For a scheme
the Fourier ansatz gives the amplification polynomial
Its roots are the amplification factors of that Fourier mode.
Centered space and leapfrog time discretization of gives
Its amplification polynomial is . The two roots have unit modulus for , but a repeated unit root at equality violates the uniform root condition.
Applying a centered leapfrog step in time and the centered second difference in space to gives
For every , each nonconstant Fourier mode has an amplification root of modulus greater than one, so the scheme is unconditionally unstable.

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