Every known boson and fermion has a corresponding anti-particle

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Discussion Overview

The discussion centers around the concept of antiparticles in particle physics, specifically addressing the claim that every known boson and fermion has a corresponding antiparticle, with a focus on the photon and its status as an antiparticle. Participants explore theoretical explanations and examples related to this topic.

Discussion Character

  • Exploratory
  • Technical explanation
  • Debate/contested

Main Points Raised

  • One participant asserts that every known boson and fermion has a corresponding antiparticle, claiming the photon is an exception.
  • Another participant counters that the photon is its own antiparticle, along with other electrically neutral particles like the Z-boson and neutral pion.
  • A participant provides a technical explanation involving charge conjugation and the transformation of the electromagnetic field, arguing that the photon must transform in a specific way to maintain invariance in interactions.
  • Discussion includes the complexity of electrically neutral particles with other types of charge, such as the neutral kaon, which cannot be its own antiparticle.
  • Some participants express confusion or lack of understanding regarding the technical details presented, indicating varying levels of expertise among contributors.
  • One participant references historical claims about antiphotons, noting that they were ultimately dismissed by the scientific community.

Areas of Agreement / Disagreement

Participants express disagreement regarding the status of the photon as an antiparticle, with some asserting it is its own antiparticle while others maintain it is an exception. The discussion remains unresolved with multiple competing views on the topic.

Contextual Notes

Participants reference various technical concepts such as charge conjugation and specific particle states, which may depend on definitions and theoretical frameworks that are not universally agreed upon.

Feeble Wonk
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Please take a moment to help enlighten a poor ignorant layperson. My understanding is that every known boson and fermion has a corresponding anti-particle, with the only exception being the photon. If true, can anyone explain WHY that that is?
 
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The photon is not an exception, it is its own antiparticle. Certain electrically neutral particles are also their own antiparticle, including the Z-boson and neutral pion.
 


fzero said:
The photon is not an exception, it is its own antiparticle. Certain electrically neutral particles are also their own antiparticle, including the Z-boson and neutral pion.

Got a link to something that explains this Fzero? Curious myself.
 


Drakkith said:
Got a link to something that explains this Fzero? Curious myself.

If we're just talking about the photon, there's a nice demonstration in Ch 10 of Weinberg V1. There he shows that the electric current transforms under charge conjugation as

[tex]C: \bar{\psi}\gamma^\mu \psi \rightarrow - \bar{\psi}\gamma^\mu \psi.[/tex]

You can work this out explicitly knowing how the Dirac spinor transforms under [tex]C[/tex]. Now, if we want [tex]C[/tex] to be a symmetric of QED (and it's known to be a symmetry of the classical theory), then the photon must transform as

[tex]C: A_\mu \rightarrow - A_\mu[/tex]

in order that the interaction term be invariant. Therefore the photon is its own antiparticle.

One could have already seen this from second-quantization, by noting that there's only one type of creation operator in the field expansion.

Things get more complicated if we're dealing with electrically neutral particles that have other types of charge. In particular, the neutral kaon has strangeness charge 1, so it cannot be it's own antiparticle. Instead there are mixed states of [tex]K^0[/tex] and [tex]\bar{K}^0[/tex] that are each their own antiparticle. The discussion on wikipedia is decent, but any particle physics text (such as Griffiths) would discuss this.
 


Heh, thanks Fzero. I have almost no idea what any of that means but that's ok. I'm not exactly studied up on that kind of math and such. =)
 


Charge conjugation, particle <-> antiparticle, reverses electric charge. To be consistent, the electromagnetic field must reverse sign. But aside from that, it stays the same as before.

Elementary fermions have antiparticles that are distinct from them. Their main bound states are mesons (quark-antiquark) and baryons (quark-quark-quark). Baryons have separate antibaryons, but mesons can be their own antiparticles. They will be that if they are flavor-neutral: flavor-antiflavor.

A neutral pion is ((up,antiup) - (down,antidown))/sqrt(2)
a mixed state

An eta meson is a mixture of ((up,antiup) + (down,antidown))/sqrt(2) and (strange,antistrange)

A J/psi meson is (charm,anticharm)

An upsilon meson is (bottom,antibottom)

Etc.
 


fzero said:
The photon is not an exception, it is its own antiparticle. Certain electrically neutral particles are also their own antiparticle, including the Z-boson and neutral pion.

There was a time a group of physicists found evidence pointing to the existence of antiphotons in their experiment. They refuted it to the point of calling it nonsense... http://www.economist.com/node/13226725?story_id=13226725 we have never found the existence of a fermionic majorana particle however.
 

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