The integration property of the Laplace transform states that if a function $f(t)$ is transformed into its Laplace form $F(s)$, then the integral of $f(t)$ from 0 to $t$ corresponds to a transformation in the Laplace domain given by $\frac{1}{s}F(s)$, where $F(s) = \mathcal{L}\{f(t)\}$. This property connects the process of integration in the time domain with multiplication by $\frac{1}{s}$ in the frequency domain, demonstrating how operations in one domain affect the other.
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