For every test function and nonzero , substitution with the orientation handled by gives
Hence the Dirac delta scaling identity is .
The derivative of a distribution is defined by integration by parts. Therefore
For a compactly supported test function ,
Thus this is the distributional derivative of the Heaviside step function: .
For both inputs vanish. Eliminating gives , and the data at give
For all , differentiating the first equation and using the second gives
Thus is continuous at zero while jumps by one. For the resulting solution is
Since , this is
where
Thus , , and the sketch of is a downward unit step at .

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