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 = 0 selection rule in Gamow-Teller transitions; The
 = 0 selection rule in Gamow-Teller transitions; The  -decay of
-decay of  Hg
HgBerry, T. A.*; Podoly k, Zs.*; Carroll, R. J.*; Lic
k, Zs.*; Carroll, R. J.*; Lic , R.*; Grawe, H.*; Timofeyuk, N. K.*; Alexander, T.*; Andreyev, A. N.; Ansari, S.*; Borge, M. J. G.*; et al.
, R.*; Grawe, H.*; Timofeyuk, N. K.*; Alexander, T.*; Andreyev, A. N.; Ansari, S.*; Borge, M. J. G.*; et al.
Physics Letters B, 793, p.271 - 275, 2019/06
被引用回数:6 パーセンタイル:46.16(Astronomy & Astrophysics)Gamow-Teller  decay is forbidden if the number of nodes in the radial wave functions of the initial and final states is different. This
 decay is forbidden if the number of nodes in the radial wave functions of the initial and final states is different. This 
 = 0 requirement plays a major role in the
 = 0 requirement plays a major role in the  decay of heavy neutron-rich nuclei, affecting the nucleosynthesis through the increased half-lives of nuclei on the astrophysical
 decay of heavy neutron-rich nuclei, affecting the nucleosynthesis through the increased half-lives of nuclei on the astrophysical  -process pathway below both
-process pathway below both  = 50 (for
 = 50 (for  82) and
 82) and  = 82 (for
 = 82 (for  126). The level of forbiddenness of the
 126). The level of forbiddenness of the 
 = 1
 = 1  1
1 0
0 transition has been investigated from the
 transition has been investigated from the  decay of the ground state of
 decay of the ground state of  Hg into the single-proton-hole nucleus
Hg into the single-proton-hole nucleus  Tl in an experiment at the ISOLDE Decay Station. From statistical observational limits on possible
Tl in an experiment at the ISOLDE Decay Station. From statistical observational limits on possible  -ray transitions depopulating the
-ray transitions depopulating the  0
0 state in
 state in  Tl, an upper limit of 3.9
Tl, an upper limit of 3.9 10
10 % was obtained for the probability of this decay, corresponding to log
 % was obtained for the probability of this decay, corresponding to log 8.8 within a 95% confidence limit. This is the most stringent test of the
 8.8 within a 95% confidence limit. This is the most stringent test of the 
 = 0 selection rule to date.
 = 0 selection rule to date.
 =28 and
=28 and  =50; Spectroscopy of
=50; Spectroscopy of  Zn
ZnShand, C. M.*; Podoly k, Zs.*; G
k, Zs.*; G rska, M.*; Doornenbal, P.*; Obertelli, A.*; Nowacki, F.*; Otsuka, T.*; Sieja, K.*; Tostevin, J. A.*; Tsunoda, T.*; et al.
rska, M.*; Doornenbal, P.*; Obertelli, A.*; Nowacki, F.*; Otsuka, T.*; Sieja, K.*; Tostevin, J. A.*; Tsunoda, T.*; et al.
Physics Letters B, 773, p.492 - 497, 2017/10
被引用回数:28 パーセンタイル:87.26(Astronomy & Astrophysics)Low-lying states in neutron-rich  Zn nuclei were measured for the first time via in-beam
Zn nuclei were measured for the first time via in-beam  -ray spectroscopy at RIKEN. These include the 4
-ray spectroscopy at RIKEN. These include the 4 to 2
 to 2 in
 in  Zn and the 2
Zn and the 2 to 0
 to 0 and 4
 and 4 to 2
 to 2 in
 in  Zn. The reduced E(
Zn. The reduced E( ) energies and increased E(4
) energies and increased E(4 )/E(2
)/E(2 ) ratios at
) ratios at  =52,54 compared to
=52,54 compared to  Zn attest that the magicity is confined just on the neutron number
Zn attest that the magicity is confined just on the neutron number  =50 only. The levels observed in
=50 only. The levels observed in  Zn suggest the onset of deformation towards heavier Zn isotopes. The data were compared to state-of-the-art shell model calculations.
Zn suggest the onset of deformation towards heavier Zn isotopes. The data were compared to state-of-the-art shell model calculations.
 Kr
KrFlavigny, F.*; Doornenbal, P.*; Obertelli, A.*; Delaroche, J.-P.*; Girod, M.*; Libert, J.*; Rodriguez, T. R.*; Authelet, G.*; 馬場 秀忠*; Calvet, D.*; et al.
Physical Review Letters, 118(24), p.242501_1 - 242501_6, 2017/06
被引用回数:41 パーセンタイル:85.80(Physics, Multidisciplinary)The first  -ray spectroscopy of very neutron rich
-ray spectroscopy of very neutron rich  Kr isotopes was carried out at the RIBF at RIKEN Nishina center. Excited states in these isotopes were populated via (p,2p) reactions using radioactive
Kr isotopes was carried out at the RIBF at RIKEN Nishina center. Excited states in these isotopes were populated via (p,2p) reactions using radioactive  Rb beams accelerated to 220 MeV/nucleon. The new data show a significant increase in deformation beyond N=60, as well as competing configurations (shape-coexistence) at low energy. The data were compared with beyond-mean-field calculations which predict level energies in good agreement with observation, and suggest oblate-prolate shape coexistence.
Rb beams accelerated to 220 MeV/nucleon. The new data show a significant increase in deformation beyond N=60, as well as competing configurations (shape-coexistence) at low energy. The data were compared with beyond-mean-field calculations which predict level energies in good agreement with observation, and suggest oblate-prolate shape coexistence.
Chen, S.*; Doornenbal, P.*; Obertelli, A.*; Rodriguez, T. R.*; Authelet, G.*; 馬場 秀忠*; Calvet, D.*; Ch teau, F.*; Corsi, A.*; Delbart, A.*; et al.
teau, F.*; Corsi, A.*; Delbart, A.*; et al.
Physical Review C, 95(4), p.041302_1 - 041302_6, 2017/04
被引用回数:31 パーセンタイル:88.91(Physics, Nuclear)Neutron-rich isotopes of selenium,  Se, where studied via in beam
Se, where studied via in beam  -ray spectroscopy after nucleon removal reactions at RIBF in RIKEN. The low-energy excitations of these nuclei were investigated using
-ray spectroscopy after nucleon removal reactions at RIBF in RIKEN. The low-energy excitations of these nuclei were investigated using  -
- coincidences, and the first and second excited 2
 coincidences, and the first and second excited 2 states were found at remarkably low energies. The analysis and comparison with self-consistent beyond-mean field calculations suggest that both shape coexistence and triaxiality are needed to describe these isotopes.
 states were found at remarkably low energies. The analysis and comparison with self-consistent beyond-mean field calculations suggest that both shape coexistence and triaxiality are needed to describe these isotopes.
 Zr
ZrPaul, N.*; Corsi, A.*; Obertelli, A.*; Doornenbal, P.*; Authelet, G.*; 馬場 秀忠*; Bally, B.*; Bender, M.*; Calvet, D.*; Ch teau, F.*; et al.
teau, F.*; et al.
Physical Review Letters, 118(3), p.032501_1 - 032501_7, 2017/01
被引用回数:46 パーセンタイル:87.79(Physics, Multidisciplinary)The first measurement of  rays emitted by the very neutron rich nuclei
 rays emitted by the very neutron rich nuclei  Mo (Z=42) and
Mo (Z=42) and  Zr (Z=40) was carried out at the RIBF facility at RIKEN. These data shine light on the postulated N=70 harmonic oscillator shell. If the spin-orbit splitting which gives rise to the N=82 shell gap is reduced in very neutron-rich nuclei, the harmonic oscillator gap at N=70 should open instead. However, both the measured energy of the first excited state
Zr (Z=40) was carried out at the RIBF facility at RIKEN. These data shine light on the postulated N=70 harmonic oscillator shell. If the spin-orbit splitting which gives rise to the N=82 shell gap is reduced in very neutron-rich nuclei, the harmonic oscillator gap at N=70 should open instead. However, both the measured energy of the first excited state  Mo and
Mo and  Zr, respectively 235(7) keV and 185(11) keV, and their E(4
Zr, respectively 235(7) keV and 185(11) keV, and their E(4 )/E(2
)/E(2 ) ratio, indicate that these nuclei are good rotors, and exclude the shell stabilization scenario at Z=40 and N=70. These results were compared to state-of-the-art density functional theoretical calculations using Gogny and Skyrme effective interactions.
) ratio, indicate that these nuclei are good rotors, and exclude the shell stabilization scenario at Z=40 and N=70. These results were compared to state-of-the-art density functional theoretical calculations using Gogny and Skyrme effective interactions.