Time-ordering fermion operators

In summary, the standard definition of T(AB) for fermionic operators involves a negative sign in the case of A and B being time-like separated. This is for convenience and is consistent with the anticommutator relations for space-like separated arguments. This is necessary for preserving Lorentz invariance and ensuring that the time-ordering symbol has no effect on operators at space-like separated arguments.
  • #1
Coriolis1
2
0
If A and B are fermionic operators, and T the time-ordering operator, then the standard definition is

T(AB) = AB, if B precedes A
= - BA, if A precedes B.

Why is there a negative sign? If A and B are space-like separated then it makes sense to assume that A and B anticommute. But if they are time-like separated we don't know if
they anticommute. What am I missing?
 
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  • #2
For time-like separation of arguments it's just for convenience, and this is indeed consistent with exactly what you mention concerning anticommutator relations for space-like separated arguments (where you can always find a reference frame, where the time arguments are equal and thus the canonical equal-time anti-commutation relations for fermion fields are valied): For local fermionic operators that anticommute (particularly those at space-like separated arguments) the time-ordering shouldn't do anything. If you define it otherwise, you get into trouble with Lorentz invariance, because only for time-like separated events (space-time points in Minkowski space) the time ordering is frame-independent. So T must do nothing for operators at space-like separated arguments, and for fermionic operators it means you must have this additional minus sign in the definition of the time-ordering symbol, because fermionic operators anti-commute rather than commute. For the same reason there must not be any sign in the bosonic case!
 

1. What are time-ordering fermion operators?

Time-ordering fermion operators are mathematical operators used in quantum field theory to describe the behavior of fermions (particles with half-integer spin). They represent the order in which fermion fields are created or destroyed in a quantum system over a period of time.

2. How are time-ordering fermion operators different from bosonic operators?

Time-ordering fermion operators differ from bosonic operators in that they follow the anti-commutation rule, while bosonic operators follow the commutation rule. This means that the order in which fermion operators are multiplied matters, while for bosonic operators, the order does not matter.

3. What is the significance of using time-ordering fermion operators?

Time-ordering fermion operators are significant because they allow us to accurately describe the behavior of fermions in a quantum system. They help us understand the interactions between fermions and their environment over a period of time, and are crucial in calculating measurable quantities such as particle scattering amplitudes.

4. Are there any limitations to using time-ordering fermion operators?

Yes, there are limitations to using time-ordering fermion operators. They are only applicable to systems in which fermions are the dominant particles, and cannot be used to describe systems with a mix of fermions and bosons. Additionally, they are not valid in systems with strong interactions, where other techniques such as perturbation theory must be used.

5. How are time-ordering fermion operators related to Feynman diagrams?

Time-ordering fermion operators are used to simplify the calculation of Feynman diagrams, which are graphical representations of particle interactions in quantum field theory. The fermion operators help to keep track of the order of interactions in a system, which is crucial in constructing and interpreting Feynman diagrams.

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