The C=O length is invariant under every operation, so its stretch is . If are the two C–H bond-length changes, their sum and difference give
Hence . These are stretching symmetry coordinates; the two motions can mix in actual normal modes, and mass-weighted atomic motions need not have the schematic arrow lengths below.
Figure 1.
Original formaldehyde stretching symmetry sketches in the paper's plane
. Details.

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