I know that the Lorentz transform, when two frames $\mathcal{S}$ and $\mathcal{S}'$ are in standard configuration (the axes are all parallel to their counterparts in the other inertial frame) is given by
$$L~=~\left( \begin{array}{cccc} \gamma & \beta \gamma & 0 & 0 \\ -\beta \gamma & \gamma & 0 & 0 \\ 0 & 0 & 1 & 0 \\ 0 & 0 & 0 & 1 \end{array} \right)$$
Is the definition of the Lorentz transform actually just
$$L^T\cdot \eta \cdot L=\eta$$
Where $\eta=\text{diag}(-1,1,1,1)$? I am trying to find a fundamental definition of the Lorentz transformation so I can show that some transformations are LTs, e.g. an ordinary rotation is obviously a Lorentz transformation but I'd like to show this explicitly and without any reference to the Lorentz group if possible. Is the defintion simply: a transformation in Minkowski space that preserves the length of 4-vectors under the Minkowski scalar product? If so then it would be easy.