NSR Query Results
Output year order : Descending NSR database version of April 27, 2024. Search: Author = M.T.Mustonen Found 12 matches. 2018MU14 Phys.Rev. C 98, 034317 (2018) M.T.Mustonen, C.N.Gilbreth, Y.Alhassid, G.F.Bertsch Statistical theory of deformation distributions in nuclear spectra NUCLEAR STRUCTURE 148,150,152,154Sm; calculated second, third, and fourth moments of Q20 moment as a function of temperature, intrinsic quadrupole shape contours in the (β, γ) plane, probabilities of spherical, prolate, and oblate shapes as a function of temperature, first derivatives of Landau-like expansion parameters, nuclear state densities, and shape probabilities as a function of excitation energy using auxiliary-field Monte Carlo (AFMC) approach with configuration-interaction (CI) shell model.
doi: 10.1103/PhysRevC.98.034317
2017MI06 Phys.Lett. B 769, 339 (2017) K.Miki, R.G.T.Zegers, Sam M.Austin, D.Bazin, B.A.Brown, A.C.Dombos, R.K.Grzywacz, M.N.Harakeh, E.Kwan, S.N.Liddick, S.Lipschutz, E.Litvinova, M.Madurga, M.T.Mustonen, W.J.Ong, S.V.Paulauskas, G.Perdikakis, J.Pereira, W.A.Peters, C.Robin, M.Scott, A.Spyrou, C.Sullivan, R.Titus Isovector excitations in 100Nb and their decays by neutron emission studied via the 100Mo(t, 3He + n) reaction at 115 MeV/ u NUCLEAR REACTIONS 100Mo(t, 3He), E=115 MeV/nucleon; measured reaction products; deduced σ(θ, E), Gamow-Teller transition strength. Comparison with the single-particle estimate and spherical pn-(R)QRPA and pn-RQTBA calculations.
doi: 10.1016/j.physletb.2017.04.004
2016MU02 Phys.Rev. C 93, 014304 (2016) Global description of β- decay in even-even nuclei with the axially-deformed Skyrme finite-amplitude method RADIOACTIVITY Z=20-110, N=30-110, A=50-372(β-); 104,106Sr, 112,114,116,118Mo, 112Zr, 120,122,124Ru, 126,128Pd, 134Cd, 138Sn(β-); calculated half-lives, Q values, axial deformation β2, percentage of allowed contribution to the total decay rate, one-sigma uncertainty of log(T1/2) from the error model fit for 1387 even-even neutron-rich nuclei. Axially-deformed Skyrme QRPA finite-amplitude method with Skyrme energy density functional for a global description of β--decay rates for even-even nuclei. Comparison with available experimental data.
doi: 10.1103/PhysRevC.93.014304
2014MU09 Phys.Rev. C 90, 024308 (2014) M.T.Mustonen, T.Shafer, Z.Zenginerler, J.Engel Finite-amplitude method for charge-changing transitions in axially deformed nuclei RADIOACTIVITY 128,130Cd, 132Sn, 142,144,146,148,150Ba, 148,150,152Ce, 154,156Nd, 160,162Sm, 166Gd(β-); calculated half-lives, β-decay rates. 128Cd, 146,146Ba, 166Gd, 208Pb; calculated GT strength functions. Finite amplitude method.
doi: 10.1103/PhysRevC.90.024308
2013MU06 Phys.Rev. C 87, 064302 (2013) Large-scale calculations of the double-β decay of 76Ge, 130Te, 136Xe, and 150Nd in the deformed self-consistent Skyrme quasiparticle random-phase approximation RADIOACTIVITY 76Ge, 130Te, 136Xe, 150Nd(2β-); calculated neutrinoless double beta decay transition matrix elements. Large scale calculation using self-consistent axially symmetric Skyrme-HFB-QRPA method together with SkM* and SkM* modified energy-density functional. Comparison of calculated matrices with several previous theoretical calculations using different models.
doi: 10.1103/PhysRevC.87.064302
2010MU18 J.Phys.(London) G37, 064008 (2010) Nuclear and atomic contributions to beta decays with ultra-low Q values RADIOACTIVITY 115In(β-); analyzed available data; deduced the impact of atomic effects on for the decays with low Q values and dramatic consequences for the beta decays with an ultra-low Q value.
doi: 10.1088/0954-3899/37/6/064008
2010SU06 Prog.Part.Nucl.Phys. 64, 235 (2010) Nuclear matrix elements for rare decays
doi: 10.1016/j.ppnp.2009.12.018
2010YD01 Nucl.Phys. A842, 33 (2010) E.Ydrefors, M.T.Mustonen, J.Suhonen MQPM description of the structure and beta decays of the odd A=95, 97 Mo and Tc isotopes NUCLEAR STRUCTURE 95,97Mo, 95,97Tc; calculated levels, J, π using microscopic quasiparticle-phonon model. Comparison with data and previous calculations. RADIOACTIVITY 95,97Tc(β+), (EC); calculated log ft, nuclear matrix elements using microscopic quasiparticle-phonon model. Comparison with data.
doi: 10.1016/j.nuclphysa.2010.04.005
2009WI10 Phys.Rev.Lett. 103, 122501 (2009) J.S.E.Wieslander, J.Suhonen, T.Eronen, M.Hult, V.-V.Elomaa, A.Jokinen, G.Marissens, M.Misiaszek, M.T.Mustonen, S.Rahaman, C.Weber, J.Aysto Smallest Known Q Value of Any Nuclear Decay: The Rare β- Decay of 115In(9/2+) → 115Sn(3/2+) ATOMIC MASSES 115In, 115Sn; measured TOF ion-cyclotron resonance using Penning Trap mass spectrometer, Eγ, Iγ; deduced 115In-115Sn Q-value, T1/2.
doi: 10.1103/PhysRevLett.103.122501
2007HE08 J.Phys.(London) G34, 837 (2007) H.Heiskanen, M.T.Mustonen, J.Suhonen Theoretical half-life for beta decay of 96Zr RADIOACTIVITY 96Zr(β-); calculated decay matrix elements, T1/2 for decay to excited states. Proton-neutron quasiparticle RPA. NUCLEAR STRUCTURE 96Nb; calculated levels, J, π. Proton-neutron quasiparticle RPA.
doi: 10.1088/0954-3899/34/5/005
2007MU16 Phys.Lett. B 657, 38 (2007) Microscopic quasiparticle-phonon description of beta decays of 113Cd and 115In using proton-neutron phonons RADIOACTIVITY 113Cd, 115In(β-); calculated T1/2, log ft, levels, J, π, energy spectra using an updated microscopic quasiparticle-phonon model. Comparison with data.
doi: 10.1016/j.physletb.2007.09.037
2006MU10 Phys.Rev. C 73, 054301 (2006); Erratum Phys.Rev. C 76, 019901 (2007) M.T.Mustonen, M.Aunola, J.Suhonen Theoretical description of the fourth-forbidden non-unique β decays of 113Cd and 115In RADIOACTIVITY 113Cd, 115In(β-); calculated T1/2 and log ft for fourth-forbidden non-unique decay. Microscopic quasiparticle-phonon model, comparison with data. NUCLEAR STRUCTURE 113Cd, 113,115In, 115Sn; calculated levels, J, π. Microscopic quasiparticle-phonon model, comparison with data.
doi: 10.1103/PhysRevC.73.054301
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