Understanding the Center of Mass Energy in Fixed Target vs. Collider Experiments

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The discussion focuses on deriving expressions for center of mass energy in fixed target versus collider experiments. In fixed target experiments, the derived expression involves the momentum 4-vectors of the beam and target particles, leading to a formula that suggests a relationship between the beam and target masses. The textbook's claim that this expression simplifies to a form assuming equal masses raises questions about its validity under different mass conditions. Similarly, in collider experiments, the center of mass energy expression assumes equal energies for the colliding particles, which prompts skepticism about the general applicability of the approximation. Overall, the discussion highlights the need for clarity on the assumptions made in these derivations.
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Homework Statement


While not explicitly a homework question, I am having some trouble with deriving expressions for the center of mass energy in a fixed target experiment versus a collider experiment. The question is effectively, "Derive an expression for the center of mass energy in a fixed target experiment and compare this to the center of mass energy in a collider experiment."

Homework Equations


The momentum 4-vector. Also, the formula for center of mass energy ##\sqrt{s}=\sqrt{(p_1+p_2)^2}##.

The Attempt at a Solution


For a fixed target experiment, we have the two momentum 4-vectors, ##(\frac{E_b}{c},p_b)##, and ##(m_tc,0)##, for the beam particle and target particle respectively. Then, $$s=\frac{E_b^2}{c^2}+m_t^2c^2+2E_bm_t-p_b^2.$$

We can group the first and last term together to obtain ##m_b^2c^2+m_t^2c^2+2E_bm_t##. However, my textbook at this point claims that this is equivalent to ##2m^2c^2+2Em##. My question is then, would this not only hold true for ##m_b\approx m_t##?

Similarly, for a collider experiment, we have, ##s=(\frac{E_A}{c}+\frac{E_B}{c})^2\rightarrow s=\frac{(E_A+E_B)^2}{c^2}##. Again, my textbook claims that this is equivalent to ##\frac{4E^2}{c^2}##, which again I think, should only hold true for ##E_A\approx E_B##.

If I am not understanding incorrectly, why can these approximations be made?
 
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They indeed seem to be assuming the masses to be equal.
 

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