By A. Rytz, B. Grennberg, D. J. Gorman (auth.), J. H. Sanders, A. H. Wapstra (eds.)
The convention on Nuclear lots and their choice which used to be held on the Max Planck I nstitute in Mainz from 10 to twelve July 1956 ended in the formation through the foreign Union of natural and utilized Physics of a fee on Atomic plenty and similar Constants. less than the auspices of this fee meetings masking those topics have been held in Hamilton, Ontario (12-16 September, 1960), in Vienna (15-19 July 1963) and in Winnipeg (28 August-1 September 1967). After the final of those meetings the fee felt that the placement relating to nuclear plenty was once kind of strong and that to that end the elemental constants may still get extra emphasis in destiny meetings. hence they have been very happy to simply accept a suggestion from the nationwide actual Laboratory to just accept the most burden of organizing the Fourth foreign convention on Atomic lots and primary Constants. An Organizing Committee used to be appointed with the contributors: J. H. Sanders, Chairman B. W. Petley, Secretary A. Horsfield, Treasurer P. Dean A. H. Wapstra. They have been assisted by means of a application Committee which include: A. H. Wapstra, Chairman E. R. Cohen A. Horsfield W. H. Johnson, Jr. J. H. Sanders J. Terrien.
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Additional resources for Atomic Masses and Fundamental Constants 4: Proceedings of the Fourth International Conference on Atomic Masses and Fundamental Constants held at Teddington England September 1971
5 mm wide strips and a shift in the distance scale computed for each strip to compensate for the change in outgoing momentum with the change in angle. Counts were added from as many of these shifted strips as needed to give statistical accuracy. It is an advantage of the single focussing broad range spectrograph that kinematic broadening may be greatly reduced by this procedure. The procedure in the 12C measurement 1s essentially the same as that used for 24Mg and the sources of errors are similar.
This again emphasizes the importance of the ENERGY DETERMINATIONS IN MEDIUM AND ilEAVY NUCLEI 41 contribution of the source to resolution. As will be evident later such a poor line shape would make it difficult to correct for the effect of finite target thickness. Instrumentation has since been developed to allow continuous monitoring of the source size and position during experimental runs. For precision nuclear spectroscopy it is essential that the magnetic field rather than the current of each of the magnets be regulated and that hysteresis and saturation effects, hopefully small, are known.
1-MeV excitation energy measured against the two scales are seen to agree well, within the rather large uncertainties. The more accurate measurement of the excitation energy of the 11B state has just been done at Notre Dame by Browne and Stocker . The GAMMA RAY ENERGY VS. PARTICLE ENERGY MEASUREMENTS 17 TABLE IT Excitation energy from particle measurement vs. gamma ray measurement. 1 ± 1. 1 ± 1. 0 ± 1. 9 of level separations h b See text Ref. . c See text Ref. . See text Ref. . R. F.