This is a follow-up to this previous question. We are encouraged to use 4-vectors to solve these types of problems:
Decay kinematics using 4-vectors. Here we look at the kinematics of particle decays and how 4-vectors can simplify this type of problem quite considerably. The point here is to use energy-momentum 4-vectors.
I am trying to solve the same problem using the exact same recipe that was used to solve this problem using four-vectors, namely,
A particular centre-of-mass energy is needed to create a new particle. We will do the calculation in a so-called fixed-target configuration (a) and in a collider configuration (b).
(a) A particular centre-of-mass energy is needed to create a new particle. We will do the calculation in a so-called fixed-target configuration.
A particle of mass $m_1$ and total energy $E_1$ in the lab frame hits a stationary particle of mass $m_2$. Show that the required particle energy for a given $s$ is:
$$E_1=\frac{s-{m_1}^2c^4-{m_2}^2c^4}{2m_2c^2}$$ where $s$ is the square of the centre-of-mass energy. This is often called a ‘fixed target’ configuration as experiments were historically often done by colliding a beam of particles with a stationary target material.
Let $P_1$ be the four-momentum of incident particle 1.
Let $P_2$ be the four-momentum of stationary particle 2.
Let $P_T$ be the four-momentum of the centre of mass energy $\sqrt{s}$.
$P_1=\left(E_1, {\bf p_1}c\right)=\left(E_1,p_1^{x}c,0,0 \right)\qquad\text{(as these problems are all 1D)}$
$P_2=\left(E_2, {\bf 0}\right)=\left(m_2c^2,0,0,0 \right)\qquad\text{(as particle 2 is the fixed-target)}$
$P_T=\left(\sqrt s,{\ p_Tc}\right)=\left(m_Tc^2, p_T^xc, 0, 0 \right)$
In the center of momentum frame, the relevant 4-momentum conservation is
$$\begin{align}P_T &=P_1+P_2 \\&\implies {P_1}^2+2P_1\cdot P_2+{P_2}^2={{P_T}}^2\\&\implies \color{blue}{{m_1}^2c^2}-2E_1m_2c^2+\color{blue}{{m_2}^2c^2}=\color{blue}{{m_T}^2c^2}=\frac{s}{c^2}\end{align}$$
Where in the last step I have replaced the 4-vector norms by the invariant masses (marked in blue) and noting that $s={m_T}^2c^4$.
On rearrangement I get:
$$E_1=\frac{s-{m_1}^2c^4-{m_2}^2c^4}{2m_2c^4}$$
But this is not the correct result:
$$E_1=\frac{s-{m_1}^2c^4-{m_2}^2c^4}{2m_2c^2}$$
Am I making a mistake here? Or can this relation simply not be derived using 4-vectors?
If it can't be derived using 4-vectors then please explain why.
Many thanks.
EDIT:
I've just realised something: While $P_1$ & $P_2$ are four-vectors representing a physical particle, however, above I write that "Let $P_T$ be the four-momentum of the centre of mass energy $\sqrt{s}$." Is it really plausible to define a four-vector for a system of particles?