Graduate Time-ordering fermion operators

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The time-ordering operator T for fermionic operators A and B is defined such that T(AB) equals AB if B precedes A and -BA if A precedes B, with the negative sign arising from the anticommutation of fermionic operators. For space-like separated operators, T does not alter the product due to their anticommutative nature, which is consistent with local fermionic operator relations. In contrast, for time-like separated operators, the time-ordering is necessary to maintain Lorentz invariance, as it ensures frame independence. The inclusion of the negative sign is crucial for fermionic operators, while bosonic operators do not require such a sign due to their commutative properties. This distinction highlights the fundamental differences in the behavior of fermions and bosons under time-ordering in quantum field theory.
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!
 
Time reversal invariant Hamiltonians must satisfy ##[H,\Theta]=0## where ##\Theta## is time reversal operator. However, in some texts (for example see Many-body Quantum Theory in Condensed Matter Physics an introduction, HENRIK BRUUS and KARSTEN FLENSBERG, Corrected version: 14 January 2016, section 7.1.4) the time reversal invariant condition is introduced as ##H=H^*##. How these two conditions are identical?

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