Download e-book for kindle: Kernreaktionen III / Nuclear Reactions III by D. E. Alburger, I. Perlman, J. O. Rasmussen, Earl K. Hyde,

By D. E. Alburger, I. Perlman, J. O. Rasmussen, Earl K. Hyde, Glenn T. Seaborg, George R. Bishop, Richard Wilson, S. Devons, L. J. B. Goldfarb, R. J. Blin-Stoyle, M. A. Grace

ISBN-10: 3642458785

ISBN-13: 9783642458781

ISBN-10: 3642458807

ISBN-13: 9783642458804

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Extra resources for Kernreaktionen III / Nuclear Reactions III

Sample text

The data of nuclear isomers were compiled and reviewed in 1952 by GOLDHABER and HILL [Go 52J (see also [Ko 54a]). In addition to their critical analysis of a large amount of well-established information they pointed out numerous problems such as uncertain mass assignments and doubtful information on the levels in many of the isotopes. During the intervening years some of the outstanding problems have been solved and many new isomeric states have been discovered. In this section data on nuclear isomers are presented based on information available up to about the end of 1955 1 .

This results in K lines which are broader than the individual L lines. e. the K line, being of lower energy, may be more seriously affected by scattering in the source than the L electron lines. In all cases where variations in line width are present one must either find the areas under the curves or make other suitable corrections. To a first approximation the product of peak height by the line half-width in percent is proportional to the intensity. Areas may be found in two equivalent ways. If the spectrum is plotted as spectrometer yield versus momentum the area under each peak is measured with, for example, a planimeter and divided by the momentum value at the center of the line.

General remark on delayed coincidence and time-channel methods. In an actual experimental measurement of a half-life using the delayed coincidence, time-channel or triggered oscilloscope methods it is desirable to select the resolving time or channel width so as to obtain the optimum data, if only a single channel point is recorded at a time. Consider for example, a half-life measurement of a 100 ILsec isomeric state using a time-channel analyzer with a single sliding channel. Adjusting the channel width to only 5 or 10 ILsec would mean that a relatively small number of counts would be recorded in a given time at each delay setting.

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Kernreaktionen III / Nuclear Reactions III by D. E. Alburger, I. Perlman, J. O. Rasmussen, Earl K. Hyde, Glenn T. Seaborg, George R. Bishop, Richard Wilson, S. Devons, L. J. B. Goldfarb, R. J. Blin-Stoyle, M. A. Grace


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