Harmonic oscillations are isochronous, but so are oscillations in any potential that is shear-equivalent to a harmonic potential. We demonstrate the converse: that every possible isochronous potential is shear-equivalent to a harmonic potential. To do this we show that every potential is shear-equivalent to a unique symmetric potential, and that every isochronous symmetric potential is harmonic. Shearing is thus the only possible period-preserving transformation for potentials with fixed energy.

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We do not demand a positive concavity: the potential could have a vanishing second derivative at its minimum. While we do not explicitly consider the unlikely case of a vanishing second derivative on a neighborhood of the minimum (a horizontal line segment), the argument can be extended to cover this case with minor modification.
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The maxima in between them could be symmetrized as well.
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