80 GeV?
It'd be 200 GeV of energy if they hit head on with the same speed. ymc^2=200 GeV -> y = 200 -> v=0.9999875 c in the original reference system. Then we Lorentztransform that with another 0.9999875 c. That gives 1 - 7.81261722 × 10^-11 c. That gives a y of 1 / sqrt(1 - (((0.9999875 + 0.9999875) / (1 + (0.9999875^2)))^2)) = 79 999.3998 = 80000, so the energy is 80000 GeV=80 TeV
80 TeV is right.
I calculated it with the four-momentum and the conservation of its inner product (note that c=1):
In the center of mass system the momentum is zero, and the energy is just the mass, so that the product is (400GeV)^2. This has to be conserved.
in the lab system the first particle has (E,p) and the second has (m=1GeV,0). Adding them together and taking the product results in E^2 + 2E*m + m^2 - p^2. E^2 - p^2 is m^2, resulting in 2m^2 which can be ignored, because they're small.
So because of the conservation:
(400GeV)^2 = 2E*m -> E = (400GeV)^2 / (2*1GeV) = 80 TeV
The last formula is for all highly relativistic collisions where the target is stationary. Because it is quadratic, the required energy rises fast compared to the case where two particles are colliding with the same speed, where it rises linearly with the energy.
Your turn.