We propose that the odd-frequency wave ( wave)
superconducting gap function, which is usually unstable in the bulk, naturally
emerges at the edge of wave superconductors. This prediction is based on
the surface spin fluctuation pairing mechanism owing to the zero-energy surface
Andreev bound state. The interference between bulk and edge gap functions
triggers the state, and the generated spin current is a useful
signal uncovering the hidden'' odd-frequency gap. In addition, the edge $s^{\rm{odd}}$ gap can be determined via the proximity effect on the diffusive normal metal. Furthermore, this study provides a decisive validation of the Hermite odd-frequency gap function,‘’ which has been an open fundamental
challenge to this field.

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