NSR Query Results


Output year order : Descending
Format : Normal

NSR database version of May 24, 2024.

Search: Author = E.Teruya

Found 15 matches.

Back to query form



2020HI12      J.Phys.(London) G47, 035102 (2020)

K.Higashiyama, K.Yanase, N.Yoshinaga, A.Umeya, A.Uehara, E.Teruya

Nuclear matrix elements of neutrinoless double beta decay for masses 130 and 136 in the shell model

RADIOACTIVITY 130Te, 136Xe(2β-); calculated nuclear matrix elements of neutrinoless double beta decay using the nuclear shell model.

doi: 10.1088/1361-6471/ab5400
Citations: PlumX Metrics


2019KA36      Phys.Rev. C 100, 024323 (2019)

L.Kaya, A.Vogt, P.Reiter, M.Siciliano, N.Shimizu, Y.Utsuno, H.-K.Wang, A.Gargano, L.Coraggio, N.Itaco, K.Arnswald, D.Bazzacco, B.Birkenbach, A.Blazhev, A.Bracco, B.Bruyneel, L.Corradi, F.C.L.Crespi, G.de Angelis, M.Droste, J.Eberth, A.Esmaylzadeh, E.Farnea, E.Fioretto, C.Fransen, A.Gadea, A.Giaz, A.Gorgen, A.Gottardo, K.Hadynska-Klek, H.Hess, R.Hirsch, P.R.John, J.Jolie, A.Jungclaus, V.Karayonchev, L.Kornwebel, W.Korten, S.Leoni, L.Lewandowski, S.Lunardi, R.Menegazzo, D.Mengoni, C.Michelagnoli, T.Mijatovic, G.Montagnoli, D.Montanari, C.Muller-Gatermann, D.Napoli, Zs.Podolyak, G.Pollarolo, F.Recchia, J.-M.Regis, N.Saed-Samii, E.Sahin, F.Scarlassara, K.Schomacker, M.Seidlitz, B.Siebeck, P.-A.Soderstrom, A.M.Stefanini, O.Stezowski, S.Szilner, B.Szpak, E.Teruya, C.Ur, J.J.Valiente-Dobon, K.Wolf, K.Yanase, N.Yoshinaga, K.O.Zell

Isomer spectroscopy in 133Ba and high-spin structure of 134Ba

NUCLEAR REACTIONS 124Sn(13C, X)133Ba/134Ba, E=55 MeV from FN tandem accelerator at Cologne; 208Pb(136Xe, X)134Ba, E=6.84 MeV/nucleon from PIAVE+ALPI accelerator complex at LNL-Legnaro; measured Eγ, Iγ, γγ-coin, γγ(θ), half-lives of isomers by γγ(t) using eight HPGe and 12 LaBr3(ce) detectors at Cologne, and magnetic spectrometer PRISMA with AGATA array at Legnaro. 133,134Ba; deduced high-spin levels, isomers, J, π, multipolarities, alignments, bands, backbending, configurations, B(E1), B(E2). Comparison with shell-model calculations for 134Ba, and with previous experimental results. Systematics of positive- and negative-parity yrast states in N=78 nuclei: 130Te, 132Xe, 134Ba, 136Ce, 138Nd, 140Sm, 142Gd, and Z=56 nuclei: 126,128,130,132,134,136,138Ba.

NUCLEAR STRUCTURE 134Ba; calculated levels, J, π using GCN50:82, SN100PN, SNV, PQM130, and realistic SM interactions. Comparison with experimental data.

doi: 10.1103/PhysRevC.100.024323
Citations: PlumX Metrics

Data from this article have been entered in the XUNDL database. For more information, click here.


2018KA27      Phys.Rev. C 98, 014309 (2018)

L.Kaya, A.Vogt, P.Reiter, M.Siciliano, B.Birkenbach, A.Blazhev, L.Coraggio, E.Teruya, N.Yoshinaga, K.Higashiyama, K.Arnswald, D.Bazzacco, A.Bracco, B.Bruyneel, L.Corradi, F.C.L.Crespi, G.de Angelis, J.Eberth, E.Farnea, E.Fioretto, C.Fransen, B.Fu, A.Gadea, A.Gargano, A.Giaz, A.Gorgen, A.Gottardo, K.Hadynska-Klek, H.Hess, R.Hetzenegger, R.Hirsch, N.Itaco, P.R.John, J.Jolie, A.Jungclaus, W.Korten, S.Leoni, L.Lewandowski, S.Lunardi, R.Menegazzo, D.Mengoni, C.Michelagnoli, T.Mijatovic, G.Montagnoli, D.Montanari, C.Muller-Gatermann, D.Napoli, Zs.Podolyak, G.Pollarolo, A.Pullia, M.Queiser, F.Recchia, D.Rosiak, N.Saed-Samii, E.Sahin, F.Scarlassara, D.Schneiders, M.Seidlitz, B.Siebeck, J.F.Smith, P.-A.Soderstrom, A.M.Stefanini, T.Steinbach, O.Stezowski, S.Szilner, B.Szpak, C.Ur, J.J.Valiente-Dobon, K.Wolf, K.O.Zell

High-spin structure in the transitional nucleus 131Xe: Competitive neutron and proton alignment in the vicinity of the N=82 shell closure

NUCLEAR REACTIONS 208Pb(136Xe, X), E=6.84 MeV/nucleon; 238U(136Xe, X), E=7.35 MeV/nucleon; measured projectile-like reaction fragments using PRISMA magnetic spectrometer, Eγ, Iγ, γγ- and (131Xe)γ-coin using AGATA demonstrator array for γ detection at LNL-Legnaro. 124Sn(11B, 3np), E=54 MeV; measured Eγ, Iγ, γγ and pγ-coin, γγ(θ) using HORUS array at Cologne for γ detection and annular double-sided silicon strip detector (DSSSD) for particles. 131Xe; deduced levels, J, π, high-spin states. Comparison with shell-model calculations using several different interactions; discussed systematics of high-spin states in Z=54 nuclei of 123,125,127,129,131Xe, and N=77 nuclei of 127Sn, 129Te131Xe, 133Ba, 135Ce, 137Nd, 139Sm, 141Gd; compiled experimental total aligned angular momentum versus rotational frequency plots for yrast bands in A=117-132 Xe isotopes.

NUCLEAR STRUCTURE 131Xe; calculated levels, J, π, contribution of proton and neutron configurations for selected states, proton and neutron occupation numbers in h11/2 orbital, total aligned angular momenta as function of rotational frequency, and B(E2) using shell-model calculations with PQM130, SN100PN, GCN50:82, realistic SM, and SN100-KTH interactions. 129Xe; calculated proton and neutron occupation numbers in h11/2 orbital, total aligned angular momenta as function rotational frequency using shell model. Comparison with experimental data.

doi: 10.1103/PhysRevC.98.014309
Citations: PlumX Metrics

Data from this article have been entered in the XUNDL database. For more information, click here.


2018YA13      Phys.Rev. C 98, 014308 (2018)

K.Yanase, E.Teruya, K.Higashiyama, N.Yoshinaga

Shell-model study of Pb, Bi, Po, At, Rn, and Fr isotopes with masses from 210 to 217

NUCLEAR STRUCTURE 210,211,212Pb, 210,211,212,213Bi, 211,212,213,214Po, 212,213,214,215At, 213,214,215,216Rn, 214,215,216,217Fr; calculated level energies, B(E2), magnetic dipole and electric quadrupole moments, isomeric states, and expected number of neutron and proton pairs in 212,214Po and 214,216Rn states using large scale shell-model calculations. Comparison with available experimental data.

doi: 10.1103/PhysRevC.98.014308
Citations: PlumX Metrics


2018YO01      Prog.Theor.Exp.Phys. 2018, 023D02 (2018)

N.Yoshinaga, K.Yanase, K.Higashiyama, E.Teruya, D.Taguchi

Structure of nuclei with masses 76 and 82 and nuclear matrix elements of neutrinoless double beta decay

NUCLEAR STRUCTURE 82Se, 82Kr, 76Ge, 76Se; calculated energy levels, J, π, B(E2) values, nuclear matrix elements, T1/2. Comparison with available data.

doi: 10.1093/ptep/ptx174
Citations: PlumX Metrics


2018YO12      Phys.Rev. C 98, 044321 (2018)

N.Yoshinaga, K.Yanase, K.Higashiyama, E.Teruya

Octupole phonon model based on the shell model for octupole vibrational states

NUCLEAR STRUCTURE 200,202,204,206,208,210,212,214,216Pb, 200,202,204,206,208,210,212,214,216,218Po, 200,202,204,206,208,210,212,214,216,218,220,222Rn, 206,208,210,212,214,216,218,220,222,224,226,228,230,232Ra, 216,218,220,222,224,226,228,230,232,234,236Th; calculated E(first 4+)/E(first 2+) ratios, and energies of first 3- states. 206,210Pb, 210,212,214Po, 214,216Rn, 212At, 214Fr; calculated levels, J, π, B(E3). Shell model calculations with one-octupole-phonon representing collective octupole vibration across the magic core. Comparison with experimental values.

doi: 10.1103/PhysRevC.98.044321
Citations: PlumX Metrics


2017TE02      Phys.Rev. C 96, 015501 (2017)

E.Teruya, N.Yoshinaga, K.Higashiyama, K.Asahi

Effects of particle-hole excitations to nuclear Schiff moments in Xe isotopes

NUCLEAR MOMENTS 135,133,131,129Xe; calculated nuclear Schiff moments induced by the interaction violating parity and time reversal invariance using shell-model wave functions. Comparison with other theoretical calculations. 129Xe; calculated proton-single-particle energies, strength functions of Schiff moment operator as function of energy, energy weighted sum function for the Schiff moment; estimated upper limit for the electric dipole moment (EDM).

doi: 10.1103/PhysRevC.96.015501
Citations: PlumX Metrics


2017VO01      Phys.Rev. C 95, 024316 (2017)

A.Vogt, B.Birkenbach, P.Reiter, A.Blazhev, M.Siciliano, K.Hadynska-Klek, J.J.Valiente-Dobon, C.Wheldon, E.Teruya, N.Yoshinaga, K.Arnswald, D.Bazzacco, M.Bowry, A.Bracco, B.Bruyneel, R.S.Chakrawarthy, R.Chapman, D.Cline, L.Corradi, F.C.L.Crespi, M.Cromaz, G.de Angelis, J.Eberth, P.Fallon, E.Farnea, E.Fioretto, S.J.Freeman, B.Fu, A.Gadea, K.Geibel, W.Gelletly, A.Gengelbach, A.Giaz, A.Gorgen, A.Gottardo, A.B.Hayes, H.Hess, R.Hirsch, H.Hua, P.R.John, J.Jolie, A.Jungclaus, L.Kaya, W.Korten, I.Y.Lee, S.Leoni, L.Lewandowski, X.Liang, S.Lunardi, A.O.Macchiavelli, R.Menegazzo, D.Mengoni, C.Michelagnoli, T.Mijatovic, G.Montagnoli, D.Montanari, C.Muller-Gatermann, D.Napoli, C.J.Pearson, L.Pellegri, Zs.Podolyak, G.Pollarolo, A.Pullia, M.Queiser, F.Radeck, F.Recchia, P.H.Regan, D.Rosiak, N.Saed-Samii, E.Sahin, F.Scarlassara, D.Schneiders, M.Seidlitz, B.Siebeck, G.Sletten, J.F.Smith, P.-A.Soderstrom, A.M.Stefanini, T.Steinbach, O.Stezowski, S.Szilner, B.Szpak, R.Teng, C.Ur, V.Vandone, D.D.Warner, A.Wiens, C.Y.Wu, K.O.Zell

Isomers and high-spin structures in the N=81 isotones 135Xe and 137Ba

NUCLEAR REACTIONS 238U(136Xe, X), E=1 GeV; 208Pb(136Xe, X), E=930 MeV; 198Pt(136Xe, X), E=850 MeV; 130Te(11B, 3np)137Ba, E=54 MeV; measured reaction products, Eγ, Iγ, (particle)γ-coin, γγ-coin, (TKEL)γ-coin, half-lives of isomers by γγ(t). Four experiments carried out using 136Xe beam with 208Pb and 238U targets using PRISMA magnetic mass spectrometer and AGATA demonstrator array at Legnaro PIAVE+ALPI accelerator, 136Xe beam with 198Pt target using GAMMASPHERE and CHICO particle detector arrays at LBNL-cyclotron facility, and 11B beam with 130Te target using HORUS array at Cologne FN Tandem accelerator. 135Xe, 137Ba; deduced levels, J, π, isomers, configurations, B(E2). Comparison with shell-model calculations. Systematics of levels and isomers in N=81 nuclides 131Sn, 133Te, 135Xe, 137Ba, 139Ce, 141Nd, 143Sm and 145Gd.

NUCLEAR STRUCTURE 135Xe, 137Ba; calculated levels, J, π, B(E2) using large-scale shell-model with PQM130 and SN100PN interactions, average proton occupation numbers in each single particle orbit of the gdsh model space. Comparison with experimental data.

doi: 10.1103/PhysRevC.95.024316
Citations: PlumX Metrics

Data from this article have been entered in the XUNDL database. For more information, click here.


2017VO06      Phys.Rev. C 96, 024321 (2017)

A.Vogt, M.Siciliano, B.Birkenbach, P.Reiter, K.Hadynska-Klek, C.Wheldon, J.J.Valiente-Dobon, E.Teruya, N.Yoshinaga, K.Arnswald, D.Bazzacco, A.Blazhev, A.Bracco, B.Bruyneel, R.S.Chakrawarthy, R.Chapman, D.Cline, L.Corradi, F.C.L.Crespi, M.Cromaz, G.de Angelis, J.Eberth, P.Fallon, E.Farnea, E.Fioretto, C.Fransen, S.J.Freeman, B.Fu, A.Gadea, W.Gelletly, A.Giaz, A.Gorgen, A.Gottardo, A.B.Hayes, H.Hess, R.Hetzenegger, R.Hirsch, H.Hua, P.R.John, J.Jolie, A.Jungclaus, V.Karayonchev, L.Kaya, W.Korten, I.Y.Lee, S.Leoni, X.Liang, S.Lunardi, A.O.Macchiavelli, R.Menegazzo, D.Mengoni, C.Michelagnoli, T.Mijatovic, G.Montagnoli, D.Montanari, C.Muller-Gatermann, D.Napoli, C.J.Pearson, Zs.Podolyak, G.Pollarolo, A.Pullia, M.Queiser, F.Recchia, P.H.Regan, J.-M.Regis, N.Saed-Samii, E.Sahin, F.Scarlassara, M.Seidlitz, B.Siebeck, G.Sletten, J.F.Smith, P.-A.Soderstrom, A.M.Stefanini, O.Stezowski, S.Szilner, B.Szpak, R.Teng, C.Ur, D.D.Warner, K.Wolf, C.Y.Wu, K.O.Zell

High-spin structures in 132Xe and 133Xe and evidence for isomers along the N=79 isotones

NUCLEAR REACTIONS 208Pb(136Xe, X)132Xe/133Xe, E=6.84 MeV/nucleon from the PIAVE+ALPI accelerator complex at LNL-Legnaro; 198Pt(136Xe, X)132Xe/133Xe, E=6.25 MeV/nucleon from the LBNL cyclotron facility; 130Te(α, nγ), (α, 2nγ), E=19 MeV from Cologne FN Tandem accelerator; measured Eγ, Iγ, γγ-, (particle)γ-coin using Advanced GAmma Tracking Array (AGATA) in a demonstrator configuration, and magnetic spectrometer PRISMA for particle identification, (particle)γ-coin using Gammasphere array and CHICO gas-detector array, γγ(θ) using HORUS array at Cologne. 132,133Xe; deduced high-spin levels, J, π, half-life of a micro-sec isomer in 133Xe with Jπ=(23/2+), multipolarities, mixing ratios. Comparison with shell-model calculations using PQM130 and SN100PN interactions. Systematics of level energies in N=78 and 79 isotones from Z=50 to 64, and even-A A=120-136 Xe isotopes.

doi: 10.1103/PhysRevC.96.024321
Citations: PlumX Metrics

Data from this article have been entered in the XUNDL database. For more information, click here.


2016TE06      Phys.Rev. C 93, 064327 (2016)

E.Teruya, K.Higashiyama, N.Yoshinaga

Large-scale shell-model calculations of nuclei around mass 210

NUCLEAR STRUCTURE 203,204,205,206Pb, 204,205,206,207,208Bi, 205,206,207,208,209,210Po, 206,207,208,209,210,211At, 207,208,209,210,211,212Rn, 208,209,210,211,212,213Fr; calculated levels, J, π, B(E2), magnetic dipole moments and the electric quadrupole moments. Large-scale shell-model calculations assuming 208Pb as core, and including all the orbitals 0h9/2, 1f7/2, 0i13/2, 2p3/2, 1f5/2, and 2p1/2 between N=82 and 126 magic numbers using monopole pairing, quadrupole-quadrupole, and multipole-pairing interactions. Comparison with experimental data.

doi: 10.1103/PhysRevC.93.064327
Citations: PlumX Metrics


2016TE08      Phys.Rev. C 94, 014317 (2016)

E.Teruya, N.Yoshinaga, K.Higashiyama, H.Nishibata, A.Odahara, T.Shimoda

Large-scale shell model study of the newly found isomer in 136La

NUCLEAR STRUCTURE 136La; calculated levels, J, π, kinematic moment of inertia, B(E2), B(M1), B(M1)/B(E2) ratios, configurations, occupation proton and neutron numbers in s1/2, d3/2, d5/2, g7/2 and h11/2 orbitals. Large-scale shell model calculation with two-body interaction consisting of multipole-pairing interactions, and pairing plus quadrupole-quadrupole interaction. Comparison with experimental data.

doi: 10.1103/PhysRevC.94.014317
Citations: PlumX Metrics


2015TE05      Phys.Rev. C 92, 034320 (2015)

E.Teruya, N.Yoshinaga, K.Higashiyama, A.Odahara

Shell-model calculations of nuclei around mass 130

NUCLEAR STRUCTURE 126,127,128,129,130Sn, 127,128,129,130,131,132Sb, 128,129,130,131,132,133,134Te, 129,130,131,132,133,134,135I, 130,131,132,133,134,135,136Xe, 131,132,133,134,135,136,137Cs, 132,133,134,135,136,137,138Ba; calculated levels, J, π, bands, isomers, B(M1), B(E2), magnetic dipole and the electric quadrupole moments. Shell model calculations with monopole and quadrupole pairing plus quadrupole-quadrupole interactions. Comparison with experimental values.

doi: 10.1103/PhysRevC.92.034320
Citations: PlumX Metrics


2014YO02      Phys.Rev. C 89, 045501 (2014)

N.Yoshinaga, K.Higashiyama, R.Arai, E.Teruya

Nuclear electric dipole moments for the lowest 1/2+ states in Xe and Ba isotopes

NUCLEAR STRUCTURE 129Xe, 131Ba; calculated levels, J, π, and comparison with experimental spectrum, density of 1/2- states, strength function for nuclear electric dipole moment (EDM) operator, off-diagonal potential matrix elements between first 1/2+ state and k-th 1/2- state for the isoscalar interaction, partial contribution to EDM for isoscalar (I=0), isovector (I=1) and isotensor (J=2) type two-body interaction. 129,131,133,135Xe, 131,133,135,137Ba; calculated isoscalar (I=0), isovector (I=1) and isotensor (J=2) nuclear electric dipole moments (EDM), neutron quenching factors and upper limit of the nuclear EDM for 1/2+ states. Nuclear shell model with two-body nucleon interactions violating parity and time-reversal invariance.

doi: 10.1103/PhysRevC.89.045501
Citations: PlumX Metrics


2013FO31      Phys.Rev. C 88, 064315 (2013)

N.Fotiades, J.A.Cizewski, K.Higashiyama, N.Yoshinaga, E.Teruya, R.Krucken, R.M.Clark, P.Fallon, I.Y.Lee, A.O.Macchiavelli, W.Younes

Medium-spin states in 135Cs

NUCLEAR REACTIONS 208Pb(18O, X)135Cs, E=91 MeV; measured Eγ, Iγ, γγ-coin using Gammasphere array at LBNL cyclotron facility. 135Cs; deduced high-spin levels, J, π, B(E2), configuration. 85,86Br, 95Y; observed γ from complementary fission fragments. Systematics of level structures in 133I, 134Xe, 135Cs, 136Ba. Comparison with shell-model calculations.

NUCLEAR STRUCTURE 135Cs; calculated levels, J, π, B(E2) using shell model. Comparison with experimental data.

doi: 10.1103/PhysRevC.88.064315
Citations: PlumX Metrics

Data from this article have been entered in the XUNDL database. For more information, click here.


2013YO01      Phys.Rev. C 87, 044332 (2013); Erratum Phys.Rev. C 89, 069902 (2014)

N.Yoshinaga, K.Higashiyama, R.Arai, E.Teruya

Nuclear Schiff moments for the lowest 1/2+ states in Xe isotopes

NUCLEAR STRUCTURE 129,131,133,135Xe; calculated levels, J, π, Schiff moments. 129Xe; calculated upper limit of the electric dipole moment (EDM) of neutral atom. Nuclear shell model with two-body interactions violating parity and time-reversal invariance. Comparison of level structures with experimental data.

doi: 10.1103/PhysRevC.87.044332
Citations: PlumX Metrics


Back to query form