{"title":"作为原子质量主要标准的56Fe的独特性","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":"{\"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}","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}
Uniqueness of 56Fe as a primary standard for atomic masses
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.