1990Journal of Physics G Nuclear and Particle PhysicsRequires access

Isotope shifts and hyperfine splitting in144-154Sm I

Jonathan G. England, I. S. Grant, J.A.R. Griffith, David E. Evans, D.A. Eastham, G. W. A. Newton, P. M. Walker

Open publisher page 32 citations

Abstract

The isotope shifts and hyperfine splitting have been measured in 144-154 Sm I using the crossed-beam laser fluorescence method. Transitions at 598.98 nm and 570.68 nm were investigated for all isotopes except 146 Sm and 153 Sm, in which measurements were only obtained at 570.68 nm. Laser-induced fluorescence has not previously been reported for 145 Sm: the hyperfine structure for the ground state of this isotope leads to mu =1.123 mu N , Q(spectroscopic)=-0.60e 2 b 2 and delta (r 2 ) (144-145)=0.11 fm 2 . The magnetic dipole and electric quadrupole moments of the odd isotopes and the changes in mean square radii of the even ones are shown to be consistent with the information obtained from nuclear spectroscopy.

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The isotope shifts and hyperfine splitting have been measured in 144-154 Sm I using the crossed-beam laser fluorescence method. Transitions at 598.98 nm and 570.68 nm were investigated for all isotopes except 146 Sm and 153 Sm, in which measurements were only obtained at 570.68 nm. Laser-induced fluorescence has not previously been reported for 145 Sm: the hyperfine structure for the ground state of this isotope leads to mu =1.123 mu N , Q(spectroscopic)=-0.60e 2 b 2 and delta (r 2 ) (144-145)=0.11 fm 2 . The magnetic dipole and electric quadrupole moments of the odd isotopes and the changes in mean square radii of the even ones are shown to be consistent with the information obtained from nuclear spectroscopy.

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Available abstract

The isotope shifts and hyperfine splitting have been measured in 144-154 Sm I using the crossed-beam laser fluorescence method. Transitions at 598.98 nm and 570.68 nm were investigated for all isotopes except 146 Sm and 153 Sm, in which measurements were only obtained at 570.68 nm. Laser-induced fluorescence has not previously been reported for 145 Sm: the hyperfine structure for the ground state of this isotope leads to mu =1.123 mu N , Q(spectroscopic)=-0.60e 2 b 2 and delta (r 2 ) (144-145)=0.11 fm 2 . The magnetic dipole and electric quadrupole moments of the odd isotopes and the changes in mean square radii of the even ones are shown to be consistent with the information obtained from nuclear spectroscopy.

Key concepts: Hyperfine structure, Isotope, Quadrupole, Physics, Atomic physics, Spectroscopy, Analytical Chemistry (journal), Chemistry

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