(16) rv = (r′v + qt′)/√(1 - ),

r = r′,

t = (qr′v + t′)/√(1 - ),

Now we shall make a very important observation about the vectors u and u′. We can again introduce the indices 1, 2, 3, 4, so that we write (x₁′, x₂′, x₃′, x₄′) instead of (x′, y′, z′, it′) and ρ₁′, ρ₂′, ρ₃′, ρ₄′ instead of (ρ′u′{x′}, ρ′u′{y′}, ρ′u′{z′}, iρ′).

Like the rotation round the Z-axis, the transformation (4), and more generally the transformations (10), (11), (12), are also linear transformations with the determinant + 1, so that

(17) x₁² + x₂² + x₃² + x₄² i. e. + + - ,

is transformed into

x₁′² + x₂′² + x₃′² + x₄′² i. e. x′² + y′² + z′² - t′².

On the basis of the equations (13), (14), we shall have (ρ₁² + ρ₂² + ρ₃² + ρ₄²) = ρ²(1 - u, -u, -u) = ρ²(1 - ) transformed into ρ²(1 - ) or in other words,

(18) ρ√(1 - )