Undergrad Head-on collision of an electron and a proton

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In a head-on collision between an electron and a proton, the energy available for the reaction can be calculated using the invariant mass formula, where s is defined as the square of the total four-momentum. The equation includes the term 1 - cos(θ) to account for the angle between the particles' trajectories, with θ being zero in a head-on collision. The presence of 1 in the equation arises from the temporal components of the four-momenta, indicating that both particles are moving in the same direction at the same speed. This distinction is crucial for accurately determining the energy and momentum in particle collisions. Understanding these concepts is essential for analyzing high-energy physics interactions.
Philip Land
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Hey!

Let's say we have an electron and proton colliding head-on.

We will have ##|p| \sim E##

Where ##p_1=(E_1, \vec{p_1})## &##p_2=(E_2, \vec{p_2})##

If we want the available energy. We can calculate ##\sqrt{s} = \sqrt{(p_1 + p_2)^2}##

We get $$s= p_1^2 + p_2^2 + 2p_1p_2 = m_e^2 + m_p^2 + 2E_1E_2(1-cos(\theta)).$$

My question is why we get ##1-cos(\theta)## and not just ##cos(\theta)## which is one since the angle is zero?
 
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Philip Land said:
Let's say we have an electron and proton colliding head-on.
Philip Land said:
My question is why we get ##1-cos(\theta)## and not just ##cos(\theta)## which is one since the angle is zero?
How do you define the angle?
 
The 1 is from the temporal components of the 4-momenta.
 
An angle of zero means the particles fly in the same direction with the same speed.
 

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