NSR Query Results
Output year order : Descending NSR database version of March 18, 2024. Search: Author = I.Boztosun Found 51 matches. 2022DA12 Eur.Phys.J. A 58, 85 (2022) A realistic numerical treatment of Coulomb potential in comparison with the analytical approximations
doi: 10.1140/epja/s10050-022-00728-4
2022KO11 Int.J.Mod.Phys. E31, 2250032 (2022) G.Kocak, S.Akkoyun, I.Boztosun, H.Dapo Energy transitions and half-life determinations of 47Sc isotopes from photonuclear reaction on Ti target RADIOACTIVITY 47Sc(β-) [from Ti(γ, X), E<18 MeV]; measured decay products, Eγ, Iγ; deduced γ-ray energies, levels, T1/2. Comparison with available data.
doi: 10.1142/S021830132250032X
2022KU22 Eur.Phys.J. A 58, 97 (2022) Y.Kucuk, T.K.Zholdybayev, B.Canbula, Zh.Mukan, B.M.Sadykov, M.Nassurlla, K.M.Ismailov, M.B.Yucel, I.Boztosun A new proton spectra for natCu(p, xp) reaction at Ep = 7 and 30 MeV NUCLEAR REACTIONS Cu(p, xp), E=7, 30 MeV; measured reaction products, Ep, Ip; deduced σ(θ), σ(E). Comparison with theoretical calculations. Isochronous cyclotron U-150M, at the Institute of Nuclear Physics of Kazakhstan.
doi: 10.1140/epja/s10050-022-00740-8
2021KA26 Few-Body Systems 62, 14 (2021) S.Karatepe Celik, I.Boztosun, M.Dogru An Analysis of Elastic Scattering Angular Distributions of 17F on a 208Pb Target at Different Energies NUCLEAR REACTIONS 208Pb(17F, 17F), E=90.4 MeV; analyzed available data; deduced σ, σ(θ) using the Continuum-Discretized Coupled Channels (CDCC) method.
doi: 10.1007/s00601-021-01599-z
2021NA14 Eur.Phys.J. A 57, 231 (2021) M.Nassurlla, N.Burtebayev, B.K.Karakozov, S.B.Sakuta, I.Boztosun, N.Amangeldi, A.K.Morzabayev, G.Yergaliuly, D.K.Alimov, J.Burtebayeva, M.Nassurlla, B.Mauyey, Y.Kucuk, Sh.Hamada, A.Sabidolda, R.Khojayev New measurements and analysis of elastic scattering of 13C by 9Be nuclei in a wide energy range NUCLEAR REACTIONS 9Be(13C, 13C), E=16.25, 19.5, 22.75, 28.12, 36.15, 57.77, 72.88 MeV; measured reaction products; deduced σ, σ(θ). OM and DWBA method, FRESCO program.
doi: 10.1140/epja/s10050-021-00539-z
2020FI09 Universe 6, 129 (2020) P.Finocchiaro, L.Acosta, C.Agodi, C.Altana, P.Amador-Valenzuela, I.Boztosun, S.Brasolin, G.A.Brischetto, O.Brunasso, S.Calabrese, L.Calabretta, D.Calvo, V.Capirossi, F.Cappuzzello, D.Carbone, M.Cavallaro, E.R.Chavez Lomeli, I.Ciraldo, G.D'Agostino, F.Delaunay, H.Djapo, C.Ferraresi, M.Fisichella, D.C.Flechas Garcia, F.Iazzi, L.La Fauci, G.Lanzalone, F.La Via, R.Linares, N.H.Medina, P.Mereu, M.Moralles, J.R.B.Oliveira, L.Pandola, A.Pappalardo, H.Petrascu, F.Pinna, A.D.Russo, D.Sartirana, O.Sgouros, S.O.Solakci, V.Soukeras, A.Spatafora, D.Torresi, S.Tudisco, A.Yildirim, V.A.B.Zagatto The NUMEN Heavy Ion Multidetector for a Complementary Approach to the Neutrinoless Double Beta Decay
doi: 10.3390/universe6090129
2020NA30 Chin.Phys.C 44, 104103 (2020) M.Nassurlla, N.Burtebayev, T.Kh.Sadykov, I.Boztosun, N.Amangeldi, D.Alimov, Z.Kerimkulov, J.Burtebayeva, M.Nassurlla, A.Kurakhmedov, S.B.Sakuta, M.Karakoc, A.A.Ibraheem, K.W.Kemper, S.Hamada New measurements and reanalysis of 14N elastic scattering on 10B target NUCLEAR REACTIONS 10B(14N, 14N), E= 38-94.0 MeV; measured reaction products; deduced σ(θ), possible contribution of the α-cluster exchange mechanism, spectroscopic amplitudes using the optical model and the distorted waves Born approximation method.
doi: 10.1088/1674-1137/abab89
2019TA11 Nucl.Phys. A987, 79 (2019) M.Tamkas, E.Aciksoz, J.Isaak, T.Beck, N.Benouaret, M.Bhike, I.Boztosun, A.Durusoy, U.Gayer, Krishichayan, B.Loher, N.Pietralla, D.Savran, W.Tornow, V.Werner, A.Zilges, M.Zweidinger Low-lying dipole strength in the well-deformed nucleus 156Gd NUCLEAR REACTIONS 156Gd(γ, γ), E=7.1 MeV[bremsstrahlung end-point energy]; measured Eγ, Iγ using three HPGe with BGO active anti-Compton shield; deduced γ-ray energy spectra; 156Gd(polarized γ, γ), E=2.9-6.2 MeV[linearly polarized quasi-monochromatical photon beams from laser Compton backscattering]; measured Eγ, Iγ, γγ-coin at High Intensity γ-ray Source (HIγS) at TUNL; deduced γ-ray measured and deconvoluted energy spectra, asymmetries for observed single states and average asymmetry for each beam energy setting using deconvoluted spectra, expectation B(E1), B(M1) transition values; deduced, extracted photo absorption σγ vs E* and its decomposition to the gs and to the first excited state.
doi: 10.1016/j.nuclphysa.2019.03.014
2018CA16 Eur.Phys.J. A 54, 72 (2018) F.Cappuzzello, C.Agodi, M.Cavallaro, D.Carbone, S.Tudisco, D.Lo Presti, J.R.B.Oliveira, P.Finocchiaro, M.Colonna, D.Rifuggiato, L.Calabretta, D.Calvo, L.Pandola, L.Acosta, N.Auerbach, J.Bellone, R.Bijker, D.Bonanno, D.Bongiovanni, T.Borello-Lewin, I.Boztosun, O.Brunasso, S.Burrello, S.Calabrese, A.Calanna, E.R.Chavez-Lomeli, G.D'Agostino, P.N.De Faria, G.De Geronimo, F.Delaunay, N.Deshmukh, J.L.Ferreira, M.Fisichella, A.Foti, G.Gallo, H.Garcia-Tecocoatzi, V.Greco, A.Hacisalihoglu, F.Iazzi, R.Introzzi, G.Lanzalone, J.A.Lay, F.La Via, H.Lenske, R.Linares, G.Litrico, F.Longhitano, J.Lubian, N.H.Medina, D.R.Mendes, M.Moralles, A.Muoio, A.Pakou, H.Petrascu, F.Pinna, S.Reito, A.D.Russo, G.Russo, G.Santagati, E.Santopinto, R.B.B.Santos, O.Sgouros, M.A.G.da Silveira, S.O.Solakci, G.Souliotis, V.Soukeras, A.Spatafora, D.Torresi, R.Magana Vsevolodovna, A.Yildirim, V.A.B.Zagatto The NUMEN project: NUclear Matrix Elements for Neutrinoless double beta decay
doi: 10.1140/epja/i2018-12509-3
2018CA17 Acta Phys.Pol. B49, 275 (2018) S.Calabrese, F.Cappuzzello, D.Carbone, M.Cavallaro, C.Agodi, L.Acosta, D.Bonanno, D.Bongiovanni, T.Borello-Lewin, I.Boztosun, D.Calvo, E.R.Chavez-Lomeli, N.Deshmukh, P.N.de Faria, P.Finocchiaro, M.Fisichella, A.Foti, G.Gallo, A.Hacisalihoglu, F.Iazzi, R.Introzzi, G.Lanzalone, R.Linares, F.Longhitano, D.Lo Presti, N.Medina, A.Muoio, J.R.B.Oliveira, A.Pakou, L.Pandola, F.Pinna, S.Reito, G.Russo, G.Santagati, O.Sgouros, S.O.Solakci, V.Soukeras, G.Souliotis, A.Spatafora, D.Torresi, S.Tudisco, A.Yildirim, V.A.B.Zagatto First Measurement of the 116Cd(20Ne, 20O)116Sn Reaction at 15 A MeV NUCLEAR REACTIONS 116Cd(20Ne, 20O)116Sn, E=15 MeV/nucleon; measured outgoing 20O ejectiles momentum by the MAGNEX spectrometer and detected by its Focal Plane Detector (FPD), other reaction products using K800 Superconducting cyclotron at INFN-LNS Catania coupled to carbon post-stripper; deduced identified 20O ejectiles. The 116Cd(20Ne, 20O)116Sn reaction has been measured for the first time; Double Charge-Exchange (DCE) measure with heavy ions successful, PID and ray-reconstruction procedures led to excellent signal-to-noise ratio.
doi: 10.5506/aphyspolb.49.275
2016AK04 Int.J.Mod.Phys. E25, 1650045 (2016) S.Akkoyun, T.Bayram, F.Dulger, H.Dapo, I.Boztosun Energy level and half-life determinations from photonuclear reaction on Ga target RADIOACTIVITY 68Ge(EC), 70,72Ge(β-) [from Ga(γ, X), E<18 MeV]; measured decay products, Eγ, Iγ; deduced T1/2. Comparison with available data.
doi: 10.1142/S0218301316500452
2016AY07 Appl.Radiat.Isot. 115, 97 (2016) M.Aygun, A.Cesur, M.Dogru, I.Boztosun, H.Dapo, M.Kanarya, M.F.Kuluozturk, S.S.Bal, S.Karatepe Using a clinical linac to determine the energy levels of 92mNb via the photonuclear reaction RADIOACTIVITY 92Nb(EC) [from 93Nb(γ, n), E<18 MeV]; measured decay products, Eγ, Iγ. 92mNb; deduced γ-ray energies, energy levels. Comparison with available data.
doi: 10.1016/j.apradiso.2016.06.007
2016BA65 Int.J.Mod.Phys. E25, 1650107 (2016) T.Bayram, Se.Akkoyun, S.Uruk, H.Dapo, F.Dulger, I.Boztosun Transition energy and half-life determinations of photonuclear reaction products of erbium nuclei NUCLEAR REACTIONS Er(γ, X)161Ho, E<14 MeV; measured reaction products, Eγ, Iγ; deduced energy levels, J, π. Comparison with available data.
doi: 10.1142/S021830131650107X
2016SE12 Int.J.Mod.Phys. E25, 1650071 (2016) Radial sensitivity of the optical model potentials for 4He+120Sn and 6He+120Sn NUCLEAR REACTIONS 120Sn(α, α), (6He, 6He), E=17.4-30.8 MeV; calculated σ(θ), radii; deduced potential parameters. Comparison with experimental data.
doi: 10.1142/S0218301316500713
2014AY02 Few-Body Systems 55, 203 (2014) An Extended Analysis of the Elastic Scattering of 6Li(6He, 6He)6Li system at 17.9 MeV NUCLEAR REACTIONS 6Li(6He, 6He), E=17.9 MeV; analyzed available data; deduced σ(θ), proton and neutron density distributions. Optical and no-core shell models.
doi: 10.1007/s00601-014-0856-9
2014BO01 Turk.J.Phys. 38, 1 (2014) I.Boztosun, H.Dapo, S.F.Ozmen, Y.Cecen, M.Karakoc, A.Coban, A.Cesur, T.Caner, E.Bayram, G.B.Keller, B.Kucuk, A.Guvendi, M.Derman, D.Kaya The results of the first photonuclear reaction performed in Turkey: the zinc example RADIOACTIVITY 63,65Zn(EC), 69Zn, 67Cu(β-); measured decay products, Eγ, Iγ; deduced T1/2. Comparison with available data.
doi: 10.3906/fiz-1305-19
2014KA27 Phys.Rev. C 89, 064313 (2014) M.Karakoc, R.G.T.Zegers, B.A.Brown, Y.Fujita, T.Adachi, I.Boztosun, H.Fujita, M.Csatlos, J.M.Deaven, C.J.Guess, J.Gulyas, K.Hatanaka, K.Hirota, D.Ishikawa, A.Krasznahorkay, H.Matsubara, R.Meharchand, F.Molina, H.Okamura, H.J.Ong, G.Perdikakis, C.Scholl, Y.Shimbara, G.Susoy, T.Suzuki, A.Tamii, J.H.Thies, J.Zenihiro Gamow-Teller transitions in the A=40 isoquintet of relevance for neutrino captures in 40Ar NUCLEAR REACTIONS 40Ar(3He, t), E=140 MeV/nucleon; measured triton spectra, σ using Grand-Raiden spectrometer at RCNP facility. 40K; deduced levels, J, π, B(GT) DWBA analysis. Main focus on 1+ states at 2290 and 2730 keV. Other details to appear in a future publication. 40Ar(p, n)40K; 40Ti(β+), (EC); analyzed previous experimental results, and compared Gamow-Teller B(GT) strengths in all three studies. Comparison with shell-model calculations in the sd-pf shell with a new interaction (WBMB-C) to study differences between structure of transitions from 40Ar and 40Ti. Discussed ratio of the cross sections for low-lying 1+ states populated in 40Ar(p, n) and 40Ar(3He, t) reactions. Relevance of 40Ar in the use of liquid argon as a medium for neutrino detection.
doi: 10.1103/PhysRevC.89.064313
2014UN04 Phys.Rev. C 89, 057605 (2014) A.Un, Y.Kucuk, T.Caner, I.Boztosun Role of the surface potential in explaining the 11Li+28Si system NUCLEAR REACTIONS 28Si(11Li, 11Li), E=29 MeV/nucleon; analyzed elastic and quasielastic σ(θ) data in the framework of the coupled-channels model using double-folding potential with a Woods-Saxon type of imaginary part, and modified shape of the real and imaginary potentials simultaneously in the surface region.
doi: 10.1103/PhysRevC.89.057605
2012CO10 Phys.Rev. C 85, 044324 (2012) A.Coban, O.Bayrak, A.Soylu, I.Boztosun Effect of nuclear deformation on α-decay half-lives RADIOACTIVITY 106,107,108,109Te, 113I, 112,113Xe, 114Ba, 144Nd, 145Pm, 146,147Sm, 147,148Eu, 148,151,152Gd, 151,152Dy, 152,154Ho, 152,153Er, 153,155Tm, 154,155Yb, 157,158Hf, 160,162W, 160,162Re, 162,166Os, 166,169Ir, 168,170,172,174,176,178,180,182,184,186,188,190,192,194Pt, 170,183Au, 174,177Hg, 177,179Tl, 186,188Pb, 190,192Po, 196,198At, 198,201Rn, 201,203Fr, 205,206Ra, 206,208Ac, 213,216Th, 217,219Pa, 226,228U, 232,234Pu, 238,246Cm, 240,245Cf, 251,253Es, 248,250Fm, 252,254No, 260Sg, 261Bh, 269,270,271,273Ds, 268Mt, 264,265,266,267,269Hs, 264,265,266,267Bh, 261,263,265,266Sg (α); calculated Q(α), T1/2. Wentzel-Kramers-Brillouin (WKB) method and Bohr-Sommerfeld quantization condition. Deformed phenomenological Wood-Saxon form and deformed Coulomb potential. Comparison with experimental data.
doi: 10.1103/PhysRevC.85.044324
2012DA02 Phys.Rev. C 85, 044602 (2012) H.Dapo, I.Boztosun, G.Kocak, A.B.Balantekin Influence of long-range effects on low-energy cross sections of He and HeX: The lithium problem NUCLEAR REACTIONS 2H(α, γ)6Li, E<10 MeV; calculated cross section, dependence of σ on charge and mass for 2H(α, γ)6Li and 2H(αX, X)6Li. Optical model and DWBA analysis. Relevance to 6,7Li in big-bang nucleosynthesis. Comparison with experimental data.
doi: 10.1103/PhysRevC.85.044602
2012SO15 Eur.Phys.J. A 48, 128 (2012) A.Soylu, Y.Sert, O.Bayrak, I.Boztosun Role of the cluster deformations in explaining the exotic decay half-lives RADIOACTIVITY 221Fr, 221,222,223,224,226Ra, 225Ac(14C), 228Th(20O), 230Th, 233U(24Ne), 230U(22Ne), 234U(24Ne), (26Ne), (28Mg), 236Pu(28Mg), 238Pu(28Mg), (30Mg), (32Si), 242Cm(34Si); calculated T1/2 using WKB with Bohr-Sommerfeld condition and considering deformations of daughter nucleus and of the emitted cluster. Compared with data.
doi: 10.1140/epja/i2012-12128-0
2011BA03 Phys.Atomic Nuclei 74, 13 (2011) Semiclassical description of the 6He+12C elastic scattering NUCLEAR REACTIONS 12C(6He, 6He), E=18 MeV; calculated σ(θ), turning points. WKB method, comparison with experimental data.
doi: 10.1134/S1063778811010042
2011IN03 Phys.Rev. C 84, 024309 (2011) I.Inci, D.Bonatsos, I.Boztosun Electric quadrupole transitions of the Bohr Hamiltonian with the Morse potential NUCLEAR STRUCTURE 98,100,102,104Ru, 102,104,106,108Pd, 108,110,112,114,116,118Cd, 118,120,124,128Xe, 130,132,134,142Ba, 148Nd, 152Gd, 154Dy, 192,194,196,198Pt, 154Sm, 156Gd, 158Gd, 158,160Dy, 162Dy, 164Dy, 156,162,164,166,168,170Er, 166,168,170,172,174,176Yb, 174,176,178Hf, 182,184,186W, 186,188Os, 230,232Th, 234,236,238U, 238Pu, 250Cf; calculated B(E2) ratios for ground-state bands and interband transitions in γ-soft and deformed nuclei. Asymptotic iteration method (AIM) for collective Bohr Hamiltonian with the Morse potential. Comparison with experimental data.
doi: 10.1103/PhysRevC.84.024309
2010AY08 Nucl.Phys. A848, 245 (2010) M.Aygun, Y.Kucuk, I.Boztosun, Awad A.Ibraheem Microscopic few-body and Gaussian-shaped density distributions for the analysis of the 6He exotic nucleus with different target nuclei NUCLEAR REACTIONS 12C(6He, 6He), E=5.9, 9.9 MeV; 27Al(6He, 6He), E=9.5, 11, 12, 13.4 MeV; 58Ni(6He, 6He), E=9, 10 MeV; 64Zn(6He, 6He), E=10, 13.6 MeV; 65Cu(6He, 6He), E=19.5, 30 MeV; 197Au(6He, 6He), E=27, 29, 40 MeV; 208Pb(6He, 6He), E=14, 16, 18, 22, 27 MeV; 209Bi(6He, 6He), E=16.25, 17.8, 19, 22.01, 22.5 MeV; calculated σ(θ) using few body and Gaussian density distributions within a double-folding model. Comparison with data.
doi: 10.1016/j.nuclphysa.2010.09.005
2010BO25 J.Phys.:Conf.Ser. 205, 012020 (2010) D.Bonatsos, I.Boztosun, I.Inci A long sought result: Closed analytical solutions of the Bohr Hamiltonian with the Morse potential NUCLEAR STRUCTURE 98,100,102,104Ru, 102,104,106,108,110,112,114,116Pd, 106,108,110,112,114,116,118,120Cd, 118,120,122,124,126,128,130,132,134Xe, 130,132,134,136,142Ba, 134,136,138Ce, 140,148,150Nd, 140,142,152,154Sm, 142,144,152,154,156,158,160,162Gd, 158,160,162,164,166Dy, 156,160,162,164,166,168,170Er, 164,166,168,170,172,174,176,178Yb, 168,170,172,174,176,178,180Hf, 176,178,180,182,184,186W, 178,180,184,186,188Os, 186,188,190,192,194,196,198,200Pt, 228Ra, 228,230,232Th, 232,234,236,238U, 238,240,242,248Cm, 250Cf; calculated low-lying 0+, 2+, 4+ states, β and γ bandheads, deformation using Bohr Hamiltonian with Morse potential; deduced Morse potential shapes. Compared with data.
doi: 10.1088/1742-6596/205/1/012020
2010KO07 Phys.Rev. C 81, 024615 (2010) G.Kocak, M.Karakoc, I.Boztosun, A.B.Balantekin Effects of α-cluster potentials for the 16O+16O fusion reaction and S factor NUCLEAR REACTIONS 16O(16O, 16O), E(cm)=2-15 MeV; analyzed σ and S-factors. 16O(16O, 16O), E(cm)=12.5, 14, 15.5, 20.5, 24.5, 29.5 MeV; analyzed σ(θ). Optical model using Woods-Saxon and α-α double folding α-cluster potentials for fusion reactions.
doi: 10.1103/PhysRevC.81.024615
2009KU11 Phys.Rev. C 79, 067601 (2009) Onset of nuclear structure effects in near-barrier elastic scattering of weakly bound nuclei: 6He and 6Li compared NUCLEAR REACTIONS 58Ni(6He, 6He), E=11.0, 16.0 MeV; 208Pb(6He, 6He), (6Li, 6Li), E=22.0, 33.0 MeV; 58Ni(6Li, 6Li), E not given; 120Sn, 144Sm, 181Ta(6He, 6He), (6Li, 6Li), E not given; calculated σ(θ) using continuum discretized coupled channels calculations. Comparison with experimental data.
doi: 10.1103/PhysRevC.79.067601
2009KU25 Phys.Rev. C 80, 054602 (2009) Global optical potential for the elastic scattering of 6He at low energies NUCLEAR REACTIONS 12C(6He, 6He), E=8.79, 9.18, 18.0 MeV; 27Al(6He, 6He), E=9.5, 11.0, 12.0, 13.4 MeV; 58Ni(6He, 6He), E=9.0 MeV; 64Zn(6He, 6He), E=10.0 MeV; 65Cu(6He, 6He), E=22.6 MeV; 197Au(6He, 6He), E=27.0, 29, 40.0 MeV; 208Pb(6He, 6He), E=14.0, 16.0, 18.0, 22.0, 27.0 MeV; 209Bi(6He, 6He), E=14.7, 16.3, 17.8, 19.0, 22.5 MeV; analyzed elastic scattering σ and angular distributions using optical model analysis; deduced global optical model potential parameters. Comparison with experimental data.
doi: 10.1103/PhysRevC.80.054602
2008BO15 Phys.Rev. C 77, 044302 (2008) I.Boztosun, D.Bonatsos, I.Inci Analytical solutions of the Bohr Hamiltonian with the Morse potential NUCLEAR STRUCTURE 98,100,102,104Ru, 102,104,106,108,110,112,114,116Pd, 106,108,110,112,114,116,118,120Cd, 118,120,122,124,126,128,130,132,134Xe, 130,132,134,136,142Ba, 134,136,138Ce, 140,148,150Nd, 140,142,152,154Sm, 142,144,152,154,156,158,160,162Gd, 154,158,160,162,164,166Dy, 156,160,162,164,166,168,170Er, 164,166,168,170,172,174,176,178Yb, 168,170,172,174,176,178,180Hf, 176,178,180,182,184,186W, 186,188,190,192,194,196,198,200Pt; 178,180,184,186,188Os, 228Ra, 228,230,232Th, 232,234,236,238U, 238,240,242Pu, 248Cm, 250Cf, calculated Bohr Hamilton and Morse Potential, angular momenta, bandheads and energy spacings of g.s., first 2+ and 4+ states.
doi: 10.1103/PhysRevC.77.044302
2008BO19 Phys.Rev. C 77, 064608 (2008) I.Boztosun, M.Karakoc, Y.Kucuk Microscopic double folding potential description of the 6He+12C reaction NUCLEAR REACTIONS 12C(6He, 6He), (6He, 6He'), (6He, α), E=18.0 MeV; calculated proton and neutron density distributions, real and imaginary potentials and deformations, σ. Coupled-channel Born approximation. Comparison with experimental data.
doi: 10.1103/PhysRevC.77.064608
2007FR17 Phys.Rev. C 76, 034320 (2007) M.Freer, I.Boztosun, C.A.Bremner, S.P.G.Chappell, R.L.Cowin, G.K.Dillon, B.R.Fulton, B.J.Greenhalgh, T.Munoz-Britton, M.P.Nicoli, W.D.M.Rae, S.M.Singer, N.Sparks, D.L.Watson, D.C.Weisser Reexamination of the excited states of 12C NUCLEAR REACTIONS 12C(12C, 3α), E=82-106 MeV; analyzed energy and angular distributions data. 8Be deduced levels.
doi: 10.1103/PhysRevC.76.034320
2007KO15 Phys.Atomic Nuclei 70, 290 (2007) G.Kocak, M.Karakoc, I.Boztosun Examination of the 16O + 28Si system with microscopic and phenomenological potentials NUCLEAR REACTIONS 28Si(16O, 16O), E=29-44 MeV; calculated σ(θ). Results for microscopic and phenomenological potentials compared with data.
doi: 10.1134/S106377880702010X
2006AH04 Int.J.Mod.Phys. E15, 1209 (2006) A.I.Ahmadov, I.Boztosun, R.Kh.Muradov, A.Soylu, E.A.Dadashov Higher twist effects in proton-proton collisions NUCLEAR REACTIONS 1H(p, π+X), E=high; calculated pion production σ, higher-twist contributions.
doi: 10.1142/S0218301306004843
2006KA23 Phys.Rev. C 73, 047601 (2006) α-α double folding cluster potential description of the 12C + 24Mg system NUCLEAR REACTIONS 24Mg(12C, 12C), E=20, 21, 22 MeV; 24Mg(12C, X), E(cm) ≈ 13-16 MeV; analyzed elastic σ(θ) and fusion σ. α-α double folding cluster potential.
doi: 10.1103/PhysRevC.73.047601
2006KA43 Int.J.Mod.Phys. E15, 1317 (2006) Microscopic potential description of the elastic scattering and fusion cross-section data of the 12C + 24Mg system NUCLEAR REACTIONS 24Mg(12C, 12C), E=20, 21, 22, 23, 24 MeV; calculated σ(θ). 24Mg(12C, X), E=20, 21, 22, 23, 24 MeV; calculated fusion σ. Microscopic potential, comparison with data.
doi: 10.1142/S0218301306004867
2006KU06 Nucl.Phys. A764, 160 (2006) Global examination of the 12C + 12C reaction data at low and intermediate energies NUCLEAR REACTIONS 12C(12C, 12C), E=32-70.7 MeV; analyzed σ(θ, E). Coupled channels and optical models compared.
doi: 10.1016/j.nuclphysa.2005.09.013
2005BO28 Int.J.Mod.Phys. E14, 663 (2005) I.Boztosun, O.Bayrak, Y.Dagdemir A comparative study of the 12C + 24Mg system with deep and shallow potentials NUCLEAR REACTIONS 24Mg(12C, 12C), E=16-24 MeV; calculated σ(θ) with deep and shallow optical potentials. Comparison with data.
doi: 10.1142/S0218301305003442
2005BO31 Yad.Fiz. 68, 1201 (2005); Phys.Atomic Nuclei 68, 1153 (2005) I.Boztosun, Y.Dagdemir, O.Bayrak The Examination of the 12C + 24Mg Elastic Scattering around the Coulomb Barrier NUCLEAR REACTIONS 24Mg(12C, 12C), E=16-24 MeV; calculated σ(θ). Modified optical model approach, comparison with data.
doi: 10.1134/1.1992570
2005DU26 Phys.Rev. C 72, 054604 (2005) A.Duisebayev, K.M.Ismailov, I.Boztosun Inclusive cross-sections of (p, xp) and (p, xα) reactions on 56Fe at Ep = 29.9 MeV NUCLEAR REACTIONS 56Fe(p, pX), (p, αX), E=29.9 MeV; measured Ep, Eα, σ(E); deduced multistep direct and compound process contributions.
doi: 10.1103/PhysRevC.72.054604
2005ER05 J.Phys.(London) G31, S1837 (2005) S.Erturk, I.Boztosun, Y.Kucuk, M.Karakoc, S.Aydin Failure of the standard coupled-channels method in describing inelastic reaction data: on the use of a new shape for the coupling potential NUCLEAR REACTIONS 12C(12C, 12C), (12C, 12C'), E=73.4, 93.8, 126.7 MeV; analyzed σ(θ); deduced coupling potential features.
doi: 10.1088/0954-3899/31/10/083
2005FR14 Phys.Rev. C 71, 047305 (2005) M.Freer, I.Boztosun, C.A.Bremner, S.P.G.Chappell, R.L.Cowin, G.K.Dillon, B.R.Fulton, B.J.Greenhalgh, M.P.Nicoli, W.D.M.Rae, S.M.Singer, D.L.Watson, D.C.Weisser 8Be + 12C(0+2) decay of excited states in 20Ne NUCLEAR REACTIONS 12C(12C, 8Be12C), E=82-120 MeV; measured particle spectra, angular distributions. 20Ne deduced possible resonance states energies, J, π.
doi: 10.1103/PhysRevC.71.047305
2004FR34 Phys.Rev. C 70, 064311 (2004) M.Freer, M.P.Nicoli, S.M.Singer, C.A.Bremner, S.P.G.Chappell, W.D.M.Rae, I.Boztosun, B.R.Fulton, D.L.Watson, B.J.Greenhalgh, G.K.Dillon, R.L.Cowin, D.C.Weisser 8Be+8Be decay of excited states in 16O NUCLEAR REACTIONS 12C(12C, 28Be), E=82-120 MeV; measured excitation energy spectra, angular correlations. 16O deduced levels, J, π. Comparison with model predictions.
doi: 10.1103/PhysRevC.70.064311
2003DU09 Phys.Rev. C 67, 044608 (2003) A.Duisebayev, K.M.Ismailov, I.Boztosun Inclusive spectra of (p, xp) and (p, xd) reactions on 90, 92Zr and 92Mo nuclei at Ep = 30.3 MeV NUCLEAR REACTIONS 90,92Zr, 92Mo(p, pX), (p, dX), E=30.3 MeV; measured Ep, Ed, σ(E, θ); deduced reaction mechanism features.
doi: 10.1103/PhysRevC.67.044608
2002BO03 Phys.Rev. C65, 024603 (2002) Global Potential Analysis of the 16O + 28Si Reaction using a New Type of Coupling Potential NUCLEAR REACTIONS 28Si(16O, 16O), (16O, 16O'), E=29.0-142.5 MeV; calculated σ(θ). New coupling potential, comparison with data.
doi: 10.1103/PhysRevC.65.024603
2002BO17 Yad.Fiz. 65, 639 (2002); Phys.Atomic Nuclei 65, 607 (2002) Systematic Investigation of Light Heavy-Ion Reactions NUCLEAR REACTIONS 28Si(16O, 16O'), E=29-143 MeV; 12C(12C, 12C'), E=20-140 MeV; 24Mg(16O, 16O'), (12C, 12C'), E not given; analyzed σ, σ(E, θ). New coupling potential.
doi: 10.1134/1.1471259
2002BO40 Phys.Rev. C66, 024610 (2002) New results in the analysis of 16O+ 28Si elastic scattering by modifying the optical potential NUCLEAR REACTIONS 28Si(16O, 16O), E=29.0-142.5 MeV; analyzed σ(θ). Optical model, modified potential.
doi: 10.1103/PhysRevC.66.024610
2002BO58 Phys.Rev. C 66, 064602 (2002) Investigation of the coupling potential by means of S-matrix inversion NUCLEAR REACTIONS 12C, 24Mg(12C, 12C), 28Si(16O, 16O), E=93.8, 126.7 MeV; calculated coupling potential, effect on inelastic scattering potential. S-matrix inversion.
doi: 10.1103/PhysRevC.66.064602
2002BR43 Phys.Rev. C66, 034605 (2002) C.A.Bremner, S.P.G.Chappell, W.D.M.Rae, I.Boztosun, M.Freer, M.P.Nicoli, S.M.Singer, B.R.Fulton, D.L.Watson, B.J.Greenhalgh, G.K.Dillon, R.L.Cowin Excitation Function Measurements for 12C + 12C Inelastic Scattering Channels NUCLEAR REACTIONS 12C(12C, 12C'), E(cm)=40-59 MeV; measured excitation energy spectra, σ(E); deduced excitation functions, resonance features.
doi: 10.1103/PhysRevC.66.034605
2001BO18 Phys.Rev. C63, 054607 (2001) Analysis of the 12C + 12C Reaction using a New Type of Coupling Potential NUCLEAR REACTIONS 12C(12C, 12C), (12C, 12C'), E=32.0-126.7 MeV; calculated σ(θ), excitation functions. Coupled-channels approach, new potential, comparisons with data.
doi: 10.1103/PhysRevC.63.054607
2001BO41 Phys.Lett. 518B, 229 (2001) A New Coupling Potential for the Analysis of Deformed Light Heavy-Ion Reactions NUCLEAR REACTIONS 12C(12C, 12C), (12C, 12C'), E=20.0-126.7 MeV; 28Si(16O, 16O), (16O, 16O'), E=29.0-142.5 MeV; 24Mg(12C, 12C), (12C, 12C'), E=16.0-24.0 MeV; calculated σ(θ). New coupling potential, comparisons with data.
doi: 10.1016/S0370-2693(01)01063-2
2001BO46 Phys.Rev. C64, 054607 (2001); Erratum Phys.Rev. C66, 049904 (2002) Analysis of the 12C + 24Mg Reaction using a New Coupling Potential NUCLEAR REACTIONS 24Mg(12C, 12C), (12C, 12C'), E=16-24 MeV; calculated σ(θ). Coupled-channels approach, second-derivative coupling potential, comparison with data.
doi: 10.1103/PhysRevC.64.054607
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