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NSR database version of May 24, 2024.

Search: Author = T.Cap

Found 24 matches.

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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; 249,250,251,252Cf(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 sinj 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 θplane vs θflow 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 θflow 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 249,250,251,252Cf(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 293,294,295,296Og 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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