Meir Achuz said:
2. A single gamma cannot-->e-p. It is forbidden by E and p conservation.
Pair production usually occurs in the electric field of a nearby nucleus.
QUOTE]
Your answer contradicts an earlier reply, who is right?
Also, I don't see why a single gamma -->e-p violates any law of conservation. The only conservation law I can think of is the conservation of lepton # which appears to be preserved by virtue of the e-p pair. Please explain your comment.
Meir Achuz is right. I think that Kvantti meant his comment is in the context of a bubble chamber where there is stuff available to carry off the excess energy. But then it wouldn't really be a single gamma ray turning into an electron and a positron, it would have something else involved.
A single gamma can't go to an e and p because it can never have enough energy to pay for the masses of the electron and proton (after balancing conservation of momentum). Another way of saying the same thing is that the photon always has too much momentum for the electron and positron to conserve momentum (assuming that the energies balance). Yet another way of saying this is that if you want to get the best rocket ship drive, use photons because they have the highest possible ratio of momentum to energy. Maybe one of these will help you remember it, if not, make up your own.
Here is the calculation, assume the photon travels in the +z direction:
Gamma ray energy-momentum 4-vector:
[tex](E_{\gamma},0,0,P_{\gamma})[/tex]
First electron 4-vector:
[tex](E_1,Px,Py,Pz)[/tex]
Second electron 4-vector (to get energy and momentum to add up):
[tex](E_\gamma - E_1,-Px,-Py,P_\gamma-Pz)[/tex]
Now if that were all there is to it, then sure, you could do the deed. (And in fact, you could if these were virtual particles that you will learn about much later in your career.) But that's not all there is to it. The particles have masses and the masses satisfy an equation like the following (forgive me, it's been 20 years so I could easily have a sign wrong):
[tex]E_\gamma^2 = P_\gamma^2c^2[/tex]
[tex]E_1^2 = (Px^2 + Py^2 + Pz^2)c^2 - m^2c^4[/tex]
[tex](E_\gamma-E_1)^2 = (Px^2 + Py^2 + (P_\gamma-Pz)^2)c^2 - m^2c^4[/tex]
where m is the mass of an electron = mass of a positron.
If you subtract the third equation from the second one you get:
[tex]E_\gamma^2 -2E_1\;E_\gamma = (P_\gamma^2 -2Pz\;P_\gamma)c^2[/tex]
Taking into account the first equation gives you:
[tex]E_1 = Pz\;c[/tex]
Squaring this and subtracting from the 2nd equation, you get three non negative terms on the right and zero on the left. Therefore the three non negative terms, [tex]Px\;c, Py\;c, m^2c^4[/tex] must all be zero. But [tex]m^2c^4[/tex] cannot be zero.
From this, you see that if one massless particle decays into two particles, the two created particles have to be both massless and they both have to have the same momentum. In other words, they have to travel on a path just like the original massless particle. And if all the interesting quantum numbers are conserved, how could you know that a decay took place?
Carl