The Laplace transform is defined as:
[tex]\mathcal{L}\lbrace f(t)\rbrace = \int_0^{\infty} e^{-st}f(t) dt[/tex]
Now, let's put in
[tex]f(t) = g(t) u(t-b)[/tex]
where u(t-b) is zero for t<b and 1 for t>b. Plugging this in:[tex]\int_0^{\infty} e^{-st}f(t) dt = \int_0^{\infty} e^{-st}g(t) u(t-b) dt[/tex]
Now split this integral into two parts:
[tex]\int_0^{\infty} e^{-st}g(t) u(t-b) dt = \int_0^{b} e^{-st}g(t) u(t-b) dt + \int_b^{\infty} e^{-st}g(t) u(t-b) dt[/tex]
The first integral vanishes, since u(t-b) is zero on the integration domain. In the second the u-function is simply 1. I'll let you solve the remaining steps.