For the specified time operator, , because the derivatives of cancel between and . Expanding the derivatives of gives
For completeness, the extra derivative terms before simplification are . Substituting turns their derivative contribution into .
Applying to the original linear integral equation and using cancels its right side. Thus
Part (a) gives . Therefore the exact requested identity is
Since , this becomes homogeneous too. The same uniqueness argument gives ; it is not necessary to assume a separate uniqueness theorem for the differential time equation.

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