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

In summary, the conversation discussed the factor in the matrix element amplitude for a two body decay process and how to evaluate it using the process kinematics. The mistake made was setting the energies of the particles equal, when in fact their magnitudes are equal. Correcting this mistake results in a different factor, as seen in references.
  • #1
Safinaz
259
8
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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  • #2
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:
  • #3
Many thanks.
 

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

1. What is the definition of "Kinematics of two body decay"?

Kinematics of two body decay is a branch of physics that studies the motion of two particles that are produced from the decay of a single parent particle. It focuses on the mathematical description of the particles' trajectory, velocity, and energy.

2. How is the momentum of the two particles related in a two body decay?

In a two body decay, the total momentum of the parent particle is equal to the sum of the momentums of the two daughter particles. This is known as conservation of momentum and is a fundamental principle of physics.

3. What is the difference between elastic and inelastic two body decay?

Elastic two body decay is a process in which the total kinetic energy of the particles after the decay is equal to the total kinetic energy of the parent particle. In contrast, inelastic two body decay is a process in which the total kinetic energy of the particles after the decay is less than the total kinetic energy of the parent particle.

4. How is the energy distribution of the daughter particles determined in a two body decay?

The energy distribution of the daughter particles in a two body decay is determined by the conservation of energy. This means that the total energy of the daughter particles must equal the total energy of the parent particle. The specific energy distribution depends on the masses of the particles and the type of decay.

5. Can the kinematics of two body decay be used to determine the properties of the parent particle?

Yes, the kinematics of two body decay can provide valuable information about the properties of the parent particle. By analyzing the trajectories, velocities, and energies of the daughter particles, physicists can infer the mass, spin, and other characteristics of the parent particle.

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