Eigenmodes for the quadratic-finite-element method (QFEM) are expressed as
a linear combination of two conventional semi-discrete Fourier modes. Each
of these Fourier modes moves at a different phase speed, but both modes hav
e the same group velocity. This representation of the QFEM eigenmodes clari
fies the significance of the negative phase speeds that naturally arise as
part of the conventional analysis. (C) 2000 Academic Press.