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NSR database version of May 2, 2024.

Search: Author = T.Cap

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2024ZA01      Nuovo Cim. C 47, 62 (2024)

C.Zagami, E.V.Pagano, P.Russotto, E.De Filippo, L.Acosta, T.Cap, G.Cardella, F.Fichera, E.Geraci, B.Gnoffo, C.Guazzoni, G.Lanzalone, C.Maiolino, N.S.Martorana, T.Matulewicz, A.Pagano, M.Papa, K.Piasecki, S.Pirrone, M.Piscopo, R.Planeta, G.Politi, F.Risitano, F.Rizzo, G.Sacca, G.Santagati, K.Siwek-Wilczynska, I.Skwira-Chalot, M.Trimarchi

FARCOS detector in the CHIFAR experiment

doi: 10.1393/ncc/i2024-24062-7
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2022CA11      Phys.Rev. C 105, L051601 (2022)

T.Cap, M.Kowal, K.Siwek-Wilczynska

Diffusion as a possible mechanism controlling the production of superheavy nuclei in cold fusion reactions

NUCLEAR REACTIONS ²⁰⁸Pb(⁴⁸Ca, X), E(cm)=160-225 MeV; ²⁰⁸Pb(⁵⁰Ti, X), E(cm)=180-245 MeV; ²⁰⁸Pb(⁵⁴Cr, X), E(cm)=190-265; calculated fusion σ(E), averaged fusion probability. Discussed role of the difference in values of the rotational energies in the fusion saddle point and contact (sticking) configuration of the projectile-target system. Fusion-by-diffusion model (FbD). Injection point systematics obtained for the set of 1n cold fusion reactions on ²⁰⁷Pb, ²⁰⁸Pb, ²⁰⁹Bi targets. Comparison to experimental data.

doi: 10.1103/PhysRevC.105.L051601
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2022CA26      Eur.Phys.J. A 58, 231 (2022)

T.Cap, M.Kowal, K.Siwek-Wilczynska

The Fusion-by-Diffusion model as a tool to calculate cross sections for the production of superheavy nuclei

NUCLEAR REACTIONS ²⁰⁸Pb, ²³⁸U, ²⁴⁸Cm(⁴⁸Ca, X), ²⁰⁸Pb(⁵⁰Ti, X), E(cm)<230 MeV; analyzed available data; deduced the injection point systematics obtained for the set of cold and hot fusion reactions, the internal fusion barriers, averaged survival and fusion probabilities, fusion σ within the Fusion-by-Diffusion (FBD) model using the new nuclear data tables by Jachimowicz et al. (At Data Nucl Data Tables 138, 101393, 2021).

doi: 10.1140/epja/s10050-022-00891-8
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2020OV01      Acta Phys.Pol. B51, 731 (2020)

J.D.Ovejas, A.Knyazev, I.Martel, O.Tengblad, M.J.G.Borge, J.Cederkall, N.Keeley, K.Rusek, C.Garcia-Ramos, L.A.Acosta, A.A.Arokiaraj, M.Babo, T.Cap, N.Ceylan, G.De Angelis, A.Di Pietro, J.P.Fernandez, P.Figuera, L.Fraile, H.Fynbo, D.Galviz, J.H.Jensen, B.Jonson, R.Kotak, T.Kurtukian, M.Madurga, G.Marquinez-Duran, M.Munch, A.K.Orduz, R.Honorio, A.Pakou, T.Perez, L.Peralta, A.Perea, R.Raabe, M.Renaud, K.Riisager, A.M.Sanchez-Benitez, J.Sanchez-Segovia, O.Sgouros, V.Soukeras, P.Teubig, S.Vinals, M.Wolinska-Cichocka, R.Wolski, J.Yang

Halo Effects in the Low-Energy Scattering of ¹⁵C with Heavy Targets

doi: 10.5506/APhysPolB.51.731
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2020PA19      Eur.Phys.J. A 56, 102 (2020)

A.Pagano, E.De Filippo, E.Geraci, E.V.Pagano, P.Russotto, K.Siwek-Wilczynska, L.Acosta, L.Auditore, T.Cap, G.Cardella, M.B.Chatterjee, M.Colonna, B.Gnoffo, F.Favela, G.Lanzalone, C.Maiolino, N.S.Martorana, M.Papa, S.Pirrone, G.Politi, E.Piasecki, L.Quattrocchi, F.Rizzo, A.Trifiro, M.Trimarchi

Nuclear neck-density determination at Fermi energy with CHIMERA detector

doi: 10.1140/epja/s10050-020-00105-z
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2020RU02      Eur.Phys.J. A 56, 12 (2020)

P.Russotto, E.De Filippo, E.V.Pagano, L.Acosta, L.Auditore, T.Cap, G.Cardella, S.De Luca, E.Geraci, B.Gnoffo, G.Lanzalone, I.Lombardo, C.Maiolino, N.S.Martorana, T.Minniti, S.Norella, A.Pagano, M.Papa, E.Piasecki, S.Pirrone, G.Politi, F.Porto, L.Quattrocchi, F.Rizzo, E.Rosato, K.Siwek-Wilczynska, A.Trifiro, M.Trimarchi, G.Verde, J.Wilczynski

Dynamical versus statistical production of Intermediate Mass Fragments at Fermi Energies

doi: 10.1140/epja/s10050-019-00011-z
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2019CA34      Acta Phys.Pol. B50, 501 (2019)

T.Cap, K.Siwek-Wilczynska, J.Wilczynski, L.Auditore, G.Cardella, E.De Filippo, E.Geraci, A.Grzeszczuk, E.La Guidara, G.Gnoffo, T.Kozik, G.Lanzalone, I.Lombardo, M.Martorama, R.Najman, N.G.Nicolis, A.Pagano, E.V.Pagano, M.Papa, E.Piasecki, S.Pirrone, R.Planeta, G.Politi, F.Rizzo, P.Russotto, I.Skwira-Chalot, A.Trifiro, M.Trimarchi, G.Verde, W.Zipper

Competition Between Dynamical and Sequential Reaction Channels in ¹⁹⁷Au+¹⁹⁷Au Collisions at a Bombarding Energy of 23A MeV

NUCLEAR REACTIONS ¹⁹⁷Au(¹⁹⁷Au, X), E=23 MeV/nucleon; measured reaction products, fragment energies; deduced total kinetic energies, fragment mass distribution. CHIMERA 4π detector at INFIN-LNS.

doi: 10.5506/aphyspolb.50.501
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2019SI19      Phys.Rev. C 99, 054603 (2019)

K.Siwek-Wilczynska, T.Cap, M.Kowal

Exploring the production of new superheavy nuclei with proton and α-particle evaporation channels

NUCLEAR REACTIONS ²⁴⁹Bk(⁵⁰Ti, 2n), (⁵⁰Ti, 3n), (⁵⁰Ti, 4n)²⁹⁵119/²⁹⁶119/²⁹⁷119, E(cm)=206-244 MeV; ²⁵⁴Es(⁴⁸Ca, 2n), (⁴⁸Ca, 3n), (⁴⁸Ca, 4n), (⁴⁸Ca, 5n)²⁹⁷119/²⁹⁸119/²⁹⁹119/³⁰⁰119, E(cm)=196-234 MeV; ²⁴⁸Cm(⁵¹V, 3n), (⁵¹V, 4n), (⁵¹V, 5n), (⁵¹V, 6n)²⁹³119/²⁹⁴119/²⁹⁵119/²⁹⁶119, E(cm)=216-264 MeV; ²⁴⁸Cm(⁵⁴Cr, 2n), (⁵⁴Cr, 3n), (⁵⁴Cr, 4n)²⁹⁸120/²⁹⁹120/³⁰⁰120, E(cm)=220-260 MeV; ²⁴²Pu(⁴⁸Ca, np), (⁴⁸Ca, 2np), (⁴⁸Ca, 3np)²⁸⁶Nh/²⁸⁷Nh/²⁸⁸Nh, E(cm)=190-222 MeV; ²⁴⁴Pu(⁴⁸Ca, np), (⁴⁸Ca, 2np), (⁴⁸Ca, 3np)²⁸⁸Nh/²⁸⁹Nh/²⁹⁰Nh, E(cm)=190-220 MeV; ²⁴⁸Cm(⁴⁸Ca, np), (⁴⁸Ca, 2np), (⁴⁸Ca, 3np)²⁹²Mc/²⁹³Mc/²⁹⁴Mc, E(cm)=190-222 MeV; ²⁴⁹Bk(⁴⁸Ca, np), (⁴⁸Ca, 2np), (⁴⁸Ca, 3np)²⁹³Lv/²⁹⁴Lv/²⁹⁵Lv, E(cm)=190-222 MeV; ^{249,250,251,252}Cf(⁴⁸Ca, xnp)²⁹⁵Ts/²⁹⁶Ts/²⁹⁷Ts, E(cm)=200-228 MeV; ²⁴⁴Pu(⁴⁸Ca, nα), (⁴⁸Ca, 2nα), (⁴⁸Ca, 3nα)²⁸⁵Cn/²⁸⁶Cn/²⁸⁷Cn, E(cm)=186-214 MeV; ²⁴⁸Cm(⁴⁸Ca, nα), (⁴⁸Ca, 2nα), (⁴⁸Ca, 3nα)²⁸⁹Fl/²⁹⁰Fl/²⁹¹Fl, E(cm)=190-224 MeV; ²⁴⁹Bk(⁴⁸Ca, nα), (⁴⁸Ca, 2nα), (⁴⁸Ca, 3nα)²⁹⁰Mc/²⁹¹Mc/²⁹²Mc, E(cm)=196-226 MeV; ²⁵¹Cf(⁴⁸Ca, nα), (⁴⁸Ca, 2nα), (⁴⁸Ca, 3nα)²⁹²Lv/²⁹³Lv/²⁹⁴Lv, E(cm)=196-226 MeV; calculated production σ(E) for superheavy nuclides using fusion-by-diffusion model (FDB). Z=114-118; systematics of experimental values of the injection point distance parameter s_inj as a function of the kinetic energy excess above the mean barrier.

doi: 10.1103/PhysRevC.99.054603
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2016CA14      Acta Phys.Pol. B47, 983 (2016)

T.Cap, K.Siwek-Wilczynska, J.Wilczynski, F.Amorini, L.Auditore, G.Cardella, E.De Filippo, E.Geraci, L.Grassi, A.Grzeszczuk, E.La Guidara, J.Han, T.Kozik, G.Lanzalone, I.Lombardo, R.Najman, N.G.Nicolis, A.Pagano, M.Papa, E.Piasecki, S.Pirrone, R.Planeta, G.Politi, F.Rizzo, P.Russotto, I.Skwira-Chalot, A.Trifiro, M.Trimarchi, G.Verde, W.Zipper

Determination of Impact Parameters in Aligned Breakup of Projectile-like Fragments in ¹⁹⁷Au + ¹⁹⁷Au Collisions at 23A MeV

NUCLEAR REACTIONS ¹⁹⁷Au(¹⁹⁷Au, X), E=23 MeV/nucleon; measured reaction products; deduced asymmetry parameter, average mass numbers of fragments, total kinetic energies.

doi: 10.5506/APhysPolB.47.983
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2016NA49      Acta Phys.Pol. B47, 975 (2016)

R.Najman, R.Planeta, A.Sochocka, F.Amorini, L.Auditore, T.Cap, G.Cardella, E.De Filippo, E.Geraci, A.Grzeszczuk, S.Kowalski, T.Kozik, G.Lanzalone, I.Lombardo, Z.Majka, N.G.Nicolis, A.Pagano, E.Piasecki, S.Pirrone, G.Politi, F.Rizzo, P.Russotto, K.Siwek-Wilczynska, I.Skwira-Chalot, A.Trifiro, M.Trimarchi, J.Wilczynski, W.Zipper

Investigation of the Freeze-out Configuration in the ¹⁹⁷Au + ¹⁹⁷Au Reaction at 23 A MeV

NUCLEAR REACTIONS ¹⁹⁷Au(¹⁹⁷Au, x), E=23 MeV/nucleon; measured reaction products using CHIMERA detector with ΔE-E technique for fragments punching through Si detectors and ToF method for fragments stopped in Si detectors; deduced θ_plane vs θ_flow dependence, efficiency factor (for possible toroidal-shape); calculated fragment flow σ for different groups of fragments using QMD (Quantum Molecular Dynamics) model and using ETNA (Expecting Toroidal Nuclear Agglomeration) model.

doi: 10.5506/APhysPolB.47.975
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2015NA21      Phys.Rev. C 92, 064614 (2015)

R.Najman, R.Planeta, A.Sochocka, F.Amorini, L.Auditore, T.Cap, G.Cardella, E.De Filippo, E.Geraci, A.Grzeszczuk, S.Kowalski, T.Kozik, G.Lanzalone, I.Lombardo, Z.Majka, N.G.Nicolis, A.Pagano, E.Piasecki, S.Pirrone, G.Politi, F.Rizzo, P.Russotto, K.Siwek-Wilczynska, I.Skwira-Chalot, A.Trifiro, M.Trimarchi, J.Wilczynski, W.Zipper

Freeze-out configuration properties in the ¹⁹⁷Au + ¹⁹⁷Au reaction at 23 A MeV

NUCLEAR REACTIONS ¹⁹⁷Au(¹⁹⁷Au, X), E=23 MeV/nucleon; measured reaction products, ΔE-TOF distributions using CHIMERA multidetector telescope at INFN-LNS, Catania Superconducting Cyclotron facility; deduced correlations between mass and energy for fragments, between total charge of identified fragments and their total parallel momenta, and between mass of identified fragments and parallel velocity, multiplicity distributions of fragments, coplanarity vs sphericity distributions, impact parameter versus θ_flow dependence, distribution of relative velocities of fragments pairs, mean values of mass standard deviation of the fragments and relative velocities of fragment pairs. Comparison with ETNA model for simulation of the decay of a nuclear system, and predictions of quantum molecular dynamics (QMD) model.

doi: 10.1103/PhysRevC.92.064614
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2015RU01      Phys.Rev. C 91, 014610 (2015)

P.Russotto, E.De Filippo, A.Pagano, L.Acosta, L.Auditore, V.Baran, I.Berceanu, B.Borderie, R.Bougault, M.Bruno, T.Cap, G.Cardella, S.Cavallaro, M.B.Chatterjee, A.Chbihi, M.Colonna, M.D'Agostino, M.Di Toro, L.Francalanza, J.Frankland, E.Galichet, W.Gawlikowicz, E.Geraci, B.Gnoffo, A.Grzeszczuk, P.Guazzoni, S.Kowalski, G.Lanzalone, G.Lanzano, N.Le Neindre, I.Lombardo, C.Maiolino, T.Minniti, E.V.Pagano, M.Papa, E.Piasecki, S.Pirrone, R.Planeta, G.Politi, F.Porto, L.Quattrocchi, M.F.Rivet, E.Rosato, F.Rizzo, K.Schmidt, K.Siwek-Wilczynska, I.Skwira-Chalot, A.Trifiro, M.Trimarchi, G.Verde, M.Vigilante, J.P.Wieleczko, J.Wilczynski, L.Zetta, W.Zipper

Production cross sections for intermediate mass fragments from dynamical and statistical decay of projectile-like fragments in ¹²⁴Sn + ⁶⁴Ni and ¹¹²Sn + ⁵⁸Ni collisions at 35 A MeV

NUCLEAR REACTIONS ⁵⁸Ni(¹¹²Sn, X), ⁶⁴Ni(¹²⁴Sn, X), E=35 MeV/nucleon; measured reaction products, yields of intermediate mass fragments (IMF) and projectile-like and target-like fragments (PLF and TLF), IMF multiplicities, relative velocity between PLF and IMF, dynamical IMF emission cross sections using 4π multidetector CHIMERA array at INFN-LNS Superconducting Cyclotron facility; deduced IMF emission more probable for neutron-rich system.

doi: 10.1103/PhysRevC.91.014610
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2014CA06      Phys.Scr. 89, 054005 (2014)

T.Cap, K.Siwek-Wilczynska, I.Skwira-Chalot, J.Wilczynski, F.Amorini, L.Auditore, G.Cardella, E.De Filippo, E.Geraci, L.Grassi, A.Grzeszczuk, E.La Guidara, J.Han, T.Kozik, G.Lanzalone, I.Lombardo, R.Najman, N.G.Nicolis, A.Pagano, M.Papa, E.Piasecki, S.Pirrone, R.Planeta, G.Politi, F.Rizzo, P.Russotto, A.Trifiro, M.Trimarchi, G.Verde, W.Zipper

Aligned ternary partitioning of the ¹⁹⁷Au + ¹⁹⁷Au system at 23 A MeV beam energy

NUCLEAR REACTIONS ¹⁹⁷Au(¹⁹⁷Au, X), E=23 MeV/nucleon; measured reaction intermediate mass fragments; deduced σ(θ), mass number distribution.

doi: 10.1088/0031-8949/89/5/054005
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2013CA12      Phys.Scr. T154, 014007 (2013)

T.Cap, K.Siwek-Wilczynska, I.Skwira-Chalot, J.Wilczynski, for THE CHIMERA Collaboration

Fragment production in the ¹⁹⁷Au + ¹⁹⁷Au reaction at 23A MeV

NUCLEAR REACTIONS ¹⁹⁷Au(¹⁹⁷Au, X), E=23 MeV/nucleon; measured reaction fragments; deduced partitioning processes leading to the neck emission of intermediate mass fragments and sequential breakup of projectile-like or target-like fragments.

doi: 10.1088/0031-8949/2013/T154/014007
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2013CA19      Phys.Rev. C 88, 037603 (2013)

T.Cap, K.Siwek-Wilczynska, M.Kowal, J.Wilczynski

Calculations of the cross sections for the synthesis of new ^293-296118 isotopes in ^249-252Cf(⁴⁸Ca, xn) reactions

NUCLEAR REACTIONS ^{249,250,251,252}Cf(⁴⁸Ca, 2n), (⁴⁸Ca, 3n), (⁴⁸Ca, 4n), (⁴⁸Ca, 5n)²⁹²Og/²⁹³Og/²⁹⁴Og/²⁹⁵Og/²⁹⁶Og, ²⁹⁷Og/²⁹⁸Og, E(cm)=194-230 MeV; calculated evaporation residue σ(E), weighted σ(E) for ^{293,294,295,296}Og based on isotopic abundance of Cf. Fusion-by-diffusion (FBD) model.

doi: 10.1103/PhysRevC.88.037603
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2013SI16      Phys.Scr. T154, 014005 (2013)

K.Siwek-Wilczynska, T.Cap, M.Kowal, J.Wilczynski

Calculations of synthesis cross sections of Z = 104 113 superheavy nuclei in the fusion-by-diffusion model with the Warsaw macro micro-model fission barriers

NUCLEAR REACTIONS ²⁰⁸Pb(⁵⁰Ti, n)²⁵⁷Rf, ²⁰⁹Bi(⁵⁴Cr, n)²⁶²Bh, ²⁰⁸Pb(⁵⁹Co, n)²⁶⁶Mt, E(cm)<250 MeV; calculated σ. FBD model, fusion-by-diffusion model with the Warsaw macro-micro-model fission barriers, comparison with available data.

doi: 10.1088/0031-8949/2013/T154/014005
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2012CA06      Acta Phys.Pol. B43, 297 (2012)

T.Cap, K.Siwek-Wilczynska, I.Skwira-Chalot, J.Wilczynski

Extension of the Fusion by Diffusion Model for Description of the Synthesis of Superheavy Nuclei in (Fusion, xn) Reactions

NUCLEAR REACTIONS ²⁰⁸Pb(⁵⁰Ti, xn)²⁵⁸Rf/²⁵⁶Rf/²⁵⁵Rf, ²⁰⁹Bi(⁵⁰Ti, xn)²⁵⁹Db/²⁵⁷Db/²⁵⁶Db, ²⁰⁸Pb(⁵⁴Cr, xn)²⁶²Sg/²⁶⁰Sg/²⁵⁹Sg, ²⁰⁹Bi(⁵¹V, 2n), ²⁰⁹Bi(⁵⁴Cr, 2n)²⁶¹Bh, ²⁰⁸Pb(⁵⁸Fe, 2n)²⁶⁴Hs, ²⁰⁸Pb(⁵⁰Ti, 2n)²⁵⁶Rf, ²⁰⁸Pb(⁴⁸Ti, 2n)²⁵⁴Rf, ²⁰⁹Bi(⁵⁰Ti, 2n)²⁵⁷Db, ²⁰⁸Pb(⁵¹V, 2n)²⁵⁷Db, ²⁰⁸Pb(⁵²Cr, 2n)²⁵⁸Sg, ²⁰⁹Bi(⁵⁴Cr, 2n)²⁶¹Bh, ²⁰⁸Pb(⁵⁴Cr, 2n)²⁶¹Bh, ²⁰⁸Pb(⁵⁵Mn, 2n)²⁶¹Bh, E not given; analyzed experimental data, 1n-, 2n-, 3n- σ, injection point distances.

doi: 10.5506/APhysPolB.43.297
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2012DE13      Phys.Rev. C 86, 014610 (2012)

E.De Filippo, A.Pagano, P.Russotto, F.Amorini, A.Anzalone, L.Auditore, V.Baran, I.Berceanu, B.Borderie, R.Bougault, M.Bruno, T.Cap, G.Cardella, S.Cavallaro, M.B.Chatterjee, A.Chbihi, M.Colonna, M.D'Agostino, R.Dayras, M.Di Toro, J.Frankland, E.Galichet, W.Gawlikowicz, E.Geraci, A.Grzeszczuk, P.Guazzoni, S.Kowalski, E.La Guidara, G.Lanzalone, G.Lanzano, N.Le Neindre, I.Lombardo, C.Maiolino, M.Papa, E.Piasecki, S.Pirrone, R.Planeta, G.Politi, A.Pop, F.Porto, M.F.Rivet, F.Rizzo, E.Rosato, K.Schmidt, K.Siwek-Wilczynska, I.Skwira-Chalot, A.Trifiro, M.Trimarchi, G.Verde, M.Vigilante, J.P.Wieleczko, J.Wilczynski, L.Zetta, W.Zipper

Correlations between emission timescale of fragments and isospin dynamics in ¹²⁴Sn+⁶⁴Ni and ¹¹²Sn+⁵⁸Ni reactions at 35 A MeV

NUCLEAR REACTIONS ⁶⁴Ni(¹²⁴Sn, X), ⁵⁸Ni(¹¹²Sn, X), E=35 MeV/nucleon; measured spectra of reaction products, charge distribution, yields, N/Z ratio of intermediate mass fragments (IMFs) as a function of Z number, using 4π multidetector CHIMERA. Comparison with stochastic mean field model.

doi: 10.1103/PhysRevC.86.014610
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2012SI13      Phys.Rev. C 86, 014611 (2012)

K.Siwek-Wilczynska, T.Cap, M.Kowal, A.Sobiczewski, J.Wilczynski

Predictions of the fusion-by-diffusion model for the synthesis cross sections of Z=114-120 elements based on macroscopic-microscopic fission barriers

NUCLEAR REACTIONS ²⁴³Am, ²⁴⁴Pu, ^245,248Cm, ²⁴⁹Bk, ²⁴⁹Cf, ^252,254Es(⁴⁸Ca, xn)²⁸⁷Fl/²⁸⁸Fl/²⁸⁹Fl/²⁸⁷Mc/²⁸⁸Mc/²⁸⁹Mc/²⁸⁹Lv/²⁹⁰Lv/²⁹¹Lv/²⁹²Lv/²⁹³Lv/²⁹⁴Lv/²⁹²Ts/²⁹³Ts/²⁹⁴Ts/²⁹⁵Ts/²⁹³Og/²⁹⁴Og/²⁹⁵Og/²⁹⁵119/²⁹⁶119/²⁹⁷119/²⁹⁸119/²⁹⁹119/³⁰⁰119, E(cm)=185-235 MeV; ^249,251Cf, ²⁴⁹Bk(⁵⁰Ti, xn)²⁹⁵119/²⁹⁶119/²⁹⁷119/²⁹⁴120/²⁹⁵120/²⁹⁶120/²⁹⁷120/²⁹⁸120/²⁹⁹120, E(cm)=205-255 MeV; ²⁴⁸Cm(⁵⁴Cr, xn)²⁹⁸120/²⁹⁹120/³⁰⁰120, E=220-260 MeV; calculated synthesis σ using fusion-by-diffusion (FBD) model. Predictions of σ for the formation of Z=119, 120 superheavy elements.

doi: 10.1103/PhysRevC.86.014611
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2012SK01      Int.J.Mod.Phys. E21, 1250033 (2012)

I.Skwira-Chalot, T.Cap, K.Siwek-Wilczynska, J.Wilczynski

Neutron enrichment of the neck-originated intermediate mass fragments in predictions of QMD model

NUCLEAR REACTIONS ¹²⁴Sn(⁶⁴Ni, X)⁷Be/⁹Be/¹⁰Be/¹⁰B/¹²B/¹²C/¹⁴C, E=35 MeV/nucleon; calculated σ(θ), isotopic ratio. QMD model, comparison with available data.

doi: 10.1142/S0218301312500334
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2011CA08      Int.J.Mod.Phys. E20, 308 (2011)

T.Cap, K.Siwek-Wilczynska, J.Wilczynski

Fusion by diffusion model revisited

NUCLEAR REACTIONS ²⁰⁸Pb(⁵⁰Ti, n), (⁴⁸Ti, n), ²⁰⁹Bi(⁵⁰Ti, n), (⁵¹V, n), ²⁰⁸Pb(⁵⁴Cr, n), (⁵²Cr, n), ²⁰⁹Bi(⁵⁴Cr, n), (⁵²Cr, n), (⁵⁵Mn, n), (⁵⁸Fe, n), (⁶⁴Ni, n), (⁷⁰Zn, n), ²⁰⁸Pb(⁵⁸Fe, n), (⁵⁶Fe, n), (⁵⁹Co, n), (⁶⁴Ni, n), (⁶²Ni, n), ²⁰⁷Pb(⁶²Ni, n), (⁶⁵Cu, n), (⁷⁰Zn, n), E(cm)<270 MeV; calculated σ. Comparison with experimental data.

doi: 10.1142/S0218301311017661
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2011CA14      Phys.Rev. C 83, 054602 (2011)

T.Cap, K.Siwek-Wilczynska, J.Wilczynski

Nucleus-nucleus cold fusion reactions analyzed with the l-dependent "fusion by diffusion" model

NUCLEAR REACTIONS ²⁰⁸Pb(⁵⁰Ti, n)²⁵⁷Rf, E(cm)=176-200 MeV; ²⁰⁹Bi(⁵⁰Ti, n)²⁵⁸Db, E(cm)=180-196 MeV; ²⁰⁸Pb, (⁵⁴Cr, n)²⁶¹Sg, E(cm)=195-212 MeV; ²⁰⁹Bi(⁵⁴Cr, n)²⁶²Bh, E(cm)=198-217 MeV; ²⁰⁸Pb(⁵⁸Fe, n)²⁶⁵Hs, E(cm)=212-228 MeV; ²⁰⁹Bi(⁵⁸Fe, n)²⁶⁶Mt, E(cm)=217-230 MeV; ²⁰⁸Pb(⁶⁴Ni, n)²⁷¹Ds, E(cm)=234-247 MeV; ²⁰⁹Bi(⁶⁴Ni, n)²⁷²Rg, E(cm)=236-250 MeV; ²⁰⁸Pb(⁷⁰Zn, n)²⁷⁷Cn, E(cm)=250-264 MeV; ²⁰⁹Bi(⁷⁰Zn, n)²⁷⁸Nh, E(cm)=254-269 MeV; ²⁰⁸Pb(⁷⁴Ge, n)²⁸¹Fl, E(cm)=270-287 MeV; ²⁰⁸Pb(⁷⁶Ge, n)²⁸³Fl, E(cm)=270-287 MeV; ²⁰⁹Bi(⁷⁴Ge, n)²⁸²Mc, E(cm)=272-292 MeV; ²⁰⁹Bi(⁷⁶Ge, n)²⁸⁴Mc, E(cm)=272-292 MeV; calculated excitation functions, cold fusion cross sections for superheavy nuclei and compared with experimental data from GSI, RIKEN and LBNL. Fusion by Diffusion model.

doi: 10.1103/PhysRevC.83.054602
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2011SK03      Int.J.Mod.Phys. E20, 546 (2011)

I.Skwira-Chalot, T.Cap, K.Siwek-Wilczynska, J.Wilczynski

Isotopic effects in emission of intermediate mass fragments in the ¹²⁴Sn + ⁶⁴Ni reaction at 35 MeV/nucleon

NUCLEAR REACTIONS ⁶⁴Ni(¹²⁴Sn, X), E=35 MeV/nucleon; measured reaction fragments; deduced fragment, velocity and angular distributions distributions, isotopic ratios.

doi: 10.1142/S0218301311017983
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2010SI09      Int.J.Mod.Phys. E19, 500 (2010)

K.Siwek-Wilczynska, T.Cap, J.Wilczynski

How can one synthesize the element Z = 120?

NUCLEAR REACTIONS ²⁴⁹Cf(⁵⁰Ti, X), ²⁴⁸Cm(⁵⁴Cr, X), ²⁴⁴Pu(⁵⁸Fe, X), ²³⁸U(⁶⁴Ni, X), E(cm)=200-300 MeV; calculated σ. Fusion by Diffusion model.

doi: 10.1142/S021830131001490X
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