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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...

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Detalles Bibliográficos
Autores principales: 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.
Lenguaje:eng
Publicado: 2014
Materias:
Acceso en línea:https://dx.doi.org/10.1103/PhysRevC.90.014317
http://cds.cern.ch/record/1728182
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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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