Understanding the Relationship Between Ward Identity and Charge Conservation

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In summary, the conversation discusses the WT identity, which states that a gauge transformation on a vector boson does not contribute to physical amplitudes. This is equivalent to gauge invariance and conservation of charge. This identity is a reflection of the continuous symmetries present in the system and can be viewed as a restriction on correlation functions. It is similar to Noether's theorem for classical systems, which associates continuous symmetries with conserved charges.
  • #1
Bobhawke
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There are two things about this identity that I don't understand:

1. Why is it equivalent to a statement of charge conservation?
2. Wikipedia claims that it is like a quantum version of the classical noether's theorem. In what sense is this true?

Thanks
 
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  • #2
WT identity says (VERY roughly) that if you replace a polarization vector with a momentum then the amplitude vanishes.

Remembering that momentum = derivative, this is saying that if you do a gauge transformation on the vector boson, then the gauge transformation part does not contribute to physical amplitudes.

This is the same statement as gauge invariance.

This is the same statement as conservation of charge.
 
  • #3
A more general statement is that a Ward Identity is a reflection of the (continious) symmetries present in the system. You can, in some sense, view them as restrictions on the correlation functions.

Noether's theorem is a similar statement for classical systems. Furthermore, continious symmetries are associated with conserved charges (= Noether's theorem).

So, given a continuous symmetry of the system you can ask: what is the implication on the correlation functions, i.e. the physical observables? The answer is that they are restricted by the associated Ward identities.
 

Related to Understanding the Relationship Between Ward Identity and Charge Conservation

What is the Ward Takahashi identity?

The Ward Takahashi identity is a mathematical relation that connects the S-matrix elements of a quantum field theory. It is named after the physicists John Ward and Yasushi Takahashi, who independently discovered it in the 1950s.

Why is the Ward Takahashi identity important?

The Ward Takahashi identity is important because it is a fundamental symmetry in quantum field theory. It helps to ensure the consistency and validity of the theory by relating different physical quantities to each other.

How is the Ward Takahashi identity derived?

The Ward Takahashi identity is derived from the Noether's theorem, which states that for every continuous symmetry of a physical system, there exists a corresponding conserved quantity. In the case of the Ward Takahashi identity, the symmetry is the gauge symmetry of the theory, and the conserved quantity is the current associated with that symmetry.

What is the physical interpretation of the Ward Takahashi identity?

The Ward Takahashi identity can be interpreted as a statement of the conservation of electric charge in quantum field theory. It relates the scattering of particles with different electric charges to the exchange of gauge bosons, which carry the electric charge.

How is the Ward Takahashi identity used in practical applications?

The Ward Takahashi identity is used in various calculations in quantum field theory, such as in the perturbative expansion of scattering amplitudes. It is also used in the development of new theories and models, as it provides a powerful tool for analyzing and understanding the behavior of particles and their interactions.

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