Directly integrating the definition, \(\mathcal{L}\{f(t-T)\} = \int_0^\infty f(t-T)e^{-st}\,dt\). Substituting \(\tau=t-T\) turns this into \(e^{-sT}\displaystyle\int_0^\infty f(\tau)e^{-s\tau}\,d\tau = e^{-sT}F(s)\).
The result can also be confirmed using the standard transform pair for a delayed unit step multiplying a delayed function, which is a cornerstone of Laplace transform tables. The rule states that delaying a time function by \(T\) is equivalent, in the s-domain, to multiplying the original transform by \(e^{-sT}\), because the exponential kernel \(e^{-st}\) itself picks up exactly this multiplicative factor whenever the time origin of the function is pushed forward by \(T\).
Therefore, the correct answer is \(e^{-sT}F(s)\).