Electromagnetic moments of 215,217Bi: Probing shell evolution beyond N = 126
Andrei N. Andreyev, Anatoly E. Barzakh, M. D. Seliverstov, Zhenxing Yue et autres
9 pages, 8 figures, 1 table
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Andrei N. Andreyev, Anatoly E. Barzakh, M. D. Seliverstov, Zhenxing Yue et autres
9 pages, 8 figures, 1 table
Anatoly E. Barzakh, Andrei N. Andreyev, Zhenxing Yue, L. Nies et autres
The changes in the mean-squared charge radii relative to Bi 126 209 ( δ 〈 r 2 〉 N , 126 ) and the magnetic dipole and electric quadrupole moments in Bi 214 − 218 have been measured using the in-source resonance-ionization …
jp, gb, ch, es, hu, uz, sk, om, de, it, ro, be, ca, dk, fi, se, cn, fr, us, au (code pays fourni par la source)
David Lunney, V. Manea, Mathilde Mougeot, L. Nies et autres
The onset of collective nuclear behavior in the $N=60$, $A\ensuremath{\approx}100$ region is examined through high-precision mass measurements of $^{96\ensuremath{-}98}\mathrm{Kr}$, performed with the ISOLTRAP mass spectrometer at ISOLDE, CERN. Our results for $^{96\ensuremath{-}97}\mathrm{Kr}$ agree with previous measurements, with our new $^{97}\mathrm{Kr}$ Penning-trap mass …
fr, de, ch, sa, gb, es, au (code pays fourni par la source)
A. E. Barzakh, A. N. Andreyev, Z. Yue, L. Nies et autres
The changes in the mean-squared charge radii relative to 209Bi126(𝛿⟨𝑟2⟩𝑁,126) and the magnetic dipole and electric quadrupole moments in 214−218Bihave been measured using the in-source resonance-ionization spectroscopy technique at ISOLDE (CERN). Magnetic moments of odd-odd bismuth nuclei have been analyzed by the …
de (code pays fourni par la source)
A. N. Andreyev, A. E. Barzakh, M. D. Seliverstov, Z. Yue et autres
de (code pays fourni par la source)
L. Nies, L. Cañete, D. D. Dao, S. Giraud et autres
Isomers close to doubly magic $_{28}^{78}{\mathrm{Ni}}_{50}$ provide essential information on the shell evolution and shape coexistence near the $Z=28$ and $N=50$ double shell closure. We report the excitation energy measurement of the $1/{2}^{+}$ isomer in $_{30}^{79}{\mathrm{Zn}}_{49}$ through independent high-precision mass measurements with …
de, ch, gb, fi, fr, tr, ro (code pays fourni par la source)
L. Nies, L. Cañete, D. D. Dao, S. Giraud et autres
Isomers close to doubly magic _{28}^{78}Ni_{50} provide essential information on the shell evolution and shape coexistence near the Z=28 and N=50 double shell closure. We report the excitation energy measurement of the 1/2^{+} isomer in _{30}^{79}Zn_{49} through independent high-precision mass measurements with …
de, ch, gb, fi, fr, tr, ro (code pays fourni par la source)
I. Kulikov, Alejandro Algora, D. Atanasov, P. Ascher et autres
de, es, hu, fr, tr, ch (code pays fourni par la source)
M. Mougeot, D. Atanasov, C. Barbieri, K. Blaum et autres
The strength of the $N=28$ magic number in neutron-rich argon isotopes is examined through high-precision mass measurements of $^{46\text{--}48}\mathrm{Ar}$, performed with the ISOLTRAP mass spectrometer at ISOLDE/CERN. The new mass values are up to 90 times more precise than previous measurements. While …
fr, de, it, gb, ch, be, ca, au (code pays fourni par la source)
V. Manea, J. Karthein, D. Atanasov, M. Bender et autres
We probe the N=82 nuclear shell closure by mass measurements of neutron-rich cadmium isotopes with the ISOLTRAP spectrometer at ISOLDE-CERN. The new mass of ^{132}Cd offers the first value of the N=82, two-neutron shell gap below Z=50 and confirms the phenomenon of …
de, ch, be, fr, ca, es, jp (code pays fourni par la source)
W. J. Huang, D. Atanasov, G. Audi, K. Blaum et autres
High-precision mass measurements of stable and beta-decaying nuclides 52-57Cr, 55Mn, 56,59Fe, 59Co, 75, 77-79Ga, and the lanthanide nuclides 140Ce, 140Nd, 160Yb, 168Lu, 178Yb have been performed with the Penning-trap mass spectrometer ISOLTRAP at ISOLDE/CERN. The new data are entered into the Atomic …
fr, de, ch, tr, jp (code pays fourni par la source)
P. C.-O. Ranitzsch, C. Hassel, Mathias Wegner, Daniel Hengstler et autres
The isotope $^{163}\mathrm{Ho}$ is in many ways the best candidate to perform experiments to investigate the value of the electron neutrino mass. It undergoes an electron capture process to $^{163}\mathrm{Dy}$ with an energy available to the decay, ${Q}_{\mathrm{EC}}$, of about 2.8 keV. …
de, ch (code pays fourni par la source)
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