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NSR database version of April 11, 2024.

Search: Author = I.Boztosun

Found 51 matches.

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2022DA12      Eur.Phys.J. A 58, 85 (2022)

H.Dapo, Y.Kucuk, I.Boztosun

A realistic numerical treatment of Coulomb potential in comparison with the analytical approximations

doi: 10.1140/epja/s10050-022-00728-4
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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
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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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD8049.


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
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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
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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
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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
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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
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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
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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
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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
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Data from this article have been entered in the XUNDL database. For more information, click here.


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
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Data from this article have been entered in the XUNDL database. For more information, click here.


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
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Data from this article have been entered in the XUNDL database. For more information, click here.


2016SE12      Int.J.Mod.Phys. E25, 1650071 (2016)

Y.Sert, I.Boztosun

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
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2014AY02      Few-Body Systems 55, 203 (2014)

M.Aygun, I.Boztosun

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
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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
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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
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Data from this article have been entered in the XUNDL database. For more information, click here.


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
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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
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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
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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
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2011BA03      Phys.Atomic Nuclei 74, 13 (2011)

O.Bayrak, I.Boztosun

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
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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
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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
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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
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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
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2009KU11      Phys.Rev. C 79, 067601 (2009)

Y.Kucuk, I.Boztosun, N.Keeley

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
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2009KU25      Phys.Rev. C 80, 054602 (2009)

Y.Kucuk, I.Boztosun, T.Topel

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
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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
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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
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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
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Data from this article have been entered in the XUNDL database. For more information, click here.


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
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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
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2006KA23      Phys.Rev. C 73, 047601 (2006)

M.Karakoc, I.Boztosun

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
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2006KA43      Int.J.Mod.Phys. E15, 1317 (2006)

M.Karakoc, I.Boztosun

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
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2006KU06      Nucl.Phys. A764, 160 (2006)

Y.Kucuk, I.Boztosun

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
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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
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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
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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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO1307.


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
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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
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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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD0277.


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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO1060.


2002BO03      Phys.Rev. C65, 024603 (2002)

I.Boztosun, W.D.M.Rae

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
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2002BO17      Yad.Fiz. 65, 639 (2002); Phys.Atomic Nuclei 65, 607 (2002)

I.Boztosun

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
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2002BO40      Phys.Rev. C66, 024610 (2002)

I.Boztosun

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
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2002BO58      Phys.Rev. C 66, 064602 (2002)

I.Boztosun, R.S.Mackintosh

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
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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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD0436.


2001BO18      Phys.Rev. C63, 054607 (2001)

I.Boztosun, W.D.M.Rae

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
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2001BO41      Phys.Lett. 518B, 229 (2001)

I.Boztosun, W.D.M.Rae

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
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2001BO46      Phys.Rev. C64, 054607 (2001); Erratum Phys.Rev. C66, 049904 (2002)

I.Boztosun, W.D.M.Rae

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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