Time-ordering fermion operators

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SUMMARY

The discussion centers on the time-ordering of fermionic operators A and B, emphasizing the significance of the negative sign in the time-ordering operator T. When A precedes B, T(AB) results in -BA due to the anticommutation relations of fermionic operators, particularly in time-like separations. This negative sign is essential to maintain Lorentz invariance, as time-ordering must not alter the behavior of operators at space-like separations. The conversation clarifies that for local fermionic operators, the time-ordering operator does not affect the outcome when arguments are space-like separated.

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  • Understanding of fermionic operators and their properties
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Coriolis1
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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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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!
 

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