How Does Photon Energy Relate to Mass Loss in Particle Decay?

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vladimir69
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Homework Statement


Set the speed of light c=1.
A particle of rest mass [itex]m_{0}[/itex] decays at rest into a photon and loses rest mass [itex]\delta[/itex] in the bargain. Show that the photon energy is [itex]\omega=\delta(1- \frac{\delta}{2m_{0}})[/itex] in the particle's rest frame before the decay.

Homework Equations


[tex]\mathbf{K}=(\omega,k)[/tex] is the photon momentum
[tex]\mathbf{P_{1}}=(m_{0},0)[/tex] is the initial momentum of the particle
[tex]\mathbf{P_{2}}=(\gamma(m_{0}-\delta),\gamma(m_{0}-\delta)v)[/tex] is the final momentum of the particle

initial momentum = final momentum
"dot" product invariant
[tex](a,b) \cdot (x,y) = ax-by[/tex]

The Attempt at a Solution


Firstly conservation of momentum
[tex]\mathbf{P_{1}}=\mathbf{P_{2}}+\mathbf{K}[/tex]
[tex]\mathbf{P_{1}}\cdot \mathbf{P_{1}} = \mathbf{P_{2}} \cdot \mathbf{P_{2}} +2\mathbf{K}\cdot\mathbf{P_{2}}[/tex]
The first equation gives us
[tex]m_{0} = \gamma(m_{0}-\delta) +\omega[/tex]
[tex]0= \gamma(m_{0}-\delta)v + k[/tex]
The second equation gives us
[tex]m_{0}^2=(m_{0}-\delta)^2+2(\omega\gamma(m_{0}-\delta)-kv\gamma(m_{0}-\delta))[/tex]
Stirring all these into the mixing pot and going on an algebraic safari out pops
[tex]\omega=\delta[/tex] which of course is wrong

But just where did I go wrong?

Isn't it true that [itex]\omega-k=0[/itex] in a world of just 1 spatial dimension and 1 dimension of time?
 
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hi vladimir69! :smile:

(have an omega: ω and a delta: δ :wink:)
vladimir69 said:
Set the speed of light c=1.
A particle of rest mass [itex]m_{0}[/itex] decays at rest into a photon and loses rest mass [itex]\delta[/itex] in the bargain. Show that the photon energy is [itex]\omega=\delta(1- \frac{\delta}{2m_{0}})[/itex] in the particle's rest frame before the decay.

hmm … do you really think this particle is going to move at a relativistic speed? :wink:

try it without the relativity (and yes, ω = |k|) :smile:
 
I thought this question must use relativistic principles since it was asked in the special relativity chapter.
The solution does it as
[tex] \mathbf{P_{2}}=\mathbf{P_{1}}-\mathbf{K}[/tex]
[tex] \mathbf{P_{2}}^2=\mathbf{P_{1}}^2-2\mathbf{KP_{1}}[/tex]
[tex](m_{0}-\delta)^2=m_{0}^2-2m_{0}\omega[/tex]
Solving for omega reveals the correct result, just wondering why my method didn't work