A perfectly inelastic central collision of two equal relativistic particles whose kinetic energies are equal to their resting energies results a single relativistic particle (and nothing but it). The mass of the resulting particle is greater than the sum of the masses of the particles that collided, but why and how?
2 Answers
In relativity the mass of a system is $$m^2 c^2 = E^2/c^2 - p^2$$ For a system of multiple parts you add the $E$ for each part and the $\vec p$ for each part to get the $E$ and $\vec p$ for the whole system. Then you find the resulting $m$ for the system using the formula above.
So for $(E,\vec p) = (E_1 + E_2,\vec p_1+ \vec p_2)$ we have $$m^2 c^2 = E^2/c^2 - p^2 = (E_1+E_2)^2/c^2-|\vec p_1 + \vec p_2|^2$$$$>(E_1{}^2/c^2-p_1{}^2)+(E_2{}^2/c^2-p_2{}^2)=m_1{}^2 c^2 + m_2{}^2 c^2$$
So the mass of a system is always greater than the sum of the masses of the parts. This is just the triangle inequality $A^2+B^2>C^2$ from the Pythagorean theorem, but modified for spacetime.
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(An extension of my original comment)
If you draw an energy-momentum diagram of the totally-inelastic collision (using the conservation of total 4-momentum), you get a triangle with future-timelike legs.
This is similar to the spacetime diagram of the clock-effect/twin-paradox, where the total proper time of the traveling twin between the separation and reunion events is less than that of the inertial twin.
Possibly useful: my answer https://physics.stackexchange.com/a/318858/148184 to Mass Addition in Special Relativity
Ultimately, it's due to the "reverse-triangle inequality" property of Minkowski spacetime. See, for instance, my answer to Is there a space-like equivalent of the Twin Paradox? (I see @Dale made a similar comment.)
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