Special Relativity - energy-momentum conservation

rak576
Messages
2
Reaction score
0

Homework Statement



A positron of rest mass me, kinetic energy equal to its rest mass-energy, strikes an electron at rest. They annihilate, creating two high energy photons a and b. The photon a is emitted at the angle of 90 degress with respect to the direction of the incident positron.

(a) Split 4-vector law of energy-momentum conservation into energy and momentum conservation laws in the rest frame of the electron.

(b) Show that the total energy of the emitted photons Ea+Eb=3me*c^2 and that Eb^2 = Ea^2 + (p^2)*(c^2) where p is 3momentum of positron and Ea, Eb are energies of photons a and b.

(c) Use these results and identity E^2 = (p^2)*(c^2) + m0^2*c^4 to show Eb = 2me*c^2 and Ea = me*c^2. Find the direction of motion of photon b. In particular show that the angle between its direction and the direction of the positron is theta = arcsin(1/2)



Homework Equations





The Attempt at a Solution



Qp, Qe = 4momenta of positron and electron
Pa, Pb = 4momenta of photon a and b.

Qp = (2me*c, me*v) v=velocity of positron
Qe = (me*c, 0)
Pa = (Ea/c, Ea/c n) n=direction of photon
Pe = (Eb/c, Eb/c n)

This is far as I can get! Can anybody please help? Have I split up the conservation law okay?
Thanks
 
Physics news on Phys.org
A conservation law is usually represented as an equation. Here, a "split" would be to say

Momentum before = Momentum after
Energy before = Energy after

You have not done that.
 
Sorry, I didn't put that in.

Qp + Qe = Pa + Pb
 
That's only one equation. You need two plus you need to put in symbols for the rest masses, speed of positron, etc. in these two equations.
 
##|\Psi|^2=\frac{1}{\sqrt{\pi b^2}}\exp(\frac{-(x-x_0)^2}{b^2}).## ##\braket{x}=\frac{1}{\sqrt{\pi b^2}}\int_{-\infty}^{\infty}dx\,x\exp(-\frac{(x-x_0)^2}{b^2}).## ##y=x-x_0 \quad x=y+x_0 \quad dy=dx.## The boundaries remain infinite, I believe. ##\frac{1}{\sqrt{\pi b^2}}\int_{-\infty}^{\infty}dy(y+x_0)\exp(\frac{-y^2}{b^2}).## ##\frac{2}{\sqrt{\pi b^2}}\int_0^{\infty}dy\,y\exp(\frac{-y^2}{b^2})+\frac{2x_0}{\sqrt{\pi b^2}}\int_0^{\infty}dy\,\exp(-\frac{y^2}{b^2}).## I then resolved the two...
It's given a gas of particles all identical which has T fixed and spin S. Let's ##g(\epsilon)## the density of orbital states and ##g(\epsilon) = g_0## for ##\forall \epsilon \in [\epsilon_0, \epsilon_1]##, zero otherwise. How to compute the number of accessible quantum states of one particle? This is my attempt, and I suspect that is not good. Let S=0 and then bosons in a system. Simply, if we have the density of orbitals we have to integrate ##g(\epsilon)## and we have...
Back
Top