ISSN:
1572-9540
Source:
Springer Online Journal Archives 1860-2000
Topics:
Physics
Notes:
Conclusion In Table 3 we have listed the Q values of165Ho and181Ta obtained by the pionic methods from this experiment and the one from Ebersoldet. al. and also the results by the muonic methods.4, 5 They are all in good agreements within the experimental uncertainties around 1%. The large discrepency between the Q values of181Ta from Ref. 5 and Ref. 7 was discussed and explained in detail in Ref. 5. The εo obtained in165Ho is comparable to the εo calculated by using the Kisslinger's potential. However, the experimental εo for181Ta from this experiment is 28% larger than the theoretical value by Scheck3 by using the perturbation method. As it was mentioned at the beginning of this paper that the strong interaction quadrupole effect introduces characteristic level broadening to each components of the multiplet. The excellent fit between the calculated composite curve with the observed experimental h.f.s. spectra could be obtained only by varying all three independent parameters Qeff, εo and Γo. Without Γo, or Γ2, no satisfactory fitting could be obtained. That this illustrates the intrigue strong quadrupole effects on each components of a multiplet do behave as predicted by Scheck.3
Type of Medium:
Electronic Resource
URL:
http://dx.doi.org/10.1007/BF01021813
