Lorentz transformation lab to CM system

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The discussion focuses on the Lorentz transformation needed to convert from the lab frame to the center of mass (CM) frame in particle reactions. The velocity of the CM is derived from the momenta of the two particles, leading to a specific Lorentz transformation matrix. The transformation is defined to ensure that the total momentum in the CM frame is zero, which is a fundamental requirement. The equations presented show how to apply the transformation to the four-momenta of the particles, ultimately confirming that the total momentum in the CM frame is indeed zero. This establishes the correctness of the transformation and its physical significance in particle physics.
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Which Lorentz transformation takes the lab system to the CM system?

Lab system: p_a = (E^{lab}_a, \vec{p}_a) and p_b = (m_b, \vec{0})
CM system: p_a = (E^{CM}_a, \vec{p}) and p_b = (E^{CM}_b, -\vec{p})

For a binary reaction a+b->c+d, the textbooks I have say quite a lot about the kinematics of such reactions (Mandelstam variables and all that) but how do I go about doing a Lorentz transformation between the lab and CM system? That must be possible to do.
 
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Anyone?
 
The velocity of CM in the scattering of two particles with rest mass m_1 and m_2 is given by

\vec{u}_{CM}=\frac{\vec{p}_1+\vec{p}_2}{E_1+E_2}\,c^2

from which you can find the Lorentz transformation.
 
So a lorentz transformation from the lab frame to the CM frame would be
<br /> \left[ \begin{array}{cccc} \gamma &amp; -\beta \gamma &amp; 0 &amp; 0 \\ -\beta \gamma &amp; \gamma &amp; 0 &amp; 0 \\ 0 &amp; 0 &amp; 1 &amp; 0 \\ 0 &amp; 0 &amp; 0 &amp; 1 \end{array} \right]<br />
with \beta = ||\vec{u_{CM}}|| and \gamma = (1-\beta^2)^{-1/2}?
It doesn't make any sense to me.
 
It doesn't make any sense to me.

The crusial thing is to make sense in nature, not to any of us.
First system of center of mass for two particles is defined by the requirement, that (\vec{p}_1+\vec{p}_2)_{CM}=0. The general Lorentz transormation (c=1) is

\Lambda=\begin{pmatrix} \gamma&amp; \gamma\,\vec{\beta} \cr \gamma\,\vec{\beta} &amp; \delta_{\alpha\beta}+\frac{\gamma-1}{\beta^2}\,\beta_\alpha\,\beta_\beta \end{pmatrix}

Take now the 4-vector p^\alpha_1=(E_1,\vec{p}_1) and apply \Lambda with \beta=\frac{\vec{p}_1+\vec{p}_2}{E_1+E_2}, to get for the 3-momentum \vec{P}_1,\,\vec{P}_2 to the CM system:

\vec{P}_1=\Lambda\,\vec{p}_1\Rightarrow \vec{P}_1=\gamma\,\left(E_1+\frac{\gamma}{\gamma+1}\,\vec{\beta}\,\vec{p}_1\right)\,\vec{\beta}+\vec{p}_1[/itex]<br /> \vec{P}_2=\Lambda\,\vec{p}_2\Rightarrow \vec{P}_2=\gamma\,\left(E_2+\frac{\gamma}{\gamma+1}\,\vec{\beta}\,\vec{p}_2\right)\,\vec{\beta}+\vec{p}_2[/itex]&lt;br /&gt; &lt;br /&gt; Adding now the two equations we get&lt;br /&gt; &lt;br /&gt; \vec{P}_1+\vec{P}_2=\gamma\,\left(E_1+E_2+\frac{\gamma}{\gamma+1}\,\vec{\beta}\,(\vec{p}_1+\vec{p}_2)\right)\,\vec{\beta}+\left(\vec{p}_1+\vec{p}_2\right)\Rightarrow \vec{P}_1+\vec{P}_2=\gamma\,\left(E_1+E_2+\frac{\gamma}{\gamma+1}\,\vec{\beta}\,(E_1+E_2)\,\vec{\beta}\right)\,\vec{\beta}+\left(E_1+E_2\right)\,\vec{\beta}\Rightarrow&lt;br /&gt; \vec{P}_1+\vec{P}_2=\gamma\,(E_1+E_2)\,\left(1+\frac{\gamma}{\gamma+1}\,\beta^2\right)\,\vec{\beta}+\left(E_1+E_2\right)\,\vec{\beta}\Rightarrow \vec{P}_1+\vec{P}_2=0&lt;br /&gt; &lt;br /&gt; Now does it makes sense?
 
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