Given $f:\Bbb R^n \to \Bbb R$. Let $\hat{f} = \mathcal{F}(f)$ be its Fourier transform. The inverse Fourier transform of $\hat{f}$ is defined as: $$ [\mathcal{F}^{-1}(\hat{f})](x) =\frac{1}{(2\pi)^{n/2}} \int_{\Bbb R^n}\hat{f}(\xi)\exp(i \xi \cdot x)\,d\xi $$
Further, if $f \in L^1(R^n)$ such that $\hat{f} \in L^1(\Bbb R^n)$ then $f=\mathcal{F}^{-1}(\hat{f})$ a.e. in $\Bbb R^n$.
Let $\hat{f}:\Bbb R^n \to \Bbb R$ be defined as: $$ \hat{f}(\xi)=\frac{1}{(2\pi)^{n/2}}\frac{1}{\lambda+|\xi|^2} $$ with $\lambda >0$.
Prove that: $$ f(x) = \mathcal{F}^{-1}(\hat{f}) = \int_0^{\infty}\exp(-\lambda t)(4\pi t)^{-n/2}\exp(-\frac{|x|^2}{4t})\,dt $$
Attempt: I applied the inverse Fourier transform to $\hat{f}$ but didn't know where the $t$ in the question came from.