scholarly journals Nuclear structure information obtained from charge radii

1985 ◽  
Vol 164 (4-6) ◽  
pp. 241-244 ◽  
Author(s):  
C.E. Alonso ◽  
J.M. Arias ◽  
F. Iachello
Author(s):  
A. HEUSLER ◽  
P. VON BRENTANO ◽  
T. FAESTERMANN ◽  
G. GRAW ◽  
R. HERTENBERGER ◽  
...  

1972 ◽  
Vol 187 (2) ◽  
pp. 314-322 ◽  
Author(s):  
L.R.B. Elton ◽  
O. Sundberg

2006 ◽  
Vol 15 (07) ◽  
pp. 1637-1644 ◽  
Author(s):  
P. M. WALKER

As a subset of radioactive beams, isomer beams open up the dimensions of excitation energy and angular momentum. The problem of isomer decay rates is briefly presented, as they are not yet well understood. The use of isomer beams for nuclear structure investigations is reviewed, using examples related to exotic decay modes, charge radii, and Coulomb excitation. There are also unique possibilities for the study of induced electromagnetic depopulation. A key aspect is beam purification, for which different techniques are discussed.


1977 ◽  
Vol 55 (19) ◽  
pp. 1657-1686 ◽  
Author(s):  
J. D. Panar ◽  
O. Straume ◽  
D. G. Burke

The (3He,d) and (α,t) reactions have been used to study odd proton states in 157,159,161,163Ho. The beams were provided by tandem Van de Graaff accelerators and the light reaction products were analyzed with magnetic spectrographs and detected with photographic emulsions. Spectra were studied up to excitation energies of ~1.5 MeV for each nuclide with resolutions (FWHM) of ~14 keV for the (3He,d) reaction and ~12 keV for the (α,t) reaction. Information on the l-values was obtained from the ratios of (3He,d) and (α,t) cross sections and from (3He,d) angular distributions. The results are interpreted in terms of the Nilsson model with pairing and Coriolis mixing included. Nuclear structure factors were extracted from the experimental data with the aid of DWBA calculations. Nilsson assignments from previous gamma-ray studies have been confirmed for many low-lying rotational bands. In addition, many new assignments have been made, particularly in the lighter isotopes for which very little nuclear structure information existed previously. A relatively strong l = 0 transition is found in each nuclide and arguments are made to suggest these Iπ = 1/2+ states are gamma vibrations based on the 5/2+[402] states. Similarly, strong l = 2 transitions populate states which may be Iπ = 3/2+ gamma vibrations based on the 7/2+[404] orbitals. Some interesting systematics of the behaviour of single particle states in this region are presented and some anomalies in the populations of the 1/2+[411] and 3/2+[411] states are pointed out.


1964 ◽  
Vol 136 (4B) ◽  
pp. B1006-B1022 ◽  
Author(s):  
G. Bassani ◽  
Norton M. Hintz ◽  
C. D. Kavaloski

1978 ◽  
Vol 18 (2) ◽  
pp. 991-1002 ◽  
Author(s):  
N. A. Detorie ◽  
P. L. Jolivette ◽  
C. P. Browne ◽  
A. A. Rollefson

2016 ◽  
Vol 94 (5) ◽  
Author(s):  
H. Heylen ◽  
C. Babcock ◽  
R. Beerwerth ◽  
J. Billowes ◽  
M. L. Bissell ◽  
...  

2019 ◽  
Vol 204 ◽  
pp. 05005 ◽  
Author(s):  
R. N. Faustov ◽  
A. A. Krutov ◽  
A. P. Martynenko ◽  
F. A. Martynenko ◽  
O. S. Sukhorukova

We calculate corrections of orders α4, α5, α6 to the (1S – 2S) fine structure interval in muonic hydrogen (μp), muonic tritium (μt) and muonic helium ion $$((\mu _2^3He) + )$$. They are determined by the effects of vacuum polarization, nuclear structure and recoil and relativistic corrections. The nuclear structure effects are taken into account in terms of the charge radii of the nuclei in one-photon interaction and in terms of electromagnetic form-factors in the case of two-photon interaction. The obtained results for the (1S – 2S) splitting can be used for a comparison with future experimental data.


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