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Barber, R. C., N. N. Greenwood, A. Z. Hrynkiewics, Y. P. Jeanin, M. Lefort, M. Sakai, I. I. Uleuhla, A. H. Wapstra, and D. H. Wilkinson. Prog. Part. Nucl. Phys. 29, 453 (1992). Druin, V. A., A. G. Demin, Yu. P. Kharitonov, G. N. Akap ev, V. I. Rud, G. Y. Sung-Chin-Yang, L. P. Chelnokov, and K. A. Gavrilov. Yad. Fiz. 13, 251 (1971). Folden, C. M. et al. Phys. Rev. Lett. 93, 212702 (2004). Ghiorso, A., M. Nurmia, J. Harris, K. Eskola, and P. Eskola. Phys. Rev. Lett. 22, 1317 (1969). Ghiorso, A., M. Nurmia, K. Eskola, J. Harris, and P. Eskola. Phys. Rev. Lett. 24, 1498 (1970). Ghiorso, A., J. M. Nitschke, J. R. Alonso, C. T. Alonso, M. Nurmia, G. T. Seaborg, E. K. Hulet, and R. W. Lougheed. Phys. Rev. Lett. 33, 1490 (1974). Ghiorso, A., et al. Nucl. Phys. A583, 861 (1995a). Ghiorso, A., et al. Phys. Rev. C51, R2293 (1995b). Gilchriese, M., A. Sessler, G. Trilling, and R. Vogt. Lawrence Berkeley National Laboratory Report, LBNL-51773 (2003). Ginter, T. N., et al. Phys. Rev. C 67, 064609 (2003). Gregorich, K. E., M. R. Lane, M. F. Mohar, D. M. Lee, C. D. Kacher, E. R. Sylwester, and D. C. Hoffman. Phys. Rev. Lett. 72, 1423 (1994). Gregorich, K. E., et al. Eur. Phys. J. A 18, 633 (2003). Hofmann, S. Rep. Prog. Phys. 61, 639 (1998). Hofmann, S., and G. Munzenberg. Rev. Mod. Phys. 72, 733 (2000).

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Stretching constants have the dimension N/m or N/cm. In the latter case, the same numerical value is obtained as with the dimension mdyn/a, which continues to be used. A dimension of deformation constants is N.cm/rad2. However, deformation constants are often given in the same dimension as stretching constants. In this case the dimension is adjusted by dividing it by I cm2/rad2. If two different coordinates (ri and 1',) occur in one potential energy term, interaction force constants are obtained. Their value differs from zero if distortions in one coordinate I'; change the equilibrium position in rJ. The mathematical procedures for the calculation of force constants are described in Section 5.2 of this book. For calculations involving small (triatomic) species, the book by Fadini and Schnepel (1985) is recommended. A review covering force constant calculations has been presented by Becher (1968). In this chapter only relevant aspects are discussed. Force constant calculations mainly rely on correct assignments of the observed frequencies. These are compared with calculated frequencies, which can be obtained, for example, by the Wilson method (Wilson et al., 1955). First, the G-matrix based on the known or an assumed geometry is calculated. The eigenvalues (frequencies) of the vibrations for different sets of force constants are then calculated. Their values are derived mostly from the force constants of similar species. Since the measured frequencies can be reproduced with an infinite number of sets of force constants, additional experimentally

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