Design of the JINR four-meter isochronous cyclotron with smoothly regulated heavy-ion energies

1971 ◽  
Vol 30 (6) ◽  
pp. 635-640
Author(s):  
I. A. Shelaev ◽  
E. D. Vorob'ev ◽  
B. A. Zager ◽  
S. I. Kozlov ◽  
V. I. Kuznetsov ◽  
...  
1971 ◽  
Vol 93 (3) ◽  
pp. 557-561 ◽  
Author(s):  
I.A. Shelaev ◽  
E.D. Vorobiev ◽  
B.A. Zager ◽  
S.I. Kozlov ◽  
V.I. Kuznetsov ◽  
...  

2000 ◽  
Vol 62 (6) ◽  
Author(s):  
M. Bleicher ◽  
W. Greiner ◽  
H. Stöcker ◽  
N. Xu

Measurements are discussed in which the technique of accelerator mass spectrometry was applied to problems involving heavy radioisotopes. These measurements, which depend on the ion energies that can be reached with the new heavy-ion accelerator facilities, were performed at the Argonne tandem linac accelerator system (atlas) and at the unilac accelerator at GSI. The topics include a discussion of measurements of long nuclear lifetimes, of radioisotope detection of interest to solar neutrino experiments, and of a determination of the 41 Ca concentration in natural samples of terrestrial origin by m aking use of isotopic pre-enrichm ent in an isotope separator. A long-known m ethod of isobar separation, employing a gas-filled m agnetic field region, has been revived for some of these m easurem ents and its characteristics and advantages are briefly reviewed.


1971 ◽  
Vol 18 (3) ◽  
pp. 332-334
Author(s):  
I. A. Shelaev ◽  
E. D. Vorobiev ◽  
B. A. Zager ◽  
S. I. Kozlov ◽  
V. I. Kuznetsov ◽  
...  

1971 ◽  
Vol 31 (2) ◽  
pp. 851-852
Author(s):  
V. S. Alfeev ◽  
E. D. Vorob'ev ◽  
G. N. Zorin ◽  
Yu. I. Kharitonov

Vacuum ◽  
1995 ◽  
Vol 46 (8-10) ◽  
pp. 813-815
Author(s):  
AI Ivanenko ◽  
IV Kolesov

1988 ◽  
Vol 102 ◽  
pp. 339-342
Author(s):  
J.M. Laming ◽  
J.D. Silver ◽  
R. Barnsley ◽  
J. Dunn ◽  
K.D. Evans ◽  
...  

AbstractNew observations of x-ray spectra from foil-excited heavy ion beams are reported. By observing the target in a direction along the beam axis, an improvement in spectral resolution, δλ/λ, by about a factor of two is achieved, due to the reduced Doppler broadening in this geometry.


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