Keep the Courant number fixed and write . An exact solution of is . Substituting it into the update gives the defect
where and is evaluated at . The constant, first-derivative and second-derivative terms cancel. Dividing by gives a second-order consistency error. Hence for fixed , , the scheme has order two.
At the special value , the update reduces to . This is exactly the transport over two time steps, since , so the defect vanishes identically. With exact data at both starting levels it transports their values exactly; errors in those starting levels are still present, and the even and odd time subsequences evolve separately.
For a Fourier mode, the amplification polynomial is
Put and . The roots become
If , the square root is real, both roots have modulus one, and their separation is at least . The companion matrix has eigenvectors , so their uniform separation gives a mesh-independent bound on its powers. By power boundedness of a two-level Fourier scheme and the discrete Fourier transform, this proves stability for .
If , choose . The roots have product of modulus one and unequal moduli, so one has modulus greater than one. The scheme is unstable.
The boundary cases require more than a root-modulus check. At , gives , while gives . The companion matrices have nontrivial Jordan blocks and solutions of the form . Their linear growth rules out a uniform stability bound. This mode occurs on even periodic grids, which are enough to disprove mesh-uniform stability at the endpoints.
Therefore the stable range is exactly
Within this range, second-order convergence additionally requires two appropriately accurate starting time levels. The unit-modulus parasitic root near does not decay, so poor initialization cannot be repaired by the scheme.

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