NSR Query Results
Output year order : Descending NSR database version of April 11, 2024. Search: Author = A.Trzcinska Found 68 matches. 2023RU03 Iader.Fiz.Enerh. 24, 22 (2023) A.T.Rudchik, A.A.Rudchik, V.V.Khejlo, K.Rusek, K.W.Kemper, E.Piasecki, A.Stolarz, A.Trzcinska, V.M.Pirnak, O.A.Ponkratenko, E.I.Koshchy, O.E.Kutsyk, A.P.Ilyin, Y.M.Stepanenko, V.V.Uleshchenko, Y.O.Shyrma Reaction 10B(15N, 14C)11C at energy 81 MeV, spectroscopic factors and interaction of 14C + 11C nuclei NUCLEAR REACTIONS 10B(15N, 14C), E=81 MeV; measured reaction products; deduced σ(θ) within the coupled-reaction-channels (CRC) method. ICARE data.
doi: 10.15407/jnpae2023.01.022
2022AR03 Eur.Phys.J. A 58, 24 (2022) S.V.Artemov, R.Yarmukhamedov, N.Burtebayev, B.K.Karakozov, F.Kh.Ergashev, M.Nassurlla, S.B.Igamov, N.Amangeldi, A.Morzabayev, J.Burtebayeva, V.S.Zhdanov, G.Yergaliuly, E.Piasecki, K.Rusek, S.B.Sakuta, A.Demyanova, O.R.Tojiboev, A.Trzcinska, A.Sabidolda, R.Khojayev, K.I.Tursunmakhatov, M.Nassurlla, M.Wolinska-Cichocka, T.Kh.Sadykov, N.Saduyev Asymptotic normalization coefficient for 12C + p → 13N from the 12C(10B, 9Be)13N reaction and the 12C(p, γ)13N astrophysical S factor NUCLEAR REACTIONS 12C(10B, 9Be), E=41.3 MeV; measured reaction products. 13N; deduced σ(θ), S factor and thermonuclear reaction rates for 12C(p, γ) reaction, the "indirectly determined" ANC. The modified distorted wave Born approximation (MDWBA) method. The U-200P cyclotron (HIL of the University of Warsaw).
doi: 10.1140/epja/s10050-021-00652-z
2022ER02 Acta Phys.Pol. B53, 5 (2022) F.Kh.Ergashev, S.V.Artemov, O.R.Tojiboev, A.A.Karakhodzhaev, K.Rusek, A.Trzcinska, M.Wolinska-Cichocka, E.Piasecki, N.Burtebayev, S.B.Sakuta, M.Nassurlla, M.Nassurlla, R.F.Rumi Asymptotic normalization coefficients for the 17F → 16O+p configuration from the 16O(10B, 9Be)17F reaction and extimation of the 16O(p, γ)17F astrophysical S-factor NUCLEAR REACTIONS 16O(10B, 9Be), (10B, 10B), E=41.3 MeV; measured reaction products; deduced σ(θ), optical model parameters, asymptotic normalization coefficients (ANCs), S-factors. The U-200P cyclotron of the Heavy Ion Laboratory (University of Warsaw).
doi: 10.5506/APhysPolB.53.9-A5
2022RU07 Iader.Fiz.Enerh. 23, 153 (2022) A.T.Rudchik, A.A.Rudchik, V.V.Khejlo, K.Rusek, K.W.Kemper, E.Piasecki, A.Stolarz, A.Trzcinska, V.M.Pirnak, O.A.Ponkratenko, E.I.Koshchy, O.E.Kutsyk, S.Y.Mezhevych, A.P.Ilyin, Y.M.Stepanenko, V.V.Uleshchenko, Y.O.Shyrma Elastic and inelastic scattering of 15N ions by 10B at energy 81 MeV. Isotopic effects in scattering of 15N + 10B, 15N + 11B 14N + 10B nuclei NUCLEAR REACTIONS 12C(15N, 15N), (15N, 15N'), E=81 MeV; measured reaction products; deduced σ(θ).
doi: 10.15407/jnpae2022.03.153
2021RU08 Phys.Rev. C 103, 044614 (2021) A.T.Rudchik, A.A.Rudchik, O.O.Chepurnov, K.Rusek, N.Keeley, K.W.Kemper, S.Kliczewski, E.Piasecki, A.Trzcinska, Val.M.Pirnak, O.A.Ponkratenko, I.Strojek, E.I.Koshchy, R.Siudak, S.B.Sakuta, A.P.Ilyin, Yu.M.Stepanenko, Yu.O.Shyrma, V.V.Uleshchenko, K.A.Chercas, H.M.Maridi, N.Burtebayev 6Li + 15N interaction at Ec.m. = 23.1 MeV: Validation of the α + d cluster model of 6Li NUCLEAR REACTIONS 6Li(15N, 15N), (15N, 15N'), (15N, 6Li'), E=81 MeV from the U-200P cyclotron of University of Warsaw]; measured reaction products 15N and 6Li, σ(θ) using four ΔE-E telescopes of silicon detectors. 6Li; deduced differential cross sections for the resonances in 6Li, cluster structure of 6Li and the role of 6Li to α+d breakup. Comparison with optical model (OM), coupled-channel (CC) and coupled discretized continuum channel (CDCC) calculations using FRESCO code by including 6Li to α+d breakup, excitation of 15N levels, and the 15N(6Li, 7Li)14N one-neutron pickup reaction channel.
doi: 10.1103/PhysRevC.103.044614
2020AM01 Acta Phys.Pol. B51, 757 (2020) N.Amangeldi, N.Burtebayev, S.B.Sakuta, M.Nassurlla, J.Burtebayeva, M.Nassurlla, G.Yergaliuly, A.Sabidolda, K.Rusek, A.Trzcinska, M.Wolinska-Cichocka, B.Mauyey Study of Elastic Scattering of 10B Ions on 12C Nuclei at the Energy of 17.5 MeV
doi: 10.5506/APhysPolB.51.757
2020DI05 Phys.Lett. B 811, 135962 (2020) J.Diaz-Cortes, J.Benlliure, J.L.Rodriguez-Sanchez, H.Alvarez-Pol, T.Aumann, C.A.Bertulani, B.Blank, E.Casarejos, D.Cortina-Gil, D.Dragosavac, V.Fohr, A.Gargano, M.Gascon, W.Gawlikowicz, A.Heinz, K.Helariutta, A.Kelic-Heil, S.Lukic, F.Montes, D.Perez-Loureiro, L.Pienkowski, K.-H.Schmidt, M.Staniou, K.Subotic, K.Summerer, J.Taieb, A.Trzcinska Systematic reduction of the proton-removal cross section in neutron-rich medium-mass nuclei NUCLEAR REACTIONS 9Be(238U, X)132Sn/131Sn/131In/128Sn/130Sn/136Sn, E=950 MeV/nucleon; 9Be(132Xe, X)119Sn/124Sn/126Sn, E=1200 MeV/nucleon; 9Be(119Sn, X), (124Sn, X), (126Sn, X), (130Sn, X), (131Sn, X), (132Sn, X), (128Sn, X), (136Sn, X), (131Sn, X), E ∼ 1000 MeV/nucleon; measured reaction products, TOF; deduced single neutron and single proton removal σ. Comparison with the advanced Liege intra-nuclear cascade (INCL) model calculations.
doi: 10.1016/j.physletb.2020.135962
2020JA06 Acta Phys.Pol. B51, 861 (2020) J.Jastrzebski, N.Zandi, J.Choinski, M.Sitarz, A.Stolarz, A.Trzcinska, M.Vagheian Investigation of the Production of the Auger Electron Emitter 135La Using Medical Cyclotrons
doi: 10.5506/APhysPolB.51.861
2020PA05 Phys.Rev. C 101, 024602 (2020) A.Pakou, O.Sgouros, V.Soukeras, F.Cappuzzello, L.Acosta, C.Agodi, A.Boiano, S.Calabrese, D.Carbone, M.Cavallaro, N.N.Deshmukh, A.Foti, A.Hacisalihoglu, N.Keeley, M.La Commara, I.Martel, M.Mazzocco, A.Muoio, C.Parascandolo, D.Pierroutsakou, K.Rusek, A.M.Sanchez-Benitez, G.Santagati, G.Souliotis, A.Spatafora, E.Strano, D.Torresi, A.Trzcinska 9Be + p breakup at 5.67A MeV in a full kinematics approach NUCLEAR REACTIONS 1H(9Be, X), E=51 MeV; measured ΔE-E spectra for the recoils, ααp-coin using EXPADES module at the MAGNEX facility of INFN-LNS-Catania; deduced α-α relative energy spectrum from analysis of triple coincidence events, energy spectrum of recoiling protons, rates of three breakup modes: α+α+n, 8Be+n and 5He+4He for the 9Be Borromean nucleus.
doi: 10.1103/PhysRevC.101.024602
2020TR03 Phys.Rev. C 102, 034617 (2020) A.Trzcinska, E.Piasecki, G.Cardella, D.Dell'Aquila, E.De Filippo, S.De Luca, B.Gnoffo, M.Kowalczyk, G.Lanzalone, I.Lombardo, C.Maiolino, N.S.Martorana, A.Pagano, E.V.Pagano, S.Pirrone, G.Politi, L.Quattrocchi, F.Rizzo, P.Russotto, A.Trifiro, M.Trimarchi, M.Vigilante Barrier distributions of the 24Mg + 90, 92Zr systems: Influence of energy dissipation NUCLEAR REACTIONS 90,92Zr(24Mg, 24Mg), (24Mg, 24Mg'), E=68-88 MeV; measured scattered 24Mg ions using the multidetector CHIMERA system, and backscattered ions by rings of Si detectors placed at different angles, σ(E, θ) at the Tandem MP accelerator of the LNS-INFN-Catania; deduced Coulomb barrier distributions as function of incident beam energy and angle, influence of energy dissipation. Comparison with predictions of the standard coupled channels calculations, and with coupled channels plus random matrix theory (CC+RMT).
doi: 10.1103/PhysRevC.102.034617
2019BU10 Eur.Phys.J. A 55, 38 (2019) N.Burtebayev, S.B.Sakuta, M.Nassurlla, N.Saduyev, M.Nassurlla, T.Kh.Sadykov, A.Trzcinska, M.Wolinska-Cichocka, R.Khojayev Mechanism of the 11B(α, t)12C reaction at an energy of 40 MeV, role of exchange processes and collective excitations NUCLEAR REACTIONS 11B(α, t)12C, E=40 MeV; measured Et, It(θ); deduced triton σ(E), σ(θ) to gs and to E*=4.44, 7.65, 9.64, 14.08 MeV; calculated σ, σ(θ) using coupled reaction channels code FRESCO considering 8Be cluster exchange mechanism, optical potential in the entrance channel fitted to the published scattering data; deduced spectroscopic amplitudes to the selected discrete states in 12C; deduced little effect of couplings between excited states, arising from 12C nonsphericity in forward hemisphere, but strongly affect σ, dσ at large angles.
doi: 10.1140/epja/i2019-12712-8
2019BU13 Int.J.Mod.Phys. E28, 1950028 (2019) N.Burtebayev, M.Nassurlla, A.Sabidolda, S.B.Sakuta, A.A.Karakhodjaev, F.X.Ergashev, K.Rusek, E.Piasecki, A.Trzcinska, M.Wolinska-Cichocka, M.Kowalczyk, B.Mauyey, D.Janseitov, B.Zalewski, Sh.Hamada, K.W.Kemper, A.A.Ibraheem Measurement and analysis of 10B + 12C elastic scattering at energy of 41.3 MeV NUCLEAR REACTIONS 12C(10B, 10B), E=41.3 MeV; measured reaction products; deduced σ(θ), optical model parameters.
doi: 10.1142/S0218301319500289
2019BU28 Acta Phys.Pol. B50, 703 (2019) N.Burtebayev, Zh.K.Kerimkulov, M.Nassurlla, J.T.Burtebayeva, M.Nassurlla, S.B.Sakuta, T.Suzuki, K.Rusek, A.Trzcinska, M.Wolinska-Cichocka Study of the 7Li(d, t)6Li Reaction at the Energy of 14.5 MeV NUCLEAR REACTIONS 7Li(d, t), E=14.5 MeV; measured reaction products; deduced elastic and inelastic σ(θ). Comparison with coupled reaction channels (CRC) calculations.
doi: 10.5506/aphyspolb.50.703
2019KE02 Phys.Rev. C 99, 014615 (2019) N.Keeley, A.Pakou, V.Soukeras, F.Cappuzzello, L.Acosta, C.Agodi, A.Boiano, S.Calabrese, D.Carbone, M.Cavallaro, N.Deshmukh, A.Foti, A.Hacisalihoglu, M.La Commara, I.Martel, M.Mazzocco, A.Muoio, C.Parascandolo, D.Pierroutsakou, K.Rusek, A.M.Sanchez-Benitez, G.Santagati, O.Sgouros, G.Souliotis, A.Spatafora, E.Strano, D.Torresi, A.Trzcinska Coherent coupled-reaction-channels analysis of existing and new p + 9Be data between 1.7 and 15 MeV/nucleon NUCLEAR REACTIONS 1H(9Be, 9Be), E=15, 22, 51 MeV; measured scattered 9Be particles, σ(E, θ) using the large acceptance MAGNEX spectrometer at INFN-LNS-Catania. 9Be(p, p), (p, p'), (p, d), (polarized p, p), E=3, 68, 10, 15, MeV/nucleon; analyzed differential σ(θ, E), and vector analyzing powers Ay(θ); deduced renormalized differential σ(θ, E), and optical model parameters. Coupled-reaction-channels model using FRESCO code.
doi: 10.1103/PhysRevC.99.014615
2019PE09 Phys.Rev. C 99, 054606 (2019) D.Perez-Loureiro, J.Benlliure, J.Diaz-Cortes, J.L.Rodriguez-Sanchez, H.Alvarez-Pol, B.Blank, E.Casarejos, D.Dragosavac, V.Fohr, M.Gascon, W.Gawlikowicz, A.Heinz, K.Helariutta, A.Kelic-Heil, S.Lukic, F.Montes, L.Pienkowski, K-H.Schmidt, M.Staniou, K.Subotic, K.Summerer, J.Taieb, A.Trzcinska Neutron-rich fragments produced by in-flight fission of 238U NUCLEAR REACTIONS 208Pb(238U, F)90Kr/91Kr/94Rb/95Rb/96Rb/97Rb/98Rb/99Rb/100Rb/96Sr/97Sr/98Sr/99Sr/100Sr/101Sr/102Sr/103Sr/99Y/100Y/101Y/102Y/103Y/104Y/105Y/106Y/102Zr/103Zr/104Zr/105Zr/106Zr/107Zr/108Zr/109Zr/104Nb/105Nb/106Nb/107Nb/108Nb/109Nb/110Nb/111Nb/107Mo/108Mo/109Mo/110Mo/111Mo/112Mo/113Mo/110Tc/111Tc/112Tc/113Tc/114Tc/115Tc/116Tc/117Tc/112Ru/113Ru/114Ru/115Ru/116Ru/117Ru/118Ru/119Ru/115Rh/116Rh/117Rh/118Rh/119Rh/120Rh/121Rh/122Rh/118Pd/119Pd/120Pd/121Pd/122Pd/123Pd/124Pd/125Pd/120Ag/121Ag/122Ag/123Ag/124Ag/125Ag/126Ag/127Ag/128Ag/123Cd/124Cd/125Cd/126Cd/127Cd/128Cd/129Cd/130Cd/131Cd/126In/127In/128In/129In/130In/131In/132In/133In/134In/135In/128Sn/129Sn/130Sn/131Sn/132Sn/133Sn/134Sn/135Sn/136Sn/137Sn/132Sb/133Sb/134Sb/135Sb/136Sb/137Sb/138Sb/139Sb/135Te/136Te/137Te/138Te/139Te/140Te/141Te/142Te/137I/138I/139I/140I/141I/142I/143I/144I/141Xe/142Xe/143Xe/144Xe/145Xe/146Xe/147Xe/144Cs/145Cs/146Cs/147Cs/148Cs/149Cs/145Ba/146Ba/147Ba/148Ba/149Ba/150Ba/151Ba/148La/149La/150La/151La/152La/153La/151Ce/152Ce/153Ce/154Ce/152Pr/153Pr/155Pr/155Nd/156Nd, E=950 MeV/nucleon; 9Be(238U, F)80Ga/84Ga/79Ge/80Ge/82Ge/83Ge/84Ge/81As/82As/83As/85As/86As/87As/88As/84Se/85Se/87Se/88Se/89Se/90Se/86Br/87Br/88Br/89Br/91Br/92Br/93Br/94Br/89Kr/90Kr/91Kr/92Kr/93Kr/94Kr/95Kr/96Kr/97Kr/92Rb/93Rb/94Rb/95Rb/96Rb/97Rb/98Rb/99Rb/100Rb/101Rb/94Sr/95Sr/96Sr/97Sr/98Sr/99Sr/100Sr/101Sr/102Sr/103Sr/99Zr/100Zr/101Zr/102Zr/103Zr/104Zr/105Zr/106Zr/107Zr/108Zr/109Zr/102Nb/103Nb/104Nb/105Nb/106Nb/107Nb/108Nb/109Nb/110Nb/111Nb/112Nb/105Mo/106Mo/107Mo/108Mo/109Mo/110Mo/111Mo/112Mo/113Mo/114Mo/115Mo/107Tc/108Tc/109Tc/110Tc/111Tc/112Tc/113Tc/114Tc/115Tc/116Tc/117Tc/118Tc/110Ru/111Ru/112Ru/113Ru/114Ru/115Ru/116Ru/117Ru/118Ru/119Ru/120Ru/113Rh/114Rh/117Pd/118Pd/119Pd/120Pd/121Pd/122Pd/123Pd/124Pd/125Pd/118Ag/119Ag/120Ag/121Ag/122Ag/123Ag/124Ag/125Ag/126Ag/127Ag/128Ag/121Cd/122Cd/123Cd/124Cd/125Cd/126Cd/127Cd/128Cd/129Cd/130Cd/131Cd/132Cd/123In/124In/125In/126In/127In/128In/129In/130In/131In/132In/133In/134In/126Sn/127Sn/128Sn/129Sn/130Sn/131Sn/132Sn/133Sn/134Sn/135Sn/136Sn/137Sn/129Sb/133Te/134Te/135Te/136Te/137Te/138Te/139Te/140Te/141Te/142Te/143Te/135I/136I/137I/138I/139I/140I/141I/142I/143I/144I/145I/137Xe/138Xe/139Xe/140Xe/141Xe/142Xe/143Xe/144Xe/145Xe/146Xe/147Xe/140Cs/141Cs/142Cs/143Cs/144Cs/145Cs/146Cs/147Cs/148Cs/149Cs/143Ba/144Ba/145Ba/146Ba/147Ba/148Ba/149Ba/150Ba/151Ba/152Ba/146La/147La/148La/149La, E=950 MeV/nucleon; measured fission fragments, isotopic distributions of the fission fragments, production σ and yields using zero-degree magnetic spectrometer Fragment Separator at GSI accelerator facilities; deduced mean neutron-to-proton ratio of fission fragments, role of Coulomb and nuclear excitation mechanisms in the neutron excess of the final fragments.
doi: 10.1103/PhysRevC.99.054606
2019PI10 Phys.Rev. C 100, 014616 (2019) E.Piasecki, M.Kowalczyk, S.Yusa, A.Trzcinska, K.Hagino Dissipation and tunneling in heavy-ion reactions near the Coulomb barrier NUCLEAR REACTIONS 58,60,61Ni(20Ne, 20Ne), E(effective)=32-44 MeV; 90,92Zr(20Ne, 20Ne), E(effective)=40-62 MeV; 118Sn(20Ne, 20Ne), E(effective)=52-74 MeV; 208Pb(20Ne, 20Ne), E(effective)=82-110 MeV; calculated σ(E), barrier distributions, and barrier penetrabilities. 92Zr(20Ne, X), E(cm)=42-66 MeV; calculated fusion σ(E). Coupled channel (CC) calculations plus random matrix theory (RMT), including dissipation effects. Comparison with experimental data.
doi: 10.1103/PhysRevC.100.014616
2019RU01 Acta Phys.Pol. B50, 753 (2019) A.T.Rudchik, A.A.Rudchik, O.E.Kutsyk, K.W.Kemper, S.Kliczewski, K.Rusek, E.Piasecki, A.Trzcinska, E.I.Koshchy, Val.M.Pirnak, O.A.Ponkratenko, I.Strojek, V.A.Plujko, A.Stolarz, S.B.Sakuta, R.Siudak, O.V.Herashchenko, A.P.Ilyin, Yu.M.Stepanenko, Yu.O.Shyrma, V.V.Uleshchenko Elastic and Inelastic Scattering of 15N Ions by 12C at 81 MeV and the Effect of Transfer Channels NUCLEAR REACTIONS 12C(15N, 15N), (15N, 15N'), E=81 MeV; measured reaction products; deduced σ(θ), deformation parameters, parameters of Woods-Saxon potentials.
doi: 10.5506/APhysPolB.50.753
2019RU04 Nucl.Phys. A992, 121638 (2019) A.T.Rudchik, A.A.Rudchik, O.E.Kutsyk, K.W.Kemper, K.Rusek, E.Piasecki, A.Trzcinska, S.Kliczewski, E.I.Koshchy, Val.M.Pirnak, O.A.Ponkratenko, I.Strojek, V.A.Plujko, S.B.Sakuta, R.Siudak, A.P.Ilyin, Yu.M.Stepanenko, Yu.O.Shyrma, V.V.Uleshchenko 12C(15N, 14C)13N reaction at 81 MeV. Competition between one and two particle transfers
doi: 10.1016/j.nuclphysa.2019.121638
2018BU18 Int.J.Mod.Phys. E27, 1850094 (2018) N.Burtebayev, M.Nassurlla, M.Nassurlla, N.Saduyev, A.Sabidolda, D.Zazulin, T.Kh.Sadykov, S.B.Sakuta, A.Trzcinska, M.Wolinska-Cichocka Scattering of α-particles by 11B nuclei at an energy of 40 MeV and role of the exchange mechanism with transfer of 7Li NUCLEAR REACTIONS 11B(α, α'), (α, α), E=40 MeV; measured reaction products, Eα, Iα; deduced σ(θ).
doi: 10.1142/S0218301318500945
2018RU03 Nucl.Phys. A971, 138 (2018) A.T.Rudchik, A.A.Rudchik, L.M.Muravynets, K.W.Kemper, K.Rusek, E.I.Koshchy, E.Piasecki, A.Trzcinska, Val.M.Pirnak, O.A.Ponkratenko, I.Strojek, A.Stolarz, V.A.Plujko, S.B.Sakuta, R.Siudak, A.P.Ilyin, Yu.M.Stepanenko, Yu.O.Shyrma, V.V.Uleshchenko 7Li(15N, 14C)8Be reaction at 81 MeV and 14C + 8Be interaction versus that of 13C + 8Be NUCLEAR REACTIONS 7Li(15N, 14C)8Be, E=81 MeV; measured reaction products angular distributions to 8Be gs and first two excited states; deduced σ(θ); calculated σ(θ) using CRC (Coupled Reaction Channels) FRESCO code with potential from earlier analyses and spectroscopic amplitudes using TISM (Translationally Invariant Shell Model) code DESNA. 8Be(14C, 13C), E not given;13C(8Be, 7Li), E not given; calculated σ(θ) using CRC; deduced WS potential parameters to be used for the 7Li(15N, 14C)8Be.
doi: 10.1016/j.nuclphysa.2018.01.014
2018TR06 Acta Phys.Pol. B49, 393 (2018) A.Trzcinska, E.Piasecki, M.Kowalczyk, G.Cardella, E.De Filippo, D.Dell'Aquila, S.De Luca, B.Gnoffo, G.Lanzalone, I.Lombardo, C.Maiolino, N.S.Martorana, S.Norella, A.Pagano, E.V.Pagano, M.Papa, S.Pirrone, G.Politi, L.Quattrocchi, F.Rizzo, P.Russotto, A.Trifiro, M.Trimarchi, M.Vigilante Influence of Single Particle Excitations on Barrier Distributions: 24Mg + 90, 92Zr NUCLEAR REACTIONS 90,92Zr(24Mg, x), E=68-88.5 MeV; measured back-scattered ions using Si detectors at 6 backward angles and 4 detectors at forward angles; deduced Rutherford σ, energy spectra of emitted ions, barrier heights distributions; calculated measured reactions using Coupled Channels (CC); deduced discrepancy between predictions and data; deduced possibility of cumulative effect of many individual weak channels (such as non-collective excitations of the target). Preliminary.
doi: 10.5506/aphyspolb.49.393
2018WO01 Acta Phys.Pol. B49, 387 (2018) D.Wojcik, A.Trzcinska, E.Piasecki, M.Kisielinski, M.Kowalczyk, M.Wolinska-Cichocka, C.Bordeanu, B.Gnoffo, H.Jia, C.Lin, N.S.Martorana, M.Mutterer, E.V.Pagano, K.Piasecki, P.Russotto, L.Quatrocchi, W.H.Trzaska, G.Tiurin, R.Wolski, H.Zhang Transfer Cross Sections at Near-barrier Energy for the 24Mg + 90, 92Zr Systems NUCLEAR REACTIONS 90,92Zr(24Mg, x), E=76 MeV; measured using multidetector system ICARE with start signal bz the Microchannel Plate (MCP) and stop signal by one of Si detectors placed at polar angle 142, used also to measure the energy of reaction products, and beam energy monitored by Si detectors at 30; deduced E-ToF spectra of backscattered ions; measured stripping reactions involving up up to 4 nucleons and reaction channels up to 2 nucleons picked up (i.e. the product mass from A-6 to A+2, A is the target mass); deduced transfer σtr(θ) and lacking structure of distribution of barrier heights, the cross sections are considerably smaller than those for 20Ne projectile. Preliminary.
doi: 10.5506/aphyspolb.49.387
2017RU01 Nucl.Phys. A958, 234 (2017) A.T.Rudchik, A.A.Rudchik, L.M.Muravynets, K.W.Kemper, K.Rusek, E.Piasecki, A.Trzcinska, E.I.Koshchy, Val.M.Pirnak, O.A.Ponkratenko, I.Strojek, A.Stolarz, O.V.Herashchenko, Yu.M.Stepanenko, V.A.Plujko, S.B.Sakuta, R.Siudak, A.Szczurek Elastic and inelastic scattering of 15N ions by 7Li at 81 MeV versus that of 14N ions by 7Li at 80 and 110 MeV NUCLEAR REACTIONS 7Li(15N, 15N), (15N, 15N'), E=81 MeV;7Li(14N, 14N), (14N, 14N'), E=80, 110 MeV. 7Li measured E(7Li), I(θ, 7Li) using ΔE-E Si telescopes; deduced σ(θ); calculated spectroscopic amplitudes, deformation. σ(θ), reaction σ using CC within TISM (Translational Invariant Shell Model); deduced potential parameters.
doi: 10.1016/j.nuclphysa.2016.12.007
2016RU02 Nucl.Phys. A947, 161 (2016) A.T.Rudchik, K.A.Chercas, K.W.Kemper, K.Rusek, A.A.Rudchik, O.V.Herashchenko, E.I.Koshchy, Val.M.Pirnak, E.Piasecki, A.Trzcinska, S.B.Sakuta, R.Siudak, I.Strojek, A.Stolarz, A.P.Ilyin, O.A.Ponkratenko, Yu.M.Stepanenko, Yu.O.Shyrma, A.Szczurek, V.V.Uleshchenko Elastic and inelastic scattering of 15N ions by 9Be at 84 MeV NUCLEAR REACTIONS 9Be(15N, 15N), (15N, 15N'), E=84 MeV; measured reaction products by four ΔE-E telescopes at different angles; deduced σ(θ) to discrete states; calculated 9Be+15N double-folding potential using M3Y potential and charge distribution in both nuclei from literature, σ(θ) using optical model and CRC; deduced reaction mechanism, potential parameters, deformation.
doi: 10.1016/j.nuclphysa.2016.01.002
2016SZ04 Appl.Radiat.Isot. 118, 182 (2016) K.Szkliniarz, M.Sitarz, R.Walczak, J.Jastrzebski, A.Bilewicz, J.Choinski, A.Jakubowski, A.Majkowska, A.Stolarz, A.Trzcinska, W.Zipper Production of medical Sc radioisotopes with an alpha particle beam NUCLEAR REACTIONS Ca, K, 42Ca(α, X)43Sc/44Sc, E=29 MeV; measured reaction products, Eγ, Iγ; deduced σ, thick target yields. Comparison with EMPIRE code calculations.
doi: 10.1016/j.apradiso.2016.07.001
2016TR05 Phys.Rev. C 93, 054604 (2016) A.Trzcinska, E.Piasecki, A.Amar, W.Czarnacki, N.Keeley, M.Kisielinski, S.Kliczewski, M.Kowalczyk, B.Lommel, M.Mutterer, R.Siudak, A.Stolarz, I.Strojek, G.Tiourin, W.H.Trzaska Examination of the influence of transfer channels on the barrier height distribution: Scattering of 20Ne on 58Ni, 60Ni, and 61Ni at near-barrier energies NUCLEAR REACTIONS 20Ne(58Ni, X), (60Ni, X), (61Ni, X), E=51 MeV; measured reaction products based on time-of-flight and ΔE-E methods, angular distributions, transfer probabilities and transfer cross sections for 1p, 1n, 2n, 2p and α pickup and stripping channels. Experiments carried out at Warsaw U200-P cyclotron facility. Comparison with coupled reaction channel calculations.
doi: 10.1103/PhysRevC.93.054604
2015BU07 Acta Phys.Pol. B46, 1037 (2015) N.Burtebayev, J.T.Burtebayeva, A.Duisebayev, Zh.K.Kerimkulov, M.Nassurlla, T.Zholdybayev, S.V.Artemov, A.A.Karakhodzhayev, U.S.Salikhbayev, S.B.Sakuta, S.Kliczewski, E.Piasecki, K.Rusek, R.Siudak, A.Trzcinska, M.Wolinska-Cichocka, A.Amar Mechanism of the 7Li(d, t)6Li Reaction at 25 MeV Energy of Deuterons, Values of Spectroscopic Factors and Asymptotic Normalization Coefficients for the 7Li → 6Li + n Vertex NUCLEAR REACTIONS 7Li(d, d), (d, d'), (d, t), E=25 MeV; measured reaction products; deduced deformation lenghts and spectroscopic factors, σ(θ). Comparison with CRC and the DWBA calculations.
doi: 10.5506/APhysPolB.46.1037
2015PA24 Eur.Phys.J. A 51, 55 (2015) A.Pakou, D.Pierroutsakou, M.Mazzocco, L.Acosta, X.Aslanoglou, A.Boiano, C.Boiano, D.Carbone, M.Cavallaro, J.Grebosz, N.Keeley, M.La Commara, C.Manea, G.Marquinez-Duran, I.Martel, C.Parascandolo, K.Rusek, A.M.Sanchez-Benitez, O.Sgouros, C.Signorini, F.Soramel, V.Soukeras, E.Stiliaris, E.Strano, D.Torresi, A.Trzcinska, Y.X.Watanabe, H.Yamaguchi Total reaction cross sections for 8Li + 90Zr at near-barrier energies NUCLEAR REACTIONS 90Zr(8Li, 8Li'), E=18.5-21.5 MeV; measured halo nucleus reaction products; deduced quasielastic scattering σ(θ), total reaction σ, ratio direct-to-total σ and systematics of total σ using data from other reactions; calculated quasielastic scattering σ(θ) using optical model with double-folded potentials based on BDM3Y1, ratio direct-to-total σ using CC.
doi: 10.1140/epja/i2015-15055-6
2015PA33 Eur.Phys.J. A 51, 90 (2015) A.Pakou, N.Keeley, D.Pierroutsakou, M.Mazzocco, L.Acosta, X.Aslanoglou, A.Boiano, C.Boiano, D.Carbone, M.Cavallaro, J.Grebosz, M.La Commara, C.Manea, G.Marquinez-Duran, I.Martel, C.Parascandolo, K.Rusek, A.M.Sanchez-Benitez, O.Sgouros, C.Signorini, F.Soramel, V.Soukeras, E.Stiliaris, E.Strano, D.Torresi, A.Trzcinska, Y.X.Watanabe, H.Yamaguchi Important influence of single neutron stripping coupling on near-barrier 8Li + 90Zr quasi-elastic scattering NUCLEAR REACTIONS 90Zr(8Li, 8Li'), E=18.5 MeV; measured Li ions using EXOTIC detector array telescopes; deduced σ(θ); calculated σ(θ) (also for 6,7Li+90Zr), B(E2) using no-coupling and CC with optical potential with double-folded real part and deformation from 6Li+90Zr; deduced strong coupling effect for single neutron stripping.
doi: 10.1140/epja/i2015-15090-3
2015RU06 Nucl.Phys. A941, 167 (2015) A.T.Rudchik, O.V.Herashchenko, K.W.Kemper, K.Rusek, S.Kliczewski, K.A.Chercas, A.A.Rudchik, E.I.Koshchy, Val.M.Pirnak, E.Piasecki, A.Trzcinska, S.B.Sakuta, R.Siudak, I.Strojek, A.Stolarz, S.O.Odzhikovskyi, A.P.Ilyin, O.A.Ponkratenko, Yu.M.Stepanenko, Yu.O.Shyrma, V.V.Uleshchenko, A.Szczurek Elastic and inelastic scattering of 14N ions by 11B at 88 MeV versus that of 15N + 11B at 84 MeV NUCLEAR REACTIONS 11B(14N, 14N), (14N, 14N'), E=88 MeV;11B(15N, 15N), E=84 MeV; measured nitrogen energy spectra at angles; deduced σ(θ); calculated σ(θ) using optical model and CC with reorientation and one- and two-step transfer reactions; deduced reaction mechanisms, optical model parameters, spectroscopic amplitudes for different (mainly d, t, 3He, α) clusters, deformation.
doi: 10.1016/j.nuclphysa.2015.06.012
2015TR06 Phys.Rev. C 92, 034619 (2015) A.Trzcinska, E.Piasecki, K.Hagino, W.Czarnacki, P.Decowski, N.Keeley, M.Kisielinski, P.Koczon, A.Kordyasz, E.Koshchiy, M.Kowalczyk, B.Lommel, A.Stolarz, I.Strojek, K.Zerva Quasielastic barrier distributions for the 20Ne + 58, 60, 61Ni systems: Influence of weak channels NUCLEAR REACTIONS 58,60,62Ni(20Ne, 20Ne'), E=43-62 MeV; measured excitation function for back-scattered ions, σ(E) at Heavy Ion Laboratory, University of Warsaw; deduced barrier height distributions. Comparisons with predictions by coupled-channel (CC) calculations.
doi: 10.1103/PhysRevC.92.034619
2014SA43 Acta Phys.Pol. B45, 1853 (2014) S.B.Sakuta, N.Burtebayev, J.T.Burtebayeva, A.Duisebayev, N.V.Glushchenko, M.Nassurlla, A.Amar, S.V.Artemov, S.Kliczewski, E.Piasecki, K.Rusek, R.Siudak, A.Trzcinska, M.Wolinska-Cichocka The Channel Coupling and Triton Cluster Exchange Effects in 3He Scattering on 6Li Nuclei NUCLEAR REACTIONS 6Li(3He, 3He), (3He, X), E=18-217 MeV; analyzed available data; deduced phenomenological potentials, parameters, σ. Comparison with available data, predictions of the microscopic theory.
doi: 10.5506/APhysPolB.45.1853
2014TR03 Acta Phys.Pol. B45, 383 (2014) A.Trzcinska, E.Piasecki, W.Czarnacki, P.Decowski, N.Keeley, M.Kisielinski, S.Kliczewski, P.Koczon, A.Kordyasz, M.Kowalczyk, S.Khlebnikov, E.Koshchiy, T.Krogulski, B.Lommel, T.Loktev, M.Mutterer, K.Piasecki, I.Strojek, W.H.Trzaska, S.Smirnov, A.Stolarz, G.Tiourin Barrier Height Distributions - the Influence of Weak Channels
doi: 10.5506/APhysPolB.45.383
2013SG01 Int.J.Mod.Phys. E22, 1350073 (2013) O.Sgouros, V.Soukeras, A.Pakou, N.Patronis, K.Zerva, N.Keeley, I.Strojek, A.Trzcinska, E.Piasecki, K.Rusek, E.Stiliaris, M.Mazzocco Backward angle structure in the 20Ne+28Si quasielastic scattering NUCLEAR REACTIONS 28Si(20Ne, 20Ne), E=42.5, 52.3 MeV; 28Si(20Ne, 24Mg), (20Ne, 16O), (20Ne, 12C), E=52.3 MeV; measured transfer reaction products; deduced spectroscopic amplitudes, σ, σ(θ). Comparison with coupled channels calculations.
doi: 10.1142/S0218301313500730
2012PA02 Phys.Rev. C 85, 024609 (2012) N.Patronis, A.Pakou, D.Pierroutsakou, A.M.Sanchez-Benitez, L.Acosta, N.Alamanos, A.Boiano, G.Inglima, D.Filipescu, T.Glodariu, A.Guglielmetti, M.La Commara, G.Lalazissis, I.Martel, C.Mazzocchi, M.Mazzocco, P.Molini, C.Parascandolo, M.Sandoli, C.Signorini, R.Silvestri, F.Soramel, E.Stiliaris, M.Romoli, A.Trzcinska, K.Zerva, E.Vardaci, A.Vitturi Probing the 17F+p potential by elastic scattering at near-barrier energies NUCLEAR REACTIONS 1H(17F, p), E=3.5, 4.3 MeV/nucleon; measured particle spectra, elastic scattering, full angular distribution in c.m. system; deduced total reaction cross section. Comparison with optical model, macroscopic and microscopic analyses. Possible halo structure of the proton-rich nucleus.
doi: 10.1103/PhysRevC.85.024609
2012PI08 Phys.Rev. C 85, 054604 (2012); Pub.Note Phys.Rev. C 85, 059903 (2012) E.Piasecki, W.Czarnacki, N.Keeley, M.Kisielinski, S.Kliczewski, A.Kordyasz, M.Kowalczyk, S.Khlebnikov, E.Koshchiy, T.Krogulski, T.Loktev, M.Mutterer, A.Piorkowska, K.Rusek, M.Sillanpaa, A.Staudt, I.Strojek, S.Smirnov, W.H.Trzaska, A.Trzcinska Weak channels in backscattering of 20Ne on natNi, 118Sn, and 208Pb NUCLEAR REACTIONS Ni(20Ne, X), E=51.7 MeV; 118Sn(20Ne, X), E=72.1 MeV; 208Pb(20Ne, X), E=102.0 MeV; measured particle spectra, time of flight, energy loss, transfer σ; deduced mass distribution of reaction products, inelastic Q-spectra. 90Zr(20Ne, X), E=62.8 MeV; 92Zr(20Ne, X), E=62.6 MeV; analyzed data. Comparison with coupled-channels (CC) calculations.
doi: 10.1103/PhysRevC.85.054604
2012PI09 Phys.Rev. C 85, 054608 (2012); Pub.Note Phys.Rev. C 85, 059902 (2012) E.Piasecki, L.Swiderski, N.Keeley, M.Kisielinski, M.Kowalczyk, S.Khlebnikov, T.Krogulski, K.Piasecki, G.Tiourin, M.Sillanpaa, W.H.Trzaska, A.Trzcinska Smoothing of structure in the fusion and quasielastic barrier distributions for the 20Ne + 208Pb system NUCLEAR REACTIONS 208Pb(20Ne, 20Ne), (20Ne, X), E=93-117 MeV; measured time of flight spectrum for fission fragments, fusion σ(E), quasielastic scattering σ(E); deduced fusion and quasielastic barrier height distributions. Comparison with coupled-channels calculations.
doi: 10.1103/PhysRevC.85.054608
2012ST03 Acta Phys.Pol. B43, 339 (2012) I.Strojek, W.Czarnacki, W.Gawlikowicz, N.Keeley, M.Kisielinski, S.Kliczewski, A.Kordyasz, E.Koshchiy, M.Kowalczyk, E.Piasecki, A.Piorkowska, K.Rusek, R.Siudak, A.Staudt, A.Trzcinska Structure Effects in 20Ne + 208Pb Quasi-elastic Scattering NUCLEAR REACTIONS 208Pb(20Ne, 20Ne'), E=108.6, 115 MeV; measured reaction products, Eγ, Iγ; deduced σ, quasi-elastic barrier height distribution, nuclear deformation length. Comparison with coupled-channel calculations.
doi: 10.5506/APhysPolB.43.339
2011PE20 Phys.Lett. B 703, 552 (2011) D.Perez-Loureiro, J.Benlliure, H.Alvarez-Pol, B.Blank, E.Casarejos, D.Dragosavac, V.Fohr, M.Gascon, W.Gawlikowicz, A.Heinz, K.Helariutta, A.Kelic-Heil, S.Lukic, F.Montes, L.Pienkowski, K.-H.Schmidt, M.Staniou, K.Subotic, K.Summerer, J.Taieb, A.Trzcinska Production of neutron-rich nuclei in fragmentation reactions of 132Sn projectiles at relativistic energies NUCLEAR REACTIONS Pb(238U, X)132Sn, E=950 MeV/nucleon; Be(132Sn, X), E not given; measured reaction products; deduced σ. Comparison with code COFRA results.
doi: 10.1016/j.physletb.2011.08.037
2010BE24 Nucl.Phys. A834, 467c (2010) J.Benlliure, D.Dragosavac, D.Perez-Loureiro, H.Alvarez-Pol, B.Blank, E.Casarejos, V.Fohr, M.Gascon, W.Gawlikowicz, A.Heinz, K.Helariutta, S.Lukic, F.Montes, L.Pienkowski, M.Staniou, K.Subotic, K.Summerer, J.Taieb, A.Trzcinska, M.Veselsky Investigating the radial distributions of medium-mass nuclei NUCLEAR REACTIONS 9Be(111Sn, X), (112Sn, X), (113Sn, X), (114Sn, X), (115Sn, X), (117Sn, X), (118Sn, X), (119Sn, X), (120Sn, X), (121Sn, X), (123Sn, X), (124Sn, X), (125Sn, X), (126Sn, X), (127Sn, X), (128Sn, X), (129Sn, X), (130Sn, X), (131Sn, X), (132Sn, X), (133Sn, X), (134Sn, X), (135Sn, X), E not given; measured total σ; analyzed σ, radii dependence, halo nuclei, neutron skin. Calculations using Glauber model optical limit and "black disk". Transmission method with FRS at GSI.
doi: 10.1016/j.nuclphysa.2010.01.066
2010WI04 Int.J.Mod.Phys. E19, 672 (2010) A.Wieloch, Z.Sosin, P.Banka, A.Gonciarz, J.Peter, A.Drouart, R.Dayras, K.Lojek, Ch.Stodel, M.Adamczyk, B.Avez, P.Lasko, L.Zosiak, T.Kozik, N.Alamanos, A.Gillibert, S.Grevy, F.Hanappe, F.Hannachi, R.Hue, A.Khouaja, A.Lopez-Martens, L.Manduci, F.De Oliveira Santos, G.Politi, M.G.Saint-Laurent, L.Stuttge, Ch.Vandamme, J.P.Wieleczko, E.Piasecki, A.Trzcinska, W.Gawlikowicz, M.Kisielewski, M.Kowalczyk, A.Kordyasz, J.Blocki New detector system for super heavy elements detection
doi: 10.1142/S0218301310015084
2009PE12 Acta Phys.Pol. B40, 863 (2009) D.Perez-Loureiro, H.Alvarez-Pol, J.Benlliure, B.Blank, E.Casarejos, D.Dragosavac, V.Fohr, M.Gascon, W.Gawlikowicz, A.Heinz, K.Helariutta, A.Kelic, S.Lukic, F.Montes, L.Pienkowski, K.-H.Schmidt, M.Staniou, K.Subotic, K.Summerer, J.Taieb, A.Trzcinska Production of Medium-Mass Neutron Rich Nuclei from Fragmentation of Fission Residues Around Sn
2009PI08 Acta Phys.Pol. B40, 849 (2009) E.Piasecki, A.Trzcinska, W.Gawlikowicz, J.Jastrzebski, N.Keeley, M.Kisielinski, S.Kliczewski, A.Kordyasz, M.Kowalczyk, S.Khlebnikov, E.Koshchiy, E.Kozulin, T.Krogulski, T.Lotkiev, M.Mutterer, K.Piasecki, A.Piorkowska, K.Rusek, A.Staudt, I.Strojek, W.H.Trzaska, M.Sillanpaa, S.Smirnov, G.Tiourin, K.Hagino, N.Rowley Are the Weak Channels Really Weak?
2009PI15 Phys.Rev. C 80, 054613 (2009) E.Piasecki, L.Swiderski, W.Gawlikowicz, J.Jastrzebski, N.Keeley, M.Kisielinski, S.Kliczewski, A.Kordyasz, M.Kowalczyk, S.Khlebnikov, E.Koshchiy, E.Kozulin, T.Krogulski, T.Loktev, M.Mutterer, K.Piasecki, A.Piorkowska, K.Rusek, A.Staudt, M.Sillanpaa, S.Smirnov, I.Strojek, G.Tiourin, W.H.Trzaska, A.Trzcinska, K.Hagino, N.Rowley Effects of weakly coupled channels on quasielastic barrier distributions NUCLEAR REACTIONS 90,92Zr(20Ne, X), E=36-64 MeV; measured backscattered particle spectra, quasielastic σ; deduced barrier distributions, inelastic Q-value spectra and particle-transfer σ. Comparison with coupled-channel calculations.
doi: 10.1103/PhysRevC.80.054613
2007BR22 Phys.Rev. C 76, 034305 (2007) B.A.Brown, G.Shen, G.C.Hillhouse, J.Meng, A.Trzcinska Neutron skin deduced from antiprotonic atom data
doi: 10.1103/PhysRevC.76.034305
2007KL02 Phys.Rev. C 76, 014311 (2007) B.Klos, A.Trzcinska, J.Jastrzebski, T.Czosnyka, M.Kisielinski, P.Lubinski, P.Napiorkowski, L.Pienkowski, F.J.Hartmann, B.Ketzer, P.Ring, R.Schmidt, T.von Egidy, R.Smolanczuk, S.Wycech, K.Gulda, W.Kurcewicz, E.Widmann, B.A.Brown Neutron density distributions from antiprotonic 208Pb and 209Bi atoms NUCLEAR REACTIONS 208Pb, 209Bi(p-bar, X-ray), E at 106 MeV/c; measured x-ray cascade from antiprotonic atoms. Deduced neutron densities and rms radii.
doi: 10.1103/PhysRevC.76.014311
2007WY02 Phys.Rev. C 76, 034316 (2007) S.Wycech, F.J.Hartmann, J.Jastrzebski, B.Klos, A.Trzcinska, T.von Egidy Nuclear surface studies with antiprotonic atom x rays
doi: 10.1103/PhysRevC.76.034316
2005SW02 Phys.Rev. C 71, 047301 (2005) W.J.Swiatecki, A.Trzcinska, J.Jastrzebski Difference of the root-mean-square sizes of neutron and proton distributions in nuclei: Comparison of theory with data NUCLEAR STRUCTURE 40,48Ca, 54,56,57Fe, 58,60,64Ni, 59Co, 90,96Zr, 106,116Cd, 112,116,120,124Sn, 122,124,126,128Te, 208Pb, 209Bi, 232Th, 238U; calculated neutron-proton radius difference. Droplet model, comparison with data.
doi: 10.1103/PhysRevC.71.047301
2004FR32 Nucl.Phys. A746, 384c (2004) T.Fritioff, M.Grieser, M.Lindroos, A.Trzcinska A low energy storage ring for partly stripped radioactive ions
doi: 10.1016/j.nuclphysa.2004.09.055
2004JA03 Int.J.Mod.Phys. E13, 343 (2004) J.Jastrzebski, A.Trzcinska, P.Lubinski, B.Klos, F.J.Hartmann, T.von Egidy, S.Wycech Neutron density distributions from antiprotonic atoms compared with hadron scattering data NUCLEAR STRUCTURE 40,48Ca, 54,56,57Fe, 58,60,64Ni, 59Co, 90,96Zr, 106,116Cd, 112,116,120,124Sn, 122,124,126,128,130Te, 208Pb, 209Bi, 232Th, 238U; analyzed antiproton annihilation data; deduced neutron and proton density distributions, radii.
doi: 10.1142/S0218301304002168
2004KL06 Phys.Rev. C 69, 044311 (2004) B.Klos, S.Wycech, A.Trzcinska, J.Jastrzebski, T.Czosnyka, M.Kisielinski, P.Lubinski, P.Napiorkowski, L.Pienkowski, F.J.Hartmann, B.Ketzer, R.Schmidt, T.von Egidy, J.Cugnon, K.Gulda, W.Kurcewicz, E.Widmann Strong interaction and E2 effect in even-A antiprotonic Te atoms ATOMIC PHYSICS 122,124,126,128,130Te(p-bar, X), E at 106, 300 MeV/c; measured X-ray spectra from antiprotonic atoms; deduced level widths and shifts, nuclear resonance effect. 122,124,126,128,130Te deduced relative neutron, proton radii, neutron density at periphery.
doi: 10.1103/PhysRevC.69.044311
2004TR02 Nucl.Instrum.Methods Phys.Res. B214, 157 (2004) A.Trzcinska, J.Jastrzebski, P.Lubinski, F.J.Hartmann, R.Schmidt, T.von Egidy, B.Klos Information on the nuclear periphery deduced from the properties of heavy antiprotonic atoms NUCLEAR STRUCTURE 48Ca, 58Ni, 96Zr, 106,116Cd, 112,124Sn, 128Te, 208Pb; analyzed antiprotonic-atom X-ray data; deduced neutron and proton density distributions, radii.
doi: 10.1016/j.nimb.2003.08.017
2003SC13 Phys.Rev. C 67, 044308 (2003) R.Schmidt, A.Trzcinska, T.Czosnyka, T.von Egidy, K.Gulda, F.J.Hartmann, J.Jastrzebski, B.Ketzer, M.Kisielinski, B.Klos, W.Kurcewicz, P.Lubinski, P.Napiorkowski, L.Pienkowski, R.Smolanczuk, E.Widmann, S.Wycech Nucleon density in the nuclear periphery determined with antiprotonic x rays: Cadmium and tin isotopes NUCLEAR REACTIONS 106,116Cd, 112,116,120,124Sn(p-bar, X), E at rest; measured antiprotonic x-ray spectra. 106,116Cd, 112,116,120,124Sn deduced nucleon density distributions, radii. Comparison with previous data and model predictions. ATOMIC PHYSICS 106,116Cd, 112,116,120,124Sn; measured antiprotonic x-ray spectra; deduced atomic level widths and shifts.
doi: 10.1103/PhysRevC.67.044308
2002HA01 Phys.Rev. C65, 014306 (2002) F.J.Hartmann, R.Schmidt, B.Ketzer, T.von Egidy, S.Wycech, R.Smolanczuk, T.Czosnyka, J.Jastrzebski, M.Kisielinski, P.Lubinski, P.Napiorkowski, L.Pienkowski, A.Trzcinska, B.Klos, K.Gulda, W.Kurcewicz, E.Widmann Nucleon Density in the Nuclear Periphery Determined with Antiprotonic X Rays: Calcium isotopes ATOMIC PHYSICS 16O, 40,42,43,44,48Ca(p-bar, X), E at rest; measured antiprotonic X-ray spectra; deduced level widths. 40,42,43,44,48Ca deduced neutron density distribution features. NUCLEAR REACTIONS 16O, 40,42,43,44,48Ca(p-bar, X), E at rest; measured antiprotonic X-ray spectra; deduced level widths. 40,42,43,44,48Ca deduced neutron density distribution features.
doi: 10.1103/PhysRevC.65.014306
2002LU12 Phys.Rev. C66, 044616 (2002) P.Lubinski, A.Grochulska, T.von Egidy, K.Gulda, F.J.Hartmann, J.Jastrzebski, W.Kurcewicz, L.Pienkowski, A.Stolarz, A.Trzcinska Gold fragmentation induced by stopped antiprotons NUCLEAR REACTIONS 197Au(p-bar, X), E=0-6.5 MeV; measured fragment isotopic yields; deduced mass and charge distributions, reaction mechanism features. Comparisons with previous results.
doi: 10.1103/PhysRevC.66.044616
2001HA49 Acta Phys.Hung.N.S. 13, 51 (2001) F.J.Hartmann, R.Schmidt, T.von Egidy, J.Jastrzebski, P.Lubinski, L.Pienkowski, A.Trzcinska, R.Smolanczuk, S.Wycech, B.Klos Study of the Nuclear Periphery and Antiprotons
doi: 10.1556/APH.13.2001.1-3.7
2001TR03 Acta Phys.Pol. B32, 917 (2001) A.Trzcinska, J.Jastrzebski, P.Lubinski, F.J.Hartmann, R.Schmidt, T.von Egidy, B.Klos Information on the Nuclear Periphery from Antiprotonic Atoms NUCLEAR STRUCTURE 48Ca, 58Ni, 96Zr, 112,124Sn, 208Pb; analyzed antiprotonic atom annihilation data; deduced proton, neutron peripheral density features.
2001TR19 Phys.Rev.Lett. 87, 082501 (2001) A.Trzcinska, J.Jastrzebski, P.Lubinski, F.J.Hartmann, R.Schmidt, T.von Egidy, B.Klos Neutron Density Distributions Deduced from Antiprotonic Atoms NUCLEAR REACTIONS 40,48Ca, 54,56,57Fe, 59Co, 58,60,64Ni, 90,96Zr, 112,116,120,124Sn, 116Cd, 128Te, 208Pb, 209Bi, 232Th, 238U(p-bar, X), E at rest; measured x-ray spectra, residual annihilation yields. 40,48Ca, 54,56,57Fe, 59Co, 58,60,64Ni, 90,96Zr, 112,116,120,124Sn, 116Cd, 128Te, 208Pb, 209Bi, 232Th, 238U deduced neutron radii, density distributions.
doi: 10.1103/PhysRevLett.87.082501
2001TR23 Nucl.Phys. A692, 176c (2001) A.Trzcinska, J.Jastrzebski, T.Czosnyka, T.von Egidy, K.Gulda, F.J.Hartmann, J.Iwanicki, B.Ketzer, M.Kisielinski, B.Klos, W.Kurcewicz, P.Lubinski, P.J.Napiorkowski, L.Pienkowski, R.Schmidt, E.Widmann Information on Antiprotonic Atoms and the Nuclear Periphery from the PS209 Experiment NUCLEAR STRUCTURE 48Ca, 112,116,120,124Sn, 208Pb; analyzed antiproton annihilation data; deduced neutron-to-proton density ratios. ATOMIC PHYSICS 16O, 40,42,43,44,48Ca, 54,56,57,58Fe, 59Co, 58,60,62,64Ni, 90,96Zr, 106,116Cd, 112,116,120,124Sn, 122,124,126,128,130Te, 172,176Yb, 208Pb, 209Bi, 232Th, 238U; measured antiprotonic atoms strong interaction level widths, shifts.
doi: 10.1016/S0375-9474(01)01176-9
1999HA41 Nucl.Phys. A655, 289c (1999) F.J.Hartmann, T.Czosnyka, K.Gulda, J.Jastrzebski, B.Ketzer, M.Kisielinski, B.Klos, J.Kulpa, W.Kurcewicz, P.Lubinski, P.Napiorkowski, L.Pienkowski, R.Schmidt, R.Smolanczuk, A.Trzcinska, T.von Egidy, E.Widmann, S.Wycech Antiprotonic Atoms as a Tool to Study the Nuclear Periphery
doi: 10.1016/S0375-9474(99)00215-8
1999SC35 Phys.Rev. C60, 054309 (1999) R.Schmidt, F.J.Hartmann, B.Ketzer, T.von Egidy, T.Czosnyka, J.Jastrzebski, M.Kisielinski, P.Lubinski, P.Napiorkowski, L.Pienkowski, A.Trzcinska, B.Klos, R.Smolanczuk, S.Wycech, W.Poschl, K.Gulda, W.Kurcewicz, E.Widmann Composition of the Nuclear Periphery from Antiproton Absorption using Short-Lived Residual Nuclei NUCLEAR REACTIONS 48Ca, 100Mo, 104Ru, 112,124Sn, 116Cd(p-bar, X), E at rest; measured Eγ, Iγ(t) following residual nucleus decay; deduced yields, isomeric ratios. 48Ca, 100Mo, 104Ru, 112,124Sn, 116Cd deduced peripheral neutron-to-proton ratios, effective scattering lengths of antiprotons. Comparison with Hartree-Fock-Bogoliubov calculations.
doi: 10.1103/PhysRevC.60.054309
1999SC49 Hyperfine Interactions 118, 67 (1999) R.Schmidt, T.Czosnyka, K.Gulda, F.J.Hartmann, J.Jastrzebski, B.Ketzer, B.Klos, J.Kulpa, W.Kurcewicz, P.Lubinski, P.Napiorkowski, L.Pienkowski, R.Smolanczuk, A.Trzcinska, T.von Egidy, E.Widmann, S.Wycech Determination of the proton and neutron densities at the nuclear periphery with antiprotonic X-rays and (p-bar)-nucleus reactions NUCLEAR REACTIONS 172,176Yb(p-bar, X), E at rest; measured X-ray spectra; deduced strong interaction shifts, widths. 172,176Yb deduced surface nucleon densities. ATOMIC PHYSICS 172,176Yb(p-bar, X), E at rest; measured X-ray spectra; deduced strong interaction shifts, widths. 172,176Yb deduced surface nucleon densities.
doi: 10.1023/A:1012680402100
1999WY01 Nucl.Phys. A655, 257c (1999) S.Wycech, T.Czosnyka, T.von Egidy, E.J.Hartmann, J.Jastrzebski, B.Klos, J.Kulpa, P.Lubinski, L.Pienkowski, R.Smolanczuk, R.Schmidt, A.Trzcinska Nuclear Interactions of Antiprotons: Theory
doi: 10.1016/S0375-9474(99)00210-9
1998LU05 Phys.Rev. C57, 2962 (1998) P.Lubinski, J.Jastrzebski, A.Trzcinska, W.Kurcewicz, F.J.Hartmann, W.Schmid, T.von Egidy, R.Smolanczuk, S.Wycech Composition of the Nuclear Periphery from Antiproton Absorption NUCLEAR REACTIONS 45Sc, 56Fe, 58Ni, 96Zr, 96Ru, Cd, 106Cd, 128,130Te, Te, 144,154Sm, 148Nd, Eu, 160Gd, Yb, 176Yb, 206Pb, 232Th, 238U(p-bar, X), E at rest; measured Eγ, Iγ; deduced annihilation products yields, isomeric ratios, charge exchange processes. 58Ni, 96Ru, 96Zr, 106Cd, 128,130Te, 144,154Sm, 148Nd, 160Gd, 176Yb, 232Th, 238U deduced nuclear periphery neutron-to-proton density ratios, related features. Radiochemical methods. Shell model calculations.
doi: 10.1103/PhysRevC.57.2962
1998SC43 Phys.Rev. C58, 3195 (1998) R.Schmidt, F.J.Hartmann, T.von Egidy, T.Czosnyka, J.Iwanicki, J.Jastrzebski, M.Kisielinski, P.Lubinski, P.Napiorkowski, L.Pienkowski, A.Trzcinska, J.Kulpa, R.Smolanczuk, S.Wycech, B.Klos, K.Gulda, W.Kurcewicz, E.Widmann Nucleon Density of 172Yb and 176Yb at the Nuclear Periphery Determined with Antiprotonic x Rays NUCLEAR REACTIONS 172,176Yb(p-bar, X), E at rest; measured x-ray spectra; deduced widths and shifts due to strong interaction. 172,176Yb deduced nucleon density at nuclear periphery.
doi: 10.1103/PhysRevC.58.3195
1995JA09 Acta Phys.Pol. B26, 527 (1995) J.Jastrzebski, P.Lubinski, A.Trzcinska Nuclear Structure and Nuclear Excitations from Antiproton-Nucleus Interaction NUCLEAR REACTIONS 63Cu(p-bar, X), (p, X), E=3.9 GeV; 197Au(p, X), E=1, 6 GeV; 197Au(p-bar, X), E=1, 1.2 GeV; compiled, reviewed heavy residues mass, yields, production data, analyses; deduced nuclear surface related features. Other reactions, other aspects discussed, new nuclear periphery study method.
1995VO14 Z.Naturforsch. 50a, 1077 (1995) T.von Egidy, F.J.Hartmann, S.Schmid, W.Schmid, K.Gulda, J.Jastrzebski, W.Kurcewicz, P.Lubinski, L.Pienkowski, A.Trzcinska, D.Hilscher, W.Bohne, F.Goldenbaum, U.Jahnke, D.Polster, H.Rossner, A.S.Iljinov, D.I.Ivanov, M.V.Mebel, V.G.Nedorezov, A.S.Sudov, J.Eades, S.Neumaier Nuclear Physics with Antiprotons NUCLEAR REACTIONS 197Au(p-bar, X), E at rest; 197Au(p-bar, X), E=1.2 GeV; 197Au(p, X), E=1, 6 GeV; compiled, reviewed residuals yields vs mass number. 234U(p-bar, F), E at rest; 234U(p-bar, F), E=fast; measured neutron spectra following fission; deduced absolute fission probabilities.
1994LU13 Phys.Rev.Lett. 73, 3199 (1994) P.Lubinski, J.Jastrzebski, A.Grochulska, A.Stolarz, A.Trzcinska, W.Kurcewicz, F.J.Hartmann, W.Schmid, T.von Egidy, J.Skalski, R.Smolanczuk, S.Wycech, D.Hilscher, D.Polster, H.Rossner Neutron Halo in Heavy Nuclei from Antiproton Absorption NUCLEAR REACTIONS 58Ni, 96Zr, 96Ru, 130Te, 154,144Sm, 176Yb, 232Th, U(p-bar, X), E at 200 MeV/c; measured residuals production yield; deduced neutron halo features.
doi: 10.1103/PhysRevLett.73.3199
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