The square of momentum denoted by ² becomes important for relativistic dynamics where and when its directional invariance properties emerged as the velocity component approaches lightspeed. It appears within the physical definition of 4-vectors. This is an extension of the idea of vectors, which has so far considered to have only three spatial components, but now to include a time component. That is to say there will be vectors with four components, three of which are like the components of an ordinary vector; the fourth component is defined as the time component. If these 4-vectors are translated in a uniform linear motion then the time component is translated as a scalar quantity and these 4-vectors are then equivalent to the transformation of quaternion. On the other hand, if the 4-vectors undergo rotational Lorentz transformation such that the space-time interval remains a relativistic invariance, and which eventually provides a general covariance then the time component becomes the energy and the three space components become the three components of linear momentum.
Since relativistic geometry is now given as a Lorentzian hyperbolic non-Euclidean geometry, the square of the mass as the hypotenuse is given, not by the sum of the square of energy and momentum, but by their difference: ²²²=²-²² and if =1 then ²=²-². Solving for square of momentum gives ²=²-². This alternative formulation clearly suggests the scalar property of the square momentum, which is plausible only by constructing its corresponding quadratic form given by ²=Q(2)=(₂-₁)²=₁₁|₁|²₁₁+ ₂₂|₂|²₂₂-₁₂|₁||₂|₁₂-₂₁|₂||₁|₂₁ where |₂|=|₁|=, ₁₁= ₂₂=0° or 180°, ₁₂= ₂₁=90° or 270°, and ₁₁=₂₂=½ such that ²=½|₁|²+½|₂|² and orthogonality of ₂ and ₁ implies (₂-₁)²=(₁-₂)²=(₁+₂)² wherever and whenever expanded as their respective quadratic forms.


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