Effect of a Diffuse Nuclear Charge Distribution on the Hyperfine-Structure Interaction

1972 ◽  
Vol 5 (5) ◽  
pp. 1992-2000 ◽  
Author(s):  
H. J. Rosenberg ◽  
H. H. Stroke

Three lines in the atomic spectrum of tin, λ 3262 Å, λ 3283 Å and λ 6454Å have been studied in emission under high resolution with the use of light sources containing enriched isotopic samples. Results are reported for isotope shifts in these lines for the abundant stable isotopes ( A ≽ 116). Pressure-scanned Fabry–Perot etalons provided the necessary resolution; the spectrograms for λ 6454 Å were recorded and analysed by digital techniques, and for this line hyperfine structure constants required in the interpretation of the data were also evaluated. The results for the three lines are not in good agreement with earlier work, but are shown to be self-consistent by means of a King plot. Their interpretation in terms of the nuclear charge distribution is considered in the following paper.


1954 ◽  
Vol 94 (6) ◽  
pp. 1617-1629 ◽  
Author(s):  
David L. Hill ◽  
Kenneth W. Ford

Physica ◽  
1956 ◽  
Vol 22 (6-12) ◽  
pp. 1195-1196 ◽  
Author(s):  
J. Fregeau ◽  
R.H. Helm ◽  
R. Hofstadter

1985 ◽  
Vol 31 (4) ◽  
pp. 1334-1339 ◽  
Author(s):  
Larry Robinson ◽  
Arthur C. Wahl ◽  
Tomasz M. Semkow ◽  
Andrew E. Norris

1956 ◽  
Vol 9 (4) ◽  
pp. 407 ◽  
Author(s):  
LJ Tassie

A model of nuclear shape oscillations is set up for an arbitrary nuclear charge distribution. For a uniform charge distribution the model reduces to the liquid drop model. The model is used to consider ?-transitions and electron excitation of nuclei. Explicit expressions are obtained for four charge distributions: (a) uniform, (b) Gaussian, (c) exponential, (d) uniform with Gaussian "edge". The theory predicts a relative angular distribution of electrons scattered by the 4�43 MeV level of 12C in agreement with the experimental results of Fregeau and Hofstadter (1955), but gives a scattered intensity seven times too large.


1966 ◽  
Vol 144 (3) ◽  
pp. 984-993 ◽  
Author(s):  
P. O. Strom ◽  
D. L. Love ◽  
A. E. Greendale ◽  
A. A. Delucchi ◽  
D. Sam ◽  
...  

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