Max Energy Λ in Σ0 Decay: Explained & Calculated

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Homework Help Overview

The discussion revolves around the decay of a Σ0 baryon into a Λ baryon and a photon, specifically focusing on the conditions that maximize the energy of the Λ after the decay. The problem involves relativistic kinematics and conservation laws, with participants exploring the implications of energy and momentum conservation in different reference frames.

Discussion Character

  • Exploratory, Conceptual clarification, Mathematical reasoning, Assumption checking

Approaches and Questions Raised

  • Participants discuss the conditions under which the Λ baryon carries maximum energy, questioning whether this occurs when the photon travels in opposite directions. They explore energy conservation equations and the implications of momentum conservation in both the rest frame of the Σ0 and the center of mass frame.

Discussion Status

There is an ongoing exploration of the relationships between the energies and momenta of the particles involved. Some participants suggest starting from conservation equations, while others express uncertainty about the conditions for maximum energy. Guidance has been offered regarding the need to express energies in terms of the baryon masses and to clarify the roles of momentum vectors.

Contextual Notes

Participants note the importance of the Σ0's initial energy of 2 GeV and its implications in the rest frame. There is also mention of the need to consider the massless nature of the photon in the context of energy and momentum relations.

Matt atkinson
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Homework Statement


A Σ0 baryon, traveling with an energy of 2 GeV, decays electromagnetically into a Λ and a photon.
What condition results in the Λ carrying the maximum possible energy after the decay? Sketch how the decay appears in this case, and calculate this energy. Explain your reasoning.
[Mass of Σ0 is 1.193 GeV/c2; mass of Λ is 1.116 GeV/c2]

Homework Equations


Relativistic kinematic equations;
CoM invariant mass

The Attempt at a Solution


So I am not sure on the condition for maximum energy of the Λ, is it when the photon is traveling with opposite momenta?
because the photon is a mass less particle it couldn't have 0 velocity right?
 
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What energy will the ##\Lambda## have in the rest frame of the ##\Sigma##?
 
So in the rest frame of the ##\Sigma##
The energy would be
$$E_{\Lambda}=E_{\Sigma^o}+p_{photon}c$$
Right?
Because if The ##\Sigma## decays at rest then the momenta of the ##\Lambda## and photon will be equal and opposite.
 
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What does energy and momentum conservation tell you?
 
If we are looking at the rest frame of the ##\Sigma## energy conservation gave me tee equation above and doesn't momentum conservation just tell me that;
$$0=p_{photon}-p_{\Lambda}$$
$$p_{photon}=p_{\Lambda}$$
 
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I was wondering should use that $$W^2=(\sum E)^2-(\sum p)^2$$
for both the lab frame of the ##\Sigma## and then the center of mass frame after the decay?

which gives
$$(E_{\Sigma^o})^2-(p_{\Sigma^o})^2=(E_{\Lambda}+E_{photon})^2-(p_{\Lambda}-p_{photon})^2$$
 
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Im not quite sure what the condition is to give the ##\Lambda## max energy.
 
What does ##(E_{\Sigma^o})^2-(p_{\Sigma^o})^2## evaluate to? What is the relation between the ##\Lambda## and photon energies and momenta?
 
So ##E_{\Sigma}^2-p_{\Sigma}^2=m_{\Sigma}^2##, as for the second question I'm not sure.
 
  • #10
How about what you just wrote down, but for the ##\Lambda## and for the photon instead?

Matt atkinson said:
If we are looking at the rest frame of the Σ\Sigma energy conservation gave me tee equation above


Your formula for energy conservation is a bit off and you should correct it.
 
  • #11
So for the photon and ##\Lambda##
$$(E_{\Lambda}+E_{photon})^2-(p_{\Lambda}+p_{photon})^2$$
And the Energy conservation should be ##E_{\Sigma}=E_{\Lambda}+p_{photon}c##
Right? And expanding the relation before you get;
$$E_{\Lambda}^2+p_{photon}^2+2E_{\Lambda}p_{photon} - p_{\lambda}^2-p_{photon}^2 -2p_{photon}p_{\Lambda}$$?
 
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  • #12
I suggest starting from just the conservation equations without squaring. The only interesting thing at the moment being: What is the energy of the ##\Lambda## in the rest frame of the decaying ##\Sigma##?
 
  • #13
So to consider the problem with the entire problem with everything in the rest frame of ##\Sigma^0##?
In which case if the energy of the ##\Lambda## is;
$$E_{\Lambda}=E_{\Sigma^0}-E_{photon}$$
and The momentum would be;
$$p_{\Sigma^0}=p_{\Lambda}+p_{photon}=0$$
Therefore;
$$p_{\Lambda}=-p_{photon}$$
Which would give;
$$E_{\Lambda}=E_{\Sigma^0}-p_{photon}=E_{\Sigma^0}+p_{\Lambda}$$
because photon has E=pc, so;
$$E_{\Lambda}-p_{\Lambda}=E_{\Sigma}$$
is that correct?
And does this mean that the condition for maximum energy is, to consider the ##\Lambda## in the rest frame with the electron traveling in the opposite direction?
 
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  • #14
I just don't understand where the ##2GeV## energy of the ##\Sigma## comes into it if, we are looking at the rest frame because in that frame it has 0 momentum and ##E_{\Sigma}=mc^2##
 
  • #15
Matt atkinson said:
So to consider the problem with the entire problem with everything in the rest frame of ##\Sigma^0##?
In which case if the energy of the ##\Lambda## is;
$$E_{\Lambda}=E_{\Sigma^0}-E_{photon}$$
and The momentum would be;
$$p_{\Sigma^0}=p_{\Lambda}+p_{photon}=0$$
Therefore;
$$p_{\Lambda}=-p_{photon}$$
This equation tells you that the ##\Lambda## and the photon have equal and opposite momenta.

Which would give;
$$E_{\Lambda}=E_{\Sigma^0}-p_{photon}=E_{\Sigma^0}+p_{\Lambda}$$
because photon has E=pc, so;
$$E_{\Lambda}-p_{\Lambda}=E_{\Sigma}$$
is that correct?
The signs are probably going to mess you up here. You should keep in mind that momentum is a vector, so it's really ##E_\gamma = \lvert p_\gamma \rvert## for the photon.

You need to somehow get rid of ##E_\gamma##, ##p_\gamma##, and ##p_\Lambda## because they're all unknowns. You want to solve for ##E_\Lambda## in terms of the masses of the ##\Lambda^0## and ##\Sigma^0##.
And does this mean that the condition for maximum energy is, to consider the ##\Lambda## in the rest frame with the electron traveling in the opposite direction?
I think you meant photon, not electron. As you found above, conservation of momentum requires that the ##\Lambda^0## and photon go in opposite directions in the rest frame, so no, it's not the condition for maximum energy.

As Orodruin has suggested, first solve for the energy of the ##\Lambda^0## in the rest frame of the ##\Sigma^0##. This may help give you insight into what the maximum energy condition is.
 
  • #16
Ah sorry yes I did mean photon not electron.
So when I'm using the fact that the photon has no mass, it should be E_{\gamma}=|p_{\gamma}| because ##E_{\gamma}^2=p_{\gamma}^2+0^2##, and as you said momentum is a vector so the energy isn't, so the energy is just the magnitude of the momentum vector.
Thank you both so much for your help, I managed to get the solution after a lot of work.
 

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