In mathematics, the inverse Laplace transform of a function ${\displaystyle F}$ is a real function ${\displaystyle f}$ that is piecewise-continuous, exponentially-restricted (that is, ${\displaystyle |f(t)|\leq Me^{\alpha t}}$ ${\displaystyle \forall t\geq 0}$ for some constants ${\displaystyle M>0}$ and ⁠${\displaystyle \alpha \in \mathbb {R} }$⁠) and has the property:

where ${\displaystyle {\mathcal {L}}}$ denotes the Laplace transform.

It can be proven that, if a function ${\displaystyle F}$ has the inverse Laplace transform ⁠${\displaystyle f}$⁠, then ${\displaystyle f}$ is uniquely determined (considering functions that differ from each other only on a point set having Lebesgue measure zero as the same). This result was first proven by Mathias Lerch in 1903 and is known as Lerch's theorem.

The Laplace transform and the inverse Laplace transform together have a number of properties that make them useful for analysing linear dynamical systems.

There is an integral formula for the inverse Laplace transform, called the Bromwich's inversion formula and is given by the line integral:

where the integration is done along the vertical line ${\displaystyle {\textrm {Re}}(s)=\gamma }$ in the complex plane such that ${\displaystyle \gamma }$ is greater than the real part of all singularities of ${\displaystyle F}$ and ${\displaystyle F}$ is bounded on the line, for example if the contour path is in the region of convergence.

In the common special case where all singularities, ⁠${\displaystyle s_{k}}$⁠, satisfy ${\displaystyle \Re (s_{k})<0}$ (i.e., lie in the open left half‑plane), or ${\displaystyle F}$ is an entire function, then ${\displaystyle \gamma }$ can be set to zero and the above inverse integral formula becomes identical to the inverse Fourier transform.

In practice, computing the complex integral can be done by using the Cauchy residue theorem.