Kinetic Energies of Neutron and Pion After Lambda Hyperon Decay?

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Homework Help Overview

The problem involves the decay of a lambda hyperon (\Lambda^{0}) at rest into a neutron and a pion, with the goal of determining the kinetic energies of the resulting particles in the lab frame. The subject area includes particle physics and conservation laws.

Discussion Character

  • Exploratory, Conceptual clarification, Mathematical reasoning

Approaches and Questions Raised

  • Participants discuss the use of conservation of energy and momentum equations, questioning the relevance of certain equations and the inclusion of particle masses. There is an exploration of how to express the problem in terms of one variable to simplify the equations.

Discussion Status

The discussion is ongoing, with participants providing guidance on focusing the equations and suggesting alternative approaches to solve for the unknowns. There is a recognition of the complexity involved in the algebraic manipulation required to find a solution.

Contextual Notes

Participants note the challenge of working with multiple unknowns and the need to derive equations that relate the kinetic energies of the decay products without directly solving for them initially. There is an emphasis on ensuring that all relevant masses are included in the equations.

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Homework Statement


A lambda hyperon \Lambda^{0} (mass = 1115.7 MeV/c^2) at rest in the lab frame decays into a neutron n (mass = 939.6 MeV/c^2) and a pion \pi^{0}: \Lambda^{0} \rightarrow n + \pi^{0}

What are the kinetic energies (in the lab frame) of the neutron and pion after the decay?


Homework Equations


KE = m c^{2} - m_{0} c^{2} = m_{0} c^{2} (\gamma - 1)
Conservation of Momentum: p_{n} = - p_{\pi}
p = \gamma m v


The Attempt at a Solution



Using the relevant equations, there are two equations and two unknowns (v_{n} and v_{\pi}). However, all my algebra attempts failed here. Any ideas? Is the above what I should be starting with?
 
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Your first "relevant equation" isn't particularly relevant.

Note that the pion and proton masses aren't anywhere in your equations. Does this seem right to you?
 
Last edited:
Vanadium 50 said:
Your first "relevant equation" isn't particularly relevant.

Note that the pion and proton masses aren't anywhere in your equations. Does this seem right to you?

I suppose I should've filled in more what I implied by the first equation.
E_{i}= E_{f}

E_{i}= m_{\Lambda} c^{2}

E_{f}= \gamma_{n} m_{n} c^{2} + \gamma_{\pi} m_{\pi} c^{2}

for the first equation, conservation of energy.

And

\gamma_{n} m_{n} v_{n} = - \gamma_{\pi} m_{\pi} v_{\pi}

for the conservation of momentum. Those are the two equations and two unknowns I used, where

\gamma_{i} = \left( \sqrt{1- (\frac{v_{i}}{c})^{2} } \right) ^{-1}
 
The gammas aren't helping. You might want to find an equation without them.
 
Or rather...the gammas aren't helping right away.

You need to start by getting one equation in one unknown. What would be the most useful thing to solve for? Hint: it's common to both decay particles.
 
Ah, right. Good ol' E^2 = p^2 c^2 + m_{i}^{2} c^4 The momentums are equal so can set both p's to be the same, we know the initial energy, we know the masses, solve for momentum, etc...

Not pretty math, but it works out.

Thanks Vanadium 50.
 

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