Every known boson and fermion has a corresponding anti-particle

In summary, every known boson and fermion has an antiparticle, except for the photon which is its own antiparticle. This is due to the way the electric current transforms under charge conjugation. Certain electrically neutral particles, such as the Z-boson and neutral pion, are also their own antiparticle. However, for particles with other types of charge, such as the neutral kaon, there are mixed states that are each their own antiparticle. While there was some initial speculation about the existence of antiphotons, it has not been confirmed. Additionally, there has never been evidence for the existence of a fermionic majorana particle.
  • #1
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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  • #2


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.
 
  • #3


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.
 
  • #4


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.
 
  • #5


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. =)
 
  • #6


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.
 
  • #7


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.
 

FAQ: Every known boson and fermion has a corresponding anti-particle

What is a boson and fermion?

A boson and fermion are two types of subatomic particles that make up the basic building blocks of matter. Bosons are particles that have integer spin, while fermions have half-integer spin.

What is an anti-particle?

An anti-particle is a particle with the same mass but opposite charge as its corresponding particle. For example, the anti-particle of an electron is a positron, which has the same mass as an electron but a positive charge.

Why do bosons and fermions have corresponding anti-particles?

This is due to the laws of quantum mechanics, which state that every particle has an anti-particle with opposite charge. This allows for the conservation of certain properties, such as electric charge, in particle interactions.

Can anti-particles be created or destroyed?

Yes, anti-particles can be created or destroyed through particle interactions. When a particle and its corresponding anti-particle collide, they can annihilate each other and release energy in the form of photons.

What is the significance of this concept in particle physics?

The existence of anti-particles plays a crucial role in our understanding of the fundamental forces and interactions in the universe. It also has practical applications in fields such as medical imaging and particle accelerators.

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