What is the Correct Factor in the Kinematics of Two Body Decay?

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SUMMARY

The discussion focuses on the kinematics involved in the two-body decay process represented by the equation ## B \to l \nu ##. A critical factor in the matrix element amplitude is identified as ##| \bar{l} (1-\gamma_5)\nu|^2##, which simplifies to ##8 p_l \cdot p_\nu## after taking the trace. The error in the original calculation stems from incorrectly equating the energies of the lepton and neutrino, while their momenta are equal. The correct expressions for the energies of the lepton and neutrino are derived, emphasizing the importance of distinguishing between energy and momentum in decay kinematics.

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Safinaz
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Hi there,

In a two body decay process like ## B \to l \nu ##, there is a factor ##| \bar{l} (1-\gamma_5)\nu|^2 ## in the matrix element amplitude, in which equals

##| \bar{l} (1-\gamma_5)\nu|^2 = (/\!\!\! p_l+m_l) (1-\gamma_5) /\!\!\! p_\nu(1+\gamma_5) = 2(/\!\!\! p_l+m_l) /\!\!\! p_\nu(1+\gamma_5) = 8 p_l. p_\nu ~##(1) , after taking the trace.

To evaluate (1) I set the process kinematics as

## p_l = ( E_l,\bf{p_l}) ## and ## p_\nu= ( E_\nu,- E_\nu) ##, where

## -E_\nu = -\bf{p_\nu} \equiv - \bf{p_l}, ~ \bf{p_l}^2= E_l^2 - m_l^2, ~ E_l =E_\nu = m_B/2##, then

## p_l. p_\nu = E_l E_\nu +\bf{p_l}^2 = 2E_l^2 - m_l^2 = m_B^2/ 2 - m_l^2 = m_B^2/ 2 ( 1 - \frac{2m_l^2}{m_B^2}) ##, so I got a factor
## ( 1 - \frac{2m_l^2}{m_B^2}) ##, while in references as [hep-ph/0306037v2] equ. 5, (1) gave a factor ## ( 1 - \frac{m_l^2}{m_B^2}) ## instead,
So what's wrong I made?

Bests.
 
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Let's start with the kinematics. In the rest frame of the decaying B meson you have
$$p_l=(E_l,\vec{p}), \quad p_{\nu}=(E_{\nu},-\vec{p}).$$
This means
$$s=(p_l+p_{\nu})^2=m_{B}^2$$
but
$$s=m_B^2=m_l^2+m_{\nu}^2+2 p_l \cdot p_{\nu},$$
which gives
$$2 p_l \cdot p_{\nu}=m_B^2-m_l^2-m_{\nu}^2 \simeq m_B^2-m_l^2=m_B^2 \left (1-\frac{m_l^2}{m_B^2} \right).$$
Your mistake is setting ##E_l## and ##E_{\nu}## equal. However the magnitudes of the momenta are equal, not the energies.

To get the cm. energies we use that
$$s=m_l^2+m_{\nu}^2+2(E_l E_{\nu}+P^2)=m_l^2+m_{\nu}^2+2 (E_l \sqrt{s}-m_1^2) \; \Rightarrow \; E_l=\frac{m_B^2+m_l^2-m_{\nu}^2}{2m_B}.$$
In the 2nd step we've used ##\sqrt{s}=E_1+E_2##. Exchanging the labels ##l## and ##\nu## in the above calculation gives
$$E_{\nu}=\frac{m_B^2+m_{\nu}^2-m_{l}^2}{2m_B} \neq E_l.$$
 
Last edited:
Many thanks.
 

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