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Lorentz Transformations

These transformations ensure that the laws of physics are the same in all inertial frames.
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The statement of the theorem

For two inertial frames SS and SS' moving relative to each other with a constant relative velocity v\mathbf{v}, the transformation of coordinates xμ=(ct,x,y,z)x^{\mu} = (ct, x, y, z) is given by the Lorentz transformation matrix Λμν\Lambda^{\mu}{}_{\nu}:\nxμ=Λμνxνx'^{\mu} = \Lambda^{\mu}{}_{\nu} x^{\nu} \nFor a boost along the xx-axis, the matrix elements are:\nΛ=(γγβ00γβγ0000100001)\Lambda = \begin{pmatrix} \gamma & -\gamma \beta & 0 & 0 \\ -\gamma \beta & \gamma & 0 & 0 \\ 0 & 0 & 1 & 0 \\ 0 & 0 & 0 & 1 \end{pmatrix} \nWhere β=v/c\beta = v/c and γ=11β2\gamma = \frac{1}{\sqrt{1 - \beta^2}}.
Source: Wikipedia