Anomalous Isotope Shift of the Nuclear Charge Radius

1966 ◽  
Vol 17 (6) ◽  
pp. 324-328 ◽  
Author(s):  
F. G. Perey ◽  
J. P. Schiffer
2009 ◽  
Vol 87 (7) ◽  
pp. 807-815 ◽  
Author(s):  
George A. Noble ◽  
William A. van Wijngaarden

Precise isotope shift and fine structure measurements are critically reviewed. Each experiment was checked for whether the data found for different transitions yielded consistent values for the difference in mean-square nuclear charge radius Δr2 of 6,7Li. Experiments that passed this test found Δr2 = 0.735 ± 0.036, 0.755 ± 0.023, and 0.739 ± 0.013 fm2 by studying the Li+ 1s2s 3S→1s2p 3P transition, the Li D lines and the Li 2S1/2→3S1/2 transition, respectively. These data determine the difference in mean-square nuclear charge radius 25 times more accurately than electron scattering. Similarly, averaging the fine structure data from the same experiments gives 62 678.75 ± 0.55 MHz for the 7Li+ 1s2p 3P1–2 interval, in good agreement with theory. The results for the 6,7Li 2P fine structure intervals, 10 0.52.954 ± 0.049 and 10 053.154 ± 0.040 MHz, exceed computed values by 2 MHz and yield a splitting isotope shift, which is nearly a factor of 2 lower than a theoretical estimate.


2005 ◽  
Vol 83 (4) ◽  
pp. 311-325 ◽  
Author(s):  
G WF Drake ◽  
W Nörtershäuser ◽  
Z -C Yan

It is now well established that accurate relative values of the rms nuclear charge radius for light atoms can be extracted from a comparison between high-precision theory and experiment for the isotope shift in atomic transition frequencies. Results are available for isotopes of helium and lithium. This paper reviews and updates the interpretation of earlier measurements for 3He relative to 4He, and 6Li relative to 7Li. New results are presented for the quantum electrodynamic recoil corrections. Recent measurements for the halo nucleus 6He, and the short-lived nuclei 8Li, and 9Li are discussed. The derived nuclear charge radii of 2.054(14), 2.30(4), and 2.24(4)~fm, respectively, are compared with the predictions of various nuclear structure models.PACS Nos.: 31.15.Pf, 31.30.Jv, and 32.10.Hq


LASER 2006 ◽  
2007 ◽  
pp. 189-195
Author(s):  
M. Žáková ◽  
Ch. Geppert ◽  
A. Herlert ◽  
H.-J. Kluge ◽  
R. Sánchez ◽  
...  

1966 ◽  
Vol 22 (5) ◽  
pp. 623-624 ◽  
Author(s):  
H. Theissen ◽  
R. Engfer ◽  
G.J.C. Van Niftrik

1971 ◽  
Vol 26 (3) ◽  
pp. 357-367 ◽  
Author(s):  
W.H. Kapfhammer ◽  
W. Maurer ◽  
F.E. Wagner ◽  
P.E. Kienle

Abstract The Mössbauer scattering of the 145.4 keV γ-rays of 141Pr was observed in a number of praseodymium compounds. From the isomer shifts between trivalent and tetravalent fluorine compounds the value Δ/(r2) = + 12 · 10-3 fm2 was derived for the change of the nuclear charge radius. The magnetic moment of the 145.4 keV state, μ7/2= (2.8 ± 0.2) μN, was deduced from the magnetic hyperfine pattern observed with scatterers of antiferromagnetic PrO2 .


1972 ◽  
Vol 6 (3) ◽  
pp. 1093-1098 ◽  
Author(s):  
P. Boolchand ◽  
David Langhammer ◽  
Ching-Lu Lin ◽  
S. Jha ◽  
Neal F. Peek

2009 ◽  
Vol 51 (1) ◽  
pp. 123-125 ◽  
Author(s):  
Lei Yi-An ◽  
Zhang Zhen-Hua ◽  
Zeng Jin-Yan

1992 ◽  
Vol 46 (2) ◽  
pp. 797-800 ◽  
Author(s):  
P. Lievens ◽  
L. Vermeeren ◽  
R. E. Silverans ◽  
E. Arnold ◽  
R. Neugart ◽  
...  

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