If you consider the expression for the superposition of two uniform plane waves propagating symmetrically with respect to the z-axis, you will see that it contains a factor in the form of [tex]sin(\beta x \ cos\ \theta)[/tex]. This factor describes the the standing wave character (here, in the x-direction). When this factor is zero (i.e., when [tex]\beta x \ cos\ \theta =\ m\pi[/tex] where [tex]m = 0, 1, 2, 3, ...[/tex]) the electric field is, of course, also zero.
This is interesting because it means we can place two perfectly conducting sheets in the planes [tex]x = 0[/tex] and [tex]x = m\lambda /(2\ cos\ \theta)[/tex], without violating the boundary conditions (i.e., zero tangential electric field etc).
The fields will have m number of one-half apparent wavelengths in the x-direction between the plates.
This line of reasoning can be extended to a three-dimensional case where a quick glance at the field expressions for TE and TM waves will reveal why TM1,1 and TE1,0 or 0,1 are the lowest possible modes. Plug in m=n=0 for in the expression for TE waves or m = 0 or n = 0 for TM waves and see what happens.