Can photons and antiphotons annihilate when they collide?

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In summary, the concept of antiphotons is not well-defined as photons are their own antiparticles. This is because they are eigenstates of the charge conjugation operator with an eigenvalue of -1. While photons can interact and annihilate with other particles, they cannot annihilate with each other unless they are traveling in different directions. This is due to the fact that their energies can be different depending on the reference system.
  • #1
Ranku
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Why is a photon considered to be its own antiparticle? What distinguishes a photon from an antiphoton? When photon and antiphoton collide do they annihilate?
 
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  • #2
I'm not very good at particle physics, but I think only charged particles can have an antiparticle. The neutron has an antiparticle, but it is made of different charged quarks.
 
  • #3
Actually, it would be more correct to say that antiphoton does not exist.
 
  • #4
Demystifier said:
Actually, it would be more correct to say that antiphoton does not exist.

So how do you define the antiparticle of a photon, if antiphoton doesn't exist? Which of the quantum numbers of a photon are 'opposite/different' in its antiparticle?
 
  • #5
Ranku said:
So how do you define the antiparticle of a photon, if antiphoton doesn't exist? Which of the quantum numbers of a photon are 'opposite/different' in its antiparticle?

Can't the same question be asked of any "force carrier" particle? Photons are (massless) carriers of the EM force, and are emitted when charge-carrying particle/antiparticle pairs annihilate. Gluons are the (also massless) carriers of the strong force, and are emitted when color-carrying particle/antiparticle pairs annihilate. So perhaps it is generally true that these massless carrier particles have no antiparticles? I guess that may be a bit ambiguous, since QCD requires 8 distinct kinds of gluons, and I guess none of them have ever been observed directly, but I have not read that they are generally organized into gluon-antigluon pairs.

Anyhow, what would be emitted in the annihilation of a putative photon-antiphoton pair? I mean, energy and momentum have to be conserved, right?

EDIT: so, to further qualify my own question, I know electron-positron pair production is possible if the photon energy is high enough ... I am trying to understand the general situation that would be valid at all photon energies.
 
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  • #6
Particles like the photon and the pi zero that are their own antiparticles are eigenstates of the charge conjugation multiplicative operator C. The photon has eigenvalue -1, and the pi zero has eignevalue +1.
 
  • #7
Meir Achuz said:
Particles like the photon and the pi zero that are their own antiparticles are eigenstates of the charge conjugation multiplicative operator C. The photon has eigenvalue -1, and the pi zero has eignevalue +1.

Ok, my understanding of QFT is far from comprehensive, so forgive me if this makes no sense, but if a photon is its own antiparticle, doesn't that mean that for a photon with and arbitrarily chosen set of properties (e.g. energy, wave-vector, polarization), there should be also exist a photon with the set of properties that would "annihilate" the original one? How can such a process conserve energy, if we ignore energies above the pair-production threshold? (I guess we can get momentum conservation if we choose counter-propagating wave-vectors.)

I guess this amounts to what the OP was asking in the first place ...
 
  • #8
Two photons can ( and do) annihilate into other particles in just the same way that an electron and a positron can.
 
  • #9
Meir Achuz said:
Two photons can ( and do) annihilate into other particles in just the same way that an electron and a positron can.

Fine ... but I can't find any qualitative descriptions of photon-photon annihilation at energies below 1 GeV or so. It seems that if photons have antiparticles and can undergo annihilation, there shouldn't be any energy restrictions on it. So what is the antiparticle of (say) a 532 nm green photon, and what particles are produced when they annihilate?

Again, I am just following my intuition here, so please forgive me if these are naive questions ...
 
  • #10
SpectraCat said:
Can't the same question be asked of any "force carrier" particle? Photons are (massless) carriers of the EM force, and are emitted when charge-carrying particle/antiparticle pairs annihilate. Gluons are the (also massless) carriers of the strong force, and are emitted when color-carrying particle/antiparticle pairs annihilate. So perhaps it is generally true that these massless carrier particles have no antiparticles? I guess that may be a bit ambiguous, since QCD requires 8 distinct kinds of gluons, and I guess none of them have ever been observed directly, but I have not read that they are generally organized into gluon-antigluon pairs.

The photon is different from the QCD gluons. As opposed to the photon those actually carry a nonzero charge with respect to the force they mediate. This is because their associated gauge group SU(3) is noncommutative. Their charges are denoted by e.g. "red-antigreen", "green-antiblue", and so on. Therefore they each have an antiparticle with the opposite colour charges. The charge of the antiparticle to the red-antigreen gluon would be green-antired.

Torquil
 
  • #11
Meir Achuz said:
Particles like the photon and the pi zero that are their own antiparticles are eigenstates of the charge conjugation multiplicative operator C. The photon has eigenvalue -1, and the pi zero has eignevalue +1.

From what I know of eigenstates, or rather energy eigenstates, is that they represent the states of a system that correspond to definite values of quantized energy. So does a photon and an antiphoton have different energies?
 
  • #12
They can have different energies, but note that this depends on the reference system.
The two photons can only anihilate if they do not travel exactly in the same direction. But then you can find a reference system where one is red shifted and the other one blue shifted so that their energies coincide and they impact head on. This is analogous to the scattering of massive particles in the laboratory frame vs the rest frame of the center of mass.
 
  • #13
They can have different energies, but note that this depends on the reference system.
The two photons can only anihilate if they do not travel exactly in the same direction. But then you can find a reference system where one is red shifted and the other one blue shifted so that their energies coincide and they impact head on. This is analogous to the scattering of massive particles in the laboratory frame vs the rest frame of the center of mass.
 
  • #14
DrDu said:
They can have different energies, but note that this depends on the reference system.
The two photons can only anihilate if they do not travel exactly in the same direction. But then you can find a reference system where one is red shifted and the other one blue shifted so that their energies coincide and they impact head on. This is analogous to the scattering of massive particles in the laboratory frame vs the rest frame of the center of mass.

Can you please describe such an annihilation experiment more fully, for the case of a low energy photon, such as a 532 nm photon propagating in the +x direction and plane polarized along the y-axis in some lab-fixed frame. What are the characteristics of the "antiphoton" corresponding to this particle, and what is emitted during the annihilation event to conserve energy?

I can't see how any other particles besides more photons could be emitted in this case, and in that case, how can you tell the difference between an annihilation event and a scattering event? Of course, I am not familiar with the full "menagerie" of sub-atomic particles ... are there other candidates for emission in such an annihilation?
 
  • #15
Ranku said:
From what I know of eigenstates, or rather energy eigenstates, is that they represent the states of a system that correspond to definite values of quantized energy. So does a photon and an antiphoton have different energies?

The concept of "eigenstate" also applies to other quantities besides energy. An energy eigenstate has a definite energy, but (in general) indefinite values of other physical quantities. An eigenstate of some other quantity has a definite value for that quantity, but (in general) indefinite values for other physical properties (including energy). Important exeption: if the operators for two quantities commute, then the system can be in a simultaneous eigenstate of both quantitles.
 
  • #16
SpectraCat said:
Can you please describe such an annihilation experiment more fully, for the case of a low energy photon, such as a 532 nm photon propagating in the +x direction and plane polarized along the y-axis in some lab-fixed frame. What are the characteristics of the "antiphoton" corresponding to this particle, and what is emitted during the annihilation event to conserve energy?

I can't see how any other particles besides more photons could be emitted in this case, and in that case, how can you tell the difference between an annihilation event and a scattering event? Of course, I am not familiar with the full "menagerie" of sub-atomic particles ... are there other candidates for emission in such an annihilation?

If they DID produce a scattering event: 1.) I'd wet myself before I died and, 2.) How does a packet of energy scatter into anything but more energy? Photons would have to scatter into a different EM quanta... so no, you are not suffering from a knowledge gap here.
 
  • #17
Two photons may anihilate e.g. into an electron and a positron. This requires at least two photons having 511 keV, the rest energy of the two electrons formed. I think the only anihilation process possible for visible light would be the production of a neutrino and an antineutrino which are nearly massless, which is a phantastically improbable.
 
  • #18
DrDu said:
Two photons may anihilate e.g. into an electron and a positron. This requires at least two photons having 511 keV, the rest energy of the two electrons formed. I think the only anihilation process possible for visible light would be the production of a neutrino and an antineutrino which are nearly massless, which is a phantastically improbable.

What would be the mechanism of this annihilation? It sounds more like spontaneous pair production. I'm confused.
 
  • #19
The anihilation of two photons with the formation of an electron and a positron is just the time reverse of the anihilation of an electron and a positron to form two gamma photons.
What else do you expect to happen in the anihilation process? The energy is conserved, so new particles have to be produced.
 
  • #20
DrDu said:
The anihilation of two photons with the formation of an electron and a positron is just the time reverse of the anihilation of an electron and a positron to form two gamma photons.
What else do you expect to happen in the anihilation process? The energy is conserved, so new particles have to be produced.

...And does this occur in nature?
 
  • #21
Frame Dragger said:
...And does this occur in nature?

Actually, yes ... it's a form of Compton scattering and it doesn't even require two photons ... a single photon with at least a 1.022 MeV energy can cause spontaneous pair production, if there is a massive body nearby to allow momentum conservation.

The two photon case is easier to think about ... basically any photon-photon interaction which has a) more than 1.022 MeV energy and b) conserves momentum (such as two counter propagating 511 keV gamma rays) has the potential to generate spontaneous pair production.

Krane's "Introductory Nuclear Physics" (Wiley, 1988) has a description of this on pp. 198-204, and I guess similar accounts can be found in other nuclear physics texts.

EDIT: fixed the unit error identified by Torquil in post #23
 
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  • #22
DrDu said:
Two photons may anihilate e.g. into an electron and a positron. This requires at least two photons having 511 keV, the rest energy of the two electrons formed. I think the only anihilation process possible for visible light would be the production of a neutrino and an antineutrino which are nearly massless, which is a phantastically improbable.


Ok .. I wondered about that .. I don't know much about neutrinos ... other than they are produced during beta decay (well, technically that's an anti-neutrino). Can they really be generated from this hypothetical low-energy photon-photon annihilation we are discussing? I have looked for a description of that in the literature, but with no luck so far.
 
  • #23
SpectraCat said:
The two photon case is easier to think about ... basically any photon-photon interaction which has a) more than 1.022 GeV energy and b) conserves momentum (such as two counter propagating 511 MeV gamma rays) has the potential to generate spontaneous pair production.

I think you meant 1.022MeV and 511keV

Torquil
 
  • #24
torquil said:
I think you meant 1.022MeV and 511keV

Torquil

Yep :redface: .. thanks .. I'll fix it.
 
  • #25
Hmmm, makes sense. I stand corrected.
 
  • #26
Dear SpectraCat,

I think that the neutrino-anti-neutrino production is the only process possible at least in principle which at least satisfies energy conversion. I think it would be a process in higher order in both the electromagnetic and the weak interaction, so that in fact there is no chance to observe it in the lifetime of the universe. E. g. in a first step, a virtual W^+ W^- pair could be formed, then both vector bosons decay into electron antielectron, neutrino and antineutrino and in a last step, the electron and antielectron anihilate the second photon, leaving the neutrino and anti-neutrino.
 

1. What is a photon and its antiparticle?

A photon is a fundamental particle of light, while its antiparticle is known as an antiphoton. They both have the same mass and spin, but have opposite electric charge.

2. How are photons and antiphotons created?

Photons and antiphotons can be created through various processes, such as particle-antiparticle annihilation or through certain nuclear reactions. They can also be created in high-energy collisions, such as those that occur in particle accelerators.

3. What are the properties of photons and antiphotons?

Photons and antiphotons have zero rest mass, travel at the speed of light, and do not experience the passage of time. They also have a wave-particle duality, meaning they can behave as both particles and waves.

4. How do photons and antiphotons interact with matter?

Photons and antiphotons can interact with matter through a process known as pair production, where they can create an electron-positron pair. They can also be absorbed or reflected by matter, depending on the properties of the material.

5. Can photons and antiphotons be used in practical applications?

Yes, photons and antiphotons have a wide range of practical applications, such as in telecommunications, solar panels, and medical imaging. They are also being studied for use in quantum computing and encryption.

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