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Laser spectroscopy of francium isotopes at the borders of the region of reflection asymmetry
The magnetic dipole moments and changes in mean-square charge radii of the neutron-rich $^{218m,219,229,231}\text{Fr}$ isotopes were measured with the newly-installed Collinear Resonance Ionization Spectroscopy (CRIS) beam line at ISOLDE, CERN, probing the $7s~^{2}S_{1/2}$ to $8p~^{2}P_{3/2}$ atomic...
Autores principales: | , , , , , , , , , , , , , , , , , , , |
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Lenguaje: | eng |
Publicado: |
2014
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Materias: | |
Acceso en línea: | https://dx.doi.org/10.1103/PhysRevC.90.014317 http://cds.cern.ch/record/1728182 |
_version_ | 1780939993882034176 |
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author | Budinčević, I. Billowes, J. Bissell, M.L. Cocolios, T.E. de Groote, R.P. De Schepper, S. Fedosseev, V.N. Flanagan, K.T. Franchoo, S. Garcia Ruiz, R.F. Heylen, H. Lynch, K.M. Marsh, B.A. Neyens, G. Procter, T.J. Rossel, R.E. Rothe, S. Strashnov, I. Stroke, H.H. Wendt, K.D.A. |
author_facet | Budinčević, I. Billowes, J. Bissell, M.L. Cocolios, T.E. de Groote, R.P. De Schepper, S. Fedosseev, V.N. Flanagan, K.T. Franchoo, S. Garcia Ruiz, R.F. Heylen, H. Lynch, K.M. Marsh, B.A. Neyens, G. Procter, T.J. Rossel, R.E. Rothe, S. Strashnov, I. Stroke, H.H. Wendt, K.D.A. |
author_sort | Budinčević, I. |
collection | CERN |
description | The magnetic dipole moments and changes in mean-square charge radii of the neutron-rich $^{218m,219,229,231}\text{Fr}$ isotopes were measured with the newly-installed Collinear Resonance Ionization Spectroscopy (CRIS) beam line at ISOLDE, CERN, probing the $7s~^{2}S_{1/2}$ to $8p~^{2}P_{3/2}$ atomic transition. The $\delta\langle r^{2}\rangle^{A,221}$ values for $^{218m,219}\text{Fr}$ and $^{229,231}\text{Fr}$ follow the observed increasing slope of the charge radii beyond $N~=~126$. The charge radii odd-even staggering in this neutron-rich region is discussed, showing that $^{220}\text{Fr}$ has a weakly inverted odd-even staggering while $^{228}\text{Fr}$ has normal staggering. This suggests that both isotopes reside at the borders of a region of inverted staggering, which has been associated with reflection-asymmetric shapes. The $g(^{219}\text{Fr}) = +0.69(1)$ value supports a $\pi 1h_{9/2}$ shell model configuration for the ground state. The $g(^{229,231}\text{Fr})$ values support the tentative $I^{\pi}(^{229,231}\text{Fr}) = (1/2^{+})$ spin, and point to a $\pi s_{1/2}^{-1}$ intruder ground state configuration. |
id | cern-1728182 |
institution | Organización Europea para la Investigación Nuclear |
language | eng |
publishDate | 2014 |
record_format | invenio |
spelling | cern-17281822022-03-31T02:11:39Zdoi:10.1103/PhysRevC.90.014317http://cds.cern.ch/record/1728182engBudinčević, I.Billowes, J.Bissell, M.L.Cocolios, T.E.de Groote, R.P.De Schepper, S.Fedosseev, V.N.Flanagan, K.T.Franchoo, S.Garcia Ruiz, R.F.Heylen, H.Lynch, K.M.Marsh, B.A.Neyens, G.Procter, T.J.Rossel, R.E.Rothe, S.Strashnov, I.Stroke, H.H.Wendt, K.D.A.Laser spectroscopy of francium isotopes at the borders of the region of reflection asymmetrynucl-exThe magnetic dipole moments and changes in mean-square charge radii of the neutron-rich $^{218m,219,229,231}\text{Fr}$ isotopes were measured with the newly-installed Collinear Resonance Ionization Spectroscopy (CRIS) beam line at ISOLDE, CERN, probing the $7s~^{2}S_{1/2}$ to $8p~^{2}P_{3/2}$ atomic transition. The $\delta\langle r^{2}\rangle^{A,221}$ values for $^{218m,219}\text{Fr}$ and $^{229,231}\text{Fr}$ follow the observed increasing slope of the charge radii beyond $N~=~126$. The charge radii odd-even staggering in this neutron-rich region is discussed, showing that $^{220}\text{Fr}$ has a weakly inverted odd-even staggering while $^{228}\text{Fr}$ has normal staggering. This suggests that both isotopes reside at the borders of a region of inverted staggering, which has been associated with reflection-asymmetric shapes. The $g(^{219}\text{Fr}) = +0.69(1)$ value supports a $\pi 1h_{9/2}$ shell model configuration for the ground state. The $g(^{229,231}\text{Fr})$ values support the tentative $I^{\pi}(^{229,231}\text{Fr}) = (1/2^{+})$ spin, and point to a $\pi s_{1/2}^{-1}$ intruder ground state configuration.<p>The magnetic dipole moments and changes in mean-square charge radii of the neutron-rich <inline-formula><mml:math><mml:mrow><mml:msup><mml:mrow></mml:mrow><mml:mrow><mml:mn>218</mml:mn><mml:mi>m</mml:mi><mml:mo>,</mml:mo><mml:mn>219</mml:mn><mml:mo>,</mml:mo><mml:mn>229</mml:mn><mml:mo>,</mml:mo><mml:mn>231</mml:mn></mml:mrow></mml:msup><mml:mi>Fr</mml:mi></mml:mrow></mml:math></inline-formula> isotopes were measured with the newly installed Collinear Resonance Ionization Spectroscopy (CRIS) beam line at the On-Line Isotope Mass Separator (ISOLDE), CERN, probing the <inline-formula><mml:math><mml:mrow><mml:mn>7</mml:mn><mml:msup><mml:mi>s</mml:mi><mml:mn>2</mml:mn></mml:msup><mml:msub><mml:mi>S</mml:mi><mml:mrow><mml:mn>1</mml:mn><mml:mo>/</mml:mo><mml:mn>2</mml:mn></mml:mrow></mml:msub></mml:mrow></mml:math></inline-formula> to <inline-formula><mml:math><mml:mrow><mml:mn>8</mml:mn><mml:msup><mml:mi>p</mml:mi><mml:mn>2</mml:mn></mml:msup><mml:msub><mml:mi>P</mml:mi><mml:mrow><mml:mn>3</mml:mn><mml:mo>/</mml:mo><mml:mn>2</mml:mn></mml:mrow></mml:msub></mml:mrow></mml:math></inline-formula> atomic transition. The <inline-formula><mml:math><mml:mrow><mml:mi>δ</mml:mi><mml:msup><mml:mrow><mml:mo>〈</mml:mo><mml:msup><mml:mi>r</mml:mi><mml:mn>2</mml:mn></mml:msup><mml:mo>〉</mml:mo></mml:mrow><mml:mrow><mml:mi>A</mml:mi><mml:mo>,</mml:mo><mml:mn>221</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula> values for <inline-formula><mml:math><mml:mrow><mml:msup><mml:mrow></mml:mrow><mml:mrow><mml:mn>218</mml:mn><mml:mi>m</mml:mi><mml:mo>,</mml:mo><mml:mn>219</mml:mn></mml:mrow></mml:msup><mml:mi>Fr</mml:mi></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math><mml:mrow><mml:msup><mml:mrow></mml:mrow><mml:mrow><mml:mn>229</mml:mn><mml:mo>,</mml:mo><mml:mn>231</mml:mn></mml:mrow></mml:msup><mml:mi>Fr</mml:mi></mml:mrow></mml:math></inline-formula> follow the observed increasing slope of the charge radii beyond <inline-formula><mml:math><mml:mrow><mml:mi>N</mml:mi><mml:mo>=</mml:mo><mml:mn>126</mml:mn></mml:mrow></mml:math></inline-formula>. The charge radii odd-even staggering in this neutron-rich region is discussed, showing that <inline-formula><mml:math><mml:mrow><mml:msup><mml:mrow></mml:mrow><mml:mn>220</mml:mn></mml:msup><mml:mi>Fr</mml:mi></mml:mrow></mml:math></inline-formula> has a weakly inverted odd-even staggering while <inline-formula><mml:math><mml:mrow><mml:msup><mml:mrow></mml:mrow><mml:mn>228</mml:mn></mml:msup><mml:mi>Fr</mml:mi></mml:mrow></mml:math></inline-formula> has normal staggering. This suggests that both isotopes reside at the borders of a region of inverted staggering, which has been associated with reflection-asymmetric shapes. The <inline-formula><mml:math><mml:mrow><mml:mi>g</mml:mi><mml:mrow><mml:msup><mml:mo>(</mml:mo><mml:mn>219</mml:mn></mml:msup><mml:mi>Fr</mml:mi><mml:mo>)</mml:mo></mml:mrow><mml:mo>=</mml:mo><mml:mo>+</mml:mo><mml:mn>0.69</mml:mn><mml:mspace width="0.16em"></mml:mspace><mml:mrow><mml:mo>(</mml:mo><mml:mn>1</mml:mn><mml:mo>)</mml:mo></mml:mrow></mml:mrow></mml:math></inline-formula> value supports a <inline-formula><mml:math><mml:mrow><mml:mi>π</mml:mi><mml:mn>1</mml:mn><mml:msub><mml:mi>h</mml:mi><mml:mrow><mml:mn>9</mml:mn><mml:mo>/</mml:mo><mml:mn>2</mml:mn></mml:mrow></mml:msub></mml:mrow></mml:math></inline-formula> shell-model configuration for the ground state. The <inline-formula><mml:math><mml:mrow><mml:mi>g</mml:mi><mml:msup><mml:mo>(</mml:mo><mml:mrow><mml:mn>229</mml:mn><mml:mo>,</mml:mo><mml:mn>231</mml:mn></mml:mrow></mml:msup><mml:mi>Fr</mml:mi><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula> values support the tentative <inline-formula><mml:math><mml:mrow><mml:msup><mml:mi>I</mml:mi><mml:mi>π</mml:mi></mml:msup><mml:mrow><mml:msup><mml:mo>(</mml:mo><mml:mrow><mml:mn>229</mml:mn><mml:mo>,</mml:mo><mml:mn>231</mml:mn></mml:mrow></mml:msup><mml:mi>Fr</mml:mi><mml:mo>)</mml:mo></mml:mrow><mml:mo>=</mml:mo><mml:mrow><mml:mo>(</mml:mo><mml:mn>1</mml:mn><mml:mo>/</mml:mo><mml:msup><mml:mn>2</mml:mn><mml:mo>+</mml:mo></mml:msup><mml:mo>)</mml:mo></mml:mrow></mml:mrow></mml:math></inline-formula> spin and point to a <inline-formula><mml:math><mml:mrow><mml:mi>π</mml:mi><mml:msubsup><mml:mi>s</mml:mi><mml:mrow><mml:mn>1</mml:mn><mml:mo>/</mml:mo><mml:mn>2</mml:mn></mml:mrow><mml:mrow><mml:mo>−</mml:mo><mml:mn>1</mml:mn></mml:mrow></mml:msubsup></mml:mrow></mml:math></inline-formula> intruder ground-state configuration.</p>The magnetic dipole moments and changes in mean-square charge radii of the neutron-rich $^{218m,219,229,231}\text{Fr}$ isotopes were measured with the newly-installed Collinear Resonance Ionization Spectroscopy (CRIS) beam line at ISOLDE, CERN, probing the $7s~^{2}S_{1/2}$ to $8p~^{2}P_{3/2}$ atomic transition. The $\delta\langle r^{2}\rangle^{A,221}$ values for $^{218m,219}\text{Fr}$ and $^{229,231}\text{Fr}$ follow the observed increasing slope of the charge radii beyond $N~=~126$. The charge radii odd-even staggering in this neutron-rich region is discussed, showing that $^{220}\text{Fr}$ has a weakly inverted odd-even staggering while $^{228}\text{Fr}$ has normal staggering. This suggests that both isotopes reside at the borders of a region of inverted staggering, which has been associated with reflection-asymmetric shapes. The $g(^{219}\text{Fr}) = +0.69(1)$ value supports a $\pi 1h_{9/2}$ shell model configuration for the ground state. The $g(^{229,231}\text{Fr})$ values support the tentative $I^{\pi}(^{229,231}\text{Fr}) = (1/2^{+})$ spin, and point to a $\pi s_{1/2}^{-1}$ intruder ground state configuration.arXiv:1407.0563oai:cds.cern.ch:17281822014-07-02 |
spellingShingle | nucl-ex Budinčević, I. Billowes, J. Bissell, M.L. Cocolios, T.E. de Groote, R.P. De Schepper, S. Fedosseev, V.N. Flanagan, K.T. Franchoo, S. Garcia Ruiz, R.F. Heylen, H. Lynch, K.M. Marsh, B.A. Neyens, G. Procter, T.J. Rossel, R.E. Rothe, S. Strashnov, I. Stroke, H.H. Wendt, K.D.A. Laser spectroscopy of francium isotopes at the borders of the region of reflection asymmetry |
title | Laser spectroscopy of francium isotopes at the borders of the region of reflection asymmetry |
title_full | Laser spectroscopy of francium isotopes at the borders of the region of reflection asymmetry |
title_fullStr | Laser spectroscopy of francium isotopes at the borders of the region of reflection asymmetry |
title_full_unstemmed | Laser spectroscopy of francium isotopes at the borders of the region of reflection asymmetry |
title_short | Laser spectroscopy of francium isotopes at the borders of the region of reflection asymmetry |
title_sort | laser spectroscopy of francium isotopes at the borders of the region of reflection asymmetry |
topic | nucl-ex |
url | https://dx.doi.org/10.1103/PhysRevC.90.014317 http://cds.cern.ch/record/1728182 |
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