Conservation of momentum and HUP in PET

In summary: V gamma rays. Momentum conservation requires that the two gamma ray photons are emitted in opposite directions from the point of annihilation. Positron emission tomography exploits the fact that the detection of two oppositely-directed gamma rays defines a line on which the point of annihilation occurs."In summary, during positron emission, the combined mass of the electron-positron pair is converted into energy in the form of two gamma rays. These gamma rays are emitted in opposite directions from the point of annihilation, allowing for precise detection and localization of this point. This principle is utilized in medical imaging techniques such
  • #1
El Hombre Invisible
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"When a positron emitted in beta+ decay annihilates with an electron, the combined mass of the two particles, m = 2me, is converted into an amount of energy 2mec^2 in the form of two 511 keV gamma rays. Momentum conservation requires that the two gamma ray photons are emitted in opposite directions from the point of annihilation. Positron emission tomography exploits the fact that the detection of two oppositely-directed gamma rays defines a line on which the point of annihilation occurs."

I haven't put this in college homework because this was just a side note in my textbook and is not something I imagine I will get asked about. As such, I imagine there are some details skimmed over. What these are will hopefully get cleared up with answers to the following questions. I'm an undergrad, and we've only studied QM to a relatively low level, so please don't baffle me with stuff there's no chance I'll understand. :cry:

1. If the total momentum of the photons MUST be zero, then the total momentum of the electron-positron pair must also be zero. Why do such pairs only annihilate when they have equal and opposite momenta? What would happen if an electron and positron met with unequal momenta, either in magnitude or direction?

2. If the total momentum of the pair must be equal and opposite, and we can determine the position of annihilation from the trajectories of the photons, where is the uncertainty?

3. Presupposing an answer to the last question, I assume that proximity, and so precise position, is not an issue for pair annihilation, and that maybe the pair will annihilate if they are in the same quantum state. If so, what is the meaning of the point of annihilation?

Thanks to all in advance.
 
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  • #2
El Hombre Invisible said:
1. If the total momentum of the photons MUST be zero, then the total momentum of the electron-positron pair must also be zero. Why do such pairs only annihilate when they have equal and opposite momenta? What would happen if an electron and positron met with unequal momenta, either in magnitude or direction?

No, this simply means that you should (for your own easiness) work in the center of gravity of the the electron-positron pair. You can always find such a center of gravity reference frame, and all that is written applies in THAT COG.

2. If the total momentum of the pair must be equal and opposite, and we can determine the position of annihilation from the trajectories of the photons, where is the uncertainty?

Your detector is not necessarily in that COG frame ! The uncertainty resides in the uncertainty in what is the COG frame. You could only work it backwards from your photon detections if you knew perfectly the momentum AND impact positions ; but you can't because of the HUP, so you have an intrinsic uncertainty in this calculating back of the COG frame.


3. Presupposing an answer to the last question, I assume that proximity, and so precise position, is not an issue for pair annihilation, and that maybe the pair will annihilate if they are in the same quantum state. If so, what is the meaning of the point of annihilation?

See answer to 2.

cheers,
Patrick.
 
  • #3
vanesch said:
No, this simply means that you should (for your own easiness) work in the center of gravity of the the electron-positron pair. You can always find such a center of gravity reference frame, and all that is written applies in THAT COG.

Your detector is not necessarily in that COG frame ! The uncertainty resides in the uncertainty in what is the COG frame. You could only work it backwards from your photon detections if you knew perfectly the momentum AND impact positions ; but you can't because of the HUP, so you have an intrinsic uncertainty in this calculating back of the COG frame.
Hi Patrick. Thanks for the response.

If I follow you correctly (doubtful :smile: ), then what you're saying is that in a reference frame chosen such that the centre of gravity of the electron-positron pair is at rest, the momenta of each will be equal and opposite. That, I dig.

But momentum is conserved within a frame of reference. Surely then if the apparatus is set up such that the COG is not at rest in its frame (and this is by far the most likely situation), then the total momenta of the pair will not be zero. As such, the total momenta of the photon pair should not be zero.

The above looks like an argument but it's really a question. I can follow how you can choose your frame such that the COG is at rest, but the only frame of any import I see is the frame of the apparatus.
 
  • #4
El Hombre Invisible said:
But momentum is conserved within a frame of reference. Surely then if the apparatus is set up such that the COG is not at rest in its frame (and this is by far the most likely situation), then the total momenta of the pair will not be zero. As such, the total momenta of the photon pair should not be zero.

That's correct. And they will thus not be back-to-back either.

The above looks like an argument but it's really a question. I can follow how you can choose your frame such that the COG is at rest, but the only frame of any import I see is the frame of the apparatus.

Exactly, and in that frame of the apparatus (the lab frame, say) the momenta are not exactly back-to-back.
 
  • #5
vanesch said:
That's correct. And they will thus not be back-to-back either.

Exactly, and in that frame of the apparatus (the lab frame, say) the momenta are not exactly back-to-back.
Ahhh, I see. So what you're saying is the momenta of the photon pair are not likely to be exactly equal and opposite, but close enough to pin the point of annihilation down with some uncertainty?
 
  • #6
El Hombre Invisible said:
"When a positron emitted in beta+ decay annihilates with an electron, the combined mass of the two particles, m = 2me, is converted into an amount of energy 2mec^2 in the form of two 511 keV gamma rays. Momentum conservation requires that the two gamma ray photons are emitted in opposite directions from the point of annihilation. Positron emission tomography exploits the fact that the detection of two oppositely-directed gamma rays defines a line on which the point of annihilation occurs."

1. If the total momentum of the photons MUST be zero, then the total momentum of the electron-positron pair must also be zero. Why do such pairs only annihilate when they have equal and opposite momenta? What would happen if an electron and positron met with unequal momenta, either in magnitude or direction?

It looks like you've read a little too deeply into the question and inserted things that aren't there.

Total momentum doesn't need to be 0...it just needs to be conserved. Positrons carry some amount of kinetic energy when emitted. Usually by the time a positron interacts with an electron, much of it's initial energy has been lost through collisions and interactions and it ends up with 0 or very little energy. The annihilation photons get emitted 180° to each other.

When the positron annihilates with an electron before losing a substantial fraction of it's energy, then conservation of momentum still requires the annihilation photons be emitted in opposite directions, but the angle becomes less than 180° Whatever momentum the positron had prior to annihilation is converted to the photons' momentum.
 
  • #7
imabug, ur2l8. Patrick had it covered, thanks, and with less dubious presumptions. My suspicion that the text was oversimplifying for succintness was correct, but the issue was confused by a poster on an earlier thread I've been on stating that the total momentum of an annihilating pair had to be zero. I thought that was wrong, but when I read the quoted text I started doubting my sanity.

Anyway, I'm done here. Thanks again for the help. :smile:
 

1. What is the conservation of momentum in PET?

The conservation of momentum in PET (Positron Emission Tomography) refers to the fundamental law of physics that states that the total momentum of a system remains constant, unless an external force acts upon it. In PET, this principle is applied to the detection of positrons emitted from radioactive tracers in the body, allowing for the creation of 3D images of biological processes.

2. How does the HUP (Heisenberg Uncertainty Principle) relate to PET?

The HUP, a principle in quantum mechanics, states that the more precisely we know the position of a particle, the less precisely we can know its momentum, and vice versa. This is important in PET because the detection of positrons relies on measuring their position and momentum simultaneously, and the HUP sets a limit on how precisely we can do so.

3. Can the conservation of momentum and HUP be violated in PET?

No, the conservation of momentum and HUP are fundamental laws of physics and cannot be violated. PET technology and techniques are designed to work within the boundaries of these principles.

4. How are the conservation of momentum and HUP used in PET imaging?

In PET imaging, the conservation of momentum is used to accurately detect the positrons emitted from the radioactive tracers in the body. The HUP is used to determine the position and momentum of the positrons, which are then used to create 3D images of the biological processes in the body.

5. Are the conservation of momentum and HUP important in other medical imaging techniques?

Yes, the conservation of momentum and HUP play important roles in other medical imaging techniques such as MRI and CT scans. These principles are essential for accurately detecting and creating images of biological processes in the body.

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