NSR Query Results
Output year order : Descending NSR database version of May 2, 2024. Search: Author = J.Pinter Found 14 matches. 2010TR03 Phys.Rev.Lett. 104, 129202 (2010) V.Tripathi, S.L.Tabor, P.F.Mantica, Y.Utsuno, P.Bender, J.Cook, C.R.Hoffman, S.Lee, T.Otsuka, J.Pereira, M.Perry, K.Pepper, J.S.Pinter, J.Stoker, A.Volya, D.Weisshaar Reply: "Intruder Configurations in the A=33 Isobars: 33Mg and 33Al" NUCLEAR STRUCTURE 33Mg; analyzed 33Mg β-decay data; deduced 33Mg π.
doi: 10.1103/PhysRevLett.104.129202
2009EA01 Phys.Rev. C 79, 024303 (2009); Publishers note Phys.Rev. C 80, 019907 (2009) M.C.East, A.E.Stuchbery, S.K.Chamoli, A.N.Wilson, H.L.Crawford, J.S.Pinter, T.Kibedi, P.F.Mantica g factor of the first excited state in 56Fe and implications for transient-field calibration in the Fe region NUCLEAR REACTIONS C(56Fe, 56Fe'), (57Fe, 57Fe'), E=2 MeV/nucleon; measured Eγ, Iγ(θ), γγ-, 12C-γ coin, angular correlations, precession angles. 56,57Fe; deduced g factors. NUCLEAR MOMENTS 56Fe, 57Fe; measured g factor of first 2+ state of 56Fe relative to that of the first 5/2- state in 57Fe using transient-field technique in Coulomb excitation.
doi: 10.1103/PhysRevC.79.024303
2009EA02 Phys.Rev. C 79, 024304 (2009); Publishers note Phys.Rev. C 80, 019908 (2009) M.C.East, A.E.Stuchbery, S.K.Chamoli, J.S.Pinter, H.L.Crawford, A.N.Wilson, T.Kibedi, P.F.Mantica Relative g-factor measurements in 54Fe, 56Fe, and 58Fe NUCLEAR REACTIONS C(54Fe, 54Fe'), (56Fe, 56Fe'), (58Fe, 58Fe), E=110 MeV/nucleon; measured Eγ, Iγ(θ), γγ-, 12C-γ coin, precession angles. 54,56,58Fe; deduced g factors. NUCLEAR MOMENTS 54,56,58Fe; measured g factors of first 2+ states of 54Fe and 58Fe relative to that of the first 2+ state in 56Fe using transient-field technique in Coulomb excitation in inverse kinematics. Comparison with shell-model calculations in fp model space.
doi: 10.1103/PhysRevC.79.024304
2008BA53 Phys.Rev.Lett. 101, 252501 (2008) D.Bazin, F.Montes, A.Becerril, G.Lorusso, A.Amthor, T.Baumann, H.Crawford, A.Estrade, A.Gade, T.Ginter, C.J.Guess, M.Hausmann, G.W.Hitt, P.Mantica, M.Matos, R.Meharchand, K.Minamisono, G.Perdikakis, J.Pereira, J.Pinter, M.Portillo, H.Schatz, K.Smith, J.Stoker, A.Stolz, R.G.T.Zegers Production and β Decay of rp-Process Nuclei 96Cd, 98In, and 100Sn NUCLEAR REACTIONS 9Be(112Sn, X)96Cd/98In/100Sn, E=120 MeV/nucleon; measured cross sections. RADIOACTIVITY 96Cd, 98In, 100Sn; measured decay spectra, half-lives.
doi: 10.1103/PhysRevLett.101.252501
2008MA01 Phys.Rev. C 77, 014313 (2008) P.F.Mantica, R.Broda, H.L.Crawford, A.Damaske, B.Fornal, A.A.Hecht, C.Hoffman, M.Horoi, N.Hoteling, R.V.F.Janssens, J.Pereira, J.S.Pinter, J.B.Stoker, S.L.Tabor, T.Sumikama, W.B.Walters, X.Wang, S.Zhu β decay of neutron-rich 53-56Ca RADIOACTIVITY 53,54,55,56Ca(β-) [from 9Be(76Ge, X), E=140 MeV/nucleon; measured Eγ, Iγ, βγ-coin, half-lives. 54Ca; deduced Iβ, logft. 54Sc; levels, J, π, half-lives, B(M1), B(E2), comparison with calculations. NUCLEAR REACTIONS 9Be(76Ge, X)49Cl/50Ar/51Ar/52K/53K/54K/53Ca/54Ca/55Ca/56Ca/55Sc/56Sc/57Sc/57Ti/58Ti/59Ti/60V, E=140 MeV/nucleon; measured reaction yields.
doi: 10.1103/PhysRevC.77.014313
2008MA59 Bull.Am.Phys.Soc. 53, 64 ED.02 (2008) P.F.Mantica, H.L.Crawford, J.Pereira, J.S.Pinter, J.B.Stoker, R.Broda, B.Fornal, R.V.F.Janssens, X.Wang, S.Zhu, N.Hoteling, W.B.Walters, C.R.Hoffman, S.L.Tabor β decay of 51, 52Ar RADIOACTIVITY 51,52Ar(β-) [from Be(76Ge, X), E=130 MeV/nucleon]; measured decay products, Eβ, Iβ; deduced T1/2. NSCL beta counting system.
2008MI07 Phys.Lett. B 662, 389 (2008) K.Minamisono, P.F.Mantica, H.L.Crawford, J.S.Pinter, J.B.Stoker, Y.Utsuno, R.R.Weerasiri Quadrupole moment of 37K RADIOACTIVITY 37K(β+); measured electric quadrupole moment using the β-NQR technique. 35S, 37Ar, 35,37,39K, 39Ca; analyzed electric quadrupole moment using shell model and effective charge dependency.
doi: 10.1016/j.physletb.2008.03.049
2008TR04 Phys.Rev. C 77, 034310 (2008) V.Tripathi, S.L.Tabor, P.Bender, C.R.Hoffman, S.Lee, K.Pepper, M.Perry, P.F.Mantica, J.M.Cook, J.Pereira, J.S.Pinter, J.B.Stoker, D.Weisshaar, Y.Utsuno, T.Otsuka Excited intruder states in 32Mg NUCLEAR REACTIONS 9Be(48Ca, X)30Na/31Na/32Na/33Mg, E=140 MeV/nucleon; measured yields. RADIOACTIVITY 32Na(β-), (β-n) [from 9Be(48Ca, X), E=140 MeV/nucleon]; measured Eγ, Iγ, γγ-coin, half-lives; deduced Iβ, B(GT), logft. 32Mg; deduced levels, Jπ. 26,28,30,34,36Mg, 28,30,32,34,36,38Si; systematics. Comparison with shell-model calculations.
doi: 10.1103/PhysRevC.77.034310
2008TR07 Phys.Rev.Lett. 101, 142504 (2008) V.Tripathi, S.L.Tabor, P.F.Mantica, Y.Utsuno, P.Bender, J.Cook, C.R.Hoffman, S.Lee, T.Otsuka, J.Pereira, M.Perry, K.Pepper, J.S.Pinter, J.Stoker, A.Volya, D.Weisshaar Intruder Configurations in the A=33 Isobars: 33Mg and 33Al RADIOACTIVITY 33Mg(β-); measured Eγ, Iγ. 33Al; deduced levels, J, π, configurations. Compared results to model calculations.
doi: 10.1103/PhysRevLett.101.142504
2007GR23 Phys.Rev. C 76, 054608 (2007) D.E.Groh, J.S.Pinter, P.F.Mantica, T.J.Mertzimekis, A.E.Stuchbery, D.T.Khoa Nuclear spin polarization following intermediate-energy heavy-ion reactions NUCLEAR REACTIONS 197Au(14N, X)12B, E=39.4 MeV/nucleon; 197Au(15N, X)13B, E=68, 109.6 MeV/nucleon; 93Nb(15N, X)13B, E=67.3 MeV/nucleon; 27Al(15N, X)13B, E=68 MeV/nucleon; 9Be(36Ar, X)37K, E=150.0 MeV/nucleon; 9Be(36S, X)34Al, E=77.6 MeV/nucleon; 9Be, 184W(58Ni, X)55Ni, E=140 MeV/nucleon; calculated polarization coefficients.
doi: 10.1103/PhysRevC.76.054608
2007HO22 Phys.Rev. C 76, 044324 (2007) N.Hoteling, W.B.Walters, B.E.Tomlin, P.F.Mantica, J.Pereira, A.Becerril, T.Fleckenstein, A.A.Hecht, G.Lorusso, M.Quinn, J.S.Pinter, J.B.Stoker Onset of isomers in 125, 126, 127, 128Cd and weakened neutron-neutron interaction strength NUCLEAR REACTIONS Be(136Xe, X), E=120 MeV/nucleon; measured Eγ, Iγ. 125Cd, 126Cd, 127Cd, 128Cd deduced levels, J, π, isomers, half-lives, band structure; 100,115,117,119,121,122,123,124Cd; level systematics.
doi: 10.1103/PhysRevC.76.044324
2007MI48 Eur.Phys.J. Special Topics 150, 145 (2007) K.Minamisono, P.F.Mantica, T.J.Mertzimekis, A.D.Davies, M.Hass, J.Pereira, J.S.Pinter, W.F.Rogers, J.B.Stoker, B.E.Tomlin, R.R.Weerasiri Nuclear magnetic moment of 57Cu ground state RADIOACTIVITY 57Cu(β+); measured ground state magnetic moment using the β-NMR technique. Deduced spin expectation value.
doi: 10.1140/epjst/e2007-00289-1
2007TR08 Phys.Rev. C 76, 021301 (2007), Erratum Phys.Rev. C 76, 049902 (2007) V.Tripathi, S.L.Tabor, P.F.Mantica, Y.Utsuno, P.Bender, J.Cook, C.R.Hoffman, S.Lee, T.Otsuka, J.Pereira, M.Perry, K.Pepper, J.S.Pinter, J.Stoker, A.Volya, D.Weisshaar Competition between normal and intruder states inside the "island of inversion" RADIOACTIVITY 30Ne(β-) [from Be(48Ca, X), E=140 MeV/nucleon]; measured Eγ, Iγ, βγ-coinc, T1/2. 30Na deduced levels, J, π. Compared results to model calculations.
doi: 10.1103/PhysRevC.76.021301
2006MI07 Phys.Rev.Lett. 96, 102501 (2006) K.Minamisono, P.F.Mantica, T.J.Mertzimekis, A.D.Davies, M.Hass, J.Pereira, J.S.Pinter, W.F.Rogers, J.B.Stoker, B.E.Tomlin, R.R.Weerasiri Nuclear Magnetic Moment of the 57Cu Ground State RADIOACTIVITY 57Cu(EC), (β+) [from Be(58Ni, X)]; measured β-asymmetry, β-NMR spectrum from polarized source. 57Cu deduced ground-state μ. Comparison with shell-model predictions.
doi: 10.1103/PhysRevLett.96.102501
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