NSR Query Results
Output year order : Descending NSR database version of March 21, 2024. Search: Author = K.Muto Found 68 matches. 2023KI02 Phys.Lett. B 836, 137629 (2023) S.Kim, J.W.Hwang, Y.Satou, N.A.Orr, T.Nakamura, Y.Kondo, J.Gibelin, N.L.Achouri, T.Aumann, H.Baba, F.Delaunay, P.Doornenbal, N.Fukuda, N.Inabe, T.Isobe, D.Kameda, D.Kanno, N.Kobayashi, T.Kobayashi, T.Kubo, S.Leblond, J.Lee, F.M.Marques, R.Minakata, T.Motobayashi, D.Murai, T.Murakami, K.Muto, T.Nakashima, N.Nakatsuka, A.Navin, S.Nishi, S.Ogoshi, H.Otsu, H.Sato, Y.Shimizu, H.Suzuki, K.Takahashi, H.Takeda, S.Takeuchi, R.Tanaka, Y.Togano, A.G.Tuff, M.Vandebrouck, K.Yoneda Unbound states in 17C and p-sd shell-model interactions NUCLEAR REACTIONS C(18C, n)17C, E=245 MeV/nucleon; measured reaction products. 16C; deduced resonance energies and parameters, partial σ, spectroscopic factors, J, π. Comparison with shell-model (YSOX) calculations. The BigRIPS fragment separator at the RIKEN–RIBF laboratory.
doi: 10.1016/j.physletb.2022.137629
2022KI06 Few-Body Systems 63, 21 (2022) S.Kim, J.Hwang, Y.Satou, N.A.Orr, T.Nakamura, Y.Kondo, J.Gibelin, N.L.Achouri, T.Aumann, H.Baba, F.Delaunay, P.Doornenbal, N.Fukuda, N.Inabe, T.Isobe, D.Kameda, D.Kanno, N.Kobayashi, T.Kobayashi, T.Kubo, S.Leblond, J.Lee, F.M.Marques, R.Minakata, T.Motobayashi, D.Murai, T.Murakami, K.Muto, T.Nakashima, N.Nakatsuka, A.Navin, S.Nishi, S.Ogoshi, H.Otsu, H.Sato, Y.Shimizu, H.Suzuki, K.Takahashi, H.Takeda, S.Takeuchi, R.Tanaka, Y.Togano, A.G.Tuff, M.Vandebrouck, K.-i.Yoneda Spectroscopy of 17C Above the Neutron Separation Energy NUCLEAR REACTIONS C(18C, X)17C/16C, E<245 MeV/nucleon; measured reaction products, Eγ, Iγ; deduced σ(E), six resonances, partial σ. SAMURAI spectrometer at RIBF of RIKEN.
doi: 10.1007/s00601-022-01725-5
2020CO07 Phys.Rev.Lett. 124, 212503 (2020) K.J.Cook, T.Nakamura, Y.Kondo, K.Hagino, K.Ogata, A.T.Saito, N.L.Achouri, T.Aumann, H.Baba, F.Delaunay, Q.Deshayes, P.Doornenbal, N.Fukuda, J.Gibelin, J.W.Hwang, N.Inabe, T.Isobe, D.Kameda, D.Kanno, S.Kim, N.Kobayashi, T.Kobayashi, T.Kubo, S.Leblond, J.Lee, F.M.Marques, R.Minakata, T.Motobayashi, K.Muto, T.Murakami, D.Murai, T.Nakashima, N.Nakatsuka, A.Navin, S.Nishi, S.Ogoshi, N.A.Orr, H.Otsu, H.Sato, Y.Satou, Y.Shimizu, H.Suzuki, K.Takahashi, H.Takeda, S.Takeuchi, R.Tanaka, Y.Togano, J.Tsubota, A.G.Tuff, M.Vandebrouck, K.Yoneda Halo Structure of the Neutron-Dripline Nucleus 19B NUCLEAR REACTIONS Pb, C(19B, 2n)17B, E=220 MeV/nucleon; measured reaction products, Eγ, Iγ. 19B; deduced σ(E), exclusive and inclusive neutron removal σ, Coulomb dissociation σ, two-neutron probability densities, B(E1).
doi: 10.1103/PhysRevLett.124.212503
2018LE18 Phys.Rev.Lett. 121, 262502 (2018) S.Leblond, F.M.Marques, J.Gibelin, N.A.Orr, Y.Kondo, T.Nakamura, J.Bonnard, N.Michel, N.L.Achouri, T.Aumann, H.Baba, F.Delaunay, Q.Deshayes, P.Doornenbal, N.Fukuda, J.W.Hwang, N.Inabe, T.Isobe, D.Kameda, D.Kanno, S.Kim, N.Kobayashi, T.Kobayashi, T.Kubo, J.Lee, R.Minakata, T.Motobayashi, D.Murai, T.Murakami, K.Muto, T.Nakashima, N.Nakatsuka, A.Navin, S.Nishi, S.Ogoshi, H.Otsu, H.Sato, Y.Satou, Y.Shimizu, H.Suzuki, K.Takahashi, H.Takeda, S.Takeuchi, R.Tanaka, Y.Togano, A.G.Tuff, M.Vandebrouck, K.Yoneda First Observation of 20B and 21B NUCLEAR REACTIONS 12C(22N, 2p)20B, E=225 MeV/nucleon; 12C(22C, p)21B, E=233 MeV/nucleon; measured reaction products; deduced energy levels, J, π, one- and two-neutron separation energies. Comparison with shell model calculations.
doi: 10.1103/PhysRevLett.121.262502
2017HW02 Phys.Lett. B 769, 503 (2017); Corrigendum Phys.Lett. B 774, 723 (2017) J.W.Hwang, S.Kim, Y.Satou, N.A.Orr, Y.Kondo, T.Nakamura, J.Gibelin, N.L.Achouri, T.Aumann, H.Baba, F.Delaunay, P.Doornenbal, N.Fukuda, N.Inabe, T.Isobe, D.Kameda, D.Kanno, N.Kobayashi, T.Kobayashi, T.Kubo, S.Leblond, J.Lee, F.M.Marques, R.Minakata, T.Motobayashi, D.Murai, T.Murakami, K.Muto, T.Nakashima, N.Nakatsuka, A.Navin, S.Nishi, S.Ogoshi, H.Otsu, H.Sato, Y.Shimizu, H.Suzuki, K.Takahashi, H.Takeda, S.Takeuchi, R.Tanaka, Y.Togano, A.G.Tuff, M.Vandebrouck, K.Yoneda Single-neutron knockout from 20C and the structure of 19C NUCLEAR REACTIONS C(20C, n)19C, E=280 MeV/nucleon; measured reaction products; deduced σ(E), partial σ, resonance widths. Comparison with theoretical calculations using YSOX shell-model interaction.
doi: 10.1016/j.physletb.2017.04.019
2016KO11 Phys.Rev.Lett. 116, 102503 (2016) Y.Kondo, T.Nakamura, R.Tanaka, R.Minakata, S.Ogoshi, N.A.Orr, N.L.Achouri, T.Aumann, H.Baba, F.Delaunay, P.Doornenbal, N.Fukuda, J.Gibelin, J.W.Hwang, N.Inabe, T.Isobe, D.Kameda, D.Kanno, S.Kim, N.Kobayashi, T.Kobayashi, T.Kubo, S.Leblond, J.Lee, F.M.Marques, T.Motobayashi, D.Murai, T.Murakami, K.Muto, T.Nakashima, N.Nakatsuka, A.Navin, S.Nishi, H.Otsu, H.Sato, Y.Satou, Y.Shimizu, H.Suzuki, K.Takahashi, H.Takeda, S.Takeuchi, Y.Togano, A.G.Tuff, M.Vandebrouck, K.Yoneda Nucleus 26O: A Barely Unbound System beyond the Drip Line NUCLEAR REACTIONS Be(27F, p)26O, E=201 MeV/nucleon; C(26F, p)25O, E=201 MeV/nucleon; measured reaction products, En, In; deduced first excited and ground state energies, J, π, resonance widths. Comparison with shell model calculations.
doi: 10.1103/PhysRevLett.116.102503
2016TO10 Phys.Lett. B 761, 412 (2016) Y.Togano, T.Nakamura, Y.Kondo, J.A.Tostevin, A.T.Saito, J.Gibelin, N.A.Orr, N.L.Achouri, T.Aumann, H.Baba, F.Delaunay, P.Doornenbal, N.Fukuda, J.W.Hwang, N.Inabe, T.Isobe, D.Kameda, D.Kanno, S.Kim, N.Kobayashi, T.Kobayashi, T.Kubo, S.Leblond, J.Lee, F.M.Marques, R.Minakata, T.Motobayashi, D.Murai, T.Murakami, K.Muto, T.Nakashima, N.Nakatsuka, A.Navin, S.Nishi, S.Ogoshi, H.Otsu, H.Sato, Y.Satou, Y.Shimizu, H.Suzuki, K.Takahashi, H.Takeda, S.Takeuchi, R.Tanaka, A.G.Tuff, M.Vandebrouck, K.Yoneda Interaction cross section study of the two-neutron halo nucleus 22C NUCLEAR REACTIONS C(19C, X), E=307 MeV/nucleon; C(20C, X), E=280 MeV/nucleon; C(22C, X), E=235 MeV/nucleon; measured reaction products, Eγ, Iγ. 19,20,22C; deduced σ, rms matter radii. A four-body Glauber reaction model.
doi: 10.1016/j.physletb.2016.08.062
2016UM03 Nucl.Phys. A955, 194 (2016) Roles of NN-interaction components in shell-structure evolution NUCLEAR STRUCTURE 16O, 20Ne, 24Mg, 28Si, 32S, 36Ar, 40Ca; calculated sp energy, spin-orbit energy splitting using shell model with and without tensor, spin-orbit and ALS interactions with multipole expansion.
doi: 10.1016/j.nuclphysa.2016.06.011
2014FU02 Phys.Rev.Lett. 112, 112502 (2014) Y.Fujita, H.Fujita, T.Adachi, C.L.Bai, A.Algora, G.P.A.Berg, P.von Brentano, G.Colo, M.Csatlos, J.M.Deaven, E.Estevez Aguado, C.Fransen, D.De Frenne, K.Fujita, E.Ganioglu, C.J.Guess, J.Gulyas, K.Hatanaka, K.Hirota, M.Honma, D.Ishikawa, E.Jacobs, A.Krasznahorkay, H.Matsubara, K.Matsuyanagi, R.Meharchand, F.Molina, K.Muto, K.Nakanishi, A.Negret, H.Okamura, H.J.Ong, T.Otsuka, N.Pietralla, G.Perdikakis, L.Popescu, B.Rubio, H.Sagawa, P.Sarriguren, C.Scholl, Y.Shimbara, Y.Shimizu, G.Susoy, T.Suzuki, Y.Tameshige, A.Tamii, J.H.Thies, M.Uchida, T.Wakasa, M.Yosoi, R.G.T.Zegers, K.O.Zell, J.Zenihiro Observation of Low- and High-Energy Gamow-Teller Phonon Excitations in Nuclei NUCLEAR REACTIONS 42Ca, 46Ti, 50Cr, 54Fe(3He, t), E=140 MeV/nucleon; measured reaction products, Eγ, Iγ; deduced cumulative-sum strengths of the experimental B(GT) values in the final nuclei, two kinds of GT phonon states. GXPF1J, quasi particle random phase approximation (QRPA) framework based on a self-consistent Hartree-Fock mean field with Skyrme interaction calculations, comparison with available data.
doi: 10.1103/PhysRevLett.112.112502
2013ST17 Phys.Rev. C 88, 025503 (2013) D.Stefanik, F.Simkovic, K.Muto, A.Faessler Two-neutrino double-β decay Fermi transition and two-nucleon interaction
doi: 10.1103/PhysRevC.88.025503
2012SA23 Phys.Rev. C 85, 061301 (2012) M.Sasano, H.Sakai, K.Yako, T.Wakasa, M.Dozono, V.Rodin, A.Faessler, K.Fujita, M.B.Greenfield, K.Hatanaka, K.Itoh, T.Kawabata, H.Kuboki, Y.Maeda, K.Miki, K.Muto, S.Noji, H.Okamura, Y.Sakemi, K.Sekiguchi, Y.Shimizu, Y.Sasamoto, Y.Tameshige, A.Tamii, T.Uesaka Gamow-Teller transition strengths in the intermediate nucleus of the 116Cd double-β decay by the 116Cd(p, n)116In and 116Sn(n, p)116In reactions at 300 MeV NUCLEAR REACTIONS 116Cd(p, n), E=295 MeV; 116Sn(n, p), E=293 MeV; measured E(n), I(n) using n-TOF method, E(p), I(p), double-differential σ, σ(θ); deduced B(GT) strengths for transitions to 1+ states in 116In in β- and β+ channels. Comparison with QRPA predictions including IVSM component. Relevance to nuclear matrix element of the 116Cd ββ decay.
doi: 10.1103/PhysRevC.85.061301
2011DV01 Phys.Rev. C 83, 045502 (2011) R.Dvornicky, K.Muto, F.Simkovic, A.Faessler Absolute mass of neutrinos and the first unique forbidden β decay of 187Re RADIOACTIVITY 187Re(β-); calculated end points of the Kurie plot of the electron spectrum from first-forbidden unique β decay of 187Re for various values of the effective neutrino mass. Relevance to planned MARE-I and MARE-II experiments.
doi: 10.1103/PhysRevC.83.045502
2010MU01 Prog.Part.Nucl.Phys. 64, 228 (2010) K.Muto, R.Dvornicky, F.Simkovic Nuclear structure aspects of single and double beta decays for neutrino mass NUCLEAR STRUCTURE 187Re; calculated log ft.
doi: 10.1016/j.ppnp.2009.12.016
2009UM05 Nucl.Phys. A829, 13 (2009) Shell-model calculation of E2 effective charges: Application to carbon isotopes NUCLEAR STRUCTURE 11,12,13,14,15,16,17,18,19,20,21,22C; calculated levels, J, π, single particle energies, B(E2), effective charge, quadrupole matrix elements using a shell model. Comparison with data.
doi: 10.1016/j.nuclphysa.2009.08.004
2009YA07 Phys.Rev.Lett. 103, 012503 (2009) K.Yako, M.Sasano, K.Miki, H.Sakai, M.Dozono, D.Frekers, M.B.Greenfield, K.Hatanaka, E.Ihara, M.Kato, T.Kawabata, H.Kuboki, Y.Maeda, H.Matsubara, K.Muto, S.Noji, H.Okamura, T.H.Okabe, S.Sakaguchi, Y.Sakemi, Y.Sasamoto, K.Sekiguchi, Y.Shimizu, K.Suda, Y.Tameshige, A.Tamii, T.Uesaka, T.Wakasa, H.Zheng Gamow-Teller Strength Distributions in 48Sc by the 48Ca(p, n) and 48Ti(n, p) Reactions and Two-Neutrino Double-β Decay Nuclear Matrix Elements NUCLEAR REACTIONS 48Ca(p, n), 48Ti(n, p), E=300 MeV; measured Ep, Ip, En, In; deduced σ(E, θ), Gamow-Teller strengths. Comparison with GXPF1A shell model.
doi: 10.1103/PhysRevLett.103.012503
2008OH05 Phys.Rev. C 77, 051303 (2008) T.Ohsaki, M.Igashira, Y.Nagai, M.Segawa, K.Muto Role of multiparticle-multihole states of 18, 19O in 18O(n, γ)19O reactions at keV energy NUCLEAR REACTIONS 18O(n, γ), E=10-80 keV; measured Eγ, Iγ, σγ. 19O; deduced levels, J, π. Comparison with theory. 13C, 17O, 18O; systematics.
doi: 10.1103/PhysRevC.77.051303
2008UM01 Phys.Rev. C 77, 034318 (2008) A.Umeya, S.Nagai, G.Kaneko, K.Muto Monopole and quadrupole interactions in binding energies of sd-shell nuclei NUCLEAR STRUCTURE 20,28Ne, 24,28Mg, 24,26,28,30,32,34Si, 28F, 28Na, 28Al, 32S, 36Ar, 40Ca; calculated binding energies, investigated multipole and spin-tensor decompositions, monopole and quadrupole interactions.
doi: 10.1103/PhysRevC.77.034318
2008UM02 Phys.Rev. C 77, 044301 (2008) A.Umeya, G.Kaneko, T.Haneda, K.Muto Enhancement of neutron quadrupole motion beyond N = 8 NUCLEAR STRUCTURE 10,12,14,16Be, 12,14,16,18C; calculated configurations, B(E2), quadrupole matrix elements, single particle energies; deduced levels. Comparison with experimental data. Shell model.
doi: 10.1103/PhysRevC.77.044301
2007NA26 Phys.Rev. C 76, 051301 (2007) Y.Nagai, M.Segawa, T.Ohsaki, H.Matsue, K.Muto Role of multiparticle-multihole states in 18, 19O in thermal neutron capture of 18O NUCLEAR REACTIONS 18O(n, γ), E=thermal; measured Eγ, Iγ, γγ-coin, cross sections; deduced levels, J, π, configurations, B(E1). 13C, 17,19O; systematics.
doi: 10.1103/PhysRevC.76.051301
2007SA47 Nucl.Phys. A788, 76c (2007) M.Sasano, H.Sakai, K.Yako, H.Kuboki, K.Miki, S.Noji, T.Wakasa, M.Dozono, K.Sekiguchi, T.Uesaka, T.Kawabata, Y.Maeda, S.Sakaguchi, Y.Sasamoto, K.Suda, K.Itoh, K.Hatanaka, H.Okamura, A.Tamii, K.Muto, D.Frekers, M.B.Greenfield Determination of the Gamow-Teller transition strength to 116In(g.s.) by the 116Cd(p, n) reaction at 300 MeV for the study of the nuclear matrix element of the two-neutrino double beta decay NUCLEAR REACTIONS 116Cd(p, n), E=300 MeV; measured excitation energy spectrum. 116In deduced Gamow-Teller strength distribution, nuclear matrix elements. Comparison with other data.
doi: 10.1016/j.nuclphysa.2007.01.051
2006UM05 Phys.Rev. C 74, 034330 (2006) Single-particle energies in neutron-rich nuclei by shell model sum rule
doi: 10.1103/PhysRevC.74.034330
2004UM01 Phys.Rev. C 69, 024306 (2004) Triplet-even channel attraction for shell gaps NUCLEAR STRUCTURE 10He, 11Li, 12Be, 13B, 14C, 15N, 16O; calculated single-particle energies, shell gap features, contribution from triplet-even component of NN interaction.
doi: 10.1103/PhysRevC.69.024306
2003UM02 Nucl.Phys. A722, 558c (2003) Shell model study on E2 effective charges in light neutron-rich nuclei NUCLEAR STRUCTURE 6,7,8,9Li, 9Be, 10,11,12,13,14,15,17B, 11C, 14,18N, 17O; calculated quadrupole moments, isocalar and isovector effective charge.
doi: 10.1016/S0375-9474(03)01427-1
1996HO23 Phys.Rev. C54, 2972 (1996) H.Homma, E.Bender, M.Hirsch, K.Muto, H.V.Klapdor-Kleingrothaus, T.Oda Systematic Study of Nuclear Beta Decay NUCLEAR STRUCTURE Z=15-61; N=21-83; analyzed β-decay T1/2, other systematics. Quasiparaticle RPA, schematic Gamow-Teller residual interaction.
doi: 10.1103/PhysRevC.54.2972
1996MU17 Phys.Lett. 391B, 243 (1996) Extended Quasiparticle RPA and Double-Beta-Decay Nuclear Matrix Elements RADIOACTIVITY 76Ge(2β); calculated 0ν-, 2ν-accompanied 2β-decay matrix elements; deduced neutrino mass for 0ν-accompanied 2β-decay. Quasiparticle, renormalized quasiparticle, extented quasiparticle RPA approaches. NUCLEAR STRUCTURE 76Se; calculated quasiparticles number. Quasiparticle, renormalized quasiparticle, extended quasiparticle RPA approaches.
doi: 10.1016/S0370-2693(96)01481-5
1996NA05 Phys.Rev.Lett. 76, 881 (1996) S.Nakamura, K.Muto, M.Oka, S.Takeuchi, T.Oda Up-Down Quark Mass Difference Effect in Nuclear Many-Body Systems NUCLEAR STRUCTURE 19O, 20F, 24m,24Al, 27,28Mg, 24Na; calculated isospin matrix elements. Quark cluster model.
doi: 10.1103/PhysRevLett.76.881
1996NA17 Nucl.Phys. A607, 235 (1996) Realistic Shell-Model Calculations of the 2νββ Nuclear Matrix Elements and the Role of the Shell Structure in Intermediate States RADIOACTIVITY 36Ar, 54Fe(2EC); 58Ni(2EC), (β+EC); calculated 2ν-accompanied 2β-decay T1/2. Realistic shell model.
doi: 10.1016/S0375-9474(96)00227-8
1995HI13 Z.Phys. A352, 33 (1995) M.Hirsch, O.Kadowaki, H.V.Klapdor-Kleingrothaus, K.Muto, T.Oda Extended Operator Expansion Method for Neutrinoless Double Beta Decay RADIOACTIVITY 76Ge(2β); calculated 0ν-accompanied 2β-decay associated Gamow-Teller, Fermi matrix elements vs parameter g(pp). Extended operator expansion method.
doi: 10.1007/BF01292759
1994HI03 Z.Phys. A347, 151 (1994) M.Hirsch, K.Muto, T.Oda, H.V.Klapdor-Kleingrothaus Nuclear Structure Calculation of β+β+, β+/EC and EC/EC Decay Matrix Elements RADIOACTIVITY 58Ni, 78Kr, 96Ru, 106Cd, 124Xe, 130Ba, 136Ce(2β), (2EC), (β+), (EC); calculated T1/2, nuclear matrix elements in 2ν-, 0ν-accompanied decay modes. Proton-neutron quasiparticle RPA.
doi: 10.1007/BF01292371
1994MU17 Nucl.Phys. A577, 415c (1994) Neutrinoless Double Beta Decay Beyond Closure Approximation RADIOACTIVITY 76Ge, 130Te(2β); calculated 0ν-accompanied Gamow-Teller-Fermi-decay, matrix element difference vs pn-interaction strength.
doi: 10.1016/0375-9474(94)90890-7
1994MU23 Prog.Theor.Phys.(Kyoto) 91, 287 (1994) Charge-Independence-Breaking Interactions in sd-Shell Nuclei NUCLEAR STRUCTURE A=18-38; analyzed isospin multiplet mass differences; deduced charge independence breaking coefficient of isospin multiplet mass equation.
doi: 10.1143/ptp/91.2.287
1994NA11 Nucl.Phys. A575, 1 (1994) Isospin-Forbidden Beta Decays in 1s0d-Shell Nuclei NUCLEAR STRUCTURE A=18-39; calculated isospin symmetry breaking interactions matrix elements, mass shifts, Q(β+), Q(β-), isobaric analog states, β+-decay log ft.
doi: 10.1016/0375-9474(94)90135-X
1994OD01 At.Data Nucl.Data Tables 56, 231 (1994) T.Oda, M.Hino, K.Muto, M.Takahara, K.Sato Rate Tables for the Weak Processes of sd-Shell Nuclei in Stellar Matter NUCLEAR STRUCTURE A=1-39; calculated weak interaction rates; deduced weak interaction rates in stellar matter.
doi: 10.1006/adnd.1994.1007
1994SC40 Z.Phys. A350, 215 (1994) W.-D.Schmidt-Ott, K.Asahi, Y.Fujita, H.Geissel, K.-D.Gross, T.Hild, H.Irnich, M.Ishihara, K.Krumbholz, V.Kunze, A.Magel, F.Meissner, K.Muto, F.Nickel, H.Okuno, M.Pfutzner, C.Scheidenberger, K.Suzuki, M.Weber, C.Wennemann Spin Alignment of 43Sc Produced in the Fragmentation of 500 MeV/u 46Ti NUCLEAR REACTIONS 9Be(46Ti, X), E=500 MeV/nucleon; measured γ(θ, H, t). 43mSc deduced spin alignment. Projectile fragmentation.
doi: 10.1007/BF01289585
1993HI08 At.Data Nucl.Data Tables 53, 165 (1993) M.Hirsch, A.Staudt, K.Muto, H.V.Klapdor-Kleingrothaus Microscopic Predictions of β+/EC-Decay Half-Lives RADIOACTIVITY Z=10-108; calculated β+-decay, EC-decay T1/2. Proton-neutron quasiparticle RPA.
doi: 10.1006/adnd.1993.1004
1993MU08 Phys.Rev. C48, 402 (1993) Coulomb Effect in Operator Expansion Method for Two-Neutrino Double Beta Decay RADIOACTIVITY 76Ge, 130Te(2β); calculated 2ν-accompanied 2β-decay matrix element. Operator expansion method, Coulomb effect.
doi: 10.1103/PhysRevC.48.402
1993NA08 Phys.Lett. 311B, 15 (1993) Charge-Symmetry-Breaking Nucleon-Nucleon Interaction in the 1s0d-Shell Nuclei NUCLEAR STRUCTURE 19O, 20F, 24m,24Al, 24Na, 27,28Mg; calculated isospin mixing matrix element. Charge symmetry breaking nucleon-nucleon interaction.
doi: 10.1016/0370-2693(93)90525-M
1992KI23 Phys.Rev. C46, 2364 (1992) H.Kitazawa, M.Igashira, M.Shimizu, K.Muto, T.Oda, Y.Achiha, Y.-H.Lee, N.Mukai Electric and Magnetic Dipole Transitions from Broad s-Wave Neutron Resonance in Even-Even sd-Shell Nuclei NUCLEAR REACTIONS 24Mg(n, γ), E=658 keV; 28Si(n, γ), E=180 keV; 32S(n, γ), E=103 keV; measured Eγ, Iγ, σ(E, Eγ) at 125°. 25Mg, 29Si, 33S levels deduced transition γ-multipolarity, partial radiative widths. Valence capture shell models, configuration mixing.
doi: 10.1103/PhysRevC.46.2364
1992MU04 Phys.Lett. 277B, 13 (1992) Sum Rules for Double Gamow-Teller Excitation RADIOACTIVITY 22,24,26,28,30Ne; calculated double Gamow-Teller strength distribution. Model-independent term in sum rules.
doi: 10.1016/0370-2693(92)90948-4
1992NA16 Phys.Lett. 297B, 14 (1992) Effective Isospin Non-Conserving Interaction and Isospin-Forbidden Beta Decays in the 1s0d Shell NUCLEAR STRUCTURE 19O, 20F, 24Na, 24,24mAl, 27,28Mg; calculated isospin mixing matrix element. A=18-40; calculated charge rms radii. Effective isospin nonconserving NN-interaction.
doi: 10.1016/0370-2693(92)91061-D
1991HI18 Nucl.Phys. A535, 62 (1991) M.Hirsch, A.Staudt, K.Muto, H.V.Klapdor-Kleingrothaus Microscopic Calculation of β+/EC Decay Half-Lives with Atomic Numbers Z = 10-30 RADIOACTIVITY 52Ca; calculated Gamow-Teller T1/2. 38Ca; calculated Gamow-Teller T1/2, β-strength function. 30S, 27,28P, 31Ar; calculated (β+/EC) T1/2 relative to experiment. Quasiparticle RPA.
doi: 10.1016/0375-9474(91)90515-8
1991MU02 Phys.Rev. C43, 1487 (1991) β+ Decays of Very Proton-Rich sd-Shell Nuclei NUCLEAR STRUCTURE A=18-36; calculated allowed β+-decay T1/2; deduced (β+2p)-decay candidates. Shell model.
doi: 10.1103/PhysRevC.43.1487
1991MU10 Z.Phys. A339, 435 (1991) K.Muto, E.Bender, H.V.Klapdor-Kleingrothaus A Comparative Study of Double Beta Decay by Shell MOdel and Quasiparticle RPA RADIOACTIVITY 48Ca, 76Ge(2β); calculated 2β-decay matrix elements. Shell, quasiparticle RPA models.
doi: 10.1007/BF01288427
1991ST08 Phys.Lett. 268B, 312 (1991) A.Staudt, K.Muto, H.V.Klapdor-Kleingrothaus Nuclear Matrix Elements for Double Positron Emission RADIOACTIVITY 78Kr, 96Ru, 106Cd, 124Xe, 130Ba, 136Ce, 148Gd(2β); calculated 2ν-, 0ν- accompanied two-β+ decay T1/2. Proton-neutron quasiparticle RPA.
doi: 10.1016/0370-2693(91)91582-G
1990FU07 Phys.Lett. 247B, 219 (1990) Y.Fujita, T.Yanagihara, M.Fujiwara, I.Katayama, K.Hosono, S.Morinobu, T.Yamazaki, S.I.Hayakawa, K.Katori, K.Muto, H.Ikegami New High-Spin Stretched States in 208Pb Observed by the (p, p') Reaction NUCLEAR REACTIONS 208Pb(p, p'), E=80 MeV; measured σ(Ep'), σ(θ). 208Pb deduced levels, J, π, configuration. Shell model.
doi: 10.1016/0370-2693(90)90885-A
1990ST08 At.Data Nucl.Data Tables 44, 79 (1990) A.Staudt, E.Bender, K.Muto, H.V.Klapdor-Kleingrothaus Second-Generation Microscopic Predictions of Beta-Decay Half-Lives of Neutron-Rich Nuclei RADIOACTIVITY Z=6-108; calculated β-decay T1/2. Quasiparticle RPA.
doi: 10.1016/0092-640X(90)90020-K
1990ST21 Phys.Rev.Lett. 65, 1543 (1990) A.Staudt, M.Hirsch, K.Muto, H.V.Klapdor-Kleingrothaus Calculation of β-Delayed Fission of 180Tl and Application of the Quasiparticle Random-Phase Approximation to the Prediction of β+-Decay Half-Lives of Neutron-Deficient Isotopes RADIOACTIVITY 180Tl(β-); calculated β strength distribution, β-delayed fission probability; deduced fission barrier height. A=39-52; A=64-73; A=98-105; calculated (β+)/(EC) T1/2. Quasiparticle RPA.
doi: 10.1103/PhysRevLett.65.1543
1990ST23 Europhys.Lett. 13, 31 (1990) A.Staudt, K.Muto, H.V.Klapdor-Kleingrothaus Calculation of 2ν and 0ν Double-Beta Decay Rates RADIOACTIVITY A=70-244; calculated 0ν, 2ν double β-decay rates, T1/2. Quasiparticle RPA.
doi: 10.1209/0295-5075/13/1/006
1989MU14 Z.Phys. A334, 187 (1989) Nuclear Structure Effects on the Neutrinoless Double Beta Decay RADIOACTIVITY 76Se, 82Se, 100Mo, 128,130Te, 136Xe, 150Nd(2β); calculated zero-neutrino accompanied ββ-decay matrix elements. 128Te(2β); analyzed different mode decay T1/2; deduced effective ν mass. Quasiparticle RPA.
1989ST14 Z.Phys. A334, 47 (1989) A.Staudt, E.Bender, K.Muto, H.V.Klapdor Microscopic Calculations of Beta Decay Far from Stability RADIOACTIVITY 128,129Cd, 157,158Pm; A=67-184; calculated β-decay T1/2. Proton-neutron quasiparticle RPA, Gamow-Teller residual interaction.
1989TA26 Nucl.Phys. A504, 167 (1989) M.Takahara, M.Hino, T.Oda, K.Muto, A.A.Wolters, P.W.M.Glaudemans, K.Sato Microscopic Calculation of the Rates of Electron Captures which Induce the Collapse of O + Ne + Mg Cores NUCLEAR STRUCTURE 20Ne, 20F, 24Mg, 24Na; calculated Gamow-Teller transition log ft, electron capture rates; deduced O+Ne+Mg core evolution consequences. Shell model.
doi: 10.1016/0375-9474(89)90288-1
1988BE23 Phys.Lett. 208B, 53 (1988) Calculation of β--Decay Half-Lives with the Proton-Neutron Quasiparticle RPA RADIOACTIVITY 58,59Cr, 61,62,63Mn, 63,64Fe, 65,66,67Co, 67,69Ni; calculated β-decay T1/2. Quasiparticle RPA.
doi: 10.1016/0370-2693(88)91202-6
1988HI05 Phys.Rev. C37, 1328 (1988) Total Gamow-Teller Strength and Effect of Configuration Mixing and Proton-Neutron Correlation in the Even-Even sd-Shell Nuclei NUCLEAR STRUCTURE 20,22,24Ne, 24,26,28Mg, 28,30,32Si, 32,34,36S, 36,38Ar; calculated lowest configuration Gamow-Teller strength.
doi: 10.1103/PhysRevC.37.1328
1988MU03 Phys.Lett. 201B, 420 (1988) Calculation of 2ν Double Beta Decay of 76Ge, 82Se, 128,130Te RADIOACTIVITY 76Ge, 82Se, 128,130Te(2β); calculated two-neutrino mode decay T1/2. Quasiparticle RPA.
doi: 10.1016/0370-2693(88)90594-1
1988MU20 Phys.Lett. 213B, 115 (1988) Reduction of Stretched-Magnetic-Transition Strengths by Core Polarization NUCLEAR STRUCTURE 16O; calculated stretched magnetic transition strengths.
doi: 10.1016/0370-2693(88)91009-X
1987HI08 J.Phys.(London) G13, 1119 (1987) Systematics of the Total Strength and the Contribution of Orbital Current for the M1 Excitations in the Even-Even sd-Shell Nuclei NUCLEAR STRUCTURE 20,22Ne, 24,26Mg, 28,30Si, 32,34S, 36,38Ar; calculated total M1, Gamow-Teller transition strengths; deduced total M1 strength systematics. Shell model.
doi: 10.1088/0305-4616/13/9/013
1987OD01 Phys.Lett. 190B, 14 (1987) The Orbital Current for the 0+(gr) → 1+ M1 Excitations in the Even-Even f7/2 Shell Nuclei NUCLEAR STRUCTURE 44,46,48Ti, 48,50Cr, 52Fe; calculated M1 transition strengths. Free, effective g factors, full configuration space.
doi: 10.1016/0370-2693(87)90832-X
1986MU03 Nucl.Phys. A451, 481 (1986) The ΔT(z) = +1 Gamow-Teller Excitation of N = 28 Isotopes NUCLEAR STRUCTURE 50Sc, 52V, 54Mn; calculated Gamow-Teller transition strength distribution, B(M1). 50Ti, 52Cr, 54Fe; calculated B(M1). Shell model, (p, p'), (e, e') data input.
doi: 10.1016/0375-9474(86)90072-2
1986OH03 Nucl.Phys. A456, 61 (1986) H.Ohnuma, B.A.Brown, D.Dehnhard, K.Furukawa, T.Hasegawa, S.Hayakawa, N.Hoshino, K.Ieki, M.Kabasawa, K.Maeda, K.Miura, K.Muto, T.Nakagawa, K.Nisimura, H.Orihara, T.Suehiro, T.Tohei, M.Yasue A Comparative Study of the 13C(p, p')13C and 13C(p, n)13N Reactions at E(p) = 35 MeV NUCLEAR REACTIONS 13C(polarized p, n), (polarized p, p'), E=35 MeV; measured σ(θ), A(θ). 13C level deduced transition isoscalar component. Enriched target. DWBA analysis.
doi: 10.1016/0375-9474(86)90366-0
1985MU06 Nucl.Phys. A440, 254 (1985) Shell-Model Study on Magnetic Dipole Excitation of N = 28 Isotopes NUCLEAR REACTIONS 51V(p, p'), E=200 MeV; 51V(e, e'), E=38, 49, 57 MeV; calculated σ(Ep'), σ(E(e')). NUCLEAR STRUCTURE 48Ca, 50Ti, 52Cr, 54Fe, 51V; calculated B(M1) strength distribution, g.
doi: 10.1016/0375-9474(85)90340-9
1985MU15 Phys.Lett. 162B, 233 (1985) Non-Proportional Cross Sections of 50Ti(p, p') and 49Ti(d, p) Reactions for Magnetic Dipole States of 50Ti NUCLEAR STRUCTURE 50Ti; calculated B(M1), f5/2 neutron pickup strengths, spectroscopic factors. 49Ti; calculated magnetic multipole moments. Shell model.
doi: 10.1016/0370-2693(85)90912-8
1985MU23 Phys.Lett. 165B, 25 (1985) K.Muto, H.Yamazaki, T.Oda, H.Horie Shell-Model Study on Gamow-Teller Excitation of 90Zr NUCLEAR REACTIONS 90Zr(p, n), E=120 MeV; calculated Gamow-Teller transition strength distribution. Shell model.
doi: 10.1016/0370-2693(85)90683-5
1984MU03 Phys.Lett. 135B, 349 (1984) Neutron Core-Excited High-Spin States in N = 50 Nuclei NUCLEAR STRUCTURE 94Rb, 91Nb; calculated high-spin levels. Shell model.
doi: 10.1016/0370-2693(84)90291-0
1984MU09 Phys.Lett. 138B, 9 (1984) Shell-Model Study on M1 Strength Distributions in N = 28 Isotones NUCLEAR STRUCTURE 48Ca, 50Ti, 52Cr, 54Fe; analyzed electron, proton inelastic scattering data; deduced B(M1) vs excitation, reduction factor. Shell model.
doi: 10.1016/0370-2693(84)91861-6
1984TS05 Phys.Lett. 143B, 293 (1984) Double Beta Decay Nuclear Matrix Element of 48Ca RADIOACTIVITY 48Ca(2β); calculated T1/2, nuclear matrix elements, average β-decay energies, lepton conserving mode. Shell model.
doi: 10.1016/0370-2693(84)91468-0
1983MU14 Phys.Lett. 127B, 291 (1983) Monte Carlo Calculation of Gamow-Teller Transition Strength Function NUCLEAR STRUCTURE 208Bi; calculated Gamow-Teller resonances, Γ, transition strength distribution; deduced particle, hole spreading interference effects. Monte Carlo calculation.
doi: 10.1016/0370-2693(83)91002-X
1982MU16 Phys.Lett. 118B, 261 (1982) Shell-Model Study of the Gamow-Teller Giant Resonance in 208Bi NUCLEAR STRUCTURE 208Bi; calculated Gamow-Teller resonance fragmentation, transition strength distribution. Shell model.
doi: 10.1016/0370-2693(82)90180-0
1978MU17 Prog.Theor.Phys. 60, 1350 (1978) A Shell-Model Study of f7/2-Shell Nuclei in the Pure f(n)7/2 Configuration NUCLEAR STRUCTURE 41,42,43Ca, 41,43,44,45,46,47Sc, 45,47,49Ti, 48,49,50,51V, 49,51Cr, 51,52,53Mn, 54Fe, 55Co; calculated energy levels, electromagnetic properties, β-decay. Pure f7/2 shell model, effective interaction.
doi: 10.1143/PTP.60.1350
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