{"title":"Uniqueness of 56Fe as a primary standard for atomic masses","authors":"A. Durnford","doi":"10.1088/0305-4470/5/10/005","DOIUrl":null,"url":null,"abstract":"A recent evaluation of atomic masses confirms that 56Fe has uniquely the 'least' atomic mass per baryon, ZAM/A. Thus, with 56Fe as the primary standard (2656M=56) all other atomic masses would be greater than the mass number A and the corresponding 'mass excesses' would be not only 'positive' but also 'maxima'. Moreover, a mass excess relative to 56Fe is potentially the largest 'portion' of the atomic mass that can be transformed into energy (assuming conservation of baryon number); it therefore has a unique physical significance. Accordingly, a plot of the mass excesses against A and Z would provide a unique 'potential-energy surface' which should be useful in the representation of nuclidic transformations that involve a change in A(eg alpha decay) as well as those with A=constant.","PeriodicalId":54612,"journal":{"name":"Physics-A Journal of General and Applied Physics","volume":"12 1","pages":""},"PeriodicalIF":0.0000,"publicationDate":"1972-10-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"Physics-A Journal of General and Applied Physics","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1088/0305-4470/5/10/005","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
引用次数: 0
Abstract
A recent evaluation of atomic masses confirms that 56Fe has uniquely the 'least' atomic mass per baryon, ZAM/A. Thus, with 56Fe as the primary standard (2656M=56) all other atomic masses would be greater than the mass number A and the corresponding 'mass excesses' would be not only 'positive' but also 'maxima'. Moreover, a mass excess relative to 56Fe is potentially the largest 'portion' of the atomic mass that can be transformed into energy (assuming conservation of baryon number); it therefore has a unique physical significance. Accordingly, a plot of the mass excesses against A and Z would provide a unique 'potential-energy surface' which should be useful in the representation of nuclidic transformations that involve a change in A(eg alpha decay) as well as those with A=constant.