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 S
S郷 慎太郎*; 井手口 栄治*; 横山 輪*; 青井 考*; Azaiez, F.*; 古高 和禎; 初川 雄一; 木村 敦; 木佐森 慶一*; 小林 幹*; et al.
Physical Review C, 103(3), p.034327_1 - 034327_8, 2021/03
被引用回数:4 パーセンタイル:42.40(Physics, Nuclear)Excited states in  S were investigated by in-beam
S were investigated by in-beam  -ray spectroscopy using the
-ray spectroscopy using the  Mg(
Mg( O, 2
O, 2 1
1 ) fusion-evaporation reaction. The de-exciting
) fusion-evaporation reaction. The de-exciting  -rays were measured with germanium detector arrays along with the measurement of evaporated charged particles in a
-rays were measured with germanium detector arrays along with the measurement of evaporated charged particles in a  segmented Si detector array. The level scheme was extended up to 12470 keV. The obtained level structure is compared with the large-scale shell-model calculations. The possibility of isoscalar-pair excited states is discussed for
 segmented Si detector array. The level scheme was extended up to 12470 keV. The obtained level structure is compared with the large-scale shell-model calculations. The possibility of isoscalar-pair excited states is discussed for  states with comparison between the experimental and theoretical results.
 states with comparison between the experimental and theoretical results.
 state of
 state of  Al; Investigation on the neutron
Al; Investigation on the neutron  excitation across
 excitation across  in the island of inversion
 in the island of inversionXu, Z. Y.*; Heylen, H.*; 旭 耕一郎*; Boulay, F.*; Daugas, J. M.*; de Groote, R. P.*; Gins, W.*; Kamalou, O.*; Koszor s,
s,  .*; Lykiardopoupou, M.*; et al.
.*; Lykiardopoupou, M.*; et al.
Physics Letters B, 782, p.619 - 626, 2018/07
被引用回数:8 パーセンタイル:52.07(Astronomy & Astrophysics)GANIL研究所において、 Sからのフラグメンテーション反応によって中性子過剰核
Sからのフラグメンテーション反応によって中性子過剰核 Alにおける核異性体である
Alにおける核異性体である 状態を生成し、その磁気双極子モーメントと電気的四重極モーメント(Qモーメント)をそれぞれ
状態を生成し、その磁気双極子モーメントと電気的四重極モーメント(Qモーメント)をそれぞれ -NMR法および
-NMR法および -NQR法を用いて測定した。この状態は中性子数20の殻ギャップを越えて励起したものであり、その性質を実験的に押さえることは、この原子核の周辺で知られている逆転の島(基底状態で既に殻ギャップを越えた励起が起こるとされる原子核の一団)の発現のメカニズムを解明するための有益な情報を与える。測定されたg因子の絶対値は
-NQR法を用いて測定した。この状態は中性子数20の殻ギャップを越えて励起したものであり、その性質を実験的に押さえることは、この原子核の周辺で知られている逆転の島(基底状態で既に殻ギャップを越えた励起が起こるとされる原子核の一団)の発現のメカニズムを解明するための有益な情報を与える。測定されたg因子の絶対値は 、Qモーメントの絶対値は38(5)mbとなった。これらの値は、大規模殻模型計算による予言値に近く、模型の高い記述能力を確かめることができた。
、Qモーメントの絶対値は38(5)mbとなった。これらの値は、大規模殻模型計算による予言値に近く、模型の高い記述能力を確かめることができた。
 -decaying millisecond isomeric state in
-decaying millisecond isomeric state in  Cd
Cd
Jungclaus, A.*; Grawe, H.*; 西村 俊二*; Doornenbal, P.*; Lorusso, G.*; Simpson, G. S.*; S derstr
derstr m, P.-A.*; 炭竃 聡之*; Taprogge, J.*; Xu, Z. Y.*; et al.
m, P.-A.*; 炭竃 聡之*; Taprogge, J.*; Xu, Z. Y.*; et al.
Physics Letters B, 772, p.483 - 488, 2017/09
被引用回数:8 パーセンタイル:51.26(Astronomy & Astrophysics)A new high-spin isomer in the neutron-rich nucleus  Cd was populated in the projectile fission of a
Cd was populated in the projectile fission of a  U beam at the Radioactive Isotope Beam Factory at RIKEN. A half-life of T
U beam at the Radioactive Isotope Beam Factory at RIKEN. A half-life of T = 6.3(8) ms was measured for the new state which was tentatively assigned a spin/parity of (15
 = 6.3(8) ms was measured for the new state which was tentatively assigned a spin/parity of (15 ). The isomeric state decays via the emission of a 309-keV
). The isomeric state decays via the emission of a 309-keV  ray with
 ray with  multipolarity. The experimental results are compared to shell model calculations performed using state-of-the-art realistic effective interactions and to the neighbouring nucleus
 multipolarity. The experimental results are compared to shell model calculations performed using state-of-the-art realistic effective interactions and to the neighbouring nucleus  Cd. The comparison with calculations shows that adjustments of the pairing and multipole parts of the effective interaction derived from the CD-Bonn nucleon-nucleon potential are required in order to describe the properties of nuclei in the region around
Cd. The comparison with calculations shows that adjustments of the pairing and multipole parts of the effective interaction derived from the CD-Bonn nucleon-nucleon potential are required in order to describe the properties of nuclei in the region around  Sn.
Sn.
 decay of semi-magic
 decay of semi-magic  Cd; Revision and extension of the level scheme of
Cd; Revision and extension of the level scheme of  In
InJungclaus, A.*; Grawe, H.*; 西村 俊二*; Doornenbal, P.*; Lorusso, G.*; Simpson, G. S.*; S derstr
derstr m, P. A.*; 炭竃 聡之*; Taprogge, J.*; Xu, Z. Y.*; et al.
m, P. A.*; 炭竃 聡之*; Taprogge, J.*; Xu, Z. Y.*; et al.
Physical Review C, 94(2), p.024303_1 - 024303_8, 2016/08
被引用回数:19 パーセンタイル:75.32(Physics, Nuclear)The  decay of the semi-magic nucleus
 decay of the semi-magic nucleus  Cd has been studied at the RIBF facility at the RIKEN Nishina Center. The high statistics of the present experiment allowed for a revision of the established level scheme of
Cd has been studied at the RIBF facility at the RIKEN Nishina Center. The high statistics of the present experiment allowed for a revision of the established level scheme of  In and the observation of additional
In and the observation of additional  feeding to high lying core-excited states in
 feeding to high lying core-excited states in  In. The experimental results are compared to shell-model calculations employing a model space consisting of the full major
In. The experimental results are compared to shell-model calculations employing a model space consisting of the full major  neutron and
 neutron and  proton shells, and good agreement is found.
 proton shells, and good agreement is found.
 rays emitted from excited states south-east of
 rays emitted from excited states south-east of  Sn; The
Sn; The  g
 g 
  
  multiplet of
 multiplet of  In
In
Jungclaus, A.*; Gargano, A.*; Grawe, H.*; Taprogge, J.*; 西村 俊二*; Doornenbal, P.*; Lorusso, G.*; Shimizu, Y.*; Simpson, G. S.*; S derstr
derstr m, P.-A.*; et al.
m, P.-A.*; et al.
Physical Review C, 93(4), p.041301_1 - 041301_6, 2016/04
被引用回数:18 パーセンタイル:73.91(Physics, Nuclear)For the first time, the decay of excited states in a nucleus situated "south-east" of  Sn have been observed, in a region where experimental information is limited to ground-state properties. Six
Sn have been observed, in a region where experimental information is limited to ground-state properties. Six  rays from
 rays from  Cd, produced in the fragmentation of a
Cd, produced in the fragmentation of a  U beam at RIBF at RIKEN. The
U beam at RIBF at RIKEN. The  rays were studied using the EURICA array of Ge detectors. The new experimental information is compared to results from realistic shell-model calculations, which are the first in this region far from stability. Comparison with calculations suggests that at least four out of six new transitions can be attributed to the particle-hole configuration of one neutron in the
 rays were studied using the EURICA array of Ge detectors. The new experimental information is compared to results from realistic shell-model calculations, which are the first in this region far from stability. Comparison with calculations suggests that at least four out of six new transitions can be attributed to the particle-hole configuration of one neutron in the  and one proton hole in the
 and one proton hole in the  orbits, respectively. This work constitutes an important first step towards the exploration of nuclear structure in this unknown region of the nuclear chart.
 orbits, respectively. This work constitutes an important first step towards the exploration of nuclear structure in this unknown region of the nuclear chart.
 S
S郷 慎太郎*; 井手口 栄治*; 横山 輪*; 小林 幹*; 木佐森 慶一*; 高木 基伸*; 宮 裕之*; 大田 晋輔*; 道正 新一郎*; 下浦 享*; et al.
JPS Conference Proceedings (Internet), 6, p.030005_1 - 030005_4, 2015/06
The high-spin states in  S were investigated at Tandem-ALTO facility in Institut de Physique Nucl
S were investigated at Tandem-ALTO facility in Institut de Physique Nucl aire d'Orsay The
aire d'Orsay The  Mg(
Mg( O, 2
O, 2 1n)
1n) S fusion evaporation reaction was used to populate high-spin states in
S fusion evaporation reaction was used to populate high-spin states in  S. The germanium
S. The germanium  -ray detector array ORGAM was employed to measure
-ray detector array ORGAM was employed to measure  rays from high-spin states and charged particles evaporated from the compound nuclei were detected by a segmented silicon detector, Si-Ball. A level scheme for
 rays from high-spin states and charged particles evaporated from the compound nuclei were detected by a segmented silicon detector, Si-Ball. A level scheme for  S was deduced based on the gamma-gamma-coincidence analysis and
S was deduced based on the gamma-gamma-coincidence analysis and  -ray angular correlation analysis. The half-life of the transition in the superdeformed band was estimated by measuring the residual Doppler shift. The deduced half-life shows the large collectivity of the band.
-ray angular correlation analysis. The half-life of the transition in the superdeformed band was estimated by measuring the residual Doppler shift. The deduced half-life shows the large collectivity of the band.
 decay of
 decay of  Cd and excited states in
Cd and excited states in  In
InTaprogge, J.*; Jungclaus, A.*; Grawe, H.*; 西村 俊二*; Doornenbal, P.*; Lorusso, G.*; Simpson, G. S.*; S derstr
derstr m, P.-A.*; 炭竃 聡之*; Xu, Z. Y.*; et al.
m, P.-A.*; 炭竃 聡之*; Xu, Z. Y.*; et al.
Physical Review C, 91(5), p.054324_1 - 054324_11, 2015/05
被引用回数:25 パーセンタイル:80.55(Physics, Nuclear)The  decay of
 decay of  Cd, produced in relativistic fission of a
Cd, produced in relativistic fission of a  U beam, was studied at the RIKEN Nishina Center. From the
U beam, was studied at the RIKEN Nishina Center. From the  -ray analysis, 31 excited states and 69
-ray analysis, 31 excited states and 69  ray transitions were established in the level scheme of
 ray transitions were established in the level scheme of  In, and compared with state-of-the-art shell-model calculations. It was found that the
In, and compared with state-of-the-art shell-model calculations. It was found that the  decay of
 decay of  Cd is dominated by Gamow teller transitions, but a non-negligible contribution to the
Cd is dominated by Gamow teller transitions, but a non-negligible contribution to the  decay is also made by first-forbidden transitions. To estimate the contribution of first-forbidden transitions is important for calculations of the
 decay is also made by first-forbidden transitions. To estimate the contribution of first-forbidden transitions is important for calculations of the  -decay half-lives of nuclei in this region.
-decay half-lives of nuclei in this region.
 -decay half-lives of 110 neutron-rich nuclei across the
-decay half-lives of 110 neutron-rich nuclei across the  =82 shell gap; Implications for the mechanism and universality of the astrophysical
=82 shell gap; Implications for the mechanism and universality of the astrophysical  process
 processLorusso, G.*; 西村 俊二*; Xu, Z. Y.*; Jungclaus, A.*; Shimizu, Y.*; Simpson, G. S.*; S derstr
derstr m, P.-A.*; Watanabe, H.*; Browne, F.*; Doornenbal, P.*; et al.
m, P.-A.*; Watanabe, H.*; Browne, F.*; Doornenbal, P.*; et al.
Physical Review Letters, 114(19), p.192501_1 - 192501_7, 2015/05
被引用回数:180 パーセンタイル:97.84(Physics, Multidisciplinary)The  -decay half-lives of 110 neutron-rich isotopes of the elements from Rb to Sn were measured at the RIBF Facility at RIKEN, Japan. The new data demonstrate the persistence of shell structure far from stability and have direct implications for the
-decay half-lives of 110 neutron-rich isotopes of the elements from Rb to Sn were measured at the RIBF Facility at RIKEN, Japan. The new data demonstrate the persistence of shell structure far from stability and have direct implications for the  -process calculations. In particular, the new half-lives have a global impact on the calculated
-process calculations. In particular, the new half-lives have a global impact on the calculated  -process elemental abundances, and alleviate the underproduction of isotopes just above and below the A=130 peak, which in the past required the introduction of shell structure modifications. Reaction-network calculations based on the new data reinforce the notion that the r-process abundance pattern may result from the freeze-out of a (n,
-process elemental abundances, and alleviate the underproduction of isotopes just above and below the A=130 peak, which in the past required the introduction of shell structure modifications. Reaction-network calculations based on the new data reinforce the notion that the r-process abundance pattern may result from the freeze-out of a (n, )
) (
( ,n) equilibrium.
,n) equilibrium.
 Cd
Cd via the detection of internal conversion and Compton electrons
 via the detection of internal conversion and Compton electronsTaprogge, J.*; Jungclaus, A.*; Grawe, H.*; 西村 俊二*; Xu, Z. Y.*; Doornenbal, P.*; Lorusso, G.*; N cher, E.*; Simpson, G. S.*; S
cher, E.*; Simpson, G. S.*; S derstr
derstr m, P.-A.*; et al.
m, P.-A.*; et al.
Physics Letters B, 738, p.223 - 227, 2014/11
被引用回数:23 パーセンタイル:78.09(Astronomy & Astrophysics)The decay of an isomeric state in the neutron-rich nucleus  Cd was observed via the detection of internal conversion and Compton electrons. This measurement provided the first experimental information on excited states in this nucleus. The isomer was populated in the projectile fission of a
Cd was observed via the detection of internal conversion and Compton electrons. This measurement provided the first experimental information on excited states in this nucleus. The isomer was populated in the projectile fission of a  U beam at the RIBF facility at RIKEN. From the measured yields of
U beam at the RIBF facility at RIKEN. From the measured yields of  rays and internal conversion electrons, E3 multipolarity was tentatively assigned to the isomeric transition. A half-life of 3.6(2) ms was determined for this new state which, by comparison with shell-model calculations, was tentatively assigned a spin of (21/2
 rays and internal conversion electrons, E3 multipolarity was tentatively assigned to the isomeric transition. A half-life of 3.6(2) ms was determined for this new state which, by comparison with shell-model calculations, was tentatively assigned a spin of (21/2 ).
).
 seniority isomers of
 seniority isomers of  Sn
SnSimpson, G. S.*; Gey, G.*; Jungclaus, A.*; Taprogge, J.*; 西村 俊二*; Sieja, K.*; Doornenbal, P.*; Lorusso, G.*; S derstr
derstr m, P.-A.*; 炭竃 聡之*; et al.
m, P.-A.*; 炭竃 聡之*; et al.
Physical Review Letters, 113(13), p.132502_1 - 132502_6, 2014/09
被引用回数:71 パーセンタイル:91.31(Physics, Multidisciplinary)Delayed  -ray cascades, originating from the decay of 6
-ray cascades, originating from the decay of 6 isomeric states, in the very neutron-rich, semimagic isotopes
 isomeric states, in the very neutron-rich, semimagic isotopes  Sn were observed following the projectile fission of a
Sn were observed following the projectile fission of a  U beam at RIBF, RIKEN. The wave functions of these isomeric states are proposed to be predominantly a fully aligned pair of f
U beam at RIBF, RIKEN. The wave functions of these isomeric states are proposed to be predominantly a fully aligned pair of f neutrons. Shell-model calculations, performed using a realistic effective interaction, reproduce well the energies of the excited states of these nuclei and the measured transition rates, with the exception of the
 neutrons. Shell-model calculations, performed using a realistic effective interaction, reproduce well the energies of the excited states of these nuclei and the measured transition rates, with the exception of the  2;6
2;6 ) rate of
) rate of  Sn, which deviates from a simple seniority scheme. Empirically reducing the
Sn, which deviates from a simple seniority scheme. Empirically reducing the 
 orbit matrix elements produces a 4+1 state with almost equal seniority 2 and 4 components, correctly reproducing the experimental
 orbit matrix elements produces a 4+1 state with almost equal seniority 2 and 4 components, correctly reproducing the experimental  2;6
2;6 ) rate of
) rate of  Sn. These data provide a key benchmark for shell-model interactions far from stability.
Sn. These data provide a key benchmark for shell-model interactions far from stability.
 Sn explored with the long-lived isomer in
Sn explored with the long-lived isomer in  Pd
PdWatanabe, H.*; Lorusso, G.*; 西村 俊二*; Otsuka, T.*; Ogawa, K.*; Xu, Z. Y.*; 炭竃 聡之*; S derstr
derstr m, P.-A.*; Doornenbal, P.*; Li, Z.*; et al.
m, P.-A.*; Doornenbal, P.*; Li, Z.*; et al.
Physical Review Letters, 113(4), p.042502_1 - 042502_6, 2014/07
被引用回数:26 パーセンタイル:75.71(Physics, Multidisciplinary)A new isomer with a half-life of 23.0(8) ms has been identified in  Pd at 2406 keV excitation. The proposed spin and parity configuration is 10
Pd at 2406 keV excitation. The proposed spin and parity configuration is 10 , with maximally aligned configuration of two
, with maximally aligned configuration of two 
 neutron hole.
 neutron hole.  -decay from the long-lived isomer was also observed to populated excited states at high spins in
-decay from the long-lived isomer was also observed to populated excited states at high spins in  Ag. The small energy difference between the 10
Ag. The small energy difference between the 10 and 7
 and 7 isomers in
 isomers in  Pd was interpreted in the frame of the monopole shift of the 1
Pd was interpreted in the frame of the monopole shift of the 1
 neutron orbit. The effects of the monopole interaction on the evolution of single-neutron energies below
 neutron orbit. The effects of the monopole interaction on the evolution of single-neutron energies below  Sn are discussed in terms of central and tensor forces.
Sn are discussed in terms of central and tensor forces.
 proton-hole state in
 proton-hole state in  Sn and the shell structure along
Sn and the shell structure along  =82
=82Taprogge, J.*; Jungclaus, A.*; Grawe, H.*; 西村 俊二*; Doornenbal, P.*; Lorusso, G.*; Simpson, G.*; S derstr
derstr m, P.-A.*; 炭竃 聡之*; Xu, Z. Y.*; et al.
m, P.-A.*; 炭竃 聡之*; Xu, Z. Y.*; et al.
Physical Review Letters, 112(13), p.132501_1 - 132501_6, 2014/04
被引用回数:56 パーセンタイル:88.12(Physics, Multidisciplinary)A low-lying state in  In, the one-proton hole nucleus with respect to double magic
In, the one-proton hole nucleus with respect to double magic  Sn, was observed by its
Sn, was observed by its  decay to the beta emitting isomer. The new state, which was populated both in the beta decay of
 decay to the beta emitting isomer. The new state, which was populated both in the beta decay of  Cd and after beta-delayed neutron emission from
Cd and after beta-delayed neutron emission from  Cd, was identified, at an excitation energy of 1353 keV, as the previously unknown single-hole state with respect to the
Cd, was identified, at an excitation energy of 1353 keV, as the previously unknown single-hole state with respect to the  Sn core. Exploiting this crucial new experimental information, shell-model calculations were performed to study the structure of experimentally inaccessible
Sn core. Exploiting this crucial new experimental information, shell-model calculations were performed to study the structure of experimentally inaccessible  =82 isotones below
=82 isotones below  Sn. The results evidence a surprising absence of proton subshell closures along the chain of
Sn. The results evidence a surprising absence of proton subshell closures along the chain of  =82 isotones. This finding bears consequences on the evolution of the
=82 isotones. This finding bears consequences on the evolution of the  =82 shell gap along the r-process path.
=82 shell gap along the r-process path.
杉山 晃一*; 郷 慎太郎*; 富松 太郎*; 甲斐 民人*; 長江 大輔*; 石橋 優一*; 松永 壮太郎*; 永田 優斗*; 西畑 洸希*; 鷲山 広平*; et al.
no journal, ,
中性子過剰重アクチノイド核の励起準位構造を明らかにするため、アイソマースコープ法を用いたアクチノイド核のインビーム 線分光実験を実施した。中性子過剰重アクチノイド核は、原子力機構タンデム加速器で加速したO-18(
線分光実験を実施した。中性子過剰重アクチノイド核は、原子力機構タンデム加速器で加速したO-18( O)ビームをCm-248(
O)ビームをCm-248( Cm)標的に照射して多核子移行反応で合成した。後方に散乱したビーム様粒子をSi E-
Cm)標的に照射して多核子移行反応で合成した。後方に散乱したビーム様粒子をSi E- E検出器で検出して生成核を識別し、前方方向に散乱された標的様粒子の核異性体を60mm程度下流に設置したアルミ板で捕集した。アルミ板の周囲に4台のGe検出器及び4台のLaBr検出器を設置して、捕集された核異性体からの
E検出器で検出して生成核を識別し、前方方向に散乱された標的様粒子の核異性体を60mm程度下流に設置したアルミ板で捕集した。アルミ板の周囲に4台のGe検出器及び4台のLaBr検出器を設置して、捕集された核異性体からの 線を測定した。標的と検出器の間にタングステン遮蔽を設置して標的から放出される多量の
線を測定した。標的と検出器の間にタングステン遮蔽を設置して標的から放出される多量の 線を遮蔽し、アクチノイド核異性体からの
線を遮蔽し、アクチノイド核異性体からの 線を感度良く検出することに成功した。
線を感度良く検出することに成功した。