As written in Wikipedia, the Dirac delta function is the derivative of the Heaviside function $${\displaystyle \delta (x)={\frac {d}{dx}}H(x)}$$ Hence the Heaviside function can be considered to be the integral of the Dirac delta function$$ {\displaystyle H(x):=\int _{-\infty }^{x}\delta (s)\,ds}$$ In this context, the Heaviside function is the cumulative distribution function of a random variable which is almost surely $0$.
I would like to show that the Heaviside function is a càdlàg adapted process of finite variation. Could you please help me?