Abstract

with q2 n = q2 nx + q2 ny + q2 nz and n = 1,2, . . . . After Eq. (4) the symbols qx , qy , and qz should be replaced by qnx , qny , and qnz, respectively. The changes do not affect the numerical calculations presented in Sec. V performed at qnx = 0 for the generic nth backward modes that have a qny component much larger than qnx . The article J. Jorzick, S. O. Demokritov, C. Mathieu, B. Hillebrands, B. Bartenlian, C. Chappert, F. Rousseaux, and A. N. Slavin, Phys. Rev. 60, 15194 (1999) is cited twice, both as Ref. 12 and as Ref. 15.

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