 93Nb(p, X)88Zr, E<70 MeV; analyzed available data; deduced integral (physical) yields.

doi: 10.1016/j.apradiso.2020.109469
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2021ST02      Appl.Radiat.Isot. 168, 109514 (2021)

G.F.Steyn, M.A.Motetshwane, F.Szelecsenyi, J.W.Brummer

Pairing of thorium with selected primary target materials in tandem configurations: Co-production of 225Ac/213Bi and 230U/226Th generators with a 70 MeV H- cyclotron

NUCLEAR REACTIONS 232Th(p, X)225Ac/225Ra/230Pa, Mg(p, X)22Na/24Na, E<70 MeV; measured reaction products, Eγ, Iγ; deduced σ, integral (physical) yield. Comparison with available data.

doi: 10.1016/j.apradiso.2020.109514
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD1013.


2020AC02      Nucl.Phys. A996, 121795 (2020)

J.Acharya, S.Mukherjee, G.F.Steyn, S.V.Fortsch, F.D.Smit, R.T.Newman, J.J.Lawrie, O.V.Fotina, A.Chatterjee

Non-equilibrium emission of alpha particles in the interaction of 14N with 59Co and 93Nb at incident energy of 250 MeV

doi: 10.1016/j.nuclphysa.2020.121695
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD0975.


2020DO11      Phys.Rev. C 102, 064327 (2020)

L.M.Donaldson, J.Carter, P.von Neumann-Cosel, V.O.Nesterenko, R.Neveling, P.-G.Reinhard, I.T.Usman, P.Adsley, C.A.Bertulani, J.W.Brummer, E.Z.Buthelezi, G.R.J.Cooper, R.W.Fearick, S.V.Fortsch, H.Fujita, Y.Fujita, M.Jingo, N.Y.Kheswa, W.Kleinig, C.O.Kureba, J.Kvasil, M.Latif, K.C.W.Li, J.P.Mira, F.Nemulodi, P.Papka, L.Pellegri, N.Pietralla, V.Yu.Ponomarev, B.Rebeiro, A.Richter, N.Yu.Shirikova, E.Sideras-Haddad, A.V.Sushkov, F.D.Smit, G.F.Steyn, J.A.Swartz, A.Tamii

Fine structure of the isovector giant dipole resonance in 142-150Nd and 152Sm

NUCLEAR REACTIONS 142,144,146,148,150Nd, 152Sm(p, p'), E=200 MeV from the Separated Sector Cyclotron (SSC) at iThemba LABS; measured reaction products, E(p), I(p), time-of-flight using the K600 magnetic spectrometer, two multiwire drift chambers (MWDCs) and two plastic scintillators; deduced double-differential σ(E*=10-22 MeV), equivalent photoabsorption spectra, excitation-energy spectra, wavelet power spectra, fine structure of the isovector giant-dipole resonance (IVGDR), fragmentation of the one-particle-one-hole (1p1h) strength into several dominant transitions serving as doorway states in the spherical and intermediate spherical/deformed nuclei. Comparison with predictions of quasiparticle phonon model (QPM), and Skyrme separable random phase approximation (SSRPA).

doi: 10.1103/PhysRevC.102.064327
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD0860.


2018AC05      Phys.Rev. C 97, 034607 (2018)

Ja.Acharya, S.Mukherjee, A.Chatterjee, N.L.Singh, K.Ramachandran, P.C.Rout, K.Mahata, V.Desai, E.T.Mirgule, S.V.Suryanarayana, B.K.Nayak, A.Saxena, G.F.Steyn

Neutron emission in 19F-induced reactions

NUCLEAR REACTIONS 51V, 89Y, 181Ta(19F, X), E=130, 140, 145, 150 MeV; measured neutron energy spectra by time-of-flight method, neutron emission differential σ(θ, E) at BARC-TIFR Pelletron-LINAC facility. Comparison with theoretical cross sections from the nuclear reaction code ALICE2014 with two density models. Comparison of experimental n(θ) with theoretical calculations using statistical model code Projection Angular-Momentum Coupled Evaporation (PACE4) and ALICE2014.

doi: 10.1103/PhysRevC.97.034607
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD6339.


2018DO01      Phys.Lett. B 776, 133 (2018)

L.M.Donaldson, C.A.Bertulani, J.Carter, V.O.Nesterenko, P.von Neumann-Cosel, R.Neveling, V.Yu.Ponomarev, P.-G.Reinhard, I.T.Usman, P.Adsley, J.W.Brummer, E.Z.Buthelezi, G.R.J.Cooper, R.W.Fearick, S.V.Fortsch, H.Fujita, Y.Fujita, M.Jingo, W.Kleinig, C.O.Kureba, J.Kvasil, M.Latif, K.C.W.Li, J.P.Mira, F.Nemulodi, P.Papka, L.Pellegri, N.Pietralla, A.Richter, E.Sideras-Haddad, F.D.Smit, G.F.Steyn, J.A.Swartz, A.Tamii

Deformation dependence of the isovector giant dipole resonance: The neodymium isotopic chain revisited

NUCLEAR REACTIONS 144,146,148,150Nd, 152Sm(p, p'), E=200 MeV; measured reaction products, Eγ, Iγ; deduced σ, σ(θ, E), σ(θ). Comparison with DWBA calculations.

doi: 10.1016/j.physletb.2017.11.025
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD0860. Data from this article have been entered in the XUNDL database. For more information, click here.


2018MU16      Phys.Rev. C 98, 051302 (2018)

N.J.Mukwevho, B.M.Rebeiro, D.J.Marin-Lambarri, S.Triambak, P.Adsley, N.Y.Kheswa, R.Neveling, L.Pellegri, V.Pesudo, F.D.Smit, E.H.Akakpo, J.W.Brummer, S.Jongile, M.Kamil, P.Z.Mabika, F.Nemulodi, J.N.Orce, P.Papka, G.F.Steyn, W.Yahia-Cherif

Second T=3/2 state in 9B and the isobaric multiplet mass equation

NUCLEAR REACTIONS 9Be(3He, t), (3He, d), E=50.61 MeV pulsed beam; measured E(t), I(t), E(d), I(d), and time-of-flight using the K600 magnetic spectrometer with multiwire drift chamber and plastic scintillator for particle identification at the cyclotron facility of iThemba LABS. 9B; deduced levels, J, π, isospin, energy of the second T=3/2 state. Comparison with previous experimental data. Discussed implications for the cubic isobaric multiplet mass equation (IMME) for the A=9 system.

doi: 10.1103/PhysRevC.98.051302
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Data from this article have been entered in the XUNDL database. For more information, click here.


2016AC01      Phys.Rev. C 93, 024608 (2016)

J.Acharya, S.Mukherjee, G.F.Steyn, N.L.Singh, A.Chatterjee

Excitation functions of heavy residues produced in the 14N + 103Rh reaction up to 400 MeV: Analysis of the pre-equilibrium mechanism with the hybrid Monte Carlo simulation model

NUCLEAR REACTIONS 103Rh(14N, X)94Tc/95Tc/96Tc/95Ru/97Ru/97Rh/99Rh/101Rh/99Pd/100Pd/101Pd/103Ag/104Ag/105Ag/104Cd, E=89.4-400.0 MeV; measured Eγ, Iγ, σ(E) by activation method at iThemba LABS. Comparison with theoretical calculations using the hybrid Monte Carlo simulation model and ALICE2014 code with different level density models. Best agreement with Obninsk level densities.

doi: 10.1103/PhysRevC.93.024608
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD0792.


2016VA06      Appl.Radiat.Isot. 115, 125 (2016)

N.P.van der Meulen, G.F.Steyn, C.Vermeulen, T.J.van Rooyen

Production of 28Mg by bombardment of natCl with 200 MeV protons: Proof-of-concept study for a stacked LiCl target

NUCLEAR REACTIONS Cl(p, X)28Mg, E=200 MeV; measured reaction products, Eγ, Iγ; deduced yields, σ. Comparison with MCNP calculations, TENDL-2015 library.

doi: 10.1016/j.apradiso.2016.04.026
Citations: PlumX Metrics


2015SW01      Phys.Rev. C 91, 034317 (2015)

J.A.Swartz, B.A.Brown, P.Papka, F.D.Smit, R.Neveling, E.Z.Buthelezi, S.V.Fortsch, M.Freer, Tz.Kokalova, J.P.Mira, F.Nemulodi, J.N.Orce, W.A.Richter, G.F.Steyn

Spectroscopy of narrow, high-lying, low-spin states in 20Ne

NUCLEAR REACTIONS 22Ne(p, t), E=60 MeV; measured triton spectra, σ(θ) using QDD magnetic spectrometer at iThemba Labs. 20Ne; deduced levels, J, π, possible 5α cluster state, isospin T=2 states in 20Ne, 20O and 20F. Comparison of angular distributions with calculations using FRESCO code, and structure data with shell-model calculations using OXBASH code.

doi: 10.1103/PhysRevC.91.034317
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD0768. Data from this article have been entered in the XUNDL database. For more information, click here.


2015SZ04      Nucl.Instrum.Methods Phys.Res. B343, 173 (2015); Erratum Nucl.Instrum.Methods Phys.Res. B447, 113 (2019)

F.Szelecsenyi, G.F.Steyn, Z.Kovacs, C.Vermeulen, K.Nagatsu, M.-R.Zhang, K.Suzuki

Excitation functions of natZr + p nuclear processes up to 70 MeV: New measurements and compilation

NUCLEAR REACTIONS Zr(p, X)89Nb/90Nb/91Nb/92Nb/95Nb/96Nb/86Zr/87Zr/88Zr/89Zr/95Zr/85Y/86Y/87Y/88Y/90Y/91Y/85Sr, E<70 MeV; measured reaction products, Eγ, Iγ; deduced σ. Comparison with TALYS nuclear model code calculations.

doi: 10.1016/j.nimb.2014.11.081
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD4317.


2015VA04      Phys.Rev. C 91, 024614 (2015)

J.J.van Zyl, A.A.Cowley, R.Neveling, E.Z.Buthelezi, S.V.Fortsch, J.Mabiala, J.P.Mira, F.Nemulodi, F.D.Smit, G.F.Steyn, J.A.Swartz, I.T.Usman

Incident-energy dependence of angular distributions of cross section and analyzing power for the 58Ni (p(pol) 3He) reaction between 80 and 120 MeV

NUCLEAR REACTIONS 58Ni(polarized p, 3He)56Co, E=80, 100, 118 MeV; measured 3He spectra, σ(θ), analyzing powers at cyclotron facility of iThemba LABS. 56Co; deduced levels, l-transfers, J, π, spectroscopic factors. Optical model, and macroscopic zero-range distorted-wave Born approximation (DWBA) analyses. Comparison with previous experimental results.

doi: 10.1103/PhysRevC.91.024614
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD0766. Data from this article have been entered in the XUNDL database. For more information, click here.


2014ST01      Nucl.Instrum.Methods Phys.Res. B319, 128 (2014)

G.F.Steyn, C.Vermeulen, F.Szelecsenyi, Z.Kovacs, A.Hohn, N.P.van der Meulen, R.Schibli, T.N.van der Walt

Cross sections of proton-induced reactions on 152Gd, 155Gd and 159Tb with emphasis on the production of selected Tb radionuclides

NUCLEAR REACTIONS Cu(p, xn)62Zn, Tb(p, X)153Dy/155Dy/157Dy/159Dy, 152,155Gd(p, 4n), 159Tb(p, 5n), (p, 3n), Tb(p, X)153Tb/154Tb/155Tb/156Tb/151Gd/153Gd, E<70 MeV; measured reaction products, Eγ, Iγ; deduced σ, integral yields. Comparison with ALICE/ASH and TENDL 2012 calculations.

doi: 10.1016/j.nimb.2013.11.013
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2013VA01      Appl.Radiat.Isot. 72, 96 (2013); Erratum Appl.Radiat.Isot. 83, 36 (2014)

N.P.van der Meulen, T.N.van der Walt, G.F.Steyn, H.G.Raubenheimer

The production of 82Sr using larger format RbCl targets

NUCLEAR REACTIONS Rb(p, X)82Sr, E=66 MeV; measured reaction products, Eγ, Iγ; deduced yields. Radiochemical separation.

doi: 10.1016/j.apradiso.2012.09.017
Citations: PlumX Metrics


2012SM06      Phys.Rev. C 86, 037301 (2012)

F.D.Smit, F.Nemulodi, Z.Buthelezi, J.Carter, R.W.Fearick, S.V.Fortsch, M.Freer, H.Fujita, M.Jingo, C.O.Kureba, J.Mabiala, J.Mira, R.Neveling, P.Papka, G.F.Steyn, J.A.Swartz, I.T.Usman, J.J.van Zyl

No evidence of an 11.16 MeV 2+ state in 12C

NUCLEAR REACTIONS 11B(3He, d)12C, E=44 MeV; measured Ed, Id, energy loss, time of flight using magnetic spectrometer, σ(θ). R-matrix analysis; deduced level; no evidence for a previously reported 2+ state at 11.16 MeV.

doi: 10.1103/PhysRevC.86.037301
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Data from this article have been entered in the XUNDL database. For more information, click here.


2012VE02      Nucl.Instrum.Methods Phys.Res. B275, 24 (2012)

C.Vermeulen, G.F.Steyn, F.Szelecsenyi, Z.Kovacs, K.Suzuki, K.Nagatsu, T.Fukumura, A.Hohn, T.N.van der Walt

Cross sections of proton-induced reactions on natGd with special emphasis on the production possibilities of 152Tb and 155Tb

NUCLEAR REACTIONS Gd(p, X)151Tb/152Tb/153Tb/154Tb/155Tb/156Tb/160Tb, E<66 MeV; measured reaction products, Eγ, Iγ; deduced σ, yields. Comparison with ALICE/ASH nuclear model calculations.

doi: 10.1016/j.nimb.2011.12.064
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD4267.


2011SP02      J.Korean Phys.Soc. 59, 1983s (2011)

I.Sphan, M.M.Shehata, S.Spellerberg, B.Scholten, H.H.Coenen, S.Q.Qaim, G.F.Steyn, C.Vermeulen, Z.Kovacs, F.Szelecsenyi

Investigation of Production Possibilities of Radiobromines for Diagnostic and Therapeutic Applications

NUCLEAR REACTIONS 77Se(p, n), (p, 2n), 78Se(p, 2n), (p, 3n)E=21-66 MeV;80Se(p, n)80mBr, E=2.5-18 MeV;80Se(p, 4n), (p, 5n), E=21-85 MeV; measured induced Eγ, Iγ using stacked-foil; deduced σ, 75,76,77,80mBr integral yields. Considered radioisotopic purity of produced medical isotopes.

doi: 10.3938/jkps.59.1983
Citations: PlumX Metrics


2011ST26      J.Korean Phys.Soc. 59, 1991s (2011)

G.F.Steyn, C.Vermeulen, F.Szelecsenyi, Z.Kovacs, K.Suzuki, T.Fukumura, K.Nagatsu

Excitation Functions of Proton Induced Reactions on 89Y and 93Nb with Emphasis on the Production of Selected Radio-Zirconiums

NUCLEAR REACTIONS 89Y(p, n), (p, 2n), E=0-70 MeV;93Nb(p, αn), (p, 3n2p), (p, α2n), (p, 4n2p), E=0-70 MeV;93Nb(p, 2np), (p, 3np), E=0-70 MeV; measured off-line Eγ, Iγ using stacked foil; deduced σ. Compared with other data. 89Y(p, n), (p, 2n), 93Nb(p, α2n), (p, 2np), E=10-70 MeV; measured thick target yields.

doi: 10.3938/jkps.59.1991
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD0629.


2010SP05      Radiochim.Acta 98, 749 (2010)

I.Spahn, G.F.Steyn, C.Vermeulen, Z.Kovacs, F.Szelecsenyi, M.M.Shehata, S.Spellerberg, B.Scholten, H.H.Coenen, S.M.Qaim

New cross section measurements for the production of the Auger electron emitters 77Br and 80mBr

NUCLEAR REACTIONS 77,78,80Se(p, n), (p, 2n), (p, 4n)77Br, 80Se(p, n), E=21-85 MeV; measured Eγ, Iγ; deduced σ and their uncertainties, integral yields.

doi: 10.1524/ract.2010.1781
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD4239.


2010SZ03      Nucl.Instrum.Methods Phys.Res. B268, 3306 (2010)

F.Szelecsenyi, C.Vermeulen, G.F.Steyn, Z.Kovacs, K.Aardaneh, T.N.van der Walt

Excitation functions of 186, 187, 188, 189, 190, 192Ir formed in proton-induced reactions on highly enriched 192Os up to 66 MeV

NUCLEAR REACTIONS 192Os(p, n), (p, 3n), (p, 4n), (p, 5n), (p, 6n), Cu(p, n)65Zn, Al(p, X)24Na, Cu(p, X)62Zn E < 66 MeV; measured reaction products, Eγ, Iγ; deduced σ, integral yields. Comparison with model code ALICE/ASH.

doi: 10.1016/j.nimb.2010.07.010
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD0633.


2009CO01      Europhys.Lett. 85, 22001 (2009)

A.A.Cowley, J.Mabiala, E.Z.Buthelezi, S.V.Fortsch, R.Neveling, F.D.Smit, G.F.Steyn, J.J.van Zyl

Analyzing power distribution in the 12C(p, pα)8Be(g.s.) reaction at an incident energy of 100 MeV

NUCLEAR REACTIONS 12C(p, pα), E=101 MeV; measured cross section and analyzing power.

doi: 10.1209/0295-5075/85/22001
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO1724.


2009MA21      Phys.Rev. C 79, 054612 (2009)

J.Mabiala, A.A.Cowley, S.V.Fortsch, E.Z.Buthelezi, R.Neveling, F.D.Smit, G.F.Steyn, J.J.Van Zyl

Analyzing power and cross section distributions of the 12C(p, pα)8Be cluster knockout reaction at an incident energy of 100 MeV

NUCLEAR REACTIONS 12C(polarized p, pα)8Be, E=100 MeV; measured particle spectra, (particle)(particle)-coin, σ, σ(θ), vector analyzing powers; deduced energy sharing cross sections with different optical potential model parameters and spectroscopic factors. Distorted-wave impulse approximation (DWIA) analysis.

doi: 10.1103/PhysRevC.79.054612
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC1704.


2009SP01      Radiochim.Acta 465, 535 (2009)

I.Spahn, G.F.Steyn, C.Vermeulen, Z.Kovacs, F.Szelecsenyi, H.H.Coenen, S.M.Qaim

New cross section measurements for production of the positron emitters 75Br and 76Br via intermediate energy proton induced reactions

NUCLEAR REACTIONS 77,78,80Se(p, xn)75Br/76Br, E<85 MeV; measured Eγ, Iγ; deduced σ, yields. Comparison with ALICE-IPPE code.

doi: 10.1524/ract.2009.1636
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD0568.


2009SZ01      Nucl.Instrum.Methods Phys.Res. B267, 1877 (2009)

F.Szelecsenyi, G.F.Steyn, S.G.Dolley, Z.Kovacs, C.Vermeulen, T.N.van der Walt

Investigation of the 68Zn(p, 2p)67Cu nuclear reaction: New measurements up to 40 MeV and compilation up to 100 MeV

NUCLEAR REACTIONS 68Zn(p, 2p), E=19.2-39.7 MeV; Measured σ; compiled and evaluated earlier measurements.

doi: 10.1016/j.nimb.2009.03.097
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD0574.


2009SZ03      J.Radioanal.Nucl.Chem. 282, 261 (2009)

F.Szelecsenyi, G.F.Steyn, Z.Kovacs, K.Aardaneh, C.Vermeulen, T.N.van der Walt

Production possibility of 186Re via the 192Os(p, α3n)186Re

NUCLEAR REACTIONS 192Os(p, α3n), 186W(p, n), (d, 2n), Cu(p, X)65Zn, Al(p, X)24Na, E<66.7 MeV; measured reaction products, Eγ, Iγ; deduced σ, uncertainties.

doi: 10.1007/s10967-009-0147-y
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2009VA05      Appl.Radiat.Isot. 67, 1320 (2009)

N.P.van der Meulen, T.N.van der Walt, G.F.Steyn, F.Szelecsenyi, Z.Kovacs, C.M.Perrang, H.G.Raubenheimer

The production of 88Y in the proton bombardment of natSr: New excitation and separation studies

NUCLEAR REACTIONS 88Sr(p, n), Cu(p, x), E=5-20 MeV; 65Zn; Measured σ. SrCl2 target. Ion exchange chromatographic methods.

doi: 10.1016/j.apradiso.2009.02.058
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2008AA03      J.Radioanal.Nucl.Chem. 276, 831 (2008)

K.Aardaneh, C.Naidoo, G.F.Steyn

Radiochemical separation of 109Cd from a silver target

doi: 10.1007/s10967-008-0640-8
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2008NE04      Phys.Rev. C 77, 037601 (2008); Erratum Phys.Rev. C 78, 069902 (2008)

R.Neveling, A.A.Cowley, Z.Buthelezi, S.V.Fortsch, H.Fujita, G.C.Hillhouse, J.J.Lawrie, G.F.Steyn, F.D.Smit, S.M.Wyngaardt, N.T.Botha, L.Mudau, S.S.Ntshangase

Analyzing power of the 40Ca(p(pol), pα) reaction at 100 MeV

NUCLEAR REACTIONS 40Ca(polarized p, pα), E=100 MeV; measured analyzing powers. comparisons with model calculations. 36Ar; deduced levels, J. DWIA calculations.

doi: 10.1103/PhysRevC.77.037601
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2007CO14      Phys.Rev. C 75, 054617 (2007)

A.A.Cowley, J.Bezuidenhout, S.S.Dimitrova, P.E.Hodgson, S.V.Fortsch, G.C.Hillhouse, N.M.Jacobs, R.Neveling, F.D.Smit, J.A.Stander, G.F.Steyn, J.J.van Zyl

Multistep direct mechanism in the (p(pol), 3He) inclusive reaction on 59Co and 93Nb at incident energies between 100 and 160 MeV

NUCLEAR REACTIONS 59Co, 93Nb(polarized p, 3He), E=40-160 MeV; measured σ, angular distributions and analyzing powers. Compared results to model calculations.

doi: 10.1103/PhysRevC.75.054617
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2007FO10      Nucl.Phys. A797, 1 (2007)

S.V.Fortsch, F.Cerutti, P.Colleoni, E.Gadioli, E.Gadioli Erba, A.Mairani, G.F.Steyn, J.J.Lawrie, F.D.Smit, S.H.Connell, R.W.Fearick, T.Thovhogi

Contributions of complete fusion and break-up-fusion to intermediate mass fragment production in the low energy interaction of 12C and 27Al

NUCLEAR REACTIONS 27Al(12C, X)7Be/9Be/10B/11B/11C/12C/13C/13N/14N/15N/16O/19F/22Ne/23Na/24Mg/26Mg/26Al/27Al/Si, E=156 MeV; 12C(27Al, X)7Be/9Be/10B/11B/11C/12C/13C/13N/14N/15N/16O/19F/22Ne/23Na/24Mg/26Mg/Si, E=348 MeV; measured intermediate mass fragment spectra, σ(θ, E) from fusion and fragmentation. Comparison with Boltzmann Master Equations theory.

doi: 10.1016/j.nuclphysa.2007.09.007
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2007QA01      Appl.Radiat.Isot. 65, 247 (2007)

S.M.Qaim, G.F.Steyn, I.Spahn, S.Spellerberg, T.N.van der Walt, H.H.Coenen

Yield and purity of 82Sr produced via the natRb(p, xn)82Sr process

NUCLEAR REACTIONS Rb(p, xn)85Sr, E=25-45 MeV; measured σ. Rb(p, xn)82Sr/85Sr, E ≈ 5-80 MeV; compiled, analyzed σ; deduced integral yields.

doi: 10.1016/j.apradiso.2006.08.001
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2007SP05      Appl.Radiat.Isot. 65, 1057 (2007)

I.Spahn, G.F.Steyn, F.M.Nortier, H.H.Coenen, S.M.Qaim

Excitation functions of natGe(p, xn)71, 72, 73, 74As reactions up to 100 MeV with a focus on the production of 72As for medical and 73As for environmental studies

NUCLEAR REACTIONS Ge(p, xn)71/72/73/74As, E=18-99 MeV; measured Eγ, Iγ, cross sections and excitation functions using stacked foil activation.

doi: 10.1016/j.apradiso.2007.04.012
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2007VE02      Nucl.Instrum.Methods Phys.Res. B255, 331 (2007)

C.Vermeulen, G.F.Steyn, F.M.Nortier, F.Szelecsenyi, Z.Kovacs, S.M.Qaim

Production of 139Ce by proton-induced reactions on 141Pr and natLa

NUCLEAR REACTIONS 141Pr(p, X)132Ce/133mCe/135Ce/137mCe/139Ce, E ≈ 21-97 MeV; La(p, X)139Ce, E ≈ 4-11 MeV; measured production σ; deduced thick-target yields.

doi: 10.1016/j.nimb.2006.12.145
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2006BU10      Eur.Phys.J. A 28, 193 (2006)

E.Z.Buthelezi, F.Cerutti, E.Gadioli, G.F.Steyn, A.Pepe, S.H.Connell, A.A.Cowley

Excitation functions of evaporation residues in the interaction of 16O with 103Rh at incident energies up to 400 MeV

NUCLEAR REACTIONS 103Rh(16C, X), E=40-400 MeV; measured evaporation residues isotopic production σ, excitation functions. Activation technique, Monte Carlo calculations, Boltzmann Master Equation theory.

doi: 10.1140/epja/i2006-10054-4
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2006ST20      Nucl.Instrum.Methods Phys.Res. B252, 149 (2006)

G.F.Steyn, C.Vermeulen, F.M.Nortier, F.Szelecsenyi, Z.Kovacs, S.M.Qaim

Production of no-carrier-added 139Pr via precursor decay in the proton bombardment of natPr

NUCLEAR REACTIONS Pr(p, X)135Nd/136Nd/137Nd/138Nd/139Nd/139mNd/141Nd/136Pr/137Pr/138mPr, E ≈ 7-97 MeV; measured production σ. Stacked-foil activation technique.

doi: 10.1016/j.nimb.2006.08.012
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2006SZ03      Appl.Radiat.Isot. 64, 789 (2006)

F.Szelecsenyi, G.F.Steyn, Z.Kovacs, T.N.van der Walt, K.Suzuki

Comments on the feasibility of 61Cu production by proton irradiation of natZn on a medical cyclotron

NUCLEAR REACTIONS Zn(p, X)60Cu/61Cu/64Cu, E=7-30 MeV; analyzed σ. Feasibility of large-scale production discussed.

doi: 10.1016/j.apradiso.2006.01.011
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2005AU05      Phys.Rev. C 71, 064606 (2005)

A.Auce, A.Ingemarsson, R.Johansson, M.Lantz, G.Tibell, R.F.Carlson, M.J.Shachno, A.A.Cowley, G.C.Hillhouse, N.M.Jacobs, J.A.Stander, J.J.van Zyl, S.V.Fortsch, J.J.Lawrie, F.D.Smit, G.F.Steyn

Reaction cross sections for protons on 12C, 40Ca, 90Zr, and 208Pb at energies between 80 and 180 MeV

NUCLEAR REACTIONS 12C, 40Ca, 90Zr, 208Pb(p, X), E=80-180 MeV; 58Ni(p, X), E=81 MeV; measured reaction σ. Comparison with model predictions.

doi: 10.1103/PhysRevC.71.064606
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2005BU12      Nucl.Phys. A753, 29 (2005)

E.Z.Buthelezi, F.Cerutti, E.Gadioli, G.F.Steyn, S.H.Connell, A.A.Cowley

Excitation functions of residues in the interaction of 12C with 103Rh up to an incident energy of 400 MeV

NUCLEAR REACTIONS 103Rh(12C, X), E=40-400 MeV; measured evaporation residues isotopic production σ, excitation functions. Activation technique, Monte Carlo calculations, Boltzmann Master Equation theory.

doi: 10.1016/j.nuclphysa.2005.02.126
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2005CA29      Nucl.Instrum.Methods Phys.Res. A547, 541 (2005)

R.F.Carlson, A.Ingemarsson, M.Lantz, G.J.Arendse, A.Auce, A.J.Cox, S.V.Fortsch, N.M.Jacobs, R.Johansson, J.Nyberg, J.Peavy, P.-U.Renberg, O.Sundberg, J.A.Stander, G.F.Steyn, G.Tibell, R.Zorro

A method for measuring light ion reaction cross-sections

NUCLEAR REACTIONS 12C(p, X), E=180 MeV; 12C(α, X), E=192.4 MeV; measured reaction σ. 3,4He(p, p), E ≈ 40 MeV; measured σ(θ). 40Ca(3He, 3He'), E=167 MeV; measured particle spectra. Modified attenuation technique for reaction cross section measurement.

doi: 10.1016/j.nima.2005.04.004
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2005MU28      Nucl.Phys. A761, 190 (2005)

L.J.Mudau, F.Cerutti, E.Gadioli, A.Mairani, S.V.Fortsch, E.Z.Buthelezi, G.F.Steyn, S.H.Connell, J.J.Lawrie, R.Neveling, E.Sideras-Haddad

Production of 3He and 6He fragments in the interaction of 12C with 93Nb at 400 MeV

NUCLEAR REACTIONS 93Nb(12C, 3HeX), (12C, 6HeX), E=400 MeV; measured particle spectra, σ(E, θ); deduced projectile breakup and nucleon coalescence contributions.

doi: 10.1016/j.nuclphysa.2005.07.014
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2005ST02      Nucl.Instrum.Methods Phys.Res. A538, 559 (2005)

G.F.Steyn, S.V.Fortsch, J.J.Lawrie, R.Bassini, E.Gadioli, C.Birattari, S.H.Connell

Detection of single and resonant projectile fragments in 12C-induced reactions to the continuum

doi: 10.1016/j.nima.2004.08.112
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2005SZ02      Nucl.Instrum.Methods Phys.Res. B234, 375 (2005)

F.Szelecsenyi, G.F.Steyn, Z.Kovacs, T.N.van der Walt, K.Suzuki, K.Okada, K.Mukai

New cross-section data for the 66Zn(p, n)66Ga, 68Zn(p, 3n)66Ga, natZn(p, x)66Ga, 68Zn(p, 2n)67Ga and natZn(p, x)67Ga nuclear reactions up to 100 Mev

NUCLEAR REACTIONS 66Zn(p, n), 68Zn(p, 2n), (p, 3n), E ≈ 5-100 MeV; Zn(p, X)66Ga/67Ga, E ≈ 5-100 MeV; measured production σ. Stacked-foil activation, comparison with previous results.

doi: 10.1016/j.nimb.2005.02.011
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2005SZ04      Nucl.Instrum.Methods Phys.Res. B240, 625 (2005)

F.Szelecsenyi, G.F.Steyn, Z.Kovacs, C.Vermeulen, N.P.van der Meulen, S.G.Dolley, T.N.van der Walt, K.Suzuki, K.Mukai

Investigation of the 66Zn(p, 2pn)64Cu and 68Zn(p, x)64Cu nuclear processes up to 100 MeV: Production of 64Cu

NUCLEAR REACTIONS Zn, 68Zn(p, X)64Cu, E ≈ 18-100 MeV; 66Zn(p, n2p), E ≈ 35-100 MeV; measured production σ. Stacked-foil activation technique.

doi: 10.1016/j.nimb.2005.05.057
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2004BU09      Nucl.Phys. A734, 553 (2004)

E.Z.Buthelezi, E.Gadioli, G.F.Steyn, F.Albertini, C.Birattari, M.Cavinato, F.Cerutti, S.H.Connell, A.A.Cowley, E.Fabrici, E.Gadioli Erba

Incomplete fusion of projectile fragments in the interaction of 12C with 103Rh up to 33 MeV per nucleon

NUCLEAR REACTIONS 103Rh(12C, X)105Ag/104Ag/101Pd/100Pd/102Rh/99Rh/97Ru/95Ru/95Tc/94Tc/93mMo/90Mo/90Nb/86Zr/87Y, E=70-400 MeV; analyzed excitation functions; deduced reaction mechanism features.

doi: 10.1016/j.nuclphysa.2004.01.103
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2004KE05      Appl.Radiat.Isot. 60, 939 (2004)

K.Kettern, Yu.N.Shubin, G.F.Steyn, T.N.van der Walt, H.H.Coenen, S.M.Qaim

Formation of short-lived positron emitters in reactions of protons of energies up to 200 MeV with the target elements carbon, nitrogen and oxygen

NUCLEAR REACTIONS C(p, X)11C, E=12-200 MeV; N(p, X)11C/13N, E=7-200 MeV; O(p, X)11C/13N, E=54-200 MeV; measured excitation functions. Stacked-foil activation technique.

doi: 10.1016/j.apradiso.2004.02.007
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2003BE62      Eur.Phys.J. A 18, 639 (2003)

B.Becker, F.Albertini, E.Gadioli, G.F.Steyn, M.Cavinato, S.H.Connell, A.A.Cowley, E.Fabrici, S.V.Fortsch, E.Gadioli Erba, J.J.Lawrie, E.Sideras-Haddad

Emission of Li, 7, 9Be and B fragments in the interaction of 12C with 93Nb between 200 and 400 MeV

NUCLEAR REACTIONS 93Nb(12C, X), E=200-400 MeV; measured intermediate mass fragments σ(E, θ); deduced binary fragmentation contribution, other reaction mechanism features.

doi: 10.1140/epja/i2003-10091-5
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2003BU21      J.Radioanal.Nucl.Chem. 258, 649 (2003)

E.Z.Buthelezi, K.Aardaneh, G.F.Steyn, E.Gadioli, T.N.Van der Walt, F.Albertini, F.Cerutti, S.H.Connell, A.A.Cowley, F.M.Nortier

Isobaric yields and radiochemistry of near-target residues in the interaction of 12C and 16O with 103Rh at an incident energy of 400 MeV

NUCLEAR REACTIONS 103Rh(12C, X), (16O, X), E=400 MeV; measured target-like fragments isotopic production σ. Radiochemical separation.

doi: 10.1023/B:JRNC.0000011764.30879.fb
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2003GA15      Eur.Phys.J. A 17, 195 (2003)

E.Gadioli, G.F.Steyn, F.Albertini, C.Birattari, M.Cavinato, S.H.Connell, A.A.Cowley, E.Fabrici, S.V.Fortsch, E.Gadioli Erba, J.J.Lawrie, M.Pigni, J.P.F.Sellschop, E.Sideras-Haddad

Emission of intermediate-mass fragments in the interaction of 16O with 59Co, 93Nb and 197Au

NUCLEAR REACTIONS 59Co, 93Nb, 197Au(16O, X), E=6-25 MeV/nucleon; measured intermediate mass fragment yields, spectra, σ(E, θ); deduced reaction mechanism features.

doi: 10.1140/epja/i2003-10007-5
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2003SZ01      Appl.Radiat.Isot. 58, 377 (2003)

F.Szelecsenyi, Z.Kovacs, T.N.van der Walt, G.F.Steyn, K.Suzuki, K.Okada

Investigation of the natZn(p, x)62Zn nuclear process up to 70MeV: a new 62Zn/62Cu generator

NUCLEAR REACTIONS Zn(p, X)62Zn/66Ga, E ≈ 24-70 MeV; 66Zn(p, n), (p, 4np), E ≈ 35-67 MeV; measured production σ; deduced thick-target yields. Stacked-foil activation technique.

doi: 10.1016/S0969-8043(02)00345-7
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2002GA32      Nucl.Phys. A708, 391 (2002)

E.Gadioli, G.F.Steyn, C.Birattari, C.Catarisano, M.Cavinato, S.H.Connell, A.A.Cowley, E.Fabrici, S.V.Fortsch, E.Gadioli Erba, J.J.Lawrie, J.P.F.Sellschop, E.Sideras-Haddad

Interplay of Mean Field and Nucleon-Nucleon Interactions in the Production of Carbon Fragments in 16O Induced Reactions at Incident Energies up to 25 MeV/amu

NUCLEAR REACTIONS 59Co, 93Nb(16O, X), E=100, 250, 400 MeV; measured carbon fragments spectra, σ(θ); deduced projectile breakup and nucleon coalescence contributions.

doi: 10.1016/S0375-9474(02)01021-7
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2002GA51      Acta Phys.Hung.N.S. 16, 359 (2002)

E.Gadioli, G.F.Steyn, C.Birattari, C.Catarisano, M.Cavinato, S.H.Connell, E.Fabrici, S.V.Fortsch, E.Gadioli Erba, J.J.Lawrie, F.M.Nortier, J.P.F.Sellschop, E.Sideras-Haddad

Nucleon Coalescence in the Interaction of 16O with 59Co at an Incident Energy of 250 MeV

NUCLEAR REACTIONS 59Co(16O, X), E=250 MeV; measured intermediate mass fragment yields, energy and angular distributions; deduced nucleon coalescence, related reaction mechanism features.

doi: 10.1556/APH.16.2002.1-4.38
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2002NE12      Phys.Rev. C66, 034602 (2002)

R.Neveling, A.A.Cowley, G.F.Steyn, S.V.Fortsch, G.C.Hillhouse, J.Mano, S.M.Wyngaardt

Analyzing Power and Cross Section Distributions of the Knockout Reaction 208Pb(p(pol), 2p)207Tl at an Incident Energy of 202 MeV

NUCLEAR REACTIONS 208Pb(polarized p, 2p), E=202 MeV; measured Ep, σ(θ), Ay(θ); deduced nucleon-nucleon interaction features. Comparison with model predictions.

doi: 10.1103/PhysRevC.66.034602
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2001CA23      Phys.Rev. C63, 057602 (2001)

J.Carter, A.A.Cowley, H.Diesener, R.W.Fearick, S.V.Fortsch, J.J.Lawrie, P.von Neumann-Cosel, J.V.Pilcher, A.Richter, K.Schweda, F.D.Smit, G.F.Steyn, S.Strauch

Role of Knockout Contributions in Giant Resonance Studies with (p, p'x) Reactions

NUCLEAR REACTIONS 48Ca(p, p'n), E=100 MeV; 40Ca(p, 2p), (p, p'α), E=100 MeV; measured proton spectra, σ(θ), angular correlations. Comparison with DWIA calculations.

doi: 10.1103/PhysRevC.63.057602
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2001GA47      Eur.Phys.J. A 11, 161 (2001)

E.Gadioli, G.F.Steyn, C.Birattari, M.Cavinato, S.H.Connell, A.A.Cowley, E.Fabrici, S.V.Fortsch, E.Gadioli Erba, J.J.Lawrie, F.M.Nortier, J.P.F.Sellschop, E.Sideras-Haddad

Emission of 8Begs in the Interaction of 12C with Nuclei at Incident Energies up to 33 MeV/amu

NUCLEAR REACTIONS 59Co, 93Nb, 197Au(12C, X), E=100-400 MeV; measured σ(θ) vs 8Be energy for 8Be emission, break-up and coalescence contributions. Breakup mechanisms discussed.

doi: 10.1007/s100500170082
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2001IN03      Nucl.Phys. A696, 3 (2001)

A.Ingemarsson, G.J.Arendse, A.Auce, R.F.Carlson, A.A.Cowley, A.J.Cox, S.V.Fortsch, R.Johansson, B.R.Karlson, M.Lantz, J.Peavy, J.A.Stander, G.F.Steyn, G.Tibell

Reaction Cross Sections of Intermediate Energy 3He-Particles on Targets from 9Be to 208Pb

NUCLEAR REACTIONS 9Be, 12C, 16O, 28Si, 40Ca, 58,60Ni, 112,116,118,120,124Sn, 208Pb(3He, X), E=96, 138, 167 MeV; measured reaction σ; deduced reaction mechanism features. Comparison with optical model predictions.

doi: 10.1016/S0375-9474(01)01116-2
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2001RI01      Phys.Rev. C63, 014610 (2001)

D.Ridikas, W.Mittig, H.Savajols, P.Roussel-Chomaz, S.V.Fortsch, J.J.Lawrie, G.F.Steyn

Inclusive Proton Production Cross Sections in (d, xp) Reactions Induced by 100 MeV Deuterons

NUCLEAR REACTIONS 9Be, 12C, 27Al, 58Ni, 93Nb, 181Ta, 208Pb, 238U(d, pX), E=100 MeV; measured proton spectra, σ(E, θ); deduced reaction mechanism features. Comparisons with model predictions.

doi: 10.1103/PhysRevC.63.014610
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2001SC25      Phys.Lett. 506B, 247 (2001)

K.Schweda, J.Carter, A.A.Cowley, H.Diesener, R.W.Fearick, S.V.Fortsch, J.J.Lawrie, P.von Neumann-Cosel, J.V.Pilcher, A.Richter, F.D.Smit, G.F.Steyn, S.Strauch

Low-Energy Isocalar Quadrupole Strength in 40Ca and 48Ca from (p, p'x) Reactions

NUCLEAR REACTIONS 40Ca(p, pα), (p, 2p), 48Ca(p, np), E=100 MeV; measured σ(θ). 40,48Ca deduced B(E2) distributions vs excitation energy. Comparison with (e, e') results. DWBA analysis.

doi: 10.1016/S0370-2693(01)00230-1
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2000CO28      Phys.Rev. C62, 064604 (2000)

A.A.Cowley, G.F.Steyn, Y.Watanabe, T.Noro, K.Tamura, M.Kawabata, K.Hatanaka, H.Sakaguchi, H.Takeda, M.Itoh

Inclusive Reaction 40Ca(p, p'x) at an Incident Energy of 392 MeV

NUCLEAR REACTIONS 40Ca(p, p'X), E=392 MeV; measured proton spectra, σ(E, θ); deduced reaction mechanism features. Semiclassical distorted wave analysis.

doi: 10.1103/PhysRevC.62.064604
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2000CO29      Phys.Rev. C62, 064605 (2000)

A.A.Cowley, G.F.Steyn, S.S.Dimitrova, P.E.Hodgson, G.J.Arendse, S.V.Fortsch, G.C.Hillhouse, J.J.Lawrie, R.Neveling, W.A.Richter, J.A.Stander, S.M.Wyngaardt

Multistep Direct Mechanism in the (p(pol), 3He) Inclusive Reaction on 59Co and 93Nb at an Incident Energy of 100 MeV

NUCLEAR REACTIONS 59Co, 93Nb(polarized p, 3He), E=100 MeV; measured σ(E, θ), Ay(θ); deduced one-step, multistep process contributions, other reaction mechanism features. Comparison with model predictions.

doi: 10.1103/PhysRevC.62.064605
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2000GA39      Eur.Phys.J. A 8, 373 (2000)

E.Gadioli, M.Cavinato, E.Fabrici, E.Gadioli Erba, R.Bassini, C.Birattari, S.Crippa, G.F.Steyn, S.V.Fortsch, J.J.Lawrie, F.M.Nortier, S.H.Connell, E.Sideras-Haddad, J.P.F.Sellschop, A.A.Cowley

Evidence for a Dissipative Friction Mechanism Based on 8Be Fragments from the Interaction of 12C with 59Co

NUCLEAR REACTIONS 59Co(12C, 8Be), E=8.3-33.3 MeV/nucleon; measured σ(θ), αα-coin. Effect of projectile break up discussed. Comparison with model predictions.

doi: 10.1007/s100500070089
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1999CH50      Nucl.Phys. (Supplement) A654, 1051c (1999)

M.B.Chadwick, D.T.L.Jones, G.J.Arendse, A.A.Cowley, W.A.Richter, J.J.Lawrie, R.T.Newman, J.V.Pilcher, F.D.Smit, G.F.Steyn, J.W.Koen, J.A.Stander

Nuclear Interaction Cross Sections for Proton Radiotherapy

NUCLEAR REACTIONS 12C(p, pX), (p, dX), E=150 MeV; 16O(p, αX), (p, tX), E=200 MeV; measured σ(E, θ). 12C, 16O(p, pX), E=200 MeV; calculated proton spectra, σ(θ). 16O(p, X)7Li/7Be/9Be/10Be/10B/11B/10C/11C/14C/13N/14O/15O, E ≈ 5-250 MeV; calculated production σ.

doi: 10.1016/S0375-9474(00)88598-X
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1999GA39      Nucl.Phys. A654, 523 (1999)

E.Gadioli, M.Cavinato, E.Fabrici, E.Gadioli Erba, C.Birattari, I.Mica, S.Solia, G.F.Steyn, S.V.Fortsch, J.J.Lawrie, F.M.Nortier, T.G.Stevens, S.H.Connell, J.P.F.Sellschop, A.A.Cowley

Alpha Particle Emission in the Interaction of 12C with 59Co and 93Nb at Incident Energies of 300 and 400 MeV

NUCLEAR REACTIONS 59Co, 93Nb(12C, αX), E=300, 400 MeV; measured α spectra, σ(Eα, θ); deduced reaction mechanism features.

doi: 10.1016/S0375-9474(00)88492-4
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1999ST06      Phys.Rev. C59, 2097 (1999)

G.F.Steyn, S.V.Fortsch, A.A.Cowley, J.J.Lawrie, G.J.Arendse, G.C.Hillhouse, J.V.Pilcher, F.D.Smit, R.Neveling

α-Clustering Probabilities Extracted from the 12C(α, 2α)8Be Reaction at 200 MeV

NUCLEAR REACTIONS 12C(α, 2α), E=200 MeV; measured Eα, αα-coin, σ(E, θ); deduced α-cluster spectroscopic factors. DWIA analysis.

doi: 10.1103/PhysRevC.59.2097
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1998CA11      Nucl.Phys. A630, 631 (1998)

J.Carter, A.A.Cowley, H.Diesener, R.W.Fearick, S.V.Fortsch, M.N.Harakeh, J.J.Lawrie, S.J.Mills, P.von Neumann-Cosel, R.T.Newman, J.V.Pilcher, A.Richter, K.Schweda, F.D.Smit, G.F.Steyn, S.Strauch, D.M.Whittal

Isoscalar Quadrupole Strength in 40Ca from the (p, p'α0) Reaction at E(p) = 100 MeV

NUCLEAR REACTIONS 40Ca(p, p'α), E=99.5 MeV; measured σ(θ(p), θ(α), E(x)); deduced α0 channel multipole distribution, isoscalar E2 strength distribution.

doi: 10.1016/S0375-9474(98)00656-3
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1998CO13      Phys.Rev. C57, 3185 (1998)

A.A.Cowley, G.J.Arendse, R.F.Visser, G.F.Steyn, S.V.Fortsch, J.J.Lawrie, J.V.Pilcher, T.Noro, T.Baba, K.Hatanaka, M.Kawabata, N.Matsuoka, Y.Mizuno, M.Nomachi, K.Takahisa, K.Tamura, Y.Yuasa, H.Sakaguchi, T.Itoh, H.Takeda, Y.Watanabe

Rescattering in Knockout Reactions as Manifested in 40Ca(p, p'p'') at an Incident Energy of 392 MeV

NUCLEAR REACTIONS 40Ca(p, 2p), E=392 MeV; measured σ(E(p1), E(p2), θ); deduced reaction mechanism. DWIA analysis.

doi: 10.1103/PhysRevC.57.3185
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1998GA32      Acta Phys.Hung.N.S. 7, 275 (1998)

E.Gadioli, C.Birattari, M.Cavinato, E.Fabrici, E.Gadioli Erba, V.Allori, G.Bello, F.Cerutti, A.Di Filippo, T.G.Stevens, S.H.Connell, J.P.F.Sellschop, F.M.Nortier, G.F.Steyn, C.Marchetta

The Interaction of 12C and 16O with 103Rh

NUCLEAR REACTIONS 103Rh(12C, X)113Sn/111In/110Sn/108In/105Ag/102Rh, E=50-400 MeV; 103Rh(16O, X)115Sb/113Sn/110Sn/111In/108In/105Ag/103Ag/101Pd/101Rh/100Rh/95Ru/94Tc, E=50-400 MeV; calculated excitation functions; deduced pre-equilibrium emission, other reaction mechanism features. Comparison with data.


1998GA36      Nucl.Phys. A641, 271 (1998)

E.Gadioli, C.Birattari, M.Cavinato, E.Fabrici, E.Gadioli Erba, V.Allori, F.Cerutti, A.Di Filippo, S.Vailati, T.G.Stevens, S.H.Connell, J.P.F.Sellschop, F.M.Nortier, G.F.Steyn, C.Marchetta

Angular Distributions and Forward Recoil Range Distributions of Residues Created in the Interaction of 12C and 16O Ions with 103Rh

NUCLEAR REACTIONS 103Rh(12C, X), E=151, 228 MeV; measured residual nuclei angular distributions, yields; 103Rh(12C, X), E=402 MeV; 103Rh(16O, X), E=303 MeV; measured residual nudlei yields, recoil range distributions; deduced reaction mechanism features, incomplete fusion. Activation technique.

doi: 10.1016/S0375-9474(98)00472-2
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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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1997CO05      Phys.Rev. C55, 1843 (1997)

A.A.Cowley, G.J.Arendse, G.F.Steyn, J.A.Stander, W.A.Richter, S.S.Dimitrova, P.Demetriou, P.E.Hodgson

Inclusive (p, 3He) Reactions on 59Co and 197Au at Incident Energies of 120, 160, and 200 MeV

NUCLEAR REACTIONS 59Co, 197Au(p, 3He), E=120, 160, 200 MeV; measured σ(θ) vs E; deduced multi-step mechanisms role. Statistical multi-step direct reaction theory.

doi: 10.1103/PhysRevC.55.1843
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1997GA09      Phys.Lett. 394B, 29 (1997)

E.Gadioli, C.Birattari, M.Cavinato, E.Fabrici, E.Gadioli Erba, V.Allori, C.Bovati, F.Cerutti, A.Di Filippo, E.Galbiati, T.G.Stevens, S.H.Connell, J.P.F.Sellschop, S.J.Mills, F.M.Nortier, G.F.Steyn, C.Marchetta

Comprehensive Study of the Reactions Induced by 12C on 103Rh up to 33 MeV/nucleon

NUCLEAR REACTIONS 103Rh(12C, X)113Sb/110In/108In/107In/111In/105Ag/104Ag/103Ag/102Ag/101Pd/100Pd/99Rh/98Rh/97Ru/96Tc/95Ru/94Tc/93Mo/93mMo/90Nb, E=45-400 MeV; measured residuals production σ(E). Activation technique.

doi: 10.1016/S0370-2693(97)00003-8
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1996BI19      Phys.Rev. C54, 3051 (1996)

C.Birattari, M.Bonardi, M.Cavinato, E.Fabrici, E.Gadioli, E.Gadioli Erba, F.Groppi, M.Bello, C.Bovati, A.Di Filippo, T.G.Stevens, S.H.Connell, J.P.F.Sellschop, S.J.Mills, F.M.Nortier, G.F.Steyn, C.Marchetta

Preequilibrium Processes in the Fusion of 12C with 103Rh up to 20 MeV/nucleon

NUCLEAR REACTIONS, ICPND 103Rh(12C, xnyp)113Sb/111Sn/110Sn/109Sn/108Sn/113Sn/111In/110In/110mIn, E=40-210 MeV; measured residuals production σ(E); deduced fusion σ, multiplicity of pre-equilibrium particles, mean-field interaction. Boltzmann master equation calculation.

doi: 10.1103/PhysRevC.54.3051
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1996CO12      Phys.Rev. C54, 778 (1996)

A.A.Cowley, G.J.Arendse, J.W.Koen, W.A.Richter, J.A.Stander, G.F.Steyn, P.Demetriou, P.E.Hodgson, Y.Watanabe

Inclusive (p, α) Reactions on 27Al, 59Co, and 197Au at Incident Energies of 120, 160, and 200 MeV

NUCLEAR REACTIONS 27Al, 59Co, 197Au(p, α), E=120, 160, 200 MeV; measured σ(Eα, θ); deduced higher-step contributions role. Multi-step DWBA analysis.

doi: 10.1103/PhysRevC.54.778
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1996ST25      Phys.Rev. C54, 2485 (1996)

G.F.Steyn, S.V.Fortsch, J.J.Lawrie, F.D.Smit, R.T.Newman, A.A.Cowley, R.Lindsay

Single-Nucleon Transfer to Unbound States by Means of the 4He(α, 3He)5He Reaction at 158 and 200 MeV

NUCLEAR REACTIONS 4He(α, 3He), E(cm)=158, 200 MeV; measured yield vs E(3He), 3He spectra, σ(θ). 4He(α, α), E(cm)=158, 200 MeV; measured σ(θ); deduced model parameters, strength factor. DWBA analysis.

doi: 10.1103/PhysRevC.54.2485
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1995NO08      Appl.Radiat.Isot. 46, 1377 (1995)

F.M.Nortier, S.J.Mills, G.F.Steyn

Excitation Functions for the Production of Some Radioisotopes of Cs, Xe and I in Proton Bombardment of (nat)Xe up to 100 MeV

NUCLEAR REACTIONS, ICPND Xe(p, X)125Cs/127Cs/129Cs/130Cs/132Cs/136Cs/136mCs/122Xe/123Xe/125Xe/125mXe/127Xe/127mXe/129Xe/129mXe/124I/126I/130I/130mI/131I, E=threshold-100 MeV; measured residuals production σ(E). Geometry-dependent hybrid model.

doi: 10.1016/0969-8043(95)00216-Z
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1994CO16      Phys.Rev. C50, 2449 (1994)

A.A.Cowley, G.F.Steyn, S.V.Fortsch, J.J.Lawrie, J.V.Pilcher, F.D.Smit, D.M.Whittal

Quasifree Knockout in 9Be(α, 2α)5He at an Incident Energy of 197 MeV

NUCLEAR REACTIONS 9Be(α, 2α), E=197 MeV; measured σ(θ1, θ2). 4He(α, α), E=197 MeV; measured σ(θ); deduced dependence of α-clustering probability, model parameters. 9Be deduced spectroscopic factors. DWIA analysis.

doi: 10.1103/PhysRevC.50.2449
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1994NO10      Appl.Radiat.Isot. 45, 1051 (1994)

F.M.Nortier, S.J.Mills, G.F.Steyn

Excitation Function of the 111Cd(p, n)111m,111gIn Reaction

NUCLEAR REACTIONS, ICPND 111Cd(p, n), E ≤ 30 MeV; compiled, reviewed σ(E) data.

doi: 10.1016/0969-8043(94)90177-5
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1992CO04      Phys.Rev. C45, 1745 (1992)

A.A.Cowley, P.G.Roos, J.J.Lawrie, F.D.Smit, J.V.Pilcher, S.V.Fortsch, G.F.Steyn, G.C.Hillhouse

Quasifree Subthreshold Pion Production in the Reaction 12C(p, dπ+)11B

NUCLEAR REACTIONS 12C(p, dπ+), E=223 MeV; measured σ(θπ, θd, Ed); deduced reaction mechanism. DWIA.

doi: 10.1103/PhysRevC.45.1745
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1992MI14      Appl.Radiat.Isot. 43, 1019 (1992)

S.J.Mills, G.F.Steyn, F.M.Nortier

Experimental and Theoretical Excitation Functions of Radionuclides Produced in Proton Bombardment of Copper up to 200 MeV

NUCLEAR REACTIONS, ICPND Cu(p, X)60Co/52Fe/59Fe/52Mn/54Mn/56Mn/48Cr/49Cr/51Cr/48V/44Sc/44mSc/46Sc, E=200 MeV; measured residuals production effective σ. Model comparison.

doi: 10.1016/0883-2889(92)90221-Y
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1992ST15      Appl.Radiat.Isot. 43, 1323 (1992)

G.F.Steyn, B.R.S.Simpson, S.J.Mills, F.M.Nortier

The Production of 55Fe with Medium-Energy Protons

NUCLEAR REACTIONS 55Mn, 59Co, Ni(p, X)55Fe, E=threshold-100 MeV; measured residual production rates. Thick target. Model comparison.

doi: 10.1016/0883-2889(92)90003-W
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1991NO02      Appl.Radiat.Isot. 42, 353 (1991)

F.M.Nortier, S.J.Mills, G.F.Steyn

Excitation Functions and Yields of Relevance to the Production of 67Ga by Proton Bombardment of (nat)Zn and (nat)Ge up to 100 MeV

NUCLEAR REACTIONS, ICPND Zn(p, X)65Ga/66Ga/67Ga/68Ga, E=8.4-99.6 MeV; Ge(p, X)65Ga/66Ga/67Ga/68Ga/72Ga, E=4.9-97.9 MeV; measured residuals production σ, thick target yields.

doi: 10.1016/0883-2889(91)90138-Q
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1991NO06      Appl.Radiat.Isot. 42, 1105 (1991)

F.M.Nortier, S.J.Mills, G.F.Steyn

Excitation Functions for the Production of 109Cd, 109In and 109Sn in Proton Bombardment of Indium up to 200 MeV

NUCLEAR REACTIONS, ICPND In(p, X)109Cd/109In/109Sn, E ≤ 200 MeV; measured residuals production σ(E). Model calculations.

doi: 10.1016/0883-2889(91)90021-R
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1991ST02      Appl.Radiat.Isot. 42, 361 (1991)

G.F.Steyn, S.J.Mills, F.M.Nortier, F.J.Haasbroek

Integral Excitation Functions for (nat)Kr + p up to 116 MeV and Optimization of the Production of 81Rb for 81mKr Generators

NUCLEAR REACTIONS, ICPND Kr(p, X)79Rb/81Rb/81mRb/82Rb/82mRb/83Rb/84Rb/84mRb/86Rb/77Kr/79Kr/85Kr/85mKr/77Br/82Br, E=threshold-116 MeV; measured thick target production rates, σ(E). Geometry dependent hybrid model.

doi: 10.1016/0883-2889(91)90139-R
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1990NO11      Appl.Radiat.Isot. 41, 1201 (1990)

F.M.Nortier, S.J.Mills, G.F.Steyn

Excitation Functions and Production Rates of Relevance to the Production of 111In by Proton Bombardment of (nat)Cd and (nat)In up to 100 MeV

NUCLEAR REACTIONS, ICPND Cd(p, xn)111In, In(p, xn)111Sn, E=threshold-100 MeV; measured residual production σ(E); deduced thick target production rates.

doi: 10.1016/0883-2889(90)90207-W
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1990ST03      Appl.Radiat.Isot. 41, 315 (1990)

G.F.Steyn, S.J.Mills, F.M.Nortier, B.R.S.Simpson, B.R.Meyer

Production of 52Fe via Proton-Induced Reactions on Manganese and Nickel

NUCLEAR REACTIONS, ICPND 55Mn(p, 4n), E=40-200 MeV; 27Al(p, X)22Na, E=75-200 MeV; Ni(p, X)52Fe, E=45-200 MeV; measured residual production σ(E).

doi: 10.1016/0883-2889(90)90197-O
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