Charge Conjugate of the Vacuum

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SUMMARY

The charge conjugation operator, denoted as C, acts on the vacuum state |0⟩ such that C|0⟩ = |0⟩ in theories with charge conjugation invariance. This indicates that the vacuum possesses even charge parity. The discussion clarifies that creation and annihilation operators for particles and antiparticles are distinct, with C swapping these operators. The conclusion emphasizes that while the vacuum's charge parity can be defined as even, it is ultimately a matter of convention, as no observable difference arises from assuming an odd charge parity vacuum state.

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  • Understanding of quantum field theory concepts, specifically vacuum states.
  • Familiarity with creation and annihilation operators in particle physics.
  • Knowledge of charge conjugation invariance and its implications.
  • Basic grasp of particle-antiparticle relationships in quantum mechanics.
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  • Study the implications of charge conjugation invariance in quantum field theories.
  • Explore the role of creation and annihilation operators in quantum field theory.
  • Investigate the concept of charge parity and its significance in particle physics.
  • Learn about the distinctions between particles and antiparticles in various quantum theories.
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Quantum physicists, theoretical physicists, and students of quantum field theory seeking to deepen their understanding of charge conjugation and vacuum states.

ChrisVer
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What is the result of the charge conjugation acting on the state of vacuum?
C|0>=...
I have two intuitive problems... If I see the vacuum as something which has no particles, then the charge conjugate would have to lead in the vacuum itself...

C|0>=|0>

However, if I think of the vacuum as the state on which creation operators act to create states, the above result doesn't seem correct. For example I would guess that the C acting on the vacuum would create a new vacuum:

C|0>=|\bar{0}>
On which now the creation operators will act destructively (because they would have to create particle in the antiparticle vacuum- the exact opposite of destruction operator acting on the initial vacuum)... On the other hand the destruction operators will bring out antiparticle states...

I am seeing the creation operators as particles and destruction operators as antiparticles, since they propagate (in momentum space) to opposite directions...

Which is correct (I already know it's the 1st) and more importantly, why?
 
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C|0> = |0> in a theory with charge conjugation invariance.

I think maybe you are a little confused about creation/annihilation operators and particles/antiparticles. There are separate creation/annihilation operators for particles and antiparticles. C swaps the particle creation operators with the antiparticle creation operators, and similarly for the annihilation operators. |0> is annihilated by both particle and antiparticle annihilation operators.

For example, let ##a^\dagger## create particles and ##b^\dagger## create antiparticles. The charge conjugation operator obeys ##C a^\dagger C = b^\dagger## and ##C b^\dagger C = a^\dagger## and ##CC = 1##. Then if we act on a state of a single particle with ##C##, we get a state of one antiparticle, as expected:

##C a^\dagger | 0 \rangle = C a^\dagger CC | 0 \rangle = b^\dagger C | 0 \rangle = b^\dagger |0\rangle##.

Note that we used the fact that ##C|0\rangle = |0\rangle##.
 
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The_Duck said:
C|0> = |0> in a theory with charge conjugation invariance.
Yes, bearing this in mind...

Jauch and Rohrlich said:
C|0> = |0> states that the charge parity of the vacuum is even. This is consistent with the definition of the vacuum state, but it is an arbitrary convention. We could just as well assume a vacuum state of odd charge parity. Then the charge parity of all other states would be reversed. There is no observable difference between the two assumptions.
 

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