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NSR database version of April 26, 2024.

Search: Author = N.Sokolowska

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2022CI04      Phys.Rev. C 106, 014317 (2022)

A.A.Ciemny, C.Mazzocchi, W.Dominik, A.Fijalkowska, J.Hooker, C.Hunt, H.Jayatissa, L.Janiak, G.Kaminski, E.Koshchiy, M.Pfutzner, M.Pomorski, B.Roeder, G.V.Rogachev, A.Saastamoinen, S.Sharma, N.Sokolowska, W.Satula, J.Singh

β-delayed charged-particle decay of ^{22, 23}Si

RADIOACTIVITY ^22,23Si(β⁺), (β⁺p), (β⁺2p); ²³Si(β⁺3p), (β⁺α)[^22,23Si activities from Ni(²⁸Si, X), E=45 MeV/nucleon at the Texas A and M University K500 superconducting cyclotron, followed by separation of fragments using momentum achromat recoil separator (MARS)]; measured reaction fragments, particle spectra, E(p), I(p) using optical-readout time-projection chamber (OTPC). ²³Al, ²²Mg, ²¹Na; deduced levels, J, π. ²²Si, ²³Si; deduced T_1/2 of ground states, and absolute branching ratios for the observed decay modes; calculated Gamow-Teller matrix elements using angular-momentum-projected (AMP) method with DFT-NCCI module. ²³Al; calculated levels, J, π using multireference density-functional-rooted (DFT) calculations, and compared with shell-model calculations in literature. Comparison with previous experimental results.

doi: 10.1103/PhysRevC.106.014317
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Data from this article have been entered in the XUNDL database. For more information, click here.

2021KU30      Phys.Rev. C 104, 064610 (2021)

A.Kubiela, H.Suzuki, O.B.Tarasov, M.Pfutzner, D.-S.Ahn, H.Baba, A.Bezbakh, A.A.Ciemny, W.Dominik, N.Fukuda, A.Giska, R.Grzywacz, Y.Ichikawa, Z.Janas, L.Janiak, G.Kaminski, K.Kawata, T.Kubo, M.Madurga, C.Mazzocchi, H.Nishibata, M.Pomorski, Y.Shimizu, N.Sokolowska, D.Suzuki, P.Szymkiewicz, A.Swiercz, M.Tajima, A.Takamine, H.Takeda, Y.Takeuchi, C.R.Thornsberry, H.Ueno, H.Yamazaki, R.Yokoyama, K.Yoshida

Production of the most neutron-deficient Zn isotopes by projectile fragmentation of ⁷⁸Kr

NUCLEAR REACTIONS ⁹Be(⁷⁸Kr, X)⁵⁴Zn/⁵⁵Zn/⁵⁶Zn, E=345 MeV/nucleon; measured reaction products, production σ using BigRIPS separator at the RIBF-RIKEN facility. Comparison of measured σ for Zn isotopes in this work, and for germanium, selenium, and krypton isotopes in other studies with predictions of the EPAX3 parametrization, LISE++ abrasion-ablation model using the HFB22 mass model and the AME2020 mass tables. Relevance to production of nuclei decaying by 2p radioactivity such as ⁵⁴Zn.

doi: 10.1103/PhysRevC.104.064610
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetE2730.

2017JA05      Phys.Rev. C 95, 034315 (2017)

L.Janiak, N.Sokolowska, A.A.Bezbakh, A.A.Ciemny, H.Czyrkowski, R.Dabrowski, W.Dominik, A.S.Fomichev, M.S.Golovkov, A.V.Gorshkov, Z.Janas, G.Kaminski, A.G.Knyazev, S.A.Krupko, M.Kuich, C.Mazzocchi, M.Mentel, M.Pfutzner, P.Plucinski, M.Pomorski, R.S.Slepniev, B.Zalewski

β-delayed proton emission from ²⁶P and ²⁷S

RADIOACTIVITY ²⁶P, ²⁷S(β⁺p), (β⁺2p)[from ⁹Be(³²S, X), E=51.3 MeV/nucleon using ACCULINNA fragment separator at FLNR-Dubna facility]; measured E(p), I(p), (implants)(proton), β⁺p and β⁺2p events using gaseous optical time projection chamber (OTPC) detector, half-lives; deduced branching ratios for β⁺p and β⁺2p decay modes. ²⁷P; deduced levels, J, π. Comparison of decay branching ratios and half-lives with previous experimental values. Discussed γ-to-proton emission probability ratio Γ_γ/Γ_p relevant to ²⁶Si(p, γ)²⁷P reaction rate.

doi: 10.1103/PhysRevC.95.034315
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Data from this article have been entered in the XUNDL database. For more information, click here.