NSR Query Results
Output year order : Descending NSR database version of April 26, 2024. Search: Author = M.Gotz Found 13 matches. 2023CO04 Phys.Rev. C 107, L021301 (2023) D.M.Cox, A.Saamark-Roth, D.Rudolph, L.G.Sarmiento, R.M.Clark, J.L.Egido, P.Golubev, J.Heery, A.Yakushev, S.AAberg, H.M.Albers, M.Albertsson, M.Block, H.Brand, T.Calverley, R.Cantemir, B.G.Carlsson, Ch.E.Dullmann, J.Eberth, C.Fahlander, U.Forsberg, J.M.Gates, F.Giacoppo, M.Gotz, S.Gotz, R.-D.Herzberg, Y.Hrabar, E.Jager, D.Judson, J.Khuyagbaatar, B.Kindler, I.Kojouharov, J.V.Kratz, J.Krier, N.Kurz, L.Lens, J.Ljungberg, B.Lommel, J.Louko, C.-C.Meyer, A.Mistry, C.Mokry, P.Papadakis, E.Parr, J.L.Pore, I.Ragnarsson, J.Runke, M.Schadel, H.Schaffner, B.Schausten, D.A.Shaughnessy, P.Thorle-Pospiech, N.Trautmann, J.Uusitalo Spectroscopy along flerovium decay chains. II. Fine structure in odd-A 289Fl RADIOACTIVITY 289Fl(α) [from 244Pu(48Ca, X), E=6.02 MeV/nucleon]; 285Cn(α) [from 289Fl(α)]; 281Ds(α) [from 285Cn(α)]; 277Hs(SF) [from 281Ds(α)]; measured decay products, Eα, Iα, Eβ, Iβ αβ-coin, αα-coin, (fragment)αα-coin; deduced Q-values, T1/2, branching ratios, hindrance factor. 289Fl, 285Cn, 281Ds; deduced J, π and δ assignments based on the derived decay path. Comparison with structure calculations based on the symmetry-conserving configuration mixing theory. Gas-filled recoil separator TASCA was used to transmit, select, and focus the flerovium ions into an upgraded version of the TASISpec decay station consisting of implantation DSSD, veto DSSD and set of HPGe detectors (GSI).
doi: 10.1103/PhysRevC.107.L021301
2023SA03 Phys.Rev. C 107, 024301 (2023) A.Saamark-Roth, D.M.Cox, D.Rudolph, L.G.Sarmiento, M.Albertsson, B.G.Carlsson, J.L.Egido, P.Golubev, J.Heery, A.Yakushev, S.AAberg, H.M.Albers, M.Block, H.Brand, T.Calverley, R.Cantemir, R.M.Clark, Ch.E.Dullmann, J.Eberth, C.Fahlander, U.Forsberg, J.M.Gates, F.Giacoppo, M.Gotz, S.Gotz, R.-D.Herzberg, Y.Hrabar, E.Jager, D.Judson, J.Khuyagbaatar, B.Kindler, I.Kojouharov, J.V.Kratz, J.Krier, N.Kurz, L.Lens, J.Ljungberg, B.Lommel, J.Louko, C.-C.Meyer, A.Mistry, C.Mokry, P.Papadakis, E.Parr, J.L.Pore, I.Ragnarsson, J.Runke, M.Schadel, H.Schaffner, B.Schausten, D.A.Shaughnessy, P.Thorle-Pospiech, N.Trautmann, J.Uusitalo Spectroscopy along flerovium decay chains. III. Details on experiment, analysis, 282Cn, and spontaneous fission branches RADIOACTIVITY 290,288,286,284Fl(α)(SF) [from 244Pu(48Ca, X), E=6.02 MeV/nucleon]; 282Cn(α)(SF) [286Fl(α)]; 284Cn(α)(SF) [from 288Fl(α)]; 286Cn(α)(SF) [290Fl(α)]; 282Ds(α)(SF) [from 286Cn(α)]; 280Ds(α)(SF) [from 284Cn(α)]; measured decay products, Eα, Iα, Eβ, Iβ αβ-coin, αα-coin, (fragment)αα-coin; deduced Q-values, T1/2, branching ratios, hindrance factor. 282Cn; deduced levels, J, π, T1/2 of excited states, transition rates, monopole transition strengths. Comparison to macroscopic-microscopic finite-range liquid-drop model, self-consistent Hartree-Fock-Bogoliubov calculations and other experimental data. Gas-filled recoil separator TASCA was used to transmit, select, and focus the flerovium ions into an upgraded version of the TASISpec decay station consisting of implantation DSSD, veto DSSD and set of HPGe detectors (GSI).
doi: 10.1103/PhysRevC.107.024301
2021KH03 Phys.Rev. C 103, 064303 (2021) J.Khuyagbaatar, H.Brand, R.A.Cantemir, Ch.E.Dullmann, M.Gotz, S.Gotz, F.P.Hessberger, E.Jager, B.Kindler, J.Krier, N.Kurz, B.Lommel, B.Schausten, A.Yakushev Isomeric states in 256Rf RADIOACTIVITY 256mRf(IT)[from 207,208Pb(50Ti, xn), E=237.5, 242.5 MeV at the Trans-Actinide Separator and Chemistry Apparatus (TASCA) at GSI and implanted in double-sided silicon strip detector (DSSD)]; measured evaporation residues (ER) and fission (ER-FI) and ER-conversion electrons-fission (ER-CE-FI) correlated events, half-lives of the two isomers from correlated decay curves by a triggerless method. 256Rf; deduced two isomeric activities a low-spin and a high-spin, population rates, two-quasiparticle configurations with K-quantum number assignments, third isomer in 256Rf in earlier literature not observed perhaps due to low statistics.
doi: 10.1103/PhysRevC.103.064303
2021SA01 Phys.Rev.Lett. 126, 032503 (2021) A.Samark-Roth, D.M.Cox, D.Rudolph, L.G.Sarmiento, B.G.Carlsson, J.L.Egido, P.Golubev, J.Heery, A.Yakushev, S.Aberg, H.M.Albers, M.Albertsson, M.Block, H.Brand, T.Calverley, R.Cantemir, R.M.Clark, C.E.Dullmann, J.Eberth, C.Fahlander, U.Forsberg, J.M.Gates, F.Giacoppo, M.Gotz, S.Gotz, R.-D.Herzberg, Y.Hrabar, E.Jager, D.Judson, J.Khuyagbaatar, B.Kindler, I.Kojouharov, J.V.Kratz, J.Krier, N.Kurz, L.Lens, J.Ljungberg, B.Lommel, J.Louko, C.-C.Meyer, A.Mistry, C.Mokry, P.Papadakis, E.Parr, J.L.Pore, I.Ragnarsson, J.Runke, M.Schadel, H.Schaffner, B.Schausten, D.A.Shaughnessy, P.Thorle-Pospiech, N.Trautmann, J.Uusitalo Spectroscopy along Flerovium Decay Chains: Discovery of 280Ds and an Excited State in 282Cn RADIOACTIVITY 286,288Fl, 284Cn(α), 282Cn, 280Ds(SF) [from 242,244Pu(48Ca, X)286Fl/288Fl, E=6.021 MeV/nucleon]; measured decay products, Eα, Iα, Eβ, Iβ α-β coin.; deduced Q-values, T1/2, J, π. Comparison with theoretical calculations. The gas-filled separator TASCA at the GSI.
doi: 10.1103/PhysRevLett.126.032503
2020KH08 Phys.Rev.Lett. 125, 142504 (2020) J.Khuyagbaatar, H.M.Albers, M.Block, H.Brand, R.A.Cantemir, A.Di Nitto, C.E.Dullmann, M.Gotz, S.Gotz, F.P.Hessberger, E.Jager, B.Kindler, J.V.Kratz, J.Krier, N.Kurz, B.Lommel, L.Lens, A.Mistry, B.Schausten, J.Uusitalo, and A.Yakushev Search for Electron-Capture Delayed Fission in the New Isotope 244Md RADIOACTIVITY 244,245Md(α), (EC) [from 197Au(50Ti, X), E=239.8, 231.5 MeV]; measured decay products, Eα, Iα; deduced α-particles energies, T1/2. Comparison with available data.
doi: 10.1103/PhysRevLett.125.142504
2017GO06 Nucl.Phys. A961, 1 (2017) M.Gotz, S.Gotz, J.V.Kratz, Ch.E.Dullmann, Ch.Mokry, J.Runke, P.Thorle-Pospiech, N.Wiehl, M.Schadel, J.Ballof, H.Dorrer, J.Grund, D.Huber, E.Jager, O.Keller, J.Krier, J.Khuyagbaatar, L.Lens, B.Lommel, M.Mendel, K.J.Moody, P.Scharrer, B.Schausten, D.Shaughnessy, M.Schmitt, J.Steiner, N.Trautmann, A.Yakushev, V.Yakusheva Radiochemical study of the kinematics of multi-nucleon transfer reactions in 48Ca + 248Cm collisions 10 percent above the Coulomb barrier NUCLEAR REACTIONS 248Cm(48Ca, x), E=262 MeV; measured multinucleon transfer reaction products, Eα, Iα (for identification of the fragments); deduced TKE vs θ, E* vs θ for target-like (trans-target ones, like Fm, Es, Cf, Bk and others) fragments using radiochemical methods.
doi: 10.1016/j.nuclphysa.2017.02.006
2014ST16 Nucl.Data Sheets 119, 422 (2014) M.Stefanik, P.Bem, M.Gotz, K.Katovsky, M.Majerle, J.Novak, E.Simeckova Neutron Spectrum Determination of the p(35 MeV)-Be Source Reaction by the Dosimetry Foils Method NUCLEAR REACTIONS 9Be(p, n), E=35 MeV; measured thick target activation Eγ, Iγ; deduced neutron flux for different target thickness with unfolding using SAND-II code. Ti, Ni, Fe, 27Al, 59Co, 89Y, 93Nb, 115In, 176Lu, Lu, 197Au, 209Bi(n, x), E= 35 MeV; calculated σ; deduced σ, C/E.
doi: 10.1016/j.nds.2014.08.119
2011HO16 J.Korean Phys.Soc. 59, 1374s (2011) M.Honusek, P.Bem, V.Burjan, M.Gotz, V.Kroha, J.Novak, E.Simeckova, U.Fischer, S.P.Simakov Neutron Activation Experiments on Niobium in NPI p-7Li Quasi-monoenergetic Neutron Field NUCLEAR REACTIONS 93Nb(n, 2n), (n, 3n), (n, 4n), (n, α), (n, 3He), (n, 2nα), ≈15-35 MeV[from 7Li(p, n), E=19.8-37.4 MeV]; measured Eγ, Iγ; deduced σ using activation technique. Comparison with data (EXFOR) and EAF-2007.
doi: 10.3938/jkps.59.1374
2011NO16 J.Korean Phys.Soc. 59, 1577s (2011) J.Novak, P.Bem, M.Gotz, M.Honusek, E.Simeckova, M.Stefanik, U.Fischer, S.P.Simakov Spectral Flux of the p-7Li(C) Q-M Neutron Source Measured by Proton Recoil Telescope
doi: 10.3938/jkps.59.1577
2011SI26 J.Korean Phys.Soc. 59, 1801s (2011) E.Simeckova, P.Bem, V.Burjan, M.Gotz, M.Honusek, V.Kroha, J.Novak, U.Fischer, S.P.Simakov, R.A.Forrest The Measurement of Neutron Activation Cross Section of 59Co Below 36 MeV NUCLEAR REACTIONS 59Co(n, p), (n, α).(n, 2nα), (n, 3n), (n, 2n), E=0-20 MeV; measured Eγ, Iγ; deduced σ using activation method. 58Co deduced isomeric and ground-state σ. Compared with data, EAF-2007.
doi: 10.3938/jkps.59.1801
2011SI27 J.Korean Phys.Soc. 59, 1856s (2011) S.P.Simakov, U.Fischer, P.Bem, V.Burjan, M.Gotz, M.Honusek, V.Kroha, J.Novak, E.Simeckova, R.A.Forrest Analysis of the Dosimetry Cross Sections Measurements up to 35 MeV with a 7Li(p, xn) Quasi-Monoenergetic Neutron Source NUCLEAR REACTIONS 7Li, C(n, nx), E=0-40 MeV;197Au(n, 2n), (n, nx), E=0-45 MeV;209Bi(n, 3n), E=15-40 MeV; measured Eγ, Iγ; deduced σ using activation method. Compared with data, EAF2007, ENDF/B-VII, IEAF2001, IRDF.
doi: 10.3938/jkps.59.1856
2001BE42 Nucl.Instrum.Methods Phys.Res. A466, 509 (2001) P.Bem, V.Burjan, F.Cvachovec, M.Gotz, M.Kralik, V.Kroha, E.Lukasova, E.Simeckova, V.Vincour Fast Neutrons from Thick Helium Target Irradiated by 17 MeV Deuterons NUCLEAR REACTIONS He(d, nX), E=17 MeV; measured neutron spectra, thick target yields, angular distributions.
doi: 10.1016/S0168-9002(01)00291-1
1999BE18 Nucl.Instrum.Methods Phys.Res. A425, 522 (1999) P.Bem, V.Burjan, F.Cvachovec, M.Gotz, V.Kroha, E.Yu.Nikolsky, E.Simeckova, J.Vincour Fast Neutrons from Thick Deuterium Target Irradiated by 15.8 MeV Protons and 14.1 MeV Deuterons NUCLEAR REACTIONS 2H(p, n), E=15.6 MeV; 2H(d, n), E=14.1 MeV; measured neutron spectra, thick target yields.
doi: 10.1016/S0168-9002(98)01412-0
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